Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude

The solar wind undergoes significant heating as it propagates away from the Sun; the exact mechanisms responsible for this heating are not yet fully understood. We present for the first time a statistical test for one of the proposed mechanisms: stochastic ion heating. We use the amplitude of magnet...

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Main Authors: Vech, Daniel, Klein, Kristopher G., Kasper, Justin C.
Other Authors: Univ Arizona, Lunar & Planetary Lab
Language:en
Published: IOP PUBLISHING LTD 2017
Subjects:
Online Access:http://hdl.handle.net/10150/626264
http://arizona.openrepository.com/arizona/handle/10150/626264
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spelling ndltd-arizona.edu-oai-arizona.openrepository.com-10150-6262642017-12-22T03:00:43Z Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude Vech, Daniel Klein, Kristopher G. Kasper, Justin C. Univ Arizona, Lunar & Planetary Lab plasmas solar wind turbulence waves The solar wind undergoes significant heating as it propagates away from the Sun; the exact mechanisms responsible for this heating are not yet fully understood. We present for the first time a statistical test for one of the proposed mechanisms: stochastic ion heating. We use the amplitude of magnetic field fluctuations near the proton gyroscale as a proxy for the ratio of gyroscale velocity fluctuations to perpendicular (with respect to the magnetic field) proton thermal speed, defined as epsilon(p). Enhanced proton temperatures are observed when epsilon(p) is larger than a critical value (similar to 0.019-0.025). This enhancement strongly depends on the proton plasma beta (beta parallel to(p)); when beta parallel to(p) << 1 only the perpendicular proton temperature T-perpendicular to increases, while for beta parallel to(p) similar to 1 increased parallel and perpendicular proton temperatures are both observed. For epsilon(p) smaller than the critical value and beta parallel to(p) << 1 no enhancement of Tp is observed, while for beta parallel to(p) similar to 1 minor increases in T-parallel to are measured. The observed change of proton temperatures across a critical threshold for velocity fluctuations is in agreement with the stochastic ion heating model of Chandran et al. We find that epsilon(p) > epsilon(crit) in 76% of the studied periods, implying that stochastic heating may operate most of the time in the solar wind at 1 au. 2017-11-16 Article Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude 2017, 850 (1):L11 The Astrophysical Journal 2041-8213 10.3847/2041-8213/aa9887 http://hdl.handle.net/10150/626264 http://arizona.openrepository.com/arizona/handle/10150/626264 The Astrophysical Journal Letters en http://stacks.iop.org/2041-8205/850/i=1/a=L11?key=crossref.6b0ff345ea76324426771fad0f6cbc2b © 2017. The American Astronomical Society. IOP PUBLISHING LTD
collection NDLTD
language en
sources NDLTD
topic plasmas
solar wind
turbulence
waves
spellingShingle plasmas
solar wind
turbulence
waves
Vech, Daniel
Klein, Kristopher G.
Kasper, Justin C.
Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude
description The solar wind undergoes significant heating as it propagates away from the Sun; the exact mechanisms responsible for this heating are not yet fully understood. We present for the first time a statistical test for one of the proposed mechanisms: stochastic ion heating. We use the amplitude of magnetic field fluctuations near the proton gyroscale as a proxy for the ratio of gyroscale velocity fluctuations to perpendicular (with respect to the magnetic field) proton thermal speed, defined as epsilon(p). Enhanced proton temperatures are observed when epsilon(p) is larger than a critical value (similar to 0.019-0.025). This enhancement strongly depends on the proton plasma beta (beta parallel to(p)); when beta parallel to(p) << 1 only the perpendicular proton temperature T-perpendicular to increases, while for beta parallel to(p) similar to 1 increased parallel and perpendicular proton temperatures are both observed. For epsilon(p) smaller than the critical value and beta parallel to(p) << 1 no enhancement of Tp is observed, while for beta parallel to(p) similar to 1 minor increases in T-parallel to are measured. The observed change of proton temperatures across a critical threshold for velocity fluctuations is in agreement with the stochastic ion heating model of Chandran et al. We find that epsilon(p) > epsilon(crit) in 76% of the studied periods, implying that stochastic heating may operate most of the time in the solar wind at 1 au.
author2 Univ Arizona, Lunar & Planetary Lab
author_facet Univ Arizona, Lunar & Planetary Lab
Vech, Daniel
Klein, Kristopher G.
Kasper, Justin C.
author Vech, Daniel
Klein, Kristopher G.
Kasper, Justin C.
author_sort Vech, Daniel
title Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude
title_short Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude
title_full Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude
title_fullStr Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude
title_full_unstemmed Nature of Stochastic Ion Heating in the Solar Wind: Testing the Dependence on Plasma Beta and Turbulence Amplitude
title_sort nature of stochastic ion heating in the solar wind: testing the dependence on plasma beta and turbulence amplitude
publisher IOP PUBLISHING LTD
publishDate 2017
url http://hdl.handle.net/10150/626264
http://arizona.openrepository.com/arizona/handle/10150/626264
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AT kasperjustinc natureofstochasticionheatinginthesolarwindtestingthedependenceonplasmabetaandturbulenceamplitude
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