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Co-Authored-By: Claude Fable 5.1 <[email protected]>
141 lines
4.9 KiB
Rust
141 lines
4.9 KiB
Rust
//! S2-5 host ladder: DFG 2D-1 (Re 20) on a periodic-z slab of 4 cells with
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//! every knob of the cut wall read from the environment — the instrument
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//! for host-only prototypes (`RTX_E3_PRESSURE_CENTROID=1`). Reference
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//! c_D 5.57954, c_L 0.010619, Δp 0.117520. `RTX_E3_DFG_NY` (default 62).
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use rtx_cfd::solvers::incompressible::ConvectionScheme;
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use rtx_cfd::solvers::incompressible::embedded3::{
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Body, Boundaries, Field, Fluid, Grid, Parameters, Side, Solver, WallScheme,
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};
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const H: f64 = 0.41;
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const L: f64 = 2.2;
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const D: f64 = 0.1;
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const CX: f64 = 0.2;
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const CY: f64 = 0.2;
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const U_M: f64 = 0.3;
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const U_BAR: f64 = 2.0 / 3.0 * U_M;
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const RHO: f64 = 1.0;
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const NU: f64 = 1e-3;
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fn inflow(y: f64, _z: f64) -> f64 {
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4.0 * U_M * y * (H - y) / (H * H)
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}
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#[test]
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#[ignore = "host DFG at ny 31 with the routes split (about half an hour)"]
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fn dfg_2d1_on_the_host() {
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let ny: usize = std::env::var("RTX_E3_DFG_NY")
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.ok()
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.and_then(|v| v.parse().ok())
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.unwrap_or(62);
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let h = H / ny as f64;
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let nx = (L / h).round() as usize;
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let nz = 4;
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let lz = nz as f64 * h;
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let dt = (0.3 * h / U_M).min(0.5 * h * h / (6.0 * NU));
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let mut solver = Solver::new(
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Fluid {
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density: RHO,
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viscosity: RHO * NU,
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reference_velocity: U_BAR,
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reference_length: D,
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},
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Parameters {
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corrector_steps: 2,
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tolerance: 1e-8,
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convection_scheme: ConvectionScheme::TvdVanAlbada,
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wall_scheme: WallScheme::CutCell,
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boundaries: Boundaries {
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x1: Side::PressureOutlet,
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z0: Side::Periodic,
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z1: Side::Periodic,
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..Boundaries::default()
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},
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..Parameters::default()
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},
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);
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solver.set_boundary_velocity(|x, y, z, _t| {
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if x <= 0.0 {
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(inflow(y, z), 0.0, 0.0)
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} else {
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(0.0, 0.0, 0.0)
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}
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});
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solver.set_body(Body::extruded(
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rtx_cfd::solvers::incompressible::EmbeddedBody::circle(CX, CY, 0.5 * D),
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lz,
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));
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let g = Grid::cubic(nx, ny, nz, h);
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let mut field = Field::new(g);
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for k in 0..nz {
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for j in 0..ny {
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let u0 = inflow((j as f64 + 0.5) * h, (k as f64 + 0.5) * h);
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for i in 0..=nx {
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field.u[g.uface(k, j, i)] = u0;
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}
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}
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}
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solver.initialize(&mut field);
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let coef = 2.0 / (RHO * U_BAR * U_BAR * D * lz);
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let steps = (12.0 / dt).ceil() as usize;
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let start = std::time::Instant::now();
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let mut last = (0.0, 0.0);
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for step in 0..steps {
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let r = solver.advance(&mut field, dt);
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if (step + 1) % (steps / 20).max(1) == 0 || step + 1 == steps {
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let t = solver.time();
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let mask = solver.mask().unwrap();
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let body = solver.body().unwrap();
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let mu = RHO * NU;
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let (po, so) = mask.cut_wall_force_parts(body, &field, mu, t).unwrap();
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let ex = mask
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.cut_wall_exchange_force(body, &field, mu, RHO, t, None)
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.unwrap();
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let (pr, sr) = mask
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.cut_wall_force_reconstructed_parts(body, &field, mu, t, None)
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.unwrap();
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let margin = 1.5 * D;
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let ci = |x: f64| ((x / h).round() as usize).clamp(2, nx - 2);
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let cj = |y: f64| ((y / h).round() as usize).clamp(2, ny - 2);
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let bx = (
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ci(CX - margin),
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ci(CX + margin),
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cj(CY - 0.15),
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cj(CY + 0.15),
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0,
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nz,
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);
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let fcv = mask.control_volume_force_with_walls(&field, dt, RHO, mu, None, bx, false);
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let cd = |f: [f64; 3]| coef * f[0];
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println!(
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" t {t:7.3}: c_D operator {:.4} (p {:.4} + s {:.4} + exchange {:.4}) | reconstructed {:.4} (p {:.4} + s {:.4}) | box {:.4} c_L {:.5} Δp {:.5}; residual {:.1e} [{:.0} s]",
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cd(po) + cd(so) + cd(ex),
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cd(po),
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cd(so),
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cd(ex),
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cd(pr) + cd(sr),
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cd(pr),
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cd(sr),
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cd(fcv),
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coef * (po[1] + so[1] + ex[1]),
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mask.pressure_at(&field.p, CX - 0.5 * D, CY, 0.5 * lz)
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.unwrap_or(f64::NAN)
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- mask
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.pressure_at(&field.p, CX + 0.5 * D, CY, 0.5 * lz)
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.unwrap_or(f64::NAN),
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r.final_residual,
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start.elapsed().as_secs_f64()
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);
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let now = (cd(po) + cd(so) + cd(ex), cd(fcv));
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if (now.0 - last.0).abs() < 1e-4 * now.0.abs()
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&& (now.1 - last.1).abs() < 1e-4 * now.1.abs()
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&& t > 2.0
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{
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println!(" settled");
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break;
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}
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last = now;
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}
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}
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}
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