{"id":795241,"date":"2025-04-11T14:46:05","date_gmt":"2025-04-11T19:46:05","guid":{"rendered":"http:\/\/spaceweekly.com\/?p=795241"},"modified":"2025-04-11T14:46:05","modified_gmt":"2025-04-11T19:46:05","slug":"the-arrl-solar-report-10","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=795241","title":{"rendered":"The ARRL Solar Report"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">04\/11\/2025<\/span><\/p>\n<p>Due to most of the regions on the solar disk being fairly simple in<br \/>their magnetic complexity, solar activity is expected to remain at<br \/>low levels with a chance for M-class flares (R1 to R2, or Minor to<br \/>Moderate).<\/p>\n<p>Solar wind parameters are expected to trend further towards nominal<br \/>levels as the Coronal Hole High-Speed Stream effects continue to<br \/>wane.<\/p>\n<p>Additional enhancements from another negative polarity Coronal Hole<br \/>is likely on April 12, combined with potential effects from the<br \/>glancing blow of a Coronal Mass Ejection that left the Sun on April<br \/>8.\u00a0 Elevated conditions are likely to continue through April 13 as<br \/>the influences persist of the Coronal Hole.<\/p>\n<p>Solar activity has been at moderate levels for the past 24 hours.<br \/>There are currently 8 numbered sunspot regions on the disk.\u00a0 Solar<br \/>activity is expected to be low with a chance for M-class flares on<br \/>April 12.<\/p>\n<p>The long range forecast of Solar and Geomagnetic Activity for April<br \/>12 to May 3:<\/p>\n<p>The declining trend in solar flux and activity is expected to bottom<br \/>out around April 15, after which a slowly increasing period is<br \/>expected. The anticipated return on April 22 of the active<br \/>longitudes that gave rise to Region AR4046 (responsible for X-flare<br \/>activity) should bring solar activity to moderate and occasionally<br \/>high levels through the end of the forecast period.<\/p>\n<p>No proton events are expected at geosynchronous orbit until the<br \/>expected increase in flare activity beginning on April 22. Then<br \/>there will be an increasing chance for an isolated proton event as<br \/>the more potent regions approach the west limb by the end of the<br \/>forecast period.<\/p>\n<p>Flux will subside to moderate levels after April 12 as the effects<br \/>from the fast stream wane. April 19 is expected to bring a return to<br \/>high levels, again in response to another recurrent fast stream. The<br \/>elevated conditions are expected to remain through April 28 before<br \/>returning to moderate levels.<\/p>\n<p>Geomagnetic field activity is expected to be primarily quiet to<br \/>unsettled, with an isolated active period, until the return of a<br \/>recurrent geoeffective coronal hole between April 19 to 21. Active<br \/>conditions are expected to prevail through April 24 before the fast<br \/>solar wind stream wanes.<\/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>The predicted Planetary A Index for April 12 to 18 is 12, 12, 12, 8,<br \/>5, 5, and 5, with a mean of 8.4.\u00a0 The predicted Planetary K Index is<br \/>3, 3, 3, 3, 2, 2, and 2, with a mean of 2.6.\u00a0 Predicted 10.7<br \/>centimeter flux is 140, 140, 140, 135, 140, 140, and 145, with a<br \/>mean of 140.<\/p>\n<p>\u00a0<\/p>\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"http:\/\/www.arrl.org\/news\/view\/the-arrl-solar-report-9?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>04\/11\/2025 Due to most of the regions on the solar disk being fairly simple intheir magnetic complexity, solar activity is expected to remain atlow levels with a chance for M-class&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-795241","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\/795241","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=795241"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/795241\/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=795241"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=795241"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=795241"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}