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The theoretical background of this method is offered by the classical equilibrium theory of adsorption.
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By adopting the classical equilibrium moment or setting the so-called "magic" parameter to 1/12, the anisotropic term can be eliminated, which is found from the present third-order analysis and also validated numerically.
Recently, many authors have generalized the classical equilibrium problem introduced in [22] by introducing 'perturbation' to the function Θ.
At the same time, thermodynamics developed from the classical equilibrium theory to theories not limited by equilibrium, space or time homogeneity.
If in (1.1), then GEP(1.1) reduces to the classical equilibrium problem (EP) and is denoted by, that is, (1.3).
Note that the problem (1.2) is the classical equilibrium problem and we denote its solution set by (EP(F_{1})).
To move on, we recall the classical equilibrium problem, and classical Nash equilibrium problem (NEP) [21].
For this the classical, equilibrium, or bifurcation approach is taken.
If (lambda=1), then the generalized equilibrium problem (1.2) reduces to the classical equilibrium problem (1.1).
Thus, the so-called generalized mixed equilibrium problem reduces to the classical equilibrium problem for the bifunction Γ.
Then G n coincides with the classical equilibrium problem and satisfies (A1 - A4).
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