“…Within the proposed mesoscopic irreversible thermodynamic framework, the steady‐state rate of any activated materials process occurring inside a nonequilibrium condensed system, which converts an ideal reacting mixture 31,34,35 at its initial α‐state into a product at the final β‐state, may be approximately expressed as 26–28 where ρ : global steady‐state process‐rate (mol m −2 s −1 ), R : gas constant (8.314 J mol −1 K −1 ), T : thermodynamic temperature (K), Щ : molar mobility of the reacting species (m mol s −1 N −1 ), c α : concentration of the ideal reacting mixture at the initial α‐state (mol m −3 ), δ : length of the mesoscopic process path between the initial α‐state and the final β‐state (m), Æ : activation enthalpy for the isothermal, isobaric materials process (J mol −1 ), with its magnitude greater than RT – the thermal energy provided by the surroundings, A ≡ −Δ r μ = [ μ (α)− μ (β)]: affinity (J mol −1 ), that is, difference between the totaled chemical potentials, μ , at the initial reactant‐state, α, and final product‐state, β, of the isothermal process, k a ≡ { RTЩδ −1 } × {exp[− Æ /( RT )]} = { R K } × {exp[− Æ /( RT )]}: a highly temperature‐dependent kinetic factor of the process, containing an activation enthalpy exponential term, {exp[− Æ /( RT )]}, and a pre‐exponential frequency coefficient, R K ≡ { RTЩδ −1 }, Φ IT ≡ {1−exp[− A /( RT )]}: general driving force of any isothermal materials process—a nonlinear function of the affinity, A , of the process.…”