Ali and Islam (1997, 1998) considered only asphaltene deposition and resorted to a simplified, single phase formation damage modeling approach according to Gruesbeck and Collins (1982). Here, their model is presented in a manner consistent with the rest of the presentation of this article. Also, a few missing equations are supplied. Note that this model applies for undersaturated oils. The rate of deposition in the plugging paths is given by:



The deposition in the nonplugging paths is expressed by:


The fluid flux in the plugging pathways is given by:


Note that Ali and Islam (1997, 1998) used the original Gruesbeck and Collins (1982) equation, which misses the fp and fnp terms in Eq. 14-48 instead of the corrected Eq. 14-48 given independently by Civan (1992) and Schechter (1992). The flow in the nonplugging pathways is given by:

Following Gruesbeck and Collins (1982), Ali and Islam (1997) assumed fp and fnp as some characteristic values of the porous medium and determined them to match the model predictions to experimental data. The permeability impairments in the plugging and nonplugging pathways were represented by the Gruesbeck and Collins (1982) empirical expressions, given, respectively, by:



where Kpo and Knpo denote the permeabilities of the plugging and nonplugging pathways before damage, and aand β are some adjustable constants. Ali and Islam (1997) assumed the same concentrations in the plugging and nonplugging pathways. Thus, the mass balance of the suspended particles of asphaltene in the flowing fluid can be expressed as (Civan, 1995, 1996):


In laboratory core tests, the mass rate of phase L added per unit volume of phase L is zero:


The mass rate of asphaltene particles added to phase L is given by:


where Ԑp and Ԑeap denote the retention by filtration and adsorption, respectively. The formulation by Ali and Islam (1997) implies that they expressed the dispersion coefficient as a linear function of the interstitial velocity of the fluid:


where A, is an empirically determined coefficient and VL is the interstitial velocity, given by:



Assuming a constant rate injection of oil into a core plug and constant oil density and applying Eqs. 14-54 through 57, Eq. 14-53 can be written as:


It can be shown that Eq. 14-58 can be reformulated in the form given by Ali and Islam (1997). However, the last term in their equation appears to probably have a typographical error, because o in their equation should be replaced by 3a/3r The same error has been repeated by Ali and Islam (1998). The initial and boundary conditions for Eq. 14-58 are given by:


Ali and Islam (1998) obtained the results presented in Figures 14-48 through 14-50.


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