The Zeroth Law of Thermodynamics and Volume-Preserving Conservative Dynamics with Equilibrium Stochastic Damping

preprint2013arXivOpen access

Abstract

We propose a mathematical formulation of the zeroth law of thermodynamics and develop a stochastic dynamical theory, with a consistent irreversible thermodynamics, for systems possessing sustained conservative stationary current in phase space while in equilibrium with a heat bath. The theory generalizes underdamped mechanical equilibrium: dx=gdt+{−D∇ϕdt+2DdB(t)}dx=gdt+\{-D\nablaϕdt+\sqrt{2D}dB(t)\}, with ∇⋅g=0\nabla\cdot g=0 and {⋯ }\{\cdots\} respectively representing phase-volume preserving dynamics and stochastic damping. The zeroth law implies stationary distribution uss(x)=e−ϕ(x)u^{ss}(x)=e^{-ϕ(x)}. We find an orthogonality ∇ϕ⋅g=0\nablaϕ\cdot g=0 as a hallmark of the system. Stochastic thermodynamics based on time reversal (t,ϕ,g)→(−t,ϕ,−g)\big(t,ϕ,g\big)\rightarrow\big(-t,ϕ,-g\big) is formulated: entropy production ep#(t)=−dF(t)/dte_p^{\#}(t)=-dF(t)/dt; generalized "heat" hd#(t)=−dU(t)/dth_d^{\#}(t)=-dU(t)/dt, U(t)=∫Rnϕ(x)u(x,t)dxU(t)=\int_{\mathbb{R}^n} ϕ(x)u(x,t)dx being "internal energy", and "free energy" F(t)=U(t)+∫Rnu(x,t)ln⁡u(x,t)dxF(t)=U(t)+\int_{\mathbb{R}^n} u(x,t)\ln u(x,t)dx never increases. Entropy follows dSdt=ep#−hd#\frac{dS}{dt}=e_p^{\#}-h_d^{\#}. Our formulation is shown to be consistent with an earlier theory of P. Ao. Its contradistinctions to other theories, potential-flux decomposition, stochastic Hamiltonian system with even and odd variables, Klein-Kramers equation, Freidlin-Wentzell's theory, and GENERIC, are discussed.

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