Week 9 Flashcards

1
Q

SFL pitch =

A

angle it makes on the fault plane with the strike

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2
Q

Stereonet; “SFL pitching XX N/E/S/W”

A

Count XX in on fault plane FROM N/E/S/W direction

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3
Q

Recap; how to read off stereonet

A

Line up point with horizontal

Count in = dip/plunge

Dash on side of circle in line with point

Rotate to a pole and read

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4
Q

Andersonian faults stereonet; fault planes cross suggest

A

Normal fault and slightly inclined σ2 = slightly oblique (N.B. think about focal mechanism)

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5
Q

Andersonian faults stereonet; scenario - one fault, know reverse/normal/strike-slip, given SLF

A
  • go through normal steps
  • assume acute angle 60’; σ1 = 30’ from SF on σ1σ3 plane (direction determined from fault type)
  • theoretical conjugate fault goes through σ2
  • σ3 90’ from σ1
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6
Q

Is σn +ve or -ve for tensile strength?

A

-ve, where crosses negative x axis in Coulomb-Naiver failure criterion graph

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7
Q

How to determine cohesion for Coulomb-Naiver criterion graph?

A

When σn = 0

y=intercept

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8
Q

Typical values, irrespective of rock type for:

φ
μ
θ

A
φ = 30-40'
μ = 0.58-0.85
θ = 50-60'
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9
Q

What are the two modes of frictional sliding at low confining P

A
  1. Stable sliding (aseismic)

2. Stick-slip (seismogenic)

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10
Q

What causes frictional resistance along fault surface?

A

Interlocking asperities

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11
Q

Amonton’s Law

A

Ease due of sliding due to:

  • orientation
  • frictional properties
  • confining pressure (σ3)

Increase depth = increase σn = forces asperities together = increases slip RESISTANCE

τf = μsσn

μs = coefficient of sliding friction

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12
Q

Byerlee’s law

A

Shallow depths <10km τf = 0.85σn

Greater depths τf = 0.5 + 0.6σn

I.E. FAULTS ARE STRONGER WITH DEPTH

Wide range of values (not so much for water-rich clays)

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13
Q

Stable sliding (aseismic)

A

Constant rate, doesn’t increase stress

In reality = STEADY SLIP HARDENING due to slip zone damage = increase stress

Most common in uppermost crust (<3km), σn lowest

+/ clay-rich fault zone gouges

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14
Q

Stick-slip (seismiogenic)

A

Sudden slip events and periods of no slip

Release = earthquake

Magnitude due to size of stress drop

Dominant > 3km

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15
Q

What does a fault with km-scale offsets indicate?

A

Very large scale number of earthquakes

Throw rates 1-10mm/yr

Different patches slip during different events = complex displacement accumulation

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16
Q

What does it mean if a Mohr circle does not cross Byerlee’s line?

A

New fault fractures will keep being created, no frictional sliding will take place

17
Q

Determining what will happen at a fault; plotting failure envelopes for Coulomb-Naiver failure criterion and Byerlee’s law…

A
  1. Plot σ3
  2. Circle must intersect at failure (trial and error)
  3. If doesn’t cross Byerlee’s = no frictional sliding i.e. new fault fractures created
18
Q

Cataclasites

A

Indicate faulting at great depths within brittle crust

Distributed brittle deformation
‘Ductile’

19
Q

What causes pore fluid pressure (PFP)?

A

Magma

Hydrocarbons

Water

20
Q

What is hydrostatic pressure at equilibrium conditions?

A

= (water density) x g x h

21
Q

What is lithostatic pressure (confining pressure) at equilibrium conditions?

A

= (rock density) x g x h

22
Q

What is PFP at equilibrium conditions?

A

0.4 x lithostatic pressure

  • assuming free movement
  • never greater than lithostatic pressure (WOULD MEAN LIQUEFACTION)
23
Q

What causes overpressure?

A
  1. Restricted fluid movement e.g. compaction

2. Input of a new fluid e.g. diagenesis/metamorphism/hydrocarbon or magma migration

24
Q

Drained triaxial experiments

A

Pore fluid can escape

Increase confining pressure = increase σn

Fluids leak off = constant PFP

Ultimate strength rises with increasing depth

  • same as dry clay
25
Q

Undrained triaxial experiments

A

Fluids can’t escape

Increase confining pressure = increase σn

PFP increases by EQUAL AND OPPOSITE AMOUNT

= ultimate strength is constant and μ = 0

26
Q

Rock mechanical behaviour is affected by…

A

FLUID PRESSURE, I.E. NOT JUST FLUID PRESENCE

27
Q

Effective stress, σ’n =

A

σn - PFP

(since PFP effectively counteracts σn)

Gives τf = S + μσ’n

28
Q

Axial stress =

A

σ1

29
Q

Ultimate strength =

A

Differential stress at failure = σ1-σ3

30
Q

What happens when pore fluid is introduced to a Mohr circle? (Without changing normal pressure)

A

Pore fluid pressure fracturing will occur when intersects with envelope of failure
= slide circle to left

N.B. σ’n = σn-pfp i.e. can calculate PFP

Differential stress remains constant
Mean stress decreased by amount due to PFP

31
Q

What is hydraulic fracturing of ‘fresh’ rock?

A

PFP counteracts normal stresses

Apparent reduction in normal stress = failure