hes2120 lab2 2012 sem1

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1 of 9 Faculty of Engineering and Industrial Sciences HES 2120 - STRUCTURAL MECHANICS LAB. 2 - THIN WALL CYLINDER STUDENT NAME & No.:Nguyen Thanh Tung 747590x Lab. Date & Time / Demonstrator: 04-05-2012 / Hoss INTRODUCTION: The aim of this Laboratory is to compare experimental strain measurements and theoretical strain calculations for an internally pressurised aluminium thin-walled cylinder, GUNT item FL 130. Experimental strain readings will be made using a Data Logger, GUNT item FL 151. A generic view of the equipment is shown in Fig. 1 below. Two slightly different sets of equipment in use they are functionally equivalent. A sectioned view of the thin-walled cylinder, GUNT item FL 130, may be found in Fig. 3 overleaf. The equipment can act as either a closed cylinder or an open cylinder. Strain gauges provide a convenient means of measuring very small strains. A typical gauge is shown in Fig. 2a it measures linear strain ε only along its longitudinal axis. A number of strain gauges are installed at different angles to the cylinder centreline as shown in Fig. 2b. Readings from these strain gauges are monitored by FL 151 Data Logger directly as microstrain (10 -6 m/m or μm/m). Fig. 1 FL 130 Thin-wall Cylinder and FL 151 Data Logger (Generic) Fig. 2a A single Strain Gauge Fig. 2 b Strain Gauge Orientation S.G. Vers. 2A, April 2012

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Page 1: HES2120 Lab2 2012 Sem1

1 of 9

Faculty of Engineering and Industrial Sciences

HES 2120 - STRUCTURAL MECHANICS

LAB. 2 - THIN WALL CYLINDER

STUDENT NAME & No.:Nguyen Thanh Tung 747590x

Lab. Date & Time / Demonstrator: 04-05-2012 / Hoss

INTRODUCTION:

The aim of this Laboratory is to compare experimental strain measurements and theoretical strain

calculations for an internally pressurised aluminium thin-walled cylinder, GUNT item FL 130.

Experimental strain readings will be made using a Data Logger, GUNT item FL 151. A generic view

of the equipment is shown in Fig. 1 below. Two slightly different sets of equipment in use – they are

functionally equivalent. A sectioned view of the thin-walled cylinder, GUNT item FL 130, may be

found in Fig. 3 overleaf. The equipment can act as either a closed cylinder or an open cylinder.

Strain gauges provide a convenient means of measuring very small strains. A typical gauge is shown

in Fig. 2a – it measures linear strain ε only along its longitudinal axis. A number of strain gauges

are installed at different angles to the cylinder centreline as shown in Fig. 2b. Readings from these

strain gauges are monitored by FL 151 Data Logger directly as microstrain (10 -6

m/m or μm/m).

Fig. 1 – FL 130 Thin-wall Cylinder and FL 151 Data Logger (Generic)

Fig. 2a – A single Strain Gauge Fig. 2 b – Strain Gauge Orientation

S.G. – Vers. 2A, April 2012

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OPEN / CLOSED CYLINDER :

Sectioned details of FL 130 Thin-wall Cylinder Apparatus are shown in Fig. 3. The equipment can

act as either a closed or an open cylinder as follows: Screwing out the Plunger (5) seals against

Collar (7) which effectively closes end of cylinder (1). Conversely, if Plunger is screwed in, cylinder

sees no axial force and effectively acts as an open cylinder – axial reactions are carried by Frame (6).

Fig. 3 – Sectioned FL 130 Thin-wall Cylinder Apparatus (Generic)

STRAINS, STRESSES and REFERENCE AXES:

For this experiment we will use right handed reference axes as follows: centreline of cylinder is X

axis (positive to the right) and Y axis is perpendicular to this (positive up). Strain gauge angle of

inclination θ (see Fig. 4a) must be measured anti-clockwise to the positive X axis.

The Axial and Tangential (or Hoop) Stresses induced in an internally pressurised closed thin-walled

cylinder (see Fig. 4b) will therefore be in the X and Y directions respectively.

Fig. 4a – Strain Gauge Reference Axes Fig. 4b – Axial and Tangential Stresses

NOTE: x – Axis is Axial dir’n ; y – Axis is Transverse dir’n.

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EXPERIMENTAL RESULTS:

(a) OPEN CYLINDER :

(i) Release hydraulic pump Bleed Valve (if present) fully. Screw in Plunger until

pressure gauge indicates a small pre-load (say 1 Bar); this will be taken as Nominal

Zero. Screw in Bleed Valve (if present) until tight. Take strain gauge readings for

all channels using FL 151 Data Logger. (Allow readings to “settle”.)

(ii) Use hyd. pump Handle / Handwheel to increase pressure by 20 bar and hold. Take

all strain gauge readings – subtract (i) from (ii). [CAUTION : Never exceed 35

bar.]

(iii) Reduce indicated cylinder pressure to Zero.

Strain

Gauge

Channel Angle

θ

Strain p= 1 bar

(μm/m)

Strain p=21 bar

(μm/m)

Strain ∆p= 20 bar

(μm/m)

1 A1 0 o

-33 -144.1 -111.1

2 A2 - 30 o -17.7 -34.5 -16.8

3 A3 - 45 o 0.4 93 92.4

4 A4 - 60 o 18 216 197.6

5 A5 - 90 o 41.7 368.8 327.1

. .

(b) CLOSED CYLINDER: Ensure indicated pressure zero prior to start.

(iv) Release hydraulic pump Bleed Valve (if present) fully, screw out Plunger. Screw in

Bleed Valve (if present) until tight. Apply 10 bar pressure using hyd. pump Handle

/ Handwheel (to ensure Plunger seated), release Bleed Valve (if present) fully.

Screw in Plunger roughly half a turn. Screw in Bleed Valve (if present) until tight.

Apply small pre-load (say 1 Bar) using hyd. pump Handle / Handwheel; this will

be taken as our Nominal Zero. Take strain gauge readings for all channels using FL

151 Data Logger. (Allow readings to “settle”.)

(v) Increase pressure by 20 bars and hold using hyd. pump Handle / Handwheel.

Take all strain gauge readings – subtract (IV) from (v). [CAUTION: Never

exceed 35 bars.]

(vi) Reduce indicated cylinder pressure to Zero.

Strain

Gauge

Channel Angle

θ

Strain p= 1 bar

(μm/m)

Strain p= 21 bar

(μm/m)

Strain ∆p= 20 bar

(μm/m)

1 A1 0 o

120.6 174.9 54.3

2 A2 - 30 o 22.9 124 101.1

3 A3 - 45 o -90.6 69.6 160.2

4 A4 - 60 o -199.2 12 211.2

5 A5 - 90 o -333 -66.6 267

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ANALYSIS INSTRUCTIONS:

Analyse both open and closed cylinders as follows, filling out Table overleaf:

For background Theory, meaning of symbols etc. - refer to Beer, Johnston ET. Al. –

Mechanics of Materials – 5th Edition.

A. Determine Theoretical STRESS :

As the cylinder is thin-walled, the radial stress can be neglected ( Rσ = Zσ = 0) and

we have a case of Plane Stress.

Hoop or Tangential stress for a cylinder of internal radius r is determined by:

t

rp σ σ YHOOP (7.30)

Axial stress is determined: [This will of course be Zero for the open cylinder case.]

t2

rp σ σ XAXIAL (7.31)

Draw a Mohr’s Circle to scale of in-plane Stress for both open and closed cylinders

(two graphs required) – refer to Section 7.9 in Text for guidance.

B. Determine Theoretical STRAIN :

Convert stress to strain using three dimensional Hooke’s Law [Recall Zσ = 0]

E

σν.

E

σν.

E

σ ε ZYX

X (2.38)

E

σν.

E

σν.

E

σ ε ZXY

Y

C. TRANSFORM Theoretical STRAIN :

For a strain gauge inclined at an angle θ to the X axis, determine linear strain along

its own axis, ε θ , using following equation :

sinθ.cosθγθ.sinεθ.cosε ε XY

2

Y

2

Xθ (7.60)

[ Note : For this particular loading case shear stress, τXY, and hence shear strain,

γXY, will both be Zero.]

D. COMPARE with Experimental STRAIN :

At selected locations (strain gauges 1, 3 and 5), recall Experimental strains from

Results section and compare with above Theoretical strains.

Note re. Terminology used in Table overleaf: 0

θ3 45- θ,ε is the linear strain

in strain gauge No. 3, which is inclined at 045- θ .

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ANALYSIS SUMMARY TABLE:

OPEN CYLINDER - THEORY REF. QUANTITY VALUE UNITS

A XAXIAL σ σ 0 (MPa)

A YHOOP σ σ 23.3 (MPa)

B εX -107 (μm/m)

B εY 324 (μm/m)

C 0

θ1 0 θ,ε -107 (μm/m)

C 0

θ3 45- θ,ε 108.5 (μm/m)

C 0

θ5 90- θ,ε 324 (μm/m)

OPEN CYLINDER - EXPERIMENT REF. QUANTITY VALUE UNITS

D 0

θ1 0 θ,ε -111.1 (μm/m)

D 0

θ3 45- θ,ε 92.4 (μm/m)

D 0

θ5 90- θ,ε 327.1 (μm/m)

CLOSED CYLINDER - THEORY REF. QUANTITY VALUE UNITS

A XAXIAL σ σ 11.7 (MPa)

A YHOOP σ σ 23.3 (MPa)

B εX 55.7 (μm/m)

B εY 270 (μm/m)

C 0

θ1 0 θ,ε 55.7 (μm/m)

C 0

θ3 45- θ,ε 162.85 (μm/m)

C 0

θ5 90- θ,ε 270 (μm/m)

CLOSED CYLINDER - EXPERIMENT REF. QUANTITY VALUE UNITS

D 0

θ1 0 θ,ε 54.3 (μm/m)

D 0

θ3 45- θ,ε 160.2 (μm/m)

D 0

θ5 90- θ,ε 267 (μm/m)

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. .

DATA:

1 Microstrain = 10 -6

m/m or μm/m 1 bar = 105 Pa

Cylinder dimensions: Length = 400 mm; Outer diameter = 76 mm; Thickness = 3.0 mm.

Aluminium properties: Young’s Modulus, E = 72 GPa; Poisson’s ratio, ν = 0.33.

. .

LABORATORY REPORT:

Hand in your individual Lab. Report by due Date – 1 week after conducting Lab. Please scan your

report and save whole report as one PDF file (not per page), email to your demonstrator. Please

see Study Guide or Blackboard for your demonstrator’s email address. Also please refer to Subject

Outline for penalties etc.

The Report must include (in order):

(i) This 6 page handout as cover sheet /results for your report. (2 marks)

Experimental results should be recorded on page 4. Conduct analysis per enclosed

instructions for both open and closed cylinders and fill in summary of analysis in table on

page 6. Attach sample calculations as noted below.

(ii) Two Mohr’s Circles of in-plane Stress to scale (one each for open and closed cylinders)

(1 mark).

(iii) Discussion and Conclusion. Compare theoretical results with those measured and

comment on potential sources of errors (1 mark).

(iv) Sample Calculations should be included in an Appendix, attached to the end (1 mark).

The report should be brief and to the point, it is not necessary to include diagrams or a procedure

unless directly relevant to your discussion.

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Mohr’s Circle in plane Stress:

1. Mohr’s Circle of Open Cylinder in plan Stress

2. Mohr’s Circle of Close Cylinder in plan Stress

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Discussion

During the experience the data between theory and the measurement result appear a lot of

different, the data from measurement is higher or lower than theory data but that is not much. For

example, in open cylinder at angle 0 the strain is -111.1µm/m in measurements and lowers than theory

result that is -107µm/m but at angle 90 the measurement is higher than theory (327.1µm/m and

324µm/m). In closed cylinder at angle 0 the strain is 54.3µm/m lower than 55.7µm/m of theory.

Moreover, there are some impact that lead to the error of the measurement result, the most normally

result is because of the machine is not running well every time if look around and compare to other

machines people can see the different of the result. Secondly, when we applied the pressure at 1bar

and 21bar is not exactly that also given a little bit of impact to system. Addition, when we do

experiment, the hand wheel for plunger is not maximum open or tightly closed for open and closed

cylinder. The second reason is that the FL 130 Thin-wall Cylinder Apparatus is used in several years.

As the result, the values which we collected from the machine will be not accurate.

Conclusion

In conclusion, to improve the accuracy, the machine should use auto electrical pump, not

manual pump (hydraulic pump) which makes more accuracy. Moreover, we also need to maintain the

machine to make sure the values taken from the machine are similar to the first times.

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Appendix

For closed cylinder