embedded3: moving-body box route (Δ(Vu) unsteady term, Solver::previous_volumes), floor-source / closure-lag / applied-force instruments, moving.rs split; falsifier prints the route residual under each

Co-Authored-By: Claude Fable 5.1 <[email protected]>

crates/specialized/rtx-cfd/src/solvers/incompressible/embedded3/exchange.rs

@@ -140,4 +140,74 @@ impl Mask {
         }
         Some(force)
     }
+
+    /// The closure lag of a moving body's pressure correction: the
+    /// corrector applies `p'` on the STEP apertures while the operator
+    /// route reads the summed pressure on the END apertures, so the exact
+    /// discrete force carries `Σ_c p'_c (W_step,c − W_end,c)` (a force on
+    /// the body) that the route lacks. Zero for a body at rest.
+    #[must_use]
+    pub fn closure_lag(&self, p_prime: &[f64]) -> [f64; 3] {
+        let g = self.grid;
+        let area = [g.dy * g.dz, g.dx * g.dz, g.dx * g.dy];
+        let mut lag = [0.0; 3];
+        if self.step_apertures.is_none() {
+            return lag;
+        }
+        for k in 0..g.nz {
+            for j in 0..g.ny {
+                for i in 0..g.nx {
+                    let idx = g.cell(k, j, i);
+                    if !self.cell_active(idx) {
+                        continue;
+                    }
+                    let pp = p_prime[idx];
+                    if pp == 0.0 {
+                        continue;
+                    }
+                    // W_c = −Σ A_f n_f: x-part −(α_e − α_w) A_x, etc.
+                    let (ue, uw) = (g.uface(k, j, i + 1), g.uface(k, j, i));
+                    let (vn, vs) = (g.vface(k, j + 1, i), g.vface(k, j, i));
+                    let (wt, wb) = (g.wface(k + 1, j, i), g.wface(k, j, i));
+                    let d = [
+                        (self.au_step(ue) - self.a_u(ue)) - (self.au_step(uw) - self.a_u(uw)),
+                        (self.av_step(vn) - self.a_v(vn)) - (self.av_step(vs) - self.a_v(vs)),
+                        (self.aw_step(wt) - self.a_w(wt)) - (self.aw_step(wb) - self.a_w(wb)),
+                    ];
+                    for c in 0..3 {
+                        lag[c] += pp * (-d[c]) * area[c];
+                    }
+                }
+            }
+        }
+        lag
+    }
+
+    /// The force the discrete momentum equation actually applied over the
+    /// last step, read post-step: the pressure part on the end field, the
+    /// implicit wall shear on the PREDICTED velocities `u*` (the corrector
+    /// moves `u` without re-applying the shear) and the explicit wall
+    /// exchange on the OLD velocities. On a body at rest at a steady state
+    /// this equals `cut_wall_force`; on a moving body it is the number the
+    /// box route should reproduce.
+    pub fn cut_wall_force_applied(
+        &self,
+        body: &Body,
+        f: &Field,
+        mu: f64,
+        rho: f64,
+        t: f64,
+    ) -> Option<[f64; 3]> {
+        let mut star = f.clone();
+        star.u.copy_from_slice(&f.u_star);
+        star.v.copy_from_slice(&f.v_star);
+        star.w.copy_from_slice(&f.w_star);
+        let (p, s) = self.cut_wall_force_parts(body, &star, mu, t)?;
+        let mut old = f.clone();
+        old.u.copy_from_slice(&f.u_old);
+        old.v.copy_from_slice(&f.v_old);
+        old.w.copy_from_slice(&f.w_old);
+        let x = self.cut_wall_exchange_force(body, &old, mu, rho, t, None)?;
+        Some([p[0] + s[0] + x[0], p[1] + s[1] + x[1], p[2] + s[2] + x[2]])
+    }
 }

crates/specialized/rtx-cfd/src/solvers/incompressible/embedded3/loads.rs

@@ -288,6 +288,25 @@ impl Mask {
     /// without it (slip or periodic sides) the z faces carry nothing.
     #[allow(clippy::too_many_arguments)]
     pub fn control_volume_force_with_walls(
+        &self,
+        f: &Field,
+        dt: f64,
+        rho: f64,
+        mu: f64,
+        source: Option<&dyn Fn(f64, f64, f64) -> (f64, f64, f64)>,
+        bx: (usize, usize, usize, usize, usize, usize),
+        no_slip_z: bool,
+    ) -> [f64; 3] {
+        self.control_volume_force_moving(f, dt, rho, mu, source, bx, no_slip_z, None)
+    }
+
+    /// The box route on a moving body: the unsteady term is the change of
+    /// the momentum `ρ V u` over the step with the previous step's cell
+    /// volumes `vol_old` (`Solver::previous_volumes`), so the fluid the
+    /// wall sweeps counts (`Σ ρ V (u − uⁿ)/dt` misses `ρ (V − Vⁿ) uⁿ/dt`).
+    /// `None` falls back to the fixed-volume form.
+    #[allow(clippy::too_many_arguments)]
+    pub fn control_volume_force_moving(
         &self,
         f: &Field,
         dt: f64,
@@ -296,6 +315,7 @@ impl Mask {
         source: Option<&dyn Fn(f64, f64, f64) -> (f64, f64, f64)>,
         (i0, i1, j0, j1, k0, k1): (usize, usize, usize, usize, usize, usize),
         no_slip_z: bool,
+        vol_old: Option<&[f64]>,
     ) -> [f64; 3] {
         let g = self.grid();
         let (nx, ny, nz, dx, dy, dz) = (g.nx, g.ny, g.nz, g.dx, g.dy, g.dz);
@@ -427,19 +447,28 @@ impl Mask {
             for j in j0..j1 {
                 for i in i0..i1 {
                     let idx = g.cell(k, j, i);
-                    if !self.is_fluid_cell(idx) {
+                    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]);
+                    if v_new == 0.0 && v_old == 0.0 {
                         continue;
                     }
-                    let dv = dv * self.vol(idx);
                     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));
-                    let du = 0.5 * ((u[fu0] - f.u_old[fu0]) + (u[fu1] - f.u_old[fu1]));
+                    let cen = |a: &[f64], b: &[f64], f0: usize, f1: usize| {
-                    let dvv = 0.5 * ((v[fv0] - f.v_old[fv0]) + (v[fv1] - f.v_old[fv1]));
+                        (0.5 * (a[f0] + a[f1]), 0.5 * (b[f0] + b[f1]))
-                    let dw = 0.5 * ((w[fw0] - f.w_old[fw0]) + (w[fw1] - f.w_old[fw1]));
+                    };
-                    force[0] -= rho * du / dt * dv;
+                    let (un, uo) = cen(u, &f.u_old, fu0, fu1);
-                    force[1] -= rho * dvv / dt * dv;
+                    let (vn, vo) = cen(v, &f.v_old, fv0, fv1);
-                    force[2] -= rho * dw / dt * dv;
+                    let (wn, wo) = cen(w, &f.w_old, fw0, fw1);
+                    force[0] -= rho * (v_new * un - v_old * uo) / dt * dv;
+                    force[1] -= rho * (v_new * vn - v_old * vo) / dt * dv;
+                    force[2] -= rho * (v_new * wn - v_old * wo) / dt * dv;
+                    let dv = dv * v_new;
                     if let Some(s) = source {
                         let (sx, sy, sz) = s(
                             (i as f64 + 0.5) * dx,

crates/specialized/rtx-cfd/src/solvers/incompressible/embedded3/step/cut_predictor.rs

@@ -25,6 +25,7 @@ impl Solver {
         let periodic = self.params.boundaries.periodic_z();
         let lat = mask.lattice();
         let w_range = if periodic { 0..nz } else { 1..nz };
+        let mut floor = [0.0; 3];
         for c in 0..3 {
             let (ir, jr, kr) = match c {
                 0 => (1..nx, 0..ny, 0..nz),
@@ -45,7 +46,9 @@ impl Solver {
                         }
                         let p = [i as i64, j as i64, k as i64];
                         let idx = lat.face(c, p).expect("face");
-                        updates.push((idx, self.cut_face_update(field, c, p, dt, t_old)));
+                        let (val, src) = self.cut_face_update(field, c, p, dt, t_old);
+                        floor[c] += src;
+                        updates.push((idx, val));
                     }
                 }
             }
@@ -58,6 +61,7 @@ impl Solver {
                 out[idx] = val;
             }
         }
+        self.floor_source.set(floor);
         if periodic {
             for j in 0..ny {
                 for i in 0..nx {
@@ -68,9 +72,17 @@ impl Solver {
     }
 
     /// The predicted value of the unknown face of component `c` at lattice
-    /// `p` from the old field.
+    /// `p` from the old field, with the momentum the inertia floor added
+    /// on this face, `ρ (V_eff − V_α)(u* − uⁿ)/dt`.
     #[allow(clippy::too_many_lines)]
-    fn cut_face_update(&self, field: &Field, c: usize, p: [i64; 3], dt: f64, t_old: f64) -> f64 {
+    fn cut_face_update(
+        &self,
+        field: &Field,
+        c: usize,
+        p: [i64; 3],
+        dt: f64,
+        t_old: f64,
+    ) -> (f64, f64) {
         let mask = self.mask.as_ref().expect("cut mask");
         let body = self.body.as_ref().expect("body");
         let g = field.grid;
@@ -223,6 +235,9 @@ impl Solver {
         };
         let v_eff = fraction.max(INERTIA_FLOOR) * h[c] * area[c];
         let inertia = rho * v_eff / dt;
-        (inertia * u0 - conv + diff + pressure + source + shear * ub) / (inertia + shear)
+        let u_star =
+            (inertia * u0 - conv + diff + pressure + source + shear * ub) / (inertia + shear);
+        let v_alpha = fraction * h[c] * area[c];
+        (u_star, rho * (v_eff - v_alpha) * (u_star - u0) / dt)
     }
 }

crates/specialized/rtx-cfd/src/solvers/incompressible/embedded3/step/mod.rs

@@ -7,6 +7,7 @@
 mod cut_predictor;
 #[cfg(feature = "cuda")]
 pub mod device;
+mod moving;
 mod predictor;
 mod projection;
 
@@ -128,6 +129,17 @@ pub struct Solver {
     pub fluid: Fluid,
     pub params: Parameters,
     pub(super) momentum_source: Option<Vec3Fn>,
+    /// The momentum the small-cell inertia floor added over the last
+    /// step, `Σ ρ (V_eff − V_α)(u* − uⁿ)/dt` over the unknown faces (host
+    /// cut predictor only): the box route counts it, the operator route
+    /// does not.
+    pub(super) floor_source: std::cell::Cell<[f64; 3]>,
+    /// The closure lag of the pressure corrections over the last step
+    /// (`Mask::closure_lag` summed over the correctors; host path).
+    pub(super) pressure_lag: std::cell::Cell<[f64; 3]>,
+    /// The previous mask's cell volumes (moving bodies; the box route's
+    /// unsteady term).
+    pub(super) vol_old: Vec<f64>,
     boundary_velocity: Option<Vec3Fn>,
     body: Option<Body>,
     /// The body moves: the mask is rebuilt at every step's new time.
@@ -158,6 +170,9 @@ impl Solver {
             fluid,
             params,
             momentum_source: None,
+            floor_source: std::cell::Cell::new([0.0; 3]),
+            pressure_lag: std::cell::Cell::new([0.0; 3]),
+            vol_old: Vec::new(),
             boundary_velocity: None,
             body: None,
             moving: false,
@@ -221,6 +236,27 @@ impl Solver {
         .expect("embedded mask")
     }
 
+    /// The small-cell floor's momentum source over the last step (a force
+    /// on the fluid; host cut predictor only, zero otherwise).
+    #[must_use]
+    pub fn floor_source(&self) -> [f64; 3] {
+        self.floor_source.get()
+    }
+
+    /// The pressure corrections' closure lag over the last step (a force
+    /// on the body the operator route lacks on a moving body; host path).
+    #[must_use]
+    pub fn pressure_lag(&self) -> [f64; 3] {
+        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_volumes(&self) -> Option<&[f64]> {
+        (!self.vol_old.is_empty()).then_some(self.vol_old.as_slice())
+    }
+
     #[must_use]
     pub fn body(&self) -> Option<&Body> {
         self.body.as_ref()
@@ -506,69 +542,6 @@ impl Solver {
         &self.wall_fluxes
     }
 
-    /// The moving body's mask at the end-of-step geometry `t_new`: the
-    /// pressure of the cells that just became fluid refilled from their
-    /// neighbours (fluid in both masks), the new mask's prescribed and
-    /// ghost values imposed from the previous corrected field, the
-    /// step-averaged apertures and the GCL wall-flux table (cut wall).
-    /// Returns the fresh-cell count. `field` holds the predicted field.
-    pub fn rebuild_moving_mask(&mut self, field: &mut Field, dt: f64, t_new: f64) -> usize {
-        let Some(body) = &self.body else {
-            return 0;
-        };
-        let mut fresh_cells = 0;
-        let mut new_mask = self.build_mask(body, field.grid, t_new, dt);
-        if let Some(old_mask) = &self.mask {
-            fresh_cells = refill_fresh_cells(old_mask, &new_mask, field);
-            let n_in = self.params.aperture_substeps;
-            if n_in == 0 {
-                new_mask.set_step_apertures(old_mask);
-            } else {
-                // The intermediate geometries, each within the band of the
-                // previous one.
-                let g = field.grid;
-                let h = g.dx.min(g.dy).min(g.dz);
-                let t_old = t_new - dt;
-                let mut inner: Vec<CutGeometry> = Vec::with_capacity(n_in);
-                for m in 1..=n_in {
-                    let tm = t_old + dt * m as f64 / (n_in + 1) as f64;
-                    let prev: Option<(&CutGeometry, f64, f64)> = match (
-                        self.params.max_surface_speed,
-                        inner.last().or(old_mask.cut()),
-                    ) {
-                        (Some(speed), Some(c)) => {
-                            Some((c, 3.0 * h, speed * dt / (n_in + 1) as f64))
-                        }
-                        _ => None,
-                    };
-                    inner.push(CutGeometry::build_from(body, g, tm, prev));
-                }
-                let refs: Vec<&CutGeometry> = inner.iter().collect();
-                new_mask.set_step_apertures_with(old_mask, &refs);
-            }
-        }
-        new_mask.impose_from(
-            body,
-            &field.u_old,
-            &field.v_old,
-            &field.w_old,
-            &mut field.u,
-            &mut field.v,
-            &mut field.w,
-            t_new,
-        );
-        if new_mask.cut().is_some() {
-            let (table, correction) = match &self.mask {
-                Some(old_mask) => new_mask.gcl_flux_table(old_mask, dt),
-                None => new_mask.wall_flux_table(body, t_new),
-            };
-            self.wall_fluxes = table;
-            self.last_ghost_correction = correction;
-        }
-        self.mask = Some(new_mask);
-        fresh_cells
-    }
-
     /// One step of `dt`: predictor, correctors, clock.
     pub fn advance(&mut self, field: &mut Field, dt: f64) -> StepResult {
         assert!(
@@ -581,6 +554,7 @@ impl Solver {
         let t_old = self.time;
         let t_new = t_old + dt;
         field.update_old_values();
+        self.pressure_lag.set([0.0; 3]);
         self.momentum_predictor(field, dt, t_old);
         self.apply_boundary_normals(field, t_new);
         // A moving body: the mask at the end-of-step geometry.
@@ -607,6 +581,14 @@ impl Solver {
         let mut poisson_iterations = 0;
         for corrector in 0..self.params.corrector_steps.max(1) {
             let sol = self.solve_correction(field, dt, corrector == 0);
+            if let Some(m) = self.mask.as_ref() {
+                let l = m.closure_lag(&field.p_prime);
+                let mut acc = self.pressure_lag.get();
+                for c in 0..3 {
+                    acc[c] += l[c];
+                }
+                self.pressure_lag.set(acc);
+            }
             poisson_iterations += sol.iterations;
             let mass_residual = self.apply_correction(field, dt);
             if std::env::var_os("RTX_E3_DEBUG").is_some() {
@@ -637,61 +619,3 @@ impl Solver {
         }
     }
 }
-
-/// Refill the pressure of the cells fluid in `new` and not in `old` from
-/// their face neighbours fluid in both; returns their count.
-fn refill_fresh_cells(old: &Mask, new: &Mask, field: &mut Field) -> usize {
-    let g = field.grid;
-    let (nx, ny, nz) = (g.nx, g.ny, g.nz);
-    let periodic = new.periodic_z();
-    let mut fresh = 0;
-    let mut refills = Vec::new();
-    for k in 0..nz {
-        for j in 0..ny {
-            for i in 0..nx {
-                let idx = g.cell(k, j, i);
-                if !(new.is_fluid_cell(idx) && !old.is_fluid_cell(idx)) {
-                    continue;
-                }
-                fresh += 1;
-                let mut sum = 0.0;
-                let mut count = 0usize;
-                let mut visit = |nb: usize| {
-                    if new.is_fluid_cell(nb) && old.is_fluid_cell(nb) {
-                        sum += field.p[nb];
-                        count += 1;
-                    }
-                };
-                if i + 1 < nx {
-                    visit(g.cell(k, j, i + 1));
-                }
-                if i > 0 {
-                    visit(g.cell(k, j, i - 1));
-                }
-                if j + 1 < ny {
-                    visit(g.cell(k, j + 1, i));
-                }
-                if j > 0 {
-                    visit(g.cell(k, j - 1, i));
-                }
-                if k + 1 < nz {
-                    visit(g.cell(k + 1, j, i));
-                } else if periodic && nz > 1 {
-                    visit(g.cell(0, j, i));
-                }
-                if k > 0 {
-                    visit(g.cell(k - 1, j, i));
-                } else if periodic && nz > 1 {
-                    visit(g.cell(nz - 1, j, i));
-                }
-                if count > 0 {
-                    refills.push((idx, sum / count as f64));
-                }
-            }
-        }
-    }
-    for (idx, p) in refills {
-        field.p[idx] = p;
-    }
-    fresh
-}

crates/specialized/rtx-cfd/src/solvers/incompressible/embedded3/step/moving.rs

@@ -0,0 +1,141 @@
+//! The moving body's per-step mask rebuild: fresh-cell pressure refill,
+//! imposition from history, step-averaged apertures, the GCL wall-flux
+//! table and the previous volumes for the box route.
+use super::super::cut::CutGeometry;
+use super::super::field::Field;
+use super::super::wall::{Mask, WallScheme};
+use super::Solver;
+
+impl Solver {
+    /// The moving body's mask at the end-of-step geometry `t_new`: the
+    /// pressure of the cells that just became fluid refilled from their
+    /// neighbours (fluid in both masks), the new mask's prescribed and
+    /// ghost values imposed from the previous corrected field, the
+    /// step-averaged apertures and the GCL wall-flux table (cut wall).
+    /// Returns the fresh-cell count. `field` holds the predicted field.
+    pub fn rebuild_moving_mask(&mut self, field: &mut Field, dt: f64, t_new: f64) -> usize {
+        let Some(body) = &self.body else {
+            return 0;
+        };
+        let mut fresh_cells = 0;
+        let mut new_mask = self.build_mask(body, field.grid, t_new, dt);
+        if let Some(old_mask) = &self.mask {
+            fresh_cells = refill_fresh_cells(old_mask, &new_mask, field);
+            let n_in = self.params.aperture_substeps;
+            if n_in == 0 {
+                new_mask.set_step_apertures(old_mask);
+            } else {
+                // The intermediate geometries, each within the band of the
+                // previous one.
+                let g = field.grid;
+                let h = g.dx.min(g.dy).min(g.dz);
+                let t_old = t_new - dt;
+                let mut inner: Vec<CutGeometry> = Vec::with_capacity(n_in);
+                for m in 1..=n_in {
+                    let tm = t_old + dt * m as f64 / (n_in + 1) as f64;
+                    let prev: Option<(&CutGeometry, f64, f64)> = match (
+                        self.params.max_surface_speed,
+                        inner.last().or(old_mask.cut()),
+                    ) {
+                        (Some(speed), Some(c)) => {
+                            Some((c, 3.0 * h, speed * dt / (n_in + 1) as f64))
+                        }
+                        _ => None,
+                    };
+                    inner.push(CutGeometry::build_from(body, g, tm, prev));
+                }
+                let refs: Vec<&CutGeometry> = inner.iter().collect();
+                new_mask.set_step_apertures_with(old_mask, &refs);
+            }
+        }
+        new_mask.impose_from(
+            body,
+            &field.u_old,
+            &field.v_old,
+            &field.w_old,
+            &mut field.u,
+            &mut field.v,
+            &mut field.w,
+            t_new,
+        );
+        if new_mask.cut().is_some() {
+            let (table, correction) = match &self.mask {
+                Some(old_mask) => new_mask.gcl_flux_table(old_mask, dt),
+                None => new_mask.wall_flux_table(body, t_new),
+            };
+            self.wall_fluxes = table;
+            self.last_ghost_correction = correction;
+        }
+        if let Some(old) = &self.mask {
+            self.vol_old = (0..field.grid.cells())
+                .map(|i| {
+                    if old.is_fluid_cell(i) {
+                        old.vol(i)
+                    } else {
+                        0.0
+                    }
+                })
+                .collect();
+        }
+        self.mask = Some(new_mask);
+        fresh_cells
+    }
+}
+
+/// Refill the pressure of the cells fluid in `new` and not in `old` from
+/// their face neighbours fluid in both; returns their count.
+fn refill_fresh_cells(old: &Mask, new: &Mask, field: &mut Field) -> usize {
+    let g = field.grid;
+    let (nx, ny, nz) = (g.nx, g.ny, g.nz);
+    let periodic = new.periodic_z();
+    let mut fresh = 0;
+    let mut refills = Vec::new();
+    for k in 0..nz {
+        for j in 0..ny {
+            for i in 0..nx {
+                let idx = g.cell(k, j, i);
+                if !(new.is_fluid_cell(idx) && !old.is_fluid_cell(idx)) {
+                    continue;
+                }
+                fresh += 1;
+                let mut sum = 0.0;
+                let mut count = 0usize;
+                let mut visit = |nb: usize| {
+                    if new.is_fluid_cell(nb) && old.is_fluid_cell(nb) {
+                        sum += field.p[nb];
+                        count += 1;
+                    }
+                };
+                if i + 1 < nx {
+                    visit(g.cell(k, j, i + 1));
+                }
+                if i > 0 {
+                    visit(g.cell(k, j, i - 1));
+                }
+                if j + 1 < ny {
+                    visit(g.cell(k, j + 1, i));
+                }
+                if j > 0 {
+                    visit(g.cell(k, j - 1, i));
+                }
+                if k + 1 < nz {
+                    visit(g.cell(k + 1, j, i));
+                } else if periodic && nz > 1 {
+                    visit(g.cell(0, j, i));
+                }
+                if k > 0 {
+                    visit(g.cell(k - 1, j, i));
+                } else if periodic && nz > 1 {
+                    visit(g.cell(nz - 1, j, i));
+                }
+                if count > 0 {
+                    refills.push((idx, sum / count as f64));
+                }
+            }
+        }
+    }
+    for (idx, p) in refills {
+        field.p[idx] = p;
+    }
+    fresh
+}

crates/specialized/rtx-cfd/tests/embedded3_falsifier.rs

@@ -204,6 +204,12 @@ struct Record {
     /// Load per unit span by the control-volume route (a box of whole
     /// cells around the body, reading no near-wall value).
     fy_cv: f64,
+    /// The inertia floor's momentum source per unit span (cut wall).
+    fy_floor: f64,
+    /// The pressure corrections' closure lag per unit span (cut wall).
+    fy_lag: f64,
+    /// The force the momentum equation applied (shear on u*, exchange on uⁿ).
+    fy_applied: f64,
     fresh: usize,
     skipped: usize,
     p_far: f64,
@@ -294,14 +300,25 @@ fn run(scheme: WallScheme, moving: bool, dt: f64, t_end: f64) -> Run {
             }
         }
         fy /= lz;
+        let fy_floor = solver.floor_source()[1] / lz;
+        let fy_lag = solver.pressure_lag()[1] / lz;
+        let fy_applied = if scheme == WallScheme::CutCell {
+            mask.cut_wall_force_applied(body, &field, MU, RHO, t)
+                .expect("applied")[1]
+                / lz
+        } else {
+            0.0
+        };
         let margin = 8;
-        let fy_cv = mask.control_volume_force(
+        let fy_cv = mask.control_volume_force_moving(
             &field,
             dt,
             RHO,
             MU,
             None,
             (margin, N - margin, margin, N - margin, 0, nz),
+            false,
+            solver.previous_volumes(),
         )[1] / lz;
         let p_far = field.p[g.cell(kp, jp, ip)];
         let mut ke = 0.0;
@@ -337,12 +354,36 @@ fn run(scheme: WallScheme, moving: bool, dt: f64, t_end: f64) -> Run {
             t,
             fy,
             fy_cv,
+            fy_floor,
+            fy_lag,
+            fy_applied,
             fresh: result.fresh_cells,
             skipped,
             p_far,
             ke,
         });
     }
+    if scheme == WallScheme::CutCell {
+        let n = records.len().max(1) as f64;
+        let rms = |f: &dyn Fn(&Record) -> f64| {
+            (records.iter().map(|r| f(r) * f(r)).sum::<f64>() / n).sqrt()
+        };
+        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}",
+            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),
+            mean(&|r| r.fy),
+            mean(&|r| r.fy_cv),
+            mean(&|r| r.fy_floor),
+            mean(&|r| r.fy_lag),
+            rms(&|r| r.fy_cv)
+        );
+    }
     Run {
         records,
         energy_per_flip,