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23 - Deep Foundations

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23 - Deep Foundations

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Source: GEOTECHNICAL ENGINEERING

23 Deep Foundations

23.1 OVERVIEW

23.1.1 Pile-Up
Putting structures on posts is not a new idea, but dates back at least 6000 years, to
a time when the European climate was warming after centuries of cold, drought,
and misery, and lake levels were rising. That was the time of ‘‘Ötzi,’’ the Ice Man
of the Italian Alps, whose discovery set off a crime investigation that must be the
ultimate in cold case files.

Prehistoric builders burned the ends of tree trunks to sharpen them, and probably
wielded rocks to drive the posts into soft ground. Today’s piles are driven with
pile drivers that range from drop hammers to steam or diesel operation.

The most common use of piles is to keep structures from sinking into the ground,
but piles also prevent bridge supports from being undercut by scour during
periods of rapid current and high water. The famous London Bridge—the one
that young children are taught is falling down, thereby fostering an unwarranted
disenchantment with civil engineering—was on wooden piles, and it did not fall
down; it was pushed down by river ice. It then was repaired and lasted for another
550 years. Somebody should write a song about that.

23.1.2 Deep Foundations


Piles are structural columns that extend down into soil. They are either
end-bearing if they extend all of the way to rock or hard soil, or they are friction
piles if they are mainly supported by friction along the sides, although friction
piles also usually develop some end support. Timber piles are driven top down to
take advantage of their taper for increasing friction, and a taper often is
incorporated into concrete piles. Compaction piles are driven into loose sand to
densify it and increase its bearing capacity.
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Deep Foundations 669

Modern piles are wood, steel, concrete, or composite if they are composed of more
than one material. An example of a composite pile is when a wood pile section is
used under a groundwater table where it is preserved by reducing conditions, and is
connected to a concrete section that extends through aerobic surroundings above
the water table.

Whereas piles are driven or can be jacked into the ground, piers are large-diameter
supports that are placed in pre-bored holes. Caissons are large tubes used for
construction below water, as in rivers, and may be pressurized to keep water out.
‘‘Caisson foundation’’ sometimes is applied to bored piers, and piers also are
sometimes called shafts or piles, leading to some deep confusion.

Some types of piles and piers are shown in Fig. 23.1.

23.1.3 Intermediate Foundations


A growing class of foundations can be referred to as intermediate foundations.
These are similar to deep foundations because vertical members transfer stress
down into soil, but unlike conventional deep foundations they are not rigid
columns of wood, concrete, or steel, but are composed of compacted coarse
aggregate or stabilized soil. Intermediate foundations include stone columns,
Rammed Aggregate Piers, and columns of soil stabilized in situ, and are discussed
in the next chapter.

23.2 PILE FOUNDATIONS

23.2.1 End-Bearing Piles


Settlement of a structure supported on end-bearing piles is limited to compres-
sion of hard materials under the ends plus elastic compression of the pile itself.

Figure 23.1
Deep,
intermediate, and
shallow
foundations.

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670 Geotechnical Engineering

Although end-bearing piles are long, slender columns, they are not free columns
and derive considerable lateral support against buckling from passive resistance of
the soil. Failure by buckling is virtually unknown unless the piles extend for long
distances through air or water. A different kind of bending of steel pile can occur
during driving, if the pile hits a glancing blow on a large boulder deep within
the soil. There have been rare occurrences where a driven steel pile has done a
1808 bend and emerged at the ground surface.

23.2.2 Friction Piles


By transferring a foundation load downward into soil, friction piles also can cause
a substantial reduction in settlement, even in a normally consolidated soil, because
of the increase in soil density and modulus with depth. In this connection it is
helpful to review the e-log p curve in Fig. 16.9, where because of the logarithmic
scale a given increase in pressure results in smaller changes in void ratio with
increasing depth.

23.2.3 Horizontal Deflections and Batter


Piles may be driven vertically or they may be driven at an angle to better resist
horizontal components of a foundation load. Batter piles are sometimes referred
to as spur piles. Batter is expressed as a fraction in which the horizontal leg of the
slope triangle is the numerator and the vertical leg is the denominator. Thus, a
batter of 1:3 means a slope of 1 horizontal to 3 vertical.

Vertical piles also may be designed to resist horizontal loading, particularly when
horizontal loading is not constant, as in wharves.

23.2.4 Positive and Negative Skin Friction


A pile or pier that moves downward relative to the surrounding soil will derive
support from side friction. However, there also can be situations where end bearing
results in the soil moving downward relative to the pile. In that case frictional
forces are directed downward and add to the weight that must be carried by the pile
(Fig. 23.2(b)). Side friction that acts downward is called negative skin friction.

Negative skin friction is much more common than might be anticipated


because it can be mobilized by even a relatively small lowering of the ground-
water table reducing buoyant support for the soil. Friction can be reduced by
using smooth piling or coating the sides with a lubricant such as soft asphalt.
A failure to recognize a potential for negative skin friction can lead to future
difficulties.

Although positive skin friction aids in support of a pile or pier foundation, it does
not peak out simultaneously with end support, particularly for long piles, because
of compression of the piles. That is, as a pile or pier is loaded, support initially
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Deep Foundations 671

Figure 23.2
Combined friction and end bearing: (a) ideal development, (b) negative skin
friction adds soil weight to the pile; (c) during loading, side friction develops
first and decreases, mobilizing end bearing.

derives from skin friction along the upper part, and then as additional load is
applied and the pile compresses, more friction is mobilized until finally the load
reaches the end of the pile or pier and starts building up end support. This is
illustrated in Fig. 23.2(c). It also means that with a factor of safety of 2 little or no
load may reach the lower end of the pile or pier.

23.2.5 Kinds of Rigid Piles and Piers


The foundation elements shown in Fig. 23.1, and other types that are not shown,
have certain advantages and disadvantages, depending on the kind of soil, anti-
cipated load, whether the pile is to be end-bearing or frictional, pile availability,
time, and cost.

Wood Piles
Timber piles were first, and still are commonly used depending on cost and
availability. Plain or untreated wood is highly susceptible to decay in aerobic wet
conditions, and most wood piles now are chemically treated. Older buildings
founded on untreated wood piles may suffer damage because of lowering of the
groundwater table. The length and bearing capacity of wood piles also is limited,
depending on the kind and size of the trees. In the U.S., southern pine is often
used and is limited to a length of about 80 ft (25 m).

Marine borers, both crustaceans and mollusks, are difficult to separate from their
appetites, and even wood piles whose surface has been impregnated with creosote
may last only 15 to 50 years, depending on climatic factors. The useful life can be
extended by periodic maintenance that involves caulking or coating damaged
areas.
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672 Geotechnical Engineering

Steel H-Beams
Steel H-beam sections are especially useful to penetrate through loose or weath-
ered rock layers to obtain end bearing in solid rock. To minimize end damage
and bending they may be fitted with hardened steel shoes that are welded on at the
job site. Because of their small cross-sectional area, H-piles can be driven into
sand and gravel where it would be difficult to drive displacement piles such as
timber or concrete.

Steel H-beams also are used for trestle structures in which the piles serve both as
bearing piles and as braced columns.

Side friction on steel H-piles derives about one-half from soil-to-steel friction on
the outer surface of the flanges, and the other half from soil friction as soil
between the flanges moves with the pile. A driving shoe that is larger than the pile
oversizes the hole and reduces side friction, so H-piles intended for side friction
should not have such a shoe. However, the lower friction and side area are
advantageous for reducing negative skin friction.

When steel piles are exposed to the air or to alternate wetting and drying above a
groundwater table they are subject to corrosion, the same as any steel structure
under similar conditions. H-beam piles above ground can be protected from
corrosion by painting, or they may be encased in concrete for several feet above
and below the ground line.

23.2.6 Classes of Concrete Piles


Because concrete is readily available, transportation costs often are lower
compared with other piles. Concrete piles are in two general classes, cast-in-place
and precast. Precast concrete piles are driven, whereas cast-in-place may either use
a driven steel shell that is filled with concrete or may involve boring a hole in
which to cast the pile. A wide variety of independently developed cast-in-place
construction methods is used, leading to some confusion in nomenclature.

Generally, drilled-and-cast piles are now referred to as ‘‘drilled shafts’’ or ‘‘drilled


piers,’’ but they also are called ‘‘drilled caissons,’’ ‘‘bored piles,’’ or simply
‘‘caissons.’’ These are discussed in the next section.

23.2.7 Driven Precast Piles


Precast concrete piles are cast horizontally, and therefore are made square or
octagonal instead of circular. They can be tapered uniformly or tapered in segments
from tip to butt, but longer lengths normally are tapered only for about 4 or 5 ft
(1.2–1.5 m) from the lower end for easier handling. Piles are reinforced with
longitudinal bars and transverse steel that may be in the form of separate loops
or continuous spirals. The transverse steel is spaced closer together for 3 or 4 ft
(1–1.2 m) at each end of the pile because driving stresses are highest near the ends.
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Deep Foundations 673

Because handling and driving stresses are severe, steel reinforcement often is either
pre-tensioned or post-tensioned. Sufficient flexural strength is obtained with only
about one-fourth to one-third the usual level of prestressing for more orthodox
structural members. Prestressing also can help to prevent piles from breaking in
tension during driving, as compression waves going down the pile pass and add to
wave displacements echoing up from the bottom.

Whether prestressed or not, precast piles must be carefully handled and lifted by
slings under the one-third points to reduce bending stresses to a minimum.
Uniformly tapered precast piles are limited in length to about 40 ft (12 m) because
of the small cross-sectional area of the lower end. Parallel-sided piles with tapered
ends can be over 100 ft (30 m) long. Octagonal precast piles may be up to 36 in.
(0.9 m) in diameter, in which case a hole may be cast along the center axis to
reduce their weight.

In order to reduce transportation costs, precast piles are usually manufactured in


a temporary casting yard near the site where they are to be used. Steel driving
shoes may be cast into the concrete to resist hard driving conditions.

23.2.8 Driven Shells


Driven steel shells may be tapered or parallel-sided shells or steel pipes. After
driving they are filled with concrete.

As an illustration of the procedures that are involved, one type of tapered driven-
shell pile is made as follows:

1. A thin corrugated steel shell is closed at the bottom with a steel boot.
2. A steel mandrel or core is placed inside the shell.
3. The mandrel and shell are driven into the ground.
4. When a predetermined driving resistance has been reached, driving stops and
the mandrel is withdrawn.
5. The open lined hole is inspected for damage.
6. The shell is filled with concrete.

The driving mandrel protects the shell during driving. This type of shell can be
tapered uniformly from the bottom to top, or they may be step-tapered with
different-sized shells attached end to end. An advantage of the step-taper is that
the driving mandrel distributes driving energy along the length of the shell instead
of concentrating it at the bottom.

Another type of driven shell has a scalloped cross-section formed by a series of


vertical flutings running the full length of the shell. This shell is driven without
a mandrel and is uniformly tapered and closed at the bottom by a steel boot.

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674 Geotechnical Engineering

The thinnest shells that can be used for this type of pile are about 18 in. (3 mm)
thick, but thicknesses of l.5 to 2 times this value are more common, depending on
the length and diameter of the pile.

A parallel-sided, dropped-in shell pile that is designed solely for tip resistance is
constructed by driving a heavy steel pipe, usually 16 in. (400 mm) in diameter and
½ in. (12.7 mm) thick, with the aid of a steel mandrel, then pulling out the
mandrel and inserting a thin metal shell such as a corrugated-metal culvert pipe,
filling it with concrete, and withdrawing the drive pipe.

Another alternative is to drive a steel pipe pile with either a closed end or an open
end. The closed-end pipe is filled with concrete. Sometimes a pipe is driven all in
one piece, or it may be made of several pieces of pipe either welded together or
fitted together with special internal sleeves. The open-end steel pipe is used to
obtain better penetration through weathered rock to find hard rock, and then
either flushed out with water and air or with a miniature orange-peel dredging
bucket. The open pipe then is given a few extra blows, pumped out, and filled with
concrete. By sealing into the rock, a pile installed in this manner in effect is a
small-diameter caisson and has a high bearing capacity.

23.2.9 Pedestal Piles


A modification that produces a bulb of concrete at the bottom of a pile is called
the Franki method. The procedure is as follows:

1. A heavy steel pipe containing a mandrel or core is driven into the ground.
2. The mandrel is removed and a small charge of concrete is poured into the
pipe.
3. The mandrel is reintroduced and lowered to the top of the concrete.
4. The pipe is pulled upward 2 or 3 ft (23 to 1 m).
5. The mandrel is again driven with the pile-driving hammer, which forces
concrete out of the end of the pipe to form a bulb-shaped mass.
6. The mandrel is removed, and the pipe is filled with concrete up to the top.
7. The mandrel is reintroduced to hold the concrete down while the steel drive
pipe is pulled out of the ground.

23.2.10 Composite Piles


Composite piles of timber and concrete combine the low cost of wood piles with
the durability of concrete piles. The wood section is driven until its upper end is
about at the ground surface, then topped off with a concrete pile that is driven
until the wood pile is below the groundwater level. An important element is the
joint between the wood and concrete sections so that there is a good bearing
surface and the joint has strength to resist tension and bending.
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Deep Foundations 675

23.2.11 Minipiles
Minipiles or micropiles are any small-diameter piles that are installed in
borings, jacked in, driven, or vibrated in. They are useful where there is little
headroom for installation, for example inside existing buildings. Hollow pipes
are used for higher loads and the ends pressure grouted. A simple adaptation used
for light underpinning is reinforcing steel bars that are jack-hammered into
the soil near a foundation, then bent back underneath a footing and encased in
concrete.

23.3 PILE DRIVING

23.3.1 Types of Hammers


Early pile-driving hammers were simply weights that were repeatedly lifted along
guides and dropped on top of a pile. In later innovations the hammers were lifted
by steam, which gave the option of either single operation with steam only doing
the lifting, or double operation with steam also powering the down cycle. Steam
hammers are capable of applying from 50 to 110 blows/min.

Diesel hammers (Fig. 23.3) have a self-contained power source. The ram acts as a
vertical piston that when dropped compresses an air-fuel mixture inside a cylinder,
causing it to explode and propel the ram back up again. Burned gases exhaust

Figure 23.3
Diesel hammer
puffing smoke as it
drives a steel pipe
pile.

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676 Geotechnical Engineering

through a port, additional fuel is injected into the cylinder, and the cycle repeats
automatically until the fuel is shut off. The ram also impacts an anvil that drives
the pile. Pile resistance is needed to keep a diesel hammer actuated, so if a pile
breaks or goes through very soft soil the hammer may stop.

23.3.2 Protecting the Pile Head


Driving a wood pile tends to crush the wood fibers at the top of the pile, which is
called ‘‘brooming.’’ Wood pile also may split vertically. Damaged portions of the
piles are cut off, so piles should have sufficient extra length to allow for the cutoff.
A heavy steel ring may be placed over the head of a wood pile to reduce the
amount of brooming and splitting.

The head of a precast concrete pile is protected by a metal drive cap or helmet.
As shown in Fig. 23.4, a cushion that usually consists of blocks or layers of
wood is used to reduce the impact of the hammer. The amount of energy lost
becomes apparent when the wood block smolders or catches on fire and must be
periodically replaced.

23.3.3 Driving Formulas


The efficiency of pile driving in terms of energy per unit of driving depends on the
resistance of the soil. Because the load-bearing capacity of the pile also depends
on the resistance of the soil, one may expect that there will be a relationship
between pile-bearing capacity and driving energy. Unfortunately, energy loss
factors are substantial and highly variable, which reduces the reliability of such
projections. As a result many empirical pile-driving formulas have been suggested
to try and improve the relationships.

Figure 23.4
(a) Driver setup
showing ram,
wood
cushion, helmet
and pile.
(b) Single-acting
steam,
(c) double-acting,
(d) diesel, and
(e) vibratory
hammers. (After
Vesic, 1977.)

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Deep Foundations 677

The most common driving formula also is one of the oldest, the Engineering
News formula that was suggested in 1888 by A. M. Wellington, the editor of that
magazine before it became Engineering News Record. The formula is based
on the principle of conservation of energy—energy in equals energy out—but
it also includes a generous and arbitrary energy loss factor. The formula is as
follows:
1 WH
Qp ¼ ð23:1Þ
6 S
where Qp ¼ allowable bearing capacity (tons);
W ¼ hammer weight (tons);
H ¼ height of fall (ft);
S ¼ penetration with one hammer blow (ft, inches in final formulas);
WH ¼ pile-driving energy per blow (ft-tons);
1/6 ¼ energy loss factor.

An additional adjustment is made to account for hammer friction losses, which


are assumed to be constant, and therefore can be represented by an arbitrary value
added to the denominator. For convenience, distance S is converted to inches
while the height of fall remains in feet. With these adjustments,
2WH
Qp ¼ for drop hammers ð23:2Þ
Sþ1
2WH
Qp ¼ for single-acting steam hammers ð23:3Þ
S þ 0:1
where S is the settlement per blow in inches. SI equivalents are

815WSI HSI
Qp ¼ for drop hammers ð23:2aÞ
SSI þ 25

815WSI HSI
Qp ¼ for single-acting steam hammers ð23:3aÞ
SSI þ 2:5

where WSI ¼ hammer weight (kN);

HSI ¼ height of fall (m);


SSI ¼ penetration with one hammer blow (mm).

For double-acting hammers where power is added during the hammer stroke,
energy from the manufacturers’ specifications is substituted for WH. The
minimum hammer blow for piles that will carry 25 tons (220 kN) is 15,000 ft-lb
(20 kilojoules or kilonewton-meters).
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678 Geotechnical Engineering

Figure 23.5
Engineering News
and Michigan
formulas applied
to results of pile
load tests from
several sources
(Spangler and
Mumma, 1958).

The Engineering News formula was developed when practically all piles were
of wood and were driven by drop hammers that now are considered light in
weight. The formula ignores pile length, weight, cross-section, taper, material,
and soil response, which can change with time. A graph comparing the formula
with over 100 load tests is shown in Fig. 23.5, where it will be seen that the
energy loss factor of 1/6 is valid to the extent that none of the piles had over
6 times the predicted capacity. The test piles included a wide variety of types,
lengths, sizes, soil conditions, and geographic locations. Included are 69 load
tests by the Michigan State Highway Commission at three sites, one having a
hard cohesive soil, another a soft cohesive soil, and the third a deep granular
deposit with interbedded organic materials. Pile types included H-section,
pipe, flute-tapered monotube, and step-tapered shell.

Despite obvious spread of the data in Fig. 23.5, according to these data the
probability of having a factor of safety less than 1.0 with the Engineering News
formula is less than 1 in 20, and will be further diminished for piles acting in
a group. The average factor of safety is about 2. Since the energy loss factor
nominally is 6, on the average about two-thirds of the driving energy is lost.
However, the wide range in factors of safety leaves room for improvement.

Example 23.1
The final penetration resistance for a pile driven with a 30,000 ft-lb (42 kJ or 42 kN-m) drop
hammer is 0.6 in./blow (15 mm/blow). Predict the bearing capacity according to the
Engineering News formula.
Answer:
2WH 2  15 ft-tons
Qp ¼ ¼ ¼ 19 tons, or
Sþ1 0:6 þ 1 ðin:Þ

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Deep Foundations 679

815  42
¼ ¼ 860 kN
15 þ 25
Note that there actually is only one significant figure.

23.3.4 Michigan Formula


Many modifications have been made to the Engineering News formula. A relatively
simple change by Hiley was adapted by the Michigan State Highway Commis-
sion(1965) to account for the mass of the pile in terms of its weight, Wp, and a ‘‘coef-
ficient of restitution,’’ e, that depends on the pile composition and the cushion.

The coefficient or restitution is defined as the square root of the ratio of energy
out to energy in for the driving cushion, and therefore is dimensionless. The value
of e was established empirically and varies from 0.25 for timber pile and for a
concrete or steel pile with a soft wood cushion, to about 0.55 for a steel pile with
no cushion. A value of 0.5 is most commonly used to represent a common practice
of driving steel or concrete piles with an oak hardwood cushion. A special Micarta
cushion has e ¼ 0.8.

The Michigan formula gives a correction factor that is applied to the Engineering
News formula, and therefore still incorporates the driving energy loss factor of 6.
The correction factor is
Wr þ e2 Wp
Em ¼ 1:25 ð23:4Þ
Wr þ Wp
where Em ¼ a multiplier for the result from the EN formula and is dimensionless;
Wr ¼ weight of the hammer ram;
Wp ¼ weight of the pile;
e ¼ coefficient of restitution.
Results from the Michigan pile study in Fig. 23.5 show considerable improvement
over the EN formula by removing evaluations having a low factor of safety, so
this modification is recommended.

Example 23.2
The pile of the previous example is a steel pipe pile 40 ft (12 m) long, 12 in. (0.30 m) in
diameter, weighing 17.86 lb/ft (260 N/m). It is driven by a 10,000 lb (44.5 kN) single-acting
steam-driven ram operating on an oak cushion with e ¼ 0.5. Calculate Em.
Answer: The weight of the pile is Wp ¼ 40 ft  17.86 lb/ft ¼ 714 lb, or 12 m  260 N/
m ¼ 310 N.
Em ¼ 1:25½ð10,000 þ ð0:5Þ2  714=ð10,000 þ 714Þ ¼ 1:2, or
¼ 1:25½ð44,500 þ ð0:5Þ2  310=ð44,500 þ 310Þ ¼ 1:2

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680 Geotechnical Engineering

23.3.5 The Wave Equation


The effects of pile mass and a coefficient of restitution that were added in the
Michigan formula are more elegantly treated in the wave equation developed in
1960 by E. A. L. Smith of the Raymond Pile Co.

The wave equation treats the pile as a rod that is set into vibration by being hit on
the end with a hammer. The behavior can be demonstrated by suspending a pile
horizontally on cables, when instrumentation shows that a compression wave
travels down the pile from one end to the other; then the far end snaps back and
generates another compression wave that goes in the opposite direction. Tension
may develop instantaneously as two compression waves traveling in opposite
directions pass one another. The method received a considerable boost when some
long concrete bridge piles broke in load tests, and when pulled were found to have
broken in tension—an obvious conundrum because a hammer can push but not
pull.

Smith’s model is shown in Fig. 23.6. A pile is divided into an arbitrary series of
segments each 8 to 10 ft (2.5 to 3 m) long and having a mass W. Soil resistance to
driving is represented by individual R values along the sides or at the tip. Each
segment is connected to adjoining segments by an elastic connector represented
by a spring, K.

A ratio of tip to side resistance is assumed, and data for hammer energy and
elastic constants and mass of the pile are entered. Equations relate compression
and force in each connector spring to displacement, velocity, and accelerating
force of each segment. The equations are solved at discrete millisecond time
intervals starting when the hammer hits. This generates a record of forces and
displacements in time throughout the length of the pile, as shown in Fig. 23.7.
Time zero is when the ram hits the pile, and intercepts along the x time-zero axis
show the compression wave moving down the pile to the tip section D12. After
15 milliseconds the pile tip has moved downward 0.2 in., whereas the top of the
pile has moved down 0.86 in. and is bouncing back upward. There is a temporary
disconnect between the pile cap D2 and the upper end of the pile D3 at about
12.5 ms.

The pile-bearing capacity is obtained by summing all of the R’s that represent
both side friction and point bearing. The analysis is repeated with different
assumed R values to generate a graph relating pile capacity to blows per foot
(0.3 m), as shown in Fig. 23.8.

The wave equation addresses driving variables but it still does not take into
account time-related changes in the soil such as drainage of excess pore water
pressure and thixotropic hardening. These effects become obvious when driving is
stopped for a few hours and the pile has developed ‘‘set’’ or ‘‘freeze.’’ Re-driving a
test pile after a day or two then gives a new penetration resistance that is divided

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Deep Foundations 681

Figure 23.6
Smith’s wave
equation model for
driven piles.

by the earlier resistance to give a ‘‘setup factor,’’ B/A in Fig. 23.8. The setup factor
varies from 1 for sands to 2 or more for clays. The setup factor reduces the
number of blows per foot required for a pile to reach a desired bearing capacity.

Because of the many equations and data entries required, the wave equation is
most conveniently solved with the aid of a computer, and programs are available.

23.4 DRILLED PIERS AND AUGERCAST PILES

23.4.1 Installing Drilled Piers


Borings for drilled piers are made by turning a relatively short auger section until
the auger is filled, quickly raised it out of the boring, and rapidly rotating it to
spin off the soil. This procedure is repeated until the boring reaches the desired
depth. Soil is pulled away from the top of the boring with a shovel to prevent it
from falling back in. The system requires a drill that can extend to the maximum

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682 Geotechnical Engineering

Figure 23.7
Example of wave
equation analysis.
(From Smith,
1960, with
permission of the
American Society
of Civil
Engineers.)

depth of the pier with a square stem that slides up and down through a power
sleeve called a ‘‘kelly.’’ Holes may be bored dry, or to prevent caving they can be
kept full of mud. In clay soils this often is made on-site by mixing soil and water.
In this case a casing can be set to restrain the soil while the mud is being removed
by bailing. (This probably is how the name became ‘‘caisson.’’) Another
procedure is to leave the mud in the hole, lower the steel reinforcing cage, and
pour concrete through a canvas chute or tremie that extends to the bottom of
the hole. The fluid concrete because of its higher density then replaces the mud
from the bottom up.

23.4.2 Belled Piers


A special type of drilled pier that can be constructed only in soil that can stand
without caving is called a ‘‘belled’’ or under-reamed pier that increases the end-
bearing area. The procedure is to bore a hole to a predetermined depth, then insert
a reamer with expandable blades (Fig. 23.9). The blades open out to an angle of
about 308 to 458. The hole then is cleaned out and the bottom inspected for loose
soil, after which the boring is filled with concrete. Manual inspection and cleanout
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Deep Foundations 683

Figure 23.8
Evaluating and
applying a setup
factor, B/A, to a
wave equation
analysis.

Figure 23.9
Expandable cutter
used for belling out
the bottom of
drilled piers to
increase the
end-bearing area.
(Photo courtesy of
Dr. Lyman C.
Reese.)

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684 Geotechnical Engineering

of the bottoms of belled piers is a colorful occupation that requires a positive


outlook, and the popularity of this method is fading.

23.4.3 Augercast Piles


Augercast piles were invented in the 1940s by the Intrusion-PrePakt Co. They are
installed with a continuous hollow-stem helical auger that equals or exceeds the
length of the pile (Fig. 23.10). The auger is bored to the desired depth and then
the soil-filled auger is slowly raised while cement mortar is pumped down to fill
the space left by the auger. The auger therefore confines the mortar so that it
builds up pressure against the soil.

Augercast piles usually are smaller in diameter than drilled piers and more
expensive than driven piles, but are adapted for caving soils with difficult
groundwater conditions. Augercast piles do not require casing, and installation
does not generate the noise and tremors of pile driving. The pumping pressure
is monitored to ensure positive pressure as the auger is withdrawn, leaving a
continuous column of grout. A cardboard or plastic cylinder is added at the top
and filled with grout to the desired elevation, and reinforcing steel can then be
lowered into the fluid grout.

The grout used in augercast piles consists of Portland cement, sand, fly ash, and
water. Fly ash is a byproduct from burning powdered coal in electric power
plants; it is a pozzolan, meaning that it reacts with lime liberated by the hydrating
cement to create additional cementitious compounds. The fine spherical particles

Figure 23.10
Continuous flight
auger and guide
for making
augercast piles.
After boring to full
depth, hoses carry
liquid grout to the
top of the
hollow-stemmed
auger for pumping
to the bottom of
the hole as the
auger is lifted and
confines the grout.
The horizontal bar
near the top is a
torque arm.

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Deep Foundations 685

of fly ash reduce friction during pumping. Fluidizing agents and an expanding
agent such as aluminum powder, which reacts with alkali to give off hydrogen
bubbles, also may be added to help aid pumping and maintain positive pressure
through expansion until the grout sets.

A recent modification of the augercast method that is intended to eliminate spoil


from the boring incorporates a reverse-pitch section of auger, so instead of soil
being taken out of the boring it is pushed together and forced to move laterally.
This increases lateral stress, but is difficult to accomplish in stiff soils because of
the power requirements.

23.5 SOIL MECHANICS OF PILES AND PIERS

23.5.1 Overview: Side Friction and End Bearing


The total supporting capacity Q of a pile or pier is the sum of side friction and end
bearing, and can be expressed by
Q ¼ Qs þQb ð23:5Þ
where Qs derives from side friction and Qb is from end bearing at the base.

Side friction depends in part on normal stress exerted by soil on a pile or pier,
which for the most part has seldom been measured except indirectly through pull
tests. The coefficient of friction can be compromised by several factors including
remolding.

Prediction of an end bearing of deep foundations from soil mechanics consi-


derations requires a model for bearing capacity failure. Three models are shown in
Fig. 23.11. As in the case of shallow foundations, Terzaghi’s model assumes that
soil above the bottom of the foundation contributes only a surcharge pressure,
whereas Meyerhof incorporates shearing resistance of the soil above that base
elevation. While this appears more reasonable for deep foundations, the develop-
ment of shearing resistance may be progressive, so yielding does not occur
simultaneously along the entire slip surface, particularly since shearing stresses
decrease rapidly with radial distance in a three-dimensional arrangement. Even
though the model appears to be unrealistic, the Terzaghi factors corrected for
a round base are very close to those determined by Vesic (1963) from model tests.

23.5.2 Soil Factors


Factors that have been identified as influencing both driving resistance and pile
capacity are as follows:
 Remolding obviously must occur in soil adjacent to driven piles and occurs to a
lesser degree in the perimeter of borings for drilled piers and augercast pile.

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686 Geotechnical Engineering

Figure 23.11
Models for side
friction and end
bearing of piles
and piers. Other
things being
equal, side
support increases
as the length and
the diameter, and
end bearing as
the square of the
diameter.

Side friction has been shown to be increased if boring surfaces are rough or
grooved.
 Temporary high pore water pressures have been measured in soil adjacent to
driven piles, and excess pore pressure also are likely to occur during ramming
of the bottom bulb of pedestal piles.
 Temporary liquefaction was discovered in soil near Rammed Aggregate Piers,
described in the next chapter, and probably occurs near the bulb of pedestal
piles. Liquefaction also may occur in weak, saturated soil near tapered piles
and would aid driving, but those occurrences have not been verified.
 Radial tension cracks have been conjectured to occur near driven piles to
explain rapid dissipation of pore water pressure, and have been confirmed in
the elastic zone near Rammed Aggregate Piers. Radial cracking may be an
important phenomenon for facilitating drainage of excess pore pressure near
displacement piles and piers.
 Lateral stress directly influences side friction and to some extent end bearing of
deep foundations, but for the most part has not been measured except
indirectly from pullout resistance. Displacement from pile driving should
increase lateral stress, and lateral stress temporarily is decreased by borings and
reinstated by fluid pressure of concrete. The contact stress then can change as
load is applied. Lateral stress is the least known of the variables affecting pile
capacity.

The following discussions follow recommendations of Reese and O’Neil (1989).


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Deep Foundations 687

23.5.3 Side Friction in Clay


Lateral pressure from the fluid pressure from the concrete should enable a
calculation of side friction. However, Reese et al. (1976) found that water from
the concrete migrates into adjacent clay soil, which should contribute to excess
pore pressure during load testing and weaken the soil. A representative series of
tests is shown in Fig. 23.12, where side friction does increase with depth
down to about 10 to 12 feet (3 to 4 m) and peaks out at about 75 percent of the
shearing strength of the unaltered soil. At depths less than about 5 ft (1.5 m),
low side friction is attributed to desiccation shrinking of clay away from the pier.
Side friction can be seen to decrease during the final load increment, indicating
remolding.

Another complicating factor in Fig. 23.12 is a nearly complete loss of side friction
near the bottom of the pier. This can be expected if, as the base of the pier settles,
it carries a surrounding bulb of soil along with it.

Based on these and similar results, Reese and O’Neil recommend calculating side
friction of a pier in clay using an ‘‘alpha factor,’’ which represents a portion of the
undrained shear strength of the soil acting along a shaft length that excludes the
upper 5 ft (1.5 m) and the lower 5 ft (1.5 m) plus the length of a bell. The  factor
experimentally was determined to have an average value of 0.55. Hence

qs ¼ 0:55c and ð23:6Þ

Qs ¼ qs Ls D ð23:7Þ

where qs is the developed cohesion, Ls is the shaft length after deduction for end
effects, and D is the shaft diameter.

Figure 23.12
Development of
skin friction during
loading of a drilled
test pier in
expansive Houston
clay. (After Reese
et al., 1976, with
permission of the
American Society
of Civil Engineers.)

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688 Geotechnical Engineering

Example 23.3
Calculate the side friction for a 2.5 ft (0.76 m) diameter drilled pier 15 ft (4.6 m) long
penetrating clay with c ¼ 5 ton/ft2 (480 kPa). There is no bell.

Answer:
qs ¼ 0:55  5 ton=ft2 ¼ 2:75 ton=ft2
Qs ¼ 2:75 ton=ft2  ½ð15  5  5Þ  2:5 ft2 ¼ 108 tons, or
qs ¼ 5:5  480 kPa ¼ 2640 kPa or 2640 kN=m2
Qs ¼ 2640 kN=m2  ½ð4:6  1:5  1:5Þ  0:76 m2 ¼ 10:1 MN

23.5.4 End Bearing in Clay


The Terzaghi bearing capacity equation for shallow foundations is
B
qb ¼ N þ cNc þ DNq ð22:7Þ
2
where qb is the end-bearing capacity in force per unit area,  is the soil unit weight,
B is the foundation width, c is soil cohesion, D is depth of the foundation, and the
N values are bearing capacity factors.

If  is assumed to be zero in clay to represent undrained conditions, from


Table 22.3 the three respective N bearing capacity factors for a round base are 0,
6.2, and 1.0. The first (width) term in the equation therefore is eliminated, the
second (cohesion) term is retained, and the third (depth) term equals the amount
subtracted to obtain a net bearing capacity, based on the approximate equivalence
of the soil and concrete unit weights. The net bearing capacity at the ground
surface then becomes
qbnet ¼ 6:2c

However, back-calculations from load tests indicate a closer approximation if


Nc ¼ 9, which corresponds to a partially drained friction angle of about 68. Then
qbnet ¼ 9c ð23:8Þ
where qbnet is the net end-bearing pressure and c is the average soil cohesion for a
depth of two diameters below the base. Multiplying by the base area gives
Qbnet ¼ ðB=2Þ2 c
Qbnet ¼ 7cB2 ð23:9Þ
0
where B is the base diameter. In normally consolidated soils, c increases with
depth so there is an increase in end bearing even though c in the equation
represents a partially drained shear strength.

Example 23.4
Calculate allowable total net bearing capacity of the 2.5 ft (0.75 m) diameter, 15 ft (4.6 m)
long pier of the previous example on the same overconsolidated clay.

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Deep Foundations 689

Answer:
Qbnet ¼ ð7Þð5 tons=ft2 Þ  ½ð1:25Þ2  ft2 ¼ 17 tons: Adding side resistance gives
Qnet ¼ 108 þ 7 ¼ 115 tons: With a factor of safety of 2,
Qa ¼ 52 tons, of which most is side friction, or
Qbnet ¼ ð7Þð480 kPaÞ  ½ð0:38Þ2  m2 ¼ 0:49 MN
Qnet ¼ 10:1 þ 0:5 ¼ 10:6 MN; Qa ¼ 5:3 MN:

23.5.5 Depth Factor for End Bearing in Clay


Reese and O’Neil (1989) suggest a modification to eq. (23.8) to incorporate a
moderate depth influence as follows:
qbnet ¼ 6½1 þ 0:2ðL=BÞc  40 tons=ft2 ð3:8 MPaÞ ð23:10Þ
where L is the pier length and B is the base diameter, both having the same units.

Example 23.5
Recalculate the previous example using eq. (23.10).

Answer:
L=B ¼ 15=2:5 ¼ 6:0ð4:6=0:75 ¼ 6Þ
qbnet ¼ 6½1 þ 0:2ð6Þ 5 ton=ft2 ¼ 66 tons=ft2 ; use 40 tons=ft2
Qbnet ¼ 40ð1:25 ftÞ2 ¼ 196 tons, compared with 170 tons
from the previous example:
Qnet ¼ 196 þ 67 ¼ 263 tons: With a factor of safety of 2,
Qa ¼ 130 tons instead of 118 tons, or
qbnet ¼ 6½1 þ 0:2ð6Þ 480 kPa ¼ 6:3 MPa; use 3:8 MPa:

23.5.6 Settlement on Clay


The larger the base of a pier the deeper the pressure bulb, and the larger the
amount of settlement. Reese and O’Neil therefore suggest an empirical bearing
pressure reduction factor for piers up to 11 ft (3.5 m) in diameter:
2:5
Fr ¼ 1 ð23:11Þ
1 bþ
B 2

where Bb is the base width in inches. The two factors are

1 ¼ f0:0071 þ 0:0021ðL=Bb Þg  0:015 ð23:12Þ


p
2 ¼ 1:125 c and 0:5  2  0:15 ð23:13Þ
2
where c is the undrained cohesive shear strength in kips/ft . As 2 is not
dimensionless, SI units should be converted before making this correction.

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690 Geotechnical Engineering

Example 23.6
Determine the settlement correction factor to bearing capacity in the preceding
example.

Answer:
1 ¼ f0:0071 þ 0:0021ð15=2:5Þg ¼ 0:020; use 0:015
p 2
2 ¼ 1:125 10 kips=ft ¼ 3:56; use 0:15
Fr ¼ 2:5=½0:015 ð2:5Þ þ 0:15 ¼ 13:3 > 1:0; use 1:0, no reduction

23.5.7 Side Friction in Sand


Side friction of a drilled pier in sand is calculated in a similar manner but uses an
empirical beta () factor that incorporates influences of both friction angle and
lateral stress. The relationship is
qsi ¼ zi0 ð23:14Þ

where qsi is side friction per unit area of a section of pier passing through a soil
layer and  zi0 is the vertical effective stress in soil at the middle of the layer. Beta is
evaluated from
p
 ¼ 1:5  0:35 zi , and 0:25    1:20 ð23:15Þ

where the depth zi is in feet, or


p
 ¼ 1:5  0:63 zi , and 0:25    1:20 ð23:15aÞ

where zi is in meters. Because, according to eq. (23.15),  is not linear


with depth, a sand is divided into sublayers for calculations. There is no
decrease in side friction at the top or bottom of a pier, and no belling allowed in
sand.

Example 23.7
Calculate the maximum side friction on a 20 ft (6.1 m) long, 2.5 ft (0.76 m) diameter
straight pier in sand having a unit weight of 120 lb/ft3 (18.9 kN/m3). The ground-
water table is at 10 ft (3.05 m) depth.

Answer: Arbitrarily divide the sand into two layers, zi ¼ 5 ft and 15 ft (1.5 and 4.6 m).
Respective  values are 0.72 and 0.25. Respective qsi values are

Upper qsi ¼ 0:72ð5 ftÞð120 lb=ft3 Þ ¼ 432 lb=ft2 , or


¼ 0:72ð1:5 mÞð18:9 kN=m3 Þ ¼ 20:4 kPa
Lower qsi ¼ 0:25½ð10Þð120Þ þ 5ð120  62:4Þ ¼ 329 lb=ft2 ð15:8 kPaÞ
Qs ¼ ð2:5Þð10Þð432Þ þ ð2:5Þð10Þð329Þ ¼ 33,900 þ 25,800 lb ¼ 30 tons
¼ ð0:76Þð3:05Þð20:4Þ þ ð0:76Þð3:05Þð15:8Þ ¼ 149 þ 115 kPa ¼ 264 kPa

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Deep Foundations 691

23.5.8 End Bearing in Sand


If cohesion is zero, eq. (22.7) for bearing capacity becomes
 
B
qb ¼  0 N þ LNq ð23:16Þ
2

where  0 is the effective soil unit weight, B is the pile diameter, and L the length of
the pile.

The bearing capacity factors depend on the friction angle of the sand, which
because of the difficulty of sampling for laboratory testing generally is evaluated
from in-situ tests. The most satisfactory option would be direct measurement, but
most common are penetration tests that are routinely conducted during site
evaluations.

Standard Penetration Test (SPT) results are in blows per foot of penetration of the
special sampler and are designated by N. As discussed in Chapter 26, several
correction factors have been proposed depending on the testing depth and on the
driving energy. The following formula was developed using uncorrected N values:

qo ¼ 0:6N  45 tons=ft2 , or
ð23:17Þ
qo ¼ 0:06 N  4:3 MN=m2

where N is the average standard penetration resistance of soil in blows per ft


(0.3 m) to a distance 2B below the bottom of the pier.

Example 23.8
Evaluate end-bearing and allowable bearing capacity for the 2.5 ft (0.76 m) diameter drilled
pier in the previous example if Nav ¼ 26 blows/ft at the bearing depth.
Answer:
q0 ¼ 0:6ð26Þ ¼ 15:6 tons=ft2
Qo ¼ ð1:25Þ2 ð15:6Þ ¼ 77 tons: Adding side friction,
Q ¼ 30 þ 77 ¼ 107 tons: Dividing by a factor of safety of 2 gives
Qa ¼ 53 tons, or
qo ¼ 0:06ð26Þ ¼ 1:6 MN=m2
Qo ¼ ð0:38Þ2 ð1:6Þ ¼ 730 kN
Q ¼ 264 þ 730 ¼ 994 MN
Qa ¼ 500 MN

Question: With the allowable bearing pressure, what percentages of the side and
base resistance theoretically will be mobilized?

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692 Geotechnical Engineering

Answer: 100% and about 30%. However, side friction may decrease when the pier
is loaded, which will increase the base percentage.

23.5.9 Soil Mechanics Approach to Side Friction for Sand


Many engineers prefer to compare different methods to obtain answers, which is
useful to check for major errors. Also, any empirical approach may not be valid in
the universe that exists outside of the test conditions. A logical next step is to
develop a rational method that applies to all conditions, but this approach is
possible only if relevant soil information is available. A rational approach also has
an advantage of pointing out variables that otherwise may remain buried in the
empirical correlations.

Critical parameters for side friction are the normal effective stress and the
developed friction angle. The normal stress following a concrete pour equals that
imposed by the fluid concrete, but it sometimes is assumed that in time soil pressure
will be relieved to its initial K0 condition, which is difficult to evaluate. Pier loading
can induce an increase in lateral stress because of rotation of the principal stress
directions, and dilation or compression of the soil. Finally, there is the developed
friction angle between the soil and the pier that because of the movement involved
will represent a residual strength without a dilatant component. A typical
assumption is that the angle of side friction is defined by tan  ¼ 0.8 tan .

Example 23.9
Evaluate side friction using a soil mechanics approach for the pier in the preceding
example, the groundwater table being at a depth of 10 ft (3.05 m).
Answer: According to a criterion presented later in this book, an uncorrected N ¼ 26
corresponds to a friction angle in sand of about 358. An estimate of the developed side
friction is tan  ¼ 0.8 tan , or  ¼ 298.

Option 1: For a maximum value use K0 for fluid concrete of 1.0 and a unit weight of
150 lb/ft3. The average normal stresses at mid-depths in the layers above and below the
groundwater table and corresponding side friction are:
Above gwt: h ¼ 1:0ð5Þð150Þ ¼ 750lb=ft2 ; Ss ¼ 750ð2:5Þð10Þ tan 298 ¼ 32,600 lb
Below gwt: h ¼ 1:0½10ð150Þ þ 5ð150  62:4Þ
¼ 1940 lb=ft2 ; Ss ¼ 1940ð2:5Þð10Þ tan 29
¼ 84,400 lb
Total ¼ 58 tons

Option 2: For a minimum value use the soil normally consolidated Ko ¼ 1 – sin  and the
unit weight of the soil.
Above gwt: h ¼ ð1  sin 35 Þð5Þð120Þ ¼ 256 lb=ft2 ; Ss ¼ 256ð2:5Þð10Þ tan 29
¼ 11,100 lb

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Deep Foundations 693

Below gwt: h ¼ ð1  sin 35 Þ½ð10Þð120Þ þ 5ð120  62:4Þ ¼ 635 lb=ft2 ;


Ss ¼ 635ð2:5Þð10Þ tan 29 ¼ 27,600 lb
Total ¼ 20 tons

The two options therefore bracket the answer obtained by the empirical method. The same
procedures can be followed using SI units. Obviously for a soil mechanics approach to be
valid the friction angle and lateral stress must be accurately evaluated.

23.5.10 Settlement of a Pile or Pier in Sand


In sand, particularly in loose sand, settlement may be a more important criterion
than a bearing capacity failure. However, the prediction of settlement is compli-
cated because a substantial part of the load is carried by skin friction, so after
application of a factor of safety the bottom of a pile or pier may receive very little
stress. Settlement therefore is predicted on the basis of stress reaching the bottom of
the pier, and therefore is subject to errors in determination of side friction.

Settlement in sand is limited by a correction factor applied to the load-bearing


capacity of large pier bases in sand:
50
Fr ¼ when Bb > 50 inches, or ð23:18Þ
Bb
1:25
Fr ¼ when Bb > 1:25 m ð23:18aÞ
Bb

23.6 LOAD TESTS

23.6.1 Compression Load Test


Load tests are more easily arranged for piles and piers than for shallow
foundations because no massive dead load is required. Instead, a test is conducted
by jacking against a horizontal beam with ends attached to uplift piles or piers, as
shown in Fig. 23.13. As the anchor piles or piers are in tension they must be
reinforced, and the reinforcing steel is extended upward where it is bolted or
welded to the horizontal reaction beam.

For piers having a large base-bearing capacity four anchors may be required to
generate a sufficient side friction, in which case the reaction beams are assembled
as a letter H. Loads ordinarily are increased incrementally until they reach two
times the design capacity, to confirm a factor of safety of 2.

As test loads are applied, settlement is measured with dial gauges or transducers
on opposite sides of the pile or pier so that averages may be used to compensate
for bending. The gauges are supported on small independently supported beams

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694 Geotechnical Engineering

Figure 23.13
Load test of a
drilled pier using
hydraulic jacks
and two
independently
supported dial
gauges.
Sunshade is to
prevent thermal
warping from
affecting the
readings.

that are transverse to the pile row to avoid influences from ground heave. The
arrangement is shaded to reduce error from thermal expansion and warping of
gauge supports.

Test loads may be applied continuously or in cycles. In the continuous method,


which is most common, a test load is applied in increments until two times the
design load is reached or else a plunging failure occurs. Each load increment is
held constant for 2 hours while settlement is measured after various time intervals
(ASTM Designation D-143). The final load is left on for 48 hours. Unloading also
is in steps, and a final reading is made at least 12 hours after all load has been
removed. The load-settlement curve thus obtained is known as a total-settlement
curve or gross-settlement curve.

In the cyclic method, a load increment is applied, and the settlement is measured.
The load is released and the pile is permitted to rebound. Repeating this process
for several increments will permit data to be obtained for plotting a net or plastic-
settlement curve. The distinction between the two types of tests can be seen by
comparing the initial load curve starting at zero in Fig. 23.14 with the reloading
curve.

23.6.2 Defining a Failure Load


Load deflection curves are curvilinear, and a sharp break in a load-settlement
curve is called a ‘‘plunge,’’ which normally indicates end-bearing capacity failure.
This occurs after full mobilization and partial reduction of side friction. Plunge
occurs near point F in Fig. 23.14.
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Deep Foundations 695

Figure 23.14
Pile load test and
failure criteria
based on
settlement, net
settlement, and
settlement per unit
of load.

The maximum test load seldom is sufficient to generate plunge, so many dif-
ferent criteria have been proposed to define acceptability without plunging
failure. No single criterion will be found that can apply to all load tests, and
a common procedure is to define failure on the basis of several criteria and
select the most relevant for a particular situation. For example, if settlement
cannot exceed a certain value, that settlement value becomes the criterion
for acceptability.

Some common criteria are as follows. In this connection ‘‘gross settlement’’ equals
total settlement, and ‘‘net settlement’’ is the gross settlement corrected for
rebound during unloading.
 As indicated above, gross settlement may be limited to a specific value, for
example 0.5 or 1.0 in. (12 to 25 mm). This is the simplest criterion because it is
read directly from the load-settlement curve, as point H in Fig. 23.14, and is
based on the amount of settlement that can be tolerated by a structure instead
of depending on shifting pile-soil interactions.
 Gross settlement can be defined as a function of rate, for example 0.01, 0.02, or
0.05 in./ton (0.03, 0.06, or 0.15 mm/kN). These criteria are shown by the slopes
of lines OA, OA0 , and OA00 in Fig. 23.14. A failure load is found by shifting
the selected line until it is tangent with the load-settlement curve. A factor of
safety of 2 then is applied. The steepest line, OA00 , probably defines a realistic

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696 Geotechnical Engineering

failure load for this pile. A limitation of this criterion is that the slope may
not be attained in the load test because of limits imposed by the jacks and
anchors.
 The net settlement rate may be limited to an arbitrary value as in paragraph 1,
and a factor of safety of 2 applied. This in effect rotates the allowable
slope base line by an angle  in Fig. 23.14 so that it is parallel to the rebound
curve, giving slopes OB, OB0 , and OB00 in the figure. The line then is shifted until
it is tangent to the load curve as in the preceding criterion. Net settle-
ment eliminates most of the elastic compression that depends on pile length
and material, but it should be recognized that some compression remains
after full removal of load because of residual side forces that act upward on the
lower part of the pile and downward on the upper part as the pile rebounds
elastically.
 Net settlement may be limited to a specific value, for example 0.25 or 0.5 in.
(6 or 12 mm), in which case the failure load is obtained by parallel shifting of
the rebound curve so that it intersects the desired settlement value, and reading
where this line intersects the load curve, for example G in Fig. 23.14. A factor
of safety of 2 usually is applied.

Other criteria such as defining a ‘‘break in the curve,’’ or using a point defined by
tangents drawn on either side of a break, are more arbitrary and depend on the
scale of the plot and the maximum applied load. Another criterion is to define an
allowable settlement for a given load increment, in which case that load increment
must be defined.

The safe load for a pile or pier is one in which settlement is not excessive for the
intended use. A factor of safety is necessary to cover variable soil and pile
conditions and to a lesser extent unanticipated loading conditions. Since most
pile-soil systems gain strength with time, the eventual mean factor of safety
ordinarily will increase over that defined by the load test.

23.6.3 Uplift Test


Piles or piers that are intended to resist uplift also can be tested with an
arrangement similar to that in Fig. 23.13 except that the center pile is attached to
the cross-beam that is jacked against the end piles. A pullout test of course
mobilizes only side friction with no end bearing.

23.6.4 Two-Way Osterberg Test


A recent innovation by Dr. Jorg Osterberg, an emeritus professor at Northwestern
University, pushes up on a pile or pier while pushing down on soil at its base,
by use of an expanding hydraulic load cell, called an Ostberg cell or ‘‘O-cell.’’
A schematic diagram is shown in Fig. 23.15. Two telltales or vertical rods
are attached to opposite sides of the cell and extended to the ground surface
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Deep Foundations 697

Figure 23.15
Schematic of the
Osterberg cell for
pushing upward on
a pile or pier.

to provide a base for strain measurements. The O-cell is particularly useful for
large-capacity piers that would require a massive reaction beam and jacking
capability. A special version of the device can be attached to the ends of driven
piles. However, the O-cell is not recovered after a test, which adds to the cost of
the test.

As can be seen from the data in Fig. 23.16, the maximum load depends on which
yields first, side friction or end bearing. In most cases side friction is the first to
peak out, and end bearing is estimated by extrapolation. The data in Fig. 23.16
indicate a failure load of about 7400 plus about 8000 tons (65 plus 55 MN). This is
one of the largest capacity piers ever tested.

With the O-cell side friction and bottom bearing are developed simultaneously,
whereas when a pile or pier is put into service with top-down loading, side friction
initially will carry all of the load prior to activation of bottom bearing. This
introduces a depth variable in the test, as side friction generally is higher at depth
because of higher normal stresses. If and when side friction is fully mobilized in
the test, indicated by side shear movement equaling and exceeding bottom
movement, it should make no difference whether shearing is acting upward or
downward. The predicted settlement then may equal bottom movement plus
elastic compression of the pile or pier, taking into account the cumulative nature
of side shear with depth.

23.6.5 Electronic Analyzers


An electronic ‘‘pile analyzer’’ consists of transducers and accelerometers attached
to the top of a pile in order to monitor the force transmitted to the pile and its
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698 Geotechnical Engineering

Figure 23.16
O-cell data for a
9 ft diameter pier
50 ft deep at
Apalachicola
River, Florida.
(after Osterberg,
2004).

velocity during driving. This bypasses the effect of an important uncontrolled


variable, e, of the wooden cap blocks. The procedure is more direct than a wave
equation analysis but still incorporates an arbitrary soil ‘‘damping constant.’’
Testing is repeated after a waiting time to evaluate a setup factor.

Flaws and Integrity Testing


Flaws in concrete piles or piers can remain undetected until one breaks during a
load test. This is indicated by a sharp plunge, and is symptomatic of improperly
cured concrete, cracks from handling, tension cracks from driving, or soil falling
or pushing into a boring to displace fluid grout or concrete. Failure during a load
test is painful for everybody involved, particularly if other foundation elements
already are in the ground.

Failure of a single high-capacity pier ordinarily cannot be tolerated, so if a test


fails, one alternative is to diamond-bit core for the full length of every pier to
ensure its integrity. A far simpler procedure that is less definitive involves
attaching a transducer to the top of the foundation element and hitting with a
hand-held hammer. A plot of pulse versus time will reveal flaws that are
sufficiently large that they will create multiple echoes in addition to an echo
emanating from the bottom of a pile or pier. This test is most useful for pile
lengths that are less than 30 diameters.

The high cost of pulling and replacing weak or broken piles or piers can result in
project abandonment, or in shifting to a slightly different footprint that will allow
installation of all new foundation elements. Far better is to get things right the
first time.

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Deep Foundations 699

23.7 END BEARING ON ROCK

23.7.1 Knowing the Geology


It often is assumed that the safest foundation is on rock, and end bearing can be
based on the unconfined compressive strength. However, the rock may be a mix of
weak and strong layers of shale, limestone, and sandstone, or it may be deeply
weathered. As the rock surface cannot be inspected except in borings, these are
only some of many what-ifs. Rock avoids some soil problems but substitutes
others, most having to do with competence of the rock.

23.7.2 Depth to Sound Rock


A first requirement is to measure the depth to rock by drilling or seismic
exploration, in order to determine if end bearing on rock is economically feasible.
As most major cities and nearly all bridges are founded on or adjacent to river
floodplains, the most common soil cover for rock encountered in engineering
is alluvium. The depth to rock obviously depends on thickness of the alluvium,
which can be considerable, caused by the 400 þ ft (120 þ m) rise in sea level at
the end of the Pleistocene, which caused all graded river valleys to fill with sand
and gravel.

Even after solid rock is encountered in exploration borings, they may be


continued for a set distance such as 10 ft (3 m) into the rock to ensure that it is not
an isolated mass that slid down some primordial slope and happened to be
encountered by the test boring. There still remains a possibility for vertical
discontinuities such as clay-filled faults or fractures that most likely will be missed
by exploration drilling. For example, if vertical discontinuities constitute
a 5 percent area coverage, the probability of encounter by a single boring is
only 1 in 20, or by 10 borings still only 1 in 2. Such discontinuities often are
discovered later in foundation excavations or pier borings, where they may require
remedial ‘‘dental treatment’’ or grouting.

23.7.3 Gradational Contact


Rock weathers along fractures and bedding planes that allowed infiltration
of surface water at the time when the rock was exposed at the ground
surface. A common result is a gradual transition with depth from residual soil
at the buried former ground surface to soil containing rock fragments to solid
rock. Driven piles with hardened steel points are often used to penetrate through
the weathered zone into solid rock. For bored piers the boring machine must
have sufficient power to penetrate through the weathered zone and create a
‘‘rock socket.’’

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700 Geotechnical Engineering

Side Friction
Side friction generally is not included in design of end bearing on rock, but is a
consideration for development of negative skin friction.

Rock Competence
The competence of rock commonly is estimated from the percentage of com-
petent core recovered during exploration drilling. This is the ‘‘rock quality
designation’’ or RQD. The modulus of a rock with weathered seams is mainly
a function of the thickness and spacing of the seams, which contain material
that may not be normally consolidated because of support from arching action.
The modulus therefore decreases rapidly and somewhat erratically depending
on the RQD, a 30 percent decrease in RQD causing about an 80 percent decrease
in modulus. Clues can be obtained from cross-hole seismic testing, and a modulus
can be more accurately evaluated with rock pressuremeter tests (Failmezger et al.
(2005)).

Experience in local areas often leads to bearing capacity criteria for particular
rocks and may become the basis for local building code requirements. Obviously,
caution must be used in applying such criteria to other areas and in particular to
other rock types, as even a rock name such as ‘‘shale’’ or ‘‘limestone’’ can cover a
wide range of strength properties.

One approach to design is to consider only the material in weathered seams as


contributing to settlement, and test that material in a consolidation test. Results
then are reduced by a percentage that represents the amount of dilution by rock
fragments. For example, if the rock is 90 percent sound rock fragments, test data
on soil separating the fragments can apply to only 10 percent of the weathered
rock mass and therefore can be divided by 10. This method is only approximate
and is sensitive to the bearing load because of the influence of arching action.
The answer for design usually is in load tests of completed piles or piers, and the
final answer is in the performance.

23.8 PILE GROUPS

23.8.1 Pile Interaction


Piles frequently are used in groups in order to obtain a required bearing
capacity. The pile group usually is connected at the top with a concrete pile
cap so that loading is simultaneous and stress fields around and under
the piles overlap. For example, if two adjacent friction piles are loaded
simultaneously, soil between the piles will be subjected to a downward force
on both sides and will tend to compress more than if it were adjacent to a
single pile.

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Deep Foundations 701

The bearing capacity of a pile group therefore includes a factor for efficiency:

Qg ¼ EnQ ð23:20Þ
where Qg ¼ bearing capacity of the pile group;
E ¼ efficiency;
n ¼ number of piles in the group;
Q ¼ bearing capacity of individual pile.

Simultaneous downloading of a group of piles is difficult because of the large


forces involved, but loading can be accomplished with Osterberg cells. Another
approach is to use scale models, but in order to meet physical requirements as
dimensions are scaled down, unit weights should be scaled up. This can be
accomplished in a centrifuge.

23.8.2 The Feld Rule


A simple procedure to account for pile interactions was introduced by Jacob Feld,
and involves reducing the bearing capacity of each pile by one-sixteenth for each
adjacent pile, whether on a diagonal or a straight row. The rule derives from the
assumption that frictional resistance is compromised along arc distance a in
Fig. 23.17. The minimum ratio of spacing to diameter, S/D, is approximately 2.5,
in which case
tanð0:5Þ ¼ ð0:5SÞ=L

Figure 23.17
Derivation and
example of the
Feld rule.

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702 Geotechnical Engineering

Substituting S ¼ 2.5D,
tanð=2Þ ¼ ð0:5DÞ=2:5D ¼ 0:20
a ¼ 22:6
22:6=360 ¼ 0:063 ¼ 1=16

Example 23.10
Calculate efficiency of a 9-pile group in Fig. 23.17 using the Feld rule.

Answer: There are 5 piles, and summing the reductions gives 16/16. This is the equivalent
of 5 – 1 ¼ 4 stand-alone piles, for an efficiency of 80%.

Question: Would eliminating the center pile increase the efficiency? Would it reduce the
load-carrying capacity?

Model tests summarized by Poulos and Davis (1980) indicate that, for a spacing of
2.5D in various size groups the efficiency varied from 0.7 to 0.9, averaging about
0.8. With larger spacings the efficiency is slightly higher. Pile group reduction
factors are appropriate for friction piles in clay but not for end-bearing or for
driven piles in sand, where the efficiency is 1.0 and may exceed 1.0 because of
densification of the sand.

23.8.3 Bearing Capacity of a Pile Group


Terzaghi and Peck (1967) introduced a concept that a large pile group should be
tested for bearing capacity failure as a group that in effect is acting as a single
foundation (Fig. 23.18). This is unlikely to occur in soils having internal friction
because the depth factor Nq in the bearing capacity equation will be quite large.
The evaluation therefore is most appropriate for poorly drained clay, as in
eq. (23.8). Applying this equation to a pile group and adding perimeter shear
resistance gives
Qg ¼ cð9BAÞþcð2BLþ2ALÞ

Figure 23.18
Bearing capacity
of a pile group.

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Deep Foundations 703

Qg ¼ cf9BA þ 2LðB þ AÞg ð23:21Þ

where Qg is the net bearing capacity of the group, c is the undrained soil cohesion,
B and A are the plan dimensions of the group, and L is the pile length. Every large
pile group should be checked for this failure mode, particularly in soft soil with
short pile lengths.

Example 23.11
Find the maximum allowable net bearing capacity of a pile group with L ¼ 20 ft (6.1 m),
D ¼ 1 ft (0.3 m), A ¼ 30 ft (9.1 m), and B ¼ 20 ft (6.1 m), and compare with the bearing
capacity using the Feld rule. The soil is clay, c ¼ 500 lb/ft2 (23.9 kPa), and  sub ¼ 60 lb/ft3
(9.4 kN/m3).

Answer: From eq. (23.21), for the pile group,

Qg ¼ 500 lb=ft2 ½9ð30Þð20Þ þ 2ð20Þð30 þ 20Þ ft2 ¼ 500½5400 þ 2000


¼ 1850 tons, or ¼ 23:9 kPa ½9ð9:1Þð6:1Þ þ 2ð6:1Þð9:1 þ 6:1Þ m2 ¼ 16:4 MN

Single pile:
Qs ¼ cLðB=2Þ2 ¼ 500ð20Þð3:14Þð0:5Þ2 ¼ 7850 lb
Qbnet ¼ 7cB2 ¼ 7ð500Þð1Þ2 ¼ 3500 lb
Q ¼ 7850 þ 3500 ¼ 11,350 lb ¼ 5:68 tons ð50:5 kNÞ

Feld rule: Assume a spacing of 2.5D, or 2.5 ft center to center. The group will be
(30/2.5 – 1) ¼ 11 piles in the A direction and (20/2.5 – 1) ¼ 7 piles in the B direction, or
77 piles total. This will include:
4 corner piles each having an efficiency of 13/16, giving 4  13/16 ¼ 3.25 pile equivalencies.

2(7 – 2) þ 2(11 – 2) ¼ 45 edge piles, each with 9/16, which gives 25.3 equivalencies.

77 – 45 – 4 ¼ 29 center piles, each with 8/16, which gives 14.5 equivalencies for a total of
3.25 þ 25.3 þ 14.5 ¼ 43, or an efficiency of 43/77 ¼ 56%.

Q ¼ 0.56(77)(45) ¼ 1940 tons (17.3 MN) or approximately the same as the group bearing
capacity.

23.8.4 What Is an Appropriate Factor of Safety?


It will be recalled from the previous chapter that the factor of safety that is
based on a foundation load is not the same as the factor of safety against shear
failure in the soil, which is smaller. Global factors of safety for pile, pier, and
pile group bearing capacities are a mix, as they include both a load criterion
for punching shear and a shear strength criterion for side friction. For example,
at the right in Fig. 23.16 when side friction is fully mobilized and its factor of
safety is 1.0, end-bearing is not fully mobilized and its factor of safety is greater
than 1.0.

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704 Geotechnical Engineering

Because of reliance on load tests, a factor of safety of 2 for load is generally


considered acceptable for deep foundations even though in terms of shear failure
it is lower than that.

23.9 SETTLEMENT OF PILE GROUPS

23.9.1 Overview
The larger the base area, the deeper the pressure bulb and the more soil will be
involved in consolidation settlement. A procedure suggested by Terzaghi and Peck
(1967) is widely used and is somewhat similar to that used for bearing capacity of
a pile group but with an important difference: the center of action is assumed
to be at two-thirds of the depth of the pile (Fig. 23.19). In other words, for
settlement calculations it is as if the pile group is replaced by a shallow foundation
having the same size and extending to a depth equal to two-thirds of the lengths
of the piles.

Fellenius (1991) suggested a rationale for this procedure, that settlement of soil
adjacent to the pile creates negative skin friction on the upper part of the pile.
As this is opposed by positive skin friction on the lower part, there exists a neutral
plane where there is no shearing stress and no shearing movement between the soil
and the pile. The load from the pile group therefore can be conceptually replaced
with a foundation at the elevation of the neutral plane. For friction piles the
neutral plane is at about the one-third point, and for end-bearing piles it is at
the bottom of the piles. The position of the neutral plane dictates the level of the
equivalent foundation.

Figure 23.19
Terzaghi-Peck equivalent foundation method for predicting settlement of a pile group. Negative
skin friction can be caused by surface loading of the soil and/or lowering of the groundwater
table.

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Deep Foundations 705

Example 23.12
A 1000 ton (8.9 MN) surface load is supported by a 24 ft pile group 20  40 ft
(6.1  12.2 m), on soil having a cohesion of 400 lb/ft2 (19.2 kPa). Estimate the vertical
stress at a depth of 8 ft below the bottom of the piles.

Answer: A depth of 8 ft below the pile tips is 8 þ (24/3) ¼ 16 ft (4.9 m) below the neutral
plane. With a 2:1 slope this extends the base dimension 16/2 ¼ 8 ft in four directions, giving
an expanded area of (20 þ 16)(40 þ 16) ¼ 2016 ft2 (57.1 m2). The pressure at this level is
1000/2016 ¼ 0.5 ton/ft2 ¼ 1000 lb/ft2 (48 kPa).

23.10 SPECIAL TOPICS

23.10.1 Soils that Can Lift and Pull Piles


Deep foundations often are used to isolate a structure from the effects of clay
expansion, where a structure founded on shallow foundations would be racked
and destroyed. During the expansion cycle of such a clay, the normal stress
against the sides of a pile can be multiplied by as much as 6 or 8 times in the active
zone of the soil, which can extend from 7 to 10 ft (2 to 3 m) below the ground
surface. This adds friction to cohesion so expansion also can lift the pile itself.
In fact, in areas of severe expansive clay problems bell-bottomed piers may be
used, not for their larger bearing area but to prevent uplift.

Side shear can be reduced by using protective sheaths that can slip on the pile, or
coating the pile with soft mastic layers. Foundation elements of course must be
reinforced to withstand tensile forces.

Where structures are supported on piles, floors that normally would be in contact
with the soil also must be supported or they can be lifted by clay expansion. This
is called a ‘‘structural floor,’’ and is supported on beams connected to the pile.
It also is critical that a sufficient clear space be left under the floor to allow for
clay expansion.

A similar problem can occur as a result of freezing of soil to the surface of a pile or
pier, followed by frost heave of the soil. This mainly occurs in frost-susceptible
silty soils with access to water. In permafrost areas, foundations can be extended
into the permafrost where they may be presumed to remain permanently frozen,
subject to climatic influences.

23.10.2 Lateral Loading


Lateral loads commonly are imparted to pile foundations from the following
causes:
 Wind.
 Earthquakes.
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706 Geotechnical Engineering

 Bridge pier supports, from current, floating debris, and ice.


 Wharves, piers, and offshore structures, from wind, waves, ice, moored ships,
and ships coming to berth. Unbraced piles intended to absorb ship impacts are
called fender piles.
 Railway bridges, from train sway, traction, braking, and centrifugal force on
curves.
 Machinery vibrations, especially large, horizontal compressors.

Lateral forces can be provided for in design by combining vertical and nonvertical
or ‘‘battered’’ piles in the same pile group, the latter to act as braces. In some
applications, such as for bridges, lateral forces can be expected to come from one
direction, whereas in other situations, such as an earthquake, they may come from
any direction. Design with batter piles is simply a matter of drawing force
diagrams with forces parallel to the pile directions, or of calculating the horizontal
component of batter pile resistance and comparing to anticipated lateral loads.
If appropriately pinned and reinforced, batter pile may act in tension as well as in
compression.

Example 23.13
A bridge pier will exert a vertical force of 440 tons (3.9 MN). Select an array
of 50 ton (443 kN) piles with 70% efficiency due to group action, to support this load
plus a maximum anticipated lateral load of 44 tons (390 kN) caused by current, ice,
and debris.

Answer: Each pile capacity is 0.7  50 ¼ 35 tons (310 kN). The horizontal capacity of this
pile driven at 208 batter is 35 sin 208 ¼ 12 tons (106 kN), To meet the required 44 tons, four
piles in the group must be battered at that angle. The next step is to determine the vertical
capacity of the four battered piles, which is 4  35 cos 208 ¼ 131 tons (1165 kN). The required
number of vertical pile therefore is (440 – 121)/35 ¼ 8.8, so the pile group will have 9 vertical
piles plus 4 battered at 208.

23.10.3 Pile Design for Lateral Loads


Another option is to design vertical piles to resist lateral forces, the
two criteria being deflection and maximum resistance to a lateral load. The
first criterion, the amount of allowable deflection, can be approached by
assuming ideal elastic behavior, but a more common procedure is to use the
same modulus as used in pavement design, called the modulus of subgrade
reaction. Test data show this modulus to increase with depth, so the inter-
action between soil resistance and bending moment is defined by a ‘‘p-y curve,’’
where p indicates pressure and y indicates depth. Determination of a p-y curve
is beyond the scope of this book and usually is accomplished with a com-
puter program. For descriptions of analytic methods see Prakash and Sharma
(1990).

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Deep Foundations 707

23.10.4 Wind, Signs, and Light Poles


Shallow foundations are not practical for resisting wind forces on elevated signs
because of the large pad area and weight required to develop a large resisting
moment. One solution is to simply insert the poles deep enough into the soil so
they will not tip and tear out a chunk of soil, like a spade when the handle is
pushed down. In this case the amount of deflection is less important than the
lateral bearing capacity. A simple procedure was devised by Rutledge (1947)
to determine a minimum embedment depth. (The authors are indebted to
Dr. John Schmertmann for pointing out this method.)

Rutledge based his procedure on lateral pull-tests using a 1.5-inch diameter steel
auger, and significantly, signposts that have endured a hurricane generally are
bent instead of being ripped out of the ground. The assumed stress distribution is
shown at the right in Fig. 23.20, which also includes Rutledge’s nomograph that
can be used for a solution. A factor of safety is incorporated into the soil strength
data, and a deeper embedment is required in sands because of the dependence of
frictional strength on overburden pressure. It is recommended that SI units be
converted to ft-lb-sec for use of this method.

A diagram of wind pressure versus velocity is shown in Fig. 23.21. Arrows


indicate pressures from a 100 mph (160 km/hr) wind.

Example 23.14
Determine the embedment depth in soil having an unconfined compressive strength
of 2000 lb/ft2 for a 20 ft long, 1.5 ft diameter pole supporting a sign having an area of 20 ft2,
to resist a wind of 100 mph.

Figure 23.20
Nomograph for
calculating
required
embedment depth
for pole
structures.
(Redrawn from
Rutledge, 1947.)

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708 Geotechnical Engineering

Figure 23.21
Wind pressure as
a function of
velocity. Arrows
show pressures
from 199 mph
(320 km/hr) wind.
(Drawn from data
of Farr, 1980.)

Answer: With a factor of safety of 2 the allowable horizontal stress is 1000 lb/ft2, which is
entered on the left scale. The wind force is 1.5  20  16 þ 20  25 ¼ 980 lb, which is entered
on the P scale. A line through these two points reads 0.97 on the C scale. Then draw a line
through 0.97 and 18 in. on the b scale and read 0.68 on the L scale. A horizontal line from
0.68 intersects the H ¼ 10 ft mid-height to give 5 ft embedment.

23.10.5 Increase in Pile Friction from Lateral Load


Lateral loading can substantially increase the bearing capacity of piles by
increasing normal stress and therefore the side friction as the pile tends to rotate
about a point near the center (John Schmertmann, personal communication). This
has been confirmed by pullout tests and may be an important factor that can aid
design to withstand hurricane-force winds, but does not appear to have been
incorporated into design. The concept is relatively straightforward: a lateral force
at the top of a pile will develop an opposing couple from a triangular distribution
of pressure that is a maximum at the ground surface and at the bottom of the pile.
These forces multiplied by a coefficient of friction equals the increase in side
resistance. This will be accompanied by decreases in normal stress and friction on
the opposite sides of the pile, but the increase should be substantially larger than
the decrease. A trial calculation indicates as much as a 100 percent increase in
pullout capacity, depending on the soil, which may have saved more than a few
structures from tipping over in a strong wind.

Problems
23.1. What are friction piles? End-bearing piles? Compaction piles? Describe the
soil requirements for each. What distinguishes between a pile, a pier, and a
caisson?
23.2. What are the principal materials in deep foundation piles?
23.3. What are batter or spur piles and why are they used?

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Deep Foundations 709

23.4. A bridge pier in a navigable stream is supported on bearing piles. What


functions do the piles perform in addition to increasing the load-carrying
capacity of the pier?
23.5. What precautions can be taken to increase the useful life of wood pile?
23.6. What is a bored-and-belled pier and how is it installed?
23.7. Cite some advantages of steel H-beam piles for end bearing. Can steel
H-beams be used as friction pile? Explain.
23.8. Join appropriate pairs:

A. Franki a. negative skin friction


B. end-bearing b. pier
C. bored and cast-in-place c. taper
D. driven pile d. pedestal
E. steel shell e. mandrel

23.9. A pile is driven by a drop hammer weighing 17.8 kM (4000 lb). The height
of fall is 3 m (10 ft) and the average penetration of the last few blows is
1.27 mm (0.05 in.). What is the bearing capacity of the piles according to
the Engineering News formula?
23.10. The pile of Problem 23.15 is concrete, 254  254 mm (10  10 in.)  9.1 m
(30 ft) long. The driving cushion is oak. What is the bearing capacity by
the Michigan formula?
23.11. A pile is driven by a single-acting steam hammer which weighs 8.9 kM
(2000 lb). The height of fall is 1.2 m (4 ft) and the average penetration
under the last few blows is 8.4 mm (0.33 in). What is the bearing capacity
of the pile by the Engineering News formula?
23.12. Explain how driving forces can induce tension in a pile.
23.13. A second test pile is driven under the same conditions as in Fig. 23.8 until
the driving resistance is 50 blows/0.3 m (ft). Two weeks later the pile is
re-driven with the same hammer, and 16 blows were found to be necessary
to advance the pile 25 m (1 in.). What is the setup factor? How is this
used in design?
23.14. As a professional engineer you review a foundation design with piers
appropriately belled out to rest on a top of a layer of stiff clay, and above
the clay is a saturated sand. Is this design acceptable? Why (not)? What is
meant by ‘‘buildable?’’
23.15. An 0.9 m (3 ft) diameter straight bored pier is founded at a depth of 10.4 m
(34 ft) in clay which has an average unconfined compressive strength of
47.9 kPa (1000 lb/ft2). Calculate end bearing, side friction, and the allow-
able bearing capacity with a factor of safety of 2.0.
23.16. Check the previous answer for settlement.
23.17. The pier of Problem 23.15 was installed and tested, and settled excessively
at 180% of the design load. Revise the design with a longer pier that will

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Deep Foundations

710 Geotechnical Engineering

provide a factor of safety of 2.2 and explain why you require 2.2 instead of
the target 2.0.
23.18. Design a pier that will carry 20 tons in end bearing on sand with an
average blow count of 12 blow/ft and check for settlement. The factor of
safety will be 2.0.
23.19. Make a preliminary estimate of side friction and end bearing of a 15 ft, 1 ft
diameter pile driven in soil with an unconfined compressive strength of
800 lb/ft2. What assumptions are made in your analysis?
23.20. A 10 ft, 0.5 ft diameter pipe pile is driven in sand having an internal
friction angle of 308. Calculate side friction assuming that K ¼ 1.0,
 ¼ 120 lb/ft3, and contact friction is 80% of the internal friction.
23.21. A group of 24 piles 0.3 m (1 ft) in diameter is driven in four rows of six
piles each. They are spaced 1.1 m (3.5 ft) center to center. If each individual
pile has a bearing capacity of 214 kN (24 tons), determine the bearing
capacity of the group and indicate the criterion.
23.22. If the piles in Problem 23.21 are driven 6.1 m (20 ft) into cohesive soil
having an unconfined compression strength of 19.2 kPa (400 lb/in.2), check
to determine stability of the whole group.
23.23. What area should be used to determine the average vertical stress in soil at
the bottom of the piles in Problems 23.21 and 23.22?
23.24. Calculate vertical soil stress imposed by the pile group in Problems 23.21
and 23.22 at a depth 10 ft below the bottom. How would this value be used
to predict settlement?
23.25. Sketch the arrangement for a pile load test, indicating jacks, reinforced
anchor piles, and dial gauges. What loading sequence should be used for a
pile with a design load of 120 tons?
23.26. What are the failure loads and working loads of the pile in Fig. 23.14
according to the 29 mm/N (0.01 in./ton) gross settlement and net
settlement criteria? Are these reasonable criteria for this test?
23.27. Deep foundation elements are to be installed in a soil with the
groundwater table at a depth of 8 ft. Soil samples show mottled gray
and brown colors to a depth of 18 ft. What water table depth should be
used in design? How will this affect a design?
23.28. Give reasons why the natural groundwater table generally is lowered in
cities.
23.29. Calculate the maximum tensile and net uplift forces on a 0.3 m (12 in.)
diameter end-bearing pile extending through 6.1 m (20 ft) of expansive
clay, one-third of which is below the permanent water table. Assume
c0 ¼ 14 kPa (2 lb/in.2).
23.30. Design a vertical and batter 6-pile system to sustain bidirectional
lateral loads equal to 30% of the vertical load, all piles being equal in
length.

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Deep Foundations

Deep Foundations 711

23.31. Telephone poles averaging 20 inches in diameter with an above-ground


height of 30 ft long are designed for a wind speed of 120 mph. Ignore wind
pressure on the cross-bars and lines and determine the embedment depth
in soil having an unconfined compressive strength of 1600 lb/ft2.

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