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Scaling Issues Regarding The Formation of Fault Zones and Fluid Flow

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Title: Scaling Issues Regarding The Formation of Fault Zones and Fluid Flow


1
Scaling Issues Regarding The Formation of Fault
Zones and Fluid Flow
  • Stephen J. Martel
  • University of Hawaii
  • Matthew dAlessio
  • University of California
  • Sponsored by U.S. Department of Energy

2
Objectives
  • To understand fault growth processes, their
    variety and effects, and how/if they change with
    scale
  • Focus on low porosity, homogeneous, crystalline
    rocks

3
The Problem of Fault Formation
Brace Bombolakis (1963)
  • Scholz (1990)
  • we are still left with the difficulty
    concerning the inability of shear cracks to
    propagate within their own planes. How, then, do
    faults form and grow to their often great
    lengths?

4
Approach
  • To investigate the faulting process by field
    observations and mechanical analyses
  • To infer how the fracture connectivity develops
    and where the large aperture (high conductivity)
    fractures are likely to be

5
Alternative Approaches
Fractal/Statistical Laboratory
6
Faults as Slipped Joints
7
Fault Linkages and Fluid Flow
8
Fault Structure Affects Fault Linkage
9
Faults from Cooling Joints, Hawaii
10
Critique
  • Several field studies have documented cases in
    which faults formed by the linking together of
    joints These cases, however, do not provide a
    satisfactory general explanation for fault
    formation. If this were always the mechanism of
    fault initiation, every case of faulting would
    have to be preceded by an early stress field that
    has an appropriate orientation to form the
    tensile fractures later reactivated in shear
    Furthermore, in these examples, the length of the
    reactivated joints is limited for general
    applicability the initial tensile fractures would
    have to be persistent enough to form the long
    fault systems observed. (Scholz, 1990)

11
Fault as a Slipped Dike,Grimsel, Switzerland
12
Fault as a Slipped Dike,Grimsel, Switzerland
13
Echelon Fractures in a Dike,Sierra Nevada,
California
14
Fault as a Slipped Dike, Sierra Nevada,
California
15
The Great Dike, Zimbabwe
http//images.jsc.nasa.gov/images/pao/STS54/100654
88.htm
16
Independence Dike Swarm, Sierra Nevada,California
http//www.geosci.unc.edu/Petunia/IDS_Web_Site/IDS
_14.html
17
Implications
  • Mode I can and does precede mode II over a broad
    range of scale
  • Structural hydrologic heterogeneity increase
    as flaw size decreases (2-D representation of
    3-D mechanical process)

18
Scaling of Secondary Fracturing Isolated
Faults (Ls/Lf0.01)
19
Scaling of Secondary Fracturing Interacting
Faults (Ls/Lflt0.001)
20
Conclusions (I)
  • Even in homogeneous rocks, pre-existing
    heterogeneities control fault growth
  • Heterogeneities vary with scale and location
  • The distribution of flaws affect how they
    interact and link
  • Although simple scaling rules might capture the
    gross behavior of faults, by themselves they can
    not capture the rich variety of structure and
    processes that occur along natural faults and
    that effect fluid flow

21
Conclusions (II)
  • Fault linkages affect fluid flow
  • Conductivity high at edges of original flaws
  • Structural and hydrologic heterogeneity should
    increase as original flaw size decreases
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