{"id":62924,"date":"2025-01-31T20:39:29","date_gmt":"2025-01-31T20:39:29","guid":{"rendered":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/?p=62924"},"modified":"2025-01-31T21:04:02","modified_gmt":"2025-01-31T21:04:02","slug":"lightningcast-version-2","status":"publish","type":"post","link":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/archives\/62924","title":{"rendered":"LightningCast version 2"},"content":{"rendered":"\n<p>The <a href=\"https:\/\/cimss.ssec.wisc.edu\/pltg.html\">ProbSevere LightningCast<\/a> version 1 (v1) model uses machine learning and GOES-R Advanced Baseline Imager (ABI) data to predict the probability of lightning in the next 60 minutes. This version will be operational at NOAA later in 2025.<\/p>\n\n\n\n<p>As research and development continues, a new version of the model (LightningCast v2) adds Multi-Radar Multi-Sensor (MRMS) Reflectivity at -10<sup>o<\/sup>C as a predictor. Reflectivity at -10<sup>o<\/sup>C is well correlated with imminent lightning activity due to its ability to depict hydrometeors in the mixed-phase region of convection (generally 0<sup>o<\/sup>C to -20<sup>o<\/sup>C). Other radar-derived parameters are being investigated as well.<\/p>\n\n\n\n<p>Preliminary results demonstrate that the radar-derived predictor adds value to the problem of short-term lightning prediction, without diminishing the power of the satellite predictors&#8212;<strong>that is, the model appears to have learned and uses the strengths of each data source for making better predictions.<\/strong> <\/p>\n\n\n\n<p>Here are two recent examples. First, in Ohio and Pennsylvania, warm air advection at 850 and 700 mb forced some elevated but shallow thunderstorms. <\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"385\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/850-700mb_WAA-1024x385.png\" alt=\"\" class=\"wp-image-62925\" srcset=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/850-700mb_WAA-1024x385.png 1024w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/850-700mb_WAA-300x113.png 300w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/850-700mb_WAA-768x289.png 768w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/850-700mb_WAA-1536x577.png 1536w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/850-700mb_WAA-2048x770.png 2048w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\">Figure 1: 850 mb (left) and 700 mb (right) analyses from the Storm Prediction Center&#8217;s mesoscale analysis page (from 16-17 UTC on 01\/31\/2025). The filled red areas are regions with warm air advection.<\/figcaption><\/figure>\n\n\n\n<p>A short-term model profile from the NAM 3-km model also shows the elevated but abbreviated extent of CAPE.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"899\" height=\"1024\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/profile_20250131-899x1024.png\" alt=\"\" class=\"wp-image-62928\" style=\"width:600px\" srcset=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/profile_20250131-899x1024.png 899w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/profile_20250131-263x300.png 263w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/profile_20250131-768x875.png 768w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/profile_20250131.png 1152w\" sizes=\"auto, (max-width: 899px) 100vw, 899px\" \/><figcaption class=\"wp-element-caption\">Figure 2: A skew-T log-P chart showing the thermal and moisture profile from southwest Pennsylvania at 18Z on 01\/31\/2025. The profile is from <a href=\"http:\/\/www.pivotalweather.com\">www.pivotalweather.com<\/a> and powered by <a href=\"https:\/\/sharp.weather.ou.edu\/dev\/\">SHARPpy<\/a>.<\/figcaption><\/figure>\n<\/div>\n\n\n<p>The first animation below is from LightningCast v1. The shallow nature of the storms and the thick layer of ice clouds above the convection obscures key signatures for the satellite-only model, resulting in poor probabilistic guidance. <\/p>\n\n\n\n<figure class=\"wp-block-video\"><video height=\"720\" style=\"aspect-ratio: 1280 \/ 720;\" width=\"1280\" controls src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/abi_20250131.mp4\"><\/video><figcaption class=\"wp-element-caption\">Figure 3: Animation of LightningCast v1 (contours), GOES-16 day-cloud-phase-distinction RGB (background), and GLM flash-extent density (foreground).<\/figcaption><\/figure>\n\n\n\n<p>The animation below uses the LightningCast v2 model.  While not a cure-all, the reflectivity at -10<sup>o<\/sup>C clearly helps the model provide better guidance to lightning, albeit with little lead time to lightning initiation in this case. <\/p>\n\n\n\n<figure class=\"wp-block-video\"><video height=\"720\" style=\"aspect-ratio: 1280 \/ 720;\" width=\"1280\" controls src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/abi-mrms_20250131.mp4\"><\/video><figcaption class=\"wp-element-caption\">Figure 4: Animation of LightningCast 2 (contours), GOES-16 day-cloud-phase-distinction RGB (background), and GLM flash-extent density (foreground).<\/figcaption><\/figure>\n\n\n\n<p>The day prior, weak 850 mb warm air advection forced convective development in northeast Colorado and southwest Nebraska. The thermal profile appeared to be too cold to generate much CAPE or lightning.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"771\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1024x771.png\" alt=\"\" class=\"wp-image-62935\" style=\"width:850px\" srcset=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1024x771.png 1024w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-300x226.png 300w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-768x578.png 768w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1536x1156.png 1536w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image.png 2020w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\">Figure 5: 850 mb analysis from the Storm Prediction Center&#8217;s mesoscale analysis page<\/figcaption><\/figure>\n<\/div>\n\n\n<p>However, from a satellite perspective, the convection certainly <em>looks<\/em> like it could produce lightning. Thus, the LightningCast v1 output shows high probabilities of lightning (animation below).<\/p>\n\n\n\n<figure class=\"wp-block-video\"><video height=\"720\" style=\"aspect-ratio: 1280 \/ 720;\" width=\"1280\" controls src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/c02051315_20250130_NE.mp4\"><\/video><figcaption class=\"wp-element-caption\">Figure 6: Animation of LightningCast v1 (contours), GOES-16 day-cloud-phase-distinction RGB (background), and GLM flash-extent density (foreground).<\/figcaption><\/figure>\n\n\n\n<p>But the reflectivity at -10<sup>o<\/sup>C predictor generally has convective cores of only 25-30 dBZ. Typically 35-40 dBZ is needed for lightning at this isotherm.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"656\" src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1-1024x656.png\" alt=\"\" class=\"wp-image-62939\" style=\"width:700px\" srcset=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1-1024x656.png 1024w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1-300x192.png 300w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1-768x492.png 768w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1-1536x984.png 1536w, https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/image-1.png 2002w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\">Figure 7: MRMS reflectivity at -10<sup>o<\/sup>C, from the <a href=\"https:\/\/mrms.nssl.noaa.gov\/qvs\/product_viewer\/\">MRMS operational product viewer<\/a>.<\/figcaption><\/figure>\n<\/div>\n\n\n<p>The radar predictor helped reduce the false alarm predictions of lightning markedly. See the animation of LightningCast v2 predictions below.<\/p>\n\n\n\n<figure class=\"wp-block-video\"><video height=\"720\" style=\"aspect-ratio: 1280 \/ 720;\" width=\"1280\" controls src=\"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-content\/uploads\/sites\/5\/2025\/01\/ref10_20250130_NE.mp4\"><\/video><figcaption class=\"wp-element-caption\">Figure 8: Animation of LightningCast 2 (contours), GOES-16 day-cloud-phase-distinction RGB (background), and GLM flash-extent density (foreground).<\/figcaption><\/figure>\n\n\n\n<p>Overall, we&#8217;ve found that LightningCast v2 improves the critical success index over the contiguous U.S. (CONUS), while not harming predictions outside of the CONUS. In the image below, red regions show improvement of v2 over v1, whereas blue regions show degradation of performance in v2, with respect to v1 (note that this is a limited sample).<\/p>\n\n\n\n<figure class=\"wp-block-image\"><img decoding=\"async\" src=\"https:\/\/lh7-rt.googleusercontent.com\/slidesz\/AGV_vUfPQcCFLsE2HYHfrl_rw9m9_D5c0yK7_ZmHEUYHE4abvIJd6XXislfRponXdAT2alPOcLRpI2NmLmPLCkoeNtmzQR3qiD5FPrhVNnncgL0cboCbxHOlJU8K4lmKbWMByZYX04hzbBpm1ozpEsMTfDWln0FWS6Q=s2048?key=TTfUQ18hqFGM4UCOA9GoeA\" alt=\"\" \/><figcaption class=\"wp-element-caption\">Figure 9: The difference in performance between LightningCast v2 and LightningCast v1 (red is where v2 is better; blue is where v1 is better). Note that these results are preliminary. <\/figcaption><\/figure>\n\n\n\n<p>An assessment of lead time to lightning initiation (LI) has shown that rather than diminishing lead time to LI, LightningCast v2 actually appears to increase lead time to LI over the CONUS by a small amount. Work is on-going to quantify how much ABI predictors alone increase lead time to LI ahead of a radar-only lightning nowcasting model. We hope to have forecasters evaluate LightningCast v2 at the 2025 Hazardous Weather Testbed. <\/p>\n","protected":false},"excerpt":{"rendered":"<p>The ProbSevere LightningCast version 1 (v1) model uses machine learning and GOES-R Advanced Baseline Imager (ABI) data to predict the probability of lightning in the next 60 minutes. This version will be operational at NOAA later in 2025. As research and development continues, a new version of the model (LightningCast v2) adds Multi-Radar Multi-Sensor (MRMS) [&hellip;]<\/p>\n","protected":false},"author":14,"featured_media":62935,"comment_status":"closed","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"footnotes":""},"categories":[10,74,115,59],"tags":[85,84,111,87],"class_list":["post-62924","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-general-interpretation","category-goes-16","category-lightningcast","category-probsevere","tag-glm","tag-goes-16","tag-lightningcast","tag-probsevere"],"acf":[],"_links":{"self":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/62924","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\/14"}],"replies":[{"embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/comments?post=62924"}],"version-history":[{"count":10,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/62924\/revisions"}],"predecessor-version":[{"id":62960,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/posts\/62924\/revisions\/62960"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/media\/62935"}],"wp:attachment":[{"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/media?parent=62924"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/categories?post=62924"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/cimss.ssec.wisc.edu\/satellite-blog\/wp-json\/wp\/v2\/tags?post=62924"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}