forked from 1b-agent/fieldcraft-upstream
* ui.capture: the whole window drawn offscreen and rasterised on the CPU ui.screenshot falls back to it when no frame is presented (hidden window, locked screen), so agents can look at panels and the toolbar. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm * Draw the open design and imported surfaces in the viewport DisplayMesh keeps node labels on every element primitive (for results), gains add_surface (geometry faces and their boundaries, coincident points welded) and displaced (elements moved by nodal offsets). Bodies are tessellated at a thousandth of their size; meshed models show the geometry as boundaries only. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm * results.* commands: deformed shape, contours, mode shapes, animation, reaction sums The results display is session state (ResultsView), set by commands that are not edits. Nodal fields (displacement, von Mises, principal and component stresses; principal stresses in closed form after Smith 1961) and reaction force and moment sums per set. Results kept from an earlier revision stay viewable, marked stale; solve.probe says when a result is stale. The Results tab's display and reaction entries are ready. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm * Results display: deformed shape, contours with legend, mode shapes and animation, probe, reaction sums The viewport draws the session's results view: elements moved by their nodes' displacements or a mode shape (automatic or given scale), faces split exactly along contour band boundaries into flat-coloured pieces (same on GPU and CPU), a legend with levels and extremes, a results panel whose controls run the results.* commands, a click probing the nearest node (solve.probe), and stale results marked. Solving from the form shows the result on the Results tab. sample::cantilever is a solvable model for tests and demos. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm * Simplify the results display (review) One Contour in the plot; the results scene reuses scene::build; a solve shows its result through the engine (ResultsView::for_result) and the UI raises the Results tab when a view appears; the plot's scale and contour values are kept across animation frames; design bodies are tessellated once per design; the first content is framed where the display is rebuilt; field_values in one match; probe reuses results::displacements. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm * Results display for explicit steps: field frames, energy histories The results view works on the engine's step results (static, frequency, explicit): ResultsView.frame and results.frame {frame | time} pick an explicit field frame; the deformed shape (true scale) and contours (element stresses averaged to the nodes, velocity) follow it; animation runs through the frames. The Results panel has a frame slider and plots the kinetic, internal, hourglass and external energies with their values at the frame. sample::impact is a steel bar flying onto a rigid wall. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm * docs/features.md after the rebase Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm --------- Co-authored-by: jyviko <2501648+jyviko@users.noreply.github.com> Co-authored-by: Claude Opus 5.5 <noreply@anthropic.com>
162 lines
6.9 KiB
Rust
162 lines
6.9 KiB
Rust
//! Linear elastic constitutive matrices.
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//!
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//! Stress and strain are 6-vectors in the order xx, yy, zz, xy, xz, yz, with engineering shear
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//! strains (γ = 2ε), so σ = D ε. The order puts the orthotropic shear moduli G₁₂, G₁₃, G₂₃ on
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//! the diagonal in the order the model lists them. Material axes are the global axes until the
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//! model has material orientations.
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//!
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//! Orthotropic stiffness is the inverse of the compliance written with engineering constants
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//! (R. M. Jones, *Mechanics of Composite Materials*, 2nd ed., Taylor & Francis 1999, §2.4):
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//! S₁₁ = 1/E₁, S₁₂ = −ν₁₂/E₁, S₁₃ = −ν₁₃/E₁, S₂₃ = −ν₂₃/E₂ (ν_ji/E_j = ν_ij/E_i), and
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//! 1/G on the shear diagonal.
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use modelcraft_model::Elastic;
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use crate::dense::inverse3;
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use crate::{Error, Result};
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/// A 6 × 6 elasticity matrix, row-major.
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pub type Elasticity = [[f64; 6]; 6];
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/// The isotropic elasticity matrix.
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pub fn isotropic(young: f64, poisson: f64) -> Result<Elasticity> {
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if !(young > 0.0 && young.is_finite() && poisson > -1.0 && poisson < 0.5) {
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return Err(Error::Invalid(format!("isotropic constants E = {young}, ν = {poisson} are not a stable material")));
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}
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let lambda = young * poisson / ((1.0 + poisson) * (1.0 - 2.0 * poisson));
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let mu = young / (2.0 * (1.0 + poisson));
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let mut d = [[0.0; 6]; 6];
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for i in 0..3 {
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for j in 0..3 {
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d[i][j] = lambda;
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}
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d[i][i] = lambda + 2.0 * mu;
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d[i + 3][i + 3] = mu;
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}
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Ok(d)
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}
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/// The orthotropic elasticity matrix from engineering constants.
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pub fn orthotropic(young: [f64; 3], poisson: [f64; 3], shear: [f64; 3]) -> Result<Elasticity> {
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let [e1, e2, e3] = young;
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let [n12, n13, n23] = poisson;
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let s = [[1.0 / e1, -n12 / e1, -n13 / e1], [-n12 / e1, 1.0 / e2, -n23 / e2], [-n13 / e1, -n23 / e2, 1.0 / e3]];
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let scale = (1.0 / e1) * (1.0 / e2) * (1.0 / e3);
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let inverse = inverse3(&s).filter(|(_, det)| *det > 1e-12 * scale);
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let Some((normal, _)) = inverse.filter(|_| shear.iter().all(|g| *g > 0.0 && g.is_finite())) else {
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return Err(Error::Invalid("the orthotropic constants do not describe a stable material".into()));
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};
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let mut d = [[0.0; 6]; 6];
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for i in 0..3 {
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d[i][..3].copy_from_slice(&normal[i]);
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}
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for (k, g) in shear.iter().enumerate() {
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d[3 + k][3 + k] = *g;
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}
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Ok(d)
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}
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/// The elasticity matrix of a model material's elastic behaviour.
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pub fn elasticity(e: &Elastic) -> Result<Elasticity> {
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match *e {
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Elastic::Isotropic { young, poisson } => isotropic(young, poisson),
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Elastic::EngineeringConstants { young, poisson, shear } => orthotropic(young, poisson, shear),
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}
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}
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/// The von Mises equivalent stress of a stress 6-vector.
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pub fn von_mises(s: &[f64; 6]) -> f64 {
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let [xx, yy, zz, xy, xz, yz] = *s;
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let normal = (xx - yy) * (xx - yy) + (yy - zz) * (yy - zz) + (zz - xx) * (zz - xx);
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(0.5 * normal + 3.0 * (xy * xy + xz * xz + yz * yz)).sqrt()
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}
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/// The principal stresses of a stress 6-vector, largest first: the eigenvalues of the symmetric
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/// stress tensor in closed form (O. K. Smith, "Eigenvalues of a symmetric 3 × 3 matrix",
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/// Commun. ACM 4(4):168, 1961).
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pub fn principal(s: &[f64; 6]) -> [f64; 3] {
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let [xx, yy, zz, xy, xz, yz] = *s;
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let off = xy * xy + xz * xz + yz * yz;
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let q = (xx + yy + zz) / 3.0;
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let (a, b, c) = (xx - q, yy - q, zz - q);
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let p = ((a * a + b * b + c * c + 2.0 * off) / 6.0).sqrt();
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if !(p > 0.0) || off == 0.0 {
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let mut d = [xx, yy, zz];
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d.sort_by(|u, v| v.total_cmp(u));
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return d;
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}
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// det(A − qI) / (2 p³), the cosine of three times the angle, within [−1, 1].
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let det = a * (b * c - yz * yz) - xy * (xy * c - yz * xz) + xz * (xy * yz - b * xz);
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let r = (det / (2.0 * p * p * p)).clamp(-1.0, 1.0);
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let phi = r.acos() / 3.0;
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let first = q + 2.0 * p * phi.cos();
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let third = q + 2.0 * p * (phi + 2.0 * std::f64::consts::FRAC_PI_3).cos();
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[first, 3.0 * q - first - third, third]
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}
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/// σ = D ε.
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pub fn stress(d: &Elasticity, strain: &[f64; 6]) -> [f64; 6] {
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let mut s = [0.0; 6];
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for (si, row) in s.iter_mut().zip(d) {
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*si = row.iter().zip(strain).map(|(a, b)| a * b).sum();
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}
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s
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}
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#[cfg(test)]
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mod tests {
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use super::*;
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#[test]
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fn orthotropic_with_isotropic_constants_is_isotropic() {
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let (e, nu) = (210e3, 0.3);
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let g = e / (2.0 * (1.0 + nu));
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let a = isotropic(e, nu).unwrap();
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let b = orthotropic([e; 3], [nu; 3], [g; 3]).unwrap();
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for i in 0..6 {
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for j in 0..6 {
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assert!((a[i][j] - b[i][j]).abs() < 1e-9 * e, "{i} {j}: {} vs {}", a[i][j], b[i][j]);
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}
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}
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assert!(isotropic(1.0, 0.5).is_err());
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assert!(orthotropic([1.0; 3], [0.9; 3], [1.0; 3]).is_err());
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}
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#[test]
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fn principal_stresses_are_the_tensor_eigenvalues() {
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let close = |a: [f64; 3], b: [f64; 3]| a.iter().zip(b).all(|(x, y)| (x - y).abs() < 1e-9 * (1.0 + y.abs()));
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// Diagonal: sorted, largest first.
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assert_eq!(principal(&[1.0, 3.0, -2.0, 0.0, 0.0, 0.0]), [3.0, 1.0, -2.0]);
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// Pure shear τ in the xy plane: ±τ and 0.
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assert!(close(principal(&[0.0, 0.0, 0.0, 5.0, 0.0, 0.0]), [5.0, 0.0, -5.0]));
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// Hydrostatic: three equal.
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assert!(close(principal(&[-7.0, -7.0, -7.0, 0.0, 0.0, 0.0]), [-7.0; 3]));
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// A general tensor: the sum is the trace, and each is a root of det(σ − λI) = 0.
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let s = [10.0, -4.0, 3.0, 2.0, -1.5, 6.0];
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let l = principal(&s);
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assert!(l[0] >= l[1] && l[1] >= l[2]);
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assert!((l.iter().sum::<f64>() - (s[0] + s[1] + s[2])).abs() < 1e-9);
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for x in l {
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let (a, b, c) = (s[0] - x, s[1] - x, s[2] - x);
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let det = a * (b * c - s[5] * s[5]) - s[3] * (s[3] * c - s[5] * s[4]) + s[4] * (s[3] * s[5] - b * s[4]);
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assert!(det.abs() < 1e-7, "{x}: {det}");
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}
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// Von Mises from the principal values agrees.
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let vm = (0.5 * ((l[0] - l[1]).powi(2) + (l[1] - l[2]).powi(2) + (l[2] - l[0]).powi(2))).sqrt();
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assert!((vm - von_mises(&s)).abs() < 1e-9);
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assert!(principal(&[f64::NAN; 6]).iter().all(|v| v.is_nan()));
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}
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#[test]
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fn orthotropic_uniaxial_response() {
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// Stress along 1 alone gives strains σ/E1, −ν12 σ/E1, −ν13 σ/E1.
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let (young, poisson) = ([140e3, 10e3, 12e3], [0.3, 0.25, 0.4]);
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let d = orthotropic(young, poisson, [5e3, 4e3, 3.8e3]).unwrap();
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let strain = [1.0 / young[0], -poisson[0] / young[0], -poisson[1] / young[0], 0.0, 0.0, 0.0];
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let s = stress(&d, &strain);
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assert!((s[0] - 1.0).abs() < 1e-12 && s[1].abs() < 1e-12 && s[2].abs() < 1e-12, "{s:?}");
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assert!((von_mises(&[1.0, 0.0, 0.0, 0.0, 0.0, 0.0]) - 1.0).abs() < 1e-15);
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assert!((von_mises(&[0.0, 0.0, 0.0, 1.0, 0.0, 0.0]) - 3f64.sqrt()).abs() < 1e-15);
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}
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}
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