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Capturing CO2 from ambient air - David Keith

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The prototype has three particle filters. Process <strong>air</strong> leaves the main body of the prototype through four<br />

4x8 in rectangular openings in the top of the donut, spaced evenly around the perimeter. The primary<br />

particle trap is housed in each opening. Most of the volume of entrained liquid is caught here and drips<br />

down to the cone to join the bulk of the return flow. This filter is considered analogous in function to the<br />

particle trap that would be required in a full-scale system.<br />

Past the primary particle trap, <strong>air</strong> enters 8 in diameter flexible ducts attached to each opening and<br />

then a custom-built filter box. The filter box houses two additional filters for safety reasons. The first<br />

is a standard fabric home furnace filter which acts as an inexpensive pre-filter. The second is a microglass<br />

media, mini-pleat duct filter rated for > 95% removal of PM2.5 (Filter Group catalog # 40102). Air<br />

leaving the filter box travels through a p<strong>air</strong> of ducts to the blower, which vents to the room. Considering<br />

the efficiencies of the particle traps and a conservative estimate for the concentration of entrained fine<br />

particles, <strong>air</strong> leaving the blower should have caustic particle content well below (by perhaps an order of<br />

magnitude) OSHA standards.<br />

B.1.4 Liquid handling<br />

The design goal of the liquid system provides the necessary flowrate of NaOH solution to the nozzle at<br />

sufficient and adjustable pressure, allowing measurement of the flowrate and pressure at the nozzle. Also,<br />

since <strong>CO2</strong> absorption by the portion of fluid hitting the walls of the reaction chamber is not counted in<br />

most calculations, the flow on the walls should be measurable so that it can be subtracted out.<br />

A schematic of the liquid system is shown in Figure B.6. For most trials, the liquid handling system<br />

was arranged as shown in a simple loop with a reservoir at the bottom, so that the working solution is<br />

recirculated. Reservoir residence times were 3–15 minutes. Most of the system is comprised of 3/8 in<br />

nylon tubing with stainless steel Swagelok valves and fittings. Additional branches of the system (not<br />

shown) allowed for in-line sample collection, rinsing, and solution transfer between reservoirs.<br />

A pump was required to provide up to 6 L/min of flow at a total head of up to about 650 kPa (lifting<br />

6 m, a target maximum nozzle pressure of 550 kPa, and frictional losses). A centrifugal pump was first<br />

tried. Though it was rated for far higher flows, it could not reach pressures at the nozzle above 300 kPa.<br />

A rotary-vane pump was then used and achieved higher pressures. However, pump performance was not<br />

consistent, and with the high-flow nozzle, the highest pressure reliably achieved was 380 kPa. This limited<br />

the range of pressures tested on the high-flow nozzle, although the pump was rated for more than 800 kPa.<br />

Air entrained in solution seemed to cause vibration and reduced performance. Measures such as arranging<br />

the return flow line to minimize splashing in the reservoir improved this.<br />

Eight different nozzles were tested for use in the prototype. Nozzles were visually observed spraying<br />

water <strong>from</strong> a height of 3 m, and seven of the eight were also characterized with a Malvern laser diffraction<br />

spray analyzer. The two with the smallest mean drop size were selected for use in experiments. Both<br />

nozzles have full-cone spray patterns.<br />

77

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