Implement midpoint integrator for free bodies.
PiperOrigin-RevId: 899043541 Change-Id: I0bb38f6ad94e189b45ab16777a04ad6fefc6adf7
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@@ -27,8 +27,13 @@ General
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(``jnt_stiffness``, ``dof_damping``, etc.) continue to hold the linear coefficient and are unchanged.
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The polynomial order is defined by the new constant :ref:`mjNPOLY<glNumericSizes>`. A future breaking C-API change
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may unify the linear and higher-order coefficients into a single array.
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- Introduced :ref:`mjpEncoder`, the counterpart to :ref:`mjpDecoder` for encoding of :ref:`mjSpec` and :ref:`mjModel` into :ref:`mjResource`.
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- Added :ref:`midpoint integration<geMidpoint>` for standalone free bodies in ``implicit`` and ``implicitfast``
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:ref:`integrators<geIntegrators>`. This applies the implicit midpoint rule to the rotational dynamics of free bodies
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with no children, exactly conserving kinetic energy and angular momentum in the absence of external torques. The
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:ref:`invdiscrete<option-flag-invdiscrete>` flag now also disables midpoint integration, providing an opt-out
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mechanism.
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- Introduced :ref:`mjpEncoder`, the counterpart to :ref:`mjpDecoder` for encoding of :ref:`mjSpec` and :ref:`mjModel`
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into :ref:`mjResource`.
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- Added :ref:`mj_encode`, :ref:`mjp_registerEncoder`, :ref:`mjp_defaultEncoder`, and :ref:`mjp_findEncoder`.
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