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Formation of stable 1,2,3-benzodithiazolyl radicals by thermolysis of 1,3,2,4-benzodithiadiazines

 

作者: Victor A. Bagryansky,  

 

期刊: Mendeleev Communications  (RSC Available online 2000)
卷期: Volume 10, issue 1  

页码: 5-7

 

ISSN:0959-9436

 

年代: 2000

 

出版商: RSC

 

数据来源: RSC

 

摘要:

Mendeleev Communications Electronic Version, Issue 1, 2000 (pp. 1–42) Formation of stable 1,2,3-benzodithiazolyl radicals by thermolysis of 1,3,2,4-benzodithiadiazines Victor A. Bagryansky,*a Ivan V. Vlasyuk,b Yuri V. Gatilov,c Alexander Yu. Makarov,c Yuri N. Molin,a Vladimir V. Shcherbukhind and Andrey V. Zibarev*c a Institute of Chemical Kinetics and Combustion, Siberian Branch of the Russian Academy of Sciences, 630090 Novosibirsk, Russian Federation.Fax: +7 3832 34 2350; e-mail: vbag@kinetics.nsc.ru b Department of Natural Sciences, Novosibirsk State University, 630090 Novosibirsk, Russian Federation c N. N. Vorozhtsov Novosibirsk Institute of Organic Chemistry, Siberian Branch of the Russian Academy of Sciences, 630090 Novosibirsk, Russian Federation. Fax: +7 3832 34 4752; e-mail: zibarev@nioch.nsc.ru d N.D. Zelinsky Institute of Organic Chemistry, Russian Academy of Sciences, 117913 Moscow, Russian Federation. Fax: +7 095 135 5328 DOI: 10.1070/MC2000v010n01ABEH001198 Mild thermolysis (at 110–150 °C) of 1,3,2,4-benzodithiadiazine 1 and its derivatives 2–6 in hydrocarbon solvents quantitatively yielded stable 1,2,3-benzodithiazolyl p-radicals via a first-order reaction (Ea = 76.2 kJ mol–1, k0 = 4.34×105 s–1 for 1).The heteroatom reactivity of 1,3,2,4-benzodithiadiazine1 1 and its derivatives2,3 (Scheme 1) which exhibit formal features of antiaromaticity4 (such as a planar or nearly planar geometry, a united molecular 12p-electron system, and low-energy excited states)1–3,5,6 is poorly known.1,3,7 Reasonably, the first step in studying the chemistry of these compounds is the investigation of their thermal stability and the identification of decomposition products.We found that mild (~110–150 °C) thermolysis of 1–6 in hydrocarbon solvents (squalane, trans-decalin, cyclohexane or hexane) resulted with nearly quantitative yields in stable radicals 1·–6·, which were identified by EPR spectroscopy (Figures 1 and 2, Table 1).† The EPR spectra of these radicals generated from 1–3 corresponded to those published earlier for 1,2,3- benzodithiazolyl p-radicals 1·–3· prepared by other methods,8–11 mainly by reduction of corresponding Herz salts (1,2,3-arenodithiazolium chlorides12).‡ Radicals 1·–3· were initially assigned the 1,2-benzothiazetyl structure8,9 (Scheme 1), which was further corrected to 1,2,3-benzodithiazolyl on the basis of EPR experiments with 33S-enriched species. These experiments indicated the presence of two nonequivalent sulfur atoms.11 The 1,2,3-benzodithiazolyl structure is also consistent with the fact that the radicals can be oxidised into Herz salts by molecular chlorine.10 Radicals 4·–6· have been synthesised for the first time; thus, this approach is superior to methods reported previously.8–11 In particular, the corresponding Herz salts12 were not yet described.The assignment of HFI constants in 1·–6· (Table 1) was based on earlier data,8–11 substitutional effects and the results of the ab initio B3LYP/CC-pVDZ calculations of spin density distribution. The calculated constants were consistent with the experimental data (Table 1). 10 G 1· 2· 3· Experiment Simulation Figure 1 Experimental (in squalane) and simulated EPR spectra of 1·–3·. Differences in the HF line widths were ignored in simulating the spectra. R4 R1 R3 R2 S N S N R4 R1 R3 R2 S S N R4 R1 R3 R2 S N or D 1–6 1·–6· 1, 1· R1 = R2 = R3 = R4 = H 2, 2· R1 = R2 = R4 = H, R3 = Me 3, 3· R1 = R2 = R4 = H, R3 = OMe 4, 4· R1 = R2 = R3 = R4 = F 5, 5· R1 = R2 = R4 = H, R3 = F 6, 6· R1 = R3 = R4 = H, R2 = FMendeleev Communications Electronic Version, Issue 1, 2000 (pp. 1–42) The kinetic build-up curve of radical 1· in the thermolysis of compound 1 in squalane (Figure 3) was adequately approximated by the first-order equation A = B(1 – e–kt) (where B and k are † Compounds 1–6 were synthesised and purified as described earlier.1–3 The EPR spectra were recorded on a Bruker EMX spectrometer (MW power, 0.64 mW; modulation frequency, 100 KHz; modulation amplitude, 0.1 G).The spectra simulation was performed with the Simfonia-Bruker program. The spin density distribution and HFI constants were calculated at the B3LYP/CC-pVDZ level of theory using the Gaussian 94™ program.13 In a typical experiment, 10–3 M solutions of 1–6 in a hydrocarbon (squalane, trans-decalin, cyclohexane or hexane), outgassed by three freeze–pump–thaw cycles, was gradually heated in an EPR valve-equipped quartz capillary up to 150 °C (in squalane, the detectable amounts of radicals appeared at 110 °C, whereas in cyclohexane even at 90 °C).After holding for 1 h at this temperature, the sample was cooled to 20 °C, and the EPR spectrum was measured. The g-factors of 1·–6· were measured using a DPPH standard.Nearly quantitative conversion of 1–6 into 1·–6· was determined by a CuCl2·2H2O standard with an accuracy of ±15%. At 20 °C, the concentrations of 1·–6· in air-protected solutions decreased only by 30% for 3 weeks. In the presence of oxygen, the radicals are less stable, especially under heating.Thus, in an air-saturated solution at 150 °C, the EPR signal completely decayed in 5 min. ‡ 1,2,3-Benzodithiazolium chloride12 is readily reduced to 1· with Ph3Sb in toluene at 20 °C. The EPR spectrum is identical to that of the radical arising from the thermolysis of 1. the optimised parameters: B is the concentration of radicals at t = •, k is the reaction rate constant).The results are summarized in Table 2. The activation energy Ea = 76.2 kJ mol–1 and the pre-exponential factor k0 = 4.34×105 s–1 were calculated from the equation ln k = ln k0 – Ea/RT (Figure 4). Thus, a novel promising approach to the synthesis of thermally stable 1,2,3-benzodithiazolyl radicals was developed. This method provides the basis for further in-depth studies of these interesting species including their individual isolation and structural characterization.a3H (Me). b3H (OMe). cInterchangeable values. Table 1 HFI constants (in parentheses, theoretical values), G, and g-factors of radicals 1·–6·. N R1 R2 R3 R4 g 1· 8.22 (8.1) 2.93 (–2.5) 0.97 (1.2) 3.73 (–2.9) 0.81 (1.2) 2.0080 2· 8.38 (8.2) 2.94 (–2.4) 1.03 (1.1) 3.97a (3.2) 0.75 (1.3) 2.0076 3· 8.67 (8.4) 2.93 (–2.3) 1.08 (0.9) 0.44b (0.7) 0.47 (1.2) 2.0076 4· 8.15 (8.1) 5.67 (7.3) 3.52 (–3.6) 9.96 (10.2) 2.56 (–4.1) 2.0078 5· 8.55 (8.3) 3.15 (–2.6) 1.06 (1.0) 8.55 (9.6) 0.71 (1.3) 2.0079 6· 7.88 (7.7) 2.44c (–2.3) 2.65c (–3.3) 3.87 (–3.0) 0.92 (1.2) 2.0081 aB is the concentration of 1 at t = •, and N is the initial concentration of 1.b±15%.Table 2 Rate constant k of thermolysis of 1 at different temperatures.a T/°C k/s–1 B/Nb 110 1.55×10–5 0.95 125 5.80×10–5 0.92 145 1.42×10–4 0.95 150 1.83×10–4 0.80 10 G 4· 5· 6· Experiment Simulation Figure 2 Experimental (in squalane) and simulated EPR spectra of 4·–6·. Note minor extra lines of an unidentified radical in the spectrum of 5·. Differences in the HF line widths were ignored in simulating the spectra.Conversion t/min 1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 0 100 200 300 400 500 600 700 Figure 3 The kinetic build-up curve of 1· by thermolysis of 1 in squalane at 125 °C (initial concentration of 1 was equal to 10–3 mol dm–3).Mendeleev Communications Electronic Version, Issue 1, 2000 (pp. 1–42) This work was supported in part by the Russian Foundation for Basic Research (grant no. 99-03-33115) and by the Leading Scientific Schools Programme (grant no. 96-15-97564). References 1 A. W. Cordes, M. Hojo, H. Koenig, M. C. Noble, R. T. Oakley and W. T. Pennington, I norg. Chem., 1986, 25, 1137. 2 A. V. Zibarev, Yu. V. Gatilov and A. O.Miller, Polyhedron, 1992, 11, 1137. 3 I. Yu. Bagryanskaya, Yu. V. Gatilov, A. Yu. Makarov, A.M. Maksimov, A. O. Miller, M. M. Shakirov and A. V. Zibarev, Heteroatom Chem., 1999, 10, 113. 4 V. I. Minkin, B. Ya. Simkin and M. N. Glukhovzev, Aromaticity and Antiaromaticity. Electronic and Structural Aspects, Wiley–Interscience, New York, 1994. 5 A. P. Hitchcock, R. S. DeWitte, J.M. van Esbroek, P. Aebi, C. L. French, R. T. Oakley and N. P. C. Westwood, J. Electron Spectrosc.Relat. Phenom., 1991, 57, 165. 6 N. E. Petrachenko, Yu. V. Gatilov and A. V. Zibarev, J. Electron Spectrosc. Relat. Phenom., 1994, 67, 489. 7 A. V. Zibarev, Yu. V. Gatilov, I. Yu. Bagryanskaya, A. M. Maksimov and A. O. Miller, J. Chem. Soc., Chem. Commun., 1993, 298. 8 R. Mayer, S. Bleisch, G. Domschke, A. Tkac, A. Stasko and A. Bartl, Org. Magn. Reson., 1979, 12, 532. 9 S.Bleisch, G. Domschke and R. Mayer, GDR Patent 138 062DI, 1979 (Chem. Abstr., 1980, 92, 128892). 10 R. Mayer, S. Bleisch, G. Domschke and A. Bartl, Z. Chem., 1981, 21, 146. 11 R. Mayer, G. Domschke, S. Bleisch, J. Fabian, A. Bartl and A. Stasko, Collect. Czech. Chem. Commun., 1984, 49, 684. 12 G. Kirsch, in Methoden der Organische Chemie (Houben-Weyl), ed. E. Schaumann, Thieme, Stuttgart, 1994, vol. E8d, pp. 3–12. 13 M. J. Frisch, G.W. Trucks, H. B. Schlegel, P. M.W. Gill, B. G. Johnson, M. A. Robb, J. R. Cheeseman, T. Keith, G. A. Petersson, J. A. Montgomery, K. Raghavachari, M. A. Al-Latam, V. G. Zakrzewski, J. V. Ortiz, J. B. Foresman, J. Cioslowski, B. B. Stefanov, A. Nanayakkara, M. Challacombe, C. Y. Peng, P. Y. Ayala, W. Chen, M.W.Wong, J. L. Andres, E. S. Replogle, R. Gomperts, R. L. Martin, D. J. Fox, J. S. Binkley, D. J. Defrees, J. Baker, J. P. Stewart, M. Head-Gordon, C. Gonzales and J. A. Pople, Gaussian 94™. Revision C.3, Gaussian Inc., Pittsburg PA, 1995. ln k T–1/10–3 K–1 –8.5 –9.0 –9.5 –10.0 –10.5 –11.0 –11.5 2.30 2.35 2.40 2.45 2.50 2.55 2.60 2.65 Figure 4 Arrhenius plot of the formation rate constant of 1· in squalane. Received: 17th August 1999; Com. 99/1526

 



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