Nakanotani Masaru, Camata Renato P, Arslanbekov Robert R, Zank Gary P
Center for Space Plasma and Aeronomic Research (CSPAR), University of Alabama in Huntsville, Huntsville, Alabama 35805, USA.
Department of Physics, University of Alabama at Birmingham, Birmingham, Alabama 35294, USA.
Phys Rev E. 2022 Apr;105(4-2):045209. doi: 10.1103/PhysRevE.105.045209.
Although collisional electrostatic shock waves have been investigated extensively via theory, simulations, and experiments, there are comparatively few studies about collisional magnetized shock waves. We investigate collisional magnetized shocks by performing one-dimensional full particle-in-cell simulations that incorporate ion-ion, electron-electron, and ion-electron Coulomb collisions, for perpendicular and quasiparallel shock waves. The effect of Coulomb collisions is to drive a shock wave into a more laminar state. For a perpendicular shock, the magnetic overshoot becomes small because the electron pressure perpendicular to the magnetic field is isotropized and decreases due to electron-electron collisions. For the quasiparallel case, we find that ion-electron collisions severely suppress the standing whistler wave, which is present in the form of large amplitude waves in a collisionless shock wave.
尽管碰撞静电激波已通过理论、模拟和实验进行了广泛研究,但关于碰撞磁化激波的研究相对较少。我们通过进行一维全粒子模拟来研究碰撞磁化激波,该模拟纳入了离子 - 离子、电子 - 电子和离子 - 电子库仑碰撞,用于垂直和平行激波。库仑碰撞的作用是将激波驱动到更层流的状态。对于垂直激波,垂直于磁场的电子压力各向同性化,并且由于电子 - 电子碰撞而减小,导致磁超调变小。对于准平行情况,我们发现离子 - 电子碰撞严重抑制了驻波哨声波,该波在无碰撞激波中以大振幅波的形式存在。