Heterogeneously Catalyzed Oxidation Reactions Using ... - CHEC
Heterogeneously Catalyzed Oxidation Reactions Using ... - CHEC
Heterogeneously Catalyzed Oxidation Reactions Using ... - CHEC
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
CHAPTER 6<br />
6.2.4 Catalyst characterization after reaction<br />
Powder X‐ray diffraction patterns were recorded on a Siemens D5000 diffractometer equipped with<br />
a Ni filter using Cu Kα‐radiation. Measurements were performed in the 2Θ range from 5 to 55° with a<br />
step size of 0.01° and a step time of 2 s. Scanning Electron Microscopy (SEM) was measured with a<br />
Gemini 1530 (Zeiss) instrument.<br />
6.2.5 Flame atomic absorption spectroscopy (F-AAS)<br />
For leaching experiments, 15 mL of the reaction solution were concentrated and the remaining solid<br />
transferred into a crucible and treated at 700 °C in air for 4 h. The remainder was dissolved in aqua<br />
regia and diluted to 10.0 mL with distilled water. The Co concentration was measured on a Varian<br />
SpectrAA 220FS equipped with a cobalt SpectrAA lamp (Varian; λ = 240.7 nm). Concentrations were<br />
determined vs. standard solutions prepared from cobalt metal dissolved in HNO3.<br />
6.2.6 X-ray absorption spectroscopy (XAS)<br />
Ex situ samples were measured at the ANKA XAS beamline at the ANKA synchrotron facility at the<br />
Karlsruhe Institute of Technology (Karlsruhe, Germany). The synchrotron ring was operated at 2.5<br />
GeV and a typical ring current of 85‐180 mA. Measurements were conducted in transmission mode<br />
at the Co K‐edge around 7.7 keV with a Si(111) double monochromator in step scanning mode. The<br />
beam intensity was measured by means of three ionization chambers placed before and after the<br />
sample as well as after the reference (Co foil). In situ experiments were conducted at the X1<br />
beamline at the Hamburger Synchrotronstrahlungslabor (HASYLAB) at the Deutsche Elektronen‐<br />
Synchrotron (DESY, Hamburg, Germany). XAS spectra were recorded in transmission mode at the Co<br />
K‐edge around 7.7 keV with a Si(111) double monochromator in step scanning mode in a specially<br />
designed spectroscopic liquid phase cell applicable up to 200 bar [39, 40]. The beam intensity was<br />
measured with ion chambers before and after the sample. Co foil for referencing was measured<br />
extra. Prior to the experiment a thin catalyst pellet (30 mg) was pressed and adjusted to the X‐ray<br />
path. DMF (3 mL) and (E)‐stilbene (20 mg) were added, the cell was closed, pressurized with oxygen<br />
(2 bar) and heated to 100 °C. XANES spectra were processed by energy calibration, deglitching where<br />
necessary, background subtraction, and normalization using the WinXAS 3.1 software [41]. EXAFS<br />
spectra were extracted from the XAS spectra after analogous treatment and Fourier‐transformation<br />
and fitted in R‐space. Phase shifts were calculated with the FEFF 7.0 code [42].<br />
6.2.7 Electron paramagnetic resonance (EPR)<br />
The spectrometer used was an X‐band Bruker EMX continuous wave instrument equipped with a TM<br />
type cavity. The microwave power applied was 20 mW. The sample temperature in the cavity was<br />
controlled with a Eurotherm liquid nitrogen evaporator and heater. In situ experiments were carried<br />
156