156
W. Huang et al. / Journal of Molecular Structure 885 (2008) 154–160
Table 1
2.5. X-ray data collection and solution
Summary of crystal data, experimental details and refinement results for 1
and 3
Single-crystal samples of 1 and 3 were glue-covered and
mounted on glass fibers and then used for data collection
using graphite mono-chromated MoKa radiation
Compound
1
3
Empirical formula
Formula weight
Crystal system
Space group
Unit cell dimensions
C31H47NO2
465.70
Monoclinic
P21/c
C27H34NClO3
456.00
Orthorhombic
Fdd2
˚
(k = 0.71073 A). Crystallographic data of 1 were collected
at 291(2) K on a Bruker SMART 1 K CCD diffractometer,
while those of 3 were collected at 100(2) K on a Rigaku
Mercury CCD area-detector, using graphite mono-chro-
˚
˚
11.0245(13) A
25.878(5) A
˚
˚
18.770(2) A
46.488(9) A
˚
˚
˚
28.840(4) A
8.485(2) A
mated MoKa radiation (k = 0.71073 A). In the case of
b = 97.247(3)°
5920.3(12)
8
1.045
0.064
b = 90°
10208(4)
16
1.187
0.177
Rigaku system, the original data files generated by CRYS-
TALCLEAR [14] were transformed to SHELXTL97 for-
mat by TEXSAN program [15].
3
˚
V/A
Z
D/g cmꢀ3
Absorption coefficient/mmꢀ1
Crystal size [mm]
Temperature [K]
h Range for data collection
Index ranges
The crystal systems of 1 and 3 were determined by laue
symmetry and the space groups were assigned on the basis
of systematic absences using XPREP. Absorption correc-
tions were performed to all data and the structures were
solved by direct methods and refined by full-matrix least-
squares method on F 2obs by using the SHELXTL-PC soft-
ware package [16]. All non-H atoms were anisotropically
refined and all hydrogen atoms were inserted in the calcu-
lated positions assigned fixed isotropic thermal parameters
and allowed to ride on their respective parent atoms. As for
the crystal data of 3, it was difficult to grow good single
crystals especially for smaller ones (samples in large size
and high Rint values were found) and the room temperature
data were not good enough although we have tried many
times. That is why we collected the low temperature data
for 3 at 100 K. Only several ‘‘C alerts” were reported at this
time when checked by Platon, which indicated that the
structure mode of 3 was reliable. The summary of the crys-
tal data, experimental details and refinement results for 1
and 3 is listed in Table 1.
0.20 ꢂ 0.30 ꢂ 0.40 0.20 ꢂ 0.30 ꢂ 0.40
291(2)
100(2)
1.79–26.00
ꢀ13 6 h 6 8
ꢀ22 6 k 6 23
ꢀ35 6 l 6 34
31,324
3.06–25.00
ꢀ30 6 h 6 30
ꢀ49 6 k 6 54
ꢀ10 6 l 6 8
21,282
No. of reflections collected
No. of independent reflections/ 11,639/637
parameters
4334/298
Absorption correction
Observed data [I > 2r(I)]
Goodness-of-fit on F2
F (000)
Multi-scan
8041
1.187
Multi-scan
4076
1.160
2048
3904
Flack parameter
–
0.01(11)
Final R indices [I > 2r(I)]
R1 = 0.0553
wR2 = 0.1452
R1 = 0.0812
wR1 = 0.1503
0.152/ꢀ0.149
R1 = 0.0748
wR2 = 0.1774
R1 = 0.0793
wR1 = 0.1799
0.383/ꢀ0.300
R indices (all data)
Largest diff. peak and hole
ꢀ3
˚
(e A
)
R1 = RkFo| ꢀ |Fck/R|Fo|, wR2 = [R[w(Fo2 ꢀ Fc2)2]/Rw(Fo2)2]1/2
.
3. Results and discussion
and the PhACH2AN@CH2 intermediate (isomerising to
PhACH@NACH3) is formed. At the next reversible step,
one aldehyde group from another 3,5-di-tert-butyl-2-
hydroxybenzaldehyde molecule is added to the imine nitro-
gen atom forming intermediate a, and finally the six-mem-
bered ring contraction occurs and N,O-benzoheterocycle 1
is formed. Because of the strong spatial crowding effects of
two bulky tert-butyl groups, the reaction stops here and 1
is the main by-product in a yield of ꢁ35%. By contrast, for
the starting materials of 2-tert-butyl-4-methylphenol, the
main by-product is also the six-membered N,O-benzohet-
erocycle 2. But the yield is very low (<15%) and it is hard
to isolate from the mixture. As for 2,4-dimethylphenol, the
yielded 3,5-dimethyl-2-hydroxybenzaldehyde can form
intermediate a first, nevertheless it can further react with
another 2,4-dimethylphenol molecule to form 3 in a yield
of ꢁ40%, overwhelming the formation of N,O-benzohet-
erocycle. On considering the ESI-MS peak corresponding
to 1,3-benzoxazine motif is not observed in the case of
compound 3, which is due to the low steric hindrance of
two phenyl-substituted methyl groups. One can conclude
that the steric effects are vital in the formylation reaction
of 2,4-dialkylphenol in forming different by-products.
3.1. Synthesis and spectral characterizations
The structures of 1 and 3 are confirmed by the combina-
tion of the results of EA (ratio of C, H, N), FT-IR, H
1
NMR and ESI-MS (M+1 peak). In our experiments, we
applied Larrow’s method [13] to synthesize 3,5-dialkyl-2-
hydroxybenzaldehydes (dialkyl = t-Bu/t-Bu, t-Bu/Me and
Me/Me), and it is found that the resulting 3,5-dialkyl-2-
hydroxybenzaldehydes can further react with HMT to dif-
ferent extent. In the case of starting material 2,4-di-tert-
butylphenol, 3,5-di-tert-butyl-2-hydroxybenzaldehyde is
the main product whose structure has been reported previ-
ously in our group [17]. However, some of produced 3,5-di-
tert-butyl-2-hydroxybenzaldehyde molecules can further
react with HMT under our experimental condition. The
proposed mechanism for the formation of compound 1 is
shown in Scheme 2. HMT molecule can be decomposed
into CH3ANH2 first by losing NH3 molecule under the
acidic condition, and then CH3ANH2 is added to the
C@O group of 3,5-di-tert-butyl-2-hydroxybenzaldehyde.
Finally, one water molecule is removed by b-elimination