K.G. Gavin
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36 records found
1
A structured four-step approach is adopted. Step 1 performs one-dimensional (1D), two-dimensional (2D), and 3D site response analyses (SRA) in linear elastic soil, validating the numerical setup against analytical solutions. Step 2 introduces the pile and superstructure, modelled with linear elastic material, in the same medium to assess the dynamic characteristics and their response under steady-state monoharmonic excitation, allowing verification of the SSI model against benchmarks from the literature. To capture more realistic soil behaviour, the framework then incorporates the SANISAND-MS constitutive model, which accounts for nonlinear cyclic sand response, including strain accumulation and stiffness degradation. In Step 3, SRAs with displacement input motions of varying amplitude are performed under both broadband Ormsby and steady-state monoharmonic excitation to evaluate the influence of nonlinearity on free-field response. Finally, Step 4 couples the nonlinear soil with the structure to examine the fully integrated dynamic characteristics under nonlinear SSI conditions.
Overall, the analyses establish best practice boundary conditions and numerical setups for seismic SRA and SSI modelling in PLAXIS 3D for linear elastic soil (Steps 1 and 2), and quantify the transition from inertial to kinematic dominance in the i response of a flexible pile (Step 2). In the nonlinear domain, the results from Step 3 highlight the critical role of loading type in capturing key features of nonlinear free-field response. More specifically, with steady-state monoharmonic excitation of increasing amplitude, the transition from linear to nonlinear behaviour is captured, along with a shift of predominant frequencies to lower values compared to the linear elastic SRA. In contrast, when the same procedure is applied with the broadband impulse load Ormsby wavelet, post-impulse stiffening effects are revealed, expressed as an upshift in resonance frequency. In Step 4, the dynamic characteristics of the monopile-superstructure system are assessed under nonlinear SSI conditions. However, computational cost prevents the execution of full amplitude sweeps, underscoring the practical trade-off between accuracy and run time in high-fidelity 3D nonlinear SSI modelling. Instead, the 1995 Kobe earthquake record is employed to assess the system’s behaviour under real, multi-harmonic excitation. Altogether, the work demonstrates the potential of advanced 3D FE tools to enhance the seismic design of monopiles. ...
A structured four-step approach is adopted. Step 1 performs one-dimensional (1D), two-dimensional (2D), and 3D site response analyses (SRA) in linear elastic soil, validating the numerical setup against analytical solutions. Step 2 introduces the pile and superstructure, modelled with linear elastic material, in the same medium to assess the dynamic characteristics and their response under steady-state monoharmonic excitation, allowing verification of the SSI model against benchmarks from the literature. To capture more realistic soil behaviour, the framework then incorporates the SANISAND-MS constitutive model, which accounts for nonlinear cyclic sand response, including strain accumulation and stiffness degradation. In Step 3, SRAs with displacement input motions of varying amplitude are performed under both broadband Ormsby and steady-state monoharmonic excitation to evaluate the influence of nonlinearity on free-field response. Finally, Step 4 couples the nonlinear soil with the structure to examine the fully integrated dynamic characteristics under nonlinear SSI conditions.
Overall, the analyses establish best practice boundary conditions and numerical setups for seismic SRA and SSI modelling in PLAXIS 3D for linear elastic soil (Steps 1 and 2), and quantify the transition from inertial to kinematic dominance in the i response of a flexible pile (Step 2). In the nonlinear domain, the results from Step 3 highlight the critical role of loading type in capturing key features of nonlinear free-field response. More specifically, with steady-state monoharmonic excitation of increasing amplitude, the transition from linear to nonlinear behaviour is captured, along with a shift of predominant frequencies to lower values compared to the linear elastic SRA. In contrast, when the same procedure is applied with the broadband impulse load Ormsby wavelet, post-impulse stiffening effects are revealed, expressed as an upshift in resonance frequency. In Step 4, the dynamic characteristics of the monopile-superstructure system are assessed under nonlinear SSI conditions. However, computational cost prevents the execution of full amplitude sweeps, underscoring the practical trade-off between accuracy and run time in high-fidelity 3D nonlinear SSI modelling. Instead, the 1995 Kobe earthquake record is employed to assess the system’s behaviour under real, multi-harmonic excitation. Altogether, the work demonstrates the potential of advanced 3D FE tools to enhance the seismic design of monopiles.
Pile run prediction utilizing SRD methods
A study on the current drivability prediction methods, focusing on SRD limitations for intermediate soils and rate effects
This research investigates pile run by focusing on the limitations of current static Soil Resistance to Driving (SRD) prediction methods and the influence of soil consolidation on pile driveability. Traditional SRD approaches, such as Alm and Hamre, that relies on CPT data are reviewed critically and their limitations are assessed. Studies show that while this method performs well for clean sands and clays, it is unreliable for soil mixtures and intermediate soils, where discrepancies arise due to different consolidation conditions during CPT testing and driving.
To address these limitations, the study evaluates penetration rate effects by comparing drainage conditions during CPT testing and during driving, using GRLWEAP software to calculate the driving velocities. Adjustments are then made to the SRD predictions applying reduction factors that represent the changes in drainage conditions and loss of soil resistance due to consolidation effects.
This study shows that in regions where unpredicted pile runs occurred the adoption of those reduction factors help in the identification of pile run risk regions. However, a more extensive database of soil tests considering different soil density, fines content, and consolidation state should be analyzed to propose definitive reduction factors that can be widely used for different soil conditions around the globe.
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This research investigates pile run by focusing on the limitations of current static Soil Resistance to Driving (SRD) prediction methods and the influence of soil consolidation on pile driveability. Traditional SRD approaches, such as Alm and Hamre, that relies on CPT data are reviewed critically and their limitations are assessed. Studies show that while this method performs well for clean sands and clays, it is unreliable for soil mixtures and intermediate soils, where discrepancies arise due to different consolidation conditions during CPT testing and driving.
To address these limitations, the study evaluates penetration rate effects by comparing drainage conditions during CPT testing and during driving, using GRLWEAP software to calculate the driving velocities. Adjustments are then made to the SRD predictions applying reduction factors that represent the changes in drainage conditions and loss of soil resistance due to consolidation effects.
This study shows that in regions where unpredicted pile runs occurred the adoption of those reduction factors help in the identification of pile run risk regions. However, a more extensive database of soil tests considering different soil density, fines content, and consolidation state should be analyzed to propose definitive reduction factors that can be widely used for different soil conditions around the globe.
Digital Twin-Based Scour Monitoring of Masonry Bridges
Case Study of the Regent Bridge
This study explores the use of digital twin (DT) technology to overcome the shortcomings of current monitoring and maintenance strategies. By integrating real-world monitoring measurements with finite element modeling, the DT framework provides the opportunity to simulate "what-if" scenarios under high-fidelity conditions. Such advancements offer novel prospects for detecting scour-induced damage and intervening for the maintenance. This study utilizes DT technology within the context of a scour monitoring project for a masonry bridge in Northern Ireland, United Kingdom. A digital twin-based SHM and maintenance framework is developed to achieve seamless communication between the virtual model and the physical structure using sensor data. The developed model addresses limitations associated with traditional monitoring and maintenance approaches and demonstrates the potential of digital twins in forward model calibration and backward decision-making. ...
This study explores the use of digital twin (DT) technology to overcome the shortcomings of current monitoring and maintenance strategies. By integrating real-world monitoring measurements with finite element modeling, the DT framework provides the opportunity to simulate "what-if" scenarios under high-fidelity conditions. Such advancements offer novel prospects for detecting scour-induced damage and intervening for the maintenance. This study utilizes DT technology within the context of a scour monitoring project for a masonry bridge in Northern Ireland, United Kingdom. A digital twin-based SHM and maintenance framework is developed to achieve seamless communication between the virtual model and the physical structure using sensor data. The developed model addresses limitations associated with traditional monitoring and maintenance approaches and demonstrates the potential of digital twins in forward model calibration and backward decision-making.
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The 3DSSI model includes soil modelled by the subgrade reaction model (spring model) the steel sheet pile is modelled with shell elements in the finite element software DIANA FEA. The model includes both physical nonlinear and geometrical nonlinear behaviour and captures the soil-structure interaction. Also oblique bending, which is an existing phenomena of older, existing double U-sheet piles, can be captured with interface elements in the 3DSSI model. Nowadays, sheet piles are also designed using the subgrade reaction model and the sheet pile is modelled as a beam with the appropriate stiffness. The 3DSSI model is able to illustrate the 3D behaviour of the sheet pile, without having to model the soil with solid elements as well. This is beneficial with respect to calculation time.
With the 3DSSI model, the hole weakening of sheet piles can be studied. The influence of different parameters on the sheet pile resistance and behaviour is studied. The parameters studied, based on literature findings, are: hole diameter, hole location (level of the hole in depth), hole spacing (hole centre to centre distance in width), hole in-pan (compression zone) or out-pan (tension zone), sheet pile cross-section class 2 and 3 and oblique bending.
The influence of hole weakening on sheet pile behaviour and resistance is studied by finding in the parameter study for each case the load-displacement curve and from this load-displacement curve, the stiffness is derived. The load-displacement curve and stiffness curve include both steel and soil behaviour.
Resulting from the parameter study, the holes significantly reduce the sheet pile resistance and behaviour. The cases with holes in tension show less reduction in resistance and stiffness reduction. The hole diameter is also influencing the results, but the influence of hole location and hole spacing is relatively small. The failure modes are for holes in compression zone is plasticity around the hole and local buckling in the webs. For holes in tension zone, the failure mode is also plasticity around the hole, but also local buckling in the compression flange. For cases including oblique bending and holes in tension zone do not show local buckling in the compression flange, but in the compression web, due to the inclined neutral axis caused by oblique bending.
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The 3DSSI model includes soil modelled by the subgrade reaction model (spring model) the steel sheet pile is modelled with shell elements in the finite element software DIANA FEA. The model includes both physical nonlinear and geometrical nonlinear behaviour and captures the soil-structure interaction. Also oblique bending, which is an existing phenomena of older, existing double U-sheet piles, can be captured with interface elements in the 3DSSI model. Nowadays, sheet piles are also designed using the subgrade reaction model and the sheet pile is modelled as a beam with the appropriate stiffness. The 3DSSI model is able to illustrate the 3D behaviour of the sheet pile, without having to model the soil with solid elements as well. This is beneficial with respect to calculation time.
With the 3DSSI model, the hole weakening of sheet piles can be studied. The influence of different parameters on the sheet pile resistance and behaviour is studied. The parameters studied, based on literature findings, are: hole diameter, hole location (level of the hole in depth), hole spacing (hole centre to centre distance in width), hole in-pan (compression zone) or out-pan (tension zone), sheet pile cross-section class 2 and 3 and oblique bending.
The influence of hole weakening on sheet pile behaviour and resistance is studied by finding in the parameter study for each case the load-displacement curve and from this load-displacement curve, the stiffness is derived. The load-displacement curve and stiffness curve include both steel and soil behaviour.
Resulting from the parameter study, the holes significantly reduce the sheet pile resistance and behaviour. The cases with holes in tension show less reduction in resistance and stiffness reduction. The hole diameter is also influencing the results, but the influence of hole location and hole spacing is relatively small. The failure modes are for holes in compression zone is plasticity around the hole and local buckling in the webs. For holes in tension zone, the failure mode is also plasticity around the hole, but also local buckling in the compression flange. For cases including oblique bending and holes in tension zone do not show local buckling in the compression flange, but in the compression web, due to the inclined neutral axis caused by oblique bending.
The objective of this thesis is to look at the spatial variability in the vertical direction of the Pleistocene sand from the Kreftenheye and Boxtel Formation in the Port of Rotterdam and see if the river Meuse has any influence on the spatial variability in the vertical direction. An additional question is asked if the spatial variability has any influence on the computation of the pile base capacity for a single foundation pile and what are the implications of the answer to that question. To answer these questions, four sites in the Maasvlakte, Botlek and Pernis were selected and the cone penetration tests (CPTs) taken at the twelve sites were used for this thesis. An empirical method which uses CPT data to identify soil layers was used to identify the Pleistocene sand layer in the CPT data. The first part of the thesis uses the cone resistance data of the CPTs to estimate the spatial variability of the sites. The second part of the thesis focuses on the additional research question by using random field theory. Per site, the mean, standard deviation and vertical scale of fluctuation θv were used to generate simulations of cone resistance data. For each combination of standard deviation and θv 500 simulations were carried out. For each simulation the pile base capacity was computed with two CPT-based averaging methods, Koppejan method and LCPC method. The coefficient of variation of pile base capacity is used to measure the uncertainty of the computed pile base capacity.
The results show that the range θv values are: 0.26 – 2 m in the Maasvlakte, 0.24 – 1.76 m in the Botlek and 0.14 – 1.18 m in Pernis. In terms of the mean θv, you see a gradual increase from the upstream area (Pernis) to the downstream area (Maasvlakte). The increase is from 0.27 – 0.63 m in Pernis to 0.64 – 0.80 m in Botlek to 0.84 – 1.86 m in Maasvlakte. However, it is not clear if this is due to the Meuse or due to the existence of sublayers in the geological formation or due to some other factor. Further investigation is needed before a conclusive answer can be given. The answer for the second part is that as long θv is significantly larger than the pile diameter D (θv ≥ 4D), it does not influence the uncertainty of the computed pile base capacity. However, the mean and standard deviation of cone resistance does influence the uncertainty of the computed pile base capacities. Finally, it is observed that spatial variability does not play a role in the uncertainty of the computed pile base capacity if the coefficient of variation of the cone resistance cv (qc) is small (cv (qc) ≤ 0.15). The implication for the uncertainty of the computed pile base capacity and therefore the pile design is that one can afford to have a less accurate description of the spatial variability from using fewer CPTs if θv ≥ 4D. The same holds true if cv(qc) ≤ 0.15.
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The objective of this thesis is to look at the spatial variability in the vertical direction of the Pleistocene sand from the Kreftenheye and Boxtel Formation in the Port of Rotterdam and see if the river Meuse has any influence on the spatial variability in the vertical direction. An additional question is asked if the spatial variability has any influence on the computation of the pile base capacity for a single foundation pile and what are the implications of the answer to that question. To answer these questions, four sites in the Maasvlakte, Botlek and Pernis were selected and the cone penetration tests (CPTs) taken at the twelve sites were used for this thesis. An empirical method which uses CPT data to identify soil layers was used to identify the Pleistocene sand layer in the CPT data. The first part of the thesis uses the cone resistance data of the CPTs to estimate the spatial variability of the sites. The second part of the thesis focuses on the additional research question by using random field theory. Per site, the mean, standard deviation and vertical scale of fluctuation θv were used to generate simulations of cone resistance data. For each combination of standard deviation and θv 500 simulations were carried out. For each simulation the pile base capacity was computed with two CPT-based averaging methods, Koppejan method and LCPC method. The coefficient of variation of pile base capacity is used to measure the uncertainty of the computed pile base capacity.
The results show that the range θv values are: 0.26 – 2 m in the Maasvlakte, 0.24 – 1.76 m in the Botlek and 0.14 – 1.18 m in Pernis. In terms of the mean θv, you see a gradual increase from the upstream area (Pernis) to the downstream area (Maasvlakte). The increase is from 0.27 – 0.63 m in Pernis to 0.64 – 0.80 m in Botlek to 0.84 – 1.86 m in Maasvlakte. However, it is not clear if this is due to the Meuse or due to the existence of sublayers in the geological formation or due to some other factor. Further investigation is needed before a conclusive answer can be given. The answer for the second part is that as long θv is significantly larger than the pile diameter D (θv ≥ 4D), it does not influence the uncertainty of the computed pile base capacity. However, the mean and standard deviation of cone resistance does influence the uncertainty of the computed pile base capacities. Finally, it is observed that spatial variability does not play a role in the uncertainty of the computed pile base capacity if the coefficient of variation of the cone resistance cv (qc) is small (cv (qc) ≤ 0.15). The implication for the uncertainty of the computed pile base capacity and therefore the pile design is that one can afford to have a less accurate description of the spatial variability from using fewer CPTs if θv ≥ 4D. The same holds true if cv(qc) ≤ 0.15.
The influence of vertical loading on the lateral behaviour of rigid monopile foundation in clay soil
An analysis using 3D Finite Element Modeling
All analysis in this study was performed using 3D finite element modeling in PLAXIS 3D software. The NGI-ADP constitutive model was adopted to simulate the nonlinear mechanical behaviour of clay. Considered in the analysis is a short rigid pile with a diameter of 10 m (L/D = 3) and a long flexible pile with a diameter of 2 m (L/D = 15). The analyzed clay soil profiles consist of a normally consolidated clay soil and an overconsolidated clay soil with a constant undrained shear strength profile equal to 30 kPa. For each pile in each type of clay soil, a pure lateral loading scenario is performed first to assess the validity of current design methods. Subsequently, a combined loading scenario is performed to assess the influence of vertical loading on the lateral behaviour of rigid monopile in clay soil.
Results of the pure lateral loading scenario suggest that current design methods heavily underestimate the lateral capacity of rigid monopile foundations in both clay soil profiles analyzed. According to the findings of this study, it can be concluded that current design methods are not fit to provide an accurate assessment regarding the lateral load response of rigid monopile in clay soil. In order to correctly assess the lateral load response of rigid monopile in clay soil, a method consisting of a 3D finite element model akin to the model used in the research or a PISA design model is advised. A potential third design method, the 1D rotational spring model, is also proposed.
Results of the combined loading scenario suggest that the presence of vertical loading causes a decrease in lateral and moment capacity of the rigid pile in both clay soil profiles analyzed. However, the influence is negligible when the vertical load magnitude is smaller than 50% of its bearing capacity. To quantify the influence of vertical load on a monopile foundation, a series of load analysis were performed on a real offshore wind turbine with a 5MW power capacity. It was found that the vertical load on a typical monopile foundation in clay is around 27% of its bearing capacity. According to the findings of this study, it can be concluded that the influence of vertical load on the lateral response of rigid monopiles in clay soil is limited and can be ignored in foundation design.
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All analysis in this study was performed using 3D finite element modeling in PLAXIS 3D software. The NGI-ADP constitutive model was adopted to simulate the nonlinear mechanical behaviour of clay. Considered in the analysis is a short rigid pile with a diameter of 10 m (L/D = 3) and a long flexible pile with a diameter of 2 m (L/D = 15). The analyzed clay soil profiles consist of a normally consolidated clay soil and an overconsolidated clay soil with a constant undrained shear strength profile equal to 30 kPa. For each pile in each type of clay soil, a pure lateral loading scenario is performed first to assess the validity of current design methods. Subsequently, a combined loading scenario is performed to assess the influence of vertical loading on the lateral behaviour of rigid monopile in clay soil.
Results of the pure lateral loading scenario suggest that current design methods heavily underestimate the lateral capacity of rigid monopile foundations in both clay soil profiles analyzed. According to the findings of this study, it can be concluded that current design methods are not fit to provide an accurate assessment regarding the lateral load response of rigid monopile in clay soil. In order to correctly assess the lateral load response of rigid monopile in clay soil, a method consisting of a 3D finite element model akin to the model used in the research or a PISA design model is advised. A potential third design method, the 1D rotational spring model, is also proposed.
Results of the combined loading scenario suggest that the presence of vertical loading causes a decrease in lateral and moment capacity of the rigid pile in both clay soil profiles analyzed. However, the influence is negligible when the vertical load magnitude is smaller than 50% of its bearing capacity. To quantify the influence of vertical load on a monopile foundation, a series of load analysis were performed on a real offshore wind turbine with a 5MW power capacity. It was found that the vertical load on a typical monopile foundation in clay is around 27% of its bearing capacity. According to the findings of this study, it can be concluded that the influence of vertical load on the lateral response of rigid monopiles in clay soil is limited and can be ignored in foundation design.
The thesis compares measurements of pile load tests to the load-settlement behaviour of fully displacing and (partly) soil replacing piles, including the effect of limiting qc to a maximum of 15 MPa for shaft friction. From appropriately instrumented tests, αp and αs factors are determined and compared to the prescribed factors. Additionally, a shear box test is performed in order to investigate debonding between the grout body and steel tube of a screw-injection pile.
Interpretation of the load tests strongly signify that the load-settlement behaviour of screw and screw-injection piles does not resemble that of fully displacing piles, but rather (partly) soil replacing piles. Determined values of αp range from 0.23 to 0.35, while values for αs in sand range from 0.011 to 0.012. Limiting qc along the shaft is shown to produce less realistic capacity and behaviour predictions when compared to measured test data. The shear box experiments indicate that in dense soils with high qc values, debonding between the grout and steel tube of a screw-injection pile under high load can occur. ...
The thesis compares measurements of pile load tests to the load-settlement behaviour of fully displacing and (partly) soil replacing piles, including the effect of limiting qc to a maximum of 15 MPa for shaft friction. From appropriately instrumented tests, αp and αs factors are determined and compared to the prescribed factors. Additionally, a shear box test is performed in order to investigate debonding between the grout body and steel tube of a screw-injection pile.
Interpretation of the load tests strongly signify that the load-settlement behaviour of screw and screw-injection piles does not resemble that of fully displacing piles, but rather (partly) soil replacing piles. Determined values of αp range from 0.23 to 0.35, while values for αs in sand range from 0.011 to 0.012. Limiting qc along the shaft is shown to produce less realistic capacity and behaviour predictions when compared to measured test data. The shear box experiments indicate that in dense soils with high qc values, debonding between the grout and steel tube of a screw-injection pile under high load can occur.
Geotechnical bearing capacity of MV piles
Improving the design based on full scale load tests in the Port of Rotterdam
Dike stabilisation under uplift conditions using stabilisation columns
A study on the technical potential of stabilisation columns for improving inner slope stability under uplift conditions
Development and Evaluation of a Sand Pluviator
An Approach to Standardized Sample Preparation for Physical Modelling in Geotechnics
Optimizing The Installation of steel, Open-Ended Piles Through Impact Hammering For Offshore Applications
A Parametric, Experimental Study In The Geocentrifuge
Additionally, a sensitivity analysis was done to show which parameters influence the calculation results, the design and the suitability of a permanent SFRUCF. The suitability of an SFRUCF is determined by the column loads in the final phase and the presence of a stiff raft. It was concluded that an SLS check should be included in the CUR 77 for water tightness, crack width and deformations if an SFRUCF is to be used permanently. The interaction between the raft can be modelled in Plaxis 2D with the plate element that has the behaviour of SFRC. For cases that do not include a stiff raft simpler models can be used such as the Plaxis model with springs or even a beam model with SFRC input. ...
Additionally, a sensitivity analysis was done to show which parameters influence the calculation results, the design and the suitability of a permanent SFRUCF. The suitability of an SFRUCF is determined by the column loads in the final phase and the presence of a stiff raft. It was concluded that an SLS check should be included in the CUR 77 for water tightness, crack width and deformations if an SFRUCF is to be used permanently. The interaction between the raft can be modelled in Plaxis 2D with the plate element that has the behaviour of SFRC. For cases that do not include a stiff raft simpler models can be used such as the Plaxis model with springs or even a beam model with SFRC input.