Articolo in rivista, 2022, ENG, 10.1017/S0022377822000010
C. Granier, D. Borgogno, D. Grasso, E. Tassi
Université Côte d'Azur, CNRS, Observatoire de la Côte d'Azur, Laboratoire J. L. Lagrange, Boulevard de l'Observatoire, CS 34229, 06304 Nice Cedex 4, France; Istituto dei Sistemi Complessi - CNR and Dipartimento di Energia, Politecnico di Torino, Torino 10129, Italy
The linear and nonlinear evolutions of the tearing instability in a collisionless plasma with a strong guide field are analysed on the basis of a two-field Hamiltonian gyrofluid model. The model is valid for a low ion temperature and a finite ?e. The finite ?e effect implies a magnetic perturbation along the guide field direction, and electron finite Larmor radius effects. A Hamiltonian derivation of the model is presented. A new dispersion relation of the tearing instability is derived for the case ?e = 0 and tested against numerical simulations. For ?e 1 the equilibrium electron temperature is seen to enhance the linear growth rate, whereas we observe a stabilizing role when electron finite Larmor radius effects become more relevant. In the nonlinear phase, stall phases and faster than exponential phases are observed, similarly to what occurs in the presence of ion finite Larmor radius effects. Energy transfers are analysed and the conservation laws associated with the Casimir invariants of the model are also discussed. Numerical simulations seem to indicate that finite ?e effects do not produce qualitative modifications in the structures of the Lagrangian invariants associated with Casimirs of the model
Journal of plasma physics (Print) 88 (1)
strophysical plasmas; plasma instabilities; space plasma physics
Granier Camille, Borgogno Dario, Grasso Daniela
ID: 470998
Year: 2022
Type: Articolo in rivista
Creation: 2022-09-20 11:53:53.000
Last update: 2022-10-03 09:07:17.000
CNR authors
CNR institutes
External IDs
CNR OAI-PMH: oai:it.cnr:prodotti:470998
DOI: 10.1017/S0022377822000010