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27
main.js
27
main.js
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@ -8,6 +8,7 @@ import { EulerUniverse, Universe, default as init, set_panic_hook as setPanicHoo
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const wasm = await init("./maxwell_bg.wasm");
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setPanicHook();
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const DIAMOND = false;
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const UPWIND = true;
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const canvas = document.getElementById("glCanvas");
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@ -103,7 +104,7 @@ import { EulerUniverse, Universe, default as init, set_panic_hook as setPanicHoo
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for (let j = 0; j < height; j += 1) {
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for (let i = 0; i < width; i += 1) {
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const n = width*j + i;
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x[n] = 10.0*(i / (width - 1.0) - 0.5);
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x[n] = 20.0*(i / (width - 1.0));
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y[n] = 20.0*(j / (height - 1.0));
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@ -201,7 +202,7 @@ import { EulerUniverse, Universe, default as init, set_panic_hook as setPanicHoo
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};
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chosenField.cycle();
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universe.init(0, 10);
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universe.init(10, 10);
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/**
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* Integrates and draws the next iteration
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@ -237,8 +238,8 @@ import { EulerUniverse, Universe, default as init, set_panic_hook as setPanicHoo
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};
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const field = new Float32Array(wasm.memory.buffer, fieldPtr, width*height);
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gl.bufferData(gl.ARRAY_BUFFER, field, gl.DYNAMIC_DRAW);
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console.log(field.reduce((min, v) => v < min ? v : min));
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console.log(field.reduce((max, v) => v > max ? v : max));
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// console.log(field.reduce((min, v) => v < min ? v : min));
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// console.log(field.reduce((max, v) => v > max ? v : max));
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{
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const offset = 0;
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@ -247,8 +248,13 @@ import { EulerUniverse, Universe, default as init, set_panic_hook as setPanicHoo
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gl.drawElements(gl.TRIANGLES, vertexCount, type, offset);
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}
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universe.advance(dt/2);
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universe.advance(dt/2);
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if (UPWIND) {
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universe.advance_upwind(dt/2);
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universe.advance_upwind(dt/2);
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} else {
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universe.advance(dt/2);
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universe.advance(dt/2);
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}
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window.requestAnimationFrame(drawMe);
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}
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@ -271,7 +277,14 @@ import { EulerUniverse, Universe, default as init, set_panic_hook as setPanicHoo
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// Must adjust for bbox and transformations for x/y
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const mousex = event.clientX / window.innerWidth;
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const mousey = event.clientY / window.innerHeight;
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universe.init(10*(mousex-0.5), 20.0*(1.0 - mousey));
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const normx = mousex;
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const normy = 1.0 - mousey;
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universe.init(
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(bbox[1] - bbox[0])*normx + bbox[0],
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(bbox[3] - bbox[2])*normy + bbox[2],
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);
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}, {"passive": true});
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resizeCanvas();
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225
src/euler.rs
225
src/euler.rs
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@ -121,7 +121,6 @@ impl Field {
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}
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}
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#[allow(unused)]
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pub(crate) fn advance_upwind<UO>(
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prev: &Field,
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fut: &mut Field,
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@ -176,12 +175,6 @@ pub(crate) fn advance_upwind<UO>(
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.apply(|y1, &y0, &k1, &k2, &k3, &k4| *y1 = y0 + dt / 6.0 * (k1 + 2.0 * k2 + 2.0 * k3 + k4));
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}
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/// Solving (Au)_x + (Bu)_y
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/// with:
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/// A B
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/// [ 0, 0, 0] [ 0, 1, 0]
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/// [ 0, 0, -1] [ 1, 0, 0]
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/// [ 0, -1, 0] [ 0, 0, 0]
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pub(crate) fn advance<SBP>(
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prev: &Field,
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fut: &mut Field,
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@ -241,42 +234,32 @@ fn pressure(gamma: f32, rho: f32, rhou: f32, rhov: f32, e: f32) -> f32 {
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}
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#[allow(non_snake_case)]
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/// This flux is rotated by the grid metrics
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/// (Au)_x + (Bu)_y = 1/J [
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/// (J xi_x Au)_xi + (J eta_x Au)_eta
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/// (J xi_y Bu)_xi + (J eta_y Bu)_eta
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/// ]
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/// where J is the grid determinant
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///
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/// This is used both in fluxes and SAT terms
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fn RHS<SBP: SbpOperator>(
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k: &mut Field,
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y: &Field,
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grid: &Grid<SBP>,
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boundaries: &BoundaryTerms,
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tmp: &mut (Field, Field, Field, Field),
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tmp: &mut (Field, Field, Field, Field, Field, Field),
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) {
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let ehat = &mut tmp.0;
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let fhat = &mut tmp.1;
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fluxes([ehat, fhat], y, grid);
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let de = &mut tmp.2;
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let df = &mut tmp.3;
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fluxes((ehat, fhat), y, grid);
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let dE = &mut tmp.2;
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let dF = &mut tmp.3;
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SBP::diffxi(ehat.rho(), de.rho_mut());
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SBP::diffxi(ehat.rhou(), de.rhou_mut());
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SBP::diffxi(ehat.rhov(), de.rhov_mut());
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SBP::diffxi(ehat.e(), de.e_mut());
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SBP::diffxi(ehat.rho(), dE.rho_mut());
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SBP::diffxi(ehat.rhou(), dE.rhou_mut());
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SBP::diffxi(ehat.rhov(), dE.rhov_mut());
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SBP::diffxi(ehat.e(), dE.e_mut());
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SBP::diffeta(fhat.rho(), df.rho_mut());
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SBP::diffeta(fhat.rhou(), df.rhou_mut());
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SBP::diffeta(fhat.rhov(), df.rhov_mut());
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SBP::diffeta(fhat.e(), df.e_mut());
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SBP::diffeta(fhat.rho(), dF.rho_mut());
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SBP::diffeta(fhat.rhou(), dF.rhou_mut());
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SBP::diffeta(fhat.rhov(), dF.rhov_mut());
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SBP::diffeta(fhat.e(), dF.e_mut());
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// And dissipation...
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ndarray::azip!((out in &mut k.0,
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eflux in &de.0,
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fflux in &df.0,
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azip!((out in &mut k.0,
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eflux in &dE.0,
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fflux in &dF.0,
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detj in &grid.detj.broadcast((4, y.ny(), y.nx())).unwrap()) {
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*out = (-eflux - fflux)/detj
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});
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@ -285,26 +268,100 @@ fn RHS<SBP: SbpOperator>(
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}
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#[allow(non_snake_case)]
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#[allow(unused)]
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fn RHS_upwind<UO: UpwindOperator>(
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k: &mut Field,
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y: &Field,
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grid: &Grid<UO>,
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boundaries: &BoundaryTerms,
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tmp: &mut (Field, Field, Field, Field),
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tmp: &mut (Field, Field, Field, Field, Field, Field),
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) {
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// fluxes(k, y, grid, tmp);
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// dissipation(k, y, grid, tmp);
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let ehat = &mut tmp.0;
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let fhat = &mut tmp.1;
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fluxes((ehat, fhat), y, grid);
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let dE = &mut tmp.2;
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let dF = &mut tmp.3;
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UO::diffxi(ehat.rho(), dE.rho_mut());
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UO::diffxi(ehat.rhou(), dE.rhou_mut());
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UO::diffxi(ehat.rhov(), dE.rhov_mut());
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UO::diffxi(ehat.e(), dE.e_mut());
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UO::diffeta(fhat.rho(), dF.rho_mut());
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UO::diffeta(fhat.rhou(), dF.rhou_mut());
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UO::diffeta(fhat.rhov(), dF.rhov_mut());
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UO::diffeta(fhat.e(), dF.e_mut());
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let ad_xi = &mut tmp.4;
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let ad_eta = &mut tmp.5;
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upwind_dissipation((ad_xi, ad_eta), y, grid, (&mut tmp.0, &mut tmp.1));
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azip!((out in &mut k.0,
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eflux in &dE.0,
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fflux in &dF.0,
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ad_xi in &ad_xi.0,
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ad_eta in &ad_eta.0,
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detj in &grid.detj.broadcast((4, y.ny(), y.nx())).unwrap()) {
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*out = (-eflux - fflux + ad_xi + ad_eta)/detj
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});
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SAT_characteristics(k, y, grid, boundaries);
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azip!((k in &mut k.0,
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&detj in &grid.detj.broadcast((3, y.ny(), y.nx())).unwrap()) {
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*k /= detj;
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});
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}
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fn fluxes<SBP: SbpOperator>(k: [&mut Field; 2], y: &Field, grid: &Grid<SBP>) {
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fn upwind_dissipation<UO: UpwindOperator>(
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k: (&mut Field, &mut Field),
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y: &Field,
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grid: &Grid<UO>,
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tmp: (&mut Field, &mut Field),
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) {
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for j in 0..y.ny() {
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for i in 0..y.nx() {
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let rho = y[(0, j, i)];
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assert!(rho > 0.0);
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let rhou = y[(1, j, i)];
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let rhov = y[(2, j, i)];
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let e = y[(3, j, i)];
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let u = rhou / rho;
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let v = rhov / rho;
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let uhat = grid.detj_dxi_dx[(j, i)] / grid.detj[(j, i)] * u
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+ grid.detj_dxi_dy[(j, i)] / grid.detj[(j, i)] * v;
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let vhat = grid.detj_deta_dx[(j, i)] / grid.detj[(j, i)] * u
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+ grid.detj_deta_dy[(j, i)] / grid.detj[(j, i)] * v;
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let p = pressure(GAMMA, rho, rhou, rhov, e);
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assert!(p > 0.0);
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let c = (GAMMA * p / rho).sqrt();
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let alpha_u = uhat.abs() + c;
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let alpha_v = vhat.abs() + c;
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tmp.0[(0, j, i)] = alpha_u * rho * grid.detj[(j, i)];
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tmp.1[(0, j, i)] = alpha_v * rho * grid.detj[(j, i)];
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tmp.0[(1, j, i)] = alpha_u * rhou * grid.detj[(j, i)];
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tmp.1[(1, j, i)] = alpha_v * rhou * grid.detj[(j, i)];
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tmp.0[(2, j, i)] = alpha_u * rhov * grid.detj[(j, i)];
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tmp.1[(2, j, i)] = alpha_v * rhov * grid.detj[(j, i)];
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tmp.0[(3, j, i)] = alpha_u * e * grid.detj[(j, i)];
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tmp.1[(3, j, i)] = alpha_v * e * grid.detj[(j, i)];
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}
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}
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UO::dissxi(tmp.0.rho(), k.0.rho_mut());
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UO::dissxi(tmp.0.rhou(), k.0.rhou_mut());
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UO::dissxi(tmp.0.rhov(), k.0.rhov_mut());
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UO::dissxi(tmp.0.e(), k.0.e_mut());
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UO::disseta(tmp.1.rho(), k.1.rho_mut());
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UO::disseta(tmp.1.rhou(), k.1.rhou_mut());
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UO::disseta(tmp.1.rhov(), k.1.rhov_mut());
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UO::disseta(tmp.1.e(), k.1.e_mut());
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}
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fn fluxes<SBP: SbpOperator>(k: (&mut Field, &mut Field), y: &Field, grid: &Grid<SBP>) {
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let j_dxi_dx = grid.detj_dxi_dx.view();
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let j_dxi_dy = grid.detj_dxi_dy.view();
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let j_deta_dx = grid.detj_deta_dx.view();
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@ -318,11 +375,14 @@ fn fluxes<SBP: SbpOperator>(k: [&mut Field; 2], y: &Field, grid: &Grid<SBP>) {
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for j in 0..y.ny() {
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for i in 0..y.nx() {
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let rho = rho[(j, i)];
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assert!(rho > 0.0);
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let rhou = rhou[(j, i)];
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let rhov = rhov[(j, i)];
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let e = e[(j, i)];
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let p = pressure(GAMMA, rho, rhou, rhov, e);
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assert!(p > 0.0);
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let ef = [
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rhou,
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rhou * rhou / rho + p,
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@ -340,23 +400,13 @@ fn fluxes<SBP: SbpOperator>(k: [&mut Field; 2], y: &Field, grid: &Grid<SBP>) {
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let eflux = j_dxi_dx[(j, i)] * ef[comp] + j_dxi_dy[(j, i)] * ff[comp];
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let fflux = j_deta_dx[(j, i)] * ef[comp] + j_deta_dy[(j, i)] * ff[comp];
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k[0][(comp, j, i)] = eflux;
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k[1][(comp, j, i)] = fflux;
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k.0[(comp, j, i)] = eflux;
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k.1[(comp, j, i)] = fflux;
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}
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}
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}
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}
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#[allow(unused)]
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fn dissipation<UO: UpwindOperator>(
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k: &mut Field,
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y: &Field,
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grid: &Grid<UO>,
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tmp: &mut (Array2<f32>, Array2<f32>, Array2<f32>, Array2<f32>),
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) {
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todo!()
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}
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#[derive(Clone, Debug)]
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pub enum Boundary {
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This,
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@ -378,6 +428,16 @@ fn SAT_characteristics<SBP: SbpOperator>(
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grid: &Grid<SBP>,
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_boundaries: &BoundaryTerms,
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) {
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/* // Whean using infinite boundaries, use this...
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let steady_v = [1.0, 1.0, 0.0, {
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let M = 0.1;
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let p_inf = 1.0 / (GAMMA * M * M);
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p_inf / (GAMMA - 1.0) + 0.5
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}];
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let steady_a = ndarray::Array1::from(steady_v.to_vec());
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let steady = steady_a.broadcast((k.nx(), 4)).unwrap().reversed_axes();
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assert_eq!(steady.shape(), [4, k.nx()]);
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*/
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// North boundary
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{
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let hi = (k.ny() - 1) as f32 * SBP::h()[0];
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@ -388,6 +448,7 @@ fn SAT_characteristics<SBP: SbpOperator>(
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k.north_mut(),
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y.north(),
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y.south(), // Self South
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//steady.view(),
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hi,
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sign,
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tau,
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@ -406,6 +467,7 @@ fn SAT_characteristics<SBP: SbpOperator>(
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k.south_mut(),
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y.south(),
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y.north(), // Self North
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//steady.view(),
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hi,
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sign,
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tau,
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@ -414,17 +476,28 @@ fn SAT_characteristics<SBP: SbpOperator>(
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grid.detj_deta_dy.slice(slice),
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);
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}
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/*let steady = ndarray::Array2::from_shape_fn((4, k.ny()), |(k, _)| match k {
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0 => 1.0,
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1 => 1.0,
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2 => 0.0,
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3 => {
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let M = 0.1;
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let p_inf = 1.0 / (GAMMA * M * M);
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p_inf / (GAMMA - 1.0) + 0.5
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}
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_ => unreachable!(),
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});*/
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// West Boundary
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{
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let hi = (k.nx() - 1) as f32 * SBP::h()[0];
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let sign = 1.0;
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let tau = -1.0;
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let slice = s![.., 0];
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println!("{:?}", slice);
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SAT_characteristic(
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k.west_mut(),
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y.west(),
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y.east(), // Self East
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//steady.view(),
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hi,
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sign,
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tau,
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@ -443,6 +516,7 @@ fn SAT_characteristics<SBP: SbpOperator>(
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k.east_mut(),
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y.east(),
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y.west(), // Self West
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//steady.view(),
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hi,
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sign,
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tau,
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@ -472,14 +546,21 @@ fn SAT_characteristic(
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assert_eq!(y.shape()[0], 4);
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assert_eq!(y.shape()[1], detj.shape()[0]);
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for i in 0..z.shape()[1] {
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let rho = y[(0, i)];
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let rhou = y[(1, i)];
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let rhov = y[(2, i)];
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let e = y[(3, i)];
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for (((((mut k, y), z), detj), detj_d_dx), detj_d_dy) in k
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.axis_iter_mut(ndarray::Axis(1))
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.zip(y.axis_iter(ndarray::Axis(1)))
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.zip(z.axis_iter(ndarray::Axis(1)))
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.zip(detj.iter())
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.zip(detj_d_dx.iter())
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.zip(detj_d_dy.iter())
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{
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let rho = y[0];
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let rhou = y[1];
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let rhov = y[2];
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let e = y[3];
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let kx_ = detj_d_dx[i] / detj[i];
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let ky_ = detj_d_dy[i] / detj[i];
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let kx_ = detj_d_dx / detj;
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let ky_ = detj_d_dy / detj;
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let (kx, ky) = {
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let r = f32::hypot(kx_, ky_);
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|
@ -538,12 +619,7 @@ fn SAT_characteristic(
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],
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];
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let res = [
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rho - z[(0, i)],
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rhou - z[(1, i)],
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rhov - z[(2, i)],
|
||||
e - z[(3, i)],
|
||||
];
|
||||
let res = [rho - z[0], rhou - z[1], rhov - z[2], e - z[3]];
|
||||
let mut TIres = [0.0; 4];
|
||||
for row in 0..4 {
|
||||
for col in 0..4 {
|
||||
|
@ -566,7 +642,7 @@ fn SAT_characteristic(
|
|||
}
|
||||
|
||||
for comp in 0..4 {
|
||||
k[(comp, i)] += hi * tau * TLTIres[comp];
|
||||
k[comp] += hi * tau * TLTIres[comp];
|
||||
}
|
||||
}
|
||||
}
|
||||
|
@ -574,7 +650,7 @@ fn SAT_characteristic(
|
|||
pub struct WorkBuffers {
|
||||
y: Field,
|
||||
buf: [Field; 4],
|
||||
tmp: (Field, Field, Field, Field),
|
||||
tmp: (Field, Field, Field, Field, Field, Field),
|
||||
}
|
||||
|
||||
impl WorkBuffers {
|
||||
|
@ -583,7 +659,14 @@ impl WorkBuffers {
|
|||
Self {
|
||||
y: arr3.clone(),
|
||||
buf: [arr3.clone(), arr3.clone(), arr3.clone(), arr3.clone()],
|
||||
tmp: (arr3.clone(), arr3.clone(), arr3.clone(), arr3),
|
||||
tmp: (
|
||||
arr3.clone(),
|
||||
arr3.clone(),
|
||||
arr3.clone(),
|
||||
arr3.clone(),
|
||||
arr3.clone(),
|
||||
arr3,
|
||||
),
|
||||
}
|
||||
}
|
||||
}
|
||||
|
|
46
src/lib.rs
46
src/lib.rs
|
@ -147,10 +147,10 @@ impl EulerUniverse {
|
|||
|
||||
pub fn init(&mut self, x0: f32, y0: f32) {
|
||||
// Should parametrise such that we have radius, drop in pressure at center, etc
|
||||
let rstar = 0.5;
|
||||
let eps = 1.0;
|
||||
let rstar = 1.0;
|
||||
let eps = 3.0;
|
||||
#[allow(non_snake_case)]
|
||||
let M = 0.1;
|
||||
let M = 0.5;
|
||||
|
||||
let p_inf = 1.0 / (euler::GAMMA * M * M);
|
||||
let t = 0.0;
|
||||
|
@ -164,7 +164,7 @@ impl EulerUniverse {
|
|||
let y = self.0.grid.y[(j, i)];
|
||||
|
||||
let dx = (x - x0) - t;
|
||||
let dy = (y - y0) - t;
|
||||
let dy = y - y0;
|
||||
let f = (1.0 - (dx * dx + dy * dy)) / (rstar * rstar);
|
||||
|
||||
use euler::GAMMA;
|
||||
|
@ -180,7 +180,7 @@ impl EulerUniverse {
|
|||
1.0 / (GAMMA - 1.0),
|
||||
);
|
||||
assert!(rho > 0.0);
|
||||
let p = rho.powf(GAMMA) * p_inf;
|
||||
let p = p_inf * rho.powf(GAMMA);
|
||||
assert!(p > 0.0);
|
||||
let e = p / (GAMMA - 1.0) + rho * (u * u + v * v) / 2.0;
|
||||
assert!(e > 0.0);
|
||||
|
@ -197,8 +197,8 @@ impl EulerUniverse {
|
|||
self.0.advance(dt)
|
||||
}
|
||||
|
||||
pub fn advance_upwind(&mut self, _dt: f32) {
|
||||
todo!()
|
||||
pub fn advance_upwind(&mut self, dt: f32) {
|
||||
self.0.advance_upwind(dt)
|
||||
}
|
||||
|
||||
pub fn get_rho_ptr(&self) -> *const u8 {
|
||||
|
@ -241,11 +241,41 @@ impl<SBP: operators::SbpOperator> EulerSystem<SBP> {
|
|||
}
|
||||
}
|
||||
|
||||
impl<SBP: operators::UpwindOperator> EulerSystem<SBP> {
|
||||
pub fn advance_upwind(&mut self, dt: f32) {
|
||||
euler::advance_upwind(
|
||||
&self.sys.0,
|
||||
&mut self.sys.1,
|
||||
dt,
|
||||
&self.grid,
|
||||
Some(&mut self.wb),
|
||||
);
|
||||
std::mem::swap(&mut self.sys.0, &mut self.sys.1);
|
||||
}
|
||||
}
|
||||
|
||||
#[test]
|
||||
fn start_and_advance_euler() {
|
||||
let x = ndarray::Array2::from_shape_fn((20, 20), |(_j, i)| {
|
||||
5.0 * 2.0 * ((i as f32 / (20 - 1) as f32) - 0.5)
|
||||
});
|
||||
let y = ndarray::Array2::from_shape_fn((20, 20), |(j, _i)| {
|
||||
5.0 * 2.0 * ((j as f32 / (20 - 1) as f32) - 0.5)
|
||||
});
|
||||
let mut universe = EulerUniverse::new(x, y);
|
||||
universe.init(-1.0, 0.0);
|
||||
for _ in 0..50 {
|
||||
universe.advance(0.01);
|
||||
}
|
||||
}
|
||||
|
||||
#[test]
|
||||
fn start_and_advance_upwind_euler() {
|
||||
let x = ndarray::Array2::from_shape_fn((20, 10), |(_j, i)| i as f32 / (10 - 1) as f32);
|
||||
let y = ndarray::Array2::from_shape_fn((20, 10), |(j, _i)| j as f32 / (20 - 1) as f32);
|
||||
let mut universe = EulerUniverse::new(x, y);
|
||||
universe.init(0.5, 0.5);
|
||||
universe.advance(0.01);
|
||||
for _ in 0..50 {
|
||||
universe.advance_upwind(0.01);
|
||||
}
|
||||
}
|
||||
|
|
Loading…
Reference in New Issue