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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Draft type Height<br />
[m]<br />
Crosssectional<br />
area<br />
[m 2 ]<br />
cost per unit<br />
[$millions]<br />
cost with mods<br />
[$millions]<br />
cost per<br />
cross-section<br />
[$/m 2 ]<br />
Natural 1 90 5100 36 41 8000<br />
Forced 1 40 3000 18 18 6000<br />
Natural 2 120 7900 25–75 31–81 4000–10000<br />
Forced 2 50 280 0.5–1 0.5–1 1800–3500<br />
Table 3.2: Capital cost of cooling towers. Costs represent complete installed costs. EPA costs are <strong>from</strong><br />
1996, adjusted to 2006 dollars using the Construction Building Index. Upper bounds of ranges reflect<br />
towers with plume and noise abatement and unusually high site-specific costs.<br />
1 EPA (2002)<br />
2 Mykyntyn (2006)<br />
and foundation. We take the cost of this addition as $4 million, typical in the wind industry. For the<br />
demister, our prototype demonstrated that a wire mesh filter constructed manually of stainless steel wool<br />
can be effective with an acceptable pressure drop. However, in the full-scale system a more sophisticated<br />
system is warranted. We obtained a price quote and product specifications <strong>from</strong> a commercial particle<br />
trap manufacturer (Amistico, 2006) and apply those directly, ignoring the substantial bulk discount that<br />
is likely for a project as large as even a single <strong>air</strong> capture tower. We get 500 $/m 2 -demister. With a<br />
downward flow contactor, a reasonable placement of the demister would be as an annulus around the base<br />
of the tower. The total area of the demister can be adjusted by the height of the annulus. Demisters of this<br />
type collect drops more efficiently at higher <strong>air</strong> velocity but the pressure drop increases with <strong>air</strong> velocity.<br />
We expect that a total area of the demister of one half that of the tower cross section (demister velocity<br />
twice the tower velocity) makes a reasonable trade-off between these competing effects. This is what we<br />
assume for capital cost calculations.<br />
Forced-draft cooling towers are more directly adaptable to <strong>air</strong> capture since they already have fans and<br />
demisters. They are smaller, however – typically 20–50 m high and arrayed in square cells 10–20 m on<br />
a side. They can be constructed of concrete or fiberglass for similar costs. Again, the liquid flowrate in<br />
an <strong>air</strong> capture version would be about a tenth that of a conventional version. Also, forced draft towers<br />
have some “splash fill” material which we will not require. Air flow velocities are similar. We will apply<br />
contactor costs for forced draft cooling towers directly to an equivalently-dimensioned contactor.<br />
Table 3.2 shows capital cost estimates for power plant cooling towers and includes the cost of modifications<br />
to natural draft towers described above. Personal communication with industry experts and<br />
estimating documents <strong>from</strong> the EPA (2000, 2002) were used to arrive at the estimates. Cost is usually<br />
given per unit liquid flow, which is the primary figure for which cooling towers are generally sized. Typical<br />
flow rates and sizes were then used to calculate the implied cost per unit cross-sectional area and cost<br />
per physical structure.<br />
The costs span a f<strong>air</strong>ly wide range. This may reflect the quality of the data sources more than actual<br />
uncertainty in cooling tower construction; cost information is proprietary and industry tends to be loathe to<br />
share it. Some of the variation is due to inclusion versus exclusion of components, particularly noise and<br />
plume abatement. We will use EPA costs as the base case, and consider the lowest costs in the sensitivity<br />
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