Dynamic bulk and shear moduli due to grain-scale local fluid flow in fluid-saturated cracked poroelastic rocks: Theoretical model

2016 ◽  
Vol 92 ◽  
pp. 28-54 ◽  
Author(s):  
Yongjia Song ◽  
Hengshan Hu ◽  
John W. Rudnicki
2012 ◽  
Vol 51 ◽  
pp. 241-271 ◽  
Author(s):  
George E. Kapellos ◽  
Terpsichori S. Alexiou ◽  
Alkiviades C. Payatakes

1971 ◽  
Vol 14 (7) ◽  
pp. 1129-1130
Author(s):  
E. M. Aristov ◽  
B. A. Pavlovskii ◽  
S. F. Yuras

2014 ◽  
Vol 57 (6) ◽  
pp. 1020-1030 ◽  
Author(s):  
Jing Ba ◽  
Lin Zhang ◽  
WeiTao Sun ◽  
ZhaoBing Hao

1976 ◽  
Vol 27 (1) ◽  
pp. 131-145 ◽  
Author(s):  
P.J. Kennewell ◽  
J.R. Blake

Author(s):  
RW Dwyer

AbstractA theoretical model of the pressure drop across a fibrous cigarette filter is derived. The pressure drop is expressed as a function of the filter dimensions, the fiber tow characteristics, the filter weight, the fluid flow rate, and a filter fiber factor. The fiber factor is affected by the distribution of the fibers within the filter, the relative orientations of the fibers, and their cross-sectional shapes. The model allows one to accurately calculate the influences of these variables on the filter pressure drop. Additionally, it can be used to predict capability curves and select an optimum cellulose acetate tow for a given filter pressure drop.


Geophysics ◽  
2008 ◽  
Vol 73 (5) ◽  
pp. N35-N47 ◽  
Author(s):  
Remy Agersborg ◽  
Tor Arne Johansen ◽  
Morten Jakobsen ◽  
Jeremy Sothcott ◽  
Angus Best

The effects of fluid substitution on P- and S-wave velocities in carbonates of complex texture are still not understood fully. The often-used Gassmann equation gives ambiguous results when compared with ultrasonic velocity data. We present theoretical modeling of velocity and attenuation measurements obtained at a frequency of [Formula: see text] for six carbonate samples composed of calcite and saturated with air, brine, and kerosene. Although porosities (2%–14%) and permeabilities [Formula: see text] are relatively low, velocity variations are large. Differences between the highest and lowest P- and S-wave velocities are about 18% and 27% for brine-saturated samples at 60 and [Formula: see text] effective pressure, respectively. S-wave velocities are measured for two orthogonal polarizations; for four of six samples, anisotropy is revealed. TheGassmann model underpredicts fluid-substitution effects by [Formula: see text] for three samples and by as much as 5% for the rest of the six samples. Moreover, when dried, they also show decreasing attenuation with increasing confining pressure. To model this behavior, we examine a pore model made of two pore systems: one constitutes the main and drainable porosity, and the other is made of undrained cracklike pores that can be associated with grain-to-grain contacts. In addition, these dried rock samples are modeled to contain a fluid-filled-pore system of grain-to-grain contacts, potentially causing local fluid flow and attenuation. For the theoretical model, we use an inclusion model based on the [Formula: see text]-matrix approach, which also considers effects of pore texture and geometry, and pore fluid, global- and local-fluid flow. By using a dual-pore system, we establish a realistic physical model consistently describing the measured data.


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