SAFOD Stress
How do plate motions stress SAF ?
- Plot borehole breakouts & tensile cracks w/Z downhole
- Correlate with fault strike (orientation)
Borehole shape ∆ with depth
- Cylindrical borehole initially
- Rapidly under lotsa stress
homogeneous stress state equal diff σ1, σ2, σ3
- Shmax disturbs stress field
∴ Resolve stress orientation by msmt crack orientation
Borehole breakouts
= Elongated intervals with non-circular cross sections
2 diametrically opposed elongated zones
whose long axes share common direction
Formation
Spalling of borehole walls
Due to stress concentration in SHmin orientation (min horiz stress)
Cylindrical bore hole --> lens shaped
Tensile
Cracks
Stress reduction occurs in direction SHmax
∴ Tensile fractures form parallel to SHmax
- Tensile cracks from parallel to Shmax
5. Borehole breakouts parallel with SHmin
Orientation SHmax vs Shear Fracture
via hydraulic fracture
If SAF simple shear (theory)
30° between shear fracture & SHmax (σ1)
n.b. opening angle btwn conjugate fractures ~60° thus could be 30° either side of SHmax
Angle observed btwn SAF & SHmax
(from msmt tensile crack orientation vs SAF strike)
some places ~30°
other places - much > 30° (up to 70°)
Implications
high angle
High angle btwn local SAF strike & SHmax
yet SAF constantly creeping...
∴ Decomposed stress vector onto SAF
comprises high normal stress component
V compressive - not ideal for sliding
Measuring SHmax
Orientation tensile fractures
Invert earthquake focal mechanisms
SAFOD Stress Orientation
SHmax trends ~ NE-SW according to equake focal mech
Shmax at depth in pilot hole (0.8-2.2km)
Shmax ~50+/- 17° from SAF strike
Borehole breakouts
SHmax trends ~ NE-SW according to equake focal mech
Evidence
SHmax = σ1
∴ SAF accomodates strike slip motion only
SAF= tanspressive but folds either side accomodate compression
(since both σ1 and σ3 are horizontal for strike slip faults)
In strike slip faults, max principal stress = max horiz stress
Shear failure occurs when:
Shear stress along possible fault overcomes:
- Cohesive strength of rock
- Resistance along that plane (once shear plane formed)
Friction coefficient
Gradient of coulomb criterion in Mohr space
according to coulomb
Descriptor of frictional strength of rock
Ratio of shear & normal forces required for slide
Forces required either to
- initiate slide μs
- maintain continual slide μd
SAF Friction Coefficient
Friction coefficient μ determined for SAF & host rocks
How? Deformation of core rock material retrieved from SAFOD drill hole
via shear tests for different slip velocities
Lockner et al 2011
Fault rocks 3 times weaker vs damage zone rocks
Damage zone
μ ~ 0.6
adjacent to S & Centrally deforming zones
Fault gouge
μ ~ 0.2
actively deforming sedimentary rocks
however damage = accumulating in rock
Host rocks are stronger still