1980
DOI: 10.1007/bf00646402
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Isotopic fractionation of helium during solution: A probe for the liquid state

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Cited by 184 publications
(119 citation statements)
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“…Figure 2 shows a vertical cross section of δ 3 He in the central Indian Ocean along our sampling stations. It is well documented that 3 He is slightly less soluble (1.2 ± 0.5%) in water than 4 He (Weiss 1971;Benson and Krause 1980). The δ 3 He values in surface waters (~10 m depth) in the Indian Ocean were about -1%; they were consistent with the airsaturated seawater value of -1% within analytical error.…”
Section: Experimental Methodssupporting
confidence: 61%
“…Figure 2 shows a vertical cross section of δ 3 He in the central Indian Ocean along our sampling stations. It is well documented that 3 He is slightly less soluble (1.2 ± 0.5%) in water than 4 He (Weiss 1971;Benson and Krause 1980). The δ 3 He values in surface waters (~10 m depth) in the Indian Ocean were about -1%; they were consistent with the airsaturated seawater value of -1% within analytical error.…”
Section: Experimental Methodssupporting
confidence: 61%
“…Note that since atmospheric helium is ~ 99.9999% The second terms are derived from the solubility as a function of potential temperature and salinity of each sample, combined with the helium isotope solubility fractionation factor αS which is a function of temperature and salinity (Benson and Krause, 1980) …”
Section: Pg 21mentioning
confidence: 99%
“…The uncertainty of 3 He at a particular timepoint is estimated from the standard error of the mean of the measurements within the mixed layer. The dynamic solubility equilibrium value of δ 3 He eq for each timepoint was calculated from the solubility value of 3 He (Benson and Krause, 1980). Additionally, since in the mixed layer, completely trapped bubbles lower δ 3 He eq (Fuchs et al, 1987) and partially trapped bubbles increase δ 3 He eq , we use the one-dimensional upper ocean model described in Chapter 4 of this thesis to calculate the effect on δ 3 He eq from air injection and gas exchange.…”
Section: He Flux Gauge Calculationsmentioning
confidence: 99%
“…δ 3 He eq is a function of temperature and gas dynamics (Fuchs et al, 1987). The solubility equilibrium given only temperature considerations, δ 3 He sol , can be calculated from the relationship of Benson and Krause (1980). To determine the contribution from gas dynamics to δ 3 He eq , we added nontritiugenic 3 He to the one dimensional vertical mixed layer model described in Chapter 4 of this thesis.…”
Section: Type Of Productionmentioning
confidence: 99%