Definition of Stress
Consider a small area δA on the surface of a body (Fig. 1.1). The force acting on this area is δF
This force can be resolved into two perpendicular components
This force can be resolved into two perpendicular components
- The component of force acting normal to the area called normal force and is denoted by δFn
- The component of force acting along the plane of area is called tangential force and is denoted by δFt
Fig 1.1 Normal and Tangential Forces on a surface
When they are expressed as force per unit area they are called as normal stress and tangential stress respectively. The tangential stress is also
called shear stress
The normal stress
(1.1) |
And shear stress
(1.2) |