TABLE OF CONTENTS In the preceding chapters we have discussed, on the one hand, the kinematics of deformation of continuous media, where the principal unknowns are the displacement vector field u and the strain tensor field 
. On the other hand, we have introduced the dynamics of deformation, representing the balance of forces in terms of the stress tensor field ? as the principal unknown.
Until now we have made no attempt to relate the strain and stress fields to each other. Before we begin the discussion of the detailed nature of this relationship, we can make the following general remarks:
Description so far is clearly incomplete, because we have at our disposal only 6 kinematic relations and 3 force balance equations for the determination of the 3+6+6 unknown functions, that is, the components of displacement u, strain , and stress ?.
We are so far unable to distinguish between different materials which might assume different deformed configurations under the same external loading. Clearly structures produced out of wood, steel, or ceramic may deform in different ways, so that the complete solutions are different.
The purpose of this chapter is to establish a class of relationships between strains and stresses known as the linear elastic constitutive law and to discuss a series of basic properties of these relationships.
We shall simply assume for now that there exists a linear relationship between the components of stress and strain tensors at each point in...
