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This is due to the NAS-SC model approximation described above.
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The shedding model was formulated to work with the full TMDD model originally described by Mager and Jusko and also with the quasi-steady-state (QSS) approximation described by Gibiansky et al. Similar results were obtained using the extended full TMDD model and the QSS approximation (see Supplementary Material).
The graph is obtained using a convex approximation described here.
Various levels of model approximations to describe mechanical and thermodynamic properties are tested and critically evaluated.
The original Novak and Tyson model [ 19] which was our point of departure corresponds to (3) (4) (5) (6) (7) (8) (9) (10 1112) (13) (14) (14) where (15) The default parmater values corresponding to the wild-type cell are (16) The hybrid model approximation process is described in [ 15] and summarized further down.
A good approximation model describing the chemical processes on the basis of classical thermodynamics is also proposed.
This model approximation process is summarized in the Methods.
The exchange correlation potential in our model is described by the Perdew Zunger functional of the local density approximation (LDA.PZ).
P values greater than 0.05 and an adjusted goodness-of-fit (AGFI) greater than 0.90 with a root mean square error of approximation (RMSEA) of 0.05 (0.08) or less indicated that the model adequately described the observed data.
Using approximation (4), our model can be described as follows.
McCree's equation is an approximation that the model can describe; it is mistaken to interpret his second coefficient as a maintenance requirement.
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