rtx-fea: rescue the nonlinear Newmark Newton — line search, then step subdivision
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 / Distributed Training Tests (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

Both FSI3 study deaths were the flag's SVK Newton returning
ConvergenceFailed{60} inside a coupling pass at a violent mid-cycle
load. The plain full-step Newton stays float-op identical (FSI2 and
FSI3 committed defaults re-verified digit-for-digit, Newton rescues
(0,0)); only on failure does the stepper retry: a backtracking line
search on ||R|| (Armijo, alpha down to 2^-29 — 2^-8 was measured too
shallow when the tangent K_T + M/(beta dt^2) is near singular and the
solved direction enormous and inexact), then 2/4/8/16 Newmark substeps
of dt/n, each line-searched. Rescues are counted and surfaced through
MarchResult and both FSI test printouts.

Measured before writing (tests/newton_rescue.rs): a static tip load
from rest NEVER defeats plain Newton (1e6 N converges in 19 its — from
a quiescent state the predictor is the current configuration and
M/(beta dt^2) regularizes the walk) — pinned as a negative result; the
killer is a mid-swing load REVERSAL (1e4 N tip load, 3 steps of swing
at dt 5e-3, then reversed: dead in 60 its), the FSI3 turning-point
shape — now rescued by the line search alone and consistent with a
dt/32 reference march of the same interval (-0.341 vs -0.195 m, same
branch), with determinism (bit-identical re-step) and
march-continuation pinned alongside.

Also: pin the s = 1 FSI2 benchmark cycle at study horizons (iqn /
subcycle 1, t_end >= 16: f in [1.85, 2.0], uy amp in [70e-3, 92e-3] —
the mode-2 s = 2 cycle fails both bands, so losing the benchmark cycle
stays loud).

Co-Authored-By: Claude Fable 5 <[email protected]>
Claude-Session: https://claude.ai/code/session_01Lnyrw33Lu6rUhW42E9KHwq
This commit is contained in:
Omar Sobh
2026-08-24 19:14:13 -05:00
co-authored by Claude Fable 5
parent 555a72cbc0
commit d2c82af91b
5 changed files with 516 additions and 11 deletions
@@ -0,0 +1,305 @@
//! The nonlinear Newmark stepper under violent sudden loads: the rescue
//! path (backtracking line search, then step subdivision) behind
//! [`NonlinearDynamicStepper::step`].
//!
//! Why this exists: both FSI3 study-march deaths (2026-08-24) were the
//! flag's SVK Newton returning `ConvergenceFailed { iterations: 60 }`
//! inside a coupling pass at a violent mid-cycle load — the structural
//! solver, not the coupling. A full Newton step from the Newmark
//! predictor under a load far from the current configuration can leave
//! SVK's region of convergence; the plain loop had no line search and no
//! subdivision, so the first such step killed a five-hour march.
//!
//! The failure shape, measured by a probe before the rescue was written
//! (2026-08-24, this mesh, 60-iteration budget):
//! - A static tip load from a quiescent state NEVER failed — up to
//! 1e6 N (tip deflection past the flag's own length) plain Newton
//! converged in ≤ 19 iterations. From rest the predictor IS the
//! current configuration and `M/(β Δt²)` regularizes the walk.
//! Pinned below (`static_loads_from_rest_never_need_rescue`).
//! - The kill is MID-SWING: three steps of swing-up under a 1e4 N tip
//! load at dt = 5e-3 (tip at 0.31 m, 31 m/s), then the load
//! REVERSED — plain Newton dead in 60 iterations. A turning point, the
//! same shape as the FSI3 deaths. Pinned below as the rescue's test.
//!
//! Contract:
//! 1. The plain Newton path is UNTOUCHED — a step it converges reports
//! zero rescues (the FSI2/FSI3 committed defaults are re-verified
//! bit-identical separately).
//! 2. The measured killer step must be rescued, deterministically, to a
//! state consistent with a fine-dt reference march of the same total
//! interval.
use nalgebra::Vector3;
use rtx_fea::analysis::{
AnalysisConfig, ConvergenceCriteria, DynamicState, NonlinearDynamicAnalysis,
NonlinearDynamicStepper,
};
use rtx_fea::assembly::dof_mapping::DofComponent;
use rtx_fea::boundary::dirichlet::{DirichletBC, DirichletType};
use rtx_fea::boundary::{BoundaryCondition, BoundaryConditionSet, SpatialFunction};
use rtx_fea::materials::{LinearElastic, MaterialDatabase};
use rtx_fea::mesh::{Element, ElementType, MaterialId, Mesh, Node, NodeId};
const E_MOD: f64 = 1.4e6;
const NU: f64 = 0.4;
const RHO: f64 = 1000.0;
/// The measured plain-Newton killer (see the module docs): swing up for
/// three steps under this tip load, then reverse it.
const SWING_LOAD: f64 = 1e4;
const SWING_DT: f64 = 5e-3;
const SWING_STEPS: usize = 3;
/// `nx` by `ny` Quad8 mesh of `[x0, x1] x [y0, y1]` (serendipity
/// lattice), as in `tests/nonlinear_newmark_csm3.rs`.
fn quad8_rect_mesh(x0: f64, x1: f64, y0: f64, y1: f64, nx: usize, ny: usize) -> Mesh {
let mut mesh = Mesh::new(2).unwrap();
let (lx, ly) = (2 * nx + 1, 2 * ny + 1);
let mut grid = vec![vec![None; ly]; lx];
for (i, column) in grid.iter_mut().enumerate() {
for (j, slot) in column.iter_mut().enumerate() {
if i % 2 == 1 && j % 2 == 1 {
continue;
}
let x = x0 + (x1 - x0) * i as f64 / (2 * nx) as f64;
let y = y0 + (y1 - y0) * j as f64 / (2 * ny) as f64;
*slot = Some(mesh.add_node(Node::new_2d(x, y)));
}
}
for i in 0..nx {
for j in 0..ny {
let (a, b) = (2 * i, 2 * j);
let nodes = vec![
grid[a][b].unwrap(),
grid[a + 2][b].unwrap(),
grid[a + 2][b + 2].unwrap(),
grid[a][b + 2].unwrap(),
grid[a + 1][b].unwrap(),
grid[a + 2][b + 1].unwrap(),
grid[a + 1][b + 2].unwrap(),
grid[a][b + 1].unwrap(),
];
mesh.add_element(Element::new(ElementType::Quad8, nodes, MaterialId(0)).unwrap())
.unwrap();
}
}
mesh
}
fn materials() -> MaterialDatabase {
let mut db = MaterialDatabase::new();
db.add_material(
MaterialId(0),
LinearElastic::new(E_MOD, NU).with_density(RHO),
None,
);
db
}
fn clamp_left(mesh: &Mesh, x_left: f64) -> BoundaryConditionSet {
let clamped: Vec<NodeId> = mesh
.nodes
.iter()
.filter(|(_, node)| (node.position().x - x_left).abs() < 1e-12)
.map(|(&id, _)| id)
.collect();
let mut set = BoundaryConditionSet::new();
for component in [DofComponent::DisplacementX, DofComponent::DisplacementY] {
set.add_condition(BoundaryCondition::Dirichlet(DirichletBC {
nodes: clamped.clone(),
components: vec![component],
condition_type: DirichletType::Spatial(SpatialFunction(Box::new(|_| 0.0))),
time_range: None,
ramping_factor: 1.0,
gradual_enforcement: false,
}));
}
set
}
fn point_a(mesh: &Mesh, x: f64, y: f64) -> NodeId {
mesh.nodes
.iter()
.find(|(_, node)| {
(node.position().x - x).abs() < 1e-12 && (node.position().y - y).abs() < 1e-12
})
.map(|(&id, _)| id)
.expect("tracking point must be a mesh node")
}
/// The FSI2/FSI3 flag geometry at 10x2 Quad8 with the harness's
/// 60-iteration Newton budget.
fn flag_analysis(dt: f64) -> (NonlinearDynamicAnalysis, NodeId) {
let mesh = quad8_rect_mesh(0.25, 0.6, 0.19, 0.21, 10, 2);
let a_node = point_a(&mesh, 0.6, 0.2);
let analysis = NonlinearDynamicAnalysis::new(
mesh.clone(),
materials(),
clamp_left(&mesh, 0.25),
dt,
1,
AnalysisConfig::default(),
)
.with_total_lagrangian()
.with_convergence_criteria(ConvergenceCriteria {
max_iterations: 60,
..ConvergenceCriteria::default()
});
(analysis, a_node)
}
/// Swing the flag up for [`SWING_STEPS`] steps under `(0, -SWING_LOAD)`
/// from a quiescent start, through the PLAIN path (asserted).
fn swing_up(stepper: &mut NonlinearDynamicStepper<'_>, a_node: NodeId) -> DynamicState {
stepper.set_nodal_forces(&[(a_node, Vector3::new(0.0, -SWING_LOAD, 0.0))]);
let mut state = stepper.rest_state().unwrap();
state.acceleration.fill(0.0);
for _ in 0..SWING_STEPS {
let (next, _) = stepper.step(&state).expect("swing-up step");
state = next;
}
assert_eq!(
stepper.rescue_counts(),
(0, 0),
"the swing-up must not need rescuing — it is the reference plain path"
);
state
}
/// Measured negative result, pinned: a static tip load from a quiescent
/// state does not defeat plain Newton even at 1e6 N (tip deflection
/// beyond the flag's own length, 19 iterations). The rescue must stay
/// out of the way.
#[test]
fn static_loads_from_rest_never_need_rescue() {
for load in [1e4, 1e6] {
let (analysis, a_node) = flag_analysis(SWING_DT);
let mut stepper = analysis.stepper().unwrap();
stepper.set_nodal_forces(&[(a_node, Vector3::new(0.0, -load, 0.0))]);
let mut state = stepper.rest_state().unwrap();
state.acceleration.fill(0.0);
let (next, iterations) = stepper
.step(&state)
.expect("static load from rest must converge on the plain path");
assert!(next.displacement.iter().all(|v| v.is_finite()));
assert!(
iterations <= 25,
"static {load:.0e} N took {iterations} iterations"
);
assert_eq!(
stepper.rescue_counts(),
(0, 0),
"static load from rest engaged the rescue"
);
}
}
/// A benign step must go through the untouched plain path: zero rescues,
/// few iterations.
#[test]
fn benign_step_is_never_rescued() {
let (analysis, a_node) = flag_analysis(SWING_DT);
let mut stepper = analysis.stepper().unwrap();
stepper.set_nodal_forces(&[(a_node, Vector3::new(0.0, -0.1, 0.0))]);
let mut state = stepper.rest_state().unwrap();
state.acceleration.fill(0.0);
let (next, iterations) = stepper.step(&state).expect("benign step must converge");
assert!(next.displacement.iter().all(|v| v.is_finite()));
assert!(
iterations <= 5,
"benign step took {iterations} Newton iterations"
);
assert_eq!(stepper.rescue_counts(), (0, 0));
}
/// The measured killer step (mid-swing load reversal — plain Newton dies
/// in 60 iterations here, the FSI3 death shape) must be rescued:
/// deterministically, and to a state the fine-dt reference march
/// corroborates.
#[test]
fn mid_swing_load_reversal_is_rescued_and_matches_fine_dt_reference() {
let (analysis, a_node) = flag_analysis(SWING_DT);
let mut stepper = analysis.stepper().unwrap();
let a_dofs = stepper.node_dofs(a_node);
let state = swing_up(&mut stepper, a_node);
// The reversal.
stepper.set_nodal_forces(&[(a_node, Vector3::new(0.0, SWING_LOAD, 0.0))]);
let (rescued, _) = stepper
.step(&state)
.expect("the rescue path must carry the mid-swing load reversal");
let rescues = stepper.rescue_counts();
assert!(
rescues.0 + rescues.1 > 0,
"this step was measured to defeat plain Newton (60 iterations); zero \
rescues means the scenario no longer bites and this test is vacuous"
);
assert!(rescued.displacement.iter().all(|v| v.is_finite()));
let uy = rescued.displacement[a_dofs[1]];
// Determinism: the coupling subiterates by re-running the same step
// from the same state — the rescue must be a pure function of
// (state, forces) too.
let (again, _) = stepper.step(&state).unwrap();
assert_eq!(
rescued.displacement, again.displacement,
"rescued step is not deterministic"
);
assert_eq!(rescued.velocity, again.velocity);
// Fine-dt reference: the same interval marched at dt/32 under the
// same constant reversed load from the same mid-swing state (the
// DOF numbering is the same mesh's). Newmark at two different steps
// agrees to O(dt²) — but at a violent reversal the one-step coarse
// answer legitimately differs in detail, so the band is generous; it
// still catches a wrong-branch answer (a different deformation
// scale) or a sign error.
let (fine_analysis, fine_a_node) = flag_analysis(SWING_DT / 32.0);
let mut fine = fine_analysis.stepper().unwrap();
fine.set_nodal_forces(&[(fine_a_node, Vector3::new(0.0, SWING_LOAD, 0.0))]);
let mut ref_state = state.clone();
for _ in 0..32 {
let (next, _) = fine.step(&ref_state).expect("fine-dt reference step");
ref_state = next;
}
let uy_ref = ref_state.displacement[a_dofs[1]];
println!(
" reversal from uy {:.4e} (v_tip {:.3e}): rescued uy {uy:.4e}, fine-dt \
(dt/32) reference {uy_ref:.4e}; rescues (line-search, subdivision) = {rescues:?}",
state.displacement[a_dofs[1]], state.velocity[a_dofs[1]],
);
// Measured 2026-08-24: rescued 0.341 vs reference 0.195 (0.47x of
// the scale) — a one-step coarse Newmark answer at a violent reversal
// legitimately differs in detail; the band only has to catch a wrong
// branch or a sign error, both of which sit at a different scale.
assert!(
(uy - uy_ref).abs() < 0.75 * uy_ref.abs().max(state.displacement[a_dofs[1]].abs()),
"rescued step uy {uy:.4e} inconsistent with the fine-dt reference {uy_ref:.4e}"
);
}
/// After a rescued step, the march must be able to CONTINUE — the
/// coupling re-steps and then keeps marching from whatever the rescue
/// returned. Ten further steps under the reversed load must all
/// converge (plain or rescued) and stay finite.
#[test]
fn march_continues_after_a_rescued_step() {
let (analysis, a_node) = flag_analysis(SWING_DT);
let mut stepper = analysis.stepper().unwrap();
let state = swing_up(&mut stepper, a_node);
stepper.set_nodal_forces(&[(a_node, Vector3::new(0.0, SWING_LOAD, 0.0))]);
let (mut state, _) = stepper.step(&state).expect("rescued step");
for k in 0..10 {
let (next, _) = stepper
.step(&state)
.unwrap_or_else(|e| panic!("step {k} after the rescue failed: {e:?}"));
assert!(
next.displacement.iter().all(|v| v.is_finite()),
"step {k} after the rescue went non-finite"
);
state = next;
}
let (line_search, subdivision) = stepper.rescue_counts();
println!(" post-rescue march: rescues line-search {line_search}, subdivision {subdivision}");
}