{"id":6921,"date":"2012-06-10T18:33:45","date_gmt":"2012-06-10T17:33:45","guid":{"rendered":"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=6921"},"modified":"2012-06-11T11:24:06","modified_gmt":"2012-06-11T10:24:06","slug":"transition-state-models-for-baldwin-digonal-ring-closures","status":"publish","type":"post","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=6921","title":{"rendered":"Transition state models for Baldwin dig(onal) ring closures."},"content":{"rendered":"<div class=\"kcite-section\" kcite-section-id=\"6921\">\n<p>This is a continuation of the <a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=6874\" target=\"_blank\">previous post<\/a> exploring the transition state geometries of various types of ring closure as predicted by \u00a0Baldwin&#8217;s rules. I had dealt with bond formation to a <em>trigonal<\/em> (sp<sup>2<\/sup>) carbon; now I add a <strong><em>digonal<\/em><\/strong> (sp) example (see an interesting <a title=\"10.1021\/jo2014214\" href=\"http:\/\/dx.doi.org\/10.1021\/jo2014214\" target=\"_blank\">literature <\/a>variation).\u00a0<\/p>\n<p style=\"text-align: center;\"><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/baldwin-dig.svg\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter  wp-image-6923\" title=\"baldwin-dig\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/baldwin-dig.svg\" alt=\"\" width=\"253\" height=\"190\" \/><\/a><\/p>\n<p>As before, I have added two solvent (water) molecules to the model, since the immediate product of the closure is a zwitterionic intermediate, which is likely to be stabilised by the solvent. I also used the same nucleophile as before to facilitate comparison.<\/p>\n<table style=\"margin-left: auto; margin-right: auto;\" border=\"0\">\n<tbody>\n<tr>\n<td>\n<div id=\"attachment_6925\" style=\"width: 210px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" aria-describedby=\"caption-attachment-6925\" class=\" wp-image-6925 \" title=\"5-exo-dig\" onclick=\"jmolInitialize('..\/Jmol\/');jmolSetAppletColor('white');jmolApplet([450,450],'load wp-content\/uploads\/2012\/06\/5-exo-dig.log;frame 47; zoom 100;connect (atomno=1) (atomno=9) partial;connect (atomno=11) (atomno=15) partial;connect (atomno=14) (atomno=13) partial;connect (atomno=12) (atomno=17) partial;measure 1 9;measure 11 15;measure 14 13;measure 12 17;measure 9 1 17;vectors on;vectors 4;vectors scale 5.0; color vectors yellow; vibration 20;animation mode loop;');\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig.jpg\" alt=\"\" width=\"200\" \/><p id=\"caption-attachment-6925\" class=\"wp-caption-text\">5-exo-dig transition state. Click for 4D.<\/p><\/div><\/td>\n<td>\n<div id=\"attachment_6930\" style=\"width: 210px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" aria-describedby=\"caption-attachment-6930\" class=\"size-full wp-image-6930\" title=\"6-endo-dig\" onclick=\"jmolInitialize('..\/Jmol\/');jmolSetAppletColor('white');jmolApplet([450,450],'load wp-content\/uploads\/2012\/06\/6-endo.dig-403.314624.log;frame 15; zoom 100;connect (atomno=17) (atomno=12) partial;connect (atomno=9) (atomno=13) partial;connect (atomno=12) (atomno=11) partial;connect (atomno=10) (atomno=1) partial;measure 7 15;measure 9 13;measure 12 11;measure 10 1;measure 7 15 1;vectors on;vectors 4;vectors scale 5.0; color vectors yellow; vibration 20;animation mode loop;');\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/6-endo-dig.jpg\" alt=\"\" width=\"200\" \/><p id=\"caption-attachment-6930\" class=\"wp-caption-text\">6-endo-dig transition state. Click for 4D.<\/p><\/div><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>The digonal angle of attack is 121\u00b0 for the <a href=\"http:\/\/hdl.handle.net\/10042\/20100\" target=\"_blank\"><em>\u00a0exo<\/em> form<\/a>, and 116\u00b0 for the <em><a href=\"http:\/\/hdl.handle.net\/10042\/20103\" target=\"_blank\">endo<\/a>, <\/em>both larger than was the case in the <em>trig<\/em> systems<em>.<\/em>\u00a0The relative free energies of the two transition states is 3.6 kcal\/mol in favour of the\u00a0<em>exo<\/em>\u00a0isomer.\u00a0The hydrogen bond network is somewhat strained, since two solvent molecules cannot quite reach the forming carbanion at the optimal angle to form a good hydrogen bond to it. Instead, the water has to content itself with a \u03c0-facial hydrogen bond between the alkyne and the H-O. As a result, proton transfer to the carbon requires a separate activation step (or a stronger acid than water).\u00a0<\/p>\n<table style=\"margin-left: auto; margin-right: auto;\" border=\"0\">\n<tbody>\n<tr>\n<th colspan=\"2\">5-<em>exo-dig<\/em> transition state<\/th>\n<\/tr>\n<tr>\n<td><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig.gif\"><img decoding=\"async\" class=\"aligncenter  wp-image-6933\" title=\"5-exo-dig\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig.gif\" alt=\"\" width=\"200\" \/><\/a><\/td>\n<td><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig.svg\"><img decoding=\"async\" class=\"aligncenter  wp-image-6934\" title=\"5-exo-dig\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig.svg\" alt=\"\" width=\"200\" \/><\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<table style=\"margin-left: auto; margin-right: auto;\" border=\"0\">\n<tbody>\n<tr>\n<th colspan=\"2\">6-<em>endo-dig<\/em> transition state<\/th>\n<\/tr>\n<tr>\n<td><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/6-endo-dig.gif\"><img decoding=\"async\" class=\"aligncenter  wp-image-6937\" title=\"6-endo-dig\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/6-endo-dig.gif\" alt=\"\" width=\"200\" \/><\/a><\/td>\n<td><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/6-endo-dig.svg\"><img decoding=\"async\" class=\"aligncenter  wp-image-6938\" title=\"6-endo-dig\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/6-endo-dig.svg\" alt=\"\" width=\"200\" \/><\/a><\/td>\n<\/tr>\n<tr>\n<td colspan=\"2\"><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/6-endo-digg.svg\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter  wp-image-6939\" title=\"6-endo-digg\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/6-endo-digg.svg\" alt=\"\" width=\"318\" height=\"178\" \/><\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>The IRC for the 6-endo-dig pathway has features worth commenting upon.<\/p>\n<ol>\n<li>At IRC -12, the two solvent molecules form a triangular network with the nucleophilic amine.<\/li>\n<li>By IRC -9, one of the water molecules has split itself off from this triangle, and started to move towards the triple bond, which is gradually becoming a better acceptor of a hydrogen bond.<\/li>\n<li>At IRC -3, this water molecule is now forming a\u00a0\u00a0\u03c0-facial hydrogen bond to the alkyne, which is still largely in place at the end of this step of the mechanism.<\/li>\n<\/ol>\n<p>To complete the mechanism, I have added the final step in the reaction, a proton transfer from the amine to the carbon recipient, as facilitated by the bridge of solvent molecules connecting the start and end of the process. The <a href=\"http:\/\/hdl.handle.net\/10042\/20109\" target=\"_blank\">free energy<\/a> of this transition state is 0.3 kcal\/mol higher than the N-C bond forming reaction, making it (just) the rate determining step.<\/p>\n<table style=\"margin-left: auto; margin-right: auto;\" border=\"0\">\n<tbody>\n<tr>\n<th colspan=\"2\">Proton transfer<\/th>\n<\/tr>\n<tr>\n<td>\n<div id=\"attachment_6952\" style=\"width: 188px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-6952\" class=\" wp-image-6952 \" title=\"5-exo-dig-pt\" onclick=\"jmolInitialize('..\/Jmol\/');jmolSetAppletColor('white');jmolApplet([450,450],'load wp-content\/uploads\/2012\/06\/5-exo-dig-pt-403.319864.log;frame 25; zoom 100;connect (atomno=17) (atomno=12) partial;connect (atomno=11) (atomno=15) partial;connect (atomno=14) (atomno=13) partial;connect (atomno=13) (atomno=12) partial;measure 17 12;measure 11 15;measure 14 13;measure 13 12;vectors on;vectors 4;vectors scale 5.0; color vectors yellow; vibration 20;animation mode loop;');\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig-pt.jpg\" alt=\"\" width=\"178\" height=\"186\" \/><p id=\"caption-attachment-6952\" class=\"wp-caption-text\">Transition state for proton transfer. Click for 4D<\/p><\/div><\/td>\n<td><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig-pt.gif\"><img decoding=\"async\" class=\"aligncenter  wp-image-6964\" title=\"5-exo-dig-pt\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig-pt.gif\" alt=\"\" width=\"200\" \/><\/a><\/td>\n<\/tr>\n<tr>\n<td><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig-pt.svg\"><img decoding=\"async\" class=\"aligncenter  wp-image-6965\" title=\"5-exo-dig-pt\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig-pt.svg\" alt=\"\" width=\"200\" \/><\/a><\/td>\n<td><a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig-ptg.svg\"><img decoding=\"async\" class=\"aligncenter  wp-image-6966\" title=\"5-exo-dig-ptg\" src=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2012\/06\/5-exo-dig-ptg.svg\" alt=\"\" width=\"200\" \/><\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<ol>\n<li>The feature at IRC = 0.0 (the transition state) is the first proton transfer, from \u00a0C to O.<\/li>\n<li>The second feature at \u00a0IRC -2.5\u00a0is an O to\u00a0O proton transfer<\/li>\n<li>At IRC -4, the third and final proton transfer can be seen, from\u00a0O to N.<\/li>\n<li>At\u00a0IRC -6.5,\u00a0a weak\u00a0\u03c0-OH hydrogen bond forms.<\/li>\n<\/ol>\n<p>There is one more common type of cyclisation covered by Baldwin&#8217;s rules, this time involving <em>tet<\/em>(rahedral) or sp<sup>3<\/sup>\u00a0centres. This turns out to be the most interesting of the lot; reporting on this will have to wait a little!<\/p>\n<!-- kcite active, but no citations found -->\n<\/div> <!-- kcite-section 6921 -->","protected":false},"excerpt":{"rendered":"<p>This is a continuation of the previous post exploring the transition state geometries of various types of ring closure as predicted by \u00a0Baldwin&#8217;s rules. I had dealt with bond formation to a trigonal (sp2) carbon; now I add a digonal (sp) example (see an interesting literature variation).\u00a0 As before, I have added two solvent (water) [&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":false,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2}},"categories":[],"tags":[844,40,852,851,843],"ppma_author":[2661],"class_list":["post-6921","post","type-post","status-publish","format-standard","hentry","tag-baldwins-rules","tag-free-energy","tag-hydrogen-bond-network","tag-immediate-product","tag-reaction-mechanism"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.3 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Transition state models for Baldwin dig(onal) ring closures. - 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=6921\" \/>\n<meta property=\"og:locale\" content=\"en_GB\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Transition state models for Baldwin dig(onal) ring closures. - Henry Rzepa&#039;s Blog\" \/>\n<meta property=\"og:description\" content=\"This is a continuation of the previous post exploring the transition state geometries of various types of ring closure as predicted by \u00a0Baldwin&#8217;s rules. 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