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STABILITY AND MOTION ANALYSIS
OF THE VAIONT SLIDE
Oldrich Hungr
University of British Columbia, Canada
(ohungr@eos.ubc.ca)
Old technology: Method of Slices

General method:
1) Work out the equilibrium of each slice
2) Calculate the equilibrium of the slice assembly
3) Results depend on assumptions regarding the
interslice force X (mobilization of internal strength)
Data: Selli and Trevisan (1964)
E. Semenza (1960)
Semenza sections plus sliding surface reconstruction
Failure mechanism

(Hendron and Patton, 1984)

Side
shear

Internal shear
BEDDING
C=0, ϕ=12º

ROCK MASS
C=1500, ϕ=34º

1700

10a

5

2

Strength distribution
2D LE analysis
Bishop’s Simplified
Morgenstern-Price
MP Factors of Safety
F=0.44

F=0.66

BEDDING
C=0, ϕ=12º

F=0.43
C=0, ϕ=12º

C=0, ϕ=12º

F=2.28
ROCK MASS
C=1500, ϕ=34º
SARMA Method
(Hoek et al., 1997)

Assumption:
internal strength
fully mobilized

F=0.48 to 0.66

C=0, ϕ=12º

(rock mass
strength)
F=0.70 to 0.86
c=1500 kPa
–if available

ϕ=34º

C=0, ϕ=12º
Bishop's
Simplified

MorgensternPrice

Sarma
c=0

Sarma
c=1500 kPa

#2, x=540

0.43

0.44

0.48

0.66

#5, x=860

0.60

0.66

0.70

0.86

#10a, x=1310

0.42

0.43

No conv.

No conv.

x=1700 (rock)

2.29

2.28

circle

circle

Section

Conclusions – 1) highly asymmetric case,
2) internal strength increases F by 0 to 50%,
depending on cohesion and shape.
3D Analysis, Method of Columns (Hungr et al., 1989)

Ground

Sliding

Simplified column
assembly
Sliding
surface

Volume:
294 million m3
(excluding water)
BEDDING
C=0, ϕ=12º

ROCK MASS
C=1500, ϕ=34º

10º

Distribution of strength. Optimize sliding direction.
Single stage, Volume = 323 million m3 (including water)
Condition

Bishop's
Simplified

Bishop's
Rotated
10ᵒ

MorgensternPrice

No constraint,
uniform strength

0.42

0.47

0.46

Constraint, ϕ=34ᵒ,
c=1500 kPa

1.07

0.92

1.19

Constraint, ϕ=34ᵒ,
c=0

0.60

0.62

0.67

Conclusions – 1) direction optimization is
necessary, 2) Constraint (with cohesion) is needed
2-stage
failure?
(Superchi, 2011)
2-stage failure, Volume = 282 million m3 (including water)
Condition

Bishop's
Simplified

Bishop's
Rotated
10ᵒ

MorgensternPrice

No constraint,
uniform strength

0.46

0.51

0.51 (+9%)

Constraint, ϕ=34ᵒ,
c=1500 kPa

0.82

0.59

0.74 (-38%)

Constraint, ϕ=34ᵒ,
c=0

0.58

0.59

0.61 (-9%)

Conclusion – Partial failure is possible (likely?)
2D dynamic analysis
“Flexible block concept” (Romero and Molina, 1974)
Flexible block
ϕ=23º, ru=0.4

C=0, ϕ=12º

10-sec.
intervals
3D flexible block
model (Aaron, 2013)
Assumptions:
1) Differential movement
of columns is
permitted in the
vertical direction but
not in the horizontal
plane.
2) No shear stress on
column faces
Resultant
forces
DRIVING

RESISTING

ROTATION
Sliding mass displacement:
ϕ=23º on bedding, plus cohesive
constraint, piezometric surface

Original

Real (after slide)

Analysis
2-stage failure
10 m/s

20 m/s
CASSO

Water displacement: V MAX = 10 m/s
CASSO

Water displacement: V MAX = 20 m/s
Conclusions:
1) Landslide was highly asymmetric
2) Internal strength contributed to the stability of typical
sections, to a limited extent
3) The structural constraint on the right flank was
important
4) Cohesion of the intact rock mass played an
important role, but is difficult to quantify
5) The speed of the landslide is not difficult to explain
and was due largely to the loss of cohesion in the
interior and in the side constraint

6) The slide may have been slower than assumed
7) A two-stage failure mechanism is very plausible
REFERENCES
Hendron, A.J. and Patton, F.D. (1985) - The Vaiont Slide, a Geotechnical Analysis Based on New Geologic Observations
of the Failure Surface. Technical Report GL- 85-5, U.S. Army Engineer Waterways Experiment Station, Vicksburg, MS.
I, II.
Hoek, E. (1997) - General 2-dimensional slope stability analysis. Analytical and Computational Methods in Engineering
Rock Mechanics, 95-128, E.T. Brown, Ed., Allen and Unwin, London.
Hungr, O., Salgado, F.M. and Byrne, P.M. (1989) - Evaluation of a three-dimensional method of slope stability analysis.
Canadian Geotechnical Journal, 27: 679-686.
Romero, S.U. and Molina, R. (1974) - Kinematic aspects of the Vaiont Slide. Proceedings, 3rd. Congress
ISRM, Denver, Colorado, 2:865-870.
Selli, R., Trevisan, L., Carloni C.G., Mazzanti, R. and Ciabatti, M. (1964) - La Frana delVajont. Giornale di Geologia. serie
20, XXXII (I), 1–154.
Superchi, L. (2011) - The Vajont rockslide: new techniques and traditional methods to re-evaluate the catastrophic event.
Ph.D. Thesis, University of Padova, 188p.

THANK YOU

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STABILITY ANALYSIS OF THE VAIONT LANDSLIDE

  • 1. STABILITY AND MOTION ANALYSIS OF THE VAIONT SLIDE Oldrich Hungr University of British Columbia, Canada (ohungr@eos.ubc.ca)
  • 2. Old technology: Method of Slices General method: 1) Work out the equilibrium of each slice 2) Calculate the equilibrium of the slice assembly 3) Results depend on assumptions regarding the interslice force X (mobilization of internal strength)
  • 3. Data: Selli and Trevisan (1964)
  • 5. Semenza sections plus sliding surface reconstruction
  • 6.
  • 7. Failure mechanism (Hendron and Patton, 1984) Side shear Internal shear
  • 8. BEDDING C=0, ϕ=12º ROCK MASS C=1500, ϕ=34º 1700 10a 5 2 Strength distribution
  • 9. 2D LE analysis Bishop’s Simplified Morgenstern-Price
  • 10. MP Factors of Safety F=0.44 F=0.66 BEDDING C=0, ϕ=12º F=0.43 C=0, ϕ=12º C=0, ϕ=12º F=2.28 ROCK MASS C=1500, ϕ=34º
  • 11. SARMA Method (Hoek et al., 1997) Assumption: internal strength fully mobilized F=0.48 to 0.66 C=0, ϕ=12º (rock mass strength) F=0.70 to 0.86 c=1500 kPa –if available ϕ=34º C=0, ϕ=12º
  • 12. Bishop's Simplified MorgensternPrice Sarma c=0 Sarma c=1500 kPa #2, x=540 0.43 0.44 0.48 0.66 #5, x=860 0.60 0.66 0.70 0.86 #10a, x=1310 0.42 0.43 No conv. No conv. x=1700 (rock) 2.29 2.28 circle circle Section Conclusions – 1) highly asymmetric case, 2) internal strength increases F by 0 to 50%, depending on cohesion and shape.
  • 13. 3D Analysis, Method of Columns (Hungr et al., 1989) Ground Sliding Simplified column assembly
  • 15. BEDDING C=0, ϕ=12º ROCK MASS C=1500, ϕ=34º 10º Distribution of strength. Optimize sliding direction.
  • 16. Single stage, Volume = 323 million m3 (including water) Condition Bishop's Simplified Bishop's Rotated 10ᵒ MorgensternPrice No constraint, uniform strength 0.42 0.47 0.46 Constraint, ϕ=34ᵒ, c=1500 kPa 1.07 0.92 1.19 Constraint, ϕ=34ᵒ, c=0 0.60 0.62 0.67 Conclusions – 1) direction optimization is necessary, 2) Constraint (with cohesion) is needed
  • 18. 2-stage failure, Volume = 282 million m3 (including water) Condition Bishop's Simplified Bishop's Rotated 10ᵒ MorgensternPrice No constraint, uniform strength 0.46 0.51 0.51 (+9%) Constraint, ϕ=34ᵒ, c=1500 kPa 0.82 0.59 0.74 (-38%) Constraint, ϕ=34ᵒ, c=0 0.58 0.59 0.61 (-9%) Conclusion – Partial failure is possible (likely?)
  • 19. 2D dynamic analysis “Flexible block concept” (Romero and Molina, 1974)
  • 20. Flexible block ϕ=23º, ru=0.4 C=0, ϕ=12º 10-sec. intervals
  • 21. 3D flexible block model (Aaron, 2013) Assumptions: 1) Differential movement of columns is permitted in the vertical direction but not in the horizontal plane. 2) No shear stress on column faces
  • 23. Sliding mass displacement: ϕ=23º on bedding, plus cohesive constraint, piezometric surface Original Real (after slide) Analysis
  • 25.
  • 29. Conclusions: 1) Landslide was highly asymmetric 2) Internal strength contributed to the stability of typical sections, to a limited extent 3) The structural constraint on the right flank was important 4) Cohesion of the intact rock mass played an important role, but is difficult to quantify 5) The speed of the landslide is not difficult to explain and was due largely to the loss of cohesion in the interior and in the side constraint 6) The slide may have been slower than assumed 7) A two-stage failure mechanism is very plausible
  • 30. REFERENCES Hendron, A.J. and Patton, F.D. (1985) - The Vaiont Slide, a Geotechnical Analysis Based on New Geologic Observations of the Failure Surface. Technical Report GL- 85-5, U.S. Army Engineer Waterways Experiment Station, Vicksburg, MS. I, II. Hoek, E. (1997) - General 2-dimensional slope stability analysis. Analytical and Computational Methods in Engineering Rock Mechanics, 95-128, E.T. Brown, Ed., Allen and Unwin, London. Hungr, O., Salgado, F.M. and Byrne, P.M. (1989) - Evaluation of a three-dimensional method of slope stability analysis. Canadian Geotechnical Journal, 27: 679-686. Romero, S.U. and Molina, R. (1974) - Kinematic aspects of the Vaiont Slide. Proceedings, 3rd. Congress ISRM, Denver, Colorado, 2:865-870. Selli, R., Trevisan, L., Carloni C.G., Mazzanti, R. and Ciabatti, M. (1964) - La Frana delVajont. Giornale di Geologia. serie 20, XXXII (I), 1–154. Superchi, L. (2011) - The Vajont rockslide: new techniques and traditional methods to re-evaluate the catastrophic event. Ph.D. Thesis, University of Padova, 188p. THANK YOU