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A Comparison between the Discontinuous Galerkin Method and the High Resolution Wave Propagation Algorithm for the Full Two-Fluid Plasma Model
Bhuvana Srinivasan
,
Uri Shumlak
,
Nathan Kutz
Published
2006
in
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Abstract
A Comparison between the Discontinuous Galerkin Method and the High Resolution Wave Propagation Algorithm for the Full Two-Fluid Plasma Model
Topics
8 Figures and Tables
Table 6.1: Strain Waves problem: Some computational times for the wave propagation algorithm and the RKDG algorithm with both characteristic-based and component-based limiters for several grid resolutions.
Figure 6.12: Electron Acoustics problem: u Vs x for 100 cells with cs = √
Figure 6.14: Electron Acoustics problem: u Vs x for 100 and 512 cells with cs = √
Figure 6.16: Z-pinch Two Fluid Equilibrium initial conditions for electron density, zdirection momentum and pressure; ion density and pressure; and azimuthal magnetic field.
Table 6.2: Dispersive Euler Electron Acoustic Wave problem: Some computational times for the wave propagation algorithm and the RKDG algorithm with both characteristic-based and component-based limiters for several grid resolutions.
Table 6.3: Two-Fluid Plasma Model Radial Z-Pinch problem: Some computational times for the wave propagation algorithm and the RKDG algorithm with both characteristic-based and component-based limiters for several grid resolutions.
Figure 6.8: Electron Acoustics problem: Plots are of u Vs x for 40 cells with cs = √
Figure 6.9: Electron Acoustics problem: Plots are of u Vs x for 120 cells with cs = √
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