Emerging of Stochastic Dynamical Equalities and Steady State Thermodynamics from Darwinian Dynamics

Abstract

The evolutionary dynamics first conceived by Darwin and Wallace, referring to as Darwinian dynamics in the present paper, has been found to be universally valid in biology. The statistical mechanics and thermodynamics, while enormous successful in physics, have been in an awkward situation of wanting a consistent dynamical understanding. Here we present from a formal point of view an exploration of the connection between thermodynamics and Darwinian dynamics and a few related topics. We first show that the stochasticity in Darwinian dynamics implies the existence temperature, hence the canonical distribution of Boltzmann-Gibbs type. In term of relative entropy the Second Law of thermodynamics is dynamically demonstrated without detailed balance condition, and is valid regardless of size of the system. In particular, the dynamical component responsible for breaking detailed balance condition does not contribute to the change of the relative entropy. Two types of stochastic dynamical equalities of current interest are explicitly discussed in the present approach: One is based on Feynman-Kac formula and another is a generalization of Einstein relation. Both are directly accessible to experimental tests. Our demonstration indicates that Darwinian dynamics represents logically a simple and straightforward starting point for statistical mechanics and thermodynamics and is complementary to and consistent with conservative dynamics that dominates the physical sciences. Present exploration suggests the existence of a unified stochastic dynamical framework both near and far from equilibrium.

Fig. 1

Adaptive landscape with in potential contour representation. + : local basin; − : local peak; × : pass (saddle point). Darwinian dynamics was conceived graphically by Wright^[6] as the motion of the system in an adaptive landscape in genetic space (for an illustration, see Fig. 1).

Fig. 2

Carnot cycle. (a) The μ-λ representation. (b) The θ-S representation. In this temperature-entropy representation, the Carnot cycle is a rectangular.