Capturing CO2 from ambient air - David Keith
Capturing CO2 from ambient air - David Keith
Capturing CO2 from ambient air - David Keith
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Appendix B<br />
Experimental details and procedure<br />
This section documents many experimental decisions and design details related to the construction and<br />
testing of the prototype contactor. It is meant to allow future interested researchers to reproduce or critique<br />
the techniques.<br />
B.1 Physical apparatus<br />
B.1.1 Basic size and structural design<br />
In setting out to build a prototype contactor based on NaOH drops, the nature of drop generation was<br />
central to determining the overall form. Though there are various means of generating small drops at very<br />
small flow rates (electrostatic augmentation of flow <strong>from</strong> an orifice, sonic disruption of falling streams or<br />
sheets), we reasoned that any full-scale contactor would rely on spray nozzles. To realistically simulate the<br />
conditions in the full-scale system, the prototype would need to accommodate a spray nozzle. Additionally,<br />
since the prototype is meant to simulate the average conditions in a very wide, very tall tower, edge<br />
effects should be minimized. That is, distortions to the rate of mass transfer caused by liquid on the walls,<br />
transient spray characteristics (escape velocity and angle <strong>from</strong> the nozzle), and the collection mechanism<br />
at the bottom should be minimized. Without significant edge effects, the prototype results can more easily<br />
be compared with theory and more justifiably scaled up to a full size contactor.<br />
So the use of a spray nozzle introduces several primary constraints on the structural form of the prototype:<br />
(1) The tower should be wide enough that most of the spray falls through without hitting the walls,<br />
(2) the length of the fall should be long enough that initial transient conditions as fluid leaves the nozzle<br />
(escape angle and velocity) are relatively unimportant compared with time drops spend falling at terminal<br />
velocity in a uniform pattern, and (3) since some spray inevitably hits the walls, this portion of the flow<br />
should be measurable for analytical reasons.<br />
Though nozzles with narrow (15-30 ◦ ) spray patterns are available, wider patterns are much more common,<br />
starting with 60 ◦ patterns (both of the nozzles ultimately used for data collection were 60 ◦ nozzles).<br />
All told, we seemed to require a tower diameter of at least 1 m and fall distance of several meters. Additionally,<br />
smooth, straight walls would aid measurement of flow hitting the walls.<br />
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