Abstract
In astrophysical plasmas, the magnetic field line random walk (FLRW) plays an important role in guiding particle transport. The FLRW behavior is scaled by the Kubo number R = (b/B0 )(ℓ∥/ ℓ⊥) for rms magnetic fluctuation b, large-scale mean field B0, and coherence scales parallel (ℓ∥) and perpendicular (ℓ⊥) to B0. Here we use a nonperturbative analytic framework based on Corrsin's hypothesis, together with direct computer simulations, to examine the R-scaling of the FLRW for varying B0 with finite b and isotropic fluctuations with ℓ∥/ℓ⊥ = 1, instead of the well-studied route of varying for ℓ∥/ℓ⊥ for b ≪ B0. The FLRW for isotropic magnetic fluctuations is also of astrophysical interest regarding transport processes in the interstellar medium. With a mean field, fluctuations may have variance anisotropy, so we consider limiting cases of isotropic variance and transverse variance (with bz = 0). We obtain analytic theories, and closed-form solutions for extreme cases. Padé approximants are provided to interpolate all versions of theory and simulations to any B0. We demonstrate that, for isotropic turbulence, Corrsin-based theories generally work well, and with increasing R there is a transition from quasilinear to Bohm diffusion. This holds even with bz = 0, when different routes R → ∞ to are mathematically equivalent; in contrast with previous studies, we find that a Corrsin-based theory with random ballistic decorrelation works well even up to R = 400, where the effects of trapping are barely perceptible in simulation results.
| Original language | English |
|---|---|
| Article number | 20 |
| Journal | Astrophysical Journal, Supplement Series |
| Volume | 225 |
| Issue number | 2 |
| DOIs | |
| Publication status | Published - Aug 2016 |
| Externally published | Yes |
Keywords
- diffusion
- magnetic fields
- turbulence
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