{"id":799046,"date":"2025-11-07T19:34:29","date_gmt":"2025-11-08T00:34:29","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=799046"},"modified":"2025-11-07T19:34:29","modified_gmt":"2025-11-08T00:34:29","slug":"the-arrl-solar-update-7","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=799046","title":{"rendered":"The ARRL Solar Update"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">11\/07\/2025<\/span><\/p>\n<p>Solar activity has reached high levels due to a pair of X-class<br \/>flares.<br \/>\u00a0<br \/>The first was an X1.8 on November 4 from Region 4274. Associated<br \/>with the flare were Type IV radio sweeps, 160 sfu Tenflare, and a<br \/>partial halo coronal mass ejection (CME) directed mostly off the NE<br \/>limb in coronagraph imagery. Although the majority of the ejecta is<br \/>expected to pass behind Earth, there is the possibility of a shock<br \/>enhancement late on November 6 to early on November 7. Region 4274<br \/>continued to be in a growth phase; however, the intermediate spots<br \/>appeared to begin to separate from the larger trailing spots.<br \/>\u00a0<br \/>An X1.1 flare was also observed on November 4 from a region just<br \/>beyond E limb near S15. Associated with this flare were a Type IV<br \/>radio sweep and a non-Earth directed CME observed off the SE limb on<br \/>November 4.<br \/>\u00a0<br \/>Solar wind parameters were mildly enhanced, but in decline. Solar<br \/>wind speed decreased from approximately 480 km\/s to nearly 420 km\/s. <\/p>\n<p>Solar activity is expected to be at moderate levels on November 3 to<br \/>17 to the delayed return of Regions 4246 and 4248, that seem to be<br \/>rotating into the Earthside solar disk between November 3 to 4. At<br \/>least two other regions are expected to emerge from the East limb<br \/>until November 10, as observed at GONG farside images.<\/p>\n<p>G1 storm is likely on November 7 to 8 due to reccurrence of CH HSS<br \/>influences. R1\/R2 radio blackouts are possible during the November 3<br \/>to 9 period due to the returning Regions 4246 and 4248. <\/p>\n<p>Weekly Commentary on the Sun, the Magnetosphere, and the Earth&#8217;s<br \/>Ionosphere, November 6, 2025, by F. K. Janda, OK1HH:<\/p>\n<p>The minimum activity of the Sun during its last rotation was recorded<br \/>at the end of October. The solar radio flux fell from 162 s.f.u.,<br \/>measured on October 15, to 115 s.f.u. on November 1. During the same<br \/>period, the number of sunspot groups on the solar disk decreased from<br \/>ten to two. However, coronal mass ejections, observed mainly near the<br \/>eastern limb of the solar disk, indicated that the level of activity<br \/>would soon increase rapidly.<\/p>\n<p>The solar flux then began to rise quickly, reaching 159 s.f.u. on<br \/>November 4. Energetically significant flares were produced mainly by<br \/>active region No. 4274, while the Earth&#8217;s atmosphere was hit by<br \/>protons with energies up to 10 MeV. The significantly intensified<br \/>solar wind was caused by the extensive coronal hole No. 94, which<br \/>passes through the central meridian at the same time. The onset of<br \/>the expected intense geomagnetic disturbance was predicted for<br \/>November 6, but it began a day earlier. On the evening of November 5,<br \/>it reached grade G3, with three-day indices up to K=6, while<br \/>continued until the forenoon hours of UTC the following day. The<br \/>effect on the ionosphere was very strong; from the beginning of the<br \/>disturbance, MUF values dropped significantly and remained very low<br \/>even on November 6.<\/p>\n<p>It appears that active region No. 4274 has enough energy in reserve<br \/>to continue its eruptive activity in the coming days. As the coronal<br \/>hole No. 94 shows no signs of shrinking, we can expect not only a<br \/>further increase in solar activity in the first half of November, but<br \/>also several geomagnetic disturbances. The effects on the Earth&#8217;s<br \/>ionosphere will be highly probable. Although MUF values will often<br \/>increase at the onset of disturbances, this will be followed by a<br \/>decrease accompanied by increased attenuation. This will very often<br \/>be accompanied by the scattering of radio waves on ionospheric<br \/>inhomogeneities.<\/p>\n<p>The latest video report from Dr. Tamitha Skov, WX6SWW, can be found<br \/>on YouTube.<\/p>\n<p>The Predicted Planetary A Index for November 8 to 14 is 25, 18, 12,<br \/>10, 5, 5, 5 with a mean of 11.4. Predicted Planetary K Index is 5, 4,<br \/>4, 3, 2, 2, 2 with a mean of 3.1. 10.7 centimeter flux 135, 135, 132,<br \/>140, 140, 145, 145 with a mean of 138.8.<\/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;Understanding Solar Indices&#8221; from September 2002 QST.<br \/>\u00a0<\/p>\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"http:\/\/www.arrl.org\/news\/view\/the-arrl-solar-update-8?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>11\/07\/2025 Solar activity has reached high levels due to a pair of X-classflares.\u00a0The first was an X1.8 on November 4 from Region 4274. Associatedwith the flare were Type IV radio&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-799046","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\/799046","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=799046"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/799046\/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=799046"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=799046"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=799046"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}