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Revision 1.14 by greg, Tue Oct 11 16:54:26 2005 UTC vs.
Revision 1.22 by greg, Sun Jun 14 18:21:58 2009 UTC

# Line 7 | Line 7 | rtcontrib - compute contribution coefficients in a RAD
7   [
8   .B "\-n nprocs"
9   ][
10 + .B \-V
11 + ][
12 + .B "\-c count"
13 + ][
14   .B \-fo
15   |
16   .B \-r
# Line 39 | Line 43 | rtrace options
43   .B "rtcontrib [ options ] \-defaults"
44   .SH DESCRIPTION
45   .I Rtcontrib
46 < computes ray contributions (i.e., color coefficients)
46 > computes ray coefficients
47   for objects whose modifiers are named in one or more
48   .I \-m
49   settings.
# Line 54 | Line 58 | this file.
58   (No search takes place if a file name begins with a '.', '/' or '~'
59   character.)\0
60   .PP
61 + If the
62 + .I \-n
63 + option is specified with a value greater than 1, multiple
64 + .I rtrace
65 + processes will be used to accelerate computation on a shared
66 + memory machine.
67 + Note that there is no benefit to using more processes
68 + than there are local CPUs available to do the work, and the
69 + .I rtcontrib
70 + process itself may use a considerable amount of CPU time.
71 + .PP
72 + By setting the boolean
73 + .I \-V
74 + option, you may instruct
75 + .I rtcontrib
76 + to report the contribution from each material rather than the ray
77 + coefficient.
78 + This is particularly useful for light sources with directional output
79 + distributions, whose value would otherwise be lost in the shuffle.
80 + With the default
81 + .I -V-
82 + setting, the output of rtcontrib is a coefficient that must be multiplied
83 + by the radiance of each material to arrive at a final contribution.
84 + This is more convenient for computing daylight coefficeints, or cases
85 + where the actual radiance is not desired.
86 + Use the
87 + .I -V+
88 + setting when you wish to simply sum together contributions
89 + (with possible adjustment factors) to obtain a final radiance value.
90 + Combined with the
91 + .I \-i
92 + or
93 + .I \-I
94 + option, irradiance contributions are reported by
95 + .I \-V+
96 + rather than radiance, and
97 + .I \-V-
98 + coefficients contain an additonal factor of PI.
99 + .PP
100 + The
101 + .I \-c
102 + option tells
103 + .I rtcontrib
104 + how many rays to accumulate for each record.
105 + The default value is 1, meaning a full record will be produced for
106 + each input ray.
107 + For values greater than 1, contributions will be averaged together
108 + over the given number of input rays.
109 + If set to zero, only a single record will be produced at the very
110 + end, corresponding to the sum of all rays given on the input
111 + (rather than the average).
112 + This is equivalent to passing all the output records through a program like
113 + .I total(1)
114 + to sum RGB values together, but is much more efficient.
115 + Using this option, it is possible to reverse sampling, sending rays from
116 + a parallel source such as the sun to a diffuse surface, for example.
117 + Note that output flushing via zero-direction rays is disabled
118 + for accumulated evaluations.
119 + .PP
120   The output of
121   .I rtcontrib
122   has many potential uses.
# Line 68 | Line 131 | systems, such as luminaires, light pipes, and shading
131   .I Rtcontrib
132   calls
133   .I rtrace(1)
134 < with the -oTW option to calculate the daughter ray
134 > with the \-oTW (or \-oTV) option to calculate the daughter ray
135   contributions for each input ray, and the output tallies
136   are sent to one or more destinations according to the given
137   .I \-o
# Line 82 | Line 145 | option is given.
145   If instead the
146   .I \-r
147   option is specified, data recovery is attempted on existing files.
148 + (If
149 + .I "\-c 0"
150 + is used together with the
151 + .I \-r
152 + option, existing files are read in and new ray evaluations are added
153 + to the previous results, providing a convenient means for
154 + progressive simulation.)\0
155   If an output specification contains a "%s" format, this will be
156   replaced by the modifier name.
157   The
# Line 96 | Line 166 | If the number of bins is known in advance, it should b
166   .I \-bn
167   option, and this is critical for output files containing multiple values
168   per record.
169 + A variable or constant name may be given for this parameter if
170 + it has been defined via a previous
171 + .I \-f
172 + or
173 + .I \-e
174 + option.
175   Since bin numbers start from 0, the bin count is always equal to
176   the last bin plus 1.
177   Set the this value to 0 if the bin count is unknown (the default).
# Line 106 | Line 182 | and
182   .I \-o
183   options to the left of each
184   .I \-m
185 < setting affect only that modifier.
186 < (The ordering of other options is unimportant.)\0
185 > setting are the ones used for that modifier.
186 > The ordering of other options is unimportant, except for
187 > .I \-x
188 > and
189 > .I \-y
190 > if the
191 > .I \-c
192 > is 0, when they control the resolution string
193 > produced in the corresponding output.
194   .PP
195   If a
196   .I \-b
# Line 182 | Line 265 | suitable for manipulation with
265   .I pcomb(1)
266   and related tools.
267   .PP
185 If the
186 .I \-n
187 option is specified with a value greater than 1, multiple
188 .I rtrace
189 processes will be used to accelerate computation on a shared
190 memory machine.
191 Note that there is no benefit to using more processes
192 than there are local CPUs available to do the work, and the
193 .I rtcontrib
194 process itself may use a considerable amount of CPU time.
195 .PP
268   Options may be given on the command line and/or read from the
269   environment and/or read from a file.
270   A command argument beginning with a dollar sign ('$') is immediately
# Line 203 | Line 275 | replaced by the contents of the given file.
275   To compute the proportional contributions from sources modified
276   by "light1" vs. "light2" on a set of illuminance values:
277   .IP "" .2i
278 < rtcontrib -I+ @render.opt -o c_%s.dat -m light1 -m light2 scene.oct < test.dat
278 > rtcontrib \-I+ @render.opt \-o c_%s.dat \-m light1 \-m light2 scene.oct < test.dat
279   .PP
280   To generate a pair of images corresponding to these two lights'
281   contributions:
282   .IP "" .2i
283 < vwrays -ff -x 1024 -y 1024 -vf best.vf |
284 < rtcontrib -ffc `vwrays -d -x 1024 -y 1024 -vf best.vf`
285 < @render.opt -o c_%s.pic -m light1 -m light2 scene.oct
283 > vwrays \-ff \-x 1024 \-y 1024 \-vf best.vf |
284 > rtcontrib \-ffc `vwrays \-d \-x 1024 \-y 1024 \-vf best.vf`
285 > @render.opt \-o c_%s.hdr \-m light1 \-m light2 scene.oct
286   .PP
287   These images may then be recombined using the desired outputs
288   of light1 and light2:
289   .IP "" .2i
290 < pcomb -c 100 90 75 c_light1.pic -c 50 55 57 c_light2.pic > combined.pic
290 > pcomb \-c 100 90 75 c_light1.hdr \-c 50 55 57 c_light2.hdr > combined.hdr
291   .PP
292   To compute an array of illuminance contributions according to a Tregenza sky:
293   .IP "" .2i
294 < rtcontrib -I+ -b tbin -o sky.dat -m skyglow -b 0 -o ground.dat -m groundglow
295 < @render.opt -f tregenza.cal scene.oct < test.dat
294 > rtcontrib \-I+ \-b tbin \-o sky.dat \-m skyglow \-b 0 \-o ground.dat \-m groundglow
295 > @render.opt \-f tregenza.cal scene.oct < test.dat
296   .SH ENVIRONMENT
297 < RAYPATH         path to search for -f and -M files
297 > RAYPATH         path to search for \-f and \-M files
298   .SH AUTHOR
299   Greg Ward
300   .SH "SEE ALSO"
301 < cnt(1), getinfo(1), pcomb(1), pfilt(1), ra_rgbe(1),
302 < rcalc(1), rpict(1), rtrace(1), vwrays(1), ximage(1)
301 > cnt(1), genklemsamp(1), getinfo(1), pcomb(1), pfilt(1), ra_rgbe(1),
302 > rcalc(1), rpict(1), rtrace(1), total(1), vwrays(1), ximage(1)

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