PERPENDICULAR ION HEATING BY LOW-FREQUENCY ALFVÉN-WAVE TURBULENCE IN THE SOLAR WIND
By B. Chandran, Bo Li, B. Rogers, E. Quataert, K. Germaschewski. 2010
251 citations recorded by the source corpus.
We consider ion heating by turbulent Alfvén waves (AWs) and kinetic Alfvén waves (KAWs) with wavelengths (measured perpendicular to the magnetic field) that are comparable to the ion gyroradius and frequencies ω smaller than the ion cyclotron frequency Ω. We focus on plasmas in which β ≲ 1, where β is the ratio of plasma pressure to magnetic pressure. As in previous studies, we find that when the turbulence amplitude exceeds a certain threshold, an ion's orbit becomes chaotic. The ion then interacts stochastically with the time-varying electrostatic potential, and the ion's energy undergoes a random walk. Using phenomenological arguments, we derive an analytic expression for the rates at which different ion species are heated, which we test by simulating test particles interacting with a spectrum of randomly phased AWs and KAWs. We find that the stochastic heating rate depends sensitively on the quantity ε = δvρ/v⊥, where v⊥ (v∥) is the component of the ion velocity perpendicular (parallel) to the background magnetic field B0, and δvρ (δBρ) is the rms amplitude of the velocity (magnetic-field) fluctuations at the gyroradius scale. In the case of thermal protons, when ε ≪ εcrit, where εcrit is a constant, a proton's magnetic moment is nearly conserved and stochastic heating is extremely weak. However, when ε>εcrit, the proton heating rate exceeds half the cascade power that would be present in strong balanced KAW turbulence with the same value of δvρ, and magnetic-moment conservation is violated even when ω ≪ Ω. For the random-phase waves in our test-particle simulations, εcrit = 0.19. For protons in low-β plasmas, ε ≃ β−1/2δBρ/B0, and ε can exceed εcrit even when δBρ/B0 ≪ εcrit. The heating is anisotropic, increasing v2⊥ much more than v2∥ when β ≪ 1. (In contrast, at β ≳ 1 Landau damping and transit-time damping of KAWs lead to strong parallel heating of protons.) At comparable temperatures, alpha particles and minor ions have larger values of ε than protons and are heated more efficiently as a result. We discuss the implications of our results for ion heating in coronal holes and the solar wind.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/1319274d733f9e8071ad504d530e5602b38866e0
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In Astronomy and Astrophysics
- C. Chen
- Gregory G. Howes
- E. Quataert
- S. Bale
- B. Chandran
- T. Dennis
- Justin C. Kasper
- William H. Matthaeus
In Nuclear and High Energy Physics
- Gregory G. Howes
- E. Quataert
- C. Chen
- J. Giacalone
- Ramesh Narayan
- F. Yuan
- B. Metzger
- C. Faucher-Giguére
Citations in the corpus
- INCORPORATING KINETIC PHYSICS INTO A TWO-FLUID SOLAR-WIND MODEL WITH TEMPERATURE ANISOTROPY AND LOW-FREQUENCY ALFVÉN-WAVE TURBULENCE (2011, methodology): “Chandran et al. (2010) found thatc2 = 0.34 for randomly phased AWs and KAWs, but conjectured thatc2 is smaller (and hence stochastic heating is more effective) in strong AW/KAW turbulence, because much of the dissipation in strong AW/KAW turbulence occurs within coherent structures in which the…”
- Recent progress in astrophysical plasma turbulence from solar wind observations (2016, background): “ssibilities have been proposed, including ion cyclotron damping (e.g., Coleman 1968; Smith et al. 2012), Landau damping (e.g., Howes et al. 2008; TenBarge & Howes 2013), stochastic heating (e.g., Chandran et al. 2010), entropy cascade (Schekochihin et al. 2009), and reconnection associated mecha”
- Integrated Science Investigation of the Sun (ISIS): Design of the Energetic Particle Investigation (2016, background): “Acceleration via reconnection can be complex, involving direct acceleration, trapping particles in collapsing magnetic islands (Drake et al. 2006), stochastic acceleration (Le Roux et al. 2002; Chandran et al. 2010), and perpendicular betatron acceleration (Dmitruk et al. 2004; Dalena et al. 2014).”
- A prescription for the turbulent heating of astrophysical plasmas (2010, background): “…the solar corona (Velli 2003; Verdini et al. 2009; Chandran 2010), the solar wind (Saito et al. 2008; Valentini et al. 2008; Breech et al. 2009; Cranmer et al. 2009; Lehe et al. 2009; Chandran et al. 2010), and the magnetospheres of the Earth (Chaston et al. 2008) and of other planets (Saur 2004).”