embedded3 S2-3d: face-momentum unsteady term for the box (Mask::box_momentum_rates, Solver::previous_apertures); falsifier prints the residual against it
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Co-Authored-By: Claude Fable 5.1 <[email protected]>
This commit is contained in:
Omar Sobh
2026-09-18 12:58:30 -05:00
co-authored by Claude Fable 5.1
parent cdd5ad0b66
commit 9ae0e42dcd
4 changed files with 111 additions and 1 deletions
@@ -485,3 +485,86 @@ impl Mask {
force
}
}
impl Mask {
/// S2-3d: the rate of change of the momentum the SCHEME carries in a
/// box — on the face control volumes, `Σ_f ρ h A (α_f u_f α_fⁿ u_fⁿ)/dt`
/// (faces on the box's own surfaces at half weight) — against the
/// cell-volume form of the box route's unsteady term, returned second.
/// Near an accelerating wall the two differ at O(h) in the cut cells.
#[must_use]
pub fn box_momentum_rates(
&self,
f: &Field,
dt: f64,
rho: f64,
(i0, i1, j0, j1, k0, k1): (usize, usize, usize, usize, usize, usize),
apertures_old: Option<&[Vec<f64>; 3]>,
vol_old: Option<&[f64]>,
) -> ([f64; 3], [f64; 3]) {
let g = self.grid();
let dv = g.dx * g.dy * g.dz;
let mut faces = [0.0; 3];
let mut cells = [0.0; 3];
let old = |c: usize, idx: usize, new: f64| apertures_old.map_or(new, |a| a[c][idx]);
for k in k0..k1 {
for j in j0..j1 {
for i in i0..=i1 {
let idx = g.uface(k, j, i);
let w = if i == i0 || i == i1 { 0.5 } else { 1.0 };
let a = self.a_u(idx);
faces[0] += w * rho * dv * (a * f.u[idx] - old(0, idx, a) * f.u_old[idx]) / dt;
}
}
for j in j0..=j1 {
for i in i0..i1 {
let idx = g.vface(k, j, i);
let w = if j == j0 || j == j1 { 0.5 } else { 1.0 };
let a = self.a_v(idx);
faces[1] += w * rho * dv * (a * f.v[idx] - old(1, idx, a) * f.v_old[idx]) / dt;
}
}
}
for k in k0..=k1 {
for j in j0..j1 {
for i in i0..i1 {
let kk = if k == g.nz && self.periodic_z() { 0 } else { k };
let idx = g.wface(kk, j, i);
let w = if (k == k0 || k == k1) && !self.periodic_z() {
0.5
} else if k == k1 {
0.0
} else {
1.0
};
let a = self.a_w(idx);
faces[2] += w * rho * dv * (a * f.w[idx] - old(2, idx, a) * f.w_old[idx]) / dt;
}
}
}
for k in k0..k1 {
for j in j0..j1 {
for i in i0..i1 {
let idx = g.cell(k, j, i);
let v_new = if self.is_fluid_cell(idx) {
self.vol(idx)
} else {
0.0
};
let v_old = vol_old.map_or(v_new, |vo| vo[idx]);
let c = |a: &[f64], f0: usize, f1: usize| 0.5 * (a[f0] + a[f1]);
let (fu0, fu1) = (g.uface(k, j, i), g.uface(k, j, i + 1));
let (fv0, fv1) = (g.vface(k, j, i), g.vface(k, j + 1, i));
let (fw0, fw1) = (g.wface(k, j, i), g.wface(k + 1, j, i));
cells[0] +=
rho * dv * (v_new * c(&f.u, fu0, fu1) - v_old * c(&f.u_old, fu0, fu1)) / dt;
cells[1] +=
rho * dv * (v_new * c(&f.v, fv0, fv1) - v_old * c(&f.v_old, fv0, fv1)) / dt;
cells[2] +=
rho * dv * (v_new * c(&f.w, fw0, fw1) - v_old * c(&f.w_old, fw0, fw1)) / dt;
}
}
}
(faces, cells)
}
}
@@ -183,6 +183,8 @@ pub struct Solver {
/// The previous mask's cell volumes (moving bodies; the box route's
/// unsteady term).
pub(super) vol_old: Vec<f64>,
/// The previous mask's face apertures (moving bodies; S2-3d).
pub(super) apertures_old: Option<[Vec<f64>; 3]>,
boundary_velocity: Option<Vec3Fn>,
body: Option<Body>,
/// The body moves: the mask is rebuilt at every step's new time.
@@ -216,6 +218,7 @@ impl Solver {
floor_source: std::cell::Cell::new([0.0; 3]),
pressure_lag: std::cell::Cell::new([0.0; 3]),
vol_old: Vec::new(),
apertures_old: None,
boundary_velocity: None,
body: None,
moving: false,
@@ -310,6 +313,13 @@ impl Solver {
self.pressure_lag.get()
}
/// The previous step's cell volumes (fraction of the cell; 0 for a
/// solid cell), once a moving body's mask has been rebuilt.
#[must_use]
pub fn previous_apertures(&self) -> Option<&[Vec<f64>; 3]> {
self.apertures_old.as_ref()
}
/// The previous step's cell volumes (fraction of the cell; 0 for a
/// solid cell), once a moving body's mask has been rebuilt.
#[must_use]
@@ -70,6 +70,9 @@ impl Solver {
self.last_ghost_correction = correction;
}
if let Some(old) = &self.mask {
self.apertures_old = old
.cut()
.map(|c| [c.a_u.clone(), c.a_v.clone(), c.a_w.clone()]);
self.vol_old = (0..field.grid.cells())
.map(|i| {
if old.is_fluid_cell(i) {
@@ -210,6 +210,8 @@ struct Record {
fy_lag: f64,
/// The force the momentum equation applied (shear on u*, exchange on uⁿ).
fy_applied: f64,
/// The box route with the scheme's own (face control volume) momentum rate.
fy_cv_faces: f64,
fresh: usize,
skipped: usize,
p_far: f64,
@@ -320,6 +322,15 @@ fn run(scheme: WallScheme, moving: bool, dt: f64, t_end: f64) -> Run {
false,
solver.previous_volumes(),
)[1] / lz;
let (rate_faces, rate_cells) = mask.box_momentum_rates(
&field,
dt,
RHO,
(margin, N - margin, margin, N - margin, 0, nz),
solver.previous_apertures(),
solver.previous_volumes(),
);
let fy_cv_faces = fy_cv + (rate_cells[1] - rate_faces[1]) / lz;
let p_far = field.p[g.cell(kp, jp, ip)];
let mut ke = 0.0;
for k in 0..nz {
@@ -357,6 +368,7 @@ fn run(scheme: WallScheme, moving: bool, dt: f64, t_end: f64) -> Run {
fy_floor,
fy_lag,
fy_applied,
fy_cv_faces,
fresh: result.fresh_cells,
skipped,
p_far,
@@ -370,13 +382,15 @@ fn run(scheme: WallScheme, moving: bool, dt: f64, t_end: f64) -> Run {
};
let mean = |f: &dyn Fn(&Record) -> f64| records.iter().map(f).sum::<f64>() / n;
println!(
" route residual (wall box) RMS {:.3e} → with the floor source {:.3e}, with the closure lag {:.3e}, both {:.3e}, APPLIED form {:.3e} (mean {:+.3e}); means wall {:+.3e} box {:+.3e} floor {:+.3e} lag {:+.3e}; box RMS {:.3e}",
" route residual (wall box) RMS {:.3e} → with the floor source {:.3e}, with the closure lag {:.3e}, both {:.3e}, APPLIED form {:.3e} (mean {:+.3e}), against the FACE-momentum box {:.3e} (its mean {:+.3e}); means wall {:+.3e} box {:+.3e} floor {:+.3e} lag {:+.3e}; box RMS {:.3e}",
rms(&|r| r.fy - r.fy_cv),
rms(&|r| r.fy + r.fy_floor - r.fy_cv),
rms(&|r| r.fy + r.fy_lag - r.fy_cv),
rms(&|r| r.fy + r.fy_floor + r.fy_lag - r.fy_cv),
rms(&|r| r.fy_applied - r.fy_cv),
mean(&|r| r.fy_applied),
rms(&|r| r.fy - r.fy_cv_faces),
mean(&|r| r.fy_cv_faces),
mean(&|r| r.fy),
mean(&|r| r.fy_cv),
mean(&|r| r.fy_floor),