Thermal assessment invariant correction¶
The older creep_hot_wall_assessment.py demo used a two-dimensional deviator
with trace divided by two for a plane-strain von Mises assessment. That is
not the three-dimensional J2 invariant: the constitutively constrained
out-of-plane stress must participate. The core standard result projection
already performs this reconstruction, including thermal eigenstrain.
The demo now consumes that existing MISES field and exports it alongside
displacement, temperature and stress. It uses the maximum DG0 cell-average
invariant, explicitly, rather than adding another hand-written stress formula.
This migration does not change equilibrium, thermal conduction or the K-R law.
Independent checks¶
Four affine planar tests (plane stress/strain, with/without thermal expansion) compare standard output with a full 3D Hooke stress and its principal-stress invariant. They pass at 1e-12 relative tolerance. On the actual reduced hot-wall mesh, an independent full-3D thermal strain reconstruction gives a maximum cell-average value of 554397427.2293961 Pa; the maximum pointwise difference between the two projected fields is 4.18e-7 Pa. Corrected degree-4 quadrature sampling gives 554942269.3512055 Pa, showing separately the averaging effect.
Versioned regression, not new physical validation¶
| Quantity | Old v1 | Corrected v2 |
|---|---|---|
| Governing stress, Pa | 331321497.13443035 | 554397427.2293957 |
| Illustrative rupture estimate, h | 31308.280996458638 | 2386.718875046755 |
| Damage at 90% of illustrative rupture time | 0.4376507671 | 0.4376507671 |
The unchanged final damage follows the chosen normalized endpoint; it is not
independent validation of the rupture estimate. The old Golden rejected both
changed quantities before its reference was explicitly versioned to
q1-6x10-heat4-kr40-plane-strain-mises-2. Neither reference is an experimental
material fit, and a cell-average maximum is not hotspot mesh convergence.
This finding concerns the older illustrative hot-wall demo, not the separate
P92 research material or the composite pressing simulation.