1D Single Phase Flow in Porous Media

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SUMMARY

This discussion focuses on modeling 1D single-phase flow of a slightly compressible liquid through a rigid, incompressible porous medium using Darcy's law. The governing equation derived is εμc ∂P/∂t = ∇·(k ∇P), where ε is porosity, μ is viscosity, c is compressibility, and k is permeability. The user seeks assistance in formulating appropriate boundary conditions for the pressure P(x,t), particularly for a scenario where one end is at constant pressure and the other is insulated. The discussion highlights the challenges faced due to a lack of experience with partial differential equations (PDEs).

PREREQUISITES
  • Understanding of Darcy's law for fluid flow in porous media
  • Familiarity with the concepts of porosity, permeability, and compressibility
  • Basic knowledge of partial differential equations (PDEs)
  • Experience with fluid dynamics and pressure modeling
NEXT STEPS
  • Research boundary condition formulation for PDEs in fluid dynamics
  • Study the application of Darcy's law in various porous media scenarios
  • Learn about numerical methods for solving PDEs, such as finite difference methods
  • Explore multi-phase flow modeling techniques for future extensions of the problem
USEFUL FOR

This discussion is beneficial for students and professionals in fluid dynamics, particularly those working with porous media, as well as researchers dealing with pressure modeling in single-phase flow scenarios.

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Homework Statement



I have been asked to model the flow of a slightly compressible liquid through a rigid, incompressible porous medium in 1D, assuming the flow obeys Darcy's law. I am given a rectangular prism of cross sectional area A with length L, a source of liquid (say water) on one side with total discharge Q, along with variables concerning the properties of the medium (porosity, permeability, etc). I am ignoring dispersion and diffusion effects.

Basically I am looking to find the pressure in the tube as a function of position and time, P(x,t).

Homework Equations





The Attempt at a Solution



Combining the continuity equation,

\epsilon\frac{\partial\rho}{\partial t} + \nabla\cdot\left(\rho k \nabla v\right) = 0

Ignore above line, not showing up correctly,

\epsilon\frac{\partial\rho}{\partial t} + \nabla\cdot\left(\rho k \nabla v\right) = 0

with Darcy's law,

v = \frac{-k}{\mu}\nabla P

we get,

\epsilon\mu\frac{\partial\rho}{\partial t} = \nabla\cdot\left(\rho k \nabla P\right)

Then assuming a liquid with compressibility c,

\rho = \rho_{o}e^{c(P-P_{o}}

which combines with the above to give the governing equation:

\epsilon\mu c \frac{\partial P}{\partial t} = \nabla\cdot\left(k \nabla P\right)

Combining the constant terms together, and since we are only considering the 1D flow in the x direction:

\frac{\partial P}{\partial t} = \alpha\frac{\partial^{2}P}{\partial x^{2}}

*** The first few equations are not showing up correctly. But what is important is the final results which seem ok.

Now all I need to do is solve this equation to get P(x,t).

What I am having problems with is the boundary conditions. I haven't taken any PDE courses or anything, so I'm not sure how they are supposed to be formulated, but I'll give some guesses:

P(x,0) = Pi ie. the pressure initially is some constant throughout the medium
Q = constant ie. the input flow rate is constant for all t
P(L,inf) = ?

I am assuming a finite medium with no discharge, so the liquid, and the pressure, will build up indefinitely, but I don't know what to put for the boundary at the end.

Like I said I am unfamiliar with PDEs which makes this very difficult. Later this problem will be extended to multi-phase flow, but this was given as a warm up for now.

Any help with this problem would be greatly appreciated! Thank you!
 
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I think I have the boundary conditions:

P(0,t) = some constant (non-zero, from Darcy's law)
P(L,t) = Po ??
P(x,0) = Pi or do I use dP/dx = 0 since the end is 'insulated'

Now I know how to solve pde's for both ends at 0 or both ends insulated, but not for one end at constant presure and the other end insulated. I'm thinking in terms of the analogy of heat flow in a wire.

Again any help is very much appreciated!
 

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