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The PIC model is implemented in a FORTRAN code, QN3D.
This data will be compared to the results of a PIC model of the experiment.
We review the numerical dispersion relation of the Electromagnetic PIC model.
We have conducted numerical simulation using plasma fluid model and particle-in-cell (PIC) model as well as experimental investigations.
The PIC model is first applied to the problem of an idealized electron avalanche in a non-attaching gas.
The dust is treated with a Particle-In-Cell (PIC) model in which the dust charge varies with time according to the standard dust charging model.
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The simulation results of the two-dimensional RT-PIC model are presented here.
This RT-PIC model incorporates the resonance trapping effect of photons, to the kinetic model of the charged particles when a PD pulse develops inside a narrow channel.
The RT-PIC model presented in this paper successfully reproduces the salient features of light emission during PD pulse within a narrow channel, and yields detailed information about the extent of C C bond breakage.
The transport processes of plasmas in grid systems of krypton (Kr) ion thrusters at different acceleration voltages were simulated with a 3D-PIC model, and the result was compared with xenon (Xe) ion thrusters.
Correction to the drag law that should be employed in Coarse Multi-Phase Particle-in-Cell (MP-PIC) model simulations is examined through a two-step process: separating the coarsening of the fluid and particle phases.
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