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College of
Electrical and MechanicalEngineering
BE 335 Mechanics of Materials -IIWeek 1-2
Plane Strain and Strain Transformation
Dr. Rizwan Saeed [email protected]
Dept of Mechanical Engineering,NUST, College of E&ME, Rawalpindi,
Pakistan
mailto:[email protected]:[email protected]:[email protected] -
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College of
Electrical and MechanicalEngineering
Text books and Resources Main text book: Introduction to Solid Mechanics 3rd
Edition (Irwing H. Shames and James M. Pitarresi)
Engineering Mechanics of Solids (Egor P. Popov)
Mechanics of Materials (P. Beer, E. Russell SI
Edition) Mechanics of Materials: An Integrated Learning
System (Timothy A . Philpot)
Applied Strength of Materials 5th Edition (Robert L.
Mott) MIT OPENCOURSEWARE mechanical-
engineering/2.002
Lecture Notes Sussex University UK and The
University of Manchester UK
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College of
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About the Slide Notes Slide notes are not a substitute of lecturesand you
mustmake your own notes during lectures as manydetailed problems, derivations etc., will be covered on theboard.
Slide notes will usually have contents combined from thefollowing sources
Personal notes
Text books and reference books mentioned earlier
MecMovie Website (http://web.mst.edu/~mecmovie/) Lecture Notes of J. Walt Oler (Texas Tech University) for the
book Mechanics of Materials 3rd Edition Beer-Johnston-Dewolf, available athttp://www.mhhe.com/engcs/engmech/beerjohnston/mom/le
ctureppt.mhtml
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College of
Electrical and MechanicalEngineering
Grading , Procedure and schedules
Midterm 25%Course work (assignments, quizzes, project andclass participation (Homework and attendance)
35%
Final 40%
Rememberthat besides the 3 hours of weekly lectures
at least 6 hours of self study per week are required
Assignmentswill be due within 1 week unless specifiedotherwise.
The usual procedure for submission of assignments willbe same as for last semester.
Assignments classed as Homework will not be gradeddirectly but you should expect quizzes related toHomework
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College of
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Some general points Besides presentations/lectures I will try to have more of: Activity based learning
Come prepared for topic to be covered in next class
In the class we will have group discussion and problem
solving related to that topic The group discussion and problem solving may be graded
and will be counted towards your quizzes, assignments andclass participation.
For meetings longer than 5to10 minutes appointments
should be pre-booked (preferably through email) theschedule of available slots is displayed outside my officeand also available on the websitehttps://docs.google.com/document/d/1WgoFGxJ3aMZ-uiEtbLUdcyOYxsPkH4wOp5CAZI0BBAQ/edit?hl=en_US
https://docs.google.com/document/d/1WgoFGxJ3aMZ-uiEtbLUdcyOYxsPkH4wOp5CAZI0BBAQ/edit?hl=en_UShttps://docs.google.com/document/d/1WgoFGxJ3aMZ-uiEtbLUdcyOYxsPkH4wOp5CAZI0BBAQ/edit?hl=en_UShttps://docs.google.com/document/d/1WgoFGxJ3aMZ-uiEtbLUdcyOYxsPkH4wOp5CAZI0BBAQ/edit?hl=en_UShttps://docs.google.com/document/d/1WgoFGxJ3aMZ-uiEtbLUdcyOYxsPkH4wOp5CAZI0BBAQ/edit?hl=en_UShttps://docs.google.com/document/d/1WgoFGxJ3aMZ-uiEtbLUdcyOYxsPkH4wOp5CAZI0BBAQ/edit?hl=en_US -
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College of
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4/22/2012
Topics Chap (I.HShames)
Week (Starting Monday)
Plane Strain and StrainTransformation
8 W1 -2 (12th Sep 19th Sep)
Failure Criteria 9 W2 (19th Sep)
DelPHE visit to UK W3-4 (26th Sep - 3rd Oct) classes to be rescheduled : 2 extraclasses in each of W 5, 6 and 7
Torsion 14 W5-6 (10th Oct -17th Oct)
Beams I 10-11 W 7-8 (24h Oct -31st Oct)
Midterm exam and Eid holidays W9-10 (7th Nov 14h Nov)
Beams II- III
IV 11-12-13 W11-15 (21
st
28
th
Nov
5
th
12
th
19th Dec)
Column Buckling and ElasticStability
17 W 16-17 (26th Dec 2nd Jan )
Final Exam W18 (9th Jan)
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College of
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Revisiting Solid Mechanics - I Stress and Strain
Equilibrium, compatibility and constitutive equations.
Equilibrium equations in differential form and dynamicequilibrium cases
Enforcing compatibility (displacement continuity and boundary
conditions) Materials Properties and Constitutive Equations.
The one dimensional problems Elastic response
Isotropic plasticity, residual strains and thermal strains for one
dimensional problems. Three dimensional stress state and stress strain relations
Introduction to Energy Methods and impact analysis
Stress transformation and Mohrs Circle for stress
Plane Stress and thin walled pressure vessels
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College of
Electrical and MechanicalEngineering
Plane Strain
The state of strain where the only permissible strains(non-zero) are those that lie within a plane i.e.
i.e. deformations of the material take place in parallelplanes and are the same in each of those planes.
In tensor notation :
0 zyzxzzxyy whilezero;nonarex
zzzyzx
yzyyyx
xzxyxx
ij
000
0
0
yyyx
xyxx
ij
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College of
Electrical and MechanicalEngineering
Plane Strain The Plane Strain approximation require that,
The load is uniformly distributed along the outof plane axis of the body and acts perpendicularto it
The body is not allowed to bend stretch or
shorten.
Examples: Dams, tunnelsand thick walled pressure
vessels
Image source: http://en.wikipedia.org/wiki/Stress_analysis
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College of
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Plane Strain
Examples:A plate subjected along its edgesto a uniformly distributed load andrestrained from expanding or
contracting laterally by smooth,rigid and fixed supports [1]
Consider a long bar subjected touniformly distributed transverse
loads. State of plane stress existsin any transverse section notlocated too close to the ends of thebar [1]
[1] Lecture Notes of J. Walt Oler (Texas Tech University) for the book Mechanics of Materials3rd Edition Beer-Johnston-Dewolf,
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Plain Strain - Thick Walled
Cylinders Reading Assignment (Homework): Popov : Section 5-11
to 5-13: optional module 5-14
Remember: In MOM-I we derived the relationships forprincipal stresses thin walled pressure vessels that was
plane stress
t
prt
t= hoop stress
2 = longitudinalstress
tl
lt
pr
2
2
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College of
Electrical and MechanicalEngineering
Plain Strain - Thick Walled
Cylinders Consider a cross section cut from a long cylinder
constrained at its ends and subjected only to pressureloading Any such section away from the ends will be ina state of plane strain*
Objective: To find the in-plane stress distribution
* Please see slide notes for a more generaltreatment
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Plain Strain - Thick Walled
Cylinders
At a distance rfrom the centre the normal radial stressacting on an element is r
At a distance r +drfrom the centre is
Hoop stress tvaries with rand is equal and opposite on
the two faces
drdr
d rr
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College of
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Plain Strain - Thick Walled
Cylinders
Equilibrium:Considering our element of unit depth (i.e. along
longitudinal axis) and making use of small angleapproximation for tangential stress
Simplifying and neglecting higher ordered terms
rdr 022 ddrt ddrrdrdrd
rr
0 dr
dr
rrt
1).........(..........0
rdr
d trr
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College of
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Plain Strain - Thick Walled
Cylinders Compatibility:
Requires that the displacement uof a point due to the
radial and tangential stresses is unique
Displacement at ris u
Displacement at r + dris
Hence
drdr
duu
(2)....
dr
du
dr
udrdr
duu
r
(3)....r
u
r
rurt
2
2)(2
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Plain Strain - Thick Walled
Cylinders
Constitutive Equations
For Plane Strain
Using this result in (4) and (5)
(4)..........)(1 xtrrE
(5)...........)(1
xrttE
(6)..........)(1 trxxE
0x (7)..........)( trx
(9)..........
(8)..........
trt
trr
E
E
)1(
)21)(1(
)1()21)(1(
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College of
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Constitutive relation for Plane
Strain
rt
t
r
rt
t
rE
.
)1(2)21(
00
01)1(
0)1(
1
)21)(1(
)1(
(10)..........rtrtrtE
G
)1(2
Taking note of the fact that
From eq. (8), (9) and (10) constitutive relation for ElasticPlane Strain can be expressed as
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Plain Strain - Thick Walled
Cylinders Formulation of differential Equation
Using Equations (2) and (3) in equations (8) and (9)
Back substituting in Equations (1)
(12)..........
(11)..........
r
u
dr
duEr
u
dr
duE
t
r
)1()21)(1(
)1(
)21)(1(
13).........(..........01
22
2
r
u
dr
du
rdr
ud
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College of
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Thick Walled Cylinders - Solution ofODE
The general solution for this equation which gives theradial displacement uof any point on the cylinder cross-section is given by,
A1 and A2 from boundary conditions
-ve compression
14).........(..........
drduand
r
22
1
21
rAA
r
AAu
15).........(..........-)(
-)(
oo
ii
pr
pr
r
r
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Thick Walled Cylinders - Solution ofODE
Using (14) and (15) in (11)
solving simultaneously
16).........(..........
22
22
2
22
22
1
1
211
io
oioi
io
ooii
rr
rrpp
E
A
rrrprp
E)(A
2
212
21
2
212
21
)1()21)(1(
)1()21)(1(
oo
o
ii
i
r
ArAr
AAEp
r
ArA
r
AA
Ep
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Plain Strain - Thick Walled
Cylinders Stress Distribution With equations (16) and (14) the required stress
distribution (i.e. Equation (11) and (12)) may be found.This is given as,
Where
(17)..........-
2
21
2
2
1
r
CC
r
C
C
t
r
18).........(..........
22
22
2
22
22
1
io
oioi
io
ooii
rr
rrppC
rr
rprpC
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Discussion of Results Example 5.6 Popov Sec-5-13 (old edition Sec-3-
13)
Make a comparison of the tangential stressdistribution caused by the pressure pias given by
the equation (17) (Lames formula) with thedistribution obtained in the plane stress case where
Po= 0 , Pi 0, when
a) ro
= 1.1ri
b) ro = 4ri
For Analytical Solution see book sec-5-13
Click to open MSExcel sheet with solution (Note: pi=
10MPa)
http://1%20-%202%20week/Example%205-6%20(3-6).pnghttp://mecahanics%20of%20materials.xlsx/http://mecahanics%20of%20materials.xlsx/http://mecahanics%20of%20materials.xlsx/http://mecahanics%20of%20materials.xlsx/http://mecahanics%20of%20materials.xlsx/http://1%20-%202%20week/Example%205-6%20(3-6).png -
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Plane Strain In general does a Plane Stress situation equate to a
Plane Strain situation ???
No it is not ... as also clear from the previous example
4/22/2012
)(1
zzyyxxxx E
)(1 zzxxyyyyE
)(1 yyxxzzzzE
Gxyxy2
G
xzxz
2
G
yz
yz2
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College of
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Plane Strain vs. Plane Stress
zz
yyyx
xyxx
ij
yyyx
xyxx
ij
00
0
0
000
0
0
PlaneStrain
Plane Stress
zz
yyyx
xyxx
ij
yyyx
xyxx
ij
00
0
0
000
0
0
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College of
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Strain transformation Remember the Stress Camera Virtual experiment : (MOM-Ilecture notes week 14)
Just like the stresses the strains also vary with the orientationof element under consideration.
Assignment 1a: Submission Deadline 8th October
Note there are three parts of this assignment and youshould submit all parts together.
Prove that the form of transformation equations of planestress and plane strain is similar and for isotropicHookean materials the principal planes and plane ofmaximum shear are same for stress and strain.
(hint you may use an analytical formulation based on Taylorseries expansion of displacement field and directionalderivatives or you may use geometric relations directly using agraphical method)
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Strain transformation for plane
strain
2cos2sin2
2sin2cos
22
2sin2cos22
''
''
''
xy
xxyy
yx
xy
yyxxyyxx
yy
xy
yyxxyyxx
xx
2cos2sin2
2sin2cos22
xy
xxyy
ns
xy
yyxxyyxx
nn
x
yy
x
o
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Example 1 Strain transformation
MecMovie Example 13.1
http://1%20week/m13_01_xpl_one.swfhttp://1%20week/m13_01_xpl_one.swfhttp://1%20week/m13_01_xpl_one.swfhttp://1%20week/m13_01_xpl_one.swfhttp://1%20week/m13_01_xpl_one.swfhttp://1%20week/m13_01_xpl_one.swfhttp://1%20week/m13_01_xpl_one.swf -
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Principal Strain Angle of Principal Axis
Principal Strains
Example 8-1 on the white board
Home work Example 8-2 (Shames): Construction ofMohrs Circle for plane stain please note you will usethe same procedure for Mohrs circle as you did for planestress in last semester.
yyxx
xy
2~2tan
22
,22
xy
yyxxyyxx
ba
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Strain Gages and Rosettes
Rectangular rosette
Delta rosette
Stacked delta rosette
http://1%20week/m13_05_rosette.swfhttp://1%20week/m13_05_rosette.swfhttp://1%20week/m13_05_rosette.swfhttp://1%20week/m13_05_rosette.swfhttp://1%20week/m13_05_rosette.swfhttp://1%20week/m13_05_rosette.swf -
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Strain measurement with rossettes Strain Measurement with Rosettes: Click to open
example from MecMovie
Reading Assignments (Homework)Strain Gage Selection Criteria Case Study
Pressure Vessels (Page 29 of the document StrainGage Selection and measurement.pdf )
Measurement of principal stress using Rosettes:Click to open example from MecMovie
http://1%20-%203%20week/m13_05_rosette.swfhttp://1%20-%203%20week/m13_05_rosette.swfhttp://1%20-%203%20week/m13_06_genl_rosette.swfhttp://1%20-%203%20week/m13_06_genl_rosette.swfhttp://1%20-%203%20week/m13_06_genl_rosette.swfhttp://1%20-%203%20week/m13_06_genl_rosette.swfhttp://1%20-%203%20week/m13_06_genl_rosette.swfhttp://1%20-%203%20week/m13_05_rosette.swfhttp://1%20-%203%20week/m13_05_rosette.swfhttp://1%20-%203%20week/m13_05_rosette.swf -
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Strain Gages for Principal Stresses Assignment: 1b As part of the product development process of for a new
pump, the designer has instrumented a critical area ofthe housing with a rectangular strain gage rosette (likethe one shown). Gage 1 is aligned with the horizontalcentreline of the pump inlet passage. During the testunder high capacity operating conditions the followingreadings were taken for the three arms of the gage:1 = 950; 2 = -375; 3 = 525.The material for pump housing is aluminium2014-T6. Calculate themaximum principal stress, the minimumprincipal stress and the maximum shear stressat the location where rosette is mounted.
1 2 3
Rectangular rosette
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Strain Gages for Principal Stresses Assignment 1c:
Create a spreadsheet solution that analyses the data fromstrain gage rosette and has the following features
Assumes a biaxial stress state and that the stressperpendicular to the plane of the measured strain is zero
Finds out Principal Strains and Principal Stresses Can calculate the solution for both the rectangular and delta
rosettes
Allows the user to differentiate between max in plane shearstress and absolute max shear stress (also called true max
shear stress) Allows for input of material data E and as variables
You may create the spreadsheet solution in Microsoft Excel,Calc (OpenOffice.org) or Google Spreadsheet.
Use this spread sheet to solve the assignment 1b andcompare the results.
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Quiz
30 Mech A 30 Mech B
http://quiz/Quiz%201%20-%2030MA-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MB-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MB-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MB-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MB-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MB-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MA-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MA-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MA-01-10-2010.docxhttp://quiz/Quiz%201%20-%2030MA-01-10-2010.docx