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