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Transversely isotropic elasticity

A transversely isotropic material is symmetric with respect to a rotation about an axis of symmetry. For such a material, if e3e_{3} is the axis of symmetry, then CC matrix can be expressed as:

CC matrix has following form:

C=[C11C12C13000C12C11C13000C13C13C33000000C11C122000000C44000000C44]C=\begin{bmatrix}C_{11} & C_{12} & C_{13} & 0 & 0 & 0\\ C_{12} & C_{11} & C_{13} & 0 & 0 & 0\\ C_{13} & C_{13} & C_{33} & 0 & 0 & 0\\ 0 & 0 & 0 & \frac{C_{11}-C_{12}}{2} & 0 & 0\\ 0 & 0 & 0 & 0 & C_{44} & 0\\ 0 & 0 & 0 & 0 & 0 & C_{44} \end{bmatrix}
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We need total 5 parameters to describe a transversely isotropic material.