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8.14 FIXED EARTH-SUPPORT METHOD FOR PENETRATION INTO SANDY SOIL When using the fixed earth support method, we assume that the toe of the pile is restrained from rotating, as shown in Figure 8.31a. In the fixed earth support solution, a simplified method called the equivalent beam solution is generally used to calculate L 3  and, thus, D. The development of the equivalent  beam method is generally attributed to Blum (1931).

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8.14 FIXED EARTH-SUPPORT METHOD FOR

PENETRATION INTO SANDY SOIL 

When using the fixed earth support method, we assume

that the toe of the pile is restrained from rotating, as shown in

Figure 8.31a. In the fixed earth support solution, a simplifiedmethod called the equivalent beam solution is generally used

to calculate L3 and, thus, D. The development of the equivalent

 beam method is generally attributed to Blum (1931).

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FIGURE 8.31  Fixed earth support method for penetration sandy soil

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  In order to understand this method, compare the sheet pile

to a loaded cantilever beam  RSTU , as shown in Figure 8.32.

 Note that the support at T   for the beam is equivalent to theanchor load reaction ( F ) on the sheet pile (Figure 8.31). It can

 be seen that the point S of the beam  RSTU is the inflection

 point of the elastic line of the beam, which is equivalent to

 point I  in Figure 8.31. It the beam is cut at S  and a free support

(reaction  P  s) is provided at that point, the bending momentdiagram for portion STU  of the beam will remain unchanged.

This beam STU   will be equivalent to the section STU   of the

 beam  RSTU . The force  P’  shown in Figure 8.32a at  I will be

equivalent to the reaction P  s on the beam (Figure 8.32).

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FIGURE 8.32 Equivalent cantilever beam concept

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  Following is an approximate procedure for the design of

an anchored sheet-pile wall (Cornfield, 1975). Refer to Figure

8.31.Step 1. Determine L5, which is a function of the soil friction

angle ɸ below the dredge line, from the

following:

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  Step 2. Calculate the span of the equivalent beam as

.

Step 3. Calculate the total load of the span, W. This is the area

of the pressure diagram between O’  and I .

Step 4. Calculate the maximum moment, M max, as WL’ /8.

Step 5. Calculate P  by taking the moment about O’, or

(moment of area ACDJI  about O’ )

Step 6. Calculate D as

Step 7. Calculate the anchor force per unit length, F , by taking

the moment about I , or

(moment of area ACDJI  about I )

(8.87)

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8.11

8.6

8.14

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8.14

8.33

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  Figure 8.33

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8.15 FIELD OBSERVATIONS FOR

ANCHOR SHEET PILE WALLS 

In the preceding sections, large factors of safety wereused for the depth of penetration, D. In most cases,designers use smaller magnitudes of soil friction angle, ɸ’,thereby ensuring a built-in factor of safety for the activeearth pressure. This procedure is followed primarily becauseof the uncertainties involved in predicting the actual earth pressure to which a sheet-pile wall in the field will besubjected. In addition, Casagrande (1973) observed that, ifthe soil behind the sheet-pile wall has grain sizes that are predominantly smaller than those of coarse sand, the active

earth pressure after construction sometimes increases to anat-rest earth-pressure condition. Such an increase causes alarge increase in the anchor force, F. The following two casehistories are given by Casagrande (1973). 

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Bulkhead of Pier C — Long Beach Harbor, California

(1949)

A typical cross section of the Pier C bulkhead of the Long

Beach harbor is shown in Figure 8.34. Except for a rockfill

dike constructed with 3 in (76.2 mm) maximum-size quarry

wastes, the backfill of the sheet-pile wall consisted of fine

sand. Figure 8.35 shows the lateral earth pressure variation ofthe lateral earth pressure between May 17, 1949 and August 6,

1949 at station 27 + 30. The fine sand backfill reached the

design grade on May 24, 1949. The following general

observations are based on figure 8.35.

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1. On May 17 (Figure 8.35), the backfill was several feet below

the design grade. However, the earth pressure was greater on

this date than on may 24. This is probably because of the fact

that, due to lack of lateral yielding of the wall, the earth pressure was closer to at-rest state than the active state.

2. Due to wall yielding on May 24, the earth pressure reached an

active state (Figure 8.35b).

3. Between May 24 and June 3, the anchor resisted furtheryielding and the lateral earth pressure increased to the at-rest

state (8.35c).

4. Figures 8.35d, e, and f show how the flexibility of sheet piles

resulted in a gradual decrease in the lateral earth pressuredistribution on the sheet piles.

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Timber anchor piles:

3 ft on center

Timber piles to:

Support tie rods,

12 ft on centers

Concrete anchor cap

4.5 ft X 4.5 ft

62 ft

(19 m)

Tie rods: 3 in. dia

6 ft on centers + 4

+ 17

7

12

- 10

Figure 8.34  Pier C bulkhead — Long Beach Harbor (after Casagrande 1973) 

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  These observations show that the magnitude of the active earth

 pressure may vary with time and depends greatly on the

flexibility of the sheet piles. Also, the actual variations in the

lateral earth pressure diagram may not be identical to those

used for design.

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Bulkhead — Toledo, Ohio (1961)

A typical cross section of a Toledo bulkhead completed in 1961 is

shown in Figure 8.36. The foundation soil was primarily fine to mediumsand, but the dredge line did cut into highly overconsolidated clay. Figure

8.36 also shows the actual measured values of bending moment along the

sheet-pile wall. Casagrande (1973) used the Rankine active earthpressure

distribution to calculate the maximum bending moment according to the free

earth support method with and without Rowe’s moment reduction.

Design method Maximum predicted

bending moment, M max

Free earth support method 108klp-ft/ft

Free earth support method with Rowe’s moment

reduction

58 klp-ft/ft

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Comparisons of these magnitudes of Mmax with those actually observed show that

the field values are substantially larger. The reason probably is that the backfill

was primarily fine sand and the measured active earth-pressure distribution was

larger than that predicted theoretically.

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8.16 ANCHORS-GENERALSections 8.8 - 8.14 gave an analysis of anchored sheet-pile

walls and discussed how to obtain the force, F , per unit length

of the sheet-pile wall that has to be sustained by the anchors.

The current section covers in more detail the various types of

anchor generally used and the procedures for evaluating their

ultimate holding capacities.

The general types of anchor used in sheet-pile walls are as

follows:

1. Anchor plates and beams (deadman)

2. Tie backs

3. Vertical anchor piles

4. Anchor beams supported by batter (compression and tension)

 piles

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  Anchor plates and beams are generally made of cast

concrete blocks. (See Figure 8.37a.) The anchors are attached

to the sheet pile by tie-rods. A wale is placed at the front or

 back face of a sheet pile for the purpose of convenientlyattaching the tie-rod to the wall. To protect the tie rod from

corrosion, it is generally coated with paint or asphaltic

materials.

In the construction of tie backs, bars or cables are placedin predrilled holes (see Figure 8.37b) with concrete grout

(cables are commonly high-strength, prestressed steel

tendons). Figures 8.37c and 8.37d show a vertical anchor pile

and an anchor beam with batter piles.

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Placement of AnchorsThe resistance offered by anchor plates and beams is derived

 primarily from the passive force of the soil located in front of them.Figure 8.37a, in which AB is the sheet-pile wall , shows the best

location for maximum efficiency of an anchor plate. If the anchor is placed inside wedge ABC, which is the Rankine active zone, itwould not provide any resistance to failure. Alternatively, the anchorcould be placed in zone CFEH. Note that line DFG is the slip linefor the Rankine passive pressure. If part of the passive wedge islocated inside the active wedge ABC, full passive resistance of the

anchor cannot be realized upon failure of the sheet-pile wall.However, if the anchor is placed in zone ICH , the Rankine passivezone in front of the anchor slab or plate is located completelyoutside the Rankine active zone ABC. In this case, full passiveresistance from the anchor can be realized.

Figures 8.37b, 8.37c, and 8.37d also show the proper locationsfor the placement of tiebacks, vertical anchor piles, and anchor

 beams supported by batter piles.

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8.17 HOLDING CAPACITY OF ANCHOR

PLATES AND BEAMS IN SAND

A.   Teng’s Method : Calculation of the UltimateResistance Offered by Anchor Plates and Beams in

Sand

Teng (1962) proposed a method of determining the ultimate

of anchor plates or walls in granular soils located at or near

the ground surface (H/h ≤1.5 to 2 in Figure 8.38) 

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  Equation (8.88) is valid for the plane-strain condition. For

all practical cases, B/h > 5 may be considered to be plane

strain condition.

For B/h < about 5, considering the three dimensionalfailure surface (that is, accounting for the frictional resistance

developed at the two ends of an anchor), Teng (1962) gave the

following relation for the ultimate anchor resistance:

where K 0 = earth pressure cofficient at rest ≈ 0.4. 

(8.91)

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B. Ovesen and Stromann’s Method

Ovesen and Stromann (1972) proposed a semi-empiricalmethod for determining the ultimate resistance of anchors in

sand. Their calculations, made in three steps, are carried out as

follows:

Step 1. Basic Case consideration. Determine the depth of

embedment, H. Assume that the anchor slab has height H

and is continuous (i.e., of anchor slab perpendicular to the

cross), as shown in Figure 8.38, in which the following

notation is used:

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(8.92)

(8.93)

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Figure 8.39  basic case: continuous vertical anchor in granular soil

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Figure 8.40 (a) Variation of Ka (for δ = ɸ)(b) variation of with K  p cos δ with K  p sin δ 

(Based on Ovesen and Stromann, 1972)

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Step 2. Strip case. Determine the actual height of the anchor,

h, to be constructed. If a continous anchor of height h is

 placed in the soil so deep its dept of embedment is H, asshown in figure 8.41, the ultimate resistance per unit

  length is

FIGURE 8.41 Strip case: vertical anchor

(8.94)

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Where

 P ’ us  = ultimate resistance for the strip case

C oτ   = 19 for dense sand and 14 for loose sand

Step 3. Actual Case. In practice, the anchor plates are placed in arow with center-to-center spacing, S’, as shown in Figure8.42a. The ultimate resistance of each anchor, P u ,is

Where Be = quivalent length

The equivalent length is a function of S’, B, H, and h.Figure 8.42b shows a plot of ( Be –  B) ( H + h) against (S –  b)( H + h) for the cases of loose and dense sand. With knownvalues of S’, B, H, the value of B, can be calculated and usedin Eq. (8.95) to obtain P u.

(8.95)

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Figure 8.42

(a) Actual case for row of

anchors; (b) variation of (Be

 – B) (H + h) With (S –  B) / (H+ h) (Based on Ovesen And

Stromann, 1972) 

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C. Empirical Correlation Based on Model Tests 

Ghaly (1997) used the results of 104 laboratory tests, 15

centrifugal model tests, and 9 field tests to propose anempirical correlation for the ultimate resistance of Single

anchors (figure 8.43). The correlation can be written as

Where A = area of the anchor = Bh

Ghaly also used the model test results of Das and Seeley

(1975) to develop aload – displacement relationship for singleanchors. The relationship can be given as 

(8.96)

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