2B18-19 Principal Values and Principal Directions of Real Symmetric Tensors

Recall the definition that is a linear transformation, transforming into . Let us suppose that and are such that,

*   for every *

     *   all in

However, if the vector  is transformed parallel to itself, then

            

*     is called an Eigen vector, and

*     is the corresponding Eigen value.

For the special case of  *  being a unit vector, it is then transformed into a vector parallel to itself.

Let  be a unit eigen vector, then

or  with              

Let

Then,

 

2B18-19 contd.