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Physical completion of the Navier-Stokes equations
arXiv Math
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이 매체는 공공·자유 라이선스로 본문을 직접 표시합니다.Condensed Matter > Statistical Mechanics
[Submitted on 20 May 2026 (v1), last revised 1 Jun 2026 (this version, v2)]
Title:Physical completion of the Navier-Stokes equations
View PDF HTML (experimental)Abstract:The incompressible Navier-Stokes equations contain viscous dissipation but no thermal noise. I show, using a topological argument based on Poincaré's lemma, that the fluctuation-dissipation relation for the full nonlinear dynamics can be derived without the linearisation or structural assumptions that all previous derivations require. The nonlinear convective term is Hamiltonian (energy-preserving and phase-space-volume-preserving) and drops out of the Fokker-Planck equilibrium condition exactly, so the noise derived from linearised fluctuations near equilibrium is in fact exact for the full nonlinear system. This result proves, rather than assumes, the reversible/irreversible decomposition that the GENERIC framework postulates, provided Poincaré's lemma holds on the phase space. The resulting stochastic system, with a physical molecular-scale spectral cutoff, is trivially globally well-posed: a finite-dimensional stochastic differential equation with non-degenerate noise and a confining Lyapunov function. It has a unique Gibbs equilibrium and converges to it exponentially. The difficulty of the Clay Millennium Prize Problem arises entirely from two idealisations, zero temperature and infinite spectral resolution, neither of which is satisfied by any physical fluid.
Submission history
From: Samuel Braunstein [view email][v1] Wed, 20 May 2026 16:22:25 UTC (9 KB)
[v2] Mon, 1 Jun 2026 07:44:48 UTC (9 KB)
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