{"id":4511,"date":"2010-02-09T23:59:03","date_gmt":"2010-02-09T23:59:03","guid":{"rendered":"http:\/\/cimss.ssec.wisc.edu\/satellite-blog\/?p=4511"},"modified":"2010-02-12T22:12:28","modified_gmt":"2010-02-12T22:12:28","slug":"strong-potential-vorticity-anomaly-off-the-california-coast","status":"publish","type":"post","link":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/archives\/4511","title":{"rendered":"Strong potential vorticity anomaly off the California coast"},"content":{"rendered":"<div style=\"width: 490px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100209_g11_wv_anim.gif\"><img loading=\"lazy\" decoding=\"async\" alt=\"GOES waver vapor imagery + PV1.5 pressure + 500 hPa geopotential height\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100209_g11_wv_anim.gif\" title=\"GOES waver vapor imagery + PV1.5 pressure + 500 hPa geopotential height\" width=\"480\" height=\"459\" \/><\/a><p class=\"wp-caption-text\">GOES waver vapor imagery + PV1.5 pressure + 500 hPa geopotential height<\/p><\/div>\n<p>A strong potential vorticity (PV) anomaly was propagating southeastward just off the California coast on <strong><a href=\"http:\/\/www.hpc.ncep.noaa.gov\/dailywxmap\/index_20100209.html\">09 February 2010<\/a><\/strong> &#8212; and this feature had a  striking presentation on AWIPS images of GOES-11 water vapor channel data <strong><em>(above)<\/em><\/strong>, with a  pronounced  arc of very dry air <em>(yellow color enhancement)<\/em>  seen around the periphery of the circulation. According to the <strong><a href=\"http:\/\/cimss.ssec.wisc.edu\/cras\/\">CRAS model<\/a><\/strong> fields, the tropopause <em>(taken to be the pressure of the PV1.5 surface)<\/em> was being brought downward as low as the 600 hPa pressure level within the core of the PV anomaly.<\/p>\n<p>Images of the GOES-11 sounder Total Column Ozone derived product <strong><em>(below)<\/em><\/strong> depicted ozone values as high as 430 Dobson Units <em>(red color enhancement)<\/em> in the vicinity of the PV anomaly, supporting the idea that the tropopause height was very depressed within the circulation feature.<\/p>\n<div style=\"width: 490px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100209_g11_ozone_anim.gif\"><img loading=\"lazy\" decoding=\"async\" alt=\"GOES sounder Total Column Ozone + PV1.5 pressure + 500 hPa geoptential height\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100209_g11_ozone_anim.gif\" title=\"GOES sounder Total Column Ozone + PV1.5 pressure + 500 hPa geoptential height\" width=\"480\" height=\"459\" \/><\/a><p class=\"wp-caption-text\">GOES sounder Total Column Ozone + PV1.5 pressure + 500 hPa geoptential height<\/p><\/div>\n<p>=================================<\/p>\n<div style=\"width: 490px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100209_wv_4panel_anim.gif\"><img loading=\"lazy\" decoding=\"async\" alt=\"GOES-11 Sounder and Imager water vapor channel images\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100209_wv_4panel_anim.gif\" title=\"GOES-11 Sounder and Imager water vapor channel images\" width=\"480\" height=\"459\" \/><\/a><p class=\"wp-caption-text\">GOES-11 Sounder and Imager water vapor channel images<\/p><\/div>\n<p>A 4-panel comparison of the three water vapor channels on the GOES-11 Sounder <em>(6.5 \u00c2\u00b5m, 7.0 \u00c2\u00b5m, and 7.4 \u00c2\u00b5m)<\/em> and the GOES-11 Imager 6.7 \u00c2\u00b5m water vapor channel <strong><em>(above)<\/em><\/strong> showed that the dry air signature was even quite evident on the Sounder 6.5 \u00c2\u00b5m channel <em>(darker blue color enhancement, upper left panels)<\/em> &#8212; this particular water vapor channel weighting function normally peaks quite high in the atmosphere <em>(around 325 hPa),<\/em> where these types of water vapor gradients and signatures are usually not as well-defined. <\/p>\n<p>However, due to the dry air within the middle to upper troposphere associated with the PV anomaly, the <strong><a href=\"http:\/\/cimss.ssec.wisc.edu\/goes\/wf\/\">weighting functions<\/a><\/strong> of all 4 of the GOES-11 water vapor channels <em>(calculated using rawinsonde data from Vandenberg Air Force Base)<\/em> peaked at altitudes that were quite a bit lower  compared to the more &#8220;normal&#8221; conditions that would be seen in a US Standard Atmosphere or USSA environment <strong><em>(below)<\/em><\/strong>. Convection moving onshore across southern California that day was responsible for at least one sighting of a waterspout in the San Diego area, and inland precipitation amounts of 1.0 to 1.5 inch were widespread.<\/p>\n<div style=\"width: 490px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100210_wf_anim.gif\"><img loading=\"lazy\" decoding=\"async\" alt=\"GOES-11 sounder and imager water vapor weighting functions (Vandenberg vs USSA)\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2010\/02\/100210_wf_anim.gif\" title=\"GOES-11 sounder and imager water vapor weighting functions (Vandenberg vs USSA)\" width=\"480\" height=\"280\" \/><\/a><p class=\"wp-caption-text\">GOES-11 sounder and imager water vapor weighting functions (Vandenberg vs USSA)<\/p><\/div>\n","protected":false},"excerpt":{"rendered":"<p>A strong potential vorticity (PV) anomaly was propagating southeastward just off the California coast on 09 February 2010 &#8212; and this feature had a striking presentation on AWIPS images of GOES-11 water vapor channel data (above), with a pronounced arc of very dry air (yellow color enhancement) seen around the periphery of the circulation. According [&hellip;]<\/p>\n","protected":false},"author":18,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"footnotes":""},"categories":[15,18],"tags":[],"class_list":["post-4511","post","type-post","status-publish","format-standard","hentry","category-goes-sounder","category-goes-11"],"acf":[],"_links":{"self":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/4511","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/users\/18"}],"replies":[{"embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/comments?post=4511"}],"version-history":[{"count":8,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/4511\/revisions"}],"predecessor-version":[{"id":4535,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/4511\/revisions\/4535"}],"wp:attachment":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/media?parent=4511"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/categories?post=4511"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/tags?post=4511"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}