When we obtain a proton decoupled 13C spectrum the intensities of many of the carbon resonances increases significantly above those observed in a proton-coupled experiment carbon atoms with hydrogen atom directly attached are enhanced the most and the enhancement increases (but not always linearly) as more hydrogen are attached. This effect is known as the nuclear overhauser enhancement.
The nuclear overhauser effect is general, showing up when one of the two different types of atoms is irradiated while the NMR spectrum of the other type is determined.
The effect can be either positive or negative depending on which atom type are involved. In the case of carbon-13 interacting with hydrogen-1, the effect is positive irradiating the hydrogen increases the intensities of the carbon signals. The maximum enhancement that can be observed is given by the relationship,
NOE max = 1/2(r irr/r obs)
For a proton decoupled 13C spectrum
NOE max = 1/2 (2.675/0.6728) = 1.988
This value is a theoretical maximum and most actual cases exhibit less than ideal enhancement.
The nuclear overhauser effect is general, showing up when one of the two different types of atoms is irradiated while the NMR spectrum of the other type is determined.
The effect can be either positive or negative depending on which atom type are involved. In the case of carbon-13 interacting with hydrogen-1, the effect is positive irradiating the hydrogen increases the intensities of the carbon signals. The maximum enhancement that can be observed is given by the relationship,
NOE max = 1/2(r irr/r obs)
For a proton decoupled 13C spectrum
NOE max = 1/2 (2.675/0.6728) = 1.988
This value is a theoretical maximum and most actual cases exhibit less than ideal enhancement.
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