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    European Union Brite EuRam III

    Structural and economic

    comparison of bridges made

    of inverted T-beams

    with topping

    EuroLightCon

    Economic Design and Construction with

    Light Weight Aggregate Concrete

    Document BE96-3942/R33, June 2000

    Project funded by the European Union

    under the Industrial & Materials Technologies Programme (Brite-EuRamIII)

    Contract BRPR-CT97-0381, Project BE96-3942

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    The European Union Brite EuRam III

    Structural and economic comparison of

    bridges made of inverted T-beams with topping

    EuroLightCon

    Economic Design and Construction with

    Light Weight Aggregate Concrete

    Document BE96-3942/R33, June 2000Contract BRPR-CT97-0381, Project BE96-3942

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    Although the project consortium does its best to ensure that any information given is accurate, no liability or responsi-

    bility of any kind (including liability for negligence) is accepted in this respect by the project consortium, the au-

    thors/editors and those who contributed to the report.

    Acknowledgements

    This report is written by: Aleksandar Milenkovic (Spanbeton bv / CZ Civiele Techniek bv) and M.R. Trouw (Spanbeton

    bv). The illustrations are made by C. v/d Ploeg (Spanbeton bv)

    Information

    Information regarding the report:

    Spanbeton bv., Hoogewaard 209, 2396 AS Koudekerk aan den Rijn, The Netherlands;

    Tel: +31 (0)71 3419115; E-mail [email protected]

    Information regarding the project in general:

    Jan P.G. Mijnsbergen, CUR, PO Box 420, NL-2800 AK Gouda, the Netherlands

    Tel: +31 182 540620, Email: [email protected]

    Information on the project and the partners on the internet:: http://www.sintef.no/bygg/sement/elcon

    ISBN 90 376 02 68 1

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    The European Union Brite EuRam III

    Structural and economic comparison of

    bridges made of inverted T-beams with topping

    EuroLightCon

    Economic Design and Construction with

    Light Weight Aggregate Concrete

    Document BE96-3942/R33, June 2000

    Contract BRPR-CT97-0381, Project BE96-3942

    Selmer ASA, NO

    SINTEF, the Foundation for Scientific and Industrial Research at theNorwegian Institute of Technology, NO

    NTNU, University of Technology and Science, NO

    ExClay International, NO

    Beton Son B.V., NL

    B.V. VASIM, NL

    CUR, Centre for Civil Engineering Research and Codes, NL

    Smals B.V., NL

    Delft University of Technology, NL

    IceConsult, Lnuhnnun hf., IS

    The Icelandic Building Research Institute, ISTaywood Engineering Limited, GB

    Lias-Franken Leichtbaustoffe GmbH & Co KG, DE

    Dragados y Construcciones S.A., ES

    Eindhoven University of Technology, NL

    Spanbeton B.V., NL

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    BE96-3942 EuroLightCon 5

    Table of Contents

    PREFACE 7

    SUMMARY 10

    SYMBOLS 11

    1. INTRODUCTION 17

    2. GENERAL 20

    2.1 Standards and starting points 20

    2.2 Materials 20

    2.3 Geometry 212.4 Loads 25

    2.4.1 Permanent loads 25

    2.4.2 Live loads 26

    2.4.3 Loads combinations 29

    2.5 Computer programs 30

    2.5.1 Theory of shear force calculation 30

    2.5.2 The Spreid program 32

    2.5.3 The Span program 33

    2.6 Superstructure calculation 33

    2.6.1 Data obtained from computer programs 33

    2.6.2 Beam 35

    2.6.3 Topping 39

    2.6.4 Composite structure 41

    2.7 Substructure 48

    3. COMPARISON 50

    3.1 Quantities 50

    3.1.1 Bridge with a span of 20 m 50

    3.1.2 Bridge with a span of 30 m 51

    3.1.3 Bridge with a span of 40 m 51

    3.2 Costs per quantity 52

    3.3 Project costs 53

    3.3.1 Bridge with a span of 20 m 53

    3.3.2 Bridge with a span of 30 m 54

    3.3.3 Bridge with a span of 40 m 54

    4. CONCLUSIONS 55

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    APPENDIX: MIXTURE COMPOSITION 56

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    PREFACEThe lower density and higher insulating capacity are the most obvious characteristics of Light-

    Weight Aggregate Concrete (LWAC) by which it distinguishes itself from ordinary Normal

    Weight Concrete (NWC). However, these are by no means the only characteristics, which jus-

    tify the increasing attention for this (construction) material. If that were the case most of the

    design, production and execution rules would apply for LWAC as for normal weight concrete,

    without any amendments.

    LightWeight Aggregate (LWA) and LightWeight Aggregate Concrete are not new materials.

    LWAC has been known since the early days of the Roman Empire: both the Colosseum and thePantheon were partly constructed with materials that can be characterised as lightweight aggre-

    gate concrete (aggregates of crushed lava, crushed brick and pumice). In the United States, over

    100 World War II ships were built in LWAC, ranging in capacity from 3000 to 140000 tons and

    their successful performance led, at that time, to an extended use of structural LWAC in build-

    ings and bridges.

    It is the objective of the EuroLightCon-project to develop a reliable and cost effective design and

    construction methodology for structural concrete with LWA. The project addresses LWA manu-

    factured from geological sources (clay, pumice etc.) as well as from waste/secondary materials

    (fly-ash etc.). The methodology shall enable the European concrete and construction industry toenhance its capabilities in terms of cost-effective and environmentally friendly construction,

    combining the building of lightweight structures with the utilisation of secondary aggregate

    sources.

    The major research tasks are:

    L igh tweight aggregates: The identification and evaluation of new and unexploited sources spe-

    cifically addressing the environmental issue by utilising alternative materials from waste. Further

    the development of more generally applicable classification and quality assurance systems for

    aggregates and aggregate production.

    L ightweight aggregate concrete production: The development of a mix design methodology toaccount for all relevant materials and concrete production and in-use properties. This will include

    assessment of test methods and quality assurance for production.

    L ightweight aggregate concrete properties: The establishing of basic materials relations, the

    influence of materials characteristics on mechanical properties and durability.

    L ightweight aggregate concrete structur es: The development of design criteria and -rules

    with special emphasis on high performance structures. The identification of new areas for appli-

    cation.

    The project is being carried out in five technical tasks and a task for co-ordination/management

    and dissemination and exploitation. The objectives of all technical tasks are summarised below.

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    Starting point of the project, the project baseline, are the results of international research work

    combined with the experience of the partners in the project whilst using LWAC. This subject is

    dealt with in the first task.

    Tasks 2-5 address the respective research tasks as mentioned above: the LWA itself, production

    of LWAC, properties of LWAC and LWAC structures.

    Sixteen partners from six European countries, representing aggregate manufacturers and suppli-

    ers, contractors, consultants research organisations and universities are involved in the Eu-

    roLightCon-project. In addition, the project established co-operation with national clusters and

    European working groups on guidelines and standards to increase the benefit, dissemination and

    exploitation.

    At the time the project is being performed, a Working Group under the international concrete

    association fib(the former CEB and FIP) is preparing an addendum to the CEB-FIP Model

    Code 1990, to make the Model Code applicable for LWAC. Basis for this work is a state-of-the-

    art report referring mainly to European and North-American Standards and Codes. Partners in

    the project are also active in the fibWorking Group.

    General information on the EuroLightCon-project, including links to the individual project part-

    ners, is available through the web site of the project:

    http://www.sintef.no/bygg/sement/elcon/

    At the time of publication of this report, following EuroLightCon-reports have been published:

    R1 Definitions and International Consensus Report. April 1998

    R1a LightWeight Aggregates Datasheets. Update September 1998

    R2 LWAC Material Properties State-of-the-Art. December 1998

    R3 Chloride penetration into concrete with lightweight aggregates. March 1999

    R4 Methods for testing fresh lightweight aggregate concrete, December 1999

    R5 A rational mix design method for lightweight aggregate concrete using typical UK mate-

    rials, January 2000

    R6 Properties of Lytag-based concrete mixtures strength class B15-B55, January 2000

    R7 Grading and composition of the aggregate, March 2000

    R8 Properties of lightweight concretes containing Lytag and Liapor, March 2000

    R9 Technical and economic mixture optimisation of high strength lightweight aggregate con-

    crete, March 2000

    R10 Paste optimisation based on flow properties and compressive strength, March 2000

    R11 Pumping of LWAC based on expanded clay in Europe, March 2000

    R12 Applicability of the particle-matrix model to LWAC, March 2000

    R13 Large-scale chloride penetration test on LWAC-beams exposed to thermal and hygral

    cycles, March 2000

    R14 Structural LWAC. Specification and guideline for materials and production, June 200

    R15 Light Weight Aggregates, June 200

    R16 In-situ tests on existing lightweight aggregate concrete structures, June 200

    R17 Properties of LWAC made with natural lightweight aggregates, June 2000

    R18 Durability of LWAC made with natural lightweight aggregates, June 2000

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    R19 Evaluation of the early age cracking of lightweight aggregate concrete, June 2000

    R20 The effect of the moisture history on the water absorption of lightweight aggregates,

    June 2000

    R21 Stability and pumpability of lightweight aggregate concrete. Test methods, June 2000

    R22 The economic potential of lightweight aggregate concrete in c.i.p. concrete bridges, June

    2000

    R23 Mechanical properties of lightweight aggregate concrete, June 2000

    R24 Prefabricated bridges, June 2000

    R25 Chemical stability, wear resistance and freeze-thaw resistance of lightweight aggregate

    concrete, June 2000

    R26 Recycling lightweight aggregate concrete, June 2000

    R27 Mechanical properties of LWAC compared with both NWC and HSC, June 2000

    R28 Prestressed beams loaded with shear force and/or torsional moment, June 2000

    R29 A prestressed steel-LWAconcrete bridge system under fatigue loading

    R30 Creep properties of LWAC, June 2000

    R31 Long-term effects in LWAC: Strength under sustained loading; Shrinkage of High

    Strength LWAC, June 2000

    R32 Tensile strength as design parameter, June 2000

    R33 Structural and economical comparison of bridges made of inverted T-beams with top-

    ping, June 2000

    R34 Fatigue of normal weight concrete and lightweight concrete, June 2000

    R35 Composite models for short- and long-term strength and deformation properties of

    LWAC, June 2000

    R36 High strength LWAC in construction elements, June 2000

    R37 Comparison of bridges made of NWC and LWAC. Part 1: Steel concrete composite

    bridges, June 2000

    R38 Comparing high strength LWAC and HSC with the aid of a computer model, June 2000

    R39 Proposal for a Recommendation on design rules for high strength LWAC, June 2000

    R40 Comparison of bridges made of NWC and LWAC. Part 2: Bridges made of box beams

    post-tensioned in transversal direction, June 2000

    R41 LWA concrete under fatigue loading. A literature survey and a number of conducted

    fatigue tests, June 2000

    R42 The shear capacity of prestressed beams, June 2000

    R43 A prestressed steel-LWA concrete bridge system under fatigue loading, June 2000

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    SUMMARYLightweight aggregate concrete (LWAC) contains certain properties that could be of influence

    upon the total project costs. A possible negative influence can be found in the higher material

    costs of LWAC compared to the material costs of NDC, while a possible positive influence can

    be found in the lower density, which can reduce the sub-, superstructure-, transport- and assem-

    bling costs.

    To find the influence of the application of LWAC (instead of NDC) on the total project costs,

    this research is done with two variable factors: the change in application of LWAC in the beam

    and topping, and the change in bridge span (20m, 30m and 40m).

    The height of the beams is chosen in relation with the span of the bridge. To comply to fatigueregulations, the beam and the topping height are further assumed variable.

    The width of the bridge is 18m, realised by 15 inverted T-beams with a structural topping of 210

    mm.

    The calculations are based on two regulations used for bridge calculations:

    The Dutch standard V.B.C. 1995, calculation methods and structural demands for concreteapplication.

    The Dutch standard V.B.B. 1995, calculation methods and structural demands for bridges

    The load spreading calculation of the bridge is based on the theory of Guyon and Massonnet.

    The bending and torsional moments of inertia, in both directions, are based on the theory of elas-

    ticity.

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    SYMBOLSGreek symbols

    torsion factor used in loads spreading calculationangle for shear calculations.

    factor used in fatigue calculationf loading factorm material factorsd safety factor for calculating design values fictive height, used in the theory of Timoshenko for stiffness calculation

    max maximal shrinkage value dependent on the fckand the relative humidityc basic shrinkage dependent on the relative humidityrtopping representative creep value of the toppingrbeam representative creep value of the beam stiffness factor used in the loads spreading calculation ratio of bond strength of pre-stressing steel and high bond reinforcing steel. Poissons ratio density of the concrete [kg/m3]perm stress due to permanent loadss representative tensile stress in the reinforcement

    bmd mean compressive stress due to the normal force with inclusion of thepre-stress load of Nd / Ab

    s;107;rep representative value of the fatigue limit of the reinforcement at 107 cycless;n;rep representative value of the fatigue limit of the reinforcementc;max maximum compressive stress at a fibre under the frequent combinations of

    actions

    s;d;max design value of the tensile stress of the reinforcements;d;min minimal design value of the tensile strength in the reinforcements;u(n) ultimate tensile stress in the reinforcement at n cycles

    b;90 compressive stress at 90 mm from the bottom of the beamtemp representative stress at the bottom caused by temperature influences1 limit value of the shear stress without shear reinforcement2 limit value of the shear stress with shear reinforcementd design value of the shear stressn part of the normal force in the shear capacityn+1 limit value of the shear stress without shear reinforcement with inclusion of

    the pre-stress force

    red reduced d due to the vertical component of the pre-stress steel forcebeam calculated creep factor of the beam

    topping calculated creep factor of the topping

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    max maximal creep values diameter of reinforcementkm diameter of the top reinforcementof the topping

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    Latin lower case symbols

    a half of the theoretical span of the bridge

    b half of the effective width of the bridge

    b half of the real width of the bridge

    b1 fictive width of the topping (part 1) used in the theory of Timoshenko

    b2 fictive width of the web (part 2) used in the theory of Timoshenko

    b3 fictive width of the flange (part 3) used in the theory of Timoshenko

    bt real width of the topping

    bw width of the web

    c coverage of the reinforcement, dependent on the environment classification

    ctop coverage of the top reinforcement of the topping

    dbeam useful height of the beam

    dend distance between the centre of gravity of the reinforcement and the bottom

    of the beam in the end section.

    dmiddle distance between the centre of gravity of the reinforcement and the bottom

    of the beam in the middle section.

    fb design value of the compressive strength of the concrete

    fbuv(n) see Su(n)

    fck characteristic compressive strength of the concrete

    fb design value of the tensile strength of the concrete

    fbrep representative value of the tensile strength of the concrete

    fs design value of the tensile strength of the reinforcement

    h construction height

    hf height of the flange

    hm fictive thickness of the section

    ht height of the topping

    hw height of the web

    i moment of inertia in longitudinal direction

    io torsion moment of inertia in longitudinal direction

    j moment of inertia in transversal direction

    jo torsion moment of inertia in transversal direction

    k1, k2, k3 cracking factors

    kb shrinkage factor dependent on the factor fck

    kc creep factor dependent on the relative humidity

    kd creep factor dependent on the age of the concrete

    kh shrinkage factor dependent on (hm).

    kp shrinkage factor dependent on the amount of reinforcement

    kt shrinkage factor dependent on the age of the concrete

    l1 spacing between the two considered beams

    m factor dependent ofs;107;repn number of load cycles

    n1 number of beams

    pd design value of the equally divided live load

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    prep representative value of the equally divided live load

    qd design value of the line load

    qrep representative value of the line load

    s spacing of the reinforcement bars in the cracking calculation

    wb the fictive width of the topping used in the calculation of i

    x the deformation of the beam due to the pre-stress force

    xu height of the compressive zone in the cross section

    y the deformation of the beam due to the self weight of the beam and topping

    and the permanent loads

    z internal distance between the compressive force and the tensile force

    zb distance between centre of gravity and the top of the beam.

    zo distance between centre of gravity and the bottom of the beam.

    Latin upper case symbols

    Abot bottomreinforcement of the topping

    Ac cross-section surface of the beam

    As cross-section surface of reinforcement by tensile force

    As cross-section surface of reinforcement by compressive force

    Atop top reinforcement of the topping

    Atot total fictive area used in the theory of Timoshenko

    Bv load length factor

    C factor for calculating the dynamic factor

    Ebeam modulus of elasticity of the beam

    Etopping modulus of elasticity of the topping

    Es modulus of elasticity of the reinforcement

    Fpw pre-stress force

    Fwheel the wheel load

    G sliding modulus

    L loads

    Lb beam length

    LC loads combination

    Lth theoretical span of the bridge

    M1 / M2 moments used in fatigue calculationMb moment due to compressive stress in the concrete

    Md design moment

    Md;l decisive moment of Mfirst and Msecond obtained from load spreading

    calculation

    Mfirst moment caused by the first load system

    Msecond moment caused by the second load system

    Mneg;rep negative moment due to the local wheel load (topping reinforcement)

    Mperm moment due to the permanent loads

    Mpos;rep positive moment due to the local wheel load and global q-load

    Mpre-stress moment due to the pre-stress force

    Ms

    moment due to the increasing tensile stress in the reinforcement, caused by

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    cycle load

    Msw;beam moment due to the self weight of the beam

    Msw;topping moment due to the self weight of the topping

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    Ms moment due to the increasing compressive stress in the top reinforcement,

    caused by cycle load

    Mu ULS moment

    Nb compressive force in the concrete

    Ns compressive force in the reinforcement due to the compressive stress in the

    concrete

    Q factor for traffic type

    R ratio of minimum and maximum relative stress (R = c;min / c;max )S dynamic factor

    Sc;d;max general fatigue quantity

    Su(n) design value of the material strength in fatigue at n cycles

    Vd;vertical design shear force (summation of the shear forces due to the self weight of

    the beam, topping, permanent and live loads).

    Vd;horizontal design shear force (summation of shear forces due to permanent and

    live loads).

    VRd1 design shear resistance

    Vred shear force due to the vertical pre-stress force

    Vrep shear resistance.

    Vrep;max maximum representative shear force due to dead load, pre-tensioning and

    maximum of the variable actions;

    Wbeam;top moment of resistance in the top of the beam

    Wbeam;bot moment of resistance in the bottom of the beam

    Wcs moment of resistance in the composite structure

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    1. INTRODUCTIONThis sub-task is set up in the EuroLightCon project, to find the economical consequences of the

    application of Light Weight Aggregate Concrete (LWAC) compared to Normal Density Con-

    crete (NDC) in a bridge structure.

    Two concrete compositions, two compressive strengths and three different spans are used to get

    a clear view in the relation of total strength, stiffness, material- and project costs.

    The bridge consists of 15 standard VIP beams (inverted T-beams) with a concrete of C45/55

    strength, and a topping of 210mm height and C30/37 strength.

    Such a choice of bridge structure produces four material combinations: One with a reference bridge configuration completely executed in ordinary NDC The other three with an individual application of LWAC in the beam, topping or both.Spans of 20, 30 and 40 m are used in this research, with respectively VIP 700, VIP 1100 and

    VIP 1600 beams.

    The figures given in this document are based on a bridge span of 30m, unless me n-

    tioned otherwise.

    Superstructure

    Length (of the beams) :30.35 mWidth : 18.00 m

    Theoretical span : 30.35m - 2 * 0.30 = 29.75 m (fig. 1 and 3).

    Beams : 15 VIP 1100 beams with an individual width of 1.18m and

    15 joints of 20 mm

    Transversal end beams : at both bridge ends with a size of 0.55 m * 1.325 m (fig. 3 )

    Topping : 210 mm

    Figure 1 Longitudinal section of the superstructure of the bridge

    Beam length = 30350 mm

    Lt = 29750 mm

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    The topping and the edge beams are made in-situ after placing the inverted T-beams at the sub-

    structure. The edge beams are made at the supports to connect the inverted T-beams in trans-

    versal direction.

    The width of the bridge is big enough to place four different lanes and two pedestrian strokes.

    Although the bridge design could be interpreted as suitable for situations where side collision can

    occur, it is omitted by this research due to the large difference in the international regulations.

    Figure 2 Cross section of the bridge.

    To calculate the spreading of permanent and live loads, the representative stresses and the de-formations of the beam two computer programs are used:

    Spreid to calculate the spreading of permanent- and live loads over the bridge construction. Span , to calculate the representative stresses and deformations by the use of static quanti-

    ties obtained from the load spreading calculation

    Substructure (fig 3)

    The substructure is divided in two land abutments and a number of piles.

    Land abutment

    The shape of the land abutment is designed to enable optimal support of the inverted T-beamsand the dynamic plate, as well as the accomplishment of the transitional joint.

    Piles

    The size of the piles is chosen at 250x250 mm2

    with a length of 15 m. The piles are placed in

    groups of two and equally divided over the land abutment. To take the horizontal force which is

    caused by the breaking forces of the live loads, the piles are placed in the ground at a slight an-

    gle.

    15*1180 [VIP.1100] + 15*20 [joint] = 18000 [mm]

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    Dynamic plate

    Transitional joint

    Structural topping

    Transversal end beam

    Inverted T-beam

    Land abutment

    Piles

    Figure 3 Detail of the joint between the super- and substructure of the bridge

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    2. GENERALThe used calculation procedures are based on real bridge calculations, while the project only

    concerns a fictive bridge.

    2.1 Standards and starting pointsIn structural bridge calculations the following standards and starting points are used:

    Standards

    V.B.C. 1995. (Dutch standard for calculation methods and structural demands by the con-crete application)

    V.B.B. 1995. (Dutch standard for calculation methods and structural demands for bridges)

    Starting points

    Environmental class 3 (Moist surrounding in combination with thaw minerals). Relative humidity of 75%. Due to the ground configurations in the Netherlands, piles of 15m are used in the substructure

    calculation.

    2.2 MaterialsThe materials comply with the materials used in the real bridges. In such a way a realistic

    comparison between LWAC and NDC is obtained.

    Beams concrete strength by releasing the tension 30 N/mm2

    (prefabricated) concrete strength (28 days) B55 (C45/55)

    pre-stressing steel (VIP 700 and 1100) FeP (fp) 1860 , 12,5 mm,

    with Ap = 93 mm2

    (VIP 1600) FeP (fp) 1860 , 15,7 mm,

    with Ap = 150 mm2

    reinforcement: FeB (fy) 500

    Topping (in-situ) concrete strength B35 (C30/37)reinforcement: FeB (fy) 500

    Transversal end concrete strength b 35 (C30/37)beam (in-situ) reinforcement: FeB (fy) 500

    Land abutment concrete strength B35 (C30/37)(in-situ) (normal density)

    piles 250 x 250 mm2 B45 (C35/45)(prefabricated) (normal density)

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    2.3 GeometryThe geometry of the beam is expressed in four static quantities:

    i = moment of inertia in longitudinal direction [mm4

    /mm1

    ] j = moment of inertia in transversal direction [mm4/mm1] i0= torsion moment of inertia in longitudinal direction [mm4/mm1] j0 = torsion moment of inertia in transversal direction [mm4/mm1]

    The moment of inertia in longitudinal direction is obtained confirm the theory of elasticity of the

    composite structure. The torsion moments of inertia are calculated by the theory of Bredt and

    the membrane theory.

    To obtain comparable stiffnesses for calculating the -factor and the -factor, the moments ofinertia in longitudinal direction are multiplied by the modulus of elasticity of the beam, and the

    moments of inertia in transversal direction are multiplied by the modulus of elasticity of the top-

    ping.

    Figure 4 Cross section of the composite structure (VIP 1100 and topping)

    Moment of inertia in longitudinal direction ( i )

    This moment of inertia is calculated of the composite structure. Due to the E-modulus difference

    between the beam and topping, the width of the topping (wb) changes, based on the following

    formula:

    This results in a change of the moment of inertia when LWAC applied

    in the beam, topping or both.w bE

    Eb ttopping

    beam

    =

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    Moment of inertia in transversal direction ( j )

    In this section only the topping is present, therefore this moment of inertia only is based on the

    height of the topping.

    j

    b h

    bh

    t t

    t

    t= =

    1

    12 1

    12

    3

    3[mm4/mm1]

    Torsion moment of inertia in longitudinal direction ( i 0 )

    The calculation of the torsion moment of inertia is based on the Timoshenko theory of elasticity

    and is an approximation of the real cross section by three rectangles (figure 5).

    Figure 5 Torsion stiffness calculation by the method of Timoshenko

    Where:

    Part 1(topping) 2(web) 3(bottom flange)

    b bt x 0.5 x (Et / Eb) bw bt -10 mm

    H ht hw + 0.25ht + 0.175 hf hf

    db 2 xb1-b2 2 x b2 2 x b3-b2

    A h1 x b1 h2 x b2 h3 x b3

    bt

    bt

    0.175

    0.65

    0.175

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    db is the second fictive width used in the calculation

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    To calculate the torsion moment of inertia (io) these data are used in the following formula:

    iw

    Adb

    h

    h dbb

    tot

    t w f

    t w f0

    2

    1 2 3

    31 2 31 4 13= +

    , ,, ,

    , , , , or: i wAdb

    h

    h dbb

    tot

    t w f

    t w f0

    2

    1 2 3

    31 2 31 4 13= +

    , ,, ,

    , , , ,

    This formula is composed of the theory of Bredt (first part) and the Membrane theory (second

    part)

    Torsion moment of inertia in transversal direction (j0)

    The torsion moment of inertia is calculated taking in account only the present height of the top-

    ping.

    j

    b h

    bh

    t t

    t

    t0

    3

    3

    1

    6 1

    6= = [mm4/mm1]

    Review of the moments of inertia and the torsion moments of inertia

    Combinations

    Topping-beam

    i [mm4/mm1] j [mm4/mm1] i0

    [mm4/mm1]

    j0

    [mm4/mm1]

    NDC-NDC 129.2E+6 771.8E+3 5.36E+6 1.54E+6 0.162 1.118

    LWAC-NDC 113.6E+6 771.8E+3 5.03E+6 1.54E+6 0.177 1.163NDC-LWAC 145.8E+6 771.8E+3 5.79E+6 1.54E+6 0.152 1.073

    LWAC-LWAC 129.4E+6 771.8E+3 5.36E+6 1.54E+6 0.162 1.119

    where:

    =b

    a

    i

    j24 and

    ( ) =

    +

    G i j

    E i j

    0 0

    2=

    ( )0 2 0 0, i ji j

    +

    ( v = 0,2)

    Review of the stiffness

    Combinations:Topping-beam

    Modulus of elastic-ity

    (topping-beam)

    stiffness(EI): i

    Stiffness(EI): j

    torsionstiffness

    (EI) :i0

    torsionstiffness

    (EI): j0

    NDC NDC 31000-36000 4650E+9 23.9E+9 192.9E+9 47.85E+9

    LWAC NDC 23276-36000 4088E+9 18.0E+9 181.2E+9 35.93E+9

    NDC LWAC 31000-27030 3941E+9 23.9E+9 156.6E+9 47.85E+9

    LWAC LWAC 23276-27030 3487E+9 18.0E+9 144.9E+9 35.93E+9

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    2.4 LoadsThe representative loads are divided into permanent and live loads

    2.4.1 Permanent loads

    Figure 6 Detail of the location of the loads at the side and at the middle of the bridge

    The next permanent loads (L) are determined:

    L1: Railing

    L2: Crash barriers at both sides of the bridge

    L3: Crash barrier at the middle of the bridge

    L4: Side element at both sides of the bridge

    L5: Dump in the middle and at both sides of the bridge

    L6: Asphalt layer

    The railing and the side element are placed directly at the side of the bridge. The crash barriers are placed in the middle and at 1400 mm from the sides of the bridge.

    The dump is present between 500 and 1200 mm from the side of the bridge. The asphalt layer is present from 1200 mm form the side of the bridge.

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    Figure 7 Detail of the place and size of the permanent loads

    2.4.2 Live loads

    Live loads can be divided into an equally divided square load and axle pressures of two loads

    systems. The representative forces of these live loads are obtained from following table:

    Mobileclass

    subscription equal dividedsquare load

    three axlepressures

    axle pressuredivided over:

    60 Bridges admitted in roads

    where the traffic cannot be

    diverted.

    Prep = 4 kN/m2

    Frep= 200kN 4 wheels

    These loads are multiplied with the dynamic factor to include the impact of the entering vehicles

    at the bridge.

    Dynamic factor for load spreading calculation, S CL

    h L

    th

    th= +

    +1

    100( )

    For NDC (C = 0.7) : 1 + 0.7 * 29.75 / (1.325 * 129.75) = 1.12

    For LWAC (C = 0,8) :1 + 0.8 * 29.75 / (1.325 * 129.75) = 1.14

    Review of the dynamic factors that are calculated by different spans and concrete composi-

    tions.

    Span / material NDC LWAC

    20 m 1.12 1.14

    30 m

    40 m

    1.12

    1.11

    1.14

    1.12

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    First load system Second load system

    The next live loads (L) are determined:

    L7: Equal divided mobile load is present from 1200 mm of both sides of the bridge

    Loads 8 and 9 are obtained from the load spreading calculation, based on the most unfavourable

    positions.

    L 8: Simple load system. (position of the first load system in figures 8a and 9)

    L 9: Double load system is used to calculate the moment in longitudinal direction according

    to figures 8a and 9

    Loads 10 and 11 have standard positions.

    L10: Double load system is used to calculate the negative moment in transversal

    direction(simple load system at both sides of the bridge, fig 9).

    L11: Second load system is used to calculate the fatigue and an extreme loading

    case (second load system in figures 8a and 9)

    L12: Extreme loading case (wheel directly at the side of the bridge, in case of an accident),

    figure 8b.

    Figure 8a Wheel configurations of two load systems in SLS

    Figure 8b Wheel configuration of two load systems in ULS

    Figure 8c Wheel configurations that are causing the largest bending moment in longitu-

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    dinal direction

    Lth

    Figure 9 Place of the traffic loads with regard to the load combinations

    2.4.3 Loads combinations

    The next load combinations are used for calculation of the representative moment:

    LC 1: L1 + L2 + L3 + L4 + L5 + L6 (Permanent load)

    LC 2: LC1 + L7 + L8 (Simple load system)

    LC 3: LC1 + 0.8 L7 + 0.8 L9 (Double load system, longitudinal

    direction)

    LC 4: LC1 + 0.8 L7 + 0.8 L10 (Double load system, transversal

    direction)

    LC 5: LC1 + L7 + 1.2 L12 (Extreme loading case, simple load

    system)

    LC 6: LC1 + 0.8 L7 + 0.8 L11 + 1.2 L12 (Extreme loading case, double load

    system)

    When two load systems are applied at the same time (in LC3, LC4 , LC6), the result of bothload systems are then multiplied with = 0.8, according to Dutch regulations.

    L 12 (included in LC5 and LC6) is multiplied with 1,2 according to Dutch regulations

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    2.5 Computer programsThe shear forces, caused by the live loads, are calculated in paragraph 2.5.1.

    The other calculations in this report are based on two computer programs, which calculate thespreading of the loads, the representative moments and shear forces (the Spreid program) and

    the representative stresses and deformations in the elements (the Span program).

    2.5.1 Theory of shear force calculation

    The representative decisive shear force is calculated in two live loading situations:

    1. Simple loading case where only one load system placed at the bridge.

    2. Double loading case where two load systems is placed at the bridge.

    The largest shear force is chosen in those two loading cases

    Simple load system:

    Vrep.

    1

    Lth

    Lth

    a 5000

    X3

    Lth

    a 1000

    X2

    Lth

    a

    X1

    =

    +

    +

    axle load +

    1

    2 P S lrep th

    Figure 10 Simple load system

    Where:

    ( )x a c1 22

    3= +

    ( )x a c2 2 10002

    3= + +

    ( )x a c b3 50002

    3= + + +

    Where:a = 500 mm

    b = 1400 mm

    c = 1750 mm

    Load system

    B

    X1X2

    X3

    a 1000 4000

    Lth

    b

    c

    =tan23

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    Double load system

    V axle load1

    Lth

    Lth

    a 9500

    X6

    Lth

    a 5500

    X5

    Lth

    a 500

    X4

    Lth

    a 5000

    X3

    Lth

    a 1000

    X2

    Lth

    a

    X1

    rep. =

    +

    +

    +

    +

    +

    4

    0,8 +1

    20 8 p S lrep th. ,

    Where:

    ( )x a c1 22

    3= +

    ( )x a c2 2 10002

    3= + +

    ( )x a b c3 5000

    2

    3= + + +

    ( )x a c4 2 45002

    32 1000= + + +

    ( )x a c5 2 55002

    31000= + + +

    ( )x a b c6 95002

    32 1000= + + + +

    a = 500 mm

    b = 1400 mm

    c = 1750 mm

    Figure 11 Double load system

    2.5.2 The Spreid program

    This computer program is based on the theory of Guyon & Massonnet. The calculations of the

    representative moments and shear forces are done with this theory for every composite beam

    structure individually, in longitudinal direction and every joint in transversal direction.For practical reasons, the beam with the governing moments and shear forces is representative

    for all the beams. Therefore all other beams are equally pre-stressed and reinforced.

    The theory uses the following equations for the calculation of the spreading of the loads:

    = 0 2.

    =b

    a

    i

    j24 with b

    n

    nb=

    1

    1 1'

    ( )

    =+

    G i j

    E i j

    0 0

    2with

    ( )G

    E=

    +2 1

    ( ) =

    +

    0 2 0 0, i j

    i j

    Load system

    Load system

    c

    c

    Lth

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    2.5.3 The Span program

    This computer program is based on the theory of elasticity and calculates i.e. the geometry, the

    representative stresses and deformations of the composite structure.

    The program checks the cross-sections of the beam in SLS and ULS.

    2.6 Superstructure calculationBoth computer programs and the spreadsheet for live shear force are used in this calculation.

    2.6.1 Data obtained from computer programs

    The used data in the calculations are obtained from the computer programs and are divided into:

    The moments and shear forces due to self-weight of the topping and the beam. The moments and shear forces due to permanent loads and the moments due to live loads. The shear force due to live loads.

    2.6.1.1 Moments and shear forces due to self weight

    The moments and shear forces caused by self-weight are obtained from the representative

    stresses and deformations calculation.

    Combinations topping-beam Moments (kNm) Shear force (kN)

    beam Topping beam topping

    NDC-NDC 1080 683 145 92

    LWAC-NDC 1080 530 145 71

    NDC-LWAC 837 683 113 92

    LWAC-LWAC 837 530 113 71

    2.6.1.2 Data due to loads spreading calculationThe moments caused by the permanent and live loads, and the shear forces caused by the per-

    manent loads, are obtained from the loads spreading calculation and are divided into longitudinal

    and transversal direction. In longitudinal direction the moments and shear forces are calculated in

    the beam; in transversal direction the moments and shear forces are calculated in the topping.The shear force caused by the live loads in longitudinal direction is calculated using the theory of

    paragraph 2.5.1.

    Longitudinal direction

    The moments and shear forces, given in the following table, are used for the stress and deforma-

    tion calculation of the beam. The dynamic factor is included in the results.

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    Combinations

    topping-beam

    Moment (kNm) Shear force (kN)

    permanent loads live loads Permanent loads live loads

    NDC-NDC 578 1395 80 290

    LWAC-NDC 585 1412 80 295

    NDC-LWAC 573 1463 80 295

    LWAC-LWAC 578 1420 80 295

    Transversal direction

    This calculation can be divided into two situations: overall and local.

    Overall situationA car is placed at both sides of the bridge, by which, theoretically, the bridge bends upwards in

    transversal direction. This loading situation is resulting in the following moments.

    Combinations

    topping-beam

    Decisive moment

    normal situation;

    positive (LC 1-4)

    normal situation;

    negative (LC 1-4)

    extreme situation;

    negative (LC 5,6)

    NDC-NDC 33 -11 -21

    LWAC-NDC 31 -9 -19

    NDC-LWAC 34 -13 -23

    LWAC-LWAC 34 -11 -21

    Local situationThe wheel load of a vehicle causes an extra positive moment in the topping, when standing pre-

    cisely between the two beams (the most unfavourable position). These moments are used to cal-

    culate the topping reinforcement.

    Mneg;rep : Fwheel

    qd

    l1 l1 l1

    Mpos;rep

    M q lpos rep d; =1

    24 12

    ( = 0.3 kNm)

    M q lneg rep d ; =1

    12 12

    ( = 0.6 kNm)

    M F lpos rep wheel; =1

    8

    1 (= 6.4 kNm)

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    Shear calculations

    The shear calculations are done in the web of the beam (vertical direction) and in transitional

    zone between beam and topping (horizontal direction, due to the deformation of the construc-

    tion). This horizontal stress is present near the top of the stirrup and therefore influences the stir-

    rup composition at the top. A standard stirrup composition is used with three sections at the top

    (according to fig 14).

    The vertical component caused by the pre-stress force (fig 12) is used to reduce the shear force

    in the web (vertical direction).

    Vd;vertical = design shear force (summation of shear forces due to self weight beam, topping,

    permanent and live loads).

    Vd;horizontal = design shear force (summation of shear forces due to only permanent and live

    loads).

    Combinations

    Topping-beamVertical Vd

    (kN)

    vertical component

    pre-stress force

    (kN)

    horizontal Vd (kN)

    NDC-NDC 607 -75 370

    LWAC-NDC 592 -74 376

    NDC-LWAC 579 -65 375

    LWAC-LWAC 559 -63 375

    2.6.2 Beam

    2.6.2.1 Pre-stress steel calculationThe numbers of pre-stress strands are determined full filling all demands in ULS and SLS, in the

    transitional (assembling) phase of the construction as well as at the end stage.

    In this case, deformations of the beam were decisive.

    The exact place of the strands in the beam is based on the application of fig 12 and 13.

    Two strands are needed at the top of the beam for the application of the stirrups. The position of the strands in the cross section is chosen to cover as good as possible the ex-

    pecting moments of the beam under all the loadings.

    Cross section B Cross section A

    dmiddle dend

    3/8 x Lth

    Lth

    Vertical component of

    the pre-stress force

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    Figure 12 Position of the centre of gravity of the pre-stress strands over the beam length

    Topping

    Beam

    Cross section A Cross section B

    Figure 13 Details of the place of the pre-stress strands in the cross section

    The deformation of the beam is calculated in the several development stadiums: from the time

    the beam is fabricated, until the moment when the beam is loaded by live loads (period of 12

    months)

    The deformation is checked in agreement with specific regulations, based on the next formula:

    x - 1,1 y > 1 where: 1 = Lth / 2000 [mm]

    2.6.2.2 Check in extreme loading caseThe moment in extreme loading case is checked at the maximum moment, with the formula:

    M M M M Mu extremeloadingcase sw beam sw topping prestress + + +; ;

    Where:

    ( )( )M LC LC LC LCextreme loadingcase = + + + 1 0 1 0 8 7 11 1 0 12, , ,

    Mu, Msw;beam , Msw;topping and Mprestress , are obtained from the representative stresses and deforma-

    tions calculations

    2.6.2.3 ShearThe shear reinforcement is first calculated in the beam and then checked with the horizontal

    shear in the transitional zone between the beam and topping.

    a) The shear force in the web of the beam

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    The shear force is divided into live and permanent part.

    Live part

    The shear in the beam is calculated with a simple and double load system, according to the fig-

    ures 10 and 11.

    Permanent part

    The representative shear force is obtained from the loads spreading calculation.

    The shear reinforcement is calculated by the following figure which is based on Dutch stan-

    dards.

    dd

    w

    V

    b d=

    d = h-c ; where: d

    c(bottom)=30 mm d;red.

    c(top) = 40 mm 0,2d(n+1)

    n bmd = 0 15, ; Where bmdpw

    c

    F

    A= 1

    n n+ = +1 1 200 - 1300

    1 0 4= , b ;Whereff f

    b

    brep

    m

    ck= = +

    0 7 1 05 0 05

    1 4

    , ( , , ' )

    ,

    2 = 0 2, ' f k kb n ;Where f bf ck

    '. '

    ,=

    0 72

    1 2; k

    fnbmd

    b

    =

    5

    31 10

    '

    '. ; k = 10.

    redred

    w

    V

    b d=

    ; WhereV

    d d

    L

    Fredend middle

    th

    pw=

    3

    8

    (based on the following figure)

    dmiddle dend

    3/8 x Lth

    Lth

    When LWAC applied, certain factors are changing:

    2 =

    0 2 1, ' f k k kb n

    k1 0 4 0 6 2300= + , .

    = 0.9 (

    = 1900 kg/m3)

    Fpw

    top surface

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    ff k f

    b

    brep

    m

    ck=

    = + 1 0 7 1 05 0 05 0 9

    1 4

    , ( , , ' ) ,

    ,

    Other agreements: The shear reinforcement is calculated at 200mm from the beam end. The transfer length, is estimated at 1500 mm from the beam end. The shear stress in the middle of the span, is estimated at 20 % of the calculated d The intersection between the d line and the n+1 line is calculated by the equality of triangles. The distance from the support to the intersection must be reinforced. This distance is sub-

    divided into three equal distances in which:

    Part 1 is calculated for: 5/9 of the total surface

    Part 2 is calculated for: 3/9 of the top surface

    Part 3 is calculated for: 1/9 of the top surface

    The calculation of the shear reinforcement, is based on the next procedures:

    1.Needed reinforcement surface is calculated by the above-described method.

    2. The practical reinforcement is chosen (based on diameter and spacing) compared to the

    needed reinforcement.

    3. The maximum number of stirrups is calculated by :re orcement dis ce

    spacing

    inf tan

    4. The optimisation of the reinforcement by choosing a second spacing, is based on the follow-

    ing example :

    End of a considered reinforcement part

    8-100 assume a stirrup reinforcement witha spacing of 100 mm and that four stirrups

    can be reduced at the end of the rein-

    forcement section.

    When a second spacing of 200 mm is used,

    a distance of 800 mm is needed to get this

    reduction.

    8-200

    In the more complex cases, this distance can be calculated by the formula below:

    reduced stirrups

    spacing first spacing

    first spacing

    spacingsec.

    sec.

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    b) Shear force in transitional zone

    The transitional zone between the beam and the topping must be reinforced because of the hori-

    zontal shear stress occurring when the construction is under permanent and live load.

    The shear stress in the transitional zone is calculated by the formulas below:

    dd

    w

    V S

    b I=

    1 0 3= , 'f ck

    The difference between dand 1 is reinforced. This length is divided into 5 parts by which the

    first part is calculated by 9/25 part of the surface, the second part 7/25, the third part 5/25, the

    fourth part 3/25 and the last part 1/25.The stirrup calculation in this zone is equal to the calculation procedure of the shear in the web.

    3 sections in transitional zone

    Figure 14 Detail of the stirrup composition in transitional layer between topping and

    beam

    2.6.3 Topping

    The reinforcement is calculated in two loading situations:

    1. The ultimate limit state (ULS)

    2. The serviceability limit state (SLS)

    In ULS, the positive and negative moments are calculated in normal (sd = 1,5) and extremesituation (

    sd= 1,0). The representative moments in normal situations are divided into local and

    topping

    beam

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    overall moments. The representative moments in extreme situation exist only of a global mo-

    ment.

    The moments in overall situation are obtained from the load spreading calculation.

    The moments in local situation are calculated by the figure below:

    Mneg;rep : Fwheel

    qd

    l1 l1 l1

    Mpos;rep

    The total positive moment is based on a summation of the wheel- and q-load. The total negative moment is based only on the q load. The wheel load cannot occur in the

    situation when each of two cars stands at the side of the bridge.

    The necessary reinforcement in the topping in transversal direction is determined in ULS

    In SLS, already chosen reinforcement is checked on cracking. This check is done according to

    the Dutch regulation, which includes two methods:

    Complete developed cracking pattern (M

    Wf

    rep

    bm )

    Incomplete developed cracking pattern ( MW

    frep

    bm )

    Agreements by a complete developed cracking pattern according to the Dutch regula-

    tions

    One of the two agreements below has to be correct:

    a) ss

    k1

    b) s k

    s

    100 132

    ,

    Agreements by an incomplete developed cracking pattern according to the Dutch

    regulations

    ( )

    +

    +km

    ck

    sr s sr s

    k f kand

    3

    2

    150

    '

    s

    s

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    src r bm

    s

    A k f

    A=

    5 4. s s

    rep

    u

    fcalculated mm

    present mm

    M

    M=

    2

    2

    kr = 0,9-0,5h2.6.4 Composite structure

    2.6.4.1 Stresses due to shrinkage , creep and temperatureDue to the difference in the humidity and the temperature of the surroundings and the fresh con-

    crete, a part of the mix water of the concrete can evaporate resulting in the shrinkage of the

    concrete. Creep, however, depends only on the loading and loading time. Theoretically, the creep

    reduces the shrinkage.

    The differences of the temperature at the top and the bottom of the bridge also influences the

    stresses in the construction.

    Shrinkage

    According to the Dutch standard, the shrinkage factor 'r(for NDC) is calculated by the

    multiplication of several variable factors:

    ' ' 'maxr c b h p t k k k k =

    Where:

    kp =1

    1 0 2+ , o

    kt =t

    t hm+ 0 043,

    with t in days; and hm =2

    2

    +

    ( )

    ( )

    L h

    L h

    When using LWAC:

    ' ' 'maxr c b h p t k k k k k = 5

    k5 = : 1.2 for a strength fck > 25 N/mm2: 1.5 for a strength fck = 15 N/mm

    2

    strength values between 15 and 25 N/mm2

    are linear interpolated

    kt =t

    t hm+with t in days

    Creep

    Creep factor is dependent on several variable factors:

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    = k k k k k c d b h t max

    Where:

    hm =

    2

    2

    +

    ( )

    ( )

    L h

    L h

    kt =t

    t hm+ 0 043,

    with t in days

    Stresses due to shrinkage and creep

    The shrinkage difference between the topping (fresh concrete) and the beam (aged concrete)

    causes a horizontal force and moment which is given by the following figure and formulas:

    ------- F ( )F E Ar topping r beamtopping topping

    = ' ; ' ;

    M F hh

    ztopping

    o=

    2

    These two forces cause stresses in the construction, which are calculated using the next formu-

    las:

    F

    Atopping

    F

    A

    E

    Etotal

    topping

    beam

    ( )M h z

    W

    h h z

    total b

    beam top

    topping b

    ,

    M

    W

    E

    Ebeam top

    topping

    beam,

    M

    Wbeam top,

    + + =

    F

    Atotal

    M

    Wbeam bottom, ' , ,r beam bottom

    The total stress at the bottom of the beam is calculated by the formulas below:

    Topping

    Beam

    ht / 2

    zo

    h

    M

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    beam bottom; = (creepreduction beam + creepreduction topping) x ', ,r beam bottom

    Where:

    Creep reduction of the beam = 1

    ebeam

    beam

    Creep reduction of the topping =1

    e topping

    topping

    ' , ,r beam bottom= Stress caused by shrinkage

    Temperature

    The temperature of the surroundings causes extra stress in the construction. When certain tem-

    perature on the top of the bridge is reached, an extra stress occurs at the bottom of the construc-

    tion. This extra stress together with the present stress (due to loading) needs to be checked tothe maximal stress.

    In this situation a tensile stress occurs at the bottom of the beam and therefore checked with the

    present tensile stress.

    The mean temperature Tmean is calculated by the next formula:

    TA

    T x b x dxmeanc x

    x

    = 1

    1

    2

    ( ) ( )

    The temperature difference Tb is calculated by the formula:

    Th

    IT x b x x dxb

    x

    x

    = ( ) ( )1

    2

    The temperature of the construction Te ( ) is calculated by the formula:

    { } T x T T x T xmean b e( ) ( ) ( ) + =

    T x T T T xmean b e( ) ( ) =1

    6

    7

    18

    4

    9

    01

    6

    7

    54

    8

    27 = T T T xmean b e ( )

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    01

    6

    7

    18

    2

    9 = T T T xmean b e ( )

    temperature beam beam bottomE T= ,

    Where:

    = -1.0 x 105

    T beam bottom = 016

    718

    29

    = T T T xmean b e ( )

    The total extra stress (caused by shrinkage and creep differences and temperature influence) is

    added to the present tensile stress (caused by permanent and live loading). And is given by the

    following formula:

    b admissible b present shrinkage creep temperature, , , + +

    2.6.4.2 Fatigue

    Fatigue in the construction is caused by the load cycles due to the passing traffic (live load).These load cycles are influencing in time the representative stresses. Such behaviour can cause

    fatigue in the construction parts due to which the construction can collapse without exceeding

    the maximum calculated stress.

    Fatigue in longitudinal direction

    The fatigue moment is calculated with the next formula:

    M M Bfatigue d l v= ;

    Where:

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    ( )B Lv th= =0 8 20 0 004 0 839, , .

    ( ) = f Ke12

    1 0.

    f Lth1 0 01 0 15 0 4475= + =, , .

    KK

    K Ke=

    +1

    1 2

    KM

    M

    first

    1 =max

    KM

    Mond

    2 =sec

    ma x

    The load spreading calculation (LC8 and LC11) calculates Mfirst and Msecond

    Mmax is calculated by the following figure:

    Lth

    x 1000 4000 y

    Fwheel Fwheel Fwheel

    Ra Rb

    500

    Schematical longitudinal section of the bridge

    ( )R

    x F

    Lbwheel

    th

    = + 3 6000

    R y Fb wheel ma x ( )= + 4000 4000

    Topping (longitudinal direction)

    The representative stress caused by fatigue is checked by the maximal stress according to the

    formulas below:

    tot buv n u nf S =' ( )( ) ( )

    Where:

    tot perm fatigue= +

    fatiguefatigue

    c s

    M

    W=

    ;

    ( ) ( ) ( )S R n f u n bv= 1 0 1 1, log '

    Where:

    RM

    M

    bd

    d

    permanent= =

    '

    '

    ;min

    ;max max

    middle of the span

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    n = 1,1 x 109

    = 1.0

    ( )f fbvb rep k

    m

    '' , ,; ;= +

    1

    2 0 85 30 0 85 30

    f fb rep k ck ' . '; ; = 0 85

    m = 1 2,

    Beam (longitudinal direction)

    The representative stress caused by fatigue is compared with the maximal stress according to

    the formulas below: tot buv n u nf S =' ( )( ) ( )

    Where:

    tot perm fatigue= +

    fatiguefatigue

    c s

    M

    W=

    ;

    ( ) ( ) ( )S R n f u n bv= 1 0 1 1, log '

    Where:

    RM

    M

    bd

    d

    permanent= =

    '

    '

    ;min

    ;max max

    n = 1,1 x 109 = 1.0

    ( )f

    f

    bv

    b rep k

    m

    '

    ' , ,; ;=

    + 1

    20 85 30 0 85 30

    f fb rep k ck ' . '; ; = 0 85

    m = 1 2,

    Tension in pre-stress steel

    The tension leap is calculated by:

    s rep s u; ;

    Where:

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    s u s ds rep

    m

    m

    n; ; ;min

    ; ;

    = +

    10

    7

    7

    10

    n = 1.1 x 108

    m = 11,

    s rep bn; =

    n =E

    Es

    b0 6, b

    fatigue

    liveload

    b mm

    M

    M=

    ;90

    Transversal direction

    The representative moment is checked by the chosen top and bottom reinforcement of the top-ping. It appeared in all cases that the earlier calculated bottom reinforcement was too small to

    comply with the fatigue regulations, hence a new reinforcement had to be chosen. This new re-

    inforcement is again checked on cracking.

    M Mrep s. < (Tensile strength reinforcement)

    M M Mrep b s. ' '< + (Compressive strength concrete and steel)

    Where:

    Mrep

    = the decisive moment of M1

    and M2

    loadlocalMM vfirst +=2

    11

    loadlocalMM vond +=2

    1sec2

    Mfirst and Msecond are calculated in the spreading calculation in LC8 and LC11

    Mpos;rep is calculated in paragraph 2.6.3

    M z Ass n rep

    m top=

    ; ;

    10 6

    Where:

    s n rep s repm

    n; ; ; ;=

    10

    7

    7

    10

    m = 1.15z = d - 1/3 x

    Mpos;rep

    Mpos;rep

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    Where:

    ( ) ( )x n A A n A A n c A A dtop bot top bot top km top bot = + + + + + + 2

    2

    2 10001

    2

    and is obtained from the two equations:

    N A E A Ed

    xs s s s s s bs

    ' ' ' ' ''

    = =

    1 and

    N A E A Ed

    xs s s s s s bs= =

    ' 1

    ( )

    M

    x A S d x

    b

    top u n

    ' = 12

    1000 13

    106

    ( ) ( ) ( )S R n f u n bv= 1 0 1 1, log '

    Where:

    RM

    M

    bd

    d

    permanent= =

    '

    '

    ;min

    ;max max

    n = 1,1 x 109

    = 1.0

    ( )f

    f

    bv

    b rep k

    m

    '

    ' , ,; ;=

    + 1

    20 85 30 0 85 30

    f fb rep k ck ' . '; ; = 0 85

    m = 1 2,

    M

    A E cx

    d c

    s

    top s bu

    top km

    top km

    '

    '

    =

    +

    10 1

    1

    2 12

    10

    3

    6

    2.7 SubstructureA land abutment is placed in transversal direction under both bridge ends. Both land abutments

    are supported by a number of piles, calculated according to the local (Dutch) ground regulations.

    Land abutment

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    The height of the land abutment is related to the height of the beam, therefore by an increasing

    span, the height of the beam and height of the land abutment increases. This results in a larger

    volume according to the table below:

    Span Volume land abutment

    20 1.2 m3

    / m1

    30 1.6 m3

    / m1

    40 2.0 m3

    / m1

    Piles

    The piles are calculated by inclusion of the following loads:

    Weight of the land abutment

    Weight of the beams Weight of the topping The permanent loads of the individual bridge parts (railing, asphalt layer, etc.) Equally divided live loads Live loads (two cars standing directly at the support).The total weight per span changes only when the weight of the topping and beam are changed.

    The reduction in piles can be found when LWAC is applied by different spans.

    The size of the piles is 250 x 250 mm2. Assumed is a ground resistance of 10 N/mm2. This as-

    sumption results in a maximum pile force of 625 kN.

    The calculated number of piles is rounded to an even figure. In this way the piles can be appliedin groups of two, and equally divided over the length of the land abutment.

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    3. COMPARISONThe LWAC is variable applied in the beam as well as the topping. Also the spans of the bridge

    are changed from 20, 30 up to 40 m. Combination of all this variables results in an reliable com-

    parison. First have been calculated the material quantities for every combination. The total costs

    are obtained multiplying the quantities by there costs. The total costs are excluding overhead and

    engineering costs.

    3.1 QuantitiesThe quantities are given in the tables with constant span and with variable LWAC application to

    find the influence of LWAC on the construction.

    Superstructure

    The quantities of the superstructure are expressed per square meter bridge surface. The total

    amount of concrete (C30/37) added in-situ consists of the topping layer and the two edge beams

    (figure 3).

    Substructure

    The influence of the weight reduction on the superstructure is expressed in a smaller pile force

    and where possible in reducing the number of piles. The volume of the land abutment is held

    constant by each span.

    3.1.1 Bridge with a span of 20 m

    The inverted T-beam with height of 715mm (VIP 700) is chosen from tables in relation to the

    span of the bridge.

    Lth = 20 m

    B = 18 m

    Abridge = 20 x 18 = 360m2

    Superstructure Combinations

    topping-beam

    Elements topping + 2 edge beams

    concrete

    (m3/m2)

    pre-stressing

    steel (kg/m2)

    Reinforcement

    (kg/m2)

    concrete

    (m3/m2)

    reinforcement

    (kg/m2)

    NDC-NDC 0.27 18.1 6.0 0.25 14.9

    LWAC-NDC 0.27 15.1 6.1 0.25 15.9

    NDC-LWAC 0.27 12.7 7.4 0.25 16.5

    LWAC-LWAC 0.27 12.1 7.2 0.25 17.2

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    Substructure

    Volume of the land abutment: 1,2 m3 / m1

    Combination

    Topping-beam

    Present pile force [kN] Total number of piles

    NDC-NDC 595 24

    LWAC-NDC 567 24

    NDC-LWAC 565 24

    LWAC-LWAC 536 24

    3.1.2 Bridge with a span of 30 m

    The VIP 1100 is chosen in relation to the span of the bridge.

    Lth = 30 m

    B = 18 m

    Abridge = 30 x 18 = 540m2

    In the combinations with NDC beams, the height of the beam is increased with approximately 50

    mm due to fatigue regulations. This results in a difference of 0,01 m3/m2 compared to the other

    combinations

    Superstructure

    Combinations

    topping-beam

    Elements topping + 2 edge beams

    concrete

    (m3/m2)

    pre-stressing

    steel (kg/m2)

    reinforcement

    (kg/m2)

    concrete

    (m3/m2)

    reinforcement

    (kg/m2)

    NDC-NDC 0.34 25.4 6.8 0.254 21.9

    LWAC-NDC 0.34 24.9 6.3 0.254 21.3

    NDC-LWAC 0.33 22.5 7.5 0.254 24.7

    LWAC-LWAC 0.33 21.9 7.5 0.254 26.3

    Substructure

    Volume of the land abutment: 1,6 m3 / m1

    Combination

    Topping-beam

    Present pile force

    [kN]

    total number of piles

    NDC-NDC 604 36

    LWAC-NDC 580 36

    NDC-LWAC 563 36

    LWAC-LWAC 602 32

    3.1.3 Bridge with a span of 40 m

    The VIP 1600 is chosen in relation to the span of the bridge.

    Lth = 40 m

    B = 18 m

    Abridge = 40 x 18 = 720 m2

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    In the combinations with NDC beams, the height of the beam is increased with 50 mm due to

    fatigue regulations. This resulted in a difference of 0,01 m3/m2 compared to the other combina-

    tions

    Superstructure

    Combinations

    topping-beam

    Elements topping + two edge beams

    concrete

    (m3/m2)

    pre-stressing

    steel (kg/m2)

    reinforcement

    (kg/m2)

    concrete

    (m3/m2)

    reinforcement

    (kg/m2)

    NDC-NDC 0.48 36.1 7.6 0.258 17.2

    LWAC-NDC 0.48 31.2 7.5 0.258 18.9

    NDC-LWAC 0.47 26.3 8.8 0.258 19.3

    LWAC-LWAC 0.47 26.3 8.5 0.258 21.8

    Substructure

    Volume of the land abutment: 2,0 m3 / m1

    Combination

    topping-beam

    Present pile force [kN] total number of piles

    NDC-NDC 620 52

    LWAC-NDC 594 52

    NDC-LWAC 612 48

    LWAC-LWAC 583 48

    3.2 Costs per quantityThe costs in the table below are average prices of spans 20, 30 and 40m and they are based on

    mean Dutch prices.

    Materials Units Material costs

    (euros)

    labour costs

    (euros)

    Topping NDC C30/37 m3 81 157

    Topping LWAC C30/37 m3 79 157

    Beam NDC C45/55 m3 118 91

    Beam LWAC C45/55 m3

    110 91The material costs exist of: The labour costs exist of:

    - Concrete material - equipment costs

    - Reinforcement - moulding

    - Pre-stressing steel - assembling of prestress and reinforcing steel

    - Maintenance and energy. - casting

    - Small inserts - other

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    Transport and assembling costs

    The transport costs are obtained from the relation between the weight of the beam and the

    needed lorry; given in the table below:

    Weight of the beam costs per transport over 100 km

    (euros)

    0 - 350 kN 340

    350 450 kN 795

    450 600 kN 1248

    The assembling costs are obtained from the relation between the weight of the beam and the

    needed crane; given in the table below:

    Weight of the beam costs per hour(euros)

    0 - 480 kN 567

    480 590 kN 681

    Review transport and assembling costs

    span Beam weight transport costs

    (euros)

    assembling costs (euros)

    (2 beams / hour)

    NDC LWAC NDC LWAC NDC LWAC

    20m 162 kN 130 kN 2723*1 2723*1 4253 4253

    30m 306 kN 238 kN 5106*2 5106*2 4253 425340m 576 kN 450 kN 18720*2 11913*2 5108 4253

    *1 two beams per drive *2 one beam per drive

    3.3 Project costsTo get a clear view of the costs per bridge part, the sub- and superstructure are divided into

    parts. The costs of the land abutment are equally calculated as the costs of the topping (equal

    concrete and reinforcement price).

    The costs of the piles are assumed at 410 Euro / piece (all costs included).

    3.3.1 Bridge with a span of 20 mL = 20 m

    A = 20 x 18 = 360 m2

    substructure

    (euros/m2)

    superstructure

    (euros/m2)

    total

    (euros/m2)

    topping-beam land

    abutment

    piles element topping transport assembling

    NDC-NDC 25.8 27.3 56.8 59.2 7.6 11.8 188.5

    LWAC-NDC 25.8 27.3 55.2 58.6 7.6 11.8 186.3

    NDC-LWAC 25.8 27.3 53.7 59.6 7.6 11.8 185.8

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    LWAC-LWAC 25.8 27.3 53.3 58.9 7.6 11.8 184.7

    3.3.2 Bridge with a span of 30 m

    L = 30 m

    A = 30 x 18 = 540 m2

    substructure

    (euros/m2)

    superstructure

    (euros/m2)

    total

    (euros/m2)

    topping-beam land

    abutment

    piles element topping transport assembling

    NDC-NDC 23.4 27.3 72.7 61.5 9.5 7.9 202.3

    LWAC-NDC 23.4 27.3 72.3 60.5 9.5 7.9 200.9NDC-LWAC 23.4 27.3 69.0 62.3 9.5 7.9 199.4

    LWAC-LWAC 23.4 24.3 68.7 61.8 9.5 7.9 195.6

    3.3.3 Bridge with a span of 40 m

    L = 40 m

    A = 40 x 18 = 720 m2

    substructure

    (euros/m2)

    superstructure

    (euros/m2)

    total

    (euros/m2)

    topping-beam landabutment

    piles element topping transport assembling

    NDC-NDC 22.7 29.6 102.3 61.1 26 7.1 248.8

    LWAC-NDC 22.7 29.6 99.6 60.7 26 7.1 245.7

    NDC-LWAC 22.7 27.3 94.6 61.7 16.6 5.9 228.8

    LWAC-LWAC 22.7 27.3 94.5 61.5 16.6 5.9 228.5

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    4. CONCLUSIONSIt is very important to stress again that following conclusions are based, structurally on the Dutch

    codes and regulations of concrete structures and economically on the average material and la-

    bour prices in The Netherlands. As earlier mentioned engineering and overhead costs are in this

    comparison excluded as well as the eventually investments.

    Using LWAC in stead of NDC, in the structural parts of composite bridges made of inverted T

    beams with topping, can reduce amount of needed pre-stressing steel in the elements for more

    than 30 %.

    On the other hand, amount of applied reinforcement in the LWAC elements and the topping will

    increase up to 25 %.

    LWAC used in the beams and the topping will reduce the total weight of the bridge. For the la r-

    ger bridge spans this will lead to reducing of amount of needed piles in the substructure up to 11

    %.

    The material costs of new, within Euro- LightCon project developed, LWAC (C45 / 55) are

    lower than standard NDC (C45 / 55) of some 4%. Also the material costs of LWAC (C30 / 37)

    are lower than NDC (C30 / 37).

    Especially for longer beams, the transport and assembling costs are in favour of LWAC ele-

    ments of about 32%.

    For bridges with a superstructure fully made of LWAC, the total project costs will decrease

    from 2% for span of 20m up to 8% for span of 40m, in comparison with bridge with NDC super-

    structure. The relative big costs reduction at the span of 40 m, is significantly influenced by the

    lower transportation and assembling costs (about 4%)

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    APPENDIX:MIXTURE COMPOSITIONMixture compositionsof Normal Density Concrete and LightWeight Aggregate Concrete withC30/37 and C45/55 strengths.

    Mixture composition (Normal density concrete, NDC)

    C45/55

    (kg / m3)

    costs

    / ton

    Costs / m3

    (euros)

    C30/37

    (kg / m3)

    cost

    s/

    ton

    costs /

    m3

    (euros)

    Cem | 52.5 R 120 84.7 10.16 - - -Cem ||| A 52.5 245 81.1 19.87 320 81.1 25.95

    Additive Cugla MO 20 6.5 499 3.24 - - -

    Water 160 0.87 0.14 144 0.87 0.13

    Sand 0-4 mm 775 8.5 6.59 885 8.5 7.52

    Concrete granulate 0-16 135 10.6 1.43 140 10.6 1.48

    Gravel 4-16mm 950 11.9 11.31 910 11.9 10.83

    Total 2392 52.7 2399 45.9

    Mixture composition (Light weight aggregate concrete, LWCA)

    C45/55

    (kg/m3)

    cost

    s/

    ton

    Costs /

    m3

    (euros)

    C30/37

    (kg/m3)

    costs/

    ton

    costs /

    m3

    (euros)

    Cem | 52.5 R 350 84.7 29.65 - - -

    Cem | 32.5 R - - - 320 81.2 26.3

    Additive Tillman ON2 1.75 454 0.79 - - -

    Additive Tillman Oft3 2.45 454 1.11 - - -

    Limestone 25 77.1 1.93 - - -

    Water 151 0.87 0.13 150 0.87 0.13

    Sand 0-2 mm 489 9.0 4.40 761 9.0 6.85

    Lytag 0,5-4 mm 99 17.2 1.71 72 17.2 1.24

    Lytag 0.5-6 mm 258 17.2 4.45 186 17.2 3.21

    Lytag 6-12 mm 377 17.2 6.50 272 17.2 4.69

    Total 1753*1 50.7 1761*

    1 42.4

    *1 This is the dry density of LWAC. When the LWA particles are fully saturated, a wet density

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    of approximately 1900 kg/m3 is obtained.