Evaluation Only. Created with Aspose.PDF. Copyright 2002-2021 Aspose Pty Ltd.
1636 J. Phys. Chem. B, Vol. 108, No. 5, 2004
Mitchell et al.
due to DMMP measured for a very long period of time, typically
24-28 h, so that all of the DMMP flows through the infrared
cell. The integrated infrared signal then corresponds to the dose
amount. A straight line fit for a series of integrated intensities
vs dose amounts then formed the response curve for DMMP.
The precision of the measurement is not as good as it is for the
measurement of methanol and DMMP, but it is good enough
to be able to draw important conclusions regarding the
decomposition yields.
and detected using a room-temperature InGaAs detector. The
neat powder samples were placed in capillary tubes for data
collection.
Results
Microreactor Studies. Prior to describing the dosing experi-
ments, it is useful to describe the results from several different
control experiments that were carried out to help evaluate the
results. In the first, a mixture of methanol in helium, 253 ppm
from Matheson Gas, was allowed to flow continuously through
the adsorbent bed at 25 °C. No conversion to dimethyl ether
was observed, although conversion to dimethyl ether can be
observed at 150 °C. Similarly, a mixture of dimethyl ether in
helium, 490 ppm from Matheson Gas, gave no conversion to
methanol at 25 °C. Finally, the DMMP in helium mixture
flowing into an empty reactor did not yield any measurable
decomposition products.
Initially, it was thought that 20-24 h would be more than
sufficient to allow for all of the reaction products to flow from
the adsorbent bed. In studies that we had carried out previously
using the microreactor setup, both methanol and dimethyl ether
were observed to flow from the bed relatively quickly.26,27
However, those experiments were carried out using a continuous
flow of DMMP, and the current experiments using small doses
yield significantly different results as described below.
Variable Dose/Fixed Adsorbent Amount. A series of experi-
ments was carried out on reactive adsorbents that had been
examined in an earlier study.27 These adsorbents were prepared
using incipient wetness impregnation and included 7.5 wt %
Ce and 5.0 wt % Fe co-impregnated on γ-Al2O3, 5.0 wt % Fe
on γ-Al2O3, 7.5 wt % Ce on γ-Al2O3, and γ-Al2O3. The results
for all of these adsorbents were similar and showed an apparent
maximum in product formation of 23-27 µmol of product after
exposure to an 80 µmol or larger dose of DMMP. The products
formed represented a combination of dimethyl ether and
methanol. For dose amounts less than 30 µmol of DMMP, the
only product measured was dimethyl ether. Exposure to a 40-
50 µmol dose of DMMP resulted, for most of the solids, in the
observation of large amounts of methanol and diminishing
amounts of dimethyl ether. These results led us to suspect that
the processes leading to gas-phase products might be more
complex than originally assumed.
A new series of reactive adsorbents was developed that
showed significantly higher decomposition yields per gram of
adsorbent. Our previous work showed that higher dispersions
of CeO2 yielded higher decomposition yields, and the precipita-
tion deposition method used to prepare the new adsorbents in
the current study had been shown by Soria and co-workers to
yield high dispersions of supported cerium oxide.36,37 The most
reactive adsorbent had a composition of approximately 20 wt
% Ce on η-Al2O3 and was used to obtain all of the microreactor
results discussed. Samples with lower amounts of cerium
showed lower decomposition yields as discussed in a later
section. The decomposition product yield of DMMP as a
function of DMMP dose for this adsorbent is shown in Figure
1A and B. These graphs show the amounts of methanol and
dimethyl ether produced as a function of dose amount. The
observation of products begins at somewhat lower doses on this
solid than on those studied earlier, and the new solid is capable
of forming approximately 44% more products than the previous
formulations. These results are tabulated in Table 1.
Experiments using the pure alumina materials were carried
out multiple (more than three) times to evaluate the experimental
setup and data analysis for reproducibility. Typically, an
uncertainty of approximately (2 µmol is found for the deter-
mination of the integrated amount of methanol formed. The
uncertainty found for dimethyl ether is less than that due to the
fact that there are no interfering absorptions for the dimethyl
ether gas-phase infrared absorption bands used for quantitation,
while those of methanol are overlapped somewhat by DMMP
absorptions.
Several different types of dosing experiments were carried
out, and for each the pretreatment was carried out as described
above. In the variable dose/fixed adsorbent experiment, 60 mg
of the adsorbent was exposed to different dose amounts of
DMMP. The dose amounts are formed by exposing the
adsorbent to a flow of DMMP in He for an amount of time
necessary to dose the sample with the predetermined amount
of DMMP. The flow through the DMMP liquid is then stopped,
and pure helium is directed to flow through the microreactor
for the remaining time, at a constant flow rate of 30.0 mL/min.
Typically, the flow of helium is continued for approximately
20 h (a total flow of helium of 36-37 L), compared to a dosing
time of about 7 min for a 10 µmol dose of DMMP.
In the fixed dose/variable adsorbent experiment, several
different amounts of adsorbent were exposed to fixed doses of
DMMP, typically 20 µmol. The dose was again followed by a
20-hour continuous flow of pure helium and monitoring of
products. The incremental dose/single adsorbent experiment was
performed by dosing 60 mg of the adsorbent with successive
10 µmol doses of DMMP. Approximately 20 h were allowed
to elapse between each dose, and infrared spectra were recorded
continuously.
In Situ FT-IR Studies. The infrared diffuse reflectance
studies were carried out in much the same way as described in
an earlier publication.38 The adsorbent to be examined was
sieved and placed in a Harrick Scientific HVC-DR infrared
diffuse reflectance controlled environment cell, the cell was
closed and evacuated using an Alcatel diffusion pump. The
sample was then exposed to a mixture of 20% O2 in helium at
400 °C for approximately 30 min, and subsequently cooled to
room temperature. All of the infrared spectra were collected
using a Harrick Scientific DRA-2 optical accessory. After
collection of a background spectrum, the dilute mixture of
DMMP in helium (1:1000) was allowed to flow through the
cell over the sample. The pressure in the cell during this time
was approximately 500 mTorr. Spectra were measured during
the adsorption process to monitor for DMMP adsorption using
a Nicolet Magna 750 FT-IR and a liquid nitrogen cooled
mercury-cadmium-telluride (MCT) detector. During adsorp-
tion, 250 scans at 8 cm-1 resolution (to minimize collection
time) were co-added to form the spectra shown.
FT-Raman Studies. FT-Raman spectra were obtained using
a Nicolet Raman 950 FT-Raman spectrometer using a laser
power of approximately 250 mW. Raman scattered radiation
was collected using a 180° backscattering collection geometry
The only product observed for the lowest doses of DMMP
onto the solid, 10 and 20 µmol, is dimethyl ether. Figures 2
and 3 show the formation of the products of the DMMP