**Definitions**

The Gibbs free energy is defined as:

*G(p,T)*=*U*+*pV*−*TS*

which is the same as:

*G(p,T)*=*H*−*TS*

where:

*U*is the internal energy (SI unit: joule)*p*is pressure (SI unit: pascal)*V*is volume (SI unit: m3)*T*is the temperature (SI unit: kelvin)*S*is the entropy (SI unit: joule per kelvin)*H*is the enthalpy (SI unit: joule)

The expression for the infinitesimal reversible change in the Gibbs free energy as a function of its 'natural variables' p and T, for an open system, subjected to the operation of external forces (for instance electrical or magnetical) *X _{i}*, which cause the external parameters of the system

*a*to change by an amount d

_{i}*a*, can be derived as follows from the First Law for reversible processes:

_{i}

where:

*μ*_{i}is the chemical potential of the*i*th chemical component. (SI unit: joules per particle or joules per mole)*N*_{i}is the number of particles (or number of moles) composing the*i*th chemical component.

This is one form of **Gibbs fundamental equation**. In the infinitesimal expression, the term involving the chemical potential accounts for changes in Gibbs free energy resulting from an influx or outflux of particles. In other words, it holds for an open system. For a closed system, this term may be dropped.

Any number of extra terms may be added, depending on the particular system being considered. Aside from mechanical work, a system may, in addition, perform numerous other types of work. For example, in the infinitesimal expression, the contractile work energy associated with a thermodynamic system that is a contractile fiber that shortens by an amount −d*l* under a force *f* would result in a term *f*d*l* being added. If a quantity of charge −d*e* is acquired by a system at an electrical potential Ψ, the electrical work associated with this is −Ψd*e*, which would be included in the infinitesimal expression. Other work terms are added on per system requirements.

Each quantity in the equations above can be divided by the amount of substance, measured in moles, to form *molar Gibbs free energy*. The Gibbs free energy is one of the most important thermodynamic functions for the characterization of a system. It is a factor in determining outcomes such as the voltage of an electrochemical cell, and the equilibrium constant for a reversible reaction. In isothermal, isobaric systems, Gibbs free energy can be thought of as a "dynamic" quantity, in that it is a representative measure of the competing effects of the enthalpic and entropic driving forces involved in a thermodynamic process.

The temperature dependence of the Gibbs energy for an ideal gas is given by the Gibbs-Helmholtz equation and its pressure dependence is given by:

if the volume is known rather than pressure then it becomes:

or more conveniently as its chemical potential:

In non-ideal systems, fugacity comes into play.

Read more about this topic: Gibbs Free Energy

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