Electron Velocity Moments in the Solar Wind. II. Statistical Properties

Abstract Between 2005 January 1 and 2017 November 25, the Wind spacecraft measured 3,996,051 electron velocity distribution functions (VDFs) in the near-Earth solar wind. The instrument was calibrated, and velocity moments were calculated up to the third moment (i.e., electron heat flux). The magnetic field and ion velocity moments have been interpolated to the midpoint time of the VDFs, where we have 3,947,607 finite electron velocity moments (most prior studies used &lt;300,000 moments). The median values for the velocity moments are as follows: n e ,int ∼ 5.43 cm −3 , ∣ V oe ∣ ∼ 421 km s −1 , T e ,tot ∼ 12.7 eV, and ∣ q e ,∥ ∣ ∼4.92 μ W m −2 . The median values for the electron-to-proton temperature ratio is <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mfenced close=")" open="("> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>e</mml:mi> <mml:mo>,</mml:mo> <mml:mi mathvariant="normal">tot</mml:mi> </mml:mrow> </mml:msub> <mml:mo>/</mml:mo> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>p</mml:mi> <mml:mo>,</mml:mo> <mml:mi mathvariant="normal">tot</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:mfenced> </mml:math> ∼2.55, the electron temperature anisotropy A e = <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mfenced close=")" open="("> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>e</mml:mi> <mml:mo>,</mml:mo> <mml:mo>⊥</mml:mo> </mml:mrow> </mml:msub> <mml:mo>/</mml:mo> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>e</mml:mi> <mml:mo>,</mml:mo> <mml:mo stretchy="false">∥</mml:mo> </mml:mrow> </mml:msub> </mml:mrow> </mml:mfenced> </mml:math> ∼ 0.89, total electron beta β e ,tot ∼ 1.27, electron–electron collision frequency ν ee ​​​​ ∼ 0.18 day −1 , and electron–electron Knudsen number K n ,ee ∼ 2.57. The results are mostly consistent with previous studies except that K n ,ee is significantly larger than some other works, which implies that the near-Earth solar wind is less collisional than may have been inferred.

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Publication Details

Journal
The Astrophysical Journal
Published
2026-04-30
DOI
https://doi.org/10.3847/1538-4357/ae5d4a
Primary Topic
Ionosphere and magnetosphere dynamics
Type
article
Field-Weighted Citation Impact
0.00

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article

Electron Velocity Moments in the Solar Wind. II. Statistical Properties

L. B. Wilson, Mihailo M. Martinović, Jason TenBarge, Kristopher G. Klein et al.
The Astrophysical Journal
Ionosphere and magnetosphere dynamics
article

Electron Velocity Moments in the Solar Wind. II. Statistical Properties

L. B. Wilson, Mihailo M. Martinović, Jason TenBarge, Kristopher G. Klein, Michael L. Stevens, Stuart D. Bale, Bennett A. Maruca
article en

Abstract

Abstract Between 2005 January 1 and 2017 November 25, the Wind spacecraft measured 3,996,051 electron velocity distribution functions (VDFs) in the near-Earth solar wind. The instrument was calibrated, and velocity moments were calculated up to the third moment (i.e., electron heat flux). The magnetic field and ion velocity moments have been interpolated to the midpoint time of the VDFs, where we have 3,947,607 finite electron velocity moments (most prior studies used &lt;300,000 moments). The median values for the velocity moments are as follows: n e ,int ∼ 5.43 cm −3 , ∣ V oe ∣ ∼ 421 km s −1 , T e ,tot ∼ 12.7 eV, and ∣ q e ,∥ ∣ ∼4.92 μ W m −2 . The median values for the electron-to-proton temperature ratio is <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mfenced close=")" open="("> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>e</mml:mi> <mml:mo>,</mml:mo> <mml:mi mathvariant="normal">tot</mml:mi> </mml:mrow> </mml:msub> <mml:mo>/</mml:mo> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>p</mml:mi> <mml:mo>,</mml:mo> <mml:mi mathvariant="normal">tot</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:mfenced> </mml:math> ∼2.55, the electron temperature anisotropy A e = <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mfenced close=")" open="("> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>e</mml:mi> <mml:mo>,</mml:mo> <mml:mo>⊥</mml:mo> </mml:mrow> </mml:msub> <mml:mo>/</mml:mo> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>e</mml:mi> <mml:mo>,</mml:mo> <mml:mo stretchy="false">∥</mml:mo> </mml:mrow> </mml:msub> </mml:mrow> </mml:mfenced> </mml:math> ∼ 0.89, total electron beta β e ,tot ∼ 1.27, electron–electron collision frequency ν ee ​​​​ ∼ 0.18 day −1 , and electron–electron Knudsen number K n ,ee ∼ 2.57. The results are mostly consistent with previous studies except that K n ,ee is significantly larger than some other works, which implies that the near-Earth solar wind is less collisional than may have been inferred.

The Astrophysical JournalVol. 1002(2)
National Aeronautics and Space Administration, Royal Society
Affordable and clean energy
Openalex Percentile: Top 8%
Ionosphere and magnetosphere dynamics
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