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To prevent instabilities during simulations, a highly efficient discrete calculation scheme is presented with a variable time step.
The finite volume method is used in discrete calculation, and the SIMPLE algorithm is applied in continuity equation, momentum equation, energy equation and turbulent kinetic energy equation when solving the control.
where Δ f is the frequency spacing of the discrete calculation; N p is the number of intervals in order to approximate the integral function.
It is thus natural to suppose that this result can be found easily and more simply than the earlier discrete calculation, and that it would provide a more suitable vehicle for further development of the model, for example, in considering the shape of the interface on the reaction rates.
Following the results of the annexe (Section 9), we can turn the considered discrete calculation into a continuous case calculation: z ( i ) = G 2 π σ exp ( - j μ r 0 ) ∫ Δ r = - ∞ Δ r = + ∞ exp ( - j μ Δ r ) exp - Δ r 2 2 σ 2 d ( Δ r ) (5).
In particular, with these methods, the discrete calculation of an OG test requires many mutations in the exact same hotspots to reach statistical significance.
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This kind of formulation offers the possibility of carrying out better simulations of material properties than the discrete calculations, and with both larger length scales and longer times.
Discrete calculations were carried out with a rigid and very rough retaining wall, undergoing passive and active horizontal translation, rotation about the top and rotation about the toe.
Discrete time scheduling is preferred over floating point scheduling, because discrete calculations do not suffer from rounding errors.
This leads us to working on discrete calculations, whereas there is also rich work on continuous fractional ones.
The radius function to obtain curves is calculated from approximated piecewise curves, which is much more noise free than discrete radius calculation.
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