On elemental and isotopic fractionation of noble gases in geological fluids by molecular diffusion
Introduction
Noble gases have been widely used as natural tracers to characterize the storage, migration and origin of fluids in geological environments (Ozima and Podosek, 2002, Ballentine et al., 2002, Burnard, 2013). Interestingly, they are chemically and biologically inert and therefore are only fractionated, i.e. partially separated, by physical processes (Ozima and Podosek, 2002). Among the existing physical processes, molecular diffusion is expected to significantly induce noble gases kinetic fractionation in geo-fluids (Marty, 1984, Prinzhofer et al., 2000, Ballentine et al., 2002). Such a kinetic fractionation, simply called fractionation in the following, emerges from the relative differences between molecular diffusion of noble gases when migrating into a fluid. However, its precise quantification and its modeling are still open for debates (Bourg and Sposito, 2008, Tyroller et al., 2014, Tyroller et al., 2018, Seltzer et al., 2019), wider than the noble gas community (Watkins et al., 2017, Wanner and Hunkeler, 2019). The purpose of this article is to provide new insights on the quantification of noble gases fractionation by molecular diffusion in various geo-fluids, in particular in oil and gas.
One of the main reasons for the debate to still be ongoing is the difficulty to experimentally quantify the elemental and even more the isotopic fractionation of noble gases due to molecular diffusion in geo-fluids (Jähne et al., 1987, Tempest and Emerson, 2013, Tyroller et al., 2014, Tyroller et al., 2018, Seltzer et al., 2019). Furthermore, these experiments are mostly limited to what occurs in water at standard conditions. As an alternative to experiments, molecular dynamics (MD) simulations (Allen and Tildesley, 2017, Frenkel and Smit, 2001) proved to be an effective tool for diffusion coefficients estimation in fluids. In particular, this numerical tool was already used to successfully estimate the elemental and isotopic fractionation of noble gases by molecular diffusion in water (Bourg and Sposito, 2008). With progresses in molecular modeling, MD simulations are now able to provide accurate results for the equilibrium and transport properties of various geo-fluids under subsurface conditions, including noble gases, natural gases and oil (Martin and Siepmann, 1998, Leach, 2001, Siu et al., 2012, Marrink and Tieleman, 2013, Hoang et al., 2017, Hoang et al., 2019).
A significant number of theoretical and empirical models are already proposed in the literature to quantify mass diffusion coefficients in various environments (Chapman and Cowling, 1970, Poling et al., 2001, Cussler, 2009). However, quite surprisingly, the most common approach to quantify the fractionation by molecular diffusion, whether isotopic or elementary, is simply based on the evaluation of the inverse of the square root of the mass ratios of the two species considered whatever the geo-fluids and the pressure and temperature conditions (Ballentine et al., 2002, Watkins et al., 2017, Wanner and Hunkeler, 2019). This simple relationship (called in the following the square root law) although theoretically correct for isotopic fractionation under low-density gas condition or in the limit of ultra-tight porous medium (Marty, 1984, Ballentine et al., 2002) only, consistently describes noble gases elemental fractionation in aqueous fluids under standard conditions (Jähne et al., 1987). Nevertheless, recent experimental studies and numerical simulations showed that the square root law tends to strongly overestimate noble gas isotopes fractionation in aqueous fluids (Bourg and Sposito, 2008, Tempest and Emerson, 2013, Tyroller et al., 2014, Tyroller et al., 2018, Seltzer et al., 2019). Similar findings have been noticed for other solute elements such as alkali and alkali earth metals, halides and CO2, in both liquid water and silicate melts (Richter et al., 2006, Bourg et al., 2010, Zeebe, 2011, Watkins et al., 2017, Wanner and Hunkeler, 2019).
Thus, to rationalize all the results on noble gases, we propose in this work to systematically study the limits and capabilities of the various fractionation models applied to them in various geo-fluids, including not only water as already looked after in the seminal work of Bourg and Sposito (2008), but also gas (methane) and oil (n-hexane), using molecular simulations data. As it will be shown, this approach allowed us to explain why the square root law holds well for elemental fractionation and led us to propose a generic semi-empirical model able to provide a good estimate of noble gas isotopic fractionation by molecular diffusion whatever the geo-fluids and the thermodynamic conditions considered.
The article is organized as follows: in Section 2, we provide details on existing fractionation models and on numerical details of molecular simulations. The results obtained from molecular simulations and theoretical models are presented and discussed in 3 Results, 4 Discussion, respectively. Finally, the main results of this study are summarized in Section 5, which is the conclusion.
Section snippets
Kinetic Fractionation by molecular diffusion
Molecular diffusion processes are expected to induce both isotopic and elemental kinetic fractionation of trace elements in geo-fluids (Marty, 1984, Watkins et al., 2017, Wanner and Hunkeler, 2019). Such a fractionation is simply due to a difference in the relative migration velocity, by molecular diffusion, of the components when advection is absent. It is a complex and coupled transient phenomenon occurring only when the system is out of equilibrium, i.e. when the compositions (or more
Results
Molecular simulations were performed on noble gases (He, Ne, Ar, Kr and Xe) in: i) water under ambient conditions at T = 298 K and P = 0.1 MPa, ii) methane (gas) and iii) n-hexane (oil) under reservoir conditions at T = 423 K and P = 50 MPa and T = 323 K and P = 10 MPa, respectively. To compute the fractionation coefficient from Eq. (1), the self-diffusion coefficients of the noble gases were computed using Eq. (15) as described in Section 2.3.2.
Elemental Fractionation of Noble Gases
It has been shown that the square root law, Eq. (3), is able to provide a quantitative estimate of the elemental fractionation of 40Ar, 84Kr and 132Xe, relatively to 20Ne, in all geo-fluids studied in this work (water, gas, oil). This result is rather surprising as such a relation should only hold in the free-molecular diffusion regime, see Section 2.2, whereas the studied solvent corresponds to the dense gas and the liquid diffusion regimes. Indeed, from Eqs. (7), (10), one would expect that
Conclusions
In this work, we investigated the capability of theoretical models to predict the elemental and isotopic kinetic fractionation of noble gases due to molecular diffusion in geological fluids. First, a brief review of the available theoretical models depending on the fluid conditions was presented. It was pointed out that, among them, the square-root law, which is the most widely used approach, is theoretically valid only under the free molecular regime, i.e. far from sub-surface conditions. To
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
We gratefully acknowledge TOTAL S.A. for the post-doctoral grant awarded to one of us (HH) and for letting us publish these results. We also thank the Pau University and the MCIA for providing computational facilities. Prof. Khac Hieu Ho would like to acknowledge financial support from the Vietnam National Foundation for Science and Technology Development (NAFOSTED) under grant number 103.01-2019.49.
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