{"id":798624,"date":"2025-10-03T13:36:32","date_gmt":"2025-10-03T18:36:32","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=798624"},"modified":"2025-10-03T13:36:32","modified_gmt":"2025-10-03T18:36:32","slug":"the-arrl-solar-update-2","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=798624","title":{"rendered":"The ARRL Solar Update"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">10\/03\/2025<\/span><\/p>\n<p>Solar activity, which has been at low levels, has returned to<br \/>moderate levels. Region AR4232 produced the largest event of the<br \/>period, an impulsive M3.6 flare (R1-minor) on October 1, 2025.<\/p>\n<p>An associated Coronal Mass Ejection (CME) was observed in subsequent<br \/>SOHO LASCO\/C2 coronagraph imagery that began on September 29.<br \/>Analysis and modelling of the ejecta is ongoing.<\/p>\n<p>Newly numbered Region AR4237 remained relatively quiet as it<br \/>developed. Region AR4263 also produced an R1 event with an M1.0\/Sf<br \/>flare near the end of the reporting period.<br \/>\u00a0 <br \/>It is important to note that, after careful assessment of recent<br \/>magnetograph imagery, a spot previously associated to region AR4239<br \/>is now considered part of the AR4230, explaining its reported size<br \/>increase. A new region appeared but remained unnumbered until<br \/>further observation.<br \/>\u00a0 <br \/>With multiple regions continuing to exhibit growth, flare activity<br \/>is likely to remain at moderate levels (R1-R2\/minor-moderate) with a<br \/>slight chance for an X-class flare (R3-strong) through October 30.<br \/>\u00a0 <br \/>Weak enhancements in the solar wind environment, that began<br \/>September 29, are likely to continue as influence from a negative<br \/>polarity Coronal Hole High Speed Stream (CH HSS) persists.<\/p>\n<p>The CH HSS influences on the solar wind conditions near Earth are<br \/>expected to persist through October 5, as the planet continues to be<br \/>embedded at the CH associated co-rotating interactive region (CIR).<br \/>A recurrent negative CH was observed rotating into the East limb of<br \/>the visible solar disk during the period, but no impact is expected<br \/>from it in the upcoming days.<\/p>\n<p>Weekly Commentary on the Sun, the Magnetosphere, and the Earth&#8217;s<br \/>Ionosphere, October 2, 2025, by F. K. Janda, OK1HH:<\/p>\n<p>&#8220;During September, a relatively large number of sunspot groups were<br \/>observed on the solar disk, but there were almost no energetically<br \/>significant eruptions. It seemed to be the calm before the storm.<br \/>The question was what would cause the storm and how the disturbance<br \/>would develop. Important factors were: the proximity of the Autumn<br \/>Equinox and the configuration of areas on the solar disk.<\/p>\n<p>&#8220;The following phenomena were key to further developments:<br \/>&#8211; The Russell-McPherron effect, in which the magnetic field lines of<br \/>\u00a0 the Sun and Earth can connect around the equinox.<br \/>&#8211; The source of the intensified solar wind heading towards Earth.<\/p>\n<p>&#8220;The second condition was also met &#8211; we observed coronal holes No.<br \/>83 and 84 on the solar disk near active regions No. 4230 and 4238,<br \/>with the space between them being close enough to the central<br \/>meridian.<\/p>\n<p>&#8220;The disturbance began with a so-called positive phase on the<br \/>afternoon of September 29 UTC, while the critical frequencies in the<br \/>F2 ionospheric layer initially rose for several hours. In the<br \/>following days, the solar wind speed gradually increased to an<br \/>impressive 800 km\/s. The intensity of the geomagnetic disturbance<br \/>reached grade G3 (three-hour K indices rose to 6 to 7).<\/p>\n<p>&#8220;The return of the ionosphere to normal conditions will be slow, as<br \/>solar activity is expected to gradually decline in the first half of<br \/>October. In addition, after a slight lull, another disturbance can<br \/>be expected around October 7, and even after that, the situation<br \/>will not be very calm.&#8221;<\/p>\n<p>The latest report from Dr. Tamitha Skov, WX6SWW, can be found on<br \/>YouTube at:\u00a0  .<\/p>\n<p>The NOAA Space Weather Prediction Center has a webpage that<br \/>discusses the current solar cycle progression:<br \/> .<\/p>\n<p>The Predicted Planetary A Index for October 4 to 10 is 8, 8, 8, 5,<br \/>5, 5, and 5, with a mean of 6.3.\u00a0 The Predicted Planetary K Index is<br \/>3, 3, 3, 2, 2, 2, and 2, with a mean of 2.4.\u00a0 10.7 centimeter flux<br \/>is 170, 165, 165, 165, 155, 155, and 155, with a mean of 161.4.<\/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 Indice<\/em>s&#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-3?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>10\/03\/2025 Solar activity, which has been at low levels, has returned tomoderate levels. Region AR4232 produced the largest event of theperiod, an impulsive M3.6 flare (R1-minor) on October 1, 2025.&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-798624","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\/798624","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=798624"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/798624\/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=798624"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=798624"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=798624"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}