Title: Chap' 7
1Chap. 7 Stress and Strain
27.1 Basic Loading Conditions
- Deformation
- relative displacement of any two points
- The extent of the shape change may depend on the
magnitude, direction, and duration of the applied
forces, material properties of the body and
environmental conditions such as heat and
humidity.
Bar AB tension by F1 bending by F2 torsion by
F3
37.2 Uniaxial tension test
- uniaxial or simple tension test
- relative displacement of any two points
47.3 Load and Elongation Diagrams
For the same material
A is stiffer than B.
?,?,? lie on a single curve.
A
?,?,?
B
Stress-strain curve
Stress-strain curve
57.4 Simple Stress
- Stress force per unit area
- ML-1T-2
shear stress (tangential)
normal stress (perpendicular)
67.5 Simple Strain
d
C
B
C
B
A
D
- tensile compressive
77.5 Simple Strain
tensile
compressive
shear
87.6 Stress-Strain Diagrams
- stress-strain diagram for axial loading
U
Y
P
E
R
Y
Offset method
P
0.002
P proportionality limit E elastic limit Y
yield point, U highest point, R rupture or
failure point
- After yield point, considerable elongation
occurs. - Offset method
- In engineering application, yield point is 0.2
of strain. - Beyond the ultimate strength, necking occurs.
yield strength
97.7 Elastic Deformations
- linearly elastic material
- nonlinearly elastic material
Y
P
- Complete recovery after the load is removed.
- Youngs modulus, elastic modulus or stiffness, E
- Stiffer material vs. more compliant material
- soft tissue,bone,
- not a single Youngs modulus
- elastic region at low stress levels
Thus, we have
107.7 Elastic Deformations
- linearly elastic material
- shear modulus or modulus of rigidity, G
- larger G, more rigid
-
G
- relationship between E and G constitutive
equations
1
117.8 Hookes Law
- spring (elastic materials)
k
1
- k spring constant, or stiffness of the spring
127.9 Plastic Deformations
- Plasticity permanent deformation
- Elasticity
U
R
Y
P
elastic strain (recoverable)
plastic strain or permanent strain
(unrecoverable)
137.10 Necking
- Necking
- increased rate of deformation beyond the
ultimate strength - conventional stress
- true or actual stress
- considering actual area due to the rapid
elongation - increasing strain with decreasing stress
Necking
Conventional and actual stress-strain curve
147.11 Work and Strain Energy
Y
- elastic strain energy
- Internal work done elastic strain energy
- plastic strain energy dissipated as heat while
deforming the body
Internal work done and elastic strain energy per
unit volume
157.12 Strain Hardening
167.13 Hysteresis Loop
Hysteresis loop O?A?B?C?O
Area total strain energy dissipated as heat
to deform the body in tension and
compression
A
tensile
unloading
O
B
unloading
compressive
C
177.14 Properties Based on Stress-Strain Diagram
Material 1 is stiffer than material 2.
Slope
18Ductile material
Brittle material
engineering strain
true strain
197.15 Idealized Models of Material Behavior
Rigid
Perfectly plastic (non-strain- hardening)
Elastic-perfectly plastic (non-strain-hardening)
Elastic-plastic (strain-hardening)
Rigid-plastic (strain- hardening)
Linearly elastic
207.16 Mechanical Properties of Materials
217.17 Example Problems
- Example 7.1 tension test of a circular
cylindrical rod
Tensile strain and average tensile stress?
Deformation is
Thus, tensile strain is
Tensile stress is
227.17 Example Problems
- Example 7.2 Uniaxial tension test
aluminum
steel
237.17 Example Problems
- Example 7.3 Uniaxial tension test
A
2
B
247.17 Example Problems
- Example 7.4 bone fixation device
257.17 Example Problems
- Example 7.5 simple tension test of human
cortical bone
O(0,0), A(85, 0.005), B(114, 0.010), C(128, 0.026)
O-A linearly elastic
B-C linearly plastic
For
267.17 Example Problems
Static analysis
h
A
B
C
Geometric compatibility (deflection)
for small
Stress-strain relationship
277.17 Example Problems
h
Since
,
A
B
C
Thus, stress and strain for each steel bar