Buckley–Leverett equation
{{short description|Conservation law for two-phase flow in porous media}}
In fluid dynamics, the Buckley–Leverett equation is a conservation equation used to model two-phase flow in porous media.{{cite journal|author=S.E. Buckley and M.C. Leverett|title=Mechanism of fluid displacements in sands|url=https://www.onepetro.org/journal-paper/SPE-942107-G|journal=Transactions of the AIME|issue=146|pages=107–116|year=1942|volume=146 |doi=10.2118/942107-G |doi-access=free}} The Buckley–Leverett equation or the Buckley–Leverett displacement describes an immiscible displacement process, such as the displacement of oil by water, in a one-dimensional or quasi-one-dimensional reservoir. This equation can be derived from the mass conservation equations of two-phase flow, under the assumptions listed below.
Equation
In a quasi-1D domain, the Buckley–Leverett equation is given by:
:
\frac{\partial S_w}{\partial t} + \frac{\partial}{\partial x}\left( \frac{Q}{\phi A} f_w(S_w) \right) = 0,
where is the wetting-phase (water) saturation, is the total flow rate, is the rock porosity, is the area of the cross-section in the sample volume, and is the fractional flow function of the wetting phase. Typically, is an S-shaped, nonlinear function of the saturation , which characterizes the relative mobilities of the two phases:
:
f_w(S_w) = \frac{\lambda_w}{\lambda_w + \lambda_n} = \frac{ \frac{k_{rw}}{\mu_w} }{ \frac{k_{rw}}{\mu_w} + \frac{k_{rn}}{\mu_n} },
where and denote the wetting and non-wetting phase mobilities. and denote the relative permeability functions of each phase and and represent the phase viscosities.
Assumptions
The Buckley–Leverett equation is derived based on the following assumptions:
- Flow is linear and horizontal
- Both wetting and non-wetting phases are incompressible
- Immiscible phases
- Negligible capillary pressure effects (this implies that the pressures of the two phases are equal)
- Negligible gravitational forces
General solution
The characteristic velocity of the Buckley–Leverett equation is given by:
:
The hyperbolic nature of the equation implies that the solution of the Buckley–Leverett equation has the form , where is the characteristic velocity given above. The non-convexity of the fractional flow function also gives rise to the well known Buckley-Leverett profile, which consists of a shock wave immediately followed by a rarefaction wave.
See also
References
{{reflist}}
External links
- [http://perminc.com/resources/fundamentals-of-fluid-flow-in-porous-media/chapter-4-immiscible-displacement/buckley-leverett-theory/ Buckley-Leverett Equation and Uses in Porous Media]
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Category:Conservation equations
Category:Equations of fluid dynamics
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