loading page

Investigation of Kinetic Ballooning Instability in 2D Harris Sheet Equilibrium with Finite Normal BZ Field.
  • +3
  • Ikram Muhammad,
  • Abdullah Khan,
  • Abdullah Zafar,
  • Majid Khan,
  • Abid Ali Abid,
  • Amin Esmaeili
Ikram Muhammad
Hazara University, 21300 Mansehra, Pakistan

Corresponding Author:[email protected]

Author Profile
Abdullah Khan
CAS Key Laboratory of Geospace Environment, Department of Geospace and Planetary Science, University of Science and Technology of China, Hefei, Anhui 230026, China
Author Profile
Abdullah Zafar
Yannan Observatories, Chinese Academy of Sciences, Kunming, Yannan 650216, PR China
Author Profile
Majid Khan
Quaid-i-Azam University
Author Profile
Abid Ali Abid
University of Science and Technology of China Hefei, Anhui 230026, P. R. China
Author Profile
Amin Esmaeili
Space Physics Group, Department of Physics, Faculty of Science, Yazd University, Yazd 8919-741, Iran
Author Profile

Abstract

Substorm onset is believed to be a fundamental process for magnetic and plasma energy transport in both magnetosphere and ionosphere.Ballooning instability is one of the key trigger mechanism to examine the substorm onset scenario in the near-Earth plasma sheet. For this subject,the kinetic ballooning instability (KBI) in the near-Earth magnetotail is analyzed using the general type of two-dimensional (2D) kinetic sheet equilibria, the so-called generalized Harris sheet equilibria. The kinetic ballooning mode is unstable in the intermediate range of perpendicular wave number (ky) and the equatorial beta (eq). The growth rate of the ballooning mode reduces signicantly with the increase in electron and ion temperatures ratio (Te=Ti) and wave number ky. The kinetic ballooning mode is found to be most unstable in the thin current sheet region at the equatorial location xe ~(9-10)RE, where the ballooning drive term (βeq/LpRc) is dominant on stiffening effect due to the minimum in the normal magnetic field Bz there.Because of the stabilizing effect through the field line stiffening factor and the strong field line stabilization, the ballooning mode is stable close to the Earth and becomes marginally unstable away from the Earth. This suggests the local current sheet thinning may be also an effective trigger mechanism for the onset of ballooning instability in the near-Earth magnetotail.