{"id":798202,"date":"2025-09-12T18:21:29","date_gmt":"2025-09-12T23:21:29","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=798202"},"modified":"2025-09-12T18:21:29","modified_gmt":"2025-09-12T23:21:29","slug":"the-arrl-solar-update","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=798202","title":{"rendered":"The ARRL Solar Update"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">09\/12\/2025<\/span><\/p>\n<p>Solar activity has been at very low to low levels this past week.<br \/>\u00a0<br \/>Low level C-class flaring was observed from Regions AR4210 and<br \/>AR4207. Slight growth was observed in Regions AR4213 and AR4214. The rest of the spotted regions were either stable or in decay. Solar<br \/>activity is expected to remain at low levels, with a chance for<br \/>isolated M-class flares (R1-R2\/minor-moderate) through September 13.<br \/>\u00a0<br \/>A CME (Coronal Mass Ejection) was observed just beyond the Western<br \/>limb on September 9. No impacts are expected, and no Earth-directed<br \/>CMEs were observed.<br \/>\u00a0<br \/>Solar wind parameters continued to be enhanced under positive<br \/>polarity coronal hole high speed stream (CH HSS) influences. Solar<br \/>wind speed increased from approximately 450 km\/s to near 550 km\/s.<br \/>Elevated solar wind conditions are expected to continue into<br \/>September 12.\u00a0 Another enhancement is likely on September 14 with<br \/>the onset of negative polarity CH HSS influences and the possible<br \/>glancing effects of the September 11 CME.<br \/>\u00a0<br \/>Weekly Commentary on the Sun, the Magnetosphere, and the Earth&#8217;s<br \/>Ionosphere, September 11, 2025, by F. K. Janda, OK1HH:<\/p>\n<p>&#8220;During a seven-day interval (August 26 to September 1), when solar<br \/>flux values were above 200 s.f.u., there was a decline to below 120<br \/>s.f.u. during the first ten days of September. Which also occurred<br \/>during the previous solar rotation &#8211; on August 17-19.<\/p>\n<p>&#8220;Solar flare activity simultaneously decreased significantly, while<br \/>all sunspot groups moved to the western half of the solar disk.<br \/>Instead, we are now observing a large coronal hole, located mostly<br \/>north of the solar equator, whose boundary has already crossed the<br \/>central meridian.<\/p>\n<p>&#8220;The intensified solar wind, which is definitely blowing from its<br \/>western edge, is expected to reach Earth since September 13. It will<br \/>likely contribute to increased geomagnetic activity, which, combined<br \/>with relatively low solar activity, will have negative consequences<br \/>for the state of the ionosphere. MUF values will decrease,<br \/>attenuation will increase, and shortwave propagation conditions will<br \/>deteriorate.<\/p>\n<p>&#8220;Starting in the half of September, however, solar activity will<br \/>begin to increase, although not as significantly as it did in<br \/>August. In addition, geomagnetic activity appears to be declining at<br \/>the same time. The approaching Autumn Equinox will also have a<br \/>significant impact on the state of the ionosphere. These are already<br \/>three reasons why shortwave propagation conditions should gradually<br \/>improve.&#8221;<\/p>\n<p>The Predicted Planetary A Index for September 13 to 19 is 5, 12, 20,<br \/>15, 8, 8, and 8, with a mean of 10.9.\u00a0 Predicted Planetary K Index<br \/>is 2, 4, 5, 4, 3, 3, and 3, with a mean of 3.4.\u00a0 10.7 centimeter<br \/>flux is 120, 125, 130, 135, 135, 140, and 145, with a mean of 132.9.<\/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?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>09\/12\/2025 Solar activity has been at very low to low levels this past week.\u00a0Low level C-class flaring was observed from Regions AR4210 andAR4207. Slight growth was observed in Regions AR4213&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-798202","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\/798202","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=798202"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/798202\/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=798202"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=798202"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=798202"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}