Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar Wind

The Parker Solar Probe (PSP) and Wind spacecraft observed the same plasma flow during PSP encounter 15. The solar wind evolves from a sub-Alfvénic flow at 0.08 au to become modestly super-Alfvénic at 1 au. We study the radial evolution of the turbulence properties and deduce the spectral anisotropy...

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Main Authors: Xingyu Zhu, Gary P. Zank, Lingling Zhao, Ashok Silwal
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:The Astrophysical Journal Letters
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Online Access:https://doi.org/10.3847/2041-8213/ada354
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author Xingyu Zhu
Gary P. Zank
Lingling Zhao
Ashok Silwal
author_facet Xingyu Zhu
Gary P. Zank
Lingling Zhao
Ashok Silwal
author_sort Xingyu Zhu
collection DOAJ
description The Parker Solar Probe (PSP) and Wind spacecraft observed the same plasma flow during PSP encounter 15. The solar wind evolves from a sub-Alfvénic flow at 0.08 au to become modestly super-Alfvénic at 1 au. We study the radial evolution of the turbulence properties and deduce the spectral anisotropy based on the nearly incompressible (NI) MHD theory. We find that the spectral index of the z ^+ spectrum remains unchanged (∼−1.53), while the z ^− spectrum steepens, the index of which changes from −1.35 to −1.47. The fluctuating kinetic energy is on average greater than the fluctuating magnetic field energy in the sub-Alfvénic flow while smaller in the modestly super-Alfvénic flow. The NI MHD theory well interprets the observed Elsässer spectra. The contribution of 2D fluctuations is nonnegligible for the observed z ^− frequency spectra for both intervals. Particularly, the magnitudes of 2D and NI/slab fluctuations are comparable in the frequency domain for the modestly super-Alfvénic flow, resulting in a slightly concave shape of z ^− spectrum at 1 au. We show that, in the wavenumber domain, the power ratio of the observed forward NI/slab and 2D fluctuations is  ∼15 at 0.08 au, while it decreases to  ∼3 at 1 au, suggesting the growing significance of the 2D fluctuations as the turbulence evolves in low Mach number solar wind.
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spelling doaj-art-741fe34c054d4782b79fbdb49e5ff9a12025-01-08T08:46:18ZengIOP PublishingThe Astrophysical Journal Letters2041-82052025-01-019782L3410.3847/2041-8213/ada354Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar WindXingyu Zhu0https://orcid.org/0000-0002-1541-6397Gary P. Zank1https://orcid.org/0000-0002-4642-6192Lingling Zhao2https://orcid.org/0000-0002-4299-0490Ashok Silwal3https://orcid.org/0000-0001-6286-2106Center for Space Plasma and Aeronomic Research (CSPAR), The University of Alabama in Huntsville , Huntsville, AL 35805, USA ; xz0017@uah.eduCenter for Space Plasma and Aeronomic Research (CSPAR), The University of Alabama in Huntsville , Huntsville, AL 35805, USA ; xz0017@uah.edu; Department of Space Science, The University of Alabama in Huntsville , Huntsville, AL 35805, USACenter for Space Plasma and Aeronomic Research (CSPAR), The University of Alabama in Huntsville , Huntsville, AL 35805, USA ; xz0017@uah.edu; Department of Space Science, The University of Alabama in Huntsville , Huntsville, AL 35805, USACenter for Space Plasma and Aeronomic Research (CSPAR), The University of Alabama in Huntsville , Huntsville, AL 35805, USA ; xz0017@uah.eduThe Parker Solar Probe (PSP) and Wind spacecraft observed the same plasma flow during PSP encounter 15. The solar wind evolves from a sub-Alfvénic flow at 0.08 au to become modestly super-Alfvénic at 1 au. We study the radial evolution of the turbulence properties and deduce the spectral anisotropy based on the nearly incompressible (NI) MHD theory. We find that the spectral index of the z ^+ spectrum remains unchanged (∼−1.53), while the z ^− spectrum steepens, the index of which changes from −1.35 to −1.47. The fluctuating kinetic energy is on average greater than the fluctuating magnetic field energy in the sub-Alfvénic flow while smaller in the modestly super-Alfvénic flow. The NI MHD theory well interprets the observed Elsässer spectra. The contribution of 2D fluctuations is nonnegligible for the observed z ^− frequency spectra for both intervals. Particularly, the magnitudes of 2D and NI/slab fluctuations are comparable in the frequency domain for the modestly super-Alfvénic flow, resulting in a slightly concave shape of z ^− spectrum at 1 au. We show that, in the wavenumber domain, the power ratio of the observed forward NI/slab and 2D fluctuations is  ∼15 at 0.08 au, while it decreases to  ∼3 at 1 au, suggesting the growing significance of the 2D fluctuations as the turbulence evolves in low Mach number solar wind.https://doi.org/10.3847/2041-8213/ada354Solar windInterplanetary turbulenceSolar coronaSolar physics
spellingShingle Xingyu Zhu
Gary P. Zank
Lingling Zhao
Ashok Silwal
Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar Wind
The Astrophysical Journal Letters
Solar wind
Interplanetary turbulence
Solar corona
Solar physics
title Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar Wind
title_full Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar Wind
title_fullStr Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar Wind
title_full_unstemmed Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar Wind
title_short Radial Evolution of MHD Turbulence Anisotropy in Low Mach Number Solar Wind
title_sort radial evolution of mhd turbulence anisotropy in low mach number solar wind
topic Solar wind
Interplanetary turbulence
Solar corona
Solar physics
url https://doi.org/10.3847/2041-8213/ada354
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AT ashoksilwal radialevolutionofmhdturbulenceanisotropyinlowmachnumbersolarwind