Restrict midpoint integration to unconstrained free bodies in implicitfast

PiperOrigin-RevId: 908750768
Change-Id: I9a45a160ac757cc82bfe54871609956769988369
This commit is contained in:
Yuval Tassa
2026-05-01 08:40:53 -07:00
committed by Copybara-Service
parent 8287d9d152
commit 910b3336ed
5 changed files with 221 additions and 94 deletions
+5
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@@ -8,6 +8,11 @@ Upcoming version (not yet released)
- Added island support for the :ref:`PGS solver<soAlgorithms>`.
- Added support for :ref:`elastic2d<body-flexcomp-elastic2d>` for trilinear and quadratic flex
:ref:`dofs<body-flexcomp-dof>`.
- :ref:`Midpoint integration<geMidpoint>` is now restricted to the ``implicitfast``
:ref:`integrator<geIntegrators>` and is disabled when fluid forces are active
(nonzero :ref:`density<option-density>` or :ref:`viscosity<option-viscosity>`).
Midpoint integration treats external forces as zero-order-hold constants, which causes
energy gain in the presence of contacts and in fluid media.
Python
^^^^^^
+11 -9
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@@ -575,7 +575,7 @@ Solving for :math:`v_{t+h}`, we obtain the implicit-in-velocity update
.. _geMidpoint:
Midpoint integration for free bodies
Midpoint integration for free bodies in vacuum
The implicit-in-velocity update :eq:`eq_implicit_update` treats the acceleration as a function of velocity and
linearizes. While effective for damping-like forces, it is sub-optimal for rotational dynamics, where
Coriolis and gyroscopic forces are *quadratic* in angular velocity. For this case, a better approach is to directly
@@ -606,7 +606,9 @@ Midpoint integration for free bodies
Casimir function of the `Lie-Poisson <https://en.wikipedia.org/wiki/Poisson_bracket>`__ structure, the midpoint
method is a symmetric (time-reversible) and second-order accurate *Poisson integrator*.
**Eligibility.** Midpoint integration is only applied to free bodies with no child bodies.
**Eligibility.** Midpoint integration is only applied when using the ``implicitfast`` integrator, to
free bodies with no child bodies, and only when the medium has zero :ref:`density<option-density>` and
:ref:`viscosity<option-viscosity>`.
**Performance.** While the midpoint method carries computational overhead, we've found it to be
negligible compared to the rest of the pipeline, on the order of 1% in the worst case.
@@ -652,9 +654,8 @@ Fast implicit-in-velocity (``implicitfast``)
scenarios which are not common and already well-handled by the Runge-Kutta integrator (see below). Because the RNE
derivatives are also the main source of asymmetry of :math:`D`, by dropping them and symmetrizing, we can use the
faster :math:`L^TL` rather than :math:`LU` decomposition.
Both ``implicit`` and ``implicitfast`` apply :ref:`midpoint integration<geMidpoint>` to eligible free bodies,
providing exact energy conservation for spinning objects at negligible additional cost.
The ``implicitfast`` integrator applies :ref:`midpoint integration<geMidpoint>` to eligible free bodies in vacuum,
providing exact energy conservation for spinning objects at negligible additional cost.
4th-order Runge-Kutta (``RK4``)
One advantage of our continuous-time formulation is that we can use higher order integrators such as Runge-Kutta or
@@ -688,10 +689,11 @@ providing exact energy conservation for spinning objects at negligible additiona
increased stability, and is therefore a strict improvement. It is the recommended integrator for most models.
**implicit**:
The benefit over ``implicitfast`` is the implicit integration of Coriolis and centripetal forces for *coupled*
rotational systems such as multi-link pendula. Both ``implicitfast`` and ``implicit`` apply :ref:`midpoint
integration<geMidpoint>` to eligible free bodies with no children, for example
`gyroscopic.xml <../_static/gyroscopic.xml>`__ shows an ellipsoid rolling on an
inclined plane; both ``implicitfast`` and ``implicit`` handle this case well, while ``Euler`` quickly diverges.
rotational systems such as multi-link pendula. Note that ``implicit`` does not apply :ref:`midpoint
integration<geMidpoint>` (only ``implicitfast`` does), but its RNE derivatives provide comparable stability
for free-body rotation. For example, `gyroscopic.xml <../_static/gyroscopic.xml>`__ shows an ellipsoid rolling
on an inclined plane; both ``implicitfast`` and ``implicit`` handle this case well, while ``Euler`` quickly
diverges.
**RK4**:
This integrator is best for systems which are energy conserving, or almost energy-conserving. `pendulum.xml
<../_static/pendulum.xml>`__ shows a complicated pendulum mechanism which diverges quickly using ``Euler`` or
+71 -11
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@@ -1597,16 +1597,75 @@ static void flexInterp_solve(const mjModel* m, mjData* d, const FlexInterpContex
// return 1 if free joint is eligible for midpoint quaternion integration:
// standalone 6-DOF tree with no children
static int midpoint_eligible(const mjModel* m, int jnt) {
if (m->jnt_type[jnt] == mjJNT_FREE) {
int body = m->jnt_bodyid[jnt];
int treeid = m->dof_treeid[m->jnt_dofadr[jnt]];
return m->tree_dofnum[treeid] == 6 &&
m->body_subtreemass[body] == m->body_mass[body];
// standalone 6-DOF tree with no children, awake, and unconstrained
static int midpoint_eligible(const mjModel* m, const mjData* d, int jnt) {
if (m->jnt_type[jnt] != mjJNT_FREE) {
return 0;
}
return 0;
int body = m->jnt_bodyid[jnt];
int adr = m->jnt_dofadr[jnt];
int tree = m->dof_treeid[adr];
// must be standalone 6-DOF tree with no children
if (m->tree_dofnum[tree] != 6 ||
m->body_subtreemass[body] != m->body_mass[body]) {
return 0;
}
// must be awake
if (!d->tree_awake[tree]) {
return 0;
}
// must be unconstrained
if (d->nefc) {
// islands enabled: O(1) lookup
if (!mjDISABLED(mjDSBL_ISLAND)) {
if (d->dof_island[adr] >= 0) {
return 0;
}
}
// islands disabled: check if any constraint involves this tree
else {
for (int c=0; c < d->nefc; c++) {
int type = d->efc_type[c];
int id = d->efc_id[c];
// contact: check if either geom belongs to this body
if (type == mjCNSTR_CONTACT_FRICTIONLESS ||
type == mjCNSTR_CONTACT_PYRAMIDAL ||
type == mjCNSTR_CONTACT_ELLIPTIC) {
int g1 = d->contact[id].geom[0];
int g2 = d->contact[id].geom[1];
if (g1 >= 0 && m->geom_bodyid[g1] == body) return 0;
if (g2 >= 0 && m->geom_bodyid[g2] == body) return 0;
}
// connect or weld: check if either body is this body
else if (type == mjCNSTR_EQUALITY &&
(m->eq_type[id] == mjEQ_CONNECT || m->eq_type[id] == mjEQ_WELD)) {
int b1 = m->eq_obj1id[id];
int b2 = m->eq_obj2id[id];
if (m->eq_objtype[id] == mjOBJ_SITE) {
b1 = m->site_bodyid[b1];
b2 = m->site_bodyid[b2];
}
if (b1 == body || b2 == body) return 0;
}
// tendon limit or friction: check first two trees
else if (type == mjCNSTR_LIMIT_TENDON || type == mjCNSTR_FRICTION_TENDON) {
if (m->tendon_treeid[2*id] == tree ||
m->tendon_treeid[2*id+1] == tree) return 0;
}
}
}
}
// otherwise eligible
return 1;
}
@@ -1980,11 +2039,12 @@ void mj_implicitSkip(const mjModel* m, mjData* d, int skipfactor) {
// count and list joints of free bodies eligible for midpoint integration
int nfree = 0;
int* free_jntid = NULL;
if (!mjENABLED(mjENBL_INVDISCRETE)) {
if (!mjENABLED(mjENBL_INVDISCRETE) &&
m->opt.integrator == mjINT_IMPLICITFAST &&
m->opt.density == 0 && m->opt.viscosity == 0) {
free_jntid = mjSTACKALLOC(d, m->njnt, int);
for (int j=0; j < m->njnt; j++) {
// add to list if eligible and awake
if (midpoint_eligible(m, j) && d->tree_awake[m->dof_treeid[m->jnt_dofadr[j]]]) {
if (midpoint_eligible(m, d, j)) {
free_jntid[nfree++] = j;
}
}
-74
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@@ -1745,79 +1745,5 @@ TEST_F(DerivativeTest, FlexInterpDerivativesDeformed) {
mj_deleteModel(model);
}
TEST_F(DerivativeTest, MidpointFluidAccuracy) {
const std::string xml_path =
GetTestDataFilePath(kTumblingThinObjectEllipsoidPath);
char error[1024];
mjModel* m = mj_loadXML(xml_path.c_str(), nullptr, error, sizeof(error));
ASSERT_THAT(m, NotNull()) << error;
mjtNum dt_small = 1e-4;
mjtNum dt_large = m->opt.timestep; // 2e-3, the default
mjtNum duration = 0.5;
mjData* d_ref = mj_makeData(m);
mjData* d_midpoint = mj_makeData(m);
mjData* d_nomidpoint = mj_makeData(m);
// give initial angular velocity for tumbling
mj_resetData(m, d_ref);
mj_resetData(m, d_midpoint);
mj_resetData(m, d_nomidpoint);
d_ref->qvel[3] = 5;
d_ref->qvel[4] = 3;
d_ref->qvel[5] = 1;
d_midpoint->qvel[3] = 5;
d_midpoint->qvel[4] = 3;
d_midpoint->qvel[5] = 1;
d_nomidpoint->qvel[3] = 5;
d_nomidpoint->qvel[4] = 3;
d_nomidpoint->qvel[5] = 1;
int nsteps_large = static_cast<int>(duration / dt_large);
int substeps = static_cast<int>(dt_large / dt_small);
mjtNum error_midpoint = 0;
mjtNum error_nomidpoint = 0;
for (int i = 0; i < nsteps_large; i++) {
// reference: RK4 at small timestep
m->opt.integrator = mjINT_RK4;
m->opt.timestep = dt_small;
m->opt.enableflags &= ~mjENBL_INVDISCRETE;
for (int j = 0; j < substeps; j++) {
mj_step(m, d_ref);
}
// implicit with midpoint (default)
m->opt.integrator = mjINT_IMPLICIT;
m->opt.timestep = dt_large;
m->opt.enableflags &= ~mjENBL_INVDISCRETE;
mj_step(m, d_midpoint);
// implicit without midpoint
m->opt.enableflags |= mjENBL_INVDISCRETE;
mj_step(m, d_nomidpoint);
// accumulate position errors
for (int k = 0; k < 7; k++) {
mjtNum diff_mid = d_ref->qpos[k] - d_midpoint->qpos[k];
mjtNum diff_nomid = d_ref->qpos[k] - d_nomidpoint->qpos[k];
error_midpoint += diff_mid * diff_mid;
error_nomidpoint += diff_nomid * diff_nomid;
}
}
// expect midpoint to be more accurate
EXPECT_LT(error_midpoint, error_nomidpoint)
<< "implicit midpoint should be more accurate than implicit without "
<< "midpoint for a free body with fluid forces";
mj_deleteData(d_nomidpoint);
mj_deleteData(d_midpoint);
mj_deleteData(d_ref);
mj_deleteModel(m);
}
} // namespace
} // namespace mujoco
+134
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@@ -783,6 +783,140 @@ TEST_F(ImplicitIntegratorTest, MidpointFullNewtonConvergence) {
EXPECT_LT((mjtNum)total_iter / ncases, 3.0);
}
// verify midpoint eligibility: compare with/without invdiscrete
// if trajectories differ, midpoint was applied
// if trajectories match, midpoint was skipped
TEST_F(ImplicitIntegratorTest, MidpointEligibility) {
// free body with asymmetric inertia, optionally near a plane
static constexpr char xml[] = R"(
<mujoco>
<option integrator="implicitfast" timestep="0.01">
<flag energy="enable"/>
</option>
<worldbody>
<geom type="plane" size="5 5 0.1"/>
<body name="free" pos="0 0 2">
<freejoint/>
<geom type="ellipsoid" size="0.3 0.2 0.1" mass="1"/>
</body>
</worldbody>
</mujoco>
)";
char error[1024];
mjModel* m = LoadModelFromString(xml, error, sizeof(error));
ASSERT_THAT(m, NotNull()) << error;
mjData* d1 = mj_makeData(m);
mjData* d2 = mj_makeData(m);
int nsteps = 50;
auto spin_and_compare = [&](const char* label,
bool expect_midpoint) {
mj_resetData(m, d1);
mj_resetData(m, d2);
d1->qvel[3] = d2->qvel[3] = 5;
d1->qvel[4] = d2->qvel[4] = 3;
d1->qvel[5] = d2->qvel[5] = 1;
// d1: midpoint enabled (default)
m->opt.enableflags &= ~mjENBL_INVDISCRETE;
for (int i = 0; i < nsteps; i++) mj_step(m, d1);
// d2: midpoint disabled
m->opt.enableflags |= mjENBL_INVDISCRETE;
mj_resetData(m, d2);
d2->qvel[3] = 5; d2->qvel[4] = 3; d2->qvel[5] = 1;
for (int i = 0; i < nsteps; i++) mj_step(m, d2);
m->opt.enableflags &= ~mjENBL_INVDISCRETE;
// compare angular velocities
mjtNum diff = 0;
for (int k = 3; k < 6; k++) {
mjtNum d = d1->qvel[k] - d2->qvel[k];
diff += d * d;
}
if (expect_midpoint) {
EXPECT_GT(diff, 1e-6)
<< label << ": expected midpoint to be applied";
} else {
EXPECT_LT(diff, 1e-20)
<< label << ": expected midpoint to be skipped";
}
};
// case 1: free body in vacuum, implicitfast -> midpoint applied
m->opt.integrator = mjINT_IMPLICITFAST;
m->opt.density = 0;
m->opt.viscosity = 0;
spin_and_compare("vacuum+implicitfast", true);
// case 2: implicit integrator -> midpoint NOT applied
m->opt.integrator = mjINT_IMPLICIT;
spin_and_compare("vacuum+implicit", false);
// case 3: fluid (nonzero density) -> midpoint NOT applied
m->opt.integrator = mjINT_IMPLICITFAST;
m->opt.density = 1.2;
spin_and_compare("fluid+implicitfast", false);
m->opt.density = 0;
// case 4: fluid (nonzero viscosity) -> midpoint NOT applied
m->opt.viscosity = 0.001;
spin_and_compare("viscosity+implicitfast", false);
m->opt.viscosity = 0;
// case 5: body with active contacts -> midpoint NOT applied
// test both island-enabled and island-disabled branches
for (int disable_island = 0; disable_island < 2; disable_island++) {
m->opt.integrator = mjINT_IMPLICITFAST;
if (disable_island) {
m->opt.disableflags |= mjDSBL_ISLAND;
} else {
m->opt.disableflags &= ~mjDSBL_ISLAND;
}
mj_resetData(m, d1);
mj_resetData(m, d2);
d1->qpos[2] = d2->qpos[2] = 0.05;
d1->qvel[3] = d2->qvel[3] = 5;
d1->qvel[4] = d2->qvel[4] = 3;
d1->qvel[5] = d2->qvel[5] = 1;
// verify contacts are active
mj_forward(m, d1);
ASSERT_GT(d1->ncon, 0) << "body should be in contact with the plane";
// single step with midpoint enabled
mj_resetData(m, d1);
d1->qpos[2] = 0.05;
d1->qvel[3] = 5; d1->qvel[4] = 3; d1->qvel[5] = 1;
m->opt.enableflags &= ~mjENBL_INVDISCRETE;
mj_step(m, d1);
// single step with midpoint disabled
mj_resetData(m, d2);
d2->qpos[2] = 0.05;
d2->qvel[3] = 5; d2->qvel[4] = 3; d2->qvel[5] = 1;
m->opt.enableflags |= mjENBL_INVDISCRETE;
mj_step(m, d2);
m->opt.enableflags &= ~mjENBL_INVDISCRETE;
mjtNum diff = 0;
for (int k = 0; k < m->nv; k++) {
mjtNum d = d1->qvel[k] - d2->qvel[k];
diff += d * d;
}
EXPECT_LT(diff, 1e-20)
<< "contact (island " << (disable_island ? "disabled" : "enabled")
<< "): expected midpoint to be skipped";
}
m->opt.disableflags &= ~mjDSBL_ISLAND;
mj_deleteData(d2);
mj_deleteData(d1);
mj_deleteModel(m);
}
TEST_F(ForwardTest, ControlClamping) {
static constexpr char xml[] = R"(
<mujoco>