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.\" RCSid "$Id" |
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.\" RCSid "$Id$" |
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.\" Print using the -ms macro package |
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< |
.DA 2/17/2011 |
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> |
.DA 07/22/2025 |
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|
.LP |
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< |
.tl """Copyright \(co 2011 Regents, University of California |
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> |
.tl """Copyright \(co 2025 Regents, University of California |
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.sp 2 |
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|
.TL |
| 8 |
|
The |
| 422 |
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0 |
| 423 |
|
3 red green blue |
| 424 |
|
.DE |
| 425 |
+ |
While alternate materials that are reflective will appear as normal, |
| 426 |
+ |
indirect rays will use the mirror's reflectance rather than the |
| 427 |
+ |
alternate type. |
| 428 |
+ |
Transmitting materials are an exception, where both transmission and |
| 429 |
+ |
reflection will use the alternate type for all rays not specifically |
| 430 |
+ |
targeting virtual light sources. |
| 431 |
+ |
In this case, it is important that any reflections be purely specular |
| 432 |
+ |
(mirror-like) and equal to the mirror's reflectivity |
| 433 |
+ |
to maintain a valid result. |
| 434 |
+ |
A pure diffuse reflection may be added if desired. |
| 435 |
+ |
.PP |
| 436 |
+ |
The mirror material type reflects light sources only from the front side |
| 437 |
+ |
of a surface, regardless of any alternate material. |
| 438 |
+ |
If virtual source generation is desired on both sides, two coincident |
| 439 |
+ |
surfaces with opposite normal orientations may be employed to achieve |
| 440 |
+ |
this effect. |
| 441 |
+ |
The reflectance and alternate material type may be |
| 442 |
+ |
different for the overlapped surfaces, |
| 443 |
+ |
and the two sides will behave accordingly. |
| 444 |
|
.LP |
| 445 |
|
.UL Prism1 |
| 446 |
|
.PP |
| 641 |
|
8 red green blue spec urough vrough trans tspec |
| 642 |
|
.DE |
| 643 |
|
.LP |
| 644 |
+ |
.UL Ashik2 |
| 645 |
+ |
.PP |
| 646 |
+ |
Ashik2 is the anisotropic reflectance model by Ashikhmin & Shirley. |
| 647 |
+ |
The string arguments are the same as for plastic2, but the real |
| 648 |
+ |
arguments have additional flexibility to specify the specular color. |
| 649 |
+ |
Also, rather than roughness, specular power is used, which has no |
| 650 |
+ |
physical meaning other than larger numbers are equivalent to a smoother |
| 651 |
+ |
surface. |
| 652 |
+ |
Unlike other material types, total reflectance is the sum of |
| 653 |
+ |
diffuse and specular colors, and should be adjusted accordingly. |
| 654 |
+ |
.DS |
| 655 |
+ |
mod ashik2 id |
| 656 |
+ |
4+ ux uy uz funcfile transform |
| 657 |
+ |
0 |
| 658 |
+ |
8 dred dgrn dblu sred sgrn sblu u-power v-power |
| 659 |
+ |
.DE |
| 660 |
+ |
.LP |
| 661 |
+ |
.UL WGMDfunc |
| 662 |
+ |
.PP |
| 663 |
+ |
WGMDfunc is a more programmable version of trans2, |
| 664 |
+ |
with separate modifier paths and variables to control each component. |
| 665 |
+ |
(WGMD stands for Ward-Geisler-Moroder-Duer, which is the basis for |
| 666 |
+ |
this empirical model, similar to the previous ones beside Ashik2.)\0 |
| 667 |
+ |
The specification of this material is given below. |
| 668 |
+ |
.DS |
| 669 |
+ |
mod WGMDfunc id |
| 670 |
+ |
13+ rs_mod rs rs_urough rs_vrough |
| 671 |
+ |
ts_mod ts ts_urough ts_vrough |
| 672 |
+ |
td_mod |
| 673 |
+ |
ux uy uz funcfile transform |
| 674 |
+ |
0 |
| 675 |
+ |
9+ rfdif gfdif bfdif |
| 676 |
+ |
rbdif gbdif bbdif |
| 677 |
+ |
rtdif gtdif btdif |
| 678 |
+ |
A10 .. |
| 679 |
+ |
.DE |
| 680 |
+ |
The sum of specular reflectance ( |
| 681 |
+ |
.I rs |
| 682 |
+ |
), specular transmittance ( |
| 683 |
+ |
.I ts |
| 684 |
+ |
), diffuse reflectance ( |
| 685 |
+ |
.I "rfdif gfdif bfdif" |
| 686 |
+ |
for front and |
| 687 |
+ |
.I "rbdif gbdif bbdif" |
| 688 |
+ |
for back) |
| 689 |
+ |
and diffuse transmittance ( |
| 690 |
+ |
.I "rtdif gtdif btdif" |
| 691 |
+ |
) should be less than 1 for each |
| 692 |
+ |
channel. |
| 693 |
+ |
.PP |
| 694 |
+ |
Unique to this material, separate modifier channels are |
| 695 |
+ |
provided for each component. |
| 696 |
+ |
The main modifier is used on the diffuse reflectance, both |
| 697 |
+ |
front and back. |
| 698 |
+ |
The |
| 699 |
+ |
.I rs_mod |
| 700 |
+ |
modifier is used for specular reflectance. |
| 701 |
+ |
If "void" is given for |
| 702 |
+ |
.I rs_mod, |
| 703 |
+ |
then the specular reflection color will be white. |
| 704 |
+ |
The special "inherit" keyword may also be given, in which case |
| 705 |
+ |
specular reflectance will share the main modifier. |
| 706 |
+ |
This behavior is replicated for the specular transmittance modifier |
| 707 |
+ |
.I ts_mod, |
| 708 |
+ |
which has its own independent roughness expressions. |
| 709 |
+ |
Finally, the diffuse transmittance modifier is given as |
| 710 |
+ |
.I td_mod, |
| 711 |
+ |
which may also be "void" or "inherit". |
| 712 |
+ |
Note that any spectra or color for specular components must be |
| 713 |
+ |
carried by the named modifier(s). |
| 714 |
+ |
.PP |
| 715 |
+ |
The main advantage to this material over BRTDfunc and |
| 716 |
+ |
other programmable types described below is that the specular sampling is |
| 717 |
+ |
well-defined, so that all components are fully computed. |
| 718 |
+ |
.LP |
| 719 |
|
.UL Dielectric |
| 720 |
|
.PP |
| 721 |
|
A dielectric material is transparent, and it refracts light |
| 963 |
|
.PP |
| 964 |
|
The BSDF material type loads an XML (eXtensible Markup Language) |
| 965 |
|
file describing a bidirectional scattering distribution function. |
| 872 |
– |
|
| 966 |
|
Real arguments to this material may define additional |
| 967 |
|
diffuse components that augment the BSDF data. |
| 968 |
< |
String arguments are used to define thickness for hidden |
| 969 |
< |
objects and the "up" orientation for the material. |
| 968 |
> |
String arguments are used to define thickness for proxied |
| 969 |
> |
surfaces and the "up" orientation for the material. |
| 970 |
|
.DS |
| 971 |
|
mod BSDF id |
| 972 |
|
6+ thick BSDFfile ux uy uz funcfile transform |
| 976 |
|
rbdif gbdif bbdif |
| 977 |
|
rtdif gtdif btdif |
| 978 |
|
.DE |
| 979 |
< |
The first string argument is a "thickness" parameter that is useful |
| 980 |
< |
for hiding detail geometry for transmitting systems, e.g., |
| 981 |
< |
complex fenestration. |
| 982 |
< |
If a view or shadow ray hits a BSDF surface with non-zero specular transmission |
| 890 |
< |
and positive thickness, the ray will pass directly through with no |
| 891 |
< |
reflection or transmission due to the BSDF. |
| 979 |
> |
The first string argument is a "thickness" parameter that may be used |
| 980 |
> |
to hide detail geometry being proxied by an aggregate BSDF material. |
| 981 |
> |
If a view or shadow ray hits a BSDF proxy with non-zero thickness, |
| 982 |
> |
it will pass directly through as if the surface were not there. |
| 983 |
|
Similar to the illum type, this permits direct viewing and |
| 984 |
|
shadow testing of complex geometry. |
| 985 |
< |
In contrast, a scattered ray will use the BSDF transmission, |
| 986 |
< |
offsetting transmitted sample rays by the thickness amount |
| 987 |
< |
to avoid any intervening geometry. |
| 988 |
< |
In this manner, BSDF surfaces may act as simplified stand-ins for detailed |
| 989 |
< |
system geometry, which may still be present and visible in the simulation. |
| 990 |
< |
If the BSDF has back-side reflection data, a parallel surface should be |
| 991 |
< |
specified slightly less than the given thickness away from the front surface |
| 992 |
< |
to enclose the system geometry on both sides. |
| 993 |
< |
A zero thickness implies that the BSDF geomtery is all there is, and |
| 994 |
< |
thickness is ignored if there is no transmitted component, or transmission is |
| 995 |
< |
purely diffuse. |
| 985 |
> |
The BSDF is used when a scattered (indirect) ray hits the surface, |
| 986 |
> |
and any transmitted sample rays will be offset by the thickness amount |
| 987 |
> |
to avoid the hidden geometry and gather samples from the other side. |
| 988 |
> |
In this manner, BSDF surfaces can improve the results for indirect |
| 989 |
> |
scattering from complex systems without sacrificing appearance or |
| 990 |
> |
shadow accuracy. |
| 991 |
> |
If the BSDF has transmission and back-side reflection data, |
| 992 |
> |
a parallel BSDF surface may be |
| 993 |
> |
placed slightly less than the given thickness away from the front surface |
| 994 |
> |
to enclose the complex geometry on both sides. |
| 995 |
> |
The sign of the thickness is important, as it indicates whether the |
| 996 |
> |
proxied geometry is behind the BSDF surface (when thickness is positive) |
| 997 |
> |
or in front (when thickness is negative). |
| 998 |
|
.LP |
| 999 |
|
The second string argument is the name of the BSDF file, which is |
| 1000 |
|
found in the usual auxiliary locations. |
| 1026 |
|
Unlike other data-driven material types, the BSDF type is fully |
| 1027 |
|
supported and all parts of the distribution are properly sampled. |
| 1028 |
|
.LP |
| 1029 |
+ |
.UL aBSDF |
| 1030 |
+ |
.PP |
| 1031 |
+ |
The aBSDF material is identical to the BSDF type with two important |
| 1032 |
+ |
differences. |
| 1033 |
+ |
First, proxy geometry is not supported, so there is no thickness parameter. |
| 1034 |
+ |
Second, an aBSDF is assumed to have some specular through component |
| 1035 |
+ |
(the 'a' stands for "aperture"), which |
| 1036 |
+ |
is treated specially during the direct calculation and when viewing the |
| 1037 |
+ |
material. |
| 1038 |
+ |
Based on the BSDF data, the coefficient of specular transmission is |
| 1039 |
+ |
determined and used for modifying unscattered shadow and view rays. |
| 1040 |
+ |
.DS |
| 1041 |
+ |
mod aBSDF id |
| 1042 |
+ |
5+ BSDFfile ux uy uz funcfile transform |
| 1043 |
+ |
0 |
| 1044 |
+ |
0|3|6|9 |
| 1045 |
+ |
rfdif gfdif bfdif |
| 1046 |
+ |
rbdif gbdif bbdif |
| 1047 |
+ |
rtdif gtdif btdif |
| 1048 |
+ |
.DE |
| 1049 |
+ |
.LP |
| 1050 |
+ |
If a material has no specular transmitted component, it is much better |
| 1051 |
+ |
to use the BSDF type with a zero thickness than to use aBSDF. |
| 1052 |
+ |
.LP |
| 1053 |
|
.UL Antimatter |
| 1054 |
|
.PP |
| 1055 |
|
Antimatter is a material that can "subtract" volumes from other volumes. |
| 1064 |
|
The first modifier will also be used to shade the area leaving the |
| 1065 |
|
antimatter volume and entering the regular volume. |
| 1066 |
|
If mod1 is void, the antimatter volume is completely invisible. |
| 1067 |
< |
Antimatter does not work properly with the material type "trans", |
| 1068 |
< |
and multiple antimatter surfaces should be disjoint. |
| 1067 |
> |
If shading is desired at antimatter surfaces, it is important |
| 1068 |
> |
that the related volumes are closed with outward-facing normals. |
| 1069 |
> |
Antimatter surfaces should not intersect with other antimatter boundaries, |
| 1070 |
> |
and it is unwise to use the same modifier in nested antimatter volumes. |
| 1071 |
|
The viewpoint must be outside all volumes concerned for a correct |
| 1072 |
|
rendering. |
| 1073 |
|
.NH 3 |
| 1104 |
|
.I zdfname. |
| 1105 |
|
.DS |
| 1106 |
|
mod texdata id |
| 1107 |
< |
8+ xfunc yfunc zfunc xdfname ydfname zdfname vfname x0 x1 .. xf |
| 1107 |
> |
8+ xfunc yfunc zfunc xdfname ydfname zdfname funcfile x0 x1 .. xf |
| 1108 |
|
0 |
| 1109 |
|
n A1 A2 .. An |
| 1110 |
|
.DE |
| 1271 |
|
font such as hexbit4x1.fnt, calls for uniform spacing. |
| 1272 |
|
Reasonable magnitudes for proportional spacing are |
| 1273 |
|
between 0.1 (for tightly spaced characters) and 0.3 (for wide spacing). |
| 1274 |
+ |
.LP |
| 1275 |
+ |
.UL Spectrum |
| 1276 |
+ |
.PP |
| 1277 |
+ |
The spectrum primitive is the most basic type for introducing spectral |
| 1278 |
+ |
color to a material. |
| 1279 |
+ |
Since materials only provide RGB parameters, spectral patterns |
| 1280 |
+ |
are the only way to superimpose wavelength-dependent behavior. |
| 1281 |
+ |
.DS |
| 1282 |
+ |
mod spectrum id |
| 1283 |
+ |
0 |
| 1284 |
+ |
0 |
| 1285 |
+ |
5+ nmA nmB s1 s2 .. sN |
| 1286 |
+ |
.DE |
| 1287 |
+ |
The first two real arguments indicate the extrema of the |
| 1288 |
+ |
spectral range in nanometers. |
| 1289 |
+ |
Subsequent real values correspond to multipliers at each wavelength. |
| 1290 |
+ |
The nmA wavelength may be greater or less than nmB, |
| 1291 |
+ |
but they may not be equal, and their ordering matches |
| 1292 |
+ |
the order of the spectral values. |
| 1293 |
+ |
A minimum of 3 values must be given, which would act |
| 1294 |
+ |
more or less the same as a constant RGB multiplier. |
| 1295 |
+ |
As with RGB values, spectral quantities normally range between 0 |
| 1296 |
+ |
and 1 at each wavelength, or average to 1.0 against a standard |
| 1297 |
+ |
sensitivity functions such as V(lambda). |
| 1298 |
+ |
The best results obtain when the spectral range and number |
| 1299 |
+ |
of samples match rendering options, though resampling will handle |
| 1300 |
+ |
any differences, zero-filling wavelenths outside the nmA to nmB |
| 1301 |
+ |
range. |
| 1302 |
+ |
A warning will be issued if the given wavelength range does not |
| 1303 |
+ |
adequately cover the visible spectrum. |
| 1304 |
+ |
.LP |
| 1305 |
+ |
.UL Specfile |
| 1306 |
+ |
.PP |
| 1307 |
+ |
The specfile primitive is equivalent to the spectrum type, but |
| 1308 |
+ |
the wavelength range and values are contained in a 1-dimensional |
| 1309 |
+ |
data file. |
| 1310 |
+ |
This may be a more convenient way to specify a spectral color, |
| 1311 |
+ |
especially one corresponding to a standard illuminant such as D65 |
| 1312 |
+ |
or a library of measured spectra. |
| 1313 |
+ |
.DS |
| 1314 |
+ |
mod specfile id |
| 1315 |
+ |
1 datafile |
| 1316 |
+ |
0 |
| 1317 |
+ |
0 |
| 1318 |
+ |
.DE |
| 1319 |
+ |
As with the spectrum type, rendering wavelengths outside the defined |
| 1320 |
+ |
range will be zero-filled. |
| 1321 |
+ |
Unlike the spectrum type, the file may contain non-uniform samples. |
| 1322 |
+ |
.LP |
| 1323 |
+ |
.UL Specfunc |
| 1324 |
+ |
.PP |
| 1325 |
+ |
The specfunc primitive offers dynamic control over a spectral |
| 1326 |
+ |
pattern, similar to the colorfunc type. |
| 1327 |
+ |
.DS |
| 1328 |
+ |
mod specfunc id |
| 1329 |
+ |
2+ sfunc funcfile transform |
| 1330 |
+ |
0 |
| 1331 |
+ |
2+ nmA nmB A3 .. |
| 1332 |
+ |
.DE |
| 1333 |
+ |
Like the spectrum primitive, the wavelength range is specified |
| 1334 |
+ |
in the first two real arguments, and additional real values are |
| 1335 |
+ |
set in the evaluation context. |
| 1336 |
+ |
This function is fed a wavelenth sample |
| 1337 |
+ |
between nmA and nmB as its only argument, |
| 1338 |
+ |
and it returns the corresponding spectral intensity. |
| 1339 |
+ |
.LP |
| 1340 |
+ |
.UL Specdata |
| 1341 |
+ |
.PP |
| 1342 |
+ |
Specdata is like brightdata and colordata, but with more |
| 1343 |
+ |
than 3 specular samples. |
| 1344 |
+ |
.DS |
| 1345 |
+ |
mod specdata id |
| 1346 |
+ |
3+n+ |
| 1347 |
+ |
func datafile |
| 1348 |
+ |
funcfile x1 x2 .. xn transform |
| 1349 |
+ |
0 |
| 1350 |
+ |
m A1 A2 .. Am |
| 1351 |
+ |
.DE |
| 1352 |
+ |
The data file must have one more dimension than the coordinate |
| 1353 |
+ |
variable count, as this final dimension corresponds to the covered |
| 1354 |
+ |
spectrum. |
| 1355 |
+ |
The starting and ending wavelengths are specified in "datafile" |
| 1356 |
+ |
as well as the number of spectral samples. |
| 1357 |
+ |
The function "func" will be called with two parameters, the |
| 1358 |
+ |
interpolated spectral value for the current coordinate and the |
| 1359 |
+ |
associated wavelength. |
| 1360 |
+ |
If the spectrum is broken into 12 components, then 12 calls |
| 1361 |
+ |
will be made to "func" for the relevant ray evaluation. |
| 1362 |
+ |
.LP |
| 1363 |
+ |
.UL Specpict |
| 1364 |
+ |
.PP |
| 1365 |
+ |
Specpict is a special case of specdata, where the pattern is |
| 1366 |
+ |
a hyperspectral image stored in the common-exponent file format. |
| 1367 |
+ |
The dimensions of the image data are determined by the picture |
| 1368 |
+ |
just as with the colorpict primitive. |
| 1369 |
+ |
.DS |
| 1370 |
+ |
mod specpict id |
| 1371 |
+ |
5+ |
| 1372 |
+ |
func specfile |
| 1373 |
+ |
funcfile u v transform |
| 1374 |
+ |
0 |
| 1375 |
+ |
m A1 A2 .. Am |
| 1376 |
+ |
.DE |
| 1377 |
+ |
The function "func" is called with the interpolated pixel value |
| 1378 |
+ |
and the wavelength sample in nanometers, the same as specdata, |
| 1379 |
+ |
with as many calls made as there are components in "specfile". |
| 1380 |
|
.NH 3 |
| 1381 |
|
Mixtures |
| 1382 |
|
.PP |
| 1383 |
|
A mixture is a blend of one or more materials or textures and patterns. |
| 1384 |
+ |
Blended materials should not be light source types or virtual source types. |
| 1385 |
|
The basic types are given below. |
| 1386 |
|
.LP |
| 1387 |
|
.UL Mixfunc |
| 1714 |
|
License |
| 1715 |
|
.PP |
| 1716 |
|
.DS |
| 1717 |
< |
The Radiance Software License, Version 1.0 |
| 1717 |
> |
The Radiance Software License, Version 2.0 |
| 1718 |
|
|
| 1719 |
< |
Copyright (c) 1990 - 2008 The Regents of the University of California, |
| 1720 |
< |
through Lawrence Berkeley National Laboratory. All rights reserved. |
| 1719 |
> |
Radiance v6.0 Copyright (c) 1990 to 2025, The Regents of the University of |
| 1720 |
> |
California, through Lawrence Berkeley National Laboratory (subject to receipt |
| 1721 |
> |
of any required approvals from the U.S. Dept. of Energy). All rights reserved. |
| 1722 |
|
|
| 1723 |
|
Redistribution and use in source and binary forms, with or without |
| 1724 |
< |
modification, are permitted provided that the following conditions |
| 1498 |
< |
are met: |
| 1724 |
> |
modification, are permitted provided that the following conditions are met: |
| 1725 |
|
|
| 1726 |
< |
1. Redistributions of source code must retain the above copyright |
| 1727 |
< |
notice, this list of conditions and the following disclaimer. |
| 1726 |
> |
(1) Redistributions of source code must retain the above copyright notice, |
| 1727 |
> |
this list of conditions and the following disclaimer. |
| 1728 |
|
|
| 1729 |
< |
2. Redistributions in binary form must reproduce the above copyright |
| 1730 |
< |
notice, this list of conditions and the following disclaimer in |
| 1731 |
< |
the documentation and/or other materials provided with the |
| 1506 |
< |
distribution. |
| 1729 |
> |
(2) Redistributions in binary form must reproduce the above copyright |
| 1730 |
> |
notice, this list of conditions and the following disclaimer in the |
| 1731 |
> |
documentation and/or other materials provided with the distribution. |
| 1732 |
|
|
| 1733 |
< |
3. The end-user documentation included with the redistribution, |
| 1734 |
< |
if any, must include the following acknowledgment: |
| 1735 |
< |
"This product includes Radiance software |
| 1736 |
< |
(http://radsite.lbl.gov/) |
| 1512 |
< |
developed by the Lawrence Berkeley National Laboratory |
| 1513 |
< |
(http://www.lbl.gov/)." |
| 1514 |
< |
Alternately, this acknowledgment may appear in the software itself, |
| 1515 |
< |
if and wherever such third-party acknowledgments normally appear. |
| 1733 |
> |
(3) Neither the name of the University of California, Lawrence Berkeley |
| 1734 |
> |
National Laboratory, U.S. Dept. of Energy nor the names of its contributors |
| 1735 |
> |
may be used to endorse or promote products derived from this software |
| 1736 |
> |
without specific prior written permission. |
| 1737 |
|
|
| 1738 |
< |
4. The names "Radiance," "Lawrence Berkeley National Laboratory" |
| 1739 |
< |
and "The Regents of the University of California" must |
| 1740 |
< |
not be used to endorse or promote products derived from this |
| 1741 |
< |
software without prior written permission. For written |
| 1742 |
< |
permission, please contact [email protected]. |
| 1738 |
> |
THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS" |
| 1739 |
> |
AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE |
| 1740 |
> |
IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE |
| 1741 |
> |
ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE |
| 1742 |
> |
LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR |
| 1743 |
> |
CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF |
| 1744 |
> |
SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS |
| 1745 |
> |
INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN |
| 1746 |
> |
CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) |
| 1747 |
> |
ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE |
| 1748 |
> |
POSSIBILITY OF SUCH DAMAGE. |
| 1749 |
|
|
| 1750 |
< |
5. Products derived from this software may not be called "Radiance", |
| 1751 |
< |
nor may "Radiance" appear in their name, without prior written |
| 1752 |
< |
permission of Lawrence Berkeley National Laboratory. |
| 1753 |
< |
|
| 1754 |
< |
THIS SOFTWARE IS PROVIDED ``AS IS'' AND ANY EXPRESSED OR IMPLIED |
| 1755 |
< |
WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES |
| 1756 |
< |
OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE |
| 1757 |
< |
DISCLAIMED. IN NO EVENT SHALL Lawrence Berkeley National Laboratory OR |
| 1758 |
< |
ITS CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, |
| 1759 |
< |
SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT |
| 1533 |
< |
LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF |
| 1534 |
< |
USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND |
| 1535 |
< |
ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, |
| 1536 |
< |
OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT |
| 1537 |
< |
OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF |
| 1538 |
< |
SUCH DAMAGE. |
| 1750 |
> |
You are under no obligation whatsoever to provide any bug fixes, patches, |
| 1751 |
> |
or upgrades to the features, functionality or performance of the source |
| 1752 |
> |
code ("Enhancements") to anyone; however, if you choose to make your |
| 1753 |
> |
Enhancements available either publicly, or directly to Lawrence Berkeley |
| 1754 |
> |
National Laboratory, without imposing a separate written license agreement |
| 1755 |
> |
for such Enhancements, then you hereby grant the following license: a |
| 1756 |
> |
non-exclusive, royalty-free perpetual license to install, use, modify, |
| 1757 |
> |
prepare derivative works, incorporate into other computer software, |
| 1758 |
> |
distribute, and sublicense such enhancements or derivative works thereof, |
| 1759 |
> |
in binary and source code form. |
| 1760 |
|
.DE |
| 1761 |
|
.NH 1 |
| 1762 |
|
Acknowledgements |
| 1773 |
|
in Lausanne, Switzerland. |
| 1774 |
|
.NH 1 |
| 1775 |
|
References |
| 1776 |
+ |
.LP |
| 1777 |
+ |
Ward, Gregory J., Bruno Bueno, David Geisler-Moroder, |
| 1778 |
+ |
Lars O. Grobe, Jacob C. Jonsson, Eleanor |
| 1779 |
+ |
S. Lee, Taoning Wang, Helen Rose Wilson, |
| 1780 |
+ |
``Daylight Simulation Workflows Incorporating |
| 1781 |
+ |
Measured Bidirectional Scattering Distribution Functions,'' |
| 1782 |
+ |
.I "Energy & Buildings", |
| 1783 |
+ |
Vol. 259, No. 111890, 2022. |
| 1784 |
+ |
.LP |
| 1785 |
+ |
Wang, Taoning, Gregory Ward, Eleanor Lee, |
| 1786 |
+ |
``Efficient modeling of optically-complex, non-coplanar |
| 1787 |
+ |
exterior shading: Validation of matrix algebraic methods,'' |
| 1788 |
+ |
.I "Energy & Buildings", |
| 1789 |
+ |
vol. 174, pp. 464-83, Sept. 2018. |
| 1790 |
+ |
.LP |
| 1791 |
+ |
Lee, Eleanor S., David Geisler-Moroder, Gregory Ward, |
| 1792 |
+ |
``Modeling the direct sun component in buildings using matrix |
| 1793 |
+ |
algebraic approaches: Methods and validation,'' |
| 1794 |
+ |
.I Solar Energy, |
| 1795 |
+ |
vol. 160, 15 January 2018, pp 380-395. |
| 1796 |
+ |
.LP |
| 1797 |
+ |
Ward, G., M. Kurt & N. Bonneel, |
| 1798 |
+ |
``Reducing Anisotropic BSDF Measurement to Common Practice,'' |
| 1799 |
+ |
.I Workshop on Material Appearance Modeling, |
| 1800 |
+ |
2014. |
| 1801 |
+ |
.LP |
| 1802 |
+ |
McNeil, A., C.J. Jonsson, D. Appelfeld, G. Ward, E.S. Lee, |
| 1803 |
+ |
``A validation of a ray-tracing tool used to generate |
| 1804 |
+ |
bi-directional scattering distribution functions for |
| 1805 |
+ |
complex fenestration systems,'' |
| 1806 |
+ |
.I "Solar Energy", |
| 1807 |
+ |
98, 404-14, November 2013. |
| 1808 |
+ |
.LP |
| 1809 |
+ |
Ward, G., R. Mistrick, E.S. Lee, A. McNeil, J. Jonsson, |
| 1810 |
+ |
``Simulating the Daylight Performance of Complex Fenestration Systems |
| 1811 |
+ |
Using Bidirectional Scattering Distribution Functions within Radiance,'' |
| 1812 |
+ |
.I "Leukos", |
| 1813 |
+ |
7(4), |
| 1814 |
+ |
April 2011. |
| 1815 |
|
.LP |
| 1816 |
|
Cater, K., A. Chalmers, G. Ward, |
| 1817 |
|
``Detail to Attention: Exploiting Visual Tasks for Selective Rendering,'' |