MSR/ressources/Continuum Mechanics.md
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2024-09-25 14:50:53 +02:00

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([[Videos descriptions#continuum mechanics|video source]])
The strain tensor is the symmetric part of the gradient of the displacement field vector.
$$\varepsilon = \frac{\nabla{U} +\nabla{U}^T}{2}$$
In continuum mechanics, the force over an area is not the stress, it is traction.