KINETICS OF HEAT-INDUCED AND PHOTOCHEMICAL TRANSFORMATIONS
phenoxazines (products of heat-induced transforma-
645
tion). Disregarding the entropy factor, the energy
difference should result in the equilibrium constant of
E-quinonimine transformation into phenoxazines of
102–104 at room temperature; that was consistent with
the experimental findings. The reverse process is
possible only upon external energy supply (for
instance, under irradiation). Noteworthily, the energy
difference between tert-butyl derivative IV and the
corresponding phenoxazine was lower than in the
cases of I–III.
EXPERIMENTAL
Quinonimines I–IV were prepared as described in
[1, 4], and their structures were confirmed by IR and
NMR spectroscopy. The solvents of chemically pure
grade were purified and dried as described in [5]. Air
was removed from the reaction mixtures by repeated
freezing under a reduced pressure.
t, min
Fig. 4. Photolytic transformation of 4aН-phenoxazine
derivative B of compound I (с0 = 2.3 × 10–4 mol/L, λ =
405 nm, I0,sp = 1.23 × 1018 quant s–1 L–1; (1) is decay of the
starting compound, (2) is accumulation of quinonimine I.
Heat- and light-induced transformations were
studied in evacuated ampules equipped with Teflon
valves and quartz windows. Photolysis was performed
using the DRSh-500 mercury lamp equipped with
quartz lens and standard set of optical filters. Intensity
of the incident radiation was measured with the
actinometer based on potassium ferrioxalate [6].
Kinetics of the process was monitored by spectro-
photometry (the SF-2000 spectrophotometer, quartz
cell, optical path of 0.8 cm).
positions of the phenyl ring (two tert-butyl, two
isopropyl, two ethyl, or two methyl) as well as of their
4аН-phenoxazine derivatives were optimized by the
DFT method. Hybrid B3PW91 functional in the 6-31G
(d) basis set was used, accounting for d-polarization
functions. All simulations were performed for isolated
molecules.
Output files of GAUSSIAN package contained
electron energy of the molecules in Hartree units; that
information was used to compute energy difference
between Z- and E-isomers of quinonimines and their
4аН-phenoxazines in kJ/mol.
IR spectra of the products were registered with a
Shimadzu IRPrestige-21 instrument (KBr). The
specimens were prepared by washing the purified and
dry salt with the reaction mixture based on hexane,
followed by the solvent distillation under reduced
pressure and the cell filling with inert gas.
Table 2. Energy of ground states of quinonimines I–IV (E-
and Z-isomers) and of products of their heat-induced
transformations
Chromatomass spectrometry analysis was per-
formed using a DSQ II instrument equipped with
quadrupole mass analyzer and the MALDI Bruker
microflex LT spectrometer (ion source temperature
230°С, ionization energy 70 eV). Mass spectra of
cations were registered at the mass number range of
70–800.
Compound
I
II
III
IV
Energy difference between Z- 5.683 6.313 6.532 9.308
and E-isomers, kJ/mol [E(Z) >
E(E)]
Quantum-chemical simulation of ground state of
the quinonimines and their 4аН-phenoxazine deriva-
tives was performed using GAUSSIAN 09W software
package [7]. Starting geometry was set and the results
were presented in GaussView software [8]. The preset
geometry parameters of 4Z- and 4E-isomers of
quinonimines bearing various substituents in 2,6 or 2,5
Energy difference between the 20.78827.33625.48712.866
Z-isomer and the phenoxazine,
kJ/mol
Energy difference between the 15.10421.02318.955 3.558
E-isomer and the phenoxazine,
kJ/mol
RUSSIAN JOURNAL OF GENERAL CHEMISTRY Vol. 84 No. 4 2014