the response of p-y curve of soil-pile characterized … · 2018-12-28 · and practical...
TRANSCRIPT
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9041
THE RESPONSE OF P-Y CURVE OF SOIL-PILE CHARACTERIZED
BY THE DESIGN PARAMETERS IN LIQUEFIABLE SAND
Baydaa Hussain Maula1, Hayder Hussein Moula
2, Hussein Yousif Aziz
3 and Qais Mikhael Bahnam
1
1 Institute of Technology, Middle Technical University, Baghdad, Iraq 2Ministry of Higher Education and Scientific Research, Baghdad, Iraq
3College of Engineering, Muthanna University, Samawa, Muthanna, Iraq
E-Mail: [email protected]
ABSTRACT
This paper proposed the establishing procedure and introduced an OpenSessPL for investigating dynamic p-y
curves in liquefying ground based on the simulated shaking table tests for pile-soil-bridge structure were conducted
successfully corresponding to liquefying ground covered with clay layer simulated as a middle circumference of three
layers adopting reinforced concrete single pile-pier exposed by a series of sinusoidal and EI centro earthquake events wave
of different amplitudes and frequencies. A series of numerical simulations based on the established 3D finite element
analysis method was carried out by including earthquake events to investigate the deveplod of p-y curves due to the effect
of design parameters such as; pile stiffness, the internal angle of sand and the depth of pile insertion. The mentioned
parameters beside seismic motion shape, peak acceleration (g) and degree of ground inclination have a certain theoretical
and practical significance for seismic design related to lateral resistance and pile displacement.
Keywords: pile-soil stiffness ratio, depth of Insertion, dynamic pile response, dilation angle.
1. INTRODUCTION
It was a familiar event that pile foundations
Suffered damage by soil liquefaction due to earthquakes
[1, 2]. In fact, most of the footing destruction was
supposed to be connected with the effects occurred to the
ground prompted by liquefaction and / or lateral ground
spreading. This suggests that the effect of soil
displacement should be properly taken into consideration
when determining safely seismic design pile foundations.
An expectation of the dynamic p-y behaviors in liquefiable
soils is difficult, but achievable [3]. There are some
methods, like collecting data from investigational test and
NFEMS, which can be anticipated such manners defined
as the relationship of lateral resistance with relative
displacement between soil and pile, using a large number
of experimental data [4-9].
Figure-1. Sketch diagram of a series of shaking
table tests achieved [9].
A series of shaking table tests under the
successive support of National Natural Foundation of
China since 2002, were performed to understand the basic
mechanisms of SSPSI in Liquefiable ground, including the
cases of single piles and pile groups, low/ elevated cap pile
groups, pile groups, liquefiable / non-liquefiable ground,
different soil profile involved of two ( horizontal /slope)
[2]. Soil layers with the upper layer of thick normally
consolidated silty clay and the lower layer of thick
saturated sand beside experimental test of three horizontal
soil layers with the upper layer of thick normally
consolidated silty clay, with middle layer of deep thick
saturated sand and the lower layer of thick soft clay,
synoptically described in Figure-1.
These works have gotten the excessive value of
finding observation on the pile performance, mostly in the
soil of liquefiable trend, and have shown that the design
parameters have a significant effect on dynamic p-y
behaviour during liquefaction; however, it is indefinite
how the shape and amplitude of the diminution of p-y
curves develop through various design parameters.
Variations in soil lateral resistance during the
generation of p-y curves are required for the safe design of
pile foundations in an area subjected to tremble -induced
lateral spreading.
The main purpose of this research is to obtain
dynamic p-y curves at diverse ranges of shaking induced
liquefaction, as represented by a range of design
parameters. These constructed curves will support
computational modeling of soil-pile interaction. To report
this objective, series of modeled shaking table tests of
pile-supported structures in liquefying ground; are
conducted. In the following section parts, the
experimental-simulation, layout, procedure, and results
discussion are presented.
2. CORRELATED AND PRECEDING WORK
In previous research papers, authors reported vast
shaking table experiment in 0.2, 0.1 m diameter pile
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9042
driven into composing soil strata of liquefiable sand and
overlying soft clay. Due to the well-instrumented gauges
and sensors to the pile, bending moments imparted on the
pile shaft was measured. The Mathematical expression
represented by double integration, the moment divided by
EI concerning the length of the pile could generate soil
displacement ysoil, while double differentiation of the
bending moment achieved lateral resistance p concerning
the length of the pile.
Numerous studies and experimental researches
have been carried out at centrifuge and 1-g scales to assess
the unique behavior of the soil during liquefaction [2, 10].
Many studies; researchers realized that liquefaction
lowered the hardness and stability of the liquefiable layers.
However, such a depression was noticed. There is an
insufficiency of understanding on the shapes of the p-y
curves generated at liquefaction or during subsequent
events, for example, tests [11-12] adoption a turned S-
shaped p-y curve convex up, rather than convex down
when the surrounding soil is liquefied. Such behavior of p-
y curve designates low adjacent stability at minor to
reasonable ysoil, whereas successively gives hardening at
greater one. Liquefaction sources, deviation in p-y
manners, and the phases leading up to widespread
liquefaction have not been sufficiently examined to
contract with the p-y features.
3. NUMERICAL MODELLING OF SHAKE-TABLE
TEST
3.1 Model design and layouts
The test plan was fixed via a shake-table reported
by [2]. Including a 3D model of the soil-pile system,
shown in Figure-2, was created with OpenSeesPL. The
model dimensions are 2.0 m (long) 1.5 m (transverse) 1.9
m (height) with the same constitutive model of soil (three
layers) and (Rc) pile of 2.52m, 0.62 m part left free above
the examination system (soil-pile), with D= 0.1m as
reported by [1, 2]. The bottom of the soil domain is y m
below the pile tip. The ground surface inclination is 0, 2,
4°. Figures 2 (a) and 2 (b) and Figure 3 show the plane XZ
with an isometric view of the model, with numerical
elements respectively.
The limitation settings are factored in the
evaluating: (1) the base of the soil domain is immovable in
the three directions; (2) the boundary condition for all
planes of the model is Laminar Container and; (3) Plane of
symmetry is fixed in the y-direction and free in Z and X
direction. The base-shaking analysis is used to assess the
pile and soil behavior. Variation motion event is used as
an input motion in the longitudinal (X) direction.
The test program was exposed to a set of El
Centro and sinusoidal earthquake events with a changeable
level of shaking as characteristic ground indication
response, listed in Table-1.
Table-1. Set of seismic events.
Step event Motion Peak
acceleration (g)
A Sinusoidal 0.10g
B El Centro 0.10g
C Sinusoidal 0.20 g
(a) Plane View (b) Isotropic View
Figure-2. FEM of the SP system.
a) EDOF number b) node DOF
Figure-3. Brick element “Solid-fluid coupled 20-8 node”.
3.2 Simulation results
3.2.1 Results and interpretation
Figure-4 shows free-field displacement; pore
water pressure time histories, along with horizontal
ground displacements measured at the surface, 0.4 m, and
1.2 m depth. Generally, the Figure shows that the soil is
less displaced under case A and B.
Soil lateral displacement focuses on the surface
and the top 0.4 m of depth, as a result of liquefaction in
this area. The lowest level of liquefiable sand layer
confirmation minor effects performed comparable to an
inflexible bulk, and it's hard to slip along the base. The
upper part of the sandy soil field deforms
correspondingly.
1 2
3 4
5 6
7 8
9
10
11
12
13
14
15
16
17
18
19
20
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9043
0 2 4 6 8 10 12 14 16 18 20 22-0.06
-0.03
0.00
0.03
0.06 Soil surface
Dis
. (m
m)
0 2 4 6 8 10 12 14 16 18 20 22-0.06
-0.03
0.00
0.03
0.06 0.4 m depth
Dis
. (m
m)
0 2 4 6 8 10 12 14 16 18 20 22-0.06
-0.03
0.00
0.03
0.06 1.2 m depth
Dis
. (m
m)
0 2 4 6 8 10 12 14 16
0.0
0.2
0.4
0.6 0.4 m depth
ru
0 2 4 6 8 10 12 14 16
0.0
0.2
0.4
0.6 1.2 m depth
ru
Time (s) a) Case A
0 2 4 6 8 10 12 14 16 18 20 22-0.06
-0.03
0.00
0.03
0.06 Soil surface
Dis
. (m
m)
0 2 4 6 8 10 12 14 16 18 20 22-0.06
-0.03
0.00
0.03
0.06 0.4 m depth
Acc
. (g
)
0 2 4 6 8 10 12 14 16 18 20 22-0.06
-0.03
0.00
0.03
0.06 1.2 m depth
Dis
. (m
m)
0.0
0.3
0.6
0.9
1.2 1.2 m depth
ru
0 2 4 6 8 10 12 14 16
0.0
0.3
0.6
0.9
1.2 0.4 m depth
ru
Time (s) b) Case B
Figure-4. Times-histories of free-field [2].
3.2.2 Liquefaction characteristics of the ground
The noticeable movements in the soil skeleton,
that yield liquefaction "are as follows: Seismic influences
mainly shear waves, passing through saturated granular
layers, distort the granular structure, and cause loosely
packed groups of particles collapse. Disruptions to the
particulate structure generated by these collapses cause
transfer of load grain-of grain contacts in the pore water"
[13]
Test phenomena are shown in Figure-4 (b). The
following phenomena summarized as the most significant
moment of the OpenSess PL due to shaking that was
present at the boundary between sand and clay layers;
ground displacement, were almost the same peak, only
slightly larger than the calculated value of the surface in
the case B value. By comparing the event A and event B,
the seismic response, well demonstrates that the case B
shaking test analysis show liquefaction represented by ru
≥1 for the same time of shaking and Peak acceleration (g), the explanation of this fact is due to the motion shape
which plays an enormous role in prone liquefaction.
3.3 The progress of p-y curves
As cited previously, the strategic objective of this
paper was the p-y curves at the achievement levels of pore
water pressure ≤ 1.0. To generate these curves, design
parameters will be involved explaining the behavior of
these curves.
3.3.1 Initial pile-soil stiffness ratio Figures 5,6 shows the pile stiffness vs. peak
bending moment on the single pile, along with the
stiffness value increases, the peak moment changes with a
variation similar to that as the depth increases, the peak
moment first increased and then decreased. Meanwhile, as
the depth increases, the pile stiffness value changes caused
by peak bending moment on the pile getting smaller and
smaller. Differences in soil boundary show the peak
moment has increased trend; the peak moment is
consistent and linear change, which these three are
stiffness values, the slope of the linear variation is almost
the same, especially when the depth reaches a certain
value.
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9044
The simulation result of Figure-6 coordinates that
the flexibility of the pile; displacement of the pile head
and the displacement along the pile in the lateral load
direction were more significant. The pile displacement
was not profound to its connected stiffness, which may be
correlated to the inelasticity of the pile.
-16 -14 -12 -10 -8 -6 -4 -2 0 2 4 6 8-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
E=1e010 kPa
E=5e005 kPa
E=5e006 kPa
E=1e008 kPa
Bending moment (kN.m)
2° sloping ground
Dep
th (
m)
Figure-5. Bending moment vs. Pile length for different EI.
-0.5 0.0 0.5 1.0 1.5-1.5
-1.0
-0.5
0.0
0.5
1.0
Dis. (mm)
2° sloping ground
E=1e010 kPa
E=1e008 kPa
E=5e006 kPa
E=5e005 kPa
Dep
th (
m)
Figure-6. Impact of stiffness of the pile in Event B.
Consistent to Figure-6, it is remarkable to note
that the pile displacement is very unaffected with pile
stiffness. That is, the high stiffness pile experienced about
the same total movement as the low stiffness pile;
however, the final bending moments, as shown in Figure-
5, are vastly different. Here, the low stiffness pile
produced the highest bending moment.
The results from Figure-7 specified that the
stiffness of the pile had some effect on the p-y curve of the
single pile in the inclined shallow soil.
Model results of the inclined soil-pile system (2°)
were shown in Figure-7. The results showed the p-y curve
of the laterally loaded single pile was not sensitive to the
material modules, the p of soil "would be developed
deeper, so the transform point of the resistance moved
down, and the lateral resistance below soil increased,
which was beneficial to enhancing the lateral bearing of
the pile" [15].
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9045
-0.04 -0.02 0.00 0.02 0.04 0.06-6
-4
-2
0
2
4
6
8
E=1e010 kPa
p (
kN
/m)
-0.02 -0.01 0.00 0.01 0.02-2
-1
0
1
2
3
E=1e008 kPa
p (
kN
/m)
-0.0030 -0.0015 0.0000 0.0015 0.0030 0.0045-1
0
1
2
y (mm)
E=5e 006 kPa
p (
kN
/m)
-0.003 -0.002 -0.001 0.000 0.001 0.002 0.003-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
E=5e 005 kPa
y (mm)
p (
kN
/m)
Figure-7. Effect of the stiffness of the single pile on the p-y curves of the pile at depth 0.5 m in Event A.
3.3.2. Depth of insertion effect
Considering previous lectures and research [16]
the lateral response with increasing depth interval was
investigated as shown in Figure-8. Response at showllar
depth liquefies earlier, as related the response at the deeper
area. This behavior matches [16-17]. However, the lateral
resistance decreases with increasing depth for horizontal
(0°) (2°) and (4°) sloping ground.
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9046
-0.8 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8-60
-30
0
30
60
2D = 0.4m depth
3D = 0.6m depth
p (
kN
/m)
y (mm)
-1.0 -0.5 0.0 0.5 1.0-15
-10
-5
0
5
10
15
y (mm)
4D = 0.8 m depth
5D = 1.0 m depth
p (
kN
/m)
(a) Horizontal grounds (0°)
-0.4 0.0 0.4 0.8 1.2 1.6-40
-20
0
20
40
60
80
100
2D = 0.4m depth
3D = 0.6m depth
p (
kN
/m)
y (mm)
-0.4 0.0 0.4 0.8 1.2 1.6-15
-10
-5
0
5
10
15
y (mm)
4D = 0.8 m depth
5D = 1.0 m depth
p(k
N/m
)
(b) 2° sloping ground
0.0 0.4 0.8 1.2 1.6 2.0 2.4-40
0
40
80
120
2D = 0.4 m depth
3D = 0.6 m depth
p (
kN
/m)
y (mm)
0.0 0.4 0.8 1.2 1.6 2.0 2.4-15
-10
-5
0
5
10
15
y (mm)
4D = 0.8 m depth
5D = 1.0 m depth
p (
kN
/m)
(c) 4° sloping ground
Figure-8. Lateral response with depth concerning pile diameter in Event C.
The p-y curves for 4° sloping ground shown in
Figure-8(c) describe different types of response. For
example, the first curve at a depth of 0.4 m below the
ground surface displays greater resistance than the curves
immediately below it. The four curves from (0.4 to 1.0 m)
depth show the same manner. The two ground cases (0°)
and (2°) curves from (0.8 and 1.0 m) depth match with
each other. It’s produced greater lateral displacement,
consistent with the two cases.
The large displacement levels are more noticeable
in shallow depth than in deeper one. The reason for this
happening is due to "As the shaking continues, the
effective resistance of the soils has been reduced due to
gapping and inherent strength degradation (the latter of
which is exhibited in the curves by the lower-than-static
peak strengths for a given displacement)" [18].
3.3.3 Effect of difference between the (peaks - critical
state) friction angles
Investigation to variations of the dilation angle
was examine considering [17] definition and procedures.
In this simulation, the critical state friction angle considers
equal to 26°, while the peak friction angle is tested to vary
between 28-40°. Figure 9 illustrates the dynamic response
p-y curves at depth 0.5 m. The dynamic curves show
strain-softening behaviour. For soil with low dilation angle
(2-6°), show more lateral displacement response compared
to the higher dilation angle (8-14°) through shaking
duration.
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9047
-0.03 0.00 0.03 0.06-4
-2
0
2
4
6
y.(mm)
2°sloping ground
28°
30°
32°
p (
kN
/m)
-0.03 -0.02 -0.01 0.00 0.01 0.02 0.03-4
-3
-2
-1
0
1
2
3
4
5
y.(mm)
2°sloping ground
35°
38°
40°
p(k
N/m
)
Figure-9. Dynamic pile response with changing dilation angle (at depth 0.5m) in Event B.
4. CONCLUSIONS AND SUMMARY
a) Design Parameter analysis shows that under the
conditions of liquefaction with the increasing pile
stiffness the peak (y) & (p) are reduced. Even the
peak pile bending moment will be decreased; internal
friction angle for sand layer decrease lateral
displacement. With the depth decreases, the peak
displacement of the pile increases.
b) The p-y curves and the relative displacement (y) are
not strongly dependent on the groundwater table, but
the relative displacement (y) is strongly dependent on
the ground surface slope and pile length
c) Construction of p-y curves for inclined pile and for
pile groups (horizontal & inclined) are highly
recommended to capture the response. Effect of
ground motion parameters on p-y need to be
investigated as well.
REFERENCES
[1] Maula B.H., Ling X.Z., Liang T. & Xu P.J. 2011. 3D
FEM numerical simulation of seismic pile-support
bridge structure reaction in liquefying ground.
Research Journal of Applied Sciences, Engineering,
and Technology. 3(4): 344-355.
[2] Maula B.H., Xian Zhang L. & Liang T. 2011. Study
on dynamic behavior for pile-soil-bridge structure
seismic interaction in liquefying ground under strong
earthquake. Journal of Emerging Trends in
Engineering and Applied Sciences. 2(2): 239-244.
[3] Maula B.H. 2016. Behavior of seismic soil-pile
foundation in liquefying sloping ground controlled by
mechanical aspect. Journal of Emerging Trends in
Engineering and Applied Sciences. 7(1): 45-55.
[4] Elgamal A, Lu J. and Yang Z. 2006. OpenSeesPL
Three-Dimensional Lateral Pile-Ground Interaction
Version 1.00 User Manual, Report SSRP-06/04,
Department of Structural Engineering, University of
California San Diego, La Jolla, U.S.A.
[5] Elgamal Ahmed, et al. 2006. Liquefaction induced
lateral on the piles. In: Proceedings of the Fourth
Interational conference on earthquake engineering.
Taipei, Taiwan.
[6] Jinchi Lu, Zhaohui Yang, and Ahmed Elgamal. 2010.
OpenSeesPL 3D Lateral Pile-Ground Interaction,
Version 0.6 User Manual, University of California,
San Diego, Department of Structural Engineering.
[7] Ling X.Z., Wang C. and Wang C. 2005. Scale
modelling method of shaking table test of dynamic
interaction of pile-soil-bridge structure in ground of
soil liquefaction. Chinese Journal of Rock Mechanics
and Engineering. 23(3): 450-456 (in Chinese).
[8] Xian Zhang, L. I. N. G., et al. 2004. Large-scale
shaking table model test of dynamic soil-pile-bridge
structure interaction in ground of liquefaction. China
Civil Engineering Journal. 37.11: 67-72.
[9] Liang Tang, Pengju Xu, Ling Xian Zhang, Gao Xia.
2008. Shaking Table Test and Numerical Simulation
for seismic soil-pile-bridge structure interaction in
liquefiable ground. The 14th World Conference on
Earthquake Engineering, Beijing, October.
[10] Tao Bo, NaI Lei, Wu Faquan. 2005. Distributive law
of forces between the anti-sliding pile and the
surrounding soil mass. Journal of Jilin University:
Earth Science Edition. 35(2): 201-206.
[11] Xiong, Feng, et al. 2008. Seasonal Freezing Effects
on the Lateral Behavior of Steel Pipe Piles. The 14th
World Conference on Earthquake Engineering,
Beijing, October.
[12] Maula, Baydaa Hussain; Liang, ang; Gazal, Ali
Mahommed. 2014. Decomposition of Dynamic py
VOL. 13, NO. 23, DECEMBER 2018 ISSN 1819-6608
ARPN Journal of Engineering and Applied Sciences ©2006-2018 Asian Research Publishing Network (ARPN). All rights reserved.
www.arpnjournals.com
9048
Curves Considering Liquefaction during Earthquakes.
Research Journal of Applied Sciences, Engineering
and Technology. 7.24: 5163-5171.
[13] Samuel Tadesse. 2000. Behaviour of saturated sand
under different triaxial loading and liquefaction
(Doctoral dissertation. Norwegian University of
Science and Technology).
[14] Hussain Maula, Baydaa. 2013. Dynamic response and
simplified analysis method for bridge pile foundations
in the liquefiable sloping ground (Doctoral
dissertation, Harbin: Harbin Institute of Technology).
[15] Zhao-Ran, Xiao; Junlin, Wang. 2007. DEM in 3D
Simulation of Influencing Factors of Deformation
Properties and py Curves of a Laterally Loaded Pile.
In: International Conference on Computational
Science. Springer Berlin Heidelberg. pp. 1214-1222.
[16] Varun, Dominic Assimaki. 2011. A nonlinear
microelement for dynamic soil-structure interaction
analyses of pile foundations in liquefiable soils.
January, 10-13 5th International Conference on
Earthquake Geotechnical Engineering.
[17] Varun A. 2010. Non-Linear Dynamic Microelement
for Soil Structure Interaction Analyses in Liquefiable
Soils, PhD Dissertation, in: Civil and Environmental
Engineering, Georgia Institute of Technology,
Atlanta.
[18] Gerber Travis M.; Rollins, Kyle M. 2008. Cyclic PY
curves for a pile in cohesive soil. In: Geotechnical
Earthquake Engineering and Soil Dynamics IV. pp. 1-
.10