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src
transport
TortuosityBruggeman.h
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/**
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* @file TortuosityBase.h
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* Virtual base class to compute the increase in diffusive path length associated with
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* tortuous path diffusion through, for example, porous media.
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*/
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/*
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* Copyright (2005) Sandia Corporation. Under the terms of
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* Contract DE-AC04-94AL85000 with Sandia Corporation, the
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* U.S. Government retains certain rights in this software.
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*/
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#ifndef CT_TORTUOSITYBRUGGEMAN_H
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#define CT_TORTUOSITYBRUGGEMAN_H
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#include "
TortuosityBase.h
"
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namespace
Cantera
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{
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//! Base case to handle tortuosity corrections for diffusive transport
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//! in porous media using the Bruggeman exponential approximation
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/*!
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* Class to compute the increase in diffusive path length associated with
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* tortuous path diffusion through, for example, porous media.
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* This base class implementation relates tortuosity to volume fraction
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* through a power-law relationship that goes back to Bruggeman. The
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* exponent is referred to as the Bruggeman exponent.
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*
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* Note that the total diffusional flux is generally written as
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*
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* \f[
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* \frac{ \phi C_T D_i \nabla X_i }{ \tau^2 }
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* \f]
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*
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* where \f$ \phi \f$ is the volume fraction of the transported phase,
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* \f$ \tau \f$ is referred to as the tortuosity. (Other variables are
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* \f$ C_T \f$, the total concentration, \f$ D_i \f$, the diffusion
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* coefficient, and \f$ X_i \f$, the mole fraction with Fickian
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* transport assumed.)
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*
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* The tortuosity comes into play in conjunction the the
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*/
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class
TortuosityBruggeman
:
public
TortuosityBase
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{
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public
:
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//! Default constructor uses Bruggeman exponent of 1.5
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/*!
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* @param setPower Exponent in the Bruggeman factor. The default is 1.5
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*/
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TortuosityBruggeman
(doublereal setPower = 1.5);
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//! Copy Constructor
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/*!
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* @param right Object to be copied
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*/
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TortuosityBruggeman
(
const
TortuosityBruggeman
& right);
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//! Default destructor for TortuosityBruggeman
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virtual
~TortuosityBruggeman
();
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//! Assignment operator
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/*!
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* @param right Object to be copied
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*/
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TortuosityBruggeman
&
operator=
(
const
TortuosityBruggeman
& right);
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//! Duplication operator
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/*!
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* @return Returns a pointer to a duplicate of the current object given a
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* base class pointer
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*/
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virtual
TortuosityBase
*
duplMyselfAsTortuosityBase
()
const
;
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//! The tortuosity factor models the effective increase in the
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//! diffusive transport length.
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/*!
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* This method returns \f$ 1/\tau^2 \f$ in the description of the flux
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*
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* \f$ C_T D_i \nabla X_i / \tau^2 \f$.
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*
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*
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*/
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virtual
doublereal
tortuosityFactor
(doublereal porosity);
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//! The McMillan number is the ratio of the flux-like
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//! variable to the value it would have without porous flow.
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/**
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* The McMillan number combines the effect of tortuosity
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* and volume fraction of the transported phase. The net flux
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* observed is then the product of the McMillan number and the
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* non-porous transport rate. For a conductivity in a non-porous
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* media, \f$ \kappa_0 \f$, the conductivity in the porous media
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* would be \f$ \kappa = (\rm McMillan) \kappa_0 \f$.
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*/
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virtual
doublereal
McMillanFactor
(doublereal porosity);
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protected
:
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//! Bruggeman exponent: power to which the tortuosity depends on the volume fraction
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doublereal
expBrug_
;
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};
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}
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#endif
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