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Revision 1.33 by greg, Thu Jul 4 01:07:25 2019 UTC vs.
Revision 1.43 by greg, Fri Jun 27 15:19:58 2025 UTC

# Line 16 | Line 16 | rtrace - trace rays in RADIANCE scene
16   .B octree
17   .br
18   .B "rtrace [ options ] \-defaults"
19 + .br
20 + .B "rtrace \-features [feat1 ..]"
21   .SH DESCRIPTION
22   .I Rtrace
23   traces rays from the standard input through the RADIANCE scene given by
# Line 35 | Line 37 | value is one or zero.
37   This may be useful for programs that run
38   .I rtrace
39   as a separate process.
40 < In the second form, the default values
40 > .PP
41 > In the second form shown above, the default values
42   for the options (modified by those options present)
43   are printed with a brief explanation.
44   .PP
45 + In the third form, a list of supported features is sent
46 + to the standard output, one per line.
47 + If additional arguments follow, they are checked for presence in
48 + this list.
49 + If a feature includes subfeatures, these may be checked as well by
50 + specifying:
51 + .nf
52 +
53 +        rtrace -features FeatName=subfeat1,subfeat2
54 +
55 + .fi
56 + If any named feature or subfeature is missing, an error is
57 + reported and the program returns an error status.
58 + If all of the named features are present, a zero status is returned.
59 + .PP
60   Options may be given on the command line and/or read from the
61   environment and/or read from a file.
62   A command argument beginning with a dollar sign ('$') is immediately
# Line 188 | Line 206 | though the
206   .I \-dv
207   option (below) may be used to override this.
208   This option is especially useful in
209 < conjunction with ximage(1) for computing illuminance at scene points.
209 > conjunction with ximage(1) for computing irradiance at scene points.
210   .TP
211   .BR \-u
212   Boolean switch to control uncorrelated random sampling.
# Line 242 | Line 260 | This is mostly useful for recovering image dimensions
260   and for creating valid Radiance picture files using the color output
261   format.
262   (See the
263 < .I \-f
263 > .I \-f\*
264   option, above.)
265   .TP
266   .BI -n \ nproc
# Line 263 | Line 281 | cores available on the system or the
281   .I \-x
282   setting, which forces a wait at each flush.
283   .TP
284 + .BI -f \ source
285 + Load function and variable definitions from the file
286 + .I source
287 + and assign at the global level.
288 + This may be convenient for altering material appearance on a per-run basis.
289 + The usual set of library directories is searched based on the
290 + .I RAYPATH
291 + environment variable.
292 + These file definitions will override same-named variables
293 + and functions in "rayinit.cal".
294 + .TP
295 + .BI -e \ expr
296 + Set initial definitions from
297 + .I expr,
298 + which may include constant assignments with the ':' character.
299 + .TP
300   .BI -dj \ frac
301   Set the direct jittering to
302   .I frac.
# Line 317 | Line 351 | change greater than the
351   specification will be calculated.
352   .TP
353   .BI -dr \ N
354 < Set the number of relays for secondary sources to
354 > Set the number of relays for virtual sources to
355   .I N.
356 < A value of 0 means that secondary sources will be ignored.
356 > A value of 0 means that virtual sources will be ignored.
357   A value of 1 means that sources will be made into first generation
358 < secondary sources; a value of 2 means that first generation
359 < secondary sources will also be made into second generation secondary
358 > virtual sources; a value of 2 means that first generation
359 > virtual sources will also be made into second generation virtual
360   sources, and so on.
361   .TP
362   .BI -dp \ D
363 < Set the secondary source presampling density to D.
363 > Set the virtual source presampling density to D.
364   This is the number of samples per steradian
365   that will be used to determine ahead of time whether or not
366   it is worth following shadow rays through all the reflections and/or
367 < transmissions associated with a secondary source path.
368 < A value of 0 means that the full secondary source path will always
367 > transmissions associated with a virtual source path.
368 > A value of 0 means that the full virtual source path will always
369   be tested for shadows if it is tested at all.
370   .TP
371   .BR \-dv
# Line 444 | Line 478 | option on the input octree.
478   Set the ambient accuracy to
479   .I acc.
480   This value will approximately equal the error
481 < from indirect illuminance interpolation.
481 > from indirect irradiance interpolation.
482   A value of zero implies no interpolation.
483   .TP
484   .BI -ad \ N
485   Set the number of ambient divisions to
486   .I N.
487   The error in the Monte Carlo calculation of indirect
488 < illuminance will be inversely proportional to the square
488 > irradiance will be inversely proportional to the square
489   root of this number.
490   A value of zero implies no indirect calculation.
491   .TP
# Line 464 | Line 498 | show a significant change.
498   .BI -af \ fname
499   Set the ambient file to
500   .I fname.
501 < This is where indirect illuminance will be stored and retrieved.
502 < Normally, indirect illuminance values are kept in memory and
501 > This is where indirect irradiance will be stored and retrieved.
502 > Normally, indirect irradiance values are kept in memory and
503   lost when the program finishes or dies.
504 < By using a file, different invocations can share illuminance
504 > By using a file, different invocations can share irradiance
505   values, saving time in the computation.
506   The ambient file is in a machine-independent binary format
507   which can be examined with
# Line 671 | Line 705 | continue rays with a probability equal to the ray weig
705   divided by the given
706   .I frac.
707   .TP
708 < .BR -ld
708 > .BR \-ld
709   Boolean switch to limit ray distance.
710   If this option is set, then rays will only be traced as far as the
711   magnitude of each direction vector.
712   Otherwise, vector magnitude is ignored and rays are traced to infinity.
713   .TP
714 + .BI -cs \ Ns
715 + Use
716 + .I Ns
717 + bands for spectral sampling rather than the default RGB calculation space.
718 + The maximum setting is controlled by the compiler macro MAXCSAMP, and
719 + defaults to 24.
720 + Larger values for Ns will be reduced to MAXCSAMP.
721 + .TP
722 + .BI -cw " nmA nmB"
723 + Set extrema to the given wavelengths for spectral sampling.
724 + The default is 380 and 780 nanometers.
725 + The order specified does not matter.
726 + .TP
727 + .BR \-co
728 + Boolean switch turns on spectral data output if selected.
729 + The default is to reduce spectral results to RGB, but see the related
730 + .I \-p*
731 + options, below.
732 + .TP
733 + .BI -pc " xr yr xg yg xb yb xw yw"
734 + Use the specified chromaticity pairs for output primaries and white
735 + point rather than the standard RGB color space.
736 + .TP
737 + .BR \-pRGB
738 + Output standard RGB values (the default).
739 + .TP
740 + .BR \-pXYZ
741 + Output standard CIE XYZ tristimulus values rather than RGB.
742 + .TP
743 + .BR \-pY
744 + Produce a single output channel corresponding to photopic luminance.
745 + .TP
746 + .BR \-pS
747 + Produce a single output channel corresponding to scotopic luminance.
748 + .TP
749 + .BR \-pM
750 + Produce a single output channel corresponding to melanopic luminance.
751 + .TP
752   .BI -e \ efile
753   Send error messages and progress reports to
754   .I efile
# Line 739 | Line 811 | To compute radiance values for the rays listed in samp
811   .IP "" .2i
812   rtrace \-ov scene.oct < samples.inp > radiance.out
813   .PP
814 < To compute illuminance values at locations selected with the 't'
814 > To compute irradiance values at locations selected with the 't'
815   command of
816   .I ximage(1):
817   .IP "" .2i
# Line 754 | Line 826 | To compute an image with an unusual view mapping:
826   cnt 480 640 | rcalc \-e 'xr:640;yr:480' \-f unusual_view.cal | rtrace
827   \-x 640 \-y 480 \-fac scene.oct > unusual.hdr
828   .PP
829 < To compute ambient illuminance in photon mapping mode from a global photon
829 > To compute ambient irradiance in photon mapping mode from a global photon
830   map global.pm via one ambient bounce, and from a caustic photon map
831   caustic.pm at sensor positions in samples.inp:
832   .IP "" .2i
# Line 777 | Line 849 | option.
849   .SH AUTHOR
850   Greg Ward
851   .SH "SEE ALSO"
852 < getinfo(1), lookamb(1), mkpmap(1), oconv(1), pfilt(1), pinterp(1),
853 < pvalue(1), rcontrib(1), rpict(1), rtpict(1), rvu(1), vwrays(1), ximage(1)
852 > dctimestep(1), getinfo(1), lookamb(1),
853 > mkpmap(1), oconv(1), pfilt(1), pinterp(1),
854 > pvalue(1), rcalc(1), rcomb(1), rcontrib(1), rcrop(1),
855 > rmtxop(1), rsplit(1),
856 > rpict(1), rtpict(1), rvu(1), vwrays(1), ximage(1)

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