1972
DOI: 10.1021/j100649a025
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Vapor pressure isotope effect in aqueous systems. I. Water-water-d2 (-64.deg. to 100.deg.) and water-water18-0 (-17.deg. to 16.deg.). Ice and liquid. II. Alkali metal chloride solution in water and water-d2 (-5.deg. to 100.deg.)

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Cited by 69 publications
(57 citation statements)
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“…As seen in Fig. 2, our result on aD is close to that of MAJOUBE (1971) at the higher temperature range, and is close to that of PUPEZIN et al (1972) at the lower temperature range. The temperature dependence of aD given by the present study is similar to that of JONES (1968).…”
Section: Introductionsupporting
confidence: 83%
“…As seen in Fig. 2, our result on aD is close to that of MAJOUBE (1971) at the higher temperature range, and is close to that of PUPEZIN et al (1972) at the lower temperature range. The temperature dependence of aD given by the present study is similar to that of JONES (1968).…”
Section: Introductionsupporting
confidence: 83%
“…In the calculation the relative humidity of the surface air is assumed to be 90% and the moist air parcel is assumed to be expanded adiabatically. The fractionation factors used are those compiled by Pupezin et al (1972) for 18O between water vapor and water and also for D, and those measured by Majoube (1970) for 18O between water vapor and ice. Fig.…”
Section: The Oxygen Isotopic Composition Of the Snowmentioning
confidence: 99%
“…It is found that the liquidphase pressure and the vapor-phase pressure at the same measured position are on the either side of the extrapolated saturation pressure curve given by Pupezin et al 1 The liquidphase pressure is higher than the extrapolated saturated pressure at the same interfacial liquid temperature. The vaporphase pressure is lower than the extrapolated saturation pressure at the same interfacial vapor temperature.…”
Section: Resultsmentioning
confidence: 59%
“…By definition, the saturation pressure, P sat , at its isothermal liquid temperature, is determined at a flat surface under the equilibrium conditions. The pressure of D 2 O was experimentally measured above the triple point at 276.97 K, [1][2][3][4] whereas the experiments were seldom reported in measuring P sat directly below the triple point. Bottomley measured the vapor-pressure difference between the metastable liquid and the stable solid of D 2 O by using two 0.5 g samples in two connected glass bulbs, respectively, as the temperature was lowered to 261.35 K. 5 However, the assumption of thermal equilibrium might be difficult to reach in the experiments.…”
Section: Introductionmentioning
confidence: 99%