σ = J · F ≥ 0 — Brusselator driven oscillator & entropy production vs forcing
Prigogine (Nobel 1977): in NESS (non-equilibrium steady states), entropy production rate σ = Σ Jₖ·Fₖ ≥ 0.
Near equilibrium: Onsager reciprocal relations; σ is minimized (min entropy production theorem). Far from equilibrium: dissipative structures emerge (Turing patterns, Belousov-Zhabotinsky, Brusselator).
Brusselator: dX/dt = A − (B+1)X + X²Y, dY/dt = BX − X²Y. Hopf bifurcation at B_c = 1+A².