μ=∂G∂N i.e. it is free energy per particle in an ensemble, or energy needed for a particle to add it to the system so that the system will stay in equilibrium. (Some call it the Gibbs free energy/enthalpy. Free energy is usually the name for the Helmholtz free energy). Formal definition -
G(T,P,N)=E(T,P,N)+P⋅V(T,P,N)−T⋅S(T,P,N)
so the equilibrium state is given for minimal value of
G. If you put in contact 2 closed systems with
G1(T1,P1,N1) and
G2(T2,P2,N2) , the combined system system will seek a new equlibrium with maximal entropy and minimal
G -
G∗(T∗,P∗,N∗)=G∗1(T∗,P∗,N∗1)+G∗2(T∗,P∗,N∗2)
Because of the maximal entropy principle - one of the ways the system tries to minimize G /maximize entropy is by flow of particles from one system to another. The particles will flow from system with high value of μ to the system with low value - that according to the principle of minimizing free energy in the system.
This post imported from StackExchange Physics at 2015-08-25 07:26 (UTC), posted by SE-user Alexander