Chemistry
Corresponding Member of the Academy of Sciences of the USSR K. A. Andrianov, Ionel Haiduc,
Submitted 1963-01-01 | RussiaRxiv: ru-196301.09679 | Translated from Russian

Abstract

Full Text

Chemistry

Corresponding Member of the Academy of Sciences of the USSR K. A. Andrianov, Ionel Haiduc,
L. M. Khananashvili

Unsaturated Derivatives of Cyclotrisilazane and Their Structure

Until now, unsaturated derivatives of the trisilazane heterocycle had not been described. We obtained* vinyl derivatives of cyclosilazanes by the ammonolysis reaction of methylvinyldichlorosilane or by co-ammonolysis of methylvinyldichlorosilane with dimethyldichlorosilane in benzene:

\[ 3(\mathrm{CH}_3)_2\mathrm{SiCl}_2 + 3(\mathrm{CH}_3)(\mathrm{CH}_2=\mathrm{CH})\mathrm{SiCl}_2 + 18\,\mathrm{NH}_3 \rightarrow \]

\[ \rightarrow\ \begin{array}{c} \mathrm{H_3C}\backslash\quad /\mathrm{CH{=}CH_2}\\[-2pt] \mathrm{Si}\\[-2pt] /\ \ \backslash\\[-2pt] \mathrm{HN}\quad \mathrm{NH}\\[-2pt] |\quad\quad |\\[-2pt] \mathrm{H_3C}\backslash \mathrm{Si}\quad \mathrm{Si}/\mathrm{CH_3}\\[-2pt] \mathrm{H_3C}/\quad \backslash\mathrm{N}/\quad \backslash\mathrm{CH_3}\\[-2pt] \quad\quad \mathrm{H} \end{array} \ +\ \begin{array}{c} \mathrm{H_3C}\backslash\quad /\mathrm{CH_3}\\[-2pt] \mathrm{Si}\\[-2pt] /\ \ \backslash\\[-2pt] \mathrm{HN}\quad \mathrm{NH}\\[-2pt] |\quad\quad |\\[-2pt] \mathrm{H_3C}\backslash \mathrm{Si}\quad \mathrm{Si}/\mathrm{CH_3}\\[-2pt] \mathrm{H_2C{=}CH}/\quad \backslash\mathrm{N}/\quad \backslash\mathrm{CH{=}CH_2}\\[-2pt] \quad\quad \mathrm{H} \end{array} \ +\ 12\,\mathrm{NH_4Cl}. \]

In the ammonolysis of methylvinyldichlorosilane, trimethyltrivinylcyclotrisilazane and tetramethyltetravinylcyclotetrasilazane were isolated. In the co-ammonolysis of dimethyldichlorosilane with methylvinyldichlorosilane, pentamethylvinylcyclotrisilazane and tetramethyldivinylcyclotrisilazane were isolated. The physical properties of the compounds obtained are given in Table 1.

Table 1

Compound B.p., °C/mm Hg \(n_D^{20}\) \(d_4^{20}\) MR calculated MR found
Pentamethylvinylcyclotrisilazane
\((\mathrm{CH}_3)_5(\mathrm{CH}_2=\mathrm{CH})\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\)
54—56/3 1.4613 0.9414 67.20 67.51
Tetramethyldivinylcyclotrisilazane
\((\mathrm{CH}_3)_4(\mathrm{CH}_2=\mathrm{CH})_2\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\)
68—70/3 1.4703 0.9656 71.02 70.38
Trimethyltrivinylcyclotrisilazane
\((\mathrm{CH}_3)_3(\mathrm{CH}_2=\mathrm{CH})_3\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\)
100/7 1.4810 0.9673 75.00 75.20
Tetramethyltetravinylcyclotetrasilazane
\((\mathrm{CH}_3)_4(\mathrm{CH}_2=\mathrm{CH})_4\mathrm{Si}_4\mathrm{N}_4\mathrm{H}_4\)
103—105/1 1.4980 0.9979 100.2 100.1

The composition of the compounds obtained was confirmed by elemental analysis and by determination of the molecular weights.

In order to obtain additional data on the structure of the unsaturated derivatives of cyclosilazane, the infrared and ultraviolet absorption spectra of the compounds obtained were studied. There are few works in the literature devoted to the IR spectra of cyclosilazanes, and there are no data at all on the absorption of such compounds in the UV region. The IR spectra were recorded on a UR-10 Karl Zeiss—Jena instrument** in a thin film, without solvent; the experimental data are given in Table 2. For comparison, there was also recorded and

* M. B. Lotarev took part in the synthetic part of the work.
** The authors express their gratitude to H. Manch (Institute of Chemistry, Academy of Sciences of the RPR, Cluj, Romania) and M. Zaitseva (MITKhT) for recording the IR spectra.

IR spectrum of hexamethylcyclotrisilazane. Figure 1 gives the intensities of the bands obtained. In the spectra of all the compounds studied, an absorption band was found in the region 928–930 cm\(^{-1}\), corresponding to the asymmetric

Figure 1. Infrared absorption spectra of organocyclosilazanes: 1 — \((\mathrm{CH}_3)_3(\mathrm{CH}_2=\mathrm{CH})_3\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\), 2 — \((\mathrm{CH}_3)_5(\mathrm{CH}_2=\mathrm{CH})\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\), 3 — \((\mathrm{CH}_3)_6\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\)

Fig. 1. Infrared absorption spectra of organocyclosilazanes:
1 — \((\mathrm{CH}_3)_3(\mathrm{CH}_2=\mathrm{CH})_3\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\), 2 — \((\mathrm{CH}_3)_5(\mathrm{CH}_2=\mathrm{CH})\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\),
3 — \((\mathrm{CH}_3)_6\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\)

stretching vibration of the Si—N—Si bond in the six-membered ring \((^{1,2})\), as well as a band at 618–620 cm\(^{-1}\), corresponding to the symmetric stretching vibration of the Si—N—Si bond. Attention should be drawn to the fact

Table 2

\((\mathrm{CH}_3)_6\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_2=\mathrm{CH})(\mathrm{CH}_3)_5\cdot\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_2=\mathrm{CH})_2(\mathrm{CH}_3)_4\cdot\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_2=\mathrm{CH})_3(\mathrm{CH}_3)_3\cdot\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) Assignment
530 530 530 \(\nu'_{\mathrm{sym}}\) SiNSi
618 620 620 620 \(\nu_{\mathrm{sym}}\) SiC
678 679 677 680
730 730 730
790 791 791 789 \(\nu_{\mathrm{asym}}\) SiC
818 817 810 838 \(\rho\mathrm{CH}_3\)
867 859 853 \(\rho\mathrm{CH}_3\)
928 928 930 928 \(\nu_{\mathrm{asym}}\) SiNSi
1010 1010 1010 \(\delta'=\mathrm{C}—\mathrm{H}\)
1167 1168 1171 1168 \(\gamma\mathrm{NH}\)
1254 1254 1253 1253 \(\delta_{\mathrm{sym}}\ \mathrm{CH}_3\)
1400 1403 1403 1403 \(\delta_{\mathrm{asym}}\ \mathrm{CH}_3\)
1593 1592 1590 \(\nu\mathrm{C}=\mathrm{C}\)
2892 2890 2890 2895 \(\nu_{\mathrm{sym}}\ \mathrm{CH}_3\)
2940
2950 2951 2951 2956 \(\nu_{\mathrm{asym}}\ \mathrm{CH}_3\)
3005 3002
3042 3042
3402 3402 3402 3395 \(\nu\mathrm{NH}\)

that the stretching vibration of the C=C double bond is observed in the region 1590–1593 cm\(^{-1}\), characteristic of vibrations of conjugated double bonds. This apparently should be explained by conjugation of the \(\pi\)-electrons of the double bond with the free \(3d\)-orbitals of silicon.

Table 3

\((\mathrm{CH}_3)_3(\mathrm{CH}_2=\mathrm{CH})_3\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_3)_3(\mathrm{CH}_2=\mathrm{CH})_3\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_3)_4(\mathrm{CH}_2=\mathrm{CH})_2\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_3)_4(\mathrm{CH}_2=\mathrm{CH})_2\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_3)_5(\mathrm{CH}_2=\mathrm{CH})\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\) \((\mathrm{CH}_3)_5(\mathrm{CH}_2=\mathrm{CH})\mathrm{Si}_3\mathrm{N}_3\mathrm{H}_3\)
\(\lambda_{\max},\ \text{Å}\) \(\varepsilon\) \(\lambda_{\max},\ \text{Å}\) \(\varepsilon\) \(\lambda_{\max},\ \text{Å}\) \(\varepsilon\)
2540 4.38 2550 0.65 2480 2.03
2620 4.16 2610 0.49 2540 1.24
2650 2.70 2650 0.47 2600 0.84
2680 3.32 2680 0.45 2640 0.40
2680 0.32

In triallyltrimethylcyclotrisilazane, in comparison with vinylmethylcyclosilazanes, the shifts of the vibration frequencies toward lower frequencies

is not observed. In triallyltrimethylcyclotrisilazane, for the $C=C$ bond an absorption band is observed at 1632 cm$^{-1}$, which corresponds, as was to be expected, to a nonconjugated double bond.

This fact is also observed in the IR spectra of vinyl- and allylchlorosilanes ($^3$). There are data ($^4$) according to which the bond order of Si—N—Si is 1.18, i.e., the unshared electron pairs of nitrogen are partially delocalized with participation of the $3d$ orbitals of silicon. It was therefore of interest to determine whether the conjugation

$$ \mathrm{Si—C=C} $$

is transmitted through the inorganic ring from one vinyl group to another. In order to obtain data making it possible to judge this, we measured the absorption spectra of the compounds obtained in the UV region with a VSU-1 Carl Zeiss—Jena spectrophotometer. In the spectrum of hexamethylcyclotrisilazane we found no absorption maxima. Hexamethylcyclotrisilazane without solvent (layer thickness 0.5 cm) is transparent to UV rays with wavelength $\lambda > 3200$ Å (Fig. 2). In the spectra of vinyl derivatives of cyclotrisilazane, in the region 2400–2700 Å, several absorption maxima appear because of the presence of double bonds in the molecule of the compounds studied. Figure 2 gives the UV spectra of trimethyltrivinylcyclotrisilazane and pentamethylvinylcyclotrisilazane in $n$-hexane. Table 3 lists the wavelengths at which maxima appear ($\lambda_{\max}$) and the corresponding molar absorption coefficients ($\varepsilon$).

Fig. 2. UV spectrum of hexamethylcyclotrisilazane and methylvinylcyclosilazanes. 1—trimethyltrivinylcyclotrisilazane; 2—pentamethylvinylcyclotrisilazane; 3—hexamethylcyclotrisilazane

Fig. 2. UV spectrum of hexamethylcyclotrisilazane and methylvinylcyclosilazanes. 1—trimethyltrivinylcyclotrisilazane; 2—pentamethylvinylcyclotrisilazane; 3—hexamethylcyclotrisilazane

As follows from the values of $\varepsilon$ given in Table 3, the absorption bands found are $R$-bands, i.e., the double bonds are isolated, nonconjugated ($^5$). From this it may be concluded that in vinyl derivatives of cyclotrisilazane no conjugation of the double bonds of the vinyl groups through the inorganic heterocycle $\mathrm{Si_3N_3}$ is observed, and it is limited only outside the ring, between the silicon atom and the group —HC=CH$_2$.

Moscow Institute of Fine Chemical Technology
named after M. V. Lomonosov

Received
6 II 1963

CITED LITERATURE

  1. H. Kriegsmann, Zs. anorg. u. allg. Chem., 298, 223 (1959).
  2. G. V. Tsitsishvili, G. D. Bargatishvili et al., Izv. AN SSSR, OKhN, 1962, 1197.
  3. V. F. Mironov, N. A. Chumaevskii, DAN, 146, 1117 (1962).
  4. H. Kriegsmann, Zs. Elektrochem., 61, 1088 (1959).
  5. A. Gillam, E. Stern, Electronic Absorption Spectra of Organic Compounds, IL, 1957.

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Chemistry