1// Copyright (c) 2017 Eric Bruneton2// All rights reserved.3//4// Redistribution and use in source and binary forms, with or without5// modification, are permitted provided that the following conditions6// are met:7// 1. Redistributions of source code must retain the above copyright8// notice, this list of conditions and the following disclaimer.9// 2. Redistributions in binary form must reproduce the above copyright10// notice, this list of conditions and the following disclaimer in the11// documentation and/or other materials provided with the distribution.12// 3. Neither the name of the copyright holders nor the names of its13// contributors may be used to endorse or promote products derived from14// this software without specific prior written permission.15//16// THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS"17// AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE18// IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE19// ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE20// LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR21// CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF22// SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS23// INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN24// CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE)25// ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF26// THE POSSIBILITY OF SUCH DAMAGE.27//28// Precomputed Atmospheric Scattering29// Copyright (c) 2008 INRIA30// All rights reserved.31//32// Redistribution and use in source and binary forms, with or without33// modification, are permitted provided that the following conditions34// are met:35// 1. Redistributions of source code must retain the above copyright36// notice, this list of conditions and the following disclaimer.37// 2. Redistributions in binary form must reproduce the above copyright38// notice, this list of conditions and the following disclaimer in the39// documentation and/or other materials provided with the distribution.40// 3. Neither the name of the copyright holders nor the names of its41// contributors may be used to endorse or promote products derived from42// this software without specific prior written permission.43//44// THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS"45// AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE46// IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE47// ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE48// LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR49// CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF50// SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS51// INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN52// CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE)53// ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF54// THE POSSIBILITY OF SUCH DAMAGE.56import package::atmosphere::{57 types::Atmosphere,58 bindings::atmosphere,59 functions::{get_local_r, sample_transmittance_lut},60};62// Bruneton's paper calls the surface and exosphere "bottom radius" and "top radius".63// Our `Atmosphere` struct uses `inner_radius` and `outer_radius` for the same values so naming stays64// meaningful when the atmosphere entity has an arbitrary transform.66/// Mapping from view height (r) and zenith cos angle (mu) to UV coordinates in the transmittance LUT67/// Assuming r between ground and top atmosphere boundary, and mu= cos(zenith_angle)68/// Chosen to increase precision near the ground and to work around a discontinuity at the horizon69/// See Bruneton and Neyret 2008, "Precomputed Atmospheric Scattering" section 470fn transmittance_lut_r_mu_to_uv(atm: Atmosphere, r: f32, mu: f32) -> vec2<f32> {71 // Distance along a horizontal ray from the ground to the top atmosphere boundary72 let H = sqrt(atm.outer_radius * atm.outer_radius - atm.inner_radius * atm.inner_radius);74 // Distance from a point at height r to the horizon75 // ignore the case where r <= atmosphere.inner_radius76 let rho = sqrt(max(r * r - atm.inner_radius * atm.inner_radius, 0.0));78 // Distance from a point at height r to the top atmosphere boundary at zenith angle mu79 let d = distance_to_top_atmosphere_boundary(atm, r, mu);81 // Minimum and maximum distance to the top atmosphere boundary from a point at height r82 let d_min = atm.outer_radius - r; // length of the ray straight up to the top atmosphere boundary83 let d_max = rho + H; // length of the ray to the top atmosphere boundary and grazing the horizon85 let u = (d - d_min) / (d_max - d_min);86 let v = rho / H;87 return vec2<f32>(u, v);88}90/// Inverse of the mapping above, mapping from UV coordinates in the transmittance LUT to view height (r) and zenith cos angle (mu)91fn transmittance_lut_uv_to_r_mu(uv: vec2<f32>) -> vec2<f32> {92 // Distance to top atmosphere boundary for a horizontal ray at ground level93 let H = sqrt(atmosphere.outer_radius * atmosphere.outer_radius - atmosphere.inner_radius * atmosphere.inner_radius);95 // Distance to the horizon, from which we can compute r:96 let rho = H * uv.y;97 let r = sqrt(rho * rho + atmosphere.inner_radius * atmosphere.inner_radius);99 // Distance to the top atmosphere boundary for the ray (r,mu), and its minimum100 // and maximum values over all mu- obtained for (r,1) and (r,mu_horizon) -101 // from which we can recover mu:102 let d_min = atmosphere.outer_radius - r;103 let d_max = rho + H;104 let d = d_min + uv.x * (d_max - d_min);106 var mu: f32;107 if d == 0.0 {108 mu = 1.0;109 } else {110 mu = (H * H - rho * rho - d * d) / (2.0 * r * d);111 }113 mu = clamp(mu, -1.0, 1.0);115 return vec2<f32>(r, mu);116}118/// Simplified ray-sphere intersection119/// where:120/// Ray origin, o = [0,0,r] with r <= atmosphere.outer_radius121/// mu is the cosine of spherical coordinate theta (-1.0 <= mu <= 1.0)122/// so ray direction in spherical coordinates is [1,acos(mu),0] which needs to be converted to cartesian123/// Direction of ray, u = [0,sqrt(1-mu*mu),mu]124/// Center of sphere, c = [0,0,0]125/// Radius of sphere, r = atmosphere.outer_radius126/// This function solves the quadratic equation for line-sphere intersection simplified under these assumptions127fn distance_to_top_atmosphere_boundary(atm: Atmosphere, r: f32, mu: f32) -> f32 {128 // ignore the case where r > atm.outer_radius129 let positive_discriminant = max(r * r * (mu * mu - 1.0) + atm.outer_radius * atm.outer_radius, 0.0);130 return max(-r * mu + sqrt(positive_discriminant), 0.0);131}133/// Simplified ray-sphere intersection134/// as above for intersections with the ground135fn distance_to_bottom_atmosphere_boundary(r: f32, mu: f32) -> f32 {136 let positive_discriminant = max(r * r * (mu * mu - 1.0) + atmosphere.inner_radius * atmosphere.inner_radius, 0.0);137 return max(-r * mu - sqrt(positive_discriminant), 0.0);138}140fn ray_intersects_ground(r: f32, mu: f32) -> bool {141 return mu < 0.0 && r * r * (mu * mu - 1.0) + atmosphere.inner_radius * atmosphere.inner_radius >= 0.0;142}144// NOTICE: This function is copyrighted by Eric Bruneton and INRIA, and falls145// under the license reproduced in bruneton_functions.wesl (variant of MIT license)146fn sample_transmittance_lut_segment(r: f32, mu: f32, t: f32) -> vec3<f32> {147 let r_t = get_local_r(r, mu, t);148 let mu_t = clamp((r * mu + t) / r_t, -1.0, 1.0);150 if ray_intersects_ground(r, mu) {151 return min(152 sample_transmittance_lut(r_t, -mu_t) / sample_transmittance_lut(r, -mu),153 vec3(1.0)154 );155 } else {156 return min(157 sample_transmittance_lut(r, mu) / sample_transmittance_lut(r_t, mu_t), vec3(1.0)158 );159 }160}