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MohrCoulomb failure

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s1 is the maximum principal stress direction, s2 is the intermediate principal ... Lithostatic stress as static stress generated by mass of overlying rocks ... – PowerPoint PPT presentation

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Title: MohrCoulomb failure


1
Mohr-Coulomb failure
Goal To understand relationship between stress,
brittle failure, and frictional faulting and to
use this relationship to predict rock behavior
2
Stress review
  • Stress Force/Area
  • 3 principal vectors s1, s2, and s3 at right
    angles to each other
  • s1 s2 s3
  • s1 is the maximum principal stress direction, s2
    is the intermediate principal stress direction,
    and s3 is the minimum principal stress direction

3
We also define
  • Static stress as s1 s2 s3
  • Lithostatic stress as static stress generated by
    mass of overlying rocks
  • Differential stress (sd) as (s1 - s3)
  • Confining pressure as s2 s3 for the conditions
    s1 gt s2 s3

4
Shear stress and normal stress
  • For any plane in a stress field defined by s1,
    s2, and s3 with strike parallel with s2

s1
?
s3
s3
s1
5
  • The stress is resolved into 2 components
  • Shear stress (ss), acting parallel with the plane
  • Normal stress (sn), acting perpendicular to the
    plane

s1
sn
?
ss
ss
s3
s3
sn
s1
6
  • Stress components are related by
  • ss ½(s1 - s3)sin(2?)
  • sn ½(s1 s3) - ½(s1 - s3)cos(2?)
  • where ? angle between plane and s1

s1
sn
?
ss
ss
s3
s3
sn
s1
7
Mohr diagram for stress
  • Relationship between s1, s3, ss, and sn is
    plotted graphically in Cartesian coordinates

ss
sn
8
  • Mohr circle for stress circle with diameter sd
    plotted on mohr diagram
  • Center on the sn-axis at point ½(s1 s3)

ss
sn
s1
s3
½(s1 s3)
9
Finding ss, and sn
  • Can use a Mohr circle to find ss, and sn for any
    plane

ss
sn
s1
s3
10
  • Plot a line from center to edge of circle at
    angle 2?-clockwise from sn-axis

ss
2?
sn
s1
s3
11
  • X- and y-coordinates of intersection of line and
    circle define ss and sn for the plane

(ss, sn) of plane
ss
sn
s1
s3
12
Coulombs failure criterion
  • Every homogeneous material has a characteristic
    failure envelope for brittle shear fracturing
  • Combinations of ss and sn outside of the envelope
    result in fracture

13
Determining failure envelope
  • Experimental rock deformation

Holger Stunitz in the lab at Basel University
14
The Coulomb envelope
ss
Shear Fracture
Stable
2?
Tensile Fracture
sn
s1
s3
Stable
Shear Fracture
15
Coulomb law of failure
sc s0 tan(f)sn
ss
f
s0
sn
16
sc s0 tan(f)sn
  • Formula defines shear stress under which rocks
    will fracture
  • sc critical shear stress ss at failure
  • s0 cohesive strength ss when sn 0
  • f angle of internal friction f 90 - 2?

17
  • For most rocks, angle of internal friction 30
  • Therefore, ? at failure is also 30
  • ss is greatest when ? 45

18
Failure envelopes for different rocks
19
Slip on pre-existing fractures
  • Pre-existing fractures have no cohesive strength,
    s0 0
  • Failure envelopes for pre-existing fractures
    derived experimentally

20
Envelope of sliding friction
ss
ff angle of sliding friction
sn
21
Byerlees law
  • Describes frictional sliding envelope
  • sc tan(ff)sn
  • ff 40 for low confining pressures and 35
    for high confining pressures

22
Byerlees law for different rock types
23
Effect of pore-fluid pressure
  • Pore fluid pressure (Pf) effectively lowers the
    stress in all directions
  • The effective stresses (s1eff, s2eff, and s3eff)
    principal stresses - Pf
  • s1eff s1 - Pf s2eff s2 - Pf s3eff
    s3 - Pf

24
Stable stress conditions
ss
s1
sn
s3
25
Increase in pore fluid pressure can drive
faulting!!
ss
s1eff
s1
sn
s3
s3eff
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