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Homogeni z ation and porous media. by Ulrich Hornung Chapter 1: I ntroduction. Heike Gramberg , CASA Seminar Wednesday 23 February 2005. Overview. Diffusion in periodic media Special case: layered media Diffusion in media with obstacles Stokes problem: derivation of Darcy’s law.
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Homogenization and porous media by Ulrich Hornung Chapter 1: Introduction Heike Gramberg, CASA Seminar Wednesday 23 February 2005
Overview • Diffusion in periodic media • Special case: layered media • Diffusion in media with obstacles • Stokes problem: derivation of Darcy’s law
Diffusion equation (Review) • We start with the following Problem • Let with bounded and smooth • Diffusion equation
Assumptions • is rapidly oscillating i.e. • a=a(y) is Y-periodic in with periodicity cell
Ansatz • has an asymptotic expansion of the form • and are treated as independent variables
Substitution of expansion • Comparing terms of different powers yields • where
Solution • Terms of order : • since is Y-periodic we find
Terms of order : separation of variables where is Y-periodic solution of
Terms of order integration over Y • using for all Y-periodic g(y):
Propositions Proposition 1: The homogenizationof the diffusion problem is given by where is given by
Proposition 2: • The tensor A is symmetric • If a satisfies a(y)>a>0 for all y then A is positive definite
Remarks • are uniquely defined up to a constant • are uniquely defined • Problem can be generalized by considering • Eigenvalues l of A satisfy Voigt-Reiss inequality: where
Example: Layered Media • Assumption: • Then and is Y-periodic solution of
Proposition 3: • If , then • The coefficients are given by
Remarks • Effective Diffusivity in direction parallel to layers is given by arithmeticmean of a(y) • Effective Diffusivity in direction normal to layers is given by geometricmean of a(y) • Extreme example of Voigt-Reiss inequality
e Media with obstacles • Medium has periodic arrangement of obstacles
Formal description of geometry • Standard periodicity cell • Geometric structure within • Assumption:
Diffusion problem • Diffusion only in • Assumptions: and
Substitution of expansion • Comparing terms of different powers yields
Lemmas • Lemma 1: for and • Lemma 2 (Divergence Theorem): for Y-periodic
Solution • Terms of order : for • using Lemmas 1 and 2 we find • therefore
Terms of order : for • with boundary condition for
separation of variables where is Y-periodic solution of
Terms of order • using Lemma 2 and boundary conditions: • hence is solution of
Proposition Proposition 4: The homogenizationof the diffusion problem on geometry with obstacles is given by where is given by
Remarks • Due to the homogeneous Neumann conditions on integrals over boundary disappear • Weak formulation of the cell problem where is characteristic function of
Stokes problem • For media with obstacles • Assumptions
Solution • Comparing coefficients of the sameorder • Stokes equation: • Conservation of mass: • Boundary conditions:
With we get for • Separation of variables for both where are solution of
Darcy’s law • Averaging velocity over where is given by
Conservation of mass • Term of order in conservation of mass • Integration over yields
Proposition Proposition 5: The homogenization of the Stokes problem is given by Proposition 6: The tensorKis symmetric and positive definite
Conclusions • We have looked at homogenization of the Diffusion problem and the Stokes problem on media with obstacles • Solutions of the homogenized problems can be expressed in terms of solutions of cell problems • The homogenization of the Stokes problem leads to the derivation of Darcy’s law