Gyroscopic stability
47 · Bodies
A T-handle spun about its intermediate principal axis in zero gravity flips over periodically (the Dzhanibekov effect). Steel integrates single free bodies with an energy-preserving update, so the flips stay periodic instead of drifting. The script sets angular damping to zero; the default is 0.05 s⁻¹, as in PhysX.
What to look at
- The handle flips every 2.9 s.
- Spin speed rises at each flip while energy and angular momentum stay constant.
Key parameter
steel:rigid_body_angular_dampingPer body [1/s], default 0.05. Damps free bodies and floating bases only.
Try changing
- Spin about the long axis instead.
- Restore the default damping and run for 60 s.
Concept
Energy-preserving gyroscopics
What it is
A spinning rigid body's angular momentum is constant, but its angular velocity changes as inertia rotates. An explicit update of that term adds energy. Steel updates single free bodies with Cayley steps that preserve kinetic energy exactly, using 1 to 32 microsteps.
In this scene
The T-handle flips about every 2.9 s and keeps doing so; spin rises to 9.4 rad/s at each flip.
Considerations
- Cost
- A few small 3×3 solves per body per step.
- Interactions
- Angular damping (default 0.05 s⁻¹) slowly removes energy; set it to 0 to compare.
- Use it when
- Automatic for free single bodies.
The script
cd tutorials && python 47_gyroscopic.py prints each variant's final metric; --record out.json also writes the replay. Every tutorial imports replay.py from the same folder.
# SPDX-FileCopyrightText: Copyright (c) 2026 Skild AI and the Steel contributors# SPDX-License-Identifier: Apache-2.0
"""Free-body gyroscopics: a T-handle spun about its middle axis flips (Dzhanibekov effect)."""
import newtonimport numpy as npimport warp as wpfrom newton.solvers import SolverSteel
from replay import Recorder
DT = 1.0 / 240.0SUBSTEPS = 8
def build(): builder = newton.ModelBuilder(gravity=(0.0, 0.0, 0.0)) SolverSteel.register_custom_attributes(builder) body = builder.add_body(xform=wp.transform((0.0, 0.0, 0.6), wp.quat_identity())) along_x = wp.quat_from_axis_angle(wp.vec3(0.0, 1.0, 0.0), np.pi / 2) along_y = wp.quat_from_axis_angle(wp.vec3(1.0, 0.0, 0.0), np.pi / 2) builder.add_shape_capsule( body, xform=wp.transform((0.0, 0.0, 0.0), along_x), radius=0.02, half_height=0.18 ) builder.add_shape_capsule( body, xform=wp.transform((0.0, 0.09, 0.0), along_y), radius=0.025, half_height=0.07 ) model = builder.finalize() model.steel.rigid_body_angular_damping.fill_(0.0) # default 0.05 1/s, as in PhysX # spin about the handle's middle axis model.joint_qd.assign(np.array([0.0, 0.0, 0.0, 0.02, 8.0, 0.01], dtype=np.float32)) return model
def simulate(rec, label): model = build() solver = SolverSteel(model) pipeline = newton.CollisionPipeline(model) contacts = pipeline.contacts() state_0, state_1, control = model.state(), model.state(), model.control() newton.eval_fk(model, model.joint_q, model.joint_qd, state_0)
run = rec.variant(label, model) for _ in range(rec.frames(8.0)): x, y, z, w = state_0.body_q.numpy()[0, 3:] handle_y = 1.0 - 2.0 * (x * x + z * z) # world y of the body's y axis run.frame(state_0, handle_y=handle_y, omega=np.linalg.norm(state_0.body_qd.numpy()[0, 3:])) for _ in range(SUBSTEPS): pipeline.collide(state_0, contacts) solver.step(state_0, state_1, control, contacts, DT) state_0, state_1 = state_1, state_0 run.check(solver)
if __name__ == "__main__": rec = Recorder() simulate(rec, "spin about the intermediate axis") rec.save()# SPDX-FileCopyrightText: Copyright (c) 2026 Skild AI and the Steel contributors# SPDX-License-Identifier: Apache-2.0
"""Record Steel tutorial runs as replay JSON for the tutorials page, or print a summary.
Every tutorial imports this module. ``python NN_name.py`` runs the variants and printsthe final metric of each; ``--record out.json`` also writes body poses, shapes and metricseries that the page replays in 3D."""
import argparseimport base64import jsonimport osimport subprocessimport sysimport time
import newtonimport numpy as npimport warp as wp
from source_hash import source_sha256
_RENDERED_TYPES = { newton.GeoType.PLANE, newton.GeoType.SPHERE, newton.GeoType.CAPSULE, newton.GeoType.ELLIPSOID, newton.GeoType.CYLINDER, newton.GeoType.BOX, newton.GeoType.MESH, newton.GeoType.CONE, newton.GeoType.CONVEX_MESH,}
class Recorder: """Collect the variants of one tutorial; ``fps`` is the replay frame rate."""
def __init__(self, fps: int = 30): parser = argparse.ArgumentParser() parser.add_argument( "--record", metavar="OUT.json", help="write a replay file for the tutorials page" ) parser.add_argument("--device", default=None, help="Warp device, for example cuda:0") self.args = parser.parse_args() if self.args.device: wp.set_device(self.args.device) self.fps = fps self.script = os.path.abspath(sys.argv[0]) self.variants: list[Variant] = []
def frames(self, seconds: float) -> int: """Number of replay frames in ``seconds``, including the first.""" return int(round(seconds * self.fps)) + 1
def variant( self, label: str, model: newton.Model, *, ghost: bool = False, slot: int | None = None, scene: str | None = None, ) -> "Variant": """Start one run; ``ghost`` overlays run ``slot``, ``scene`` groups runs for charts.""" variant = Variant(label, model, self.fps, ghost, slot, scene) self.variants.append(variant) return variant
def save(self) -> None: """Print a summary and, with ``--record``, write the replay file.""" for variant in self.variants: last = variant.metrics[-1] if variant.metrics else {} flag = " (rows dropped)" if variant.overflow else "" print(f"{variant.label:<48} {json.dumps(last)} {variant.wall:.2f} s{flag}") if not self.args.record: return source_sha = source_sha256(self.script) doc = { "script": os.path.basename(self.script), "script_sha256": source_sha, "newton_commit": _newton_commit(), "newton_version": newton.__version__, "warp_version": wp.config.version, "gpu": wp.get_device().name, "fps": self.fps, "variants": [v.to_json() for v in self.variants], } with open(self.args.record, "w") as f: json.dump(doc, f, separators=(",", ":")) print(f"wrote {self.args.record}")
class Variant: """One recorded run: a pose per frame for every body, plus named metric values."""
def __init__(self, label, model, fps, ghost, slot, scene): self.label, self.model, self.fps, self.ghost, self.slot = label, model, fps, ghost, slot self.scene = scene self.poses: list[np.ndarray] = [] self.metrics: list[dict] = [] self.awake: list[list[int]] = [] self.particles: list[np.ndarray] = [] self.overflow = False self.start = time.perf_counter() self.wall = 0.0
def frame(self, state: newton.State, awake=None, particles=None, **metrics) -> None: """Record ``state.body_q``, optional awake flags, particle positions and metric values.""" self.poses.append(state.body_q.numpy().astype(np.float32).copy()) if particles is not None: self.particles.append(particles.numpy().astype(np.float32).copy()) self.metrics.append({k: _round(v) for k, v in metrics.items()}) if awake is not None: self.awake.append([int(x) for x in awake.numpy()]) self.wall = time.perf_counter() - self.start
def check(self, solver) -> None: """Note whether the solver dropped rows; call once after the run.""" try: solver.check_constraint_capacity() except RuntimeError: self.overflow = True
def to_json(self) -> dict: poses = ( np.stack(self.poses) if self.poses else np.zeros((0, self.model.body_count, 7), np.float32) ) return { "label": self.label, "fps": self.fps, "ghost": self.ghost, "slot": self.slot, "scene": self.scene, "bodies": int(self.model.body_count), "frames": int(poses.shape[0]), "poses": base64.b64encode(poses.astype(np.float32).tobytes()).decode(), "shapes": _shape_table(self.model), "metric": self.metrics, "awake": self.awake or None, "particles": self._particles_json(), "wall_s": round(self.wall, 3), "overflow": self.overflow, }
def _particles_json(self): if not self.particles: return None frames = np.stack(self.particles) tris = self.model.tri_indices radius = self.model.particle_radius.numpy() return { "count": int(frames.shape[1]), "frames": base64.b64encode(frames.astype(np.float32).tobytes()).decode(), "radius": round(float(radius.mean()), 5) if radius.size else 0.0, "tris": [int(v) for v in tris.numpy().reshape(-1)] if tris is not None and tris.shape[0] else None, }
def _shape_table(model): types = model.shape_type.numpy() scales = model.shape_scale.numpy() xforms = model.shape_transform.numpy() bodies = model.shape_body.numpy() flags = model.shape_flags.numpy() shapes = [] for i, t in enumerate(types): if int(t) not in _RENDERED_TYPES or not flags[i] & int(newton.ShapeFlags.VISIBLE): continue shape = { "b": int(bodies[i]), "t": int(t), "s": [round(float(v), 5) for v in scales[i]], "x": [round(float(v), 6) for v in xforms[i]], } if int(t) in (newton.GeoType.MESH, newton.GeoType.CONVEX_MESH): mesh = model.shape_source[i] shape["v"] = [round(float(v), 5) for v in np.asarray(mesh.vertices).reshape(-1)] shape["i"] = [int(v) for v in np.asarray(mesh.indices).reshape(-1)] shapes.append(shape) return shapes
def _round(value): value = float(value) return round(value, 5) if np.isfinite(value) else None
def _newton_commit(): if os.environ.get("NEWTON_COMMIT"): return os.environ["NEWTON_COMMIT"] try: root = os.path.dirname(os.path.dirname(newton.__file__)) return subprocess.check_output(["git", "-C", root, "rev-parse", "HEAD"], text=True).strip() except (OSError, subprocess.CalledProcessError): return NoneRecorded with SolverSteel on Newton 1.9.0.dev0, Warp 1.19.0, NVIDIA RTX PRO 6000 Blackwell Server Edition. Replays read the state back every frame, so they are not a speed benchmark. Script · page text
Steel docs and tutorials are licensed under Apache-2.0. Third-party notices. "Skild", "Skild AI" and the Skild logo are trademarks of Skild AI and are not licensed under Apache-2.0.