1 Introduction

Soft soil generally refers to the soft-fluid-plastic clay with several engineering characteristics, such as high water content, large void ratio, high compressibility and low shear strength. The soft soil in China is widely distributed and is mainly located in coastal, plain, inland lake basin, depression and river banks. The soft soil in coastal and plain areas is mostly located in the river downstream into the sea delta or alluvial plain, such as the Pearl River Delta [1, 2], Tanggu and Minjiang estuary plain [3]. The inland lake basins and depressions are represented by Dongting Lake, Hongze Lake, Jiuhu Lake and Dianchi Lake [4, 5]. In engineering, soft soil is often subdivided into soft clay soil, silty soil, silt, peat soil and peat soil [6].

In recent years, great attention has been paid to stability problems associated with deep foundation pit excavation because of the continuous development of urban rail transit construction. Construction projects are often affected by external factors, such as site conditions during construction and tight construction schedule, etc. In the process of pursuing foundation pit excavation, mechanical properties of soft soil foundation and other conditions are easy to be ignored by the builders, which often becomes the pain point and difficulty in engineering construction. Under such conditions, the detection and protection of the whole excavation process must be strengthened in the excavation process, and thus minimize the risks causing heave of the pit bottom and even the collapse of the foundation pit [7].

Numerical simulation is an effective method to simulate the process of foundation pit excavation [8,9,10]. The constitutive models commonly used in numerical simulation are linear elastic model, Duncan-Chang (DC) model, Mohr–Coulomb(MC) model (including MMC model), Drucker-Prager(DP) model [11,12,13,14,15]. DC model is a nonlinear elastic model, which mainly describes the nonlinear characteristics of stress–strain relationship of soil mass. This model cannot reflect the dilatancy, softening and anisotropy of soil under shear, so it has some limitations. M-C model can reflect the strength of soil, which is more widely used in the simulation of geotechnical slope stability and tunnel excavation [16, 17]. However, the influence of unloading on soil deformation modulus is not considered in the model, which leads to large uplift deformation during foundation pit excavation, so it is not suitable for the simulation of foundation pit excavation. Although the Drucker-Prager model is easy to program, it’s not appropriate to describe the actual behavior of earth. The defects of the MC model also apply to the DP mode. Considering the stress dependence of soil stiffness, the MMC model can simulate soil deformation under different stress paths and stress histories under loading and unloading.

In our study site in Tianjin, the soil is soft soil and its geological environment is fragile. Based on the MMC model setup for Tianjin, this paper simulates the excavation process of a transfer station of the Tianjin city subway lines 11 (under construction) and line 6. Compared with the MC model, the MMC model introduces three stiffness parameters: reference secant modulus (\({\mathrm{E}}_{50}^{\mathrm{ref}}\)), reference tangent modulus (\({\mathrm{E}}_{\mathrm{oed}}^{\mathrm{ref}}\)) and unloading and reloading modulus (\({\mathrm{E}}_{\mathrm{ur}}^{\mathrm{ref}}\)), which solves the unreasonable loading and unloading problems of the MC model. Therefore, the MMC model is more suitable for the numerical simulation of foundation pit excavation. The determination of the stiffness parameters (\({\mathrm{E}}_{\mathrm{ur}}^{\mathrm{ref}}\),\({\mathrm{E}}_{50}^{\mathrm{ref}}\) and \({\mathrm{E}}_{\mathrm{oed}}^{\mathrm{ref}}\)) is more difficult to obtain than that of other strength parameters. For example, the stiffness parameters of the soil will change with the change of the stress state of the soil, and the stiffness parameters obtained by different stress paths will also be different. The study of Brinkgreve [18] showed that the undrained Young's modulus was three times higher than the shear modulus, while the drained Young's modulus was 1.5–2 times lower than the shear modulus, indicating that the stiffness parameters differed greatly under different conditions. Therefore, the sensitivity study of stiffness parameter plays an important role in the study of foundation pit deformation in soft soil area.

There are two methods to select the soil model parameters. One is to take the undisturbed soil for laboratory test and analyze the model parameters according to the test results [19,20,21,22]. However, the process of collecting and preparing soil samples may have an impact on the soil. The other method is based on the measured data and numerical calculation for parameter inversion, the main idea is that by changing the soil parameters, the calculated results are constantly close to the measured results, so as to obtain the soil mechanical parameterss [23,24,25].

In order to quantitatively judge the influence of these three parameters on the model results and determine the value most in line with the actual field situation, sensitivity analysis was conducted on \({\mathrm{E}}_{\mathrm{ur}}^{\mathrm{ref}}\),\({\mathrm{E}}_{50}^{\mathrm{ref}}\) and \({\mathrm{E}}_{\mathrm{oed}}^{\mathrm{ref}}\) respectively. Sensitivity analysis can not only reduce the computational cost of further uncertainty analysis, but also help restoring the real environmental conditions to the greatest extent, providing a theoretical basis for risk analysis and model calibration in subsequent engineering construction.Therefore, the objective of this study is to determine the optimal value of \({\mathrm{E}}_{\mathrm{ur}}^{\mathrm{ref}}\),\({\mathrm{E}}_{50}^{\mathrm{ref}}\) and \({\mathrm{E}}_{\mathrm{oed}}^{\mathrm{ref}}\) in the MMC model for foundation pit excavation by applying the sensitivity analysis using the Latin Hypercube One Factor (LH-OAT) method and comparing the monitoring data with the numerical simulation results. In the next section, we introduce the general situation of the research area and the research methods. Section 3 shows the relation between the three parameters and the horizontal displacement of the ground diaphragm wall. In Sect. 4, we present the relationships between stiffness parameters in different regions. Finally, Sect. 5 present conclusions drawn from the study. The results from this study will also provide theoretical support for foundation pit excavation in water-rich soft soil area.

2 Materials and methods

2.1 Overview and study area

The Mohr–Coulomb model (MC) is an ideal elastic–plastic model, its linear criterion may be expressed as follow [ \* MERGEFORMAT 26]:

$$\frac{{\upsigma }_{1}-{\upsigma }_{3}}{2}=\mathrm{ccos\;\varphi }+\frac{{\upsigma }_{1}-{\upsigma }_{3}}{2}\mathrm{sin\;\varphi }$$
(1)

where \({\upsigma }_{1}\) and \({\upsigma }_{3}\) is the major and minor principal stress components, respectively; \(\mathrm{\varphi }\) is the frictional angle.

In Eq. (1), the elastic modulus is adopted in the process of excavation and unloading. However, the stress–strain relationship before failure is linear elastic, so the nonlinear deformation behavior of soil cannot be well described, and the influence of stress path on the mechanical properties of soil cannot be considered [27].

The modified Mohr–Coulomb model (MMC) combines the nonlinear elastic model with the elastic–plastic model to establish the double yield surface elastic–plastic model. This model assumes that the axial strain \({\upvarepsilon }_{1}\) and the deflection stress q of the triaxial drainage loading test behaves as hyperbola pattern (Fig. 1). Based on the Mohr–Coulomb failure criterion, \({\mathrm{E}}_{\mathrm{ur}}^{\mathrm{ref}}\),\({\mathrm{E}}_{50}^{\mathrm{ref}}\) and \({\mathrm{E}}_{\mathrm{oed}}^{\mathrm{ref}}\) were used to describe the soil strength, which solved the unreasonable loading and unloading problem of the Mohr–Coulomb model (Table 1).

Fig. 1
figure 1

Hyperbolic stress–strain relationship of conventional triaxial drainage test, where E50 is secant Young’s modulus at 50% of the ultimate deviatoric stress, Eur is unloading–reloading secant Young’s modulus

Table 1 Parameters of the Mohr–Coulomb model

The stress–strain relationship of MMC model during elastic deformation is shown as follows [28,29,30]:

$${\varepsilon }_{1}=\frac{2-{R}_{f}}{2{E}_{50}}\frac{q}{1-q/{q}_{a}}$$
(2)
$$E_{50} = E_{50}^{{{\text{ref}}}} \left( {\frac{{\sigma_{3} + \cot^{ - 1} \varphi }}{{\sigma^{{{\text{ref}}}} + \cot^{ - 1} \varphi }}} \right)^{m}$$
(3)
$${q}_{a}=\frac{{q}_{f}}{{R}_{f}}$$
(4)

At the stage of plastic deformation, the shear yield function Fs is described by the following equations:

$${F}_{s}=\frac{{q}_{a}}{{E}_{50}}\frac{q}{{q}_{a}-q}-\frac{2q}{{E}_{ur}}-{\gamma }_{p}=0$$
(5)
$${\gamma }_{p}={\varepsilon }_{1}^{p}-{\varepsilon }_{2}^{p}-{\varepsilon }_{3}^{p}\approx 2{\varepsilon }_{1}^{p}$$
(6)
$$E_{{{\text{ur}}}} = E_{{{\text{ur}}}}^{{{\text{ref}}}} \left( {\frac{{\sigma_{3} + \cot^{ - 1} \varphi }}{{\sigma^{ref} + \cot^{ - 1} \varphi }}} \right)^{m}$$
(7)

The non-associated plastic flow rule is derived from the following plastic potential function:

$${Q}_{s}=\frac{{\sigma }_{1}-{\sigma }_{3}}{2}-\frac{{\sigma }_{1}+{\sigma }_{3}}{2}\mathrm{sin}{\psi }_{m}$$
(8)

Compression yield function Fv is expressed in the following form:

$${F}_{V}=\frac{{\widetilde{q}}^{2}}{{M}^{2}}+{p}^{2}-{p}_{0}^{2}$$
(9)

The plastic potential function of the compressed yield surface which adopts the associated flow rule is given by:

$${Q}_{V}=\frac{{\widetilde{q}}^{2}}{{M}^{2}}+{p}^{2}$$
(10)

where qf is the ultimate deviatoric stress; qa is the asymptotic deviatoric stress;\({\varepsilon }_{1}^{p}\)\({\varepsilon }_{2}^{p}\)\({\varepsilon }_{3}^{p}\) are the plastic strains in three principal stress directions; p is the mean effective pressure; p0 is the pre-consolidation pressure; \(\widetilde{q}\) is Roscoe’s invariant of deviatoric part of the stress tensor. Other parameters of the model are shown in the following table:

2.2 LH-OAT

Common sampling methods include Monte Carlo method, First-order quadratic matrix analysis method, etc. Monte Carlo method is relatively simple and easy to operate, but it requires a lot of calculation. The first-order quadratic matrix analysis method cannot be used for highly nonlinear functions and error analysis. Latin hypercube sampling (LHS) improves the calculation accuracy and efficiency by reducing the variance. Sensitivity analysis can be divided into local Sensitivity analysis methods and global Sensitivity analysis methods, such as Morris, Sobol', Fourier Amplitude Sensitivity Test, etc. Morris could not calculate sensitivity quantitatively, and Sobol's calculation cost was high [32]. Fourier Amplitude Sensitivity Test cannot obtain the Sensitivity of the interaction between parameters [33]. The OAT (One-factor-At-a-Time) method, which changes one input factor at a time while keeping the others fixed between two successive model evaluations, is a global sensitivity analysis method. It has low computational cost and simple calculation. This paper applies LH-OAT method for subsequent research.

The LHS method divides the distribution of each parameter into N and guarantees equal-probability sampling. Its computation is effective [34]. However, the sensitivity analysis of one specific parameter can't be obtained by this strategy [35]. The LH-OAT sensitivity analysis method combines OAT design and the LH sampling by taking the LH sampling as initial points for an OAT design [36]. In this study, the sensitivity, S, for each parameter, xj, is then calculated as [37]:

$$S=\frac{\left|f\left({x}_{1},{x}_{2},{x}_{3},\dots ,{x}_{j}(1+{\Delta }_{i})\right)-{f\left({x}_{1},{x}_{2},{x}_{3},\dots ,{x}_{j}\right)}_{min}\right|}{{f\left({x}_{1},{x}_{2},{x}_{3},\dots ,{x}_{j}\right)}_{min}}$$
(11)
$$\overline{S }=\frac{1}{n} \mathop{\sum}\limits_{i=1}^{n}S$$
(12)

where f() refers to the model function, f()min is the minimum value of the function, \({\Delta }_{i}\) is the fraction by which the parameter is changed, j refers to a LH point, each LH sample point is varied for i times.

2.3 Study area

Tianjin city, located in the north part of The North China Plain, west of the Bohai Sea, is a typical soft soil area in China. Its strata have obvious characteristics of sea and land cross deposition. The soft soil layer of Tianjin plain was mainly formed in the Huanghua Transgression period of 8000–2500 years ago. At the same time, because Tianjin is located in the low-lying center of Tianjin plain and was affected by diversion of the ancient Yellow River three times, the southern Plain of Tianjin is mainly composed of alluvium, lacustrine and Marine deposits. The northern and central parts are dominated by continental impulse and impulse deposits [3, 38, 39].

According to the existing geotechnical investigation, the foundation soils of our study site, the transfer station of the Tianjin city subway line 11 (under construction) and line 6 are all Quaternary unconsolidated sediments. The whole formation consists of three marine strata (6, 10, 12) and five continental strata (4, 7, 8, 9, 11) which are refined into 10 layers according to their physical and mechanical properties, as shown in Table 2. The soft soil in the study area has a high water content, ranging from 19.5% to 31.4%, with an average water content of 26.65%.

Table 2 Strata and their physical and mechanical properties [40]

2.4 Sensitivity calculation scheme

Numerical simulation method was applied to establish a model for the deep foundation pit. The model was established according to the actual engineering size, with x direction of 350 m, y direction of 380 m and Z direction of 60 m. During the modeling process, solid elements were used for soil, beam elements were used for the bracing structures, and plate elements were used for ground wall. The simulation process is consistent with the actual construction steps. According to the design, the foundation pit and the bracing structure are established in five steps, each step includes soil excavation and bracing structure construction. The depth of the first excavation was 7.2 m. The excavation depths of the other four stages are 6.2 m, 5.4 m, 5.6 m and 2.8 m, respectively. The bracing structures are located at depths of 0 m, 7.2 m, 13.4 m, 23.2 m and 26 m respectively.

In the calculation, the structural stress is ignored, the initial stress field is assumed to be the gravity stress field, and the soil is regarded as an elastic–plastic continuum, which is simulated by the MMC model. Since the horizontal displacement of diaphragm wall is an important index to measure the deformation of foundation pit and is also a common index for monitoring the construction process of foundation pit, this research selects the horizontal displacement of diaphragm wall as parameter evaluation index.

In order to understand the influence of three stiffness parameters on the horizontal displacement of diaphragm wall during simulation, LH-OAT method was used to analyze the influence of \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) on diaphragm wall of different soil layers (Table 2). The LH method divides the distribution of each parameter into 5 strata with a probability of occurrence equal to \(\frac{1}{5}\). According to the OAT method, changing the value of only one factor while keeping the others fixed, the perturbation amplitude of three stiffness parameters is (± 20%) and (± 40%). The sensitivity of each soil layer under the disturbance of different parameters can be obtained by Formula (11), and the mean value of sensitivity calculation results is calculated by using Formula (12). Based on the sensitivity calculation results, the horizontal displacement of diaphragm wall in different soil layers is compared with the monitoring data, so as to obtain the optimal parameters for soft soil layer modeling in Tianjin.

3 Results

3.1 Correlation analysis for \({{\varvec{E}}}_{{\varvec{u}}{\varvec{r}}}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\),\({{\varvec{E}}}_{50}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\) and \({{\varvec{E}}}_{{\varvec{o}}{\varvec{e}}{\varvec{d}}}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\)

In the same soil layer, two parameters are fixed and the other parameter is disturbed by (± 20%) and (± 40%) to calculate the horizontal displacement of diaphragm wall caused by changes in \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\). Figure 24 gives the horizontal displacement curves of three parameters at different depth. Figure 2 shows the horizontal displacement of the diaphragm wall caused by (-40%) of the disturbance of \({E}_{ur}^{ref}\) having maximum deformation of 10.41 mm and maximum deformation of 4.61 mm caused by 40% of the disturbance. The difference is 5.80 mm. Figure 3 shows the horizontal displacement of the diaphragm wall caused by (± 40%) of the disturbance of \({E}_{50}^{ref}\) having a maximum value of deformation equal to 8.86 mm and 5.74 mm. Figure 4 shows the horizontal displacement of the diaphragm wall caused by (± 40%) of the disturbance of \({E}_{oed}^{ref}\) having a maximum value of deformation equal to 7.37 mm and 6.45 mm. The corresponding difference of \({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\), are 3.12 mm and 0.92 mm, respectively. It can be seen that the absolute values of horizontal displacement were highest when disturbances of parameters are (-40%). The influence of parameters in the same soil layer is ranked as \({E}_{ur}^{ref}\)>\({E}_{50}^{ref}\)>\({E}_{oed}^{ref}\) and parameters are negatively correlated with the horizontal displacement.

Fig. 2
figure 2

Horizontal displacement curves of the diaphragm wall caused by \({E}_{ur}^{ref}\)

Fig. 3
figure 3

Horizontal displacement curves of the diaphragm wall caused by \({E}_{50}^{ref}\)

Fig. 4
figure 4

Horizontal displacement curves of the diaphragm wall caused by \({E}_{oed}^{ref}\)

3.2 Sensitivity analysis for \({{\varvec{E}}}_{{\varvec{u}}{\varvec{r}}}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\),\({{\varvec{E}}}_{50}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\) and \({{\varvec{E}}}_{{\varvec{o}}{\varvec{e}}{\varvec{d}}}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\)

A sensitivity analysis for the three parameters by the LH-OAT method is conducted in 10 soil layers. The correlation sensitivity of the variation of the diaphragm wall in different soil layers is compared. It can be seen from the calculation results (demonstrated in Fig. 5) of the model that the horizontal displacements caused by \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) produce corresponding fluctuations for different soils. However, the ranking of the parameters is almost invariant. According to all analysis, \({E}_{ur}^{ref}\), is the parameter that has the largest influences the uncertainty in the MMC model. \({E}_{oed}^{ref}\) is the least sensitive to horizontal displacement of diaphragm wall, that is, \({E}_{ur}^{ref}\)>\({E}_{50}^{ref}\)>\({E}_{oed}^{ref}\) (Fig. 5). By comparing the sensitivities of different soil layers with the same parameter, it can be seen that silty clay 4–1 is less sensitive to changes in parameters, which may be explained by that silty clay 4–1 has a higher moisture content.

Fig. 5
figure 5

Sensitivities of \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) in different soil layers

The average sensitivities values of all soil layers of \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) are 0.23 ± 0.07, 0.11 ± 0.04, 0.04 ± 0.01, respectively. The sensitivities of \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) are consistent with the sensitivities of three stiffness parameters in different soil layers, the difference between the measures of sensitivity for \({E}_{ur}^{ref}\) and the rest of the parameters is significant.

3.3 Determination of \({{\varvec{E}}}_{{\varvec{u}}{\varvec{r}}}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\),\({{\varvec{E}}}_{50}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\) and \({{\varvec{E}}}_{{\varvec{o}}{\varvec{e}}{\varvec{d}}}^{{\varvec{r}}{\varvec{e}}{\varvec{f}}}\)

Horizontal displacement of diaphragm wall in different construction stages in different soil layers was compared with the monitoring data, and the horizontal displacement diagram was drawn (Fig. 6). Figure 6 shows that the horizontal displacement of diaphragm wall is closest to the measured value for the five steps of foundation pit excavation. The parameter Settings that form the effect of Fig. 6 are shown in Table 3. Thus, it can be concluded that when \({E}_{ur}^{ref}\)=3 \({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) = 1.5 \({E}_{50}^{ref}\), better simulation effect can be obtained. The values of \({E}_{50}^{ref}\),\({E}_{oed}^{ref}\) and \({E}_{ur}^{ref}\) required as input stiffness parameters of the MMC for each soil layer are summarized in Table 3, other parameters are selected according to Table 2.

Fig. 6
figure 6

Calculated and measured horizontal displacement curves of the diaphragm wall

Table 3 Specific parameters of \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\)

4 Discussion

Soil stiffness parameters directly affect the deformation of foundation pit excavation. Through regional research results and analysis of correlation between stiffness parameters, the relationships between stiffness parameters in different regions are not the same. Regional experience stiffness parameter values for three regions are shown in Table 4. The results of soil stiffness parameters explored by different researchers in different regions are shown in Table 5.

Table 4 Regional experience stiffness parameter values
Table 5 \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) explored by different researchers

To investigate the stiffness parameters of Tianjin water-rich soft soil relevant to simulation of deep excavation, a sensitivity analysis is conducted with a series of parameters taken by LH-OAT methods. Regardless of the same or different soil layers, \({E}_{ur}^{ref}\) is most sensitive to horizontal displacement. The ratios (\({E}_{ur}^{ref}\)=3 \({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) = 1.5 \({E}_{50}^{ref}\)) determined in this study accord with common stiffness parameters and achieve good simulation results, which can provide reference for other foundation pit engineering simulation in Tianjin area.

Es is the compression modulus of soil; E0 is the elastic modulus of soil.

5 Conclusion

The MMC model is applied to simulate the foundation pit construction of the transfer station of the Tianjin city subway lines 11 (under construction) and 6 in this study. A sensitivity analysis by the LH-OAT method is conducted for the three parameters of the MMC model in 10 soil layers and the results of simulation are compared with the measured data, by taking the horizontal displacement of diaphragm wall as the evaluation target. It has been observed that the three parameters have a significant influence on the simulation of foundation pit excavation process.

For the horizontal displacement of diaphragm wall, the perturbation amplitude of 40% has been observed as the value results in minimal deformation while the perturbation amplitude of (-40%) represented the maximum deformation. The impact of \({E}_{ur}^{ref}\),\({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) can be ranked as follows:\({E}_{ur}^{ref}>{E}_{50}^{ref}>{E}_{oed}^{ref}\).

The sensitivity were normalized and sorted, and the sensitivity degree of each parameter to the control target was finally summarized. Comparing the sensitivities of the three parameters in different soil layers, it can be seen that \({E}_{ur}^{ref}\) is the parameter that has the largest influence the uncertainty in the MMC model. \({E}_{oed}^{ref}\) is the least sensitive to horizontal displacement of diaphragm wall.

On this basis, the stiffness ratio relationship suitable for foundation pit simulation in Tianjin water-rich soft soil area is obtained. the proportion relationship between stiffness parameters can be summarized as: \({E}_{ur}^{ref}\)=3 \({E}_{50}^{ref}\) and \({E}_{oed}^{ref}\) = 1.5 \({E}_{50}^{ref}\).

In this paper, the influence of each parameter on the excavation process of foundation pit is determined by normalization. The subsequent construction can strictly monitor the sensitive parameters to reduce the deviation in the construction process as much as possible. The relationship between the stiffness parameters can provide reference for the deformation research of similar projects in the future.