{"id":31248,"date":"2019-01-02T23:59:29","date_gmt":"2019-01-02T23:59:29","guid":{"rendered":"http:\/\/cimss.ssec.wisc.edu\/satellite-blog\/?p=31248"},"modified":"2019-01-03T20:15:31","modified_gmt":"2019-01-03T20:15:31","slug":"strong-jet-stream-over-the-north-pacific-ocean","status":"publish","type":"post","link":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/archives\/31248","title":{"rendered":"Strong jet stream over the North Pacific Ocean"},"content":{"rendered":"<div style=\"width: 653px\" class=\"wp-caption aligncenter\"><a class=\"thumbnail\" href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes17_waterVapor_250hPa_isotachs_North_Pacific_anim.gif\"><img loading=\"lazy\" decoding=\"async\" class=\"thumbnail\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/g17_wv_jet-20190102_180038.png\" alt=\"GOES-17 Mid-level Water Vapor (6.9 \u00b5m) images, with 250 hPa wind isotachs [click to play animation | MP4]\" width=\"643\" height=\"371\" \/><\/a><p class=\"wp-caption-text\">GOES-17 Mid-level Water Vapor <em>(6.9 \u00b5m)<\/em> images, with 250 hPa wind isotachs [click to play animation | <a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes17_waterVapor_250hPa_isotachs_North_Pacific_anim.mp4\"><strong>MP4<\/strong><\/a>]<\/p><\/div>\n<p style=\"text-align: center;\"><em>* GOES-17 images shown here are preliminary and non-operational *<\/em><\/p>\n<p>GOES-17 Mid-level Water Vapor (<a href=\"http:\/\/cimss.ssec.wisc.edu\/goes\/OCLOFactSheetPDFs\/ABIQuickGuide_Band09.pdf\"><strong>6.9 \u00b5m<\/strong><\/a>) images with an overlay of 250 hPa wind isotachs from the GFS90 model <em><strong>(above)<\/strong><\/em> showed a string of disturbances (<a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_18utc_surface_analysis_N_Pacific.png\"><strong>surface analysis<\/strong><\/a>) along the axis of a 180-knot &#8220;Japan Jet&#8221; across the North Pacific Ocean on 02 January 2019.<\/p>\n<p>GOES-17 <a href=\"http:\/\/cimss.ssec.wisc.edu\/goes\/OCLOFactSheetPDFs\/ABIQuickGuide_SplitOzoneDiff.pdf\"><strong>Split Ozone<\/strong><\/a> (<a href=\"http:\/\/cimss.ssec.wisc.edu\/goes\/OCLOFactSheetPDFs\/ABIQuickGuide_Band12.pdf\"><strong>9.6 \u00b5m<\/strong><\/a> &#8211; <strong><a href=\"http:\/\/cimss.ssec.wisc.edu\/goes\/OCLOFactSheetPDFs\/ABIQuickGuide_Band13.pdf\">10.3 \u00b5m<\/a><\/strong>) Brightness Temperature Difference images <em><strong>(below)<\/strong><\/em> include an overlay of PV1.5 pressure (an indicator of the height of the &#8220;dynamic tropopause&#8221;) &#8212; they showed the difference between cold polar air having a low tropopause <em>(shades of cyan to blue)<\/em> north of the jet stream and warm tropical air having a much higher tropopause<em> (shades of yellow)<\/em>. The Split Ozone BTD is the Green component of the Air Mass Red-Green-Blue (RGB) product.<\/p>\n<p><div style=\"width: 650px\" class=\"wp-caption aligncenter\"><a class=\"thumbnail\" href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes17_splitOzone_pv1.5pressure_North_Pacific_anim.gif\"><img loading=\"lazy\" decoding=\"async\" class=\"thumbnail\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/g17_splitOzone_pv1.5-20190102_180038.png\" alt=\"GOES-17 Split Ozone (9.6 - 10.3 \u00b5m) images, with contours of PV1.5 pressure [click to play animation | MP4]\" width=\"640\" height=\"369\" \/><\/a><p class=\"wp-caption-text\">GOES-17 Split Ozone <em>(9.6 &#8211; 10.3 \u00b5m)<\/em> images, with contours of PV1.5 pressure [click to play animation | <a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes17_splitOzone_pv1.5pressure_North_Pacific_anim.mp4\"><strong>MP4<\/strong><\/a>]<\/p><\/div><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_PASN_PHLI_RAOBS.TEXT\"><strong>Rawinsonde data<\/strong><\/a> also showed the significant difference in tropopause height between St. Paul Island, Alaska <em>(pressure=314 hPa, height=8.1 km)<\/em> in the polar air of the Bering Sea and Lihue, Hawai&#8217;i <em>(pressure=82 hPa, height=17.9 km)<\/em> in the tropical air of the central Pacific <em><strong>(below)<\/strong><\/em>.<\/p>\n<p><div style=\"width: 650px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_PASN_RAOBS.GIF\"><img loading=\"lazy\" decoding=\"async\" class=\"\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_PASN_RAOBS.GIF\" alt=\"Plots of rawinsonde data from St. Paul Island, Alaska [click to enlarge]\" width=\"640\" height=\"425\" \/><\/a><p class=\"wp-caption-text\">Plots of rawinsonde data from St. Paul Island, Alaska [click to enlarge]<\/p><\/div><div style=\"width: 651px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_PHLI_RAOBS.GIF\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_PHLI_RAOBS.GIF\" alt=\"Plots of rawinsonde data from Lihue, Hawai'i [click to enlarge]\" width=\"641\" height=\"426\" \/><\/a><p class=\"wp-caption-text\">Plots of rawinsonde data from Lihue, Hawai&#8217;i [click to enlarge]<\/p><\/div>GOES-17 <a href=\"http:\/\/rammb.cira.colostate.edu\/training\/visit\/quick_guides\/QuickGuide_GOESR_AirMassRGB_final.pdf\"><strong>Air Mass RGB<\/strong><\/a> images from the <a href=\"https:\/\/www.aos.wisc.edu\/weather\/wx_obs\/GOES17.html\"><strong>UW-AOS<\/strong><\/a> site <em><strong>(below)<\/strong><\/em> further illustrated the sharp contrast between the cold\/dry polar air to the north and warm\/moist tropical air to the south of the strong jet stream. The purple hues along the northwestern edge of the scan are a result of the &#8220;limb cooling&#8221; effect, as the satellite&#8217;s infrared detectors sense radiation from colder upper levels of the atmosphere at large viewing angles.<\/p>\n<p><div style=\"width: 651px\" class=\"wp-caption aligncenter\"><a class=\"thumbnail\" href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes17_airmassRGB_North_Pacific_anim.gif\"><img loading=\"lazy\" decoding=\"async\" class=\"thumbnail\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/20190102180038_npac.jpg\" alt=\"GOES-17 Air Mass RGB images [click to play animation | MP4]\" width=\"641\" height=\"429\" \/><\/a><p class=\"wp-caption-text\">GOES-17 Air Mass RGB images [click to play animation | <a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes17_airmassRGB_North_Pacific_anim.mp4\"><strong>MP4<\/strong><\/a>]<\/p><\/div>In addition to the series of larger disturbances along the jet stream axis, there were also some smaller-scale storms apparent in the Bering Sea (<a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_surface_analyses_West_Pacific_anim.gif\"><strong>surface analyses<\/strong><\/a>). Better detail of these high-latitude features could be seen using Suomi NPP VIIRS Day\/Night Band (0.7 \u00b5m) and Infrared Window (11.45 \u00b5m) images separated by 10 hours <em><strong>(below)<\/strong><\/em>.<\/p>\n<p><div style=\"width: 651px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_suomiNPP_viirs_dayNightBand_infraredWindow_Bering_Sea_anim.gif\"><img loading=\"lazy\" decoding=\"async\" class=\"\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_suomiNPP_viirs_dayNightBand_infraredWindow_Bering_Sea_anim.gif\" alt=\"Suomi NPP VIIRS Day\/Night Band (0.7 \u00b5m) and Infrared Window (11.45 \u00b5m) images at 1427 UTC and 0022 UTC [click to enlarge]\" width=\"641\" height=\"370\" \/><\/a><p class=\"wp-caption-text\">Suomi NPP VIIRS Day\/Night Band (0.7 \u00b5m) and Infrared Window (11.45 \u00b5m) images at 1427 UTC and 0022 UTC [click to enlarge]<\/p><\/div>Regarding the strong Japan Jet, GOES-15 <em>(GOES-West)<\/em> Derived Motion Winds (<a href=\"http:\/\/tropic.ssec.wisc.edu\/real-time\/windmain.php?&amp;basin=eastpac&amp;sat=wg9&amp;prod=wvir&amp;zoom=&amp;time=\"><strong>source<\/strong><\/a>) tracked targets having velocities as high as 200 knots at <a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_03utc_wvwinds.png\"><strong>03 UTC<\/strong><\/a> <em><strong>(below)<\/strong><\/em>.<\/p>\n<div style=\"width: 649px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes15_waterVapor_winds_North_Pacific_anim.gif\"><img loading=\"lazy\" decoding=\"async\" class=\"\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2019\/01\/190102_goes15_waterVapor_winds_North_Pacific_anim.gif\" alt=\"GOES-15 Water Vapor (6.5 \u00b5m) Derived Motion Winds [click to enlarge]\" width=\"639\" height=\"484\" \/><\/a><p class=\"wp-caption-text\">GOES-15 Water Vapor <em>(6.5 \u00b5m)<\/em> Derived Motion Winds [click to enlarge]<\/p><\/div>\n","protected":false},"excerpt":{"rendered":"<p>* GOES-17 images shown here are preliminary and non-operational * GOES-17 Mid-level Water Vapor (6.9 \u00b5m) images with an overlay of 250 hPa wind isotachs from the GFS90 model (above) showed a string of disturbances (surface analysis) along the axis of a 180-knot &#8220;Japan Jet&#8221; across the North Pacific Ocean on 02 January 2019. GOES-17 [&hellip;]<\/p>\n","protected":false},"author":18,"featured_media":31250,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"footnotes":""},"categories":[43,80,45,25,49,48],"tags":[],"class_list":["post-31248","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-goes-15","category-goes-17","category-redgreenblue-rgb-images","category-satellite-winds","category-suomi_npp","category-viirs"],"acf":[],"_links":{"self":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/31248","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=31248"}],"version-history":[{"count":11,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/31248\/revisions"}],"predecessor-version":[{"id":31260,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/31248\/revisions\/31260"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/media\/31250"}],"wp:attachment":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/media?parent=31248"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/categories?post=31248"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/tags?post=31248"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}