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Copy file name to clipboardExpand all lines: docs/src/topics/nonlinear-solver.md
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@@ -66,7 +66,7 @@ A simple linear viscoelastic material model in 1D in weak form is:
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\end{aligned}
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Assuming we have a single 1D element $\Omega = [-1,1]$ with linear ansatz functions and Gauss-Legendre quadrature (i.e. 2 points) the Neumann conditon $\partial_x u(1,t) = 1$ and the Dirichlet condition $u(-1,t) = 0$, then applying a Galerkin semi-discretization yields the following linear DAE in mass matrix form:
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Assuming we have a single 1D element $\Omega = [-1,1]$ with linear ansatz functions and Gauss-Legendre quadrature (i.e. 2 points) the Neumann condition $\partial_x u(1,t) = 1$ and the Dirichlet condition $u(-1,t) = 0$, then applying a Galerkin semi-discretization yields the following linear DAE in mass matrix form:
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