SPE Journal
Volume 11,
Number 4,
December 2006,
pp. 480-487
Summary
A multimechanistic flow environment is the result of the combined action of
a Darcian flow component (the macroscopic flow of the phase caused by pressure
gradients) and a Fickian-like or diffusive flow component (diffusive flow
caused by molecular concentration gradients) taking place in a hydrocarbon
reservoir. The present work presents the framework needed for the assessment of
the impact of multimechanistic flow on systems where complex fluid
behavior—such as that of retrograde gas-condensate fluids—requires the
implementation of compositional reservoir simulators. Because of the complex
fluid behavior nature of gas-condensate fluids, a fully-implicit (IMPISC-type)
compositional model is implemented and the model is used for the study of the
isothermal depletion of naturally fractured retrograde gas reservoirs. In these
systems, especially those tight systems with very low permeability (k
< 0.1 md), bulk fluid flow as predicted by Darcy’s law might not take
place despite the presence of large pressure gradients. The use of an
effective diffusion coefficient in the gas phase—which accounts for the
combined effect of the different diffusion mechanisms that could take place in
a porous medium—and its relative contribution to fluid recovery is discussed.
The compositional tracking capabilities of the model are tested, and the
conditions where Fickian flow can be the major player in recovery predictions
and considerably overcome the flow impairment to gas flow posed by the eventual
appearance of a condensate barrier—typical of gas-condensate systems—are
investigated. Finally, a mapping that defines different domains where
multimechanistic flow can be expected in compositional simulators of retrograde
gas-condensate reservoirs is presented.
Introduction
In typical natural-gas reservoirs, all hydrocarbons exist as a single free
gas phase at conditions of discovery. Depending on the composition of the
initial hydrocarbon mixture in place and their depletion behavior, we recognize
up to three kinds of natural gas reservoirs: dry gas reservoirs, wet gas
reservoirs, and retrograde gas or gas-condensate reservoirs. The latter is the
richest in terms of heavy hydrocarbons, and thus it is very likely to develop a
second heavier hydrocarbon phase (liquid condensate) upon isothermal depletion.
This situation is illustrated by Fig. 1. In contrast, dry gases and wet gases
do not undergo phase changes upon reservoir depletion, as their phase
envelope’s cricondentherms are found to the left of the reservoir temperature
isotherm.
© 2006. Society of Petroleum Engineers
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History
- Original manuscript received:
28 February 2005
- Revised manuscript received:
5 May 2006
- Manuscript approved:
9 May 2006
- Version of record:
20 December 2006