Conveners
1.2 Computational Plasma Physics I
- John W. Luginsland (Confluent Sciences)
Description
Session Chair: John Luginsland
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Prof. Lay Kee Ang (Singapore University of Technology and Design)24/06/2019, 09:451.2 Computational Plasma Physics;Oral
In numerical modeling, it is common to solve coupled differential equations in one-, two- or three- dimensions (1D, 2D, or 3D) with corresponding boundary conditions. For some complicated objects, the dimension may be strictly 1D, 2D or 3D, where the normal computational approach may be expensive. By using fractional models that had been developed mathematicians, the complicated object is...
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Jeffrey Haack (Los Alamos National Laboratory)24/06/2019, 10:001.2 Computational Plasma Physics;Invited
We derive a conservative multispecies BGK model that follows the spirit of the original, single species BGK model by ensuring pairwise conservation of momentum and kinetic energy and that the model satisfies Boltzmann’s H-Theorem. The derivation emphasizes the connection to the Boltzmann operator, which allows for direct inclusion of information from a molecular dynamics validated effective...
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Dr Andrew Chap (Tech-X Corporation)24/06/2019, 10:451.2 Computational Plasma Physics;Oral
Speed-limited particle-in-cell simulation (SLPIC) is a method of increasing the time-step in a PIC simulation by slowing down the fastest particles in such a way that the end state of the simulation is unaffected, while significantly reducing the number of time-steps required to reach this end state. SLPIC is useful when the simulation requires a kinetic treatment of fast particles (e.g....
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Dr Yangyang Fu (Michigan State University)24/06/2019, 11:001.2 Computational Plasma Physics;Oral
Similarity laws are often employed when the characteristics of two or more discharge systems are compared. The classical similarity laws were previously validated and applied for weakly ionized plasma discharges [1, 2]. However, similarity relations are not valid for all plasma regimes [3, 4]. Especially for strongly ionized regimes, scaling laws are not well understood. In this study, we...
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Dr Andrew Fierro (Sandia National Laboratories)24/06/2019, 11:301.2 Computational Plasma Physics;Either
A particle-in-cell (PIC), direct simulation Monte Carlo (DSMC) simulation is presented for a coaxial low-temperature plasma. Depending on the ratio of the area of the electron collector ($A_e$) to ion collector ($A_w$), different sheath structures may form$^1$. In the case of the $A_e / A_w < \sqrt{2.3m_e / m_i}$ where $m_e$ is and $m_i$ are the electron and ion mass respectively, an electron...
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