This quantity is equal to the negative of Boltzmann's constant times temperature times
In the grand canonical ensemble model, the grand potential is equal to this quantity minus thechemical potential times the number of particles in a system. Thermodynamic integration is usuallyused to compute the difference in this quantity between two states of interest in a system, and theGibbs-Bogoliubov inequality gives the lower bound of this as the configurational internal energy.This quantity is equal to the negative of Boltzmann's constant times temperature times the (*) naturallogarithm of the canonical ensemble partition function, and it is minimized for a system in thermal contactwith a reservoir. It is the difference between internal energy and the product of temperature and entropy.For 10 points, name this quantity that is the maximum amount of work obtainable from a reversible processat constant temperature and volume.
In the grand canonical ensemble model, the grand potential is equal to this quantity minus thechemical potential times the number of particles in a system.
Helmholtz free energy [prompt on free energy]