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Solar Wind Turbulence and the Role of Ion Instabilities

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arxiv 1306.5336 v1 pith:TCRPBFAK submitted 2013-06-22 astro-ph.SR physics.space-ph

Solar Wind Turbulence and the Role of Ion Instabilities

classification astro-ph.SR physics.space-ph
keywords scalesturbulencemagneticsolarwindcascadedissipationelectron
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Solar wind is probably the best laboratory to study turbulence in astrophysical plasmas. In addition to the presence of magnetic field, the differences with neutral fluid isotropic turbulence are: weakness of collisional dissipation and presence of several characteristic space and time scales. In this paper we discuss observational properties of solar wind turbulence in a large range from the MHD to the electron scales. At MHD scales, within the inertial range, turbulence cascade of magnetic fluctuations develops mostly in the plane perpendicular to the mean field. Solar wind turbulence is compressible in nature. The spectrum of velocity fluctuations do not follow magnetic field one. Probability distribution functions of different plasma parameters are not Gaussian, indicating presence of intermittency. At the moment there is no global model taking into account all these observed properties of the inertial range. At ion scales, turbulent spectra have a break, compressibility increases and the density fluctuation spectrum has a local flattening. Around ion scales, magnetic spectra are variable and ion instabilities occur as a function of the local plasma parameters. Between ion and electron scales, a small scale turbulent cascade seems to be established. Approaching electron scales, the fluctuations are no more self-similar: an exponential cut-off is usually observed indicating an onset of dissipation. The nature of the small scale cascade and a possible dissipation mechanism are still under debate.

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Cited by 1 Pith paper

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  1. Solar Wind Proton Heating and its Effect on Temperature Anisotropy Evolution between 0.05 and 1 au

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    Solar wind protons experience substantial perpendicular, but not parallel, heating from 0.05 to 1 au, reducing the expected adiabatic growth of temperature anisotropy.