{"id":798901,"date":"2025-10-27T15:09:29","date_gmt":"2025-10-27T20:09:29","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=798901"},"modified":"2025-10-27T15:09:29","modified_gmt":"2025-10-27T20:09:29","slug":"the-arrl-solar-update-5","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=798901","title":{"rendered":"The ARRL Solar Update"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">10\/24\/2025<\/span><\/p>\n<p>Solar activity reached moderate levels this past week, but has now<br \/>returned to, and remains at, lower levels. Region 4248 produced an<br \/>M1.1 flare on October 20, which was the largest event of the period.<br \/>Region 4261 was numbered this period as it rotated into better<br \/>viewing conditions.<\/p>\n<p>Region 4262 was numbered this period as well, splitting it from<br \/>Region 4257. Additionally, new spots were noted near N08W00 and<br \/>N09E67 but went unnumbered due to a lack of flaring and time of<br \/>emergence. No Earth-directed CMEs were observed in available<br \/>coronagraph imagery. Solar activity is expected to remain low, with<br \/>a chance for isolated M-class flares (R1-R2\/minor-moderate).<br \/>\u00a0<br \/>Additional notable activity included a type II radio sweep with an<br \/>estimated speed of 2,474 km\/s and a type IV radio sweep that began<br \/>on October 21. Significant field line movement, appearing to<br \/>originate from beyond the northwestern limb, was observed in GOES<br \/>SUVI imagery beginning on October 21.\u00a0 The subsequent coronal mass<br \/>ejection (CME) was then first seen on LASCO C2 coronagraph imagery<br \/>on October 21. This event has been analyzed as a far-sided<br \/>asymmetric halo.<br \/>\u00a0<br \/>Solar wind parameters were mildly enhanced this period due to<br \/>negative polarity coronal hole high speed stream (CH HSS)<br \/>influences. Solar wind speeds exhibited a decreasing trend from<br \/>approximately 600 km\/s to under 500 km\/s by the period&#8217;s end. Phi<br \/>was predominantly positive while undertaking brief excursions into<br \/>the positive solar sector. Mildly enhanced solar wind conditions and<br \/>waning negative polarity CH HSS influences were expected to<br \/>continue.<\/p>\n<p>Solar activity is expected to be at moderate levels from October 31<br \/>to November 15 due to the return of Region 4246. Low levels are<br \/>expected to prevail to October 30, and then on November 14 and 15.<br \/>Geomagnetic field activity is expected to reach G1-G2<br \/>(Minor-Moderate) storm levels on October 28 to 30.<\/p>\n<p>Weekly Commentary on the Sun, the Magnetosphere, and the Earth&#8217;s<br \/>Ionosphere, October 23, 2025, by F. K. Janda, OK1HH:<\/p>\n<p>&#8220;Although it may not seem so at first glance, solar activity is<br \/>still at the peak of its 25th cycle. Although the number of sunspot<br \/>groups fell to six in mid-October, a week later it had risen to ten.<br \/>Few eruptions were observed on the solar disk, or the side of the<br \/>Sun facing Earth, including only a few that could be classified as<br \/>moderately strong based on the intensity of X-ray emissions.<\/p>\n<p>&#8220;However, something is brewing on the far side of the Sun. This is<br \/>evidenced by the occurrence of three CMEs, the first on October 21<br \/>and the other two on October 22. The increased concentration of<br \/>protons with an energy of 10 MeV (and a lower concentration of 100<br \/>MeV) in the solar wind confirms that this is significant activity.<br \/>To analyze the development of the relevant activity, we will have to<br \/>wait until it appears on the eastern limb of the solar disk.<\/p>\n<p>&#8220;The geomagnetic field has calmed down in recent days. The next<br \/>disturbance is expected around October 28. At first glance, this is<br \/>very good news for shortwave propagation conditions during the<br \/>weekend of October 25-26, but if geomagnetic activity increases<br \/>during these days, it will come as no surprise.<\/p>\n<p>&#8220;In fact, with the right timing of the disturbance, it could be<br \/>followed by an increase in MUF and an overall improvement. Although<br \/>a significant deterioration in propagation conditions is expected<br \/>with a relatively high probability only after the aforementioned<br \/>disturbance (i.e., around October 29), it may occur earlier.&#8221;<\/p>\n<p>The Predicted Planetary A Index for October 25 to 31 is 10, 5, 5,<br \/>25, 35, 25, and 15, with a mean of 17.1.\u00a0 Predicted Planetary K<br \/>Index is 3, 2, 2, 5, 6, 5, and 4, with a mean of 3.9.\u00a0 10.7-centimeter flux is 150, 150, 150, 145, 145, 145, and 140, with a mean of 146.4.<\/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-6?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>10\/24\/2025 Solar activity reached moderate levels this past week, but has nowreturned to, and remains at, lower levels. Region 4248 produced anM1.1 flare on October 20, which was the largest&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-798901","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\/798901","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=798901"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/798901\/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=798901"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=798901"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=798901"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}