{"id":785132,"date":"2024-07-02T13:15:54","date_gmt":"2024-07-02T18:15:54","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=785132"},"modified":"2024-07-02T13:15:54","modified_gmt":"2024-07-02T18:15:54","slug":"energetics-of-compressive-waves-in-the-solar-corona","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=785132","title":{"rendered":"Energetics of compressive waves in the solar corona"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n<div class=\"article-gallery lightGallery\">\n<div data-thumb=\"https:\/\/scx1.b-cdn.net\/csz\/news\/tmb\/2024\/energetics-of-compress.jpg\" data-src=\"https:\/\/scx2.b-cdn.net\/gfx\/news\/2024\/energetics-of-compress.jpg\" data-sub-html=\"Left: Available power per unit mass (erg\/g\/s) using perpendicular velocity fluctuations. The solid and dashed lines correspond to the range (20\u201370) km~s&lt;sup&gt;\u22121&lt;\/sup&gt; (black) from frequency broadening measurements, and (20\u201340) km~s&lt;sup&gt;\u22121&lt;\/sup&gt; for r&lt;1.4 R\u2299 for non-thermal velocities from coronal lines (red). Right: Coronal heating rate per unit mass (erg\/g\/s) from Landau damping of ion-sound waves. The solid and dashed lines show the results for the nominal density fluctuation amplitude for anisotropy factors \u03b1=0.25 and \u03b1=0.4, and the gray area corresponds to the range of values from one-half to double the nominal density fluctuation amplitude, taking both values of \u03b1 into account. Credit: Azzollini et al, ApJ 968 72 (2024)\">\n<figure class=\"article-img\">\n            <figcaption class=\"text-darken text-low-up text-truncate-js text-truncate mt-3\">\n                Left: Available power per unit mass (erg\/g\/s) using perpendicular velocity fluctuations. The solid and dashed lines correspond to the range (20\u201370) km~s<sup>\u22121<\/sup> (black) from frequency broadening measurements, and (20\u201340) km~s<sup>\u22121<\/sup> for r        <\/figcaption><\/figure>\n<\/p><\/div>\n<\/div>\n<p>Inelastic scattering off moving or oscillating density fluctuations leads to broadening of radio signals propagating in the solar corona and solar wind. Using an anisotropic density fluctuation model from the kinetic scattering theory for solar radio bursts, it is possible to deduce the plasma velocities (perpendicular to the line of sight) required to explain observations of spacecraft signal frequency broadening.<\/p>\n<p>The kinetic energy associated with these inferred bulk velocities cascades to smaller and smaller scales, where it is ultimately dissipated through damping of ion-sound waves. The inferred energy deposition rate associated with this process compares very favorably with those required to heat the corona and drive the solar wind.<\/p>\n<p>Considering a distant point source, Francesco Azzollini and others calculate the effects of inelastic scattering in the presence of motions perpendicular to the line of sight, and they derive the associated diffusion tensor for radio waves in anisotropic turbulent plasma. The research is published in <i>The Astrophysical Journal<\/i>.<\/p>\n<p>The inferred velocities are consistent with motions that are dominated by the solar wind at distances \u227310 R\u2299, but the levels of frequency broadening for \u227210 R\u2299 require additional radial speeds of about 300 km s<sup>\u22121<\/sup> and\/or transverse speeds of about (20\u201370) km s<sup>\u22121<\/sup>.<\/p>\n<p>The inferred radial velocities also appear consistent with the sound or proton thermal speeds, while the speeds perpendicular to the radial direction are consistent with non-thermal motions measured via coronal Doppler-line broadening, interpreted as Alfv\u00e9nic fluctuations.<\/p>\n<p>Landau damping of parallel propagating ion-sound (slow MHD) waves results in a proton heating rate that is comparable to the rates available from a turbulent cascade of Alfv\u00e9nic waves at large scales, suggesting a coherent picture of energy transfer, via the cascade or\/and parametric decay of Alfv\u00e9n waves to the small scales where heating takes place.<\/p>\n<div class=\"article-main__more p-4\">\n<p><strong>More information:<\/strong><br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tFrancesco Azzollini et al, Plasma Motions and Compressive Wave Energetics in the Solar Corona and Solar Wind from Radio Wave Scattering Observations, <i>The Astrophysical Journal<\/i> (2024). DOI: 10.3847\/1538-4357\/ad4154<\/p>\n<\/p><\/div>\n<div class=\"d-inline-block text-medium mt-4\">\n<p>\n\t\t\t\t\t\t\t\t\t\t\t\t\tProvided by<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\tCommunity of European Solar Radio Astronomers<\/p>\n<p>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<svg>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<use href=\"https:\/\/phys.b-cdn.net\/tmpl\/v6\/img\/svg\/sprite.svg#icon_open\" x=\"0\" y=\"0\"\/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/svg><\/p>\n<\/p><\/div>\n<p>\t\t\t\t\t\t\t\t\t\t<!-- print only --><\/p>\n<div class=\"d-none d-print-block\">\n<p>\n\t\t\t\t\t\t\t\t\t\t\t\t<strong>Citation<\/strong>:<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tEnergetics of compressive waves in the solar corona (2024, July 2)<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tretrieved 2 July 2024<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tfrom\n\t\t\t\t\t\t\t\t\t\t\t <\/p>\n<p>\n\t\t\t\t\t\t\t\t\t\t\t This document is subject to copyright. Apart from any fair dealing for the purpose of private study or research, no<br \/>\n\t\t\t\t\t\t\t\t\t\t\t part may be reproduced without the written permission. The content is provided for information purposes only.\n\t\t\t\t\t\t\t\t\t\t\t <\/p>\n<\/p><\/div>\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"https:\/\/phys.org\/news\/2024-07-energetics-compressive-solar-corona.html\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Left: Available power per unit mass (erg\/g\/s) using perpendicular velocity fluctuations. The solid and dashed lines correspond to the range (20\u201370) km~s\u22121 (black) from frequency broadening measurements, and (20\u201340) km~s\u22121&hellip; <\/p>\n","protected":false},"author":1,"featured_media":785133,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[41],"tags":[],"class_list":["post-785132","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-phys-org"],"_links":{"self":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/785132","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=785132"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/785132\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/media\/785133"}],"wp:attachment":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=785132"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=785132"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=785132"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}