This is a live 3D render of the racket's actual orientation — not a canned animation. Its shape comes directly from the geometry sliders. The rotation each frame comes from numerically solving the real rigid-body equations of motion (Euler's equations) for the spin it started with. If Control is off, you're watching the raw spin of the racket. If Control is on, an attitude controller is actively steering it toward the chosen target axis.
The Hamiltonian represents the total energy of the system, in this case, the racket's rotational kinetic energy. The dashed lines show the energy the racket would have if spinning purely about each of its three axes. The racket's actual energy (solid line) stays trapped between the smallest and largest of these forever. With Control on, the dashed line becomes the chosen target energy instead, and the solid line is no longer flat — it climbs or falls as the controller does real work to get there.
This display shows the spin rate (radians/second) about each of the racket's principal axes, over time — long, intermediate, and short. Near the intermediate axis, all three swing through large, coupled oscillations instead of settling down, which is the visible signature of the instability. Near a stable axis (long or short), one component dominates while the other two stay as small, bounded wobbles.
A Casimir is a conserved quantity, built into the physics itself rather than something we choose — here, it's the racket's total angular momentum. Since it never changes during a free spin, every trajectory stays confined to this sphere's surface. The light-blue and coral dots are the six equilibrium spins (stable and unstable); starting exactly on one, undisturbed, leaves the state frozen forever, since every derivative vanishes there. The orange separatrices pass exactly through the unstable points, marking the boundary between the nearby blue wobbling loops and a full flip. The yellow dot is the racket's actual state right now — under Control or Wind it can leave this sphere entirely, since angular momentum is only conserved for a truly free spin.