A systematic study of Raman spectra has been made for a large number of carboxylic acids and their salts dissolved in water. In particular, malonic acid and its two sodium salts, and malonic‐d2 acid‐d2 and its disodium salt, have been studied in detail. The substitution of deuterium in this molecule permits the vibrations arising primarily from the — CH2 group to be distinguished from those arising primarily from the carboxyl groups. The Raman spectrum of deuterium oxide has been redetermined in connection with these studies. The following general conclusions have been reached: (1) The powerful ``carbonyl'' frequency near 1700 cm—1 is always found when an un‐ionized carboxyl group is present, and always vanishes on ionization of the carboxyl. (2) One or more intense Raman lines near 1400 cm—1 can always be found in a substance containing an ionized carboxyl group. Such lines are definitely polarized, and presumably correspond to a symmetrical valence oscillation of the COO group. Like the ``C=O'' frequency near 1700, these lines are almost unaffected by deuterium substitution. Deformation frequencies arising from —CH2 or —CH3 groups commonly lie in the same range; the marked effect of deuterium substitution, however, clearly differentiates these from the vibrations of the —COO group. (3) Other Raman lines, near 1330 and 1580 cm—1, are frequently but not invariably found in substances containing ionized carboxyl groups. (4) Most of the substances studied show strong Raman lines between 700 and 950 cm—1, which increase in frequency by 30 to 50 cm—1 on ionization. These lines are strongly polarized, and in malonic acid are noticeably depressed in frequency by deuterium substitution. (5) Certain frequencies below 600 cm—1 are virtually unaffected either by ionization or by deuterium substitution. These presumably represent bending or twisting vibrations of the heavy molecular framework. The ``C=C'' frequency near 1650 in crotonic and maleic acids is unchanged by the ionization of a neighboring carboxyl group. The Raman spectra of d‐tartaric acid and of mesotartaric acid, although very similar, show definite differences which are well beyond the experimental error. The structure of the ionized carboxyl group is undoubtedly closely related to that of the nitro group. Both show intense polarized Raman lines near 1400, probably corresponding to the same type of oscillation in both cases; and the bond strength in the two groups is probably nearly the same.

1.
J. T.
Edsall
,
J. Chem. Phys.
4
,
1
(
1936
).
2.
J. T.
Edsall
,
J. Phys. Chem.
41
,
133
(
1937
).
3.
J. T.
Edsall
,
J. Chem. Phys.
5
,
225
(
1937
).
4.
J. O.
Halford
and
L. C.
Anderson
,
J. Am. Chem. Soc.
58
,
736
(
1936
).
5.
W. R.
Angus
,
A. H.
Leckie
, and
C. L.
Wilson
,
Proc. Roy. Soc. A
,
155
,
183
(
1936
).
6.
Engler
,
Zeits. f. Physik. Chemie
B32
,
471
(
1936
).
7.
Other modes of vibration in these molecules undoubtedly exist, in which the hydrogens of the CH2 or CD2 groups play an important part (for instance, a bending frequency involving a motion of the hydrogens approximately parallel to the plane of the three carbon atoms). Such frequencies, however, if they do give rise to any of the observed Raman lines, are much less affected by deuterium substitution than the three listed in Table II. Raman lines arising from the carboxylic O‐H and O‐D groups might be expected to appear, but have not been found. Quite probably they coincide with the intense bands arising from the solvent H2O or D2O.
8.
Another very weak frequency near 2075 was found in malonic‐d2 acid‐d2 and its disodium salt (see Table V).
9.
Similarly the C=Ofrequency which lies near 1670 in CH3COOH, decreases only to 1657 in CD3COOD (reference 5).
10.
K. W. F.
Kohlrausch
and
F.
Koppl
,
Zeits. f. Physik. Chemie
B26
,
209
(
1934
).
11.
A.
Dadieu
,
A.
Pongratz
, and
K. W. F.
Kohlrausch
,
Ber. Wiener Akad. Wiss IIa
,
140
,
353
,
647
(
1931
) studied the Raman spectrum of pure crotonic acid above its melting point and found one frequency in this range at 1654, while we obtain two frequencies (1658 and 1700) in the aqueous solution. In pure liquid fatty acids, the C=Ofrequency is about 50 cm−1 lower than in their aqueous solutions (reference 1). Similarly the C=Ofrequency in pure crotonic acid should lie near 1650, where it will coincide with the C=C” frequency and not be observed. This probably explains the difference between Kohlrausch’s observations and ours.
12.
In addition to the data given in Table IV,
J. C.
Ghosh
and
B. C.
Kar
,
J. Phys. Chem.
35
,
1735
(
1931
) have reported a very strong Raman line at 1402 in sodium benzoate, although benzoic acid shows no frequency in this range. This line also may therefore be attributed to the ionized carboxyl group.
13.
K. W. F.
Kohlrausch
,
F.
Köppl
, and
A.
Pongratz
,
Zeits. f. Physik. Chemie
B21
,
242
(
1933
)
and
K. W. F.
Kohlrausch
,
F.
Köppl
, and
A.
Pongratz
,
22
,
359
(
1933
) have concluded that a frequency near 1410 is characteristic of the un‐ionized carboxyl group in the fatty acids. This frequency is much weaker than the 1400 line arising from the ionized group; its polarization character is not yet known. Whether both frequencies arise from a fundamentally similar mode of vibration is a question that cannot yet be answered.
14.
J. M. Robertson and I. Woodward, J. Chem. Soc. 1817 (1936).
15.
S. B.
Hendricks
and
M. E.
Jefferson
,
J. Chem. Phys.
4
,
102
(
1936
).
16.
J.
Cabannes
and
A.
Rousset
,
Ann. de Physique
19
,
269
(
1933
).
17.
See
G. B. B. M.
Sutherland
and
D. M.
Dennison
,
Proc. Roy. Soc.
A148
,
250
(
1935
) for the normal modes of vibration of a molecule of this type (formaldehyde). The vibration shown above is ν1 in their notation.
18.
This interpretation of the 1351 line in the formate ion has already been proposed by
J.
Gupta
,
Indian J. Phys.
10
,
313
(
1936
), who has found the line to be highly polarized (ρ = 0.16).
Gupta
has also (
Indian J. Phys.
10
,
199
,
465
(
1936
)) attempted an interpretation of the spectrum of the oxalate ion, whose structure is closely related to that of ethylene. He attributes the intense doublet near 1470 in this ion to what is essentially a symmetrical valence oscillation of the two COO groups, in agreement with the view adopted here.
19.
A group of three similar masses held together by single bonds has a much lower characteristic frequency for this type of symmetric oscillation. Thus the value for propane is 867, and for dimethyl amine, 931 (3).
20.
L.
Pauling
,
L. O.
Brockway
, and
J. Y.
Beach
,
J. Am. Chem. Soc.
57
,
2705
(
1935
).
21.
J. H.
Hibben
,
J. Chem. Phys.
3
,
675
(
1935
).
22.
H.
Nisi
,
Jap. J. Phys.
7
,
1
(
1931
).
23.
For a complete list of references up to the end of 1935, see
J. H.
Hibben
,
Chem. Rev.
18
,
1
(
1936
). References and complete tables of Raman spectra up to about the same period are given by J. Weiler in Landolt‐Börnstein’s Tabellen, fifth edition, 3rd Ergänzungsband, Part II.
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