Buckley–Leverett equation

Buckley–Leverett equation

In fluid dynamics, the Buckley–Leverett equation is a transport 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|journal=Transactions of the AIME|issue=146|pages=107–116|date=1942] . The Buckley–Leverett equation or the Buckley–Leverett "displacement" can be interpreted as a way of incorporating the microscopic effects to due capillary pressure in two-phase flow into Darcy's law.

In a 1D sample (control volume), let S(x,t) be the water saturation, then the Buckley–Leverett equation is

:frac{partial S}{partial t} = U(S)frac{partial S}{partial x}

where

:U(S) = frac{Q}{phi A} frac{mathrm{d} f}{mathrm{d} S}.

f is the fractional flow rate, Q is the total flow, phi is porosity and A is area of the cross-section in the sample volume.

Assumptions for validity

The Buckley–Leverett equation is derived for a 1D sample given
* mass conservation
* capillary pressure p_c(S) is a function of water saturation S only
* mathrm{d}p_c/mathrm{d}S = 0 causing the pressure gradients of the two phases to be equal.

General solution

The solution of the Buckley–Leverett equation has the form S(x,t) = S(x-U(S)t) which means that U(S) is the front velocity of the fluids at saturation S.

ee also

* Capillary pressure
* Permeability (fluid)
* Relative permeability
* Darcy's law

References


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