Pure shear

In mechanics and geology, pure shear is a three-dimensional homogeneous flattening of a body.^[1] It is an example of irrotational strain in which body is elongated in one direction while being shortened perpendicularly. For soft materials, such as rubber, a strain state of pure shear is often used for characterizing hyperelastic and fracture mechanical behaviour.^[2] Pure shear is differentiated from simple shear in that pure shear involves no rigid body rotation. ^{[3] [4]}

The deformation gradient for pure shear is given by:

${\displaystyle F={\begin{bmatrix}1&\gamma &0\\\gamma &1&0\0円&0&1\end{bmatrix}}}${\displaystyle F={\begin{bmatrix}1&\gamma &0\\\gamma &1&0\0円&0&1\end{bmatrix}}}

Note that this gives a Green-Lagrange strain of:

${\displaystyle E={\frac {1}{2}}{\begin{bmatrix}\gamma ^{2}&2\gamma &0\2円\gamma &\gamma ^{2}&0\0円&0&0\end{bmatrix}}}${\displaystyle E={\frac {1}{2}}{\begin{bmatrix}\gamma ^{2}&2\gamma &0\2円\gamma &\gamma ^{2}&0\0円&0&0\end{bmatrix}}}

Here there is no rotation occurring, which can be seen from the equal off-diagonal components of the strain tensor. The linear approximation to the Green-Lagrange strain shows that the small strain tensor is:

${\displaystyle \epsilon ={\frac {1}{2}}{\begin{bmatrix}0&2\gamma &0\2円\gamma &0&0\0円&0&0\end{bmatrix}}}${\displaystyle \epsilon ={\frac {1}{2}}{\begin{bmatrix}0&2\gamma &0\2円\gamma &0&0\0円&0&0\end{bmatrix}}}

which has only shearing components.

• Simple shear
• Squeeze mapping

• Fluid mechanics
• Continuum mechanics
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