Symplectic Reduction & Coadjoint Orbits of SO(3)

Symplectic reduction (Marsden-Weinstein 1974) shows that conserved quantities correspond to symmetries via the momentum map J: T*Q → g*. For SO(3), coadjoint orbits are spheres in ℝ³ — the geometric home of angular momentum. Each sphere is itself a symplectic manifold.

|L|² = (conserved)
L_z =
Energy =
Orbit type:
L = (L_x, L_y, L_z) ∈ so(3)* coadjoint orbit: |L|² = const Euler's eqns: İ = L × (I⁻¹L)