model: nonlinear static steps and neo-Hookean hyperelasticity, mapped by the deck writers

A nonlinear_static procedure (nonlinear geometry, initial/min/max increments,
increment and iteration caps, force/displacement/energy tolerances, line
search), validated with caps against hostile values. Materials gain an
explicit hyperelastic option (decoupled compressible neo-Hookean on the
isotropic constants). Abaqus writes *STEP, NLGEOM, INC / *STATIC with the
increments and *HYPERELASTIC, NEO HOOKE; LS-DYNA writes the ramped implicit
run with full Newton and *CONTROL_IMPLICIT_AUTO; Nastran refuses SOL 400 by
name, as LS-DYNA does hyperelastic materials in nonlinear steps. Explicit
dynamics refuses hyperelastic materials by name; solve.run names the solver
still to come.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm
This commit is contained in:
jyvikoandClaude Opus 5.5 authored and Irakli Kourtis committed 2026-10-14 04:00:21 -04:00
1 parent d2fe8a8303
commit bc9fe2191a
13 files changed
+408 -19

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+2 -1
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@@ -322,6 +322,7 @@ impl Model {
Procedure::ExplicitDynamic(_) => "is dynamic",
Procedure::HeatTransfer { transient: Some(_) } => "is transient heat transfer",
Procedure::Static {}
| Procedure::NonlinearStatic(_)
| Procedure::Fluid { .. }
| Procedure::HeatTransfer { transient: None }
| Procedure::CoupledTemperatureDisplacement {} => {
@@ -469,7 +470,7 @@ impl Model {
}
}
match &s.procedure {
Procedure::Static {} => {
Procedure::Static {} | Procedure::NonlinearStatic(_) => {
if s.loads.is_empty() && !prescribes_motion {
d.warning(&subject, "nothing loads the model in this step");
}
+3 -2
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@@ -57,12 +57,13 @@ pub use discrete::{Direction, Mass, PointMass, ResolvedDirection, ResolvedMass,
pub use fluids::{BoxFace, BoxFaces, FaceCondition, FluidBoundary, FluidDomain, Profile, SurfaceBoundary, SurfaceCondition};
pub use geometry::{Classification, Entity, GeometryRef};
pub use loads::{Distribution, Load, centrifugal_acceleration};
pub use materials::{Damage, Directional, Elastic, Erosion, Fluid, Hardening, HardeningPoint, Material, Plastic, Thermal};
pub use materials::{Damage, Directional, Elastic, Erosion, Fluid, Hardening, HardeningPoint, Hyperelastic, Material, Plastic, Thermal};
pub use mesh::{Element, ElementEdge, ElementFace, ElementKind, Node, check_coordinates};
pub use sections::{BeamProfile, Extent, Formulation, Integration, Section, SectionKind};
pub use sets::Set;
pub use steps::{
BulkViscosity, ExplicitDynamic, Hourglass, HourglassKind, InitialVelocity, OutputVariable, Procedure, RigidWall, Step, StressRate, Transient,
BulkViscosity, ExplicitDynamic, Hourglass, HourglassKind, InitialVelocity, MAX_NONLINEAR_INCREMENTS, MAX_NONLINEAR_ITERATIONS, NonlinearStatic,
OutputVariable, Procedure, RigidWall, Step, StressRate, Tolerances, Transient,
};
pub use units::UnitSystem;
+66
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@@ -74,6 +74,37 @@ impl Elastic {
}
}
/// Hyperelastic behaviour of an isotropic material at large strain, in nonlinear steps.
///
/// The constants are the material's isotropic elastic ones: the shear modulus μ = E / (2(1 + ν))
/// and the bulk modulus κ = E / (3(1 − 2ν)), so at small strain the material is that linear
/// elastic one (linear steps use it so). Without this option an elastic material in a nonlinear
/// step is St Venant–Kirchhoff (the second Piola–Kirchhoff stress linear in the Green–Lagrange
/// strain), which is right for large rotations with small strains.
#[derive(Debug, Clone, Copy, PartialEq, Serialize, Deserialize)]
#[serde(tag = "type", rename_all = "snake_case", deny_unknown_fields)]
pub enum Hyperelastic {
/// Compressible neo-Hookean with the isochoric–volumetric split: the strain energy per
/// reference volume W = μ/2 (Ī₁ − 3) + κ/2 (J − 1)², with Ī₁ = J^(−2/3) tr C (C₁₀ = μ/2,
/// D₁ = 2/κ in the usual polynomial notation).
NeoHookean {},
}
impl Hyperelastic {
/// The shear and bulk moduli μ = E / (2(1 + ν)) and κ = E / (3(1 − 2ν)) the model takes from
/// the isotropic constants.
pub fn moduli(young: f64, poisson: f64) -> (f64, f64) {
(young / (2.0 * (1.0 + poisson)), young / (3.0 * (1.0 - 2.0 * poisson)))
}
/// The name of the model, for messages.
pub fn name(&self) -> &'static str {
match self {
Hyperelastic::NeoHookean {} => "neo-Hookean",
}
}
}
/// Fluid behaviour.
#[derive(Debug, Clone, Copy, PartialEq, Serialize, Deserialize)]
#[serde(tag = "type", rename_all = "snake_case", deny_unknown_fields)]
@@ -332,6 +363,9 @@ pub struct Erosion {
pub struct Material {
#[serde(default, skip_serializing_if = "Option::is_none")]
pub elastic: Option<Elastic>,
/// Large-strain behaviour in nonlinear steps, built on the isotropic elastic constants.
#[serde(default, skip_serializing_if = "Option::is_none")]
pub hyperelastic: Option<Hyperelastic>,
/// Mass per volume, needed by frequency steps, gravity and transient heat transfer.
#[serde(default, skip_serializing_if = "Option::is_none")]
pub density: Option<f64>,
@@ -366,6 +400,14 @@ impl Material {
if let Some(e) = &self.elastic {
e.validate()?;
}
if let Some(h) = &self.hyperelastic {
if !matches!(self.elastic, Some(Elastic::Isotropic { .. })) {
return Err(Error::Invalid(format!("{} hyperelasticity needs isotropic elastic constants", h.name())));
}
if self.plastic.is_some() {
return Err(Error::Invalid(format!("plasticity of a {} hyperelastic material is not supported yet", h.name())));
}
}
if let Some(d) = self.density {
positive("density", d)?;
}
@@ -412,6 +454,11 @@ impl Model {
self.materials.get(name)
}
/// The hyperelastic materials some section uses, by name.
pub fn hyperelastic_in_use(&self) -> std::collections::BTreeSet<&str> {
self.sections.values().map(|s| s.material.as_str()).filter(|m| self.material(m).is_some_and(|m| m.hyperelastic.is_some())).collect()
}
pub fn add_material(&mut self, name: &str, material: Material) -> Result<()> {
material.validate().map_err(|e| context("material", name, e))?;
insert_new(&mut self.materials, "material", name, material)
@@ -544,6 +591,25 @@ mod tests {
assert_eq!(serde_json::from_str::<Material>(&text).unwrap(), Material { plastic: Some(jc()), damage: Some(damage), ..steel() });
}
#[test]
fn hyperelasticity_builds_on_isotropic_constants() {
let m: Material = serde_json::from_value(serde_json::json!({
"elastic": {"type": "isotropic", "young": 3.0, "poisson": 0.49}, "hyperelastic": {"type": "neo_hookean"}
}))
.unwrap();
m.validate().unwrap();
assert_eq!(m.hyperelastic, Some(Hyperelastic::NeoHookean {}));
let back: Material = serde_json::from_value(serde_json::to_value(&m).unwrap()).unwrap();
assert_eq!(back, m);
assert!(serde_json::from_value::<Material>(serde_json::json!({"hyperelastic": {"type": "neo_hookean", "c10": 1}})).is_err());
let alone = Material { hyperelastic: Some(Hyperelastic::NeoHookean {}), density: Some(1.0), ..Material::default() };
assert!(alone.validate().is_err(), "needs isotropic constants");
let ortho = Elastic::EngineeringConstants { young: [1.0; 3], poisson: [0.0; 3], shear: [1.0; 3] };
assert!(Material { elastic: Some(ortho), ..alone }.validate().is_err());
let plastic = Plastic::Bilinear { yield_stress: 1.0, hardening_modulus: 0.0, hardening: Hardening::Isotropic };
assert!(Material { plastic: Some(plastic), ..m }.validate().is_err());
}
#[test]
fn thermal_properties() {
let m: Material = serde_json::from_value(serde_json::json!({
+151 -2
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@@ -86,6 +86,114 @@ pub enum Procedure {
/// Steady heat conduction and the static equilibrium of the thermal strains it causes,
/// together: every boundary condition and load of the step acts.
CoupledTemperatureDisplacement {},
/// Static equilibrium followed in load increments with Newton–Raphson iterations: large
/// displacements, rotations and strains (`nonlinear_geometry`), hyperelastic materials and
/// follower pressure. Loads and prescribed displacements grow in proportion to the step's
/// load factor, from 0 to 1.
NonlinearStatic(NonlinearStatic),
}
/// Most load increments a nonlinear static step may take.
pub const MAX_NONLINEAR_INCREMENTS: u32 = 100_000;
/// Most Newton iterations a nonlinear static step may take in one increment.
pub const MAX_NONLINEAR_ITERATIONS: u32 = 1000;
/// The settings of a nonlinear static step.
///
/// The step's load factor λ runs from 0 to 1: every load is λ times its value and every
/// prescribed displacement λ times its value (a linear ramp). Increments are fractions of the
/// step: the first is `initial_increment`; an increment that converges quickly lets the next
/// grow (up to `max_increment`), one that diverges, fails to converge in `max_iterations` or
/// inverts an element is retried with a quarter of its size, and the step fails, naming the
/// load factor and the reason, when an increment would fall below `min_increment` or the step
/// has taken `max_increments` increments.
#[derive(Debug, Clone, PartialEq, Serialize, Deserialize)]
#[serde(default, deny_unknown_fields)]
pub struct NonlinearStatic {
/// Large displacements, rotations and strains (total Lagrangian elements, follower
/// pressure); `false` keeps the kinematics of small displacements (only the materials are
/// nonlinear).
pub nonlinear_geometry: bool,
/// The first increment, as a fraction of the step.
pub initial_increment: f64,
/// The smallest increment a cutback may reach.
pub min_increment: f64,
/// The largest increment.
pub max_increment: f64,
/// Cap on the increments (cutbacks included).
pub max_increments: u32,
/// Cap on the Newton iterations of one increment.
pub max_iterations: u32,
/// Convergence tolerances.
pub tolerances: Tolerances,
/// A line search along each Newton correction (off by default: full Newton steps converge
/// best for elastic large-rotation problems; a search helps where the material softens).
pub line_search: bool,
}
/// When an increment's Newton iterations have converged: all three hold.
#[derive(Debug, Clone, Copy, PartialEq, Serialize, Deserialize)]
#[serde(default, deny_unknown_fields)]
pub struct Tolerances {
/// The largest residual force component over the largest force (applied, internal or
/// reaction) the step has seen.
pub force: f64,
/// The largest displacement correction over the largest displacement of the increment.
pub displacement: f64,
/// The work of the last correction against the residual over that of the first.
pub energy: f64,
}
impl Default for Tolerances {
fn default() -> Tolerances {
Tolerances { force: 1e-6, displacement: 1e-5, energy: 1e-10 }
}
}
impl Default for NonlinearStatic {
fn default() -> NonlinearStatic {
NonlinearStatic {
nonlinear_geometry: true,
initial_increment: 0.1,
min_increment: 1e-5,
max_increment: 1.0,
max_increments: 100,
max_iterations: 16,
tolerances: Tolerances::default(),
line_search: false,
}
}
}
impl NonlinearStatic {
pub fn validate(&self) -> Result<()> {
let fraction = |what: &str, v: f64| {
if v > 0.0 && v <= 1.0 { Ok(v) } else { Err(Error::Invalid(format!("the {what} is a fraction of the step in (0, 1], got {v}"))) }
};
let initial = fraction("initial increment", self.initial_increment)?;
let min = fraction("minimum increment", self.min_increment)?;
let max = fraction("maximum increment", self.max_increment)?;
if !(min <= initial && initial <= max) {
return Err(Error::Invalid(format!("the increments must satisfy minimum ≤ initial ≤ maximum, got {min}, {initial} and {max}")));
}
if !(1..=MAX_NONLINEAR_INCREMENTS).contains(&self.max_increments) {
return Err(Error::Invalid(format!("a nonlinear step takes 1 to {MAX_NONLINEAR_INCREMENTS} increments, got {}", self.max_increments)));
}
if !(1..=MAX_NONLINEAR_ITERATIONS).contains(&self.max_iterations) {
return Err(Error::Invalid(format!(
"a nonlinear step takes 1 to {MAX_NONLINEAR_ITERATIONS} iterations per increment, got {}",
self.max_iterations
)));
}
let t = self.tolerances;
for (what, v) in [("force", t.force), ("displacement", t.displacement), ("energy", t.energy)] {
if !(v > 0.0 && v < 1.0) {
return Err(Error::Invalid(format!("the {what} tolerance is in (0, 1), got {v}")));
}
}
Ok(())
}
}
/// Most time increments of a transient heat transfer step.
@@ -386,7 +494,7 @@ impl BulkViscosity {
}
impl Procedure {
/// `static` or `frequency`.
/// The procedure's type, as the model file names it.
pub fn name(&self) -> &'static str {
match self {
Procedure::Static {} => "static",
@@ -395,6 +503,7 @@ impl Procedure {
Procedure::HeatTransfer { .. } => "heat_transfer",
Procedure::CoupledTemperatureDisplacement {} => "coupled_temperature_displacement",
Procedure::Fluid { .. } => "fluid",
Procedure::NonlinearStatic(_) => "nonlinear_static",
}
}
@@ -435,6 +544,9 @@ impl Procedure {
if let Procedure::ExplicitDynamic(e) = self {
return e.validate();
}
if let Procedure::NonlinearStatic(n) = self {
return n.validate();
}
if let Procedure::Fluid { end_time, steps, time_step, frames, magic, .. } = *self {
match (end_time, steps) {
(Some(t), None) => {
@@ -480,7 +592,7 @@ impl Procedure {
/// The output a step of this procedure requests unless told otherwise.
pub fn default_output(&self) -> BTreeSet<OutputVariable> {
match self {
Procedure::Static {} => OutputVariable::ALL.into_iter().collect(),
Procedure::Static {} | Procedure::NonlinearStatic(_) => OutputVariable::ALL.into_iter().collect(),
Procedure::Frequency { .. } => [OutputVariable::Displacement].into_iter().collect(),
Procedure::ExplicitDynamic(_) => [OutputVariable::Displacement, OutputVariable::Stress].into_iter().collect(),
// Velocity, pressure and wall forces, always.
@@ -753,6 +865,43 @@ mod tests {
assert!(serde_json::from_value::<Procedure>(serde_json::json!({"type": "explicit_dynamic", "end_time": 1, "dt": 2})).is_err());
}
#[test]
fn nonlinear_static_steps_validate_their_controls() {
let p: Procedure = serde_json::from_value(serde_json::json!({"type": "nonlinear_static"})).unwrap();
assert_eq!(p, Procedure::NonlinearStatic(NonlinearStatic::default()));
assert_eq!(p.name(), "nonlinear_static");
assert!(p.validate().is_ok() && p.is_structural() && !p.is_dynamic());
assert_eq!(p.default_output(), Procedure::Static {}.default_output());
let p: Procedure = serde_json::from_value(serde_json::json!({
"type": "nonlinear_static", "nonlinear_geometry": false, "initial_increment": 0.5, "min_increment": 0.01,
"max_increments": 20, "max_iterations": 8, "tolerances": {"force": 1e-4}, "line_search": true
}))
.unwrap();
let Procedure::NonlinearStatic(n) = &p else { panic!("{p:?}") };
assert_eq!((n.nonlinear_geometry, n.max_increment, n.tolerances.force, n.tolerances.energy), (false, 1.0, 1e-4, 1e-10));
let back: Procedure = serde_json::from_value(serde_json::to_value(&p).unwrap()).unwrap();
assert_eq!(back, p);
let base = NonlinearStatic::default();
let bad = [
NonlinearStatic { initial_increment: 0.0, ..base.clone() },
NonlinearStatic { initial_increment: f64::NAN, ..base.clone() },
NonlinearStatic { initial_increment: 2.0, max_increment: 2.0, ..base.clone() },
NonlinearStatic { min_increment: 0.5, initial_increment: 0.1, ..base.clone() },
NonlinearStatic { max_increment: 0.05, ..base.clone() },
NonlinearStatic { max_increments: 0, ..base.clone() },
NonlinearStatic { max_increments: MAX_NONLINEAR_INCREMENTS + 1, ..base.clone() },
NonlinearStatic { max_iterations: 0, ..base.clone() },
NonlinearStatic { max_iterations: u32::MAX, ..base.clone() },
NonlinearStatic { tolerances: Tolerances { force: 0.0, ..Tolerances::default() }, ..base.clone() },
NonlinearStatic { tolerances: Tolerances { energy: f64::INFINITY, ..Tolerances::default() }, ..base.clone() },
NonlinearStatic { tolerances: Tolerances { displacement: 1.0, ..Tolerances::default() }, ..base.clone() },
];
for b in bad {
assert!(Procedure::NonlinearStatic(b.clone()).validate().is_err(), "{b:?}");
}
assert!(serde_json::from_value::<Procedure>(serde_json::json!({"type": "nonlinear_static", "nlgeom": true})).is_err());
}
#[test]
fn heat_transfer_procedures() {
let steady: Procedure = serde_json::from_value(serde_json::json!({"type": "heat_transfer"})).unwrap();