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A new fourth-order six-stage Runge Kutta numerical integrator that requires 2N-storage (N is the number of degrees of freedom of the system) with low dissipation and dispersion and a relatively large stability interval is proposed.
In fact the stability interval is a subset of converges interval.
The EI is usually selected as the value corresponding to the stability interval in this plot.
Thus, we can control the stability interval by sensitive parameters which have important implications for practical applications.
The optimal step size for the FxLMS algorithm lies in the middle of stability interval [43, 44].
Next, we compare stability intervals I τ M ( h ) with the stability interval of (3), which we denote I τ ∗ = ( − π / ( 2 τ ), 0 ).
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The wall temperature stability intervals of these modes changed with the CO H2 ratio.
To achieve this goal we use the stability intervals based on PROMETHEE II (Preference Ranking Organization METHod for Enrichment of Evaluations) as weight constraints in DEA.
Optimal methods with respect to large stability intervals on the imaginary axis and with respect to the eigenvalue spectra of the underlying pseudospectral discretizations are developed.
We emphasize that the stability regions are captured just by stability intervals for values of parameter b.
Next assertion describes the relation between stability intervals I τ M ( h ) with respect to stepsize h.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com