Md-03 Stress and Deformation
Transcript of Md-03 Stress and Deformation
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330:148 (g)
Machine Design
Nageswara Rao Posinasetti
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3. Stress and Deformation
Objectives
Review the types of stresses caused from axial,
bending, shear, and torsion loading. Review the relationship between stresses in the
part and the strength or stress-carrying ability ofthe part, and begin to appreciate the relationshipbetween the two.
Distinguish between the ability of a material tocarry loads in shear versus axial loading, and therelationship between these types of stresses.
Contd
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3. Stress and Deformation
Objectives (contd..) Review the principles of deformation
and whether those levels ofdeformation are acceptable to thedesign being analyzed.
Review beam deflection formulas and
their use in design problems.
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Introduction to Failure Analysis
Failure definition A part fails whenever it no longer
fulfils its required function
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Failure Analysis
Type of failures Static loads
Dynamic loads
fatigue failure Modes of failure
Ductile appreciable deformation Brittle relatively no deformation
Wear due to friction Creep elevated temperatures
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Modes of failure
Stress Deformation Wear Corrosion Vibration Environmental damage
Loosening of fastening devices
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Fig. 3.2 Tension, Compression and Shear
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Static Force
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Direct tensile force
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Static Force
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Direct compressive force
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Tensile Strength
A
F
Area
Force
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Stress, S =
Strain,
= lengthOriginal
lengthinChange
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Deformation
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lengthOriginal
nDeformatio
Strain
E
StressStrain
Area
ForceStress
AE
lF
AreaE
lengthOriginalForcen,Deformatio
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Poissons Ratio
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Axialexpansion
Lateralcompression
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Poissons Ratio
Axial strain =
Lateral strain =
Poissons ratio =
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dimensionAxial
nDeformatioAxial
dimensionLateral
nDeformatioLateral
StrainAxialStrainLateral
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Stresses and Deflections due to Bending
Beam must be primarily in purebending (no axial and shear loads)
Beam is not subjected to torsion
Beam material has the samemodulus of elasticity in tension andcompression
Beam is not subjected to localizedbuckling
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Bending moment
Reference is to a beam, assumed forconvenience to be horizontal and loadedand supported by forces, all of which lie in
a vertical plane. The bending momentat any section of the
beam is the moment of all forces that acton the beam to the left of that section,
taken about the horizontal axis of thesection.
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Bending moment
The bending moment is positive whenclockwise and negative whencounterclockwise; a positive bending
moment therefore bends the beam so thatit is concave upward, and a negativebending moment bends it so that it isconcave downward.
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Shear Force
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Negative
Counterclockwise
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3.5 Shear Force
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PositiveClockwise
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Shear force sign convention
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Positive
Clockwise
NegativeCounter clockwise
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Direct shear stress, SS
Force tends to cut through amember Punch and Die
Shear on a key in a shaft
Similar to calculating direct
tensile stressSS = Shear force / Area in shear
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3.6 Torsional Shear Stresses
Torsional shear stress, SS =
J = Polar moment of inertia = c = radius of the shaft
T = Torque d = diameter of shaft
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Torque
J
cT
32
d4
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Shear Stress in a shaft
Shear stress, SS =Where T = torque d = diameter of the shaft
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Torque
3
16
d
T
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Angular Deformation in a shaft
Angular twist, =
Where T = torque l = length of the shaft G = Modulus of rigidity of shaft material J = Polar moment of inertia of the shaft
=
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Torque
GJ
lT
32
4d