PNNL-13501 - Pacific Northwest National Laboratory
PNNL-13501 - Pacific Northwest National Laboratory
PNNL-13501 - Pacific Northwest National Laboratory
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Figure 2 demonstrates the rapid thermal-swing capability<br />
for an all-metal microscale adsorber in a series of<br />
1-minute cycle heating and cooling curves. (In separate<br />
tests, it was determined that the heat-exchange surfacemeasured<br />
temperatures depicted in the figure are<br />
representative of the zeolite bed temperature to within<br />
1 to 2°C.) As the heat-exchange fluid flow rate was<br />
increased from 20 to 80 mL/min, the maximum and<br />
minimum adsorber temperatures approached the hot<br />
(70°C) and cold (5°C) reservoir temperatures. A larger<br />
temperature differential between adsorption and<br />
desorption cycles increases the zeolite working capacity,<br />
and therefore a higher adsorbent working capacity is<br />
expected as the water flow rate is increased. This was<br />
verified experimentally. Figure 2 also shows that the<br />
approach to the maximum (or minimum) temperatures is<br />
faster with increasing heat-exchange fluid flow rate. The<br />
heating curves were fit to exponential decay functions,<br />
and the exponential time constants were estimated. The<br />
time constants were approximately 6, 9, and 19 seconds<br />
for water flow rates of 80, 40, and 20 mL/min,<br />
respectively. These data validate, from a heat transfer<br />
perspective, the potential for rapid thermal cycling in<br />
microscale adsorbers.<br />
Adsorber Temperature (C)<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
0 20 40 60 80 100 120<br />
Elapsed Time (s)<br />
Heat Xfer Fluid<br />
Flow Rate<br />
(mL/min)<br />
Figure 2. Effect of heat exchange fluid flow rate on<br />
temperature profiles for a metal microscale adsorber in<br />
1-minute adsorption and desorption cycles<br />
Both heat and mass transfer must be effective for rapid<br />
adsorption/desorption cycles to work well. Figures 3 and<br />
4 demonstrate the simultaneous heat and mass transfer<br />
effectiveness for metal, plastic, and metal-plastic<br />
composite microscale adsorbers. Figure 3 shows<br />
measured bed temperatures in an all-metal device for a<br />
series of 0.5-, 1-, 3-, and 5-minute adsorption/desorption<br />
cycles. The figure also shows the volume of gas<br />
measured at the end of each desorption cycle (open<br />
circles). In the tests, water flowed through the heat<br />
exchanger at 80 mL/min, and the hot and cold reservoirs<br />
344 FY 2000 <strong>Laboratory</strong> Directed Research and Development Annual Report<br />
20<br />
40<br />
80<br />
were set to 90° and 5°C, respectively. Pure CO2 was fed<br />
to the zeolite at the rate of 50 mL/min during the cooling<br />
cycles, and the feed stream bypassed the adsorber bed<br />
during desorption cycles (Figure 1). The desorbed CO2<br />
volume consistently reached 46 mL for longer cycle<br />
times, fell slightly (~42 mL) in 1-minute cycles, and<br />
dropped significantly (~22 mL) in 0.5-minute cycles. The<br />
recovered volumes in the faster cycles were limited, at<br />
least in part, because of the lower temperature<br />
differentials attained in the cycles. A primary limitation<br />
for the 0.5-minute cycles was the feed gas flow rate; only<br />
~25 mL CO2 was delivered to the bed during the<br />
adsorption swing. (Tests with higher feed flow rates<br />
resulted in larger recovered gas volumes for 0.5-minute<br />
cycles.) The theoretical working capacities, based on<br />
measured temperature differentials, were ~52 mL for the<br />
3- and 5-minute cycles and ~47 mL for the 1-minute<br />
cycle. Therefore, better than 80% of the theoretical<br />
working capacity was achieved in each of these cycles.<br />
Factors affecting the actual working capacity are<br />
discussed later in this section. Figure 3 also indicates<br />
excellent cycle-to-cycle consistency—for example,<br />
volumes evolved in 3- and 5-minute cycles late in the<br />
sequence were identical to those measured early on.<br />
Adsorber Temperature (C)<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
0 5 10 15 20 25 30 35<br />
Elapsed Time (min)<br />
Figure 3. Temperature profile and desorbed gas volumes<br />
(open circles) for a metal microscale adsorber in a series of<br />
adsorption and desorption cycles<br />
Figure 4 compares the thermal and mass transfer<br />
performance of three different microscale adsorption<br />
devices during desorption cycles. In all cases, water was<br />
delivered to the adsorber heat exchangers from a 90°C<br />
reservoir at 80 mL/min. Figure 4a indicates a somewhat<br />
lower rate of temperature change in the all-plastic device<br />
than in the all-metal and metal-plastic composite devices.<br />
However, after ~70 seconds the temperatures in the allplastic<br />
device match those in the all-metal device, and at<br />
longer times the temperatures in the all-plastic device<br />
50<br />
45<br />
40<br />
35<br />
30<br />
25<br />
20<br />
15<br />
10<br />
5<br />
Gas Volume Desorbed (mL)