Experimental and Numerical Investigations of Fluid Flow for Natural Single Rock Fractures
Abstract (Summary)
To quantify the roughness of natural rock fracture surfaces, a two dimensional
version of the modified divider method was adopted. The parameter Dr2d×Cx was found
to be suitable to quantify the roughness of natural rock fractures. In addition to the mean
aperture, a modified 3D box counting method was used to quantify aperture distributions
of the same fractures. The modified 3D box counting method produced fractal
dimensions in the range 2.3104 to 2.5661.
The following new functional relations were developed for aperture parameters: (a)
power-functionally decreasing mean aperture with increasing normal stress, (b) powerfunctionally
decreasing 3D box fractal dimension with increasing normal stress, (c)
linearly increasing mean aperture with increasing 3D box fractal dimension, (d) linearly
decreasing mean aperture with increasing fracture closure, and (e) linearly decreasing 3D
box fractal dimension with increasing fracture closure.
Fluid flow through nine natural single rock fractures was measured at different
normal stresses. The flow calculated for three out of the nine fractures according to
sample scale cubic law using mean apertures overestimated the experimental flow by 2.2
~ 235.0 times within a normal stress range of 0 ~ 8 MPa. The elementally applied cubic
law (EACL) through a finite element model (FEM) also overestimated the experimental
flow by 1.9 ~ 111.7 times within the same normal stress range. As the normal stress
applied on a natural rock fracture increases, the overestimation increases due to
increasing contact areas and increasing tortuous behavior of flow. These findings clearly
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show the inapplicability of the cubic law to estimate flow through natural rock fractures
especially under high normal stresses. New hyperbolic functions were developed to
relate mean aperture to the power n to applied normal stress at both the sample and finite
element scales.
The following new functional relations were developed between fluid flow rate and
the aperture parameters: (a) power-functionally increasing flow rate per unit head with
increasing mean aperture, (b) exponentially decreasing flow rate per unit head with
increasing fracture closure, and (c) power-functionally increasing flow rate per unit head
with increasing 3D box fractal dimension.
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Bibliographical Information:
Advisor:
School:The University of Arizona
School Location:USA - Arizona
Source Type:Master's Thesis
Keywords:
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