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gas hydrate - CCOP

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STOMP-HYD: A New Numerical Simulator for Analysis of<br />

Methane Hydrate Production from Geologic Formations<br />

Mark White 1) and Pete McGrail 2)<br />

1) Hydrology Group, Pacific Northwest National Laboratory, U.S.A.<br />

2) Applied Geology and Geochemistry, Pacific Northwest National Laboratory, U.S.A.<br />

ABSTRACT: Conventional methods of <strong>gas</strong> <strong>hydrate</strong> production include reservoir<br />

depressurization, thermal stimulation, and inhibitor injection. A leading<br />

unconventional approach for <strong>gas</strong> <strong>hydrate</strong> production involves the exchange of CO 2<br />

for CH 4 . This unconventional concept has several distinct benefits over the<br />

conventional methods: 1) the heat of formation of CO 2 <strong>hydrate</strong> is greater than the<br />

heat of dissociation of CH 4 <strong>hydrate</strong>, providing a low-grade heat source to support<br />

additional methane <strong>hydrate</strong> dissociation, 2) exchanging CO 2 with CH 4 will<br />

maintain the mechanical stability of the geologic formation, and 3) the process is<br />

environmentally friendly, providing a sequestration mechanism for the injected CO 2 .<br />

An operational mode of the STOMP simulator has been developed at the Pacific<br />

Northwest National Laboratory that solves the coupled flow and transport<br />

equations for the mixed CH 4 -CO 2 <strong>hydrate</strong> system under nonisothermal conditions,<br />

with the option for considering NaCl as an inhibitor in the pore water. The<br />

simulator solves the coupled nonlinear governing equations for conservation of<br />

water, CH 4 , CO 2 , and NaCl mass and thermal energy on structured orthogonal grid<br />

systems. Recognized mobile phases in the order of decreasing wettability include:<br />

aqueous, liquid CO 2 , and <strong>gas</strong>. Immobile phases include: <strong>hydrate</strong>, ice, and<br />

precipitated salt; where the <strong>hydrate</strong> and ice phases are presumed to be occluded by<br />

the aqueous phase. Gas <strong>hydrate</strong> equilibrium temperature is calculated as a function<br />

of <strong>gas</strong> vapor pressure and mole fraction of <strong>hydrate</strong> formers from tabular data<br />

generated using a fugacity-based equilibrium model. Corrections for inhibitors as a<br />

function of aqueous concentration are calculated from a generalized empirical<br />

formulation.<br />

Hydrate-aqueous and ice-aqueous interfacial radii are computed as a function of<br />

the system temperature and <strong>hydrate</strong> or ice equilibrium temperature, respectively.<br />

Interfacial radii are converted to interfacial pressures via interfacial tensions,<br />

which are then used to compute saturations via scaled capillary pressure-saturation<br />

functions. This approach, combined with the assumption that the aqueous phase<br />

never disappears, yields four phase conditions and two primary variable sets. The<br />

simulator is demonstrated on a variety of <strong>hydrate</strong> production scenarios, including<br />

liquid-CO 2 microemulsion injection and CO 2 exchange.<br />

Keywords: numerical simulation, STOMP, methane <strong>hydrate</strong>, CO 2 exchange,<br />

depressurization, thermal stimulation, inhibitor.<br />

New Energy Resources in the <strong>CCOP</strong> Region - Gas Hydrates and Coalbed Methane 77

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