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But the component called artificial viscosity is a fiction it is not being used to reliably model the shock.
For transonic flows containing shocks, shock capturing is used to model the shock impulse (the unsteady load due to the harmonic motion of the shock).
For the MES-induced seizure model, the shock level was set at 160 V and the duration was set at 5.4 s with continuous wave under the eighth configuration, using a physiological and pharmacological electronic stimulator (Jinan, Shandong, China).
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These are chosen as to model the shock-turbulence interaction in fluid dynamical systems.
Computational fluid dynamics (CFD) is used to model the shock-wave induced spray process (SISP).
Under this model, the shocks to the cyclical component are as important as the shocks to the trend component.
In this paper, a new approach to predicting shock absorber structure-borne noise is proposed; it consists in modelling the shock absorber and including the main nonlinear phenomena responsible for discontinuities in the response.
We are presently using three separate models to provide these predictions: the Interplanetary Shock Propagation Model (ISPM), the Shock Time of Arrival model (STOA), and the Hakamada-Akasofu-Fry (HAF) model.
However, the structural response and the maximum amplification factors obtained using FE simulations of the complete model are nearly similar to that of the effective model, when the shock loading moves at the critical velocity.
The mathematical model for the shock test machine is created to predict its dynamic performance and analyze its mechanism.
Interpolation model of the shock wave excited by explosion in the ionosphere is obtained.
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