Module 1 : Introduction : Review of Basic Concepts in Mechanics
Lecture 3 : Constitutive Relations and Compatibility Conditions
 
1.3.1

Modulus of Elasticity

 

Hooke's Law provides us the relation for uniaxial stress

 

       (1.5)
 

The constant of proportionality is called the elastic modulus , modulus of elasticity or Young's modulus . Since is dimensionless the unit of E is same as that of uniaxial stress (e.g. ).

1.3.2
Poison's Ratio
 

Uniaxial forces case strains not only in its direction, but also in the transverse/lateral directions. For a tensile strain in the axial direction, there will always be compressive strains in the lateral directions, and vice versa. Poisson's Ratio ( ) relates the lateral strains to the axial strain

 

(1.6)
 

Note that this ratio is always a dimensionless positive number.

1.3.3

Coefficient of Linear Thermal Expansion

 

Linear thermal strain ( ) due to change in temperature ( ) is obtained by using this coefficient ( )

 

(1.7)
  has units of per degrees Centigrade (or Fahrenheit)
1.3.4
Shear Modulus
 

For shear stress ( ) and shear strain ( ), we have a constitutive relation similar to the Hooke's Law for linear stress and strain.

 
(1.8)
 

The constant of proportionality ( G ) is known as the shear modulus or modulus of rigidity . It has same units as modulus of elasticity ( E ). It can be proved that:

 
(1.9)
1.3.5

Dilatation and Bulk Modulus

 

Dilatation ( e ) is defined as the change of volume per unit volume

 
(1.10)
 

If a three-dimensional body is subjected to uniform hydrostatic pressure p , then the ratio of this (compressive) pressure to the dilatation is known as the bulk modulus ( k )

 
(1.11)
 

k is also called the modulus of compression .