Abstract:In the present work we develop a 1d3v (1D in space and 3D in velocity) kinetic Particle-in-cell model of the magnetised plasma-wall transition layer, where the charged and neutral particle dynamics and interaction between them is included in a fully self-consistent way. The plasma-surface interactions are described via fixed emission coefficients for the secondary particles. We obtained different profiles of plasma and neutral particles and cross-checked classical boundary conditions, which are usually formula… Show more
“…Interesting to note that this number has been derived few decades ago when the number of simulation time steps was typically of the order of N t ∼ 10 4 . From (15) we obtain ω = ω 0 (1 − 1/24(ω 0 ∆t)…”
Section: Accuracy and Stability Of The Particle Movermentioning
This paper is the first in a series of three papers to summarize the recent work of an European-wide collaboration which is ongoing since about one decade using Particle-in-Cell (PIC) methods in low temperature plasma physics. In the present first paper the main aspects of this computational technique will be presented. In the second paper, an overview of applications in low-temperature plasma modelling will be given, whereas the third part will put emphasis on the specific results of modelling ion thrusters.
“…Interesting to note that this number has been derived few decades ago when the number of simulation time steps was typically of the order of N t ∼ 10 4 . From (15) we obtain ω = ω 0 (1 − 1/24(ω 0 ∆t)…”
Section: Accuracy and Stability Of The Particle Movermentioning
This paper is the first in a series of three papers to summarize the recent work of an European-wide collaboration which is ongoing since about one decade using Particle-in-Cell (PIC) methods in low temperature plasma physics. In the present first paper the main aspects of this computational technique will be presented. In the second paper, an overview of applications in low-temperature plasma modelling will be given, whereas the third part will put emphasis on the specific results of modelling ion thrusters.
“…Atomic/molecular collisions in BIT1 code are performed via nonlinear binary null-collision method introduced in [14]. The collision operator consists of two steps, finding of collision pairs and the collision itself (for details see [14]). Collection and derivation of the corresponding collision crosssections represents a complex task and will be discussed in details.…”
Section: Implementation Of Recombination Processesmentioning
confidence: 99%
“…In the present paper we consider a qualitative model keeping simulated plasma edge as simple as possible: the model includes electrons, deuterium ions and atoms, impurity atoms and ions (C,C + ) and nonlinear interaction between them: elastic, excitation, ionization, charge exchange and recombination collisions (e.g. see [13,14]). Plasma recycling coefficients at the divertors are assumed to be 1.…”
Implementation of self-consistent model of plasma recombination into the BIT1 PIC code and the simulation of detached SOL plasma are described. Our simulations indicate that in a strongly recombining plasma edge the sheath properties do not change qualitatively. The most affected parameter is the sheath heat transmission coefficient, which can increase by order of magnitude.
“…In the problems run to date, the time spent in the plasma-neutral collision routines is too small compared with the rest of the code (see section 2.5) to justify the implementation of a more efficient algorithm, e.g., as in [28].…”
Section: Treatment Of Ionization and Charge Exchangementioning
Abstract. An approach to coupling two kinetic particle codes for the simulation of neutral-plasma interactions in magnetic fusion devices is described. The behavior of the neutral atoms and molecules is modeled with a Monte Carlo code. The plasma species are simulated with a particle-in-cell code that integrates the guiding center equations of motion and computes a self-consistent electric field. The coupling algorithm is designed to conserve mass in the neutral-plasma exchanges to statistical accuracy. Although energy is not fully conserved due to the velocity dependence of the charge exchange cross section and the kinetic character of both species, the impact of this non-conservation on the overall simulation is negligible.
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