{"id":8733,"date":"2012-12-19T09:52:14","date_gmt":"2012-12-19T09:52:14","guid":{"rendered":"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=8733"},"modified":"2023-03-10T15:40:30","modified_gmt":"2023-03-10T15:40:30","slug":"non-covalent-interactions-in-the-sharpless-transition-state-for-asymmetric-epoxidation","status":"publish","type":"post","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=8733","title":{"rendered":"Non covalent interactions in the Sharpless transition state for asymmetric epoxidation."},"content":{"rendered":"<div class=\"kcite-section\" kcite-section-id=\"8733\">\n<p>The Sharpless epoxidation of an allylic alcohol had a big impact on synthetic chemistry when it was introduced in the 1980s, and led the way for the discovery (design?) of many new asymmetric catalytic systems. Each achieves its chiral magic by control of the geometry at the transition state for the reaction, and the stabilizations (or destabilizations) that occur at that geometry. These in turn can originate from factors such as stereoelectronic control or simply by the overall sum of many small attractions and repulsions we call <em>dispersion interactions<\/em>. Here I take an initial look at these for the binuclear transition state shown schematically below.<\/p>\n<p><img decoding=\"async\" class=\"aligncenter size-full wp-image-8659\" alt=\"sharpless-binuclear\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/12\/sharpless-binuclear.svg\" \/><\/p>\n<p>The NCI method was described recently<span id=\"cite_ITEM-8733-0\" name=\"citation\"><a href=\"#ITEM-8733-0\">[1]<\/a><\/span> as a method for probing the non-covalent electron density in a molecule. It does this by cleverly filtering out the covalent density <em>via<\/em> computing a first derivative of the density \u03c1(r) called the <i>reduced density gradient<\/i> and taking the band of values appropriate for non-covalent densities. By inspecting the <a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=2183\" target=\"_blank\" rel=\"noopener\">Laplacian<\/a> of these densities at any point in space, the region can be characterised as attractive, repulsive or neutral. Visually, this information can be transformed into isosurfaces which are colour coded depending on whether the region is attractive (=blue to green) or repulsive (yellow to red). In the <a href=\"connect (atomno=9) (atomno=97) PARTIAL;connect (atomno=9) (atomno=96) PARTIAL;connect (atomno=9) (atomno=10) PARTIAL;connect (atomno=9) (atomno=2) PARTIAL;connect (atomno=1) (atomno=2) NONE;\" target=\"_blank\" rel=\"noopener\">previous post<\/a>, it turned out that the attractive contributions to the dispersion energies differed for the two diasteromeric transition states (in the conformations calculated) by about 2.6 kcal\/mol. Shown below are the two NCI surfaces for these which allow one to get some insight into where this overall contribution might come from (together with weak hydrogen bonds and other non-covalent contributions).<\/p>\n<table class=\"aligncenter\" border=\"0\" align=\"center\">\n<tbody>\n<tr>\n<td>\n<div id=\"attachment_8738\" style=\"width: 220px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" aria-describedby=\"caption-attachment-8738\" class=\" wp-image-8738 \"\nonclick=\"jmolApplet([210,210],'load wp-content\/uploads\/2012\/12\/R_den.cub.xyz;isosurface wp-content\/uploads\/2012\/12\/R_den.cub.jvxl translucent;zoom 100;','c1');\"  alt=\"(R)-diastereomer. NCI surfaces\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/12\/R-NCI.jpg\" width=\"210\" \/><p id=\"caption-attachment-8738\" class=\"wp-caption-text\">(R)-diastereomer. Click for NCI surfaces<\/p><\/div>\n<\/td>\n<td>\n<div id=\"attachment_8739\" style=\"width: 220px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" aria-describedby=\"caption-attachment-8739\" class=\" wp-image-8739 \" \nonclick=\"jmolApplet([210,210],'load wp-content\/uploads\/2012\/12\/S_den.cub.xyz;isosurface wp-content\/uploads\/2012\/12\/S_den.cub.jvxl translucent;zoom 100;','c2');\"  alt=\"(S)-diastereomer.  Click for  NCI surfaces.\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/12\/S-NCI.jpg\" width=\"210\" \/><p id=\"caption-attachment-8739\" class=\"wp-caption-text\">(S)-diastereomer. Click for NCI surfaces.<\/p><\/div>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>Yes, it is a very complex diagram, and you really do need to study it by obtaining the 3D model and rotating it around to explore the 3D space. I would note that it is possible to integrate the NCI function (see <span id=\"cite_ITEM-8733-1\" name=\"citation\"><a href=\"#ITEM-8733-1\">[2]<\/a><\/span> for an example and leading references) and hence try to obtain further insights. I highlight just one here; \u00a0the terminal \u00a0=CH<sub>2<\/sub> of the allyl alcohol points into empty space for \u00a0(R), but folds back to interact with the catalyst for \u00a0(S).\u00a0<\/p>\n<p>Finally, in case you are asking how do I obtain an NCI surface, I have created a little <a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/cub2nci\/\" target=\"_blank\" rel=\"noopener\">web site<\/a>\u00a0where you can submit a computed (or indeed experimental) electron density cube for processing using Jmol. Give it a go and see how it works (and thanks to \u00a0Julia \u00a0Contreras-Garcia and \u00a0Bob Hanson for putting this together).<\/p>\n<h2>References<\/h2>\n    <ol class=\"kcite-bibliography csl-bib-body\"><li id=\"ITEM-8733-0\">E.R. Johnson, S. Keinan, P. Mori-S\u00e1nchez, J. Contreras-Garc\u00eda, A.J. Cohen, and W. Yang, \"Revealing Noncovalent Interactions\", <i>Journal of the American Chemical Society<\/i>, vol. 132, pp. 6498-6506, 2010. <a href=\"https:\/\/doi.org\/10.1021\/ja100936w\">https:\/\/doi.org\/10.1021\/ja100936w<\/a>\n\n<\/li>\n<li id=\"ITEM-8733-1\">J.L. Arbour, H.S. Rzepa, J. Contreras\u2010Garc\u00eda, L.A. Adrio, E.M. Barreiro, and K.K.(. Hii, \"Silver\u2010Catalysed Enantioselective Addition of O\uf8ffH and N\uf8ffH Bonds to Allenes: A New Model for Stereoselectivity Based on Noncovalent Interactions\", <i>Chemistry \u2013 A European Journal<\/i>, vol. 18, pp. 11317-11324, 2012. <a href=\"https:\/\/doi.org\/10.1002\/chem.201200547\">https:\/\/doi.org\/10.1002\/chem.201200547<\/a>\n\n<\/li>\n<\/ol>\n\n<\/div> <!-- kcite-section 8733 -->","protected":false},"excerpt":{"rendered":"<p>The Sharpless epoxidation of an allylic alcohol had a big impact on synthetic chemistry when it was introduced in the 1980s, and led the way for the discovery (design?) of many new asymmetric catalytic systems. Each achieves its chiral magic by control of the geometry at the transition state for the reaction, and the stabilizations [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"activitypub_content_warning":"","activitypub_content_visibility":"","activitypub_max_image_attachments":5,"activitypub_interaction_policy_quote":"anyone","activitypub_status":"","footnotes":"","jetpack_publicize_message":"","jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2}},"categories":[4],"tags":[965,839,1138,249,964,958,959,843,966],"ppma_author":[2661],"class_list":["post-8733","post","type-post","status-publish","format-standard","hentry","category-interesting-chemistry","tag-asymmetric-catalytic-systems","tag-bob-hanson","tag-catalysis","tag-julia-contreras-garcia","tag-little-web-site","tag-nci","tag-non-covalent-analysis","tag-reaction-mechanism","tag-terminal-ch"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.3 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Non covalent interactions in the Sharpless transition state for asymmetric epoxidation. - Henry Rzepa&#039;s Blog<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=8733\" \/>\n<meta property=\"og:locale\" content=\"en_GB\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Non covalent interactions in the Sharpless transition state for asymmetric epoxidation. - Henry Rzepa&#039;s Blog\" \/>\n<meta property=\"og:description\" content=\"The Sharpless epoxidation of an allylic alcohol had a big impact on synthetic chemistry when it was introduced in the 1980s, and led the way for the discovery (design?) of many new asymmetric catalytic systems. Each achieves its chiral magic by control of the geometry at the transition state for the reaction, and the stabilizations [&hellip;]\" \/>\n<meta property=\"og:url\" content=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=8733\" \/>\n<meta property=\"og:site_name\" content=\"Henry Rzepa&#039;s Blog\" \/>\n<meta property=\"article:published_time\" content=\"2012-12-19T09:52:14+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2023-03-10T15:40:30+00:00\" \/>\n<meta property=\"og:image\" content=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/12\/sharpless-binuclear.svg\" \/>\n<meta name=\"author\" content=\"Henry Rzepa\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<meta name=\"twitter:label1\" content=\"Written by\" \/>\n\t<meta name=\"twitter:data1\" content=\"Henry Rzepa\" \/>\n\t<meta name=\"twitter:label2\" content=\"Estimated reading time\" \/>\n\t<meta name=\"twitter:data2\" content=\"2 minutes\" \/>\n<!-- \/ Yoast SEO plugin. -->","yoast_head_json":{"title":"Non covalent interactions in the Sharpless transition state for asymmetric epoxidation. - Henry Rzepa&#039;s Blog","robots":{"index":"index","follow":"follow","max-snippet":"max-snippet:-1","max-image-preview":"max-image-preview:large","max-video-preview":"max-video-preview:-1"},"canonical":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=8733","og_locale":"en_GB","og_type":"article","og_title":"Non covalent interactions in the Sharpless transition state for asymmetric epoxidation. - Henry Rzepa&#039;s Blog","og_description":"The Sharpless epoxidation of an allylic alcohol had a big impact on synthetic chemistry when it was introduced in the 1980s, and led the way for the discovery (design?) of many new asymmetric catalytic systems. 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