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Joint International Conference on Long-term Experiments ...

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n = - 1 ⁄ 2 [1]-[4]. The later model is applied when the water surface is rugous (with<br />

tides).<br />

Table nr.2<br />

___________________________________________________________Solubility<br />

Symbol C<strong>on</strong>versi<strong>on</strong> to SA<br />

___________________________________________________________<br />

For using with pA humid = pA dry (1 - pH2O/P)<br />

−3<br />

β A 6 mmol m<br />

Bunsen coefficient βA SA = × 10 −1<br />

VA mol l<br />

Solubility functi<strong>on</strong> F<br />

F<br />

3<br />

6 mmol m<br />

−<br />

SA =<br />

× 10<br />

( P − p ) −1<br />

H2O<br />

mol l<br />

______________________________________________________________________<br />

For using with pA dry<br />

β<br />

−3<br />

6<br />

Bunsen coefficient βA SA =<br />

A mmol m<br />

× 10 −1<br />

V mol l<br />

A<br />

−3<br />

F 6 mmol m<br />

Solubility functi<strong>on</strong> F SA = × 10 −1<br />

p mol l<br />

It can be observed that a not so soluble gas as O2 has an exchange rate larger than a<br />

more soluble gas as CO2. This fact is perfectly compatible with the important role of the<br />

bubbles in the gas exchange process previously discussed. The not so soluble gases<br />

exchange is increased by a bigger fracti<strong>on</strong>al quantity when the bubbles are developed,<br />

due to the fact that the gases with a lower solubility have a lower transfer coefficient<br />

transversal to the air-sea interface than the gases with bigger solubility. The bubbles<br />

transfer could be separately discussed. A result of the laboratory studies is: it<br />

dem<strong>on</strong>strates that the sensibility of gases exchange for a variety of c<strong>on</strong>diti<strong>on</strong>s, that are<br />

difficult to reproduce in a laboratory situati<strong>on</strong>.<br />

A series of techniques for studying the gases exchange in a more realistic mode<br />

were developed, in the field c<strong>on</strong>diti<strong>on</strong>s. There are three such techniques:<br />

• The method of the rad<strong>on</strong> deficiency<br />

• The method of the oceanic radiocarb<strong>on</strong> inventory, and<br />

• The dual method of a tracer.<br />

We will refer to in situ (in field) studies, describing them and presenting here <strong>on</strong>ly the<br />

method of the rad<strong>on</strong> deficiency.<br />

(a) The method of the rad<strong>on</strong> deficiency is based <strong>on</strong> the Rad<strong>on</strong>-222 distributi<strong>on</strong> at<br />

the ocean surface. This radioisotope, with the de half value life time of 3,825 days, is<br />

formed by the decay of Radiu-226 at oceanic water surface. We know from<br />

393

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