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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)

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