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Evaluation of Shear Strength of High Strength Concrete Beams Submitted by Attaullah Shah Department of Civil Engineering University of Engineering & Technology Taxila-Pakistan June 2009

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Page 1: Evaluation of Shear Strength of High Strength Concrete Beamsprr.hec.gov.pk/jspui/bitstream/123456789/1796/1/909S.pdf · 2018-07-23 · taking lunch with the Concrete and Structure

Evaluation of Shear Strength of High

Strength Concrete Beams

Submitted by

Attaullah Shah

Department of Civil Engineering

University of Engineering & Technology

Taxila-Pakistan

June 2009

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Evaluation of Shear Strength of High

Strength Concrete Beams

Submitted by

Attaullah Shah (Registration No.01/UET/PhD/CE-02)

This thesis is submitted in partial fulfillment of the requirements for the PhD Civil Engineering

PhD Supervisor

Prof Dr. Saeed Ahmad

Department of Civil Engineering

University of Engineering & Technology

Taxila-Pakistan

June 2009

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Abstract

In this thesis, the shear properties of High Strength Reinforced Concrete (HSRC)

beams have been investigated on the basis of available research data and

experimental work at Structural Laboratories of University of Engineering and

Technology Taxila-Pakistan. The shear capacity of High Strength Reinforced

Concrete (HSRC) beams is relatively less investigated in the contemporary

research, as most of the research data available is based on the results from

normal strength reinforced concrete with compressive strength of 40MPa or less.

There is a general consensus amongst the researchers in the field of Structural

Engineering and Concrete Technology that the shear strength of HSRC beams,

unlike the Normal Strength Reinforced Concrete (NSRC) does not increase, in

the same proportion as the increase in the compressive strength of concrete, due

to brittle behaviour of the High Strength Concrete. Hence the current empirical

equations proposed by most of the building and bridges codes for shear strength

of HSRC beams are less conservative as compared to the Normal Strength

Reinforced Concrete (NSRC) beams. This major observation by the researchers

is the main focus of this research.

An extensive literature review of the shear properties of Normal Strength

Reinforced Concrete (NSRC) beams and High Strength Reinforced Concrete

(HSRC) beams was undertaken. Additionally the shear strength of disturbed

region (D-Region) was also studied. In disturbed region the ordinary beams

theory based on Bernoulli’s theorem is not applicable. In the literature review of

disturbed regions special emphasis was laid over Strut and Tie Model (STM),

which is an emerging analysis and design tool in the current research in

reinforced concrete.

The literature review was followed by the experimental work, which comprised of

70 high strength reinforced concrete beams and 9 two ways high strength

concrete cobles. Beams were cast in two sets of 35 beams each, one set without

web reinforcement and other with web reinforcement. For each set of 35 beams

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five values of longitudinal reinforcement and seven values of shear span to depth

ratio were selected to mainly study the behaviour of slender beams, where

typical shear failure can be anticipated. These beams were tested under

monotonic load at the mid span to examine the contribution of various

parameters like longitudinal steel, shear span to depth ratio, and web

reinforcement, on the shear capacity of HSRC beams. It has been observed that

the shear strength of beams has been increased with the increase in longitudinal

steel and shear reinforcement but it has reduced with the increase in the shear

span to depth ratio. The beams with low longitudinal steel ratio and no web

reinforcement failed mainly due to shear flexure cracks. However the beams with

longitudinal steel ratio of 1% and more failed mainly due to beam action in shear

tension failure. The beams with small shear span to depth ratio and large values

of longitudinal steel ratio however failed due to shear compression failure.

The shear failure of HSC beams with large values of longitudinal steel and shear

span to depth ratio was however more sudden and brittle, giving no sufficient

warning before failure, which has been observed as serious phenomena in the

shear failure of HSC beams.

The addition of web reinforcement increased the shear strength of all beams

tested. The failure mode was also affected. The obvious contribution of the

minimum web reinforcement was avoiding the sudden failure of the HSC beams.

These test results were also compared with the equations of some international

building and bridges codes and methods for shear strength of HSRC beams. It

has been noticed that these equations do not provide equal level of safety in the

shear design of HSRC beams. Some of the codes are over conservative, while

few others are less conservative for the shear design of HSRC beams.

Comparison of the observed shear strength of tested HSRC beams with the

results of the codes equations used, reveal that most of these equations are less

conservative for shear design of HSRC beams at lower values of longitudinal

steel for both cases of beams with and without web reinforcement, particularly for

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longitudinal steel ratio less than1%. Hence additional care may be required for

shear design of HSRC beams at large values of shear span to depth ratios.

To analyze the behaviour of typical disturbed region in concrete structures, the

basic rationale of Strut and Tie Model (STM) was used for the analysis and

design of two way corbels. These corbels were tested under monotonic loads

applied at the overhanging portion of the corbels. The actual shear capacities of

these corbels were compared with the theoretical shear capacities of the corbels

worked out with the STM. The actual and theoretical values of the shear were

falling close to each other. Their comparison reveals that STM can be further

tested as more simple and reliable tool for analysis and design of disturbed

region (D-Region) in concrete structures, through more experimental research.

Further research work on shear properties of HSRC beams with higher values of

compressive strength of concrete in the beam region and more experimental

research on the disturbed region including pile caps, deep beams, dapped ended

beams and corbels has been recommended at Engineering University-Taxila

Pakistan.

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Acknowledgement

The higher study has been both my ambition and dream since my graduation but

the job and family commitments always impeded to realize it. The historic

decision of Higher Education Commission (HEC)-Pakistan, to strengthen the

Universities in Pakistan and taking initiatives for promoting research, ushered a

new era of innovation and higher education in Universities and institutes of higher

learning. I was offered PhD admission both from UET Peshawar and UET Taxila

at the same time but I preferred the later as it is closely located to my place of

job.

PhD studies at UET Taxila-Pakistan, had been an enterprising experience of my

life which transformed me from a predominantly Servicing officer into an

academician with more thirst for learning, innovation and interaction with

scholarly people. My PhD supervisor Prof Dr. Saeed Ahmad actively involved me

in the research work of post graduate students, their examination and viva voce

exams right from the beginning and provided me an opportunity to learn more

about the latest trends and developments in the Civil Engineering, besides my

core area of research. In these endeavors I had been able to work on many

projects with him which mainly included, High Range Water Reducers,

(Superplasticizers), Self Compacting Concrete, Very Early Strength (VES)

Concrete, High Strength Concrete (HSC), Retrofitting and Rehabilitation of the

damaged structures etc. These efforts on the part of my supervisor enabled me

to bridge the knowledge gap and tackle the PhD studies more seriously and

rigorously. I must appreciate his patience and straightforwardness as I have

always found him a sincere and upright person. He had been very kind

throughout the research work and provided me, his guidance at all stages of my

studies.

Interaction with the staff at UET Taxila turned a pleasant opportunity. While

working with the Laboratory staff, academicians and other administrative staff at

different times, I have received their due support and kindness. I remember

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taking lunch with the Concrete and Structure Laboratories staff during casting

and testing of beams. I always felt as part of the family of employees at UET

Taxila, and received due regards from all of them. The staff of Labs worked with

me tirelessly in the afternoon and I must appreciate their kindness and support.

I received due support from the Chairman Civil Engineering Prof. Dr M.A.Kamal

and Ex-Chairman Prof. Dr A.R Ghumman in discussing my problems regarding

the funding of faculty research project and other such matters.

The staff of Directorate of Advanced Studies Research and Technology

Development had always been very kind and cooperative in forwarding my

requests for grants to the competent authority, which enabled me to get two

grants of Rs 200,000 each for faculty research with my supervisor.

I was always duly encouraged by Prof Dr. Muhammad Ilyas UET Lahore and

Dr. Tariq Mehmood Zaib, Pakistan Atomic Energy Commission (PAEC), during

my PhD studies and editing of the thesis. Their support and positive attitudes

always provided a hope to complete my work. In the days of despair they always

encouraged me.

At last but not the least I feel highly indebted to Prof Dr. Habibullah Jamal Ex-

Vice Chancellor and incumbent Vice Chancellor UET Taxila Prof. Dr. M. Akram

Javed for their support and guidance.

Today when I am writing the closing chapter of my PhD thesis, I feel proud and

highly grateful to Almighty Allah, that in my efforts to broaden my vision and

knowledge, I was fortunate to meet with very friendly people and as a result I,

feel part of UET Taxila today. In my endeavors my parents my family and my

personal staff, always supported me. My children kept missing me while I was

working at my office in writing this thesis and conducting experimental works.

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I pray to the almighty Allah that this work may pave ways for further innovation &

research and this nation and the Engineering professionals may benefit from the

findings-Amen.

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List of Figures Figure No. Description Page

Figure 2.1 Cracks appeared when vertical load is applied at the mid span of a beam (Jose,2000)

25

Figure 2.2 Distribution of bending and shear stresses across the section of a beam element and stress state in element A2 and corresponding Mohr’s circle(Jose,2000)

27

Figure 2.3 Types of cracks expected in the reinforced concrete beams (Jose, 2000). 29

Figure 2.4 Forces acting in a beam element within the shear span and internal arches in a RC beam (Russo et al., 2004).

30

Figure 2.5 Shear in beam with no transverse reinforcement. (Stratford and Burgoyne, 2003)

32

Figure 2.6 Comparison of theoretical and test results of shear failure of beams

(Kani.1964)

33

Figure 2.7 Parallel chord truss model. The struts are intercepted by the stirrups at spacing of d (Ritter, 1989).

35

Figure 2.8 Shear strength of RC beams with shear reinforcement (ACI-ASCE,1998) 36

Figure 2.9 Size-effect law (Bažant et al. 1986). 38

Figure 2.10 Kani’s Tooth Model (Kani,1964). 44

Figure 2.11 Compression Field Theories (Mitchell and Collins,1974) 48

Figure 2.12 Description of Modified compression Field Theory (Vecchio and Collins,1986) 52

Figure 2.13 Values of β and θ for RC members with at least minimum shear reinforcement.

57

Figure 2.14 Values of β and θ for RC members with less than minimum shear reinforcement (Vecchio and Collins1986).

59

Figure 2.15 Transmission of forces across the crack. ( Bentz. et al,2006) 61

Figure 2.16 Variable truss Model of RC beams ( Mitchell, 1986) 68

Figure 2.17 Shear Friction Hypothesis of Birkeland and Birkeland (1966) 69

Figure 2.18 Comparison of CSA and ACI amounts of minimum shear reinforcement (Yoon et al, 1996).

79

Figure 3.1 World Trade Centre (USA) 88

Figure 3.2 The world Highest Tower Burj Dubai,UAE (2651 feet) (162 floors, scheduled construction, 2008)

88

Figure 3.3 Variation of compressive stress-strain curves with increasing compressive strength.( Adapted from Collins and Mitchell, (1997).

108

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Figure No. Description Page

Figure 4.1 Example of B& D-Regions in a Common Building Structure (Schlaich et al

,1987) 122

Figure 4.2 Example of B&D-Regions in a Common Bridge Structure. (Schlaich. et al. 1987).

122

Figure 4.3 Some Typical Strut and Tie models as proposed by ACI 318-06(ACI-ASCE,1996)

123

Figure 4.4 Classifications of Nodes (ACI- 318-06) 128

Figure 4.5 Proposed STM for Deep beams under applied external load 130

Figure 4.6 Proposed STM for one way corbel under applied external load. 130

Figure 4.7 Proposed STM for two way corbel under applied external load. 130

Figure 4.8 Proposed STM for dapped beam end under applied external load 131

Figure 4.9 Proposed STM for pile cap under applied external load. 131

Figure 5.1 Flowchart for use of the NCHRP simplified design method ( NHRP, 2006). 149

Figure 6.1 Details of beams used in the testing. 155

Figure 6.2 Details of loading arrangement for the testing of RC beams. 157

Figure 6.3 Details of roller supports and deflection gauges used for the beams. 157

Figure 6.4 Wet sand filled around the beams for curing. 160

Figure 6.5

Failure of beams without web reinforcement due to diagonal tension shear failure mode of the beam.

165

Figure 6.6

Failure of beams without web reinforcement due to diagonal tension shear failure mode of the beam. The failure angles have been reduced with the increase in longitudinal steel.

167

Figure 6.7 Flexural shear failure of beams without web reinforcement having a/d>5. 168

Figure 6.8

Typical shear failures of beams without web reinforcement. The failure is more brittle and sudden amongst all. The crack causing failure of the beam was not noticed in the beginning and beams failed very suddenly due to tension shear failure.

169

Figure 6.9 Effect of longitudinal Steel ratio on the shear strength of concrete beams without stirrups for same value of a/d.

171

Figure 6.10 Effect of longitudinal Steel ratio on the shear strength of concrete beams with web reinforcement for same value of a/d.

171

Figure 6.11 Effect of shear span to depth ratio on the shear strength of concrete beams without stirrups for same value of longitudinal steel ratio.

173

Figure 6.12 Effect of shear span to depth ratio on the shear strength of concrete beams without stirrups for same value of longitudinal steel ratio.

173

Figure 6.13 Beam shear failure or diagonal tension shear failure in beams with web reinforcement.

174

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Figure No. Description Page

Figure 6.14 Load deflection curves for beams without web reinforcement and ρ=0.0073 178

Figure 6.15 load deflection curves for beams without web reinforcement and ρ=0.02 179

Figure 7.1 Geometry of the proposed two way corbel and proposed STM. 181

Figure 7.2 Reinforcement Form work used for the two way corbels. 181

Figure 7.3 Loading arrangement for HSC two way corbels. 183

Figure 7.4 Details of embedment strain gauge 184

Figure 7.5 Strain Data Logging system used. 184

Figure 7.6 Member Forces in strut and Tie model for two way corbel. 185

Figure 7.7 Details of reinforcement, formwork and embedment gauges. 186

Figure 7.8 Typical shear failures of the two ways HSC corbels. 188

Figure 9.1 Plot of the proposed model generated by the software. 214

Figure 9.2 Comparison of actual values of shear stress with the predicted values by proposed regression model and other models for HSC beams without web reinforcement.

221

Figure 9.3 Comparison of actual shear stress of beams having stirrups with the proposed regression model and other models.

222

Figure A-1 Geometry of Two way corbel. 249

Figure A-2 Geometry of assumed Strut and Tie Model ( STM) 250

Figure A-3 Member Force in strut and Tie model for two way corbel. 252

Figure A-4 Reinforcement details of two way corbel designed for 80 Kips (355KN) load by STM.

254

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List of Tables

Table No. Description Page

Table 2.1 Comparison of experimental results with the full MCFT, simplified MCFT and ACI equation for shear strength of RC beams.( Bentz et al, 2006)

64

Table 2.2 Comparison of the shear strength of RC beams proposed by Zararis , ACI And EC-2 ( Zararis P.D,2003)

73

Table 3.1 Definition of HPC as per SHRP (Zia et al, 1993)

90

Table 3.2 Volume of coarse aggregate per unit of volume of concrete. (ACI-211.1)

98

Table 3.3 Upper limits of specified compressive strength of concrete for HSC and Standard test specimen. (Paultre and Mitchell (2003).

103

Table 3.4

Comparison of values of load factors, strength reduction factors and material strength reduction factor proposed by various codes (Paultre and Mitchell, 2003).

104

Table 3.5

Comparison of values of modulus of elasticity modulus of rapture and min flexure reinforcement proposed by various codes (Paultre and Mitchell (2003).

105

Table5.1 Summary of Major Code Expressions for the Concrete Contribution to Shear Resistance.

143

Table 5.2 Summary of Research Results conducted at various Universities.

144

Table 5.3 Comparison of test values and Codes values based on shear data base (NCHRP; 2006)

145

Table 6.1 Mix Proportioning/ Designing of High Strength Concrete.

154

Table 6.2 Details of reinforcing bars used in the beams 154

Table 6.3 Reinforcement details of beams.

156

Table 6. 4 Shear span to depth ratio and corresponding span of seven beams in each set of longitudinal reinforcement.

156

Table6.5 Details of Series-I beams without web reinforcement ( 35 Nos)

159

Table 6.6 Details of Series-II beams with web reinforcement ( 35 Nos) 159

Table 6.7 Total applied failure load at the beams without web reinforcement

161

Table 6.8 Total applied failure load at the beams with web reinforcement 162

Table 6.9 Shear Strength and failure angles of 35 HSC beams, without web reinforcement

163

Table 6.10 Shear Failure mode of 35 beams with web reinforcement 163

Table 6.11 Shear Strength ,failure angles and failure modes of 35 HSC beams, with web reinforcement.

164

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Table No. Description Page

Table 6.12 Effect of the longitudinal steel on the shear strength of beams for constant a/d values.

170

Table 6.13 Shear strength, failure mode and failure angles for 35 HSRC beams with web reinforcement.

175

Table 6.14 Increase in the shear strength due to addition of web reinforcement in HSRC beams.

177

Table 7.1 Mix Proportioning/ Designing of High Strength Concrete Double Corbels 182

Table 7.2 Details of technical parameters and member forces in assumed STM

186

Table 7.3 Comparison of theoretical and actual failure loads of HSC double corbels 187

Table 8.1 Comparison of the shear strength of beams without web reinforcement with the provisions of the ACI 318-08

190

Table 8.2 Comparison of the shear capacity of beams with web reinforcement with the provisions of the ACI 318-08

191

Table 8.3 Comparison of increase in shear strength due to stirrups and ACI-318 provision for stirrups contribution

192

Table 8.4 Comparison of the shear Strength of beams without web reinforcement with the provisions of the Canadian Standards (Simplified Method)

194

Table.8.5 Comparison of the shear Strength of beams with web reinforcement with the provisions of the Canadian Standards (Simplified Method)

195

Table 8.6 Comparison of the shear Strength of beams without web reinforcement with the provisions of MCFT( LRFD Method)

197

Table 8.7 Comparison of the shear Strength of beams with web reinforcement with the provisions of MCFT ( LRFD Method)

198

Table 8.8 Comparison of the shear Strength of beams without web reinforcement with the provisions of EC-02

200

Table 8.9 Comparison of the shear Strength of beams with web reinforcement with the provisions of EC-02

201

Table 8.10 Comparison of the shear Strength of beams without web reinforcement with equation proposed in new theory of Zararis,P.D.

203

Table 8.11 Comparison of the shear Strength of beams with web reinforcement with equation proposed in new theory of Zararis,P.D.

204

Table 8.12 Comparison of Vtest/VCode for ACI, CSA, MCFT, EC-02 and New Equation for beams without web reinforcement.

206

Table 8.13 Comparison of Vtest/VCode for ACI, CSA, MCFT, EC-02 and New Equation for beams with web reinforcement.

207

Table 8.14: Summary of means of the ratios of observed values and different code Values for shear strength of beams without web reinforcement

208

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Table No. Description

Page

Table 8.15

Summary of means of the ratios of observed values and different code Values for shear Strength of beams with web reinforcement.

208

Table 9.1

Comparison of actual and predicated values of shear stress of High Strength concrete beams without web reinforcement for three proposed models.

216

Table 9.2

Comparison of actual and predicted values of shear stress of high strength concrete beams with web reinforcement.

218

Table 9.3

Comparison of proposed model ACI equation and model proposed by G.Russo et al. (2004) for beams without web reinforcement..

220

Table 9.4

Comparison of actual shear stress of beams having no stirrups with the proposed model and other models of ACI, Bazant and Russo

224

Table 9.5

Comparison of test/pred by the proposed model and other models for beams without shear reinforcement ( 35 Nos). ( For constant steel ratio and variable a/d)

228

Table 9.6

Comparison of test/pred by the proposed model and other models for beams with shear reinforcement ( 35 Nos) ( For constant steel ratio and variable a/d)

229

Table 9.7

Comparison of test/pred by the proposed model and other models for beams without shear reinforcement ( 35 Nos). ( For constant a/d and variable steel ratio)

230

Table 9.8

Comparison of test/pred by the proposed model and other models for beams with shear reinforcement ( 35 Nos) ( For constant a/d and variable steel ratio)

231

Table A-1

Forces in Truss of double corbel after analysis.

251

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Table of Contents.

Chapter Description Page

1. Introduction 19

1.1 Problem Statement 20

1.2 Aim and Objectives of Research 20

1.3 Scope of the research study 20

1.4 Methodology/Programme 21

1.5 Layout of the thesis 22

Literature Review.

2. Shear strength of RC beams. 25

2.1 Introduction to shear strength of beams 25

2.2 Mode of Failure of concrete beams in shear. 28

2.3 Shear strength of Normal Strength Reinforced Concrete (NSRC) beams.

23

2.4 Factors affecting shear strength of RC beams 37

2.5 Historical development of shear design of reinforced concrete beams

43

2.6 Recent approaches in the Shear Design of reinforced Concrete beams.

47

2.7 Minimum Amount of Shear Reinforcement. 78

2.8 Future of research on shear design of RC members. 79

Chapter Appendix 2.1 Solved Example with MCFT 83

3 Shear strength of high Performance reinforced concrete beams 88

3.1 High Performance Concrete. ( HPC) 88

3.2 High Strength Concrete. 91

3.3 Codes Provisions for High Strength Concrete. 103

3.4 Mechanical properties of high strength concrete 106

3.5 Stress strain behaviour and shear strength of HSC 107

Summary 119

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Chapter Description Page

4 Shear design of disturbed region (D-region) in reinforced

concrete. 121

4.1 The basic concept of Beam and Disturbed region 121

4.2 Basic design principles for shear design of disturbed region 124

4.3 Using Strut and Tie Model for the shear design of Structural components.

124

4.4 Choosing the Strut and Tie Model (STM). 126

4.5 Procedure for shear deign of disturbed region with STM. 129

4.6 Some latest research on the shear design of disturbed region

with STM. 131

5

Provisions of international building codes for the shear design of Normal & High Strength Concrete.

136

5.1

British Standards (BS-8110) 136

5.2

European Code EC2-2003. 137

5.3

ACI Code 318-06 (American Concrete Institute) 138

5.4 Canadian Standards for design of Concrete structures. CSA A- 23.3-94.

140

5.5 AASHTO LRFD (Load Reduction Factor Design) Bridge Design

Specifications -1996. 141

5.6 Empirical methods for beams without shear reinforcement. 142

5.7 Results of High Strength concrete beams at different Universities, in near past.

143

5.8 Evaluation of shear design methods of different building codes based on test data base by National Cooperative Highway Program ( NCHRP).

145

5.9 Variations in the provisions of international building code for shear capacity of beams.

150

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Chapter Description Page

6

Experimental Program

Experimental programme and discussion of test results of HSC

beams ( B-Region). 153

6.1 Introduction to experimental programme. 153

6.2 Test Specimen. 154

6.3 Test set up 157

6.4 Experimental results. 161

6.5 Discussion of results. 165

7

Experimental Programme on disturbed Region ( D-region) in

concrete and observations. 180

7.1 Experimental Programme for testing of disturbed region in

concrete (D-region). 185

7.2 Design of the two way corbel by Strut and Tie Model

( STM) 187

7.3 Test results and discussion of two way corbel testing. 187

8

Comparison of the observed values with the provisions of

International building and bridges codes. 189

8.1 ACI Code 318-08 (American Concrete Institute) 189

8.2 Canadian Standards for design of Concrete structures. (CSA A23.3-94).

193

8.3 AASHTO’s LRFD DESIGN SPECIFICATION ( 1994). (Modified Compression Field theory-MCFT).

196

8.4 Comparison of observed values with the provisions of

Eurocode-02 200

8.5 New Theory Proposed by Prodromos D.Zararis (2003) 203

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Chapter Description Page

9

Statistical Model for the prediction of shear strength of High

Strength Concrete beams. 211

9.1 Regression model and its application in Civil Engineering. 211

9.2 Regression Model for beams with web reinforcement 213

9.3 Regression Models for shear strength of beams with web reinforcement.

217

9.4 Comparison of the proposed models with ACI-318 Code and other models:

219

9.5 Discussion on the proposed regression models 232

10

Conclusions and Recommendations. 234

10.1 Conclusions 234

10.2 Conclusions on the work in disturbed region 237

10.3 Recommendations for future work 238

References 239

Appendix A Design of Two way corbel using STM 249

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Chapter No1.

Introduction.

The strength of concrete is one of the most important properties of this versatile

construction material. High Strength Concrete has been widely used in the

construction industry for last few decades. The development of new water

reducing admixtures and the mineral admixtures is making it possible to achieve

more reliable high strength concretes in the recent years. High Performance

Concrete (HPC) is referred to the specialized series of concretes designed to

provide several benefits in the construction of concrete structures. High Strength

Concrete therefore belongs to the High Performance Concrete series, due to its

peculiar properties. The use of High Strength Concrete is likely to increase

further in 21st century with the construction of more high-rise buildings, long span

pre-stressed bridges, and pre-cast elements in concrete structures.

Concrete unlike steel is relatively non-homogenous material; hence its different

structural properties are likely to change with increase in compressive strength.

The high strength concrete is comparatively a brittle material as the sound matrix

of aggregates and cement paste provides a smoother shear failure plane, which

leads to its abrupt failure. Consequently the shear strength of High Strength

Concrete does not increase in the same way, as its compressive strength. The

availability of limited experimental work on the high strength concrete makes it

difficult to safely predict the shear capacity of high strength reinforced concrete

members.

The shear capacity of reinforced concrete members is presently evaluated on the

basis of empirical equations proposed by different International Building Codes

with certain modifications in the equations for normal strength concrete. As most

of these equations have been derived on the basis of experimental data of

concrete with compressive strength of 6000 psi (40 MPa) or less, therefore their

application to higher values of compressive strength always raise questions in

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the minds of researchers. To further rationalize and generalize, these empirical

equations for shear design of high strength reinforced concrete members,

extensive research is required. This research is therefore an effort in this

direction.

1.1 Problem Statement

To better understand the behaviour of High Strength Reinforced Concrete beams

in shear.

1.2 Aim and Objectives of Research

The main aim of the research is to improve the understanding about the

behaviour of high strength reinforced concrete members in shear and to develop

some more rational procedure for the shear design of the High Strength Concrete

members, based on the literature review and experimental work. The relative

objectives of research are further explained as follows;

- To evaluate the shear strength of High Strength Reinforced Concrete

(HSRC) beams with and without web reinforcement.

- To study the effect of various variables on the shear strength of the high

strength concrete beams.

- To compare the provisions and procedures in different International

Building and Bridges Codes and latest developments for the shear design

of high strength concrete beams.

- To discuss the latest trends in the shear design of non-linear and

disturbed regions in the high strength concrete structures, where ordinary

beams theory cannot be applied.

1.3 Scope of the research study

The scope of the research study is as follows;

- Shear Behaviour of High Strength Reinforced Concrete (HSRC) beams

having compressive strength of 52 MPa (8200psi) has been studied.

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- Slender beams with shear span to depth ratio a/d from 3 to 6 have been

selected for research and the results obtained can be generalized for only

this range of beams.

- Five levels of longitudinal steel ratio have been selected, starting from

minimum longitudinal steel ratio of 200/fy to 2% level. Hence the results

mainly cover this range of longitudinal steel ratio from 0.33% to 2%.

- The proposed regression model to predict the shear strength of HSRC

beams is based on the observations of 70 beams tested. Hence its

generalization would require further research.

- For comparison of the observed shear strength of HSRC beams with the

provisions of five building and bridges codes have been selected i.e. ACI-

318, Canadian Code, Euro code (EC-02), AASHTO LRFD bridge design

specification based on Modified Compression Field Theory ( MCFT).

- For the study the shear strength of disturbed region, the basic Strut and

Tie Model (STM), was applied to High Strength Concrete corbels.

1.4 Methodology/Programme

To study the effect of various parameters on the shear strength of HSRC beams,

the following research methodology was adopted;

The experimental work was divided into two regions namely beam region (B-

region) and disturbed region (D-region). For beam region, the following

methodology was adopted.

i. To study the shear behaviour of HSRC beams, 70 beams of size 9inx12in

(23cmx30 cm) were selected in two sets of 35 beams each, such that in

first set no web reinforcement was provided, whereas in second set of 35

beams, web reinforcement corresponding to minimum shear

reinforcement given by ACI-318-08 was provided.

ii. Five levels of longitudinal steel ratio (0.33%, 0.73%, 1%, 1.5% and 2%)

was selected to study the effect of longitudinal steel ratio on the shear

strength of HSRC beams.

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iii. To study the effect of shear span to depth ratio seven values of “a/d” were

selected as 3, 3.5, 4, 4.5, 5, 5.5 and 6 to mainly cover the behaviour of

slender HSRC beams in shear.

The beams were tested under monotonic loads and the observations were

recorded in terms of cracking pattern, failure mode, and ultimate failure capacity,

deflections of beams at mid span and critical sections at distance “d” from the

face of supports.

The shear strength of the beams was determined at the failure point and the

observed values were compared mutually and with the provisions of selected

Building and Bridges Codes. The effect of various parameters on the shear

strength of HSRC beams was studied on the basis of observations from the

testing.

An attempt was made to develop regression equation to predict the shear

strength of beams based on the sample date of tested beams; however its

generalization would require extensive experimental work.

To study the shear behaviour of RC structures in disturbed region, where the

shear span to depth ratio is less than 3.0, focus was laid on the Strut and Tie

Model (STM) and nine high strength concrete corbels designed on the basis of

STM for an assumed external load were tested. The actual and theoretical shear

failure loads were compared to check the suitability of STM for analysis and

design of disturbed region in concrete.

1.5 Layout of the thesis

The thesis has been divided into ten chapters. Next to the introduction, in

Chapter 2, shear strength of reinforced concrete and various factors affecting

shear strength of concrete have been discussed. Some latest approaches like

Modified Compression Field Theory (MCFT), Simplified Compression Field,

theory and truss approaches have been discussed in quite details. At the end of

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the chapter, two design examples on MCFT and one example on use of

specialized software Response-2000 based on MCFT, have been added.

Additionally some latest review work by using MCFT and simplified MCFT has

been included in the Chapter 2.

In Chapter 3, various properties of high performance concrete and high strength

concrete have been discussed with special emphasis over the selection of

material, admixtures, mix proportioning, transportation, placement and structural

properties of high strength concrete. Codes provision for measuring the

compressive strength, flexural strength, modulus of elasticity and other structural

properties of HSC in European code (EC-02 and CEB-MC-90), Canadian code

(CSA A23.3-94), American Concrete Institute (ACI-318-02) and New Zealand

code (NZS 3101-95) have been discussed. In literature review of shear strength

of high strength concrete, current state of the research in shear strength of high

strength reinforced concrete beams has been elucidated, which forms basis for

onwards study of the problem. Some latest approaches to address the problem

of shear in high strength concrete have also been discussed in the chapter.

In Chapter 4, shear strength of disturbed regions (D-region) in concrete

structures has been discussed, in the light of latest research. The literature

review on the shear design of disturbed region has revealed that shears design

of disturbed region with new tools like Strut and Tie Model (STM), is as an

emerging area in the shear design of high strength concrete members. However,

there are many challenges in application of STM for the design of concrete

structures. The growing use of new concept of Strut and Tie Modeling of

disturbed region in concrete structures necessitated, to dedicate some

experimental work to this emerging concept for design of concrete structures.

In Chapter 5, provisions of some important International Building and Bridges

Codes for Normal and High Strength Concrete beams have been discussed and

references to the relevant clauses of respective Building Codes has been given.

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In Chapter 6, the experimental program for beam region has been given. In the

beams region seventy beams of high strength concrete in two sets of 35 beams

with web reinforcement and 35 beams without web reinforcement have been

tested with reference to the effect of different parameters on the shear strength of

high strength concrete beams. Each set of beams is comprised of five values of

longitudinal steel ratio and seven values of shear span to depth ratio. This is

followed by the observations and test results and discussion thereon.

In Chapter 7, experimental work on disturbed region has been explained with

special reference to high strength concrete corbels. The testing setup and other

instruments used for measuring the shear strength of the corbels have been

given. The test results have been discussed in term of the suitability of STM for

shear design of two way corbels.

In Chapter 8, the actual values of the shear strength of HSC beams have been

compared with the values worked out with the equations proposed by some

international building and bridges codes.

In Chapter 9, efforts have been made to develop some statistical regression

model for predicting the shear strength of HSRC beams on the basis of

experimental results and these have been compared with some other models.

The validity and generalization of the proposed model is however limited due to

insufficient date. However graduate research to propose some more rational

models, which can best fit the available shear database of high strength concrete

beams incorporating more parameters, can be undertaken in the next phase of

research by other graduate students. This preliminary effort can pave way for the

same.

In chapter 10, conclusions and recommendations for future research have been

proposed and at the end references are given.

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Chapter No. 2

Shear strength of reinforced concrete beams

Chapter Introduction: This chapter explains the basic concepts of the shear strength of concrete beams and their application to the shear strength of Reinforced Concrete (RC) beams. The factors affecting the shear strength of RC beams are also discussed in quite details. The historical perspective and recent approaches in the area of shear strength of concrete have been elucidated and some modern research findings have been discussed in more details at the end of the chapter.

2.1 Introduction to shear strength of RC beams

The shear stress acts parallel or tangential to the section of a material. When a

simple beam is subjected to bending, the fibers above the neutral axis are in

compression and the fibers located below the neutral axis are in tension. A

concrete beam with longitudinal steel when subjected to external loads will

develop diagonal tensile stresses which will tend to produce cracks. These

cracks are vertical at the centre of the span and will become inclined as they

reach the support of the beam as shown in Figure 2.1. The stress that causes the

inclined cracks in the beam is called diagonal tension stresse (Jose M.A, 2002).

Figure 2.1 Cracks appeared when vertical load is applied at the mid span of a beam

(Jose.M.A, 2000)

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The shear stress in a homogenous elastic beam is given as

Ib

VQ (2.1)

Where , V = Shear force at section under consideration.

Q = Static moment about the neutral axis of that portion of cross section lying

between a line through point in question parallel to neutral axis and nearest face

of the beam.

I = Moment of Inertia of the cross section about neutral axis.

b = Width of the beam at a given point.

The small infinitesimal elements A1 & A2 of the rectangular beam in Figure 2.2

are shown with the tensile normal stress ft and shear stress ν across the plane a1-

a1 and a2-a2 at distance y from the neutral axis.

The internal stresses acting on elements A1 & A2 are also shown in Figure 2.2.

Using Mohr’s circle, the principal stresses for element A2 in the tensile zone

below the neutral axis can be found as

)2

(2

2(max) tt

t

fff _______________Principal tension (2.2)

)2

(2

2(max) tt

c

fff _______________________Principal compression (2.3)

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Figure 2.2: Distribution of bending and shear stresses across the section of a beam

element and stress state in element A2 and corresponding Mohr’s circle(Jose,2000)

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2.2 Mode of failure of concrete beams in shear.

Various failure modes in RC beams are shown in Figure 2.3(a). In the region of

flexural failure, cracks are mainly vertical in the middle third of the beam span

and perpendicular to the lines of principal stress. These cracks result from a very

small shear stress v and a dominant flexural stress f which results in an almost

horizontal principal stress ft(max).

Diagonal tension failure happens, if the strength of the beam in diagonal tension

is lower than its strength in flexure. The shear span-to-depth ratio is of

intermediate magnitude for diagonal failure, varying between 2.5 and 5.5 for the

case of concentrated loading. Such beams can be considered of intermediate

slenderness. Cracking starts with the development of a few fine vertical flexural

cracks at mid span, followed by the destruction of the bond between the

reinforcing steel and the surrounding concrete at the support. Thereafter, without

ample warning of impending failure, two or three diagonal cracks develop at

about 1½d to 2d distance from the face of the support in the case of reinforced

concrete beams, and usually at about a quarter of the span in the case of pre-

stressed concrete beams. As they stabilize, one of the diagonal cracks widens

into a principal diagonal tension crack and extends to the top compression fibers

of the beam, as seen in Figure 2.3 (b) (Jose,2000).

In beams having shear span to depth ratio less than 2.5, a few fine flexural

cracks start to develop at mid span and stop propagating as destruction of the

bond occurs between the longitudinal bars and the surrounding concrete at the

support region. Thereafter, an inclined crack steeper than in the diagonal tension

case suddenly develops and proceeds to propagate toward the neutral axis. The

rate of its progress is reduced with the crushing of the concrete in the top

compression fibers and a redistribution of stresses within the top region occurs.

Sudden failure takes place as the principal inclined crack dynamically joins the

crushed concrete zone, as illustrated in Figure 2.3(c). This type of failure can be

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considered relatively less brittle than the diagonal tension failure due to the

stress redistribution. Yet it is, in fact, a brittle type of failure with limited warning,

and such as design should be avoided completely. This failure is often called as

compression failure or web shear failure.

(a)

Figure 2.3 Types of cracks expected in the reinforced concrete beams (Jose, 2000).

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2.3 Shear strength of normal strength reinforced concrete beams

The research on shear strength of concrete has shown that reinforced concrete

beams without transverse reinforcement can resist the shear and flexure by

means of beam and arch actions, also sometimes called concrete mechanisms

(Russo et al, 2002). These forces acting on the beam element in its shear span

are shown in Figure 2.4. It was assumed that the resultant of the aggregates

interlocking at the crack interface can be replaced by Va as shown in the Figure

2.4, whose direction passes through the point of application of the internal

compression force C. The shear contribution due to dowel Vd is negligible at the

rotation equilibrium. The resultant bending moment is given by

Mc = Vc.x = T.jd ………………………… ……….. (2.4)

Where Vc is the shear force due to concrete resisting contribution, T is tensile

force in the longitudinal reinforcement and x is the distance between the support

and the point where crack has been appeared.

The sheer force is the derivative of the bending moment Vc = dMc/dx

Vc = jd dx

d T + T. dx

djd ............................... ( 2.5)

Forces acting in a beam element within the shear span

b. Internal arches in RC beams.

Figure 2.4 Forces acting in a beam element within the shear span and internal arches in

a RC beam (Kani, 1964., Russo et al., 2004).

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The first term in equation 2.5, is the resistance to shear as contribution of the

beam action, whereas the second part is called arch action.

In beam action, the lever arm is constant and the tensile force in the steel bars is

supposed to vary. The beam action is related to the crack pattern in the shear

span, in which the tensile zone is generally divided into blocks or teeth.

Beam action describes shear transfer by changes in the magnitude of the

compression-zone concrete and flexural reinforcement actions, with a constant

lever-arm, requiring load-transfer between the two forces. In a cracked beam,

load-transfer from the flexural reinforcement to the compression-zone occurs

through the ‘‘teeth’’ of concrete between cracks, requiring bond between the

concrete and reinforcement. Bending and failure of this concrete is studied by

tooth models.

The second part of the equation shows the shear resisting contribution due to

arch action, which is characterized by the internal variation of the lever arm jd

with the T constant. The arch mechanism transfers the vertical loads to the

supports through the arch route.

Arch action occurs in the un-cracked part of concrete near the end of a beam,

where load is carried from the compression-zone to the support by a

compressive strut. The vertical component of this strut transfers shear to the

support, while the constant horizontal component is reacted by the tensile

flexural reinforcement. Both beam action and arch action can act in the same

region (Stratford and Burgoyne,2003). Thus shear transfer in the beam can take

place by one of the two mechanisms i.e. variation in the magnitude of internal

actions and variation in the lever arm between the actions. The details are shown

in Figure 2.5. Before cracking of the beams, the shear is resisted by the beam by

all the elements of the beams shown in the paths I, II and III ( Figure 2.4).

However after the cracks, only the un-cracked part of the beams is resisting the

shear by transferring it to the supports.

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Figure 2.5 Shear in beam with no transverse reinforcement.

(Stratford and Burgoyne, 2003)

In one of the earliest research on shear failure, at University of Toronto Canada,

Kani (1964) defined the regions of beam action and arch actions for resisting the

shear in RC beams, for the first time. It was pointed out by him that initially the

shear is resisted by the teeth of cracked concrete, but after destruction of the

resistance by teeth of the cracked beam, a quite different mechanism through

tied arches in the compression zone occurs. On the basis of actual test results,

Kani (1964), reported that in the region of low values of shear span to depth ratio

(a/d), the shear capacity of the structure is determined by the strength of

remaining arch, whereas in the region with medium value of a/d, the capacity of

teeth of cracked concrete determines the shear capacity of the beams. He also

proposed an expression for the boundary point separating the two regions. In

Figure 2.6, the boundary for shear failure of the beams tested in Toronto has

been given, which shows that up to a/d of 2.5, shear failure due to arch action is

dominant whereas in the region with a/d more than 2.5 and up to 5.75 or 6 beam

action due to concrete teeth ( beam action) is dominant and the shear capacity

due to arch action is very small.

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Figure 2.6 Comparison of theoretical and test results of shear failure of beams (Kani.1964)

The joint committee ASCE-ACI-426 in 1973 and later in 1998 reported the following

five mechanisms for resisting the shear in reinforced concrete sections (NTRB,

2005).

i. Shear in the un-cracked concrete zone

In cracked concrete member, the un-cracked compression zone offers some

resistance to the shear but for slender beams with no axial force, this part is very

negligible due to small depth of compression zone.

ii. Residual tensile stresses

When concrete is cracked and loaded in uni-axial tension, it can transmit tensile

stresses until crack widths reach 0.06 mm to 0.16 mm, which adds to the shear

capacity of the concrete. When the crack opening is small, the resistance

provided by residual tensile stresses is significant. However in a large member,

the contribution of crack tip tensile stresses to shear resistance is less significant

due to the large crack widths that occur before failure in such members.

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iii. Interface shear transfer

The contribution of interface shear transfer to shear strength is a function of the

crack width and aggregate size. Thus, the magnitude decreases as the crack

width increases and as the aggregate size decreases. Consequently, this

component is also called “aggregate interlock” denoted by Va. However, it is now

considered more appropriate to use the terminology “interface shear transfer” or

"friction".

iv. Dowel action

When a crack forms across longitudinal bars, the dowelling action Vd , of the

longitudinal bars provides a resisting shear force, which depends on the amount

of concrete cover beneath the longitudinal bars and the degree to which vertical

displacements of those bars at the inclined crack are restrained by transverse

reinforcement.

v. Shear reinforcement

This forms the main part of the shear capacity of the beams with web

reinforcement and is typically modeled with 45 degree truss model.

The ASCE-ACI Committee 426 has reported the following equation for the concrete

shear strength incorporating the longitudinal reinforcement.

Vc = 10080.0

12

cf ≤ 0.192

12

cf [MPa] (2.6)

For beams with transverse reinforcement, the basic model to explain the mechanism

for carrying the shear was proposed by Ritter (1899). The load was assumed to flow

down the concrete diagonal struts and then lifted to the compression chord by

transverse tension ties on its way to support as shown in Figure 2.7 below.

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Figure 2.7 Parallel chord truss model. The struts are intercepted by the stirrups at spacing of

d (Ritter, 1989)

Traditionally one truss with stirrups at the longitudinal spacing “d” was assumed but

in fact Ritter showed that there was continuous diagonal compression carried up and

over cracks by a band of stirrups as shown in Fig 2.6

For 45 degree truss model, the capacity provided by the shear reinforcement is

equal to the capacity of an individual stirrup multiplied by the number of stirrups over

the length d, which is approximately equal to “d/s”. The shear carried by the stirrups

is given as;

Vs =

s

dfA yv (2.7)

The shear strength of RC beams with transverse reinforcement is traditionally

determined by summing the individual contribution of concrete and steel as shown in

Figure 2.7 (ACI-ASCE,1998) .i.e.

Vn = Vc+Vs (2.8)

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Figure 2.8 Shear strength of RC beams with shear reinforcement (ACI-ASCE,1998)

Experimental studies (Talbot, 1909), reported that the shear capacity of beams was

greater than predicted by the truss model and the idea of concrete contribution was

developed.

Kani (1969) provided a quite different explanation for the role of web reinforcement

in resisting the shear, called as “Rational Theory”. With the help of actual tests

results, he explained that the purpose of web reinforcement is to provide reactions to

the internal arching which supports the compression zone of the beams and not to

carry the shear force or any part of it. Hence no direct relationship can be expected

between the magnitude of shear force and requirement of web reinforcement. This

was certainly in sharp contrast with the conventional shear theory based on truss

model. He himself declared his proposed rational theory not reconciling with the

conventional shear theory.

Chana (1987), reported that the failure mechanisms of RC beams with transverse

reinforcement is different than the beams without shear reinforcement. Hence Vs and

Vc mutually influence each other and simply adding the two terms may not give valid

results.

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2.4 Factors affecting shear strength of concrete beams

One of the major reasons for limited understanding of the shear behaviour and

diagonal failure of the RC beams is greater number of parameters involved in the

problem. Kani (1967), identified the following parameters affecting the diagonal

cracking of RC beams.

i. Grade of steel (tensile strength of longitudinal steel).

ii. Compressive strength of Concrete.

iii. Cross section and shape of beams ( web width, depth etc.)

iv. Shear arm or shear span.

v. Types, arrangements, quantity and location of web reinforcement

vi. Types of loadings.

vii. Types of beams supports (Simply supported or continuous).

viii. Pre-stress forces and its point of application etc.

In addition to the basic five echanisms for shear transfer discussed in section 2.3,

the effect of the other significant parameters on the shear strength of RC beams is

explained as follows;

2.4.1 Depth of member or size effect

Size effect refers to the fact that shear strength is not constant for a given

compressive strength of concrete but varies with the size of the beam, both its depth

and length. The phenomena become more obvious for lightly reinforced RC beams.

Current design methods for shear in RC members are based almost entirely on the

results of tests specimen having maximum size of 300 mm. Hence the assumption

of constant shear strength by most of the equations like ACI318-08, simple

equation, is contradicting the actual behaviour of the RC beams.

Dimensional analysis shows that the structural size effect for geometrically similar

specimens or structures is governed by the simple relation given by Bazant et al

(1984).

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Bazant et al (1984), used the following reduction factor to account for the size effect.

o

tN

d

d

Bf

1

'

(2.9)

N = P/bd = nominal stress at failure

P = maximum load (that is, failure load);

b = thickness;

d = characteristic dimension of the specimen or structure;

'tf = direct tensile strength; and

B, do = empirical constants, do being a certain multiple of the maximum size of in

homogeneities in the material.

The size-effect law has been used by Bažant and Sun (1987); Bažant and Sener

(1988); and Bažant, Sener, and Pratt (1988) to predict the size effects for shear,

torsion, and bond pullout testing of concrete. The law has been shown in Figure 2.9

Figure 2.9 Size-effect law (Bažant et al. 1986).

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Kani (1967), pointed out, a strong size effect of RC beams in shear without

transverse reinforcement. A reduction of 40% in relative strength was observed in

the size range of 150 to 1200 mm.

Kani (1967) presented the concept of valley of diagonal shear failure for the RC

beams without web reinforcement. After testing 133 beams to study the effect of

concrete strength, longitudinal steel ratio and shear span to depth ratio “a/d”, he

came up with the following significant results;

i. The shear strength of RC beams does not depend on the compressive

strength of concrete for the range studied ( 2500< fc ’< 5000 psi)

ii. The amount of longitudinal steel reinforcement has significant effect on the

relative beam strength i.e. Mu/Mfl, where Mu is the moment corresponding to

the diagonal cracking of the beam and Mfl is the flexural moment capacity of

the beams for given longitudinal steel.

iii. The relative beam strength is much more suitable indicator rather than the

ultimate shear νc, which depend on the a/d ratio and longitudinal steel ratio.

According to Kani (1967), the web reinforcement is required to increase the Mu to

the level of Mfl, so that diagonal cracking is avoided before flexural failure of RC

beams. Hence the shear design of beams with web reinforcement is an attempt to fill

the gap between Mu and Mfl.

Kani(1967),further elaborated the effect of beam depth on the shear strength of RC

beams and showed with the help of actual tests results that increasing the beam

depth leads to considerable reduction in the relative beam strength.

The shear strength of concrete has inverse relation with the depth of the beam.

Shioya et al. (1989), has experimentally showed that the shear strength of 3000 mm

deep beam was merely one third of the shear strength of 600 mm for beams without

shear reinforcement.

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The size effect is marked for beams without transverse reinforcement. The test data

has shown that the size effect plays its role in case of beams without transverse

reinforcement. Collins et al. (1996) have demonstrated that the size effect

disappears when beams without stirrups contain well distributed longitudinal

reinforcement to restrict the propagation of shear diagonal cracks.

2.4.2 Shear span to effective depth a/d or moment to shear ratio and support

conditions

ASCE- ACI Committee 326 (1998) has showed the shear capacity as function of

shear to moment ratio. The basic equation for the shear strength of RC concrete

beams proposed by ACI-318-98, makes the shear span to depth ratio as one of the

basic parameters for calculating the shear capacity of RC section.

When the shear span to depth ratio becomes less than 2.5, the shear capacity of the

RC becomes larger than that of slender beams as the shear is directly transferred to

supports through compression struts. However the supports condition strongly

influences the formation of compression strut. Compressive strut is more likely to

form when beam is loaded from upper face and supports to the bottom face (Adebar

1994).

Kotsovos.M.D ( 1984) studied the effect of web reinforcement for the RC beams

having a/d ratio between 1 and 2.5 with the help of non linear finite element analysis

and observed that placement of web reinforcement in the middle third rather than in

the shear span results in improved ductility and load carrying capacity of RC beams.

In one of the latest studies by Kotsovos and Pavlovic (2004), they used finite

element analysis to study the size effect in beams with smaller shear span to depth

ratio less than 2 and compared the results of theoretical model with the actual

experiment. They concluded that the shear and flexural capacity of beams with

shear span to depth ratio less than 2, is independent of the size of members and the

size effect vanishes for such beams.

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The shear span to depth ratio a/d has accounted for by most of the building and

bridges codes in the world.

2.4.3 Axial force

The axial tensile force tends to decrease the shear strength of concrete members

whereas the axial compression increases the shear capacity. However members

with no shear reinforcement subjected to large axial forces may fail in brittle manner,

not giving sufficient warning. The ACI building Code approach for concrete members

subjected to axial compression has been reported as un-conservative by Gupta and

Collins (1993).

2.4.4 Crushing strength of the beam web

Some codes limit the crushing strength of concrete to 0.20 fc′ in case of vertical

stirrups and 0.25fc′ in case of 450 stirrups. ACI limits for the cracks control is given

as

v = 8 fc′ (psi) or v = 0.70 fc′ (MPa) (2.10)

2.4.5 Yielding of stirrups

The yielding of stirrups is also an important failure mode when the beam is subjected

to flexure and shear stress.

The contribution of longitudinal steel also called dowel action was assumed to be

independent of the shear reinforcement initially, but the later work of Chana (1987)

and Sarsam et al.. (1992), proved that this was an incorrect assumption as the

stirrups keep the longitudinal steel bars in place and prevent shear crack from

opening.

The shear capacity of RC beams is mostly determined on the basis of semi-

empirical or statistically derived equations. The shear capacity of the beams without

shear reinforcement Vc is simply added to the stirrups contribution Vs, which is

determined on the basis of parallel truss model with constant 450 inclinations.

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The Artificial Neural Network study of the slender beams by Chabib et al.(2006), has

shown that the assumption of superimposing the individual theoretical contribution of

concrete and steel in resisting the shear, as practiced by most of the building codes

is not justified. It was reported that the effect of shear reinforcement was more, at

lower shear reinforcement ratio than the relatively higher ratio. They further

explained that the shear strength of beams with moderate shear reinforcement is 75-

80% higher than the corresponding values calculated by ACI equation.

2.4.6 Failure of tension chord.

The tension in the longitudinal reinforcement is function of moment at distance “d”

effective depth from the nearest location of maximum moment. The ACI-318

therefore requires that the longitudinal reinforcement must be extended at least

distance “d” from the point where it is no more required.

2.4.7 Failure of stirrups anchorage

At the ultimate loads, the stress in the stirrups approaches the yield strength at every

point, where the inclined crack is intercepted by a stirrup. The upper end of crack

may be close to the compression zone hence the part of the stirrup above the crack

may fail due to slippage or failure of anchorage and hence the stirrups must be

closed looped or anchored by hook or T-heads.

2.4.8 Serviceability failure due to excessive crack width at service load

The ACI limits the maximum shear to 8√fc′ (psi) or 0.70√fc′ (MPa) to control the

crack under the Service loads.

2.4.9 Loading conditions

The shear strength of RC beams also depends on the condition of the loads applied.

M.D Brown et al. (2004) reported on the basis of 1200 tests data of beams that the

shear strength of beams subjected to uniformly distributed loads is more than the

beams subjected to concentrated loads. The current codes provisions are safe for

such types of loading. However they have reported that the provisions of ACI318-05

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are not safe for the beams subjected to concentrated loads between 2d and 6d from

the face of support, which are usually called slender beams.

2.5 Historical development of shear design of reinforced concrete beams

The American Concrete Institute (ACI) Standard Specification No.23 (1920) allowed

the shear stress of 0.025 fc′ subject to a maximum of 0.41 MPa (60 psi) for the

members without shear reinforcement. However the value of shear stress was

increased to 0.03 fc′ where the mechanical anchorage with 1800 hook was provided

for the longitudinal reinforcement.

The distinction between members with and without mechanical anchorage was

removed in 1951 when the shear stress of members without shear reinforced was

revised as 0.03 fc′ and for members with shear reinforcement as 0.12 fc′. The ACI

318-51 was based on 450 truss analogy .i.e. the beam was idealized as parallel

chord with compression diagonal inclined at 450 to the longitudinal reinforcement.

For RC members without web reinforcement, various models for shear transfer were

considered since early 1960’s, which are broadly classified into the following three

major groups; ( ASCE-ACI, 1998)

i. Mechanical or Physical models for structural behaviour and failure.

ii. Fracture mechanics approaches

iii. Non Linear Finite elements analysis

In these models, “Kani tooth model (1964)” has a pioneering role in explaining the

shear flexure cracking of RC beams. With the help of his proposed Kani’s Tooth

Model (1964), he tried to explain the development of secondary diagonal cracks due

to bending of concrete teeth between two adjacent flexural cracks. The concrete

between two flexural cracks resemble the teeth of a comb as shown in Figure 2.10.

These concrete teeth act as cantilevers attached to the compression zone and

loaded horizontally by the shear from the bonded longitudinal reinforcement. The

shear failure of RC beams takes place when one of these cantilevers fails in flexure.

This is sometimes known as famous “Kani’s hypothesis of shear failure”.

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Figure 2.10 Kani’s Tooth Model (Kani, 1964)

Fenwick and Paulay (1968) and Taylor (1974), further evaluated the Kani’s tooth

model. They explained that the teeth of cracked concrete restrict the freely bending

of beams due to resistance from crack friction and dowel action of longitudinal steel.

Many researchers later worked on the tooth model to study the flexure shear

cracking mechanism for RC slender beams without web reinforcement (Macgroger

and Walter, 1967; Hamadi and Regan, 1980; Chana, 1987).

The fracture mechanics approaches are based on the fact that when the diagonal

cracks develop in RC beams, there is a peak tensile stress at the tip of the crack,

which reduces along the crack, also called as softening of cracked zone. In case

where the failure of the RC beams is caused by single critical diagonal crack, the

application of fracture mechanics can develop more reliable results than the

empirical methods. The application of fracture mechanics involves numerical

modeling of the complex tensile stress crack displacement relationship and empirical

relationships are developed in terms of fracture mechanics parameters, having little

explanation of the structural behaviour (ACI-ASCE, 1998)

In the non linear finite element analysis, simple Strut and Tie Model is widely used

for the members like deep beams and other non prismatic members. Due to specific

geometry of the structures, significant re-distribution of the stresses after cracking

requires that sufficient steel is provided in all the direction for the ductile failure of the

RC structure. Application of Strut and Tie Model for more slender beams without

transverse reinforcement may lead to unsafe solution. In such cases the diagonal

crushing strength of concrete is required to be reduced (Collins and Mitchell, 1986).

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Kotsovos (1986) analyzed the shear behaviour of RC beams with web reinforcement

and having shear span to depth ratio greater than 2.5 under two point loads. He

compared the test results with the Finite Element Analysis (FEA) results of the same

beams and made the following significant conclusions:

i. The predicted behaviour of the beams by FEA is incompatible with

the actual shear behaviour at critical section of RC beams with

various arrangements of stirrups

ii. Shear behaviour is associated with the development of tensile stress

within the compression zone and particularly in the region of

compression zone between sections at load and sections twice the

beam depth.

iii. The stirrups resist the tensile stresses within the compression zone

rather than transforming the beam into truss as widely considered.

This negates the concept of truss model most commonly used for the

design of beams with web reinforcement.

iv. The tensile forces develop, when the destruction of bond between

steel and concrete takes place when the bond stresses are critical.

After the bond failure, the transfer of stresses from concrete to steel

is prevented. This is significant observation, which negates the

famous Kani’s hypothesis as due to failure of bond between steel and

concrete teeth; the cantilever action ceases to act.

The findings of Kotsovos (1986), led to a new era of research in the shear analysis

of RC beams, where the tensile forces developed in the compression zone after

formation of the diagonal cracks became the major focus of subsequent researches.

The famous Modified Compression Field (MCFT) theory of Vecchio and Collins

(1986) has been based on the above findings of Kotsovos (1986).

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The latest approaches are however based on the varying truss angle within certain

limits suggested on the basis of theory of plasticity, referred to as “Standard Truss

Model”, with no concrete contribution. Here the shear strength of concrete is

assumed to be mainly due to aggregate interlocking, and dowel action of concrete.

The modification of varying truss angle and concrete contribution was used in the

“Modified Truss Model”

Schaliac et al. (1987), introduced the concepts of D (disturbed) and B (Beam)

regions. The distribution of strain is non-linear in the D- region and linear in the B-

region. Mitchell and Collins (1974) abandoned the concept of linear elasticity and

introduced the concept of “Compression Field Theory” (CFT), for members

subjected to shear and flexure.

Vecchio and Collins (1986), presented the “Modified Compression theory” (MCFT)

which provided a more realistic assessment for wide range of shear reinforcement

and also for the cases with no shear reinforcement.

At the same time the general theory of shear was also developed on the basis of

constitutive laws of friction by determining the strain and deformation in the web.

According to this method, the discrete formation of cracks, the crack spacing, the

width of crack must be determined and equilibrium checked along the crack to

evaluate the crack slip mechanism.

Bentz et al.(2006), introduced the concept of simplified compression field theory for

the shear design of concrete beams. The method provides a simplified version of

MCFT, where the calculation of full load deformation analysis is not needed. The

details of these methods are given in the subsequent sections.

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2.6 Recent approaches in the shear design of reinforced concrete beams

More rational approaches for the shear design of concrete have been evolved in the

last 25 years. The more recent approaches in the shear design of concrete beams

are

i. Compression Field Theory

ii. Truss approaches with concrete contributions

iii. Shear friction theory

iv. Strut and Tie Model.

v. Some latest research work on the shear design of reinforced concrete

beams.

2.6.1 Compression field approaches

In this approach the tensile stresses along the cracked concrete is also taken into

consideration, which was neglected in the earlier approaches. The shear stress

applied to the cracked concrete section causes tensile stresses fsx in the longitudinal

reinforcement, fsy in reinforcement, and compressive stress f2 in the cracked

concrete inclined at angle θ to the longitudinal reinforcement. The value of θ is

determined by considering the deformation of the transverse reinforcement, the

longitudinal reinforcement and diagonally stressed concrete.

The truss models with diagonals were attended by Kupfer (1964) and Baumann

(1972). They presented the approaches for determining the angle θ, assuming that

the cracked concrete and reinforcement were linearly elastic. Methods for

determining the value of θ for full range of loads was developed by Collins and

Mitchell (1974) on the basis of Wagner procedure and the approach was called

“Compression Field theory (CFT)”

The basic assumptions of the CFT are shown in the Figure 2.11, which idealizes

cracked concrete as material with coinciding principal stresses and strain axes,

which are free to adopt their direction as per applied loads.

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Figure 2.11 Compression Field Theories (Mitchell and Collins,1974)

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CFT uses four conditions for the analysis of a section:

1. Equilibrium of the section is considered under external shear force, respective

components of the concrete diagonal compression force, vertical stirrups and

longitudinal steel

2. Strain compatibility of the cracked concrete

3. Stress strain relationship of reinforcement

4. Stress stains relationship of cracked concrete in compression

The shear stress in cracked section due to applied external load causes tensile

stresses fsx in the longitudinal reinforcement and fsy in the transverse reinforcement

besides compressive forces f2 in the cracked concrete, which is inclined at θ to the

longitudinal axis. Due to these stresses, the longitudinal steel is elongated by εx and

transverse reinforcement by εy whereas cracked concrete is compressed by ε2.

On the basis of experimental results Collins (1978), suggested that the following

relationship for the compressive stress max2f required to fail the concrete in

compression.

'

'

max2 /21

6.3

cm

cff

(2.11)

Where 'cf = 28 days cylindrical compressive strength of concrete

m = diameter of the strain circle (ε1+ ε2 ) and

'c = strain of the concrete at which the cylinder stress reaches maximum value of '

cf

For values of 2f less than max2f , the strain is given as

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''2

2ccf

f

(2.12)

Hence it was shown that the diagonally compressed concrete fails at relatively lower

compressive stress as the stress is transmitted through relatively wide crack.

Typically the diagonal cracks are wider than the flexural cracks. When the

longitudinal steel and transverse steel is same in magnitude, then θ is equal to 45

degrees. However practically, the transverse steel is often less than longitudinal

steel and the θ is less than 45o, then significant shear stresses are transmitted

across the cracks. The magnitude of the shear transferred across the crack depends

on the crack width, which is further related to the tensile straining of concrete. The

principal tensile strain is given by the following equation.

221 cot)( xx (2.13)

For shear stress less than the value causing the first yielding of the reinforcement, a

simple expression is given for as follows;

)1

1/()1

1(tan 4

vx nn (2.14)

Where x is longitudinal steel ratio and v transverse steel ratio.

n = modular ration=Es/Ec and '

'

c

cc

fE

(2.15)

Kotsovos M.D (1983), presented the concept of “Compressive Force Path” and

explained that there is no single cause of diagonal shear failure in RC members

Various mechanisms for the shear failure are dependent on the effect of shear force

on the compressive force path. Hence the earlier theories based on unique

mechanism of truss models may not lead to realistic design as the actual behavior of

the structures is not considered. He further argued that even if such procedures are

effective in preventing the diagonal failure in the shear span, localized brittle failure

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due to uni-axial compression of concrete outside the shear span may lead to

collapse of the RC structure. Hence the shear brittle failure can be avoided by

identifying the possible location of such failure on one hand and ensuring the ductile

failure of concrete by increasing its strength to the required level on the other hand.

Kotsovos M.D (1988) while further elaborating his concept of “Compressive Force

Path” observed that the shear resistance associated with the region along the

compressive forces is transmitted to the supports and not by the beam below the

neutral axis. This leads to substantial increase in the concrete strength due to tri-

axial action. He further advised that the relevant provisions of the building codes

may be revised on the basis of “Compressive Force Path”, as the existing

procedures are not helpful in avoiding brittle failure of RC structures. This fact has

been verified by Collins et al (2008), in one their latest work on the shear design

procedures. Kotsovos and Bobrowski (1993) later developed a detailed design

method for flexure and shear of RC beams based on the Compressive Force Path

concept. The proposed new design method can be applied to any structural skeleton

according to them. The brittle failure of the structures can be avoided, while

developing the model on the basis of actual behaviour of RC structures, obtained

from experimental studies of such structures. The critical section for flexure and

shear can be identified with the Compressive Force Path Method and the requisite

reinforcement to avoid brittle failure of RC structures can be provided at these critical

sections, while providing nominal reinforcement in the rest of the structure.

Designing structures by this method would certainly bring economy and reliability,

but extensive experimental research will be required for substituting the existing

flexural and shear theory of beams with the Compressive Force Path Method

proposed by them.

2.6.1.1 Modified Compression Filed Theory (MCFT)

Vecchio and Collins (1986) further developed the CFT into Modified Compression

Field Theory (MCFT) that accounts for the influence of tensile stresses on the post

cracking shear behaviour of concrete. The basic theory has been described in

Figure 2.12

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Figure 2.12 Description of Modified compression Field Theory (Vecchio and Collins1986)

The equilibrium conditions when applied to the Figure 2.12, we get

1cot ff sxx (2.16)

1tan ff syv (2.17)

12 )cot(tan ff (2.18)

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The average principal tensile stress after cracking as suggested by Collins and

Mitchell (1996) is given as

1

15001

crff (psi) (2.19)

Where '4 ccr ff

The conditions at the crack are also required to be checked for equilibrium as

In X-direction 0)cos()cos)sin( crcrcicrxsxcr AAAf

In y-direction 0)sin()sin)cos( crcrcicrvsxcr AAAf

Where crA is the crack plane, ci is the interface shear stress at the crack

From the above equation we can deduce

cotcot cixsxcrf (2.20)

tantan civsxcrf (2.21)

Form these equations; it is apparent that as ci at a crack increases, the stress in the

longitudinal reinforcement increases but the stress in the transverse reinforcement

decreases. On the basis of work by Walraven (1981) and Bhide and Collins (1986),

the following limitation was imposed the shear stress at the crack by Vecchio and

Collins(1989).

63.0

2430.0

16.2 '

a

w

f cci ( psi and in) (2.22)

16

2430.0

18.0 '

a

w

f cci (MPa, mm) (2.23)

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a; stands for aggregates width.

w ; Width of crack

The crack width can be obtained as average crack width

msw 1

mymxm ss

s

cossin

/1 (2.24)

)(25.010

2 1x

bxxxmx

dk

scs

(2.25)

)(25.010

2 1v

byyymy

dk

scs

(2.26)

xc , yc distance between midsection and longitudinal and transverse reinforcement,

respectively, xs ys spacing of longitudinal and transverse reinforcement,

respectively

1k : Coefficient for bond characteristics of bars (0.4 for deformed bars, 0.8 for plain bars)

yx bb , Bar diameter of longitudinal and transverse reinforcement, respectively.

Under high loads, the average strain in the stirrups exceeds the yield strain and we

get the following equation

tan

63.0

2430.0

16.2tan

'

1

a

wf

f cci (psi and in ) (2.27)

tan

16

2430.0

18.0tan

'

1

a

wf

f cci (MPa, mm) (2.28)

This equation limits the principal tensile stress in cracked concrete, so that possible

failure of the aggregates interlock mechanism is taken into account in the MCFT,

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MCFT is an improvement of CFT, as it can predict the shear strength of those

members without shear reinforcement.

The design procedure for shear design of RC member by MCFT assumes that the

shear stress in the web is equal to the shear force divided by the effective shear

area bwdv and that the shear steel yields at failure under equilibrium. The following

steps are involved;

Vn = Vc + Vs + Vp (2.29)

Vc = Shear Strength provided by the cracked concrete.

Vs = Shear strength provided tensile stress in stirrups

Vp = Vertical component of applied Pre-stressed tendons.

pyvvwn VfAdbfV )cot(cot1 (2.30)

pyvvwcn VfAdbfV )cot(' (2.31)

β = Concrete tensile stress factor indicating the ability of diagonally cracked concrete

to resist shear. dv ≈ 0.9 d = the minimum web depth.

The shear stress resisted by the web of beam is function of the longitudinal strain

and decreases with its increase. The highest value of longitudinal strain is

approximated to the strain in the tension chord and is given by

pspss

popsuuvux AEAE

fAVNdM

cot5.05.0/ < 0.002 (2.32)

Where fp0 = stress in the tendons when the surrounding concrete is at zero stress

and is taken as 1.1 times the effective stress in the pre-stressing steel after all

losses.

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Asp = Area of the pre-stressed longitudinal reinforcement.

As = Area of the non-pre-stressed longitudinal reinforcement.

Nu = Ultimate applied load which is taken as positive when the tensile force is

resulted and negative when compression.

Mu = Ultimate moment at the section.

For RC members containing at least the minimum shear reinforcement, the values of

β and θ can be determined from the Figure 2.13, given on next page.

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Figure 2.13 values of β and θ for RC members with at least minimum shear reinforcement.

(Vecchio and Collins1986).

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For the design of RC members without shear reinforcement or shear steel less than

the minimum shear, the diagonal cracks are widely spaced as compared to beams

with shear steel due to reduced inclination of θ. For the conditions, when the value of

θ becomes 90o, the spacing is denoted by Sx. The maximum value of Sx is 2000 mm

and the maximum aggregates sizes a are taken as 19mm. For RC members with no

or less than minimum shear steel, values of θ and β for depends on the longitudinal

strain parameter, which in turn depends on the distance between of the longitudinal

steel in the vertical axis.

For RC beams having aggregates sizes other than 19 mm and less than minimum

shear steel, the equivalent spacing Sex can be determined as

Sex= Sx 16

35

a (2.33)

The values of θ and β for members having less than the minimum shear steel, is

determined from Figure 2.14

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Figure 2.14 values of β and θ for RC members with less than minimum shear reinforcement

(Vecchio and Collins1986).

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The following additional considerations and precautions are required while shear

designing of RC members by MCFT.

The first section to be checked for shear is at distance 0.5 dv Cot θ form the

face of support, which is approximately equal to d.

The required amount of shear reinforcement at other locations can be

checked at 10th points of the span.

To avoid the failure due to yielding of the longitudinal reinforcement, the

following equation must be satisfied

psspys fAfA ≥

dv

Mu

+

VpVs

VuNu50.05.0

Cot θ ] (2.34)

Value of in radians.

The reinforcement provided at the supports must be detailed such that the

tension force can be safely resisted which is given as ;

T =

ps

u VVV

50.0

Cot θ but T ≥ 0.50

p

u VV

Cot θ (2.35)

The longitudinal reinforcement must be extended by a distance “d” beyond

the point where it is no longer required to resist the flexure.

2.6.1.2 Simplified Compression Filed Theory (SCFT)

The solution of shear strength problem with the MCFT involves determination of two

important parameters β and θ. However by hand solution of such problem is difficult

as it involves a tedious process. Computer software like Response-2000 can be

used to determine the load deformations response of the reinforced concrete

membrane elements.

Bentz et al. (2006), proposed a simplified MCFT for quick and convenient calculation

of the shear strength of RC beams. This method according to authors provided

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excellent prediction of shear strength of RC concrete beams with only 13%

coefficient of variation.

According to the basic assumptions of MCFT, at yield point, the strain in transverse

reinforcement has to be more than 0.002 and the strain in the concrete along the

crack has also to be about 0.002. Hence it was shown by Bentz et al (2006) that the

maximum shear stress will be 0.28f’c, whereas for very low value of εx , it was

deduced that the failure shear stress is 0.32f’c . However as conservative estimate a

value of 0.25f’c was selected for estimating the shear stress of RC beams before

yielding of the transverse reinforcements. Based on these assumptions, the value of

β proposed was given as;

15001

cot33.0

(2.36)

The value of β must also satisfy the equation given as

)16(4231.0

18.0

gaw (2.37)

The crack width w is determined by the crack spacing s and principal tensile

strain 1 as shown in Figure 2.15 and ga represents the maximum coarse aggregate

size.

Figure 2.15 Transmission of forces across the crack.( Bentz et al, 2006)

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For elements with no transverse reinforcement, Eq. 2.37 can be expressed as

sin/686.031.0

18.0

1xes (2.38)

For high strength concrete particularly where 'cf > 70 MPa (10,000 psi), the concrete

matrix is strong enough and the shear cracks break through the aggregates and

ga is taken as zero. For maximum post cracking shear capacity of members without

transverse reinforcement will occur when Eq. 2.37 and Eq. 2.38 will give the same

values. This requirement would lead to the following equation for

1

1

5001

sin/258.10568tan

xes

(2.39)

The longitudinal strain x is related to the principal strain 1 as

1 = 5001(15000

cot)cot1(

1

42

x (2. 40)

The value of and concrete shear strength for members with no transverse

reinforcement decreases, with the increase in the crack spacing xes . That is why that

long RC beams, with no transverse reinforcement fail at lower shear stress, than

smaller beams, as the crack spacing increase in the large beams. This is also

referred to as size effect in shear.

Thus for members without transverse reinforcement, the value of depends on

the longitudinal strain x and crack spacing parameter xes . Bentz et al, called these

two effects as “strain effect factor” and “Size effect factor” respectively.

They further proposed, a simple and conservative equation for , which combines

x and xes as follows

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exx s

1000

1300.

15001

4.0

(2.41)

The simplified MCFT uses the following equation for determination of

deg752500

88.0)(7000deg29( xex

sree (2.42)

Hence the simplified MCFT, determines the value of shear strength of RC members

when several iterations are made to reach at the converged values of and

Bentz et al (2006) used the experimental results of pure shear tests of 112 beams

data to compare the experimental shear values and shear values determined by full

MCFT and simplified MCFT as well as ACI-318. The comparison has been given in

Table 2.1

The coefficient of variation (CoV) for full MCFT has been worked out as 12.2% and

for simplified MCFT as 13%. For ACI, equation the CoV is 46.7%. The comparison

shows that the simplified MCFT gives results very close to the full MCFT, hence

simplified MCFT provides a relatively quicker method for the design of RC member

failing in shear. Table 2.1 shows summary of the comparison of experimental results

with the full MCFT, simplified MCFT and ACI equation for shear strength of RC

beams. Simplified MCFT, when compared with the detailed MCFT results have

given almost similar results.

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Table 2.1 Comparison of experimental results with the full MCFT, simplified MCFT and ACI

equation for shear strength of RC beams.( Bentz et al, 2006)

Beam 'cf

MPa

x

%

yxf

MP

a

xs

mm

'/ cyz ff

Axial

load

/xf

'exp/ cf

predicted /exp

Full

MCFT

Simp

MCFT

ACI

Vecchio and Collins ( 1982) ; ag =6 mm

PV1 34.5 1.79 483 51 0.235 0 0.23 0.93 0.96 1.37

PV2 23.5 0.18 428 51 0.033 0 0.049 1.47 1.41 0.48

PV3 26.6 0.48 662 51 0.120 0 0.115 0.95 0.96 0.63

PV4 26.6 1.03 242 51 0.096 0 0.109 1.12 1.13 0.68

PV5 28.3 0.74 621 102 0.163 0 0.150 0.91 0.92 0.80

PV6 29.8 1.79 266 51 0.159 0 0.153 0.95 0.95 0.84

PV10 14.5 1.79 276 51 0.190 0 0.27 1.06 1.10 1.05

PV11 15.6 1.79 235 51 0.197 0 0.23 0.98 0.98 0.90

PV12 16.0 1.79 469 51 0.075 0 0.196 1.09 1.19 1.24

PV16 21.7 0.74 255 51 0.087 0 0.099 1.12 1.12 0.62

PV18 19.5 1.79 431 51 0.067 0 0.156 1.08 1.08 1.10

PV19 19.0 1.79 458 51 0.112 0 0.21 0.95 1.06 1.10

PV20 19.6 1.79 460 51 0.134 0 0.22 0.93 1.00 1.04

PV21 19.5 1.79 458 51 0.201 0 0.26 0.91 1.03 1.14

PV22 19.6 1.79 458 51 0.327 0 0.31 0.98 1.24 1.38

PV26 21.3 1.79 456 51 0.219 0 0.25 0.88 1.02 1.18

PV27 20.5 1.79 442 51 0.385 0 0.31 0.96 1.24 1.41

PV30 19.1 1.79 437 51 0.249 0 0.27 0.88 1.07 1.18

Bhide and Collins ag = 9mm

PB11 25.9 1.09 433 90 0 0 0.049 1.02 1.03 0.75

PB12 23.1 1.09 433 90 0 0 0.066 1.28 1.30 0.96

PB4 16.4 1.09 423 90 0 1.00 0.071 1.25 1.35 1.40

PB6 17.7 1.09 425 90 0 1.00 0.065 1.28 1.30 1.33

PB7 20.2 1.09 425 90 0 1.90 0.043 0.97 1.05 1.34

PB8 20.4 1.09 425 90 0 3.00 0.039 0.99 1.08 1.74

PB10 24.0 1.09 433 90 0 5.94 0.023 0.92 0.99 2.10

PB13 23.4 1.09 414 90 0 0 0.201* 1.04 1.06 1.06

PB24 20.4 1.10 407 90 0 0 0.236* 1.08 1.10 1.10

PB15 38.4 2.02 485 45 0 0 0.051 1.02 1.16 0.95

PB16 41.7 2.02 502. 45 0 1.96 0.035 0.98 1.13 1.61

PB14 41.1 2.02 489 45 0 3.01 0.037 1.13 1.34 2.32

PB18 25.3 2.20 402 45 0 0 0.067 1.06 1.13 1.02

PB19 20.0 2.20 411 45 0 1.01 0.064 0.98 1.09 1.40

PB20 21.7 2.20 424 45 0 2.04 0.065 1.16 1.33 2.25

PB28 22.7 2.20 424 45 0 1.98 0.067 1.23 1.40 2.32

PB21 21.8 2.20 402 45 0 3.08 0.065 1.26 1.46 3.09

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Table 2.1 Cont’d Beam '

cf

MPa

x

%

yxf

MPa

xs

mm

'/ cyz ff

Axial load

/xf

'exp/ cf

predicted /exp

Full

MCFT

Simp

MCFT

ACI

PB22 17.6 2.20 433 45 0 6.09 0.059 1.13 1.38 4.62

PB25 20.6 2.20 414 45 0 4.05 0.485* 1.10 1.10 1.10

PB29 41.6 2.02 496 45 0 2.02 0.036 1.02 1.15 1.69

PB30 40.04 2.02 496 45 0 2.96 0.037 1.10 1.27 2.29

PB31 43.4 2.02 496 45 0 5.78 0.026 0.97 1.18 3.13

Yamaguchi et al ag =20mm

S21 19.0 4.28 378 150 0.849 0 0.34 0.89 1.37 1.50

S31 30.2 4.28 378 150 0.535 0 0.28 0.80 1.10 1.52

S32 30.8 3.38 381 150 0.481 0 0.28 0.87 1.14 1.58

S33 31.4 2.58 392 150 0.323 0 0.26 0.86 1.04 1.46

S34 34.6 1.91 418 150 0.230 0 0.21 0.91 0.92 1.25

S35 34.6 1.33 370 150 0.142 0 0.163 1.15 1.15 0.97

S41 38.7 4.28 409 150 0.452 0 0.31 0.95 1.23 1.91

S42 38.7 4.28 409 150 0.452 0 0.33 1.02 1.32 2.06

S43 41.0 4.28 409 150 0.427 0 0.29 0.91 1.16 1.86

S44 41.0 4.28 409 150 0.427 0 0.30 0.94 1.19 1.91

S61 60.7 4.28 409 150 0.288 0 0.25 0.90 1.01 1.98

S62 60.7 4.28 409 150 0.288 0 0.26 0.91 1.03 2.01

S81 79.7 4.28 4.9 150 0.220 0 0.20 0.92 0.92 1.82

S82 79.7 4.28 409 150 0.220 0 0.20 0.92 0.93 1.83

Andre ag =9mm, KP ag =20mm

TPI 22.1 2.04 450 45 0.208 0 0.26 0.92 1.02 1.21

TPIA 25.6 2.04 450 45 0.179 0 0.22 0.89 0.90 1.14

KPI 25.2 2.04 430 89 0.174 0 0.22 0.89 0.90 1.12

TP2 23.1 2.04 450 45 0.199 3.00 0.114 1.01 1.02 0.72

KP2 24.3 2.04 430 89 0.180 3.00 0.106 1.03 1.06 0.68

TP3 20.8 2.04 450 45 0 3.00 0.061 1.27 1.34 2.75

KP3 21.0 2.04 430 89 0 3.00 0.054 1.15 1.22 2.47

TP4 23.2 2.04 450 45 0.396 0 0.35 1.09 1.39 1.68

TP4A 24.9 2.04 450 45 0.369 0 0.35 1.14 1.41 1.77

KP4 23.0 2.04 430 89 0.381 0 0.30 0.94 1.20 1.44

TP5 20.9 2.04 450 45 0 0 0.093 1.49 1.42 1.28

KP5 20.9 2.04 430 89 0 0 0.063 1.01 0.98 0.87

Krischner and Khalifa ag = 10 mm

SEI 42.5 2.92 492 72 0.110 0 0.159 0.90 0.94 1.04

SE5 25.9 4.50 492 72 0.855 0 0.31 0.89 1.26 1.60

SE6 40.0 2.92 492 72 0.040 0 0.094 0.95 0.99 1.02

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Table 2.1 Cont’d Beam '

cf

MPa

x

%

yxf

MPa

xs

mm

'/ cyz ff

Axial load

/xf

'exp/ cf

predicted /exp

Full

MCFT

Simp

MCFT

ACI

Porsaz and Beidermann; ag = 10 mm

SE11 70.8 2.93 478 34 0.063 0 0.093 0.83 0.90 0.91

SE12 75.9 2.94 450 72 0.060 0 0.098 0.96 1.01 0.99

SE13 80.5 6.39 509 54 0.115 0 0.149 0.82 0.86 1.34

SE14 60.4 4.48 509 72 0.378 0 0.30 1.03 1.19 2.32

Marti and Mayboom; ag = 13 mm

PPI 27 1.95 480 108 0.116 0 0.183 0.98 1.02 1.02

PP2 28.1 1.59 563 108 0.111 -0.38 0.196 1.06 1.08 0.95

PP3 27.7 1.24 684 108 0.113 -0.80 0.199 1.03 1.02 0.86

Vecchio et al ; ag = 10 mm

PA1 49.9 1.65 606 45 0.086 0 0.126 0.94 1.03 0.95

PA2 43 1.66 606 45 0.100 0 0.145 0.94 1.02 0.96

PHS1 72.2 3.25 606 44 0 0 0.037 1.07 1.08 0.97

PHS2 66.1 3.25 606 44 0.033 0 0.093 1.13 1.25 1.27

PHS3 58.4 3.25 606 44 0.074 0 0.140 0.99 1.13 1.20

PHS8 55.9 3.25 606 44 0.115 0 0.193 1.02 1.15 1.45

PC1 25.1 1.65 500 50 0.163 0 0.197 0.84 0.87 0.99

Pang and Hsu ag = 19 mm

A2 41.3 1.19 463 189 0.134 0 0.136 1.01 1.01 0.87

A3 41.6 1.79 447 189 0.192 0 0.190 0.98 0.99 1.23

A4 42.5 2.98 470 189 0.330 0 0.28 0.97 1.11 1.82

B1 45.2 1.19 463 189 0.056 0 0.092 1.01 1.08 0.87

B2 44.1 1.79 447 189 0.126 0 0.146 0.96 0.96 0.97

B3 44.9 1.79 447 189 0.057 0 0.102 0.94 1.05 0.96

B4 44.8 2.99 470 189 0.057 0 0.119 0.92 1.10 1.12

B5 44.8 2.98 470 189 0.129 0 0.177 0.89 0.96 1.16

B6 42.8 2.98 470 189 0.194 0 0.23 0.95 0.96 1.53

Zhang and Hsu ag = 19 mm

VA1 95.1 1.19 445 94 0.056 0 0.068 1.04 1.20 0.75

VA2 98.2 2.39 409 94 0.100 0 0.103 1.03 1.03 1.02

VA3 94.6 3.59 455 94 0.173 0 0.163 0.94 0.94 1.59

VA4 103.1 5.24 470 94 0.239 0 0.22 1.00 0.91 2.21

VB1 98.2 2.39 409 94 0.054 0 0.080 1.01 1.07 0.91

VB2 97.6 3.59 455 94 0.054 0 0.097 0.95 1.13 1.10

VB3 102.3 5.98 445 94 0.052 0 0.099 0.90 1.08 1.17

VB4 96.9 1.79 455 189 0.027 0 0.052 0.97 1.12 0.85

Average 1.01 1.11 1.40

CoV 12.2 13.0 46.7

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2.6.2 Truss approaches with concrete contributions

In the traditional approaches for the shear design of concrete beams, it is assumed

that compression struts are formed parallel to cracks and no stresses are transferred

across the cracks, hence the concrete contribution due to transfer of stresses

across the cracks is usually neglected, but this often leads to conservative results.

The more recent approaches also take into account the following two contributions;

Tensile stresses that exists transverse to the crack.

Shear stress that is transferred along the inclined crack by aggregates

interlocking.

The truss model was, however later on modified by Ramirez and Breen (1991) and

the nominal shear strength of concrete was given as

Vn = Vc + Vs (2.43)

The Vc suggested by Rameriz and Breen ( 1991) is given as;

Vn = dbwcr 32

1 (2.44)

Here cr = Shear stress resulting in the first diagonal tension cracking in the conc.

In some latest research work, the original truss method has been changed into the

variable angle truss model. This model accounts for the fact that the concrete struts

are generally not inclined at 45°, but may instead be in a range from about 25° to

65°. The new proposed model has been shown in Figure 2.16 (Mitchel,1986)

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Figure 2.16 Variable truss Model of RC beams. (Mitchel,1986)

2.6.3. Shear friction approach

Shear friction approach was first introduced by Birkeland and Birkeland (1966), to

deal with transfer of forces across the joints in pre-cast concrete construction as

shown in Figure 2.17. When concrete is subjected to shear and compression forces,

cracks are formed and the roughness of the crack will create separation δ between

the two halves. The reinforcement is provided across the interface, provides an

external clamping force T.

The roughness may be visualized as series of saw toothed frictionless fine saw

toothed ramp having a slope of tanθ. The separation is sufficient to yield

reinforcement across the crack. This nominal shear resistance of concrete is given

as

Vn = μ Asfy (2.45)

Where μ = 1.7 for monolithic concrete

μ = 1.4 for artificial roughened concrete and 0.80 to 1.0 for ordinary.

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Figure 2.17Shear Friction Hypothesis of Birkeland and Birkeland (1966)

The shear friction was adopted by ACI-318 code in 1973 and the value of μ has

been reduced as against suggested by Birkeland and Birkeland (1966) . The

Canadian Code has recently introduced modified friction formula.

2.6.4 Strut and Tie Model (STM)

It is essentially an equilibrium model where the designer specifies at least one load

path and ensures that no part of this path has been overstressed. The term truss is

used for Disturbed or D-region and term B is used for Beam or B-region, although

both the terms designate an assemblage of pin jointed, Uni-axially stressed

compression or tension members. In B-region the beam behaviour is expected .i.e.

plane section remains plane and uniform compression field can be found in

response to shearing load. In design of D-region, complex load paths emulate from

the concentrated load, which converge towards support or flow onwards and hence

arch action is exhibited.

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Strut and Tie Model (STM) is one of the most rational and relatively simple design

approaches for non flexural members. The STM has been used in Europe for many

years in Europe and has been adopted by Canadian Code in 1984, AASHTO LRFD

bridge design in 1994 (James et al. 2003), It was incorporated in ACI building Code

381-02 as appendix A and later was recommended as an optional design procedure

for disturbed region in ACI 318-06 building code.

The STM is based on lower bond theory of plasticity assuming that steel and

concrete are frequently plastic and efficiency factors are applied to uni-axial strength

of concrete to account for concrete softening. The STM design is not unique as it

depends on the shape of non flexural structure, material, design perception and

understanding of the structure. However the method has opened a great venue for

research in the design of disturbed regions.

The joint ACI-ASCE Committee 445(1998) report on Shear and Torsion has given

detailed commentary on the STM. The Strut and Tie Model has been used for the

design of disturbed regions like Deep beams, Dapped ended beam, corbels,

brackets, pile caps, opening in slabs and non prismatic structural members. Further

details of the STM have been given in chapter No. 5, under Shear Design of

Disturbed Region.

2.6.5: Some latest research on shear design of reinforced concrete beams.

Zararis P.D (2003), has reported a new concept for the design of shear

reinforcement, in which the shear strength of beam without shear reinforcement is

expressed as follows;

bdfd

cd

d

aV ctcr )()(2.02.1

(2.46)

Where dd

a)(2.02.1 ≥ 0.65 ( d in m )

f ct = 0.30 fc′ 2/3

c; depth of compression zone which is determined by the quadratic equation;

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0)/(

600.600

cc f

dd

d

c

fd

c (2.47)

For beams with shear reinforcement, the steel contribution is added which is

expressed as

Vs = ( 0.50 + 0.25 d

a) ρ vf yv b d

The shear of RC beams in complete form is as follows:

bdfd

af

d

cd

d

ayvvct )25.05.0()..2.02.1 . (2.48)

Zararis (2003) coampred experiemntal results of various researchers with the

theoretical shear strength of RC beams worked out with the equtaions proposed by

him and reported the least Coefficient of Variation ( CoV) for 174 beams data. The

deatils of comparison has been given in Table 2.2 Zararis (2003) reported that the

coefficient of variation proposed by his new theory was the least one, when

compared with ACI and EC-02 equations.

Arsalan G (2007) developed the following equation for predicting the diagonal

cracking shear stress of beams without stuirrups.

65.050.0 )(02.0)(15.0 cccr ff For Normal Strength Concrete (2.49)

65.0)(12.0 ccr f For High Strength Concrete (2.50)

By comparing the test values and predicted values from the propsoed model, it was

deduced that the proposed equation gave same results as the ACI simplified

equation.

Guray A (2008), further proposed the following expressions for the shear strength of

RC beams with stirrups;

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wwccn fff 65.050.0 )(02.0)(15.0 For normal strength concrtete beams (2.51)

wwccn fff 65.050.0 )(02.0)(12.0 For high strength Concrete beams (2.52)

Chi et al (2007) proposed a unified theoretical model for the shear strength of beams

with and without web reinforcement and observed that the proposed strength model

can address the slender beams in a better way.

Somo and Hong (2006) analysed the modelig error of the shear prediction models

proposed by ACI, CSA, MCFT, Shear firction method and Zustty’s equation for data

base of 1146 beams and reported that the Zustty’s equation has given the best

model amongst the models studied. However for beams with strirrups, MCFT

provides most accurate results.

Tompos and Frosch (2002) studied the effect of various parameters like beam size,

longitudinal steel abd stirrups and reported that the current shear design provisons

of ACI are based on database of the beams sizes, not commonly used sizes in

actual practice. They further reported that for longitudinal steel of 1% or low, the

shear strength of beams has been reduced for all sizes of beam.

Bokhari.I and Ahamd.S (2008) analyzed the data of shear strength of 122 HSRC

beams and reported that the shear provisons are conservative for a/d less than 2.5.

Shear Strenghtening of RC and pre-stressed beams with Carbon Fibre Reinforced

Polymers ( CRFP) has been increasisgnly used in the recent years. Whiteland and

Ibell ( 2005) worked on the fibre reinforced RC beams and gave some guidlines for

developing the basic design methods.

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Table 2.2 Comparison of the shear strength of RC beams proposed by Zararis , ACI and

EC-2 ( Zararis P.D,2003)

'cf

MPa

b

cm

d

cm

da /

Reinforcement

Exp

uV

kN

ACI EC-2 Theory of

Zararis.P

%

'

%

v yvvf

MPa

uV

kN

ACIu VV /

uV

kN

ECu VV /

uV

kN

theoryu VV /

Leonhardt and Walther ( 1962)

30.4 19 27 2.78 2.47 0.33 0.41 1.52 170.5 131 1.301 139.9 1.218 168.6 1.011

28.2 19 27 2.78 2.47 0.33 0.42 1.63 186.0 135 1.378 141.6 1.314 173.7 1.070

30.4 19 27 2.78 2.47 0.33 0.59 1.54 187.5 132 1.420 140.8 1.331 169.9 1.103

30.4 19 27 2.78 2.47 0.33 0.58 1.61 189.0 135.6 1.394 144.0 1.312 174.1 1.085

Bresler and Scorelies (1963)

24.1 30.7 46.6 3.92 1.80 0.18 0.10 0.33 233.2 170.7 1.366 179.1 1.302 210.9 1.105

24.3 30.5 46.4 4.93 2.28 0.18 0.10 0.33 244.8 172.4 1.420 183.5 1.334 216.1 1.132

24.8 23.1 46.1 3.95 2.43 0.24 0.15 0.48 222.5 147.1 1.512 154.2 1.443 185.3 1.200

23.2 22.9 46.6 4.91 2.43 0.24 0.15 0.48 200.2 142.5 1.405 149.4 1.340 191.0 1.048

29.6 15.5 46.4 3.95 1.80 0.36 0.20 0.65 156.1 114.9 1.358 120.8 1.292 143.8 1.085

23.8 15.2 46.4 4.93 3.66 0.37 0.20 0.66 161.5 110.5 1.462 111.4 1.450 156.5 1.031

Bresler and Scorelies (1964)

25.1 30.5 46.0 3.98 1.69 0.18 0.10 0.35 168.4 171.7 0.981 179.2 0.940 206.5 0.816

23.6 22.9 45.7 4.01 2.28 0.24 0.15 0.51 172.7 144.8 1.192 151.4 1.141 188.4 0.917

24.4 15.5 45.8 4.00 1.67 0.35 0.20 0.69 118.6 110.1 1.077 111.0 1.068 137.1 0.865

26.3 30.5 45.7 4.01 1.71 0.18 0.10 0.35 214.6 173.2 1.239 183.3 1.171 211.3 1.015

23.2 22.9 45.9 3.99 2.26 0.23 0.15 0.51 203.9 144.6 1.409 150.6 1.354 192.0 1.061

26.7 15.2 46.0 3.96 1.69 0.36 0.20 0.70 143.3 111.8 1.282 114.1 1.255 141.3 1.014

25.2 30.5 46.2 3.95 1.76 0.18 0.10 0.35 219.8 173.1 1.269 182.0 1.208 212.8 1.032

26.5 23.1 46.0 3.97 2.34 0.24 0.15 0.51 201.9 152.3 1.325 161.8 1.247 198.2 1.018

24.9 15.5 46.0 3.97 1.75 0.35 0.20 0.69 142.6 111.4 1.280 113.4 1.257 142.3 1.002

26.3 30.5 46.1 3.96 1.77 0.18 0.10 0.35 241.8 175.2 1.380 186.1 1.300 241.8 1.124

26.3 30.5 46.0 3.97 1.77 0.18 0.10 0.35 207.6 175.0 1.186 186.0 1.116 207.6 0.968

Bahl

26.8 24 30 3 1.26 0.22 0.15 0.66 130.0 112.4 1.157 117.7 1.104 138.1 0.941

25.1 24 60 3 1.26 0.11 0.15 0.66 252.5 220.7 1.144 196.0 1.288 246.7 1.023

26.3 24 90 3 1.26 0.07 0.15 0.66 372.5 335.2 1.111 299.1 1.245 332.6 1.119

25.4 24 120 3 1.26 0.05 0.15 0.66 468.0 442.9 1.057 393.7 1.189 440.6 1.062

Placas and Regan

26.7 15.2 27.2 3.36 1.46 0.34 0.21 0.58 79.6 61.2 1.300 67.5 1.179 78.7 1.011

29.6 15.2 27.2 3.36 1.46 0.34 0.43 1.15 104.5 86.6 1.207 91.9 1.137 111.9 0.934

29.6 15.2 27.2 3.36 0.98 0.34 0.21 0.58 75.5 62.0 1.218 65..5 1.153 73.3 1.030

26.2 15.2 27.2 3.36 0.98 0.34 0.21 0.58 89.5 61.9 1.445 71.9 1.245 83.6 1.070

33.9 15.2 27.2 3.60 4.16 0.37 0.21 0.58 117.3 70.6 1.661 82.0 1.431 105.7 1.109

32.3 15.2 27.2 3.60 4.16 0.37 0.43 1.15 160.0 93.2 1.717 101.2 1.580 137.2 1.166

29.0 15.2 27.2 3.36 1.46 0.34 0.14 0.38 89.5 54.4 1.645 62.6 1.430 69.0 1.277

29.9 15.2 27.2 3.60 4.16 1.49 0.43 1.15 149.6 91.8 1.629 98.4 1.521 130.0 1.150

31.6 15.2 27.2 3.60 4.16 2.96 0.43 1.15 149.6 92.8 1.611 100.4 1.490 125.6 1.191

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74

Table 2.2 Cont’d '

cf

MPa

b

cm

d

cm

da /

Reinforcement

Exp

uV

kN

ACI EC-2 Theory of

Zararis.P

%

'

%

v yvvfMPa

uV

kN

ACu VV /

uV

kN

ECu VV /

uV

kN

theoryu VV /

12.8 15.2 27.2 3.36 1.46 0.34 0.21 0.58 70.0 50.7 1.381 49.0 1.428 68.3 1.025

31.3 15.2 27.2 3.36 1.46 0.34 0.21 0.58 84.5 64.0 1.320 72.6 1.164 82.8 1.020

30.3 15.2 27.2 3.36 1.46 0.34 0.43 1.15 119.8 87.0 1.377 92.7 1.292 112.4 1.066

42.5 15.2 27.2 3.36 1.46 0.34 0.210 0.58 89.9 70.2 1.281 84.2 1.068 86.1 1.044

48.1 15.2 27.2 3.60 4.16 0.37 0.43 1.15 160.0 101.5 1.576 119.0 1.344 149.4 1.071

29.5 15.2 27.2 4.50 1.46 0.34 0.21 0.58 79.6 62.2 1.280 70.7 1.126 84.5 0.942

30.9 15.2 27.2 5.05 4.16 2.61 0.21 0.58 98.6 66.5 1.482 78.4 1.258 96.7 1.020

30.8 15.2 27.2 3.60 4.16 2.61 0.21 0.58 111.9 68.8 1.626 78.2 1.430 92.6 1.208

31.6 15.2 27.2 3.60 4.16 2.61 0.84 2.25 191.9 138.3 1.387 141.3 1.358 190.1 1.009

Swamy and Andriopoulos

29.4 7.6 9.5 3.00 1.97 0.22 0.16 0.44 15.6 10.2 1.522 13.7 1.142 14.7 1.061

29.4 7.6 9.5 3.00 1.97 0.22 0.38 0.79 18.1 12.8 1.417 15.9 1.138 17.9 1.005

29.4 7.6 9.5 3.00 1.97 0.22 0.43 1.09 20.5 14.9 1.372 17.9 1.146 20.6 0.995

28.7 7.6 9.5 4.00 1.97 0.22 0.06 0.17 13.6 8.0 1.695 11.7 1.162 12.2 1.114

28.3 7.6 13.2 3.00 3.95 0.16 0.12 0.31 25.4 13.9 1.828 17.2 1.480 22.2 1.144

25.9 7.6 13.2 3.00 3.95 0.16 0.34 0.61 27.8 16.5 1.682 19.0 1.460 25.4 1.094

25.9 7.6 13.2 3.00 3.95 0.16 0.60 1.33 28.9 23.8 1.216 25.5 1.132 34.1 0.848

28.3 7.6 13.2 4.00 3.95 0.16 0.12 0.31 20.0 13.3 1.500 17.2 1.166 22.3 0.897

25.9 7.6 13.2 4.00 3.95 0.16 0.34 0.61 25.6 16.0 1.600 19.0 1.344 26.3 0.973

28.3 7.6 13.2 5.00 3.95 0.16 0.12 0.31 18.9 13.0 1.454 17.2 1.100 22.4 0.844

Mphonde and Frantz

22.1 15.2 29.8 3.60 3.36 0.31 0.12 0.35 76.3 56.6 1.348 63.0 1.210 82.9 0.920

39.9 15.2 29.8 3.60 3.36 0.31 0.12 0.35 93.9 68.4 1.373 86.5 1.085 98.0 0.958

59.8 15.2 29.8 3.60 3.36 0.31 0.12 0.35 97.9 78.6 1.245 109.0 0.898 108.0 0.906

83.0 15.2 29.8 3.60 3.36 0.31 0.12 0.35 111.4 82.9 1.344 132.1 0.843 117.0 0.952

27.9 15.2 29.8 3.60 3.36 0.31 0.26 0.70 95.4 76.7 1.244 85.5 1.116 110.9 0.860

47.1 15.2 29.8 3.60 3.36 0.31 0.26 0.70 120.5 88.2 1.366 109.3 1.102 124.0 0.952

68.6 15.2 29.8 3.60 3.36 0.31 0.26 0.70 151.2 98.5 1.535 132.3 1.143 134.0 1.128

82.0 15.2 29.8 3.60 3.36 0.31 0.26 0.70 115.8 98.7 1.173 145.4 0.796 138.8 0.834

28.7 15.2 29.8 3.60 3.36 0.31 0.38 1.03 138.0 92.7 1.500 99.7 1.394 133.1 1.044

46.6 15.2 29.8 3.60 3.36 0.31 0.38 1.03 133.4 102.9 1.297 121.9 1.095 145.3 0.918

69.6 15.2 29.8 3.60 3.36 0.31 0.38 1.03 161.6 113.9 1.419 146.4 1.103 155.9 1.036

82.8 15.2 29.8 3.60 3.36 0.31 0.38 1.03 150.0 119.3 1.257 159.3 0.941 160.7 0.933

Elzanatly, Nilson, and State

62.8 17.8 26.6 4.0 3.30 0.13 0.17 0.65 149.1 97.5 1.530 132.5 1.125 139.8 1.066

40.0 17.8 26.6 4.0 2.50 0.13 0.17 0.65 111.3 83.7 1.329 105.3 1.057 117.0 0.951

20.7 17.8 26.6 4.0 2.50 0.13 0.17 0.65 78.2 70.3 1.113 77.7 1.006 94.8 0.825

Johnson and Ramirez

36.4 30.4 53.8 3.10 2.49 0.79 0.14 0.69 338.8 293.0 1.156 301.9 1.122 346.2 0.979

36.4 30.4 53.8 3.10 2.49 0.79 0.07 0.35 222.1 237.4 0.935 251.8 0.882 274.2 0.810

72.4 30.4 53.8 3.10 2.49 0.79 0.07 0.35 263.0 295.5 0.890 368.2 0.714 324.3 0.811

72.4 30.4 53.8 3.10 2.49 0.79 0.07 0.35 316.0 295.5 1.069 368.2 0.858 324.3 0.975

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75

Table 2.2 Cont’d '

cf

MPa

b

cm

d

cm

da / Reinforcement

Exp

uV

kN

ACI EC-2 Theory of

Zararis.P

%

'

%

v yvvf

MPa

uV

kN

ACu VV /

uV

kN

ECu VV /

uV

kN

theoryu VV /

55.8 30.4 53.8 3.10 2.49 0.79 0.14 0.69 382.9 330.6 1.158 367.8 1.041 377.1 1.015

51.3 30.4 53.8 3.10 2.49 0.79 0.07 0.35 280.9 267.0 1.052 303.2 0.926 298.7 0.941

51.3 30.4 53.8 3.10 2.49 0.79 0.07 0.35 258.3 267.0 0.967 303.2 0.852 298.7 0.865

29.2 40.6 34.5 2.65 2.32 1.02 0.39 2.14 460.1 441.7 1.042 444.9 1.034 526.6 0.874

32.2 40.6 34.5 2.65 2.31 1.02 0.39 2.14 549.1 447.8 1.226 456.7 1.202 533.9 1.028

32.4 40.6 34.5 2.65 2.31 1.02 0.39 2.14 504.6 448.2 1.126 457.4 1.103 533.9 0.945

33.8 40.6 34.5 2.65 2.31 1.02 0.39 2.14 584.7 450.9 1.297 462.8 1.263 538.0 1.086

Roller and Russell

120.2 35.6 55.9 2.50 1.65 ___ 0.07 0.28 298.0 340.7 0.874 542.8 0.549 363.5 0.820

120.2 35.6 55.9 2.50 3.03 ___ 0.43 1.94 100.0 689.7 1.595 877.2 1.254 863.6 1.273

120.2 35.6 55.9 2.50 4.55 ___ 0.88 4.02 658.7 124.3 1.475 249.7 1.327 402.6 1.182

120.2 35.6 55.9 2.50 6.06 ___ 1.25 5.73 944.3 485.1 1.309 556.0 1.249 844.4 1.054

120.2 35.6 55.9 2.50 6.97 ___ 1.75 8.03 239.5 955.2 1.145 968.0 1.138 403.0 0.932

72.4 45.7 76.2 3.00 1.73 ___ 0.08 0.36 665.5 619.1 1.075 713.5 0.932 581.1 1.145

72.4 45.7 76.2 3.00 1.88 ___ 0.16 0.71 788.0 744.0 1.059 842.4 0.935 745.7 1.056

125.4 45.7 76.2 3.00 1.88 ___ 0.08 0.36 482.9 622.1 0.776 1006 0.480 658.5 0.734

125.4 45.7 76.2 3.00 2.35 ___ 0.16 0.71 749.6 753.2 0.995 1138 0.658 860.8 0.871

125.4 45.7 76.2 3.00 2.89 ___ 0.23 1.04 172.4 878.8 1.334 241.8 0.944 052.3 1.114

Sarzam and Al - Musawi

40.4 18.0 23.5 4.00 2.23 0.37 0.09 0.76 114.7 79.2 1.449 100.3 1.143 111.7 1.026

75.3 18.0 23.5 4.00 2.23 0.37 0.09 0.76 122.6 94.9 1.292 137.0 0.894 124.6 0.984

75.7 18.0 23.5 4.00 2.82 0.37 0.09 0.76 138.3 96.1 1.439 137.4 1.006 132.4 1.044

70.1 18.0 23.5 4.00 3.51 0.37 0.09 0.76 147.2 95.1 1.547 132.0 1.115 137.5 1.069

Xie et al

37.7 12.7 21.6 3.00 2.07 ___ ___ ___ 36.7 30.1 1.219 44.8 0.819 37.5 0.978

40.7 12.7 20.3 3.00 3.20 1.00 0.49 1.58 87.1 71.7 1.215 81.4 1.069 94.3 0.924

98.9 12.7 21.6 3.00 2.07 ___ ___ ___ 45.7 39.5 1.157 85.3 0.536 49.3 0.927

98.3 12.7 19.8 3.00 4.54 1.03 0.51 1.65 102.4 81.1 1.262 116.1 0.882 114.2 0.897

89.8 12.7 19.8 3.00 4.54 1.03 0.65 2.10 108.3 92.4 1.172 121.7 0.889 122.6 0.883

103.2 12.7 19.8 3.00 4.54 1.03 0.78 2.53 122.6 103.2 1.187 138.7 0.884 138.0 0.888

McGormley, Creary, and Ramirez

42.2 20.3 41.9 3.27 3.03 1.20 0.34 1.45 271.5 225.2 1.205 238.9 1.136 287.3 0.945

43.2 20.3 41.9 3.27 3.03 1.20 0.34 1.45 298.1 226.0 1.319 240.9 1.237 287.8 1.035

45.5 20.3 41.9 3.27 3.03 1.20 0.34 1.45 275.9 228.4 1.208 245.5 1.123 289.1 0.954

44.4 20.3 41.9 3.27 3.03 1.20 0.34 1.45 307.0 227.2 1.351 243.3 1.262 289.0 1.062

35.3 20.3 41.9 3.27 3.03 1.20 0.34 1.45 315.9 217.4 1.453 224.6 1.406 278.8 1.133

48.3 20.3 41.9 3.27 3.03 1.20 0.34 1.45 311.5 231.1 1.347 251.0 1.241 293.3 1.062

50.0 20.3 41.9 3.27 3.03 1.20 0.34 1.45 333.7 232.8 1.433 254.3 1.312 295.7 1.128

50.5 20.3 41.9 3.27 3.03 1.20 0.34 1.45 320.4 233.3 1.373 255.2 1.255 295.8 1.083

53.4 20.3 41.9 3.27 3.03 1.20 0.34 1.45 289.2 236.0 1.225 260.7 1.109 298.3 0.970

55.1 20.3 41.9 3.27 3.03 1.20 0.34 1.45 311.5 237.6 1.311 263.8 1.180 299.6 1.039

56.7 20.3 41.9 3.27 3.03 1.20 0.34 1.45 267.0 239.0 1.117 266.8 1.001 300.2 0.890

56.1 20.3 41.9 3.27 3.03 1.20 0.34 1.45 267.0 238.5 1.119 265.7 1.005 299.9 0.890

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76

Table 2.2 cont’d '

cf

MPa

b

cm

d

cm

da /

Reinforcement

Exp

uV

kN

ACI EC-2 Theory of

Zararis.P

%

'

%

v yvvf

MPa

uV

kN

ACu VV /

uV

kN

ECu VV /

uV

kN

theoryu VV /

Yoon, Cook, and Mitchell

36.0 37.5 65.5 3.28 2.80 0.06 ___ ___ 249.0 271.4 0.917 281.0 0.886 300.0 0.830

36.0 37.5 65.5 3.28 2.80 0.06 0.08 0.35 457.0 357.3 1.279 358.3 1.275 413.5 1.105

36.0 37.5 65.5 3.28 2.80 0.06 0.08 0.35 263.0 357.3 1.016 358.3 1.013 413.5 0.878

36.0 37.5 65.5 3.28 2.80 0.06 0.12 0.50 483.0 394.2 1.225 391.5 1.234 462.1 1.045

6.70 37.5 65.5 3.28 2.80 0.06 ___ ___ 296.0 357.1 0.829 425.4 0.696 362.6 0.816

6.70 37.5 65.5 3.28 2.80 0.06 0.08 0.35 405.0 443.1 0.914 502.7 0.805 476.0 0.851

6.70 37.5 65.5 3.28 2.80 0.06 0.12 0.50 552.0 479.9 1.150 535.9 1.030 524.7 1.052

6.70 37.5 65.5 3.28 2.80 0.06 0.16 0.70 689.0 529.0 1.302 580.1 1.188 589.5 1.168

87.0 37.5 65.5 3.28 2.80 0.06 ___ ___ 327.0 362.0 0.903 506.3 0.646 389.6 0.839

87.0 37.5 65.5 3.28 2.80 0.06 0.08 0.35 483.0 448.0 1.078 583.7 0.827 503.0 0.960

87.0 37.5 65.5 3.28 2.80 0.06 0.14 0.60 598.0 509.4 1.174 638.9 0.936 584.1 1.023

87.0 37.5 65.5 3.28 2.80 0.06 0.23 1.00 721.0 647.6 1.113 727.3 0.991 713.8 1.010

Kong and Rangan

60.4 25.0 29.2 2.50 2.80 0.31 0.16 0.89 228.3 169.6 1.346 212.8 1.073 213.7 1.068

60.4 25.0 29.2 2.50 2.80 0.31 0.16 0.89 208.3 169.6 1.228 212.8 0.979 213.7 0.975

68.9 25.0 29.2 2.50 2.80 0.31 0.16 0.89 253.3 175.8 1.441 226.9 1.116 219.6 1.153

68.9 25.0 29.2 2.50 2.80 0.31 0.16 0.89 219.4 175.8 1.248 226.9 0.967 219.6 0.999

64.0 25.0 29.7 2.49 1.66 0.31 0.10 0.64 209.2 151.0 1.385 194.2 1.077 171.2 1.222

64.0 25.0 29.7 2.49 1.66 0.31 0.10 0.64 178.0 151.0 1.179 194.2 0.916 171.2 1.039

64.0 25.0 29.3 2.49 2.80 0.31 0.10 0.64 228.6 154.1 1.483 230.0 1.126 195.7 1.168

64.0 25.0 29.3 2.49 2.80 0.31 0.10 0.64 174.9 154.1 1.135 203.0 0.861 195.7 0.894

83.0 25.0 34.6 2.40 2.85 0.26 0.16 0.89 243.4 220.5 1.104 286.0 0.851 266.7 0.913

83.0 25.0 29.2 2.50 2.80 0.31 0.16 0.89 258.1 185.2 1.393 249.2 1.035 228.3 1.130

84.9 25.0 29.2 3.01 2.80 0.31 0.16 0.89 241.7 184.1 1.313 252.1 0.958 233.2 1.036

84.9 25.0 29.2 2.74 2.80 0.31 0.16 0.89 259.9 185.2 1.403 252.1 1.031 231.6 1.122

84.9 25.0 29.2 2.50 2.80 0.31 0.16 0.89 243.8 186.5 1.307 252.1 0.967 229.8 1.061

65.4 25.0 29.3 2.73 2.80 0.31 0.10 0.64 178.4 153.9 1.159 205.4 0.868 198.0 0.902

65.4 25.0 29.3 2.73 2.80 0.31 0.10 0.64 214.4 153.9 1.393 205.4 1.044 198.0 1.083

71.0 25.0 29.4 3.30 4.47 1.23 0.10 0.60 217.2 158.7 1.368 212.5 1.022 219.8 0.988

71.0 25.0 29.4 3.30 4.47 1.23 0.13 0.72 205.4 167.5 1.226 220.4 0.932 231.5 0.887

71.0 25.0 29.4 3.30 4.47 1.23 0.16 0.89 246.5 180.0 1.369 231.6 1.064 248.6 0.992

71.0 25.0 29.4 3.30 4.47 1.23 0.20 1.12 273.6 196.9 1.389 246.9 1.108 270.3 1.012

71.0 25.0 29.4 3.30 4.47 1.23 0.22 1.27 304.4 208.0 1.464 256.8 1.185 285.8 1.065

71.0 25.0 29.4 3.30 4.47 1.23 0.26 1.49 310.6 224.1 1.386 271.3 1.145 306.8 1.012

Zararis and Papadakis

24.9 14.0 23.5 3.60 1.37 0.30 ___ ___ 32.3 28.4 1.138 35.1 0.919 34.7 0.931

22.4 14.0 23.5 3.60 1.37 0.30 0.09 0.24 40.2 34.9 1.152 39.8 1.010 45.6 0.882

23.9 14.0 23.5 3.60 1.37 0.30 0.14 0.37 49.7 40.0 1.242 45.1 1.101 52.4 0.949

22.5 14.0 23.5 3.60 1.37 0.30 0.19 0.50 59.2 43.5 1.359 47.6 1.243 57.4 1.040

23.0 14.0 23.5 3.60 1.37 0.30 0.28 0.73 63.5 51.4 1.235 54.9 1.156 68.3 0.930

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77

Table 2.2 Cot’d '

cf

MPa

b

cm

d

cm

da /

Reinforcement

Exp

uV

kN

ACI EC-2 Theory of

Zararis.P

%

'

%

v yvvf

MPa

uV

kN

ACu VV /

uV

kN

ECu VV /

uV

kN

theoryu VV /

22.4 14.0 23.5 3.60 1.37 0.30 0.06 0.16 36.2 32.3 1.120 37.5 0.966 41.5 0.872

23.9 14.0 23.5 3.60 1.37 0.30 0.09 0.23 43.7 35.4 1.233 41.0 1.066 45.7 0.956

20.8 14.0 23.5 3.60 1.37 0.30 0.12 0.31 44.7 36.3 1.230 40.3 1.108 47.6 0.939

21.6 14.0 23.5 3.60 0.68 0.30 0.27 0.73 56.2 49.5 1.135 48.5 1.158 60.3 0.982

21.3 14.0 23.5 3.60 0.68 0.30 0.17 0.46 47.2 40.5 1.166 40.3 1.172 47.9 0.985

Karayiannis and Chalioris

26.0 20.0 26.0 2.77 1.47 0.59 ___ ___ 60.2 55.6 1.083 57.4 1.049 57.9 1.039

26.0 20.0 26.0 2.77 1.47 0.59 0.08 0.21 64.0 66.6 0.961 67.2 0.952 71.0 0.901

26.0 20.0 26.0 2.77 1.47 0.59 0.12 0.32 89.0 72.3 1.231 72.4 1.229 77.7 1.145

26.0 20.0 26.0 2.77 1.47 0.59 0.16 0.43 89.2 78.0 1.143 77.5 1.151 84.3 1.058

26.0 20.0 26.0 2.77 1.47 0.59 0.25 0.64 93.0 88.9 1.046 87.3 1.064 97.4 0.955

26.0 20.0 26.0 3.46 1.96 0.59 ___ ___ 71.6 56.0 1.279 63.7 1.124 62.7 1.141

26.0 20.0 26.0 3.46 1.96 0.59 0.04 0.11 71.2 61.7 1.154 68.8 1.035 70.7 1.007

26.0 20.0 26.0 3.46 1.96 0.59 0.07 0.17 71.2 64.8 1.099 71.6 0.994 74.5 0.953

26.0 20.0 26.0 3.46 1.96 0.59 0.09 0.23 76.7 67.9 1.129 74.5 1.030 78.8 0.973

26.0 20.0 26.0 3.46 1.96 0.59 0.13 0.34 84.8 73.6 1.152 79.6 1.065 86.8 0.977

Collins and Kuchma

71.0 29.5 92.0 2.50 1.03 1.03 0.16 0.80 516.0 602.0 0.857 589.1 0.875 486.0 1.061

75.0 29.5 92.0 2.50 1.36 1.36 0.16 0.80 583.0 616.7 0.945 637.3 0.914 514.7 1.132

74.0 16.9 45.9 2.72 1.03 1.03 0.13 0.65 139.0 158.5 0.877 177.4 0.783 148.0 0.939

74.0 16.9 45.9 2.72 1.16 1.16 0.13 0.65 152.0 159.1 0.955 181.6 0.836 152.8 0.995

Angelakos, Bentz, and Collins

32.0 30.0 92.5 2.92 0.50 0.14 0.08 0.40 263.0 370.2 0.710 305.4 0.861 278.1 0.946

21.0 30.0 92.5 2.92 1.01 0.14 0.08 0.40 282.0 330.7 0.852 277.9 1.014 303.9 0.928

38.0 30.0 92.5 2.92 1.01 0.14 0.08 0.40 277.0 401.0 0.690 364.0 0.761 330.2 0.839

65.0 30.0 92.5 2.92 1.01 0.14 0.08 0.40 452.0 485.3 0.931 477.7 0.946 370.0 1.221

80.0 30.0 92.5 2.92 1.01 0.14 0.08 0.40 395.0 496.2 0.796 533.8 0.740 378.3 1.044

47.0 30.0 92.5 2.92 0.76 0.14 0.08 0.40 342.0 427.4 0.800 385.3 0.887 325.4 1.051

Mean of 174 test beams 1.252 1.092 1.004

CoV ( %) 16.78 18.26 10.23

Rengina and Appleton (1997) studied the behaviour of shear strengthened beams

with jacketing and shotcrete and showed that shotcrete and mortar jackets provide

simple and efficient shear strenghthening techniques.

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Kotsovos.M.D (2007) emphasized the fact that the basic assumptions of the current

design approaches of ACI-318 and EC-02 for flexure and shear are not compatible

with the actual strcutural beavior of RC members. There is a need to revise the

current RC design meethods for shear and flexure on the basis of actual behaviour

of RC beams to make it more compatible.

2.7 Minimum Amount of Shear Reinforcement

The purpose of minimum shear reinforcement is to prevent brittle shear failures and

to provide adequate control of shear cracks at service load levels. Both the

Canadian Standards CSA Standard (CSA A23.3-84), and ACI Code required a

minimum area of shear reinforcement equal to 0.35bws/fy, such that the stirrups are

assumed to carry 50 psi minimum shear stress. This value is independent of the

concrete strength. As the concrete compressive and tensile strengths increase, the

cracking shear also increases. This increase in cracking shear requires an increase

in minimum shear reinforcement such that a brittle shear failure does not occur upon

cracking. The 1994 CSA Standard (CSA A23.3-94) makes the minimum amount of

shear reinforcement a function of not only fy, but also f’c to account for the higher

cracking shear as the specified concrete strength is increased. Where shear

reinforcement is required, the minimum area of shear reinforcement shall be such

that:

cv fA 06.0

y

w

f

sb (2.52)

Figure 2.18 gives comparison of the CSA 1994 and ACI-1999 amounts of minimum

shear reinforcement. The CSA requirements provide a more gradual increase in the

required amount of minimum shear reinforcement as the concrete strength

increases.

Tests carried out by Yoon et al (1996), on large beams with concrete strengths

varying from 36 MPa to 87 MPa indicated that the amount of minimum shear

reinforcement prescribed by the 1994 CSA Standard provides adequate control of

diagonal cracks at service load levels and provide reasonable levels of ductility.

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Figure 2.18 Comparison of CSA and ACI amounts of minimum shear reinforcement

(Yoon et al, 1996)

2.8 Future of research on shear design of RC members.

Shear is one of the most researched properties of RC members in last 6 decades.

Regan (1993), classified research on shear into three broad groups;

i. The first of kind of research relates to shear sensitive areas like shear in fire,

shear connections between members, shear in high strength concrete and

punching shear. This group of research aims at filling the knowledge gap in

the above areas.

ii. The second group relates to understand the behaviour of basic material at

fundamental level. In this group of research, topics like “ role of aggregate

interlocking in shear” , “ Size effect on shear” and other basic concepts of

fracture mechanics related to shear are investigated. This group of research

is related to more basic and fundamental topics in shear strength of RC

members.

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iii. The third group is engaged in translating the research results into a more

meaningful tool for the building codes in the form of methods and rules for the

shear analysis and design of RC members.

There is a general feeling in the minds of many researchers, that enough research

has been carried out on this topic and there seems no more room for further

research in this field. Regan (1993) tried to answer this basic question, where

research on shear is waste of time or service to humanity? After reviewing the

research of last 4-5 decades, Regan (1993), highlighted the significance of the

research on the shear of RC beams in the following ways;

i. The research on shear for 40 years has enabled the structural engineers to

design the RC members without web reinforcement, pre-stressed beams and

flat slab buildings more accurately.

ii. The research on shear has been focused on making the design provisions of

building codes more rational and comprehensive. Considerable achievements

have been made in this direction. In these endeavors many misconceptions

and doubts were also created, which were clarified in later works.

iii. Most of the proposed models developed in the meanwhile were based on the

existing data but these models could poorly predict the behaviour of actual

beams, mainly due to the fact that important variables were not considered in

the models at times.

iv. More experimental tests and researches are required for significant

improvement in the shear design concept for its further rationalization

involving parametric studies.

Despite of the fact that research on shear strength of RC beams, has been

condcuted for more than six decades,but even then the riddle of shear failure

initiated by Kani(1964) is still unexplained. The exact beahvior of RC concrete in

shear is still an active areas in contemporary research.

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Mitchell et al. (2008) in a long term project, reviwed the results of 1849 tests on the

shear strength of RC beams to judge the adequacy and safety provided by the shear

equations used in North America. The findnigs of the research provide the latest

state of researech on the shear strength the Some of the important findings and

conclusions of the research of Mitchell et al (2008) are given as follows:

i. The traditional appraoch to design the shear reinformcent for the

region where the external shear is exceeding the concrete shear

capacity dbfV wcc'2

may lead to un-conservative results and the

chances of brittle failure may enhance. Hence there is a need to

revised and rationalize the shear design equation of ACI and

particularly the simplified shear design equation.

ii. The new load factors introduced in ACI-318-02, have led to increased

flexural stresses in felxural reinforcement at service loads, which have

furrther reduced the safety agianst shear failure.

iii. The design engineers must understand that the shear strength of RC

beams is also affected by member depth, crack roughness and strain

in longitudinal reinforcement, in addition to concrete strength.

iv. The recent research data shows that for RC members without web

reinforcement, the influence of strain in longitudinal steel is more

pronounced. High strength in the longitudinal steel and wider crack

widths may decrease the shear strengths of RC members.

v. In high strength concrete with small aggreagtes sizes, the cracks

surafces are reltively somoother and can lead to reduction in the shear

capacity of RC members. The equations based on the Modfied

Compression Field Thoery ( MCFT) accounts for the strain effect, size

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effect, and concrete strength in a reliable way, hence it can considered

a suitable subsitutue of the traditional ACI equation. However the

complexity in application of MCFT for the design of RC members

would need further simplifiction.

vi. An attempt to use the Simplified Modified Compression Field theory

based equations, would reduce the complexity to some extent and it

seems more advisable that the modified MCFT is used instead of

traditional ACI equation, which would ensure ductile failure of RC

structures and at the same time would also satisfy the basic ACI

equation.

To sum up the liteature review on the shear design of normal strength RC beams,we

can infer that research on shear design of RC members will continue to be an area

of interest for many young resereachers to come and the riddle of shear failure will

continue to be the focus of future research.

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Chapter Appendix 2.1

Solved Example with Modified Compression Field Theory.

Case 1. RC beams with shear reinforcement

Applied factored shear force Vu= 200 kN

Web width of the beam bw = 300 mm

Total depth of beam= 450 mm

f'c = 55 MPa

Shear span a = 1800

Mu = 200x1800 kN-mm

Longitudinal steel = 3-700mm2 +2-300mm2

Solution.

03.0554509.0300

000,200''

cvw

u

c

u

fdb

V

f

v

cot1085.11064.1

)30027003(000,200

cot000,2005.0)405/1800000,200(cot5.05.0/

43

ss

uuvux AE

VNdM

From Figure 2.11, the value of θ for 05.0'

c

u

f

v and εx between 1.5x 10-3 and 2 x 10-3

θ =42o which gives x = 1.84 x 10-3 and β = 0.15

)270@10(270

000,200/40511.12751404053005515.0)cot('

mmmmmms

ss

dfAdbfV vyv

vwcn

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Taking case 2 from actual beams tested in the experimental program.

Beam Bs1.5,5

Applied factored shear force Vu= 1.6(67.3) +1.2 ( 2.22)= 110.34 kN

Web width of the beam bw = 225 mm

Total depth of beam h = 300 mm

f'c = 52 MPa

Clear span = 2790 mm

Shear span a = 1395 mm

Mu = 110344x1395 kN-mm

Longitudinal steel ratio=ρ = 0.015

Yield stress of longitudinal steel fyl = 414MPa

Yield stress of transverse steel fyv = 275 MPa

Solution.

0308.0523009.0225

110344''

cvw

u

c

u

fdb

V

f

v

cot1002.310128.3

3009.022501.0000,200

cot1103445.0)3009.0/139510344(cot5.05.0/

43

5

1

ss

uuvux AE

VNdM

The value is more than the admissible values of 0.002, hence we may take the

Maximum value of x =0.002. From Figure 2.10, the value of θ for 05.0'

c

u

f

v

θ =43˚ which gives

x = 0.002 and

β = 0.14

mms

ss

dfAdbfV

vyvvwcn

201

82755/27007.1275652702255214.0)cot('

Provided 7mm @150mm. O.K

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Solution of the problem with program Response-2000

Step 1. Define section properties.

Concrete cylinder strength =52 MPa

Yield strength of the longitudinal steel = 463 MPa

Yield strength of transverse steel = 275 MPa

Pre-stress steel type = None.

Width of the beam section= 225 mm

Height of the section= 300 mm

Top steel =2#10

Bottom steel= 3#20

Stirrups type= Closed loop

Stirrup area per leg = 32 mm2

Step 2. Loads

Shear load = 110.34 kN

Moment= 110344x1395 kN-mm

Step 3. Full member properties

Length subjected to shear; Shear Span = 1395 mm

Constant shear analysis

Supports on bottom

Solution:

The various graphs given by the software are shown on the next page.

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Shear design

Attaullah Shah 2009/3/4

All dimensions in millimetresClear cover to transverse reinforcement = 40 mm

Inertia (mm4) x 106

Area (mm2) x 103

yt (mm)

yb (mm)

St (mm3) x 103

Sb (mm3) x 103

69.0

517.5

150

150

3450.0

3450.0

75.0

569.8

155

145

3682.5

3922.9

Gross Conc. Trans (n=6.48)

Geometric Properties

Crack Spacing

Loading (N,M,V + dN,dM,dV)

2 x dist + 0.1 db /

0.0 , 0.0 , 0.0 + 0.0 , 1.0 , 0.0

230

300

2 - 10

Av = 32 mm2 per leg

@ 150 mm

3 - 20

Concrete

c' = 2.28 mm/m

fc' = 52.0 MPa

a = 19 mmft = 2.19 MPa (auto)

Rebar

s = 100.0 mm/m

fu = 695 MPa

Trans, fy= 275

Long, fy= 463

1. General Properties displayed by the software

Cross Section Longitudinal Strain

-3.02 12.78

top

bot

Transverse Straintop

bot

Crack Diagram

3.08

2.05

1.81

1.02

0.13

Shear Straintop

bot

Shear Stresstop

bot

Principal Compressive Stress

-52.0

top

bot

Shear on Crack

3.99

top

bot

Principal Tensile Stress

2.19

top

bot

Control : M-Phi

93.3

99.4

Control : M-ex

-2.2 5.7

99.4

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2. Details of cracking.

Cross Section Longitudinal Strain

-3.02 12.78

top

bot

Principal Tensile Strain

12.8

top

bot

Crack Diagram

3.08

2.05

1.81

1.02

0.13

Crack Widths

3.34

top

bot

Average Angle

90.0

top

bot

Long. Crack Spacing

300.0

top

bot

Transverse Crack Spacingtop

bot

Diagonal Spacing

300.0

top

bot

Control : M-Phi

93.3

99.4

Control : M-ex

-2.2 5.7

99.4

3. Reinforcement details.

Cross Section Longitudinal Strain

-3.02 12.78

top

bot

Transverse Straintop

bot

Long. Reinforcement Stress

-56.1 476.8

top

bot

Long. Reinf Stress at Crack

498.0

top

bot

Long. Average Bondtop

bot

Stirrup Stresstop

bot

Stirrup Stress at Cracktop

bot

Transverse Average Bondtop

bot

Control : M-Phi

93.3

99.4

Control : M-ex

-2.2 5.7

99.4

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Chapter No. 3

Shear strength of high performance reinforced concrete

beams

Chapter Introduction: This chapter mainly addresses the issues in the shear of High strength concrete. The chapter starts with the definition of HSC, its historical development and extensive use across the world. Then the structural properties of High Strength concrete have been discussed and lastly the shear strength of high strength concrete beams has been explained on the basis of experimental research and empirical relationship developed by different researchers in last two decades.

Figure 3.1: World Trade Centre (USA) Figure 3.2:The world Highest Tower Burj Dubai,UAE (2651 feet) (162 floors, scheduled construction, 2008)

3.1 High Performance Concrete (HPC)

The term High Performance Concrete (HPC) is used to describe concretes that are

made with carefully selected high quality ingredients, optimized mixture designs, and

which are batched, mixed, placed, consolidated and cured to the highest industry

standards. Typically, HPC will have a water-binder material ratio (w/b) of 0.4 or less.

Achievement of these low w/b concretes often depends on the effective use of

admixtures to achieve high workability, another common characteristic of HPC

mixes.

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Forster [1994] defined HPC as "a concrete made with appropriate materials

combined according to a selected mix design and properly mixed, transported,

placed, consolidated, and cured so that the resulting concrete will give excellent

performance in the structure in which it will be exposed, and with the loads to which

it will be subjected for its design life."

American Concrete Institute has defined HPC as;

“Concrete meeting special combinations of performance and uniformity requirements

that cannot always be achieved routinely using conventional constituents and normal

mixing, placing and curing practices” (ACI-318.116R,2006).

The requirements may involve enhancements of characteristics such as placement

and compaction without segregation, long-term mechanical properties, early-age

strength, volume stability, or service life in severe environments. Concretes

possessing many of these characteristics often achieve higher strength. Therefore

HPC is often of high strength, but high strength concrete may not necessarily be of

High-Performance Concrete at times.

National Concrete Bridge Council (USA) has defined HPC as; “…concrete that

attains mechanical properties, durability or constructability properties exceeding

those of normal concrete.”

Zia et al ( 1993), while working on the States Highways Research Project-USA

( SHRP) C-205, defined various types of HPC, as given in Table 3.1

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Table 3.1 Definition of HPC as per SHRP (Zia et al, 1993)

Category of HPC

Minimum Compressive

Strength

Maximum Water/

Cement Ratio

Minimum FrostDurability

Factor

1.Very early strength VES

Option A(with Type III cement)

2,000 psi (14 MPa)in 6 hours

0.40 80%

Option B(with PBC-XT cement)

2,500 psi (17.5 MPa)

in 4 hours

0.29 80%

2. High early strength (HES) (with Type III cement)

5,000 psi (17.5 MPa)

in 24 hours

0.35 80%

3. Very high strength (VHS) (with Type I cement)

10,000 psi (70 MPa)

in 28 hours

0.35 80%

More recently the term Ultra High Strength Concrete (UHSC) is also used in the

literature, which refers to the HPC having the compressive strength of concrete in

excess of 100 MPa.

The production of HPC has been possible with development of new material besides

the conventional cement and aggregates. These may include mineral and chemical

admixtures.

The use of fly ash and Silica fume, (also called condensed silica fume or micro

silica), continues to be popular element of high performance concrete, and

especially high strength concrete. Mehta (1994), Aitcin (1993), Goldman and Bentur

[1993], Bharatkumar et al (2005) and O.Kiyali (2005) examined the effects of silica

fume on mechanical behaviour. These reports confirm findings that a silica fume

tends to improve both mechanical properties and durability.

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A number of issues with frost resistance of concrete containing silica fume have

been investigated, including the need for any entrained air when working with very

low W/CM ratio concretes. According to ACI 318-95 [1995], the quantity of silica

fume in concrete, exposed to deicing salts is limited to no more than 10 percent.

The use of cementitious systems with very high quantities of fly ash has also been

investigated. Malhotra [1990] reports that performance in rapid freezing and thawing

of concrete with high volumes of class F fly ash was adequate but that the concrete

with very high quantities of fly ash performed poorly in deicer scaling tests. Naik et

al. (1994) found that although concrete made with high volumes of class C fly ash

passed ASTM C-944 for abrasion resistance, better abrasion resistance was

obtained for concrete without the high fly ash content. The small and spherical fly

ash particles filled the voids or airspaces and increased the density. The smaller

particle size of fly ash with a higher surface area and glassy phase content also

improved the pozzolanic reaction and (Isaia et al,2003). Therefore, the CFA ( Class

C-Fly ash) made the blended cement paste more homogeneous and denser as well

as having a higher pozzolanic reaction than the one containing the original fly ash,

and this resulted in an increase in the compressive strength(Mehta,2003).

The mix proportioning of HPC has been attempted in various projects. Field trials of

High Early Strength (HES), Very Early Strength (VES) and Very High Strength

(VHS) concretes in SHRP C-205 and C-206 indicated that existing proportioning

methods remain valid, with minor modifications, for these mixes.

3.2 High strength concrete:

The definition of High Strength Concrete (HSC), has been changing with time due to

advancement in the concrete and material technology. At times the compressive

strength of 40 MPa was considered as high strength, however with improved mixed

design, ultra high range water reducers (Superplasticisers), and mineral admixtures,

concretes with compressive strength above 100 MPa are easily obtained in the field.

ACI-318 committee revealed that in the 1960’s, 52 MPa (7500 psi) concrete was

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considered high-strength concrete and in the 1970’s, 62 MPa (9000psi) concrete

was considered as HSC. The committee also recognized that the definition of the

high-strength concrete varies on a geographical basis. In regions where 62 MPa

(9000 psi) concrete is already being produced commercially, high-strength concrete

might be in the range of 83 to 103 MPa (12,000 to 15,000psi). However in

developing countries like Pakistan, achieving 60 MPa concrete is still underway.

The High Strength Concrete has been successfully used in the construction of pre-

stressed bridges in the world such as Braker Lane Bridge, built in Austin, Texas,

USA in 1990, with concrete strengths ranging from 75.8 MPa to 96.5 MPa at 28

days. The Red River Cable-Stayed Bridge Guangxi, China ( 65 MPa) , Normandy

Bridge, France (60 MPa) and Portneuf Bridge Quebec, Canada (60 MPa) [ Bickley

and Mitechlles,2001]

Due to substantial increase in the strength of concrete, the term ultra High strength

Concrete is also used. In Europe, high-performance steel fiber reinforced

cementitious composite referred to as Reactive Powder Concrete (RPC) was

developed. Steam curing at 90οC and densest packing design enabled to produce

pre-cast concrete having high-performance and ultra high-strength of around 200

MPa. The actual applications of RPC have been done by around 35 projects in the

world (Toru Kawai, 2005). The High Strength Concrete has been used for the

construction of pre-cast and high rise building across the world.

Until recently, the world's tallest buildings were in the United States, but in 1993, the

tall building construction boom shifted to Asia with the erection of the 1207 ft (368 m)

Central Plaza office tower in Hong Kong. Two major high-rises in Asia are the 1371

ft (418 m) Jin Mao Tower in Shanghai, China, and the 1378 ft (420 m), Petronas twin

towers in Kuala Lumpur, Malaysia. These monumental towers use composite

structural systems, combining vertical components such as cores, columns, and

shear walls of concrete that have strengths of up to 80 MPa (11,600 psi) with

structural steel horizontal members to resist lateral and vertical forces [PCA,2005].

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The two tallest concrete buildings in the United States were completed in Chicago in

1989. Both the 969 ft (295 m), 311 South Wacker Building and the 920 ft (276 m),

Two Prudential Plaza Buildings took advantage of 83 MPa (12,000 psi) high-strength

concrete in the fabrication of cast-in-place, steel-reinforced columns and walls at the

buildings' lower levels to support the total dead and live loads of the structures. The

middle and upper levels of the buildings, where total accumulated forces are lower,

were constructed with concrete in strengths ranging from 27.6 MPa (4000 psi) to 69

MPa (10,000 psi) [PCA,2005].

The use of HSC at local level has also been increased during the last one decade

due to construction of pre-stressed bridges, girders and other infrastructure projects

in Pakistan. In multi-span bridges constructed in Pakistan Motorway project and high

rise buildings and tower being constructed, extensively use the pre-stressed

concrete technology in Pakistan. Hence HSC of compressive strength 60Mpa and

above is used in these projects. In the following sections, important considerations

in the development of high strength concrete have been discussed, which are mainly

based on the ACI-State of the Art Report on the high Strength Concrete by ACI

Committee, 363-97

3.2.1 Selection of materials for high strength concrete.

3.2.1.1 Cement: The selection of appropriate type of cement is critical for the HSC,

the ACI committee 363[2005], has given the following recommendations on testing

and selection of the cement.

Initially, silo test certificates should be obtained from potential suppliers for the

previous 6 to 12 months. If the tri-calcium silicate content varies by more than 4

percent, the ignition loss by more than 0.5 percent, or the fineness by more than 375

cm2/g (Blaine), then problems in maintaining a uniform high strength may result.

Sulfate (SO4) levels should be maintained at optimum with variations limited to

±0 .20 percent.

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3.2.1.2 Admixtures in high strength concrete.

3.2.1.2.1 Mineral admixtures;

In the use of mineral admixtures like fly ash, Silica fumes, Slag cement (Ground

granulated Blast furnace Slag), the following guiding principles may be kept in mind;

i. Specifications for fly ash are covered in ASTM C 618-08a(2008). Methods for

sampling and testing are found in ASTM C 311-07(2007), which shall be

followed for uniformity of the supply.

ii. To ensure uniform textures and properties of fly ash supply, appropriate

testing of shipments and increased frequency of sampling shall be followed.

iii. For silica fumes. Thus, it is necessary to quickly cover the surfaces of freshly

placed silica-fume concrete to prevent rapid water evaporation.

iv. Specifications for ground granulated blast furnace slag are given in ASTM C-

989-09(2009).

v. The evaluation of mineral admixtures with the laboratory tests is an important

step in the selection of mineral admixtures.

3.2.1.2.2 Chemical admixtures;

Chemical admixtures are widely used in the development of high-strength concrete.

The super-plasticizers (SP), refer to high range water reducing admixtures by ASTM

C494-05(2005). There are four major groups of super-plasticizers.

i. Sulfonated Naphthalene Formaldehyde Condense (SNF)

ii. Sulfonated Melamine Formaldehyde Condense (SMF)

iii. Modified Liognosulfate ( MLS)

iv. Other types including polyarcylatyes, polystyrene sulfonates and

polymers etc.

These high water reducing agents change the properties of fresh and hardened

concrete in the following ways (Ahmad et al. 2004)

i. Reduction in the interfacial tension

ii. Multilayered absorption of organic molecules

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iii. Protective adherent Sheath layer of water molecules

iv. Release of water trapped amongst the cement particles.

v. Retarding effect of cement hydration

vi. Change in the morphology of hydrated cement.

Various types of chemical admixtures are discussed as follows;

i. Air entraining admixtures (ASTM C-260). In concrete subjected to freezing

and thawing during initial stages, air entrainment helps in decreased water

cement ratio and improved air-void ratio. The Air entraining agents reduce the

compressive strength of concrete and its use is recommended only where the

durability of concrete is main concern.

ii. Retarding agents (ASTM C-494 Type B&D).

A retarder can control the rate of hardening in the forms to eliminate cold joints

and provide more flexibility in placement schedules.

The dosage of retarders depends on the temperature during the setting time of

concrete. Initially if the temperature is too much, high dosage of retarders is

recommended, however, it may be reduced if the temperature declines.

iii. Normal range water reducers (ASTM C-494 Type A)

These generally increase the strength of concrete without affecting the rate of

hardening. The increased dosage of normal water reducers may reduce the

strength of concrete but may improve the hardening of concrete.

iv. High range water reducers (ASTM C-494 Type F&G)

In high-strength concrete, HRWR may serve the purpose of increasing strength

at the slump or increasing slump. The method of addition should distribute the

admixture throughout the concrete. Adequate mixing is critical to uniform

performance.

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v. Accelerators (ASTM C 494, Types C and E)-

In HSC, accelerators are used selectively, where removal of the form work is

required at an early stage from columns and walls. These mostly reduce the

compressive strength of concrete in the long run.

3.2.1.3 Aggregates

For HSC fine aggregates in round shape are preferred for its particle shape and

smooth textures. Fine aggregates with fineness modulus of 2.5 may give very sticky

concrete, which may be difficult in placement, whereas for FM, of 3.0 the workability

may improve substantially. The amounts passing sieves No 50 and 100 may be

kept low but still within the requirements of ASTM C-33. The sand gradation may not

have significant effect on the early stage but at later ages, it may become an

important parameter in the strength of HSC. Hence FM between 2.5 to 3 is preferred

for HSC.

In case of coarse aggregates, the maximum sizes of ½ in or ¾ in are preferred. The

crushed stones have given better results as compared with the rounded aggregates.

For HSC, coarse aggregate should be clean, cubical, angular, 100 percent crushed

aggregate with a minimum of flat and elongated particles.

The water absorption capacity of aggregates plays an important role in the strength

development of the HSC. If aggregates are capable of absorbing a moderate

amount of water, they can act as tiny curing-water reservoirs distributed throughout

the concrete, thereby providing the added curing water which is beneficial to these

low water-cement ratio pastes in HSC. The high strength of aggregates is also an

important in selection of coarse aggregates for HSC.

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3.2.1.4 Water

Usually, water for concrete is specified to be of potable quality, available from

municipality lines or local tube wells.

3.2.2 Mix proportioning of high strength concrete

Mix proportioning of high strength concrete is more important as involves the

selection of appropriate admixtures besides other basic ingredients in the normal

concrete. For achieving the requisite strength, testing of mix designed concrete is

frequently carried out and concrete is accepted if the following conditions are

fulfilled;

a) The average of all sets of three consecutive strength test results shall equal or

exceed the required fc'.

b) No individual strength test (average of two cylinders) shall fall below fc' by more

than 500 psi (3.4 MPa). However, some designers have specified higher or lower

over design strengths than called for in ACI 318 regardless of established

performance.

The age of concrete specimen is critical to the strength of concrete. In HSC,

substantial strength gain has been observed at later ages beyond 28 days and

mostly at 56 and 90 days. Hence it is recommended to employ accelerated tests for

prediction of later age strength of concrete as per ACI- publication SP-56.

The water cement ratio mostly referred as water binder ratio in HSC, is very

important for the high strength of concrete. The increase in strength is achieved by

increasing the quantity of cementitious material and hence additional water is

required for its hydration. For HSC not containing water reducers may require a

slump of 2-4 in depending on the placement conditions and forms. The use of high

range water reducers may reduce the water requirement and a range of w/c ratio

from 0.27 to 0.50 is recommended for such kinds of HSC.

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The cement contents have also direct effect on the compressive strength of

concrete. Most commonly a range of 392 to 557 kg/m3 has been used for developing

high strength concrete.

To optimize the mix proportioning of various material in the HSC, rigorous testing of

various ingredients of HSC are very important. The type and brand of cement is also

an important consideration in the selection of material. The quantity of cement

beyond certain desirable level may lead to workability problems and reduction in the

compressive strength of concrete. The maximum desirable quantity of cement for

HSC may also depend on the temperature and retarding admixtures and ice may be

required to control the temperature of the additional cement used in HSC.

The proportioning of aggregates has direct bearing on the strength of HSC. Low fine

aggregate contents have resulted in a reduction in paste requirements and normally

have been more economical. Such proportions also have made it possible to

produce higher strengths for a given amount of cementitious materials. However, if

the proportion of sand is too low, serious problems in workability become apparent,

due to less fluidity and flow-ability of concrete. The optimum amount of coarse

aggregates for HSC will mainly depend on the properties of sand. The following

Table 3.2 illustrates the mix proportioning of aggregates as per ACI-211.1

Table 3.2 -Volume of coarse aggregate per unit of volume of concrete. (ACI-211.1)

Max sizes of

aggregates (in)

Volume of dry rodded coarse aggregates for different fine moduli of sand

2.40 2.60 2.80 3.00

3/8 0.50 0.48 0.76 0.44

½ 0.59 0.57 0.55 0.53

¾ 0.66 0.64 0.62 0.60

1 0.71 0.69 0.67 0.65

1 ½ 0.75 0.73 0.71 0.69

2 0.78 0.76 0.74 0.72

3 0.82 0.80 0.78 0.76

6 0.87 0.85 0.83 0.81

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3.2.3 Mixing, transportation and curing of high strength concrete

The control and storing of material for HSC is almost the same as normal strength

concrete. The temperature of all the constituents must be kept as low as possible

before batching and the mixing and batching facility must closer to the site.

ACI 304-05 recommends that cements and pozzolans be weighed with automatic

equipment. To maintain the proper water-cement ratios necessary to secure high

strength concrete, accurate moisture determination in the fine aggregate is essential.

In hot weather use of ice may be recommended to control the temperature rather to

use the cold water.

Canadian Standards Association’s Preliminary Standard A 266.5-M 1981, tests have

shown that high-range water-reducing admixtures are most effective and produce

the most consistent results when added at the end of the mixing cycle after all other

ingredients have been introduced and thoroughly mixed. If there is evidence of

improper mixing and non uniform slump during discharge, procedures used to

charge truck and central mixers should be modified to insure uniformity of mixing as

required by ASTM C 94-05.

Due to the relatively low water content and high cement content and the usual

absence of large coarse aggregate, the efficient mixing of high-strength concrete is

more difficult than conventional concrete. Hence it is more important in case of HSC

to check the mixer performance. ACI 304-05 recommends usual specifications, such

as 1 min for 1 cu-yd (0.75 cu-m) plus 1/4 min for each additional cu-yd of capacity,

are used as satisfactory guides for establishing mixing time.

In case of ready mix concrete, retarding admixtures are used to prolong the time the

concrete will respond to vibration after it has been placed in the forms. Withholding

some of the mixing water until the truck arrives at the job site is sometimes

desirable. Then after adding the remaining required water, an additional 30

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revolutions at mixing speed are used to incorporate the additional water into the

mixture adequately as recommended by ACI 304-05.

In case of transportation of truck mixed concrete, if the haulage is more and there

are chances of concrete hardening before placement, dry proportioned material are

mixed in the truck and transported to the site and water is added at the site and

material is mixed. However if there is some free water in the aggregates, it may

cause the hydration of the cement or part thereof. High-strength concrete is likely to

have a high cement content and small maximum size aggregate which can facilitate

concrete pumping. In the field, the pump should be located as near to the placing

areas as practicable. Direct communication is essential between the pump operator

and the concrete placing crew. Continuous pumping is desirable because if the

pump is stopped, movement of the concrete in the line may be difficult or impossible

to start again.

The delivery of concrete to the job site must be scheduled so it will be placed

promptly on arrival, particularly the first batch. Equipment for placing the concrete

must have adequate capacity to perform its functions efficiently so there will be no

delays at distance. Sufficient vibrating machinery and manpower must be available

for the mixing of concrete. Vibration almost to the point of excess may be required

for high-strength concrete to achieve its full potential.

For placement of HSC in a framed structure, all columns, floors and beams must be

placed from the same grade of high strength concrete, wherever possible. In case

the use of two different concretes is inevitable in column and floor construction, it is

important that placement of high-strength concrete in column and adjoining areas

must be carried out before the floor concrete.

For all types of concretes, curing is an essential element of quality production of

concrete. HSC must be water cured at the early age due to very high heat of

hydration in the initial stage. Additional water for curing may be required for HSC

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with low w/c ratio such as 0.29. It has been proposed that moist curing of HSC may

be continued for 28 days. The commonly used curing methods for HSC may include

immersion or pounding, sprinkling. Use of Burlap, cotton mats, rugs, and other

coverings of absorbent materials will hold water on the surface, whether horizontal

or vertical. Liquid membrane-forming curing compounds retain the original moisture

in the concrete but do not provide additional moisture.

For quality control of HSC, many researchers have recommended that the

specification for compressive strength should be modified from the typical 28-day

criterion to either 56 or 90 days. This extension of test age would then allow, for

example, the use of 7000 psi (48 MPa) concrete at 56 days in lieu of 6000 psi (41

MPa) at 28 days for design purposes. In actual field, since HSC is used in high rise

building, hence full load application of the service load is not possible at the lower

floors and more time can be provided for gaining additional strength. A close check

of the field results and maintenance of records in the form of control charts or other

means are necessary to maintain the desired control. Early-age control of concrete

strength such as the accelerated curing and testing of compression test specimens

according to ASTM C 684-99(2003) is often used, especially where later-age (56 or

90 days) strength tests are the final acceptance criterion.

For the test samples of HSC, ASTM standards specify a cylindrical specimen 6 in.

(152 mm) in diameter and 12 in. (305 mm) long. This size specimen has evolved

over a period of time, apparently from practical considerations. Designers generally

assume 6 x 12 in. (152 x 305 mm) regardless of the specimen size, as the

compressive stress is transferred through the loading platen-specimen interface, a

complex, tri-axial distribution of stresses in the specimen end may develop which

can radically alter the specimen failure mode and affect results.

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3.2.4 Structural properties of high strength concrete

The shear properties and stress strain behaviour of HSC, is separately discussed in

next chapter. Other properties of HSC may include modulus of elasticity, modulus of

rapture, poison’s ratio.

The modulus of elasticity of HSC may range from 4.5 to 6.5 x l06 psi (31 to 45 GPa).

The following relation has been reported between the compressive strength of

concrete and modulus of elasticity (Carrasquillo et al. 1981)

Ec = 40,000 'cf + 1.0 x l06 psi for 3000 psi < fc,’ < 12,000 psi (3.1)

The Poisson’s ratio of high strength concrete tends to decrease with the increase of

water cement ratio. Based on the available information, Poisson’s ratio of High-

strength concrete in the elastic range seems comparable to the expected range of

values for lower-strength concretes.

The modulus of rupture of concrete may range as

fr' = 11.7 'cf psi for 3000 psi < '

cf < 12,000 psi ( 3.2)

The tensile splitting stress of HSC is given as 7.4 'cf psi for 3000 psi < fc,’<12,000 psi.

To the extent that is known, the fatigue strength of high-strength concrete is the

same as that for concretes of lower strengths. The measured values of the unit

weight of high strength concrete are slightly higher than lower-strength concrete

made with the same materials.

The Freeze thaw resistance of HSC has been observed to increase as compared to

normal concrete due to greatly reduced freezable water contents and the increased

tensile strength of high-strength concrete.

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The shrinkage of high strength concrete containing high-range water reducers was

observed as less than for lower-strength concrete. The total creep of high strength

concrete has been observed same as the normal strength concrete.

3.2.5 Structural Designing considerations in design of HSC beams

For strain in HSC, The constant value of strain at extreme concrete compression

fiber of 0.003 prescribed by ACI 318-05 is seen to represent satisfactorily the

experimental results for high-strength as well as lower-strength concrete, although it

is not as conservative for high strength concrete.

3.3 Codes Provisions for High Strength Concrete

Paultre and Mitchell (2003), provided a detailed commentary on the HSC provisions

of four building codes used in Europe, Canada, USA and New Zealand, i.e. CEB-

MC-90, EC-02, CSA A23.3-94, ACI-318-02 and NZS 3101-95 respectively. The

important considerations of the codes are summarized as follows;

3.3.1 Concrete compressive strength

The upper limits on the compressive strength of concrete proposed by these codes

are given in Table3.3

Table 3.3 Upper limits of specified compressive strength of concrete for HSC and Standard test specimen. (Paultre and Mitchell (2003). Country /Region Code Year Max specified Concrete

compressive strength

MPa

Standard test

specimen.

(mm)

Europe CEB-FIP MC-90 1993 80 Cyl.150x300

Cube.200x300

Europe EC-02 2002 90 Cyl.150x300

Cube.200x200

Canada CSA A23.3-94 1994 80 Cyl.150x300

Cube.100x200

USA ACI318-02 2002 No limit Cyl. 152x1304

Cube. 152x304

New Zealand NZS 3101-95 1995 100 Cyl. 152x304

Cube.152x304

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3.3.2 Load and Resistance factors

The load factors, strength reduction factor and material reduction factors have been

shown in Table 3.4. Model Code MC-90 introduced the high strength reduction factor

as hsc =

5001.1

1

ckf

………………………………………………( 3.3)

ckf will be defined below.

Table 3.4 Comparison of values of load factors, strength reduction factors and material strength reduction factor proposed by various codes (Paultre and Mitchell, 2003).

3.3.3 Specified and Characteristic Strengths

ACI and NZ uses 28days compressive strength'

cf , which is less than the average

strength '

crf defined as follows;

'crf =

'cf +2.33s-3.45 ( MPa) for MPaf c 35'

………………………………………( 3.4)

'crf = 0.9

'cf +2.33s ( MPa) for MPaf c 35'

………………………………………. (3.5)

Where” s” is standard deviation of the sample data.

Code

Load Factor Strength Reduction factors Material Strength reduction factor

Dead

Live Flexure

Flexure

and Axial

load

Shear Concrete Steel

ACI318-02

1.2 1.6 0.65-0.9 0.65-0.9 0.75 - -

CSA A23.3-94 1.25 1.5 - - - 0.6 0.85

EC-02/ MC-90 1.35 1.5 - - - 1/1.15 1/1.15

NZS 3101-95 1.2 1.6 0.85 0.65-0.85 0.75 - -

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European Code, on the other hand use several values of strength based on the

characteristic strength ckf , which is related to mean compressive strength cmf as

follows; ffcmf ck where f is 1.64s and is usually taken as 8MPa.

3.3.3.1 Modulus of Elasticity, concrete tensile strength and minimum flexural

reinforcement.

Table 3.5 gives the values proposed by these codes for modulus of Elasticity and

minimum reinforcement for flexure.

Table 3.5 Comparison of values of modulus of elasticity modulus of rupture and min flexure reinforcement proposed by various codes (Paultre and Mitchell (2003).

Code Modulus of Elasticity Modulus of rapture

Min flexural reinforcement

ACI318-02

'5.1043.0 ccc fwE MPa

For Normal density

concrete

'4700 cc fE MPa

Modulus of rapture

'6.0 cffr

dbf

dbf

fA w

yw

y

cs

4.1

4

'

min

MPa and mm

EC-02/

MC-90

3.0)10

(22000 cmmc

fE

Uses direct tensile

strength ctmf

3/230.0 ckctm ff MPa

for MPafck 50

)10

1ln(12.2 cmctm

ff MPa

for MPafck 50

dbdbf

fctmA tt

yks 0013.026.0min wher

e tb is mean width of the

concrete zone in tension.

CSA

A23.3-94

5.1' )2300

)(69003200(wc

fE cc

hb

f

fA w

y

cs

'

min 2.0

Slightly more than ACI

NZS 3101-

95

'8.0 cffr dbf

dbf

fA w

yw

y

cs

4.1

4

'

min

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Due to wide variation in the Codes approaches to assess various structural

properties of HSC, Paultre and Mitchell (2003) have recommended that further

experimental and analytical studies may be initiated to better understand the

behaviour of HSC and to arrive at more rational and internationally acceptable

building code for HSC.

3.4 Mechanical properties of high strength concrete.

The various mechanical properties of HSC, as given in the “ACI Committee 363-

Roeprt on the State of the Art on High Strength Concrete” are discussed as follows;

The compressive strength of concrete has direct effect on the properties of concrete

both in fresh and hardened forms. In fresh concrete properties such as viscosity,

flow ability, workability depends on the compressive strength of concrete, as the

later depends on cement content. The high strength concrete normally involves high

cement content and low water binder ratio, leading to low workability despite of

increase in the compressive strength of concrete. In hardened form many structural

properties like flexural strength, shear strength, creep and shrinkage also depend on

the compressive strength of concrete.

The modulus of elasticity of concrete is frequently expressed as the function of its

compressive strength and is proportional to its square root value. Other properties of

concrete like modulus of rapture, workability, bond strength etc are also directly

related to the compressive strength of concrete.

The tensile splitting strength is usually measured as indirect tensile strength also

called as “Cylinder splitting strength”. The indirect tensile strength is usually 10% of

the compressive strength of concrete for normal strength concrete, but at higher

strength of concrete, it may be reduced to 5%. Further indirect tensile strength was

found as 70% of the flexural strength at 28 days. The test data on the fatigue

strength of HSC is very limited; however it has been shown that the fatigue stress of

HSC is almost the same NSC.

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The unit weight of HSC is slightly greater than the lower strength concrete made with

same material. The thermal properties of HSC fall within the range prescribed for the

NSC. The strength gain of HSC is relatively more than NSC at early ages mainly due

to 1) an increase in the internal curing temperature in the concrete cylinders due to a

higher heat of hydration and (2) shorter distance between hydrated particles in high-

strength concrete due to low water-cement ratio.

The freeze and thaw resistance of HSC has been observed as greater than NSC

due to reduced water cement ratio in concrete.

The shrinkage of HSC has been observed as same as NSC in most of the cases,

however the shrinkage of HSC having high range water reducers, has been reduced

for HSC.

The creep and shrinkage properties of High Strength Concrete were studied at

Magnel Laboratory (Taerwe, 1995); it was found that with the increase of concrete

strength, the final value of creep is overestimated for both normal and high strength

concrete. The creep rate proposed by the CEB-FIP Model Code 1990 can better

represent the creep development of high strength concrete than normal strength

concrete. Due to high heat of hydration owning to relatively more cement content,

high strength concrete elements might show some early age thermal cracking and

hence proper curing is required for HSC.

3.5 Stress strain behaviour and shear strength of HSC.

The stress strain behaviour of high strength concrete significantly varies from that of

the normal strength concrete. The stress strain relationship for various values of

compressive strengths as reported by Collins and Mitchells (1996) given in Figure

3.3 (a) , shows that the downwards sloping branch of the curve gets steeper with the

increase in the compressive strength of concrete, which means that HSC is relatively

brittle material.

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Ahmad et al. (1995) worked on the shear critical HSRC beams and showed that the

post peak branch of the mid span load deflection curve in the shear critical high

strength concrete beams is relatively steeper than that of the NSRC beams as

shown in Figure 3.3(b).

(Adapted from Collins and Mitchell, (1997).

NNN3 (41MPa) and NNH3(104Mpa)

( Adopted from Ahmad et al,1995)

Figure 3.3 Variation of compressive stress-strain curves with increasing compressive strength

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The main variations in these curves are illustrated as follows;

1. The stress strain curve is getting more linear with the increase of compressive

strength of concrete.

2. The strain at maximum stress for HSC is relatively more as compared to

NSC.

3. The descending part of the curve after the peak is steeper in case of HSC.

The brittle behavior of HSC can be explained as follows; (ACI report 363R-27,1997)

1. The difference in rigidity between cement paste and aggregates leads to

concentration of stresses at the contact zones of the two ingredient of HSC

and at certain overall stress level, a distributed micro crack pattern forms at

the contact points.

2. When the overall stress level further increases, a substantial part of the

increased energy is used in developing a clearer crack pattern. The stress

strain curve at this stage tends to deviate from linear elastic line.

3. With further increase of stresses, the micro crack pattern will provide an

efficient re-distribution of the stress and a tough and brittle failure is obtained.

As the compressive strength of concrete increases, the difference in the strength of

aggregates and cements matrix decreases and the HSC behaves like a

homogenous material and the stress-strain curve becomes more linear as compared

to NSC. This relatively uniform re-distribution of stresses leads to sudden failure of

HSC.

The shear of high strength concrete RC structure is comprised of two main parts

i. Vc - The nominal concrete contribution includes, in an undefined way, the

contributions of the still un-cracked concrete at the head of a hypothetical

diagonal crack, the resistance provided by aggregate interlock along the

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diagonal crack face, and the dowel resistance provided by the main

reinforcing steel.

ii. Vs- The shear resistance provided by the stirrups.

As already explained, the failure of HSC in uni-axial compression is sudden as

compared to NSC as the failure surface is relatively smooth along the crack plane. In

bi-axial compression, the diagonal compression from the load point and support is

combined with the diagonal tension in the perpendicular direction. In high strength

concrete, the diagonal tension cracks are expected to have smooth plane, due to

very high strength of concrete matrix. This leads to crushing of aggregates as shown

in Figure 3.4, and as result the aggregate interlocking is not playing significant role in

resisting the shear. There is a general consensus amongst the researchers, that the

aggregates interlocking decreases, when the compressive strength of RC concrete

increases, due to peculiar failure of the HSC (Cladera and Mari,2005). The decrease

of aggregates interlocking may lead to reduction in the shear strength of HSC.

Figure 3.4 Crack in high-strength concrete. The crack goes through the aggregates (Cladera and Mari,2005)

The research of Ahmed et al. (1986) have shown that the current design methods

are not conservative for HSC particularly for larger shear to depth ratio (Slender

beams a/d >3.0) and relatively low longitudinal steel ratio.

Kaufman and Ramirez (1988), demonstrated the benefits of using HSC in pre-

stressed beams, where the strength of the diagonal truss members is increased due

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to increase in the compressive strength of concrete in case of HSC. This in turn

leads to increased efficiency of web reinforcement, as more stirrups are mobilized.

Further research is however required to identify the minimum web reinforcement for

a particular level of HSC, to avoid brittle and sudden failure.

The research data on the shear strength of high strength concrete beams is limited

particularly for the compressive strength of 70 MPa and more. Following four

challenges are pointed by Duthinh and Carino (1996), while dealing with the

problem of shear design of high strength concrete.

1. The current provision and empirical equations used for the shear design by

various codes are mostly based on the research carried with concrete of 40

MPa or less. Again these equations used in various design codes for shear

strength of concrete, are at times complex and difficult to understand. Hence

there is a need to further simplify these equations for better understanding

and easy application by the designers.

2. The minimum shear reinforcement for HSC beams needs to be rationalized to

avoid brittle failure of the beams and adequate control of the shear cracks.

3. The relatively little role of the aggregate interlocking in HSC due to stronger

matrix, the shear friction of HSC can be expected 30-35% less than the NSC.

4. The compression capacity of the cracked web is reduced due to transverse

tension, which is sometimes referred to as “Softening of concrete”, which

depends on the concrete strength.

The test data shows that the aggregate interlocking decreases with the increase of

compressive strength of concrete. The data from tests by Ahmad and Khaloo (1991)

showed that the provisions of ACI-318 for shear design may be un-conservative for

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high strength concrete beams for higher shear span to depth ratios and relatively low

steel.

Duthin and Carino (1996) further pointed out that most of the current shear design

techniques either do not acknowledge the loss in the aggregate interlock mechanism

in high strength concrete or simply do not account for the influence of adding shear

reinforcement to other shear transfer mechanisms. Johnson and Ramirez (1989),

reported that for a constant low shear reinforcement, the overall reserve shear

strength after diagonal cracking diminishes with increase in the compressive

strength of concrete.

S. Sarkar, et al (1999) conducted an interesting research to study the contribution of

the compression zone concrete υcz, aggregate interlocking υa and dowel action of

the longitudinal steel υd , to the shear capacity for high strength reinforced concrete

( HSRC) beams without transverse reinforcement. The research was carried out on

beams with compressive strength ranging from 40Mpa to 110Mpa. The following

inferences were made;

1. The role of aggregate interlocking mechanism at higher concrete strengths is

slightly enhanced. In addition, this mechanism had a predominant influence

on the ultimate load carried by the beam. In other words, the contribution of

this mechanism to the total shear strength carried by the beam was around

42% for higher concrete strength beams with compressive strength of 110

Mpa as compared to 34% for NSC of 40 Mpa. However this increase in the

shear contribution due to aggregates interlocking is much less than the

increase in the compressive strength of concrete.

2. The contribution of the compression zone concrete remained fairly constant at

higher compressive strength with very little increase from 13% to 17% with

the increase of compressive strength from 40Mpa to 110Mpa.

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3. The contribution of dowel action remained the main part in the absence of the

aggregate interlocking but it decreased from 53% to 43% with the increase of

concrete strength from 40 Mpa to 110 MPa.

The earlier research by Kumar.D (1992) reported the following share of compression

zone, dowel action and aggregate interlocking in the shear strength of beams of

NSC, without web reinforcement;

Shear in compression zone Vc 20 to 40% Shear from dowel action Vd 15 to 25% Shear from aggregate interlock Va 35 to 50% Sherwood et al. (2006) has reported that at least 60% of the vertical shear is carried

by aggregate interlock at flexural cracks, with the remaining proportion being carried

in the compression zone and through dowel forces. Hence the observations by S.

Sarkar, et al (1999), need further experimental validation.

The contribution of dowel action to shear resistance is a function of the amount of

concrete cover beneath the longitudinal bars and the degree to which vertical

displacements of those bars at the inclined crack are restrained by transverse

reinforcement. Typically, little dowel action can be provided by reinforcement that is

near the tension face of a member without transverse reinforcement because that

action is then limited by the tensile strength of concrete.

Thus the aggregates interlocking appear to be a major share in resisting the vertical

shear of RC beams without web reinforcement. Experimental studies reveal that

aggregate interlock is directly related to some concrete properties such as the

tensile strength, the maximum aggregate size and the shape of the aggregate (river

or crushed aggregate). For this reason, the effect of aggregate interlock on the shear

capacity of R.C. members becomes less effective when shear cracks widen.

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Consequently, the dowel action plays a major role in preventing shear failure of

beams without web reinforcement.

S. Sarkar, et al (1999) used the Zsutty’s equation (1968) Eq-5.28, to develop an

expression for the shear capacity of HSC beams without transverse reinforcement

for the concrete strength range of 40Mpa to 110Mpa on the basis of regression

analysis. They classified the data into two categories. (i), beams having a/d≤ 2 and

(ii) beams having a/d >2.0. The general form of equation for shear stress of beams

without web reinforcement is given as;

ncn adf /.. …………………………………. (3.6)

Where

; is polynomial regression constant,

cf ; is the specified compressive strength of concrete,

; is the longitudinal steel ratio,

d ; is effective depth of beam,

a ; is shear span and

n ; The polynomial exponent.

The following two equations were developed on the basis of existing data base of

shear stress of beams without web reinforcement,

For beams having a/d≤2 66.0/..13.4 adf cn ……………… (3.7)

For beams having a/d>2 55.0/..05.3 adfcn ………….. (3.8)

Bazant and Kim (1984) proposed a very reliable expression for computing the shear

strength of RC beams, without transverse reinforcement which is given as ;

2/56/52/13/1 ).(9.206.83.0

d

af cuc ………………….. ( 3.9)

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Where

)

251/1

ad

d

; is a function taking into account the size effect of aggregates.

ad ; Max aggregates sizes

On the basis of the above equation, Russo,G .et.al (2004), proposed the following

expression for shear strength of HSC concrete beams without transverse

reinforcement.

33.296.0

38.091.02/146.0 )/(2.0.97.0 dafff

lyccuc …………. (3.10)

lyf ; yield stress of longitudinal steel

They further proposed the following expression for the shear strength of HSRC

beams with transverse reinforcement using the above expression.

33.296.0

38.091.02/146.0 )/(2.0.97.0 dafff

lyccuc + yvvb fI 75.1 (3.11)

v ; Steel ratio of web reinforcement.

yvf ; Yield stress of web reinforcement.

The factor Ib is given by the equation:

33.296.038.0

91.02/146.0

2/146.0

)/(2.0.97.0

.97.0

dafff

fI

lycc

c

b

………….. (3.12)

To check whether the shear failure is due to beam action or arch action, the author

further proposed a critical value as

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(a/d)c = 05.0

41.019.0

57.0c

ly

f

f

………………………………………………..(3.13)

Hence bI = 0.57 which means that for

i). a/d < (a/d)c bI <0.57, arch action prevails

ii). a/d > (a/d)c bI >0.57,beam action prevails

The proposed expression gave least coefficient of variation when compared with the

provisions of ACI-318, Euro code and CEB/FIB model on the basis of data of 116

beams already tested.

Ko et al (2001) researched the plastic rotation capacity of reinforced high strength

concrete beams in the range of 60-80 MPa and proposed the following new equation

for ultimate compressive strain of extreme fibers as the theoretical estimate of

003.0cu underestimates the test results.

)(00054.0)(

144.1003.0

,

2,

ccu f …………………… (3.14)

Mohiuddin A. Khan et al. (2000) applied the concept of Fracturing Truss Model

( FTM ) rather than MCFT and Strut and Tie Model ( STM), to HSC concrete beams

and compared the test results with the theoretical results. They observed that the

assumption of FTM is more consistent with actual beam failure as compared to

MCFT. They also examined the provisions of ACI-318 and recommended to include

an alternate Fracturing truss model (FTM) in the future codes. They also observed

that the concretes having different tensile stresses have significant effect on the

shear capacity of beam, concrete stresses and steel strain. Hence biaxial tests must

be conducted rather than split cylinder test for determining the exact concrete tensile

stresses.

Cladera and Mari (2004), developed an Artificial Neural Network (ANN) to predict the

shear strength of RC beams, using a large database of experimental results and

made the following important conclusions:

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1. The influence of the amount of web reinforcement on the shear strength RC

beams is not linearly proportional to the amount of web reinforcement. i.e. the

shear strength due to increase in shear reinforcement is not increasing in the

same ratio. The effectiveness of stirrups decreases with their increase within the

range of transverse steel ratio of 0.33% to 3.57%. The more the stirrups the less

effective they are.

2. Due to increase in size at low shear reinforcement, the shear strength has been

reduced by 25% when the size of beam has been increased from 250 to 750mm.

3. The influence of compressive strength of concrete also changes with the amount

of web reinforcement.

4. AASHTO LRFD design equation gives relatively good results as compared with

the ACI-318 and Eurocode-2

They further proposed a simplified shear design methods and compared the tests

results with the model.

Hamad and Najar (2001) studied the role of transverse reinforcement in confining the

tension lap in high strength concrete beams. They reported that the flexure failure in

the HSRC beams with no web reinforcement is more abrupt, whereas in beams with

web reinforcement, the failure was relatively ductile. The flexure cracks widths have

been reduced in the later case and this leads to ductile failure of the beams.

Shehta et al. (2003) developed theoretical models for the minimum flexural, shear

and torsional for RC beams made with different compressive strengths of concrete.

They reported that due to little test results available, there is great difference in the

minimum values proposed by different Codes and hence more experimental

research has been recommended by them.

Cladera and Mari (2005) worked on the HSRC beams failing in shear and reported a

very brittle failure of the HSRC beams without shear reinforcement. The failure was

observed as more sudden with further increase in the strength of concrete. However,

the failure shear strength of beams was observed to increase with the increase in

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the compressive strength for such beams. They also proposed an expression for

minimum web reinforcement of HSRC beams to avoid brittle failure of the beams,

which is given as follows;

Mpaf

sbfA

y

wmctw 5.7

,min,

(3.15)

Here mctf , stands for tensile strength of HSC, which is given as;

3,

2

30.0 cmct ff MPa if fc < 60MPa fc is specified compressive strength of

concrete

2, 58.0 cmct ff MPa if if fc > 60MPa (3.16)

They also concluded that the limitation of 2% longitudinal steel for HSRC beams with

web reinforcement is also not justified.

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Summary The definition of HSC has been changing from time to time and region to region.

Preparation of HSC requires special selection of material like aggregates, cement,

admixtures and high range water reducers. HSC also requires special

considerations in mixing, transportation, placing and curing.

The compressive stress strain curves of HSC shows that it is a relatively brittle

material as compared to NSC. The smooth plane of cracks in HSC reduces the

aggregates interlocking which leads to reduction of share of aggregates interlocking

in shear strength of concrete as compared to NSC.

Four challenges are faced in the shear design HSC members in the contemporary

research. Firstly; the available research data base is limited to research carried out

with the RC beams with compressive strength of 40MPa or less, secondly there no

consensus on the minimum shear reinforcement to avoid brittle failure of HSC

reinforced concrete beams, thirdly the decrease in the aggregate interlocking in

resisting the shear with the increase of compressive strength of concrete and finally

decrease in the compression strength of cracked web due to transverse tension,

also called softening of concrete and its measurement.

The literature review of work on the shear strength of HSRC beams thus identifies

the following research areas;

1. The relationship between aggregate interlocking share and compressive

strength of concrete in shear strength of HSRC beams. A reduction factor

may be explored to correlate the aggregates interlocking share of HSC and

compressive strength of concrete.

2. The level of minimum web reinforcement for HSRC beams, to avoid sudden

and brittle failure of beams may be identified.

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3. Parametric study for the shear strength of HSRC beams, incorporating

important parameters affecting the shear strength of HSRC beams is

required, supported by the experimental work to develop more rational

equations to determine shear strength of HSRC beams.

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Chapter No. 4

Shear Strength prediction of disturbed region (D-region) in

reinforced concrete.

Chapter Introduction: This chapter explains the basic concept of the beam (B) region and Disturbed (D) region. The need for special attention to the design of disturbed region has been discussed. The basic philosophy of Strut and Tie Model (STM) for the design of disturbed region has been given in quite details. It is followed by the explanation of basic design principles and steps for the design of D-region. At the end some STM have been given for various types of disturbed regions in concrete structures.

4.1 The basic concept of beam and disturbed region:

Structures are sometimes classified as either B- (Beam or Bernoulli) Regions or D-

(Disturbed or Discontinuity) Regions, for selection of appropriate design procedure.

B-Regions are parts of a structure in which Bernoulli's hypothesis of straight-line

strain profiles applies. D-Regions, on the other hand, are parts of a structure with a

complex variation in strain. D-Regions include portions near abrupt changes in

geometry (geometrical discontinuities) or concentrated forces (statical

discontinuities), such as deep beams, corbel, pile caps, dapped ended beams,

brackets etc.

Figure 4.1 and Figure 4.2 show examples of the division between B-Regions and D-

Regions in building and bridge structures, respectively. In these figures, the un-

shaded area with a notation B indicates B-Region, and the shaded area with a

notation D is used to indicate D-Region. The notations h1, h2, h3 ... are used to

denote the depth of structural members. The notations b1 and b2 denote the flange

width of structural members.

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Figure 4.1: Example of B & D-Regions in a Common Building Structure (Schlaich et al

,1987)

Figure 4.2: Example of B& D-Regions in a Common Bridge Structure. (Schlaich. et al. 1987)

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Figure 4.3 Typical D regions shown as shaded areas, adapted from Schlaich et al. (1987).

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4.2 Basic design principles for shear design of disturbed region

Most design practices for B-Regions are based on conventional beam theory or

flexural theory, while the design for shear is based on the well-known parallel chord

truss analogy. In contrast, the most familiar types of D-Regions, such as deep

beams, corbels, beam-column joints, and pile caps, are currently still designed by

empirical approaches or by using common detailing practices. For most other types

of D-Regions, code provisions provide little guidance to designers. Presently the

following four approaches are used for the design of disturbed region in RC

structures;

1. ACI equation and detailing methods

2. Truss analogy

3. AASHTO-LRFD Standards

4. Strut and Tie Model (STM).

The Strut-and-Tie Method (STM) is an emerging methodology for the design of all

types of D-Regions in structural concrete. It is worth noting that although the STM is

equally applicable to both B- and D-Region problems; it is not practical to apply the

method to B-Region problems. The conventional beam theory for flexure and parallel

chord truss analogy for shear are recommended for those designs. The idea of the

strut-and-tie method came from the truss analogy method introduced independently

by Ritter in the early 1900 (Riltter, 1899) for shear design of B-Regions.

This method employs the so-called truss model as its design basis. The model was

used to idealize the flow of force in a cracked concrete beam. In parallel with the

increasing availability of experimental results and the development of limit analysis

in plasticity theory, the truss analogy method has been validated and improved

considerably in the form of full member or sectional design procedures. The truss

model has also been used as the design basis for torsion.

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4.3 Use of Strut and Tie Model (STM) as a design tool for structural components.

Strut-and-Tie (STM) is a unified approach that considers all load effects (M, N, V,

and T for moment, axial force, shear force and torsion, respectively) simultaneously.

The Strut-and-Tie model (STM) approach evolved as one of the most useful design

methods for shear critical structures and for other disturbed regions in concrete

structures. The model provides a rational approach by representing a complex

structural member with an appropriate simplified truss model. There is no single,

unique STM for most design situations encountered. There are, however, some

techniques and rules which help the designer to develop an appropriate model.

However the selection of appropriate truss model is an uphill task. The STM more

accurately predicts the shear strength of the beams whereas a/d is less than 2.5. For

slender beams having a/d>2.5, a sectional model approach, that also includes Vc

caused by tensile stresses in the concrete is more appropriate.

The basic assumptions for application of STM to disturbed region are (Fu, 2005)

i. STM is a strength design method and the serviceability should also be

checked .i.e. stresses in any part of the structure must not exceed the

allowable stresses.

ii. Equilibrium of internal and external forces must be maintained

iii. Tension in concrete is neglected and usually the concrete struts are assumed

to take the compressive force and the steel the tension.

iv. Forces in struts and ties are uni-axial. Planar and uni-axial analysis is done

due to specific geometry of the structures.

v. External forces apply at nodes, like trusses.

vi. Pre-stressing is treated as a load, applied at the nodes of the truss.

vii. Detailing for adequate anchorage is provided, to ensure proper anchorage of

the steel bars.

4.4 Steps involved in the design of D-region using STM.

The joint committee report of ACI and ASCE on Shear and Torsion ( ACI-ASCE-

445,99) has given the following steps for the design of disturbed region in RC

structures

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4.4.1 Choosing a STM for the structure (D-region)

The first step in STM is to visualize the flow of forces with compressive struts

representing the flow of concentrated compressive stresses in the concrete and

tension ties representing the steel. The struts and ties are essential for the

equilibrium. Schlaich et al (1987) have suggested that the strut and tie model may be

selected on the basis of elastic analysis, so that the angles of compression

diagonals are + 15 degree of the angle of resultant. The compressive struts are

bulging between the load points and supports, causing a transverse tension

idealized by tension ties. However for simplification, the compressive struts are

idealized as straight line members following the centerline of the compressive struts

as shown in Figure 4.4. Hence most of the codes require a minimum additional

reinforcement in the struts and ties to control cracking.

Figure 4.4 Crack control reinforcement required with assumed straight-line compressive struts, proposed by Schlaich et al. (1987) ( ACI-ASCE-445R-99).

4.4.2 Checking compressive stresses in struts

In the shear design by STM, it is necessary to check that crushing of compressive

struts do not occur. Bregmeister et al. (1991) suggested the stress limit of for the

unconfined bearing plate node, the factored bearing strength as;

c

bc

fA

A

ffc 5.0))(

25.15.0( ( 4.1)

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Ramirez (1990) proposed the stress limits listed in Table 4.1 Table 4.1 Effective stress level in the concrete struts (Ramirez, 1990)

Effective Stress level

Concrete Struts Proposed by

0.80fc’ Undisturbed and uni-axial state of compressive stress that may exist for prismatic strut

Schlaich et al. (1987)

0.60fc’ Tensile strains and/or reinforcement perpendicular to the axis of the strut may cause

cracking parallel to the strut with normal crack width Schlaich et al. (1987)

0.51fc’

For skew cracks with extraordinary crack width. Skew cracks would be expected if modeling of the struts departed significantly from the theory of elasticity’s flow of internal forces

Schlaich et al. (1987)

0.34fc’ Moderately confined diagonal struts going directly from point load to support with shear

span-to-depth ratio less than 2.0 Schlaich et al. (1987)

0.75fc’ Struts forming arch mechanism Alshegeir and

Ramirez (1990)

0.50fc’ Arch members in pre-stressed beams and fan compression members Alshegeir and

Ramirez (1990)

0.95fc’ Undisturbed and highly stressed compression struts Alshegeir and

Ramirez (1990)

v2fc’ Uncracked uniaxially stressed struts or fields Alshegeir and

Ramirez (1990)

v2(0.80) fc’ Struts cracked longitudinally in bulging compression fields with transverse

reinforcement Alshegeir and Ramirez (1990)

v2(0.65) fc’ Struts cracked longitudinally in bulging compression fields without transverse

reinforcement Alshegeir and Ramirez (1990)

v2(0.60) fc’ Struts in cracked zone with transverse tensions from transverse reinforcement MacGregor (1997)

v2(0.30) fc’ Severely cracked webs of slender beams with q = 30 degrees MacGregor (1997)

v2(0.30) fc’ Severely cracked webs of slender beams with q = 45 degrees MacGregor (1997)

Note: v2 = 0.5 + 1.25/Öf ¢c in MPa after Bergmeister et al. (1991).

Jisra et al.( 1991) recommended an effective concrete strut stress level of 0.8 fc’

4.4.3 Design of nodal zones

The types of nodal zones and dimensions of struts have been shown in the following

Figure 4.5. These nodal zones are defined as

CCT: Nodal zone bounded by compression Struts and one tension ties

CCC: Nodal zone bounded by compression struts only.

CTT: Nodal zone bounded by compression struts and tension ties in two or more

directions.

TTT: Nodal zone bounded by Tension Ties only.

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Figure 4.5 Classifications of Nodes (Ref: ACI- 318-06)

The Canadian standard (“Design” 1984) limits the concrete stress in the nodal zones

to the following values:

- 0.85φfc’ in node regions bounded by compressive struts and bearing areas (CCC

nodes);

- 0.75f φfc’ in node regions anchoring a tension tie in only one direction (CCT

nodes); and

- 0. 60φfc’ in node regions anchoring tension ties in more than one direction (CTT

nodes), where f is the capacity- reduction factor for bearing.

Bergmeister et al. (1991) proposed several equations of effective concrete strength

for various kinds of nodes, including reinforcement, unconfined nodes with bearing

plates, and tri-axially confined nodes.

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4.4.4 Design of tension ties

The area of reinforcement for tension ties are determined as

usepspsyst NffAfA ))(( (4.2)

Where Ast = area of reinforcing bars; Aps = area of pre-stressed reinforcement; fy = yield strength of reinforcing bars; fps = stress in pre-stressed reinforcement at ultimate; φ= capacity-reduction factor for axial tension (0.9); and fse = stress in pre-stressing steel after all losses.

4.4.5 Anchorage of tension ties

The anchorage of tension ties must be sufficient to develop the required stress in

reinforcement. The anchorage zone must be spread over large area so that there is

no crushing of the nodal zone and the embedment of reinforcement must be

sufficient.

Some the basic models for different disturbed regions are as given in Figure 4.6 to

Figure 4.9

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a. Column with double corbel

b. Column with single corbel

c. Beams with double ledged supports

d. Beam with single ledge support.

Figure 4.6 Strut-and-tie model idealizations for brackets, ledges, and corbels (Cook and Mitchell 1988).

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Figure 4.6 Proposed STM for Deep beams under applied external load (Schlaich et al.1987)

Figure 4.7 Proposed STM for one way corbel under applied external load (Fu,2005).

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Figure 4.8 Proposed STM for two way corbel under applied external load (FU,2005).

Figure 4.9 Proposed STM for dapped beam end under applied external load (Fu,2005).

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Figure 4.10 Proposed STM for pile cap under applied external load (Fu,2005).

4.5 Some latest research on the shear design of disturbed region with STM:

Shyh-Jiann Hwang and Hung-Jen Lee (2002) developed a simple procedure on the

basis softened STM for predicting the shear strength of discontinuity region failing in

diagonal compression. A simplified equation was proposed which incorporates the

shear resisting mechanism of softened STM. The experimental values of 449

disturbed regions like deep beams, corbels, squat walls and beam column joints

were compared with the proposed model and the coefficient of variation was

observed as only 6%.

Foster and Adnan (2002) introduced an efficiency factor for softening of concrete

and other strength reduction effects such as that of transverse tension strains. They

analyzed three basic models such as (i) Models based on the concrete strength (ii)

Multi-parameter models and (iii) Model based loosely on Modified Compression

Field Theory ( MCFT). In this study, it was observed that models based on concrete

strength did not correlate well with the experimental data of non flexural members.

The multi-parameter model of Batchelor et al.(1984) and Chen also did not correlate

well with the experimental data. The model based on strut angle (Shear span to

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depth ratio) gave the best prediction of the efficiency factor to calculate the capacity

of concrete struts. They further reported that the influence of boundary effects is of

considerable importance in the determination of the mode of failure of non flexural

members.

Wight (2001) explained the key features of ACI-318-02, building Code for the use of

Strut and Tie Model by the designer, however later the methods was incorporated in

ACI318-06, as an alternate design method for some structural components.

Hamed and M.Salem (2004) introduced the concept of micro truss model for the

design and checking the non linear response of concrete structures. The micro truss

model is formulated with the simple stiffness method, where careful non linear

algorithm is applied. The micro truss model is generalized form of STM which can be

developed without much experience. It was observed in this research that the

reinforcement worked out on the basis of Micro Truss model was less than the

general STM model. The Schalaich Model of STM has been based on equilibrium of

STM and hence it is lower bound solution. Therefore over estimation of

reinforcement may exist. Again contribution of the non cracked concrete (tension

stiffening) and contribution of cracked concrete (tension softening) is neglected by

Schalaich, as reported by the researchers.

Tan et al. (2001), applied the STM for the design of pre-stressed deep beams by

proposing a simple and direct model and evaluated the results of 39 deep beams

with the proposed model. They reported that the proposed STM for pre-stressed

deep beams has given consistent and accurate prediction of small and large pre-

stressed beams for different geometrical properties, various pre-stressing force and

different web reinforcement.

Tan (2004) worked on the use of STM for the design of non prismatic members

including beams with recesses and geometric discontinuities. He reported that STM

provides a simple and straightforward solution to otherwise a complicated problem.

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Tjen et al. (2002) developed a software as Computer Aided Strut and Tie ( CAST)

for generating the STM for a particular problem, which involves all aspects of the

problem like definition of D-region, selection of STM, truss analysis, members

definitions, and design summary. This tools is being used and improved with the

feedback from users and researchers.

Vollum and Tay ( 2001), tried to estimate the effect of node dimensions on the shear

strength of short span beam as predicted under STM by testing 12 short span

beams of a/d ratio as 1.6. They also studied the influence of the concrete

compressive strength on the shear strength of beams given by the relevant

provisions of EC2, and Collins et al (MC90). From their research, they made the

following important inferences;

- STM has overestimated the influence of node dimensions on the shear strength

of RC short beams.

- STM has failed to predict the observed failure modes of the beams.

- STM could not predict the influence of concrete strength on the shear strength of

the RC short beams, if the provisions of EC2 and MC90 are used.

- MC90 has been observed as more conservative for shear design of RC short

beams.

- They have concluded that the current empirical design equations proposed by

BS8110 and EC2 are more practical for design of short span RC beams than

simple STM. The same is also true for the shear design of Beam Column

connections/. However the authors have suggested that STM can better assist in

detailing of reinforcement in the RC beams.

According to ACI 318-06, it shall be permitted to design structural concrete members

or D-regions in such members, by modeling the member or region as an idealized

truss. The truss model shall contain struts, ties, and nodes. The truss model shall be

capable of transferring all factored loads to the supports or adjacent B-regions. Strut-

and-tie models represent strength limit states and designers should also comply with

the requirements for serviceability in the code. Deflections of deep beams or similar

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members can be estimated using an elastic analysis to analyze the strut-and-tie

model. Besides ACI 318-06, Strut and Tie Model has been included in the following

building codes as well.

a. AASHTO-LRFD Bridge Design Specifications 3.3

b. CSA A23.3-94 (Canadian Code)

c. NZS 3101:1995 (New Zealand Code)

d. FIB Recommendations (Eurocode-2)

Brown (2005) worked on the use of STM for the shear design in reinforced concrete

in his doctoral studies and made the following important conclusions:

i. When the STM provisions of the ACI-318 and AASHTO RLFD of Bridge

design are applied to the test data, they provide less conservative results.

ii. Beams subjected to uniform loads exhibit increased shear strength

compared with beams with concentrated loads.

iii. Current ACI 318 provisions for sectional design result in un-conservative

estimates of strength for beams with concentrated loads between 2 and 6

times the effective depth from the support.

iv. Shear span-to-depth ratio has a large effect on shear strength.

v. The strength of beams with shear span-to-depth ratios less than two are

better represented by a direct strut mechanism.

vi. Nearly parallel shear cracks were observed just prior to failure of the beam

specimens.

vii. Failure occurs due to crushing of the strut at node-strut interfaces.

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He has made a number of recommendations for further research in the application of

STM to shear design of beams.

The Strut and Tie Model (STM) will continue as design option for both disturbed and

beam regions in concrete structures. However the experience of designers to use

the STM to various design problems and modern research shall play an active role

in standardizing the design techniques on the basis of STM. Extensive research is

therefore required to generalize the STM as an equally acceptable design tool for

concrete structures, particularly for the disturbed regions in concrete structures.

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Chapter No. 5

Provisions of International Building and Bridges Codes for

Design shear Reinforcement of Normal and High Strength

Concrete Beams.

Chapter Introduction: This chapter gives a brief summary of the provision in the selected international building and bridges codes for shear design of concrete beams. Certain research on the comparison of building codes for shear design has been given with some important findings.

The shear design of the normal and high strength concrete beams is usually done by

adopting the provisions of different codes based on various rationales. These

provisions are expressed in the form of empirical equations. Some of the most

commonly used design equations for the shear design of RC structures are as

follows;

i. British Standards (BS-8110)

ii. ACI Code 318 (American Concrete Institute)

iii. Canadian Standards for design of Concrete structures. CSA A-

23.3-94

iv. AASHTO LRFD (Load Reduction Factor Design) Bridge Design

Specifications -2004

v. European Code EC2-2003.

vi. Empirical methods for beams without shear reinforcement.

The design equations and relevant code provisions are illustrated in the following

sections.

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5.1 British Standards (BS-8110)

A semi-empirical approach was developed by Regan in 1967 and used in CP

110:1972, and also used in BS 8110. According to BS-8110, the characteristics

design equation for shear capacity is given as (BS, 2005).

4/13/121 400

100.79.0

dbd

AKKR s

mLW

c (Ref: BS 3.4.5.4, Table 3.8) ……. (5.1)

k1 is the enhancement factor for support compression, and is conservatively taken as 1, (Ref. BS 3.4.5.8)

0.125/ 3/12 cufK (Ref. BS 3.4.5.4, Table 3.8)

m = 1.25 (Ref. BS 2.4.4.1)

sA is area of tensile steel

0.50≤

bd

As100 ≤ 3.0 (Ref BS 3.4.5.4, Table 3.8)

d

400≥ 1.0 and fcu ≤ 40 N/mm2 (for calculation purpose only). (BS 3.4.5.4, Table 3.8).

The Eq. 5.1 is subject to the following conditions.

If ≤ c provide minimum stirrups defined by yvv

sv

f

b

S

A

95.0

4.0 (Ref. BS 3.4.5.3)

If c +40 ≤ ≤ max provide shear steel as yv

c

v

sv

f

b

S

A

95.0

)( (Ref. BS 3.4.5.3)

If ≥ max , a shear failure is declared. (Ref. BS 3.4.5.2, 3.4.5.12)

5.2 European Code EC2-2003.

Shear is dealt with by clause 4.3.2 and 4.3.4 of Eurocode EC2. The following four

cases are given in the code for shear design of RC structures ( Eurocode, 2003).

i. Members without shear reinforcement

ii. Strength of members with shear reinforcement

iii. Maximum shear strength that can be carried by a member.

iv. Behaviour of section close to supports.

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1RDV : The shear strength for members without shear reinforcement

2RDV : The upper limit of the shear strength to prevent web crushing failures.

3RDV : The shear strength for members with shear reinforcement.

dbkV wlrdRD )402.1(1 ( SI units) (5.2)

)51(,5.2

x

d an enhancement factor can be applied if the member is loaded by a

concentrated load situated at a distance dx 5.2 from the face of the support

RD : Basic design shear strength = 05.025.0 ckf

05.0ckf : Lower 5% fractile characteristic tensile strength= ctmf7.0

ctmf : mean value of the tensile concrete strength=3/2)(3.0 ckf

0.1)1000/6.1( dk

ckf = characteristic cylinder compressive strength of concrete '9.0 cf

dbA wsll / wb= effective web width, = effective depth

Thus, the above equation can be simplified to the following equation.

dbfkV wlckRD)402.1()(0525.0 3/2

1 (SI units) (5.3)

)9.0(5.01

dbfV wcdRD

(SI units) (5.4)

cdf Factored design strength= 15/ckf

(For analysis purpose cdf = ckf is considered to be appropriate)

: The effectiveness factor 5.0200

7.0 kf c (may taken as 0.6)

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5.3 ACI Code 318-06 (American Concrete Institute)

The ACI building code 318-06 is no doubt the most widely applied Code for the

shear design of concrete. The nominal shear capacity of reinforced concrete beam

Vn, is given as the sum of Concrete contribution Vc, and contributions of stirrups Vs

.i.e.

Vn = Vc + Vs

For beams without shear reinforcement, the shear capacity is given as;

Reinforced Concrete Members: (limit < 70 MPa)

dbf

Vc wc

6

'

(SI units) (ACI 11.3) (5.5

7

120' db

M

dVfVc w

u

uc

(SI units) (ACI 11.5)

Or dbM

dVfVc w

u

uwc

25009.1 '

(English units) (5.6)

When 0.1.0.5ln/ u

u

M

dVandd

Where '

cf = Compressive strength of concrete

w = Longitudinal steel ratio

wb = Width of the beam web.

uM Factored Moment at the section

dV

M

u

uExpression for the shear span to depth ratio a/d

ACI code limits the value of cf to 100 psi (8.3 MPa) unless the amount of web

reinforcement is increased as per Clause 11.1.2.1 by the ratio.

cf /3.45 ≤ 3.0 (ACI 11.1.2.1)

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y

wv f

sbA 345.0 (ACI 11.13) (5.7)

For High Strength Concrete (HSC), the minimum shear reinforcement is given as

y

ww

y

cv

y

wv f

sbsb

f

fA

f

sbA 035.1

01.0345.0

'

for 69MPa≤ 'cf (ACI 11.1.2.1) (5.8)

For members subjected to compression, the shear strength is given as;

dbfA

NVc wc

g

u '

200012

( English units) ( ACI 11.3.1.2) (5.9)

Subject to maximum value of

dbfA

NVc wc

g

u '

50015.3

( English units) (ACI 11.3.2.2) (5.10)

Where Nu is ultimate compression force and Ag is gross area of the compression member.

For members subjected to significant axial tension, the shear strength is given as

dbfA

NVc wc

g

u '

50012

( ACI 11.3.2.3) (5.11)

For members having pre-stressed forces;

dbM

dVfVc w

u

puc

7006.0 '

( ACI 11.4.2) (5.12)

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5.4 Canadian Standards for design of Concrete structures. CSA A- 23.3-94

The General design method of Canadian Code has been based on Modified

Compression Field Theory (MCFT) and applies to concrete up to 81 MPa (16000

psi). The factored shear resistance of non pre-stressed section is given as

sgcgrg VVV (5.13)

vwcccg dbfV ')12(3.1 (CSA 11.18) (5.14)

sdfAV vyvssg /)cot(cot (CSA 11.20) (5.15)

rgV ; Factored shear strength of RC member

;cgV Concrete contribution

sgV ; Steel contribution

=Angle of inclined stirrup to longitudinal axis.

= Factor accounting for shear resistance of cracked concrete.

= Factor accounting for density of concrete; 1 for normal density concrete

= Angle of inclination of diagonal compressive stresses to longitudinal axis member

sc , = material factor for concrete and steel 85.0,60.0, sc

y

wcv f

sbfA '06.0min (CSA 11.1) (5.16)

The method for determining of the values of has already been explained in the

MCFT.

A more simplified design method gives

dbfdbfd

V wcwcc

1.0

100

260 (5.17)

if y

wc

v f

sbfA

06.0 d≥300mm ( CSA 11.7) (5.18)

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s

dfAs

V yvs i.e. =45 degrees, 90 degrees (CSA 11.20) (5.19)

5.5 AASHTO LRFD (Load Reduction Factor Design) Bridge Design Specifications -

1996.

It is based on MCFT applicable to both non-pre stressed and pre-stressed concrete,

for 16 cf 70 MPa range.

The nominal shear strength of RC beams is given as

Vn = Vc + Vs.

vvcvvcc dbfdbfV '' 25.0083.0 (5.20)

. indicates ability of diagonally cracked concrete to transmit tension.

=2 for d≤400mm

This is 38% more than the Canadian Code.

For culverts less than 600 mm or more fill,

Where 0.1u

u

M

dV

y

vvcv f

sdbfA '083.0

(5.21)

5.6 Empirical methods for beams without shear reinforcement

Zsutty’s (1968) proposed the following empirical equation on the basis of regression

analysis of database of shear strength of 151 beams;

vvcc dba

dfV 3/12.2 for a/d ≥ 2 (5.22)

The empirical equation of Okumura (1986), Niwa (1986) included all the important

parameters for the shear strength of beams without shear reinforcement.

Vc = 0.20 ρ 1/3 /d ¼ (fc′)1/3 (0.75 + 1.40 bw d) fc' in MPa. …………………… (5.23)

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Table5.1 Summary of Major Code Expressions for the Concrete Contribution to Shear Resistance

Codes or Researcher

Equations Factors

Accounted ACI 318-95 (1995) db

fVc w

c

6

'

(SI units) Simplified Equation

dbfdb

M

dVfVc wc

w

u

u

wc

'' 3.07

120

(SI units)- Detailed Eq.

f'c, (a/d),

AASHTO LRFD 1996 vvcvvcc dbfdbfV '' 25.0083.0

f'c, (d), (a/d), (), agg

Canadian Standard

CSA A23.3-94 (1994)

dbfVc wc'2.0 (SI Units) if sb

f

fA w

y

cv

'06.0 or mmd 300

dbfdbfd

V wcwcc

1.0

1000

260 (SI units) if

sbf

fA w

y

cv

'06.0 , d>300mm

f'c, d, a/d

Eurocode EC2, Part 1 (1990) dbkV wlrdRD )402.1(1 where ,5

5.21

x

d

,0.1)1000/6.1( dk 5.0200/7.0 ylf

f'c, d, a/d,

British Standard BS 8110 (1985)

4/13/121 400

100.79.0

dbd

AKKR s

mLW

c (SI units) for a/d ≥ 2

f'c, d,

Zsutty’s equation (1968)

vvcc dba

dfV 3/12.2 (SI units) for a/d ≥ 2

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5.7 Research on high strength concrete beams and its comparison with building

codes at different Universities in near past.

A number of researchers have dealt with shear problem in different ways and the

experimental results vary from case to case. Some of research results have been

given in Table 5.2, which shows the findings of these researches on high strength

concrete beams and its comparison with the building codes. The results of Cornel

University tests and Purdue University tests have given some important results for

further verification. The findings of the earlier tests, describing the provisions of ACI

Code for shear strength of HSC as un-conservative by 10-30% are a significant

outcome. Similarly the later findings at Purdue University, requiring increase in the

minimum web reinforcement for compressive strength more than 10,000 psi are also

an important recommendation.

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Table 5.2 Summary of Research Results conducted at various Universities.

University Researchers Design Parameters Results/Findings.

Cornel University

Elzanti and Nilson ( 1987) Nilson and Slalte ( 1986)

Beams with web Reinf. fc’ = 9100 psi ( 1 beam) fc’ = 5800 psi ( 1 beam)

ACI Code equation is un-conservative by 10% to 30% for high strength and medium strength Concrete

Connecticut University

Maphonde and Frantz ( 1984) Rotter and Russel ( 1990)

Beams without web steel. fc’≤ 6500 psi ( 11 beams) at a/d = 3.6 Beams with web reinf. fc’ ≥ 6000 psi ( 12 beams) fc’= 5000 psi to 10500 psi

The following equation was proposed as compared with Zustty’s equation; Vu = 63.40 ( ρ fc’ d/a) 1/3 - Proposed the following equation on the basis of Regression analysis. Vn= 1.15 √fc’ +90+1.6Avfy/bs - The ACI 318-99 provisions require an increase in the minimum reinforcement for fc’≥ 10,000 psi

Purdue University

Johnson and Rameriz ( 1989)

fc’= 5000 psi to 10500 psi The result justified the ACI code provisions to limit fc’ to 10,000 psi and increase in the min web reinf by fc’/5000

Norwegian University

Torenfeldt Draug Sholt ( 1990)

Beams without web reinf. (Under two point load) fc’ = 7800 to 14200 psi a/d = 2.30 to 4.0 ρ = 1.8 % to 3.20 %

The tensile strength remained constant after fc’= 10,000 psi. The ultimate shear strength increased with increase in the shear span to depth ratio.

Korean Test Kim amd Park (1994)

Beams with web reinf fc’ = 5300psi ( 20 Nos) Beams without web reinf fc’ = 5300psi ( 06 Nos)

- CEB- FIB gave the closer results. - BS 8110 is excessively conservative. - ACI equation is safe for large beams. Effect of ρ and a/d ration has not been significantly improved by concrete strength - The size effect for HSC is same as NSC.

Comparison of ACI and AASTO LRFD method

Shahwy and Batchelor( 1996)

AASHTO type II ( 1989) 20 pre-tensioned beams and compared it with AASHTO LRFD specs.

- AASHTO 1989 based on ACI 1994 provisions give excellent predictions of girders having shear reinf, between 1 and required by the Code ( R) The LRFD code over estimates the shear strength of over designed girders (2R<ρv<3R) and under estimates the under designed girders (0<ρv<R/2> - For ρv = R , ASSHTO 1989, provide better estimates.

University of Japan

Tagaki and Kanoh ( 1991)

-Used high strength steel of 800 MPa ( 116000 psi) as shear reinforcement.

- Use of high strength stirrups is efficient for high strength concrete.- The effectiveness of high strength stirrups in NSC is not ensured yet.

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5.8 National Cooperative Highway Research Program (USA), for the evaluation of

shear design for simplified shear design method for structural concrete members

(NCHRP, 2005)

National Cooperative Highway Research Program (NCHP) was initiated by

Transportation Research Board (National Academies -USA) in 2005 to develop

“Simplified Shear Design of Structural Concrete Members”. This research was

performed by the University of Illinois at Urbana-Champaign. The objectives of the

research program are given as follows;

i. The simplified provisions must be directly usable without iteration for shear

design and evaluation of the shear capacity of the members.

ii. Must be useful in conducting field evaluation to estimate the failure loads for

the shear cracking by the site Engineers.

iii. Must be easy to explain by the Engineers to others.

iv. Allow reliable and hand based design method.

v. Provide safe and accurate estimates for the RC members in the selected test

database.

vi. The shear reinforcement as a result must be reasonable.

5.8.1 Evaluation of shear design methods using test database

The shear test database of 1359 beams of NSC was studied by National

Cooperative Highway Research Program (NCHRP),USA which consisted of 878 RC

beams and 481 pre-stressed concrete beams. In total of 1359, those containing

shear reinforcement were 160 whereas 718 did not contain shear reinforcement.

The test results Vtest were compared with the code values Vcode for the six different

codes and the mean and coefficient of variation ( CoV) were determined from the

Vtest/Vcode values as tabulated below in Table 5.3

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Table 5.3 Comparison of test values and Codes values based on shear data base (NCHRP; 2006)

Member Type All RC-beams Pre-stressed beams. Inferences

With or

without AV

No

Both

RC

No Av

RC

With Av

Both PC

No Av

PC

With Av

- CSA and

LRFD has given

best results

particularly

Nos.

Code

1359 878 718 160 481 321 160

ACI

Mean 1.44 1.51 1.54 1.35 1.32 1.38 1.21

CoV 0.371 0.404 0.418 0.277 0.248 0.247 0.221

LRFD

Mean 1.38 1.37 1.39 1.27 1.40 1.44 1.32

CoV 0.262 0.262 0.266 0.224 0.261 0.290 0.154

CSA

Mean 1.31 1.25 1.27 1.19 1.41 1.46 1.31

CoV 0.275 0.274 0.282 0.218 0.261 0.287 0.147

JSCE

Mean 1.51 1.36 1.35 1.38 1.80 1.85 1.70

CoV 0.321 0.28 0.293 0.216 0.292 0.297 0.272

EC2

Mean 1.85 1.75 1.75 1.70 2.06 2.13 1.91

CoV 0.409 0.328 0.328 0.373 0.470 0.43 0.687

DIN

Mean 2.05 2.10 2.10 1.25 2.25 2.59 1.58

CoV 0.395 0.327 0.327 0.267 0.413 0.345 0.357

Av; stands for beams with shear reinforcement.

The following results have been inferred from the analysis of database.

CSA (Canadian Code) and LRFD (AASHTO) have given best results

particularly for Prestressed concrete (PC) beams with shear reinforcement.

ACI provisions are poor predictor of shear for reinforced concrete (RC) &

prestressed concrete (PC) beams with no transverse reinforcement but for

beams with Av, these are reasonably good, hence Av is required where

Vu≥φVC/2

DIN (Denmark Code) is very poor predictor followed by JSCE (Japan Society

of Civil Engineers Code).

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The following major variations were reported by NCHRP the shear design

provisions of building codes;

i. The amount of shear reinforcement calculated by different codes widely

varies and in some cases, it is even two to three times for the same

section and external forces, when calculated with different codes.

ii. The minimum shear reinforcement also varies substantially from code to

code and in some cases it is double, than the others.

iii. Some codes require providing the minimum shear beyond the section,

where the factored deign shear force is half the design strength of

concrete while others require it when the factored shear exceeds the

design strength of the section.

iv. Again there is great variation in the maximum allowed shear reinforcement

by different codes.

v. The depth effect also called the size effect has been taken into account by

very few codes. In practice, the depth has substantial effect on the shear

capacity

vi. The shear design provisions are based on the experimental data,

equilibrium conditions, and comprehensive behaviour of the model for

capacity.

5.8.2 Simplified shear design method proposed by NCHRP

As a result of the project, an alternative and simplified shear design method was

proposed to overcome the limitations of the LRFD sectional design model. The

following simplified provisions were recommended by the project.

1. The web shear cracking Vcw was simplified as

pvvpcccw VdbffV )30.09.1( ' ( in English System) (5.24)

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pcf ; Compressive stress in concrete after all pre-stress losses have occurred either at

centroid of the cross-section resisting live load or at the junction of the web and flange when

the centroid lies in the flange.

Vp is the pre-stress force applied to the section.

2. Flexure-shear cracking strength is given as

pcri

dvvcci VM

MVVdbfV

max

'632.0 (5.25)

Vd = shear carried by dowel action; shear force at section due to un-factored dead load.

Vi =factored shear force at section due to externally applied loads occurring

simultaneously with Mmax

Mcr = cracking moment.

3. Contribution of shear reinforcement is given as

cots

fAV yv

s

( 5.26)

For value of

8.1095.00.1'

c

pc

f

fCot

When Vcw < Vct ( where stresses given in psi)

Hence for no pre-stress, fpc = 0 and cotθ= 1.0 and θ = 45degree

4. vvcsc dbfVVVn '25.0 ( 5.27)

Where vvcc dbfV ' ( 5.28)

sfAV yvs

sin)cot(cot

( 5.29)

3102.0

)(2

__5.0/

ppss

pspspuuvux AEAE

fAVVNdM (5.30)

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For members having less than Avmin, the equivalent crack spacing is determined as;

)63.0(

38.1

g

xex a

SS

(5.31)

Where ga is maximum aggregate size.

To determine the shear resistance of the cracked concrete, ß = 4.8

The minimum shear reinforcement is given as :

y

vcv f

sbfA

'

min (5.32)

For members having at least minimum shear reinforcement, the angle of diagonal

compression is given as;

x 700029

and is obtained as above.

The simplified design method of NCHRP, when applied to the shear data base gave

relatively less coefficient of variation. The flow chart for the simplified design method

is given in Figure 5.1

5.8.3 Recommendation of the NCHRP

The research project of NCHRP further made the following recommendations;

i. Web based national data base of shear test results may be established.

ii. More research is required on the types of beams and material, for which

very little or no database is available.

iii. Data on high strength concrete beams is very little and further research is

required.

iv. The range of applicability of size effect and its relationship to minimum

shear reinforcement needs to be better understood. The size effect rather

than the compressive strength of concrete may be the best estimator for

minimum shear reinforcement.

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No

Figure 5.1 Flowchart for use of the NCHRP simplified design method (NHRP, 2006).

START

Given bv,dv,Mmax,fc’, Vp, Nu, fp, Ap…

Where f'c in Ksi

Vn/φ>0.25f’cbvdv+Vp?

RC members

vvcc dbfV ,06.0 Prestressed Members (PC)

cV is lesser of

vvccri

dvvcci dbfM

MVVdbfV ,

max

, 06.006.0

and

pvvpocc VdbffV )3.006.0( ,

Required shear strength for shear reinforcement:

9.0

whereVV

Vs cu

Calculate required shear reinforcement:

min)/(cot

/ sAordf

VsA v

vy

sv

Where y

vcv f

bfsA '

min 0316.0)/(

For value of cot : For RC members 0.1cot For PC members if cwci VV or 0.1 CotMM cru

Otherwise 8.130.1' pe

f

fCot

End

Increase the section

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5.8.4 Summary of literature review of shear strength of beams ( B-region) and

Disturbed (D-region) in RC members.

The literature reviewed in this study has revealed the following broader facts in the

contemporary research on the shear design of reinforced concrete structures,

including beams (B- region) and Disturbed region (D-region).

i. The shear strength of HSRC beams is not increasing in the same

magnitude as in case of the NSRC beams with the increase in

compressive strength of the concrete. This may be mainly due to loss

in the shear resistance due to aggregate interlocking.

ii. The shear failure of HSRC beams is relatively brittle. This failure

becomes even more brittle and sudden with further increase in the

compressive strength of concrete. Hence the HSRC beams without

web reinforcement poses severe design threat.

iii. The research data on the shear strength of HSRC beams is limited and

cannot be used for some major changes in the provisions of building

codes.

iv. The minimum web reinforcement for the shear design of beams is

required to be rationalized to ensure ductile failure of the HSRC

beams.

v. The Codes provisions provide very little information about the shear

design of HSRC beams with compressive strength of 90Mpa and

more.

vi. There are wide variations in the required web reinforcement under

different building codes for external applied loading conditions. Hence

joint work is required to rationalize and generalize the provisions of

these building codes. Even for minimum web reinforcement, the values

proposed by various building codes vary significantly.

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vii. The latest concepts of shear design of HSRC beams are relatively

rational but complicated and require more simplification for the use of

designers.

viii. Though extensive research has been carried out in the last six

decades to comprehend the shear behaviour of RC beams, yet the

shear strength of HSRC structures is relatively newer area and more

research is required in this direction.

ix. The design of disturbed region in concrete structures requires serious

considerations in the contemporary research.

x. The Strut and Tie Model (STM) has been used to analyze and design

both the beam and disturbed regions in structural concrete more

frequently in the latest research around the world. However the use of

STM for practicing structural engineers in the field still poses many

challenges.

xi. The selection of an appropriate STM is the most difficult part of the

design decision of disturbed region with STM. Some computerized

models have been developed, which uses a number of iterations to

reach at identifying the most critical truss path. However application of

the STM tool for the design of shear critical structures would require

more experimental research.

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Chapter No. 6

Experimental programme and discussion of test results

Of HSC beams (B-region)

Chapter Introduction: This chapter is based on the experimental program of research in the HSC beam, followed by the discussion of the experimental results, failure modes of the beams and effects of various parameters on the shear strength of HSC beams. At the end general comments on the shear behaviour of HSRC beams with and without web reinforcement has been given.

6.1 Introduction to experimental programme

Experimental programme to better understand the shear behaviour of high strength

concrete was conducted at Structural Engineering Laboratory of Civil Engineering

Department, University of Engineering & Technology, Taxila Pakistan.

6.1.1 Objectives of the experimental programme are as follows;

1. To study the effect of shear span to depth ratio on the shear capacity

of HSRC beams.

2. To study the effect of longitudinal steel on the shear capacity of HSRC

beam.

3. To identify the minimum longitudinal steel level for ensuring the shear

failure of the HSRC beams.

4. To study the contribution of shear reinforcement in HSC beams for

various levels of longitudinal steel.

5. To compare the provisions of building Codes for shear design with the

observed values and their degree of safety.

6. To check the effectiveness of minimum shear reinforcement towards

increasing the shear capacity of the beams and avoiding the brittle

failure of HSRC beams.

7. To make further recommendations on the basis of observations for

future research in Pakistan in the shear design of HSC.

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6.1.2 Material used 6.1.2.1 Concrete.

The details of mix design of concrete and average 28 days compressive strength

obtained are given in Table. 6.1

Table 6.1 Mix Proportioning/ Designing of High Strength Concrete.

Constituent Mix proportioning Type- I Cement 628 kg/m3

Fine aggregates 484 kg/m3

Coarse aggregates 1128 kg/m3

HRWR @ by weight of cement 10.70 kg/m3

Water @ 0.25 w/c ratio 157 kg/m3

Average Cylinder Compressive strength ( 28 days) fc′

52.0 MPa

6.1.2.2 Reinforcing Steel

Deformed steel bars of specified 60,000 psi (414 MPa) yield stress were used. The

sizes of bars used are English sizes #3, #4, #6 and #7 and corresponding metric

sizes as #10, #13, #19 and #22 respectively. The bars were selected from the same

batch of re-bars.

For web reinforcement plain bars of size #2 ( 2/8 in), equal to 6mm sizes of specified

yield strength of 40,000 psi( 275MPa) were provided at 15cm c/c ( 6 in c/c).

Various parameters of the steel bars are given in Table 6.2

Table 6.2 Details of reinforcing bars used in the beams.

Nominal size Nominal Areas Average

Yield strength

Average

Ultimate strength

% elongation

US Metric in2 mm2 psi MPa psi MPa

#2 #6 0.05 32 45240 312 60121 414.62 13.21

#3 #10 0.11 71 66752 460 106653 735.54 12.50

#4 #13 0.20 129 67648 466 106483 734.37 15.63

#6 #19 0.44 284 67025 462 106836 736.80 14.06

#7 #22 0.60 387 64340 444 100678 694.33 15.23

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6.1.3 Details of test specimens

In total 70 beams of size 23 cm x 30 cm were cast, out of which 35 beams were cast

without web reinforcement called as series-I beams and designated as B1,B2,B3,B4

and B5. 35 beams in series-II, were cast with web reinforcement and designated as

Bs1,Bs2,Bs3,Bs4 and Bs5. The shear reinforcement in series-II, was used as per

minimum web reinforcement required under ACI-318.

As the longitudinal steel was one of the basic variable of study, therefore five values

of ρ=0.33%, 0.75%, 1%, 1.5% and 2% were used. The second variable of the study

was shear to span ratio a/d. Hence for each values of ρ, seven values of a/d were

used as a/d=3,3.5,4,4.5,5,5.5 and 6. The third variable of study was web

reinforcement. Min web reinforcement was used in 35 beams of series-II, while

keeping the values of ρ and a/d same as used in 35 beams of series-I.

The details of test specimen and steel bars used as longitudinal and transverse

reinforcement are given in Figure 6.1and Table 6.3.

6.1 (a) Without web reinforcement.

6.1(b) With web reinforcement

Figure 6.1 Details of beams used in the testing.

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Table 6.3 Reinforcement details of beams

7 (SI units of bar # given in Metric sizes and corresponding US sizes given in parenthesis) ρ=As/bd, Where As= Area of steel bars in the cross section of the beam, b is width of the beam=23 cm, d is effective depth of the beam =30 cm.

As the effective depth of the test specimen was constant, therefore the span of the

beams were selected such that the shear span to depth ratio of the beams to be

tested for each set of longitudinal steel ratio becomes a/d =3,3.5,4,4.5,5,5.5,6

(seven values). The details of span of the beams are given in Table 6.4

Table 6.4 shear span to depth ratio and corresponding span of seven beams in each set of

longitudinal reinforcement.

a/d 3.0 3.5 4.0 4.5 5.0 5.5 6.0

clear span of

beams ( cm) 150 178 203 229 254 280 305

The final details of 70 beams , 35 each in series-I and 35 in series-II are given in

Table 6.5 and Table 6.6 respectively.

Beams without stirrups Beams with stirrups

Bea

m T

itle

Steel

Bea

m T

itle

Tension steel Comp Steel

Transverse steel Tension

Bars ρ% Bars ρ(%) Bars ρ (%)

Stirrups ρv (%)

B1 1#10+1#13 (1#3+1#4)

0.33 Bs1

1#10+1#13 (1#3+1#4)

0.33

2#10 (2#3)

0.25 #6@15 cm (#2@6in)

0.16

B2 2#10+2#13 (2#3+2#4)

0.73 Bs2

2#10+2#13 (2#3+2#34)

0.73

2#10 (2#3)

0.25 #6@15 cm (#2@6in)

0.16

B3

2#19 (2#6)

1.00 Bs3

2#19 (2#6)

1.00 2#10 (2#3) 0.25 #6@15 cm

(#2@6in) 0.16

B4

3#19 (3#6)

1.50

Bs4

3#19 (3#6)

1.50 2#10 (2#3)

0.25 #6@15 cm (#2@6in)

0.16

B5

2#22 (2#7)

2.00

Bs5

2#22 (2#7)

2.00

2#10 (2#3)

0.25 #6@15 cm (#2@6in)

0.16

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Table6.5 Details of Series-I beams without web

reinforcement ( 35 Nos)

am

Title

b

cm

h

cm

Steel

ratio

ρ

Span

cm

a/d

B1-1 23 30 0.0033 152.40

3.0

B1-2 23 30 0.0033 177.80

3.5

B1-3 23 30 0.0033 203.20

4.0

B1-4 23 30 0.0033 228.60

4.5

B1-5 23 30 0.0033 254.00

5.0

B1-6 23 30 0.0033 279.40

5.5

B1-7 23 30 0.0033 304.80

6.0

B2-1 23 30 0.0073 152.40

3.0

B2-2 23 30 0.0073 177.80

3.5

B2-3 23 30 0.0073 203.20

4.0

B2-4 23 30 0.0073 228.60

4.5

B2-5 23 30 0.0073 254.00

5.0

B2-6 23 30 0.0073 279.40

5.5

B2-7 23 30 0.0073 304.80

6.0

B3-1 23 30 0.010 152.40

3.0

B3-2 23 30 0.010 177.80

3.5

B3-3 23 30 0.010 203.20

4.0

B3-4 23 30 0.010 228.60

4.5

B3-5 23 30 0.010 254.00

5.0

B3-6 23 30 0.010 279.40

5.5

B3-7 23 30 0.010 304.80

6.0

B4-1 23 30 0.015 152.40

3.0

B4-2 23 30 0.015 177.80

3.5

B4-3 23 30 0.015 203.20

4.0

B4-4 23 30 0.015 228.60

4.5

B4-5 23 30 0.015 254.00

5.0

B4-6 23 30 0.015 279.40

5.5

B4-7 23 30 0.015 304.80

6.0

B5-1 23 30 0.020 152.40

3.0

B5-2 23 30 0.020 177.80

3.5

B5-3 23 30 0.020 203.20

4.0

B5-4 23 30 0.020 228.60

4.5

B5-5 23 30 0.020 254.00

5.0

B5-6 23 30 0.020 279.40

5.5

B5-7 23 30 0.020 304.80 6.0

Table 6.6 Details of Series-II beams with web

reinforcement ( 35 Nos)

Beam

Title

b

cm

h

cm

Steel

ratio

ρ

Span

cm

a/d) Shear

steel

(ρv)

Bs1-1 23 30 0.0033 152.4

3.0 0.16 %

Bs1-2 23 30 0.0033 177.8

3.5 0.16 %

Bs1-3 23 30 0.0033 203.2

4.0 0.16 %

Bs1-4 23 30 0.0033 228.6

4.5 0.16 %

Bs1-5 23 30 0.0033 254.0

5.0 0.16 %

Bs1-6 23 30 0.0033 279.4

5.5 0.16 %

Bs1-7 23 30 0.0033 304.8

6.0 0.16 %

Bs2-1 23 30 0.0073 152.4

3.0 0.16 %

Bs2-2 23 30 0.0073 177.8

3.5 0.16 %

Bs2-3 23 30 0.0073 203.2

4.0 0.16 %

Bs2-4 23 30 0.0073 228.6

4.5 0.16 %

Bs2-5 23 30 0.0073 254.0

5.0 0.16 %

Bs2-6 23 30 0.0073 279.4

5.5 0.16 %

Bs2-7 23 30 0.0073 304.8

6.0 0.16 %

Bs3-1 23 30 0.010 152.4

3.0 0.16 %

Bs3-2 23 30 0.010 177.8

3.5 0.16 %

Bs3-3 23 30 0.010 203.2

4.0 0.16 %

Bs3-4 23 30 0.010 228.6

4.5 0.16 %

Bs3-5 23 30 0.010 254.0

5.0 0.16 %

Bs3-6 23 30 0.010 279.4

5.5 0.16 %

Bs3-7 23 30 0.010 304.8

6.0 0.16 %

Bs4-1 23 30 0.015 152.4

3.0 0.16 %

Bs4-2 23 30 0.015 177.8

3.5 0.16 %

Bs4-3 23 30 0.015 203.2

4.0 0.16 %

Bs4-4 23 30 0.015 228.6

4.5 0.16 %

Bs4-5 23 30 0.015 254.0

5.0 0.16 %

Bs4-6 23 30 0.015 279.4

5.5 0.16 %

Bs4-7 23 30 0.015 304.8

6.0 0.16 %

Bs5-1 23 30 0.020 152.4

3.0 0.16 %

Bs5-2 23 30 0.020 177.8

3.5 0.16 %

Bs5-3 23 30 0.020 203.2

4.0 0.16 %

Bs5-4 23 30 0.020 228.6

4.5 0.16 %

Bs5-5 23 30 0.020 254.0

5.0 0.16 %

Bs5-6 23 30 0.020 279.4

5.5 0.16 %

Bs5-7 23 30 0.020 304.8

6.0 0.16 %

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Proper curing of the beams was ensured with wet sand and the spaces around the

beams were filled with sand, which was kept continuously wet with clean water.

Curing was continued for 28 days. In Figure 6.2, all the 70 beams and wet sand

curing of these beams have been given.

Figure 6.2 Wet sand filled around the beams for curing.

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6.3 Test set up

6.3.1 Loading arrangement and supports conditions

For application of loads at the mid span of the beams, the loading frame fabricated

at the structural laboratory of Engineering University Taxila-Pakistan was used.

Loads were applied through the hydraulic system attached to proving ring and the

readings were taken accordingly. The ends of the beams were placed at roller

supports, so that the beams can behave like simply supported beams without lateral

constraint. The details of loading arrangements and supports are shown in Figure

6.3 and Figure 6.4 respectively.

Figure 6.3 Details of loading arrangement for the testing of RC beams.

Figure 6.3 Details of roller supports and deflection gauges used for the beams.

Clear Span

Proving Ring

Hydraulic Jack

Deflection Gauge

Shear Span=a=L/2

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6.3.2 Instrumentation for loading and deflection measurement For measurement of loads applied at the mid span of the beams, high tensile

proving ring was used and the loads were applied through the hydraulic system at

the mid span of the beams. The reading taken from the proving ring was converted

into equivalent “kN” from the conversion chart provided by the manufacturer of the

proving ring. Deflection gauges were provided at the mid span and critical sections

for shear at distance “d” from both supports.

6.3.3 Loading procedure

After locating the midpoint of the beams, the beams were placed under the

concentrated load of the hydraulic system and the loads were applied as shown in

Figure 6.2. Loads were applied at uniform rate of about 5kN per second, so that the

application of load is gradual and monotonic. The readings of the calibrated proving

rings were taken after every increment of 5kN, the beams were continuously

observed from both sides. The deflection of the gauges placed under the mid span

and critical sections for shear were taken for each 5kN increment of load. The cracks

appearing in the beams were carefully observed and the corresponding load applied

was recorded at the point, where the crack initiated. The crack path and the

respective loading were also marked on both sides of every beam. The application

of loading was continued till the failure of the beams.

Proper curing of the beams was ensured with wet sand and the spaces around the

beams were filled with sand, which was kept continuously wet with clean water.

Curing was continued for 28 days. In Figure 6.4, all the 70 beams and wet sand

curing of these beams have been given.

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6.4 Experimental results

6.4.1 Failure loads of the beams

The failure load for beams without web reinforcement for various values of

longitudinal steel ratio and shear span to depth ratio a/d, has been shown in Table

6.7, which includes the self weight of the beams and external loads applied at the

point of failure of the beams. Similarly the values of failure load for 35 beams with

web reinforcement beams has been shown in Table 6.8

Table 6.7 Total applied failure load at the beams without web reinforcement.

Pu(tets); Total failure load

Beam Title

Revised

Beam Title

Steel ratio (ρ)

a/d Applied Failure

load (KN)

Self weight (KN)

Total applied load at failure

( KN) Pu(test)

B1

B0.33,3

0.33

3.0 68.08 2.40 70.48 B0.33.3.5 3.5 57.56 2.98 60.54 B0.33,4 4.0 47.02 3.20 50.22 B0.33,4.5 4.5 44.24 3.60 47.84 B0.33,5 5.0 38.12 4.00 42.12 B0.33,5.5 5.5 33.36 4.40 37.76 B0.33,6 6.0 27.28 4.80 32.08

B2

B0.73,3

0.73

3.0 120.48 2.40 122.88 B0.73.3.5 3.5 110.46 2.98 113.44 B0.73,4 4.0 100.28 3.20 103.48 B0.73,4.5 4.5 89.96 3.60 93.56 B0.73,5 5.0 80.02 4.00 84.02 B0.33,5.5 5.5 69.54 4.40 73.94 B0.73,6 6.0 48.68 4.80 53.48

B3

B1,3

1.0

3.0 155.64 2.40 158.04 B1,3.5 3.5 132.94 2.98 135.92 B1,4 4.0 117.52 3.20 120.72 B1,4.5 4.5 111.12 3.60 114.72 B1,5 5.0 97.38 4.00 101.38 B1,5.5 5.5 95.12 4.40 99.52 B1,6 6.0 72.12 4.80 76.92

B4

B1.5,3

1.50

3.0 228.98 2.40 231.38 B1.5.3.5 3.5 203.64 2.98 206.62 B1.5,4 4.0 175.96 3.20 179.16 B1.5,4.5 4.5 155.56 3.60 159.16 B1.5,5 5.0 135.06 4.00 139.06 B1.5,5.5 5.5 120.64 4.40 125.04 B1.5,6 6.0 105.46 4.80 110.26

B5

B2,3

2.0

3.0 292.98 2.40 295.38 B2,.3.5 3.5 244.98 2.98 247.96 B2,4 4.0 200.02 3.20 203.22 B2,4.5 4.5 187.9 3.60 191.5 B2,5 5.0 167.36 4.00 171.36 B2,5.5 5.5 149.22 4.40 138.26 B2,6 6.0 134.48 4.80 125.35

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Table 6.8 Total applied failure load at the beams with web reinforcement

Revised Beam notation is shows with two subscripts. The first one showing the longitudinal steel ratio in % ( As/bd x100) and the second one shows the a/d ratio. For example B0.33,3, shows beam B-1 with longitudinal steel ratio of 0.33% and a/d ratio as 3.

Beam Title

Revised Beam Title

Steel ratio (ρ)

a/d Applied Failure load (KN)

Self weight (KN)

Total applied load at failure ( KN)

Pu(test)

Bs1

Bs0.33,3

0.33

3.0 77.96 2.40 80.36

Bs0.33.3.5 3.5 71 2.98 73.98

B0.33,4 4.0 60.6 3.20 63.8

B0.33,4.5 4.5 65.24 3.60 68.84

Bs0.33,5 5.0 59.16 4.00 63.16

Bs0.33,5.5 5.5 44.54 4.40 48.94

Bs0.33,6 6.0 38.78 4.80 43.58

Bs2

Bs0.73,3

0.73

3.0 161.14 2.40 163.54

Bs0.73.3.5 3.5 152.42 2.98 155.4

Bs0.73,4 4.0 131.34 3.20 134.54

Bs0.73,4.5 4.5 121.6 3.60 125.2

Bs0.73,5 5.0 111.36 4.00 115.36

Bs0.33,5.5 5.5 101.62 4.40 106.02

Bs0.73,6 6.0 91.42 4.80 96.22

Bs3

Bs1,3

1.0

3.0 188.98 2.40 191.38

Bs1,3.5 3.5 166.64 2.98 169.62

Bs1,4 4.0 154.08 3.20 157.28

Bs1,4.5 4.5 151.46 3.60 155.06

Bs1,5 5.0 141.84 4.00 145.84

Bs1,5.5 5.5 125.12 4.40 129.52

Bs1,6 6.0 101.02 4.80 105.82

Bs4

Bs1.5,3

1.50

3.0 247.96 2.40 250.36

Bs1.5.3.5 3.5 229.22 2.98 232.2

Bs1.5,4 4.0 188.64 3.20 191.84

Bs1.5,4.5 4.5 160.82 3.60 164.42

Bs1.5,5 5.0 139.68 4.00 143.68

Bs1.5,5.5 5.5 127.46 4.40 131.86

Bs1.5,6 6.0 112.72 4.80 117.52

Bs5

Bs2,3

2.0

3.0 318.68 2.40 321.08

Bs2,.3.5 3.5 267.64 2.98 270.62

Bs2,4 4.0 228.76 3.20 208.76

Bs2,4.5 4.5 221.72 3.60 202.79

Bs2,5 5.0 194.74 4.00 178.87

Bs2,5.5 5.5 77.96 2.40 80.36

Bs2,6 6.0 71 2.98 73.98

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6.4.2 Shear strength and failure angles of the beams.

The shear strength of beams is taken as half of the total load carried by the beams

at the failure point, as the beams are simply supported. The angles of diagonal

cracks causing failure of the beams were measured to the nearest 5 degrees. The

shear strength of beams and corresponding angles are shown in Table 6.9 and

Table 6.10 for both sets of beams.

Table 6.9 Shear Strength and failure angles of 35 HSC beams, without web reinforcement

Beam Title Revised Beam Title

Steel ratio (ρ)

a/d Shear taken by the beam at the failure

Vtest = Pu(test)/2 ( KN)

Approximate Failure angle.

(degrees)

B1

B0.33,3

0.33

3.0 35.24

60-70 B0.33.3.5 3.5 30.27 B0.33,4 4.0 25.11 B0.33,4.5 4.5 23.92 B0.33,5 5.0 21.06 B0.33,5.5 5.5 18.88

75-80 B0.33,6 6.0 16.04 B2

B0.73,3

0.73

3.0 61.44

55-65 B0.73.3.5 3.5 56.72 B0.73,4 4.0 51.74 B0.73,4.5 4.5 46.78 B0.73,5 5.0 42.01 B0.33,5.5 5.5 36.97

75-80 B0.73,6 6.0 26.74 B3

B1,3

1.0

3.0 79.02 40-55 B1,3.5 3.5 67.96

B1,4 4.0 60.36

45-65 B1,4.5 4.5 57.36 B1,5 5.0 50.69 B1,5.5 5.5 49.76 B1,6 6.0 38.46

B4

B1.5,3

1.50

3.0 115.69 35-50 B1.5.3.5 3.5 103.31

B1.5,4 4.0 89.58 B1.5,4.5 4.5 79.58

40-60 B1.5,5 5.0 69.53 B1.5,5.5 5.5 62.52 B1.5,6 6.0 55.13

B5

B2,3

2.0

3.0 147.69 30-50 B2,.3.5 3.5 123.98

B2,4 4.0 101.61 B2,4.5 4.5 95.75

35-60 B2,5 5.0 85.68 B2,5.5 5.5 76.81 B2,6 6.0 69.64

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Table 6.10 Shear Failure mode of 35 beams with web reinforcement

The angle of shear crack rounded to the nearest 5 degrees measure.

Beam Title Revised Beam

Title

Steel ratio (ρ)

a/d Shear taken by the beam at the

failure Vtest = Pu(test)/2

( KN)

App. Failure angle.

(degrees)

Bs1

Bs0.33,3

0.33

3.0 40.18

60-55 Bs0.33.3.5 3.5 36.99 B0.33,4 4.0 31.90 Bs0.33,4.5 4.5 34.42 B0.33,5 5.0 31.58 Bs0.33,5.5 5.5 24.47

70-80 Bs0.33,6 6.0 21.79 Bs2

Bs0.73,3

0.73

3.0 81.77

50-65 Bs0.73.3.5 3.5 77.70 B0.73,4 4.0 67.27 Bs0.73,4.5 4.5 62.60 Bs0.73,5 5.0 57.68 Bs0.33,5.5 5.5 53.01

70-80 Bs0.73,6 6.0 48.11 Bs3

Bs1,3

1.0

3.0 95.69 30-50 Bs1,3.5 3.5 84.81

Bs1,4 4.0 78.64

40-65 Bs1,4.5 4.5 77.53 Bs1,5 5.0 72.92 Bs1,5.5 5.5 64.76 Bs1,6 6.0 52.91

Bs4

Bs1.5,3

1.50

3.0 125.18 30-45 Bs1.5.3.5 3.5 116.10

Bs1.5,4 4.0 95.92 B1.5,4.5 4.5 82.21

35-60 Bs1.5,5 5.0 71.84 Bs1.5,5.5 5.5 65.93 Bs1.5,6 6.0 58.76

Bs5

Bs2,3

2.0

3.0 160.54 30-50 Bs2,.3.5 3.5 135.31

Bs2,4 4.0 115.98 Bs2,4.5 4.5 112.66

30-50 Bs2,5 5.0 99.37 Bs2,5.5 5.5 95.03 Bs2,6 6.0 77.77

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6.5 Discussion of results

6.5.1 Cracking pattern and failure modes of beams.

The cracking pattern and failure mode of the beams was closely observed. When

loads were applied to beams without web reinforcement vertical cracks appeared in

the mid span region. Initially the cracks were of small width and concentrated in the

mid span region with angles being more or less vertical. However with further

increase of load, the depth and width of cracks increased. The angles of cracks

became shallower and turned diagonal. The change in the angle of cracks can be

attributed to the cantilever action of the cracked concrete restrained by the

longitudinal reinforcement in the tension zone. When load was further increased, the

depth of some of the diagonal cracks further enhanced and crossed into the

compression zone of the beams, which ultimately caused the failure of the beams as

the cracks extended further towards the point of application of loads. The typical

shear failure of beams has been shown in Figure 6.5. This kind of failure is also

called “diagonal tension” failure, which was observed in the beams having a/d of 3

and more.

For beams having a/d>5.0 the failure has been observed predominantly due to

flexural cracks, which are also called the shear flexure failure as shown in Figure

6.6. Here the flexural cracks are dominant in the middle third region and the angle of

failure is large. These represent the values of a/d, where the beams are about to

achieve the flexural strength before shear failure on the upper boundary of famous

“Kani’s shear valley”. The theoretical flexural values and shear strength of such

beams are falling very closer to each other in this region.

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(B0.33, 3, ρ = 0.33 %, a/d = 3.00 , span = 152 cm)

( B073, 3: ρ = 0.73 % , a/d = 3 span = 152 cm)

(B1.0, 3, ρ = 1 %, a/d = 3 span = 152 cm)

Figure 6.5 Failure of beams without web reinforcement due to diagonal tension shear failure mode of the beam.

(B0.33,5.5, ρ = 0.33 % , a/d = 5.5 span = 279.4 cm)

(B0.73, 5.5 ρ = 0.73 % , a/d = 5.5 span = 279.4 cm)

(B0.73,6.0 ρ = 0.73% , a/d = 6.0 span = 279.4 cm)

Figure 6.6 Flexural shear failure of beams without web reinforcement having a/d>5.

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The failure of beams without web reinforcement and longitudinal steel of 1% or more

has been observed due to shear failure as shown in Figure 6.7. However the pattern

of shear crack has been changed with the increase of longitudinal steel and a/d

ratio. At lower values of a/d (3, 3.5 and 4.0), the failure is more like a pure shear

crack, in the form of arch action compression failure. The cracks originate closer to

the supports and gradually extend towards the mid span at relatively shallower

angle, in the range of 40 to 50 degrees. When the crack further extends to the mid

span and a clearer shear crack observed starting from the region near the supports

and reaching at the mid span to crack the beam, across a well defined path. This

kind of failure is more typical for high strength concrete beams, particularly, where

the longitudinal steel is more. This brittle failure phenomenon of the HSC beam

must be surely a point of concern in the contemporary research.

In all the three illustrations of Figure 6.8, the failure has taken place along a well

defined shear crack, very abrupt in nature and the inclination not more than 50

degrees. The research was also focused on reducing the chances of brittle failure of

HSC beams without web reinforcement, by adding minimum web reinforcement as

per ACI-381 in these beams.

(B1.0, 5 , ρ = 1% , a/d = 5 span = 254 cm)

(B1.5, 5.5, ρ = 1% , a/d = 5.5 span = 280 cm)

(B2,6ρ = 2% , a/d = 6 span = 305 cm)

Figure 6.7 Typical shear failures of beams without web reinforcement. The failure is more brittle and sudden amongst all. The crack causing failure of the beam was not noticed in the beginning and beams failed very suddenly due to tension shear failure

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The failure angles of beams, corresponding shear strength and failure modes for 35

beams without web reinforcement is shown in Table 6.11.

Table 6.11 Shear Strength, failure angles and failure modes of 35 HSC beams, without web reinforcement

Beam Title

Revised

Beam Title

Steel ratio (ρ)

a/d

Shear taken by the beam at the failure

Vtest ( KN)

Failure mode Approximate Failure angle.

(degrees)

B1

B0.33,3

0.33

3.0 35.24 Beam failure/Diagonal tension failure

60-70 B0.33.3.5 3.5 30.27 Beam failure/ Diagonal tension failure B0.33,4 4.0 25.11 Beam failure/Diagonal tension failure B0.33,4.5 4.5 23.92 Beam failure/ Diagonal tension failure

B0.33,5 5.0 21.06 Beam failure/Diagonal tension failure

B0.33,5.5 5.5 18.88 Flexural shear failure dominant 75-80 B0.33,6 6.0 16.04 Flexural shear failure dominant

B2

B0.73,3

0.73

3.0 61.44 Beam failure/Diagonal tension failure

55-65 B0.73.3.5 3.5 56.72 Beam failure/ Diagonal tension failure

B0.73,4 4.0 51.74 Beam failure/Diagonal tension failure

B0.73,4.5 4.5 46.78 Beam failure/ Diagonal tension failure

B0.73,5 5.0 42.01 Beam failure/Diagonal tension failure

B0.33,5.5 5.5 36.97 Flexural shear failure dominant 75-80 B0.73,6 6.0 26.74 Flexural shear failure dominant

B3

B1,3

1.0

3.0 79.02 Arch failure/Compression shear failure 40-55 B1,3.5 3.5 67.96 Arch failure/Compression shear failure

B1,4 4.0 60.36 Beam failure/Diagonal tension failure

45-65 B1,4.5 4.5 57.36 Beam failure/ Diagonal tension failure

B1,5 5.0 50.69 Beam failure/Diagonal tension failure

B1,5.5 5.5 49.76 Beam failure/ Diagonal tension failure

B1,6 6.0 38.46 Beam failure/Diagonal tension failure

B4

B1.5,3

1.50

3.0 115.69 Arch failure/Compression shear failure 35-50 B1.5.3.5 3.5 103.31 Arch failure/Compression shear failure

B1.5,4 4.0 89.58 Arch failure/Compression shear failure

B1.5,4.5 4.5 79.58 Beam failure/Diagonal tension failure 40-60 B1.5,5 5.0 69.53 Beam failure/ Diagonal tension failure

B1.5,5.5 5.5 62.52 Beam failure/Diagonal tension failure

B1.5,6 6.0 55.13 Beam failure/ Diagonal tension failure

B5

B2,3

2.0

3.0 147.69 Arch failure/Compression shear failure 30-50 B2,.3.5 3.5 123.98 Arch failure/Compression shear failure

B2,4 4.0 101.61 Arch failure/Compression shear failure

B2,4.5 4.5 95.75 Beam failure/Diagonal tension failure 35-60 B2,5 5.0 85.68 Beam failure/ Diagonal tension failure

B2,5.5 5.5 76.81 Beam failure/Diagonal tension failure

B2,6 6.0 69.64 Beam failure/ Diagonal tension failure

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For beams with shear reinforcement, the cracking pattern has been considerably

affected by the addition of web reinforcement in HSC beams. The number of cracks

has been increased but their widths have been decreased. The failure angles have

also been reduced. The shear resisted by the beam with web reinforcement, their

failure modes and approximate failure angle for 35 beams with web reinforcement

are given in Table 6.12. The failure modes of some of the HSRC beams with web

reinforcement are shown in Figure 6.8

Table 6.12 Shear strength, failure mode and failure angles for 35 HSRC beams with web reinforcement.

Beam Title

Revised

Beam Title

Steel ratio (ρ)

a/d

Shear taken by the beam at the failure

Vtest ( KN)

Failure mode App. Failure angle.

(degrees)

Bs1

Bs0.33,3

0.33

3.0 40.18 shear Compression failure

60-55 Bs0.33.3.5 3.5 36.99 shear Compression failure B0.33,4 4.0 31.90 shear Compression failure Bs0.33,4.5 4.5 34.42 Beam failure/ Diagonal tension failure B0.33,5 5.0 31.58 Beam failure/ Diagonal tension failure Bs0.33,5.5 5.5 24.47 Beam failure/Diagonal tension failure

70-80 Bs0.33,6 6.0 21.79 Beam failure/ Diagonal tension failure Bs2

Bs0.73,3

0.73

3.0 81.77 shear Compression failure

50-65 Bs0.73.3.5 3.5 77.70 shear Compression failure B0.73,4 4.0 67.27 Beam failure/Diagonal tension failure Bs0.73,4.5 4.5 62.60 Beam failure/ Diagonal tension failure Bs0.73,5 5.0 57.68 Beam failure/Diagonal tension failure Bs0.33,5.5 5.5 53.01 Beam failure/Diagonal tension failure

70-80 Bs0.73,6 6.0 48.11 Beam failure/Diagonal tension failure Bs3

Bs1,3

1.0

3.0 95.69 Arch failure/Compression shear failure 30-50 Bs1,3.5 3.5 84.81 Arch failure/Compression shear failure

Bs1,4 4.0 78.64 Beam failure/Diagonal tension failure

40-65 Bs1,4.5 4.5 77.53 Beam failure/ Diagonal tension failure Bs1,5 5.0 72.92 Beam failure/Diagonal tension failure Bs1,5.5 5.5 64.76 Beam failure/ Diagonal tension failure Bs1,6 6.0 52.91 Beam failure/Diagonal tension failure

Bs4

Bs1.5,3

1.50

3.0 125.18 Arch failure/Compression shear failure 30-45 Bs1.5.3.5 3.5 116.10 Arch failure/Compression shear failure

Bs1.5,4 4.0 95.92 Arch failure/Compression shear failure B1.5,4.5 4.5 82.21 Beam failure/Diagonal tension failure

35-60 Bs1.5,5 5.0 71.84 Beam failure/ Diagonal tension failure Bs1.5,5.5 5.5 65.93 Beam failure/Diagonal tension failure Bs1.5,6 6.0 58.76 Beam failure/ Diagonal tension failure

Bs5

Bs2,3

2.0

3.0 160.54 Arch failure/Compression shear failure 30-50 Bs2,.3.5 3.5 135.31 Arch failure/Compression shear failure

Bs2,4 4.0 115.98 Arch failure/Compression shear failure Bs2,4.5 4.5 112.66 Beam failure/Diagonal tension failure

30-50 Bs2,5 5.0 99.37 Beam failure/ Diagonal tension failure Bs2,5.5 5.5 95.03 Beam failure/Diagonal tension failure Bs2,6 6.0 77.77 Beam failure/ Diagonal tension failure

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(Bs0.73, 3, ρ = 0.73 % , a/d = 3 span = 152 cm)

(Bs1, 3 , ρ = 1 % , a/d = 3 span = 152 cm)

Figure 6.8 Beam shear failure or diagonal tension shear failure in beams with web reinforcement.

6.5.2 Effect of longitudinal steel ratio on the shear strength of beams

When the longitudinal steel ratio has been increased, the shear strength of beams in

both sets has been increased. However this increase in more in case of beams with

web reinforcement. The increase in shear strength of beams with the increase of

longitudinal steel is also referred as “dowel action”.

For a constant a/d ratio, when the longitudinal reinforcement was increased, the

number of cracks, their widths and failure angle reduced as shown in Figure 6.6.

This verifies the concept of bond between concrete and longitudinal steel given in

“Kani tooth model”. Due to increase in the longitudinal steel, the bond force between

the cracked concrete at the cantilever end also increased, thereby applying more

action at the free end of cracks and reducing the failure angle. The phenomena is

well illustrated by Modified Compression Filed Theory ( MCFT) of Vecchio and

Collins (1986), where the steel provided on the tension face of beams plays a

significant role in restraining the cracks and improve the shear strength of beams.

The width of the shear crack and their spacing has been observed as an important

parameter for shear failure of HSC beams. The reduction in failure angle due to

increase in the longitudinal steel is given in Figure 6.9.

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( B1.5, 3 : ρ = 1.5 % , a/d = 3 span = 152 cm)

(B2.0, 3: ρ = 2 % , a/d = 3 span = 152 cm)

Figure 6.9 Failure of beams without web reinforcement due to diagonal tension shear failure mode of the beam. The failure angles have been reduced with the increase in longitudinal steel.

The increase in the shear strength due to increase in longitudinal steel is given in

Table 6.12 and Figures 6.9 and 6.10. The increase in shear strength with the

increase of longitudinal steel ratio in beams with web reinforcement is relatively

more due to better packing of the steel bars by the stirrups.

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Table 6.12 Effect of the longitudinal steel on the shear strength of beams for constant a/d values.

Beams without web steel Beams with web steel

ρ (%) a/d Beam Title Shear Strength (KN) Beam Title Shear Strength (KN) 0.33 3.0 B0.33,3 35.24 Bs0.33,3 40.18

0.733 3.0 B0.733,3 61.44 Bs0.733,3 81.77

1.0 3.0 B1.0,3 79.02 Bs1.0,3 95.69

1.5 3.0 B1.5,3 115.69 Bs1.5,3 125.18 2 3.0 B2 3 147.69 Bs2 3 160.54

0.33 3.5 B0.33,3.5 30.27 Bs0.33,3.5 36.99

0.733 3.5 B0.733,3.5 56.72 Bs0.733,3.5 77.70

1.0 3.5 B1.0,3.5 67.96 Bs1.0,3.5 84.81

1.5 3.5 B1.5,3.5 103.31 Bs1.5,3.5 116.1

2 3.5 B2,3.5 123.98 Bs2,3.5 135.31

0.33 4.0 B0.33,4 25.11 Bs0.33,4 31.90

0.733 4.0 B0.733,4 51.74 Bs0.733,4 67.27

1.0 4.0 B1.0,4 60.36 Bs1.0,4 78.64

1.5 4.0 B1.5,4 89.58 Bs1.5,4 95.92

2 4.0 B2,4 101.61 Bs2,4 115.98

0.33 4.5 B0.33,4.5 23.92 Bs0.33,4.5 34.42

0.733 4.5 B0.733,4.5 46.78 Bs0.733,4.5 62.60

1.0 4.5 B1.0,4.5 57.36 Bs1.0,4.5 77.53

1.5 4.5 B1.5,4.5 79.58 Bs1.5,4.5 82.21

2 4.5 B2,4.5 95.75 Bs2,4.5 112.66

0.33 5.0 B0.33,5 21.06 Bs0.33,5 31.58

0.733 5.0 B0.733,5 42.01 Bs0.733,5 57.68

1.0 5.0 B1.0,5 50.69 Bs1.0,5 72.92 1.5 5.0 B1.5,5 69.53 Bs1.5,5 71.84 2 5.0 B2,5 85.68 Bs2,5 99.37

0.33 5.5 B0.33,5.5 18.88 Bs0.33,5.5 24.47

0.733 5.5 B0.733,5.5 36.97 Bs0.733,5.5 53.01

1.0 5.5 B1.0,5.5 49.76 Bs1.0,5.5 64.67 1.5 5.5 B1.5,5.5 62.52 Bs1.5,5.5 65.93

2 5.5 B2,5.5 76.81 Bs2,5.5 95.03

0.33 6.0 B0.33,6 16.04 Bs0.33,6 21.79 0.733 6.0 B0.733,6 26.74 Bs0.733,6 48.11

1.0 6.0 B1.0,6 38.46 Bs1.0,6 52.91

1.5 6.0 B1.5,6 55.13 Bs1.5,6 58.76 2 6.0 B2,6 69.64 Bs2,6 77.70

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a/d=5.0

a/d=4.0

a/d=3.0

a/d=3.5

a/d=3

a/d=5.5

a/d=6

a/d=4.5

0

20

40

60

80

100

120

140

160

0.33% 0.73% 1% 1.50% 2%

She

ar s

tren

gth

of

bea

m (

KN

)

Longitudinal steel ( %)

Effect of longitudinal steel on the shear strength of HSC beams without stirrups

a/d=3

a/d=3.5

a/d=4

a/d=4.5

a/d=5

a/d=5.5

a/d=6

Figure 6.9 Effect of longitudinal Steel ratio on the shear strength of concrete beams without stirrups for same value of a/d.

a/d=5.0

a/d=4.0

a/d=3.0

a/d=3.5

a/d=3

a/d=5.5 a/d=6

a/d=4.5

0

20

40

60

80

100

120

140

160

180

0.33% 0.73% 1% 1.50% 2%

Sh

ear str

en

gth

of b

eam

( K

N)

Longitudinal steel ( %)

Effect of longitudinal steel on the shear strength of HSC beams with web reinforcement.

a/d=3

a/d=3.5

a/d=4

a/d=4.5

a/d=5

a/d=5.5

a/d=6

Figure 6.10 Effect of longitudinal Steel ratio on the shear strength of concrete beams with web reinforcement for same value of a/d.

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6.5.3 Effect of shear span to depth (a/d) ratio on the shear strength of beams

The shear span to depth a/d ratio has a strong influence on the shear strength of

HSRC beams like NSRC beams. The shear strength decreases with the increase of

a/d values for the same longitudinal steel. However the decrease is relatively more

in case of HSRC beams without web reinforcement. The increase in shear span

increases the number of cracks formed and as result more cantilever force applied

at the cracked concrete, reducing the shear strength of concrete to greater extent.

The effect of a/d values on the shear strength of HSRC beams has been shown in

Figures 6.11 and 6.12.

The increase in shear span for a constant section of beam leads to increase in the

shear span to depth ratio. When the shear span increases, the deflection under

external loads also increases and flexural cracks are formed at relatively lower

values of external loads. The crack widths also increases which leads to reduction in

interface shear transfer and larger cracks are formed. These cracks also reduce the

depth of compression zone responsible for resisting the tensile stresses in the un-

cracked part of concrete web. The phenomena can also be explained in terms of the

cracked concrete, when the depth of the concrete cracks increases due to more

deflection of the beams, the lever arm of the cracked concrete cantilever also

increases, leading to more diagonal force on the un cracked part of the concrete

web, forcing it to fail at relatively lower value of applied load. Hence the “Tooth

model of Kani” and “ Failure of Compression zone” of Kosovo can explain this

phenomena.

The effect of a/d on the shear strength is prominent at lower values of longitudinal

steel, where the tendency of flexural cracking is more, due to early bond failure at

one hand and large deflection of beams at other hand. Thus larger tensile strain due

to small longitudinal steel can lead to reduced shear capacity of the RC beams

without web reinforcement.

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In the corresponding beams with web reinforcement, the reduction in shear strength

due to increase in the a/d ratio is relatively less, as the diagonal shear cracks are

intercepted by the stirrups in the compression zone. Thus the effect of a/d ratio on

reduction of the shear strength of beams is more pronounced in the HSC beams

without web reinforcement.

2%

1.5%

1%

0.73%

0.33%

0

20

40

60

80

100

120

140

160

a/d=3 a/d=3.5 a/d=4 a/d=4.5 a/d=5 a/d=5.5 a/d=6

Sh

ear s

tren

gth

of b

eam

( K

N)

Shear span to depth ratio ( a/d)

Ef fect of shear span to depth ration on the shear strength of HSC beams without web reinforcement

0.33%

0.73%

1%

1.50%

2%

Figure 6.11 Effect of shear span to depth ratio on the shear strength of concrete beams

without stirrups for same value of longitudinal steel ratio.

0.33%

0.73%

1%

1.5%

2%

0

20

40

60

80

100

120

140

160

180

a/d=3 a/d=3.5 a/d=4 a/d=4.5 a/d=5 a/d=5.5 a/d=6

She

ar s

tren

gth

of b

eam

( K

N)

Shear span to depth ratio ( a/d)

Effect of shear span to depth ration on the shear strength of HSC beams with web reinforcement 0.33%

0.73%

1%

1.50%

2%

Figure 6.12 Effect of shear span to depth ratio on the shear strength of concrete beams

without stirrups for same value of longitudinal steel ratio.

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6.5.4 Effect of web reinforcement on shear strength of HSC beams.

The use of web reinforcement has increased the shear strength of all beams of, as

shown in Table 6.14.

Table 6.14 Increase in the shear of HSC beams strength due to addition of web steel.

Beams without web reinforcement Beams with web reinforcement Increase in the shear strength of beams. (kN)

% increase in the shear with stirrups

Beam tiles

Steel ratio (ρ)

a/d

Shear at critical section

(kN)

Beams with web reinforcement

Shear at critical section

(kN)

B1

B0.33,3 0.33

3.0 35.24

Bs1

Bs0.33,3 40.18 4.94 14 B0.33.3.5 3.5 30.27 Bs0.33.3.5 36.99 6.72 22 B0.33,4 4.0 25.11 B0.33,4 31.90 6.79 27 B0.33,4.5 4.5 23.92 Bs0.33,4.5 34.42 10.50 44

B0.33,5 5.0 21.06 B0.33,5 31.58 10.52 50

B0.33,5.5 5.5 18.88 Bs0.33,5.5 24.47 5.59 30

B0.33,6 6.0 16.04 Bs0.33,6 21.79 5.75 36

Average 7.30 31 B2

B0.73,3

0.73

3.0 61.44

Bs2

Bs0.73,3 81.77 20.33 33

B0.73.3.5 3.5 56.72 Bs0.73.3.5 77.70 20.98 37

B0.73,4 4.0 51.74 B0.73,4 67.27 15.53 30

B0.73,4.5 4.5 46.78 Bs0.73,4.5 62.60 15.82 34

B0.73,5 5.0 42.01 Bs0.73,5 57.68 15.67 37

B0.33,5.5 5.5 36.97 Bs0.33,5.5 53.01 16.04 43

B0.73,6 6.0 26.74 Bs0.73,6 48.11 21.37 80

Average 17.96 42 B3

B1,3

1.0

3.0 79.02

Bs3

Bs1,3 95.69 16.67 21

B1,3.5 3.5 67.96 Bs1,3.5 84.81 16.85 25

B1,4 4.0 60.36 Bs1,4 78.64 18.28 30

B1,4.5 4.5 57.36 Bs1,4.5 77.53 20.17 35

B1,5 5.0 50.69 Bs1,5 72.92 22.23 44

B1,5.5 5.5 49.76 Bs1,5.5 64.76 15.00 30

B1,6 6.0 38.46 Bs1,6 52.91 14.45 38

Average 17.66 32 B4

B1.5,3

1.50

3.0 115.69

Bs4

Bs1.5,3 125.18 9.49 8

B1.5.3.5 3.5 103.31 Bs1.5.3.5 116.10 12.79 12

B1.5,4 4.0 89.58 Bs1.5,4 95.92 6.34 7

B1.5,4.5 4.5 79.58 B1.5,4.5 82.21 2.63 3

B1.5,5 5.0 69.53 Bs1.5,5 71.84 2.31 3

B1.5,5.5 5.5 62.52 Bs1.5,5.5 65.93 3.41 5

B1.5,6 6.0 55.13 Bs1.5,6 58.76 3.63 7

Average 5.80 6 B5

B2,3

2.0

3.0 147.69

Bs5

Bs2,3 160.54 12.85 9

B2,.3.5 3.5 123.98 Bs2,.3.5 135.31 11.33 9

B2,4 4.0 101.61 Bs2,4 115.98 14.37 14

B2,4.5 4.5 95.75 Bs2,4.5 112.66 16.91 18

B2,5 5.0 85.68 Bs2,5 99.37 13.69 16

B2,5.5 5.5 76.81 Bs2,5.5 95.03 18.22 24

B2,6 6.0 69.64 Bs2,6 77.77 8.13 12

Average 13.64 15

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The addition of web steel has increased the failure loads of the beams, thereby

reducing the gap between the flexural moment ( Mf ) and ultimate cracking moment

(Mu) on the famous “Kani’s valley of shear failure”. The Kani’s explanation to

increase in the shear strength with stirrups has already been given in the relevant

section. One of the arguments put forward by Kani (1967), for this increase is due to

providing supports to the part of compression arches, which are otherwise

unsupported and transfer their reactions to the supports, thereby avoiding their

failure at lower loads. This explanation is no doubt in contrast to the famous “Parallel

chord truss model of Ritter (1899)”, where the role of stirrups was assumed to lift the

load to the compression zone. The later argument seems more relevant to explain

the increase in shear strength with stirrups. The same rationale was also supported

by Kotsovos (1984) in his later work.

The increase in the shear strength is however not uniform for same values of web

reinforcement. This has supported some of the research by Shehata et al (2000),

where the shear strength provided by the addition of shear reinforcement has been

described as a complex phenomena and merely addition of the equivalent shear

strength of stirrups with the concrete shear strength would not predict the total shear

strength of RC beams. The results also support the fact that the role of web

reinforcement in increasing the shear strength of beams is still not fully understood

and there are contrasting explanations as given by Kani and Kotsovos to this

phenomenon.

The existing building and bridges Codes in most of the cases use a uniform value of

shear for certain level of web reinforcement, which is often taken as independent of

the compressive strength of concrete, longitudinal steel ratio and shear span to

depth ratio a/d. The test results have not supported this basic consideration of the

codes, as the increase in shear strength is random for uniform value of web

reinforcements. This observation deserves further research.

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The average increase in the shear strength of HSC beams with addition of web steel

is relatively more at low level of longitudinal steel ratio. In beams without web

reinforcement and lower values of longitudinal steel, flexural cracks are developed at

early stage and the depth of cracks and concrete teeth increase with further increase

of loads. The resultant cantilever action also increases and the diagonal cracking

due diagonal tension failure of beams happens. However, when the stirrups are

added to such beams, the propagation of cracks is avoided at lower values of loads

due to resistance of web steel in the compression zone, thereby increasing the

resistance to the diagonal cracking, leading to increase in the shear strength of HSC

beams.

At higher values of longitudinal steel, the diagonal cracks are formed at relatively

higher values of loads and hence the role of stirrups comes into play at later stage at

higher loads, which leads to yielding of web reinforcement with less increase in the

applied load. Thus when the longitudinal steel is increased, a decrease in the

contribution of web steel to resist the diagonal failure can be expected. This further

supports the earlier argument that the role of web reinforcement towards increase in

shear strength of HSC beams cannot be thought as independent of the longitudinal

steel.

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6.5.5 Load deflection curves for beams:

The load deflection curves of the beams have been developed by observing to study

the general behaviour of HSRC beams. Some of the load deflection curves has been

given in Figure 6.14 and Figure 6.15.

0

20

40

60

80

100

120

140

160

0 1 2 3 4 5 6

She

ar s

tren

gth

of b

eam

( K

N)

mid span defeltion ( mm)

load defelction curve for beam (B0.73,3)

020406080

100120140160

0 0.5 1 1.5 2 2.5 3 3.5

She

ar s

tren

gth

of b

eam

(

KN

)

mid span defeltion ( mm)

load defelction curve for beam (B0.73,5)

020406080

100120140160

0 0.5 1 1.5 2 2.5She

ar s

tren

gth

of b

eam

(

KN

)

mid span defeltion ( mm)

load defelction curve for beam (B0.73,6)

Figure 6.14 load deflection curves for beams without web reinforcement and ρ=0.0073

Load ( kN) Deflection (mm)

10 0.2

20 0.3

25 0.71

35 1.0

45 1.21

55 1.55

65 2.02

75 2.39

85 2.88

90 3.3 100 3.8

110 4.28

Load ( kN) Deflection (mm)

10 0.32

20 0.42

25 0.98

35 1.65

45 1.89

55 2.12

Load ( kN) Deflection (mm)

10 0.28

20 0.39

25 0.85

35 1.35

45 1.48

55 1.75

65 2.35

75 2.90

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0

20

40

60

80

100

120

140

160

0 0.5 1 1.5 2 2.5 3

She

ar s

tren

gth

of b

eam

( K

N)

mid span defeltion ( mm)

load defelction curve for beam (B2.0,,3)

020406080

100120140160

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

She

ar s

tren

gth

of

beam

( K

N)

mid span defeltion ( mm)

load defelction curve for beam (B2.0,5)

Figure 6.15 load deflection curves for beams without web reinforcement and ρ=0.02

Load ( kN) Deflection (mm) 20 0.10 40 0.16 60 0.25 80 0.46 100 0.66 120 0.75 140 1.01 160 1.15 180 1.26 200 1.80 220 2.03 240 2.50 260 2.80

Load ( kN) Deflection (mm)

10 0.05 20 0.20 35 0.25 55 0.35 75 0.60 100 0.89 120 1.09 140 1.25 150 1.45

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Chapter No.7

Experimental programme and discussion of

results of two way HSC corbels.

Chapter Introduction: This chapter is based on the experimental program of research on the D-region based on Strut and Tie Model (STM). Two way corbels were designed on the basis of Strut and Tie Model against assumed external loads. Later 9 two way corbels were experimentally investigated. The results were then compared with the theoretical values of the shear strength.

7.1 Experimental Programme for testing of disturbed region in concrete ( D-

region)

To study the shear strength of the disturbed region (D-region) in concrete

structures, the Strut and Tie Model (STM) was selected for the design, which was

applied to high strength concrete two way corbels.

The objectives of the testing of two way corbels as D-region are as follows;

- To study the behaviour of two way corbels in shear.

- Modeling of corbels with Strut and Tie Model (STM), under assumed service

load.

- Checking the shear strength of these corbels and comparing the actual and

theoretical values.

- To check the reasonability of the STM for the selected structures.

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7.1.1 Geometry of the corbels

The assumed geometry of the proposed two way cobles is given in Figure 7.1

Figure 7.1 Geometry of the proposed two way corbel and proposed STM.

The details of form work used for the test specimen is given in Figure 7.2

Figure 7.2 Reinforcement Form work used for the two way corbels.

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7.1.2 Materials used

The details of mixed design for HSC used for two way corbels is given in Table

7.1

Table 7.1 Mix Proportioning/ Designing of High Strength Concrete Double Corbels

Title Nominal mix

ratio

Cement:sand:Aggt

Cme

( kg)

Sand

( kg)

Agg

( Kg)

w/c

ratio

HRWR

(lit/100kg

of cement

Slump

(cm )

Gauge

position

Comp

strength

(MPa)

DCB-1 1: ½: 1 100 500 100 0.25 1.10 Collapse Strut 60

DCB-2 1: ½: 1 100 500 100 0.29 0.70 5 Tie 58

DCB-3 1: ½: 1 100 500 100 0.29 0.70 5 - 60

DCB-4 1: 1: 1½ 100 100 150 0.25 0.60 6 - 50

DCB-5 1: 1: 1 ½ 100 100 150 0.32 0.60 6 Tie 48DCB-6 1: 1: 1½ 100 100 150 0.28 0.60 5 - 51

DCB-7 1: 1½:2 ½ 100 150 250 0.30 0.350 6 - 43

DCB-8 1: 1½:2 ½ 100 150 250 0.35 0.300 5 - 46

DCB-9 1: 1½:2 ½ 100 150 250 0.40 0.250 5 Strut 45

For steel reinforcement deformed steel bars of specified yield strength of 60,000

psi (414MPa) was used.

7.1.3 Loading arrangement

Load was applied to the overhanging parts on both end of the corbel at 4.5 in

from the face of support. The conceptual diagram for load arrangement is given

in Figure 7.3. Loads were applied through the hydraulic system placed on high

tensile steel rail at the centre of the corbel. The steel rail rested on two rollers

placed at the point of application of loads at the corbel ends, attached to the

proving ring, which gives reading for the equivalent applied load in kN. The total

load applied through the hydraulic system was read from proving ring. The high

tensile steel section further transmits the total applied load in two equal parts at

the ends of corbels.

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Figure 7.3 Loading arrangement for HSC two way corbels

7.1.4 Embedment Strain Gauge.

To measure the strain in concrete or steel inside the concrete, embedment strain

gauges are used. In two way corbels, embedment strain gauges were used.

Further details about the installation etc of the gauges are given as follows;

Installation of embedment strain gauge in reinforced beam

In reinforced or pre-stressed concrete applications, the embedment strain gauge

is usually tied to the reinforcing cage. In mass concrete applications, the gauge

may be installed either before or immediately after replacement of the concrete.

Gauges may be configured in a rosette either by direct placement in the soft

concrete or by attachment to a rosette adapter. The details of embedment gauge

have been shown in Figure

7.4. In our case the embedment strain gauge was tied to the steel along the

direction of struts and ties.

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Figure 7.4 Details of embedment strain gauge.

7.1.5 Strain Data Logger

Three terminals coming out of the embedment stain gauge were attached to

strain data logger as shown Figure 7.5, and strain was recorded for various

levels of applied loads.

Support Bars

Cable Ties

Data Cable

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Figure 7.5 Strain Data Logging system used.

7.2 Design of the two way corbel by Strut and Tie Model ( STM)

Strut and Tie Model was used for the design of two way corbels. The detailed

design steps adopted for the corbels are given in Appendix-A. The final member

forces under assumed external loads on each end, for the assumed STM have

are given in Figure 7.6.

A A '

B

C

B '

C '

V u = 8 0 k ip s V u = 8 0 k ip s

85.3

8 ki

ps

85.3

8 ki

ps

80 k

ips

2 9 . 8 4 k ip s

80 k

ips

8 0 k ip s8 0 k ip s

2 9 . 8 4 k ip s

Figure 7.6 Member Force in strut and Tie model for two way corbel.

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Nine HSC corbels were cast in three sets and the details of assumed external

loads, concrete compressive strength, member forces, reinforcement and other

relevant details are given in Table 7.2.

Table 7.2 Details of technical parameters and member forces in assumed STM

Corbel CB-1 to CB-3 CB-4 to CB-6 CB-7 to CB-9

Technical Parameters

fc′ (ksi)

8.5 (59MPa)

7.50 ( 52Mpa)

6.5 ( 45 MPa)

As provided (in2) ( SI units)

3#4 ( 0.60) (3#10)

3#4+1#3 ( 0.71)

( 3#10+1#13)

4#4 ( 0.81) ( 4#13)

Theoretical Shear capacity (kips)

60 ( 269 kN)

70 ( 311kN)

80 ( 356kN)

Truss Forces & Geometry

Strut (kips) 65.84 ( 292kN)

76.84 ( 342kN)

87.84 ( 390kN)

Tie (kips) 27.11 ( 120kN)

31.70 ( 141kN)

36.28 ( 161kN)

Strut AA width (in) 2.05 ( 5.2cm)

2.32 (5.89cm)

2.68 ( 6.8cm)

Strut A width (in) 1.80 ( 4.57cm)

1.79 ( 4.5cm)

1.77 ( 4.49cm)

The actual reinforcement of the corbels is given in Figure 7.6

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Figure 7.7 Details of reinforcement, formwork and embedment gauges.

7.3 Test results and discussion of two way corbel testing: The results are given in Table 7.3. Table 7.3 Comparison of theoretical and actual failure loads of HSC double corbels

Corbel CB-1 to CB-3 CB-4 to CB-6 CB-7 to CB-9

Technical Parameters fc′

(ksi) 8.5

(59MPa) 7.50

( 52Mpa) 6.5

( 45 MPa) As provided (in2)

( SI units) 3#4

( 0.60) (3#10)

3#4+1#3 ( 0.71)

( 3#10+1#13)

4#4 ( 0.81) ( 4#13)

Theoretical Shear capacity (kips)

60 ( 269 kN)

70 ( 311kN)

80 ( 356kN)

Truss Forces & Geometry

Strut (kips) 65.84 ( 292kN)

76.84 ( 342kN)

87.84 ( 390kN)

Tie (kips) 27.11 ( 120kN)

31.70 ( 141kN)

36.28 ( 161kN)

Strut AA width (in) 2.05 ( 5.2cm)

2.32 (5.89cm)

2.68 ( 6.8cm)

Strut A width (in) 1.80 ( 4.57cm)

1.79 ( 4.5cm)

1.77 ( 4.49cm)

Strut Angle Theoretical 67.55 67.58 67.62

Actual 67 66.97 72.75 Failure Shear Loads

Theoretical (kN) 60 ( 269 kN)

70 ( 311kN)

80 ( 356kN)

Actual 63 68 72

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( 280kN) ( 302kN) ( 320kN) % variation 5% 3% 10%

Strain in tie ( 10-6 , µs) 209 285 300

The HSC two way corbels were tested under two point loads applied at the

centre line of bearing plats at both ends. The loads were gradually increased at

5kN/sec and the cracks developed in the corbels were closely observed. The

cracks start from the edge of the plates and gradually extended down towards

the connection of corbel and column, showing a typical shear cracks. With further

increase of applied load, the crack surface widened and became more

prominent, ultimately caused failure of the corbel. The corbels have been failed

mainly due to failure of compression struts as shown in Figure 7.8. The

inclination of the struts, causing the failure of the corbels was measured, which

are falling in the range of 670 to 720, against the theoretical values of 670. The

failure is more brittle and sudden. The theoretical shear capacity of the corbels

for given reinforcement, material stresses and truss geometry was compared

with the actual values in Table 7.3.

The theoretical and observed values of the shear capacity are relatively closer for

fc′=6500 psi (45MPa), but the variation is more in case of high strength concrete

fc′=7500, 8500 psi (50,55MPa). The strut angle in case of high strength concrete

corbels is also steeper. This may be mainly due to reduction in the aggregates

interlocking at higher strength of concrete. The concrete has been cracked

across the aggregates rather than at the contract points of the aggregates and

mortar and the failure is more brittle and sudden.

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vii. Corbel CB-1

viii. Corbel CB-3

Figure 7.8 Shear failure of Corbels CB-1 and CB-2, fc′ = 59 MPa, As= 387 mm2 (0.71in2

). The failure is more sudden and brittle typical for shear failure of HSC structure in shear. Figure 7.8 Cont’d

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Figure 7.8 (c) CB-4 fc′ = 52 MPa, As= 477 mm2 (0.71in2)

Figure 7.8 (d) CB-5, fc′ = 52 MPa, As= 477 mm2 (0.71 in2 )

Figure 7.8 (e) CB-5, fc′ = 45 MPa, As= 522 mm2 (0.81in2)

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Chapter No. 8

Comparison of the shear strength of HSC beams with

the provisions of international building and bridges

codes.

Chapter Introduction: In this chapter, the observed test values of the shear strength of HSC beams have been compared with the provision of the International Building and bridges Codes for shear design of concrete beams and the results have been evaluated in the light of recent research.

As already described in the literature review, different Codes have proposed

certain empirical equations for the shear design of high strength concrete based

on various approaches to the shear failure of concrete. To compare the observed

values with these provisions, the following most commonly used codes are

considered.

American Concrete Institute building code 318-08

Canadian Standards: Design of Concrete Structures,1994

AASHTO’s LRFD (Load Reduction Factor Design) Bridge design

Specification.

Eurocode-2002

New theory proposed in ACI structural Journal (March, April 2003)

8.1 American Concrete Institute (ACI) Code 318-08

The relevant equation of ACI-318 are already given as;

Eq (5.5) dbf

Vc wc

6

'

(SI units) –ACI Simplified equation

Eq (5.6) dbfdb

M

dVfVc wc

w

u

u

wc

'' 3.07

120

(SI units) –ACI detailed

equation.

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The comparison of actual and ACI-318 results for shear strength of HSC beams

with and without web reinforcement has been given in Tables 8.1 and Table 8.2

respectively.

Table No. 8.1 Comparison of the shear strength of beams without web reinforcement with the provisions of the ACI 318-08

Beam Title

ρ (%)

a/d

Shear Strength ( KN)

Vtest/VACI Vtest VACI

B1

B0.33,3

0.33

3.0 35.24 45.28 0.78

B0.33.3.5 3.5 30.27 45.16 0.67

B0.33,4 4.0 25.11 45.07 0.56

B0.33,4.5 4.5 23.92 45.00 0.53

B0.33,5 5.0 21.06 44.94 0.47

B0.33,5.5 5.5 18.88 44.90 0.42

B0.33,6 6.0 16.04 44.86 0.36

B2

B0.73,3

0.733

3.0 61.44 46.29 1.33

B0.73.3.5 3.5 56.72 46.03 1.23

B0.73,4 4.0 51.74 45.83 1.13

B0.73,4.5 4.5 46.78 45.68 1.02

B0.73,5 5.0 42.01 45.55 0.92

B0.33,5.5 5.5 36.97 45.45 0.81

B0.73,6 6.0 26.74 45.37 0.59

B3

B1,3

1.00

3.0 79.02 44.70 1.77

B1,3.5 3.5 67.96 44.66 1.52

B1,4 4.0 60.36 44.64 1.35

B1,4.5 4.5 57.36 44.61 1.29

B1,5 5.0 50.69 44.60 1.14

B1,5.5 5.5 49.76 44.58 1.12

B1,6 6.0 38.46 44.57 0.86

B4

B1.5,3

1.50

3.0 115.69 48.22 2.40

B1.5.3.5 3.5 103.31 47.68 2.17

B1.5,4 4.0 89.58 47.28 1.89

B1.5,4.5 4.5 79.58 46.96 1.69

B1.5,5 5.0 69.53 46.71 1.49

B1.5,5.5 5.5 62.52 46.50 1.34

B1.5,6 6.0 55.13 46.33 1.19

B5

B2,3

2.0

3.0 147.69 49.48 2.99

B2,.3.5 3.5 123.98 48.76 2.54

B2,4 4.0 101.61 48.22 2.11

B2,4.5 4.5 95.75 47.80 2.00

B2,5 5.0 85.68 47.46 1.81

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B2,5.5 5.5 76.81 47.19 1.63

B2,6 6.0 69.64 46.96 1.48

Table No. 8.2 Comparison of the shear capacity of beams with web reinforcement with the provisions of the ACI 318-08

Beam Title

a/d

ρ

(%)

a/d

Vtest ( KN)

Shear capacity as ACI provisions

( KN)

VACI = Vc+Vs

( KN)

Vntest/VACI

Vc

Vs Bs1

Bs0.33,3

0.33

3.0 40.18 45.28 11.65 56.93 0.75 Bs0.33.3.5 3.5 36.99 45.16 11.65 56.81 0.69 Bs0.33,4 4.0 31.90 45.07 11.65 56.72 0.60 B0.33,4.5 4.5 34.42 45.00 11.65 56.65 0.65 Bs0.33,5 5.0 31.58 44.94 11.65 56.59 0.60 Bs0.33,5.5 5.5 24.47 44.90 11.65 56.55 0.46 Bs0.33,6 6.0 21.79 44.86 11.65 56.51 0.41

Bs2

Bs0.73,3

0.733

3.0 81.77 46.29 11.65 57.94 1.51 Bs0.73.3.5 3.5 77.70 46.03 11.65 57.68 1.44 Bs0.73,4 4.0 67.27 45.83 11.65 57.48 1.25 Bs0.73,4.5 4.5 62.60 45.68 11.65 57.33 1.16 Bs0.73,5 5.0 57.68 45.55 11.65 57.20 1.08 Bs0.33,5.5 5.5 53.01 45.45 11.65 57.10 0.99 Bs0.73,6 6.0 48.11 45.37 11.65 57.02 0.90

B3

Bs1,3

1.00

3.0 95.69 44.70 11.65 56.35 1.81 Bs1,3.5 3.5 84.81 44.66 11.65 56.31 1.61 Bs1,4 4.0 78.64 44.64 11.65 56.29 1.49 Bs1,4.5 4.5 77.53 44.61 11.65 56.26 1.47 Bs1,5 5.0 72.92 44.60 11.65 56.25 1.38 Bs1,5.5 5.5 64.76 44.58 11.65 56.23 1.23 Bs1,6 6.0 52.91 44.57 11.65 56.22 1.00

Bs4

Bs1.5,3

1.50

3.0 125.18 48.22 11.65 59.87 2.23 Bs1.5.3.5 3.5 116.10 47.68 11.65 59.33 2.09 Bs1.5,4 4.0 95.92 47.28 11.65 58.93 1.74 Bs1.5,4.5 4.5 82.21 46.96 11.65 58.61 1.50 Bs1.5,5 5.0 71.84 46.71 11.65 58.36 1.31 Bs1.5,5.5 5.5 65.93 46.50 11.65 58.15 1.21 Bs1.5,6 6.0 58.76 46.33 11.65 57.98 1.08

Bs5

Bs2,3

2.0

3.0 160.54 49.48 11.65 61.13 2.80 Bs2,.3.5 3.5 135.31 48.76 11.65 60.41 2.39 Bs2,4 4.0 115.98 48.22 11.65 59.87 2.07 Bs2,4.5 4.5 112.66 47.80 11.65 59.45 2.02 Bs2,5 5.0 99.37 47.46 11.65 59.11 1.79 Bs2,5.5 5.5 95.03 47.19 11.65 58.84 1.72

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Bs2,6 6.0 77.77 46.96 11.65 58.61 1.42

The increase in the shear strength of beams with the additions of stirrups is given

in Table 8.3

Table No. 8.3 Comparison of increase in shear strength due to stirrups and ACI-318

provision for stirrups contribution.

Beam Title

ρ

(%)

a/d Vtest of beams ( KN)

Vs

VsACI

Without shear steel

With shear steel

1 2 3 4 5 6 7=6-5 8

Bs1

Bs0.33,3

0.33

3.0 35.24 40.18 4.94 11.65 Bs0.33.3.5 3.5 30.27 36.99 6.72 11.65 Bs0.33,4 4.0 25.11 31.90 6.79 11.65 B0.33,4.5 4.5 23.92 34.42 10.5 11.65 Bs0.33,5 5.0 21.06 31.58 10.52 11.65 Bs0.33,5.5 5.5 18.88 24.47 5.59 11.65 Bs0.33,6 6.0 16.04 21.79 5.75 11.65

Bs2

Bs0.73,3

0.733

3.0 61.44 81.77 20.33 11.65 Bs0.73.3.5 3.5 56.72 77.70 20.98 11.65 Bs0.73,4 4.0 51.74 67.27 15.53 11.65 Bs0.73,4.5 4.5 46.78 62.60 15.82 11.65 Bs0.73,5 5.0 42.01 57.68 15.67 11.65 Bs0.33,5.5 5.5 36.97 53.01 16.04 11.65 Bs0.73,6 6.0 26.74 48.11 21.37 11.65

B3

Bs1,3

1.00

3.0 79.02 95.69 16.67 11.65 Bs1,3.5 3.5 67.96 84.81 16.85 11.65 Bs1,4 4.0 60.36 78.64 18.28 11.65 Bs1,4.5 4.5 57.36 77.53 20.17 11.65 Bs1,5 5.0 50.69 72.92 22.23 11.65 Bs1,5.5 5.5 49.76 64.76 15 11.65 Bs1,6 6.0 38.46 52.91 14.45 11.65

Bs4

Bs1.5,3

1.50

3.0 115.69 125.18 9.49 11.65 Bs1.5.3.5 3.5 103.31 116.10 12.79 11.65 Bs1.5,4 4.0 89.58 95.92 6.34 11.65 Bs1.5,4.5 4.5 79.58 82.21 2.63 11.65 Bs1.5,5 5.0 69.53 71.84 2.31 11.65 Bs1.5,5.5 5.5 62.52 65.93 3.41 11.65 Bs1.5,6 6.0 55.13 58.76 3.63 11.65

Bs2,3

3.0 147.69 160.54 12.85 11.65 Bs2,.3.5 3.5 123.98 135.31 11.33 11.65

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Bs5

Bs2,4 2.0

4.0 101.61 115.98 14.37 11.65 Bs2,4.5 4.5 95.75 112.66 16.91 11.65 Bs2,5 5.0 85.68 99.37 13.69 11.65 Bs2,5.5 5.5 76.81 95.03 18.22 11.65 Bs2,6 6.0 69.64 77.77 8.13 11.65

Comparison of actual test results of shear strength of HSC beams with the

results given by ACI-318 in Tables 8.1, 8.2 and 8.3 equations gives the following

general observations;

1. The ACI-318 provision for shear strength of HSC beams is un-

conservative for small values of longitudinal steel both for beams with and

without web reinforcement.

2. The shear strength given by ACI-318 for ρ≥1% are however reasonably

good and becomes more conservative for ρ =1.5% and 2%.

3. The increase in shear strength of HSC beams due to addition of same

amount of stirrups in all beams is not same, as given by ACI-318. Hence

the superposition of the two contributions (concrete and transverse steel)

has not been shown in the results.

8.2 Canadian Standards for the design of concrete structures (CSA A23.3-94).

The general design method of CSA A23.3-94 is based on the Modified

Compression Filed Theory (MCFT), which requires the maximum longitudinal

strain in the concrete, which depends on the factored shear force at the section,

crack angle and longitudinal steel. However the simplified design method is

based on the concrete compressive strength only. The relevant equations are

given below;

Eq (5.17) dbfVc wc

'2.0 (SI Units) if sbf

fA w

y

cv

'06.0 or mmd 300

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Eq(5.16) dbfdbf

dV wcwcc

1.0

1000

260 if sb

f

fA w

y

cv

'06.0 ,d>300mm

All terms have been already defined.

Since detailed MCFT has been discussed in next sections, therefore only

simplified design method of Canadian Standards has been used for comparison

here and the results have been given in Table 8.4 and 8.5.

Table No. 8.4 Comparison of the shear Strength of beams without web reinforcement with the provisions of the Canadian Standards (Simplified Method)

Beam Title

ρ (%) a/d

Shear Strength Vtest/VCSA Vtest

( KN) VCSA

(KN)

B1

B0.33,3

0.33

3.0 35.24 40.303 0.87 B0.33.3.5 3.5 30.27 40.303 0.75 B0.33,4 4.0 25.11 40.303 0.62 B0.33,4.5 4.5 23.92 40.303 0.59 B0.33,5 5.0 21.06 40.303 0.52 B0.33,5.5 5.5 18.88 40.303 0.47 B0.33,6 6.0 16.04 40.303 0.40

B2

B0.73,3

0.733

3.0 61.44 40.303 1.52 B0.73.3.5 3.5 56.72 40.303 1.41 B0.73,4 4.0 51.74 40.303 1.28 B0.73,4.5 4.5 46.78 40.303 1.16 B0.73,5 5.0 42.01 40.303 1.04 B0.33,5.5 5.5 36.97 40.303 0.92 B0.73,6 6.0 26.74 40.303 0.66

B3

B1,3

1.00

3.0 79.02 40.303 1.96 B1,3.5 3.5 67.96 40.303 1.69 B1,4 4.0 60.36 40.303 1.50 B1,4.5 4.5 57.36 40.303 1.42 B1,5 5.0 50.69 40.303 1.26 B1,5.5 5.5 49.76 40.303 1.23 B1,6 6.0 38.46 40.303 0.95

B4

B1.5,3

1.50

3.0 115.69 40.303 2.87 B1.5.3.5 3.5 103.31 40.303 2.56 B1.5,4 4.0 89.58 40.303 2.22 B1.5,4.5 4.5 79.58 40.303 1.97 B1.5,5 5.0 69.53 40.303 1.73 B1.5,5.5 5.5 62.52 40.303 1.55 B1.5,6 6.0 55.13 40.303 1.37

B5

B2,3

2.0

3.0 147.69 40.303 3.66 B2,.3.5 3.5 123.98 40.303 3.08 B2,4 4.0 101.61 40.303 2.52 B2,4.5 4.5 95.75 40.303 2.38 B2,5 5.0 85.68 40.303 2.13

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B2,5.5 5.5 76.81 40.303 1.91 B2,6 6.0 69.64 40.303 1.73

Table No. 8.5 Comparison of the shear Strength of beams with web reinforcement with the provisions of the Canadian Standards (Simplified Method)

Beam Title

a/d

ρ (%)

Vtest ( KN)

Shear capacity as per CSA provisions

( KN)

VCSA = Vc+Vs

( KN)

Vtest/VCSA

Vc

Vs Bs1

Bs0.33,3

0.33

3.0 40.18 40.303 16.67 56.98 0.71 Bs0.33.3.5 3.5 36.99 40.303 16.67 56.98 0.65 Bs0.33,4 4.0 31.90 40.303 16.67 56.98 0.56 B0.33,4.5 4.5 34.42 40.303 16.67 56.98 0.60 Bs0.33,5 5.0 31.58 40.303 16.67 56.98 0.55 Bs0.33,5.5 5.5 24.47 40.303 16.67 56.98 0.43 Bs0.33,6 6.0 21.79 40.303 16.67 56.98 0.38

Bs2

Bs0.73,3

0.733

3.0 81.77 40.303 16.67 56.98 1.44 Bs0.73.3.5 3.5 77.70 40.303 16.67 56.98 1.36 Bs0.73,4 4.0 67.27 40.303 16.67 56.98 1.18 Bs0.73,4.5 4.5 62.60 40.303 16.67 56.98 1.10 Bs0.73,5 5.0 57.68 40.303 16.67 56.98 1.01 Bs0.33,5.5 5.5 53.01 40.303 16.67 56.98 0.93 Bs0.73,6 6.0 48.11 40.303 16.67 56.98 0.84

Bs3

Bs1,3

1.00

3.0 95.69 40.303 16.67 56.98 1.68 Bs1,3.5 3.5 84.81 40.303 16.67 56.98 1.49 Bs1,4 4.0 78.64 40.303 16.67 56.98 1.38 Bs1,4.5 4.5 77.53 40.303 16.67 56.98 1.36 Bs1,5 5.0 72.92 40.303 16.67 56.98 1.28 Bs1,5.5 5.5 64.76 40.303 16.67 56.98 1.14 Bs1,6 6.0 52.91 40.303 16.67 56.98 0.93

Bs4

Bs1.5,3

1.50

3.0 125.18 40.303 16.67 56.98 2.20 Bs1.5.3.5 3.5 116.10 40.303 16.67 56.98 2.04 Bs1.5,4 4.0 95.92 40.303 16.67 56.98 1.68 Bs1.5,4.5 4.5 82.21 40.303 16.67 56.98 1.44 Bs1.5,5 5.0 71.84 40.303 16.67 56.98 1.26 Bs1.5,5.5 5.5 65.93 40.303 16.67 56.98 1.16 Bs1.5,6 6.0 58.76 40.303 16.67 56.98 1.03

Bs5

Bs2,3

2.0

3.0 160.54 40.303 16.67 56.98 2.82 Bs2,.3.5 3.5 135.31 40.303 16.67 56.98 2.37 Bs2,4 4.0 115.98 40.303 16.67 56.98 2.04

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Bs2,4.5 4.5 112.66 40.303 16.67 56.98 1.98 Bs2,5 5.0 99.37 40.303 16.67 56.98 1.74 Bs2,5.5 5.5 95.03 40.303 16.67 56.98 1.67 Bs2,6 6.0 77.77 40.303 16.67 56.98 1.36

The increase in the shear strength of beams with the additions of stirrups and its

comparison with CSA, is given in Table 8.6

Table No. 8.6 Comparison of increase in shear strength due to stirrups and CSA

provision for stirrups contribution.

Beam Title

ρ

(%)

a/d Vtest of beams ( KN)

Vs-test

VsACI

Without shear steel

With shear steel

1 2 3 4 5 6 7=6-5 8

Bs1

Bs0.33,3

0.33

3.0 35.24 40.18 4.94 16.67 Bs0.33.3.5 3.5 30.27 36.99 6.72 16.67 Bs0.33,4 4.0 25.11 31.90 6.79 16.67 B0.33,4.5 4.5 23.92 34.42 10.5 16.67 Bs0.33,5 5.0 21.06 31.58 10.52 16.67 Bs0.33,5.5 5.5 18.88 24.47 5.59 16.67 Bs0.33,6 6.0 16.04 21.79 5.75 16.67

Bs2

Bs0.73,3

0.733

3.0 61.44 81.77 20.33 16.67 Bs0.73.3.5 3.5 56.72 77.70 20.98 16.67 Bs0.73,4 4.0 51.74 67.27 15.53 16.67 Bs0.73,4.5 4.5 46.78 62.60 15.82 16.67 Bs0.73,5 5.0 42.01 57.68 15.67 16.67 Bs0.33,5.5 5.5 36.97 53.01 16.04 16.67 Bs0.73,6 6.0 26.74 48.11 21.37 16.67

B3

Bs1,3

1.00

3.0 79.02 95.69 16.67 16.67 Bs1,3.5 3.5 67.96 84.81 16.85 16.67 Bs1,4 4.0 60.36 78.64 18.28 16.67 Bs1,4.5 4.5 57.36 77.53 20.17 16.67 Bs1,5 5.0 50.69 72.92 22.23 16.67 Bs1,5.5 5.5 49.76 64.76 15 16.67 Bs1,6 6.0 38.46 52.91 14.45 16.67

Bs4

Bs1.5,3

1.50

3.0 115.69 125.18 9.49 16.67 Bs1.5.3.5 3.5 103.31 116.10 12.79 16.67 Bs1.5,4 4.0 89.58 95.92 6.34 16.67 Bs1.5,4.5 4.5 79.58 82.21 2.63 16.67 Bs1.5,5 5.0 69.53 71.84 2.31 16.67 Bs1.5,5.5 5.5 62.52 65.93 3.41 16.67 Bs1.5,6 6.0 55.13 58.76 3.63 16.67

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Bs5

Bs2,3

2.0

3.0 147.69 160.54 12.85 16.67 Bs2,.3.5 3.5 123.98 135.31 11.33 16.67 Bs2,4 4.0 101.61 115.98 14.37 16.67 Bs2,4.5 4.5 95.75 112.66 16.91 16.67 Bs2,5 5.0 85.68 99.37 13.69 16.67 Bs2,5.5 5.5 76.81 95.03 18.22 16.67 Bs2,6 6.0 69.64 77.77 8.13 16.67

Comparison of actual test results of shear strength of HSC beams with the

results given by CSA equations in Tables 8.4, 8.5 and 8.6, gives the following

general observations;

1. Like ACI-318 provision, the provisions of CSA for shear strength of

HSC un-conservative for small values of longitudinal steel both for

beams with and without web reinforcement.

2. The shear strength given by CSA for ρ≥1,1.5% are however

reasonably good and becomes more conservative for 2%.

3. The increase in shear strength of HSC beams due to addition of same

amount of stirrups in all beams is not same, as given in CSA like ACI-

318. Hence the superposition of the two contributions (concrete and

transverse steel) has not been shown in the results by CSA as well.

8.3 AASHTO’s LRFD DESIGN SPECIFICATION (1994)

(Based on Modified Compression Field theory-MCFT)

The values of shear strength are given by the following equations;

Eq (5.20) vvcvvcc dbfdbfV '' 25.0083.0

The actual and calculated values of shear strength are compared with the values

proposed by AASHTO’s LRFD design specification based on Modified

Compression Field theory in Tables 8.7 & 8.8.

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Table 8.7 Comparison of the shear Strength of beams without web reinforcement with the provisions of MCFT( LRFD Method)

Beam Title ρ (%) a/d

Shear Strength Vtest/VMCFT Vtest

( KN) VMCFT

(KN)

B1

B0.33,3

0.33

3.0 35.24 46.94 0.75 B0.33.3.5 3.5 30.27 46.94 0.64 B0.33,4 4.0 25.11 46.94 0.53 B0.33,4.5 4.5 23.92 46.94 0.51 B0.33,5 5.0 21.06 46.94 0.45 B0.33,5.5 5.5 18.88 46.94 0.40 B0.33,6 6.0 16.04 46.94 0.34

B2

B0.73,3

0.733

3.0 61.44 46.94 1.31 B0.73.3.5 3.5 56.72 46.94 1.21 B0.73,4 4.0 51.74 46.94 1.10 B0.73,4.5 4.5 46.78 46.94 1.00 B0.73,5 5.0 42.01 46.94 0.90 B0.33,5.5 5.5 36.97 46.94 0.79 B0.73,6 6.0 26.74 46.94 0.57

B3

B1,3

1.00

3.0 79.02 46.94 1.68 B1,3.5 3.5 67.96 46.94 1.45 B1,4 4.0 60.36 46.94 1.29 B1,4.5 4.5 57.36 46.94 1.22 B1,5 5.0 50.69 46.94 1.08 B1,5.5 5.5 49.76 46.94 1.06 B1,6 6.0 38.46 46.94 0.82

B4

B1.5,3

1.50

3.0 115.69 47.54 2.43 B1.5.3.5 3.5 103.31 47.54 2.17 B1.5,4 4.0 89.58 47.54 1.88 B1.5,4.5 4.5 79.58 47.54 1.67 B1.5,5 5.0 69.53 47.54 1.46 B1.5,5.5 5.5 62.52 47.54 1.32 B1.5,6 6.0 55.13 47.54 1.16

B5

B2,3

2.0

3.0 147.69 50.04 2.95 B2,.3.5 3.5 123.98 50.04 2.48 B2,4 4.0 101.61 50.04 2.03 B2,4.5 4.5 95.75 50.04 1.91 B2,5 5.0 85.68 50.04 1.71

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B2,5.5 5.5 76.81 50.04 1.53 B2,6 6.0 69.64 50.04 1.39

Table 8.8 Comparison of the shear Strength of beams with web reinforcement with the provisions of MCFT ( LRFD Method)

Beam Title

a/d

ρ (%)

Vtest ( KN)

Shear capacity as MCFT provisions

( KN)

VMCFT = Vc+Vs

( KN)

Vtest/VMCFT

Vc

Vs Bs1

Bs0.33,3

0.33

3.0 40.18 46.94 19.62 66.56 0.60 Bs0.33.3.5 3.5

36.99 46.94 19.62 66.56 0.56 Bs0.33,4 4.0 31.90 46.94 19.62 66.56 0.48 B0.33,4.5 4.5

34.42 46.94 19.62 66.56 0.52 Bs0.33,5 5.0 31.58 46.94 19.62 66.56 0.47 Bs0.33,5.5 5.5

24.47 46.94 19.62 66.56 0.37 Bs0.33,6 6.0 21.79 46.94 19.62 66.56 0.33

Bs2

Bs0.73,3

0.733

3.0 81.77 46.94 19.62 66.56 1.23

Bs0.73.3.5 3.5 77.70 46.94 19.62 66.56 1.17 Bs0.73,4 4.0

67.27 46.94 19.62 66.56 1.01 Bs0.73,4.5 4.5 62.60 46.94 19.62 66.56 0.94 Bs0.73,5 5.0

57.68 46.94 19.62 66.56 0.87 Bs0.33,5.5 5.5 53.01 46.94 19.62 66.56 0.80 Bs0.73,6 6.0

48.11 46.94 19.62 66.56 0.72 B3

Bs1,3

1.00

3.0 95.69 46.94 19.62 66.56 1.44 Bs1,3.5 3.5 84.81 46.94 19.62 66.56 1.27 Bs1,4 4.0

78.64 46.94 19.62 66.56 1.18 Bs1,4.5 4.5 77.53 46.94 19.62 66.56 1.16 Bs1,5 5.0

72.92 46.94 19.62 66.56 1.10 Bs1,5.5 5.5 64.76 46.94 19.62 66.56 0.97 Bs1,6 6.0

52.91 46.94 19.62 66.56 0.79 Bs4

Bs1.5,3

1.50

3.0 125.18 47.54 19.62 67.16 1.86

Bs1.5.3.5 3.5 116.10 47.54 19.62 67.16 1.73

Bs1.5,4 4.0 95.92 47.54 19.62 67.16 1.43

Bs1.5,4.5 4.5 82.21 47.54 19.62 67.16 1.22

Bs1.5,5 5.0 71.84 47.54 19.62 67.16 1.07

Bs1.5,5.5 5.5 65.93 47.54 19.62 67.16 0.98

Bs1.5,6 6.0 58.76 47.54 19.62 67.16 0.87

Bs2,3

3.0 160.54 50.04 19.62 69.66 2.30

Bs2,.3.5 3.5 135.31 50.04 19.62 69.66 1.94

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Bs5 Bs2,4 2.0

4.0 115.98 50.04 19.62 69.66 1.66

Bs2,4.5 4.5 112.66 50.04 19.62 69.66 1.62

Bs2,5 5.0 99.37 50.04 19.62 69.66 1.43

Bs2,5.5 5.5 95.03 50.04 19.62 69.66 1.36

Bs2,6 6.0 77.77 50.04 19.62 69.66 1.12

The increase in the shear strength of beams with the additions of stirrups and its

comparison with MCFT, is given in Table 8.9

Table No. 8.9 Comparison of increase in shear strength due to stirrups and MCFT

provision for stirrups contribution.

Beam Title

ρ

(%)

a/d Vtest of beams ( KN)

Vs-test

VsMCFT

Without shear steel

With shear steel

1 2 3 4 5 6 7=6-5 8

Bs1

Bs0.33,3

0.33

3.0 35.24 40.18 4.94 19.62 Bs0.33.3.5 3.5 30.27 36.99 6.72 19.62 Bs0.33,4 4.0 25.11 31.90 6.79 19.62 B0.33,4.5 4.5 23.92 34.42 10.5 19.62 Bs0.33,5 5.0 21.06 31.58 10.52 19.62 Bs0.33,5.5 5.5 18.88 24.47 5.59 19.62 Bs0.33,6 6.0 16.04 21.79 5.75 19.62

Bs2

Bs0.73,3

0.733

3.0 61.44 81.77 20.33 19.62 Bs0.73.3.5 3.5 56.72 77.70 20.98 19.62 Bs0.73,4 4.0 51.74 67.27 15.53 19.62 Bs0.73,4.5 4.5 46.78 62.60 15.82 19.62 Bs0.73,5 5.0 42.01 57.68 15.67 19.62 Bs0.33,5.5 5.5 36.97 53.01 16.04 19.62 Bs0.73,6 6.0 26.74 48.11 21.37 19.62

B3

Bs1,3

1.00

3.0 79.02 95.69 16.67 19.62 Bs1,3.5 3.5 67.96 84.81 16.85 19.62 Bs1,4 4.0 60.36 78.64 18.28 19.62 Bs1,4.5 4.5 57.36 77.53 20.17 19.62 Bs1,5 5.0 50.69 72.92 22.23 19.62 Bs1,5.5 5.5 49.76 64.76 15 19.62 Bs1,6 6.0 38.46 52.91 14.45 19.62

Bs4

Bs1.5,3

1.50

3.0 115.69 125.18 9.49 19.62 Bs1.5.3.5 3.5 103.31 116.10 12.79 19.62 Bs1.5,4 4.0 89.58 95.92 6.34 19.62 Bs1.5,4.5 4.5 79.58 82.21 2.63 19.62 Bs1.5,5 5.0 69.53 71.84 2.31 19.62 Bs1.5,5.5 5.5 62.52 65.93 3.41 19.62 Bs1.5,6 6.0 55.13 58.76 3.63 19.62

Bs2,3 3.0 147.69 160.54 12.85 19.62

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Bs5

Bs2,.3.5

2.0

3.5 123.98 135.31 11.33 19.62 Bs2,4 4.0 101.61 115.98 14.37 19.62 Bs2,4.5 4.5 95.75 112.66 16.91 19.62 Bs2,5 5.0 85.68 99.37 13.69 19.62 Bs2,5.5 5.5 76.81 95.03 18.22 19.62 Bs2,6 6.0 69.64 77.77 8.13 19.62

Comparison of actual test results of HSC beams with the values given by LRFD

(MCFT) methods in Table 8.6 ,Table 8.7 and Table 8.9, give the following

general observations;

1. Except for minimum value of ρ, LRFD gives reasonably good prediction of

the shear strength of HSC beams for ρ≤1%.

2. For ρ = 1.5% and 2%, LFRD gives conservative results.

3. Uniform increase in the shear strength due to addition of stirrups as given

in the Code, is not experimentally demonstrated.

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8.4 Comparison of observed values with the provisions of Eurocode-02 The relevant equations of EC-02 are given as follows;

Eq (5.2) dbkV wlrdRD )402.1(1 Where ,5

5.21

x

d

,0.1)1000/6.1( dk 5.0200/7.0 ylf

The results are given in Tables 8.10 and 8.11 Table 8.10 Comparison of the shear Strength of beams without web reinforcement with the provisions of EC-02

Beam Title

ρ (%) a/d

Shear Strength Vtest/VEC02 Vtest

( KN) VEC-02

(KN)

B1

B0.33,3

0.33

3.0 35.24 36.70 0.96 B0.33.3.5 3.5 30.27 36.70 0.82 B0.33,4 4.0 25.11 36.70 0.68 B0.33,4.5 4.5 23.92 36.70 0.65 B0.33,5 5.0 21.06 36.70 0.57 B0.33,5.5 5.5 18.88 36.70 0.51 B0.33,6 6.0 16.04 36.70 0.44

B2

B0.73,3

0.733

3.0 61.44 41.14 1.49 B0.73.3.5 3.5 56.72 41.14 1.38 B0.73,4 4.0 51.74 41.14 1.26 B0.73,4.5 4.5 46.78 41.14 1.14 B0.73,5 5.0 42.01 41.14 1.02 B0.33,5.5 5.5 36.97 41.14 0.90 B0.73,6 6.0 26.74 41.14 0.65

B3

B1,3

1.00

3.0 79.02 44.08 1.79 B1,3.5 3.5 67.96 44.08 1.54 B1,4 4.0 60.36 44.08 1.37 B1,4.5 4.5 57.36 44.08 1.30 B1,5 5.0 50.69 44.08 1.15 B1,5.5 5.5 49.76 44.08 1.13 B1,6 6.0 38.46 44.08 0.87

B4

B1.5,3

1.50

3.0 115.69 49.59 2.33 B1.5.3.5 3.5 103.31 49.59 2.08 B1.5,4 4.0 89.58 49.59 1.81 B1.5,4.5 4.5 79.58 49.59 1.60 B1.5,5 5.0 69.53 49.59 1.40 B1.5,5.5 5.5 62.52 49.59 1.26 B1.5,6 6.0 55.13 49.59 1.11

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B5

B2,3

2.0

3.0 147.69 55.10 2.68 B2,.3.5 3.5 123.98 55.10 2.25 B2,4 4.0 101.61 55.10 1.84 B2,4.5 4.5 95.75 55.10 1.74 B2,5 5.0 85.68 55.10 1.56 B2,5.5 5.5 76.81 55.10 1.39 B2,6 6.0 69.64 55.10 1.26

Table No. 8.11 Comparison of the shear Strength of beams with web reinforcement with the provisions of EC-02

Beam Title

a/d

ρ

(%)

Vtest ( KN)

Shear capacity as per EC-02 provisions

( KN)

V EC02 = Vc+Vs

( KN)

Vtest/VEC02

Vc Vs

Bs1

Bs0.33,3

0.33

3.0 40.18 36.70 17.08 53.77 0.75 Bs0.33.3.5 3.5 36.99 36.70 17.08 53.77 0.69 Bs0.33,4 4.0 31.90 36.70 17.08 53.77 0.59 B0.33,4.5 4.5 34.42 36.70 17.08 53.77 0.64 Bs0.33,5 5.0 31.58 36.70 17.08 53.77 0.59 Bs0.33,5.5 5.5 24.47 36.70 17.08 53.77 0.46 Bs0.33,6 6.0 21.79 36.70 17.08 53.77 0.41

Bs2

Bs0.73,3

0.733

3.0 81.77 41.14 17.08 58.21 1.40 Bs0.73.3.5 3.5 77.70 41.14 17.08 58.21 1.33 Bs0.73,4 4.0 67.27 41.14 17.08 58.21 1.16 Bs0.73,4.5 4.5 62.60 41.14 17.08 58.21 1.08 Bs0.73,5 5.0 57.68 41.14 17.08 58.21 0.99 Bs0.33,5.5 5.5 53.01 41.14 17.08 58.21 0.91 Bs0.73,6 6.0 48.11 41.14 17.08 58.21 0.83

B3

Bs1,3

1.00

3.0 95.69 44.08 17.08 61.16 1.56 Bs1,3.5 3.5 84.81 44.08 17.08 61.16 1.39 Bs1,4 4.0 78.64 44.08 17.08 61.16 1.29 Bs1,4.5 4.5 77.53 44.08 17.08 61.16 1.27 Bs1,5 5.0 72.92 44.08 17.08 61.16 1.19 Bs1,5.5 5.5 64.76 44.08 17.08 61.16 1.06 Bs1,6 6.0 52.91 44.08 17.08 61.16 0.87

Bs4

Bs1.5,3

1.50

3.0 125.18 49.59 17.08 66.67 1.88 Bs1.5.3.5 3.5 116.10 49.59 17.08 66.67 1.74 Bs1.5,4 4.0 95.92 49.59 17.08 66.67 1.44 Bs1.5,4.5 4.5 82.21 49.59 17.08 66.67 1.23 Bs1.5,5 5.0 71.84 49.59 17.08 66.67 1.08 Bs1.5,5.5 5.5 65.93 49.59 17.08 66.67 0.99 Bs1.5,6 6.0 58.76 49.59 17.08 66.67 0.88

Bs5

Bs2,3

2.0

3.0 160.54 55.10 17.08 72.18 2.22 Bs2,.3.5 3.5 135.31 55.10 17.08 72.18 1.87 Bs2,4 4.0 115.98 55.10 17.08 72.18 1.61 Bs2,4.5 4.5 112.66 55.10 17.08 72.18 1.56 Bs2,5 5.0 99.37 55.10 17.08 72.18 1.38

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Bs2,5.5 5.5 95.03 55.10 17.08 72.18 1.32 Bs2,6 6.0 77.77 55.10 17.08 69.66 1.08

The increase in the shear strength of beams with the additions of stirrups and its

comparison with EC-02, is given in Table 8.12

Table No. 8.12 Comparison of increase in shear strength due to stirrups and EC-02

provision for stirrups contribution.

Beam Title

ρ

(%)

a/d Vtest of beams ( KN)

Vs-test

VsEC-02

Without shear steel

With shear steel

1 2 3 4 5 6 7=6-5 8

Bs1

Bs0.33,3

0.33

3.0 35.24 40.18 4.94 17.08 Bs0.33.3.5 3.5 30.27 36.99 6.72 17.08 Bs0.33,4 4.0 25.11 31.90 6.79 17.08 B0.33,4.5 4.5 23.92 34.42 10.5 17.08 Bs0.33,5 5.0 21.06 31.58 10.52 17.08 Bs0.33,5.5 5.5 18.88 24.47 5.59 17.08 Bs0.33,6 6.0 16.04 21.79 5.75 17.08

Bs2

Bs0.73,3

0.733

3.0 61.44 81.77 20.33 17.08 Bs0.73.3.5 3.5 56.72 77.70 20.98 17.08 Bs0.73,4 4.0 51.74 67.27 15.53 17.08 Bs0.73,4.5 4.5 46.78 62.60 15.82 17.08 Bs0.73,5 5.0 42.01 57.68 15.67 17.08 Bs0.33,5.5 5.5 36.97 53.01 16.04 17.08 Bs0.73,6 6.0 26.74 48.11 21.37 17.08

B3

Bs1,3

1.00

3.0 79.02 95.69 16.67 17.08 Bs1,3.5 3.5 67.96 84.81 16.85 17.08 Bs1,4 4.0 60.36 78.64 18.28 17.08 Bs1,4.5 4.5 57.36 77.53 20.17 17.08 Bs1,5 5.0 50.69 72.92 22.23 17.08 Bs1,5.5 5.5 49.76 64.76 15 17.08 Bs1,6 6.0 38.46 52.91 14.45 17.08

Bs4

Bs1.5,3

1.50

3.0 115.69 125.18 9.49 17.08 Bs1.5.3.5 3.5 103.31 116.10 12.79 17.08 Bs1.5,4 4.0 89.58 95.92 6.34 17.08 Bs1.5,4.5 4.5 79.58 82.21 2.63 17.08 Bs1.5,5 5.0 69.53 71.84 2.31 17.08 Bs1.5,5.5 5.5 62.52 65.93 3.41 17.08 Bs1.5,6 6.0 55.13 58.76 3.63 17.08

Bs2,3 3.0 147.69 160.54 12.85 17.08

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Bs5

Bs2,.3.5

2.0

3.5 123.98 135.31 11.33 17.08 Bs2,4 4.0 101.61 115.98 14.37 17.08 Bs2,4.5 4.5 95.75 112.66 16.91 17.08 Bs2,5 5.0 85.68 99.37 13.69 17.08 Bs2,5.5 5.5 76.81 95.03 18.22 17.08 Bs2,6 6.0 69.64 77.77 8.13 17.08

Comparison of actual test results of HSC beams with the values given by EC-02,

in Table 8.10, 8.11 and Table 8.12 give the following general observations;

1. Except for minimum value of ρ, EC-02 gives reasonably good prediction of

the shear strength of HSC beams for ρ up to 1%.

2. For ρ = 1.5% and 2%, EC-02is conservative. However the degree of

safety is relatively less when compared with the other equations already

discussed.

3. Uniform increase in the shear strength due to addition of stirrups as given

in EC-02 Code, is not exhibited.

8.5 New Theory Proposed by Prodromos D.Zararis (2003) P. D.Zararis (2003), has reported a new equation for the design of shear strength

and minimum shear reinforcement of RC beams, in ACI structural Journal March-

April, 2003. The actual and theoretical values given by the proposed equations

are compared in Table 8.13 and Table 8.14.

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Table No. 8.13 Comparison of the shear Strength of beams without web reinforcement with equation proposed in new theory of Zararis,P.D.

Beam Title

ρ (%) a/d

Shear Strength Vtest/VNew Theo Vtest

( KN) VNew Theo

(KN)

B1

B0.33,3

0.33

3.0 35.24 41.50 0.85 B0.33.3.5 3.5 30.27 38.31 0.79 B0.33,4 4.0 25.11 30.62 0.82 B0.33,4.5 4.5 23.92 24.35 0.98 B0.33,5 5.0 21.06 21.02 1.00 B0.33,5.5 5.5 18.88 17.75 1.06 B0.33,6 6.0 16.04 10.83 1.48

B2

B0.73,3

0.733

3.0 61.44 41.50 1.48 B0.73.3.5 3.5 56.72 38.31 1.48 B0.73,4 4.0 51.74 34.93 1.48 B0.73,4.5 4.5 46.78 31.58 1.48 B0.73,5 5.0 42.01 28.36 1.48 B0.33,5.5 5.5 36.97 24.95 1.48 B0.73,6 6.0 26.74 18.05 1.48

B3

B1,3

1.00

3.0 79.02 43.17 1.83 B1,3.5 3.5 67.96 41.93 1.62 B1,4 4.0 60.36 38.48 1.57 B1,4.5 4.5 57.36 35.23 1.63 B1,5 5.0 50.69 31.88 1.59 B1,5.5 5.5 49.76 28.66 1.74 B1,6 6.0 38.46 25.25 1.52

B4

B1.5,3

1.50

3.0 115.69 81.13 1.43 B1.5.3.5 3.5 103.31 73.33 1.41 B1.5,4 4.0 89.58 70.66 1.27 B1.5,4.5 4.5 79.58 60.41 1.32 B1.5,5 5.0 69.53 57.21 1.22 B1.5,5.5 5.5 62.52 50.84 1.23 B1.5,6 6.0 55.13 46.90 1.18

B5

B2,3

2.0

3.0 147.69 73.21 2.02 B2,.3.5 3.5 123.98 69.41 1.79 B2,4 4.0 101.61 67.39 1.51 B2,4.5 4.5 95.75 59.75 1.60 B2,5 5.0 85.68 53.51 1.60 B2,5.5 5.5 76.81 50.47 1.52 B2,6 6.0 69.64 46.90 1.48

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Table No. 8.14 Comparison of the shear Strength of beams with web reinforcement with equation proposed in new theory of Zararis,P.D (2003).

Beam Title

ρ

(%)

a/d Vtest ( KN)

Shear capacity as New theory eq of

Zararis ( KN)

Vnew theory

= (Vc+Vs) ( KN)

Vtest/Vnew theory

Vc

Vs Bs1

Bs0.33,3

0.33

3.0 40.18 41.50 13.62 55.12 0.73 Bs0.33.3.5 3.5 36.99 38.31 14.98 53.29 0.69 Bs0.33,4 4.0 31.90 30.62 16.34 46.96 0.68 B0.33,4.5 4.5 34.42 24.35 17.70 42.05 0.82 Bs0.33,5 5.0 31.58 21.02 19.06 40.08 0.79 Bs0.33,5.5 5.5 24.47 17.75 20.42 38.17 0.64 Bs0.33,6 6.0 21.79 10.83 21.78 32.61 0.67

Bs2

Bs0.73,3

0.733

3.0 81.77 41.50 13.62 55.12 1.48 Bs0.73.3.5 3.5 77.70 38.31 14.98 53.29 1.46 Bs0.73,4 4.0 67.27 34.93 16.34 51.27 1.31 Bs0.73,4.5 4.5 62.60 31.58 17.70 49.28 1.27 Bs0.73,5 5.0 57.68 28.36 19.06 47.42 1.22 Bs0.33,5.5 5.5 53.01 24.95 20.42 45.38 1.17 Bs0.73,6 6.0 48.11 18.05 21.78 39.83 1.21

B3

Bs1,3

1.00

3.0 95.69 43.17 13.62 56.79 1.69 Bs1,3.5 3.5 84.81 41.93 14.98 56.91 1.49 Bs1,4 4.0 78.64 38.48 16.34 54.82 1.43 Bs1,4.5 4.5 77.53 35.23 17.70 52.93 1.46 Bs1,5 5.0 72.92 31.88 19.06 50.94 1.43 Bs1,5.5 5.5 64.76 28.66 20.42 49.08 1.32 Bs1,6 6.0 52.91 25.25 21.78 47.04 1.12

Bs4

Bs1.5,3

1.50

3.0 125.18 81.13 13.62 94.75 1.32 Bs1.5.3.5 3.5 116.10 73.33 14.98 88.30 1.31 Bs1.5,4 4.0 95.92 70.66 16.34 87.00 1.10 Bs1.5,4.5 4.5 82.21 60.41 17.70 78.12 1.05 Bs1.5,5 5.0 71.84 57.21 19.06 76.27 0.94 Bs1.5,5.5 5.5 65.93 50.84 20.42 71.26 0.93 Bs1.5,6 6.0 58.76 46.90 21.78 68.69 0.86

Bs5

Bs2,3

2.0

3.0 160.54 73.21 13.62 86.83 1.85 Bs2,.3.5 3.5 135.31 69.41 14.98 84.38 1.60 Bs2,4 4.0 115.98 67.39 16.34 83.73 1.39 Bs2,4.5 4.5 112.66 59.75 17.70 77.45 1.45 Bs2,5 5.0 99.37 53.51 19.06 72.57 1.37

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Bs2,5.5 5.5 95.03 50.47 20.42 70.90 1.34 Bs2,6 6.0 77.77 46.90 21.78 68.69 1.13

The increase in the shear strength of beams with the additions of stirrups and its

comparison with EC-02, is given in Table 8.12

Table No. 8.15 Comparison of increase in shear strength due to stirrups and New theory

of Zararis.P (2003) for stirrups contribution.

Beam Title

ρ

(%)

a/d Vtest of beams ( KN)

Vs-test

Vsnew theory

Without shear steel

With shear steel

1 2 3 4 5 6 7=6-5 8

Bs1

Bs0.33,3

0.33

3.0 35.24 40.18 4.94 13.62 Bs0.33.3.5 3.5 30.27 36.99 6.72 14.98 Bs0.33,4 4.0 25.11 31.90 6.79 16.34 B0.33,4.5 4.5 23.92 34.42 10.5 17.70 Bs0.33,5 5.0 21.06 31.58 10.52 19.06 Bs0.33,5.5 5.5 18.88 24.47 5.59 20.42 Bs0.33,6 6.0 16.04 21.79 5.75 21.78

Bs2

Bs0.73,3

0.733

3.0 61.44 81.77 20.33 13.62 Bs0.73.3.5 3.5 56.72 77.70 20.98 14.98 Bs0.73,4 4.0 51.74 67.27 15.53 16.34 Bs0.73,4.5 4.5 46.78 62.60 15.82 17.70 Bs0.73,5 5.0 42.01 57.68 15.67 19.06 Bs0.33,5.5 5.5 36.97 53.01 16.04 20.42 Bs0.73,6 6.0 26.74 48.11 21.37 21.78

B3

Bs1,3

1.00

3.0 79.02 95.69 16.67 13.62 Bs1,3.5 3.5 67.96 84.81 16.85 14.98 Bs1,4 4.0 60.36 78.64 18.28 16.34 Bs1,4.5 4.5 57.36 77.53 20.17 17.70 Bs1,5 5.0 50.69 72.92 22.23 19.06 Bs1,5.5 5.5 49.76 64.76 15 20.42 Bs1,6 6.0 38.46 52.91 14.45 21.78

Bs4

Bs1.5,3

1.50

3.0 115.69 125.18 9.49 13.62 Bs1.5.3.5 3.5 103.31 116.10 12.79 14.98 Bs1.5,4 4.0 89.58 95.92 6.34 16.34 Bs1.5,4.5 4.5 79.58 82.21 2.63 17.70 Bs1.5,5 5.0 69.53 71.84 2.31 19.06 Bs1.5,5.5 5.5 62.52 65.93 3.41 20.42 Bs1.5,6 6.0 55.13 58.76 3.63 21.78

Bs2,3

3.0 147.69 160.54 12.85 13.62 Bs2,.3.5 3.5 123.98 135.31 11.33 14.98

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Bs5

Bs2,4 2.0

4.0 101.61 115.98 14.37 16.34 Bs2,4.5 4.5 95.75 112.66 16.91 17.70 Bs2,5 5.0 85.68 99.37 13.69 19.06 Bs2,5.5 5.5 76.81 95.03 18.22 20.42 Bs2,6 6.0 69.64 77.77 8.13 21.78

The comparison of values given by the proposed new equation with the actual

values of shear strength of HSC beams shows that the new equation of Zararis

gives very closer values for almost all level of longitudinal steel, except for

minimum longitudinal steel. The equations proposed are the best estimators of

the discussed methods.

The overall comparison of Vtest/VCode for ACI, CSA, MCFT, EC-02 and New

Equation for beams without web reinforcement has been shown in Table 8.16,

whereas the values for beams with web reinforcement have been shown in Table

8.17. The final comparison of Means, Standards deviations and Coefficient of

Variation of Vtest/VCode for ACI, CSA, MCFT, EC-02 have been shown in Table

8.18 and 8.19.

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Beam Title

ρ %

a/d Vtest/VCode.

ACI CSA MCFT ( LRFD)

EC-02 New Eq.

B1

B0.33,3

0.33

3 0.78 0.87 0.75 0.96 0.75 B0.33.3.5 3.5 0.67 0.75 0.64 0.82 0.64 B0.33,4 4 0.56 0.62 0.53 0.68 0.53 B0.33,4.5 4.5 0.53 0.59 0.51 0.65 0.51 B0.33,5 5 0.47 0.52 0.45 0.57 0.45 B0.33,5.5 5.5 0.42 0.47 0.40 0.51 0.40 B0.33,6 6 0.36 0.40 0.34 0.44 0.34

Mean 0.54 0.60 0.52 0.66 0.52 Stand Dev 0.28 0.150 0.13 0.166 0.130

CoV(%) 21.17 25.15 25.09 25.29 25.09 B2

B0.73,3

0.733

3 1.33 1.52 1.31 1.49 1.31 B0.73.3.5 3.5 1.23 1.41 1.21 1.38 1.21 B0.73,4 4 1.13 1.28 1.10 1.26 1.10 B0.73,4.5 4.5 1.02 1.16 1.00 1.14 1.00 B0.73,5 5 0.92 1.04 0.90 1.02 0.90 B0.33,5.5 5.5 0.81 0.92 0.79 0.90 0.79 B0.73,6 6 0.59 0.66 0.57 0.65 0.57

Mean 1.00 1.14 0.98 1.12 0.98 Stand dev 0.236 0.274 0.235 0.268 0.235 CoV 23.59 24.05 23.99 23.95 23.99 B3

B1,3

1.00

3 1.77 1.96 1.68 1.79 1.68 B1,3.5 3.5 1.52 1.69 1.45 1.54 1.45 B1,4 4 1.35 1.50 1.29 1.37 1.29 B1,4.5 4.5 1.29 1.42 1.22 1.30 1.22 B1,5 5 1.14 1.26 1.08 1.15 1.08 B1,5.5 5.5 1.12 1.23 1.06 1.13 1.06 B1,6 6 0.86 0.95 0.82 0.87 0.82

Mean 1.29 1.43 1.23 1.31 1.23 Stand Dev 0.273 0.305 0.26 0.278 0.260 CoV 21.19 21.35 21.15 21.17 21.15 B4

B1.5,3

1.50

3 2.40 2.87 2.43 2.33 2.43 B1.5.3.5 3.5 2.17 2.56 2.17 2.08 2.17 B1.5,4 4 1.89 2.22 1.88 1.81 1.88 B1.5,4.5 4.5 1.69 1.97 1.67 1.60 1.67 B1.5,5 5 1.49 1.73 1.46 1.40 1.46 B1.5,5.5 5.5 1.34 1.55 1.32 1.26 1.32 B1.5,6 6 1.19 1.37 1.16 1.11 1.16

Mean 1.74 2.04 1.73 1.66 1.73 Stand Dev 0.408 0.504 0.427 0.411 0.42

CoV 23.50 24.73 24.67 24.75 24.67 B5

B2,3

2.0

3 2.99 3.66 2.95 2.68 2.95 B2,.3.5 3.5 2.54 3.08 2.48 2.25 2.48 B2,4 4 2.11 2.52 2.03 1.84 2.03 B2,4.5 4.5 2.00 2.38 1.91 1.74 1.91 B2,5 5 1.81 2.13 1.71 1.56 1.71 B2,5.5 5.5 1.63 1.91 1.53 1.39 1.53 B2,6 6 1.48 1.73 1.39 1.26 1.41

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Table No. 8.16 Comparison of Vtest/VCode for ACI, CSA, MCFT, EC-02 and New Equation for beams without web reinforcement. Table No. 8.17 Comparison of Vtest/VCode for ACI, CSA, MCFT, EC-02 and New Equation for beams with web reinforcement.

Mean 2.08 2.49 2.00 1.82 2.00 Stand Dev 0.490 0.629 0.510 0.462 0.506

CoV 23.57 25.78 25.49 25.41 25.32

Beam Title

ρ %

a/d Vtest/VCode.

ACI CSA MCFT( LRFD) EC-02 New Eq.

Bs1

Bs0.33,3

0.33

3 0.75 0.71 0.60 0.75 0.73 Bs0.33.3.5 3.5 0.69 0.65 0.56 0.69 0.69 Bs0.33,4 4 0.60 0.56 0.48 0.59 0.68 B0.33,4.5 4.5 0.65 0.60 0.52 0.64 0.82 Bs0.33,5 5 0.60 0.55 0.47 0.59 0.79 Bs0.33,5.5 5.5 0.46 0.43 0.37 0.46 0.64 Bs0.33,6 6 0.41 0.38 0.33 0.41 0.67

Mean 0.59 0.55 0.48 0.59 0.72 Stand Dev 0.11 0.108 0.090 0.11 0.06 CoV 19.07 19.62 18.82 18.94 8.5 Bs2

Bs0.73,3

0.733

3 1.51 1.44 1.23 1.40 1.48 Bs0.73.3.5 3.5 1.44 1.36 1.17 1.33 1.46 Bs0.73,4 4 1.25 1.18 1.01 1.16 1.31 Bs0.73,4.5 4.5 1.16 1.10 0.94 1.08 1.27 Bs0.73,5 5 1.08 1.01 0.87 0.99 1.22 Bs0.33,5.5 5.5 0.99 0.93 0.80 0.91 1.17 Bs0.73,6 6 0.90 0.84 0.72 0.83 1.21

Mean 1.19 1.12 0.96 1.10 1.30 Stand Dev 0.20 0.20 0.17 0.19 0.11 CoV 17.56 18.19 18.09 17.78 8.74 Bs3

Bs1,3

1.00

3 1.81 1.68 1.44 1.56 1.69 Bs1,3.5 3.5 1.61 1.49 1.27 1.39 1.49 Bs1,4 4 1.49 1.38 1.18 1.29 1.43 Bs1,4.5 4.5 1.47 1.36 1.16 1.27 1.46 Bs1,5 5 1.38 1.28 1.10 1.19 1.43 Bs1,5.5 5.5 1.23 1.14 0.97 1.06 1.32 Bs1,6 6 1.00 0.93 0.79 0.87 1.12

Mean 1.43 1.32 1.13 1.23 1.42 Stand Dev 0.24 0.22 0.193 0.206 0.16 CoV 16.91 16.93 17.09 16.82 11.28 Bs4

Bs1.5,3

1.50

3 2.23 2.20 1.86 1.88 1.32 Bs1.5.3.5 3.5 2.09 2.04 1.73 1.74 1.31 Bs1.5,4 4 1.74 1.68 1.43 1.44 1.10 Bs1.5,4.5 4.5 1.50 1.44 1.22 1.23 1.05 Bs1.5,5 5 1.31 1.26 1.07 1.08 0.94 Bs1.5,5.5 5.5 1.21 1.16 0.98 0.99 0.93 Bs1.5,6 6 1.08 1.03 0.87 0.88 0.86

Mean 1.59 1.54 1.31 1.32 1.37 Stand Dev 0.409 0.41 0.35 0.35 0.34 CoV 25.75 26.86 26.78 26.75 24.98 Bs5

Bs2,3

2.0

3 2.80 2.82 2.30 2.22 1.85 Bs2,.3.5 3.5 2.39 2.37 1.94 1.87 1.60 Bs2,4 4 2.07 2.04 1.66 1.61 1.39 Bs2,4.5 4.5 2.02 1.98 1.62 1.56 1.45 Bs2,5 5 1.79 1.74 1.43 1.38 1.37 Bs2,5.5 5.5 1.72 1.67 1.36 1.32 1.34

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Table 8.18 Summary of means of the ratios of observed values and different code

values For shear strength of beams without web reinforcement

Statistical

Parameters Vtest/Vcode

ACI Canadian MCFT Eurocode New theory ρ = 0.33%

Mean 0.54 0.60 0.52 0.66 0.52 Stand Dev 0.28 0.150 0.13 0.166 0.130 CoV 21.17 25.15 25.09 25.29 25.09 ρ = 0.73%Mean 1.00 1.14 0.98 1.12 0.98 Stand Dev 0.236 0.274 0.235 0.268 0.235 CoV 23.59 24.05 23.99 23.95 23.99 ρ = 1%Mean 1.29 1.43 1.23 1.31 1.23 Stand Dev 0.273 0.305 0.26 0.278 0.260 CoV 21.19 21.35 21.15 21.17 21.15 ρ = 1.5% Mean 1.59 1.54 1.31 1.32 1.37 Stand Dev 0.409 0.41 0.35 0.35 0.34 CoV 25.75 26.86 26.78 26.75 24.98 ρ = 2% Mean 2.08 2.49 2.00 1.82 2.00 Stand Dev 0.490 0.629 0.510 0.462 0.506 CoV 23.57 25.78 25.49 25.41 25.32 Mean of Means 1.300 1.44 1.208 1.246 1.22

Table 8.19 Summary of means of the ratios of observed values and different code

values for shear Strength of beams with web reinforcement.

Statistical Parameters

Vtest/VcodeACI Canadian MCFT Eurocode New theory

ρ = 0.33%

Mean 0.59 0.55 0.48 0.59 0.72 Stand Dev 0.11 0.108 0.090 0.11 0.06 CoV 19.07 19.62 18.82 18.94 8.5 ρ = 0.73%Mean 1.19 1.12 0.96 1.10 1.30 Stand Dev 0.20 0.20 0.17 0.19 0.11 CoV 17.56 18.19 18.09 17.78 8.74 ρ = 1%Mean 1.43 1.32 1.13 1.23 1.42 Stand Dev 0.24 0.22 0.193 0.206 0.16 CoV 16.91 16.93 17.09 16.82 11.28 ρ = 1.5%Mean 1.59 1.54 1.31 1.32 1.37

Bs2,6 6 1.42 1.36 1.12 1.08 1.13 Mean 2.03 2.00 1.63 1.58 1.45 Stand Dev 0.42 0.45 0.36 0.35 0.21 CoV 20.82 22.34 22.23 22.09 14.41

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Stand Dev 0.409 0.41 0.35 0.35 0.34 CoV 25.75 26.86 26.78 26.75 24.98 ρ = 2% Mean 2.03 2.00 1.63 1.58 1.45 Stand Dev 0.42 0.45 0.36 0.35 0.21 CoV 20.82 22.34 22.23 22.09 14.41 Mean of Means 1.37 1.31 1.102 1.164 1.252

From the comparison of Vtest/Vcode given in tables 8.16 thru 8.19, the following

general comments can be made;

1. All the equation of various codes and methods discussed in the study are

not safe for the shear design of HSC beams for minimum longitudinal steel

ratio for both beams with and without web reinforcement.

2. For beams without web reinforcement, the corresponding values Vtest/Vcode

have increased for ρ=0.33% and 0.73% for all equations but these are still

un-conservative. Hence the equations given by most of the codes and

methods discussed are un-conservative for HSC beams with ρ<1% for both

the cases with and without web reinforcement.

3. The equations are giving reasonably good predictions of the shear strength

of HSC beams without web reinforcement for ρ = 1% and 1.5%.

4. For large values of ρ = 2%, all the equations are giving half of the actual test

values. Hence the equations considered are over conservative for ρ=2%.

5. The additions of stirrups have increased the shear strength of all HSC

beams, as generally given by the equations of shear design. But the

increase is random and irregular. The basic assumption of most of the

building codes and shear design equation for summing up the individual

contribution of concrete and stirrups has not been observed.

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6. The shear design of HSC beams at low level of longitudinal steel by all the

methods and equations considered need further work and verification of the

improvement of the equations.

7. The shear strength of HSC beams with web reinforcement is generally

considered as the sum of the individual contributions of the concrete and

web steel but in fact is more complicated phenomena as their roles are not

independent. The addition of web steel also affects the role of concrete

contribution and its capacity, as pointed out by Kani( 1964,1969) and

Kotsovos (1984,1989).

8. MCFT and New Equation proposed by Zararis,P.D give reasonably good

estimate of the HSC beams with web reinforcement.

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Chapter No.9

Statistical Model for the prediction of shear strength of

High Strength Concrete beams.

Chapter Introduction: In this chapter, efforts have been made to develop the non linear regression models for the shear strength of HSC beams based on the observed data. Coefficient of variation has been worked out for the observed values and predicted values by the proposed statistical model. These are also compared with the ACI models and some other models.

9.1 Regression model and its application in Civil Engineering.

In statistics, regression analysis is a collective name used for techniques and

methods to model and analyze the numerical data consisting of values of a

dependent variable (also called response variable or measurement) and of one

or more independent variables (also known as explanatory variables or

predictors). The dependent variable in the regression equation is modeled as a

function of the independent variables, corresponding parameters ("constants"),

and an error term. The error term is treated as a random variable. It represents

unexplained variation in the dependent variable. The parameters are estimated

so as to give a "best fit" of the data. Most commonly the best fit is evaluated by

using the least squares method, but other criteria have also been used.

Regression equation has been used extensively in Civil Engineering for

predicting the compressive strength and shear strength of RC members, besides

other engineering properties of concrete in the fresh and hardened form. Zain et

al (2006) developed a multiple regression model for predicting the compressive

strength of High Performance Concrete (HPC). The equation used the following

parameters for predicting the compressive strength of HPC at various ages of

concrete.

i. Mix proportioning of HPC, including the proportioning of cement, fly ash,

silica fumes, water, fine and coarse aggregates.

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ii. Slump test of the concrete in fresh form.

iii. Density of concrete.

They used their proposed model for the prediction of the compressive strength of

HPC, which gave a high correlation of 99%.

As already discussed in the literature review, Prodromos D.Zararis (2003) has

reported the following models for the shear strength of beams without web

reinforcement

Eq(2.46) bdf

d

cd

d

aV ctcr )()(2.02.1

The shear Strength of RC beams in complete form is as follows:

Eq (2.49) bdf

d

af

d

cd

d

ayvvct )25.05.0()..2.02.1 .

Karim et al (2000) proposed the following equation for prediction of ultimate shear

stress in beams without web reinforcement.

adfbd

Vc

uc /4.0 dA310 ( SI Units)

(9.4)

Where Ad = d

a for 1.0 < a/d<2.5 and 2.5 for a/d > 2.5

Guray Arsalan, used the Zsutty’s equation vvcc dba

dfV 3/12.2 for a/d ≥ 2

for multiple regression of the values of shear strength of RC beams and deduced

the following models;

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65.050.0 )(02.0)(15.0 ccc ff (For normal strength of concrete).

(9.5)

65.050.0 )(02.0)(15.0 ccc ff (For high strength concrete). (

9.6)

Razak and Wong ( 2004) used the data of 750 specimen of HPC and developed

a regression equation on the basis of best fit relationship between tensile

strength &compressive strength as well as stiffness & compressive strength of

HPC. They also reported that for HPC, the square root function recommended by

most of the codes for the tensile strength of HPC is not valid.

9.2 Regression equation for HSC beams without web reinforcement

The shear strength of HSC beams without stirrups has studied in this research

depends on three following parameters, studied in the experimental program;

Longitudinal steel ρ = bd

As expressed in percentage (%)

Shear span to depth ratio ( a/d)

Compressive strength of concrete; fc' ( Mpa)

Regression models have been developed on the basis of the test data of 70

beams, by using the trial version 9 of DtatFit software of Oakdale Engineering.

The following three models were tried for the shear stress in beams without web

reinforcement.

)/(' dacbaflc

(9.7)

ddacbaflc )/(

(9.8)

ddacbaflce

)/( (9.9)

The results generated for three model 1 has been given as follows;

Model1. )/( dacbaflc )/(208.067.50026.0 ' daf

lc

(9.10)

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Number of observations = 35 Number of missing observations = 0 Solver type: Nonlinear Nonlinear iteration limit = 250 Diverging nonlinear iteration limit =10 Number of nonlinear iterations performed = 11 Residual tolerance = 0.0000000001 Sum of Residuals = -3.20488143509065E-02 Average Residual = -9.15680410025899E-04 Residual Sum of Squares (Absolute) = 0.564293097380102 Residual Sum of Squares (Relative) = 0.564 Standard Error of the Estimate = 0.132793671886608 Coefficient of Multiple Determination (R^2) = 0.90 Proportion of Variance Explained = 90.4097492% Adjusted coefficient of multiple determination (Ra^2) = 0.8981035852 Durbin-Watson statistic = 0.448319312620612 Regression Variable Results: a = .026, b =50.678 , c= -0.208

The software has also generated the scatter diagram and proposed regression line passing through the data,

shown in Figure 9.1

Figure 9.1 Plot of the proposed model generated by the software.

Model 2 gdacbaflc )/( 765.0)/(204.032.480407.0 ' daf

lc

(9.11)

Solver type: Nonlinear Nonlinear iteration limit = 250 Diverging nonlinear iteration limit =12 Number of nonlinear iterations performed = 13 Residual tolerance = 0.0000000001 Sum of Residuals = -2.2048814350 E-02

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Average Residual = -9.1532410025899E-04 Residual Sum of Squares (Absolute) = 0.564293097380102 Residual Sum of Squares (Relative) = 0.664 Standard Error of the Estimate = 0.132793671886608 Coefficient of Multiple Determination (R^2) = 0.94 Proportion of Variance Explained = 90.4097492% Adjusted coefficient of multiple determination (Ra^2) = 0.8981035852 Durbin-Watson statistic = 0.448319312620612 Regression Variable Results: a = 0.0407, b =48.32 , c= -0.204 , g= -0.765

Model 3. 174.3)/(189.031.44065.0 ' daf

lce (9.12)

Solver type: Nonlinear Nonlinear iteration limit = 250 Diverging nonlinear iteration limit =12 Number of nonlinear iterations performed = 13 Residual tolerance = 0.0000000001 Sum of Residuals = -2.2048814350 E-02 Average Residual = -8.1532410025899E-04 Residual Sum of Squares (Absolute) = 0.564293097380102 Residual Sum of Squares (Relative) = 0.664 Standard Error of the Estimate = 0.132793671886608 Coefficient of Multiple Determination (R^2) = 0.94 Proportion of Variance Explained = 90.4097492% Adjusted coefficient of multiple determination (Ra^2) = 0.8981035852 Durbin-Watson statistic = 0.448319312620612 Regression Variable Results: a = 0.065, b =44.31 , c= -0.189 , d= -3.174

Table 9.1 Comparison of actual and predicated values of shear stress of High Strength concrete

beams without web reinforcement for three proposed models.

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The validity of the proposed model can be questioned on the basis of limited test

data and very few parameters considered in the model, however it is expected

that the initial work shall be further elaborated and new equations shall be

Beam Title fc΄

(MPa)

(ρ)

( %)

a/d Shear Stress

( MPa)

Absolute Residual

Actual Predicted Model 1

Model 2

Model 3

Model 1

Model 2

Model 3

B1

B0.33,3 50

0.33

3.00 0.95 0.84 0.82 0.74 0.09 0.13 0.21 B0.33.3. 50 3.50 0.88 0.74 0.72 0.67 0.03 0.16 0.21 B0.33,4 50 4.00 0.70 0.63 0.61 0.61 0.20 0.09 0.09 B0.33,4. 50 4.50 0.56 0.53 0.51 0.55 0.17 0.05 0.01 B0.33,5 50 5.00 0.48 0.43 0.41 0.50 0.14 0.07 0.02 B0.33,5. 50 5.50 0.41 0.32 0.31 0.46 0.11 0.10 0.05 B0.33,6 50 6.00 0.25 0.22 0.21 0.42 0.08 0.04 0.17

B2

B0.73,3 54

0.73

3.00 0.95 1.15 1.18 1.14 0.06 0.23 0.19 B0.73.3. 54 3.50 0.88 1.05 1.07 1.04 0.12 0.19 0.16 B0.73,4 54 4.00 0.80 0.94 0.97 0.95 0.19 0.17 0.15 B0.73,4. 54 4.50 0.73 0.84 0.87 0.86 0.12 0.14 0.13 B0.73,5 54 5.00 0.65 0.73 0.77 0.78 0.09 0.12 0.13 B0.33,5. 54 5.50 0.57 0.63 0.67 0.71 0.06 0.10 0.14 B0.73,6 54 6.00 0.41 0.53 0.56 0.65 0.04 0.15 0.24

B3

B1,3 50

1.00

3.00 0.99 1.18 1.14 0.99 0.00 0.15 0.00 B1,3.5 50 3.50 0.96 1.08 1.04 0.90 0.02 0.08 0.06 B1,4 50 4.00 0.88 0.97 0.94 0.82 0.29 0.06 0.06 B1,4.5 50 4.50 0.81 0.87 0.84 0.75 0.22 0.03 0.06 B1,5 50 5.00 0.73 0.77 0.73 0.68 0.26 0.00 0.05 B1,5.5 50 5.50 0.66 0.66 0.63 0.62 0.14 0.03 0.04 B1,6 50 6.00 0.58 0.56 0.53 0.56 0.16 0.05 0.02

B4

B1.5,3 55

1.50

3.00 1.86 1.57 1.59 1.72 0.12 0.27 0.14 B1.5.3.5 55 3.50 1.68 1.46 1.49 1.56 0.14 0.19 0.12 B1.5,4 55 4.00 1.62 1.36 1.38 1.42 0.09 0.24 0.20 B1.5,4.5 55 4.50 1.39 1.25 1.28 1.29 0.07 0.11 0.10 B1.5,5 55 5.00 1.31 1.15 1.18 1.18 0.01 0.13 0.13 B1.5,5.5 55 5.50 1.17 1.05 1.08 1.07 0.09 0.09 0.10 B1.5,6 55 6.00 1.08 0.94 0.98 0.97 0.12 0.10 0.11

B5

B2,3 53

2.00

3.00 1.68 1.77 1.75 1.88 0.09 0.07 0.20 B2,.3.5 53 3.50 1.59 1.66 1.65 1.71 0.06 0.06 0.12 B2,4 53 4.00 1.55 1.56 1.54 1.55 0.09 0.01 0.00 B2,4.5 53 4.50 1.37 1.46 1.44 1.41 0.03 0.07 0.04 B2,5 53 5.00 1.23 1.35 1.34 1.29 0.20 0.11 0.06 B2,5.5 53 5.50 1.16 1.25 1.24 1.17 0.17 0.08 0.01 B2,6 53 6.00 1.08 1.14 1.14 1.06 0.14 0.06 0.02

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developed by other graduate students at UET Taxila. This preliminary work will

pave way for further research in this direction. The comparison of the actual

values of shear stress and predicted values by the three proposed models has

shown in Table 9.1 for HSC beams without web reinforcement.

9.3 Regression Models for shear strength of beams with web reinforcement

The shear strength of the HSC beams with web reinforcement was additionally

assumed to depend on the transverse steel ratio. Hence the three models

worked out by the mentioned software are as follows;

)()/('vgdacbaf

lc

(9.13)

EDdacbaf vc l )()/(

(9.14)

EDdaCBAf vlce )()/( (9.15)

Out of the three models run by the software, first model gave somehow

reasonable values, as the coefficient of determination was very less for the

remaining two models ( R2< 50%) . The actual and predicted values have been

given in Table 9.2

)(64.7)/(256.059.00107.0

)()/('

'

v

v

daf

gdacbaf

lc

lc

(9.16)

Solver type: Nonlinear Nonlinear iteration limit = 250 Diverging nonlinear iteration limit =12 Number of nonlinear iterations performed = 13 Residual tolerance = 0.0000000001 Sum of Residuals = -2.2048814350 E-02 Average Residual = -8.1532410025899E-04 Residual Sum of Squares (Absolute) = 0.564293097380102 Residual Sum of Squares (Relative) = 0.664 Standard Error of the Estimate = 0.132793671886608 Coefficient of Multiple Determination (R^2) = 0.74 Proportion of Variance Explained = 74.4097492% Adjusted coefficient of multiple determination (Ra^2) = 0.7381 Durbin-Watson statistic = 0.448319312620612 Regression Variable Results: a = 0.0107, b =0.59 , c= -0.256 , g= 7.64

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Table: 9.2 Comparison of actual and predicted values of shear stress of High Strength

concrete beams with web reinforcement.

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9.4 Comparison of the proposed models with ACI-318 Code and other models:

Beam Title fc΄

(MPa)

(ρ)

(%)

(ρv)

(%)

a/d Shear Stress ( MPa) Residual details

Actual Predicted

Model 1

Absolute

Residual

Absolute

Residual % Bs1

Bs0.33,3 50

0.33

0.16

3.00 0.99 1.19 0.21 0.20

Bs0.33.3 50 3.50 0.88 1.06 0.21 0.18

Bs0.33,4 50 4.00 0.8 0.94 0.09 0.14

B0.33,4.5 50 4.50 0.73 0.80 0.01 0.07

Bs0.33,5 50 5.00 0.57 0.68 0.02 0.11

Bs0.33,5 50 5.50 0.46 0.55 0.05 0.09

Bs0.33,6 50 6.00 0.41 0.42 0.17 0.01

Bs2

Bs0.73,3 54

0.73

0.16

3.00 1.7 1.47 0.19 0.23

Bs0.73.3 54 3.50 1.38 1.34 0.16 0.04

Bs0.73,4 54 4.00 1.22 1.22 0.15 0.00

Bs0.73,4 54 4.50 1.06 1.09 0.13 0.03

Bs0.73,5 54 5.00 0.98 0.96 0.13 0.02

Bs0.33,5 54 5.50 0.82 0.83 0.14 0.01

Bs0.73,6 54 6.00 0.75 0.70 0.24 0.05

Bs3

Bs1,3 50

1.00

0.16

3.00 1.7 1.59 0.00 0.11

Bs1,3.5 50 3.50 1.54 1.46 0.06 0.08

Bs1,4 50 4.00 1.45 1.34 0.06 0.11

Bs1,4.5 50 4.50 1.39 1.20 0.06 0.19

Bs1,5 50 5.00 1.23 1.08 0.05 0.15

Bs1,5.5 50 5.50 1.07 0.95 0.04 0.12

Bs1,6 50 6.00 0.91 0.82 0.02 0.09

Bs4

Bs1.5,3 55

1.50

0.16

3.00 1.86 1.94 0.14 0.08

Bs1.5.3. 55 3.50 1.8 1.81 0.12 0.01

Bs1.5,4 55 4.00 1.71 1.68 0.20 0.03

Bs1.5,4. 55 4.50 1.6 1.55 0.10 0.05

Bs1.5,5 55 5.00 1.56 1.43 0.13 0.13

Bs1.5,5. 55 5.50 1.24 1.30 0.10 0.06

Bs1.5,6 55 6.00 1.08 1.17 0.11 0.09

Bs5

Bs2,3 53

2.00

0.16

3.00 2.19 2.21 0.20 0.02

Bs2,.3.5 53 3.50 1.94 2.09 0.12 0.15

Bs2,4 53 4.00 1.88 1.95 0.00 0.07

Bs2,4.5 53 4.50 1.8 1.83 0.04 0.03

Bs2,5 53 5.00 1.73 1.70 0.06 0.03

Bs2,5.5 53 5.50 1.57 1.57 0.01 0.00

Bs2,6 53 6.00 1.24 1.45 0.02 0.21

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9.4.1 Beams without shear reinforcement.

The ACI building Code is widely applied for the shear design of concrete. The

nominal shear capacity of reinforced concrete beam Vn, is given as the sum of

Concrete contribution Vc, and contributions of stirrups Vs .i.e. scn VVV

The shear stress of the beams was worked out with the ACI equation and other

models proposed by, Bazant and Kim (1984) and Russo et al.( 2004) have for

the tested beams. Regression equations were worked out for the shear stress of

HSC beams based on the test data. The actual shear stress and values given by

proposed model and other equations have been compared in Table 9.3 and

Figure 9.2

9.4.2 Beams with shear reinforcement.

For beams with web reinforcement, the proposed model for shear stress has

been compared with ACI equation and model proposed by G.Russo et al. (2004)

and shown Table 9.4 and Figure 9.3.

Table 9.3 Comparison of proposed model ACI equation and model proposed by G.Russo et al. (2004) for beams without web reinforcement.

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Beam Title

fc΄

(ρ) (%) a/d

Shear Stress ( MPa) ACI

Bazant et al

Russo G. et al Actual Predicted

B0.33,3 50

0.33

3.00 0.95 0.84 0.94 0.80 0.49 B0.33.3.5 50 3.50 0.88 0.74 0.94 0.77 0.46 B0.33,4 50 4.00 0.70 0.63 0.94 0.76 0.45 B0.33,4.5 50 4.50 0.56 0.53 0.94 0.75 0.43 B0.33,5 50 5.00 0.48 0.43 0.94 0.74 0.43 B0.33,5.5 50 5.50 0.41 0.32 0.94 0.73 0.42 B0.33,6 50 6.00 0.25 0.22 0.94 0.73 0.42 B0.73,3 54

0.73

3.00 0.95 1.15 0.98 1.14 0.80 B0.73.3.5 54 3.50 0.88 1.05 0.98 1.08 0.74 B0.73,4 54 4.00 0.80 0.94 0.98 1.05 0.70 B0.73,4.5 54 4.50 0.73 0.84 0.98 1.03 0.67 B0.73,5 54 5.00 0.65 0.73 0.98 1.01 0.66 B0.33,5.5 54 5.50 0.57 0.63 0.98 1.00 0.64 B0.73,6 54 6.00 0.41 0.53 0.98 0.99 0.63 B1,3 50

1.00

3.00 0.99 1.18 0.94 1.26 0.93 B1,3.5 50 3.50 0.96 1.08 0.94 1.18 0.85 B1,4 50 4.00 0.88 0.97 0.94 1.14 0.80 B1,4.5 50 4.50 0.81 0.87 0.94 1.11 0.76 B1,5 50 5.00 0.73 0.77 0.94 1.09 0.74 B1,5.5 50 5.50 0.66 0.66 0.94 1.08 0.73 B1,6 50 6.00 0.58 0.56 0.94 1.07 0.71 B1.5,3 55

1.50

3.00 1.86 1.57 0.99 1.55 1.24 B1.5.3.5 55 3.50 1.68 1.46 0.99 1.45 1.12 B1.5,4 55 4.00 1.62 1.36 0.99 1.39 1.04 B1.5,4.5 55 4.50 1.39 1.25 0.99 1.35 0.99 B1.5,5 55 5.00 1.31 1.15 0.99 1.32 0.96 B1.5,5.5 55 5.50 1.17 1.05 0.99 1.30 0.93 B1.5,6 55 6.00 1.08 0.94 0.99 1.29 0.91 B2,3 53

2.00

3.00 1.68 1.77 0.97 1.74 1.45 B2,.3.5 53 3.50 1.59 1.66 0.97 1.61 1.29 B2,4 53 4.00 1.55 1.56 0.97 1.53 1.20 B2,4.5 53 4.50 1.37 1.46 0.97 1.48 1.14 B2,5 53 5.00 1.23 1.35 0.97 1.44 1.09 B2,5.5 53 5.50 1.16 1.25 0.97 0.80 1.06 B2,6 53 6.00 1.08 1.14 0.97 0.77 1.04

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0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

3 3.50 4.00 4.50 5.00 5.5 6

Shea

r stre

ss o

f bea

m (M

Pa)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams without web reinforcement bypropsoed model and other models for ρ= 0.33% and fc'=50Mpa

Actual

Predicted

ACI

Bazant

Russo

Figure 9.2 (a) =0.33%

0

0.2

0.4

0.6

0.8

1

1.2

1.4

3 3.50 4.00 4.50 5.00 5.5 6

She

ar s

tress

of b

eam

(MP

a)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams without web reinforcement bypropsoed model and other models for

ρ= 0.73% and fc'=54Mpa

Actual

Predicted

ACI

Bazant

Russo

Figure 9.2 (b) =0.73%

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Figure 9.2 Comparison of actual values of shear stress with the predicted values by proposed regression model and other models for HSC beams without web reinforcement. Figure 9.2 Cont’d

0

0.2

0.4

0.6

0.8

1

1.2

1.4

3 3.50 4.00 4.50 5.00 5.5 6

Sh

ea

r str

ess

of b

ea

m (M

Pa

)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams without web reinforcement bypropsoed model and other models for ρ= 1%. and

fc'=50Mpa

Actual

Predicted

ACI

Bazant

Russo

Figure 9.2 (c) =1 %

0

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

2

3 3.50 4.00 4.50 5.00 5.5 6

Sh

ear s

tres

s o

f bea

m (M

Pa)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams without web reinforcement bypropsoed model and other models for

ρ= 1.5%. and fc'=55Mpa

Actual

Predicted

ACI

Bazant

Russo

Figure 9.2 (d) =1.5 %

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Figure 9.2 cont’d

0

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

2

3 3.50 4.00 4.50 5.00 5.5 6

She

ar s

tress

of b

eam

(Mpa

)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams without web reinforcement by propsed models and other models for

ρ= 2% and fc'=53Mpa

Actual

Predicted

ACI

Bazant

Russo

Figure 9.2 (e) =1.5 %

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Table9.4 Comparison of actual and predicted values of shear stress of High Strength

concrete beams having stirrups with the models proposed by ACI and Russo.

Beam fc΄ (ρ) a/d (ρV) ρVfy Shear Stress ACI Russo

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Title Mpa

( %) (%) ( MPa) G.et al Actual Predicted

1 2 3 4 5 6 7 8 9 10 Bs0.33,3 50 0.33 3.00 0.16 0.27 0.99 1.19 1.14 1.00

Bs0.33.3. 50 0.33 3.50 0.16 0.27 0.88 1.06 1.14 0.99

Bs0.33,4 50 0.33 4.00 0.16 0.27 0.8 0.94 1.14 0.99

B0.33,4.5 50 0.33 4.50 0.16 0.27 0.73 0.80 1.14 0.98

Bs0.33,5 50 0.33 5.00 0.16 0.27 0.57 0.68 1.14 0.98

Bs0.33,5. 50 0.33 5.50 0.16 0.27 0.46 0.55 1.14 0.98

Bs0.33,6 50 0.33 6.00 0.16 0.27 0.41 0.42 1.14 0.98

Bs0.73,3 54 0.73 3.00 0.16 0.27 1.7 1.47 1.18 1.36

Bs0.73.3. 54 0.73 3.50 0.16 0.27 1.38 1.34 1.18 1.31

Bs0.73,4 54 0.73 4.00 0.16 0.27 1.22 1.22 1.18 1.28

Bs0.73,4. 54 0.73 4.50 0.16 0.27 1.06 1.09 1.18 1.26

Bs0.73,5 54 0.73 5.00 0.16 0.27 0.98 0.96 1.18 1.26

Bs0.33,5. 54 0.73 5.50 0.16 0.27 0.82 0.83 1.18 1.25

Bs0.73,6 54 0.73 6.00 0.16 0.27 0.75 0.70 1.18 1.24

Bs1,3 50 1.0 3.0 0.16 0.27 1.7 1.59 1.14 1.50

Bs1,3.5 50 1.0 3.5 0.16 0.27 1.54 1.46 1.14 1.44

Bs1,4 50 1.0 4.0 0.16 0.27 1.45 1.34 1.14 1.40

Bs1,4.5 50 1.0 4.5 0.16 0.27 1.39 1.20 1.14 1.37

Bs1,5 50 1.0 5.0 0.16 0.27 1.23 1.08 1.14 1.36

Bs1,5.5 50 1.0 5.5 0.16 0.27 1.07 0.95 1.14 1.35

Bs1,6 50 1.0 6.0 0.16 0.27 0.91 0.82 1.14 1.34

Bs1.5,3 55 1.5 3.0 0.16 0.27 1.86 1.94 1.19 1.87

Bs1.5.3.5 55 1.5 3.5 0.16 0.27 1.8 1.81 1.19 1.76

Bs1.5,4 55 1.5 4.0 0.16 0.27 1.71 1.68 1.19 1.69

Bs1.5,4.5 55 1.5 4.5 0.16 0.27 1.6 1.55 1.19 1.64

Bs1.5,5 55 1.5 5.0 0.16 0.27 1.56 1.43 1.19 1.62

Bs1.5,5.5 55 1.5 5.5 0.16 0.27 1.24 1.30 1.19 1.60

Bs1.5,6 55 1.5 6.0 0.16 0.27 1.08 1.17 1.19 1.58

Bs2,3 53 2.0 3.0 0.16 0.27 2.19 2.21 1.17 2.12

Bs2,.3.5 53 2.0 3.5 0.16 0.27 1.94 2.09 1.17 1.96

Bs2,4 53 2.0 4.0 0.16 0.27 1.88 1.95 1.17 1.88

Bs2,4.5 53 2.0 4.5 0.16 0.27 1.8 1.83 1.17 1.82

Bs2,5 53 2.0 5.0 0.16 0.27 1.73 1.70 1.17 1.78

Bs2,5.5 53 2.0 5.5 0.16 0.27 1.57 1.57 1.17 1.75

Bs2,6 53 2.0 6.0 0.16 0.27 1.24 1.45 1.17 1.73

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0

0.2

0.4

0.6

0.8

1

1.2

1.4

3 3.50 4.00 4.50 5.00 5.5 6

Sh

ea

r str

ess

of

be

am

(Mp

a)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams with web reinforcement by propsed models and other models for

ρ= 0.33% and fc'=50Mpa

Actual

Predicted

ACI

Russo

Figure 9.3 (a) =0.33 %

0

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

3 3.50 4.00 4.50 5.00 5.5 6

Sh

ear s

tres

s o

f bea

m (M

pa)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams with web reinforcement by propsed models and other models for

ρ= 0.73% and fc'=50Mpa

Actual

Predicted

ACI

Russo

Figure 9.3 (b) =0.73 %

Figure 9.3 Comparison of actual shear stress of beams having stirrups with the proposed regression model and other models.

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Figure 9.3 cont’d

0

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

3 3.50 4.00 4.50 5.00 5.5 6

Sh

ear s

tres

s o

f bea

m (M

pa)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams with web reinforcement by propsed models and other models for

ρ= 1% and fc'=54Mpa

Actual

Predicted

ACI

Russo

Figure 9.3 (c) =1 %

0

0.5

1

1.5

2

2.5

3 3.50 4.00 4.50 5.00 5.5 6

Sh

ear s

tres

s o

f bea

m (M

Pa)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams with web reinforcement bypropsoed model and other models for ρ= 1.5% and fc'=55Mpa

Actual

Predicted

ACI

Russo

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Figure 9.3 (d) =1.5 %

Figure 9.3 cont’d

0

0.5

1

1.5

2

2.5

3 3.50 4.00 4.50 5.00 5.5 6

Sh

ea

r str

en

gth

of b

ea

m (M

pa

)

shear span to depth ratio a/d

Comparison of actual and predicted values of shear stress of beams without web reinforcement by propsed models and other models for ρ= 2% and

fc'=53Mpa

Actual

Predicted

ACI

Russo

Figure 9.3 (d) =2%

The ratios of actual values of shear stress and the values predicted by various

models have been compared and the coefficient of variation are given in Table

9.5 and Table 9.6 for beams with and without web reinforcement respectively.

The proposed model gives least CoV for beams without web reinforcement.

Whereas for HSC beams with web steel Russo Model gives minimum variation.

The coefficient of variation for keeping a/d constant and varying is given in

Table 9.7 and for keeping constant and a/d varying in Table 9.8. The

proposed model gives minimum variation for beams without web steel, whereas

for beams with web steel, Russo Model gives best prediction.

Beam

Title

%

a/d Shear Stress ( MPa)

ACI Bazant et al Russo

G. et al

test/pred test/ACI test/Bazan test/Rus

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Table 9.5 Comparison of test/pred by the proposed model and other models for beams without shear reinforcement ( 35 Nos). ( For constant steel ratio and variable a/d) Table 9.6 Comparison of test/pred by the proposed model and other models for beams with shear reinforcement ( 35 Nos) ( For constant steel ratio and variable a/d)

0.33

Actual Predicted

B0.33,3 3 0.95 0.84 0.94 0.80 0.49 1.13 1.01 1.19 1.94 B0.33.3.5 3.5 0.88 0.74 0.94 0.77 0.46 1.19 0.94 1.14 1.91 B0.33,4 4 0.70 0.63 0.94 0.76 0.45 1.11 0.74 0.92 1.56 B0.33,4.5 4.5 0.56 0.53 0.94 0.75 0.43 1.06 0.60 0.75 1.30 B0.33,5 5 0.48 0.43 0.94 0.74 0.43 1.12 0.51 0.65 1.12 B0.33,5.5 5.5 0.41 0.32 0.94 0.73 0.42 1.28 0.44 0.56 0.98 B0.33,6 6 0.25 0.22 0.94 0.73 0.42 1.14 0.27 0.34 0.60 B0.73,3

0.73

3 0.95 1.15 0.98 1.14 0.80 0.83 0.97 0.83 1.19 B0.73.3.5 3.5 0.88 1.05 0.98 1.08 0.74 0.84 0.90 0.81 1.19 B0.73,4 4 0.80 0.94 0.98 1.05 0.70 0.85 0.82 0.76 1.14 B0.73,4.5 4.5 0.73 0.84 0.98 1.03 0.67 0.87 0.74 0.71 1.09 B0.73,5 5 0.65 0.73 0.98 1.01 0.66 0.89 0.66 0.64 0.98 B0.33,5.5 5.5 0.57 0.63 0.98 1.00 0.64 0.90 0.58 0.57 0.89 B0.73,6 6 0.41 0.53 0.98 0.99 0.63 0.77 0.42 0.41 0.65 B1,3

1

3 0.99 1.18 0.94 1.26 0.93 0.84 1.05 0.79 1.06 B1,3.5 3.5 0.96 1.08 0.94 1.18 0.85 0.89 1.02 0.81 1.13 B1,4 4 0.88 0.97 0.94 1.14 0.80 0.91 0.94 0.77 1.10 B1,4.5 4.5 0.81 0.87 0.94 1.11 0.76 0.93 0.86 0.73 1.07 B1,5 5 0.73 0.77 0.94 1.09 0.74 0.95 0.78 0.67 0.99 B1,5.5 5.5 0.66 0.66 0.94 1.08 0.73 1.00 0.70 0.61 0.90 B1,6 6 0.58 0.56 0.94 1.07 0.71 1.04 0.62 0.54 0.82 B1.5,3

1.5

3 1.86 1.57 0.99 1.55 1.24 1.18 1.88 1.20 1.50 B1.5.3.5 3.5 1.68 1.46 0.99 1.45 1.12 1.15 1.70 1.16 1.50 B1.5,4 4 1.62 1.36 0.99 1.39 1.04 1.19 1.64 1.17 1.56 B1.5,4.5 4.5 1.39 1.25 0.99 1.35 0.99 1.11 1.40 1.03 1.40 B1.5,5 5 1.31 1.15 0.99 1.32 0.96 1.14 1.32 0.99 1.36 B1.5,5.5 5.5 1.17 1.05 0.99 1.30 0.93 1.11 1.18 0.90 1.26 B1.5,6 6 1.08 0.94 0.99 1.29 0.91 1.15 1.09 0.84 1.19 B2,3

2

3 1.68 1.77 0.97 1.74 1.45 0.95 1.73 0.97 1.16 B2,.3.5 3.5 1.59 1.66 0.97 1.61 1.29 0.96 1.64 0.99 1.23 B2,4 4 1.55 1.56 0.97 1.53 1.20 0.99 1.60 1.01 1.29 B2,4.5 4.5 1.37 1.46 0.97 1.48 1.14 0.94 1.41 0.93 1.20 B2,5 5 1.23 1.35 0.97 1.44 1.09 0.91 1.27 0.85 1.13 B2,5.5 5.5 1.16 1.25 0.97 0.80 1.06 0.93 1.20 1.45 1.09 B2,6 6 1.08 1.14 0.97 0.77 1.04 0.95 1.11 1.40 1.04

Mean 1.01 1.02 0.86 1.19

CoV 12.80% 40.09% 7.69% 24.2%

Beam Title

% a/d Shear Stress ( MPa)

ACI Russo G.et al

test/pred test/ACI test/Russo

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241

Table 9.7 Comparison of test/pred by the proposed model and other models for beams without shear reinforcement ( 35 Nos). ( For constant a/d and variable steel ratio)

Actual Predicted

Bs0.33,3

0.33

3 0.99 1.19 1.14 1.00 0.83 0.87 0.99 Bs0.33.3.5 3.5 0.88 1.06 1.14 0.99 0.83 0.77 0.89 Bs0.33,4 4 0.8 0.94 1.14 0.99 0.85 0.70 0.81 B0.33,4.5 4.5 0.73 0.80 1.14 0.98 0.91 0.64 0.74 Bs0.33,5 5 0.57 0.68 1.14 0.98 0.84 0.50 0.58 Bs0.33,5.5 5.5 0.46 0.55 1.14 0.98 0.84 0.40 0.47 Bs0.33,6 6 0.41 0.42 1.14 0.98 0.98 0.36 0.42 Bs0.73,3

0.73

3 1.7 1.47 1.18 1.36 1.16 1.44 1.25 Bs0.73.3.5 3.5 1.38 1.34 1.18 1.31 1.03 1.17 1.05 Bs0.73,4 4 1.22 1.22 1.18 1.28 1.00 1.03 0.95 Bs0.73,4.5 4.5 1.06 1.09 1.18 1.26 0.97 0.90 0.84 Bs0.73,5 5 0.98 0.96 1.18 1.26 1.02 0.83 0.78 Bs0.33,5.5 5.5 0.82 0.83 1.18 1.25 0.99 0.69 0.66 Bs0.73,6 6 0.75 0.70 1.18 1.24 1.07 0.64 0.60 Bs1,3

1

3 1.7 1.59 1.14 1.50 1.07 1.49 1.13 Bs1,3.5 3.5 1.54 1.46 1.14 1.44 1.05 1.35 1.07 Bs1,4 4 1.45 1.34 1.14 1.40 1.08 1.27 1.04 Bs1,4.5 4.5 1.39 1.20 1.14 1.37 1.16 1.22 1.01 Bs1,5 5 1.23 1.08 1.14 1.36 1.14 1.08 0.90 Bs1,5.5 5.5 1.07 0.95 1.14 1.35 1.13 0.94 0.79 Bs1,6 6 0.91 0.82 1.14 1.34 1.11 0.80 0.68 Bs1.5,3

1.5

3 1.86 1.94 1.19 1.87 0.96 1.56 0.99

Bs1.5.3.5 3.5 1.8 1.81 1.19 1.76 0.99 1.51 1.02

Bs1.5,4 4 1.71 1.68 1.19 1.69 1.02 1.44 1.01

Bs1.5,4.5 4.5 1.6 1.55 1.19 1.64 1.03 1.34 0.98 Bs1.5,5 5 1.56 1.43 1.19 1.62 1.09 1.31 0.96 Bs1.5,5.5 5.5 1.24 1.30 1.19 1.60 0.95 1.04 0.78 Bs1.5,6 6 1.08 1.17 1.19 1.58 0.92 0.91 0.68 Bs2,3

2

3 2.19 2.21 1.17 2.12 0.99 1.87 1.03 Bs2,.3.5 3.5 1.94 2.09 1.17 1.96 0.93 1.66 0.99 Bs2,4 4 1.88 1.95 1.17 1.88 0.96 1.61 1.00 Bs2,4.5 4.5 1.8 1.83 1.17 1.82 0.98 1.54 0.99 Bs2,5 5 1.73 1.70 1.17 1.78

1.02 1.48 0.97 Bs2,5.5 5.5 1.57 1.57 1.17 1.75 1.00 1.34 0.90 Bs2,6 6 1.24 1.45 1.17 1.73

0.86 1.06 0.72

Mean 0.99 1.11 0.88

CoV 9.60% 34.9% 4.07%

Beam

Title

a/d

% Shear Stress

( MPa) ACI Bazant

et al Russo G. et al

test/pred test/ACI test/Bazan test/Rus

Actual Predicted

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Table 9.8 Comparison of test/pred by the proposed model and other models for beams with shear reinforcement ( 35 Nos) ( For constant a/d and variable steel ratio)

B0.33,3

3

0.33 0.95 0.84 0.94 0.80 0.49 1.13 1.01 1.19 1.94

B0.73,3 0.73 0.95 1.15 0.98 1.14 0.80 0.83 0.97 0.83 1.19

B1,3 1 0.99 1.18 0.94 1.26 0.93 0.84 1.05 0.79 1.06

B1.5,3 1.5 1.86 1.57 0.99 1.55 1.24 1.18 1.88 1.20 1.50

B2,3 2 1.68 1.77 0.97 1.74 1.45 0.95 1.73 0.97 1.16

B0.33.3.5

3.5

0.33 0.88 0.74 0.94 0.77 0.46 1.19 0.94 1.14 1.91

B0.73,3.5 0.73 0.88 1.05 0.98 1.08 0.74 0.84 0.90 0.81 1.19

B1..3.5 1 0.96 1.08 0.94 1.18 0.85 0.89 1.02 0.81 1.13

B1,5,3.5 1.5 1.68 1.46 0.99 1.45 1.12 1.15 1.70 1.16 1.50

B2,.3.5 2 1.59 1.66 0.97 1.61 1.29 0.96 1.64 0.99 1.23

B0.33,4

4.0

0.33 0.70 0.63 0.94 0.76 0.45 1.11 0.74 0.92 1.56

B0.73,4 0.73 0.80 0.94 0.98 1.05 0.70 0.85 0.82 0.76 1.14

B1,4 1 0.88 0.97 0.94 1.14 0.80 0.91 0.94 0.77 1.10

B1.5,4 1.5 1.62 1.36 0.99 1.39 1.04 1.19 1.64 1.17 1.56

B2,4 2.0 1.55 1.56 0.97 1.53 1.20 0.99 1.60 1.01 1.29

B0.33,4.5

4.5

0.33 0.56 0.53 0.94 0.75 0.43 1.06 0.60 0.75 1.30

B0.73,4.5 0.73 0.73 0.84 0.98 1.03 0.67 0.87 0.74 0.71 1.09

B1,4.5 1 0.81 0.87 0.94 1.11 0.76 0.93 0.86 0.73 1.07

B1.5,4.5 1.5 1.39 1.25 0.99 1.35 0.99 1.11 1.40 1.03 1.40

B2,4.5 2.0 1.37 1.46 0.97 1.48 1.14 0.94 1.41 0.93 1.20

B0.33,5

5.0

0.33 0.41 0.32 0.94 0.73 0.42 1.28 0.44 0.56 0.98

B0.73,5 0.73 0.48 0.43 0.94 0.74 0.43 1.12 0.51 0.65 1.12

B1,5 1 0.73 0.77 0.94 1.09 0.74 0.95 0.78 0.67 0.99

B1,5.5 1.31 1.15 0.99 1.32 0.96 1.14 1.32 0.99 1.36 1.5

B2,5 2.0 1.23 1.35 0.97 1.44 1.09 0.91 1.27 0.85 1.13

B0.33,5.5

5.5

0.33 0.41 0.32 0.94 0.73 0.42 1.28 0.44 0.56 0.98

B0.73,5.5 0.73 0.57 0.63 0.98 1.00 0.64 0.90 0.58 0.57 0.89

B1,.5.5.5 1 0.66 0.66 0.94 1.08 0.73 1.00 0.70 0.61 0.90

B1.5,5.5 1.5 1.17 1.05 0.99 1.30 0.93 1.11 1.18 0.90 1.26

B2,,5.5 2 1.16 1.25 0.97 0.80 1.06 0.93 1.20 1.45 1.09

B0.33,6

6.0

0.33 0.25 0.22 0.94 0.73 0.42 1.14 0.27 0.34 0.60

B0.73,6 0.73 0.41 0.53 0.98 0.99 0.63 0.77 0.42 0.41 0.65

B1,6 1 0.58 0.56 0.94 1.07 0.71 1.04 0.62 0.54 0.82

B1.5,6 1.5 1.08 1.14 0.97 0.77 1.04 0.95 1.11 1.40 1.04

B2,6 2.0 1.08 0.94 0.99 1.29 0.91 1.15 1.09 0.84 1.19

Mean 1.01 1.01 0.86 1.19 CoV(%) 2.3 10.11 6.8 5.1

a/d Beam Title

% a

%/d

Shear Stress ( MPa)

ACI Russo G.et al

test/pred test/ACI test/Russo

Actual Predicted

Bs0.33,3 0.33 0.99 1.19 1.14

1.00 0.83 0.87 0.99

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9.5 Discussion on the proposed regression models.

The models proposed in the above arguments have inherent weaknesses of

limited data and few parameters. A polynomial regression model incorporating

more parameters can be developed on the basis of available test results on

Bs0.73,3

3

0.73 1.7 1.47 1.18

1.36 1.16 1.44 1.25 Bs1,3 1 1.7 1.59 1.1

41.50 1.07 1.49 1.13

Bs1.5,3 1.5 1.86 1.94 1.19

1.87 0.96 1.56 0.99 Bs2,.3.5 2 2.19 2.21 1.1

72.12 0.99 1.87 1.03

Bs0.33.3.5

3.5

0.33 0.88 1.06 1.14

0.99 0.83 0.77 0.89 Bs0.73.3.5 0.73 1.54 1.46 1.1

41.44 1.05 1.35 1.07

Bs1,3.5 1 1.54 1.46 1.14 1.44 1.05 1.35 1.07

Bs1.5.3.5 1.5 1.8 1.81 1.19

1.76 0.99 1.51 1.02 Bs2,3.5 2 1.94 2.09 1.17 1.96 0.93 1.66 0.99

Bs0.33,4

4.0

0.33 1.38 1.34 1.18

1.31 1.03 1.17 1.05 Bs0.73,4 0.73 1.22 1.22 1.18 1.28 1.00 1.03 0.95

Bs1,4 1 1.45 1.34 1.14

1.40 1.08 1.27 1.04 Bs1.5,4 1.5 1.71 1.68 1.19 1.69 1.02 1.44 1.01

Bs2,4 2.0 1.88 1.95 1.17 1.88 0.96 1.61 1.00

B0.33,4.5

4.5

0.33 0.73 0.80 1.14

0.98 0.91 0.64 0.74 Bs0.73,4.5 0.73 1.06 1.09 1.18 1.26 0.97 0.90 0.84

Bs1,4.5 1 1.45 1.34 1.14 1.40 1.08 1.27 1.04

Bs1.5,4.5 1.5 1.71 1.68 1.19 1.69 1.02 1.44 1.01

Bs2,4.5 2.0 1.8 1.83 1.17 1.82 0.98 1.54 0.99

Bs0.33,5

5.0

0.33 0.57 0.68 1.14

0.98 0.84 0.50 0.58 Bs0.73,5 0.73 0.98 0.96 1.18 1.26 1.02 0.83 0.78

Bs1,5 1 1.23 1.08 1.14 1.36 1.14 1.08 0.90

Bs1,5 1.5 1.56 1.43 1.19 1.62 1.09 1.31 0.96

Bs2,5 2.0 1.73 1.70 1.17 1.78 1.02 1.48 0.97

Bs0.33,5.5

5.5

0.33 0.55 1.14

0.98 0.84 0.40 0.47 0.46 Bs0.73,5.5 0.73 0.82 0.83 1.18 1.25 0.99 0.69 0.66

Bs1,5.5 1.0 1.07 0.95 1.14 1.35 1.13 0.94 0.79

Bs1.5,5.5 1.5 1.24 1.30 1.19 1.60 0.95 1.04 0.78

Bs1.5,5.5 2.0 1.57 1.57 1.17 1.75 1.00 1.34 0.90

Bs0.33,6

6.0

0.33 0.41 0.42 1.14

0.98 0.98 0.36 0.42 Bs0.73,6 0.73 0.75 0.70 1.18 1.24 1.07 0.64 0.60

Bs1,6 1 0.91 0.82 1.14 1.34 1.11 0.80 0.68

Bs1.5,6 1.5 1.08 1.17 1.19 1.58 0.92 0.91 0.68 Bs2,6 2.0 1.24 1.45 1.17 1.73 0.86 1.06 0.72

Mean 1.15 1.09 0.84

CoV 11% 12% 6%

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shear strength of HSC beams from the database in the future research work.

However the following results are derived from the above discussions.

i. ACI equation for shear strength of high strength concrete beams is

conservative for both the cases with and without web reinforcement.

ii. The proposed model for beams with web and without web reinforcement

has given less values of coefficient of variations as compared to ACI

equation and hence the models may better estimates the shear strength of

the beams for given range of compressive strength of concrete, than ACI

equation.

a. The Coefficient of variation of Bazant Model for beams without

shear reinforcement is less of all the models. Hence Bazant model

may better estimates the shear strength of beams without shear

reinforcement.

b. The Russo model for shear strength of beams with shear

reinforcement has given the least coefficient of variation as

compared to other equations. Hence the Russo model may better

estimate the shear strength of beams with shear reinforcement.

c. The proposed two non linear regression models with reasonable

coefficient of variation for both the cases can be further generalized

through experimental work.

d. For constant a/d and variable longitudinal steel ratio, the proposed

model gives the least coefficient of variation whereas for beams

with web steel, Russo Model gives least variation.

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e. For constant longitudinal steel ratio and variable a/d , the proposed

model gives least variation for beams without web steel and Russo

model best predict the shear stress of HSC beams tested for

beams with web steel

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Chapter No.10

Conclusions and recommendations

Chapter Introduction: The chapter at last but not the least gives the conclusions and results of the research findings and venues for future research have been identified. This will surely help the researchers of the new generations to explore more realistic and accurate models for the shear design of high strength concrete structures.

Conclusions

On the basis of testing of 70 HSC-RC beams for five values of longitudinal steel

and seven values of shear span to depth ratio, the following specific conclusions

are drawn. 1. The failure in most of the beams has been caused due to diagonal tension

cracking; however it was more dominant failure mode for beams without web

reinforcement and having ρ≥1%. For beams with ρ<1%, flexural shear failure

was obvious failure mode.

2. For beams without web reinforcement and having large values of longitudinal

steel (ρ=1% and 1.5%), the shear failure is more brittle and sudden, giving

no sufficient warning.

3. The HSC beams with web reinforcement, the failure has been caused mainly

by diagonal tension shear cracking even for small longitudinal steel ratio,

instead.

4. The shear strength of all the beams has been increased for all values of

longitudinal steel and “a/d” ratio with the addition of stirrups, but in a very

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random manner. Hence uniform increase in shear strength of beams as

given in most of the Codes was not observed. This increase is more

prominent at lower steel ratios.

5. The addition of web reinforcement has avoided the brittle failure of the beam

at higher values of longitudinal steel and the ductility of beams has increased.

6. The shear strength of the HSC beams has been increased with the increases

of longitudinal steel in both the caes without and with web reinforcement. This

increase is relatively more in case of beams with web reinforcement.

7. For both types of beams, the shear strength of HSC beams has been

decreased with the increase of a/d ratio. However this decrease is relatively

more in the beams without web reinforcement.

8. The shear equation of ACI-318, Canadian Code (CSA), EuroCode (EC-02) ,

LRFD( MCFT) studied in this research are less give the shear strength more

than the actual test values for beams with ρ<1.0 and hence these are not

safe. But these equation are reasonably good predictor of shear strength of

beams for ρ= 1% and 1.5%. However for ρ=2%, most of the equations are

over conservativ.

9. Modified Compression Field Theory (MCFT) and new Equation proposed by

Zararis (2003) gave reasonably good estimates of the HSC beams with web

reinforcement.

10. The models proposed in the research have inherent weaknesses of limited

data and few parameters. However the proposed model estimates the shear

strength of HSC beams with and without web reinforcement better than ACI-

318 equation.

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11. Bazant model better estimates the shear strength of beams without shear

reinforcement and Russo model may better estimate the shear strength of

beams with shear reinforcement.

Conclusions on the work in disturbed region

1. For design of two HSC corbels, Strut and Tie Model used in the study gives

reasonable prediction of the shear strength of corbels.

2. The variation in actual and theoretical values of strut angles and shear

strength is less for HSC corbels.

3. The shear failure of HSC two way corbels is sudden and brittle as in case of

HSC beams without web reinforcement, due to loss in the aggregates

interlocking and failure of the HSC corbles long smooth plane.

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Recommendations for future work

1. The International building and bridges codes provisions for shear

strength of HSRC beams needs to be rationalized further particularly for

the cases where shear span to depth ratio is more than 5 and

Compressive strength of concrete is 70 Mpa or more.

2. Most of the equations given in the Building and Bridges Codes for shear

design of HSC beam having ρ≤1% are less conservative and further

research is required to work out the reduction factor as function of

concrete compressive strength.

3. Further research is required to generalize the Strut and Tie Model for

typical disturbed region in concrete structures like deep beams, pile caps,

dapped ended beams and corbels. This will require extensive

experimental evidence before generalizing the model.

4. It is proposed that a research group may be developed at the Department

of Civil Engineering, University of Engineering and Technology-Taxila,

Pakistan represented by researchers from the faculty and field to work

further on the shear design of disturbed region in reinforced concrete as

part of graduates research.

5. Graduate level research is required to develop polynomial regression

models on the basis of shear database of HSRC beams, which can be

tested and later adopted with more validity and reliability.

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Appendix-A: Design of two way corbel using Strut and Tie Model ( STM)

The step by step approach given at the website of Strut and Tie Resources (2005) was

used for the design of two way cobles as follows;

1. Geometry of the two way corbels

The geometry of the proposed two way corbel has been shown in Figure A-1

Figure A-1 : geometry of Two way corbel.

2 Design of two way corbels.

The corbels were designed against an assumed external load of 160 kips and the

following design steps were adopted using STM as per ACI-318-06.

2.1 Determine the bearing plate dimension:

Bearing plate measuring 9inx 6in is selected to transfer the load evenly to the corbel

projection, the bearing area of plate is 54 in2 .The corbel is designed to carry a load of

80Kips at each end.

The bearing stress = 80x1000/54 = 1481 psi

Thus the allowed limits of the bearing stress = φ ( 0.85ßn fc′ ) =

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C C'

B B'

A A'

= 0.75 x 0.85x 0.80x 4.76 = 2427 psi

The bearing stress of 1481 psi is less than the allowed 2427 psi and Ok

2.2 Choosing the Corbel dimension:

The depth of column face is 9 in ACI requires that the depth outside the bearing must be

at least half of the depth of column. In our case the load is applied at 4.5 in from the face

of corbel which is half the column dimension. Hence the minimum requirements are

fulfilled.

2.3 Establish Strut and Tie Model.

The geometry of assumed truss is shown in Figure A-2. The centre of the tie is assumed

to be 2 in below the top of the corbel. Hence d = 18-2 = 16 in. The horizontal strut BB’ is

assumed to lie in the horizontal line at the corbel column joint.

Figure A-2 Geometry of assumed Strut and Tie Model ( STM)

The location of strut CB centerline can be found by calculating the required compressive

force in strut CB, NCB, and the strut stress limit to obtain the strut width a. The strut CB

force is

NCB = 80 kips

The limit stress on the nodal zone B (also strut CB) is

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Here is strength reduction factor =0.75

n ; Capacity reduction factor of struts =0.85 for straight type nodes

cuf = 0.75 x (0.85 x 1 x 5,600) = 3.03 ksi

Thus, we have

bf

Na

cu

CB

= 80 / (0.75 x 3.03 x 9) = 2.93 in

This fixes the geometry of the truss and means that member AB has a horizontal

projection of 4.5 + 2.93 / 2 = 4.97 in.

2.4 Determine truss member forces:

The forces in all the members of the truss are given in Table A-1. The positive sign

indicates tension, negative compression. The finally analyzed truss is given in Figure A-

3.

Table A-1 Forces in Truss of double corbel after analysis.

Member AA' AB BB' BC

Force (kips) 29.84 -85.38 -80 -29.84

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A A '

B

C

B '

C '

V u = 8 0 k ip s V u = 8 0 k ip s

85.3

8 ki

ps

85.3

8 ki

ps

80 k

ips

2 9 . 8 4 k ip s

80 k

ips

8 0 k ip s8 0 k ip s

2 9 . 8 4 k ip s

Figure A-3 Member Force in strut and Tie model for two way corbel.

2.5 Design of Tie.

The area of reinforcement required for tie AA’ is y

AArequired f

NAs

= 29.84 / (.75 x 40,000)

=0.995 in2

And the minimum area of reinforcement is

=0.04 x 5,600/40,000 x (9 x 16)

Choose 5 # 4 bars,

As Provided = 5 x 0.2 =1 in

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2.6 Check the struts capacity

The struts will be checked by computing the strut widths and checked whether they will

fit in the space available.

The stress of the diagonal strut AB is limited to

= 0.75 x (0.85 x 0.75 x 5,600)

= 2.27 ksi

Hence, the required width for strut AB is

bf

Na

cu

AB

= = 85.38 / (0.75 x 2.27 x 9) == 4.18 in

The stress of the vertical struts CB and horizontal strut BB’ is limited to

= 0.75 x (0.85 x 1 x 5600)

= 3.03 ksi.

Hence, the required widths for strut BB’ is bf

Na

cu

BB

= 80 / (0.75 x 3.03 x 9) =

= 1 .09 in

The required width for strut CB is equal to a, i.e. 2.93 in.

As shown in Figure A-3, all the strut widths fit into the outline of the corbel region. Thus,

this solution is accepted.

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2.8 Design of Nodal zone and check for anchorages.

The width (a) of nodal zone A was chosen to satisfy the stress limits on the nodal zone.

To satisfy the nodal zone stress limit, the tie reinforcement must engage an effective

depth of concrete at least equal to

= ( 29.83 x 1000) / (0.75 x 0.85 x 0.8 x 5600 x 9)

= 1.16 in

This limit is easily satisfied since the nodal zone available is 2.93 in.

The required anchorage length for tie AA’ is

= 0.7 x 1200 x 0.5)/5600

= 5.613 in

Since this is less than the available length, i.e. 9 – 1.5 – 1/2 = 7 in., the anchorage length

is adequate. The final reinforcement has been given in Figure A-4

Figure A-4 Reinforcement details of two way corbel designed for 80 Kips (355KN) load

by STM.