
Showing posts with label 13C-14N coupling. Show all posts
Showing posts with label 13C-14N coupling. Show all posts
Friday, January 11, 2008
13C Showing J Coupling to Both 31P and 14N
Despite my efforts, some novice users still believe that all 13C resonances are sharp singlets. This is indeed the case in proton decoupled 13C spectra where there is no additional heteronuclear coupling, exchange or fast relaxation. In the BLOG entries for December 11, 2007 and October 9, 2007 , I showed 13C NMR spectra where the carbon was coupled to 14N and 19F, respectively. The spectrum below is a 13C spectrum where 13C couples with 31P and 14N. The yellow region of the full spectrum is expanded in the inset. Carbon 2 is particularly interesting as it shows coupling to both 31P and 14 N.

Tuesday, December 11, 2007
13C - 14N J coupling
It has always puzzled me how students so willingly accept the fact that 13C is J coupled to a spin I = 1 nucleus like 2H (eg. the multiplets for the 13C spectra of deuterated solvents) however they do not question the fact that 13C almost never shows a J coupling to 14N (another spin I = 1 nucleus). The reason that 13C exhibits J coupling to 2H is that the relaxation among the three energy levels of 2H is rather slow and each 13C "sees" the 2H in each of its three Zeeman states, splitting the 13C resonance into 3 lines of equal intensity. The efficiency of the relaxation among the energy levels of quadrupolar nuclei (among other things) depends on the magnitude of the quadrupolar coupling constant - the larger the quadrupolar coupling constant, the faster the relaxation. Unlike 2H, which has a very small quadrupolar coupling constant, 14N (and most other quadrupolar nuclei) has a substantial quadrupolar coupling constant and therefore the relaxation among its energy levels is very fast. The 13C therefore "sees" the 14N in a single "average" state and as a result is a singlet. There are however compounds where the 14N is in a very symmetric environment. The high symmetry make the quadrupolar coupling constant much smaller and the relaxation therefore much slower. In these cases one can observe the 13C - 14N J coupling. Depending on the relaxation of the 14N, the 13C lines can vary from being a sharp 1:1:1 triplet, to a broad unresolved triplet, to a very sharp singlet. Below is an example of a case where the 14N is in a very symmetric environment and the 13C - 14N J couplings are resolved.


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