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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