Using the Volume Averaging Technique to Perform the First Change of Scale for Natural Random Porous Media

Author(s):  
D. Bernard
2017 ◽  
Vol 60 (12) ◽  
pp. 1966-1974 ◽  
Author(s):  
ZhiHong Zhang ◽  
ZhaoGang Xu ◽  
ChengShun Xu ◽  
XiuLi Du

2018 ◽  
Vol 97 (4) ◽  
Author(s):  
Marise J. E. Westbroek ◽  
Gil-Arnaud Coche ◽  
Peter R. King ◽  
Dimitri D. Vvedensky

2003 ◽  
Vol 30 (4) ◽  
pp. 271-288 ◽  
Author(s):  
J.J. Telega ◽  
W.R. Bielski

2016 ◽  
Vol 93 (1) ◽  
Author(s):  
C. Jin ◽  
P. A. Langston ◽  
G. E. Pavlovskaya ◽  
M. R. Hall ◽  
S. P. Rigby

2002 ◽  
Vol 11 (4) ◽  
pp. 358-365 ◽  
Author(s):  
Tian Ju-Ping ◽  
Yao Kai-Lun

Author(s):  
Michel Quintard ◽  
Stephen Whitaker

Most porous media of practical importance are hierarchical in nature; that is, they are characterized by more than one length-scale. When these length-scales are disparate, the hierarchical structure can be analyzed by the method of volume averaging (Anderson and Jackson, 1967; Marie, 1967; Slattery, 1967; Whitaker, 1967). In this approach, macroscopic quantities at a given length-scale are defined in terms of a boundary value problem that describes the phenomena at a smaller length-scale, and information is filtered from one scale to another by a series of volume and area integrals. Other methods, such as ensemble averaging (Matheron, 1965; Dagan, 1989) or homogenization theory (Bensoussan et al, 1978; Sanchez-Palencia, 1980), have been used to study hierarchical systems, and developments specific to the problems under consideration in this chapter can be found in Bourgeat (1984), Auriault (1987), Amaziane and Bourgeat (1988), and Sáez et al. (1989). The transformation from the Darcy scale to the large scale is a recurrent problem in reservoir and aquifer engineering. A detailed description of reservoir properties is available through geostatistical analysis (Journel, 1996) on a fine grid with a length-scale much smaller than the scale of the blocks in the reservoir simulator. “Effective” or “pseudo” properties are assigned to the coarse grid blocks, while the forms of the large-scale equations are required to be the same as those used at the Darcy scale (Coats et al., 1967; Hearn, 1971; Jacks et al., 1972; Kyte and Berry, 1975; Dake, 1978; Killough and Foster, 1979; Yokoyama and Lake, 1981; Kortekaas, 1983; Thomas, 1983; Kossack et al., 1990). A detailed discussion of the comparison between the several approaches is beyond the scope of this chapter; however, one can read Bourgeat et al. (1988) for an introductory comparison between the method of volume averaging and the homogenization theory, and Ahmadi et al. (1993) for a discussion of the various classes of pseudofunction theories.


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