From 516c1db3beb75ec6fa4c7775972957a9626cde80 Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Jes=C3=BAs=20Mart=C3=ADnez-Frutos?= Date: Sat, 14 Nov 2026 08:24:04 +0100 Subject: [PATCH] Example hmre_vacuum_2d: comment on the solid-vacuum coupling (HyperFEM mesh-transfer) --- examples/hmre_vacuum_2d/hmre_vacuum_2d.jl | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/examples/hmre_vacuum_2d/hmre_vacuum_2d.jl b/examples/hmre_vacuum_2d/hmre_vacuum_2d.jl index 6d70c49..0d08e00 100644 --- a/examples/hmre_vacuum_2d/hmre_vacuum_2d.jl +++ b/examples/hmre_vacuum_2d/hmre_vacuum_2d.jl @@ -10,9 +10,9 @@ # results/), the setup wrapped in a function so that it can be built for each backend, and the drivers # built with `backend` (HyperFEM branch kernel-backend). The Dirichlet conditions are written through # BoundaryConditions, and the solid–vacuum coupling prescribes the state of the solid on the interface, -# BoundaryCondition("Interface", Coupling(uhair_int_)), a function of the stage parameter of the solver -# (HyperFEM PR #249 fixed the regression of the former DirichletCoupling; the Coupling prescription -# comes with the next PR). +# BoundaryCondition("Interface", Coupling(StageBlend(uh_solid⁻, uh_solid⁺))), a function of the stage parameter +# of the solver whose nodes are located in the mesh of the solid once (HyperFEM branch mesh-transfer; before it, +# the chain of interface spaces and Interpolables of the original script). # # Usage (from the repository root, benchmark environment): # julia -t auto --project=benchmark examples/hmre_vacuum_2d/hmre_vacuum_2d.jl [mode=compare|gridap|kernel]