summaryrefslogtreecommitdiffstats
path: root/res/effectlib/fresnelLayer.glsllib
blob: 60d71764c8a7b0469d338e452c3a6083141cc7cc (plain)
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
/****************************************************************************
**
** Copyright (C) 2014 NVIDIA Corporation.
** Copyright (C) 2017 The Qt Company Ltd.
** Contact: https://www.qt.io/licensing/
**
** This file is part of Qt 3D Studio.
**
** $QT_BEGIN_LICENSE:GPL$
** Commercial License Usage
** Licensees holding valid commercial Qt licenses may use this file in
** accordance with the commercial license agreement provided with the
** Software or, alternatively, in accordance with the terms contained in
** a written agreement between you and The Qt Company. For licensing terms
** and conditions see https://www.qt.io/terms-conditions. For further
** information use the contact form at https://www.qt.io/contact-us.
**
** GNU General Public License Usage
** Alternatively, this file may be used under the terms of the GNU
** General Public License version 3 or (at your option) any later version
** approved by the KDE Free Qt Foundation. The licenses are as published by
** the Free Software Foundation and appearing in the file LICENSE.GPL3
** included in the packaging of this file. Please review the following
** information to ensure the GNU General Public License requirements will
** be met: https://www.gnu.org/licenses/gpl-3.0.html.
**
** $QT_END_LICENSE$
**
****************************************************************************/


float simpleFresnel( in vec3 N, in float ior, float fresnelPower )
{
    float F = ((1.0-ior) * (1.0-ior)) / ((1.0+ior) * (1.0+ior));
    float fresnelGlancingAngle = clamp( 1.0 - dot(viewDir, N), 0.0, 1.0 );
    float ratio = F + (1.0 - F) * pow(fresnelGlancingAngle, fresnelPower);

    return ratio;
}

// PKC : A variation on the simple Schlick approach that also handles the characteristic
// "dip" that metals exhibit.  The dip is very mild or virtually nonexisting in dielectrics,
// but shows up in metals because of their strong incident reflectivity, and also allows for
// colored metals like gold or copper to show their Fresnel hue shift as well because certain
// components will have different baseline responses.
vec3 pseudoFresnel( in vec3 N, in vec3 ior, float fresnelPower )
{
    vec3 F0 = ((vec3(1.0)-ior) * (vec3(1.0)-ior)) / ((vec3(1.0)+ior) * (vec3(1.0)+ior));

    float fresnelGlancingAngle = clamp( 1.0 - dot(viewDir, N), 0.0, 1.0 );

    float fresCurve = pow(fresnelGlancingAngle, fresnelPower);
    vec3 dipCurve = F0 * sin( 3.1415926535 * fresCurve ) * 0.31830988618;

    vec3 retCol = (vec3(1.0) - F0) * fresCurve;
    retCol += F0 - dipCurve;
    return clamp(retCol, 0.0, 1.0);
}

// look here: http://en.wikipedia.org/wiki/Fresnel_equations
float fresnel( in float eta1, in float eta2, in float cosTheta1 )
{
  float etaInv = eta1 / eta2;
  float cosTheta2 = 1.0 - ( 1.0 - cosTheta1 * cosTheta1 ) * ( etaInv * etaInv );
  if ( 0.0 <= cosTheta2 )
  {
    cosTheta2 = sqrt( cosTheta2 );
    float n1t1 = eta1 * cosTheta1;
    float n1t2 = eta1 * cosTheta2;
    float n2t1 = eta2 * cosTheta1;
    float n2t2 = eta2 * cosTheta2;
    float rs = ( n1t1 - n2t2 ) / ( n1t1 + n2t2 );
    float rp = ( n1t2 - n2t1 ) / ( n1t2 + n2t1 );
    float f = 0.5 * ( rs * rs + rp * rp );
    return( clamp( f, 0.0, 1.0 ) );
  }
  else
  {
    return( 1.0 );
  }
}

// we assume, light rays run through air with ior == 1.0
// with eta = eta2 / eta1, we have
//  - when hitting a front face: eta2 == ior, eta1 == 1.0 => eta = ior
//  - when hitting a back face : eta2 == 1.0, eta1 == ior => eta = 1.0 / ior
vec3 fresnel( in vec3 N, in vec3 ior )
{
  float cosTheta1 = dot( N, viewDir );
  if ( gl_FrontFacing )
  {
    return( vec3( fresnel( 1.0, ior[0], cosTheta1 ), fresnel( 1.0, ior[1], cosTheta1 ), fresnel( 1.0, ior[2], cosTheta1 ) ) );
  }
  else
  {
    return( vec3( fresnel( ior[0], 1.0, cosTheta1 ), fresnel( ior[1], 1.0, cosTheta1 ), fresnel( ior[2], 1.0, cosTheta1 ) ) );
  }
}

vec4 fresnelLayer( in vec3 N, in vec3 ior, in float weight, in vec3 layercolor, in vec4 layer, in vec4 base, in float alpha )
{
  vec3 refl = reflect( -viewDir, N );
  float reflWt = clamp( dot( surfNormal, refl ) + 1.0, 0.0, 1.0 );

  vec3 fresColor = reflWt * weight * layercolor * pseudoFresnel( N, ior, 5.0 );

  return( vec4( mix( base.rgb, layer.rgb, fresColor ), mix(alpha, 1.0, luminance(fresColor)) ) );
}