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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

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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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    College of

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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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    College of

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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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    College of

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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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    College of

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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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    College of

    Electrical and MechanicalEngineering

    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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    College of

    Electrical and MechanicalEngineering

    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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    College of

    Electrical and MechanicalEngineering

    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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    College of

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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

    Electrical and MechanicalEngineering

    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

    Electrical and MechanicalEngineering

    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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    College of

    Electrical and MechanicalEngineering

    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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    College of

    Electrical and MechanicalEngineering

    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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    College of

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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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    College of

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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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    College of

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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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    College of

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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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    College of

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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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    College of

    Electrical and Mechanical

    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