2018
DOI: 10.1063/1.5049237
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Transport equations in magnetized plasmas for non-Maxwellian distribution functions

Abstract: Non-Maxwellian distribution functions are frequently observed in space and laboratory plasmas in (quasi-) stationary states, usually resulting from long-range nonlinear wave-particle interactions [P. H. Yoon, Phys. Plasmas 19, 012304 (2012)]. Since the collisional transport described by the Boltzmann equation with the standard collisional operator implies that the plasma distribution function evolves inexorably towards a Maxwellian, the description of the transport for stationary states outside of equilibrium… Show more

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Cited by 5 publications
(3 citation statements)
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“…Let us end this section by mentioning other selected entropic applications beyond BG in physics: long-range interacting many-body classical Hamiltonian systems (XY model [ 90 , 91 , 92 , 93 , 94 , 95 , 96 , 97 ], Heisenberg model [ 98 , 99 , 100 ], Fermi–Pasta–Ulam (FPU) model [ 101 , 102 , 103 , 104 ]) (see [ 105 , 106 ] for earlier related approaches of the original FPU model and also [ 107 ], where the existence of non-Maxwellian compact-support momenta distributions are detected for special initial conditions); quantum-entangled low-dimensional Hamiltonian systems [ 108 , 109 , 110 ]; plasma physics [ 111 , 112 , 113 , 114 , 115 ]; turbulence [ 87 , 116 ]; astrophysics, cosmology, and black holes [ 89 , 117 , 118 , 119 , 120 , 121 , 122 ]; nonlinear dynamical systems [ 123 , 124 , 125 , 126 , 127 , 128 ]; nonlinear quantum mechanics [ 129 , 130 , 131 , 132 ]; anomalous diffusion, type II superconductors, and repulsive short-range interacting systems with overdamping […”
Section: Non-boltzmannian Entropy Measures and Distributionsmentioning
confidence: 99%
“…Let us end this section by mentioning other selected entropic applications beyond BG in physics: long-range interacting many-body classical Hamiltonian systems (XY model [ 90 , 91 , 92 , 93 , 94 , 95 , 96 , 97 ], Heisenberg model [ 98 , 99 , 100 ], Fermi–Pasta–Ulam (FPU) model [ 101 , 102 , 103 , 104 ]) (see [ 105 , 106 ] for earlier related approaches of the original FPU model and also [ 107 ], where the existence of non-Maxwellian compact-support momenta distributions are detected for special initial conditions); quantum-entangled low-dimensional Hamiltonian systems [ 108 , 109 , 110 ]; plasma physics [ 111 , 112 , 113 , 114 , 115 ]; turbulence [ 87 , 116 ]; astrophysics, cosmology, and black holes [ 89 , 117 , 118 , 119 , 120 , 121 , 122 ]; nonlinear dynamical systems [ 123 , 124 , 125 , 126 , 127 , 128 ]; nonlinear quantum mechanics [ 129 , 130 , 131 , 132 ]; anomalous diffusion, type II superconductors, and repulsive short-range interacting systems with overdamping […”
Section: Non-boltzmannian Entropy Measures and Distributionsmentioning
confidence: 99%
“…Определение q -гидродинамических параметров. Энтропия Тсаллиса влечёт за собой не только обобщение статистической физики и термодинамики, но и обобщение физической кинетики и гидродинамики (Oliveira, Galvao, 2018). Простейшей макроскопической величиной является q -плотность числа частиц, которая определяется соотношением…”
Section: Q-гидродинамикиunclassified
“…The aforementioned observations are examples of kinetic effects that move the velocity distribution away from a Maxwellian function. While fluid-like descriptions of continua with non-Maxwellian distribution functions is an actively researched field [24,25], a generic fluid description of a non-equilibrium continuum is lacking and may very well not exist, although some success was found in certain limit cases. For limit cases where the drive towards a single-Maxwellian velocity distribution function is sufficiently small, however, the distribution function may be described by a multi-Maxwellian distribution function, i.e., a sum of single-Maxwellian distribution functions, if the sources each follow a Maxwellian distribution function.…”
Section: Introductionmentioning
confidence: 99%