ANALYSIS OF SLOPES, EARTH RETAINING
STRUCTURES AND UNDERGROUND STRUCTURES
CENG 6208
ARGAW.A (PHD)
36
37
38
39
FINITE SLOPES: PLANE FAILURE
SURFACE
 Translational Block Slides along single
plane of weakness or geological interface
 F = c’L + (W cosθ − uL) tanφ’ / W sinθ + Fw
BLOCK SLIDES
Limit Equilibrium: 1) Assume some circular (or other shape) failu
2) Calculate driving forces (moment about O)
3) Calculate resisting forces (moment about O
BASIC ANALYSIS APPROACH FOR
ROTATIONAL FAILURE SURFACE
Issues:
• Where is the center of mass?
• How does resistance vary along surface?
• How does normal stress vary along surface?
• Water table and seepage forces?
• Soil layering?
• More complex geometry?
METHOD OF SLICES (GENERAL)
• Assume some failure surface
• Discretize failure surface into smaller elements (slices)
• Bottom of each slice passes through one type of material
• Curved bottom of each slice approximated as chord
• More slices = more refined solution
• 10-40 slices typically sufficient (less for hand solutions)
• Calculate factor of safety for each slice (strength/stress) and overall factor of safety
• Find lowest FS for different failure surfaces
Side forces make the problem statically indeterminant
SLOPE ANALYSIS METHODS:
ROTATIONAL FAILURE SURFACE
“OMS”
“Modified Bishop’s”
FINITE SLOPES: CIRCULAR FAILURE
SURFACE
 Rotational Slides - Method of Slices
 Applies to slopes containing cohesive soils
 Ordinary Method of Slices (Fellenius’ Method)
 Bishop’s Simplified Method
 Spenser’s Method
ORDINARY METHOD OF SLICES
 Assumes that resultant of side forces on each
slice are collinear and act parallel to failure
surface and therefore cancel each other
 F = Σ[cn ln + (Wn cosαn - un ln) tanφn] / ΣWn sinαn
 Undrained analysis: F = Σ[cn ln] / ΣWn sinαn
SIDE FORCES IN ORDINARY METHOD OF
SLICES
BISHOP’S SIMPLIFIED METHOD
 Assumes that resultant of side forces on each slice
act in horizontal direction and therefore vertical
side force components cancel each other
 F = Σ[cn bn + (Wn - un bn) tanφn](1/mα) / ΣWn sinαn
 mα = cosαn + (sinαn tanαn)/F
 Undrained analysis: F = Σ[cn ln] / ΣWn sinαn
CHART FOR Mα
SIDE FORCES IN
BISHOP’S METHOD
SPENCER’S METHOD
 Assumes that the point of application of
resultant of side forces on each slice is at mid-
height of each slice but no assumption is made
regarding inclination of resultants; inclination is
determined as part of the solution
 This method is more exact than Bishop’s
FINITE SLOPES: NONCIRCULAR FAILURE
SURFACE
 Wedge Method
 Janbu’s Simplified Method
 Morgenstern-Bishop Method
WEDGE METHOD
 Failure surface consists of two or more planes
and applicable to slope containing several
planes of interfaces and weak layers
 Force equilibrium is satisfied
 Assumes that resultant of side forces on each
slice either acts horizontally or at varying
angles from horizontal (typically up to 15o)
WEDGE METHOD
Layer B
Layer A
4
3
2
1
φm
θ
WEDGE ANALYSIS
Equilibrium of Forces in
each slice is
considered to adjust
the inter-slice forces
and balance them
resulting in a correct
solution.
JANBU’S SIMPLIFIED METHOD
 A method of slices applicable to circular and
noncircular failure surfaces
 F = fo Σ{[cn bn + (Wn - un bn) tanφn](1/ cosαnmα)}
/ ΣWn tanαn
 fo is a correction factor that varies with depth to
length ratio of sliding mass and type of soil
(φ = 0, c, φ or c = 0)
Fa cto r, f
o
R a tio, d /L
φ = 0
c, φ so il
c = 0
L
d
MORGENSTERN-BISHOP METHOD
 No assumption is made regarding inclination or
point of application of resultants and these are
determined as part of the solution
 Requires computers for solving the basic
equation
 Exact but not practical
MORGENSTERN RAPID DRAWN CONDITION
GEOSYENTHITICS
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slope stability geotechnical engineering.pdf
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slope stability geotechnical engineering.pdf
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slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf
slope stability geotechnical engineering.pdf

slope stability geotechnical engineering.pdf

  • 1.
    ANALYSIS OF SLOPES,EARTH RETAINING STRUCTURES AND UNDERGROUND STRUCTURES CENG 6208 ARGAW.A (PHD)
  • 36.
  • 37.
  • 38.
  • 39.
  • 52.
    FINITE SLOPES: PLANEFAILURE SURFACE  Translational Block Slides along single plane of weakness or geological interface  F = c’L + (W cosθ − uL) tanφ’ / W sinθ + Fw
  • 53.
  • 54.
    Limit Equilibrium: 1)Assume some circular (or other shape) failu 2) Calculate driving forces (moment about O) 3) Calculate resisting forces (moment about O BASIC ANALYSIS APPROACH FOR ROTATIONAL FAILURE SURFACE Issues: • Where is the center of mass? • How does resistance vary along surface? • How does normal stress vary along surface? • Water table and seepage forces? • Soil layering? • More complex geometry?
  • 55.
    METHOD OF SLICES(GENERAL) • Assume some failure surface • Discretize failure surface into smaller elements (slices) • Bottom of each slice passes through one type of material • Curved bottom of each slice approximated as chord • More slices = more refined solution • 10-40 slices typically sufficient (less for hand solutions) • Calculate factor of safety for each slice (strength/stress) and overall factor of safety • Find lowest FS for different failure surfaces Side forces make the problem statically indeterminant
  • 56.
    SLOPE ANALYSIS METHODS: ROTATIONALFAILURE SURFACE “OMS” “Modified Bishop’s”
  • 57.
    FINITE SLOPES: CIRCULARFAILURE SURFACE  Rotational Slides - Method of Slices  Applies to slopes containing cohesive soils  Ordinary Method of Slices (Fellenius’ Method)  Bishop’s Simplified Method  Spenser’s Method
  • 61.
    ORDINARY METHOD OFSLICES  Assumes that resultant of side forces on each slice are collinear and act parallel to failure surface and therefore cancel each other  F = Σ[cn ln + (Wn cosαn - un ln) tanφn] / ΣWn sinαn  Undrained analysis: F = Σ[cn ln] / ΣWn sinαn
  • 62.
    SIDE FORCES INORDINARY METHOD OF SLICES
  • 63.
    BISHOP’S SIMPLIFIED METHOD Assumes that resultant of side forces on each slice act in horizontal direction and therefore vertical side force components cancel each other  F = Σ[cn bn + (Wn - un bn) tanφn](1/mα) / ΣWn sinαn  mα = cosαn + (sinαn tanαn)/F  Undrained analysis: F = Σ[cn ln] / ΣWn sinαn
  • 64.
  • 65.
  • 66.
    SPENCER’S METHOD  Assumesthat the point of application of resultant of side forces on each slice is at mid- height of each slice but no assumption is made regarding inclination of resultants; inclination is determined as part of the solution  This method is more exact than Bishop’s
  • 70.
    FINITE SLOPES: NONCIRCULARFAILURE SURFACE  Wedge Method  Janbu’s Simplified Method  Morgenstern-Bishop Method
  • 71.
    WEDGE METHOD  Failuresurface consists of two or more planes and applicable to slope containing several planes of interfaces and weak layers  Force equilibrium is satisfied  Assumes that resultant of side forces on each slice either acts horizontally or at varying angles from horizontal (typically up to 15o)
  • 72.
  • 73.
    WEDGE ANALYSIS Equilibrium ofForces in each slice is considered to adjust the inter-slice forces and balance them resulting in a correct solution.
  • 74.
    JANBU’S SIMPLIFIED METHOD A method of slices applicable to circular and noncircular failure surfaces  F = fo Σ{[cn bn + (Wn - un bn) tanφn](1/ cosαnmα)} / ΣWn tanαn  fo is a correction factor that varies with depth to length ratio of sliding mass and type of soil (φ = 0, c, φ or c = 0)
  • 75.
    Fa cto r,f o R a tio, d /L φ = 0 c, φ so il c = 0 L d
  • 76.
    MORGENSTERN-BISHOP METHOD  Noassumption is made regarding inclination or point of application of resultants and these are determined as part of the solution  Requires computers for solving the basic equation  Exact but not practical
  • 83.
  • 88.