M. A. SALIMOV and V. M. TATEVSKII
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Submitted 1957-01-01 | RussiaRxiv: ru-195701.03799 | Translated from Russian

Abstract

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PHYSICAL CHEMISTRY

M. A. SALIMOV and V. M. TATEVSKII

INFRARED SPECTRA OF SOME SECONDARY AROMATIC AMINES

(Presented by Academician P. A. Rehbinder, September 11, 1956)

Secondary aromatic amines are of great importance in the chemical industry as inhibitors used as additives to rubbers in rubber mixtures.

Meanwhile, no systematic study has been made of the relationship between structure and vibrational spectra in secondary amines. In Colthup’s review (^1), where, along with other aromatic compounds, aliphatic and aliphatic-aromatic amines are considered, it is mentioned that secondary amines have intense absorption bands in the regions 1200–1300 and 3600–3500 cm^−1, which the author assigns to the stretching vibrations of the C—N and N—H bonds, respectively.

Fig. 1. Infrared spectrum of dinaphthylamine

Fig. 1. Infrared spectrum of dinaphthylamine

In Bellamy’s monograph (^2) it is also noted that all secondary amines in dilute solutions have one band in the 3200–3500 cm^−1 region, while at higher concentrations, owing to hydrogen bonding, a second absorption band appears on the long-wavelength side. For the absorption band of the stretching vibration of the C—N bond the region 1280–1350 cm^−1 is given. These works, as well as a number of others, discuss the position of the absorption band of the out-of-plane deformation vibration of the N—H bond. In secondary amines the absorption band of this vibration is of low intensity; it is assumed that it should appear in the region 1480–1650 cm^−1, i.e., in the same region as the characteristic band for the in-plane deformation vibration of the C—H bond (^3). In other works (^4,^5), individual portions of the spectrum of diphenylamine are considered. Thus, the literature contains no complete consideration of the vibrational spectra of secondary aromatic amines, nor complete infrared absorption spectra. As for tetraphenylhydrazine, the literature contains no information about its vibrational spectrum.

In the present work, a study was made of the infrared absorption spectra of diphenylamine, dinaphthylamine, β-naphthyl-N-phenylamine, and tetraphenylhydrazine in the region 4000–3700 cm^−1.

Before recording, the aromatic amines were purified by repeated recrystallization. Tetraphenylhydrazine was obtained from diphenylamine

…by the method described in the literature (9). The infrared absorption spectra of all the substances studied were obtained in the solid phase by depositing from solution onto a KBr plate. The spectra of the amines and tetraphenylhydrazine were recorded on an IKS-11 infrared spectrograph. The infrared spectrum of tetraphenylhydrazine was also obtained at 100° in a thermostated cuvette. The following slits were used:

Prism Frequency interval, cm⁻¹ Spectral width, cm⁻¹
KBr 450—500 6
KBr 500—700 5
NaCl 650—800 4
NaCl 760—1075 5
NaCl 990—1340 7
NaCl 1300—1500 9
NaCl 1500—1600 11
NaCl 1600—1750 13
NaCl 1700—3500 16
LiF 2300—3500 8

The frequencies of the infrared absorption bands obtained are summarized in Table 1. The spectra obtained contain characteristic bands of the amines, as well as of the phenyl and β-naphthyl radicals, respectively.

In the region of the stretching vibration of the N—H bond, all the amines have two absorption bands: for dinaphthylamine, 3425 and 3465 cm⁻¹; for β-naphthyl-N-

Table 1

Dinaphthylamine ν, cm⁻¹ Dinaphthylamine intensity* β-Naphthyl-N-phenylamine ν, cm⁻¹ β-Naphthyl-N-phenylamine intensity Diphenylamine ν, cm⁻¹ Diphenylamine intensity Tetraphenylhydrazine ν, cm⁻¹ Tetraphenylhydrazine intensity
475 weak 460 weak 460 weak
485 weak 485 weak
615 weak
658 weak 645 weak
690 very strong 691 very strong 690 very strong
701 medium
736 very strong 735 very strong 735 very strong 740 very strong
806 very strong 820 medium
851 very strong
880 strong 860 strong 880 strong
885 weak
915 weak
968 weak 960 weak
1002 weak 1008 weak
1040 weak 1020 weak 1038 weak 1040 weak
1070 weak 1080 weak 1086 weak 1000 weak
1115 weak 1115 weak 1098 weak
1130 weak
1168 weak 1162 weak 1160 weak
1172 weak 1178 weak
1188 weak
1235 weak 1215 weak 1225 weak 1208 weak
1238 weak 1240 weak
1260 very strong 1298 very strong 1250 strong
1280 strong 1276 very strong 1312 very strong 1275 very strong
1300 strong
1380 weak
1400 weak 1400 weak 1425 medium 1420 medium
1450 weak 1460 medium 1459 medium
1405 strong 1495 very strong
1515 very strong 1500 very strong 1520 very strong
1535 very strong 1535 weak
1550 weak
1562 very strong 1562 weak
1598 very strong 1599 very strong 1598 very strong
1615 medium 1620 strong
1650 weak
1700 weak
1750 weak
1775 weak
3060 weak 3060 medium 3050 weak 3085 weak
3085 strong 3074 strong
3425 weak 3430 medium 3392 strong
3435 strong 3450 strong 3430 strong

* Band intensity: weak — weak, medium — medium, strong — strong, very strong — very strong.

aniline: 3430 and 3450 cm\(^{-1}\), and for diphenylamine: 3392 and 3430 cm\(^{-1}\), the shorter-wavelength band in all the amines being more intense than the longer-wavelength one. Apparently, the longer-wavelength band arises due to intermolecular hydrogen bonding of the amino hydrogen, while the shorter-wavelength band belongs to the stretching vibration of the N—H bond. Naturally, in tetraphenylhydrazine no absorption bands are observed in this region. As might have been expected, in the region 3050—3085 cm\(^{-1}\) all the amines have intense absorption bands, which undoubtedly belong to the stretching vibration of aromatic C—H bonds. In diphenylamine and β-naphthyl-N-phenylamine, on the long-wavelength side there is also another band, which is possibly explained by splitting of the frequency in connection with intermolecular interactions occurring in the solid phase.

Infrared spectrum of β-naphthyl-N-phenylamine

Fig. 2. Infrared spectrum of β-naphthyl-N-phenylamine

In all the amines and in tetraphenylhydrazine, intense absorption bands are present in the region 1200—1300 cm\(^{-1}\), which apparently belong to the stretching vibration of C—N bonds. However, it should be noted that if dinaphthylamine has one band with a frequency of 1280 cm\(^{-1}\), then β-naphthyl-N-phenylamine and diphenylamine have two bands each (1260, 1276 and 1298, 1312 cm\(^{-1}\), respectively). Tetraphenylhydrazine has three absorption bands in this region (1250, 1275, and 1300 cm\(^{-1}\)). Apparently one of them (probably the 1300 cm\(^{-1}\) band) belongs to the stretching vibration of the N—N bond, although for this vibration in the case of hydrazine the band 850 cm\(^{-1}\) is assigned \((^6)\). As can be seen from Table 1, we have no bands with such a frequency. It is known that tetraphenylhydrazine at temperatures above 70° readily decomposes, giving free diphenylazotyl radicals. Evidently, upon decomposition of the molecule, the intensity of the absorption band of the stretching vibration of the N—N bond should decrease. Indeed, the infrared absorption spectrum of tetraphenylhydrazine obtained at 100° (Fig. 4, dotted curve) shows a sharp decrease in the intensity of the 1300 cm\(^{-1}\) absorption band, whereas the bands at 1250 and 1275 cm\(^{-1}\) merge into one. Other regions of the spectrum show no substantial changes. The bands at 1250 and 1275 cm\(^{-1}\) apparently belong to the symmetric and antisymmetric stretching vibrations of C—N bonds. Incidentally, in two of the three amines studied, in the region 1200—1300 cm\(^{-1}\)

Infrared spectrum of diphenylamine

Fig. 3. Infrared spectrum of diphenylamine

there are two bands each, which, apparently, could also be assigned to the symmetric and antisymmetric vibrations of the C—N bonds. It does not seem possible to assign any band unambiguously to the in-plane deformation vibration of the N—H bond. When comparing the absorption bands of diphenylamine and tetraphenylhydrazine, it is not difficult to see that the bands at 1459 and 1520 cm\(^{-1}\) of diphenylamine disappear on going to tetraphenylhydrazine. The frequencies 1450 cm\(^{-1}\) in dinaphthylamine and 1460 cm\(^{-1}\) in β-naphthyl-N-phenylamine are very close to one of the above-mentioned frequencies (to 1459 cm\(^{-1}\)) of diphenylamine. These bands could tentatively be assigned to the in-plane deformation vibration of the N—H bonds in amines. Out-of-plane deformation vibrations of the N—H and C—H bonds fall in the region 700–1000 cm\(^{-1}\). From the data obtained it is not difficult to see that in this region, in addition to the band belonging to the vibrations of the C—H bonds of the phenyl and naphthyl radicals, all the amines have intense bands (860–880 cm\(^{-1}\)), while tetraphenylhydrazine has no band in this region, which once again supports our supposition. These bands, apparently, belong to out-of-plane deformation vibrations of the N—H bond. In symmetrical amines (i.e., in naphthylamine and diphenylamine) the frequencies of these bands are the same (880 cm\(^{-1}\)), while in β-naphthyl-N-phenylamine it is somewhat lowered (860 cm\(^{-1}\)). The remaining bands may be assigned to various vibrations of the phenyl and β-naphthyl radicals.

Fig. 4. Infrared spectrum of tetraphenylhydrazine

Fig. 4. Infrared spectrum of tetraphenylhydrazine

The intense bands at 690, 740, 1495, and 1598 cm\(^{-1}\) in tetraphenylhydrazine undoubtedly belong to various vibrations of the phenyl group \((^1)\). Very close in frequency and intensity are the bands of the phenyl group (691, 735, 1495, and 1599 cm\(^{-1}\)) present in diphenylamine. In considering the bands of dinaphthylamine it is not difficult to note the characteristic absorption bands of the β-naphthyl \((^7)\) radical, namely: 736, 806, and 851 cm\(^{-1}\); the remaining intense bands (1515, 1535, 1562, 1615, and 1650 cm\(^{-1}\)) are characteristic \((^8)\) of the naphthalene skeleton. The spectrum of β-naphthyl-N-phenylamine has absorption bands characteristic both of the phenyl and of the naphthyl radicals.

Thus, consideration of the infrared absorption spectra obtained makes it possible to establish a certain correspondence between the structure and the vibrational spectra of secondary aromatic amines.

Moscow State University
named after M. V. Lomonosov

Received
7 IX 1956

CITED LITERATURE

  1. B. Colthup, J. Opt. Soc. Am., 40, 397 (1950).
  2. L. J. Bellamy, The Infrared Spectra of Complex Molecules, 1955.
  3. D. A. Barr, R. N. Haszeldine, J. Chem. Soc., 1955, 4169.
  4. N. Fuson, M. Josien, R. L. Povell, E. Utterback, J. Chem. Phys., 20, 145 (1952).
  5. R. B. Barnes, R. C. Gore, U. Liddel, V. Z. Williams, Infrared Spectroscopy and its Industrial Application, 1944, p. 88.
  6. V. M. Chulanovskii, Introduction to Molecular Spectral Analysis, 1951, p. 394.
  7. R. L. Werner, W. Kennard, D. Rayson, Austr. J. Chem., 8, 346 (1955).
  8. W. B. Person, G. G. Pimentel, O. Schnepp, J. Chem. Phys., 23, 230 (1955).
  9. L. Gatterman, G. Wieland, Practical Work in Organic Chemistry, 1948, p. 397.

Submission history

M. A. SALIMOV and V. M. TATEVSKII