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Faster soft and shell assembly: closed-form element mass without mass matrix
fbshipit-source-id: 2214090b49cb8ba802ebe068b8b7793bb1363756
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‎physics/docs/concepts/actors/soft/overview.mdx‎

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@@ -63,7 +63,7 @@ $$
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\mathbf{x}(\mathbf{X}) = \sum_{i=1}^{4} N_i(\mathbf{X}) \, \mathbf{x}_i~,
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$$
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where $\mathbf{x}_i$ are the current nodal positions.
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The potentials $T$, $U$, and $R$ are then integrated numerically over each element using appropriate Gaussian quadrature rules.
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The potentials $T$, $U$, and $R$ are then integrated exactly over each element.
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The resulting dynamics are discretized in time using the general [implicit-stage formulation](../../dynamics.md#mechanical-variables), with a slight modification to accommodate the strain rate in the viscoelastic damping term.
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During stage $i$, the strain rate is approximated as

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