C. Jommi
Please Note
31 records found
1
Utilizing the Erosion Function Apparatus (EFA), performed experiments targeted changes in the structure and erosion resistance of Boom Clay under cyclic conditions. The test setup was adjusted, improved, and calibrated. It was observed that these cycles induce alterations in the clay’s erodibility, contrasting with the behavior of untreated samples.
The results demonstrated cyclic wetting and drying increases the susceptibility of the material to erosion, and the rate of erosion, and decreases the threshold of the erosion process. This study enhances our understanding of how environmental stressors influence the long-term behavior of erosion protection materials. It provides engineers and environmental planners with insights for selecting and assessing materials for erosion protection, emphasizing the importance of considering environmental conditions in their design and application. ...
Utilizing the Erosion Function Apparatus (EFA), performed experiments targeted changes in the structure and erosion resistance of Boom Clay under cyclic conditions. The test setup was adjusted, improved, and calibrated. It was observed that these cycles induce alterations in the clay’s erodibility, contrasting with the behavior of untreated samples.
The results demonstrated cyclic wetting and drying increases the susceptibility of the material to erosion, and the rate of erosion, and decreases the threshold of the erosion process. This study enhances our understanding of how environmental stressors influence the long-term behavior of erosion protection materials. It provides engineers and environmental planners with insights for selecting and assessing materials for erosion protection, emphasizing the importance of considering environmental conditions in their design and application.
Six cyclic settlement models for sand are evaluated to analyse the settlement of automatic stacking crane (ASC) rail tracks at the Rotterdam World Gateway (RWG) container terminal. During Phase 1 of the RWG container terminal settlement of the rail tracks occurred at multiple locations after the ASCs became operational. This has repeatedly led to (unplanned) downtime of parts of the RWG container terminal due to rail track maintenance. Settlements are caused by densification of the sand fill, which is a result of the cyclic load applied by ASCs moving continuously over their rail tracks.
The aim of this research is to contribute to prevent unplanned downtime in Phase 2 of the RWG container terminal due to rail track settlements. Also, reliable settlement predictions can be used to determine the intensity and extent of the ground compaction that are needed to meet the settlement requirement of 20 mm for ASC rail tracks.
The cyclic settlement models, which have been validated to predict the cyclic settlement of rail tracks and shallow foundations, are obtained from literature. The available soil data include CPT’s, boreholes and standard laboratory soil testing. In addition, settlements of the ASC rail tracks in Phase 1 had been measured for a period of almost one year. The cyclic settlement models are evaluated at six different locations, where the sand is medium to very dense and settlements up to 32 mm have been measured. The load is modelled as a quasistatic load equivalent to a vertical stress of 60 to 90 kPa applied to the ballast-sand interface. The model parameters of the cyclic settlement models are determined by correlation, (FE) modelling of the first load cycle, extrapolation and estimation.
The zone of influence was found to reach around 6 m below the shallow foundation. Densification of the sand fill is substantial within the entire zone of influence. The maximum densification was found not to coincide with the minimum void ratio, it is a variable that depends on the initial state of the sand and the loading and soil conditions. After order 104 load cycles densification of the sand was found to become negligible. To meet the settlement requirement for ASC rail tracks the sand fill must consist of sand layers with a minimum and average relative density of at least 65% and 85%, respectively.
Cyclic settlement increases with the number of load cycles, amplitude of the load and extent of the zone of influence and decreases with relative density, stiffness of the sand and volumetric threshold strain. However, correlations used to calibrate the model parameters lead to model predictions that are over- or insensitive to parameters that affect the cyclic settlement. The cyclic settlement predictions of the terminal density model are most reliable and match best with the settlement measurements, for loose and medium dense sand the model predictions underestimate the settlement.
Instead of using correlations to obtain the model parameter values and decrease their uncertainty it is recommended to measure the:
· disturbance of the sand fill underneath the ASC rail tracks due to construction;
· maximum densification of the sand underneath ASC rail tracks in Phase 1 at locations where rail track settlement has stopped, i.e. where the sand reached its maximum densification;
· model parameters that characterise the cyclic densification behaviour of sand in cyclic soil tests.
This will improve the reliability of the cyclic settlement predictions of ASC rail tracks constructed on a sand fill. To validate the cyclic settlement models for ASC rail tracks on sand, measurements of the settlement with depth as function of the number of load cycles are needed. ...
Six cyclic settlement models for sand are evaluated to analyse the settlement of automatic stacking crane (ASC) rail tracks at the Rotterdam World Gateway (RWG) container terminal. During Phase 1 of the RWG container terminal settlement of the rail tracks occurred at multiple locations after the ASCs became operational. This has repeatedly led to (unplanned) downtime of parts of the RWG container terminal due to rail track maintenance. Settlements are caused by densification of the sand fill, which is a result of the cyclic load applied by ASCs moving continuously over their rail tracks.
The aim of this research is to contribute to prevent unplanned downtime in Phase 2 of the RWG container terminal due to rail track settlements. Also, reliable settlement predictions can be used to determine the intensity and extent of the ground compaction that are needed to meet the settlement requirement of 20 mm for ASC rail tracks.
The cyclic settlement models, which have been validated to predict the cyclic settlement of rail tracks and shallow foundations, are obtained from literature. The available soil data include CPT’s, boreholes and standard laboratory soil testing. In addition, settlements of the ASC rail tracks in Phase 1 had been measured for a period of almost one year. The cyclic settlement models are evaluated at six different locations, where the sand is medium to very dense and settlements up to 32 mm have been measured. The load is modelled as a quasistatic load equivalent to a vertical stress of 60 to 90 kPa applied to the ballast-sand interface. The model parameters of the cyclic settlement models are determined by correlation, (FE) modelling of the first load cycle, extrapolation and estimation.
The zone of influence was found to reach around 6 m below the shallow foundation. Densification of the sand fill is substantial within the entire zone of influence. The maximum densification was found not to coincide with the minimum void ratio, it is a variable that depends on the initial state of the sand and the loading and soil conditions. After order 104 load cycles densification of the sand was found to become negligible. To meet the settlement requirement for ASC rail tracks the sand fill must consist of sand layers with a minimum and average relative density of at least 65% and 85%, respectively.
Cyclic settlement increases with the number of load cycles, amplitude of the load and extent of the zone of influence and decreases with relative density, stiffness of the sand and volumetric threshold strain. However, correlations used to calibrate the model parameters lead to model predictions that are over- or insensitive to parameters that affect the cyclic settlement. The cyclic settlement predictions of the terminal density model are most reliable and match best with the settlement measurements, for loose and medium dense sand the model predictions underestimate the settlement.
Instead of using correlations to obtain the model parameter values and decrease their uncertainty it is recommended to measure the:
· disturbance of the sand fill underneath the ASC rail tracks due to construction;
· maximum densification of the sand underneath ASC rail tracks in Phase 1 at locations where rail track settlement has stopped, i.e. where the sand reached its maximum densification;
· model parameters that characterise the cyclic densification behaviour of sand in cyclic soil tests.
This will improve the reliability of the cyclic settlement predictions of ASC rail tracks constructed on a sand fill. To validate the cyclic settlement models for ASC rail tracks on sand, measurements of the settlement with depth as function of the number of load cycles are needed.
The goal of this work is to determine if it is possible to better understand what is happening to K0 during creep and under unsaturated conditions and if the prediction of K0 can be improved by accounting for these phenomena, with the focus being on clays. Literature showed that for saturated samples, the value of K0 increases with time during creep. For unsaturated conditions it was found that K0 decreases with an increase of suction.
In order to see if it is possible to improve the prediction of K0, a model needed to be constructed. The starting point of this model was a saturated, elastoplastic model based on the SANICLAY model. The first step in extending this model was to include viscosity which was done by adopting Perzyna’s overstress approach. The model was validated to experimental data on OostVaardersPlassen (OVP) clay obtained from literature and the validation showed that the model was satisfactory in predicting the soil behaviour. Accounting for unsaturated conditions was done by adopting the average soil skeleton approach. Implementation was initially done in the original elastoplastic model. Again, the model was validated to experimental data obtained from the literature, this time unsaturated loading/unloading tests on London clay (LC) were used. The results showed that the model prediction was accurate up to suctions up to 600 kPa. The final step in the model development was to include both Perzyna’s and the average soil skeleton stress approach in the basic model giving an unsaturated elasto viscoplastic model version. Unsaturated creep tests on London clay were used to validate the model but the results showed that an uncoupled stress-suction approach gave inaccurate predictions. The viscous nucleus in Perzyna’s approach was changed to become suction dependent and the results showed that the experimental data could be reproduced reasonably well.
The unsaturated elasto viscoplastic model was then used to analyse K0 during the unsaturated creep tests. The results showed that the model predicted a decrease in K0 with time for low loads and high suctions. For higher loads and low to moderate suctions, the model predicted an initial increase followed by a decrease. For all cases it was found that the value of K0 decreased with suction. The role of anisotropy on the model prediction was analysed by predicting the change in K0 using an isotropic version of the model. This version also predicted a decrease at low loads and high suctions but an initial increase was no longer predicted to decrease. The decrease of K0 with suction was still observed. No experimental data was available to confirm either of the findings, comparing the results with the literature study showed that the decrease of K0 with suction was previously observed. The decrease with time on the other hand was not found in previous work. However, the creep tests in previous works were performed on saturated samples and in general for a shorter time period which could show different results.
It is concluded that by accounting for creep and unsaturated conditions, the qualitative prediction of the soil behaviour can be improved. By accounting for coupled behaviour through an unsaturated viscous nucleus, the currently available unsaturated and time dependent experimental deformation data can be simulated accurately. The prediction of the change in stress state, due to these natural phenomena, is likely to be improved as well since the outcome of the model matches findings from the literature. However, due to the lack of experimental unsaturated time dependent data stating the change in K0, no conclusions can be drawn on the importance of anisotropy and the quantitative model performance. What this work does offer is a good modelling tool to support future experiments or investigations into unsaturated creep behaviour. ...
The goal of this work is to determine if it is possible to better understand what is happening to K0 during creep and under unsaturated conditions and if the prediction of K0 can be improved by accounting for these phenomena, with the focus being on clays. Literature showed that for saturated samples, the value of K0 increases with time during creep. For unsaturated conditions it was found that K0 decreases with an increase of suction.
In order to see if it is possible to improve the prediction of K0, a model needed to be constructed. The starting point of this model was a saturated, elastoplastic model based on the SANICLAY model. The first step in extending this model was to include viscosity which was done by adopting Perzyna’s overstress approach. The model was validated to experimental data on OostVaardersPlassen (OVP) clay obtained from literature and the validation showed that the model was satisfactory in predicting the soil behaviour. Accounting for unsaturated conditions was done by adopting the average soil skeleton approach. Implementation was initially done in the original elastoplastic model. Again, the model was validated to experimental data obtained from the literature, this time unsaturated loading/unloading tests on London clay (LC) were used. The results showed that the model prediction was accurate up to suctions up to 600 kPa. The final step in the model development was to include both Perzyna’s and the average soil skeleton stress approach in the basic model giving an unsaturated elasto viscoplastic model version. Unsaturated creep tests on London clay were used to validate the model but the results showed that an uncoupled stress-suction approach gave inaccurate predictions. The viscous nucleus in Perzyna’s approach was changed to become suction dependent and the results showed that the experimental data could be reproduced reasonably well.
The unsaturated elasto viscoplastic model was then used to analyse K0 during the unsaturated creep tests. The results showed that the model predicted a decrease in K0 with time for low loads and high suctions. For higher loads and low to moderate suctions, the model predicted an initial increase followed by a decrease. For all cases it was found that the value of K0 decreased with suction. The role of anisotropy on the model prediction was analysed by predicting the change in K0 using an isotropic version of the model. This version also predicted a decrease at low loads and high suctions but an initial increase was no longer predicted to decrease. The decrease of K0 with suction was still observed. No experimental data was available to confirm either of the findings, comparing the results with the literature study showed that the decrease of K0 with suction was previously observed. The decrease with time on the other hand was not found in previous work. However, the creep tests in previous works were performed on saturated samples and in general for a shorter time period which could show different results.
It is concluded that by accounting for creep and unsaturated conditions, the qualitative prediction of the soil behaviour can be improved. By accounting for coupled behaviour through an unsaturated viscous nucleus, the currently available unsaturated and time dependent experimental deformation data can be simulated accurately. The prediction of the change in stress state, due to these natural phenomena, is likely to be improved as well since the outcome of the model matches findings from the literature. However, due to the lack of experimental unsaturated time dependent data stating the change in K0, no conclusions can be drawn on the importance of anisotropy and the quantitative model performance. What this work does offer is a good modelling tool to support future experiments or investigations into unsaturated creep behaviour.
The unexpected softening of the undrained shear strength of organic and silty clays in Rhine delta: a conceptual study
Determining the Undrained Shear Strength of soft Dutch soils using conventional laboratory equipment
This thesis aims to study the feasibility of using time series Interferometric Synthetic Aperture Radar (InSAR) as a means to monitor differential settlement in greenhouse structures. The analysis was primarily done using RADARSAT-2 data. In case of translucent surfaces of greenhouses, it was important to firstly identify the physical targets that are associated to scattering centres. This was done by analysing the statistics of the heights of the scatterers which helps in ascertaining where the radar signal is getting back-scattered from. It was inferred that the persistent and distributed scatterers are primarily identified from objects on the roof and outer walls of the greenhouses.
Moreover, the magnitude of deformation estimated from the scatterers have been corroborated with geotechnical data. It was seen that higher magnitudes of deformation was seen in locations with compressible soil types such as clay and peat close to the ground surface. It was also seen that greenhouse structures are prone to differential settlement when the depths of the piles are insufficient in areas with varying soil types. The effect of thermal contributions has also been studied and it was found that the estimation of thermal expansion does not significantly affect the estimated deformations.
From the study, it is evident that time series InSAR offers an effective means to monitor differential settlements in greenhouses. In order to check for differential settlement in individual greenhouses, it is proposed that a persistent scatter interferometric analysis be done initially and if it is seen that the density of these scatterers is insufficient, the analysis can be followed up with time series interferometry of distributed scatterers. Incorporating multiple track directions of radar data increases the number of greenhouses that can be monitored. Moreover, it was also seen that persistent scatterers were identified from additional greenhouses when Sentinel-1 data was used, despite its poorer spatial resolution. For further study, it is recommended that corner reflectors are used to validate the positions of the targets that are identified as persistent and distributed scatterers.
...
This thesis aims to study the feasibility of using time series Interferometric Synthetic Aperture Radar (InSAR) as a means to monitor differential settlement in greenhouse structures. The analysis was primarily done using RADARSAT-2 data. In case of translucent surfaces of greenhouses, it was important to firstly identify the physical targets that are associated to scattering centres. This was done by analysing the statistics of the heights of the scatterers which helps in ascertaining where the radar signal is getting back-scattered from. It was inferred that the persistent and distributed scatterers are primarily identified from objects on the roof and outer walls of the greenhouses.
Moreover, the magnitude of deformation estimated from the scatterers have been corroborated with geotechnical data. It was seen that higher magnitudes of deformation was seen in locations with compressible soil types such as clay and peat close to the ground surface. It was also seen that greenhouse structures are prone to differential settlement when the depths of the piles are insufficient in areas with varying soil types. The effect of thermal contributions has also been studied and it was found that the estimation of thermal expansion does not significantly affect the estimated deformations.
From the study, it is evident that time series InSAR offers an effective means to monitor differential settlements in greenhouses. In order to check for differential settlement in individual greenhouses, it is proposed that a persistent scatter interferometric analysis be done initially and if it is seen that the density of these scatterers is insufficient, the analysis can be followed up with time series interferometry of distributed scatterers. Incorporating multiple track directions of radar data increases the number of greenhouses that can be monitored. Moreover, it was also seen that persistent scatterers were identified from additional greenhouses when Sentinel-1 data was used, despite its poorer spatial resolution. For further study, it is recommended that corner reflectors are used to validate the positions of the targets that are identified as persistent and distributed scatterers.
Preloading of a lumpy clay fill
A study into the closure of the interlump voids of a mechanically dredged stiff clay fill
in water result in a matrix of clay lumps and an interlump void space. The collapse of the interlump void space will cause large settlements and needs to be overcome before the site can be used for construction. Preloading is
an effective method to close the interlump voids. Stiff clays soften over time due to unloading and swelling. As a result, the strength and stiffness of the clay lumps decrease over time. The presence of discontinuities accelerates
the softening process. It was proposed by Leung et al. (2001) that the interlump void space closes under a reduced
preload of 25 kPa. The interlump void space closes under a reduced preload because the lumps soften over time.
The question rises if closure occurs within a normal construction timespan, i.e., 1 - 2 years, under this reduced
preload. In this study, a combined experimental and numerical approach is applied to determine the influence of soil
characteristics, softening and the presence of discontinuities on interlump void closure. The influence of softening due to chemical and hydro-mechanical swelling is tested by experimental swell-load tests on stiff overconsolidated
Boom clay samples. Additionally, the presence of discontinuities is studied by CT images, and a miniature clay fill test is performed to study the softening time and the rearrangement effect. Furthermore, a numerical study is performed in which the influence of specific soil characteristics on void closure was researched by a sensitivity analysis. By the experimental tests, it is shown that a pore water chemistry change alters the degree of swelling and its compressibility. Furthermore, fissures were identified in the sample material by CT images. The smallest microfissures could not be identified due to the resolution of the images. Consequently, it is impossible to estimate the effect of fissures on the hydraulic conductivity. Therefore, literature data was used to estimate the hydraulic conductivity and this was used as the input in the calculations. In the numerical study, it was shown that MPM could model the softening behaviour over time. The sensitivity analysis showed that the MPM model responds consistently to parameter sensitivity analyses. This leads to the conclusion that MPM can be used as a investigation tool to increase
the understanding of the influence of parameter variability on the final interlump void closure problem. The resulting strains of the numerical model comply with the theoretically calculated strains. It was expected
that the numerical strains were smaller than the experimentally determined strains, due to the presence of interlump voids in the numerical model. But, the numerical strains are larger than the experimental strains. In the sensitivity
analysis, it was found that the final strains and closure time are highly dependant on the soil characteristics. It is likely that the input of the MPM model differs compared to the true sample material and thus different strains result.
The time until the interlump void space closes was determined by a simplified geometry in MPM under a preload of 25 kPa. For an unfissured Boom clay, interlump closure takes place after approximately 16 years while for a
fissured Boom clay it only takes 2 months. Thus, closure of the highly simplified geometry takes place within a normal construction timespan for a fissured Boom clay. It must be kept in mind that the results are highly dependant
on the geometry, lump size and soil characteristics. Therefore, these results can not be generalized into an estimate of the interlump void closure time for any stiff lumpy clay fill. In conclusion, the feasibility of MPM was explored and it turned out to be a promising method to model the interlump void closure problem. Further studies are required to check if the model gives plausible results for more advanced constitutive soil models and geometries. If the results are positive, MPM can be used as a investigation tool to increase the understanding of the interlump void closure time for more refined geometries. ...
in water result in a matrix of clay lumps and an interlump void space. The collapse of the interlump void space will cause large settlements and needs to be overcome before the site can be used for construction. Preloading is
an effective method to close the interlump voids. Stiff clays soften over time due to unloading and swelling. As a result, the strength and stiffness of the clay lumps decrease over time. The presence of discontinuities accelerates
the softening process. It was proposed by Leung et al. (2001) that the interlump void space closes under a reduced
preload of 25 kPa. The interlump void space closes under a reduced preload because the lumps soften over time.
The question rises if closure occurs within a normal construction timespan, i.e., 1 - 2 years, under this reduced
preload. In this study, a combined experimental and numerical approach is applied to determine the influence of soil
characteristics, softening and the presence of discontinuities on interlump void closure. The influence of softening due to chemical and hydro-mechanical swelling is tested by experimental swell-load tests on stiff overconsolidated
Boom clay samples. Additionally, the presence of discontinuities is studied by CT images, and a miniature clay fill test is performed to study the softening time and the rearrangement effect. Furthermore, a numerical study is performed in which the influence of specific soil characteristics on void closure was researched by a sensitivity analysis. By the experimental tests, it is shown that a pore water chemistry change alters the degree of swelling and its compressibility. Furthermore, fissures were identified in the sample material by CT images. The smallest microfissures could not be identified due to the resolution of the images. Consequently, it is impossible to estimate the effect of fissures on the hydraulic conductivity. Therefore, literature data was used to estimate the hydraulic conductivity and this was used as the input in the calculations. In the numerical study, it was shown that MPM could model the softening behaviour over time. The sensitivity analysis showed that the MPM model responds consistently to parameter sensitivity analyses. This leads to the conclusion that MPM can be used as a investigation tool to increase
the understanding of the influence of parameter variability on the final interlump void closure problem. The resulting strains of the numerical model comply with the theoretically calculated strains. It was expected
that the numerical strains were smaller than the experimentally determined strains, due to the presence of interlump voids in the numerical model. But, the numerical strains are larger than the experimental strains. In the sensitivity
analysis, it was found that the final strains and closure time are highly dependant on the soil characteristics. It is likely that the input of the MPM model differs compared to the true sample material and thus different strains result.
The time until the interlump void space closes was determined by a simplified geometry in MPM under a preload of 25 kPa. For an unfissured Boom clay, interlump closure takes place after approximately 16 years while for a
fissured Boom clay it only takes 2 months. Thus, closure of the highly simplified geometry takes place within a normal construction timespan for a fissured Boom clay. It must be kept in mind that the results are highly dependant
on the geometry, lump size and soil characteristics. Therefore, these results can not be generalized into an estimate of the interlump void closure time for any stiff lumpy clay fill. In conclusion, the feasibility of MPM was explored and it turned out to be a promising method to model the interlump void closure problem. Further studies are required to check if the model gives plausible results for more advanced constitutive soil models and geometries. If the results are positive, MPM can be used as a investigation tool to increase the understanding of the interlump void closure time for more refined geometries.
Development of the Yield Stress due to Aging
Verification of the abc-model based on K0-CRS tests
Mass stabilisation near regional flood defences
A technical feasibility study into the application of mass stabilisation for improving the inward macro-stability of regional flood defences
Neutron CT was performed on cylindrical peat samples. This technique uses a thermal neutron beam to image a sample and was available at the Reactor Institute Delft. The resolution of this imaging station is 150 $\mu$m. Since the cell walls and the peat material between the fibres in peat have both a large attenuation coefficient for neutrons, it was not possible to distinguish the fibres from the peat material between the fibres, using this technique. To gain a contrast heavy water was used to replace the water because it has a low attenuation coefficient. Flushing a peat sample with heavy water showed the most effective way to do so. The aim of this procedure was to get a contrast difference between the peat material between the fibres and the fibres itself. A triaxial setup was used to flush the sample with heavy water. Heavy water diffused in the water present in the peat inducing a decrease in attenuation of the peat material between the fibres. The reconstructed tomographic images were filtered using a 3D visualization program Avizo version 9.4. Only the air-filled fibres could be observed on the tomographic images whereas the water-filled fibres could not be observed. Samples of the same peat were scanned in a dry and wet state using a X-ray micro CT scanner present at the geoscience section of TU Delft. On the tomographic images of the wet sample, white halo were observed representing the cell walls of the fibres.
X-ray phase CT present at the Ghent University Centre for X-ray CT was performed on a peat sample coming from the same site. This method results in an image contrast using a large fixed distance for low absorbing materials like peat. The aim of this scan was to reveal more fibres than observed with the X-ray micro CT scan at TU Delft. However, edge enhancement did not occur because of the filtering needed during reconstruction of the raw data to visualize different structures in peat. \\ The white halo could be thresholded and filtered in avizo resulting in a 3D image of the rod-like fibres. These fibres were randomly orientated. On the micro CT scan of the sample in a dry state other fibrous structures than the rod-like fibres were observed. These fibres were not shown as white halo on the tomographic images of the wet samples. ...
Neutron CT was performed on cylindrical peat samples. This technique uses a thermal neutron beam to image a sample and was available at the Reactor Institute Delft. The resolution of this imaging station is 150 $\mu$m. Since the cell walls and the peat material between the fibres in peat have both a large attenuation coefficient for neutrons, it was not possible to distinguish the fibres from the peat material between the fibres, using this technique. To gain a contrast heavy water was used to replace the water because it has a low attenuation coefficient. Flushing a peat sample with heavy water showed the most effective way to do so. The aim of this procedure was to get a contrast difference between the peat material between the fibres and the fibres itself. A triaxial setup was used to flush the sample with heavy water. Heavy water diffused in the water present in the peat inducing a decrease in attenuation of the peat material between the fibres. The reconstructed tomographic images were filtered using a 3D visualization program Avizo version 9.4. Only the air-filled fibres could be observed on the tomographic images whereas the water-filled fibres could not be observed. Samples of the same peat were scanned in a dry and wet state using a X-ray micro CT scanner present at the geoscience section of TU Delft. On the tomographic images of the wet sample, white halo were observed representing the cell walls of the fibres.
X-ray phase CT present at the Ghent University Centre for X-ray CT was performed on a peat sample coming from the same site. This method results in an image contrast using a large fixed distance for low absorbing materials like peat. The aim of this scan was to reveal more fibres than observed with the X-ray micro CT scan at TU Delft. However, edge enhancement did not occur because of the filtering needed during reconstruction of the raw data to visualize different structures in peat. \\ The white halo could be thresholded and filtered in avizo resulting in a 3D image of the rod-like fibres. These fibres were randomly orientated. On the micro CT scan of the sample in a dry state other fibrous structures than the rod-like fibres were observed. These fibres were not shown as white halo on the tomographic images of the wet samples.
Implementation of the New Dutch Guidelines on the Macrostability Assessment of Dikes using Different Constitutive Models
Case study: KIJK Dike in the Netherlands
The FoS is determined with the use of the strength reduction method. Moreover, the CSSM framework is coupled with the SHANSEP (Stress History and Normalized Soil Engineering Properties) concept enabling the incorporation of the effect of stress history and the stress path characterizing the undrained shear strength in the design. The CSSM framework is applied in the design by determining the strength parameters of clays from an axial strain level equal to 25% under triaxial compression whereas for peats at 40% shear strain level under direct simple shearing conditions. In this study the strength parameters were additionally determined from the service conditions strain levels which are the 2% and 5% strain levels for clays and peats, respectively. The necessary strength parameters for the constitutive models are determined in the considered strain levels exposing their influence for both clays and peats. Moreover, the study includes the examination of the constitutive models at a single element level conducted in the Soil Test facility available in PLAXIS. When it comes to the design analysis, it was found that the SHANSEP NGI-ADP model fits properly the su determined from a cone penetration test. The HS and SS models based on the effective strength parameters may result in an undrained shear strength profile which deviates from the su that the soils exhibits in the field.
The study points out that both the strain level dependency of the strength parameters and the selection of the constitutive model at critical loading influence the results in terms of the developed failure plane and the FoS, especially in the case of Green dikes. The study also elaborates the response of the models in regard to the design requirements for the calculation of displacements and the structural forces. Finally, this study answers the knowledge gap regarding how the strain level influences the strength of the examined soils and how this should be translated in the design along with the explanation on the effects of the selected constitutive model on the results.
...
The FoS is determined with the use of the strength reduction method. Moreover, the CSSM framework is coupled with the SHANSEP (Stress History and Normalized Soil Engineering Properties) concept enabling the incorporation of the effect of stress history and the stress path characterizing the undrained shear strength in the design. The CSSM framework is applied in the design by determining the strength parameters of clays from an axial strain level equal to 25% under triaxial compression whereas for peats at 40% shear strain level under direct simple shearing conditions. In this study the strength parameters were additionally determined from the service conditions strain levels which are the 2% and 5% strain levels for clays and peats, respectively. The necessary strength parameters for the constitutive models are determined in the considered strain levels exposing their influence for both clays and peats. Moreover, the study includes the examination of the constitutive models at a single element level conducted in the Soil Test facility available in PLAXIS. When it comes to the design analysis, it was found that the SHANSEP NGI-ADP model fits properly the su determined from a cone penetration test. The HS and SS models based on the effective strength parameters may result in an undrained shear strength profile which deviates from the su that the soils exhibits in the field.
The study points out that both the strain level dependency of the strength parameters and the selection of the constitutive model at critical loading influence the results in terms of the developed failure plane and the FoS, especially in the case of Green dikes. The study also elaborates the response of the models in regard to the design requirements for the calculation of displacements and the structural forces. Finally, this study answers the knowledge gap regarding how the strain level influences the strength of the examined soils and how this should be translated in the design along with the explanation on the effects of the selected constitutive model on the results.
A driver was developed in MATLAB for the chosen constitutive model to simulate undrained triaxial loading conditions. The performance of the driver was verified against the data published from literature. Further, sensitivity analysis was carried out on chosen model parameters. This was followed by validating the model with the experimental data on kaolin clay. Particularly, model performance was examined with varying initial conditions such as change of over-consolidation ratio, change of initial anisotropy, variation of initial pressure and strain controlled loading. The obtained results from sensitivity analysis have shown to increase the strength and stiffness response of the model with increase in model parameters such as the rate of evolution of the anisotropy, bound for evolution of the anisotropy and change of initial stress-induced anisotropy. In the context of calibrating the model parameters against the experimental data, it was initially noticed that the experimental stress path in monotonic loading was not being reproduced by the model with various combinations of the initial parameters. Owing to such performance the model was subsequently assessed qualitatively. When the model is subjected to different initial loading conditions, certain aspects of the experimental behaviour were qualitatively captured by the model. These include faster rate of accumulation of pore water pressure with increase in the amplitude of cyclic loading, reduction in the rate of development of strains with increase in OCR values, increase in the hysteretic damping with increase in the amplitude of strains. However, with change of OCR there were differences in the development of stress path. Also contrasting results were observed with regard to the development of the stress-strain response with change of amplitude of cyclic loading and initial pressure. Analyzing the model formulations revealed that the chosen model did not take into consideration the fabric anisotropy and hence it explains the deviation of the stress path from the experimental stress path in monotonic conditions. In the chosen model, during the process of cyclic loading, stagnation in the evolution of stress path is observed whenever the plastic volumetric strains stop evolving. It is recommended to incorporate plastic deviatoric strains in the evolution of the bounding surface in order to stimulate the further development of stress path even when the plastic volumetric strains stop evolving. It is also suggested to validate the model against different clays since this thesis focused only on Kaolin clay. ...
A driver was developed in MATLAB for the chosen constitutive model to simulate undrained triaxial loading conditions. The performance of the driver was verified against the data published from literature. Further, sensitivity analysis was carried out on chosen model parameters. This was followed by validating the model with the experimental data on kaolin clay. Particularly, model performance was examined with varying initial conditions such as change of over-consolidation ratio, change of initial anisotropy, variation of initial pressure and strain controlled loading. The obtained results from sensitivity analysis have shown to increase the strength and stiffness response of the model with increase in model parameters such as the rate of evolution of the anisotropy, bound for evolution of the anisotropy and change of initial stress-induced anisotropy. In the context of calibrating the model parameters against the experimental data, it was initially noticed that the experimental stress path in monotonic loading was not being reproduced by the model with various combinations of the initial parameters. Owing to such performance the model was subsequently assessed qualitatively. When the model is subjected to different initial loading conditions, certain aspects of the experimental behaviour were qualitatively captured by the model. These include faster rate of accumulation of pore water pressure with increase in the amplitude of cyclic loading, reduction in the rate of development of strains with increase in OCR values, increase in the hysteretic damping with increase in the amplitude of strains. However, with change of OCR there were differences in the development of stress path. Also contrasting results were observed with regard to the development of the stress-strain response with change of amplitude of cyclic loading and initial pressure. Analyzing the model formulations revealed that the chosen model did not take into consideration the fabric anisotropy and hence it explains the deviation of the stress path from the experimental stress path in monotonic conditions. In the chosen model, during the process of cyclic loading, stagnation in the evolution of stress path is observed whenever the plastic volumetric strains stop evolving. It is recommended to incorporate plastic deviatoric strains in the evolution of the bounding surface in order to stimulate the further development of stress path even when the plastic volumetric strains stop evolving. It is also suggested to validate the model against different clays since this thesis focused only on Kaolin clay.