2005
DOI: 10.1016/j.epsl.2004.11.011
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Effects of molecular diffusion on trapped gas composition in polar ice cores

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Cited by 77 publications
(132 citation statements)
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“…Again at 216 K, X n of O 2 and N 2 within ice lattice are 2.3 Â 10 À10 and 1.4 Â 10 À10 mol m ice À3 Pa À1 , respectively [Ikeda-Fukazawa et al, 2005]. Then, the permeation coefficient D n X n is 3.6 Â 10 À21 and 1.6 Â 10 À21 mol m ice À1 s À1 Pa…”
Section: Typical Changes Of Tmentioning
confidence: 96%
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“…Again at 216 K, X n of O 2 and N 2 within ice lattice are 2.3 Â 10 À10 and 1.4 Â 10 À10 mol m ice À3 Pa À1 , respectively [Ikeda-Fukazawa et al, 2005]. Then, the permeation coefficient D n X n is 3.6 Â 10 À21 and 1.6 Â 10 À21 mol m ice À1 s À1 Pa…”
Section: Typical Changes Of Tmentioning
confidence: 96%
“…For example, overburden pressures were estimated from the density profile in Figure 3a and they are higher than the atmospheric pressure by 0.45 MPa and 0.65 MPa at z s = 78 m and z c = 104 m, respectively. It has been presumed that the differences in pressure between closing/ closed air bubbles and air in open pores drive two processes: effusion of air from closing bubbles to open pores through a small opening [Bender, 2002] and permeation of gas molecules from closed bubbles to open pores through the ice lattice [Huber et al, 2006;Ikeda-Fukazawa et al, 2005;Severinghaus and Battle, 2006]. The former process, Dp-driven effusion, was proposed by Bender [2002] as a mechanism for gas fractionation.…”
Section: A Model For Modulation Of Conditions For Gas Transport By Lomentioning
confidence: 99%
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