On the ion-inertial-range density-power spectra in solar wind turbulence
A model-independent first-principle first-order investigation of the shape of turbulent density-power spectra in the ion-inertial range of the solar wind at 1 AU is presented. Demagnetised ions in the ion-inertial range of quasi-neutral plasmas respond to Kolmogorov (K) or Iroshnikov–Kraichnan (IK)...
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Published in | Annales geophysicae (1988) Vol. 37; no. 2; pp. 183 - 199 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Katlenburg-Lindau
Copernicus GmbH
03.04.2019
Copernicus Publications |
Subjects | |
Online Access | Get full text |
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Summary: | A model-independent first-principle first-order investigation of the shape of
turbulent density-power spectra in the ion-inertial range of the solar wind
at 1 AU is presented. Demagnetised ions in the ion-inertial range of
quasi-neutral plasmas respond to Kolmogorov (K) or Iroshnikov–Kraichnan (IK)
inertial-range velocity–turbulence power spectra via the spectrum of the
velocity–turbulence-related random-mean-square
induction–electric field. Maintenance of
electrical quasi-neutrality by the ions causes deformations in the power
spectral density of the turbulent density fluctuations. Assuming
inertial-range K (IK) spectra in solar wind velocity turbulence and referring
to observations of density-power spectra suggest that the occasionally
observed scale-limited bumps in the density-power spectrum may be traced back
to the electric ion response. Magnetic power spectra react passively to the
density spectrum by warranting pressure balance. This approach still neglects
contribution of Hall currents and is restricted to the ion-inertial-range
scale. While both density and magnetic turbulence spectra in the affected
range of ion-inertial scales deviate from K or IK power law shapes, the
velocity turbulence preserves its inertial-range shape in the process to
which spectral advection turns out to be secondary but may become observable
under special external conditions. One such case observed by WIND is
analysed. We discuss various aspects of this effect, including the affected
wave-number scale range, dependence on the angle between mean flow velocity
and wave numbers, and, for a radially expanding solar wind flow, assuming
adiabatic expansion at fast solar wind speeds and a Parker dependence of the
solar wind magnetic field on radius, also the presumable limitations on the
radial location of the turbulent source region. |
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ISSN: | 1432-0576 0992-7689 1432-0576 |
DOI: | 10.5194/angeo-37-183-2019 |