Contents preface (VII) introduction 1—37


Wedge (or Sliding Block) Method



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15.4.6.2. Wedge (or Sliding Block) Method
This method is used when the slip surface can be approximated by two or three straight lines. Such a situation arises when the slope is underlain by a strong stratum such as rock or there is a weak layer included within or beneath the slope. In such circumstances, an accurate stability analysis can be carried out by dividing the trial sliding mass into two or three blocks of soil and examining the equilibrium of each block. The upper block (or wedge) is called the driving (or active) block and the lower block is called the resisting (or passive) block. In a three-wedge system, the central block is called the sliding block (Fig. 15.30).





EMBANKMENT DAMS










529







Active

Central

Passive










wedge

block

wedge










a

Assumed failure













c













W1

surface










Foundation

PA

W2

W3







e

f







b




d

PP
















(a) Dam on weak

Weak layer (Soft clay or silt or fine







foundation

sand with high pore pressure)










Driving

Resisting













wedge

wedge
















Assumed failure







surface







Core




(b) Dam on strong

Shell of strong granular




material (sand, gravel or rock)




foundation











Fig. 15.30 Conditions for applicability of wedge analysis
The factor of safety can be estimated by any of the methods discussed earlier. Alternatively, assuming that the active and passive wedges are at failure and that the total forces on the vertical planes (bc and de) are horizontal, one can estimate the factor of safety as the ratio of the force P1 available on bd to resist the movement of the central block and the unbalanced force, PAPP . This means,


F =

Cbd + ( W2

Ubd ) tan φ ′ bd

(15.34)




PA PP













where, the subscript bd is used for the plane bd and the subscript 2 is for the central block.
Example 15.5 Determine the factor of safety for the slip surface shown in Fig. 15.31 for sudden drawdown condition with the following properties of the embankment material:

1


2

2

1

3




4

5




6

8 7





Fig. 15.31 Slip surface for Example 15.5





530

IRRIGATION AND WATER RESOURCES ENGINEERING

Saturated weight

= 21.0 kN/m3

Submerged weight

= 11.0 kN/m3

Cohesion

= 24.5 kN/m2

Angle of internal friction, φ′

= 35°

Angle α, arc length, and area of different slices are given in the first four columns of Table 15.3.


Solution: Since pore pressures are not known, the driving force (T-component) and the resisting force ( N-component) are calculated using saturated and submerged weights, respectively, and are shown in Table 15.3.
Table 15.3 Data and solution for Example 15.4














T-Component

N-Component




Slice

α (degrees)

Arc length

Area of
















Weight, W

W sin α

Weight, W

W cos α










(metres)

slice (m2)










(kN/m)

(kN/m)

(kN/m)

(kN/m)














































1

54.5

6.70

12.26

257.46

209.60

134.86

78.31




2

41

3.80

19.51

409.71

268.79

214.61

161.97




3

31

3.50

21.37

448.77

231.13

235.07

201.49




4

22

3.35

20.90

438.90

164.42

229.90

213.16




5

13

3.05

19.97

419.37

94.34

219.67

214.04




6

5

3.05

16.72

351.12

30.60

183.92

183.22




7

– 3.5

3.05

12.08

253.68

– 15.49

132.88

132.63




8

– 13

4.30

6.69

140.49

– 31.60

73.59

71.70





































30.80







951.79




1256.52






























Using Eq. (15.33)


Factor of Safety = 30.80 × 24.5 + 1256.52 tan 35° = 1.72 95179.
15.4.7. Seismic Considerations in Stability Analysis
Seismic forces reduce the margin of safety of an embankment dam. Therefore, when an embankment dam is located in a seismic region, the stability analysis must also consider earthquake forces. During an earthquake, the ground surface oscillates randomly in different directions. This motion can be represented by horizontal and vertical components. A rigid structure is expected to follow the oscillations of its base in the absence of relative deformation from the base of the structure to its top. The amplitude of the oscillations and the acceleration vary along the height of the structure. An earth dam should be treated as a flexible structure for determining dynamic pressure due to earthquake. However, a simple method to account for earthquake forces in the design of structures is based on seismic coefficients. In this method, basic seismic coefficients or earthquake acceleration coefficients are used. The seismic coefficient is defined as the ratio of earthquake acceleration in a particular direction to the gravitational acceleration. If αh is the horizontal earthquake acceleration coefficient then the additional inertial force of the soil mass (of the slice under consideration) is taken as αhW in the horizontal direction. Obviously, a force equal to αhW cos α is added to the tangential forces and αhW sin α



EMBANKMENT DAMS

531

is deducted from the forces acting in the normal direction. The factor of safety, therefore, becomes




F =

Σ C + Σ ( NU − α hW sin α ) tan φ′

(15.35)




Σ (W sin α + α hW cos α)













This simple way of accounting the seismic effects in the stability analysis is based on the pseudostatic concept in which the dynamic effects of an earthquake are replaced by a static force, and in which limit equilibrium is maintained (6).

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