From 3395a5e8866bb828dd9ee9d9566ddc903227fb50 Mon Sep 17 00:00:00 2001 From: Michael Zingale Date: Wed, 1 Nov 2023 12:30:51 -0400 Subject: [PATCH] update changes --- CHANGES.md | 25 +++++++++++++++++++++++++ 1 file changed, 25 insertions(+) diff --git a/CHANGES.md b/CHANGES.md index 19e9f97746..eab4c65b2e 100644 --- a/CHANGES.md +++ b/CHANGES.md @@ -1,5 +1,20 @@ # 23.11 + * Problem GNUmakefiles have been standardized and now allow for the + problem to be compiled elsewhere (#2640, #2641, #2642, #2643) + + * The true-SDC Newton solver has been made more robust and faster + (#2586, #2602, #2605, #2606) + + * Several problems that required the initial model grid spacing to + be specified in the inputs file now automatically compute it as + needed, including `flame_wave` (#2610), `convective_flame`, + `bubble_convergence`, and `hse_convergence` (#2624), `double_bubble`, + `gamma_law_bubble`, and `hse_convergence_general` (#2612) + + * Outflow boundary conditions for the 4th order solver have been changed + to no longer use the one-sided stencil (#2607) + * The ca_rad_source hook in Fortran has been removed. The existing problem_rad_source() hook in C++ can be used instead. (#2626) @@ -7,6 +22,16 @@ manually update the auxiliary parameters, you can use an external source term or you can use the problem post-timestep hook. (#2614) + * The pressure is now always included in the x-momentum flux in 1-d + Cartesian, and this fixes an issue at jumps in refinement with the + pressure gradient (#2468) + + * A bug was fixed in the 4th order diffusion operator that was introduced + when it was originally converted to C++ (#2592) + + * The 2nd order Radau integrator had the wrong quadrature weights + (#2594) + # 23.10 * True-SDC no longer evolves density as part of the reaction system