{"id":800926,"date":"2026-02-27T15:42:32","date_gmt":"2026-02-27T20:42:32","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=800926"},"modified":"2026-02-27T15:42:32","modified_gmt":"2026-02-27T20:42:32","slug":"the-arrl-solar-update-21","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=800926","title":{"rendered":"The ARRL Solar Update"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">02\/27\/2026<\/span><\/p>\n<p>Spaceweather.com for February 27 reports about a minor CME hurling<br \/>towards Earth.<\/p>\n<p>Solar activity remains at low levels due primarily to C-class flares<br \/>just beyond the SE limb near S21. The largest was a C5.3 flare on<br \/>February 25. On the visible disk, an approximate 5-degree filament<br \/>eruption was observed centered near S08W27 with an associated C2.6<br \/>flare.<\/p>\n<p>The eruption was accompanied by a Type II radio sweep (595 km\/s) and<br \/>possibly two related coronal mass ejections (CMEs), first observed<br \/>in ST A COR2 imagery beginning on February 25. Two CMEs were<br \/>observed off the NE and E limbs in the imagery. However, SOHO\/LASCO<br \/>C2 imagery only showed the northerly CME. Analysis of the CMEs is in<br \/>progress.<br \/>\u00a0<br \/>Solar activity is likely to remain at low levels with a slight<br \/>chance for isolated M-class activity (R1-R2\/minor-moderate), as the<br \/>bright regions currently seen at the east limb rotate onto the<br \/>visible disk.<br \/>\u00a0<br \/>Solar wind parameters continued to show Coronal Hole High Speed<br \/>Stream (CH HSS) influence. Solar wind speed ranged from 530-650<br \/>km\/s. Conditions are likely to return to nominal levels as High<br \/>Speed Stream activity wanes.<\/p>\n<p>Weekly Commentary on the Sun, the Magnetosphere, and the Earth&#8217;s<br \/>Ionosphere, February 26, 2026, by F. K. Janda, OK1HH:<\/p>\n<p>&#8220;Between February 22 and 24, there was not a single spot on the<br \/>solar disk, which last happened less than four years ago. The<br \/>maximum of the 25th cycle is behind us, while the years 2024-2025<br \/>can be considered the years of cycle maximum.<\/p>\n<p>&#8220;At the same time, the Sun is in a key phase of reversing its<br \/>magnetic field. This process is a natural part of the 11-year solar<br \/>cycle, usually occurring asymmetrically (the northern and southern<br \/>hemispheres of the Sun may reverse at slightly different times, with<br \/>the process taking several months). The magnetic field in the polar<br \/>regions of the Sun gradually weakens until it completely breaks down<br \/>and reforms with the opposite polarity.<\/p>\n<p>&#8220;The next eleven-year solar minimum (the transition between the<br \/>current 25th and future 26th cycles) is expected in 2030-2031, when<br \/>the Sun&#8217;s magnetic field will stabilize again and the star will<br \/>enter a quiet period. A more precise date for the minimum will only<br \/>be possible to determine at the end of the decade based on the<br \/>current development of sunspots.<\/p>\n<p>&#8220;During the first week of March, solar activity should gradually<br \/>increase and then decrease in the following week. Changes in the<br \/>intensity of the solar wind will have the greatest impact on the<br \/>development of shortwave propagation conditions. For prediction of<br \/>these changes, it is recommended to monitor the position and area of<br \/>coronal holes and, in particular, solar flares that will be located<br \/>near their edges.<\/p>\n<p>&#8220;This can be monitored excellently at  for<br \/>example, and even professionals will confirm that you will find<br \/>everything you need here to understand the causes of ongoing events<br \/>and for operational practice. In addition, we can monitor the local<br \/>effects in the ionosphere in detail especially thanks to ionospheric<br \/>digisonde stations, dozens of which are available on the internet!&#8221;<\/p>\n<p>Active periods are likely, with a chance for G1 (Minor) storm<br \/>levels, on February 28 to March 1, due to the anticipated arrival of<br \/>a CME that left the Sun on February 25.<\/p>\n<p>The greater than 2 MeV electron flux at geosynchronous orbit is<br \/>expected to reach high levels on March 3, and then on March 6 to 8<br \/>due to anticipated influence of multiple recurrent coronal holes.<\/p>\n<p>The latest report from Dr. Tamitha Skov, WX6SWW, can be found on<br \/>YouTube at,  .<\/p>\n<p>The Predicted Planetary A Index for February 28 to March 6 is 5, 5,<br \/>5, 5, 5, 15, and 15, with a mean of 7.9.\u00a0 Predicted Planetary K<br \/>Index is 2, 2, 2, 2, 2, 4, and 4, with a mean of 2.6.<br \/>10.7-centimeter flux is 122, 122, 125, 125, 125, 125, and 130, with<br \/>a mean of 124.9.<\/p>\n<p>For more information concerning shortwave radio propagation, see<br \/> and the ARRL Technical Information<br \/>Service web page at,  For<br \/>an explanation of numbers used in this bulletin, see<br \/> . Information and<br \/>tutorials on propagation can be found at,  .<\/p>\n<p>Also, check this:<\/p>\n<p>https:\/\/bit.ly\/3Rc8Njt<\/p>\n<p>&#8220;<em>Understanding Solar Indices<\/em>&#8221; from September 2002 <em>QST<\/em>.<\/p>\n<p>\u00a0<\/p>\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"http:\/\/www.arrl.org\/news\/view\/the-arrl-solar-update-22?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>02\/27\/2026 Spaceweather.com for February 27 reports about a minor CME hurlingtowards Earth. Solar activity remains at low levels due primarily to C-class flaresjust beyond the SE limb near S21. The&hellip; <\/p>\n","protected":false},"author":1,"featured_media":771673,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7],"tags":[],"class_list":["post-800926","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-ARRL"],"_links":{"self":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/800926","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=800926"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/800926\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/media\/771673"}],"wp:attachment":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=800926"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=800926"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=800926"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}