For compound 3 a mixture of 1 mmol Sb2VO5, 0.66 mmol
NH4VO3, 0.66 mmol NiCl2·6H2O was treated with an amine–water
solution analogous to compound 1. X-ray powder diffractometry
showed reflections of at least two different compounds. Because
the black crystals grow in chunks a manual separation of the
different compounds was not possible (Fig. 12). For this reason
chemical analyses were not possible, and only the X-ray structure
is reported here.
min-1; Al2O3 crucibles) using a Netzsch STA-409CD instrument.
To determine the water content of 1 several TG measurements were
performed using products of different syntheses. For all products
the weight loss corresponded to 12 H2O molecules per formula
unit.
Acknowledgements
The financial support from the State of Schleswig-Holstein is
grateful acknowledged.
Crystal structure determination
The X-ray intensity data of a single crystal of compound 1
with dimensions 0.0542 ¥ 0.1027 ¥ 0.1476 mm3, of a crystal of
compound 2 with dimensions 0.057 ¥ 0.0728 ¥ 0.1325 mm3 and of
a crystal of 3 with dimensions 0.0395 ¥ 0.0588 ¥ 0.0686 mm3,
were collected at room temperature using a STOE-1 Imaging
Plate Diffraction System (IPDS-1) with Mo-Ka radiation (l =
Notes and references
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˚
0.71073 A). The raw intensities were treated in the usual way
applying Lorentz polarization as well as absorption correction.
Selected crystal data and details of the structure determination
are summarized in Table 1. The structures were solved with direct
methods with SHELXS-97.43 Crystal structure refinements were
done against F2 using SHELXL-97 for 2 and 3.43 For 1 a special
version of SHELXL for the refinement of very large structures
(SHELXH) was used.43 The crystal of 1 was racemically twinned
and therefore a twin refinement was performed (BASF: 0.21 (1)).
The CH and NH hydrogen atoms were positioned with idealized
geometry and refined using a riding model. The H atoms from
water could not be located in difference Fourier maps. Numerical
absorption corrections were performed (for compound 1 Tmin/Tmax
0.3990, 0.7064; for compound 2 Tmin/Tmax 0.3864, 0.5805, and for
compound 3 Tmin/Tmax 0.5243, 0.6284). After structure refinement
of compound 1 there were several residual peaks in the electron
density map indicating the presence of disordered solvent for
which no reasonable structure model could be found. Therefore,
the data were corrected for disordered solvent molecules using the
SQUEEZE option in PLATON.30 During the squeezing procedure
1476 electrons were collected. Calculation of the accessible free
3
˚
space using the program suite PLATON yields 6725.9 A as
potential solvent area for 1.
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Elemental analysis
CHN analyses were done using an EURO EA Elemental Analyzer,
fabricated by EURO VECTOR Instruments and Software. Note
that experimental CHN data for 1 indicate smaller water content
which may be explained by water loss during sample preparation.
IR spectroscopy
24 A. Wutkowski, C. Na¨ther, Ko¨gerler and W. Bensch, Inorg. Chem., 2008,
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using a Genesis FTIRTM spectrometer from ATI Mattson.
The IR spectra were measured from 400 to 4000 cm-1. The
powdered samples were mixed with dry KBr and were pressed
into transparent pills.
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Thermal analysis
29 A. Mu¨ller and J. Do¨ring, Angew. Chem., Int. Ed. Engl., 1988, 27, 1721.
30 A. L. Spek. PLATON, A multipurpose crystallographic tool, Utrecht
University, Utrecht, The Netherlands 2000.
The DTA–TG investigations were carried out in a nitrogen
atmosphere (purity: 5.0; heating rate 4 K min-1; flow rate: 75 mL
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Dalton Trans., 2012, 41, 1338–1344 | 1343
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