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Expand file tree Collapse file tree Original file line number Diff line number Diff line change @@ -63,7 +63,7 @@ per-joint stiffness values remain assembly controls on
6363modes; damping is configured directly during assembly. Solver mechanics
6464likewise use ``rod `` terminology.
6565
66- For a circular elastic material, transverse shear uses the AOUSD -compatible
66+ For a circular elastic material, transverse shear uses the OpenUSD -compatible
6767effective rigidity ``kGA `` with ``k = 0.9 ``. This is a finite
6868shear-deformable rod, not the unshearable constraint of a strict Kirchhoff
6969rod. Use section rigidities or direct joint stiffnesses when a different
Original file line number Diff line number Diff line change 1414from ..core .types import Quat , Vec3 , axis_to_vec3
1515from ..math import quat_between_vectors_robust
1616
17- # Follow AOUSD 's solid-circular-section fallback: shear rigidity = kGA,
17+ # Follow OpenUSD 's solid-circular-section fallback: shear rigidity = kGA,
1818# where k ~= 0.9. Newton uses k = 0.9.
1919_CIRCULAR_SECTION_TRANSVERSE_SHEAR_CORRECTION = 0.9
2020
@@ -157,7 +157,7 @@ class Rod:
157157 or mutually inconsistent.
158158
159159 Note:
160- Material-derived transverse shear follows the AOUSD deformable-body
160+ Material-derived transverse shear follows the OpenUSD deformable-body
161161 treatment for a solid circular section, using ``kGA`` with
162162 ``k = 0.9``. See :meth:`newton.ModelBuilder.add_rod` for rigidity
163163 discretization, direct stiffness and damping controls, and topology
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