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ionic liquids were used in their work, the heating rate would
probably be more readily affected by changes in the applied
microwave power. If the reaction temperature in their high
power experiment was attained faster, this would explain the
higher yield/conversion. Another study of HCl-catalyzed fruc-
tose dehydration to 5-HMF under microwave irradiation
showed that the 5-HMF yield and fructose conversion were in-
[10]
dependent of the applied microwave power (100–300 W). In
the present study, it is shown that furfural yield and xylose
conversion are independent of the applied microwave power,
provided that enough microwave power is supplied to sustain
the reaction temperature.
Figure 5. Cumulative forward microwave power supplied in glass and SiC re-
actor vials. The use of the SiC vial (simulated conventional heating) results in
significantly higher power input compared to the glass vial (microwave heat-
ing) for the xylose dehydration reaction.
Comparison of energy consumption
We have shown that the two heating modes result in the
same xylose conversion and furfural yield if the rest of the pro-
cess conditions are kept the same. However, a critical evalua-
tion of the process also requires an assessment of the energy
consumption of the two heating modes. However, such precise
assessment is difficult as it has been shown that the total heat
generation in microwave cavities employing resonant micro-
wave fields is very sensitive to even slight variations in the
geometric aspects of the load and the process conditions and
can also deviate significantly from the power readings provid-
the total power supplied during the entire course of the reac-
tion was 30% higher. The reflected microwave power is un-
known and can be different in the two modes of heating.
However, the difference in the supplied power can be ex-
plained by the differences in the properties of the materials.
The microwave-transparent borosilicate glass vial, which is
used in the case of volumetric microwave heating, has a signifi-
cantly lower density than the highly conductive SiC vial
[
22]
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ed by these instruments. In addition, the microwave power
generated in such cavities is not exclusively dissipated in the
load, but also in other locations of the microwave circuit (e.g.,
the magnetron) leading to significant energy losses. Detailed
energy balances in small scale microwave reactors, also ac-
counting for energy losses, have shown that the power ab-
(2.23 gmL versus 3.1 gmL , respectively) that is used to sim-
ulate conductive heating at similar heating rates as in micro-
wave heating. Consequently, more energy is required to reach
and maintain the same reaction temperature during conduc-
tive heating owing to the higher mass of the SiC vial. The ther-
mophysical properties of SiC and borosilicate glass are present-
ed in Table S1.
[
23]
sorbed by the load can be as low as 44%. An accurate esti-
mation of the total heat generation in the load requires tailor-
made microwave applicators, such as the ones used in
Refs. [24,25], in which the electromagnetic field is well defined
and the reflected power can be accurately estimated (and
minimized), for instance, by including power transfer sensors
in different parts of the system. Commercial microwave heat-
ing devices for laboratory applications do not provide such ca-
pability.
Conclusions
In this work, the dehydration of xylose to furfural using micro-
wave heating in the presence of NaCl at concentrations close
to that of seawater concentrations was studied and compared
with conventional heating. The highest furfural yield of 76%
was obtained using 3.5 wt% NaCl at 2008C, which led to com-
plete xylose conversion in 440 s. The existence of nonthermal
microwave effects was investigated in three ways: a) compari-
son of microwave heating experiments with literature results
from conventional heating experiments; b) direct comparison
of microwave and conventional heating in the same mono-
mode cavity using strongly microwave absorbing SiC vials to
simulate conventional heating; and c) comparison between ex-
periments at different microwave power levels at the same re-
action mixture temperature. The results indicate that micro-
wave heating does not have a prominent effect on the dehy-
dration reaction kinetics under the examined conditions. How-
ever, microwave heating eliminates the need for long preheat-
ing times and can thus reduce the uncertainty of kinetic
measurements in cases of slow conductive heating during the
initial stage of the experiments. Furthermore, at a laboratory
scale, the forward-emitted microwave power was 30% higher
in the case of the denser SiC vials owing to heating of a larger
The cumulative forward-emitted microwave power supplied
to a typical glass vial (microwave heating) and SiC vial (simulat-
ed conventional heating) during the preheating and the reac-
tion time was recorded, as presented in Figure 5. At the initial
stages of the experiment, high power is supplied to quickly
reach the reaction temperature of 1708C. In turn, the power is
reduced to hold the temperature constant, balancing the ther-
mal losses to the surroundings and the reaction heat. The
same power control system was used to regulate the tempera-
ture using both vials and it is based on a proportional-integral-
derivative (PID) controller built-in to the device. This system is
designed to reach the reaction temperature as fast as possible,
but also to prevent overshooting the temperature, and it leads
to the same heating rate in both vials under the conditions ex-
amined here. However, in the case of the SiC vial, the power
required to reach the set reaction temperature (preheating
period) was 43% higher compared to the glass vial, whereas
ChemSusChem 2016, 9, 1 – 9
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