Collisionless Reconnection In Magnetohydrodynamic and Kinetic Turbulence
- OSTI
It has recently been proposed (Loureiro & Boldyrev 2017; Mallet et al. 2017) that the inertial interval in magnetohydrodynamic (MHD) turbulence is terminated at small scales not by a Kolmogorov-like dissipation region, but rather by a new sub-inertial interval mediated by tearing instability. However, many astrophysical plasmas are nearly collisionless so that the MHD approximation is not applicable to turbulence at small scales. In this paper, we propose the extension of the theory of reconnection-mediated turbulence to plasmas which are so weakly collisional that the reconnection occurring in the turbulent eddies is caused by electron inertia rather than by resistivity. We find that the transition scale to reconnection-mediated turbulence depends on the plasma beta and on the assumptions of the plasma turbulence model. However, in all cases analyzed, the energy spectra in the reconnection-mediated interval range from $$E(\k_\perp) dk_\perp \propto k_\perp^{-8/3} dk_\perp$$ to $$E(k_\perp) dk_\perp \propto k_\perp^{-3} dk_\perp$$.
- Research Organization:
- Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States). Plasma Science and Fusion Center
- Sponsoring Organization:
- USDOE Office of Science (SC), Basic Energy Sciences (BES)
- DOE Contract Number:
- SC0016214
- OSTI ID:
- 1880244
- Country of Publication:
- United States
- Language:
- English
Collisionless Reconnection in Magnetohydrodynamic and Kinetic Turbulence
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journal | December 2017 |
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