twely, so that partices in planes parailied to the \( x_{3} X_{3} \) femain in thoe planes, and the square fice ABGH becomes the diamond-staped parallelogram aldy shown below. Ass from the mapping equations and Eq. 46.8 , we see that the deformation gradient \( F \) has the matrix form \[ \left|F_{A}\right|=\left[\begin{array}{lll} 1 & 0 & 0 \\ 0 & 1 & k \\ 0 & k & 1 \end{array}\right] \]
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We are given a deformation of a material where particles in planes parallel to the \( x_3 \) axis remain in those planes. The square face ABGH is deformed into a diamond-shaped parallelogram. We are given the deformation gradient \( F \) with its matrix Show more…
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