Liouville's Theorem — Phase Space Volume

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Liouville's Theorem

In Hamiltonian mechanics, the phase-space density is conserved along trajectories. A blob of initial conditions evolves — it can stretch and contort, but its total phase-space volume (area in 2D) never changes.

dρ/dt = 0, equivalently div(ẋ, ṗ) = 0.

Here, a colored blob of (q, p) points flows under H = p²/2 + ω²q²/2 + εq⁴/4. Even for the anharmonic oscillator the area is preserved — but the blob shears dramatically. The grid lines show the distortion of phase-space structure.