{"id":21250,"date":"2019-09-27T10:58:30","date_gmt":"2019-09-27T09:58:30","guid":{"rendered":"https:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=21250"},"modified":"2019-10-05T06:54:57","modified_gmt":"2019-10-05T05:54:57","slug":"the-kekule-vibration-as-a-function-of-aromatic-ring-size-a-different-perspective-using-lemniscular-rings","status":"publish","type":"post","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=21250","title":{"rendered":"The Kekul\u00e9 vibration as a function of aromatic ring size. A different perspective using lemniscular rings."},"content":{"rendered":"<div class=\"kcite-section\" kcite-section-id=\"21250\">\n<p>In the previous posts, I tried to track down the onset of bond length alternation (<strong>BLA<\/strong>) as a function of ring size in aromatic cyclocarbons, finding the answer varied dramatically depending on the type of method used to calculate it. So here I change the system to an unusual kind of aromatic ring, the <em>leminiscular<\/em> or <em>figure-eight<\/em> annulene series.<span style=\"color: #ff0000;\"><sup>\u2665<\/sup><\/span>\u00a0I explore the Kekul\u00e9 vibration for such species for which a 4n+2 \u03c0 electron count means they are cyclically M\u00f6bius aromatic.<span id=\"cite_ITEM-21250-0\" name=\"citation\"><a href=\"#ITEM-21250-0\">[1]<\/a><\/span><\/p>\n<p>The advantage of using a lemniscular motif compared to the untwisted annulene is that perturbations due to <em>trans<\/em>-annular steric interactions between inward facing substituents are minimised. Before introducing the results for this type of molecule, I should also explain why the series\u00a0C<sub>n<\/sub>F<sub>n<\/sub> is used rather than C<sub>n<\/sub>H<sub>n<\/sub>. This is because the\u00a0C-C-H bending vibration is very similar in energy to the Kekul\u00e9 C-C stretches, causing them to mix significantly and obscure the results.\u00a0Substitution with\u00a0F produces &#8220;<a href=\"https:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=485\">clean<\/a>&#8221;\u00a0Kekul\u00e9 modes. You can see this below:<\/p>\n<p><a href=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C10F10.gif\"><img decoding=\"async\" class=\"aligncenter size-full wp-image-21270\" src=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C10F10.gif\" alt=\"\" width=\"300\" \/><\/a> <a href=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C14F14.gif\"><img decoding=\"async\" class=\"aligncenter size-full wp-image-21271\" src=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C14F14.gif\" alt=\"\" width=\"400\" \/><\/a> <a href=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C18F18.gif\"><img decoding=\"async\" class=\"aligncenter size-full wp-image-21273\" src=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C18F18.gif\" alt=\"\" width=\"500\" \/><\/a><\/p>\n<p>One consequence of introducing two half-twists into the \u03c0-system is that this topology gets partitioned into true twist (T<sub>w<\/sub>) and into a different property known as writhe (W<sub>r<\/sub>),<span id=\"cite_ITEM-21250-1\" name=\"citation\"><a href=\"#ITEM-21250-1\">[2]<\/a><\/span> the overall effect of which is to reduce the\u00a0p-\u03c0\/p-\u03c0 overlaps of adjacent carbon atoms from suffering two twists to about half this. This in turn may affect the distortive tendency of the \u03c0-electrons to induce BLA in the ring.<span id=\"cite_ITEM-21250-2\" name=\"citation\"><a href=\"#ITEM-21250-2\">[3]<\/a><\/span>\u00a0\u00a0Let us now see what this change of molecule does to the value (and sign) of the Kekul\u00e9 vibration. Included are conformations for the larger rings which vary in the total number of trans F-CC-F units in the ring. All the FAIR data for these calculations is at DOI: <a href=\"https:\/\/doi.org\/10.14469\/hpc\/6139\">10.14469\/hpc\/6139<\/a><\/p>\n<p>Two density functional methods have been used, at opposite ends of the spectrum revealed in the previous posts, together with a reasonable Def2-TZVPP basis set.<sup>\u2021<\/sup>\u00a0Each ring size can have different isomers, depending on the total number of transoid motifs present. For smaller rings (n=6, 10), the B3LYP+GD3BJ and \u03c9B97XD functionals give very similar results. By n=18 however, a clear divergence has occurred, with the\u00a0Kekul\u00e9 modes being real (+ve force constant) for the former and almost equally imaginary (-ve force constant) for the latter.\u00a0<\/p>\n<table style=\"width: 72.40336134453781%; height: 224px;\" border=\"1\">\n<tbody>\n<tr style=\"height: 27px;\">\n<th style=\"height: 27px;\" rowspan=\"2\">C<sub>n<\/sub>F<sub>n<\/sub>, n=<\/th>\n<th style=\"height: 27px;\" colspan=\"2\">Kekul\u00e9 vibration (cm<sup>-1<\/sup>)<\/th>\n<\/tr>\n<tr>\n<th style=\"height: 27px;\">B3LYP+GD3BJ<\/th>\n<th style=\"height: 27px;\">\u03c9B97XD<\/th>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">6 (0 trans)<\/td>\n<td style=\"height: 22px;\">1305<\/td>\n<td style=\"height: 22px;\">1293<\/td>\n<\/tr>\n<tr>\n<td colspan=\"3\">\n<hr \/>\n<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">10 (2 trans)<\/td>\n<td style=\"height: 22px;\">1270<\/td>\n<td style=\"height: 22px;\">1067<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">10 (4 trans)<\/td>\n<td style=\"height: 22px;\">1279<\/td>\n<td style=\"height: 22px;\">1222<\/td>\n<\/tr>\n<tr>\n<td colspan=\"3\">\n<hr \/>\n<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">14 (2 trans)<\/td>\n<td style=\"height: 22px;\">1235<\/td>\n<td style=\"height: 22px;\">1012<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">14 (4 trans)<\/td>\n<td style=\"height: 22px;\">1128<\/td>\n<td style=\"height: 22px;\">-513<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">14 (6 trans)<\/td>\n<td style=\"height: 22px;\">1197<\/td>\n<td style=\"height: 22px;\">-592<\/td>\n<\/tr>\n<tr>\n<td colspan=\"3\">\n<hr \/>\n<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">18 (2 trans)<\/td>\n<td style=\"height: 22px;\">974<\/td>\n<td style=\"height: 22px;\">-987<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">18 (4 trans)<\/td>\n<td style=\"height: 22px;\">914<\/td>\n<td style=\"height: 22px;\">-1091<\/td>\n<\/tr>\n<tr style=\"height: 21px;\">\n<td style=\"height: 21px;\">18 (6 trans)<\/td>\n<td style=\"height: 21px;\">933<\/td>\n<td style=\"height: 21px;\">-1232<\/td>\n<\/tr>\n<tr>\n<td colspan=\"3\">\n<hr \/>\n<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"height: 22px;\">22 (4 trans)<\/td>\n<td style=\"height: 22px;\">888<\/td>\n<td style=\"height: 22px;\">-1309<\/td>\n<\/tr>\n<tr style=\"height: 21px;\">\n<td style=\"height: 21px;\">22 (6 trans)<\/td>\n<td style=\"height: 21px;\">757<\/td>\n<td style=\"height: 21px;\">-1811<\/td>\n<\/tr>\n<tr>\n<td colspan=\"3\">\n<hr \/>\n<\/td>\n<\/tr>\n<tr style=\"height: 21px;\">\n<td style=\"height: 21px;\">26 (6 trans)<\/td>\n<td style=\"height: 21px;\">\u2020<\/td>\n<td style=\"height: 21px;\">-2140<\/td>\n<\/tr>\n<tr style=\"height: 21px;\">\n<td style=\"height: 21px;\">26 (8 trans)<\/td>\n<td style=\"height: 21px;\">756<\/td>\n<td style=\"height: 21px;\">-2229<\/td>\n<\/tr>\n<tr style=\"height: 21px;\">\n<td style=\"height: 21px;\">26 (10 trans)<\/td>\n<td style=\"height: 21px;\">-437<\/td>\n<td style=\"height: 21px;\">-3296<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>Overall, the B3LYP+GD3BJ series shows a slow and reasonably regular decline in the\u00a0value of the Kekul\u00e9 modes. As the ring sizes gets larger, the double bond configurations of the rings start to become unstable, with C=C bond rotations occuring during geometry optimisations. At n=26 using B3LYP, we seen a sudden change from a real Kekul\u00e9 mode mode for the 8-trans isomer to an imaginary one for the 10-trans isomer. As noted above, this abrupt change occurs much earlier with the \u03c9B97XD functional at n=14, with\u00a0a discontinuity between a conformation with two transoid motifs and the ones with four and six.\u00a0I can offer no explanation (yet) for this strange abrupt onset of an imaginary Kekul\u00e9 mode, except perhaps to speculate that it might be related to the T<sub>w<\/sub>\u00a0and W<sub>r <\/sub>partitioning noted above, given that T<sub>w\u00a0<\/sub>and BLA might themselves be related. As with the <a href=\"https:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=21225\">cyclocarbons<\/a>, the BLA phenomenon seems to be peculiarly sensitive to the method used to compute it, more so than most other molecular properties.<\/p>\n<p>Something deep and important is clearly happening and the underlying cause does need to be identified. It reminds in one sense also of the discontinuous transition between planar aromatic (bond equal) and \u00a0non-planar non-aromatic (BLA) \u00a0isomers of 10-\u03c0-Dihetero[8]annulenes<span id=\"cite_ITEM-21250-3\" name=\"citation\"><a href=\"#ITEM-21250-3\">[4]<\/a><\/span> \u00a0Who might have imagined that simple aromatic rings could be so tantalisingly complex!<\/p>\n<hr \/>\n<p><span style=\"color: #ff0000;\"><sup>\u2665<\/sup><\/span> The first example of this was identified in 2005<span id=\"cite_ITEM-21250-4\" name=\"citation\"><a href=\"#ITEM-21250-4\">[5]<\/a><\/span> and is characterised by a topological chiral property known as a linking number or Lk. For lemniscular molecules, Lk = 2\u03c0, or in plainer english it contains a double half twist in the \u03c0 system around the ring. <sup>\u2021<\/sup>This investigation is a perfect example of the benefits of using a data repository. Many of these species were originally included in an article published in 2009<span id=\"cite_ITEM-21250-5\" name=\"citation\"><a href=\"#ITEM-21250-5\">[6]<\/a><\/span> with the calculations being deposited in 2007. So all the starting geometries for the present investigation were quickly obtained from that source. \u2020Bonds rotate to 10-trans isomer.<\/p>\n<h2>References<\/h2>\n    <ol class=\"kcite-bibliography csl-bib-body\"><li id=\"ITEM-21250-0\">P.L. Ayers, R.J. Boyd, P. Bultinck, M. Caffarel, R. Carb\u00f3-Dorca, M. Caus\u00e1, J. Cioslowski, J. Contreras-Garcia, D.L. Cooper, P. Coppens, C. Gatti, S. Grabowsky, P. Lazzeretti, P. Macchi, ?. Mart\u00edn Pend\u00e1s, P.L. Popelier, K. Ruedenberg, H. Rzepa, A. Savin, A. Sax, W.E. Schwarz, S. Shahbazian, B. Silvi, M. Sol\u00e0, and V. Tsirelson, \"Six questions on topology in theoretical chemistry\", <i>Computational and Theoretical Chemistry<\/i>, vol. 1053, pp. 2-16, 2015. <a href=\"https:\/\/doi.org\/10.1016\/j.comptc.2014.09.028\">https:\/\/doi.org\/10.1016\/j.comptc.2014.09.028<\/a>\n\n<\/li>\n<li id=\"ITEM-21250-1\">S.M. Rappaport, and H.S. Rzepa, \"Intrinsically Chiral Aromaticity. Rules Incorporating Linking Number, Twist, and Writhe for Higher-Twist M\u00f6bius Annulenes\", <i>Journal of the American Chemical Society<\/i>, vol. 130, pp. 7613-7619, 2008. <a href=\"https:\/\/doi.org\/10.1021\/ja710438j\">https:\/\/doi.org\/10.1021\/ja710438j<\/a>\n\n<\/li>\n<li id=\"ITEM-21250-2\">S. Shaik, A. Shurki, D. Danovich, and P.C. Hiberty, \"A Different Story of \u03c0-DelocalizationThe Distortivity of \u03c0-Electrons and Its Chemical Manifestations\", <i>Chemical Reviews<\/i>, vol. 101, pp. 1501-1540, 2001. <a href=\"https:\/\/doi.org\/10.1021\/cr990363l\">https:\/\/doi.org\/10.1021\/cr990363l<\/a>\n\n<\/li>\n<li id=\"ITEM-21250-3\">H.S. Rzepa, and N. Sanderson, \"Aromaticity on the edge of chaos: An ab initio study of the bimodal balance between aromatic and non-aromatic structures for 10\u03c0-dihetero[8]annulenes\", <i>Phys. Chem. Chem. Phys.<\/i>, vol. 6, pp. 310-313, 2004. <a href=\"https:\/\/doi.org\/10.1039\/b312724a\">https:\/\/doi.org\/10.1039\/b312724a<\/a>\n\n<\/li>\n<li id=\"ITEM-21250-4\">H.S. Rzepa, \"A Double-Twist M\u00f6bius-Aromatic Conformation of [14]Annulene\", <i>Organic Letters<\/i>, vol. 7, pp. 4637-4639, 2005. <a href=\"https:\/\/doi.org\/10.1021\/ol0518333\">https:\/\/doi.org\/10.1021\/ol0518333<\/a>\n\n<\/li>\n<li id=\"ITEM-21250-5\">C.S. Wannere, H.S. Rzepa, B.C. Rinderspacher, A. Paul, C.S.M. Allan, H.F. Schaefer, and P.V.R. Schleyer, \"The Geometry and Electronic Topology of Higher-Order Charged M\u00f6bius Annulenes\", <i>The Journal of Physical Chemistry A<\/i>, vol. 113, pp. 11619-11629, 2009. <a href=\"https:\/\/doi.org\/10.1021\/jp902176a\">https:\/\/doi.org\/10.1021\/jp902176a<\/a>\n\n<\/li>\n<\/ol>\n\n<\/div> <!-- kcite-section 21250 -->","protected":false},"excerpt":{"rendered":"<p>In the previous posts, I tried to track down the onset of bond length alternation (BLA) as a function of ring size in aromatic cyclocarbons, finding the answer varied dramatically depending on the type of method used to calculate it. So here I change the system to an unusual kind of aromatic ring, the leminiscular [&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":[],"ppma_author":[2661],"class_list":["post-21250","post","type-post","status-publish","format-standard","hentry","category-interesting-chemistry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.5 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>The Kekul\u00e9 vibration as a function of aromatic ring size. A different perspective using lemniscular rings. - 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=21250\" \/>\n<meta property=\"og:locale\" content=\"en_GB\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"The Kekul\u00e9 vibration as a function of aromatic ring size. A different perspective using lemniscular rings. - Henry Rzepa&#039;s Blog\" \/>\n<meta property=\"og:description\" content=\"In the previous posts, I tried to track down the onset of bond length alternation (BLA) as a function of ring size in aromatic cyclocarbons, finding the answer varied dramatically depending on the type of method used to calculate it. So here I change the system to an unusual kind of aromatic ring, the leminiscular [&hellip;]\" \/>\n<meta property=\"og:url\" content=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=21250\" \/>\n<meta property=\"og:site_name\" content=\"Henry Rzepa&#039;s Blog\" \/>\n<meta property=\"article:published_time\" content=\"2019-09-27T09:58:30+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2019-10-05T05:54:57+00:00\" \/>\n<meta property=\"og:image\" content=\"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C10F10.gif\" \/>\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=\"4 minutes\" \/>\n<!-- \/ Yoast SEO plugin. -->","yoast_head_json":{"title":"The Kekul\u00e9 vibration as a function of aromatic ring size. A different perspective using lemniscular rings. - 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=21250","og_locale":"en_GB","og_type":"article","og_title":"The Kekul\u00e9 vibration as a function of aromatic ring size. A different perspective using lemniscular rings. - Henry Rzepa&#039;s Blog","og_description":"In the previous posts, I tried to track down the onset of bond length alternation (BLA) as a function of ring size in aromatic cyclocarbons, finding the answer varied dramatically depending on the type of method used to calculate it. So here I change the system to an unusual kind of aromatic ring, the leminiscular [&hellip;]","og_url":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=21250","og_site_name":"Henry Rzepa&#039;s Blog","article_published_time":"2019-09-27T09:58:30+00:00","article_modified_time":"2019-10-05T05:54:57+00:00","og_image":[{"url":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/09\/C10F10.gif","type":"","width":"","height":""}],"author":"Henry Rzepa","twitter_card":"summary_large_image","twitter_misc":{"Written by":"Henry Rzepa","Estimated reading time":"4 minutes"},"schema":{"@context":"https:\/\/schema.org","@graph":[{"@type":"Article","@id":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=21250#article","isPartOf":{"@id":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=21250"},"author":{"name":"Henry Rzepa","@id":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/#\/schema\/person\/2b40f7b9c872a4dc1547e040a11b6281"},"headline":"The Kekul\u00e9 vibration as a function of aromatic ring size. 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The discussion about the norbornyl cation concentrated on whether this species existed in a single minimum symmetric energy well (the non-classical Winstein\/Olah proposal) or a double minimum well connected\u2026","rel":"","context":"In &quot;Interesting chemistry&quot;","block_context":{"text":"Interesting chemistry","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?cat=4"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":21176,"url":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=21176","url_meta":{"origin":21250,"position":1},"title":"Cyclo[18]carbon: The Kekul\u00e9 vibration calculated and hence a mystery!","author":"Henry Rzepa","date":"August 30, 2019","format":false,"excerpt":"I have discussed the vibration in benzene known as the Kekul\u00e9 mode in other posts, the first of which was all of ten years ago. It is a stretching mode that lengthens three of the bonds in benzene (a [6]-annulene) and shortens the other three, thus leading to a cyclohexatriene\u2026","rel":"","context":"In &quot;Interesting chemistry&quot;","block_context":{"text":"Interesting chemistry","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?cat=4"},"img":{"alt_text":"","src":"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2019\/08\/C18.gif?resize=350%2C200&ssl=1","width":350,"height":200},"classes":[]},{"id":8426,"url":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=8426","url_meta":{"origin":21250,"position":2},"title":"A pericyclic dichotomy.","author":"Henry Rzepa","date":"November 30, 2012","format":false,"excerpt":"A dichotomy is a division into two mutually exclusive, opposed, or contradictory groups. Consider the reaction below. The bicyclic pentadiene on the left could in principle open on heating to give the monocyclic [12]-annulene (blue or red)\u00a0via what is called an electrocyclic reaction as either a six (red) or eight\u2026","rel":"","context":"In \"M\u00f6bius\"","block_context":{"text":"M\u00f6bius","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?tag=mobius"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":399,"url":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=399","url_meta":{"origin":21250,"position":3},"title":"The Chirality of Lemniscular Octaphyrins","author":"Henry Rzepa","date":"April 28, 2009","format":false,"excerpt":"In the previous post, \u00a0it was noted that \u00a0M\u00f6bius annulenes are intrinsically chiral, and should therefore in principle be capable of resolution into enantiomers. The synthesis of such an annulene by Herges and co-workers was a racemic one; no attempt was reported at any resolution into such enantiomers. Here theory\u2026","rel":"","context":"In &quot;Interesting chemistry&quot;","block_context":{"text":"Interesting chemistry","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?cat=4"},"img":{"alt_text":"A 34-Octaphyrin. Click to see molecule","src":"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2009\/04\/qarfar.jpg?resize=350%2C200","width":350,"height":200},"classes":[]},{"id":275,"url":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=275","url_meta":{"origin":21250,"position":4},"title":"A molecule with an identity crisis: Aromatic or anti-aromatic?","author":"Henry Rzepa","date":"April 13, 2009","format":false,"excerpt":"In 1988, Wilke reported molecule 1 It was a highly unexpected outcome of a nickel-catalyzed reaction and was described as a 24-annulene with an unusual 3D shape. Little attention has been paid to this molecule since its original report, but the focus has now returned! The reason is that a\u2026","rel":"","context":"In &quot;Interesting chemistry&quot;","block_context":{"text":"Interesting chemistry","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?cat=4"},"img":{"alt_text":"A [24] annulene. Click on image for model.","src":"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2009\/04\/gaytab.jpg?resize=350%2C200","width":350,"height":200},"classes":[]},{"id":9,"url":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?p=9","url_meta":{"origin":21250,"position":5},"title":"A  Disrotatory 4n+2 electron anti-aromatic M\u00f6bius transition state for a thermal electrocyclic reaction.","author":"Henry Rzepa","date":"April 2, 2009","format":false,"excerpt":"Mauksch and Tsogoeva have recently published an article illustrating how a thermal electrocyclic reaction can proceed with distoratory ring closure, whilst simultaneously also exhibiting 4n electron M\u00f6bius-aromatic character. Why is this remarkable? Because the simple Woodward-Hoffmann rules state that a disrotatory thermal electrocyclic reaction should proceed via a H\u00fcckel-aromatic 4n+2\u2026","rel":"","context":"In &quot;pericyclic&quot;","block_context":{"text":"pericyclic","link":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/?cat=559"},"img":{"alt_text":"Electrocylization of [14] annulene","src":"https:\/\/i0.wp.com\/www.ch.ic.ac.uk\/rzepa\/blog\/wp-content\/uploads\/2009\/04\/p322.jpg?resize=350%2C200","width":350,"height":200},"classes":[]}],"jetpack_likes_enabled":false,"authors":[{"term_id":2661,"user_id":1,"is_guest":0,"slug":"admin","display_name":"Henry Rzepa","avatar_url":"https:\/\/secure.gravatar.com\/avatar\/897b6740f7f599bca7942cdf7d7914af5988937ae0e3869ab09aebb87f26a731?s=96&d=blank&r=g","0":null,"1":"","2":"","3":"","4":"","5":"","6":"","7":"","8":""}],"_links":{"self":[{"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=\/wp\/v2\/posts\/21250","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=21250"}],"version-history":[{"count":52,"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=\/wp\/v2\/posts\/21250\/revisions"}],"predecessor-version":[{"id":21373,"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=\/wp\/v2\/posts\/21250\/revisions\/21373"}],"wp:attachment":[{"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=21250"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=21250"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=21250"},{"taxonomy":"author","embeddable":true,"href":"https:\/\/www.ch.ic.ac.uk\/rzepa\/blog\/index.php?rest_route=%2Fwp%2Fv2%2Fppma_author&post=21250"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}