2016
DOI: 10.3847/2041-8205/830/2/l25
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A Stringent Limit on the Amplitude of Alfvénic Perturbations in High-Beta Low-Collisionality Plasmas

Abstract: It is shown that low-collisionality plasmas cannot support linearly polarized shear-Alfvén fluctuations above a critical amplitude d b -B B 0 1 2 , where β is the ratio of thermal to magnetic pressure. Above this cutoff, a developing fluctuation will generate a pressure anisotropy that is sufficient to destabilize itself through the parallel firehose instability. This causes the wave frequency to approach zero, interrupting the fluctuation before any oscillation. The magnetic field lines rapidly relax into a s… Show more

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Cited by 47 publications
(116 citation statements)
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“…Of these stages, (iii) is notably different from the predictions of one-dimensional Landau-fluid (LF) models [9,10]. Figure 2 shows one-dimensional (y-averaged) wave profiles.…”
mentioning
confidence: 91%
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“…Of these stages, (iii) is notably different from the predictions of one-dimensional Landau-fluid (LF) models [9,10]. Figure 2 shows one-dimensional (y-averaged) wave profiles.…”
mentioning
confidence: 91%
“…If these (now stable) fluctuations scatter particles sufficiently strongly, δB z can decay with Δp ≈ −B 2 =4π; if they do not (e.g., if they are resonantly damped [16,29,33]), δB z cannot decrease [9]. The firehose modes' evolution is governed by Δp [12], which varies in space.…”
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confidence: 99%
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“…In fact, it is almost certain that MHD and plasma process play a key role in the underlying transport processes (Squire et al 2016;Kunz et al 2015), and that these processes may be determined on scales as small as the proton gyro-radius, which for typical Virgo ICM parameters would be many orders of magnitude below the spatial scales we are probing here. However, whatever these underlying processes are, the ICM apparently behaves as an inviscid fluid on macroscopic scales.…”
Section: Discussionmentioning
confidence: 99%
“…The division of turbulence into these two regimes is convenient, but the coupling between the two can be highly nontrivial. For example, in high-beta plasmas, kinetic effects can build up a pressure anisotropy that destabilizes largescale, high-amplitude shear Alfvén waves to the firehose instability, conceivably causing a direct transfer of energy from large scales to kinetic scales, bypassing the turbulent cascade (Squire et al 2016(Squire et al , 2017. In a similar vein, in low-beta plasmas with dynamic alignment, the inertial-range energy cascade may be mediated by the collisionless tearing instability at small scales, rather than classical nonlinear eddy interactions.…”
Section: Turbulence Preliminariesmentioning
confidence: 99%