2016
DOI: 10.1016/j.asr.2015.09.013
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The Kelvin–Helmholtz instability under Parker-Spiral Interplanetary Magnetic Field conditions at the magnetospheric flanks

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Cited by 17 publications
(23 citation statements)
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“…For example, the best comparison with data and simulation in Nykyri, 2006-event was obtained when k-vector was tilted by 35 degrees from the initial shear flow plane. This result was later confirmed with 3-D simulations of the same event by Adamson et al (2016). Furthermore, the onset criteria is derived assuming infinitely thin boundary, and the real magnetopause has a finite thickness.…”
Section: Khi Under Different Imf Conditionssupporting
confidence: 58%
“…For example, the best comparison with data and simulation in Nykyri, 2006-event was obtained when k-vector was tilted by 35 degrees from the initial shear flow plane. This result was later confirmed with 3-D simulations of the same event by Adamson et al (2016). Furthermore, the onset criteria is derived assuming infinitely thin boundary, and the real magnetopause has a finite thickness.…”
Section: Khi Under Different Imf Conditionssupporting
confidence: 58%
“…Adamson et al () and Nykyri et al () demonstrated using Cluster data and 2‐D and 3‐D MHD simulations that the k vector of the KHI does not need to be aligned with maximum velocity shear but that KH waves can propagate with an angle from the equatorial plane to minimize the tangential magnetic field tension to maximize the onset criteria. Cluster data during the KH event and 2‐D MHD simulations were consistent with the propagation angle of 35° (Nykyri et al, ), whereas the 3‐D investigation of the angle maximizing the onset criteria was 48° and corresponding angle observed in 3‐D MHD simulation was 41° (Adamson et al, ). To explore this statistically for the present set of KH events, equation was applied in order to determine the propagation angle with respect to the shear flow velocity that maximized the onset criteria for each event.…”
Section: Resultsmentioning
confidence: 99%
“…Even if this model is oversimplified, it yet gives some insights about the tilt angle of oblique modes observed in the 3‐D compressible simulations starting from 1‐D equilibria with ℓ ⋆ ≠0 (Adamson et al, ; Nakamura & Daughton, ). A moderate discrepancy between the predicted ϑ max and that observed in the simulations is related to the fact that the simplified model underestimates the role of the magnetic field inside the shear layer ( false|xfalse|), where the mode amplitude is larger, while overestimates its importance in the two asymptotic region (| x |≫ ℓ ⋆ ).…”
Section: Large‐scale Dynamics Of Kh Vorticesmentioning
confidence: 99%