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MECHANICAL BEHAVIOR
OF MATERIALS
strain & Stress
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Introduction
•
The two principal responses ofmaterials to external forces aredeformation and fracture.
The deformation may beelastic, plastic, or creep (time-dependent plastic deformation).Fracture may occur suddenly orafter repeated application of
loads (fatigue).
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Introduction
•
Fracture is the breaing of amaterial into two or morepieces. !f fracture occurs before
much plastic deformationoccurs, we say that thematerial is brittle . !n contrast, ifthere has been extensi"eplastic deformation preceding
fracture, the material is
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Introduction
uctile and Brittle material
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Introduction
Ductile Fracture Brittle Fracture
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Stress
!f the state of stress is the
same e"erywhere in a body
Stress, #, is defined as theintensity of force at a point$
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Stress
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Stress• % normal stress
(compressi"e or tensile)
is one in which the forceis normal to the area onwhich it acts.
# yy & F y '%y
• % shear stress , theforce is parallel to thearea on which it acts. # y
& F y '% is the shearstress caused by a shearforce in the y-directionacting on a plane normal
to .
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Stress
The nine components o stress actin! on anin"nitesimal element# The normal stresscomponents are σxx, σyy, and σzz. The shearstress components are σyz, σzx, σxy, σzy, σxz, and
σyx.
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Stress $ transormationo a%es
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Stress
rincipal stresses!t is always possible to nd a set of axes (*, +, ) alongwhich theshear stress components "anish. !n this case the normal
stresses, σ 1, σ 2, and σ 3, are called principal stresses
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Stress
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Stress
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Stress
• Mohr(s circle, named after
hristian tto /ohr, is a two-dimensionalgraphical representation of the stress tensor.
• The /ohr circle is used to determinegraphically the stress components acting on
a rotated coordinate system.
https://en.wikipedia.org/wiki/Christian_Otto_Mohrhttps://en.wikipedia.org/wiki/Circlehttps://en.wikipedia.org/wiki/Circlehttps://en.wikipedia.org/wiki/Christian_Otto_Mohr
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Stress
• )ra*in! Mohr(s circle$
• 0raw the artesian coordinate system (σn , τn)with a horiontal σ-axis and a "ertical τ-axis.
• 1lot two points %(σx , -τxy)and 2 (σy , +τxy) in the
space corresponding to the nown stresscomponents on both perpendicular planes.
• 0raw the diameter of the circle by 3oiningpoints % and 2 with a straight line %2.
• 0raw the /ohr ircle. The centre of thecircle is the midpoint of the diameter line%2 , which corresponds to the intersection of
this line with the σn axis.
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Stress+'lane stress,
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Stress+'lane stress,
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rientations
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Sample problem+'lanestress,
• body is loaded under stresses #x & 45 /1a,
#y & *5 /1a, 6 xy & -*4 /pa.
Find$
• the three principal stresses.
• the largest shear stress in the body.
• rientation of the principal stresses the
largest shear stress.• Sol"e the problem using setch of /ohr7s
circle diagram for this stress state.
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Sample problem+'lanestress,
• %t a point of interest on the free surfaceof an engineering component, thestresses with respect to a con"enient
coordinate system in the plane of thesurface are #x & 84, #y & +4, and 6xy &+5/1a. 0etermine the principal normaland shear stresses and their coordinate
system rotations. %lso determine themaximum normal stress and themaximum shear stress.
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Solution
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Sample problem
-od. is loaded under stresses:
Find:-the three principalstresses./the lar!est shear stress
in the -od.#-Orientation of the principal stresses thelargest shear stress.
-ol!e the pro"lem usings#etch of Mohr0s circle
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9xercises
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Strain
• %n innitesimal normal strain isdened by the change of length, :, ofa line$
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Strain
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Strain
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Strain
• There are se"eral reasons that true strainsare more con"enient than engineeringstrains.
*. True strains for e;ui"alent amounts ofdeformation in tension and compressionare e;ual except for sign.
+. True strains are additi"e. For a
deformation consisting of se"eral steps,the o"erall strain is the sum of the strainsin each step.
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Strain
• Due to a loading, the plate is deformed into the
dashed shape shown in Figure below. Determine• (a) the average normal strain along the side !,
• (b) the average shear strain in the plate at relative to
the x and y axes.
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Strain
• Part (a). "ine !, #oin#ident with the y axis,
be#omes line !$ after deformation, as shown
in Figure below.%he length of !$ is
he average normal strain for ! is therefore
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Strain
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Strain• Small strains $
Normal strain+1 ),
Strain
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Strain
• Shear strain+1 ),
The total engineering shear strain,
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Strain
Small strains can -e treated astensors
St i
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Strain
• Mohr0s strain circles