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386 12 Carbon Capture and Storage
All these species are grouped as dissolved inorganic carbon (DIC). H 2 CO 3 also
reacts with dissolved limestone in the ocean, which is a result of weathering the
earth surface, and the simplified chemical reaction is
CaCO 3 þ H 2 CO 3 ! Ca 2þ þ 2HCO ð12:66Þ
3
Besides the inorganic carbons, CO 2 is also converted into particulate organic
carbon (POC) and fertilizer by photosynthesis. For example,
6CO 2 þ 6H 2 O þ uv ! C 6 H 12 O 6 þ 6O 2 ð12:67Þ
106CO 2 þ 122H 2 O þ 16HCO þ H 3 PO 4
3
ð12:68Þ
! C 106 H 263 O 110 N 16 P þ 138O 2
One way or another, CO 2 is not saturated in deep ocean as a result of these
chemical reactions and biological conversions of CO 2 into organic and inorganic
carbon compounds. Therefore, more CO 2 can be stored in deep ocean. However,
natural absorption of CO 2 into ocean is a slow process and it cannot catch up with
the increase rate of anthropogenic CO 2 in the atmosphere.
This process can be expedited by injecting CO 2 into deep ocean. Based on the
properties of liquid CO 2 in ocean, engineered deep ocean CO 2 storage can be
achieved by
• direct CO 2 dissolution, and
• liquid CO 2 isolation
The fate of the injected CO 2 depends on the injection depth in the ocean. At a
depth of about 500 m (corresponding to the pressure of 4–5 MPa and temperatures
in the range of 0–10 °C), CO 2 starts to liquefy and the liquid CO 2 has a density of
3
860–920 kg/m . The deeper into the ocean, the greater liquid CO 2 density as a
result of the greater pressure.
According to the liquid CO 2 density relative to the seawater density, the depths
can be divided into three zones where CO 2 , floats, suspends, and sinks, respec-
tively. As shown in Fig. 12.11, liquid CO 2 density is close to that of seawater at
depths of about 2,500–3,000 m. This is also referred to as thermocline. Above this
zone, CO 2 density is less than the surrounding seawater. Therefore, the liquid CO 2
droplets rise as a plume. In the transition zone, CO 2 density is nearly close to that of
seawater and it suspends in seawater due to neutral buoyance. Further deep into the
ocean, CO 2 density surpasses that of the seawater resulting in sinking CO 2 plume.
For any one of the three scenarios, most of the released CO 2 will eventually
dissolve in the ocean.
The sinking CO 2 droplets eventually reach the bottom of the ocean enabling
liquid CO 2 isolation as a liquid lake in an ocean floor depression. Such a CO 2 lake
can be made by injecting liquid CO 2 to the ocean floor depression or releasing CO 2
at a depth that is close to the target lake. Settled liquid CO 2 in the lake mixes with

