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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 193
NUMERICAL MODELING TO EVALUATE PILE HEAD DEFLECTION
UNDER THE LATERAL LOAD
Kedar C. Birid1
1
Assistant Manager, Toyo Engineering India Pvt. Ltd., Mumbai, Maharashtra, India, kedarbirid@gmail.com
Abstract
The complex behavior of pile head deflection under the lateral load can be studied using various analytical methods and the
softwares. Often the lateral pile load testing is carried out in the field to confirm the calculated lateral pile capacity. However,
even with the use of sophisticated latest softwares, the accurate deflection of pile head cannot be estimated. Hence an attempt has
been made in this paper to evaluate the pile head deflection using the field load-deflection data and the corresponding soil and
pile properties. A preliminary mathematical model has been developed using a technique of dimensional analysis (DA) to evaluate
pile head deflection under different pile diameters, different pile materials and varying soil conditions. The estimated pile head
deflection using DA equation is compared with 14nos. of measured lateral pile load test results conducted at the site. It can be
observed from this study that, the dimensional analysis can be used effectively to estimate the pile head deflection. More variables
based on more field results can be introduced in the mathematical model to increase the accuracy in the estimation of pile head
deflection.
Keywords: Pile head deflection, Lateral pile load, Dimensional analysis
--------------------------------------------------------------------***----------------------------------------------------------------------
1. INTRODUCTION
The pile foundations subjected to lateral loading involve
complex soil structure interaction. There are several
analytical methods and softwares are available to study the
pile behavior. In spite of the availability of the latest
techniques and softwares, it is invariably recommended to
carry out the field pile load tests to understand the correct
behavior of pile under the lateral loading. It would be
therefore realistic if the pile behavior is modelled directly
based on the field data on test piles. The parameters that
affect the pile head deflection under the lateral loadings can
be assigned with appropriate weightage depending on its
contribution in deflecting the pile under lateral load. The
author has attempted development of such mathematical
model using dimensional analysis to assess its applicability
in soil-structure interaction problem. The field test results of
lateral pile head deflection under free head condition were
processed using a mathematical tool of dimensional analysis
to arrive at a correlation equation.
2. NUMERICAL MODELING USING
DIMENSIONAL ANALYSIS
In physics and all science, dimensional analysis is the
practice of checking relations between physical quantities by
identifying their dimensions. The dimension of any physical
quantity is the combination of the basic physical dimensions
that compose it. Some fundamental physical dimensions are
length (L), mass (M) and time (T). All other physical
quantities can be expressed in terms of these fundamental
physical dimensions. As examples, the dimension of the
physical quantity speed is the distance (length/time) i.e. L/T
or LT−1
, and the dimension of the physical quantity force is
"mass × acceleration" or "mass×(length/time)/time" i.e.
ML/T2
or MLT−2
.
Dimensional analysis is a proven mathematical solution to
develop numerical models for various civil engineering
problems such as reinforced concrete beams subjected to
pure torsion [4], bearing capacity of footings in sand [5],
estimation of phreatic line in earthen dams [6],
determination of the corrected compressive strength of rock
[2] and others. It was therefore decided to apply the same
numerical technique for estimation of pile head deflection
under the lateral loading in the present case.
The basis of dimensional analysis and the methodology has
already been explained by Butterfield [3] and the current
paper uses same notations and symbols.
The aim of dimensional analysis is to reduce the dimension
space to a minimum in which the behavior of a specific
system might be studied by combining and arranging
systematically the assumed governing variables (v) = (v1, v2,
v3,……, vn) encompassing a total of m independent primary
dimensions (Dp) = (D1, D2, D3,…..,DN) into N= (n-m)
Dimensionless Groups (D.G.s), that are (π1, π2, π3,……,
πN), N being less than v [2].
Here D = Diameter of pile in m.
Ep = Modulus of elasticity of pile material, kN/m2
Es = Average modulus of elasticity of soil up to 5m
depth from the pile head, kN/m2
H = Lateral load on pile head, kN
y = Pile head deflection in m.
Here, we have v = {D, Ec, Es, H, y}, hence n = 5
Writing the dimensions of the variables
{v} = [M0
LT0
, ML-1
T -2
, ML-1
T -2
, MLT -2
, M0
LT0
], m = 3,
i.e. the number of repeating variables forming a set Q (i.e.
M, L & T).
Let MLT-2 =
P
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 194
Therefore, v = {L, PL-2
, PL-2
, P, L} and m = 2 (i.e. P & L).
The number of the dimensionless Pi – group is
N = (n-m) = (5-2) = 3
now R = set of variables in v which have dimensions totally
distinct from each other.
Therefore, R = {D, Ep, H}
Q is to be selected from R, therefore Q1 = {D, Ep}
Q2 = {D, H}
Q3 = {Ep, H}
Select any combination of Q e.g. Q1 = {D, Ep}
Therefore, the dimensionless groups are,
π1 = {D, Ep, Es}, π2 = { D, Ep, H}, π3 = { D, Ep, y}
Therefore, represent π1 as,
π1 = (D a
, Ep
b
, Es
c
) ---(1)
It can be written in dimensional form as,
[M0
L0
T0
] = [M0
LT0
]a
x [ML-1
T-2
]b
x [ML-1
T-2
]c
---(2)
Comparing the indices of the Left Hand Side and the Right
Hand Side, for M, L, & T from the equation (2),
M: 0 = b+c
L: 0 = a-b-c
T: 0 = -2b-2c
In order to generate relations of a, b & c with respect to each
other, select b=1
Now if b = 1, then a = 0 and c = -1
Substituting the values in the equation (1) we get,
π1 = {D0
, Ep, Es
-1
}
=
s
p
E
E
Similarly, π2 =








H
DEp
2
and π3 =
y
D
Now, let π1 = φ (π2), where φ is an unknown function.
Therefore, we can write,
3
1 )()( 


  
---(3)
Substituting the π values in the equation (3)
322
1

 














y
D
H
DE
E
E p
s
p ---(4)
To find the values of constants β1, and β2 representative field
test data have been selected based on field pile test results of
pile no. 4 (see table 1) as follows;
Diameter of pile, D = 0.45 m
Modulus of elasticity of pile material, Ep = 27386127.88
kN/m2
Average modulus of elasticity of soil, Es = 42000 kN/m2
Pls. note that, this value of Es is considered based on
average of the top 5m depth of soil from the pile head.
Lateral load on pile head, H = 72.7 kN
Measured pile head deflection, y = 2.66x10-3
m
Substituting these values in equation (4) we get
])17.169()([05.652 1
 
 ---(5)
In natural logarithmic form,
6.4801 = [ln β1 + 11.2421 β2 + 5.1309 β3] ---(6)
Solving equations (5) and (6) using trial and error we get,
β1 = 0.140, β2 = 1.018 and β3 = -0.585
Substituting the above values in equation (4) we get,
0.585- 018.1451.1018.0
14.0 
 LDEEy ps ---(7)
This universal equation (7) can be used to estimate the pile
head deflection for varying pile types, sizes, lateral loads
and soil conditions.
3. COMPARISON
The comparison of the predicted pile head deflection using
equation (7) is carried out with the field lateral load test
deflection values. 14nos. of pile lateral load tests have been
carried out as per ASTM guidelines [1] across the globe as
indicated in fig. 1 under the free head condition. The pile
types comprised of continuous flight auger (CFA) piles,
auger cast in place piles (ACIP), driven pretensioned hollow
concrete (PHC) piles, driven cast-in-situ piles, driven steel
pile and bored cast-in-situ piles of varying lengths.
The load-settlement data and the comparison of measured
and calculated pile head deflection is presented in table 1
and chart 1.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 195
Fig -1: Extent of pile test data
Chart -1: Pile head deflection-Measured Vs Calculated
from equation (7)
It can be observed from this comparison that the 64% of the
estimated values shows marginally overestimated thus
conservative results are obtained. The remaining 36%
results show lesser estimated values which can be attributed
to the inaccuracy in evaluating the soil properties and the
heterogeneous and anisotropic nature of the soil. It can also
be observed from the results of pile no. 6 and 7, both of
which from a common project in Egypt that, the ratio of
measured to actual pile head deflection is 6.45 and 7.17
respectively. Thus, there is consistency in both the results in
identical soil conditions, however the reason for such large
values of estimated pile head deflection can be attributed to
the variation in actual soil elastic modulus within top 5m
depth, as the Es value is based on the average value of top
5m soil strata below the pile head.
Table -1: Details of pile head deflection
PileNo.
Piledia,D,m
Testload,H,kN
Ep,
kN/m2
Es,kN/m2
Measuredpileheaddeflection,y,
mm
Calculatedpileheaddeflection
(usingeq.7),y,mm
1 0.60 93.5 27386128 40800 2.66 2.12
2 0.60 172.5 27386128 41400 4.84 6.01
3 0.60 124.7 27386128 42000 2.44 3.33
4 0.45 72.7 27386128 42000 2.66 2.66
5 0.45 36.4 27386128 19200 1.20 3.04
6 0.60 75.0 29580399 18432 0.87 5.61
7 0.60 100.0 29580399 18432 1.29 9.25
8 0.60 250.0 27386128 84906 7.30 3.36
9 0.60 190.0 27386128 120656 4.57 1.14
10 0.40 102.0 44721360 31033 16.22 10.61
11 0.40 260.0 44721360 34500 40.36 45.13
12 0.51 224.0 199948000 27450 43.10 27.14
13 0.51 255.0 199948000 15000 92.95 95.55
14 0.50 266.9 29580399 25777 10.70 45.27
This error can also be eliminated by introducing additional
variables related to soil properties in the mathematical
formulation based on some more field data. It shall also be
noted that all the piles in this study were behaving as long
piles with the pile head free against rotation and deflection
and hence equation (7) is applicable only for the long piles
under the free head condition. Separate field tests and the
analysis are required for the pile behaving as a short pile and
fixed head pile due to its dissimilar behavior.
4. CONCLUSION
A mathematical tool such as dimensional analysis can be
used to solve soil-structure interaction problems with a
relatively acceptable degree of accuracy for a heterogeneous
and anisotropic material like soil.
As the soil - pile analysis is one of the complex problems in
geotechnical engineering, dimensional analysis proves its
versatile applications to solve complex problems using
simple equations.
This study can be further extended using more and more
field pile test data to model the soil pile behavior with more
precision.
Egypt-2 PilesUSA-2 Piles
India-6 PilesNigeria-4 Piles
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 196
SYMBOLS
β1, β2, ….. βN constants
D Pile diameter in meter
Dp set of independent primary dimensions
D.G.S dimensionless groups represented by π1,
π2…….. πN
Ep Pile elastic modulus in kN/m2
Es Soil elastic modulus in kN/m2
H Lateral load at the pile head in kN
L length-dimension
m number of independent primary
dimensions in Dp
M mass-dimension
n number of variables or parameters
N (n-m); number of dimensionless groups
Q set of repeating variables
R set of variables in V which have
dimensions totally distinct from each other
T time-dimension
V set of independent and dependent
parameters involved in the phenomenon
y pile head deflection in meter
REFERENCES
[1]. ASTM Standard D 3966. 1990. Standard test Method
for Piles under Lateral Loads, Annual Book of ASTM
Standards, ASTM International, West Conshohocken,
PA.
[2]. Birid, K. C. 2003. Critical Assessment of
Unconfined Compressive Strength of Rock using
Modified Buckingham Method, Proceedings of Indian
Geotechnical Conference IGC, Roorkee chapter,
India,Vol-I, Dec. 18-20, 2003, pp. 529-534.
[3]. Butterfield, R. 1999. Dimensional Analysis for
Geotechnical Engineers, Geotechnique, Vol. 49, No. 3,
pp. 357-366.
[4]. Phatak, D. R. and Dhonde, H. B. 2003. Dimensional
Analysis of Reinforced Concrete Beams Subjected to
Pure Torsion, J. Structural Engineering, Vol. 129, Issue
11, pp. 1559-1564.
[5]. Phatak, D. R. and Dhonde, H. B., 2000. Discussion of
Behavior of Five Large Spread Footings in Sand, J.
Geotechnical & Geoenvironmental Engineering, Vol.
126, Issue 10, pp. 940-942.
[6]. Phatak, D. R., Pathak, S. R. and Birid, K. C. 2004.
Estimation of Phreatic Line using Dimensional
Analysis, paper no. 2.76, Proceedings: Fifth
International Conference on Case Histories in
Geotechnical Engineering, New York, NY, April 13-17,
2004, pp. 1-6.
BIOGRAPHIES
Kedar Birid: He has a masters degree from
University of Pune and has more than 15
years of diverse experience in
geotechnical engineering. He has been
associated with various multinational
geotechnical contractors, consultants and
the owners in the past. Currently he is working with Toyo
Engineering India Pvt. Ltd. as a geotechnical expert. His
research areas include application of dimensional analysis,
study of the feasibility and applications of field and lab
testing in geotechnical engineering.

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Numerical modeling to evaluate pile head deflection under the lateral load

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 193 NUMERICAL MODELING TO EVALUATE PILE HEAD DEFLECTION UNDER THE LATERAL LOAD Kedar C. Birid1 1 Assistant Manager, Toyo Engineering India Pvt. Ltd., Mumbai, Maharashtra, India, kedarbirid@gmail.com Abstract The complex behavior of pile head deflection under the lateral load can be studied using various analytical methods and the softwares. Often the lateral pile load testing is carried out in the field to confirm the calculated lateral pile capacity. However, even with the use of sophisticated latest softwares, the accurate deflection of pile head cannot be estimated. Hence an attempt has been made in this paper to evaluate the pile head deflection using the field load-deflection data and the corresponding soil and pile properties. A preliminary mathematical model has been developed using a technique of dimensional analysis (DA) to evaluate pile head deflection under different pile diameters, different pile materials and varying soil conditions. The estimated pile head deflection using DA equation is compared with 14nos. of measured lateral pile load test results conducted at the site. It can be observed from this study that, the dimensional analysis can be used effectively to estimate the pile head deflection. More variables based on more field results can be introduced in the mathematical model to increase the accuracy in the estimation of pile head deflection. Keywords: Pile head deflection, Lateral pile load, Dimensional analysis --------------------------------------------------------------------***---------------------------------------------------------------------- 1. INTRODUCTION The pile foundations subjected to lateral loading involve complex soil structure interaction. There are several analytical methods and softwares are available to study the pile behavior. In spite of the availability of the latest techniques and softwares, it is invariably recommended to carry out the field pile load tests to understand the correct behavior of pile under the lateral loading. It would be therefore realistic if the pile behavior is modelled directly based on the field data on test piles. The parameters that affect the pile head deflection under the lateral loadings can be assigned with appropriate weightage depending on its contribution in deflecting the pile under lateral load. The author has attempted development of such mathematical model using dimensional analysis to assess its applicability in soil-structure interaction problem. The field test results of lateral pile head deflection under free head condition were processed using a mathematical tool of dimensional analysis to arrive at a correlation equation. 2. NUMERICAL MODELING USING DIMENSIONAL ANALYSIS In physics and all science, dimensional analysis is the practice of checking relations between physical quantities by identifying their dimensions. The dimension of any physical quantity is the combination of the basic physical dimensions that compose it. Some fundamental physical dimensions are length (L), mass (M) and time (T). All other physical quantities can be expressed in terms of these fundamental physical dimensions. As examples, the dimension of the physical quantity speed is the distance (length/time) i.e. L/T or LT−1 , and the dimension of the physical quantity force is "mass × acceleration" or "mass×(length/time)/time" i.e. ML/T2 or MLT−2 . Dimensional analysis is a proven mathematical solution to develop numerical models for various civil engineering problems such as reinforced concrete beams subjected to pure torsion [4], bearing capacity of footings in sand [5], estimation of phreatic line in earthen dams [6], determination of the corrected compressive strength of rock [2] and others. It was therefore decided to apply the same numerical technique for estimation of pile head deflection under the lateral loading in the present case. The basis of dimensional analysis and the methodology has already been explained by Butterfield [3] and the current paper uses same notations and symbols. The aim of dimensional analysis is to reduce the dimension space to a minimum in which the behavior of a specific system might be studied by combining and arranging systematically the assumed governing variables (v) = (v1, v2, v3,……, vn) encompassing a total of m independent primary dimensions (Dp) = (D1, D2, D3,…..,DN) into N= (n-m) Dimensionless Groups (D.G.s), that are (π1, π2, π3,……, πN), N being less than v [2]. Here D = Diameter of pile in m. Ep = Modulus of elasticity of pile material, kN/m2 Es = Average modulus of elasticity of soil up to 5m depth from the pile head, kN/m2 H = Lateral load on pile head, kN y = Pile head deflection in m. Here, we have v = {D, Ec, Es, H, y}, hence n = 5 Writing the dimensions of the variables {v} = [M0 LT0 , ML-1 T -2 , ML-1 T -2 , MLT -2 , M0 LT0 ], m = 3, i.e. the number of repeating variables forming a set Q (i.e. M, L & T). Let MLT-2 = P
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 194 Therefore, v = {L, PL-2 , PL-2 , P, L} and m = 2 (i.e. P & L). The number of the dimensionless Pi – group is N = (n-m) = (5-2) = 3 now R = set of variables in v which have dimensions totally distinct from each other. Therefore, R = {D, Ep, H} Q is to be selected from R, therefore Q1 = {D, Ep} Q2 = {D, H} Q3 = {Ep, H} Select any combination of Q e.g. Q1 = {D, Ep} Therefore, the dimensionless groups are, π1 = {D, Ep, Es}, π2 = { D, Ep, H}, π3 = { D, Ep, y} Therefore, represent π1 as, π1 = (D a , Ep b , Es c ) ---(1) It can be written in dimensional form as, [M0 L0 T0 ] = [M0 LT0 ]a x [ML-1 T-2 ]b x [ML-1 T-2 ]c ---(2) Comparing the indices of the Left Hand Side and the Right Hand Side, for M, L, & T from the equation (2), M: 0 = b+c L: 0 = a-b-c T: 0 = -2b-2c In order to generate relations of a, b & c with respect to each other, select b=1 Now if b = 1, then a = 0 and c = -1 Substituting the values in the equation (1) we get, π1 = {D0 , Ep, Es -1 } = s p E E Similarly, π2 =         H DEp 2 and π3 = y D Now, let π1 = φ (π2), where φ is an unknown function. Therefore, we can write, 3 1 )()(       ---(3) Substituting the π values in the equation (3) 322 1                  y D H DE E E p s p ---(4) To find the values of constants β1, and β2 representative field test data have been selected based on field pile test results of pile no. 4 (see table 1) as follows; Diameter of pile, D = 0.45 m Modulus of elasticity of pile material, Ep = 27386127.88 kN/m2 Average modulus of elasticity of soil, Es = 42000 kN/m2 Pls. note that, this value of Es is considered based on average of the top 5m depth of soil from the pile head. Lateral load on pile head, H = 72.7 kN Measured pile head deflection, y = 2.66x10-3 m Substituting these values in equation (4) we get ])17.169()([05.652 1    ---(5) In natural logarithmic form, 6.4801 = [ln β1 + 11.2421 β2 + 5.1309 β3] ---(6) Solving equations (5) and (6) using trial and error we get, β1 = 0.140, β2 = 1.018 and β3 = -0.585 Substituting the above values in equation (4) we get, 0.585- 018.1451.1018.0 14.0   LDEEy ps ---(7) This universal equation (7) can be used to estimate the pile head deflection for varying pile types, sizes, lateral loads and soil conditions. 3. COMPARISON The comparison of the predicted pile head deflection using equation (7) is carried out with the field lateral load test deflection values. 14nos. of pile lateral load tests have been carried out as per ASTM guidelines [1] across the globe as indicated in fig. 1 under the free head condition. The pile types comprised of continuous flight auger (CFA) piles, auger cast in place piles (ACIP), driven pretensioned hollow concrete (PHC) piles, driven cast-in-situ piles, driven steel pile and bored cast-in-situ piles of varying lengths. The load-settlement data and the comparison of measured and calculated pile head deflection is presented in table 1 and chart 1.
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 195 Fig -1: Extent of pile test data Chart -1: Pile head deflection-Measured Vs Calculated from equation (7) It can be observed from this comparison that the 64% of the estimated values shows marginally overestimated thus conservative results are obtained. The remaining 36% results show lesser estimated values which can be attributed to the inaccuracy in evaluating the soil properties and the heterogeneous and anisotropic nature of the soil. It can also be observed from the results of pile no. 6 and 7, both of which from a common project in Egypt that, the ratio of measured to actual pile head deflection is 6.45 and 7.17 respectively. Thus, there is consistency in both the results in identical soil conditions, however the reason for such large values of estimated pile head deflection can be attributed to the variation in actual soil elastic modulus within top 5m depth, as the Es value is based on the average value of top 5m soil strata below the pile head. Table -1: Details of pile head deflection PileNo. Piledia,D,m Testload,H,kN Ep, kN/m2 Es,kN/m2 Measuredpileheaddeflection,y, mm Calculatedpileheaddeflection (usingeq.7),y,mm 1 0.60 93.5 27386128 40800 2.66 2.12 2 0.60 172.5 27386128 41400 4.84 6.01 3 0.60 124.7 27386128 42000 2.44 3.33 4 0.45 72.7 27386128 42000 2.66 2.66 5 0.45 36.4 27386128 19200 1.20 3.04 6 0.60 75.0 29580399 18432 0.87 5.61 7 0.60 100.0 29580399 18432 1.29 9.25 8 0.60 250.0 27386128 84906 7.30 3.36 9 0.60 190.0 27386128 120656 4.57 1.14 10 0.40 102.0 44721360 31033 16.22 10.61 11 0.40 260.0 44721360 34500 40.36 45.13 12 0.51 224.0 199948000 27450 43.10 27.14 13 0.51 255.0 199948000 15000 92.95 95.55 14 0.50 266.9 29580399 25777 10.70 45.27 This error can also be eliminated by introducing additional variables related to soil properties in the mathematical formulation based on some more field data. It shall also be noted that all the piles in this study were behaving as long piles with the pile head free against rotation and deflection and hence equation (7) is applicable only for the long piles under the free head condition. Separate field tests and the analysis are required for the pile behaving as a short pile and fixed head pile due to its dissimilar behavior. 4. CONCLUSION A mathematical tool such as dimensional analysis can be used to solve soil-structure interaction problems with a relatively acceptable degree of accuracy for a heterogeneous and anisotropic material like soil. As the soil - pile analysis is one of the complex problems in geotechnical engineering, dimensional analysis proves its versatile applications to solve complex problems using simple equations. This study can be further extended using more and more field pile test data to model the soil pile behavior with more precision. Egypt-2 PilesUSA-2 Piles India-6 PilesNigeria-4 Piles
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 196 SYMBOLS β1, β2, ….. βN constants D Pile diameter in meter Dp set of independent primary dimensions D.G.S dimensionless groups represented by π1, π2…….. πN Ep Pile elastic modulus in kN/m2 Es Soil elastic modulus in kN/m2 H Lateral load at the pile head in kN L length-dimension m number of independent primary dimensions in Dp M mass-dimension n number of variables or parameters N (n-m); number of dimensionless groups Q set of repeating variables R set of variables in V which have dimensions totally distinct from each other T time-dimension V set of independent and dependent parameters involved in the phenomenon y pile head deflection in meter REFERENCES [1]. ASTM Standard D 3966. 1990. Standard test Method for Piles under Lateral Loads, Annual Book of ASTM Standards, ASTM International, West Conshohocken, PA. [2]. Birid, K. C. 2003. Critical Assessment of Unconfined Compressive Strength of Rock using Modified Buckingham Method, Proceedings of Indian Geotechnical Conference IGC, Roorkee chapter, India,Vol-I, Dec. 18-20, 2003, pp. 529-534. [3]. Butterfield, R. 1999. Dimensional Analysis for Geotechnical Engineers, Geotechnique, Vol. 49, No. 3, pp. 357-366. [4]. Phatak, D. R. and Dhonde, H. B. 2003. Dimensional Analysis of Reinforced Concrete Beams Subjected to Pure Torsion, J. Structural Engineering, Vol. 129, Issue 11, pp. 1559-1564. [5]. Phatak, D. R. and Dhonde, H. B., 2000. Discussion of Behavior of Five Large Spread Footings in Sand, J. Geotechnical & Geoenvironmental Engineering, Vol. 126, Issue 10, pp. 940-942. [6]. Phatak, D. R., Pathak, S. R. and Birid, K. C. 2004. Estimation of Phreatic Line using Dimensional Analysis, paper no. 2.76, Proceedings: Fifth International Conference on Case Histories in Geotechnical Engineering, New York, NY, April 13-17, 2004, pp. 1-6. BIOGRAPHIES Kedar Birid: He has a masters degree from University of Pune and has more than 15 years of diverse experience in geotechnical engineering. He has been associated with various multinational geotechnical contractors, consultants and the owners in the past. Currently he is working with Toyo Engineering India Pvt. Ltd. as a geotechnical expert. His research areas include application of dimensional analysis, study of the feasibility and applications of field and lab testing in geotechnical engineering.