Add implicit integrator.
Added analytic derivatives of smooth (unconstrained) dynamics forces, with respect to velocities: - Centripetal and Coriolis forces computed by the Recursive Newton-Euler algorithm. - Damping and fluid-drag passive forces. - Actuation forces. A new implicit-in-velocity integrator is implemented using the analytic derivatives. This integrator lies between the Euler and Runge Kutta integrators in terms of both stability and computational cost. PiperOrigin-RevId: 450377010 Change-Id: Ie192b441876c22e732fb749333926f296e0a09cc
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Copybara-Service
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@@ -225,10 +225,10 @@ struct mjData_ {
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// computed by mj_fwdPosition/mj_crb
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mjtNum* crb; // com-based composite inertia and mass (nbody x 10)
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mjtNum* qM; // total inertia (nM x 1)
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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 (nM 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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mjtNum* qLDiagSqrtInv; // 1/sqrt(diag(D)) (nv x 1)
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@@ -286,6 +286,17 @@ struct mjData_ {
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mjtNum* subtree_linvel; // linear velocity of subtree com (nbody x 3)
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mjtNum* subtree_angmom; // angular momentum about subtree com (nbody x 3)
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// computed by mj_implicit
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int* D_rownnz; // non-zeros in each row (nv x 1)
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int* D_rowadr; // address of each row in D_colind (nv x 1)
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int* D_colind; // column indices of non-zeros (nD x 1)
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// computed by mj_implicit/mj_derivative
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mjtNum* qDeriv; // d (passive + actuator - bias) / d qvel (nD x 1)
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// computed by mj_implicit/mju_factorLUSparse
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mjtNum* qLU; // sparse LU of (qM - dt*qDeriv) (nD x 1)
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//-------------------------------- POSITION, VELOCITY, CONTROL/ACCELERATION dependent
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// computed by mj_fwdActuation
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