measurement was performed with a high precision pH meter,
Radiometer PHM 84 equipped with a Metrohm 6.0234.100
were refined anisotropically, using weighted full-matrix least
squares on F . Hydrogen atoms attached to hydroxyl oxygen
2
21
combination electrode. The electrode was calibrated as pH =
atoms and water ones were located in a difference map and other
hydrogen atoms were placed in calculated positions with isotropic
thermal parameters, and were not refined. All calculations were
+
−
log[H ], therefore the derived constants were stoichiometric
constants. The titrant was added with an automatic burette,
Radiometer ABU 80. The solutions were stirred at constant speed.
The titration of the free ligand was started from pH = 10.5 with
26
performed with the teXsan crystallographic software package of
Molecular Structure Corporation.
−
3
0
.2231 mol dm HCl. The concentration of the K
2
EDBHP stock
CCDC reference number 602726.
For crystallographic data in CIF or other electronic format see
DOI: 10.1039/b517192j
−
3
solution (c = 0.220 mol dm ) and the protonation constants of
the ligand were evaluated using the SUPERQUAD program. The
Al(III)–ligand samples (v
22
3
−3
−3
0
= 20.0 cm , cAl = 5.00 × 10 mol dm ,
c
L
/cAl = 1 and 1.2) at pH = 3–10.5 were titrated with 0.2215 M
Acknowledgements
KOH solution. The required equilibration time after addition of
KOH to achieve constant pH values was less than 10 min in the
ranges of pH < 5.2 and pH > 8, and substantially longer (up to over
We acknowledge OTKA T 038296 and K63388 for the financial
support, and the Tosoh Co. Ltd. for donating the EDBHP ligand.
R. J. is grateful to the Sasaki Foundation for an Environmen-
tal Sciences scholarship. The authors also thank Dr S a´ ndor
K e´ ki and his research group at the Department of Applied
Chemistry, Debrecen University for ESI-MS measurements, Dr
Mikhail Maliarik for valuable discussions and Dr David Lawrence
1
h) in the non-buffered region close to pH = 7. These data values
were not involved in the equilibrium calculations. The protonation
constants of the ligand measured in independent titrations, and
the stability constants of Al(III)–hydroxo species were kept at
fixed values during the refinement of the stability constant for the
23
9
studied Al(III)–EDBHP complexes by the PSEQUAD program
(
Link o¨ ping University) for linguistic correction of this manuscript.
(
See also Table S1 in ESI†). The uncertainties of the constants
were estimated values referring to reproducibility, rather than (the
smaller) uncertainty of the program.
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00/360 MHz H NMR spectra were recorded on a Bruker Avance
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◦
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¨
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−
3
−3
.01 mol dm AlCl
3
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standard.
Electrospray ionisation mass spectrometry
1
0 Model calculations indicate some differences between the two models
+
−
4
] at a narrow pH-range of 8–9, but the
both in [H ] and [Al(OH)
differences are very small and seem to be hardly measurable by
ESI MS measurements were performed using a Bruker BioTOF II
ESI-TOF instrument equipped with a Cole Palmers 74900 Series
pump (sample flow rate 2 ll min ) in the negative ionization
mode at 2000 V corona, 4500 V endplate, 4000 V cylinder, 2000 V
capillary enter and 120 V capillary exit voltage. The temperature
27
potentiometry or Al NMR.
−
1
11 G. Anderegg, Critical Stability Constants of EDTA Complexes, IUPAC
Chemical Data Series No. 14. Pergamon, 1977; A. E. Martell and
R. M. Smith, Critical Stability Constants, Plenum Press, New York,
1
974.
◦
of the N
2
gas used for desolvation was 100 C. The frequency of
12 I. Puigdomenech, in MEDUSA (Windows Interface to the MS-DOS
Version of INPUT, SED and PREDOM Fortran Program Drawing
Chemical Equilibrium Diagrams). Program is available at http://www.
kemi.kth.se/medusa/ or http://web.telia.com/∼u15651596/, 1997.
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L
=
−
3
0
.001 mol dm at pH ∼ 5.5.
1
1
3 J. W. Akitt, Prog. NMR Spectrosc., 1989, 21, 1.
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X-Ray diffraction
The diffraction intensities of a colourless platelet crystal
1
995, 40, 769.
1
1
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of Al (EDBHP) (OH) O) were collected with graphite
2
2
2
·2(H
2
monochromated Mo-K
a
radiation using a Rigaku RAXIS-IV
◦
Imaging Plate diffractometer at 23 C to a maximum 2h value of
◦
17 W. H. Casey, M. M. Olmstead and B. L. Phillips, Inorg. Chem., 2005,
6
5.1 . The data were corrected for Lorentz and polarisation effects.
4
4, 4888.
24
The structure was solved by heavy-atom Patterson methods and
1
8 A. Bodor, I. B a´ nyai, L. Z e´ k a´ ny and I. T o´ th, Coord. Chem. Rev., 2002,
228, 163.
2
5
expanded using Fourier techniques. All non-hydrogen atoms
226 | Dalton Trans., 2006, 3221–3227
3
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