Chapter 2: Failure Mechanics
Transcript of Chapter 2: Failure Mechanics
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Chapter 2: Failure Mechanics
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2.1. Basic Concepts
This chapter discusses the most
elementary and well known models for rock failure.
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2.1.1. Strength and related concepts
The stress level at which a rock typically
fails is commonly called the strength of the rock.
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2.1.1. Strength and related concepts
a uniaxial or triaxial test.
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Principle sketch of stress versus deformation in a
uniaxial compression test.
2.1.1. Strength and related concepts
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Several important concepts are defined in the figure:
• Elastic region
• Yield point
• Uniaxial compressive strength
• Ductile region
• Brittle region
2.1.1. Strength and related concepts
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Triaxial testing
2.1.1. Strength and related concepts
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uniaxial and triaxial tests
2.1.1. Strength and related concepts
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2.1.2. The failure surface
1 2
3 ≥ ≥
The failure surface
may be described by
the equation:
1 2 3, , 0f
(2.1)
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2.2. Tensile Failure
Tensile failure occurs when the effective tensile stress
across some plane in the sample exceeds a critical limit.
This limit is called the tensile strength, it is given the
symbol T0, and has the same unit as stress.
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2.2. Tensile Failure
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2.2. Tensile Failure
The failure criterion, which specifies the stress condition
for which tensile failure will occur, and identifies the
location of the failure surface in principal stress space, is
given as:
0T (2.2)
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2.2. Tensile Failure
For isotropic rocks, the conditions for tensile failure
will always be fulfilled first for the lowest principal
stress, so that the tensile failure criterion becomes
3 0T (2.3)
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2.3. Shear Failure
max f
This assumption is called
Mohr’s hypothesis.
(2.4)
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Fig. 2.7: Failure line, as specified by Eq(2.4)in the shear
stress–normal stress diagram. Also shown are the Mohr
circles connecting the principal stresses 1
2 3
2.3. Shear Failure
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Pure shear failure, as defined by Mohr’s hypothesis,
depends only on the minimum and maximum principal
stresses and not on the intermediate stress.
2.3. Shear Failure
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2.3. Shear Failure
By choosing specific forms of the function f(σ′), various
criteria for shear failure are obtained. The simplest
possible choice is a constant. The resulting criterion is
called the Tresca criterion. The criterion simply states that
the material will yield when a critical level of shear stress
is reached:
S0 is the inherent shear strength (also called
cohesion) of the material.
max 1 3 0
1
2S (2.5)
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2.3.1. The Mohr–Coulomb criterion
0S
Assumption : f(σ′) is a linear function of σ′
μ is the coefficient of internal friction.
(2.6)
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The latter term is clearly chosen by analogy with
sliding of a body on a surface, which to the first
approximation is described by Amontons’ law:
2.3.1. The Mohr–Coulomb criterion
(2.7)
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2.3.1. The Mohr–Coulomb criterion
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In the Figure, Mohr’s circle touches the failure
line. The angle is called the angle of internal
friction and is related to the coefficient of internal
friction by
The Tresca criterion can be considered as a
special case of the Mohr–Coulomb criterion, with
υ = 0.
tan
(2.8)
2.3.1. The Mohr–Coulomb criterion
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The attraction
(2.9)
is defined as the distance from the intersection
point to the origin .
2.3.1. The Mohr–Coulomb criterion
0 cotS
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The angle 2β gives the position of the point where
the Mohr’s circle touches the failure line. The shear
stress at this point of contact is
1 3
1sin 2
2
while the normal stress is
1 3 1 3
1 1cos2
2 2
2.3.1. The Mohr–Coulomb criterion
(2.11)
(2.10)
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2.3.1. The Mohr–Coulomb criterion
22
4 2
The allowable range for υ is from 0º to 90º
(2.13)
(2.12)
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Introducing the expressions (2.10)and (2.11) for σ′ and τ
into the failure criterion Eq. (2.6), we find
1 3 0 1 3 1 3
1 1 1sin 2 cos2
2 2 2S
(2.14)
2.3.1. The Mohr–Coulomb criterion
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1 3 0 1 3 1 3
1 1 1cos tan tan sin
2 2 2S
Replacing β and μ by υ, we obtain:
Multiplying with 2 cos υ and rearranging, we find
2 2
1 3 0 1 3cos sin 2 cos sinS
1 0 31 sin 2 cos 1 sinS
1 0 3
1 sin2 cos
1 sinS
2.3.1. The Mohr–Coulomb criterion
(2.15)
(2.16)
(2.17)
(2.18)
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The angle γ in the ( , ) plane is related to by 1
3
1 sintan
1 sin
(2.19)
or
tan 1sin
tan 1
(2.20)
2.3.1. The Mohr–Coulomb criterion
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2.3.1. The Mohr–Coulomb criterion
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An expression for the uniaxial compressive strength
C0 is obtained by putting in Eq. (2.18), giving 3 0
0 0 0
cos2 2 tan
1 sinC S S
(2.21)
2.3.1. The Mohr–Coulomb criterion
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Making use of Eqs. (2.21)and (2.12), we note that
Eq. (2.18) may be writtenin the following simple way:
2
1 0 3 tanC (2.22)
2.3.1. The Mohr–Coulomb criterion
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2.3.2. The Griffith criterion
1 3 0 1 38T 1 33 if 0
3 0T if 1 33 0
The theory is scaled in terms of the uniaxial tensile
strength T0, and the resulting failure criterion can be
written
(2.23)
(2.24)
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The uniaxial compressive strength C0 is given by
Eq. (2.23) as
In τ–σ′-coordinates, the Griffith criterion is given by
only one equation:
0 08C T (2.25)
2
0 04T T (2.26)
2.3.2. The Griffith criterion
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2.3.2. The Griffith criterion
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A result from this modified theory is that the ratio
between uniaxial compressive strength and the tensile
strength is given by
0
20
4
1
C
T
(2.27)
2.3.2. The Griffith criterion
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2.4. Compaction Failure
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In principal stress space, this type of failure is
represented by an ―end cap‖ that closes the
failure surface at high stresses, as seen on Fig.
2.13. An elliptical form is often used for such an
end:
2 2
2 2
1 11
1
q
p p
(2.28)
2.4. Compaction Failure
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2.4. Compaction Failure
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Boutéca et al. (2000) argued that the following simple
form of Eq. (2.28) (obtained by choosing γ = 0 and δ = 1)
may be an acceptable approximation for many rocks:
2 2 2q p (2.29)
2.4. Compaction Failure
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It is to be expected that the critical effective
pressure p* decreases with increasing porosity. From
theoretical considerations, Zhang et al. (1990) derived
the relation
3
2p
(2.30)
2.4. Compaction Failure
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The two cases > and < can be represented
by two lines that are symmetric around the line
as shown in Fig. 2.14.
1 3
1 3
1 3
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2.5.1 Failure Criteria in Three Dimensions
Fig. 2.14
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Fig. 2.15: The Mohr–Coulomb failure surface in principal
stress space. Fig. 2.15
2.5.1 Failure Criteria in Three Dimensions
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Fig. 2.16: Cross-section of the Mohr–Coulomb criterion in a
π-plane. The arrows represent projections of the principal
stress axes onto the plane. The friction angle φ = 30º.
2.5.1 Failure Criteria in Three Dimensions
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Typically, it is found that rocks are stronger
when > > than for the situations
where = or = .
One simple solution is to implement
rotational symmetry for the π-plane cross-
section. This approach has no physical
foundation, however it is mathematically
attractive, and is the basis for some of the most
commonly used criteria shown below.
2.5.2. Criteria depending on the intermediate
principal stress
2 1
3
2 1
3 2
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2.5.2. Criteria depending on the intermediate
principal stress
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One of these criteria is the von Mises criterion, which
can be written
C is a material parameter related to cohesion.
2 2 2 2
1 2 1 3 2 3 C
(2.31)
2.5.2. Criteria depending on the intermediate
principal stress
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2 2 2 2
1 2 1 3 2 3 1 1 2 3 2C C
The corresponding generalization of the Mohr–
Coulomb criterion is the Drucker–Prager criterion. It
can be formulated as
where C1 and C2 are material parameters, related to
internal friction and cohesion.
(2.32)
2.5.2. Criteria depending on the intermediate
principal stress
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2 2 2
1 2 1 3 2 3 0 1 2 324T
ending on the planes
1 0 2 0 3 0, ,T T T
The extended Griffith criterion predicts that the relation
between uniaxial compressive strength and tensile strength
is given by
0 012C T
(2.33)
(2.34)
(2.35)
2.5.2. Criteria depending on the intermediate
principal stress
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A modified version of the empirical failure criterion
was presented by Ewy (1999):
33
3
3 L
I
I
1 1 2 3L L LI S S S
3 1 2 3L L LI S S S (2.38)
(2.37)
(2.36)
2.5.2. Criteria depending on the intermediate
principal stress
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SL is a material parameter related to the cohesion and
the friction angle of the rock:
while ηL is related only to the internal friction:
0
tanL
SS
2 9 7sin4 tan
1 sinL
(2.40)
(2.39)
2.5.2. Criteria depending on the intermediate
principal stress
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2.5.2. Criteria depending on the intermediate
principal stress
π-plane representation
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1 2cos3LJ f f
The radial distance to a point on the failure surface is
given by Eq. (1.50). Defining two general functions f1
and f2 we may thus write a general failure criterion as
(2.41)
2.5.2. Criteria depending on the intermediate
principal stress
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A representation of the modified Lade criterion can
be obtained by expressing
and in terms of σ′, q and . and defining a
new variable x = q/(SL + σ′)
1I 3I
(2.42)
2.5.2. Criteria depending on the intermediate
principal stress
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2
3 3 3
3 cos 3 cos 3 31 ...
3 9 3 27 3
L L L
L L L
2
1 3
3 1 2 cos 31 2cos arccos 1
2cos3 3 3 3
L
L
f
2
1
3Lf S (2.44)
(2.43)
2.5.2. Criteria depending on the intermediate
principal stress
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A general, simple form for f1 may be convenient for
practical purposes. We may for instance choose
1 1 cos3f k k (2.45)
1 3 sin1
2 3 sink
(2.46)
2.5.2. Criteria depending on the intermediate
principal stress
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2 0
1 sin sin2
3 sin 3 sinf C
(2.47)
may be used as a rough approximation for the Mohr–
Coulomb criterion.
By choosing f1 appropriately, it is possible to formulate
the Mohr–Coulomb criterion exactly in terms of the
invariants. The expression
1
1
1 sin3 cos 3sin
3 sinf
(2.48)
2.5.2. Criteria depending on the intermediate
principal stress
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Physical explanations
2.5.2. Criteria depending on the intermediate
principal stress
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2.6. Fluid Effects 2.6.1. Pore pressure
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2.6.2. Partial saturation
moist sand is partially water saturated
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cp nw wep p p
The effects of partial saturation occur whenever the
pore space is filled with at least two immiscible fluids,
like for instance oil and water.
where pwe is the pressure in the wetting fluid, pnw is
the pressure in the non-wetting fluid, and pcp is called
the capillary suction.
(2.50)
2.6.2. Partial saturation
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The capillary suction has some effect on the effective
stresses in the rock, and we may define a generalized
effective stress
nw we cpp S p (2.51)
2.6.2. Partial saturation
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2.6.2. Partial saturation
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2.6.3. Chemical effects
6yield
w
MPaa
If the pore fluid is changed, for instance during drilling
or production, the chemical equilibrium may be disturbed,
and a net dissolution or deposition of minerals may occur.
This may have a strong effect on the rock properties,
typically a reduction in strength of 30–100% is seen in
many rocks due to deterioration of the cement (Broch,
1974). (2.52)
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The q–p′ plot essentially displays the maximum shear
stress versus the mean effective stress. It is based on the
parameter q, usually called the generalized shear stress
and defined as
and the parameter p′ which is identical to the mean
effective stress σ′
2.7. Presentation and Interpretation of Data from
Failure Tests
2 2 2
1 2 2 3 1 3
1
2q
1 2 3
1
3p
(2.54)
(2.53)
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2.7. Presentation and Interpretation of Data from
Failure Tests
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The von Mises criterion
2 21
2q C
the Drucker–Prager criterion
22 2
1 2
13
2q C p C
(2.55)
(2.56)
2.7. Presentation and Interpretation of Data
from Failure Tests
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the modified Lade criterion (Eq. (2.36)—with f1( , ηL)
given by Eq. (2.42); note the similarity with Eq. (2.56):
1 , L Lq f S p
the extended Griffith criterion
2
036q T p
and the compactive yield criterion
2 2 2p q p
(2.57)
(2.59)
(2.58)
2.7. Presentation and Interpretation of Data
from Failure Tests
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2.8. Beyond the Yield Point 2.8.1. Plasticity
The theory of plasticity is based on four major
concepts:
1.Plastic strain
2.A yield criterion.
3.A flow rule.
4. A hardening rule.
e p
ij ij ijd d d
1 2 3, , , 0f
(2.60)
(2.61)
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2.8.1. Plasticity
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p
ij ij kld d h
where λ is a scalar not specified by the flow rule.
Plastic flow
(2.62)
The function of the flow rule is to describe the
development of the plastic strain increments.
The basic assumption concerning plastic flow
dates back to Saint-Venant in the nineteenth
century. It states
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Plastic flow
• The assumption that the plastic strains are
independent of stress increments, is
intuitively understandable in the following
simple example.
0p
kl ij
ij
d (2.63)
p
ij
ij
gd d
(2.64)
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Plastic flow
0p
ij ij
ij
d d
p
ij
ij
fd d
One solution to the problem is Drucker’s (1950)
definition of a stable, work hardening material. Such a
material is defined by a more strict version of Eq. (2.63):
(2.65)
(2.66)
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Associated flow
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Associated flow
1 cospd d
From the figure we see that
3 csinpd d
3 1 tan 0p pd d
(2.67)
(2.68)
(2.69)
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Associated flow
1 1 tanp p
vold d
0p
vold
(2.70)
(2.71)
Eq. (2.16) may be written as:
1 30 1 3
1tan
2cos 4S
(2.72)
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Associated flow
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Associated flow
• It can thus be concluded that the inclination of
the arrow in Fig. 2.26 determines the dilatancy
of the material as follows:
• If the arrow is tilted to the left (υ ≥ 0), the
material is positively dilatant.
• If the arrow is vertical (υ = 0), the material does
not change volume.
• If the arrow is tilted to the right (υ ≤ 0), the
material is negatively dilatant , or contractant .
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Non-associated flow
1 3 1 0 3 1 0 3
1 sin, tan
1 sinf C C
(2.73)
1 3 1 0 3 1 0 3
1 sin, tan
1 sing C C
(2.74)
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Hardening
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Hardening
• There are two common ways to relate κ to the plastic
strain. One way is to assume that κ is a function of the
total plastic strain. This is called strain hardening, and
can be expressed as
p
ijSd (2.75)
where ∫S symbolizes integration over the stress path.
Another way is to relate κ to the total plastic work:
p
ij ijS
d (2.76)
This is called work hardening.
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Hardening
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2.8.2. Soil mechanics
• Voids ratio e is the volume of voids Vvoid relative to
the volume of the solid grains V solid in the material:
• Specific volume υ is the total volume (grains + voids)
divided by the volume of the solid grains, that is
void
solid
Ve
V (2.77)
1solid void
solid
V Ve
V
(2.78)
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2.8.2. Soil mechanics
• The specific volume and the voids ratio are
related to the porosity by
1
1
e
e
(2.79)
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2.8.2. Soil mechanics
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2.8.2. Soil mechanics
Normally consolidated clay:
• No peak stress in the stress–strain diagram, i.e.
the shear stress does not fall below previous
value as the strain increases.
• The sample contracts throughout the loading.
• The loading path in a q–p′-plot curves to the
left, i.e. the pore pressure increases.
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2.8.2. Soil mechanics
Strongly overconsolidated clay:
• A peak is normally observable in the stress–strain
diagram, i.e. at some point the shear stress falls
below previous values as the strain increases.
• The sample contracts initially, then dilates as
failure is approaching.
• The loading path in a q–p′-plot curves to the right
near failure, i.e. the pore pressure decreases
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Normally consolidated clays
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Normally consolidated clays
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Normally consolidated clays
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Overconsolidated clays
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Overconsolidated clays
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2.9.2. The plane of weakness model
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2.9.2. The plane of weakness model
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2.9.2. The plane of weakness model
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2.9.2. The plane of weakness model
• The corresponding failure angle is given as
• Isotropic failure criterion
• Weak plane failure criterion
4 2
ww
(2.80)
0 31 3
cos sin2
1 sin
S
(2.81)
0 3
1 3
cos sin2
sin 2 cos cos2 1 sin
w w w
w w
S
(2.82)
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2.9.3. Fractured rock
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2.9.3. Fractured rock
• Hoek and Brown (1980) derived an empirical failure
criterion for fractured rocks:
• The uniaxial compressive strength of the fractured
rock is given by
2
1 3 0 3 0bm C sC (2.83)
2
0 0fC sC (2.84)
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2.9.3. Fractured rock
0.321
b im m s (2.85)
31 3 0
0
a
bC m sC
where s → 0 and a → 0.65. Note that Eq. (2.86) is
identical to Eq. (2.83) when a = 0.5.
(2.86)
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2.10. Stress History Effects
• 2.10.1. Rate effects and delayed failure
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2.10.2. Fatigue
• Thank you