{"id":2164,"date":"2012-06-23T21:56:58","date_gmt":"2012-06-24T02:56:58","guid":{"rendered":"https:\/\/kermitmurray.com\/murray\/?p=2164"},"modified":"2019-08-03T16:11:16","modified_gmt":"2019-08-03T21:11:16","slug":"finite-element-simulation-of-infrared-laser-ablation-for-mass-spectrometry","status":"publish","type":"post","link":"https:\/\/kermitmurray.com\/research\/2012\/06\/finite-element-simulation-of-infrared-laser-ablation-for-mass-spectrometry\/","title":{"rendered":"Finite element simulation of infrared laser ablation for mass spectrometry"},"content":{"rendered":"\n<div class=\"wp-block-caxton-grid relative\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-columns caxton-grid-block\" style=\"padding-top:0;padding-left:0;padding-bottom:0;padding-right:0;grid-template-columns:repeat(12, 1fr)\" data-tablet-css=\"padding-left:em;padding-right:em;\" data-mobile-css=\"padding-left:em;padding-right:em;\">\n<div class=\"wp-block-caxton-section relative\" style=\"grid-area:span 1\/span 12\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-section-block\" style=\"padding-top:5px;padding-left:5px;padding-bottom:5px;padding-right:5px\" data-mobile-css=\"padding-left:1em;padding-right:1em;\" data-tablet-css=\"padding-left:1em;padding-right:1em;\">\n<p>F. Huang, K.K. Murray, &#8220;Finite element simulation of infrared laser ablation for mass spectrometry,&#8221; <strong>26<\/strong> (2012) 2145\u20132150. doi:<a href=\"http:\/\/doi.org\/10.1002\/rcm.6331\">10.1002\/rcm.6331<\/a>.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-caxton-grid relative\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-columns caxton-grid-block\" style=\"padding-top:0;padding-left:0;padding-bottom:0;padding-right:0;grid-template-columns:repeat(12, 1fr)\" data-tablet-css=\"padding-left:em;padding-right:em;\" data-mobile-css=\"padding-left:em;padding-right:em;\">\n<div class=\"wp-block-caxton-section relative\" style=\"grid-area:span 1\/span 8\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-section-block\" style=\"padding-top:5px;padding-left:5px;padding-bottom:5px;padding-right:5px\" data-mobile-css=\"padding-left:1em;padding-right:1em;\" data-tablet-css=\"padding-left:1em;padding-right:1em;\">\n<p><em>Abstract<\/em><\/p>\n\n\n\n<p class=\"has-small-font-size\">RATIONALE: Laser ablation is widely used in conjunction with ambient ionization techniques, and a fundamental understanding of the mechanism of material removal is important to its optimal use in mass spectrometry. Finite element analysis simulates the laser material interaction on larger time and distance scales than atomistic approaches. Here, a two-dimensional finite element model was developed to simulate infrared laser irradiation of glycerol using a wavelength-tunable infrared (IR) laser.<\/p>\n\n\n\n<p class=\"has-small-font-size\">METHODS: The laser fluence used for the simulations was varied from 1000 to 6000 J\/m(2) , the wavelength was varied from 2.7 to 3.7 \u00b5m, and both flat-top and Gaussian shape laser profiles were studied.<\/p>\n\n\n\n<p class=\"has-small-font-size\">RESULTS: Phase explosion conditions were found for laser wavelengths near 3 \u00b5m (which corresponds to the OH stretch absorption of glycerol) and fluences above 2000 J\/m(2) . This suggests that laser ablation of glycerol is driven by phase explosion in the OH stretch region. The Gaussian profile generated regions of higher glycerol temperature, whereas the flat-top profile heated a larger volume of material above the phase explosion temperature.<\/p>\n\n\n\n<p class=\"has-small-font-size\">CONCLUSIONS: These results suggest that the best performance for pulsed IR laser sample irradiation is in the wavelength range from 2.9 to 3.1 \u00b5m for materials with a strong OH stretch absorption. <\/p>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-caxton-section relative\" style=\"grid-area:span 1\/span 4\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-section-block\" style=\"padding-top:5px;padding-left:5px;padding-bottom:5px;padding-right:5px\" data-mobile-css=\"padding-left:1em;padding-right:1em;\" data-tablet-css=\"padding-left:1em;padding-right:1em;\">\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"294\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2019\/07\/Graphical-Abstract.jpg\" alt=\"\" class=\"wp-image-2165\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Graphical-Abstract.jpg 500w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Graphical-Abstract-300x176.jpg 300w\" sizes=\"auto, (max-width: 500px) 100vw, 500px\" \/><figcaption>Huang, Murray, Finite element simulation of infrared laser ablation for mass spectrometry, 26 (2012) 2145.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"671\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2019\/07\/Figure-5-1024x671.jpg\" alt=\"\" class=\"wp-image-2166\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Figure-5-1024x671.jpg 1024w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Figure-5-300x197.jpg 300w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Figure-5-768x503.jpg 768w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Figure-5-1568x1028.jpg 1568w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption>Laser wavelength dependence of glycerol surface temperature for fluences: (\u25a0) 1000 , (\u25cb) 2000, (\u25b2) 3000 , (\u25a1) 4000, (\u25cf) 5000 , and (\u0394) 6000 J\/m^2.<\/figcaption><\/figure>\n<\/div><\/div>\n<\/div><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":2166,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[81,134,5],"tags":[95,96,8,135,77],"class_list":["post-2164","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-fundamentals","category-lsu","category-publication","tag-finite-element","tag-glycerol","tag-infrared","tag-lsu","tag-publication","entry"],"_links":{"self":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2164","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/comments?post=2164"}],"version-history":[{"count":2,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2164\/revisions"}],"predecessor-version":[{"id":2168,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2164\/revisions\/2168"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/media\/2166"}],"wp:attachment":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/media?parent=2164"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/categories?post=2164"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/tags?post=2164"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}