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solver, model: imperfections from buckling modes in nonlinear steps
NonlinearStatic.imperfection {step, mode, scale}: the buckling step's mode, scaled to a largest
component of `scale`, is added to the node coordinates before the step is solved, with a warning
naming it; Abaqus and LS-DYNA decks refuse it by name. A clamped–free column with its first mode
as imperfection under half its buckling load amplifies it by 1/(1 − α) within 2.8 %.
Co-Authored-By: Claude Opus 5.5 <[email protected]>
Claude-Session: https://claude.ai/code/session_01UhhZMBTviDQxZvwnyP89fo
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@@ -193,6 +193,13 @@ buckle from, and with a shift); Nastran SOL 105 and LS-DYNA refuse it by name. V
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columns of hex20 (pinned and clamped–free, 0.18 % from Engesser's shear-corrected load) and the
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shifted form against the plain one.
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**Imperfections.** A nonlinear static step's `"imperfection": {"step": "Buckle", "mode": 1,
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"scale": 0.01}` solves that buckling step first and adds its mode, scaled to a largest component
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of `scale`, to the node coordinates; the step is solved and reported on that geometry, with a
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warning naming the mode. Abaqus and LS-DYNA decks refuse it by name (their imperfection reads a
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results file). Verified: a clamped–free column with its first mode as imperfection under half its
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buckling load deflects by δ₀ α/(1 − α) (2.8 %).
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## Nonlinear static analysis (finite strain)
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A step `{"type": "nonlinear_static", …}` (`Procedure::NonlinearStatic`, solved by
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