{"id":16402,"date":"2016-05-25T10:44:00","date_gmt":"2016-05-25T09:44:00","guid":{"rendered":"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=16402"},"modified":"2016-05-25T10:44:00","modified_gmt":"2016-05-25T09:44:00","slug":"the-mechanism-of-silylether-deprotection-using-a-tetra-alkyl-ammonium-fluoride","status":"publish","type":"post","link":"https:\/\/www.rzepa.net\/blog\/?p=16402","title":{"rendered":"The mechanism of silylether deprotection using a tetra-alkyl ammonium fluoride."},"content":{"rendered":"<div class=\"kcite-section\" kcite-section-id=\"16402\">\n<p>\n\tThe substitution of a <a href=\"https:\/\/en.wikipedia.org\/wiki\/Nucleofuge\" target=\"_blank\">nucleofuge<\/a> (a good leaving group) by a nucleophile at a carbon centre&nbsp;occurs with inversion&nbsp;of configuration at the carbon, the mechanism being known by&nbsp;the term&nbsp;S<sub>N<\/sub>2&nbsp;(a story I have also told&nbsp;in this <a href=\"http:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=4002\" target=\"_blank\">post<\/a>). Such displacement at silicon famously proceeds by a quite different mechanism, which&nbsp;I here quantify with some calculations.\n<\/p>\n<p>\n\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/Si.svg\" width=\"400\" \/>\n<\/p>\n<p>\n\tTrialkylsilyl is often used to protect OH groups, and as shown in the diagram above is specifically used to enforce the enol form of a ketone by replacing the OH with OTMS. The TMS can then be removed when required&nbsp;by utilising nucleophilic&nbsp;addition of <em>e.g.<\/em> fluoride anion from&nbsp;tetra-alkyl ammonium fluoride to form a 5-coordinate silicon intermediate, followed by collapse of this intermediate with&nbsp;expulsion of the oxygen to form an enolate anion. Before starting the calculations,&nbsp;I searched the crystal structure database for examples of R<sub>3<\/sub>SIF(OR), as in the search query below.\n<\/p>\n<p>\n\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/Si-SQ.jpg?w=400\"  \/>\n<\/p>\n<p>\n\tThere were 55 instances of such species, and show below are their geometric characteristics. In all cases, the two electronegative substituents occupy the axial positions of a&nbsp;<strong>trigonal bipyramidal<\/strong> geometry. This of course is the orientation adopted by the two electronegative substituents in the&nbsp;S<sub>N<\/sub>2 mechanism for carbon, but with silicon this carbon &quot;transition state&quot; can be replaced by a stable (and as we see often crystalline) intermediate!\n<\/p>\n<p>\n\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/SiOF.jpg?w=400\"  \/>\n<\/p>\n<p>\n\tTurning to calculations (&omega;B97XD\/6-31+G(d)\/SCRF=thf), one can locate <strong>three<\/strong> transition states for the silicon process (there is only one for the&nbsp;S<sub>N<\/sub>2 reaction with carbon).\n<\/p>\n<ol>\n<li>\n\t\tTS1 represents attack of fluoride anion along the axial position of the forming 5-coordinate silicon.<span id=\"cite_ITEM-16402-0\" name=\"citation\"><a href=\"#ITEM-16402-0\">[1]<\/a><\/span>,<span id=\"cite_ITEM-16402-1\" name=\"citation\"><a href=\"#ITEM-16402-1\">[2]<\/a><\/span> The oxygen in this instance occupies an equatorial position, and this close proximity between the incoming F(-) and the about to depart OR groups represents a <span style=\"color:#FF0000;\"><em>retention of configuration <\/em><\/span>at the Si. Note that the reaction is endo-energic. (<em>c.f.<\/em>&nbsp;<span id=\"cite_ITEM-16402-2\" name=\"citation\"><a href=\"#ITEM-16402-2\">[3]<\/a><\/span>).<br \/>\n\t\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" onclick=\"jmolInitialize('..\/Jmol\/','JmolAppletSigned.jar');jmolSetAppletColor('white');jmolApplet([500,500],'load wp-content\/uploads\/2016\/05\/TS1-876.301414.log;frame 45;vectors on;vectors 4;vectors scale 8.0;color vectors green;vibration 6;spin 3;');\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/ts1.jpg?w=400\"  \/><br \/>\n\t\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/ts1a.gif?w=400\"  \/><br \/>\n\t\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/TS1.svg\" width=\"400\" \/>\n\t<\/li>\n<li>\n\t\tThe next step, TS2<span id=\"cite_ITEM-16402-3\" name=\"citation\"><a href=\"#ITEM-16402-3\">[4]<\/a><\/span>,<span id=\"cite_ITEM-16402-4\" name=\"citation\"><a href=\"#ITEM-16402-4\">[5]<\/a><\/span>&nbsp; is to move the F ligand to an equatorial position and the OR group from equatorial&nbsp;to its own axial position so that it can depart in the manner the F adopted to arrive. This requires what is called a <span style=\"color:#FF0000;\">Berry pseudorotation<\/span>, an essentially isoenergic process.<br \/>\n\t\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" onclick=\"jmolInitialize('..\/Jmol\/','JmolAppletSigned.jar');jmolSetAppletColor('white');jmolApplet([500,500],'load wp-content\/uploads\/2016\/05\/TS2-876.297846.log;frame 129;vectors on;vectors 4;vectors scale 8.0;color vectors green;vibration 6;spin 3;');\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/ts2.jpg?w=400\"  \/><br \/>\n\t\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/ts2.gif?w=400\"  \/><br \/>\n\t\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/TS2.svg\" width=\"400\" \/><br \/>\n\t\tYou might note a &quot;hidden intermediate&quot; at IRC ~-7 (the &quot;bump&quot; in the energy profile).&nbsp;This is caused by re-organisation of the ion-pair geometry, with the tetra-alkyl ammonium cation moving its orientation.<br \/>\n\t\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/TS2G.svg\" width=\"400\" \/>\n\t<\/li>\n<li>\n\t\tTS3<span id=\"cite_ITEM-16402-5\" name=\"citation\"><a href=\"#ITEM-16402-5\">[6]<\/a><\/span>,<span id=\"cite_ITEM-16402-6\" name=\"citation\"><a href=\"#ITEM-16402-6\">[7]<\/a><\/span> now eliminates the <sup>&#8211;<\/sup>OR&nbsp;group to complete the deprotection.<br \/>\n\t\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" onclick=\"jmolInitialize('..\/Jmol\/','JmolAppletSigned.jar');jmolSetAppletColor('white');jmolApplet([500,500],'load wp-content\/uploads\/2016\/05\/TS3-876.305730.log;frame 63;vectors on;vectors 4;vectors scale 8.0;color vectors green;vibration 6;spin 3;');\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/ts3.jpg?w=400\"  \/><br \/>\n\t\t<img data-recalc-dims=\"1\" decoding=\"async\" alt=\"\" src=\"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/ts3.gif?w=400\"  \/><br \/>\n\t\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/TS3.svg\" width=\"400\" \/>\n\t<\/li>\n<\/ol>\n<p>\n\tThe free energies are summarised below. Key points include:\n<\/p>\n<ol>\n<li>\n\t\tThe overall free energy of deprotection is appropriately exo-energic.\n\t<\/li>\n<li>\n\t\tThe highest energy barrier is actually for pseudo-rotation! This suggests that tuning the deprotection with alternative alkyl or aryl groups on the silicon may be a matter of controlling the Berry pseudorotation process.\n\t<\/li>\n<li>\n\t\tTS1-3 proceed with the attacking and leaving groups in close proximity (the angle between an axial and an equatorial group is ~90&deg; of course, whereas for a di-axial relationship (the inversion of the&nbsp;S<sub>N<\/sub>2 mechanism) it is instead 180&deg;. This close proximity of nucleophile and nucleofuge minimises the required reorganisation of the ammonium counter-ion in the ion-pairs, and possibly also the dipole moments induced by the reactions, the changes of which for the three reactions are shown below:<br \/>\n\t\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/TS1DM.svg\" width=\"400\" \/><br \/>\n\t\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/TS2DM.svg\" width=\"400\" \/><br \/>\n\t\t<img decoding=\"async\" alt=\"\" src=\"http:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2016\/05\/TS3DM.svg\" width=\"400\" \/>\n\t<\/li>\n<li>\n\t\tThe 5-coordinate intermediate where both F and O are axial is in fact significantly lower in energy (a cooperative effect)&nbsp;than when only one of them is axial,&nbsp;which matches the orientations&nbsp;identified above in the 55 crystal structures. For a substitution to occur, the cooperative strengthening of the Si-O and Si-F bonds must be removed; hence the <span style=\"color:#FF0000;\"><em>retention of configuration<\/em><\/span>.\n\t<\/li>\n<\/ol>\n<table border=\"1\">\n<tbody>\n<tr>\n<th>\n\t\t\t\tSystem\n\t\t\t<\/th>\n<th>\n\t\t\t\tRelative free energy\n\t\t\t<\/th>\n<th>\n\t\t\t\tDataDOI\n\t\t\t<\/th>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tReactants\n\t\t\t<\/td>\n<td>\n\t\t\t\t0.0\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-7\" name=\"citation\"><a href=\"#ITEM-16402-7\">[8]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tTS1\n\t\t\t<\/td>\n<td>\n\t\t\t\t7.9\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-0\" name=\"citation\"><a href=\"#ITEM-16402-0\">[1]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tInt F(ax), O(eq)\n\t\t\t<\/td>\n<td>\n\t\t\t\t5.1\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-8\" name=\"citation\"><a href=\"#ITEM-16402-8\">[9]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tTS2\n\t\t\t<\/td>\n<td>\n\t\t\t\t10.2 (9.2)*\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-3\" name=\"citation\"><a href=\"#ITEM-16402-3\">[4]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tInt F(eq), O(ax)\n\t\t\t<\/td>\n<td>\n\t\t\t\t5.1\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-9\" name=\"citation\"><a href=\"#ITEM-16402-9\">[10]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tTS3\n\t\t\t<\/td>\n<td>\n\t\t\t\t5.2\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-5\" name=\"citation\"><a href=\"#ITEM-16402-5\">[6]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tProducts\n\t\t\t<\/td>\n<td>\n\t\t\t\t-4.0\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-10\" name=\"citation\"><a href=\"#ITEM-16402-10\">[11]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<tr>\n<td>\n\t\t\t\tInt F,O(ax)\n\t\t\t<\/td>\n<td>\n\t\t\t\t-2.5\n\t\t\t<\/td>\n<td>\n\t\t\t\t<span id=\"cite_ITEM-16402-11\" name=\"citation\"><a href=\"#ITEM-16402-11\">[12]<\/a><\/span>\n\t\t\t<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>\n\t*A lower energy orientation of the ion-pair has subsequently been found.<span id=\"cite_ITEM-16402-12\" name=\"citation\"><a href=\"#ITEM-16402-12\">[13]<\/a><\/span>\n<\/p>\n<p>\n\tThis analysis shows just how different the carbon and the silicon substitution reactions are&nbsp;and how it is the pseudorotation interconverting two 5-coordinate intermediates that appears to be a key step. But questions remain unanswered. What is the energy of the&nbsp;pseudorotation interconverting an intermediate with <strong>ax\/eq<\/strong> electronegative groups to one with <strong>di-axial<\/strong> electronegative groups? Are there&nbsp;transition states starting from the diaxial intermediate and resulting in elimination, and if so what are their relative energies? I leave answers to a follow up post.&nbsp;<\/p>\n<h2>References<\/h2>\n    <ol class=\"kcite-bibliography csl-bib-body\"><li id=\"ITEM-16402-0\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) 5-coordinate intermediate F axial TS\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/554\">https:\/\/doi.org\/10.14469\/hpc\/554<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-1\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) 5-coordinate intermediate F axial TS IRC\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/564\">https:\/\/doi.org\/10.14469\/hpc\/564<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-2\">L. Wozniak, M. Cypryk, J. Chojnowski, and G. Lanneau, \"Optically active silyl esters of phosphorus. II. Stereochemistry of reactions with nucleophiles\", <i>Tetrahedron<\/i>, vol. 45, pp. 4403-4414, 1989. <a href=\"https:\/\/doi.org\/10.1016\/s0040-4020(01)89077-3\">https:\/\/doi.org\/10.1016\/s0040-4020(01)89077-3<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-3\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) 5-coordinate intermediate Berry pseudorotation TS\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/551\">https:\/\/doi.org\/10.14469\/hpc\/551<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-4\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) 5-coordinate intermediate Berry pseudorotation TS IRC\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/553\">https:\/\/doi.org\/10.14469\/hpc\/553<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-5\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) TS\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/539\">https:\/\/doi.org\/10.14469\/hpc\/539<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-6\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) TS IRC\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/552\">https:\/\/doi.org\/10.14469\/hpc\/552<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-7\">H. Rzepa, \"enol + Me4N(+).F(-) Reactant\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/565\">https:\/\/doi.org\/10.14469\/hpc\/565<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-8\">H. Rzepa, \"enol + Me4N(+).F(-) 5-coordinate intermediate F axial\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/555\">https:\/\/doi.org\/10.14469\/hpc\/555<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-9\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) 5-coordinate intermediate\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/540\">https:\/\/doi.org\/10.14469\/hpc\/540<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-10\">H. Rzepa, \"enol + Me4N(+).F(-) Product\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/563\">https:\/\/doi.org\/10.14469\/hpc\/563<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-11\">H. Rzepa, \"trimethyl silyl enol + Me4N(+).F(-) 5-coordinate intermediate F\/O axial\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/550\">https:\/\/doi.org\/10.14469\/hpc\/550<\/a>\n\n<\/li>\n<li id=\"ITEM-16402-12\">H. Rzepa, \"5-coordinate intermediate Berry pseudorotation TS2 New conf?\", 2016. <a href=\"https:\/\/doi.org\/10.14469\/hpc\/577\">https:\/\/doi.org\/10.14469\/hpc\/577<\/a>\n\n<\/li>\n<\/ol>\n\n<\/div> <!-- kcite-section 16402 -->","protected":false},"excerpt":{"rendered":"<p>The substitution of a nucleofuge (a good leaving group) by a nucleophile at a carbon centre&nbsp;occurs with inversion&nbsp;of configuration at the carbon, the mechanism being known by&nbsp;the term&nbsp;SN2&nbsp;(a story I have also told&nbsp;in this post). Such displacement at silicon famously proceeds by a quite different mechanism, which&nbsp;I here quantify with some calculations. Trialkylsilyl is often [&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,"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":[1085],"tags":[1764,1784,147,938,931,164,1803,1807,1640,1817,283,1824,733,1835,1610,1846],"class_list":["post-16402","post","type-post","status-publish","format-standard","hentry","category-reaction-mechanism-2","tag-berry-mechanism","tag-elimination-reaction","tag-energy","tag-energy-barrier","tag-energy-profile","tag-free-energy","tag-leaving-group","tag-lower-energy-orientation","tag-molecular-geometry","tag-organic-reactions","tag-overall-free-energy","tag-pseudorotation","tag-search-query","tag-sn2-reaction","tag-stereochemistry","tag-trigonal-bipyramidal-molecular-geometry"],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p1gPyz-4gy","jetpack_likes_enabled":true,"_links":{"self":[{"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=\/wp\/v2\/posts\/16402","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=16402"}],"version-history":[{"count":0,"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=\/wp\/v2\/posts\/16402\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=16402"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=16402"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.rzepa.net\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=16402"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}