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Summary
- Indirect spin-spin coupling occurs between two or more groups
of protons, if these protons are
- non-equivalent and
- in sufficient proximity
(i.e., in s systems they should
be in general separated by three or fewer
s-bonds).
(Check also page 87 and the subsequent links)
- The multipilcity of the fine structure in the NMR signal of
a group of protons A due to spin-spin
coupling
- a single neighboring group X
with nX
equivalent protons can be predicted by using the following formula:
- with multiple distinct neighboring groups of protons
M, X, ...
with respectively nM,
nX, ...
equivalent protons can be predicted using the following formula:
| MA =
(nM + 1) ·
(nX + 1) ... |
(Check page 95 for detailed explanations).
- The intensities of the individual lines of a multiplet caused
by interactions with a neighboring group of protons follow a pattern
similar to the factors in a n-th degree binominal equation.
(Check page 78. for detailed explanations)
- The coupling constant
JAX is a measure of the
intensity of the indirect spin-spin coupling between the two
protons A and X.
It is defined as:
| JAX = |
Distance between two adjacent individual lines in the
multiplet signal of the proton group
A, caused by the coupling with the group
X, in Hertz. |
The value of the coupling constant is independent of the working
frequency of the spectrometer.
A list of typical values for coupling constants can be at this site
Spectroscopic
Tools at the Potsdam University. (You might also want to review
page 81 and the links branching from there).
You have now officially earned a short break before you move on to
page 109, where you will tackle a couple of simple
structural problems using 1H-NMR spectroscopy.
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