Module 3 Constitutive Equations
ection The invariance of the sti ness tensor under these transformations is expressed as follows: C ijkl= Q ipQ jqQ krQ lsC pqrs (3.15) Let’s take a brief look at various classes of material symmetry, corresponding sym-metry transformations, implications on the anisotropy of the material, and the struc-ture of the sti ness tensor: x y z c b a ...
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