Switch mjData.{qH,qLD} from reduced ("C") to full ("M") inertia matrix structure. No performance impact of extra zeros because of existing "simple dof" skipping mechanism.
PiperOrigin-RevId: 733523931 Change-Id: Ic8d8a152dda5532331c239cb6b4ce7d8d09b7fff
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Copybara-Service
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@@ -300,7 +300,7 @@ struct mjData_ {
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mjtNum* qM; // total inertia (sparse) (nM x 1)
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// computed by mj_fwdPosition/mj_factorM
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mjtNum* qLD; // L'*D*L factorization of M (sparse) (nC x 1)
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mjtNum* qLD; // L'*D*L factorization of M (sparse) (nM x 1)
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mjtNum* qLDiagInv; // 1/diag(D) (nv x 1)
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// computed by mj_collisionTree
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@@ -333,7 +333,7 @@ struct mjData_ {
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mjtNum* subtree_angmom; // angular momentum about subtree com (nbody x 3)
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// computed by mj_Euler or mj_implicit
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mjtNum* qH; // L'*D*L factorization of modified M (nC x 1)
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mjtNum* qH; // L'*D*L factorization of modified M (nM x 1)
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mjtNum* qHDiagInv; // 1/diag(D) of modified M (nv x 1)
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// computed by mj_resetData
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@@ -650,7 +650,7 @@
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X ( mjtNum, actuator_moment, nJmom, 1 ) \
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X ( mjtNum, crb, nbody, 10 ) \
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X ( mjtNum, qM, nM, 1 ) \
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X ( mjtNum, qLD, nC, 1 ) \
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X ( mjtNum, qLD, nM, 1 ) \
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X ( mjtNum, qLDiagInv, nv, 1 ) \
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XMJV( mjtNum, bvh_aabb_dyn, nbvhdynamic, 6 ) \
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XMJV( mjtByte, bvh_active, nbvh, 1 ) \
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@@ -667,7 +667,7 @@
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X ( mjtNum, qfrc_passive, nv, 1 ) \
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X ( mjtNum, subtree_linvel, nbody, 3 ) \
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X ( mjtNum, subtree_angmom, nbody, 3 ) \
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X ( mjtNum, qH, nC, 1 ) \
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X ( mjtNum, qH, nM, 1 ) \
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X ( mjtNum, qHDiagInv, nv, 1 ) \
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X ( int, B_rownnz, nbody, 1 ) \
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X ( int, B_rowadr, nbody, 1 ) \
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