30 |
|
If the direction vector is (0,0,0), a bogus record |
31 |
|
is printed and the output is flushed if the |
32 |
|
.I -x |
33 |
< |
value is unset or zero. |
33 |
> |
value is one or zero. |
34 |
|
(See the notes on this option below.)\0 |
35 |
|
This may be useful for programs that run |
36 |
|
.I rtrace |
68 |
|
ascii, 'f' for single-precision floating point, |
69 |
|
and 'd' for double-precision floating point. |
70 |
|
In addition to these three choices, the character 'c' may be used |
71 |
< |
to denote 4-byte floating point (Radiance) color format |
72 |
< |
for the output of values only |
73 |
< |
.I (\-ov |
74 |
< |
option, below). |
71 |
> |
to denote 4-byte RGBE (Radiance) color format |
72 |
> |
for the output of individual color values only, and the |
73 |
> |
.I \-x |
74 |
> |
and |
75 |
> |
.I \-y |
76 |
> |
options should also be specified to create a valid output picture. |
77 |
|
If the output character is missing, the input format is used. |
78 |
|
.IP |
79 |
|
Note that there is no space between this option and its argument. |
113 |
|
.IP |
114 |
|
M material name |
115 |
|
.IP |
116 |
+ |
r mirrored value contribution |
117 |
+ |
.IP |
118 |
+ |
x unmirrored value contribution |
119 |
+ |
.IP |
120 |
+ |
R mirrored ray length |
121 |
+ |
.IP |
122 |
+ |
X unmirrored ray length |
123 |
+ |
.IP |
124 |
|
~ tilde (end of trace marker) |
125 |
|
.IP |
126 |
|
If the letter 't' appears in |
209 |
|
.I res. |
210 |
|
The output will be flushed after every |
211 |
|
.I res |
212 |
< |
input rays. |
212 |
> |
input rays if |
213 |
> |
.I \-y |
214 |
> |
is set to zero. |
215 |
> |
A value of one means that every ray will be flushed, whatever |
216 |
> |
the setting of |
217 |
> |
.I \-y. |
218 |
|
A value of zero means that no output flushing will take place. |
219 |
|
.TP |
220 |
|
.BI -y \ res |
245 |
|
.I \-f |
246 |
|
option, above.) |
247 |
|
.TP |
248 |
+ |
.BI -n \ nproc |
249 |
+ |
Execute in parallel on |
250 |
+ |
.I nproc |
251 |
+ |
local processes. |
252 |
+ |
This option is incompatible with the |
253 |
+ |
.I \-P |
254 |
+ |
and |
255 |
+ |
.I \-PP, |
256 |
+ |
options. |
257 |
+ |
Multiple processes also do not work properly with ray tree output |
258 |
+ |
using any of the |
259 |
+ |
.I \-o*t* |
260 |
+ |
options. |
261 |
+ |
There is no benefit from specifying more processes than there are |
262 |
+ |
cores available on the system or the |
263 |
+ |
.I \-x |
264 |
+ |
setting, which forces a wait at each flush. |
265 |
+ |
.TP |
266 |
|
.BI -dj \ frac |
267 |
|
Set the direct jittering to |
268 |
|
.I frac. |
345 |
|
.I \-i |
346 |
|
option. |
347 |
|
.TP |
348 |
< |
.BI -sj \ frac |
349 |
< |
Set the specular sampling jitter to |
350 |
< |
.I frac. |
351 |
< |
This is the degree to which the highlights are sampled |
352 |
< |
for rough specular materials. |
353 |
< |
A value of one means that all highlights will be fully sampled |
354 |
< |
using distributed ray tracing. |
348 |
> |
.BI -ss \ samp |
349 |
> |
Set the specular sampling to |
350 |
> |
.I samp. |
351 |
> |
For values less than 1, this is the degree to which the highlights |
352 |
> |
are sampled for rough specular materials. |
353 |
> |
A value greater than one causes multiple ray samples to be sent |
354 |
> |
to reduce noise at a commmesurate cost. |
355 |
|
A value of zero means that no jittering will take place, and all |
356 |
|
reflections will appear sharp even when they should be diffuse. |
357 |
|
.TP |
371 |
|
.TP |
372 |
|
.BR -bv |
373 |
|
Boolean switch for back face visibility. |
374 |
< |
With this switch off, back faces of opaque objects will be invisible |
375 |
< |
to all rays. |
374 |
> |
With this switch off, back faces of all objects will be invisible |
375 |
> |
to view rays. |
376 |
|
This is dangerous unless the model was constructed such that |
377 |
< |
all surface normals on opaque objects face outward. |
377 |
> |
all surface normals face outward. |
378 |
|
Although turning off back face visibility does not save much |
379 |
|
computation time under most circumstances, it may be useful as a |
380 |
|
tool for scene debugging, or for seeing through one-sided walls from |
381 |
|
the outside. |
349 |
– |
This option has no effect on transparent or translucent materials. |
382 |
|
.TP |
383 |
|
.BI -av " red grn blu" |
384 |
|
Set the ambient value to a radiance of |
411 |
|
.BI -ab \ N |
412 |
|
Set the number of ambient bounces to |
413 |
|
.I N. |
414 |
< |
This is the maximum number of diffuse bounces |
415 |
< |
computed by the indirect calculation. |
416 |
< |
A value of zero implies no indirect calculation. |
414 |
> |
This is the maximum number of diffuse bounces computed by the indirect |
415 |
> |
calculation. A value of zero implies no indirect calculation. |
416 |
> |
.IP |
417 |
> |
This value defaults to 1 in photon mapping mode (see |
418 |
> |
.I -ap |
419 |
> |
below), implying that global photon irradiance is always computed via |
420 |
> |
.I one |
421 |
> |
ambient bounce; this behaviour applies to any positive number of ambient |
422 |
> |
bounces, regardless of the actual value specified. A negative value enables |
423 |
> |
a preview mode that directly visualises the irradiance from the global |
424 |
> |
photon map without any ambient bounces. |
425 |
|
.TP |
426 |
|
.BI -ar \ res |
427 |
|
Set the ambient resolution to |
527 |
|
except read modifiers to be included from |
528 |
|
.I file. |
529 |
|
.TP |
530 |
+ |
.BI -ap " file [bwidth1 [bwidth2]]" |
531 |
+ |
Enable photon mapping mode. Loads a photon map generated with |
532 |
+ |
.I mkpmap(1) |
533 |
+ |
from |
534 |
+ |
.I file, |
535 |
+ |
and evaluates the indirect irradiance depending on the photon type |
536 |
+ |
(automagically detected) using density estimates with a bandwidth of |
537 |
+ |
.I bwidth1 |
538 |
+ |
photons, or the default bandwidth if none is specified (a warning will be |
539 |
+ |
issued in this case). |
540 |
+ |
.IP |
541 |
+ |
Global photon irradiance is evaluated as part of the ambient calculation (see |
542 |
+ |
.I \-ab |
543 |
+ |
above), caustic photon irradiance is evaluated at primary rays, and |
544 |
+ |
indirect inscattering in |
545 |
+ |
.I mist |
546 |
+ |
is accounted for by volume photons. Contribution photons are treated as |
547 |
+ |
global photons by |
548 |
+ |
.I rtrace. |
549 |
+ |
.IP |
550 |
+ |
Additionally specifying |
551 |
+ |
.I bwidth2 |
552 |
+ |
enables bias compensation for the density estimates with a |
553 |
+ |
minimum and maximum bandwidth of |
554 |
+ |
.I bwidth1 |
555 |
+ |
and |
556 |
+ |
.I bwidth2, |
557 |
+ |
respectively. |
558 |
+ |
.IP |
559 |
+ |
Global photon irradiance may be optionally precomputed by |
560 |
+ |
.I mkpmap(1), |
561 |
+ |
in which case the bandwidth, if specified, is ignored, as the nearest photon |
562 |
+ |
is invariably looked up. |
563 |
+ |
.IP |
564 |
+ |
Using direct photons replaces the direct calculation with density estimates |
565 |
+ |
for debugging and validation of photon emission. |
566 |
+ |
.TP |
567 |
+ |
.BI -am " frac" |
568 |
+ |
Maximum search radius for photon map lookups. Without this option, an |
569 |
+ |
initial maximum search radius is estimated for each photon map from the |
570 |
+ |
average photon distance to the distribution's centre of gravity. It is then |
571 |
+ |
adapted to the photon density in subsequent lookups. This option imposes a |
572 |
+ |
global fixed maximum search radius for |
573 |
+ |
.I all |
574 |
+ |
photon maps, thus defeating the automatic adaptation. It is useful when |
575 |
+ |
multiple warnings about short photon lookups are issued. Note that this |
576 |
+ |
option does not conflict with the bandwidth specified with the |
577 |
+ |
.I \-ap |
578 |
+ |
option; the number of photons found will not exceed the latter, but may be |
579 |
+ |
lower if the maximum search radius contains fewer photons, thus resulting in |
580 |
+ |
short lookups. Setting this radius too large, on the other hand, may |
581 |
+ |
degrade performance. |
582 |
+ |
.TP |
583 |
+ |
.BI -ac " pagesize" |
584 |
+ |
Set the photon cache page size when using out-of-core photon mapping. The |
585 |
+ |
photon cache reduces disk I/O incurred by on-demand loading (paging) of |
586 |
+ |
photons, and thus increases performance. This |
587 |
+ |
is expressed as a (float) multiple of the density estimate bandwidth |
588 |
+ |
specified with |
589 |
+ |
.I \-ap |
590 |
+ |
under the assumption that photon lookups are local to a cache page. Cache |
591 |
+ |
performance is sensitive to this parameter: larger pagesizes will reduce the |
592 |
+ |
paging frequency at the expense of higher latency when paging does occur. |
593 |
+ |
Sensible values are in the range 4 (default) to 16. |
594 |
+ |
.TP |
595 |
+ |
.BI -aC " cachesize" |
596 |
+ |
Set the total number of photons cached when using out-of-core photon |
597 |
+ |
mapping, taking into account the pagesize specified by |
598 |
+ |
.I \-ac. |
599 |
+ |
Note that this is approximate as the number of cache pages is rounded to |
600 |
+ |
the nearest prime. This allows adapting the cache to the available physical |
601 |
+ |
memory. In conjunction with the |
602 |
+ |
.I \-n |
603 |
+ |
option, this is the cache size |
604 |
+ |
.I per parallel process. |
605 |
+ |
Cache performance is less sensitive to this parameter, |
606 |
+ |
and reasonable performance can obtained with as few as 10k photons. The |
607 |
+ |
default is 1M. This option recognises multiplier suffixes (k = 1e3, M = |
608 |
+ |
1e6), both in upper and lower case. |
609 |
+ |
.TP |
610 |
|
.BI -me " rext gext bext" |
611 |
|
Set the global medium extinction coefficient to the indicated color, |
612 |
|
in units of 1/distance (distance in world coordinates). |
645 |
|
.TP |
646 |
|
.BI -lr \ N |
647 |
|
Limit reflections to a maximum of |
648 |
< |
.I N. |
648 |
> |
.I N, |
649 |
> |
if N is a positive integer. |
650 |
|
If |
651 |
|
.I N |
652 |
|
is zero or negative, then Russian roulette is used for ray |
653 |
|
termination, and the |
654 |
|
.I -lw |
655 |
|
setting (below) must be positive. |
656 |
< |
If N is a negative integer, then this sets the upper limit |
657 |
< |
of reflections past which Russian roulette will not be used. |
656 |
> |
If N is a negative integer, then this limits the maximum |
657 |
> |
number of reflections even with Russian roulette. |
658 |
|
In scenes with dielectrics and total internal reflection, |
659 |
|
a setting of 0 (no limit) may cause a stack overflow. |
660 |
|
.TP |
730 |
|
on most multiprocessing platforms, since the |
731 |
|
.I fork(2) |
732 |
|
system call will share memory on a copy-on-write basis. |
733 |
+ |
.SH NOTES |
734 |
+ |
Photons are generally surface bound (an exception are volume photons), thus |
735 |
+ |
the ambient irradiance in photon mapping mode will be biased at positions |
736 |
+ |
which do not lie on a surface. |
737 |
|
.SH EXAMPLES |
738 |
|
To compute radiance values for the rays listed in samples.inp: |
739 |
|
.IP "" .2i |
753 |
|
.IP "" .2i |
754 |
|
cnt 480 640 | rcalc \-e 'xr:640;yr:480' \-f unusual_view.cal | rtrace |
755 |
|
\-x 640 \-y 480 \-fac scene.oct > unusual.hdr |
756 |
+ |
.PP |
757 |
+ |
To compute ambient illuminance in photon mapping mode from a global photon |
758 |
+ |
map global.pm via one ambient bounce, and from a caustic photon map |
759 |
+ |
caustic.pm at sensor positions in samples.inp: |
760 |
+ |
.IP "" .2i |
761 |
+ |
rtrace -h -ov -ab 1 -ap global.pm 50 -ap caustic.pm 50 scene.oct < |
762 |
+ |
samples.inp > illum.out |
763 |
|
.SH ENVIRONMENT |
764 |
|
RAYPATH the directories to check for auxiliary files. |
765 |
|
.SH FILES |
777 |
|
.SH AUTHOR |
778 |
|
Greg Ward |
779 |
|
.SH "SEE ALSO" |
780 |
< |
getinfo(1), lookamb(1), oconv(1), pfilt(1), pinterp(1), |
781 |
< |
pvalue(1), rpict(1), rtcontrib(1), rvu(1), vwrays(1), ximage(1) |
780 |
> |
getinfo(1), lookamb(1), mkpmap(1), oconv(1), pfilt(1), pinterp(1), |
781 |
> |
pvalue(1), rcontrib(1), rsplit(1), |
782 |
> |
rpict(1), rtpict(1), rvu(1), vwrays(1), ximage(1) |