htrdr

Solving radiative transfer in heterogeneous media
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commit b914ae95a0eadab9eba343bde0537f120b8a288e
parent ff3e19c8bb484fd1aaeebb2fe61fa5aa14106e42
Author: Vincent Forest <vincent.forest@meso-star.com>
Date:   Tue, 13 Jul 2021 13:56:57 +0200

Fix a typo in the htrdr-combustion man page

Diffstat:
Mdoc/htrdr-combustion.1.txt.in | 6+++---
1 file changed, 3 insertions(+), 3 deletions(-)

diff --git a/doc/htrdr-combustion.1.txt.in b/doc/htrdr-combustion.1.txt.in @@ -306,7 +306,7 @@ EXAMPLES Make htrdr-combustion verbose (option *-v*) and render an image of a combustion medium whose tetrahedral mesh is stored in *tetra.sth* and its associated -thermodynamic properties are saved in *thermprops.atrtp*. The spectrallyole +thermodynamic properties are saved in *thermprops.atrtp*. The spectrally varying indices of the medium are listed in the *refract_ids.atrri* file. The center of the laser surface emission is positioned at the origin and its direction is aligned to the Y axis. The definition of the rendered image is @@ -329,8 +329,8 @@ Add a combustion chamber to the previous example: its mesh is defined in *chamber.obj* while its materials are listed in *materials.mtls*. Save the volumetric acceleration structure in *octree.cache* or reused it if it was already populated in a previous run with compatible input data. Set the finest -resolution of this acceleration structure to 1000 along the major extend of the -medium and use a optical thickness criterion of 5 to build it. Use the *-f* +resolution of this acceleration structure to *1000* along the major extend of the +medium and use a optical thickness criterion of *5* to build it. Use the *-f* option to force the overwrite of the *output* file if it exists and use *-s* to speed up the rendering with the available SIMD instruction sets.