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greg |
1.1 |
#ifndef lint |
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schorsch |
2.18 |
static const char RCSid[] = "$Id: dielectric.c,v 2.17 2003/07/27 22:12:03 schorsch Exp $"; |
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greg |
1.1 |
#endif |
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/* |
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* dielectric.c - shading function for transparent materials. |
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greg |
2.15 |
*/ |
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greg |
2.16 |
#include "copyright.h" |
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greg |
1.1 |
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#include "ray.h" |
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#include "otypes.h" |
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schorsch |
2.18 |
#include "rtotypes.h" |
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greg |
1.1 |
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| 14 |
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#ifdef DISPERSE |
| 15 |
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#include "source.h" |
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schorsch |
2.18 |
static int disperse(OBJREC *m,RAY *r,FVECT vt,double tr,COLOR cet,COLOR abt); |
| 17 |
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static int lambda(OBJREC *m, FVECT v2, FVECT dv, FVECT lr); |
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greg |
1.1 |
#endif |
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schorsch |
2.18 |
static double mylog(double x); |
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greg |
1.1 |
/* |
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* Explicit calculations for Fresnel's equation are performed, |
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* but only one square root computation is necessary. |
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* The index of refraction is given as a Hartmann equation |
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* with lambda0 equal to zero. If the slope of Hartmann's |
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* equation is non-zero, the material disperses light upon |
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* refraction. This condition is examined on rays traced to |
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* light sources. If a ray is exiting a dielectric material, we |
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* check the sources to see if any would cause bright color to be |
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* directed to the viewer due to dispersion. This gives colorful |
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* sparkle to crystals, etc. (Only if DISPERSE is defined!) |
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* |
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* Arguments for MAT_DIELECTRIC are: |
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* red grn blu rndx Hartmann |
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* |
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* Arguments for MAT_INTERFACE are: |
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* red1 grn1 blu1 rndx1 red2 grn2 blu2 rndx2 |
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* |
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* The primaries are material transmission per unit length. |
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* MAT_INTERFACE uses dielectric1 for inside and dielectric2 for |
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* outside. |
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*/ |
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#define MLAMBDA 500 /* mean lambda */ |
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#define MAXLAMBDA 779 /* maximum lambda */ |
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#define MINLAMBDA 380 /* minimum lambda */ |
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#define MINCOS 0.997 /* minimum dot product for dispersion */ |
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greg |
2.9 |
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greg |
2.10 |
static double |
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schorsch |
2.18 |
mylog( /* special log for extinction coefficients */ |
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double x |
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) |
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greg |
2.10 |
{ |
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if (x < 1e-40) |
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return(-100.); |
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if (x >= 1.) |
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return(0.); |
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return(log(x)); |
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} |
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schorsch |
2.18 |
extern int |
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m_dielectric( /* color a ray which hit a dielectric interface */ |
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OBJREC *m, |
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register RAY *r |
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) |
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greg |
1.1 |
{ |
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double cos1, cos2, nratio; |
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greg |
2.9 |
COLOR ctrans; |
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greg |
2.11 |
COLOR talb; |
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gwlarson |
2.14 |
int hastexture; |
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greg |
1.5 |
double refl, trans; |
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greg |
1.1 |
FVECT dnorm; |
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double d1, d2; |
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RAY p; |
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register int i; |
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if (m->oargs.nfargs != (m->otype==MAT_DIELECTRIC ? 5 : 8)) |
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objerror(m, USER, "bad arguments"); |
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raytexture(r, m->omod); /* get modifiers */ |
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schorsch |
2.17 |
if ( (hastexture = DOT(r->pert,r->pert) > FTINY*FTINY) ) |
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gwlarson |
2.14 |
cos1 = raynormal(dnorm, r); /* perturb normal */ |
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else { |
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VCOPY(dnorm, r->ron); |
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cos1 = r->rod; |
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} |
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greg |
1.1 |
/* index of refraction */ |
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if (m->otype == MAT_DIELECTRIC) |
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nratio = m->oargs.farg[3] + m->oargs.farg[4]/MLAMBDA; |
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else |
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nratio = m->oargs.farg[3] / m->oargs.farg[7]; |
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if (cos1 < 0.0) { /* inside */ |
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gwlarson |
2.14 |
hastexture = -hastexture; |
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greg |
1.1 |
cos1 = -cos1; |
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dnorm[0] = -dnorm[0]; |
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dnorm[1] = -dnorm[1]; |
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dnorm[2] = -dnorm[2]; |
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greg |
2.10 |
setcolor(r->cext, -mylog(m->oargs.farg[0]*colval(r->pcol,RED)), |
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-mylog(m->oargs.farg[1]*colval(r->pcol,GRN)), |
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-mylog(m->oargs.farg[2]*colval(r->pcol,BLU))); |
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greg |
2.11 |
setcolor(r->albedo, 0., 0., 0.); |
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greg |
2.9 |
r->gecc = 0.; |
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if (m->otype == MAT_INTERFACE) { |
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setcolor(ctrans, |
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greg |
2.10 |
-mylog(m->oargs.farg[4]*colval(r->pcol,RED)), |
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-mylog(m->oargs.farg[5]*colval(r->pcol,GRN)), |
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-mylog(m->oargs.farg[6]*colval(r->pcol,BLU))); |
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greg |
2.11 |
setcolor(talb, 0., 0., 0.); |
| 117 |
greg |
2.9 |
} else { |
| 118 |
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copycolor(ctrans, cextinction); |
| 119 |
greg |
2.11 |
copycolor(talb, salbedo); |
| 120 |
greg |
2.9 |
} |
| 121 |
greg |
1.1 |
} else { /* outside */ |
| 122 |
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nratio = 1.0 / nratio; |
| 123 |
greg |
2.9 |
|
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greg |
2.10 |
setcolor(ctrans, -mylog(m->oargs.farg[0]*colval(r->pcol,RED)), |
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-mylog(m->oargs.farg[1]*colval(r->pcol,GRN)), |
| 126 |
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-mylog(m->oargs.farg[2]*colval(r->pcol,BLU))); |
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greg |
2.11 |
setcolor(talb, 0., 0., 0.); |
| 128 |
greg |
2.9 |
if (m->otype == MAT_INTERFACE) { |
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setcolor(r->cext, |
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greg |
2.10 |
-mylog(m->oargs.farg[4]*colval(r->pcol,RED)), |
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-mylog(m->oargs.farg[5]*colval(r->pcol,GRN)), |
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-mylog(m->oargs.farg[6]*colval(r->pcol,BLU))); |
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greg |
2.11 |
setcolor(r->albedo, 0., 0., 0.); |
| 134 |
greg |
2.9 |
r->gecc = 0.; |
| 135 |
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} |
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greg |
1.1 |
} |
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d2 = 1.0 - nratio*nratio*(1.0 - cos1*cos1); /* compute cos theta2 */ |
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if (d2 < FTINY) /* total reflection */ |
| 141 |
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refl = 1.0; |
| 143 |
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| 144 |
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else { /* refraction occurs */ |
| 145 |
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/* compute Fresnel's equations */ |
| 146 |
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cos2 = sqrt(d2); |
| 147 |
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d1 = cos1; |
| 148 |
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d2 = nratio*cos2; |
| 149 |
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d1 = (d1 - d2) / (d1 + d2); |
| 150 |
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refl = d1 * d1; |
| 151 |
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| 152 |
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d1 = 1.0 / cos1; |
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d2 = nratio / cos2; |
| 154 |
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d1 = (d1 - d2) / (d1 + d2); |
| 155 |
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refl += d1 * d1; |
| 156 |
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greg |
2.9 |
refl *= 0.5; |
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greg |
1.1 |
trans = 1.0 - refl; |
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greg |
2.15 |
|
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trans *= nratio*nratio; /* solid angle ratio */ |
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greg |
1.1 |
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gwlarson |
2.13 |
if (rayorigin(&p, r, REFRACTED, trans) == 0) { |
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greg |
1.1 |
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/* compute refracted ray */ |
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d1 = nratio*cos1 - cos2; |
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for (i = 0; i < 3; i++) |
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p.rdir[i] = nratio*r->rdir[i] + d1*dnorm[i]; |
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gwlarson |
2.14 |
/* accidental reflection? */ |
| 169 |
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if (hastexture && |
| 170 |
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DOT(p.rdir,r->ron)*hastexture >= -FTINY) { |
| 171 |
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d1 *= (double)hastexture; |
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for (i = 0; i < 3; i++) /* ignore texture */ |
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p.rdir[i] = nratio*r->rdir[i] + |
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d1*r->ron[i]; |
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normalize(p.rdir); /* not exact */ |
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} |
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greg |
1.1 |
#ifdef DISPERSE |
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if (m->otype != MAT_DIELECTRIC |
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|| r->rod > 0.0 |
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|| r->crtype & SHADOW |
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greg |
2.3 |
|| !directvis |
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greg |
1.1 |
|| m->oargs.farg[4] == 0.0 |
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greg |
2.12 |
|| !disperse(m, r, p.rdir, |
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trans, ctrans, talb)) |
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greg |
1.1 |
#endif |
| 186 |
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{ |
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greg |
2.9 |
copycolor(p.cext, ctrans); |
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greg |
2.11 |
copycolor(p.albedo, talb); |
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greg |
1.1 |
rayvalue(&p); |
| 190 |
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scalecolor(p.rcol, trans); |
| 191 |
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addcolor(r->rcol, p.rcol); |
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greg |
2.4 |
if (nratio >= 1.0-FTINY && nratio <= 1.0+FTINY) |
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r->rt = r->rot + p.rt; |
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greg |
1.1 |
} |
| 195 |
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} |
| 196 |
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} |
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| 198 |
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if (!(r->crtype & SHADOW) && |
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gwlarson |
2.13 |
rayorigin(&p, r, REFLECTED, refl) == 0) { |
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greg |
1.1 |
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| 201 |
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/* compute reflected ray */ |
| 202 |
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for (i = 0; i < 3; i++) |
| 203 |
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p.rdir[i] = r->rdir[i] + 2.0*cos1*dnorm[i]; |
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gwlarson |
2.14 |
/* accidental penetration? */ |
| 205 |
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if (hastexture && DOT(p.rdir,r->ron)*hastexture <= FTINY) |
| 206 |
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for (i = 0; i < 3; i++) /* ignore texture */ |
| 207 |
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p.rdir[i] = r->rdir[i] + 2.0*r->rod*r->ron[i]; |
| 208 |
greg |
1.1 |
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| 209 |
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rayvalue(&p); /* reflected ray value */ |
| 210 |
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| 211 |
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scalecolor(p.rcol, refl); /* color contribution */ |
| 212 |
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addcolor(r->rcol, p.rcol); |
| 213 |
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} |
| 214 |
greg |
2.9 |
/* rayvalue() computes absorption */ |
| 215 |
greg |
2.7 |
return(1); |
| 216 |
greg |
1.1 |
} |
| 217 |
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| 218 |
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#ifdef DISPERSE |
| 220 |
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| 221 |
schorsch |
2.18 |
static int |
| 222 |
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disperse( /* check light sources for dispersion */ |
| 223 |
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OBJREC *m, |
| 224 |
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RAY *r, |
| 225 |
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FVECT vt, |
| 226 |
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double tr, |
| 227 |
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COLOR cet, |
| 228 |
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COLOR abt |
| 229 |
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) |
| 230 |
greg |
1.1 |
{ |
| 231 |
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RAY sray, *entray; |
| 232 |
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FVECT v1, v2, n1, n2; |
| 233 |
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FVECT dv, v2Xdv; |
| 234 |
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double v2Xdvv2Xdv; |
| 235 |
greg |
1.7 |
int success = 0; |
| 236 |
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SRCINDEX si; |
| 237 |
greg |
1.1 |
FVECT vtmp1, vtmp2; |
| 238 |
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double dtmp1, dtmp2; |
| 239 |
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int l1, l2; |
| 240 |
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COLOR ctmp; |
| 241 |
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int i; |
| 242 |
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| 243 |
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/* |
| 244 |
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* This routine computes dispersion to the first order using |
| 245 |
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* the following assumptions: |
| 246 |
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* |
| 247 |
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* 1) The dependency of the index of refraction on wavelength |
| 248 |
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* is approximated by Hartmann's equation with lambda0 |
| 249 |
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* equal to zero. |
| 250 |
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* 2) The entry and exit locations are constant with respect |
| 251 |
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* to dispersion. |
| 252 |
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* |
| 253 |
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* The second assumption permits us to model dispersion without |
| 254 |
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* having to sample refracted directions. We assume that the |
| 255 |
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* geometry inside the material is constant, and concern ourselves |
| 256 |
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* only with the relationship between the entering and exiting ray. |
| 257 |
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* We compute the first derivatives of the entering and exiting |
| 258 |
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* refraction with respect to the index of refraction. This |
| 259 |
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* is then used in a first order Taylor series to determine the |
| 260 |
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* index of refraction necessary to send the exiting ray to each |
| 261 |
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* light source. |
| 262 |
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* If an exiting ray hits a light source within the refraction |
| 263 |
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* boundaries, we sum all the frequencies over the disc of the |
| 264 |
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* light source to determine the resulting color. A smaller light |
| 265 |
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* source will therefore exhibit a sharper spectrum. |
| 266 |
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*/ |
| 267 |
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| 268 |
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if (!(r->crtype & REFRACTED)) { /* ray started in material */ |
| 269 |
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VCOPY(v1, r->rdir); |
| 270 |
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n1[0] = -r->rdir[0]; n1[1] = -r->rdir[1]; n1[2] = -r->rdir[2]; |
| 271 |
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} else { |
| 272 |
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/* find entry point */ |
| 273 |
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for (entray = r; entray->rtype != REFRACTED; |
| 274 |
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entray = entray->parent) |
| 275 |
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; |
| 276 |
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entray = entray->parent; |
| 277 |
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if (entray->crtype & REFRACTED) /* too difficult */ |
| 278 |
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return(0); |
| 279 |
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VCOPY(v1, entray->rdir); |
| 280 |
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VCOPY(n1, entray->ron); |
| 281 |
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} |
| 282 |
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VCOPY(v2, vt); /* exiting ray */ |
| 283 |
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VCOPY(n2, r->ron); |
| 284 |
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| 285 |
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/* first order dispersion approx. */ |
| 286 |
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dtmp1 = DOT(n1, v1); |
| 287 |
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dtmp2 = DOT(n2, v2); |
| 288 |
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for (i = 0; i < 3; i++) |
| 289 |
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dv[i] = v1[i] + v2[i] - n1[i]/dtmp1 - n2[i]/dtmp2; |
| 290 |
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| 291 |
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if (DOT(dv, dv) <= FTINY) /* null effect */ |
| 292 |
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return(0); |
| 293 |
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/* compute plane normal */ |
| 294 |
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fcross(v2Xdv, v2, dv); |
| 295 |
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v2Xdvv2Xdv = DOT(v2Xdv, v2Xdv); |
| 296 |
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| 297 |
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/* check sources */ |
| 298 |
greg |
1.7 |
initsrcindex(&si); |
| 299 |
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while (srcray(&sray, r, &si)) { |
| 300 |
greg |
1.1 |
|
| 301 |
greg |
1.7 |
if (DOT(sray.rdir, v2) < MINCOS) |
| 302 |
greg |
1.1 |
continue; /* bad source */ |
| 303 |
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/* adjust source ray */ |
| 304 |
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| 305 |
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dtmp1 = DOT(v2Xdv, sray.rdir) / v2Xdvv2Xdv; |
| 306 |
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sray.rdir[0] -= dtmp1 * v2Xdv[0]; |
| 307 |
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sray.rdir[1] -= dtmp1 * v2Xdv[1]; |
| 308 |
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sray.rdir[2] -= dtmp1 * v2Xdv[2]; |
| 309 |
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| 310 |
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l1 = lambda(m, v2, dv, sray.rdir); /* mean lambda */ |
| 311 |
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| 312 |
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if (l1 > MAXLAMBDA || l1 < MINLAMBDA) /* not visible */ |
| 313 |
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continue; |
| 314 |
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/* trace source ray */ |
| 315 |
greg |
2.12 |
copycolor(sray.cext, cet); |
| 316 |
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copycolor(sray.albedo, abt); |
| 317 |
greg |
1.1 |
normalize(sray.rdir); |
| 318 |
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rayvalue(&sray); |
| 319 |
greg |
1.2 |
if (bright(sray.rcol) <= FTINY) /* missed it */ |
| 320 |
greg |
1.1 |
continue; |
| 321 |
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| 322 |
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/* |
| 323 |
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* Compute spectral sum over diameter of source. |
| 324 |
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* First find directions for rays going to opposite |
| 325 |
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* sides of source, then compute wavelengths for each. |
| 326 |
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*/ |
| 327 |
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| 328 |
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fcross(vtmp1, v2Xdv, sray.rdir); |
| 329 |
greg |
1.7 |
dtmp1 = sqrt(si.dom / v2Xdvv2Xdv / PI); |
| 330 |
greg |
1.1 |
|
| 331 |
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/* compute first ray */ |
| 332 |
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for (i = 0; i < 3; i++) |
| 333 |
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vtmp2[i] = sray.rdir[i] + dtmp1*vtmp1[i]; |
| 334 |
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| 335 |
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l1 = lambda(m, v2, dv, vtmp2); /* first lambda */ |
| 336 |
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if (l1 < 0) |
| 337 |
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continue; |
| 338 |
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/* compute second ray */ |
| 339 |
|
|
for (i = 0; i < 3; i++) |
| 340 |
|
|
vtmp2[i] = sray.rdir[i] - dtmp1*vtmp1[i]; |
| 341 |
|
|
|
| 342 |
|
|
l2 = lambda(m, v2, dv, vtmp2); /* second lambda */ |
| 343 |
|
|
if (l2 < 0) |
| 344 |
|
|
continue; |
| 345 |
|
|
/* compute color from spectrum */ |
| 346 |
|
|
if (l1 < l2) |
| 347 |
|
|
spec_rgb(ctmp, l1, l2); |
| 348 |
|
|
else |
| 349 |
|
|
spec_rgb(ctmp, l2, l1); |
| 350 |
|
|
multcolor(ctmp, sray.rcol); |
| 351 |
|
|
scalecolor(ctmp, tr); |
| 352 |
|
|
addcolor(r->rcol, ctmp); |
| 353 |
|
|
success++; |
| 354 |
|
|
} |
| 355 |
|
|
return(success); |
| 356 |
|
|
} |
| 357 |
|
|
|
| 358 |
|
|
|
| 359 |
|
|
static int |
| 360 |
schorsch |
2.18 |
lambda( /* compute lambda for material */ |
| 361 |
|
|
register OBJREC *m, |
| 362 |
|
|
FVECT v2, |
| 363 |
|
|
FVECT dv, |
| 364 |
|
|
FVECT lr |
| 365 |
|
|
) |
| 366 |
greg |
1.1 |
{ |
| 367 |
|
|
FVECT lrXdv, v2Xlr; |
| 368 |
|
|
double dtmp, denom; |
| 369 |
|
|
int i; |
| 370 |
|
|
|
| 371 |
|
|
fcross(lrXdv, lr, dv); |
| 372 |
|
|
for (i = 0; i < 3; i++) |
| 373 |
|
|
if (lrXdv[i] > FTINY || lrXdv[i] < -FTINY) |
| 374 |
|
|
break; |
| 375 |
|
|
if (i >= 3) |
| 376 |
|
|
return(-1); |
| 377 |
|
|
|
| 378 |
|
|
fcross(v2Xlr, v2, lr); |
| 379 |
|
|
|
| 380 |
|
|
dtmp = m->oargs.farg[4] / MLAMBDA; |
| 381 |
|
|
denom = dtmp + v2Xlr[i]/lrXdv[i] * (m->oargs.farg[3] + dtmp); |
| 382 |
|
|
|
| 383 |
|
|
if (denom < FTINY) |
| 384 |
|
|
return(-1); |
| 385 |
|
|
|
| 386 |
|
|
return(m->oargs.farg[4] / denom); |
| 387 |
|
|
} |
| 388 |
|
|
|
| 389 |
|
|
#endif /* DISPERSE */ |
