forked from 1b-agent/fieldcraft-upstream
* Heat transfer and thermal stress: thermal materials, temperature BCs, heat loads, heat transfer and coupled temperature–displacement steps, solve.heat
Model: Material.thermal (conductivity, specific heat, expansion, isotropic or
per axis; reference temperature), BoundaryCondition::Temperature (dof 11),
loads SurfaceFlux, Convection, HeatSource and Temperature (a field in static
steps), procedures HeatTransfer { transient (θ-method) } and
CoupledTemperatureDisplacement; checks for missing conductivity/specific
heat/expansion. fem: heat conduction kernels (conductivity, capacity,
source, face flux/film, heat flux) on the DofLayout (one T per node), thermal
strain load and stress D(ε − ε_th) for every solid formulation incl.
incompatible modes. Solver: steady and transient heat transfer, thermal loads
in static steps, coupled steps (exact one-way coupling). Engine: solve.heat,
temperature/heat-flux result fields, probes. Decks refuse heat transfer by
name. Analytic verification: slab, source+convection/flux, thick cylinder,
erfc semi-infinite solid, free/constrained expansion, bimetal strip, coupled
step.
Co-Authored-By: Claude Opus 5.5 <[email protected]>
Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm
* thermal: strains in 2D elements and explicit dynamics
Plane::thermal_load and stresses_with for plane stress (εzz free), plane
strain (σzz = −D₃·ε_th) and axisymmetric elements, incompatible modes
included; the solver's 2D kernels take them. Explicit dynamics turns a
step's temperature loads into a per-element thermal strain rate (reached
linearly over the step) subtracted from each strain increment, so it feeds
J2 and Johnson–Cook updates. Verified: free expansion in every 2D theory
and element, a biaxially held plate, an explicit free bar (ΔL = αΔT L,
stress-free) and a clamped bar at −EαΔT, capped at the yield stress with
perfect plasticity.
Co-Authored-By: Claude Opus 5.5 <[email protected]>
Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm
* clippy
Co-Authored-By: Claude Opus 5.5 <[email protected]>
Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm
* thermal: trusses take the axial thermal strain; keep the roadmap's M7 line
Truss::thermal_load and stresses_with project the thermal strain on the
member's tangent (Σ αₖ tₖ² ΔT); the static solver applies them to rod2/rod3
(#38). Explicit trusses take none yet and a warning says so.
Co-Authored-By: Claude Opus 5.5 <[email protected]>
Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm
---------
Co-authored-by: jyviko <[email protected]>
Co-authored-by: Claude Opus 5.5 <[email protected]>
141 lines
6.4 KiB
Rust
141 lines
6.4 KiB
Rust
//! Thermal strain in explicit dynamics: a temperature load reached slowly over the step expands
|
||
//! a free bar by α ΔT L without stress; a bar held at both ends carries σ = −E α ΔT, and with
|
||
//! perfectly plastic J2 the stress stops at the yield stress.
|
||
|
||
use modelcraft_explicit::{Limits, solve_explicit};
|
||
use modelcraft_model::*;
|
||
|
||
const YOUNG: f64 = 1.0e4;
|
||
const ALPHA: f64 = 1.0e-4;
|
||
const DT: f64 = 20.0;
|
||
const LENGTH: f64 = 4.0;
|
||
|
||
/// A 4 × 1 × 1 bar of hex8 (one-point) or Kuhn-split tet4 cells, ν = 0, heated by DT over a
|
||
/// step much longer than the wave transit, held at x = 0 (and at x = L when `clamped`) along x
|
||
/// and on the planes y = 0, z = 0.
|
||
fn bar(kind: ElementKind, clamped: bool, plastic: Option<Plastic>) -> Model {
|
||
let mut m = Model::default();
|
||
let n = 4usize;
|
||
let label = |i: usize, j: usize, k: usize| (1 + i + (n + 1) * (j + 2 * k)) as u32;
|
||
for k in 0..2 {
|
||
for j in 0..2 {
|
||
for i in 0..=n {
|
||
m.set_node(label(i, j, k), [i as f64, j as f64, k as f64]).unwrap();
|
||
}
|
||
}
|
||
}
|
||
let corners = [[0, 0, 0], [1, 0, 0], [1, 1, 0], [0, 1, 0], [0, 0, 1], [1, 0, 1], [1, 1, 1], [0, 1, 1]];
|
||
let mut next = 1;
|
||
for i in 0..n {
|
||
let at = |c: [usize; 3]| label(i + c[0], c[1], c[2]);
|
||
if kind == ElementKind::Hex8 {
|
||
m.set_element(next, kind, corners.iter().map(|c| at(*c)).collect()).unwrap();
|
||
next += 1;
|
||
continue;
|
||
}
|
||
for perm in [[0, 1, 2], [0, 2, 1], [1, 0, 2], [1, 2, 0], [2, 0, 1], [2, 1, 0]] {
|
||
let mut v = [[0usize; 3]; 4];
|
||
for s in 0..3 {
|
||
v[s + 1] = v[s];
|
||
v[s + 1][perm[s]] = 1;
|
||
}
|
||
let x = v.map(|c| c.map(|k| k as f64));
|
||
let e = |a: usize| [0, 1, 2].map(|k| x[a][k] - x[0][k]);
|
||
let (a, b, c) = (e(1), e(2), e(3));
|
||
let vol = a[0] * (b[1] * c[2] - b[2] * c[1]) - a[1] * (b[0] * c[2] - b[2] * c[0]) + a[2] * (b[0] * c[1] - b[1] * c[0]);
|
||
if vol < 0.0 {
|
||
v.swap(1, 2);
|
||
}
|
||
m.set_element(next, kind, v.iter().map(|c| at(*c)).collect()).unwrap();
|
||
next += 1;
|
||
}
|
||
}
|
||
let all: Vec<u32> = m.elements().keys().copied().collect();
|
||
let nodes: Vec<u32> = m.nodes().keys().copied().collect();
|
||
let pick = |f: &dyn Fn([f64; 3]) -> bool| -> Vec<u32> { nodes.iter().copied().filter(|l| f(m.node(*l).unwrap().xyz)).collect() };
|
||
let (x0, x1, y0, z0) = (pick(&|p| p[0] == 0.0), pick(&|p| p[0] == LENGTH), pick(&|p| p[1] == 0.0), pick(&|p| p[2] == 0.0));
|
||
m.add_set("all", Set { elements: all, nodes: nodes.clone(), ..Set::default() }).unwrap();
|
||
for (name, set) in [("x0", x0), ("x1", x1), ("y0", y0), ("z0", z0)] {
|
||
m.add_set(name, Set { nodes: set, ..Set::default() }).unwrap();
|
||
}
|
||
let thermal = Thermal { expansion: Some(Directional::Isotropic(ALPHA)), ..Thermal::default() };
|
||
m.add_material(
|
||
"Mat",
|
||
Material {
|
||
elastic: Some(Elastic::Isotropic { young: YOUNG, poisson: 0.0 }),
|
||
density: Some(1.0),
|
||
thermal: Some(thermal),
|
||
plastic,
|
||
..Material::default()
|
||
},
|
||
)
|
||
.unwrap();
|
||
let integration = if kind == ElementKind::Hex8 { Integration::Reduced } else { Integration::Full };
|
||
let formulation = Formulation { integration, ..Formulation::default() };
|
||
m.add_section("bar", Section { set: "all".into(), material: "Mat".into(), kind: SectionKind::Solid {}, formulation }).unwrap();
|
||
let mut step = Step::new("Heat", Procedure::ExplicitDynamic(ExplicitDynamic::new(20.0)));
|
||
let mut bcs = vec![("x0", Symmetry::X), ("y0", Symmetry::Y), ("z0", Symmetry::Z)];
|
||
if clamped {
|
||
bcs.push(("x1", Symmetry::X));
|
||
}
|
||
for (set, plane) in bcs {
|
||
let name = format!("hold_{set}");
|
||
m.add_boundary_condition(&name, BoundaryCondition::Symmetry { target: Target::Set(set.into()), plane }).unwrap();
|
||
step.boundary_conditions.insert(name);
|
||
}
|
||
m.add_load("warm", Load::Temperature { target: Target::Set("all".into()), value: DT }).unwrap();
|
||
step.loads.insert("warm".into());
|
||
m.add_step(step, None).unwrap();
|
||
m
|
||
}
|
||
|
||
#[test]
|
||
fn a_free_bar_expands_without_stress() {
|
||
for kind in [ElementKind::Hex8, ElementKind::Tet4] {
|
||
let r = solve_explicit(&bar(kind, false, None), None, &Limits::default()).unwrap();
|
||
let last = r.frames.last().unwrap();
|
||
let tip = r.nodes.iter().position(|l| *l == 5).unwrap();
|
||
let want = ALPHA * DT * LENGTH;
|
||
assert!((last.displacement[tip][0] - want).abs() < 0.02 * want, "{kind:?}: {:?} vs {want}", last.displacement[tip]);
|
||
let worst = last.stress.iter().flatten().fold(0.0f64, |m, s| m.max(s.abs()));
|
||
assert!(worst < 0.02 * YOUNG * ALPHA * DT, "{kind:?}: {worst}");
|
||
}
|
||
}
|
||
|
||
#[test]
|
||
fn a_clamped_bar_carries_minus_e_alpha_dt_up_to_yield() {
|
||
let sigma = -YOUNG * ALPHA * DT;
|
||
for kind in [ElementKind::Hex8, ElementKind::Tet4] {
|
||
let r = solve_explicit(&bar(kind, true, None), None, &Limits::default()).unwrap();
|
||
for s in &r.frames.last().unwrap().stress {
|
||
assert!((s[0] - sigma).abs() < 0.02 * sigma.abs(), "{kind:?}: {s:?}");
|
||
}
|
||
// Perfectly plastic at half that stress: the bar yields and the stress stays at −σ_y.
|
||
let plastic = Plastic::Bilinear { yield_stress: 0.5 * sigma.abs(), hardening_modulus: 0.0, hardening: Hardening::Isotropic };
|
||
let r = solve_explicit(&bar(kind, true, Some(plastic)), None, &Limits::default()).unwrap();
|
||
let last = r.frames.last().unwrap();
|
||
for (s, ep) in last.stress.iter().zip(&last.plastic_strain) {
|
||
let mises = modelcraft_fem::von_mises(s);
|
||
assert!((mises - 0.5 * sigma.abs()).abs() < 0.02 * sigma.abs(), "{kind:?}: {s:?}");
|
||
assert!(*ep > 0.0, "{kind:?}: plastic strain {ep}");
|
||
}
|
||
}
|
||
}
|
||
|
||
#[test]
|
||
fn orthotropic_expansion_and_heat_loads_are_refused() {
|
||
let mut m = bar(ElementKind::Hex8, false, None);
|
||
let thermal = Thermal { expansion: Some(Directional::Orthotropic([1e-5, 2e-5, 1e-5])), ..Thermal::default() };
|
||
m.replace_material(
|
||
"Mat",
|
||
Material {
|
||
elastic: Some(Elastic::Isotropic { young: YOUNG, poisson: 0.0 }),
|
||
density: Some(1.0),
|
||
thermal: Some(thermal),
|
||
..Material::default()
|
||
},
|
||
)
|
||
.unwrap();
|
||
assert!(solve_explicit(&m, None, &Limits::default()).unwrap_err().to_string().contains("orthotropic thermal expansion"));
|
||
}
|