{"id":798810,"date":"2025-10-17T14:57:34","date_gmt":"2025-10-17T19:57:34","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=798810"},"modified":"2025-10-17T14:57:34","modified_gmt":"2025-10-17T19:57:34","slug":"the-arrl-solar-update-4","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=798810","title":{"rendered":"The ARRL Solar Update"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">10\/17\/2025<\/span><\/p>\n<p>Region AR4246 underwent significant evolution, growing in overall<br \/>size while gaining multiple new spots. Subsequently, AR4246 was the<br \/>main provider of activity which included an M1.2 flare on October<br \/>13. Several coronal mass ejections (CMEs) with potential<br \/>Earth-directed components are in the mix at this time.<\/p>\n<p>Additional modeling efforts are underway to perhaps confirm those<br \/>suspicions. The largest flare was a long-duration M4.8\/2n on October<br \/>15. Modeling efforts showed the ejecta to be on a northward<br \/>trajectory and not on an Earthward course.<br \/>\u00a0<br \/>Other notable activity included a prominence eruption off the ENE<br \/>limb-first visible in LASCO C2 imagery on October 14. Given the<br \/>location of the event, initial analysis suggests this ejecta to be<br \/>well into foul-ball territory and not Earth-directed. Additional<br \/>modeling efforts are underway to perhaps confirm this suspicion.<br \/>\u00a0<br \/>Slight decay was observed in the intermediate portion of Region<br \/>AR4248 as it grew in length. Region AR4247 was in decay as well. The<br \/>remaining regions were unremarkable in comparison. No new regions<br \/>were assigned numbers this period. Minor to moderate (R1-R2) radio<br \/>blackouts are likely for the next 3 days, with a slight chance for<br \/>an isolated R3 (strong) event, due to the current and potential<br \/>flare activity of Regions AR4246 and AR4248.<br \/>\u00a0<br \/>Solar wind parameters continued to reflect the influence of a<br \/>negative polarity coronal hole high speed stream (CH HSS). Solar<br \/>wind speeds finally dipped below 600 km\/s and phi was predominantly<br \/>in the negative solar sector.<br \/>\u00a0<br \/>Solar wind parameters are expected to continue at enhanced levels,<br \/>although gradually waning, and continuing through October 17, due to<br \/>CME arrivals from the October 11 to 13 timeframe originating from<br \/>AR4246.\u00a0 Solar activity reached moderate levels due to M-class flare<br \/>activity.<\/p>\n<p>Weekly Commentary on the Sun, the Magnetosphere, and the Earth&#8217;s<br \/>Ionosphere, October 16, 2025, by F. K. Janda, OK1HH:<\/p>\n<p>&#8220;In line with forecasts, solar activity continued to gradually<br \/>increase, including several moderately strong flares. These were<br \/>mostly observed in the active region NOAA 4246, located in the<br \/>northwest of the solar disk, while approaching its limb.<\/p>\n<p>&#8220;The second of the two larger active regions is NOAA 4248, also<br \/>located in the northwest, but closer to the central meridian and the<br \/>solar equator, while relatively close to the extensive coronal hole<br \/>No. 87. In the coming days, AR NOAA 4248 will move into the active<br \/>longitudes. Therefore, its eruptive activity will increase. Between<br \/>it and the aforementioned coronal hole, a source of intensified<br \/>solar wind will form, which will hit Earth during the coming week.<\/p>\n<p>&#8220;Even earlier, on October 16, when this text is being written, we<br \/>expect a G2 geomagnetic disturbance, which will first cause a brief<br \/>improvement and then a deterioration in ionospheric propagation of<br \/>short waves, which have been rather average so far. The exception<br \/>was a shorter increase in MUF on October 15 between 1000 and 1200<br \/>UTC, probably caused by an intensification of the solar wind.<\/p>\n<p>&#8220;Solar activity should remain at current levels for the rest of the<br \/>month. Fluctuations in propagation conditions, mostly around average<br \/>with occasional deterioration, will depend on the irregular<br \/>occurrence of geomagnetic disturbances.&#8221;<br \/>\u00a0<br \/>The latest video report from Dr. Tamitha Skov, WX6SWW, can be found<br \/>on YouTube at:\u00a0  .<br \/>\u00a0<br \/>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>The Predicted Planetary A Index for October 18 to 24 is 5, 5, 15,<br \/>10, 8, 5, and 5, with a mean of 7.6.\u00a0 Predicted Planetary K Index is<br \/>2, 2, 5, 3, 3, 2, and 2, with a mean of 2.7.\u00a0 10.7-centimeter flux<br \/>is 150, 150, 150, 150, 145, 140, and 145, with a mean of 147.1.<br \/>\u00a0<\/p>\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"http:\/\/www.arrl.org\/news\/view\/the-arrl-solar-update-5?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>10\/17\/2025 Region AR4246 underwent significant evolution, growing in overallsize while gaining multiple new spots. Subsequently, AR4246 was themain provider of activity which included an M1.2 flare on October13. Several coronal&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-798810","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\/798810","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=798810"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/798810\/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=798810"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=798810"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=798810"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}