1-stress &strain-mechanics of materials.ppt
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Mechanics of Materials
Mechanics of Solid
Strength of MaterialsMechanics of Deformable Bodies
Eng. Mechanics Statics
Model Rigid Bodies
Mechanics of Materials
Model Deformable Bodies
Forces, LengthForces, Length, Section,
Mechanical Properties
of Materials
Mekanika Kekatan Bahan
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Mekanika kekuatan bahan
Stress AnalysisAnalisa Tegangan
Deflection AnalysisAnalisa Lendutan
Free!Bod"!Diagram, #nternal Forces, Stress Formla,
Deflection Formla
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Ilmuwan-Ilmuwan di bidang Mekanika
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Konsep "ang dignakan dalam
mekanika kekatan bahan
$ Keseimbangan
$ %km %ooke
$ Kompatibilitas &smsi!&smsi "ang dipakai'
! Bahan homogen
! Bahan isotropis! Deformasi relatif kecil
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How Materials Carry Load
asic modes of loading a material! Tension" com#ression and shear
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Stress!
Loads applied on a material are distribted o(er a srface.
For e)ample, the point load sho*nin the follo*ing figre might actall" be a niforml" distribted load
that has been replaced b" its e+i(alent point load.
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Stress is the load applied per nit area of the srface it is applied on.
ormal stress is the stress normal to a srface
and is denoted b" the s"mbol - - sigma/.
#n the abo(e figre the normal stress is niform o(er the srface of the bar
and is gi(en b"
Shear stress is the stress tangent to a srface. #f in the follo*ing figre the shear stress
ta/ that reslts in the shear load V is niforml" distribted o(er the srface,
then the shear stress can be calclated b" di(iding the shear force b" the area it is applied on.
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0nit Stress
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earing Stress
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Strain is the way engineers re#resent the distortion of a body&
A%ial strain 'normal strain( in a bar is a measure of the e%tension of a bar #er unit length of the bar
before deformation& The following figure shows a bar of initial length l o that is e%tended by
the a##lication of a load to the length l &
Strain!
1he a)ial strain, denoted b" epsilon/
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Shear strain, denoted b" gamma/,
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1ensile 1est0nia)ial 1esting
Machine'
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Standard 1ension 2opon
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Engineering Stress!Strain 2r(e
for mild steel
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Elastic Response
Hooke)s law!
%ooke3s la* for e)tension'
%ooke3s la* for shear'
E is the elastic modls
G is the shear modls
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Elastic!Plastic Response
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*oisson)s +atio
The relation between the elastic moduli '
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4enerali5ed %ooke3s La* for Mlia)ial Loading
isotropic materials
[ ]
[ ]
[ ])(1)(
1
)(1
y x z z
z x y y
z y x x
E
E
E
σ σ ν σ ε
σ σ ν σ ε
σ σ ν σ ε
+−=
+−=
+−=
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GG
GG
GG
zx xz zx xz
zy yz
zy yz
yx xy
yx xy
τ τ γ γ
τ τ γ γ
τ τ γ γ
===
===
===
Pre shear'
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6olmetric strain dring e)tension
6olmetric Strain e/'
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,actor of safety n/
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