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authorFerenc Arn <tagcup@yahoo.com>2017-10-04 00:19:01 -0400
committerFerenc Arn <tagcup@yahoo.com>2017-10-09 12:29:05 -0400
commit12596cb5bc17fa6209cdfb99a384aece56102d45 (patch)
tree0e7329414e650e10d7eccc366464fcf7b57b490a
parentb2046836401fe5cdaf4ae6ae32ad3323511b956d (diff)
Fix anisotropic GGX D function, and introduce and use anistropic GGX G function.
Also fixed isotropic GGX G function with Schlick approximation, and added a commented out version without the approximation. Added references.
-rw-r--r--drivers/gles3/shaders/scene.glsl77
1 files changed, 59 insertions, 18 deletions
diff --git a/drivers/gles3/shaders/scene.glsl b/drivers/gles3/shaders/scene.glsl
index 341a5bf2c7..b322a4c957 100644
--- a/drivers/gles3/shaders/scene.glsl
+++ b/drivers/gles3/shaders/scene.glsl
@@ -865,11 +865,57 @@ float contact_shadow_compute(vec3 pos, vec3 dir, float max_distance) {
#endif
-// GGX Specular
-// Source: http://www.filmicworlds.com/images/ggx-opt/optimized-ggx.hlsl
-float G1V(float dotNV, float k)
-{
- return 1.0 / (dotNV * (1.0 - k) + k);
+
+// This returns the G_GGX function divided by 2 cos_theta_m, where in practice cos_theta_m is either N.L or N.V.
+// We're dividing this factor off because the overall term we'll end up looks like
+// (see, for example, the first unnumbered equation in B. Burley, "Physically Based Shading at Disney", SIGGRAPH 2012):
+//
+// F(L.V) D(N.H) G(N.L) G(N.V) / (4 N.L N.V)
+//
+// We're basically regouping this as
+//
+// F(L.V) D(N.H) [G(N.L)/(2 N.L)] [G(N.V) / (2 N.V)]
+//
+// and thus, this function implements the [G(N.m)/(2 N.m)] part with m = L or V.
+//
+// The contents of the D and G (G1) functions (GGX) are taken from
+// E. Heitz, "Understanding the Masking-Shadowing Function in Microfacet-Based BRDFs", J. Comp. Graph. Tech. 3 (2) (2014).
+// Eqns 71-72 and 85-86 (see also Eqns 43 and 80).
+
+float G_GGX_2cos(float cos_theta_m, float alpha) {
+ // Schlick's approximation
+ // C. Schlick, "An Inexpensive BRDF Model for Physically-based Rendering", Computer Graphics Forum. 13 (3): 233 (1994)
+ // Eq. (19), although see Heitz (2014) the about the problems with his derivation.
+ // It nevertheless approximates GGX well with k = alpha/2.
+ float k = 0.5*alpha;
+ return 0.5 / (cos_theta_m * (1.0 - k) + k);
+
+ // float cos2 = cos_theta_m*cos_theta_m;
+ // float sin2 = (1.0-cos2);
+ // return 1.0 /( cos_theta_m + sqrt(cos2 + alpha*alpha*sin2) );
+}
+
+float D_GXX(float cos_theta_m, float alpha) {
+ float alpha2 = alpha*alpha;
+ float d = 1.0 + (alpha2-1.0)*cos_theta_m*cos_theta_m;
+ return alpha2/(M_PI * d * d);
+}
+
+float G_GGX_anisotropic_2cos(float cos_theta_m, float alpha_x, float alpha_y, float cos_phi, float sin_phi) {
+ float cos2 = cos_theta_m * cos_theta_m;
+ float sin2 = (1.0-cos2);
+ float s_x = alpha_x * cos_phi;
+ float s_y = alpha_y * sin_phi;
+ return 1.0 / (cos_theta_m + sqrt(cos2 + (s_x*s_x + s_y*s_y)*sin2 ));
+}
+
+float D_GXX_anisotropic(float cos_theta_m, float alpha_x, float alpha_y, float cos_phi, float sin_phi) {
+ float cos2 = cos_theta_m * cos_theta_m;
+ float sin2 = (1.0-cos2);
+ float r_x = cos_phi/alpha_x;
+ float r_y = sin_phi/alpha_y;
+ float d = cos2 + sin2*(r_x * r_x + r_y * r_y);
+ return 1.0 / (M_PI * alpha_x * alpha_y * d * d );
}
@@ -1019,7 +1065,6 @@ LIGHT_SHADER_CODE
#elif defined(SPECULAR_SCHLICK_GGX)
// shlick+ggx as default
- float alpha = roughness * roughness;
vec3 H = normalize(V + L);
@@ -1035,26 +1080,22 @@ LIGHT_SHADER_CODE
float ay = ry*ry;
float XdotH = dot( T, H );
float YdotH = dot( B, H );
- float denom = XdotH*XdotH / (ax*ax) + YdotH*YdotH / (ay*ay) + cNdotH*cNdotH;
- float D = 1.0 / ( M_PI * ax*ay * denom*denom );
+ float D = D_GXX_anisotropic(cNdotH, ax, ay, XdotH, YdotH);
+ float G = G_GGX_anisotropic_2cos(cNdotL, ax, ay, XdotH, YdotH) * G_GGX_anisotropic_2cos(cNdotV, ax, ay, XdotH, YdotH);
#else
- float alphaSqr = alpha * alpha;
- float denom = cNdotH * cNdotH * (alphaSqr - 1.0) + 1.0;
- float D = alphaSqr / (M_PI * denom * denom);
+ float alpha = roughness * roughness;
+ float D = D_GGX(cNdotH, alpha);
+ float G = G_GGX_2cos(cNdotL, alpha) * G_GGX_2cos(cNdotV, alpha);
#endif
// F
float F0 = 1.0; // FIXME
float cLdotH5 = SchlickFresnel(cLdotH);
float F = mix(cLdotH5, 1.0, F0);
- // V
- float k = alpha / 2.0f;
- float vis = G1V(cNdotL, k) * G1V(cNdotV, k);
-
- float speci = cNdotL * D * F * vis;
+ float specular_brdf_NL = cNdotL * D * F * G;
- specular_light += speci * light_color * specular_blob_intensity * attenuation;
+ specular_light += specular_brdf_NL * light_color * specular_blob_intensity * attenuation;
#endif
#if defined(LIGHT_USE_CLEARCOAT)
@@ -1069,7 +1110,7 @@ LIGHT_SHADER_CODE
#endif
float Dr = GTR1(cNdotH, mix(.1, .001, clearcoat_gloss));
float Fr = mix(.04, 1.0, cLdotH5);
- float Gr = G1V(cNdotL, .25) * G1V(cNdotV, .25);
+ float Gr = G_GGX_2cos(cNdotL, .25) * G_GGX_2cos(cNdotV, .25);
specular_light += .25*clearcoat*Gr*Fr*Dr;