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A Boltzmann formulation of the steady state equation was then fitted to the estimates to derive baseline parameter values for the slopes (sm and sh) and half-peak voltages (V2m, V2h).
It is inspired on geometric arguments on the steady state equation, involving tangent adsorption and surface reaction rate curves as a function of surface coverage, which represent the limiting cases of rate multiplicity.
For systems reducible to a single equation the criterion derived for global stability is the same as one of the conditions for uniqueness derived from the steady state equation.
We begin by considering the eigenvalue problem of the steady state equation of (2.1).
Now we go back to study competition system (2.8) and its steady state equation (2.9).
At steady state, Equation (15) produces the solution ( ∂ T s, st ∂ r * ) r w * = − q 0 k f (16).
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The steady state equations are linearized using Galerkin's method.
The system model includes non-linear steady state equations and linear vibrational equations about steady state.
We solve the steady state equations by advancing in time using a backward Euler (BE) scheme.
In The steady state equations section, we construct the set of steady state equations by introducing the supplementary variable corresponding to elapsed service time.
The set of steady state equations governing the model is constructed in 'Governing equations' section.
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