Foundation Analysis and Design: Dr. Amit Prashant
Load Tests on Piles
Load Tests on Piles
43 Note:
Piles used for initial testing are loaded to failure or at least twice the design load. Such piles are generally not used in the final construction.
Foundation Analysis and Design: Dr. Amit Prashant
Load Tests on Piles
Load Tests on Piles
44 Note:
ÆDuring this test pile should be loaded upto one and half times the working (design) load and the maximum settlement of the test should not exceed 12 mm.
ÆThese piles may be used in the final construction
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Maintained Load Test
Vertical Load Test: Maintained Load Test
The test can be initial or routinetest
The load is applied in increments of 20% of the estimated safe load. Hence the failure load is reached in 8-10 increments. Settlement is recorded for each
45
Settlement is recorded for each increment until the rate of settlement is less than 0.1 mm/hr. The ultimate load is said to have
reached when the final settlement is more than 10% of the diameter of pile or the settlement keeps on increasing at constant load.
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Maintained Load Test
Vertical Load Test: Maintained Load Test
After reaching ultimate load, theload is released in decrements of 1/6thof the total load and recovery is measured until full rebound is established and next unload is done.
46
After final unload the settlement is measured for 24 hrs to estimate full elastic recovery. Load settlement curve depends
on the type of pile
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Maintained Load Test
Vertical Load Test: Maintained Load Test
Æ
Æ
Ultimate Load
Ultimate Load
De Beer (1968):
Load settlement curve is plotted in a log-log plot and it is assumed to be a bilinear relationship with its intersection as failure load
47 load
Chin Fung Kee (1977):
Assumes hyperbolic curve. Relationship between settlement and its division with load is taken as to be bilinear with its intersection as failure load
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Maintained Load Test
Vertical Load Test: Maintained Load Test
Æ
Æ
Ultimate Load
Ultimate Load
Mazurkiewicz method:
Assumes parabolic curve.
After initial straight portion EQUAL settlement lines are dra n to intersect load a is drawn to intersect load axis.
Intersection of lines at 45º from points on load axis and next settlement line are joined to form a straight line which intersects the load axis as failure load.Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Maintained Load Test
Vertical Load Test: Maintained Load Test
Æ
Æ Safe
Safe
Load as per IS: 2911
Load as per IS: 2911
Safe Load for Single Pile:
49 Safe Load for Pile Group:
Foundation Analysis and Design: Dr. Amit Prashant
Elastic Settlement of Piles
Elastic Settlement of Piles
Total settlement of pile under vertical working load
50
ξ depends on the distribution of frictional resistance over the length of
pile. ξ =0.5 for uniform or parabolic (peak at mid point) and 0.67 for
triangular distribution.
Foundation Analysis and Design: Dr. Amit Prashant
Elastic Settlement of Piles
Elastic Settlement of Piles
51 Vesic’s (1977) semi-empirical method
Foundation Analysis and Design: Dr. Amit Prashant
Elastic Settlement of Piles
Elastic Settlement of Piles
2 0 35
L
I
+
52 Vesic’s (1977) semi-empirical method
2 0.35
wsI
D
= +
Empirically by Vesic (1977)0.93 0.16
.
s pL
C
C
D
⎛
⎞
=
⎜
⎜
+
⎟
⎟
⎝
⎠
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Constant Rate of Penetration Test
Vertical Load Test: Constant Rate of Penetration Test
This test is only used as initial test to determine rapidly
the ultimate bearing capacity of the pile and can not be
performed as routine test.
Load-settlement curve can not be used to predict the
settlement under working load conditions.
53
The rate of penetration is taken as 0.75 mm/min for
friction piles and 1.5 mm/min for predominantly end
bearing piles.
Test is continued until the deformation reaches 0.1D or
a stage where further deformation does not increase
load significantly.
The final load at the end of test is taken as ultimate load
capacity of pile.
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Cyclic Load Test
Vertical Load Test: Cyclic Load Test
Proposed by Van Weele(1957) with the aim of determining strength in friction and bearing separately.
Generally performed as initial test by loading the pile to
lti t it ultimate capacity Safe load for pile is
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Cyclic Load Test
Vertical Load Test: Cyclic Load Test
During this test, loading stages are performed as in the maintained load test.
After each loading, the pile is again unloaded to previous stage and deformation is measured
55 deformation is measured
for 15 min. Then, load is again increased up to next loading step. The process continues until failure load.
The recovered settlement is treated as elastic component and the permanent deformation as plastic.
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Cyclic Load Test
Vertical Load Test: Cyclic Load Test
Elastic recovery in each step is plotted against the load which comprises of the elastic deformation
(a) for mobilizing friction, (b) for mobilizing bearing, and
(c) due to the deformation of the pile itself. Æ Curve C1.
Assuming that elastic shortening of pile is zero, draw a line from
56 the origin parallel to the straight portion of the curve, which gives approximate value of the bearing and frictional resistance, as shown in the adjacent figure.
Assuming that elastic shortening of pile is zero, draw a line from the origin parallel to the straight portion of the curve, which gives approximate value of the bearing and frictional resistance, as shown in the adjacent figure.
Foundation Analysis and Design: Dr. Amit Prashant
Vertical Load Test: Cyclic Load Test
Vertical Load Test: Cyclic Load Test
Elastic compression of pile may be determined as
F is taken as varying linearly from top to bottom, so average = F/2
57 g
Elastic compression of sub-grade can be obtained by subtracting the elastic compression of pile from total elastic recovery. If this value as calculated comes out to be negative it is ignored.
This new value of deformation is plotted against the load Æ Curve C2. Bearing and frictional resistance are again evaluated as described on the last slide. This process is repeated 3 to 4 times to obtain reasonable values of frictional and bearing resistance of pile
Foundation Analysis and Design: Dr. Amit Prashant
Tapered
Tapered
Piles
Piles
Driven tapered piles with larger dimension at the top are believed to be more effective in sand deposits. Force components ti th il 58 acting on the pile are
given below.
Foundation Analysis and Design: Dr. Amit Prashant
Tapered
Tapered
Piles
Piles
Value of K for tapered piles is recommended between 1.7Koto 2.2Koby Bowels. Meyerhof (1976) suggested K≥1 5 59 suggested K≥1.5. Blanchet (1980) suggested K=2Ko. The frictional resistance of these piles is relatively larger than that of straight piles as indicated in the adjacent plot.Foundation Analysis and Design: Dr. Amit Prashant
Stepped Tapered Pile
Stepped Tapered Pile
(
2 2)
14
ledg i iA
=
π
r
−−
r
L
ledgD
si i iA
=
π
D L
. .
.
ledg ledg ledg q
Q
=
A
γ
L
N
iL
D
i1 sin
o iK
= −
φ
′
β
=
2
K
o. tan
φ
i′
. .
si siQ
=
A q
β
Foundation Analysis and Design: Dr. Amit Prashant
Uplift Piles in Clays
Uplift Piles in Clays
Uplift resistance of pile is mainly provided by its friction resistance and self weight.
Uplift capacity of pile with bottom bulb is taken as minimum of the following two equations by Meyerhof and Adams (1968)
.
u s s pQ
=
f A
+
W
uQ
p W sf
DQ
A K
+
W
+
W
Q
61.
.
u u s s pQ
=
c A K
+
W
+
W
(
2 2)
2.25
.
u b u pQ
=
π
D
−
D
c
+
W
p W sf
s W D uQ
b DFoundation Analysis and Design: Dr. Amit Prashant
Uplift Piles in Other Soils
Uplift Piles in Other Soils
Meyerhof and Adams (1968): Minimum of the three equations below 2 . . . tan 2 u b b u p Q =πc D L′ +πsγ′D L K φ′+W 2 ⎡ ⎤
(
. tan)
. . . u h b p Q = c′+σ′ φ π′ D L W+ L ≤ H Æ1 with its maximum value of 1
b b mL mH s D D ⎛ ⎞ = + ⎜ + ⎟ ⎝ ⎠ 62
(
)
2 2 . . . tan u b b u p Q =πc D H′ +sγ′D ⎣⎡L− L−H ⎤⎦K φ′+W(
2 2)(
)
. . . 4 b u c v q s s p Q =π D −D c N′ +σ′N +A f +W L > H Æ Bearing capacity failure ÆFoundation Analysis and Design: Dr. Amit Prashant
Dynamic Pile Formula
Dynamic Pile Formula
Sanders (1850):
W
=
H
=
S
=
uQ
=
Weight of hammer Height of fallPile resistance or Pile capacity Pile penetration for the last blow Wellington (1898):
63 Engineering News Formula
C
=
A constant accounting for energy loss during driving[1 in. or 25.4 mm for drop hammer] [0.1 in or 2.54 mm for steam hammer] A factor of safety FS = 6 is recommended for estimating the allowable capacity Note:Dynamic pile formula are not used for soft clays due to pore pressure evolution
Foundation Analysis and Design: Dr. Amit Prashant
Efficiency of Pile Driving
Efficiency of Pile Driving
Based on the Newton’s law of conservation of momentum. Assuming that coefficient of restitution of hammer to pile is zero and hammer moves along the pile after impact
(
)
1 2 . . W v = W+P v v1 W P .v2 W + ⎛ ⎞ = ⎜⎝ ⎟⎠ Efficiency as the ration on energy 0.20.3 0.4 0.5 0.6 0.7 η Heavier hammer or lighter piles give better efficiency e = 0 64
Efficiency as the ration on energy after and before the impact
2 2 2 2 2 1 . 2 1 . 2 W P v g W W P W W P v g W η ⎛ + ⎞ ⎜ ⎟ ⎝ ⎠ = = + ⎛ ⎞⎛ + ⎞ ⎜ ⎟ ⎜ ⎟⎝ ⎠ ⎝ ⎠ 0 0.1 0 1 2 W/P efficiency
Efficiency of blow with a non-zero value of the coefficient of restitution e. 2 2 For P W W Pe W Pe W P W P η + ⎛ − ⎞ > → = − ⎜ ⎟ + ⎝ + ⎠ 2 For W P W Pe W P η + > → = + negligible
Foundation Analysis and Design: Dr. Amit Prashant
Dynamic Pile Formula: Modified
Dynamic Pile Formula: Modified Hiley
Hiley Formula
Formula
W
=
H
=
S
=
uQ
=
Weight of hammer Height of fallPile resistance or Pile capacity Pile penetration for the last blow
α =
Hammer fall efficiency Efficiency of blowη =
65
Efficiency of blow
η =
Sum of temporary elastic compression of pile, dolly, packing, and ground
C
=
Hammer Fall Efficiency:
Foundation Analysis and Design: Dr. Amit Prashant
Dynamic Pile Formula: Modified Hiley Formula
Dynamic Pile Formula: Modified Hiley Formula
Coefficient of Restitution:
Foundation Analysis and Design: Dr. Amit Prashant
Dynamic Pile Formula: Modified Hiley Formula
Dynamic Pile Formula: Modified Hiley Formula
Temporary Elastic Compression
Temporary Elastic Compression
Driving without helmet or dolly but only a cushion or pad f 25 thi k h d 1 1 761 R C = 67 of 25 mm thick on head. 1 1.761 3.726 5.509 C A R A R A = =
Driving of concrete or steel piles with helmet and short dolly without cushion.
Concrete pile driven with only 75 mm packing under helmet and without dolly.
2 . 0.657R L C A = 3 0.073 2.806 p R C A = + p
A =Overall cross-sectional area of pile at toe in cm2
Foundation Analysis and Design: Dr. Amit Prashant
Dynamic Pile Formula: Simplex Formula for
Dynamic Pile Formula: Simplex Formula for
Frictional Piles
Frictional Piles
Frictional resistance of the pile is brought into the empirical relationship in this formula by measuring the total number of blows for driving the full length of pile.
68
Ultimate driving resistance in kN R
Length of pile in meters. Weight of hammer in kN. W H p N L
Total number of blows to drive the pile
s
Height of free fall in meters.
Average set i.e. penetration in cm for last blow being the average of last four blows.
Foundation Analysis and Design: Dr. Amit Prashant
Dynamic Pile Formula: Janbu Formula
Dynamic Pile Formula: Janbu Formula
Ultimate capacity (FS) U R
(
)
η(
1 1)
k C λ CEfficiency factor (0.7 to 0.4, depending on driving conditions) . .W H α λ Units: kN and m. 69 Weight of hammer/ram
(
)
0.75 0.15 d C = + P W W(
1 1)
U d c d k =C + +λ C P Weight of pile Area of pile H A 2 . . . . c W H A E S α λ = EHeight of free fall in meters.
Elastic modulus of pile
Set per blow as for Simplex formula s
L Length of pile