htrdr

Solving radiative transfer in heterogeneous media
git clone git://git.meso-star.fr/htrdr.git
Log | Files | Refs | README | LICENSE

commit 67609cd18c1bd3c08968e21e8b09f3250ea5e741
parent fa9e2298a7a29db30cacb0654973d5d6c2d3aba1
Author: Vincent Forest <vincent.forest@meso-star.com>
Date:   Tue,  6 Jul 2021 16:34:24 +0200

Take care of htrdr-combustion in the htrdr-image man page

Diffstat:
Mdoc/htrdr-image.5.txt | 61+++++++++++++++++++++++++++++++------------------------------
1 file changed, 31 insertions(+), 30 deletions(-)

diff --git a/doc/htrdr-image.5.txt b/doc/htrdr-image.5.txt @@ -32,36 +32,37 @@ thus ignored as well as empty lines. The first valid line stores 2 unsigned integers that represent the image definition, i.e. the number of pixels per line and per column. Then each line stores 8 pixel components. -If the image is a regular rendering in the visible part of the spectrum, the -pixel components are actually 4 pairs of floating points data representing the -pixel color encoded in the CIE 1931 XYZ color space and the per radiative path -computation time. The first, second and third pairs encode the estimated -integrated radiance in W/sr/m^2 of the X, Y and Z pixel components, -respectively. The first value of each pair is the expected value of the -estimated radiance while the second one is its associated standard deviation. -The fourth pair saves the estimate in microseconds of the per radiative path -computation time and its standard error. - -If the image is an infrared rendering the first and second pixel components -store the expected value and the standard error, respectively, of the -estimated brightness temperature in Kelvin. The third and fourth components -save the expected value and standard deviation of the pixel radiance that is -either an integrated radiance in W/sr/m^2 or a spectral radiance in -W/sr/m^2/nm whether this radiance is computed for a spectral range or for one -wavelength. The fifth and sixth pixel components are unused. Finally the last -2 pixel components save, as for a regular rendering, the estimate in -microseconds of the per radiative path computation time and its standard -error. - -If it was generating from a shortwave rendering the image is formatted as in -longwave rendering mode exepted that the first and second pixel components are -unused since no brightness temperature was evaluated in shortwave. - -For flux computations, the first and second pixel component stores the -expected value and the standard error of the pixel flux in W/m^2. As -previously, the seventh and eighth pixel components store the estimate of the +If the image is a regular *htrdr-atmosphere*(1) rendering in the visible part of +the spectrum, the pixel components are actually 4 pairs of floating points +data representing the pixel color encoded in the CIE 1931 XYZ color space and +the per radiative path computation time. The first, second and third pairs +encode the estimated integrated radiance in W/sr/m^2 of the X, Y and Z pixel +components, respectively. The first value of each pair is the expected value +of the estimated radiance while the second one is its associated standard +deviation. The fourth pair saves the estimate in microseconds of the per +radiative path computation time and its standard error. + +If the image is an infrared rendering computed by *htrdr-atmosphere*(1) the +first and second pixel components store the expected value and the standard +error, respectively, of the estimated brightness temperature in Kelvin. The +third and fourth components save the expected value and standard deviation of +the pixel radiance that is either an integrated radiance in W/sr/m^2 or a +spectral radiance in W/sr/m^2/nm whether this radiance is computed for a +spectral range or for one wavelength. The fifth and sixth pixel components are +unused. Finally the last 2 pixel components save, as for a regular rendering, +the estimate in microseconds of the per radiative path computation time and +its standard error. + +If the file stores a shortwave rendering of *htrdr-atmosphere*(1) or a +monochromatic image computed by *htrdr-combustion*(1) the data are formatted +as for infrared rendering exept that the first and second components of pixels +are not used because no brightness temperature has been evaluated. + +For flux density calculations, the first and second pixel components store the +expected value and standard error of the flux density of the pixel in W/m^2. +As before, the seventh and eighth pixel components store the estimate of the radiative path computation time in microseconds and its standard error. The -remaining components, i.e. the components 3 to 6, are unused. +remaining components, i.e. components 3 to 6, are unused. Pixels are sorted line by line, with the origin defined at the top left corner of the image. With an image definition of N by M pixels, with N the number of @@ -150,4 +151,4 @@ NOTES SEE ALSO -------- -*htpp*(1), *htrdr*(1) +*htpp*(1), *htrdr*(1), *htrdr-atmosphere*(1), *htrdr-combustion*(1)