S. González-Gallardo et al. / Inorganic Chemistry Communications 13 (2010) 543–545
545
was stirred for 24 h and filtered. All volatiles were removed under vacuum to
leave a white residue, which was treated with hexane (10 mL). After filtration
and drying under vacuum, 2 was obtained as a white powder. Yield 0.45 g
(85%); m.p. 220 °C; 1H NMR (300 MHz, C6D6, 25 °C): d = 1.46 (s, 12H, CH3), 2.05
(s, 12H, p–Ar–CH3), 2.17 (s, 12H, o–Ar–CH3), 2.30 (s, 12H, o–Ar–CH3), 4.87
(Al–OH, 1.875(1), 1.886(1) Å; Al–N, 1.977(1), 1.984(1) Å). The dis-
tance between the two aluminum atoms (3a, 2.963(1) Å; 3b,
2.949(2) Å) is smaller than that observed for [{iPrLAl(Cl)(
l-OH)}2]
(3.034(1) Å), all of which are larger than the sum of the covalent
radii (RcovAl, Al = 2.698 Å) [13] with no evidence suggesting any
AlꢂꢂꢂAl interaction.
(s, 2H, c
–CH), 6.76–6.79 ppm (m, 8H, m–Ar–H); 13C NMR (75.58 MHz, CDCl3,
25 °C): d = 17.9 (CH3), 20.9 (p–Ar–CH3), 22.3 (o–Ar–CH3), 96.3 (c–CH), 128.9,
133.6, 134.7, 139.9 (Ar–C), 169.6 ppm (C@N); 19F NMR (282.73 MHz, CDCl3,
25 °C) = –163.9 ppm; 27Al RMN (78.16 MHz, CDCl3, 25 °C): d = 118 ppm
It is noteworthy to mention that due to the experimental diffi-
culty in the syntheses and characterization of fluorinated aluminas,
theoretical methods have been applied to study the nature of their
active sites. In this regard, recent reports have suggested that Al3+
centers with coordination numbers lower than six are present in
b-AlF3 and are assumed to act as strong Lewis acid sites, responsi-
ble for the catalytic activity of the material [14]. Thus, it is reason-
able to suggest that the five-fold coordinated aluminum centers in
3 should exhibit a stronger Lewis acidity than the six-fold coordi-
nated Al3+ sites found in most aluminum hydroxyfluorides.
–1
~
v
(tetracoordinate Al); IR (KBr):
= 1536 cm (s, C@N); IE–EM (70 eV): m/z
(%): 774(37) [M+–H]. Due to its extreme moisture sensitivity elemental
analyses could not be performed on 2.
[6] S.D. Waezsada, F.-Q. Liu, E.F. Murphy, H.W. Roesky, M. Teichert, I. Uson, H.-G.
Schmidt, T. Albers, E. Parisini, M. Noltemeyer, Organometallics 16 (1997) 1260.
[7] Compound 3 can be obtained by two different methods: (a) To a solution of
[{LAl(F)}2(l-O)] (2) (0.45 g, 0.62 mmol) in toluene (5 mL) was added a solution
of H2O (0.62 mmol) in THF (5 mL) at ambient temperature. The reaction
mixture was stirred for 24 h upon which an abundant precipitate was formed.
The slurry was then filtered and the white solid was washed with toluene
(3 mL) and dried under vacuum to give 3 as a microcrystalline white powder
(0.47 g, 96%); (b) [LAl(H)]2(l-O) (1) (0.50 g, 0.68 mmol) and Me3SnF (0.27 g,
0.75 mmol) were weighed together in a Schlenk flask and toluene (20 mL) was
added. The reaction mixture was stirred for 24 h and filtered to remove the
insoluble material. A Schlenk flask containing the filtrate was then connected
through a glass tube to another Schlenk flask containing a solution of H2O
(0.68 mmol) in THF (6 mL). After one week, colorless crystals were obtained
which were filtered and dried under vacuum to give 3 (0.48 g, 80%). M.p. 175–
180 °C (decomp.); 13C MAS RMN (75.58 MHz, 25 °C): d = 20.2 (CH3), 21.2
Conclusions
In this work we have shown the feasibility of obtaining a struc-
turally well-defined aluminum hydroxyfluoride, using a soluble,
molecular fluorinated alumoxane as a starting material under mild
conditions. Further work on the study of the acidic properties of
this material is currently in progress.
(p–Ar–CH3), 23.1 (o–Ar–CH3), 99.9 (c–CH), 130.3, 133.2, 134.5, 146.8 (Ar–C),
169.5 ppm (C@N); 27Al MAS RMN (78.16 MHz, 25 °C): d = 30 ppm
–1
~
v
(pentacoordinate Al); IR (KBr):
= 3677 (m, AlO–H), 1540 cm (s, C@N); IE–
EM (70 eV): m/z (%): 775(10) [M+–OH]; Elemental analysis (%) calc. for
C46H60Al2F2N4O2 (792.95): C 69.7, H 7.6, N 7.1; found: C 69.5; H, 7.5; N, 7.1.
[8] J.J. Delpuech, in: P. Laszlo (Ed.), NMR of Newly Accessible Nuclei, Academic,
New York, 1983, pp. 153–195.
Acknowledgements
[9] (a) Crystal data for 3a: C46H60Al2F2N4O2 (792.94), triclinic, space group P1,
This work was supported by the CONACyT (Grant 058484). We
also thank H. Rios for his technical assistance.
a = 8.274(2) Å, b = 10.289(2) Å, c = 13.542(2) Å;
a
= 71.82(2)°, b = 77.99(2)°,
calcd = 1.251 g cmꢀ3
F(0 0 0) = 424,
. Of the 11,011 measured reflections, 3709 were
c
l
= 76.17(1)°; V = 1052.3(4) Å3, Z = 1,
(MoK
) = 0.121 mmꢀ1
q
,
a
independent (Rint = 0.0420). The final refinements converged at R1 = 0.0457
for I > 2r
(I), wR2 = 0.1192 for all data. The final difference Fourier synthesis
Appendix A. Supplementary material
gave a min/max residual electron density of 0.299/ꢀ0.251 e Å3. (b) Crystal data
for 3b: C46H60Al2F2N4O2ꢂ2CH2Cl2 (962.79), triclinic, space group P1,
CCDC 758533 and 758534 contain the supplementary crystallo-
graphic data for this paper. These data can be obtained free of
charge from The Cambridge Crystallographic Data Centre via
ated with this article can be found, in the online version, at
a = 8.861(2) Å, b = 12.478(2) Å, c = 13.223(2) Å;
a
= 63.92(3)°, b = 71.26(2)°,
F(0 0 0) = 508,
. Of the 12,505 measured reflections, 4502 were
c
l
= 76.16(2)°; V = 1235(1) Å3, Z = 1,
(MoK
) = 0.324 mmꢀ1
q ,
calcd = 1.294 g cmꢀ3
a
independent (Rint = 0.0886). The final refinements converged at R1 = 0.0669
for I > 2r
(I), wR2 = 0.1482 for all data. The final difference Fourier synthesis
gave a min/max residual electron density of 0.297/ꢀ0.269 e Å3. Crystals were
mounted on nylon loops and rapidly placed in a stream of cold nitrogen.
Diffraction data were collected on a Bruker-APEX three-circle diffractometer
using MoKa radiation (k = 0.71073 Å) at 173 K. The structures were solved by
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