Appendix BAnisotropic Elasticity

B.1 Elastic Orthotropic Body

In linear elasticity theory, only small changes in shape are considered, and a macroscopic‐homogeneous, linear‐elastic material is also assumed. Elastic deformations disappear completely after release. For orthotropic bodies the generalized Hooke's law applies with nine effective elasticity constants:

B.1equation
  • E1, E2, E3 modules of elasticity,
  • G23 = G32,  G13 = G31,  G12 = G21 shear modules,
  • ν12, ν21, ν23, ν32, ν13, ν31 Poisson numbers.

There is a relationship:

B.2equation

The linear‐elastic material behavior with respect to the associated material system can be characterized by nine elasticity constants Cij, or the equivalent by nine stiffness constants Sij:

B.3equation

The inverse of (B.3) is:

B.4equation

The relations between the elasticities Cij and stiffnesses Sij read:

B.5equation

and

B.6equation

The generalized Navier equations result from the equilibrium ...

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