1974
DOI: 10.1111/j.2153-3490.1974.tb01948.x
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Gas exchange rates between air and sea

Abstract: Gas exchange rate studies carried out in the laboratory suggest that the stagnant film model is adequate to relate the transfer coefficients of most gases between the atmosphere and sea to an accuracy of ±15%. Estimates of the average film thickness prevailing for the world ocean based on the distribution of natural radiocarbon, bomb‐produced radiocarbon, and radon are in good agreement. Radon data from the BOMEX area and from station PAPA lend support to Kanwisher's suggestion that gas exchange rates should v… Show more

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Cited by 541 publications
(247 citation statements)
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“…Osafune and Yasuda (2012) also drew from a modeling study to argue that tidal mixing could induce O 2 variations through the development of a winter mixed layer due to upward salt flux over broad areas. Here we roughly estimate O 2 oscillations through air-sea gas exchange associated with differences in mixed layer depths (Broecker & Peng, 1974) using climatological winds in the region (Kalnay et al, 1996) and a broadly used formulation of the gas transfer velocity (Wanninkhof, 1992). Even in the extreme case that dissolved O 2 , T, and S are uniform in the mixed layer, as prescribed by the winter average on the isopycnal surface of σ θ = 26.7 kg/m 3 (Figure 2c), O 2 oscillates with a maximum amplitude of about 4 μmol/kg associated with the oscillations of the thickness of the mixed layer (assuming equal to the depth of σ θ = 26.7 kg/m 3 ) between 160 m and 200 m (Figure 13c).…”
Section: (E) Winter Ventilation Associated With Variations In Mixed Lmentioning
confidence: 99%
“…Osafune and Yasuda (2012) also drew from a modeling study to argue that tidal mixing could induce O 2 variations through the development of a winter mixed layer due to upward salt flux over broad areas. Here we roughly estimate O 2 oscillations through air-sea gas exchange associated with differences in mixed layer depths (Broecker & Peng, 1974) using climatological winds in the region (Kalnay et al, 1996) and a broadly used formulation of the gas transfer velocity (Wanninkhof, 1992). Even in the extreme case that dissolved O 2 , T, and S are uniform in the mixed layer, as prescribed by the winter average on the isopycnal surface of σ θ = 26.7 kg/m 3 (Figure 2c), O 2 oscillates with a maximum amplitude of about 4 μmol/kg associated with the oscillations of the thickness of the mixed layer (assuming equal to the depth of σ θ = 26.7 kg/m 3 ) between 160 m and 200 m (Figure 13c).…”
Section: (E) Winter Ventilation Associated With Variations In Mixed Lmentioning
confidence: 99%
“…To calculate the diffusive oxygen uptake, we used Fick's first law of diffusion ) at in situ temperature and salinity (Broecker and Peng 1974).…”
Section: Oxygen Microelectrodesmentioning
confidence: 99%
“…An even larger sensitivity to the choice of k w exists for the air-sea transfer of the isotopes of CO 2 , i.e., 14 CO 2 and 13 CO 2 , since the characteristic exchange time-scale for these isotopes is about ten times longer than that for CO 2 itself (Broecker and Peng 1974). This is a consequence of the fact that isotopic equilibrium across the air-sea interface needs to be established by equilibrating all carbonate species in the surface ocean, while for CO 2 , the shortcut reaction involving HCO À 3 and CO À2 3 establish a faster equilibrium.…”
Section: Modelsmentioning
confidence: 99%