Weak solutions of the relativistic Vlasov–Maxwell system with external currents
The time evolution of a collisionless plasma is modeled by the relativistic Vlasov–Maxwell system which couples the Vlasov equation (the transport equation) with the Maxwell equations of electrodynamics. We consider the case that the plasma consists of N particle species, the particles are located i...
Saved in:
Published in | Mathematical methods in the applied sciences Vol. 44; no. 6; pp. 4770 - 4801 |
---|---|
Main Author | |
Format | Journal Article |
Language | English |
Published |
Freiburg
Wiley Subscription Services, Inc
01.04.2021
|
Subjects | |
Online Access | Get full text |
Cover
Loading…
Summary: | The time evolution of a collisionless plasma is modeled by the relativistic Vlasov–Maxwell system which couples the Vlasov equation (the transport equation) with the Maxwell equations of electrodynamics. We consider the case that the plasma consists of N particle species, the particles are located in a bounded container
Ω⊂ℝ3, and are subject to boundary conditions on ∂Ω. Furthermore, there are external currents, typically in the exterior of the container, that may serve as a control of the plasma if adjusted suitably. We do not impose perfect conductor boundary conditions for the electromagnetic fields but consider the fields as functions on whole space
ℝ3 and model objects, that are placed in space, via given matrix‐valued functions ε (the permittivity) and μ (the permeability). A weak solution concept is introduced and existence of global‐in‐time solutions is proved, as well as the redundancy of the divergence part of the Maxwell equations in this weak solution concept. |
---|---|
Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
ISSN: | 0170-4214 1099-1476 |
DOI: | 10.1002/mma.7070 |