@article{BGNY2020,
title={{LDG} approximation of large deformations of prestrained plates},
author={A. Bonito and D. Guignard and R.H. Nochetto and S. Yang},
- journal={Submitted},
- year={2020},
- url = {https://arxiv.org/abs/2011.01086}
+ journal={To appear in Journal of Computational Physics},
+ year={2021},
+ url = {https://doi.org/10.1016/j.jcp.2021.110719}
}
@article{BGNY2021,
- title={Numerical analysis of the LDG method for large deformations of prestrained plates},
+ title={Numerical analysis of the {LDG} method for large deformations of prestrained plates},
author={A. Bonito and D. Guignard and R.H. Nochetto and S. Yang},
journal={Submitted},
year={2021},
url = {https://arxiv.org/abs/2106.13877}
}
+
% ------------------------------------
% References used elsewhere
% ------------------------------------
@f[
{\rm compute\_discrete\_hessians[i][q]}, \qquad 0\leq {\rm i} < {\rm n\_dofs}, \,\, 0\leq {\rm q} < {\rm n\_q\_points},
@f]
-where <code>n_dofs = fe_values.dofs_per_cell</code> is the number of degrees of freedom per cell and <code>n_q_points = quad.size()</code> is the number of quadrature points on $K_c$. For any basis function $\varphi^n$ with support on a neighboring cell, the discrete Hessian $H_h(\varphi^n)$ evaluated on $K_c$ contains only the two lifting terms, but not the term involving $D^2)h\varphi^n$, since $\varphi^n|_{K}\equiv 0$. Moreover, only the lifting over the common face $e$ is nonzero on $K_c$, namely for all $x_q\in K_c$
+where <code>n_dofs = fe_values.dofs_per_cell</code> is the number of degrees of freedom per cell and <code>n_q_points = quad.size()</code> is the number of quadrature points on $K_c$. For any basis function $\varphi^n$ with support on a neighboring cell, the discrete Hessian $H_h(\varphi^n)$ evaluated on $K_c$ contains only the two lifting terms, but not the term involving $D^2_h\varphi^n$, since $\varphi^n|_{K}\equiv 0$. Moreover, only the lifting over the common face $e$ is nonzero on $K_c$, namely for all $x_q\in K_c$
@f[
H_h(\varphi^n)(x_q)=-r_e\left(\jump{\nabla_h\varphi^n}\right)(x_q)+b_e\left(\jump{\varphi^n}\right)(x_q).
@f]