rtx-cfd: curvilinear collocated PISO on a structured patch (overset A-P0, WIP) — PatchMesh (right-handed s,n; periodic seam with shift; face metrics), patch generators (TFI, skewed annulus, sheared/varying-skew channels), CSR + Jacobi-BiCGSTAB, the Zang–Street–Koseff incremental step with the node-based 9-point L_f, LSQ gradients, explicit and line-implicit-n predictors, adjustPhi; tests: mesh metrics (5 green), operators exact on linear fields incl. the seam (green), sparse (2 green), MMS ladder (Cartesian 16/32: 1.37–1.39x the staggered error, order 0.83; n=64 stalls at a |du/dt| floor 2e-4 — open, tolerance-scaling hypothesis), annulus/Poiseuille not yet run
CI / Distributed Training Tests (push) Canceled after 0s
Performance Benchmarks / Run Benchmarks (push) Canceled after 0s
CI / Format Check (push) Canceled after 0s
CI / Clippy Check (push) Canceled after 0s
CI / Build (macos-latest) (push) Canceled after 0s
CI / Build (ubuntu-latest) (push) Canceled after 0s
CI / Test (macos-latest) (push) Canceled after 0s
CI / Test (ubuntu-latest) (push) Canceled after 0s
CI / Build CPU-Only (Explicit) (push) Canceled after 0s
CI / Python Bindings (maturin) (macos-latest) (push) Canceled after 0s
CI / Python Bindings (maturin) (ubuntu-latest) (push) Canceled after 0s
CI / WASM Build + Size Check (push) Canceled after 0s
CI / CI Success (push) Canceled after 0s
Documentation / Build API Documentation (push) Canceled after 0s
Documentation / Build User Guide (push) Canceled after 0s

Co-Authored-By: Claude Fable 5.1 <[email protected]>
Claude-Session: https://claude.ai/code/session_01X2GmJXeQ2njUecEKiJZ1G2
This commit is contained in:
Omar Sobh
2026-09-04 05:00:08 -07:00
co-authored by Claude Fable 5.1
parent 1347bc6772
commit 52da75a3a9
13 changed files with 2659 additions and 0 deletions
@@ -0,0 +1,283 @@
//! P0 gates 1, 2, 4 (`docs/overset_metal_campaign.md` §5.3): the
//! curvilinear collocated PISO on a Cartesian patch reproduces the
//! staggered PISO's manufactured-solution order and error to within 2×
//! (not bit-identical — a different discretisation); on a skewed,
//! stretched, periodic annulus it reaches order ≥ 1.8 in the Stokes limit
//! and ≈ 1 with upwind; every step is divergence-free to the solver's
//! tolerance.
use rtx_cfd::mesh::PatchMesh;
use rtx_cfd::mesh::patch_gen::{annulus_skewed, cartesian};
use rtx_cfd::solvers::incompressible::{
CurvilinearParameters, CurvilinearPisoSolver, NormalDiffusion, PatchConvection, PatchField,
};
use rtx_cfd::{CfdConfig, CfdResult};
use std::f64::consts::PI;
const RHO: f64 = 1.0;
const MU: f64 = 0.05;
fn u_exact(x: f64, y: f64) -> f64 {
(PI * x).sin() * (PI * y).cos()
}
fn v_exact(x: f64, y: f64) -> f64 {
-(PI * x).cos() * (PI * y).sin()
}
/// `f = ρ u·∇u (if convecting) μ ∇²u + ∇p`, `p = sin(πx) sin(πy)`
/// (the `mms_piso.rs` forcing).
fn source(x: f64, y: f64, convecting: bool) -> (f64, f64) {
let conv = if convecting { RHO * 0.5 * PI } else { 0.0 };
let fx = conv * (2.0 * PI * x).sin()
+ 2.0 * PI * PI * MU * u_exact(x, y)
+ PI * (PI * x).cos() * (PI * y).sin();
let fy = conv * (2.0 * PI * y).sin()
+ 2.0 * PI * PI * MU * v_exact(x, y)
+ PI * (PI * x).sin() * (PI * y).cos();
(fx, fy)
}
struct Measurement {
l2_velocity: f64,
max_div_rel: f64,
steps: usize,
}
/// Smallest across-patch cell size (the explicit diffusion limit).
fn min_spacing(mesh: &PatchMesh) -> f64 {
let mut h = f64::INFINITY;
for c in 0..mesh.cell_count() {
for (f, _) in mesh.cell_faces(c) {
let d = mesh.faces()[f].d;
h = h.min((d[0] * d[0] + d[1] * d[1]).sqrt());
}
}
h
}
async fn march(
mesh: PatchMesh,
convection: PatchConvection,
diffusion: NormalDiffusion,
steady_tol: f64,
) -> CfdResult<Measurement> {
let nu = MU / RHO;
let h = min_spacing(&mesh);
let env = |k: &str, d: f64| {
std::env::var(k)
.ok()
.and_then(|v| v.parse().ok())
.unwrap_or(d)
};
let dt = env("RTX_CURV_DTFRAC", 0.4) * (h * h / (4.0 * nu)).min(h);
let tol = env("RTX_CURV_TOL", 1e-10);
let config = CfdConfig::new()
.with_density(RHO)
.with_viscosity(MU)
.with_reference_velocity(1.0)
.with_reference_length(1.0);
let params = CurvilinearParameters {
tolerance: tol,
convection,
normal_diffusion: diffusion,
..CurvilinearParameters::default()
};
let convecting = convection == PatchConvection::Upwind;
let mut solver = CurvilinearPisoSolver::new(config, params, mesh)?;
solver.set_boundary_velocity(|x, y, _t| (u_exact(x, y), v_exact(x, y)));
solver.set_momentum_source(move |x, y, _t| source(x, y, convecting));
let mut field = PatchField::new(solver.mesh());
solver.initialize(&mut field, |_, _| (0.0, 0.0));
let mut steady = f64::INFINITY;
let mut max_div_rel = 0.0_f64;
let mut steps = 0;
for step in 0..400_000 {
let before = (field.u.clone(), field.v.clone());
let r = solver.advance(&mut field, dt).await?;
assert!(
r.poisson_converged,
"pressure solve did not converge at step {step}: {r:?}"
);
let flux_scale: f64 = field.flux.iter().map(|f| f.abs()).sum();
max_div_rel = max_div_rel.max(r.max_divergence / flux_scale.max(1e-300));
steps = step + 1;
let change = field
.u
.iter()
.zip(&before.0)
.chain(field.v.iter().zip(&before.1))
.map(|(a, b)| (a - b).abs())
.fold(0.0, f64::max);
steady = change / dt;
if step % 20_000 == 0 && std::env::var("RTX_CURV_TRACE").is_ok() {
println!(
" step {step} t={:.2} |du/dt| {steady:.3e} poisson iters {} div {:.2e}",
solver.time(),
r.poisson_iterations,
r.max_divergence
);
}
if steady < steady_tol {
break;
}
}
assert!(
steady < steady_tol,
"no steady state: |du/dt| = {steady:.3e}"
);
let mesh = solver.mesh();
let (mut sq, mut vol) = (0.0, 0.0);
for c in 0..mesh.cell_count() {
let xy = mesh.centre(c);
let eu = field.u[c] - u_exact(xy[0], xy[1]);
let ev = field.v[c] - v_exact(xy[0], xy[1]);
sq += (eu * eu + ev * ev) * mesh.area(c);
vol += mesh.area(c);
}
Ok(Measurement {
l2_velocity: (sq / vol).sqrt(),
max_div_rel,
steps,
})
}
fn orders(errs: &[f64]) -> Vec<f64> {
errs.windows(2).map(|p| (p[0] / p[1]).log2()).collect()
}
#[tokio::test]
async fn cartesian_patch_reproduces_the_staggered_piso_order_and_error() -> CfdResult<()> {
// mms_piso.rs (staggered PISO, upwind): 3.516214e-2 / 1.953750e-2 /
// 1.037512e-2 at 16/32/64, orders 0.85 / 0.91.
let reference = [3.516214e-2, 1.953750e-2, 1.037512e-2];
let only: Option<usize> = std::env::var("RTX_CURV_N")
.ok()
.and_then(|v| v.parse().ok());
let mut errs = Vec::new();
for (&n, &r) in [16usize, 32, 64].iter().zip(&reference) {
if only.is_some_and(|o| o != n) {
continue;
}
let m = march(
cartesian(n, n, 1.0, 1.0, false)?,
PatchConvection::Upwind,
NormalDiffusion::Explicit,
1e-6,
)
.await?;
println!(
"cartesian n={n}: L2 {:.6e} (staggered {r:.6e}, ratio {:.2}), max div {:.2e}, {} steps",
m.l2_velocity,
m.l2_velocity / r,
m.max_div_rel,
m.steps
);
assert!(m.max_div_rel < 1e-9, "divergence {:.3e}", m.max_div_rel);
assert!(
m.l2_velocity < 2.0 * r,
"L2 {:.3e} > 2x staggered {r:.3e}",
m.l2_velocity
);
errs.push(m.l2_velocity);
}
let o = orders(&errs);
println!("cartesian orders {o:?}");
if only.is_none() {
assert!(o.iter().all(|&x| x > 0.75 && x < 2.3), "orders {o:?}");
}
Ok(())
}
#[tokio::test]
async fn skewed_annulus_stokes_limit_is_second_order() -> CfdResult<()> {
for diffusion in [NormalDiffusion::Explicit, NormalDiffusion::LineImplicit] {
let mut errs = Vec::new();
for ns in [32usize, 64, 128] {
let m = march(
annulus_skewed([0.0, 0.0], 0.5, 1.5, ns, ns / 4, 0.3, 3.0)?,
PatchConvection::None,
diffusion,
1e-7,
)
.await?;
println!(
"annulus {diffusion:?} ns={ns}: L2 {:.6e}, max div {:.2e}, {} steps",
m.l2_velocity, m.max_div_rel, m.steps
);
assert!(m.max_div_rel < 1e-9, "divergence {:.3e}", m.max_div_rel);
errs.push(m.l2_velocity);
}
let o = orders(&errs);
println!("annulus {diffusion:?} Stokes orders {o:?}");
assert!(
o.iter().all(|&x| x >= 1.8),
"Stokes-limit orders {o:?} (gate >= 1.8)"
);
}
Ok(())
}
#[tokio::test]
async fn skewed_annulus_with_upwind_is_first_order() -> CfdResult<()> {
let mut errs = Vec::new();
for ns in [32usize, 64, 128] {
let m = march(
annulus_skewed([0.0, 0.0], 0.5, 1.5, ns, ns / 4, 0.3, 3.0)?,
PatchConvection::Upwind,
NormalDiffusion::Explicit,
1e-6,
)
.await?;
println!(
"annulus upwind ns={ns}: L2 {:.6e}, max div {:.2e}, {} steps",
m.l2_velocity, m.max_div_rel, m.steps
);
assert!(m.max_div_rel < 1e-9, "divergence {:.3e}", m.max_div_rel);
errs.push(m.l2_velocity);
}
let o = orders(&errs);
println!("annulus upwind orders {o:?}");
assert!(o.iter().all(|&x| x > 0.7 && x < 1.6), "upwind orders {o:?}");
Ok(())
}
#[tokio::test]
async fn snapshot_restore_rerun_is_bit_identical() -> CfdResult<()> {
let mesh = annulus_skewed([0.0, 0.0], 0.5, 1.5, 24, 6, 0.3, 2.0)?;
let config = CfdConfig::new().with_density(RHO).with_viscosity(MU);
let mut solver = CurvilinearPisoSolver::new(config, CurvilinearParameters::default(), mesh)?;
solver.set_boundary_velocity(|x, y, t| (u_exact(x, y) * (1.0 + 0.1 * t), v_exact(x, y)));
solver.set_momentum_source(|x, y, _| source(x, y, true));
let mut field = PatchField::new(solver.mesh());
solver.initialize(&mut field, |x, y| (u_exact(x, y), v_exact(x, y)));
let dt = 1e-3;
for _ in 0..5 {
solver.advance(&mut field, dt).await?;
}
let saved = solver.snapshot();
let field_saved = field.clone();
for _ in 0..10 {
solver.advance(&mut field, dt).await?;
}
let reference = (field.clone(), solver.time());
solver.restore(&saved);
field = field_saved;
for _ in 0..10 {
solver.advance(&mut field, dt).await?;
}
assert_eq!(solver.time().to_bits(), reference.1.to_bits());
let mut max_diff = 0.0_f64;
for (a, b) in field
.u
.iter()
.zip(&reference.0.u)
.chain(field.v.iter().zip(&reference.0.v))
.chain(field.p.iter().zip(&reference.0.p))
.chain(field.flux.iter().zip(&reference.0.flux))
{
max_diff = max_diff.max((a - b).abs());
}
assert!(max_diff == 0.0, "re-run differs by {max_diff:.3e}");
Ok(())
}