{"id":20440,"date":"2019-01-13T14:23:57","date_gmt":"2019-01-13T14:23:57","guid":{"rendered":"https:\/\/www.ch.imperial.ac.uk\/rzepa\/blog\/?p=20440"},"modified":"2019-01-13T14:23:57","modified_gmt":"2019-01-13T14:23:57","slug":"free-energy-relationships-and-their-linearity-a-test-example","status":"publish","type":"post","link":"https:\/\/rzepa.net\/blog\/2019\/01\/13\/free-energy-relationships-and-their-linearity-a-test-example\/","title":{"rendered":"Free energy relationships and their linearity: a test example."},"content":{"rendered":"<p><a href=\"https:\/\/en.wikipedia.org\/wiki\/Free-energy_relationship\">Linear free energy relationships<\/a> (LFER) are associated with the dawn of physical organic chemistry in the late 1930s and its objectives in understanding chemical reactivity as measured by reaction rates and equilibria.<\/p>\n<p>The <a href=\"https:\/\/en.wikipedia.org\/wiki\/Hammett_equation\">Hammett equation<\/a> is the best known of the LFERs, albeit derived &#8220;intuitively&#8221;. It is normally applied to the kinetics of aromatic electrophilic substitution reactions and is expressed as;<\/p>\n<p><strong>log K<sub>R<\/sub>\/K<sub>0<\/sub> = \u03c3<sub>R<\/sub>\u03c1<\/strong> (for equilibria) and extended to <strong>log k<sub>R<\/sub>\/k<sub>0<\/sub> = \u03c3<sub>R<\/sub>\u03c1<\/strong> for rates.<\/p>\n<p>The equilibrium constants are normally derived from the ionisation of substituted benzoic acids, with K<sub>0\u00a0<\/sub>being that for benzoic acid itself and\u00a0K<sub>R\u00a0<\/sub>that of a substituted benzoic acid, with\u00a0\u03c3<sub>R<\/sub> being known as the substituent constant and\u00a0\u03c1 the reaction constant. The concept involved obtaining the substituent constants by measuring the ionisation equilibria. The value of \u03c3<sub>R\u00a0<\/sub>is then assumed to be transferable to the rates of reaction,\u00a0where the values can be used to obtain reaction constants for a given reaction. The latter would then be assumed to give insight into the electronic nature of the transition state for that reaction.<\/p>\n<p>The term\u00a0log k<sub>R<\/sub>\/k<sub>0\u00a0<\/sub>(the ratio of rates of reaction) can be related to\u00a0\u0394\u0394G = -RT ln k<sub>R<\/sub>\/k<sub>0\u00a0<\/sub>and this latter quantity can be readily obtained from quantum calculations, where \u0394\u0394G is the difference in computed reaction activation free energies for two substituents (of which one might be R=H). The most interesting such Hammett plots are the ones where a discontinuity becomes apparent. The plot comprises two separate linear relationships, but with different slopes. This is normally taken to indicate a change of mechanism, on the assumption that the two mechanisms will have different responses to substituents.\u00a0<\/p>\n<p>A test of this is available via the calculated activations energies for acid catalyzed cyclocondensation to give furanochromanes[cite]10.1039\/c8sc04302g[\/cite] which is a two-step reaction involving two transition states <strong>TS1<\/strong> and <strong>TS2<\/strong>, either of which could be rate determining. A change from one to the other would constitute a change in mechanism. In this example, <strong>TS1<\/strong> involves creation of a carbocationic centre which can be stabilized by the substituent on the Ar group;\u00a0<strong>TS2<\/strong> involves the quenching of the carbocation by a nucleophilic oxygen and hence might be expected to respond differently to the substituents on Ar. As it happens, the reaction coordinate for <strong>TS2<\/strong> is not entirely trivial, since it also includes an accompanying proton transfer which might perturb the mechanism.<\/p>\n<p><a href=\"https:\/\/rzepa.net\/blog\/wp-content\/uploads\/2019\/01\/prins.svg\"><img decoding=\"async\" class=\"aligncenter size-large wp-image-20446\" src=\"https:\/\/rzepa.net\/blog\/wp-content\/uploads\/2019\/01\/prins.svg\" alt=\"\" width=\"400\" \/><\/a><\/p>\n<p>Fortunately for this reaction we have available full FAIR data (DOI: <a href=\"https:\/\/doi.org\/10.14469\/hpc\/3943\" target=\"data\" rel=\"noopener noreferrer\">10.14469\/hpc\/3943<\/a>), which includes not only the computed free energies for both sets of transition states but also the entropy-free enthalpies for comparison. This allows the table below to be generated. For each substituent, the highest energy point is in bold, indicating the rate limiting step. The span of substituents corresponds to a range of rate constants of almost 10<sup>10<\/sup>, which in fact is rarely if ever achievable experimentally.<\/p>\n<table border=\"1\">\n<tbody>\n<tr>\n<th colspan=\"6\">\n<p>Highest free energy overall route for HCl catalysed mechanism,<\/p>\n<p>trans stereochemistry<\/p>\n<\/th>\n<\/tr>\n<tr>\n<th>Sub<\/th>\n<th>\u0394H<sup>\u2021<\/sup>\/\u0394G<sup>\u2021<\/sup><\/th>\n<th>Reactant<\/th>\n<th>\u0394H<sup>\u2021<\/sup>\/\u0394G<sup>\u2021<\/sup>, TS1<\/th>\n<th>\u0394H<sup>\u2021<\/sup>\/\u0394G<sup>\u2021<\/sup>, TS2<\/th>\n<th>RDS<\/th>\n<\/tr>\n<tr>\n<td>p-NH<sub>2<\/sub><\/td>\n<td>0.2\/6.36<\/td>\n<td>0.0\/0.0<!-- -1324.156012\/-1324.254478 --><\/td>\n<td>0.15<!-- -1324.157636 -->\/4.0<!-- -1324.248061 --><\/td>\n<td><b>0.2<\/b><!-- >-1324.155779 -->\/<b>6.4<\/b><!-- -1324.244340 --><\/td>\n<td><strong>TS2\/TS2<\/strong><\/td>\n<\/tr>\n<tr>\n<td>p-OMe<\/td>\n<td>2.7\/8.48<\/td>\n<td>0.0\/0.0<!--  -1383.327024\/-1383.429500 --><\/td>\n<td><b>2.7<\/b><!-- -1383.322774 -->\/8.45<!-- -1383.416033 --><\/td>\n<td>2.1<!-- -1383.323687 -->\/<b>8.48<!-- -1383.415986 --><\/b><\/td>\n<td><strong>TS1\/TS2<\/strong><\/td>\n<\/tr>\n<tr>\n<td>p-Me<\/td>\n<td>5.5\/10.00<\/td>\n<td>0.0\/0.0<!--  -1308.091538--><!-- -1308.192300 --><\/td>\n<td><b>5.5<\/b><!-- -1308.082813 -->\/9.9<!-- -1308.176539 --><\/td>\n<td>3.9<!-- -1308.085367 -->\/<b>10.00<\/b><!-- -1308.176306 --><\/td>\n<td><strong>TS1\/TS2<\/strong><\/td>\n<\/tr>\n<tr>\n<td>p-Cl<\/td>\n<td>7.7\/12.28<\/td>\n<td>0.0\/0.0<!--  -1728.420889\/-1728.519744 --><\/td>\n<td><b>7.7<\/b><!-- -1728.408686 -->\/<b>12.28<\/b><!-- -1728.500173 --><\/td>\n<td>5.9<!-- -1728.411418 -->\/11.84<!-- -1728.500877 --><\/td>\n<td><strong>TS1\/TS1<\/strong><\/td>\n<\/tr>\n<tr>\n<td>p-H<\/td>\n<td>7.6\/13.01<\/td>\n<td>0.0\/0.0<!--  -1268.783338\/-1268.877598 --><\/td>\n<td><b>7.6<\/b><!-- -1268.771273 -->\/<b>13.01<\/b><!-- -1268.856872 --><\/td>\n<td>5.5<!-- -1268.774541 -->\/11.51<!-- -1268.859262 --><\/td>\n<td><strong>TS1\/TS1<\/strong><\/td>\n<\/tr>\n<tr>\n<td>p-CN<\/td>\n<td>10.6\/18.02<\/td>\n<td>0.0\/0.0<!--  -1361.069390\/-1361.169493 --><\/td>\n<td><b>10.6<\/b> <!---1361.052503 -->\/17.61<!-- -1361.141415 --><\/td>\n<td>10.5<!-- -1361.052559 -->\/<b>18.02<\/b><!-- -1361.140774 --><\/td>\n<td><strong>TS1\/TS2<\/strong><\/td>\n<\/tr>\n<tr>\n<td>p-NO<sub>2<\/sub><\/td>\n<td>12.4\/19.85<\/td>\n<td>0.0\/0.0<!--  -1473.378076\/-1473.481822 --><\/td>\n<td><b>12.4<\/b><!-- -1473.358279 -->\/18.24<!-- -1473.452751 --><\/td>\n<td>12.0<!-- -1473.359007 -->\/<b>19.85<\/b><!-- -1473.450183 --><\/td>\n<td><strong>TS1\/TS2<\/strong><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>For the free energies, you can see that <strong>TS2<\/strong> is the rate limiting step for the first two electron donating substituents, and the last two electron withdrawing ones, whilst <strong>TS1<\/strong> represents the rate limiting step for the middle substituents. This represents<strong> two<\/strong> changes of rate limiting step over the entire range of substituents. A different picture emerges if only the enthalpies are used. Now <strong>TS1<\/strong> is rate limiting for essentially all the substituents. The difference of course arises because of significant changes to the entropy of the transition states. The Hammett equation, and its use of\u00a0\u00a0\u03c3<sub>R\u00a0<\/sub>constants to try to infer the electronic response of a reaction mechanism, does not really factor in entropic responses. Nor is it often if at all applied using a really wide range of substituents. So any linearity or indeed non-linearity in Hammett plots may correspond only very loosely to the underlying mechanisms involved.<\/p>\n<p>Starting in the 1940s and lasting perhaps 40-50 years, thousands of different reaction mechanisms were subjected to the Hammett treatment during the golden era of physical organic chemistry, but very few have been followed up by exploring the computed free energies, as set out above. One wonders how many of the original interpretations will fully withstand such new scrutiny and in general how influential the role of entropy is.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Linear free energy relationships (LFER) are associated with the dawn of physical organic chemistry in the late 1930s and its objectives in understanding chemical reactivity as measured by reaction rates and equilibria. The Hammett equation is the best known of the LFERs, albeit derived &#8220;intuitively&#8221;. It is normally applied to the kinetics of aromatic electrophilic [&hellip;]<\/p>\n","protected":false},"author":2,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[4,11,13],"tags":[277,467,493,495,541,542,887,924,951,952,953,1047,1134,1451,1715,1826,1928,1930,2080],"class_list":["post-20440","post","type-post","status-publish","format-standard","hentry","category-chemical-it","category-interesting-chemistry","category-reaction-mechanism-2","tag-benzoic-acid","tag-chemical-kinetics","tag-chemical-reaction","tag-chemical-reactivity","tag-chemist","tag-chemistry","tag-electrophilic-aromatic-substitution","tag-energy-point","tag-equations","tag-equilibrium-chemistry","tag-equilibrium-constant","tag-free-energy-overall-route","tag-hammett-equation","tag-linear-free-energy-relationships","tag-natural-sciences","tag-organic-chemistry","tag-physical-organic-chemistry","tag-physical-sciences","tag-reactivity"],"_links":{"self":[{"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/posts\/20440","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/comments?post=20440"}],"version-history":[{"count":0,"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/posts\/20440\/revisions"}],"wp:attachment":[{"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/media?parent=20440"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/categories?post=20440"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/rzepa.net\/blog\/wp-json\/wp\/v2\/tags?post=20440"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}