A method is developed for calculating the chemical shifts and spin‐spin coupling constants for a system of three spin‐½ nuclei (ABC) directly from the nuclear resonance spectrum. Trial‐and‐error adjustment of these parameters is avoided entirely, and the values obtained are exactly consistent with the input information. The use of experimental intensities is kept separate from that of experimental frequencies, and the former may be omitted entirely when experimental values of sufficient accuracy are not available. It is shown that previously unknown ambiguities in the assignment of parameters sometimes arise, and that conventional iterative analyses may occasionally lead to the wrong answer. The proton resonance spectra of four compounds containing vinyl groups are discussed as illustrations of the method.

1.
J. A. Pople, W. G. Schneider, and H. J. Bernstein, High Resolution Nuclear Magnetic Resonance (McGraw‐Hill Book Company, Inc., New York, 1958), Chap. 6.
2.
R. W.
Fessenden
and
J. S.
Waugh
,
J. Chem. Phys.
30
,
944
(
1959
).
3.
R. W.
Fessenden
and
J. S.
Waugh
,
J. Chem. Phys.
31
,
996
(
1959
).
4.
J. S.
Waugh
and
F. W.
Dobbs
,
J. Chem. Phys.
31
,
1235
(
1959
).
5.
N. Sheppard (private communication).
6.
J. H.
Van Vleck
,
Phys. Rev.
74
,
1168
(
1948
).
7.
W. A.
Anderson
and
H. M.
McConnell
,
J. Chem. Phys.
26
,
1496
(
1957
).
(a) The methods used in this section constitute a somewhat more complete and systematic use of the consequences of trace invariance than a similar procedure very recently described by
S.
Alexander
[
J. Chem. Phys.
32
,
1700
(
1960
)],
and are also related to the methods employed by
C. A.
Reilly
and
J. D.
Swalen
[
J. Chem. Phys.
32
,
1378
(
1960
)] in finding the eigenvalues.
8.
H. J. Bernstein (private communication).
9.
J.
Von Neumann
and
E.
Wigner
,
Physik. Z.
30
,
467
(
1929
);
see also L. D. Landau and E. M. Lifschitz, Quantum Mechanics (Addison‐Wesley Publishing Company, Reading, Massachusetts, 1958), pp. 262–266.
(a)
H. S.
Gutowsky
,
M.
Karplus
, and
D. M.
Grant
,
J. Chem. Phys.
31
,
1278
(
1959
), and other papers referred to there.
10.
E. O.
Bishop
and
R. E.
Richards
,
Mol. Phys.
3
,
114
(
1960
).
11.
The paper by E. O. Bishop and R. E. Richards10 which reached us as this manuscript was being completed, contains an analysis of the vinyl acetate spectrum which disagrees with ours in its conclusion that the gem‐coupling constant is negative. Probably their result is correct and our failure to obtain it arose because, as remarked previously, we did not exhaust the possibilities of the analysis in this case. It is significant in this connection that our coupling constants agree rather well with the ones they obtain under the assumption that all of them are positive. The sum of their final coupling constants is 19.1 cps, which agrees approximately with the second largest of our possible values of S111 (18.65 cps).
12.
Footnote reference 1, Chap. 8.
13.
S. Perlis, Theory of Matrices (Addison‐Wesley Publishing Company, Reading, Massachusetts, 1956), Chap. 9.
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