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For chemical thermodynamics, the global thermodynamic equilibrium condition, GTE, can be stated as follows: The concentrations of the various chemical species in solutions are constant in space and time. The concentrations are specified by the chemical potentials. This definition may be found in the 1970s in the work of Birgeneau, Steiner, and others. In the 1970s, thermodynamic material dispersion theory was developed under the blanket term "reactivity", and Birgeneau's definition was applied to it. A more rigorous definition of chemical thermodynamic equilibrium was proposed in 2000 by I.L. Ryabov ([35,36] and ).
For nuclear thermodynamics, a definition involving nuclear partition functions appears in the work of Bernoulli and Baym ( and ). A definition involving fission and fusion partition functions appears in the work of Delbrück and M.R. Zwanzig ( and ). A definition incorporating statistical mechanics, multiphase thermodynamics and macroscopic thermodynamics appears in the work of Adler and Baldwin ( and ).
In the 1970s, Zwanzig developed a theory of non-equilibrium relaxation that uses the concept of local thermodynamic equilibrium, and this has been emphasized by several contemporary writers, including Duval and Zwanzig  and Rössler [45, 46]
For biochemistry, a definition involving the application of Boltzmann statistics to an appropriate ensemble is given by P. Blake. Another definition of chemical equilibrium may be found in the works of Duval.
The type of equilibrium that applies to a theoretical system of ideal gases in an infinite container, and to an actual system of ideal gases in a container of finite volume at constant absolute temperature and pressure is defined as ``grand-canonical thermodynamic equilibrium''.
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