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Chapter 2: Elasticity and Plasticity. Tensile Strength Testing Machine. Elasticity. Stress–strain curves in an elastic regime. (a) Typical curve for metals and ceramics. (b) Typical curve for rubber. Strain Energy Density. Shear Stress and Strain.

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Chapter 2: Elasticity and Plasticity


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slide3

Elasticity

Stress–strain curves in an elastic regime. (a) Typical curve for metals and ceramics. (b) Typical curve for rubber.

slide5

Shear Stress and Strain

(a) Specimen subjected to shear force. (b) Strain undergone by small cube in shearregion. (c) Specimen (cylinder)subjected to torsion by a torque T.

slide6

Poisson’s Ratio

In an isotropic material, ε11 is equal to ε22.

(a) Unit cube being extended in direction Ox3. (b) Unit

cube in body subjected to tridimensional stress; only stresses

on the three exposed faces of the cube are shown.

slide8

Mohr Circle

(a) Biaxial (or bidimensional) state of stress.

(b) Mohr circle and construction of general orientation 0X1 X2

(c) Mohr circle and construction of principal stresses and

maximum shear stresses (Method I).

anisotropy of cubic system
Anisotropy of Cubic System

Zener’s anisotropy ratio

Young’s modulus

Shear modulus

Bulk modulus

Poisson’s ratio

Lame constants

polycrystal
Polycrystal

Voigt average: assume strain is same everywhere

Reuss average: assume stress is same everywhere

porosity on young s modulus
Porosity on Young’s Modulus

Watchman and Mackenzie:

microcracks vs young s modulus cont d
Microcracks vs. Young’s Modulus (cont’d)

1973: Salganik model

1974: O’connel & Budiansky model

viscoelasticity
Viscoelasticity

n=0: plastic

n=1: linear viscous (Newtonian)

n: power law

Viscosity coefficient

Fluidity:

viscoelasticity cont d
Viscoelasticity (cont’d)

Tensile storage modulus

Tensile loss modulus

rubber elasticity
Rubber Elasticity

From thermodynamics, one can derive:

Extension ratio:

slide26

Elastic Properties of Biological Materials

(a) Stress–strain response of human vena cava: circles-loading;

squares-unloading. (Adapted from Y. C. Fung, Biomechanics (New York: Springer, 1993),p. 366.)

(b) Representation of mechanical response in terms of tangent modulus (slope of stress–strain curve) vs. stress. (Adapted from Y. C. Fung. Biomechanics, New York: Springer,1993), p. 329.)

slide30

Mesostructure of Cartilage

(a) Mesostructure of cartilage (consisting of four zones) showing differences in structure as a function of distance from surface; the bone attachment is at bottom. (From G. L. Lucas, F. W. Cooke, and E. A. Friis, A Primer on Biomechanics (New York:

Springer, 1999), p. 273.)

(b) Cross-section of human cartilage showing regions drawn

schematically in (a). (Courtesy of K. D. Jadin and R. I. Shah.)

slide31

Mechanical Behavior of Superficial Zone of Cartilage

Stress–strain curve for samples from the superficial zone

of articular cartilage. Samples were cut parallel and perpendicular to collagen fiber orientation. (From

G. E. Kempson, Mechanical Properties of Articular Cartilage.

In Adult Articular Cartilage, ed. M. A. R. Freeman (London: Sir Isaac Pitman and Sons Ltd., 1973), pp. 171–228.)

slide34

Stresses Acting on a Thin Film

Effect of stresses acting on thin film on bending of

substrate; (a) tensile stresses in thin film; (b) compressive stresses in thin film.

slide35

Elastic Constant and Bonding

Two atoms with an imaginary spring between them; (a)

equilibrium position; (b) stretched configuration under tensile force; (c) compressed configuration under compressive force.

slide36

Attraction and Repulsion Between Two Atoms

(a) Interaction energies (attractive and repulsive terms) as

a function of separation; (b) Force between two atoms as a function of separation; notice decrease in slope as separation increases.