Title: Scaling Issues Regarding The Formation of Fault Zones and Fluid Flow
1Scaling 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
2Objectives
- To understand fault growth processes, their
variety and effects, and how/if they change with
scale - Focus on low porosity, homogeneous, crystalline
rocks
3The 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?
4Approach
- 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
5Alternative Approaches
Fractal/Statistical Laboratory
6Faults as Slipped Joints
7Fault Linkages and Fluid Flow
8Fault Structure Affects Fault Linkage
9Faults from Cooling Joints, Hawaii
10Critique
- 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)
11Fault as a Slipped Dike,Grimsel, Switzerland
12Fault as a Slipped Dike,Grimsel, Switzerland
13Echelon Fractures in a Dike,Sierra Nevada,
California
14Fault as a Slipped Dike, Sierra Nevada,
California
15The Great Dike, Zimbabwe
http//images.jsc.nasa.gov/images/pao/STS54/100654
88.htm
16Independence Dike Swarm, Sierra Nevada,California
http//www.geosci.unc.edu/Petunia/IDS_Web_Site/IDS
_14.html
17Implications
- 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)
18Scaling of Secondary Fracturing Isolated
Faults (Ls/Lf0.01)
19Scaling of Secondary Fracturing Interacting
Faults (Ls/Lflt0.001)
20Conclusions (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
21Conclusions (II)
- Fault linkages affect fluid flow
- Conductivity high at edges of original flaws
- Structural and hydrologic heterogeneity should
increase as original flaw size decreases