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Revision 1.25 by greg, Thu Oct 27 00:51:29 2011 UTC vs.
Revision 1.37 by greg, Mon Oct 8 20:18:27 2018 UTC

# Line 1 | Line 1
1 < .\" RCSid "$Id"
1 > .\" RCSid "$Id$"
2   .\" Print using the -ms macro package
3 < .DA 10/26/2011
3 > .DA 10/08/2018
4   .LP
5 < .tl """Copyright \(co 2011 Regents, University of California
5 > .tl """Copyright \(co 2018 Regents, University of California
6   .sp 2
7   .TL
8   The
# Line 622 | Line 622 | mod trans2 id
622   8 red green blue spec urough vrough trans tspec
623   .DE
624   .LP
625 + .UL Ashik2
626 + .PP
627 + Ashik2 is the anisotropic reflectance model by Ashikhmin & Shirley.
628 + The string arguments are the same as for plastic2, but the real
629 + arguments have additional flexibility to specify the specular color.
630 + Also, rather than roughness, specular power is used, which has no
631 + physical meaning other than larger numbers are equivalent to a smoother
632 + surface.
633 + .DS
634 + mod ashik2 id
635 + 4+ ux uy uz funcfile transform
636 + 0
637 + 8 dred dgrn dblu sred sgrn sblu u-power v-power
638 + .DE
639 + .LP
640   .UL Dielectric
641   .PP
642   A dielectric material is transparent, and it refracts light
# Line 932 | Line 947 | invisible from behind.
947   Unlike other data-driven material types, the BSDF type is fully
948   supported and all parts of the distribution are properly sampled.
949   .LP
950 + .UL aBSDF
951 + .PP
952 + The aBSDF material is identical to the BSDF type with two important
953 + differences.
954 + First, proxy geometry is not supported, so there is no thickness parameter.
955 + Second, an aBSDF is assumed to have some specular through component
956 + (the 'a' stands for "aperture"), which
957 + is treated specially during the direct calculation and when viewing the
958 + material.
959 + Based on the BSDF data, the coefficient of specular transmission is
960 + determined and used for modifying unscattered shadow and view rays.
961 + .DS
962 + mod aBSDF id
963 + 5+ BSDFfile ux uy uz funcfile transform
964 + 0
965 + 0|3|6|9
966 +     rfdif gfdif bfdif
967 +     rbdif gbdif bbdif
968 +     rtdif gtdif btdif
969 + .DE
970 + .LP
971 + If a material has no specular transmitted component, it is much better
972 + to use the BSDF type with a zero thickness than to use aBSDF.
973 + .LP
974   .UL Antimatter
975   .PP
976   Antimatter is a material that can "subtract" volumes from other volumes.
# Line 946 | Line 985 | N mod1 mod2 .. modN
985   The first modifier will also be used to shade the area leaving the
986   antimatter volume and entering the regular volume.
987   If mod1 is void, the antimatter volume is completely invisible.
988 < Antimatter does not work properly with the material type "trans",
989 < and multiple antimatter surfaces should be disjoint.
988 > If shading is desired at antimatter surfaces, it is important
989 > that the related volumes are closed with outward-facing normals.
990 > Antimatter surfaces should not intersect with other antimatter boundaries,
991 > and it is unwise to use the same modifier in nested antimatter volumes.
992   The viewpoint must be outside all volumes concerned for a correct
993   rendering.
994   .NH 3
# Line 1155 | Line 1196 | between 0.1 (for tightly spaced characters) and 0.3 (f
1196   Mixtures
1197   .PP
1198   A mixture is a blend of one or more materials or textures and patterns.
1199 + Blended materials should not be light source types or virtual source types.
1200   The basic types are given below.
1201   .LP
1202   .UL Mixfunc
# Line 1551 | Line 1593 | the Ecole Polytechnique Federale de Lausanne (EPFL Uni
1593   in Lausanne, Switzerland.
1594   .NH 1
1595   References
1596 + .LP
1597 + Wang, Taoning, Gregory Ward, Eleanor Lee,
1598 + ``Efficient modeling of optically-complex, non-coplanar
1599 + exterior shading: Validation of matrix algebraic methods,''
1600 + .I "Energy & Buildings",
1601 + vol. 174, pp. 464-83, Sept. 2018.
1602 + .LP
1603 + Lee, Eleanor S., David Geisler-Moroder, Gregory Ward,
1604 + ``Modeling the direct sun component in buildings using matrix
1605 + algebraic approaches: Methods and validation,''
1606 + .I Solar Energy,
1607 + vol. 160, 15 January 2018, pp 380-395.
1608 + .LP
1609 + Ward, G., M. Kurt & N. Bonneel,
1610 + ``Reducing Anisotropic BSDF Measurement to Common Practice,''
1611 + .I Workshop on Material Appearance Modeling,
1612 + 2014.
1613 + .LP
1614 + McNeil, A., C.J. Jonsson, D. Appelfeld, G. Ward, E.S. Lee,
1615 + ``A validation of a ray-tracing tool used to generate
1616 + bi-directional scattering distribution functions for
1617 + complex fenestration systems,''
1618 + .I "Solar Energy",
1619 + 98, 404-14, November 2013.
1620   .LP
1621   Ward, G., R. Mistrick, E.S. Lee, A. McNeil, J. Jonsson,
1622   ``Simulating the Daylight Performance of Complex Fenestration Systems

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