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Introductory discussion to 13 C-NMR
PRESENTED BY: SHEAMA FARHEEN SAVANUR
INTRODUCTION
The study of carbon nuclei through nuclear magnetic resonance
(NMR) spectroscopy is a important technique for determining the
structures of organic molecules along with infrared and proton
NMR.
It can be used to determine the number of non equivalent
carbons and to identify the types of carbon atoms that may be
present in a compound. Thus, 13C-NMR provides direct
information about carbon skeleton of a molecule.
THE 13C NUCLEUS
Carbon-12 nucleus, the most abundant isotope of carbon is NMR inactive since it
has a spin (I) of zero. Carbon-13,however has odd mass and does have nuclear
spin I=1/2
But the resonance of 13C are most difficult to observe than those of protons
mainly because of 2 reasons namely
 The natural abundance of carbon-13 is very low.
 The magnetogyric ratio of a 13C nucleus is smaller than that of hydrogen
For a given magnetic strength, the resonance of a 13C nucleus is about one-
fourth the frequency required to observe proton resonances.
CORRELATION CHARTS
Correlation charts for different functional
groups
Proton-coupled 13C spectra-spin spin splitting of
carbon-13 signals
Spectra that show the spin-spin splitting, or coupling, between carbon-
13 and the protons directly attached to it are called Proton-Coupled
Spectra or sometimes Nondecoupled Spectra.
Proton-coupled spectra for large molecules are often difficult to interpret.
The multiplets from different carbons commonly overlap because the
13C-H coupling constants are frequently larger than the chemical shift
differences of the carbons in the spectrum. Sometimes interpretation of
spectra for some molecules become difficult.
Proton decoupled 13C spectra
Most modern spectrophotometers have proton decoupler, i.e. a
second tunable radiofrequency generator.
Here the decoupling of spin-spin interactions take place, and all the
spin interactions are averaged to zero.
The decoupling technique obliterates all interactions between protons
and 13 C nuclei; therefore only singlets are observed are observed in
the decoupled 13 C NMR spectra. This technique although simplifies
the spectrum and avoids overlapping multiplets, it has its own
disadvantage that the information on attached hydrogen is lost.
Example: Ethyl phenylacetate
THANK YOU

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Introductory discussion to 13 C NMR

  • 1. Introductory discussion to 13 C-NMR PRESENTED BY: SHEAMA FARHEEN SAVANUR
  • 2. INTRODUCTION The study of carbon nuclei through nuclear magnetic resonance (NMR) spectroscopy is a important technique for determining the structures of organic molecules along with infrared and proton NMR. It can be used to determine the number of non equivalent carbons and to identify the types of carbon atoms that may be present in a compound. Thus, 13C-NMR provides direct information about carbon skeleton of a molecule.
  • 3. THE 13C NUCLEUS Carbon-12 nucleus, the most abundant isotope of carbon is NMR inactive since it has a spin (I) of zero. Carbon-13,however has odd mass and does have nuclear spin I=1/2 But the resonance of 13C are most difficult to observe than those of protons mainly because of 2 reasons namely  The natural abundance of carbon-13 is very low.  The magnetogyric ratio of a 13C nucleus is smaller than that of hydrogen For a given magnetic strength, the resonance of a 13C nucleus is about one- fourth the frequency required to observe proton resonances.
  • 5. Correlation charts for different functional groups
  • 6. Proton-coupled 13C spectra-spin spin splitting of carbon-13 signals Spectra that show the spin-spin splitting, or coupling, between carbon- 13 and the protons directly attached to it are called Proton-Coupled Spectra or sometimes Nondecoupled Spectra. Proton-coupled spectra for large molecules are often difficult to interpret. The multiplets from different carbons commonly overlap because the 13C-H coupling constants are frequently larger than the chemical shift differences of the carbons in the spectrum. Sometimes interpretation of spectra for some molecules become difficult.
  • 7. Proton decoupled 13C spectra Most modern spectrophotometers have proton decoupler, i.e. a second tunable radiofrequency generator. Here the decoupling of spin-spin interactions take place, and all the spin interactions are averaged to zero. The decoupling technique obliterates all interactions between protons and 13 C nuclei; therefore only singlets are observed are observed in the decoupled 13 C NMR spectra. This technique although simplifies the spectrum and avoids overlapping multiplets, it has its own disadvantage that the information on attached hydrogen is lost.