Coupling between Alfven wave and Kelvin-Helmholtz waves in the low latitude boundary layer

Kim, Eun-Hwa ; Johnson, Jay; Nykyri, Katariina
Issue date: 2021
Rights:
Creative Commons Attribution 4.0 International (CC BY)
Cite as:
Kim, Eun-Hwa, Johnson, Jay, & Nykyri, Katariina. (2021). Coupling between Alfven wave and Kelvin-Helmholtz waves in the low latitude boundary layer [Data set]. Princeton Plasma Physics Laboratory, Princeton University. https://doi.org/10.11578/1888256
@electronic{kim_eunhwa_2021,
  author      = {Kim, Eun-Hwa and
                Johnson, Jay and
                Nykyri, Katariina},
  title       = {{Coupling between Alfven wave and Kelvin-
                Helmholtz waves in the low latitude boun
                dary layer}},
  publisher   = {{Princeton Plasma Physics Laboratory, Pri
                nceton University}},
  year        = 2021,
  url         = {https://doi.org/10.11578/1888256}
}
Description:

The Kelvin-Helmholtz (KH) instability of magnetohydrodynamic surface waves at the low latitude boundary layer is examined using both an eigenfrequency analysis and a time-dependent wave simulation. The analysis includes the effects of sheared flow and Alfven velocity gradient. When the magnetosheath flows are perpendicular to the ambient magnetic field direction, unstable KH waves that propagate obliquely to the sheared flow direction occur at the sheared flow surface when the Alfv\'en Mach number is higher than an instability threshold. Including a shear transition layer between the magnetosphere and magnetosheath leads to secondary KH waves (driven by the sheared flow) that are coupled to the resonant surface Alfven wave. There are remarkable differences between the primary and the secondary KH waves including wave frequency, the growth rate, and the ratio between transverse and the compressional component. The secondary KH wave energy is concentrated near the shear Alfven wave frequency at the magnetosheath with a lower frequency than the primary KH waves. Although the growth rate of the secondary KH waves is lower than the primary KH waves, the threshold condition is lower, so it is expected that these types of waves will dominate at lower Mach number. Because the transverse component of the secondary KH waves is stronger than the primary KH waves, more efficient wave energy transfer from the boundary layer to the inner magnetosphere is also predicted.

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