summaryrefslogtreecommitdiff
path: root/material_dielectric.cpp
diff options
context:
space:
mode:
authorKeuin <[email protected]>2022-05-03 15:59:11 +0800
committerKeuin <[email protected]>2022-05-03 15:59:11 +0800
commit12ec4e8284afb30ed894d9926362141cdfb24b96 (patch)
tree2c1c43f953c2e19fc945d227f63881b44db893e5 /material_dielectric.cpp
parent038e32a2345b064cb793a8ece77f1eda1bd824b0 (diff)
Refactor: do not invert ri in constructor of material_dielectric.
Rewrite material_dielectric::scatter to stop using vec3::refract and switch to ri instead of ri_inv.
Diffstat (limited to 'material_dielectric.cpp')
-rw-r--r--material_dielectric.cpp56
1 files changed, 35 insertions, 21 deletions
diff --git a/material_dielectric.cpp b/material_dielectric.cpp
index 61e34ec..d44ab87 100644
--- a/material_dielectric.cpp
+++ b/material_dielectric.cpp
@@ -8,29 +8,43 @@
bool material_dielectric::scatter(ray3d &r, const object &hit_obj, double hit_t, random_uv_gen_3d &ruvg) const {
const auto hit_p = r.at(hit_t);
assert(hit_obj.is_on(hit_p));
- auto n = hit_obj.normal_vector(hit_p);
- auto ri_ = ri_inv;
- auto cos1 = dot(r.direction(), n); // -cos(a1)
- if (cos1 > 0) {
- // the ray is started from the object's inner,
- // use normal vector and ri on the surface's inner side
- n = -n;
- ri_ = 1.0 / ri_;
+ auto nv = hit_obj.normal_vector(hit_p);
+ const auto n1 = r.direction(); // incoming ray, unit vector
+ const bool outside = dot(nv, n1) < 0; // if the ray hits the outside of the surface
+ double rel_ri; // relative ri, source_ri/target_ri
+ if (!outside) {
+ nv = -nv; // use normal vector pointing to the inner
+ rel_ri = ri;
} else {
- cos1 = -cos1;
+ rel_ri = 1.0 / ri;
}
- vec3d r2;
- // determine reflection or refraction using Schlick's Approximation.
- if (reflectance(cos1, ri_) > ruvg.range01_scalar()) {
- // reflect
- TRACELOG(" reflect (dielectric material, schlick, ri=%-10f)\n", ri_);
- r2 = n.reflect(r.direction());
+ const auto cos_t1 = std::min(-dot(nv, n1), 1.0); // cos(theta1)
+ const auto sin_t1_s = 1 - cos_t1 * cos_t1; // sin(theta1)^2
+ const auto rel_ri_s = rel_ri * rel_ri;
+ const auto sin_t2_s = sin_t1_s * rel_ri_s;
+ double p_reflect; // probability of schlick reflection
+ bool reflect = false;
+ if (sin_t2_s > 1.0) {
+ TRACELOG(" reflect (TIR, ri=%f)\n", ri);
+ // sin(theta2)^2 > 1, no real solution
+ // TIR (total internal reflection)
+ reflect = true;
+ } else if ((p_reflect = reflectance(cos_t1, ri)) > ruvg.range01_scalar()) {
+ TRACELOG(" reflect (schlick, ri=%f, p=%f)\n", ri, p_reflect);
+ reflect = true;
+ }
+ if (reflect) {
+ r.direction(nv.reflect(n1));
+ r.source(hit_p);
+ return true;
} else {
- // refract
- TRACELOG(" refract (dielectric material, schlick, ri=%-10f)\n", ri_);
- r2 = n.refract<true>(r.direction(), ri_);
+ // normal refract
+ TRACELOG(" refract (forced, ri=%f)\n", ri);
+ const auto sin_t2 = sqrt(sin_t2_s);
+ const auto cos_t2 = sqrt(1 - sin_t2_s);
+ const auto n2 = (-cos_t2 * nv) + (n1 + cos_t1 * nv).unit_vec() * sin_t2;
+ r.direction(n2);
+ r.source(hit_p);
+ return true;
}
- r.direction(r2.unit_vec());
- r.source(hit_p);
- return true;
}