Transformation of components of strain (contd...)
If the axes are so chosen that they coincide with the principal axes of the surface then, 1.32 takes the form: , where are the of the new axes.
Principal axes are the roots of the equation:
![](images/image261.gif) |
(1.32) |
where is an invariant, since coefficients of 1.32 should be so.
Consider a right parallelepiped having sides OA= , OB = and OC= . Then its volume is . After deformation the right parallelepiped remains a right parallelepiped with sides , , , hence its volume is
= ![](images/image281.gif) |
(1.33) |
So that,
![](images/image283.gif) |
(1.34) |
Hence is the relative expansion in volume or the cubical expansion.
In a more general form, the ratio of a volume element in strained state to unstrained state is given as
![](images/image287.gif) |
(1.35) |
where is the cubical dilation.
|