scholarly journals Modeling the Transport of Nonthermal Particles in Flares Using Fokker–Planck Kinetic Theory

2020 ◽  
Vol 902 (1) ◽  
pp. 16
Author(s):  
Joel C. Allred ◽  
Meriem Alaoui ◽  
Adam F. Kowalski ◽  
Graham S. Kerr
Author(s):  
B. Mokdad ◽  
A. Ammar ◽  
F. Chinesta

In this work, the model of Doi-Edwards with independant alignment approximation describing the dynamics of polymer melts is simulated. The main aim of this work is the analysis of some new simulation techniques operating on the Fokker-Planck equation related to that model. For this purpose we consider the kinetic theory description of the Doi-Edwards model, implemented in the 2D and 3D cases under shear and elongational flows. The Fokker Planck equation which governs the evolution of the distribution function involves two variables: the tube orientation (described by a unit vector defining the unit surface in 3D and the unit circle in 2D) and the coordinate that locates the segment tube on the molecular chain, taking values in the unit interval. To separate both variables during the problem resolution we make use of the Alternating Direction Implicit method (ADI) which allows reducing the computation time and efforts. A model reduction technique is also proposed and analyzed. It consists of considering an optimal representation basis which is constructed during the problem resolution. Thus, a reduced number of approximation functions, now defined in the whole domain, are enough to describe the solution evolution during the entire time interval considered in the simulation, with significant CPU time savings.


2011 ◽  
Vol 4 (2) ◽  
pp. 401-426 ◽  
Author(s):  
José Antonio Alcántara ◽  
◽  
Simone Calogero ◽  

1972 ◽  
Vol 8 (3) ◽  
pp. 357-374 ◽  
Author(s):  
George Vahala

The kinetic theory of a two-dimensional one-species plasma in a uniform d.c. magnetic field is investigated in the small plasma parameter limit. The plasma consists of charged rods interacting through the logarithmic Coulomb potential. Vahala & Montgomery earlier derived a Fokker –;Planck equation for this system, but it contained a divergent integral, which had to be cut-off on physical grounds. This cut-off is compared to the standard cut-off introduced in the two-dimensional unmagnetized Fokker –;Planck equation. In the small plasma parameter limit, it is shown (under the assumption that for large integer n, γn/γn+1 = O(np), with p < 2, where γn = ωn −nΩ. with ωn the nth. Bernstein mode and Q the electron gyro frequency) that the Balescu-Lenard collision term is zero in the long time average limit if one considers only two-body interactions. The energy transfer from a test particle to an equilibrium plasma is discussed and also shown to be zero in the long time average limit. This supports the unexpected result of zero Balescu-Lenard collision term.


1994 ◽  
Vol 68 (2) ◽  
pp. 239-262 ◽  
Author(s):  
Pierre Degond ◽  
Brigitte Lucquin-Desreux

Entropy ◽  
2019 ◽  
Vol 21 (9) ◽  
pp. 841 ◽  
Author(s):  
Giorgio Kaniadakis ◽  
Antonio M. Scarfone

By using the kinetic interaction principle, the quons statistics in the framework of kinetic theory is introduced. This is done by properly generalizing the inclusion/exclusion principle of standard boson and fermion statistics within a nonlinear classical model. The related nonlinear Fokker-Planck equation is introduced and the corresponding steady distribution describing quons statistics of type I and type II is derived.


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