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Comparing ray/src/cv/mgflib/spec.txt (file contents):
Revision 1.6 by greg, Fri Sep 2 16:04:13 1994 UTC vs.
Revision 1.9 by greg, Fri Feb 28 20:19:26 2003 UTC

# Line 1 | Line 1
1                  MATERIALS AND GEOMETRY FORMAT
2 <                SCCSid "$SunId$ LBL"
2 >                RCSid "$Id$"
3  
4   Introduction
5   ============
# Line 27 | Line 27 | current transform and the current object name.
27   Each entity is given by a short keyword, followed by space- or tab-
28   delimited arguments on a single line.  A single entity may be extended
29   over multiple lines using a backslash ('\') character right before the
30 < end of line, though no extended line may exceed 512 characters in total
31 < length.  (Given the current set of entities, even approaching 80
32 < characters would be highly unusual.)
30 > end of line, though no extended line may exceed 4096 characters in total
31 > length.
32  
33   Entities and Contexts
34   =====================
# Line 84 | Line 83 | n      dx dy dz                set surface normal for current vertex
83   c       [id [= [template]]]     get/set color context
84   cxy     x y                     set CIE (x,y) chromaticity for current color
85   cspec   l_min l_max v1 v2 ..    set relative spectrum for current color
86 + cct     temperature             set spectrum based on black body temperature
87   cmix    w1 c1 w2 c2 ..          mix named colors to make current color
88   m       [id [= [template]]]     get/set material context
89   sides   {1|2}                   set number of sides for current material
# Line 92 | Line 92 | td     tau_d                   set diffuse transmittance for current mater
92   ed      epsilon_d               set diffuse emittance for current material
93   rs      rho_s alpha_r           set specular reflectance for current material
94   ts      tau_s alpha_t           set specular transmittance for current material
95 + ir      n_real n_imag           set index of refraction for current material
96   o       [name]                  begin/end object context
97   f       v1 v2 v3 ..             polygon using current material, spec. vertices
98   sph     vc radius               sphere
# Line 214 | Line 215 | A CIE xy chromaticity pair is the most basic color spe
215   full spectrum is the most general specification, and the starting (i.e.
216   minimum) and ending (i.e. maximum) wavelengths are given along with a
217   set of evenly spaced values.  Wavelengths are given in nanometers, and
218 < must be within the range of 380-780.  The spectral values themselves,
218 > should be within the range of 380-780.  The spectral values themselves,
219   which can be thought of as relative power density per nanometer, start
220   at the first wavelength and proceed at even increments to the last
221   wavelength.  The values in between will be interpolated as necessary,
222 < so there must be at least two specified points.  The color mixing
223 < entity is intended not only for the mixing of named colors, but also
224 < for color specifications  using an arbitrary set of basis functions.
225 < The mixing coefficients are in effect relative luminances for each
226 < color "primary."  The actual total of the mixing coefficients or
227 < spectral values is irrelevant, since the results will always be
228 < normalized.
222 > so there must be at least two specified points.  The color temperature
223 > entity corresponds to the spectrum of a black body at the specified
224 > temperature (in degrees Kelvin).  The color mixing entity is intended
225 > not only for the mixing of named colors, but also for color
226 > specifications  using an arbitrary set of basis functions.  The mixing
227 > coefficients are in effect relative luminances for each color
228 > "primary."  The actual total of the mixing coefficients or spectral
229 > values is irrelevant, since the results will always be normalized.
230  
231   Diffuse emittance is always given in SI units of lumens/meter^2.  Note that
232   this is emittance, not exitance, and does not include light reflected or
# Line 237 | Line 239 | be scattered.
239  
240   The sum of the diffuse and specular reflectances and transmittances
241   must be strictly less than one (with no negative values, obviously).
242 + These values are assumed to be measured at normal incidence.  If an
243 + index of refraction is given, this may modify the balance between
244 + diffuse and specular reflectance at other incident angles.  If the
245 + material is one-sided (see below), then it may be a dielectric interface.
246 + In this case, the specular transmittance given is that which would be
247 + measured at normal incidence for a pane of the material 5 mm thick.
248 + This is important for figuring the actual transmittance for non-planar
249 + geometries assuming a uniformly absorbing medium.  If the index of
250 + refraction has an imaginary part, then the surface is a metal and this
251 + implies other properties according to physics.  The default index of
252 + refraction is that of a vacuum, i.e. (1,0).
253  
254   The object entity establishes a hierarchical context, consisting of
255   this identifier and all those preceding.  It has no real meaning except
# Line 244 | Line 257 | to group the following surfaces up until an empty obje
257   under a descriptive name for improved file readability.
258  
259   Surfaces are two-sided unless the "sides" entity is used to set the
260 < number of sides for a material to one.  If a surfaces is one-sided,
260 > number of sides for a material to one.  If a surface is one-sided,
261   then it appears invisible when viewed from the back side.  This means
262   that a transmitting object will affect the light coming in through the
263   front surface and ignore the characteristics of the back surface.  As
264 < long as the characteristics are the same, the results should be
265 < correct.  If the rendering technique does not allow for one-sided
264 > long as the transmission characteristics are the same, the results should
265 > be correct.  If the rendering technique does not allow for one-sided
266   surfaces, an approximately correct result can be obtained for one-sided
267   transmitting surfaces by using the square root of the given tau_s and
268   half the given alpha_t.  If a rendering technique does not permit

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