{"id":796297,"date":"2025-05-23T18:52:04","date_gmt":"2025-05-23T23:52:04","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=796297"},"modified":"2025-05-23T18:52:04","modified_gmt":"2025-05-23T23:52:04","slug":"the-arrl-solar-report-15","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=796297","title":{"rendered":"The ARRL Solar Report"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n\t\t\t\t\t<span class=\"date\">05\/23\/2025<\/span><\/p>\n<p><span>Solar activity ranged from low to high.<span>\u00a0 <\/span>Region 4087 produced the strongest event of the period, an impulsive R3 flare on May 14 at 0825 UTC near the NE limb.<span>\u00a0 <\/span>The region also produced R2 flares at 0325 and 1119 UTC.<span>\u00a0 <\/span>Finally, three R1 events were produced by the region on May 14 and 15.<span>\u00a0 <\/span>Region 4086 also produced an R3 event, with a flare observed on May 13 at 1538 UTC. <\/span><\/p>\n<p><span>No proton events were observed at geosynchronous orbit.<span>\u00a0 <\/span>However, a weak enhancement, which peaked below the S1 threshold, was observed on May 13 following the R3 event from Region 4086. <\/span><\/p>\n<p><span>Geomagnetic field activity was at quiet levels on May 12 and 13. Late on May 16, enhancements in solar wind parameters, associated with the onset of a positive polarity CH HSS and possible influence from the southern periphery of the CME that left the Sun on May 12, increased activity to active levels. <\/span><\/p>\n<p><span>Forecast of Solar and Geomagnetic Activity May 19 &#8211; June 14 2025: <\/span><\/p>\n<p><span>Solar activity is expected to be at low levels, with a chance for R1-R2 (minor-moderate) events, over the outlook period. <\/span><\/p>\n<p><span>No proton events are expected at geosynchronous orbit. <\/span><\/p>\n<p><span>The remainder of the outlook period is expected to be at normal to moderate levels. <\/span><\/p>\n<p><span>Geomagnetic field activity is likely to be elevated above quiet levels for most of the next 27 days due to multiple, recurrent, coronal hole features.<span>\u00a0 <\/span>G2 (moderate) conditions are likely on May 29 and June 13; G1 (minor) conditions likely on May 19, May 28, and June 14; active conditions are likely on May 30 &#8211; June 01, and June 10; unsettled levels are likely on May 20-23, May 27, June 02-07, and June 11-12.<span>\u00a0 <\/span>Quiet conditions are expected for the few remaining days of the outlook period. <\/span><\/p>\n<p><span>Weekly Commentary on the Sun, the Magnetosphere, and the Earth&#8217;s Ionosphere &#8211; May 22, 2025, from F. K. Janda, OK1HH. <\/span><\/p>\n<p><span>Compared to previous months, there was a significant decrease in solar activity in May.<span>\u00a0 <\/span>For example, on May 2, there were only two groups of spots on the entire solar disk observed.<span>\u00a0 <\/span>After that, spot activity in the northern half of the solar disk increased slightly, but solar flux dropped significantly during the second third of the month.<span>\u00a0 <\/span>Additionally, a large coronal hole appeared in the southern hemisphere of the sun.<span>\u00a0 <\/span>Although this coronal hole was observed during previous rotations in March and April, it is much larger this time. <\/span><\/p>\n<p><span>Consistent with this observation, after geomagnetic activity quieted down at the end of April, we experienced several days of strong geomagnetic disturbances in the first third of May.<span>\u00a0 <\/span>Starting in the second third of May, the solar flux dropped significantly, reaching values not seen since October 2024. <\/span><\/p>\n<p><span>The combination of low solar activity and high geomagnetic activity resulted in a significant deterioration of ionospheric shortwave propagation conditions, manifested by a drop in the critical frequencies of the F2 layer and an increase in attenuation and scattering.<span>\u00a0 <\/span>This occurred especially on May 7-12 and May 14-18, and is likely to continue in the coming days. <\/span><\/p>\n<p><span>The latest attempts to forecast further developments suggest that conditions should improve by the end of May.<span>\u00a0 <\/span>The summer ionosphere of the northern hemisphere of Earth is characterized by lower maximal frequencies and higher lows, not counting the sporadic layer E surprises. <\/span><\/p>\n<p><span>The Predicted Planetary A Index for May 24 to 30 is 6, 5, 5, 8, 25, 30, and 20, with a mean of 14.1.<span>\u00a0 <\/span>The Predicted Planetary K Index is 2, 2, 2, 3, 5, 6, and 4, with a mean of 3.4.<span>\u00a0 <\/span>10.7 centimeter flux is 120, 120, 120, 130, 135, 135, and 140, with a mean of 128.5. <span>\u00a0<\/span><\/span><\/p>\n<p><span>For more information concerning shortwave radio propagation, see  and the ARRL Technical Information Service web page at,  . For an explanation of numbers used in this bulletin, see  <span>\u00a0<\/span>. Information and tutorials on propagation can be found at,  . <\/span><\/p>\n<p><span>Also, check: <span>\u00a0<\/span><\/span><\/p>\n<p><span>&#8220;Understanding Solar Indices&#8221; from September 2002 QST: <\/span><\/p>\n<p><span>https:\/\/bit.ly\/3Rc8Njt<span>\u00a0 <\/span><\/span><\/p>\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"http:\/\/www.arrl.org\/news\/view\/the-arrl-solar-report-15?rand=771671\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>05\/23\/2025 Solar activity ranged from low to high.\u00a0 Region 4087 produced the strongest event of the period, an impulsive R3 flare on May 14 at 0825 UTC near the NE&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-796297","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\/796297","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=796297"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/796297\/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=796297"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=796297"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=796297"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}