E. Kroke et al.
internal coordinates. In these cases, the specific torsion angle was
changed in steps of 58. The geometry of the molecule was completely op-
timised at every step, restricting only the torsion angle to the specified
value. This method allows access to a defined section of the potential
energy surface.
yield products derived from nucleophilic attack of the NH2
groups of melem if suitable reaction conditions are applied.
The AIM analysis[25] of 2 was performed at the B3LYP/6-311+G
ACHTUNGTRENNUNG(d,p)
Experimental Section
level of theory with the geometry taken from the X-ray structure analysis
without further optimisation. The wavefunction files for the AIM analysis
were generated in Cartesian coordinates with a basis set containing 6d
functions. The option SCF=Tight was used to prevent “charge leakage”
as described by Popelier.[43] The electron density topology was analysed
by using AIM2000.[44]
General: All solvents were purified and dried according to general proce-
dures. Commercially available chemicals were of p.a. quality and used as
obtained from the suppliers. IR spectra were recorded in the range 400–
4000 cmꢀ1 at room temperature with a Nicolet 380 FT-IR spectrometer.
The samples (KBr pellets) were prepared under N2 atmosphere. Standard
1H and 13C NMR spectra were recorded on an AVANCE DPX 400 spec-
trometer at 293 K [1H (400 MHz), 13C (101 MHz) NMR]. Chemical shifts
are reported relative to tetramethylsilane. CP/MAS 13C NMR (101 MHz)
studies were performed on a Bruker DSX Avance 400 conventional im-
pulse spectrometer with a rotation of 10 kHz and a ramp of 80%. Ele-
mental analyses were performed with a Vario Micro CHNS analyser.
UV/Vis spectra were recorded with a JASCO V-650 spectrophotometer
at room temperature. Emission spectra were recorded on a JASCO FP-
6500 instrument at room temperature with an excitation wavelength of
416 nm. Calibration curves were determined with the following concen-
trations: 446.6, 361.3, 290.8, 307.7, 177.7, 44.7 and 29.1 mmol using
307.7 mmol as sample. The thermogravimetry measurements were per-
formed with a Seiko SSC 5200 TG/DTA 22 instrument (Seiko Instru-
ments) with a heating rate of 5 Kminꢀ1, argon or air flow rate of
300 mLminꢀ1 and a maximum temperature of 8008C.
Crystal structure determination: Crystals of compound 2·CH3NO2 suita-
ble for X-ray crystallography were obtained from a solution of 2 in nitro-
methane by slow evaporation of the solvent at room temperature. Data
collection of 2·CH3NO2 was performed on a STOE IPDS-2 diffractome-
ter (image plate) equipped with a low-temperature device [T=100(2) K]
with graphite-monochromatised MoKa radiation (l=0.71073 A8) using w
and f scans. Reflections were corrected for background, Lorentzian and
polarisation effects. Preliminary structure models were derived by direct
methods[45] and the structures were refined by full-matrix least-squares
calculations based on F2 for all reflections using SHELXL.[45] All hydro-
gen atoms were included in the models in calculated positions and were
refined as constrained to the bonding atoms. The crystal data and param-
eters pertinent to the data collection and structure refinement of
2·CH3NO2 are summarised in Table 4 and selected bond lengths and
angles are presented in Table 2.
Preparation of melem (1):[11,37] Melem was obtained by following the
published procedure. In brief, melamine (25 g) was heated in a glass tube
to 3858C. At about 2508C, violent gas (ammonia) liberation began,
which continued for about 9 h. The heating at 385–3908C was continued
for 60 h. Thereafter the reaction mass was allowed to cool to room tem-
perature. Pure melem was obtained as a white-to-beige powder. Yield:
CCDC 868710 (for 2·CH3NO2) contains the supplementary crystallo-
graphic data for this paper. These data can be obtained free of charge
ac.uk/data_request/cif.
Table 4. Crystallographic and structure refinement data for 2·CH3NO2.
2·CH3NO2
ꢀ
16.87 g, 95.5%; IR (KBr): n˜ =3490, 3430 (N H), 1620, 1310 (n˜ass hepta-
zine ring), 1480, 805 cmꢀ1 (heptazine ring); elemental analysis calcd (%)
for C6N7ACHTUNGTRENNUNG(NH2)3 (218.08): C 33.03, H 2.77, N 64.20; found: C 31.93, H
2.68, N 63.47%.
chemical formula
formula mass
colour
C30H12N10O6·CH3NO2
669.54
yellow
Preparation of 2,5,8-triphthalimido-tri-s-triazine (2): Under inert condi-
tions, melem (3 g, 13.75 mmol) and phthaloyl dichloride (11.17 g,
55.03 mmol) were heated under reflux in dry 1,2-dichlorobenzene
(200 mL) for 22 h. Suction filtration of the cooled reaction mixture gave
the crude product including phthalic anhydride and unreacted melem.
Stirring in water for 30 min, suction filtration, washing with ethanol and
extensive Soxhlet extraction gave 2 as an intense yellow 1:1 adduct with
nitromethane. Yield: 0.94 g, 10.2%; m.p. >3008C; 1H NMR
([D6]DMSO): d=8.06–7.96 (m, 12H, 5-H, 6-H), 4.41 ppm (s, 3H,
CH3NO2); 13C NMR ([D6]DMSO): d=163.94 (C-3), 163.13 (C-2), 161.46
(C-1), 136.12 (C-6), 131.41 (C-4), 124.68 (C-5), 63.69 ppm (CH3NO2);
13C CP/MAS NMR: d=166.2, 164.1, 161.9, 160.3 (C=O, C6N7), 142.2,
138.1, 135.3, 131.4, 129.7, 127.2, 126.1, 123.4 (phenylene moiety),
63.4 ppm (CH3NO2); IR (KBr): n˜ =3100, 3062, 2963 (CArH), 1804, 1742
(n˜C=O), 1618, 1610 (n˜assheptazine, n˜C=CAr), 1525 (n˜C=CAr), 1470, 1329
crystal system
space group
a [ꢂ]
b [ꢂ]
c [ꢂ]
monoclinic
P21/n
7.4314(3)
25.8162(13)
14.6322(6)
93.177(3)
2802.9(2)
4
b [8]
V [ꢂ3]
Z
F
N
1368
]
1.587
m
G
]
0.120
data collection temperature [K]
q range [8]
h, k, l range
no. of coll./unique refl.
Rint
100(2)
1.58–25.00
ꢀ8/7, ꢁ30, ꢁ17
18972/4934
0.0809
ꢀ ꢀ
(heptazine ring), 1395, 1112 (s, n˜C N C), 828, 812 (heptazine ring),
710 cmꢀ1 (dC=O); UV/Vis (CH3CH2OH): l (e)=271 (2484), 236 (3004),
209 nm (2484 Lmolꢀ1 cmꢀ1); elemental analysis calcd (%) for
C30H12N10O6·CH3NO2 (669.54): C 55.61, H 2.26, N 23.01; found: C 55.35,
H 2.25, N 23.04%.
no. of refl. with [Iꢂ2s(I)]
no. of refined parameters/restraints
R1(F)[a]/wR2(F2) (all data)[b]
S (goodness of fit on F2)[c]
2937
452/0
0.0595/0.1685
1.056
Quantum chemical calculations: Quantum chemical calculations were
carried out by using the Gaussian 09 series of programs.[38] Geometries
were fully optimised by DFT using Beckeꢃs three-parameter hybrid-ex-
change functional and the correlation functional of Lee, Yang and Parr
(B3LYP).[39,40] Geometry optimisations and harmonic frequencies were
final D1max
/
[eꢂꢀ3
]
0.251/ꢀ0.327
min
CCDC number
868710
1
2
2
[a] R1=SjFo jꢀjFc j/SjFo j. [b] wR2=[Sw
G
(Fo )2] =
,
w=[s2-
2
2
2
G
(Fo ,0)+2Fc2]/3. [c] GoF=[Sw-
1
calculated for all elements with the polarised 6-311+GACHTUNTRGNEU(GN d,p) basis set for
2
(Fo ꢀFc2)2/(nobsꢀnparam)] =
2
the different conformations of 2.[41,42] The stationary points were charac-
terised by zero imaginary frequencies.
Relaxed potential energy surface scans of I and II were performed with
the Opt=ModRedundant utility in Gaussian 09 at the B3LYP/6-311+G-
ACHTUNGTRENNUNG(d,p) level of theory. This option includes the specification of redundant
&
6
&
ꢁ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 0000, 00, 0 – 0
ÝÝ
These are not the final page numbers!