The elemental analysis of the samples was performed on a CHN-3 analyzer. The IR spectra were measured on a
Spectrum BX II IR Fourier spectrometer (Perkin Elmer lnc.). The samples were deposited between KBr glasses.
1
The Н NMR spectra were recorded on a Вruker AVANCE spectrometer with the working frequency of 400 MHz.
The 90°-pulse was 0.5 µs. The relaxation delay was 10 s. The number of scans was 16 or 32. Dimethylsulfoxide-d was used
6
as a solvent.
1
The following compounds were identified. Compound II: T . 223°С; Н NMR: δ, ppm: 7.41-7.55 (12Н, arom.
m
1
protons); found, %: С 55.46, Н 2.57, and N 9.30. Calculated, %: С 55.59, Н 2.56, and N 8.95. Compound IV: T 132°С; Н
m
NMR: δ, ppm: 1.17 m (2Н, СН ), 1.45 m (2Н, СН ), 1.56 m (2Н, СН ), 2.53 m (2Н, СН С(О)), 3.08 dd (1Н, СН ), 3.27 m
2 2 2 2 2
(2Н, NСН ), 3.38 dd (1Н, СН ), 6.52 dd (1Н, СН), 7.1-7.4 m (4Н, arom. protons); found, %: С 61.45, Н 5.83, and N 9.74.
2 2
Calcualted, %: С 61.54, Н 5.81, and N 9.57.
The HPLC-MS analysis was performed on an Agilent 6210 TOF mass spectrometer (dopant KI). Ionization was
performed in the positive mode. The analysis conditions were as follows: the gas flow delivery rate 5 ml/min; temperature
150°C; time of analysis of 100 s to 3200 s; and solvent МеОН+Н О.
2
The GC-MS analysis was performed on a DFS spectrometer (Thermo Fisher Electron Corporation). The
chromatography conditions were as follows: the injector temperature 280°C; flow rate 1 ml/min; split flow 1:20; helium
carrier gas; DB-MS capillary column. The initial temperature of the oven was 120°C; the heating rate was 10 deg/min. The
final temperature of the oven was 280°C. The conditions of mass spectra measurements: electron ionization; ionizing voltage
+
70 V; mass range 50-500 Da. The electron ionization mass spectra of the single crystals of IV, m/z (I , %): М 292 (18), 266
rel.
(2), 153 (11), and 140 (100).
–3
Single crystals of the product of the interaction between compounds III and I at 2.71⋅10 mol/l of triethylamine
were obtained from an acetone solution of the compound on slow evaporation of the solvent. The single crystal XRD analysis
was performed on an automatic Bruker Smart Apex II diffractometer with a two-dimensional CCD detector. The crystals of
C H ClN O (IV) are triclinic; P-1 space group; at 23°C: а = 8.648(2) Å, b = 9.061(2) Å, c = 10.229(3) Å, α = 75.939(3)°,
15 17
2
2
3 3
β = 68.574(3)°, γ = 89.303(3)°, V = 721.2(3) Å , М = 292.76, d = 1.348 g/cm , Z = 2. The cell parameters and intensities of
x
10 049 reflections, including 3408 independent reflections, 3095 of which had I ≥ 2σ (R = 0.018), were measured at a
int
temperature of 23°C (λМоK , graphite monochromator, λ = 0.71073 Å, ϕ and ω scan mode, 2.21 ≤ θ ≤ 28.48°, index area:
α
–11 ≤ h ≤ 11, –12 ≤ k ≤ 11, –13 ≤ l ≤ 13). Absorption was introduced semiempirically using the SADABS program [2]
–1
(μMoK = 2.68 cm ). The structure was solved by the direct method and refined first in an isotropic and then anisotropic
α
approximation using the SHELXL-97 [3] and WinGX [4] programs. The hydrogen atoms were found from the difference
Fourier maps and refined isotropically. The final divergence factors are R = 0.0362 and R = 0.0951 from 3095 reflections
w
2
with F ≥ 4σ; the GOOF parameter is 1.024; 250 refined parameters. Data collection, unit cell parameters, indexation and
refinement were performed using the APEX2 software [5]. The unit cell parameters, coordinates of the atoms and their
temperature parameters have been deposited with the Cambridge Crystallographic Data Centre (http://www.ccdc.cam.ac.uk)
under no. CCDC 763965. The analysis of the intermolecular interactions and the figures were made using the PLATON
program [6].
The powder diffraction patterns were measured on an automatic Bruker D8 Advance diffractometer equipped with
Vario attachment and Vantec linear PSD. The used CuK radiation (40 kV, 40 mA) was monochromated by a curved
α
Johanson germanium monochromator. The experiments were performed at a temperature of 23°C in the Bragg–Brentano
geometry with a flat-plate sample. The compound was preliminarily pressed and prepared in the form of a thin pellet (2-
4 mm) on a glass plate, then placed into a standard sample holder that was rotated (15 rpm) throughout the data collection.
The diffraction patterns were recorded in the 2θ range of 4° to 70°; step 0.0081°; step time 0.5 s. We obtained several
diffraction patterns for each sample in different experimental modes and different step times. For compound IV, whose
structure was determined by single crystal XRD, we also calculated a theoretical powder diffraction pattern. A comparison of
the latter to the experimental diffraction patterns allowed us to identify the compound.
181