D.J.M. Ngan-Tillard
Please Note
22 records found
1
Continuum-based simulations explored various cavern sizes. Within basaltic flow core units, the stress regime was mostly moderate, with maximum principal stress less than half the uniaxial compressive strength. Tensile stresses reached 80–85% of the rock’s tensile strength, and displacements remained under 4.5 mm, suggesting cavern excavation feasibility. The ratio of horizontal to vertical in-situ stress had a greater influence on stability than rock mass parameters such as Young’s modulus, Poisson’s ratio, or compressive strength. Caverns in both planned positions along the alignment showed similar stress and displacement responses and comparable geomechanical behaviour across the two sites. Simulations involving lava breccia and volcaniclastic sandstone indicated higher instability risks: breccia exhibited potential for spalling and damage accumulation, while sandstone approached the onset of failure. Based on modelling results, two optimal cavern configurations were proposed: (i) a 20-m outer radius with a 4-m central pillar, and (ii) an 18-m radius full-span excavation without support.
This study advances understanding of large-scale underground widenings designed for road roundabouts. It also highlights the need for more site-specific data on stress fields and rock mass strength for the current project, as the models primarily relied on desk-based estimates. Complementary approaches, such as combining continuum modelling with discrete element methods and incorporating structural reinforcement, would provide further insight into brittle failure mechanisms and help evaluate the full feasibility and improvement of such cavern excavations.
...
Continuum-based simulations explored various cavern sizes. Within basaltic flow core units, the stress regime was mostly moderate, with maximum principal stress less than half the uniaxial compressive strength. Tensile stresses reached 80–85% of the rock’s tensile strength, and displacements remained under 4.5 mm, suggesting cavern excavation feasibility. The ratio of horizontal to vertical in-situ stress had a greater influence on stability than rock mass parameters such as Young’s modulus, Poisson’s ratio, or compressive strength. Caverns in both planned positions along the alignment showed similar stress and displacement responses and comparable geomechanical behaviour across the two sites. Simulations involving lava breccia and volcaniclastic sandstone indicated higher instability risks: breccia exhibited potential for spalling and damage accumulation, while sandstone approached the onset of failure. Based on modelling results, two optimal cavern configurations were proposed: (i) a 20-m outer radius with a 4-m central pillar, and (ii) an 18-m radius full-span excavation without support.
This study advances understanding of large-scale underground widenings designed for road roundabouts. It also highlights the need for more site-specific data on stress fields and rock mass strength for the current project, as the models primarily relied on desk-based estimates. Complementary approaches, such as combining continuum modelling with discrete element methods and incorporating structural reinforcement, would provide further insight into brittle failure mechanisms and help evaluate the full feasibility and improvement of such cavern excavations.
Turning sediments into soil
Effects of soil ripening and stockpile management on tensile strength and cracking of dredged material: an experimental study
Image Analysis of Granular Materials
Understanding the Effects of High Temperatures and Pressures
Analysis of friction development at microtunneling case study
Microtunneling under the river IJ, Amsterdam
All this data was analysed with the focus on the friction development over the entire boring length. The first part of data analysis was to plot and describe the findings of the available parameters, along the total route, that could have an influence on the friction. Next, the microtunnel route was divided into six sections based on changes in soil conditions and in alignment so the analysed parameters (horizontal and vertical deviations, tilt, main jacking force , front force and friction) could be correlated. In order to better understand the results, a Pearson’s correlation analysis was created to identify any statistically relevant correlation between the available parameters. The final analysis was performed to estimate the impact that subsequent pipe segment installations have on the friction over time at a specific location.
The friction development over the entire length at the boring under the river IJ (less than 2kPa, with the exception of the start) was compared with the friction coefficient value described in the NEN 3650 when overcut and lubrication are used for concrete pipes (f =7.5 kPa). The friction coefficient is overestimated during design phase and can be optimized. Also for all six sections, after a standstill, an increase in friction is observed. At locations where correlation between alignment and forces are apparently present, the horizontal deviation is observed as the influencing parameter. This is also confirmed by the Pearson’s correlation analysis results. Regarding the impact that subsequent pipe segment installations have on the friction, the results of this analysis clearly shows a tendency for a decrease in friction when considering soil type and changes in alignment.
Overall, this work indicates the need of a more thorough friction prediction calculation to be included in the design standards. One that includes more influencing parameters other than overcut and lubricant. Such understanding would enable more accurate predictions in future projects, reducing both risks and costs.
...
All this data was analysed with the focus on the friction development over the entire boring length. The first part of data analysis was to plot and describe the findings of the available parameters, along the total route, that could have an influence on the friction. Next, the microtunnel route was divided into six sections based on changes in soil conditions and in alignment so the analysed parameters (horizontal and vertical deviations, tilt, main jacking force , front force and friction) could be correlated. In order to better understand the results, a Pearson’s correlation analysis was created to identify any statistically relevant correlation between the available parameters. The final analysis was performed to estimate the impact that subsequent pipe segment installations have on the friction over time at a specific location.
The friction development over the entire length at the boring under the river IJ (less than 2kPa, with the exception of the start) was compared with the friction coefficient value described in the NEN 3650 when overcut and lubrication are used for concrete pipes (f =7.5 kPa). The friction coefficient is overestimated during design phase and can be optimized. Also for all six sections, after a standstill, an increase in friction is observed. At locations where correlation between alignment and forces are apparently present, the horizontal deviation is observed as the influencing parameter. This is also confirmed by the Pearson’s correlation analysis results. Regarding the impact that subsequent pipe segment installations have on the friction, the results of this analysis clearly shows a tendency for a decrease in friction when considering soil type and changes in alignment.
Overall, this work indicates the need of a more thorough friction prediction calculation to be included in the design standards. One that includes more influencing parameters other than overcut and lubricant. Such understanding would enable more accurate predictions in future projects, reducing both risks and costs.
This thesis develops a generic analytical framework that connects soil stress–strain behavior to track-scale mobility. The model couples a bearing-capacity-based sinkage formulation with a saturated soft-plastic shear–displacement relation. It allows the use of peak and residual shear strengths, as well as the characteristic displacement to peak strength (Kω), directly as input parameters. The framework handles traction and resistance under quasi-static, undrained conditions and applies to both straight-line and turning motion.
The results show that soil sensitivity (the ratio between peak and residual strength) and Kω control the shape of the traction-slip curve. Larger Kω shifts the peak to higher slip and delays remolding, while higher sensitivity steepens the post-peak drop and lowers available traction once the soil is remolded. Increasing the effective contact length improves traction up to a plateau, after which the additional gain becomes small. In heterogeneous (layered) soils, where strength increases with depth, traction increases with grounding pressure but at a decreasing rate. In homogeneous (uniform) soils, traction decreases with added normal load because increased grounding pressure limits shear mobilization before failure.
During turning, most of the track footprint exceeds the characteristic displacement Kω and the response becomes governed by residual strength. Turning is therefore traction-limited and controlled mainly by soil sensitivity, residual strength and geometry. A clear transition in the minimum turning radius is observed when the required thrust exceeds the residual traction level; beyond this point, small-radius turns become infeasible.
The results indicate that mobility can only be predicted reliably when post-peak soil behavior is included. Turning design should be based on remolded soil conditions, while straight-line operation should remain in the pre-peak region to prevent stalling. Design efforts should focus on optimizing contact length, adjusting grouser height to local seabed conditions, and measuring residual strength and sensitivity for the specific site.
...
This thesis develops a generic analytical framework that connects soil stress–strain behavior to track-scale mobility. The model couples a bearing-capacity-based sinkage formulation with a saturated soft-plastic shear–displacement relation. It allows the use of peak and residual shear strengths, as well as the characteristic displacement to peak strength (Kω), directly as input parameters. The framework handles traction and resistance under quasi-static, undrained conditions and applies to both straight-line and turning motion.
The results show that soil sensitivity (the ratio between peak and residual strength) and Kω control the shape of the traction-slip curve. Larger Kω shifts the peak to higher slip and delays remolding, while higher sensitivity steepens the post-peak drop and lowers available traction once the soil is remolded. Increasing the effective contact length improves traction up to a plateau, after which the additional gain becomes small. In heterogeneous (layered) soils, where strength increases with depth, traction increases with grounding pressure but at a decreasing rate. In homogeneous (uniform) soils, traction decreases with added normal load because increased grounding pressure limits shear mobilization before failure.
During turning, most of the track footprint exceeds the characteristic displacement Kω and the response becomes governed by residual strength. Turning is therefore traction-limited and controlled mainly by soil sensitivity, residual strength and geometry. A clear transition in the minimum turning radius is observed when the required thrust exceeds the residual traction level; beyond this point, small-radius turns become infeasible.
The results indicate that mobility can only be predicted reliably when post-peak soil behavior is included. Turning design should be based on remolded soil conditions, while straight-line operation should remain in the pre-peak region to prevent stalling. Design efforts should focus on optimizing contact length, adjusting grouser height to local seabed conditions, and measuring residual strength and sensitivity for the specific site.
This research aims to get a better understanding of the cavern convergence and permeation processes after abandonment. For this, a cavern convergence- and brine permeation model is made. Next to this the potential surface subsidence due to the migration of brine to more permeable layers is investigated. In the convergence model, the cavern is modelled as a stack of cylinders and a Norton-Hoff power law squeeze model is applied to the cavern. The squeeze model consists of 2 parts, a linear and a nonlinear part. The nonlinear part is most significant during the production phase and in these high-pressure deficits the squeeze model is fitted on the available production data. Recent creep tests on salt samples under lower pressure deficits (Bérest et al., 2019) have confirmed that the linear part becomes the most significant in the low-pressure deficit region and have shown that the linear creep is smaller than the linear component of existing squeeze model used for production.
Next to this a sensitivity analysis was done on the convergence model by varying the input variables of the model. The parameters that have a large uncertainty and have a large impact on the model were the linear part of the squeeze model and the width of a slice. To give a range of outputs of the convergence model a P10, P50 and P90 scenario is created where these are percentiles from the input range of the sensitivity analysis. The outcome of the convergence model at a cavern size of 1Mm3 suggests a yearly cavern convergence of around of 5, 103 and 2313 m3/year for the P10, P50 and P90 cases respectively.
Since there is an equilibrium between the cavern convergence and the brine permeation, the output of the convergence model (convergence rate) can be used as an input for the permeation model (permeation rate). For the permeation model, different paraboloid shapes are fitted on each layer and are filled with brine from the converging cavern. Once all the salt layers are filled in, the brine reaches more permeable layers and can freely flow over a larger area. The permeation model is run with the P10, P50 and P90 convergence model scenarios as an input and predicts that the system fills after 26, 588 and 12,363 years respectively. At this point there could be some subsidence because the brine can freely flow over a larger area in the more permeable layers above the Zechstein. This subsidence is 0.016 mm/year for the P50 case after 588 years. A negligible amount compared to unrelated subsidence processes.
13
To conclude the cavern convergence rates (even the P10 at 5m3/year) are high compared to the permeability of salt according to the Darcy flow law (around 17 l/year). This could have multiple explanations. From the cavern perspective, the cavern convergence rates could be lower. This could be because of a threshold pressure for salt creep to occur (van Oosterhout et al., 2022) or because of some inaccuracies in the linear component of the squeeze model. Future research could focus on determining the creep rates of salt under low-pressure deficits. From the permeation perspective, other permeation paths next to permeability could be at play as well. In the cavern there could be permeation via anhydrite alterations or via micro fractures created during the production phase of the cavern. It would be good to look at these permeation processes in the future. Next to this the secondary porosity of the salt remains a question as well. A good understanding of this porosity is needed to assess the storage capacity of the overlying salt layers before the brine enters more permeable zones. ...
This research aims to get a better understanding of the cavern convergence and permeation processes after abandonment. For this, a cavern convergence- and brine permeation model is made. Next to this the potential surface subsidence due to the migration of brine to more permeable layers is investigated. In the convergence model, the cavern is modelled as a stack of cylinders and a Norton-Hoff power law squeeze model is applied to the cavern. The squeeze model consists of 2 parts, a linear and a nonlinear part. The nonlinear part is most significant during the production phase and in these high-pressure deficits the squeeze model is fitted on the available production data. Recent creep tests on salt samples under lower pressure deficits (Bérest et al., 2019) have confirmed that the linear part becomes the most significant in the low-pressure deficit region and have shown that the linear creep is smaller than the linear component of existing squeeze model used for production.
Next to this a sensitivity analysis was done on the convergence model by varying the input variables of the model. The parameters that have a large uncertainty and have a large impact on the model were the linear part of the squeeze model and the width of a slice. To give a range of outputs of the convergence model a P10, P50 and P90 scenario is created where these are percentiles from the input range of the sensitivity analysis. The outcome of the convergence model at a cavern size of 1Mm3 suggests a yearly cavern convergence of around of 5, 103 and 2313 m3/year for the P10, P50 and P90 cases respectively.
Since there is an equilibrium between the cavern convergence and the brine permeation, the output of the convergence model (convergence rate) can be used as an input for the permeation model (permeation rate). For the permeation model, different paraboloid shapes are fitted on each layer and are filled with brine from the converging cavern. Once all the salt layers are filled in, the brine reaches more permeable layers and can freely flow over a larger area. The permeation model is run with the P10, P50 and P90 convergence model scenarios as an input and predicts that the system fills after 26, 588 and 12,363 years respectively. At this point there could be some subsidence because the brine can freely flow over a larger area in the more permeable layers above the Zechstein. This subsidence is 0.016 mm/year for the P50 case after 588 years. A negligible amount compared to unrelated subsidence processes.
13
To conclude the cavern convergence rates (even the P10 at 5m3/year) are high compared to the permeability of salt according to the Darcy flow law (around 17 l/year). This could have multiple explanations. From the cavern perspective, the cavern convergence rates could be lower. This could be because of a threshold pressure for salt creep to occur (van Oosterhout et al., 2022) or because of some inaccuracies in the linear component of the squeeze model. Future research could focus on determining the creep rates of salt under low-pressure deficits. From the permeation perspective, other permeation paths next to permeability could be at play as well. In the cavern there could be permeation via anhydrite alterations or via micro fractures created during the production phase of the cavern. It would be good to look at these permeation processes in the future. Next to this the secondary porosity of the salt remains a question as well. A good understanding of this porosity is needed to assess the storage capacity of the overlying salt layers before the brine enters more permeable zones.
First, I have examined the probability of all small Dutch gas fields being responsible for a seismic event. Based on the distance between the gas field and the nearest event, as well as the presence of other fields in the surrounding area, I have derived a classification for the likelihood that the field was associated with induced seismicity. Second, I have run a sensitivity analysis to identify which parameter was most significant. I have accomplished this by implementing a semi-analytical model that computed and depicted depletion-induced stresses and fault slip along an inclined fault. The model calculated the depletion pressure at which seismic slip starts to occur, here called the onset pressure, based on reservoir data and fault characteristics. The reservoir data contains the compaction coefficient, critical slip weakening distance, dip angle, dynamic friction coefficient, initial reservoir pressure, Poisson's ratio, porosity, reservoir depth, reservoir thickness, shear modulus, static friction coefficient and stress ratio while the fault characteristics included the absolute fault offset and whether the fault is bounding or not.
Afterwards, I have plotted the onset pressure versus the relative fault offset and assessed the sensitivity of the onset pressure whilst changing input parameter settings, namely the critical slip weakening distance, dip angle, dynamic friction coefficient, initial reservoir pressure, Poisson's ratio, porosity, reservoir thickness, shear modulus, static friction and stress ratio. The most critical parameter has turned out to be the stress ratio. I have examined the stress ratio ranges for each field in order to assess whether this parameter could predict the occurrence of seismicity for an entire region. Some fields that do not suit the optimal regional stress ratio have been considered anomalies and investigated further. The main explanations for the anomalies have been geological complexity, assumed synthetic fault offsets, over- or underestimated offsets, unregistered seismic events and substantial overpressure.
The answer to the research question is, yes, it is possible to predict whether seismicity will occur in a small Dutch gas field located in the Rotliegend formation based on reservoir data and fault characteristics. A regional stress ratio has been determined for each of the five regions. The regional stress ratio is 0.51 for NHP, 0.58 for Groningen, 0.69 for LTHP, 0.46 and 0.47 for FP and 0.50 and 0.56 for LT. Salt layers have most likely contributed to higher regional stress ratios for GRO, LT and LTHP. ...
First, I have examined the probability of all small Dutch gas fields being responsible for a seismic event. Based on the distance between the gas field and the nearest event, as well as the presence of other fields in the surrounding area, I have derived a classification for the likelihood that the field was associated with induced seismicity. Second, I have run a sensitivity analysis to identify which parameter was most significant. I have accomplished this by implementing a semi-analytical model that computed and depicted depletion-induced stresses and fault slip along an inclined fault. The model calculated the depletion pressure at which seismic slip starts to occur, here called the onset pressure, based on reservoir data and fault characteristics. The reservoir data contains the compaction coefficient, critical slip weakening distance, dip angle, dynamic friction coefficient, initial reservoir pressure, Poisson's ratio, porosity, reservoir depth, reservoir thickness, shear modulus, static friction coefficient and stress ratio while the fault characteristics included the absolute fault offset and whether the fault is bounding or not.
Afterwards, I have plotted the onset pressure versus the relative fault offset and assessed the sensitivity of the onset pressure whilst changing input parameter settings, namely the critical slip weakening distance, dip angle, dynamic friction coefficient, initial reservoir pressure, Poisson's ratio, porosity, reservoir thickness, shear modulus, static friction and stress ratio. The most critical parameter has turned out to be the stress ratio. I have examined the stress ratio ranges for each field in order to assess whether this parameter could predict the occurrence of seismicity for an entire region. Some fields that do not suit the optimal regional stress ratio have been considered anomalies and investigated further. The main explanations for the anomalies have been geological complexity, assumed synthetic fault offsets, over- or underestimated offsets, unregistered seismic events and substantial overpressure.
The answer to the research question is, yes, it is possible to predict whether seismicity will occur in a small Dutch gas field located in the Rotliegend formation based on reservoir data and fault characteristics. A regional stress ratio has been determined for each of the five regions. The regional stress ratio is 0.51 for NHP, 0.58 for Groningen, 0.69 for LTHP, 0.46 and 0.47 for FP and 0.50 and 0.56 for LT. Salt layers have most likely contributed to higher regional stress ratios for GRO, LT and LTHP.
Two suitable geophysical methods are the Ground Penetrating Radar (GPR) and seismic techniques with a focus on reflection measurements. For the GPR specifically, we choose a Common Offset Survey, which can map reflections from the subsurface. For the seismic techniques, we choose a line array measurement, among others. We use the GPR to estimate the buried rock contour of the keystone Sl2 of megalith D14, which is a bearing stone formerly supporting capstone D9. We perform several reflection tests on various rocks unrelated to D14 using different seismic sources and receivers to estimate the reflection depths. We follow a proposed approach for both methods.
To evaluate the GPR data from the field, we assume a simplified GPR with zero-dimensional antennas (GPR point model). Subsequently, we develop two mathematical models (GPR point-to-GEO and GEO-to-GPR point model), based on this conceptual model in order to I) calculate the (buried) rock surfaces from field data and II) model field data from estimated buried rock contours.
We first perform the Common Offset Survey on a non-buried boulder on the campus of the TU Delft to evaluate the accuracy of the developed GPR point-to-GEO model and to optimise the second survey on keystone Sl2. We first perform the seismic reflection measurements on several rock samples to determine the best seismic source. Finally, we perform a line array measurement on a cylindrical basalt column using 300 kHz transducers.
We calculate rock contour coordinates from the GPR data and these show a reasonable fit with the contour of the TU Delft boulder, with an accuracy of 5-10 cm. For the keystone Sl2, the maximum burial depth is determined to be 80 cm at the southern side. The bottom of the keystone is sloping downward starting from ground level at the northern side. The southern, eastern and western rock faces are steep, almost vertical, which is confirmed by historic photographs. However, the calculated (buried) rock surface coordinates consist of an incoherent set of coordinates with locally a lack of data or blind-spots. Estimating a coherent buried rock contour, therefore, requires shortcuts and a decrease of accuracy is to be expected especially for rock surfaces near blind-spots in the GPR data. Furthermore, the identification of relevant reflection surfaces is rather subjective and combined with blind spots in the acquired GPR data, this can lead to wrongful interpretations of the buried rock contour.
The seismic reflection measurements we perform give clear reflections for the 300 kHz transducers on rocks of limited size with simple geometries. However, the transducers should first be applied on rocks with increasingly more complex geometries before being applied in the field. The accuracy in the order of 1 cm can be considered promising, but its applicability for complex geometries and reflection depths larger than 0.5 m remains unknown. ...
Two suitable geophysical methods are the Ground Penetrating Radar (GPR) and seismic techniques with a focus on reflection measurements. For the GPR specifically, we choose a Common Offset Survey, which can map reflections from the subsurface. For the seismic techniques, we choose a line array measurement, among others. We use the GPR to estimate the buried rock contour of the keystone Sl2 of megalith D14, which is a bearing stone formerly supporting capstone D9. We perform several reflection tests on various rocks unrelated to D14 using different seismic sources and receivers to estimate the reflection depths. We follow a proposed approach for both methods.
To evaluate the GPR data from the field, we assume a simplified GPR with zero-dimensional antennas (GPR point model). Subsequently, we develop two mathematical models (GPR point-to-GEO and GEO-to-GPR point model), based on this conceptual model in order to I) calculate the (buried) rock surfaces from field data and II) model field data from estimated buried rock contours.
We first perform the Common Offset Survey on a non-buried boulder on the campus of the TU Delft to evaluate the accuracy of the developed GPR point-to-GEO model and to optimise the second survey on keystone Sl2. We first perform the seismic reflection measurements on several rock samples to determine the best seismic source. Finally, we perform a line array measurement on a cylindrical basalt column using 300 kHz transducers.
We calculate rock contour coordinates from the GPR data and these show a reasonable fit with the contour of the TU Delft boulder, with an accuracy of 5-10 cm. For the keystone Sl2, the maximum burial depth is determined to be 80 cm at the southern side. The bottom of the keystone is sloping downward starting from ground level at the northern side. The southern, eastern and western rock faces are steep, almost vertical, which is confirmed by historic photographs. However, the calculated (buried) rock surface coordinates consist of an incoherent set of coordinates with locally a lack of data or blind-spots. Estimating a coherent buried rock contour, therefore, requires shortcuts and a decrease of accuracy is to be expected especially for rock surfaces near blind-spots in the GPR data. Furthermore, the identification of relevant reflection surfaces is rather subjective and combined with blind spots in the acquired GPR data, this can lead to wrongful interpretations of the buried rock contour.
The seismic reflection measurements we perform give clear reflections for the 300 kHz transducers on rocks of limited size with simple geometries. However, the transducers should first be applied on rocks with increasingly more complex geometries before being applied in the field. The accuracy in the order of 1 cm can be considered promising, but its applicability for complex geometries and reflection depths larger than 0.5 m remains unknown.
Bored Tunnel Lining Behaviour in Discontinuous Rock
Railway Tunnel in Middle-East
Appraisal of Friction Coefficients Between TBM and Conditioned Soil
A Laboratory Investigation Adopting a Direct Shear Apparatus
Innovative tidal inlet design
Design methodology in Boughaz 1 inlet, Lake Bardawil
One of the recent researches that is carried out by the Dredging, Environmental and Marine Engineering (DEME), The Weather Makers (TWM) and Lanters (2016), studied how the ecosystem and the fish population of Lake Bardawil can be restored by new hydraulic interventions. This thesis is an extension of the aforementioned work, but current focus is put on the determination of an innovative design and associated methodology which is based on natural design elements and can improve the functionality of Boughaz 1 inlet.
Boughaz 1 was constructed in 1955 to allow the water exchange between the sea and the lagoon. Over the passing years, it has been subjected to a reduced tidal prism resulting in poor water quality in the lagoon, limited fish migration from the sea and sedimentation causes the need for dredging maintenance works. This led to the construction of breakwaters in 1985 until 1995 for the stabilization of the inlet and for the protection of the fish population in the lagoon. Although, the dredging works and constructed breakwaters minimized the abrupt sedimentation through the inlet and improved its stability in short term, the natural behavior of the system is gradually changed which worsen these conditions in longer term. For that reason, a design methodology is carried out to understand and improve the functionality of the Boughaz 1 inlet. The design methodology is based on the most important natural design elements, namely inlet cross sectional area, approach channel and inlet nourishment. Numerical models (Delft3D and Delft3D FM) are used to assess the influence of the different designs on the functionality of the system. A hydrodynamic analysis is carried out for each design element to define the final combined design of the initial phase of this design process. This final design is examined under hydrodynamics and the initial deposition and erosion patters. It is concluded that the functionality of the Boughaz 1 inlet can be optimized with the adapted design methodology. The tidal prism and flow velocities have been increased while the aim to mimic nature is validated with the initial deposition and erosion patterns.
...
One of the recent researches that is carried out by the Dredging, Environmental and Marine Engineering (DEME), The Weather Makers (TWM) and Lanters (2016), studied how the ecosystem and the fish population of Lake Bardawil can be restored by new hydraulic interventions. This thesis is an extension of the aforementioned work, but current focus is put on the determination of an innovative design and associated methodology which is based on natural design elements and can improve the functionality of Boughaz 1 inlet.
Boughaz 1 was constructed in 1955 to allow the water exchange between the sea and the lagoon. Over the passing years, it has been subjected to a reduced tidal prism resulting in poor water quality in the lagoon, limited fish migration from the sea and sedimentation causes the need for dredging maintenance works. This led to the construction of breakwaters in 1985 until 1995 for the stabilization of the inlet and for the protection of the fish population in the lagoon. Although, the dredging works and constructed breakwaters minimized the abrupt sedimentation through the inlet and improved its stability in short term, the natural behavior of the system is gradually changed which worsen these conditions in longer term. For that reason, a design methodology is carried out to understand and improve the functionality of the Boughaz 1 inlet. The design methodology is based on the most important natural design elements, namely inlet cross sectional area, approach channel and inlet nourishment. Numerical models (Delft3D and Delft3D FM) are used to assess the influence of the different designs on the functionality of the system. A hydrodynamic analysis is carried out for each design element to define the final combined design of the initial phase of this design process. This final design is examined under hydrodynamics and the initial deposition and erosion patters. It is concluded that the functionality of the Boughaz 1 inlet can be optimized with the adapted design methodology. The tidal prism and flow velocities have been increased while the aim to mimic nature is validated with the initial deposition and erosion patterns.
Investigation of Vertical Cutter Mining for Increased Primary Resource Recovery and Decreased Environmental Impact
A VCM Study for De Beers, Victor Pipe, Canada
Vertical cutting has been used for several decades for the construction of water retention walls in the civil engineering industry. By placing the vertical cutter system directly on top of an ore target and cutting straight, vertical trenches up to a maximum depth of 150 m, it is intended to cross over to the mining industry. Extraction with vertical cutting can occur according four extraction scenarios. Three of the scenarios are land-based, the fourth assumes flooding of the mine, and has not been considered for the Victor project.
Checkerboard mining is the base case extraction scenario with an extraction rate of approximately 30%. The long trenching scenario would increase the recovery with an additional 15% but induces a high risk of instability in the existing pit walls and the kimberlite in between the trenches. Application of backfill is the third scenario and achieves a recovery of 98%. Backfilling of the trenches requires the movement of significant volumes of additional rock as well as induces time delays due to the curing time of the backfill.
Financial evaluation of the vertical cutting scenarios shows a high dependency of the project value on a decreasing cutting performance. Cumulative cash flow analysis and NPV suggest that extending the mine life at the Victor Diamond mine with vertical cutting is favourable. Even in the case of increased rock strengths, as expected in the deeper parts of the Victor pipes, vertical cutting has a positive net present project value. Long trenching, which is considered to be of high risk for pit stability has only marginally greater project value than the base case.
The development of alternative mining solutions also aims to reduce the impact of the mining operations on the surrounding environment. Vertical cutting combines multiple mining processes into one operating piece of equipment. It reduces the GHG emissions, improves the safety of extraction process and is expected to increase the support from stakeholders. Extending operational life using conventional methods would require large expansion of the mine involving the increase of the operational fleet, pumping capacity and land usage. The application of vertical cutting has the ability to prevent the negative impact of enlarged open pit mining while maintaining the benefit of continued production. ...
Vertical cutting has been used for several decades for the construction of water retention walls in the civil engineering industry. By placing the vertical cutter system directly on top of an ore target and cutting straight, vertical trenches up to a maximum depth of 150 m, it is intended to cross over to the mining industry. Extraction with vertical cutting can occur according four extraction scenarios. Three of the scenarios are land-based, the fourth assumes flooding of the mine, and has not been considered for the Victor project.
Checkerboard mining is the base case extraction scenario with an extraction rate of approximately 30%. The long trenching scenario would increase the recovery with an additional 15% but induces a high risk of instability in the existing pit walls and the kimberlite in between the trenches. Application of backfill is the third scenario and achieves a recovery of 98%. Backfilling of the trenches requires the movement of significant volumes of additional rock as well as induces time delays due to the curing time of the backfill.
Financial evaluation of the vertical cutting scenarios shows a high dependency of the project value on a decreasing cutting performance. Cumulative cash flow analysis and NPV suggest that extending the mine life at the Victor Diamond mine with vertical cutting is favourable. Even in the case of increased rock strengths, as expected in the deeper parts of the Victor pipes, vertical cutting has a positive net present project value. Long trenching, which is considered to be of high risk for pit stability has only marginally greater project value than the base case.
The development of alternative mining solutions also aims to reduce the impact of the mining operations on the surrounding environment. Vertical cutting combines multiple mining processes into one operating piece of equipment. It reduces the GHG emissions, improves the safety of extraction process and is expected to increase the support from stakeholders. Extending operational life using conventional methods would require large expansion of the mine involving the increase of the operational fleet, pumping capacity and land usage. The application of vertical cutting has the ability to prevent the negative impact of enlarged open pit mining while maintaining the benefit of continued production.