<i>
This program was contributed by Matthias Maier (Texas A&M University),
- and Ignacio Tomas (Sandia National Laboratories, Albuquerque).
+ and Ignacio Tomas (Sandia National Laboratories$^{\!\dagger}$).
</i>
+$^\dagger$<em>Sandia National Laboratories is a multimission laboratory
+managed and operated by National Technology & Engineering Solutions of Sandia,
+LLC, a wholly owned subsidiary of Honeywell International Inc., for the U.S.
+Department of Energy's National Nuclear Security Administration under contract
+DE-NA0003525. This document describes objective technical results and analysis.
+Any subjective views or opinions that might be expressed in the paper do not
+necessarily represent the views of the U.S. Department of Energy or the United
+States Government.</em>
+
@note This tutorial step implements a first-order accurate <i>guaranteed
maximum wavespeed method</i> based on a first-order <i>graph viscosity</i>
for solving Euler's equations of gas dynamics @cite GuermondPopov2016. As
&\ \ \ \ \texttt{scatter} (\textbf{U}^n, \mathcal{I}(i), \textbf{U}_i^n)) \\
&\textbf{end}
@f}
-<<<<<<< HEAD
+
We note here that:
- This "assembly" does not require any form of quadrature or cell-loops.
- Here $\textbf{c}$ and $\textbf{U}^n$ are a global matrix and a global vector
*
* Authors: Matthias Maier, Texas A&M University;
* Ignacio Tomas, Texas A&M University, Sandia National Laboratories
+ *
+ * Sandia National Laboratories is a multimission laboratory managed and
+ * operated by National Technology & Engineering Solutions of Sandia, LLC, a
+ * wholly owned subsidiary of Honeywell International Inc., for the U.S.
+ * Department of Energy's National Nuclear Security Administration under
+ * contract DE-NA0003525. This document describes objective technical results
+ * and analysis. Any subjective views or opinions that might be expressed in
+ * the paper do not necessarily represent the views of the U.S. Department of
+ * Energy or the United States Government.
*/
// @sect3{Include files}