/ / Article

Research Article | Open Access

Volume 2019 |Article ID 1251295 | https://doi.org/10.1155/2019/1251295

Liyan Wang, Zhou Yajun, Wenxue Gong, Jinsong Li, Aimable Ishimwe, "Calculation Method of Seismic Residual Displacement of Sheet Pile Quay Walls", Advances in Civil Engineering, vol. 2019, Article ID 1251295, 15 pages, 2019. https://doi.org/10.1155/2019/1251295

# Calculation Method of Seismic Residual Displacement of Sheet Pile Quay Walls

Accepted17 Jun 2019
Published01 Aug 2019

#### Abstract

Sheet pile quay walls have widely been used in port engineering, hydraulic engineering, and civil engineering, but the sheet pile quay is a flexible retaining structure, which undergoes large deformation during earthquakes. The seismic design methods of the sheet pile quay wall in different countries are greatly different, and there is deficit of studies performed on the seismic residual displacement of the sheet pile quay walls. Based on the pseudostatic method and the calculation method for obtaining the dynamic earth pressure of clay soil, it is assumed that the cantilever part of the sheet pile quay wall bears the dynamic active earth pressure and the part in deep soil bears dynamic passive earth pressure on the side of the sea and bears dynamic active earth pressure on the side of the ground. The hydrodynamic pressure acting in front of the wall is calculated using Westergaard’s approach. The displacement of the front wall of the sheet pile quay is calculated, respectively, according to the upper part and lower part of mud surface. Based on the deflection curve differential equation and boundary conditions, the calculating formulas on seismic residual displacements of the sheet pile quay walls are derived and the proportional displacement method for determining the tension force of the pull rod is given. Combining with an engineering case, the theoretical calculation results are compared with the ADINA simulation results, and comparison results show that these two calculation methods are close under the mud, but they have little difference in the calculation results of the part above the mud because of the proportional displacement method of the tension force of the pull rod.

#### 1. Introduction and Background

##### 1.1. Introduction

Sheet pile quay walls have widely been used in coastal and inland areas with many advantages that include simple structure, low material consumption, low cost, and the main component can be prefabricated in the factory. It not only bears general actions in design but also bears seismic actions and can be destroyed due to improper design during earthquakes . For example, during Kobe Hyogo-ken earthquake in Japan, the sheet pile quay walls were severely damaged, and the steel plates were fractured (2001). It is necessary to study the stress and deformation of the sheet pile quay structure under earthquakes .

Due to the lack of corresponding observations and model tests on seismic response of sheet pile quay walls, and some simple and practical methods in some general standards, and due to the difference in experience, science technology, and economy, the seismic design methods of the sheet pile quay wall in different countries are greatly different. Therefore, it is important to study theoretical calculation methods of seismic displacements of the front walls in sheet pile quays.

##### 1.2. Background

Several theories and findings on the seismic analysis of sheet pile wharves have been developed over the last several decades through experiments with shaking table tests . The real control factor of the seismic safety of a geostructure is its deformation rather than its strength. It is gradual to become a development trend for evaluating seismic characters of geotechnical structures applying deformation as a control criterion (2005). At the present, there are many studies on the sheet pile quay wall with specific content as follows: Lee and Chang  proposed a procedure of damage inspection for the infrastructure in the harbor, which is a two-stage inspection strategy. Choudhury pertains to a study in which the effect of earthquakes along with the hydrodynamic pressure including inertial forces on such a retaining wall is observed. The hydrodynamic pressure is calculated using Westergaard’s approach, while the earth pressure is calculated using Mononobe–Okabe’s pseudostatic analysis . Tan and Lu  presented a thorough finite element (FE) parametric study of sheet pile wall deflections caused by deep dynamic compaction (DDC). Motamed and Towhata  presented experimental results of a series of 1 g shake table tests on mitigation measures for a model consisting of a 3  3 pile group and a sheet pile quay wall.

The FEM software ANSYS is used for the analysis of the interaction of steel sheet pile and soil model in Wang Xi’s study, then the two conditions of steel sheet pile when it is normal and corroded have been simulated, and the force status of the steel sheet pile and distortion of link-banked structure and soil were obtained. It can provide evidence for judging steel sheet pile safety . Bilgin  presented the results of the numerical parametric study performed and comparative analyses of the anchored sheet pile walls constructed by the finite element method. A series of calculation distribution figures in the paper can be applied to initially predict the seismic residual deformation of quay walls for engineering designers .

A pseudodynamic method for calculating the seismic residual deformation was provided, and the rationality and the reliability of the prediction method are validated by a 1 g shaking table model test and a 120 g centrifuge shaking table model test . The author studied the dynamic response of reinforced earth retaining walls under earthquake action [14, 15] and proposed a calculation method for residual deformation , prediction method of seismic residual deformation of caisson quay walls in liquefied foundation , and displacement calculation method of front wall of covered sheet pile wharves . Chiou et al.  proposed a procedure for developing seismic fragility curves for a pile-supported wharf. Based on the damage criteria and the response matrix, the fragility curves of the wharf can thus be constructed through simple statistical analysis. Shifted lognormal cumulative distribution functions are also employed to better approximate the fragility curves for practical applications. Cheng et al.  revealed that the composite steel sheet pile wall can exert the greater global bending stiffness and reduce the lateral soil pressure by the two-dimensional numerical simulations. Of course, the improvement treatment of backfill soils is an important method to reduce the displacement on sheet pile quay walls. The improvement of backfill soils includes many methods, and the authors in the paper have carried out some research on the improvement of backfill soils [21, 22].

In this paper, based on the graphical method conducted by Lin et al.  in obtaining the dynamic soil pressure of clay soil, considering structural characteristics of sheet pile quay walls and differential equation of the deflection curve, some calculating formulas on the seismic residual displacement of the front walls in the sheet pile quays are derived. A comparison is made between the theoretical calculation results and the ADINA simulation results to prove the effectiveness of the theoretical equation.

#### 2. Dynamic Earth Pressure of Cohesive Soil

##### 2.1. Calculation Model

The sheet pile quay wall has the tendency of sliding failure, while the top displacement of the front wall is large, and the bottom displacement is small under earthquakes. The wall has the tendency to rotate around the bottom, and when the wall displacement reaches a certain value along the direction from the soil under earth pressure, the backfill behind the wall slides along the back of the wall and through a plane called BC of soil where the angle between the wall base and the vertical plane is . This part of the soil is called sliding wedge OBC. The earth pressure of the front wall is caused by the sliding wedge of OBC, and the calculation model is shown in Figure 1. The wall is vertical and rough; are represented as the friction angle of the wall, cohesive force of soil after wall, internal friction angle, the dip angle of the soil surface after the wall, surface uniform load, the total seismic active earth pressure force under seismic load, and sliding wedge gravity, respectively. are horizontal and vertical seismic loads of sliding wedge, is the tension force of the pull rod, R is the reaction force on BC, C is the total cohesion on BC, is the total adhesion on OC, is the hydrostatic pressure, and is the hydrodynamic pressure.

Based on the research on the graphical method for obtaining the dynamic soil pressure of clay soil in Reference , some change has been made in the paper according to characteristics of sheet pile quay walls and has been applied to calculate seismic earth pressures of sheet pile quay walls.

##### 2.2. Acting Position of Seismic Total Earth Pressures on the Back of Sheet Pile Quay Wall

Schematic diagrams of seismic total active earth pressure calculation and forces acting on a horizontal microelement soil mass are shown in Figure 2.

Effective load acting on the surface is presented as follows:

Furthermore,where

###### 2.2.1. The Position of Active Earth Pressure

The seismic total active earth pressure of cohesive soil could be expressed as(1)When and , the distance between the acting point of dynamic active earth pressure joint forces and bottom of the wall under the earthquake is(2)When , the distance between the acting point of dynamic active earth pressure joint forces and the bottom of the wall under the earthquake is(3)When , the distance between the acting point of dynamic active earth pressure joint forces and the bottom of the wall under the earthquake is

Force analysis of passive earth pressure of horizontal microelement soil mass is shown in Figure 3.

###### 2.2.2. The Position of Dynamic Passive Earth Pressure

Passive earth pressure joint forces of cohesive soil under the earthquake is(1)When and , the distance between the acting point of dynamic passive earth pressure joint forces and the bottom of the wall under the earthquake is(2)When , the distance between the acting point of dynamic passive earth pressure joint forces and the bottom of the wall under the earthquake is(3)When , the distance between the acting point of dynamic passive earth pressure joint forces and the bottom of the wall under the earthquake is

#### 3. Calculation of the Wall Displacement for Sheet Pile Quay Wall under Earthquakes

##### 3.1. Calculation Mode

The front sheet pile walls produced larger displacement, and the sheet pile structure had the tendency of slope failure under earthquakes; thus, the upper part displacement of the sheet pile wall is larger, and the pattern of slope deformation is presented. Due to the large deformation displacement of the sheet pile wall, it is assumed that the part of the cantilever sheet pile wall bears the dynamic active earth pressure of the soil after the wall, the part of deep soil bears dynamic passive earth pressure of the soil on the side of the sea, and the part of deep sea that can bear dynamic active earth pressure of the soil on the side of the ground. When the deformation of the sheet pile wall was calculated, the sheet pile wall is divided into two parts: one is on the surface and the other is under the surface and both of all were calculated, respectively. The calculation of the part on the surface is shown in the calculation model as Figure 4(a). In the Figure, and are bending moment and shear force caused from the part under the surface to the part above the surface, respectively; and are the hydrodynamic pressure and hydrostatic pressure, respectively; and is the length of cantilever sheet pile wall part. The calculation of the part under the surface is shown in the calculation model as shown in Figure 4(b). and are bending moment and shear force caused from the part above the surface to the part under the surface, respectively. is the length of the sheet pile wall into the soil.

##### 3.2. Sheet Pile Wall Stress

(1) is the tension force of the pull rod.(2)Active earth pressure on the earthquake is . Here, can be calculated using equation (4). The position of dynamic earth pressure joint forces can be calculated using equations (8)–(10).(3)Due to free water behind the wharf, hydrodynamic pressure joint forces acting in front of the wall can be calculated by Westergaard’s method as shown in the following equation:Hydrodynamic pressure joint forces can be calculated as shown in the following equation:According to the principle of moment equivalence, joint force acting point position was determined, which can be calculated as follows:(4)Pore water restricted by soil particles, moving along with the soil particles, is called confined water. It produces hydrostatic pressure rather than hydrodynamic pressure. Hydrostatic pressure joint forces can be calculated using equation (16), and hydrostatic pressure force action point can be calculated using equation (20). Free pore water without the restriction of soil particles produces water pressure gradually with the increase of the degree of liquefaction under earthquakes. Wall back water pressure was calculated using the hydrostatic pressure equation without considering liquefaction:Hydrostatic pressure joint forces can be calculated as follows:Action point position of hydrostatic pressure joint forces can be calculated as follows:(5)Shearing force located at mud surface from the sheet pile wall can be calculated as follows:(6)Bending moment located at mud surface from the sheet pile wall can be calculated as follows:(7)Dynamic passive earth pressure on the side of the sea borne by the part in deep soil can be calculated using equation (8). The point position of dynamic passive earth pressure joint forces can be calculated using equations (12)–(14), and overload pressure is calculated as .(8)Dynamic active earth pressure on the side of the ground borne by the part in deep soil can be calculated using equation (4), and the point position of dynamic active earth pressure joint forces can be calculated using equations (5)–(7).

##### 3.3. Displacement Calculation for the Lower Part of the Mud Surface of Sheet Pile Wall

Based on mechanics of materials, the deflection curve differential equation of the elastic components part which located at mud surface of the sheet pile wall can be calculated aswhere is represented as dynamic active earth pressure joint forces between any part located at mud surface and the part under the mud surface which can be calculated as follows:where is represented as distance from dynamic active earth pressure joint forces, between any part located at mud surface and the part under the mud surface, to the bottom of the wall which can be calculated as follows:where is represented as the dynamic passive earth pressure joint forces between any part located at mud surface and the part under the mud surface which can be calculated as follows:where is represented as the distance from dynamic passive earth pressure joint forces, between any part located at mud surface and the part under the mud surface, to the bottom of the wall which can be calculated as follows:

Boundary conditions are

According to the differential solution, the answer is

##### 3.4. Calculation of the Displacement above the Mud Surface of the Sheet Pile Wall

There are six displacements of the front sheet pile wall, including the displacement caused by mud surface , the one caused by mud corner , the one caused by dynamic active earth pressure behind the wall , the one caused by tension force , the one caused by hydrostatic pressure , and the one caused by the hydrodynamic pressure .(1)Substituting in equation (27), then the displacement of front sheet pile walls located above the mud can be obtained. As is shown in the following equation:(2)Substituting in equation (26), then the displacement of front sheet pile walls located in the angle of the mud can be obtained, as is shown in the following equation:(3)The displacement of front sheet pile walls, caused by dynamic active earth pressure behind the wall, can be calculated by using the differential equation as follows:where is the represented as dynamic active earth pressure joint forces in any depth of the wharf surface, which can be calculated as follows:where is represented as the distance between the function point of dynamic active earth pressure joint forces in any depth of the wharf surface and the bottom of the wall which can be calculated as follows:Boundary conditions areThe answer is(4)Based on material mechanics equations, the displacement of front sheet pile walls caused by tension force isBoundary conditions areThe answer is(5)Based on material mechanics equations, the displacement of front sheet pile walls caused by hydrostatic pressure isBoundary conditions areThe answer iswhere:(6)Based on the material mechanics equations, the displacement of front sheet pile walls caused by hydrodynamic pressure isBoundary conditions areThe answer iswhereDisplacement of any points above the mud surface of the front sheet pile walls can be expressed asSubstituting (30), (31), (36), (41), (44), and (48) in equation (50), the solution of displacement of any points above the mud surface of the front sheet pile walls under the earthquake function can be obtained.In equation (50), except for conditions that have been known, tension force can be calculated by assuming the displacement located at the anchor point of the sheet pile walls, and by analyzing the results of finite element calculation and that of dynamic test, the deformation characteristics of the sheet pile wall can be obtained. The anchor point displacement in this paper is assumed as the following equation:Substituting from equation (50) in equation (51), the value of tension force can be obtained.

#### 4. Engineering Example

##### 4.1. Engineering Survey

The model is based on a practical engineering example. The structures of the front wall and anchor wall are the underground continuous walls. Front wall thickness is 0.8 m and buried depth is 8 m; anchor wall thickness is 1 m, the height is 4 m, and cover filling is 2 m; distance between front wall and anchorage wall is 10 m; and diameter of rod is 6 cm, and depth of sea is 6 m. The section is shown in Figure 5. Load of the wharf surface is 20 kN/m. The Kobe wave is the seismic load wave, and the waves of horizontal and vertical are loading at the same time. Maximum horizontal acceleration amplitude is 0.1 g; maximum vertical acceleration amplitude is 0.05 g. The waveform is shown in Figure 6. The soil was assumed to be a single soil layer in the process of deriving the sheet pile wharf displacement calculation theory; hence, the single soil layer can be chosen in finite element analysis.

In order to verify the rationality of the calculation method, some working conditions of increasing the internal friction and angle cohesion and reducing the elastic modulus of backfill soils were studied and the related parameters of soils are listed in Table 1. The calculated values are compared with the numerical simulation values. The parameters of the anchor wall, sheet pile wall, and bar are also shown in Table 1.

 Material type Working condition Unit weight (kN/m3) Internal friction angle (°) Cohesion (kPa) Elastic modulus (MPa) Poisson’s ratio Layer 1 ① 19.1 27.0 20 8.97 0.30 Layer 1 ② 19.1 35.0 20 8.97 0.30 Layer 1 ③ 19.1 27.0 20 8.97 0.30 Layer 1 ④ 19.1 27.0 30 4.00 0.30 Concrete 25.0 — — 2.8 × 104 0.20 Steel tie rod 78.5 — — 2.06 × 105 0.20
##### 4.2. Theoretical Calculation Results

According to the theoretical calculation of the sheet pile quay wall under earthquakes, displacement calculation data are shown in Table 2. Table 3 lists the symbols in Table 2.

 Ignoring the anchor point displacement Considering the anchor point displacement Variable Value Variable Value 0.10 2.359 0.05 −0.776 6.00 −3.084 6.011 1062.866 0.403 31.788 −0.761 65.649 −1.535 0.354 140.231 17.943 47491.034 108.474 5844.779 11949.382 40.398 2486.645 2.090 68.449 0.024 365.116 −10.880 −266.251 −63.642 −2004.722 7.181 −0.033 −159.633 0.0178 −59.919 60 The front wall displacement equations of part above the mud The front wall displacement equations of part under the mud