Kinetic Vlasov simulations of contact discontinuities
- 1Nagoya University, ISEE, Nagoya, Japan (taka.umeda@nagoya-u.jp)
- 2University of Toyama, Graduate School of Science and Engineering for Education, Toyama, Japan (d1771002@ems.u-toyama.ac.jp)
- 3University of Toyama, Faculty of Human Development, Toyama, Japan (nariyuki@edu.u-toyama.ac.jp)
The stability of contact discontinuities formed by the relaxation of two Maxwellian plasmas with different number densities but the same plasma thermal pressure is studied by means of a one-dimensional electrostatic full-Vlasov simulation. Our simulation runs with various combinations of ion-to-electron ratios of the high-density and low-density regions showed that transition layers of density and temperature without jump in the plasma thermal pressure are obtained when the electron temperatures in the high-density and low-density regions are almost equal to each other. However, the stable structure of the contact discontinuity with a sharp transition layer on the Debye scale is not maintained. It is suggested that non-Maxwellian velocity distributions are necessary for the stable structure of contact discontinuities. A direct comparison between full- and hybrid-Vlasov simulations is also made.
How to cite: Umeda, T., Tsujine, N., and Nariyuki, Y.: Kinetic Vlasov simulations of contact discontinuities, EGU General Assembly 2020, Online, 4–8 May 2020, EGU2020-48, https://doi.org/10.5194/egusphere-egu2020-48, 2019