{"id":1839,"date":"2012-04-24T19:13:06","date_gmt":"2012-04-24T23:13:06","guid":{"rendered":"http:\/\/blogs.vassar.edu\/magnes\/?p=1839"},"modified":"2013-07-11T10:29:36","modified_gmt":"2013-07-11T14:29:36","slug":"interpreting-a-c-13-nmr-spectrum","status":"publish","type":"post","link":"https:\/\/pages.vassar.edu\/magnes\/2012\/04\/24\/interpreting-a-c-13-nmr-spectrum\/","title":{"rendered":"Interpreting a C-13 NMR spectrum"},"content":{"rendered":"<p>In Vassar&#8217;s 300 MHz NMR, the Larmor frequency of an unaltered hydrogen nucleus with shielding factor <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-2163a0d6dbde567f46bb45cd1f7dc377_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#92;&#115;&#105;&#103;&#109;&#97;&#61;&#48;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"43\" style=\"vertical-align: 0px;\"\/> is 300 MHz. \u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nuclei are different than <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-d12612c700f99e015f6937d86076b314_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"5\" style=\"vertical-align: 5px;\"\/>H nuclei, and have a different Larmor frequency in the spectrometer&#8217;s 7.046 <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-58f18d11e5ffdd11dd9095c427922c8b_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#84;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"13\" style=\"vertical-align: 0px;\"\/>magnetic field. \u00a0According to Jacobsen in &#8220;NMR Spectroscopy Explained,&#8221; the Larmor frequency of unaltered\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nuclei with <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-2163a0d6dbde567f46bb45cd1f7dc377_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#92;&#115;&#105;&#103;&#109;&#97;&#61;&#48;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"43\" style=\"vertical-align: 0px;\"\/> is 75.43 MHz in this magnetic field. \u00a0The magnetogyric ratio <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-2afeb87159a4918337409f4bf56d689a_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#92;&#103;&#97;&#109;&#109;&#97;\" title=\"Rendered by QuickLaTeX.com\" height=\"12\" width=\"10\" style=\"vertical-align: -4px;\"\/>, is 672.650<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-3c8d41a48c014d0af3349b9b08519894_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#42;&#49;&#48;&#94;&#123;&#53;&#125;&#92;&#102;&#114;&#97;&#99;&#123;&#114;&#97;&#100;&#125;&#123;&#84;&#115;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"22\" width=\"57\" style=\"vertical-align: -6px;\"\/> \u00a0We bring back the equation for Larmor Frequency:<\/p>\n<p class=\"ql-center-displayed-equation\" style=\"line-height: 38px;\"><span class=\"ql-right-eqno\"> (1) <\/span><span class=\"ql-left-eqno\"> &nbsp; <\/span><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-e8cdafa2e06de8a0ecb1da3db9c52825_l3.png\" height=\"38\" width=\"129\" class=\"ql-img-displayed-equation \" alt=\"&#92;&#98;&#101;&#103;&#105;&#110;&#123;&#101;&#113;&#117;&#97;&#116;&#105;&#111;&#110;&#42;&#125; &#92;&#110;&#117;&#95;&#123;&#48;&#125;&#61;&#92;&#102;&#114;&#97;&#99;&#123;&#92;&#103;&#97;&#109;&#109;&#97;&#32;&#66;&#95;&#123;&#48;&#125;&#40;&#49;&#45;&#92;&#115;&#105;&#103;&#109;&#97;&#41;&#125;&#123;&#50;&#92;&#112;&#105;&#125; &#92;&#101;&#110;&#100;&#123;&#101;&#113;&#117;&#97;&#116;&#105;&#111;&#110;&#42;&#125;\" title=\"Rendered by QuickLaTeX.com\"\/><\/p>\n<p>You might ask why <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nuclei are the focus of carbon NMR instead of the much more common and ordinary <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-837dff2c80b886663fb89ea670070f65_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#50;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nuclei. \u00a0It comes down to the composition of the nucleus. \u00a0Only nuclei with nonzero spin are magnetically active. \u00a0 Spin is a type of angular momentum intrinsic to subatomic particles. \u00a0Particles with nonzero spin can have magnetic moments that can be influenced by a magnetic field. \u00a0Any nucleus with an even number of protons and an even number of neutrons will not be magnetically active because its spin is 0 and it has no magnetic moment. \u00a0Carbon-12 has 6 protons and 6 neutrons, so it can&#8217;t be studied with NMR. \u00a0Carbon-13 has 6 protons and<strong>\u00a07<\/strong>\u00a0neutrons, so we <strong>can<\/strong>\u00a0study it with NMR. \u00a0The structure and <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C-NMR spectrum of 3,3-dimethyl-2-butanol is shown below.<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide53.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-2251\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide53.png\" alt=\"\" width=\"283\" height=\"208\" \/><\/a><\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-C-13-NMR1.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-1862\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-C-13-NMR1.png\" alt=\"\" width=\"3300\" height=\"2550\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-C-13-NMR1.png 3300w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-C-13-NMR1-300x231.png 300w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-C-13-NMR1-1024x791.png 1024w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-C-13-NMR1-388x300.png 388w\" sizes=\"auto, (max-width: 3300px) 100vw, 3300px\" \/><\/a><\/p>\n<p>At first glance, the spectrum looks almost the same as the H-NMR spectrum. \u00a0However, there is little indication of how many carbons a single peak is referring to. \u00a0Each peak corresponds to a type of carbon in the molecule. \u00a0The triplet peak at 77 ppm represents the deuterated chloroform, CDCl<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-b76adf21feacb5d3425947b6c7bf2385_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#95;&#123;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"9\" width=\"7\" style=\"vertical-align: -3px;\"\/>, used to dissolve the sample. \u00a0Excluding that triplet, the molecule has four different kinds of carbon. \u00a0To help us find what carbons are represented here, we turn to the other two spectra of interest. \u00a0They are called the DEPT-90, and the DEPT 135. \u00a0DEPT stands for Distortionless Enhancement by Polarization Transfer. \u00a0The technique hits the sample with five successive radio pulses designed to excite either hydrogen or <img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nuclei. \u00a0The sequence of pulses is:<\/p>\n<ul>\n<li>A hydrogen pulse at 90\u00b0 from the x-axis<\/li>\n<li>A hydrogen pulse at 180\u00b0 from the x-axis \u00a0plus a carbon pulse at 90\u00b0 from the x-axis.<\/li>\n<li>A carbon pulse at 180\u00b0 from the y-axis plus a hydrogen pulse at either 45\u00b0, 90\u00b0, or 135\u00b0 from the y-axis.<\/li>\n<\/ul>\n<p>The angle of the last hydrogen pulse is the number in the DEPT label. \u00a0DEPT-90 ends with a hydrogen pulse at 90\u00b0 from the y-axis. \u00a0The pulse sequence is modeled below for DEPT-90 as an example. \u00a0Red waves are hydrogen pulses, green waves are carbon pulses:<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-1.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-1989\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-1.png\" alt=\"\" width=\"360\" height=\"366\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-1.png 360w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-1-295x300.png 295w\" sizes=\"auto, (max-width: 360px) 100vw, 360px\" \/><\/a><\/p>\n<p>DEPT-90 Pulse 1<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-2.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-1990\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-2.png\" alt=\"\" width=\"360\" height=\"366\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-2.png 360w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-2-295x300.png 295w\" sizes=\"auto, (max-width: 360px) 100vw, 360px\" \/><\/a><\/p>\n<p>DEPT-90 Pulse 2<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-3.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-1991\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-3.png\" alt=\"\" width=\"360\" height=\"366\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-3.png 360w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/DEPT-90-Pulse-3-295x300.png 295w\" sizes=\"auto, (max-width: 360px) 100vw, 360px\" \/><\/a><\/p>\n<p>DEPT-90 Pulse 3<\/p>\n<p>These combinations of pulses result in transfers of polarization between the hydrogen and carbon nuclei. \u00a0Different combinations pick out carbons with one, two, or three hydrogens attached to them. \u00a0The DEPT-90 and DEPT-135 spectra are shown below:<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-904.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-1883\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-904.png\" alt=\"\" width=\"3300\" height=\"2550\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-904.png 3300w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-904-300x231.png 300w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-904-1024x791.png 1024w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-904-388x300.png 388w\" sizes=\"auto, (max-width: 3300px) 100vw, 3300px\" \/><\/a>DEPT-90 spectrum<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-1354.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-1884\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-1354.png\" alt=\"\" width=\"3300\" height=\"2550\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-1354.png 3300w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-1354-300x231.png 300w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-1354-1024x791.png 1024w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/33-dimethyl-2-butanol-DEPT-1354-388x300.png 388w\" sizes=\"auto, (max-width: 3300px) 100vw, 3300px\" \/><\/a>DEPT-135 Spectrum<\/p>\n<p>The chemical shifts of the peaks on these two spectra are the same as they are on the\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C-NMR spectrum. \u00a0The sizes of the peaks on the two spectra are different, and this size difference is the key to understanding them. \u00a0You may have noticed the peak at 35 ppm on the\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C-NMR spectrum doesn&#8217;t appear on either of the DEPT spectra. \u00a0This is because DEPT spectra only show carbons with hydrogens attached to them. \u00a0Therefore the 35 ppm peak represents the carbon in 3,3-dimethyl-2-butanol with no hydrogens on it.<\/p>\n<p>The three peaks on the DEPT spectra are distinguished by their relative directions and sizes on each spectrum.<\/p>\n<ul>\n<li>Peaks that point up on the DEPT-135, point up on the DEPT-90, and<strong>\u00a0<\/strong>are <strong>larger<\/strong> on the DEPT-90, represent carbons with one hydrogen attached.<\/li>\n<li>Peaks that point down on the DEPT-135 represent carbons with two hydrogens attached.<\/li>\n<li>Peaks that point up on the DEPT-135, point up on the DEPT-90, and are <strong>smaller<\/strong> on the DEPT-90 represent carbons with three hydrogens attached.<\/li>\n<li>Carbons without hydrogens don&#8217;t appear on either the DEPT-135 or DEPT-90<\/li>\n<\/ul>\n<p>These are not the most general rules for interpreting DEPT-90 and DEPT-135 spectra. \u00a0Normally, carbons with two and three hydrogens\u00a0<strong>don&#8217;t appear<\/strong>\u00a0on the DEPT-90 spectra. \u00a0However, in this experiment the radio pulse used to collect the data was too long. \u00a0This causes the DEPT-90 spectrum to contain a small fraction of the DEPT-135 spectrum&#8217;s information.<\/p>\n<p>Armed with this new information from the DEPT spectra, we can determine which carbons are represented by which peaks on the\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C-NMR spectrum, and calculate their shielding factors. \u00a0A table of chemical shift and shielding factor values for each\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nucleus in 3,3-dimethyl-2-butanol is below.<\/p>\n<p>&nbsp;<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide22.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-1917\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide22.png\" alt=\"\" width=\"490\" height=\"157\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide22.png 490w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide22-300x96.png 300w\" sizes=\"auto, (max-width: 490px) 100vw, 490px\" \/><\/a><\/p>\n<p>The same trend that applies to hydrogen nuclei applies to\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nuclei. \u00a0The more negative the shielding constant, the lower the electron density around the nucleus, and the higher the effective magnetic field felt by the nucleus. \u00a0<img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/pages.vassar.edu\/magnes\/wp-content\/ql-cache\/quicklatex.com-da2979ed4cdf09c04247f6962db549d8_l3.png\" class=\"ql-img-inline-formula \" alt=\"&#94;&#123;&#49;&#51;&#125;\" title=\"Rendered by QuickLaTeX.com\" height=\"10\" width=\"13\" style=\"vertical-align: 5px;\"\/>C nuclei also experience higher chemical shifts compared to hydrogen nuclei because they are bonded to more atoms and have more opportunity to be deshielded when those atoms take electron density.<\/p>\n<p>The figures below shows the structure of 3,3-dimethyl-2-butanol with the carbons labeled with their corresponding chemical shifts. \u00a0This is the final step in reconstructing the molecule from the NMR data.<\/p>\n<p><a href=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide43.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-2252\" src=\"http:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide43.png\" alt=\"\" width=\"438\" height=\"410\" srcset=\"https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide43.png 438w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide43-300x280.png 300w, https:\/\/pages.vassar.edu\/magnes\/files\/2012\/04\/Slide43-320x300.png 320w\" sizes=\"auto, (max-width: 438px) 100vw, 438px\" \/><\/a><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>In Vassar&#8217;s 300 MHz NMR, the Larmor frequency of an unaltered hydrogen nucleus with shielding factor is 300 MHz. \u00a0C nuclei are different than H nuclei, and have a different Larmor frequency in the spectrometer&#8217;s 7.046 magnetic field. \u00a0According to Jacobsen in &#8220;NMR Spectroscopy Explained,&#8221; the Larmor frequency of unaltered\u00a0C nuclei with is 75.43 MHz [&hellip;]<\/p>\n","protected":false},"author":912,"featured_media":0,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[4101,64,29905],"tags":[],"class_list":["post-1839","post","type-post","status-publish","format-standard","hentry","category-advanced-em","category-michael","category-spring-2012"],"_links":{"self":[{"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/posts\/1839","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/users\/912"}],"replies":[{"embeddable":true,"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/comments?post=1839"}],"version-history":[{"count":71,"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/posts\/1839\/revisions"}],"predecessor-version":[{"id":2403,"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/posts\/1839\/revisions\/2403"}],"wp:attachment":[{"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/media?parent=1839"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/categories?post=1839"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/pages.vassar.edu\/magnes\/wp-json\/wp\/v2\/tags?post=1839"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}