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258 Rouzbeh G. Moghanloo et al.
tubes. The rock permeability is then related to porosity (ϕ), tortuosity
(τ), and hydraulic pore radius (r h ) as follows:
r φ
2
k 5 h ; (6.5)
c τ
When effective hydraulic pore radius, r h is substituted by the surface
area per unit of grain volume ðS gv Þ, Eq. (6.5) can be rewritten as:
2
1 φ 1 φ
k 5 ; (6.6)
c τ S gv 12φ
6.5.1 Permeability reduction: effect of surface deposition and
pore plugging
Asphaltene deposition onto a rock surface may reduce porosity and per-
meability. Wang and Civan (2001) proposed that the instantaneous local
porosity due to deposition can be calculated from the difference between
the initial porosity, φ , and the fraction of asphaltene deposits, ε:
i
φ 5 φ 2 ε (6.7)
i
Further assuming that 1 2 φ 1 and considering constant tortuosity,
Eq. (6.6) can be modified to estimate permeability change as a function
of porosity (Civan, 2001; Kord et al., 2012):
3
k φ
5 ; (6.8)
k i φ i
However, connectivity loss (pore connectivity) has not been consid-
ered in Eq. (6.8) and permeability reduction is only attributed to pore
volume reduction.
6.5.2 Plugging and nonplugging parallel pathways model
Gruesbeck and Collins (1982) proposed a permeability model based on
porous media consisting of plugging and nonplugging parallel pathways.
Pores with relatively large diameter are considered “non-plugging” path-
ways where permeability reduction is only occurring due to surface depo-
sition of particles and thus pore volume shrinkage. The flow paths that
are tortuous and have diameter relatively close to particle size are consid-
ered “plugging pathways.” In the plugging pathways, pore throats will be
blocked through retainment of particles that will potentially lead to severe