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Comparative Evaluation of Slope Reinforcement Techniques under Pseudo-Static Unsaturated and Rainfall Conditions

DOI : https://doi.org/10.5281/zenodo.18163349
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Comparative Evaluation of Slope Reinforcement Techniques under Pseudo-Static Unsaturated and Rainfall Conditions

Md Aadil Arfin

Department of Civil Engineering, Jamia Millia Islamia, New Delhi 110025

Syed Mohammad Abbas

Department of Civil Engineering, Jamia Millia Islamia, New Delhi – 110025

Abstract – This study evaluates the combined effects of rainfall infiltration and pseudo-static seismic loading on the stability of an unsaturated silty soil slope, using an unreinforced baseline condition for comparison. The baseline slope is subsequently reinforced with soil nails, geogrid layers, and Vetiver grass (Chrysopogon zizanioides) roots to assess the relative effectiveness of each stabilization technique. Rainfall-induced infiltration was modelled to capture reductions in matric suction and the associated loss of shear strength, following which pseudo-static horizontal acceleration coefficients were applied to evaluate seismic response. Key parameters examined include factor of safety, deformation patterns, and failure mechanisms for the baseline and reinforced cases. Results indicate that rainfall significantly weakens the baseline slope prior to seismic loading, thereby increasing its vulnerability to earthquake- induced deformation. Soil nailing and geogrid reinforcement provide comparable improvements in the factor of safety after rainfall, with both techniques effectively controlling deformation. Vetiver roots enhance near-surface resistance but are less effective under stronger pseudo-static loading. These findings highlight the importance of considering both rainfall- induced weakening and seismic effects when selecting reinforcement methods for unsaturated slopes.

Keywords: Soil nailing, Slope stability, Pseudo-static analysis, Unsaturated soil, Rainfall infiltration, Finite element modelling

  1. INTRODUCTION

    Slope stability under seismic loading is a critical concern in geotechnical engineering, particularly for man-made slopes such as road and railway embankments, excavated cuttings, and engineered fills. These slopes often remain in an unsaturated condition, and their behaviour is strongly influenced by rainfall infiltration [1]. Rainfall reduces matric suction and, consequently, the shear strength of the soil, making slopes more susceptible to failure if an earthquake occurs during or shortly after wet conditions. Therefore, assessing the combined effects of rainfall-induced suction loss and seismic loading is crucial for reliable stability evaluation in unsaturated soils. In this study, static effects are not considered, and only the seismic response is examined. The pseudo-static method provides a practical and widely used approach for representing seismic loading in slope stability analysis by applying equivalent horizontal acceleration coefficients. This approach has been widely used in engineering practice for evaluating seismic slope stability

    due to its simplicity and reasonable accuracy for design-level assessments [2]. However, the performance of reinforced unsaturated slopes under such conditions depends not only on seismic forces but also on the pore-water pressure changes caused by rainfall. Ignoring rainfall effects can lead to an overestimation of slope safety during earthquakes.

    In this context, the present study investigates the pseudo- static stability of an unsaturated silty soil slope after rainfall infiltration. Three reinforcement techniques, namely soil nailing, geogrid reinforcement, and Vetiver grass roots, are evaluated to assess their effectiveness in improving seismic stability. Soil nails act as deep structural inclusions, geogrids provide tensile resistance and enhance load distribution, and Vetiver roots improve shallow strength and erosion resistance.

    The aim of this study is to provide a comparative assessment of three slope reinforcement techniques, namely soil nailing, geogrid reinforcement, and Vetiver grass roots, under combined rainfall infiltration and pseudo-static seismic loading. The evaluation focuses on variations in factor of safety, deformation characteristics, and plastic strain development in order to understand the stability response and failure behaviour of reinforced unsaturated slopes. The study helps in selecting effective reinforcement methods for slopes under rainfall and seismic conditions.

  2. MATERIALS AND METHODS
    1. Materials

      The numerical analysis incorporated four components including the soil, soil nails, geogrid, and the Vetiver root system. The mechanical and physical properties of the soil are presented in Table 1, while the properties of the reinforcement elements are summarized in Table 2. Soil parameters were used in effective stress form, while the reinforcement characteristics were obtained from relevant literature and manufacturer specifications. The soil behaviour was represented using the MohrCoulomb constitutive model, which is commonly applied in slope stability studies because of its simplicity and ability to describe shear failure [3]. The required input parameters, namely effective cohesion (c), friction angle (), Youngs

      modulus (E), and effective Poissons ratio () are summarized in Table 1.

      TABLE 1. SOIL PROPERTIES ADOPTED IN THE STUDY

      Material Property Symbol Value Unit
      Soil Unit weight 20 kN/m³
      Effective Cohesion c 10 kPa
      Effective Friction angle 20 °
      Youngs modulus E 7500 kPa
      Effective

      Poissons ratio

      0.35
      Saturated permeabili

      ty

      ksat 1×10-6 m/sec

      TABLE 2. REINFORCEMENT PROPERTIES TAKEN FOR CONSIDERATION

      instead, they were digitized directly from the published figures. Although minor deviations may occur due to digitization, the overall trends were preserved, and the interpreted suctionsaturation and saturationpermeability data were implemented in ABAQUS as tabulated input. This approach ensured a realistic representation of rainfall-induced changes in the unsaturated silty soil. The adopted curves are presented in Fig. 1

      Material Property Symbol Value Unit
      Soil Nail Density 7850 kg/m³
      Youngs modulus E 2×108 kPa
      Yield stress fy 500 MPa
      Poissons ratio 0.3
      Geogrid Density 950 kg/m³
      Youngs modulus E 1300 MPa
      Poissons ratio p>0.3
      Vetiver roots Density 900 kg/m3
      Mean Diameter d 0.8 mm
      Root Area Ratio RAR 0.025

      Fig. 2 Relative permeability curve of the soil as a function of degree of saturation

      Unsaturated soil behaviour was represented using the extended effective stress concept, in which matric suction contributes to the effective stress [4].

      = ( ) + ( )

      where is the effective stress, is the total stress, and

      are the pore-air and pore-water pressures, and is the effective stress parameter. In accordance with [5], the parameter was defined as the degree of saturation, ensuring that the influence of matric suction on shear strength decreases progressively and becomes zero at full saturation.

      Rainfall effects were incorporated through the Soil Water Characteristic Curve (SWCC) and the corresponding permeability function published in [6]. In their work, these hydraulic relationships were obtained by fitting experimental data. In the present study, the curves were not recalibrated;

    2. Geometry

      For the numerical analysis, a representative manmade slope of approximately 10 m height was adopted and analysed under plane-strain conditions using 8-node biquadratic plane strain elements with coupled pore-pressure degrees of freedom (CPE8P). The configuration comprises a steeply inclined slope face with a finite crest width and a horizontal bench at the toe, forming a configuration commonly adopted in numerical stability studies of engineered slopes. The geometry was kept fixed for all analyses and is illustrated schematically in Fig. 3.

      define the regional seismic hazard through seismic zone factors and design ground acceleration [8]. The choice of the pseudo-static coefficient follows established geotechnical practice, wherein a reduced fraction of the peak ground acceleration is adopted to represent average seismic inertial effects while avoiding excessive conservatism [9].

      Fig. 3 Schematic representation of the slope configuration used in the numerical modelling

    3. Boundary conditions

      The bottom boundary of the model was fixed, preventing both horizontal and vertical displacements, while the vertical side boundaries were restrained horizontally but permitted vertical movement. Rainfall infiltration was imposed as a flux boundary condition along the exposed slope surface, with the applied flux taken as a suitable fraction of the saturated hydraulic conductivity. To simulate drainage conditions, a small outlet was incorporated at the slope base by prescribing a zero-pore pressure boundary, thereby allowing unrestricted drainage during infiltration. An initial geostatic step was executed to establish the in-situ stress equilibrium prior to the application of subsequent loading.

    4. Loading conditions

      Self-weight of the soil mass was simulated by applying gravitational loading over the entire domain. Pedestrian loading at the slope crest was idealized as a uniformly distributed surface load of 5 kPa. This value corresponds to the crowd loading intensity specified for footways in IRC:6- 2017 and was adopted here as a conservative representation of maximum possible pedestrian occupancy at the crest [7]. The slope was further subjected to rainfall infiltration over a 48-hour period. The rainfall intensity was prescribed as a fraction of the saturated hydraulic conductivity of the soil, such that the applied rate remained slightly below the infiltration capacity. This approach replicates near-saturated field conditions without immediate surface runoff, thereby enabling progressive pore-water pressure build-up within the slope, a key factor in evaluating rainfall-induced instability. The rainfall pattern was defined as linearly increasing during the first 6 hours, remaining constant for the following 36 hours, and decreasing linearly over the final 6 hours.

      Seismic loading was simulated using the pseudo-static approach, in which a constant horizontal body force corresponding to a seismic coefficient of = 0.15 was applied after rainfall-induced pore-pressure redistribution. The selected value represents approximately 50% of the expected peak ground acceleration for moderate-to-high seismic regions. IS 1893 (Part 1): 2016 was used solely to

      Only the horizontal seismic component was considered in the pseudo-static analysis, as it primarily governs slope instability through shear deformation. The vertical component was not included, since its influence in pseudo- static slope stability analyses is generally secondary and inconsistent, primarily affecting normal stresses rather than driving shear failure [9]. Slope stability was evaluated under pseudo-static loading conditions, with and without rainfall infiltration.

    5. Numerical Modelling Procedure

      The numerical analysis was conducted in ABAQUS, with soil behaviour represented by the MohrCoulomb constitutive model, a widely adopted framework for slope stability studies. Shear strength was defined in terms of effective stress parameters (c and ), while elastic properties were characterized by Youngs modulus (E) and the effective Poissons ratio (). The initial water content of the soil was maintained at 15%, which corresponded to the starting point on the SWCC and defined the initial matric suction condition for the unsaturated slope prior to rainfall infiltration. Unsaturated soil response was modelled using the Soil Water Characteristic Curve (SWCC) coupled with a permeability saturation data, capturing the variation of suction, saturation, and hydraulic conductivity under rainfall infiltration.

      The soil nails were modelled as linear-elastic beam elements embedded within the soil mass to allow the transfer of axial and bending forces from the nails into the surrounding ground, which is essential for capturing the composite action that provides slope reinforcement [10]. Each nail had a diameter of 20 mm, with lengths ranging from 3-5 m depending on their position along the slope to ensure they extended beyond the potential slip surface. The reinforcement was installed at an inclination of 36.87° to the horizontal, corresponding to a perpendicular orientation to the slope face, and the spacing followed the adopted reinforcement layout. The nail head was idealized at the slope face using a short line element with an equivalent square plate representation to account for nail headfacing load transfer.

      The geogrid reinforcement was modelled using truss elements, which carry only axial tensile forces and do not resist bending; this approach is appropriate because geogrids primarily function as tensile reinforcement in soil. Only the density and Youngs modulus of the polypropylene (PP) geogrid were taken directly from the range reported in the literature [11] and are listed in Table 2. Since Poissons ratio was not reported, a representative value of 0.30 was adopted for polypropylene geosynthetics, which lies within the commonly reported range (0.250.35) in the literature as

      reported by [12]. The analysis was performed under 2D plane-strain conditions; therefore, a uniaxial geogrid representation was adopted. Although the reference source reports tensile strengths at 5% strain and at ultimate strain, the present application involves a lightly loaded slope, where the mobilised strains are expected to remain small. Accordingly, a working-strain tensile strength of 20 kN/m at 2.5% strain was adopted, as this lies within the typical serviceability strain range (25%) for polypropylene geogrids reported in the literature [12]. Each geogrid layer was representedby truss elements with an equivalent cross-sectional area assigned through a nominal thickness, so as to reproduce the axial stiffness of the reinforcement. The first reinforcement layer was placed 0.25 m below the slope surface, followed by a second layer at a vertical spacing of 0.75 m. Subsequent

      All reinforcement elements were coupled to the soil using embedded-region constraints, a commonly adopted simplification for tensile reinforcements in numerical slope analyses.

    6. Determination of factor of safety (Strength Reduction Method)

      Slope stability was evaluated using the strength reduction method (SRM), in which the soil shear strength parameters are systematically reduced until numerical failure occurs. In this approach, the effective cohesion c and the tangent of the effective friction angle tan are divided by a trial strength reduction factor F, such that

       

      layers were installed at 1.0 m vertical intervals down the slope. Reinforcement layer lengths were varied from 2.75 m to 6.25 m depending on depth, to ensure adequate embedment

      into the stable zone beyond the potential slip surface. These

      where c and are the reduced shear strength parameters.

      values were adopted as reasonable design assumptions, r r

      consistent with ranges reported in reinforced slope practice [13].

      Vetiver roots were simulated using distributed truss elements, allowing only tensile resistance to be mobilized. A mean root diameter of 0.8 mm was adopted as a representative value. The corresponding root tensile strength and Youngs modulus were defined using the empirical diameter-dependent relationships proposed in [14], where Equation (1) estimates tensile strength as a function of root diameter (D, mm) and Equation (2) provides the associated Youngs modulus. A root area ratio (RAR) of 0.025% was selected within the experimentally reported range for Vetiver grass roots under landslide-affected and early growth conditions, as reported in [15]. For numerical modelling, the RAR was assumed to be uniformly distributed over the entire root depth as a simplifying assumption. As the empirical relationships were derived from tests conducted in clayey soils, a conservative reduction factor of 0.7 was applied to the computed root tensile strength to reflect the potentially weaker interaction between roots and silty soils. This value was selected to reflect a moderate reduction while avoiding excessive conservatism, consistent with common practice in parametric and numerical modelling where soil-specific calibration data are unavailable. The Youngs modulus values were adopted without modification.

      TR=15.239×D-0.893 (1)

      ER=342.74×D-1.399 (2)

      Where, Tr denotes the tensile strength (MPa), Er represents Youngs modulus (MPa), and D is the root diameter (mm).

      Failure was identified when the model showed numerical non-convergence or a sharp increase in displacement for a small increase in the strength reduction factor . The value of

      at failure was taken as the factor of safety. This method allows the failure mechanism to develop naturally within the finite element mesh without assuming a predefined slip surface. The procedure follows the concepts reported in [16] and [17], and is now standard practice in finite element slope stability analysis.

    7. Validation of Model

    The numerical model was verified by replicating the unsaturated slope case study presented in [18]. Their slope geometry, boundary conditions, and material properties were adopted directly, and the soilwater characteristic curve (SWCC) was digitized and interpreted from the published data. As the reference study did not report any external loading, only self-weight (gravity) was applied to represent the static condition of the slope.

    The model was first brought to an initial equilibrium state before applying rainfall infiltration. Transient pore-pressure boundary conditions were imposed following the procedures described in [18]. The resulting pore-pressure responses and displacement showed trends consistent with those reported in the original study as shown in Fig. 4 and Fig. 5 respectively. Plastic equivalent strain (PEEQ) developed at the slope toe, which aligns with the failure initiation zone identified in [18]. Although the magnitude of PEEQ differed, the plastic zone remained confined to the same region. These differences are attributed to variations in mesh density, constitutive modelling, and interpretation of the SWCC data.

    Fig. 4 Pore-water pressure distributions in the reproduced benchmark slope under initial conditions and after 72 h of rainfall infiltration

    Fig. 5 Horizontal (U) and vertical (U) displacement contours of the benchmark slope reproduced for validation of the numerical model

    Overall, the model reproduced the same failure mechanism and rainfall-induced behaviour as the reference case, demonstrating adequate accuracy for use in the subsequent analyses of both unreinforced and reinforced slopes.

  3. RESULT AND DISCUSSIONS
    1. Baseline slope

      Fig. 6(a) shows the pore-pressure distribution prior to rainfall, with the slope remaining unsaturated and exhibiting high suction near the surface that gradually decreases with depth. In contrast, Fig. 6(b) illustrates the pore-pressure condition after 48 hours of rainfall infiltration, marked by a considerable reduction in suction near the surface and the development of a wetting front within the slope.

      Fig. 7(a) corresponds to the pseudo-static loading under unsaturated conditions, where the initial matric suction is still present. In this case, the plastic equivalent strain (PEEQ) band develops along a shallower failure path, reflecting the higher apparent shear strength provided by suction. Whereas, Fig. 7(b) represents the pseudo-static loading combined with rainfall infiltration, where suction has been reduced due to wetting. Here, the PEEQ zone becomes more continuous and slightly deeper, indicating a weaker soil mass and a more pronounced tendency toward shear failure as rainfall reduces the effective strength.

      The factor of safety is 1.15 under the pseudo-static unsaturated condition, and it further decreases to 1.10 when rainfall infiltration is introduced, as shown in Fig. 8.

      Fig. 6 Pore-water pressure distributions (a) before rainfall (b) after rainfall infiltration

      Fig. 7 Plastic strain (PEEQ) contours under pseudo-static loading for (a) unsaturated and (b) rainfall-influenced conditions

      Fig. 8 Variation of displacement with factor of safety under pseudo-static loading for unsaturated and rainfall-influenced conditions

    2. Slope Reinforced with Soil Nails

      After validating the model for the baseline (unreinforced) slope, the same approach was used to analyse a soil-nailed slope. Soil nails were installed within the slope, as shown in Fig. 9, to examine how they improve the overall stability under the same boundary and loading conditions. The pore- pressure contours in Fig. 10(a) and Fig. 10(b) closely resemble the baseline state, indicating negligible hydraulic change and unchanged suction within the slope.

      Fig. 9 Layout of soil nails within the slope

      Fig. 10 Pore-water pressure distributions (a) before rainfall (b) after rainfall infiltration

      Under unsaturated conditions, higher PEEQ magnitudes are observed because matric suction enhances the apparent shear strength of the soil, allowing greater stress mobilization prior to

      yielding. Once yielding initiates under pseudo-static loading, plastic strain localizes more distinctly along the failure zone as observed in Fg. 11 (a). After rainfall, the loss of suction reduces soil stiffness and strength, resulting in lower PEEQ values, while the overall failure pattern remains similar is shown in Fig. 11(b).

      Fig. 11 Plastic strain (PEEQ) contours under pseudo-static loading for (a) unsaturated and (b) rainfall-influenced conditions

      In Fig. 12, the factor of safety (FOS) is 1.45 under pseudo-static (unsaturated) conditions and declines slightly to 1.40 when pseudo-static loading is combined with rainfall, indicating that infiltration-driven changes in suction and pore-pressure partially reduce the slopes resistance to failure.

      Fig. 12 Displacementfactor of safety response under unsaturated and rainfall-influenced conditions for pseudo-static loading

    3. Slope Reinforced with Geogrid layers

      The layout of the geogrid reinforcement adopted in the model is shown in Fig. 13, which was introduced to improve the stability of the slope relative to the baseline condition.

      Fig. 13 Geogrid-reinforced slope showing the geogrid layout

      Fig. 14 presents the pore-pressure distribution before and after rainfall. The response of the geogrid-reinforced slope differs noticeably from that of the baseline slope, particularly under rainfall conditions. A distinct pattern

      appears in which the reduction in suction penetrates deeper into the slope and along the reinforced base. This behaviour arises because the geogrid modifies the local stress and deformation fields, thereby influencing the pore- pressure evolution during infiltration.

      Although both cases exhibit a similar overall failure mechanism, the pseudo-static unsaturated condition is presented in Fig. 15(a) shows a higher peak plastic strain, reflecting greater stress mobilization while matric suction is still present. Under rainfall conditions, the reduction in matric suction and the increase in pore-water pressures lead to earlier yielding and a slightly deeper extension of the plastic zone, although the peak PEEQ values are lower, as shown in Fig. 15(b). Despite these differences, in both cases the deformation remains largely confined within the reinforced region near the toe, reaffirming the role of the geogrid in limiting the progression of the shear zone.

      The factor of safety shown in Fig. 16 is 1.45 under pseudo- static (unsaturated) loading and decreases slightly to

      1.40 when rainfall is combined with pseudo-static loading, primarily due to the reduction in matric suction and the associated increase in pore-water pressures, which lowers the soils effective strength.

      Fig. 14 Pore-water pressure distributions (a) before rainfall (b) after rainfall infiltration

      Fig. 15 Plastic strain (PEEQ) contours under pseudo-static loading for (a) unsaturated and (b) rainfall-influenced conditions

      Fig. 16 Displacementfactor of safety response under pseudo-static loading for unsaturated and rainfall-influenced conditions

    4. Soil Reinforced with Vetiver roots

      The vetiver root adopted in the soil slope is shown in Fig. 17. As shown in Fig. 18(a) and (b), the pore-pressure patterns differ very little from the baseline, indicating that the presence of vetiver roots does not significantly alter the hydraulic behaviour within the slope. In the pseudo- static unsaturated case, as shown in Fig. 19(a) the slope exhibits a localized higher peak PEEQ value near the toe, while plastic strain elsewhere remains relatively low and distributed over a broader area. In contrast, under pseudo- static rainfall conditions, the peak PEEQ value is lower; however, the plastic strain zone becomes more continuous, extends deeper, and propagates further upslope along the potential slip surface as shown in Fig. 19(b). This occurs because rainfall reduces matric suction and increases pore-water pressure, causing plastic deformation to develop over a larger portion of the slope even at lower strain levels.

      Fig. 17 Vetiver root layout within the slope

      Fig. 18 Pore-water pressure distributions (a) before rainfall (b) after rainfall infiltration

      Fig. 19 Plastic strain (PEEQ) contours under pseudo-static loading for (a) unsaturated and (b) rainfall-influenced conditions

      Fig. 20 illustrates that slope stability reduces under the combined effects of rainfall and seismic loading. The pseudo-static unsaturated case reaches a FOS of 1.20, whereas the pseudo-static rainfall condition yields the lowest value at 1.15, indicating a limited margin of safety.

      Fig. 20 Displacementfactor of safety response under pseudo-static loading for unsaturated and rainfall-influenced conditions

    5. Comparative Displacement Behaviours (Critical Case)

    Fig. 21 shows the horizontal displacement contours for all slope configurations under the critical pseudo-staticrainfall condition at their respective Factors of Safety. The baseline slope (a) develops a small and shallow deformation zone near the surface, indicating the early stage of failure, consistent with the sharp increase in horizontal displacement used to identify the critical Factor of Safety in the SRM approach. The nail-reinforced slope (b) exhibits a deeper and more distributed deformation zone compared to the baseline case, reflecting the mobilization of nail and soil interaction that transfers loads into the stable interior of the slope and promotes a deeper failure mechanism. The geogrid- reinforced slope (c) has a more confined and narrower deformation zone, especially when compared to the wider zones in (a) and (b). This localized pattern reflects the geogrids ability to restrict lateral deformation and provide effective confinement within the reinforced region. The vetiver-reinforced slope (d) shows a moderately wide deformation zone extending toward the slope face and toe, indicating improved control of shallow movements associated with root reinforcement.

    Although the absolute displacement magnitudes are not directly comparable because each configuration is plotted at its own critical Factor of Safety, the deformation patterns collectively indicate that all reinforcement types enhance stability, with structural systems providing deeper confinement and vegetation offering an effective and sustainable solution for shallow stabilization.

    Fig. 22 illustrate the vertical displacement contours for all slope configurations under the critical pseudo-static rainfall condition at their respective Factors of Safety. The baseline slope (a) shows only minor crest settlement, indicating the onset of shallow deformation. In contrast, the nail-reinforced slope (b) exhibits a more pronounced and slightly deeper crest settlement band, reflecting mobilization of shear resistance within the reinforced zone and redistribution of deformation toward the slope crest as lateral movement is restrained. The geogrid-reinforced slope (c) exhibits the largest localized crest settlement, reflecting strain concentration near the upper ends of the stiff reinforcement layers. By limiting lateral spreading, the geogrids promote vertical adjustment that becomes more evident near the crest.

    The vetiver-reinforced slope (d) exhibits limited and diffuse crest settlement, indicating an indirect reduction in crest deformation due to root reinforcement concentrated along the slope face and shallow subsurface. Overall, although the reinforced slopes exhibit larger localized crst settlements, the deformation remains confined and represents strain redistribution rather than global instability.

    Fig. 21 Horizontal displacement contours at the respective FOS under pseudo-static rainfall-influenced conditions for (a) baseline, (b) soil-nailed, (c) geogrid, and

    (d) vetiver-reinforced slope

    Fig. 22 Vertical displacement contours at the respective FOS under pseudo-static rainfall-influenced conditions for (a) baseline, (b) soil-nailed, (c) geogrid, and (d) vetiver-reinforced slope

    F. Comparison of Factor of Safety

    Fig. 23 presents that under pseudo-static unsaturated loading, both soil nails and geogrids produce a 26.09% increase in the FOS relative to the baseline slope, demonstrating strong and comparable reinforcement effects, while vetiver roots

    contribute a modest 4.35% improvement. Under rainfall- influenced conditions, the relative improvement provided by nails and geogrids increases slightly to 27.27%, indicating that their stabilizing performance remains effective despite the reduction in matric suction. Vetiver roots exhibit a small increase in relative improvement to 4.55% under rainfall conditions, reflecting a limited but consistent enhancement of slope stability.

    Fig. 23 Percentage improvement in FOS for different slope reinforcement systems under unsaturated and rainfall-influenced conditions

  4. CONCLUSIONS
    1. Under the pseudo-static loading, both the nail reinforced and the geogrid reinforced slopes showed equal improvement in FOS over the baseline condition, with values of approximately 26.1% under unsaturated case and 27.3% under rainfall-influenced condition, while the vetiver reinforced slope showed only small values of approximately 4.4% and 4.6% in the FOS improvement for unsaturated and rainfall-influenced states respectively, highlighting the much stronger effect of structural reinforcements.
    2. The horizontal displacement behaviour indicates that the different reinforcement systems develop more defined and organized deformation patterns compared to the baseline slope, reflecting a more stable distribution of lateral movements under pseudo-static conditions.
    3. Vertical displacement behaviour shows that each slope configuration develops a distinct crest-settlement pattern, with the reinforced slopes forming more localized deformation zones than the baseline case. These differences reflect the characteristic deformation response of each system under pseudo-static conditions.
    4. Plastic strain (PEEQ) patterns indicate that reinforcement promotes more favourable failure mechanisms compared to the shallow slip observed in the baseline slope. The nail and geogrid systems develop deeper, more distributed plastic zones, while the vetiver system forms a continuous and clearly developed plastic band. Overall, all reinforcement types contribute to a more stable and controlled deformation response under pseudo-static loading.
    5. The pore-pressure response under rainfall shows that the applied drainage boundary effectively dissipated infiltrated water and prevented excessive positive pore- pressure buildup, supporting a more stable hydraulic condition within the slope during analysis.
    6. The overall findings demonstrate that soil nails and geogrid reinforcement provide greater stability improvement, while vetiver roots offer a sustainable, resource-efficient option for shallow slopes, highlighting the practical applicability of these techniques under pseudo-static conditions.
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