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These microstructure-derived simulations achieve a good agreement with experimental data.
Current global simulations achieve resolutions, in the turbulent region, comparable to those of 303-703 lattines in periodic domains (Couch and O'Connor 2014; Couch and Ott 2015; Abdikamalov et al. 2015).
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This assumption is valid for our simulations because all simulations achieved a fairness index of 0.95.
The model is implemented in Matlab and tested in simulations achieving successful results.
The designed controller is implemented in Matlab/SIMULINK and tested in simulations achieving successful results.
Simulations achieved with this apparatus demonstrated small magnitudes of error in actuator position and highly repeatable flexion pathways with the specimens positioned in vertical, varus, and valgus orientations.
In the context of CCSN simulations this means that the large scale kinetic energy, a crucial quantity for the dynamics of the explosion (Couch and Ott 2015), can be faithfully captured even with simulations achieving modest Reynolds numbers.
During droplet growth in LBM simulations, achieved by increasing the density within the droplet, the contact line initially advances in the direction parallel to the stripes, therewith increasing its aspect ratio.
High voltage measurements in the time domain are performed to characterize the amplitude and the shape of the nsPEF within the exposition channels and compared to numerical simulations achieved with a 3D Finite-Difference Time-Domain code.
For all simulations achieved in this work, the ODE equations were numerically integrated by the solver ode23s built in Matlab.
The proportion of simulations achieving critical P-values of 10−3, 10−4, 10−5 and 10−6 was measured and the average −log(p) was calculated.
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