suPRAMOlECulAR CHEMIsTRy
333
Analysis 2000 software (version 4.5A). The tetraldehyde
cavitand was accurately weighed into crimped aluminium
pans and subjected to a thermal scan from room temper-
ature to 600 °C at a heating rate of 10.0 °C/min.
Acknowledgements
We gratefully acknowledge financial support by the DsT-Na-
tional Research Foundation, Centre of Excellence in Catalysis,
c*change. Dr Hitesh M. Parekh is thankful the university of Kwa-
Zulu-Natal for postdoctoral fellowship. Dr Pramod B. Pansuriya
would like to thank the DsT-National Research Foundation,
Centre of Excellence in Catalysis, c*change for a postdoctoral
fellowship.
4.3. Data collection and refinement
single-crystal X-ray diffraction data were collected on a
Bruker KAPPA APEX II DuO diffractometer using graph-
ite-monochromated Mo-Kα radiation (λ = 0.71073 Å).
Data collection was carried out at 173(2) K. Temperature
was controlled by an Oxford Cryostream cooling system
(Oxford Cryostat). Cell refinement and data reduction
were performed using the program sAINT (11). The data
were scaled and absorption correction performed using
sADABs (11). The structure was solved by direct methods
using sHElXs-97 and refined by full-matrix least-squares
methods based on F2 using sHElXl-97 (12). The program
Olex2 was used to prepare molecular graphic images (13).
All hydrogen atoms, except those of the solvent molecules
(acetonitrile and methanol), were placed in idealised posi-
tions and refined in riding models with uiso assigned the
values to be 1.2 or 1.5 times those of their parent atoms
and the constraint distances of C–H ranging from 0.95 to
1.00 Å. The hydrogen atoms of the solvent molecules are
excluded from the structure model, due to the fact that the
solvent molecules are situated on special positions with
four fold symmetry. The anisotropic displacement param-
eters (ADP) of most atoms were restrained. The atoms C7A,
C7B, C8, O4, O5, C9 to C15 were all refined with site occu-
pancy factors of 0.50. C7A and C7B were constrained at the
same position with the same ADP. There is a solvent acces-
sible void of 148 Å3 per unit cell, which could not be mod-
elled as discrete atomic sites, probably due to disorder. The
program PlATON sQuEEZE was employed to calculate the
contribution to the diffraction from the missing solvent
molecules and it produced a set of partial-solvent-free dif-
fraction intensities (9). This set of intensities was used for
final refinements. sQuEEZE estimated a total count of 86
electrons per unit cell contributed by the missing solvents,
which were excluded in the formula and subsequent cal-
culation of molecular weight, density etc. (9).
Disclosure statement
No potential conflict of interest was reported by the authors.
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1H NMR, 13C NMR and COsy spectra are given in the sup-
contains the supplementary crystallographic data for this
article. These data can be obtained free of charge from the
Cambridge Crystallographic Data Center, 12 union Road,