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Parameters used in the first application example. 

Parameters used in the first application example. 

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Article
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In this paper, the numerical solutions for groundwater flow in unsaturated layered soil using the Richards equation are presented. A linearisation process for the nonlinear Richards equation to deal with groundwater flow in unsaturated layered soil is derived. To solve one-dimensional flow in the unsaturated zone of layered soil profiles, flux cons...

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... where λ is the key parameter for solving the linearized Richards' equation in the conversion method, which can be defined as a constant λ = e αh d (Tracy 2006;Liu et al. 2015); h d is the pressure head value when the soil is dry. The relative 6 1 Background permeability coefficient is expressed as: ...
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Heavy rainfall in extreme climates often causes natural disasters such as floods, landslides, and debris flows. Rainfall-induced slope instabilities are major geological natural disasters (Glade in Environ Geol 35:160–174, 1998; Dai et al. in Eng Geol 51:279–290, 1999; Iverson in Water Resour Res 36:1897–1910, 2000; Lee and Pradhan in Landslides 4:33–41, 2007; Li et al. in Landslides 13:1109–1123, 2016a; Li et al. in Ecol Eng 91:477–486, 2016b; Wu et al. in Hydro-mechanical analysis of rainfall-induced landslides. Springer, 2020) that can result in considerable loss of life and damage to infrastructure. Extreme events such as storms, which are becoming more severe because of climate change, can trigger fatal landslides.
... Briggs et al. (2000) proposed a multi-grid correction method to quickly eliminate the iterative error in the iterative process, thereby obtaining a faster convergence rate. Recently, preconditioning methods can effectively reduce the condition number of the iterative matrix of linear equations, thereby improving the computational convergence rate (Benzi 2002;Zhu et al. 2022a, b, c), including the left preconditioning, right preconditioning, and two-side preconditioning (Liu et al. 2015). The preconditioning technique converts the original system of linear equations into a system that is easier to solve, thereby improving the convergence rate of the iterative process (Benzi 2002). ...
... The soil was assumed to be silt. The parameters of soil were described by Liu et al. (2015) and included θ s = 0.35, θ r = 0.14, α = 8 × 10 −3 , and k s = 9 × 10 −4 m/h. The boundary conditions are as follows: ...
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The linear infiltration equations obtained by discretizing Richards’ equation need to be solved iteratively, including two approaches of linear and nonlinear iterations. The first method is to use numerical methods to directly numerically discretize Richards’ equations to obtain nonlinear ordinary differential equations and then use nonlinear iterative methods to iteratively solve, such as Newton’s method (Radu et al. in On the convergence of the Newton method for the mixed finite element discretization of a class of degenerate parabolic equation. Numerical mathematics and advanced applications. Springer, pp 1194–1200, 2006), Picard method (Lehmann and Ackerer 1998), and the L -method (List and Radu 2016). The Picard method can be considered as a simplified Newton method, which linearly converges.
... Generally, RE first requires spatial discretization using numerical methods, such as finite difference method (FDM) (Liu et al., 2015;Zhu et al., 2019), finite element method (FEM) (Coombs and Augarde, 2020), mixed finite element method and finite volume method (FVM) (Eymard et al., 2006;Su et al., 2022). Additionally, the backward-Euler method is often used for time discretization (Wang and Schrefler, 1998;Pop and Schweizer, 2011). ...
... RE can be used to describe 1D rainfall infiltration in unsaturated soils, which is expressed as (Liu et al., 2015;Zha et al., 2017): ...
... In Fig. 1, the thickness of the soil is assumed to be 10 m. The model parameters includeα = 8 × 10 − 3 ,θ s = 0.35,θ r = 0.14, andK s = 1 × 10 − 4 m/h (Liu et al., 2015). The governing equation is shown in Eq. (1), the right side of which is equal to zero. ...
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... Hayek (2016) proposed a general analysis model of one-dimensional transient vertical infiltration. Although their actual applicability is limited, these are good references for theoretical analysis (Zambra et al. 2012;Liu et al. 2015;Zeng et al. 2018;Zhu et al. 2021). ...
... (7)-(8) may be simpler than that of Eq. (1). To acquire the approximate solution of Eq. (7), FDM is used for the numerical discretization (Liu et al. 2015). For a 1D unsaturated flow problem, the second-order partial derivatives in Eq. (7) only consider the z-direction. ...
... To verify the effectiveness of the proposed method, we present an example in which a 1D steady-state unsaturated flow is simulated in homogeneous porous media (Liu et al. 2015). The mathematical model is shown in Fig. 1, where the soil thickness (L) is 10 m; the other parameters are = 8 × 10 −3 , s = 0.35 , r = 0.14 , and K s = 1 × 10 −4 m/h. ...
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... Due to the complexity, the Richards equation considering the SWCC in unsaturated soils is usually solved using the numerical methods. Mesh-based numerical techniques such as the finite difference method and the finite element method are well documented and typically used to solve the unsaturated flow equation in the past [20][21][22]. ...
... The unsaturated flow in soils can be described by the following variably saturated flow equation [21] ...
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... Generally, RE first needs to use numerical methods for spatial discretization, including finite difference method (FDM) [16,17], finite element method [18,19], and finite volume method [20,21]. For time discretization, a backward-Euler finite-difference stepping scheme is usually adopted [22,23]. ...
... In addition, the relaxation factor w in the SOR method directly affects the convergence rate, but determining the optimum value of the relaxation factor is difficult. Due to some shortcomings of conventional iteration methods, increasing attention has focused on improving their convergence rate [16,31,[39][40][41][42][43]. ...
... Liu [46] used a two-sided preconditioning conjugate gradient method to solve an ill-posed linear system. Additionally, the newly developed dynamical Jacobian-inverse free method was developed to overcome the non-convergence for solving the infiltration problem in layered soils [16]. An improved Jacobi iterative method with two-side equilibration was presented to obtain the numerical solution of groundwater flow in unsaturated soils [17]. ...
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... The RE generally requires spatial discretization using numerical methods, such as finite difference method (FDM) [16,18], finite element method (FEM) [19] and finite volume method (FVM) [20]. A backward-Euler finite-difference stepping scheme is usually adopted for time discretization [21]. ...
... Furthermore, the vertex-centered finite-difference grid and the backward Euler finite-difference stepping scheme are used for the numerical discretization of Eq. (18). The matrix format of the standard Picard iteration (PI) method can be written as follows [26]: ...
... unsaturated soil parameters are g = 8 × 10 −3 , s = 0.35 , r = 0.14 , and K s = 1 × 10 −4 m/h [18]. ...
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The Hermitian and skew-Hermitian splitting iteration method (HSS) is commonly an effective linear iterative method for solving sparse non-Hermite positive definite equations. However, it is time-consuming to solve linear equations. Hence, inexact Hermitian and skew-Hermitian splitting iteration approaches with multistep preconditioner (PIHSS(m)) are proposed for analyzing underground water flow. For unsaturated porous media, an exponential model is adopted to linearize the Richards equation. The governing equations are discretized using the finite element method to produce a system of linear equations. Furthermore, the inexact Hermitian and skew-Hermitian splitting iteration methods (IHSS) and PIHSS(m) are used to solve the linear equations. The results show that PIHSS(m) can effectively solve the 1D unsaturated flow problem and 2D transient drainage problem in partially and completely saturated soils. The IHSS has higher numerical accuracy than the classical methods such as Picard method and Gauss-Seidel iterative method. Compared with IHSS, PIHSS(m) achieves faster convergence rate and higher computational efficiency, particularly for solving groundwater flow problems with high grid density. Additionally, the numerical results reveal that PIHSS(m) has excellent acceleration, that is, at least 50% acceleration compared with the IHSS.
... Due to the nonlinear nature of RE, the analytical solution is difficult to obtain, and it is often obtained based on an exponential form (Srivastava and Yeh 1991;Tracy 2006). Thus, different numerical methods were employed to solve RE (Zha et al. 2013;Zeng et al. 2018), including finite volume method (FVM), finite difference method (Liu et al. 2015), and finite element method (Pop et al. 2004). Wang and Anderson (1982) introduced the practical application of finite difference and finite element to the numerical simulation of groundwater seepage and pollution propagation. ...
... The thickness (L) of the soil layer is 10 m. Gardner model is used to represent the soil-water characteristic curve of unsaturated soils, and the parameters are a = 1 × 10 −4 /m, θ s = 0.50, θ r = 0.11, and K s = 9 × 10 −5 m/s (Liu et al. 2015). The initial condition is assumed to be h(z,t=0)=h d . ...
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... Several numerical approaches based on the meshebased methods to the modeling of flow movement in unsaturated porous media have been proposed, such as the boundary element method [26], the finite difference method (FDM) [20,21], and the finite element method [31,33]. Even though the success of meshebased methods is effective and easily implemented for dealing with unsaturated flow problems, limitations still remain while utilizing the meshebased methods including meshegeneration for complex geometries, or short time interval for the numerical convergence. ...
... We therefore compare the computed results with that of the FDM, as depicted in Fig. 9. The results agree very well with those of the FDM [20]. ...
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This paper presents a study for solving unsaturated flow in heterogeneous porous media using the meshless method with the radial basis function (RBF). For modeling the nonlinear hydrological process in unsaturated zone, an exponential model is introduced in the Richards equation such that we may obtain the linearized Richards equation. We adopt the multiquadric function as the RBF in the meshless method for solving the linearized Richards equation. For simulating the unsaturated flow problems in layered heterogeneous soils, the flux and the head must satisfy the continuity condition at the interface. Several examples are carried out for modeling the hydrological process in multi–layered unsaturated soils. The results demonstrate that we only discretize by a set of points without tedious mesh generation and significantly enhance the applicability for solving unsaturated flow problems, especially in heterogeneous multi–layered soils with extreme physical property contrasts.
... In recent years, the modeling of flows in saturated and unsaturated porous media has attracted considerable interest [1][2][3]. The analysis of saturated and unsaturated flows is crucial in practical engineering applications, especially in problems pertaining to soil science, hydrogeology, and geotechnical engineering [4][5][6]. Therefore, the modeling of saturated and unsaturated flows has emerged as a crucial research topic. ...
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In this paper, we propose a novel meshless approach that involves using space–time polyharmonic radial polynomial basis functions for modeling saturated and unsaturated flows in porous media. In this study, space–time polyharmonic radial polynomial basis functions were developed in the space–time domain using a meshless collocation method. This domain contains three sets of collocation points, namely the inner, source, and boundary points, for the spatial and temporal discretization of the governing equation. Because the initial and boundary data are accessible space–time boundaries, the solutions of groundwater flows problems are approximated by solving the inverse boundary value problem in the space–time domain without using the conventional time-marching scheme. Saturated and unsaturated flow problems were investigated to demonstrate the robustness of the proposed method. The results obtained using the proposed approach were compared with those obtained using the conventional polyharmonic spline radial basis function. The proposed space–time polyharmonic radial polynomial basis functions obtained highly accurate solutions. Moreover, in solving saturated and unsaturated flow problems, the accuracy and stability of the proposed functions were higher than those of the conventional time-marching scheme.