Inorganic Chemistry
Article
was metered as described above. The solvent was removed under
reduced pressure, and the complexes were isolated as solid powder.
Absorption and Fluorescence. Absorbance spectra were
recorded on a JASCO V-650 spectrophotometer, emission spectra
were measured on a JASCO FP-8300 spectrofluorometer. The spectra
were recorded at 20 °C with solutions of the different MEPEs and
monotopic complexes all containing a constant ligand concentration of
10−3 M in UV/vis measurements and 10−5 M in fluorescence
spectroscopy measurements.
ASSOCIATED CONTENT
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S
* Supporting Information
The Supporting Information is available free of charge on the
Details on UV−vis absorption spectroscopy, fluorescence
spectroscopy, stopped-flow, and SLS (PDF)
Stopped-Flow. The stopped-flow measurements were performed
using the fluorescent substances (1, 2, and 3) at different
concentrations between 10−5 and 10−4 M ultrasonicated in ethanol
for at least 30 min. The measurements were carried out in ethanol
instead of acetic acid solution (75 vol %) to avoid possible corrosion to
the stopped-flow apparatus. To make sure, that the ligands 1, 2, and 3
are dissolved in EtOH, emission spectra were monitored and the
intensity of the Rayleigh scattering band was checked. A low intensity
of the band indicated, that the ligands were dissolved and that there
were no scattering aggregates present in solution. These dissolved
substances were reacted with different concentrations in the range of 5
× 10−5 to 10−3 M of the respective quenching substances Fe(OAc)2·
4H2O, Co(OAc)2·4H2O, and Ni(OAc)2·4H2O in ethanol. The
coordination kinetics of MEPE and metal complexes were monitored
by fluorescence detection using a BioLogic SFM-300 stopped-flow
module attached to a JASCO J-815 spectropolarimeter with an
addition photomultiplier tube for fluorescence detection. For the
concentration range between 10−5 and 10−4 M a calibration curve was
recorded that relates ligand concentration of 1, 2, and 3 to the
emission signal, which follows a linear relationship. The slope of the
calibration curves correlates the emission signal to the concentration of
the ligand. Ligand 1 was excited at λe = 292 nm, ligand 2 at λe = 289
nm and ligand 3 at λe = 281 nm. Emission intensity between 387 and
447 nm was detected using a cutoff filter supplied by Bio-Logic. The
dead time of these experiments was 3.8 ms. Every stopped-flow mixing
experiment was performed with 151 μL of ligand, dissolved in EtOH
and 151 μL of metal acetate, dissolved in EtOH, each with a flow rate
of 4.00 mL s−1. The temperature was set to 20 °C with a FL 300
Julabo temperature controller. Fluorescence-time traces were moni-
tored using Biokine32 (BioLogic). The concentration of ligand is
related to the emission intensity via a calibration curve. In the
concentration range of 10−5 to 10−4 M we observe a linear relationship
between concentration of ligand and emission signal. Every
concentration/time plot was fitted to the following equation:
AUTHOR INFORMATION
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Corresponding Author
Notes
The authors declare no competing financial interest.
ACKNOWLEDGMENTS
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The authors would like to thank Prof. Dr. Markus Sauer and
Dr. Soren Doose of the Theodor-Boveri Institute (University
̈
Wurzburg, Germany), where the stopped-flow measurements
̈
were performed, and Christian Bauer for his help preparing the
solutions and performing the SLS measurements. Light
scattering experiments were possible through support of the
Deutsche Forschungsgemeinschaft (INST 93/774-1 FUGG).
REFERENCES
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y(t) = αt + β + γe(−δt)
(15)
Slope α and offset β correspond to the baseline, which is subtracted
after fitting. Amplitude γ and exponent δ are parameters of the
exponential term of the graph. After subtracting the baseline, the rate v
of every single exponential curve y(t) = γe(−δt) at the commencement
of the reaction, was determined by calculating the slope of the
exponential curve, and thus the first derivation at t = 0:
y′(0) = −δγ
(16)
v = | − δγ|
(17)
Static Light Scattering (SLS). These measurements were
performed with an ALV CGS-3 Multi Detection Goniometry System
(ALV, Langen, Germany), and eight fiber optical detection units
including eight simultaneously working APD avalanche diodes. The
measurements were conducted at scattering angles from 20° to 140° in
steps of 8°. The samples were thermostated in a cell with temperature
stability of 0.1 °C. All solutions were filtered separately before
measuring light scattering using 0.2 μm syringe filters in order to
remove dust particles. The specific refractive index increment (dn/dc)
of every polymer sample was measured at 20 °C using a differential
refractive index detector BI-DNDC WGE DR Bures from Wyatt
Technologies. For details concerning the theory of SLS, see Chapter 4
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Inorg. Chem. XXXX, XXX, XXX−XXX