F.F.J. Schrijer
Please Note
22 records found
1
Performance measurements and aerodynamic heating profiles of (un-)tripped propeller blades
Transition Detection on Aerodynamic Heated Propeller Blade with IR Transmission
An experimental campaign was conducted on the non-swept TUD-XPROP propeller in the TU Delft Low Turbulence Tunnel. This combines quantitative performance measurements from a rotating shaft balance with qualitative infrared thermography images of the blade suction side. A boundary-layer analysis with XFOIL resulted in four adhesive-vinyl trip-device configurations: a dart, a dotted, and two continuous line trips at different chord-wise locations. These trip devices are manufactured, applied, and verified geometrically with a laser surface scanner before testing against a clean, free-transition baseline.
The results show that forced transition does not uniformly improve or degrade propeller efficiency, its effect depends on the combination between trip geometry, chord-wise position, blade loading, and Reynolds and Mach number. The continuous line trip consistently outperformed the discrete configurations, and its optimal chord-wise location over the largest operating domain for the roughness height available is further aft from the leading-edge. Forcing transition flattened the thrust and power curves and reduced the influence of the Reynolds and Mach number on the efficiency. This resulted in an increased efficiency at low Reynolds and Mach numbers, but at higher the efficiency is reduced compared to the clean blade. The infrared measurements did not resolve a distinct transition front, but consistently captured a line over the radius of reduced intensity compared to reference cases. For increased loading, the line moves upstream, especially at the radial location where the angle of attack increases most. Due to the low resolution, it is difficult to observe the influences of the Mach and Reynolds number. And its presence is suppressed once transition is forced upstream of it. The observed trends of this line match with the behaviour of a laminar separation bubble.
Together, the performance and thermal datasets demonstrate the potential of infrared thermography to link changes in boundary-layer state to measured changes in propeller performance. Despite its limited spatial and thermal resolution when applied to a fast-rotating model, infrared thermography provides useful insight into the development of the boundary layer. The results further indicate that effective forced-transition designs should be tailored to the intended operating conditions rather than apply it as a fixed, one-size-fits-all solution. ...
An experimental campaign was conducted on the non-swept TUD-XPROP propeller in the TU Delft Low Turbulence Tunnel. This combines quantitative performance measurements from a rotating shaft balance with qualitative infrared thermography images of the blade suction side. A boundary-layer analysis with XFOIL resulted in four adhesive-vinyl trip-device configurations: a dart, a dotted, and two continuous line trips at different chord-wise locations. These trip devices are manufactured, applied, and verified geometrically with a laser surface scanner before testing against a clean, free-transition baseline.
The results show that forced transition does not uniformly improve or degrade propeller efficiency, its effect depends on the combination between trip geometry, chord-wise position, blade loading, and Reynolds and Mach number. The continuous line trip consistently outperformed the discrete configurations, and its optimal chord-wise location over the largest operating domain for the roughness height available is further aft from the leading-edge. Forcing transition flattened the thrust and power curves and reduced the influence of the Reynolds and Mach number on the efficiency. This resulted in an increased efficiency at low Reynolds and Mach numbers, but at higher the efficiency is reduced compared to the clean blade. The infrared measurements did not resolve a distinct transition front, but consistently captured a line over the radius of reduced intensity compared to reference cases. For increased loading, the line moves upstream, especially at the radial location where the angle of attack increases most. Due to the low resolution, it is difficult to observe the influences of the Mach and Reynolds number. And its presence is suppressed once transition is forced upstream of it. The observed trends of this line match with the behaviour of a laminar separation bubble.
Together, the performance and thermal datasets demonstrate the potential of infrared thermography to link changes in boundary-layer state to measured changes in propeller performance. Despite its limited spatial and thermal resolution when applied to a fast-rotating model, infrared thermography provides useful insight into the development of the boundary layer. The results further indicate that effective forced-transition designs should be tailored to the intended operating conditions rather than apply it as a fixed, one-size-fits-all solution.
The surface did not sublimate uniformly. It eroded into upright millimetre-scale spikes that thinned at their base, detached, and were carried upward. Over 10,000 grain trajectories were reconstructed. A temperature-dependent Hertz-Knudsen model accounts for most of the measured mass loss, and a free-molecular force balance shows the ejected grains cannot be compact ice. Extrapolated to icy moon conditions, the Enceladus South Polar Terrain is the one environment considered that is warm enough to eject grains, indicating a passive thermodynamic pathway for generating porous regolith. ...
The surface did not sublimate uniformly. It eroded into upright millimetre-scale spikes that thinned at their base, detached, and were carried upward. Over 10,000 grain trajectories were reconstructed. A temperature-dependent Hertz-Knudsen model accounts for most of the measured mass loss, and a free-molecular force balance shows the ejected grains cannot be compact ice. Extrapolated to icy moon conditions, the Enceladus South Polar Terrain is the one environment considered that is warm enough to eject grains, indicating a passive thermodynamic pathway for generating porous regolith.
Coupled DSMC Simulation of an Air-Breathing Electric Propulsion Intake and Thruster Interface
Effects of thruster interface, and Chamber Shape on Neutral Gas Delivery
The framework is first validated against the non-gridded conical intake and applied to four passive baseline configurations combining two intake profiles with two discharge-chamber geometries. The intake profile produces sub-percent differences at the throat and discharge-exit planes, as expected because diffuse re-emission removes the directional memory the profile would otherwise carry. The chamber geometry produces a measurable effect on the throat measurement, indicating that the throat responds to the downstream boundary at the level of a passive chamber wall alone.
The framework is then applied to the SITAEL split-ring architecture, scaled to a 16U CubeSat platform and coupled to the RIT-µ3 ion optics at 215 km. The interface is modelled as an absorbing-diffuse boundary at the neutral transparency τn = 0.25, with the central blank resolved as a physical surface. Resolving the interface changes the reported performance. The chamber density is 1.67× the fully absorbing-boundary prediction, the delivered flux is 0.43× it, and the residence time is 4.05× it. These corrections exceed the differences between the intake geometries reported in the literature.
The study then examines three geometric parameters at the exit face against the resolved interface: the blank surface profile, the intake capture area, and the discharge-chamber cross-section. The blank surface profile redirects the returned population within the chamber without altering the flux delivered to the thruster. The intake capture area enters the reported collection efficiency through its normalization alone and leaves the delivered flux unchanged at fixed exit geometry. Only the discharge-chamber cross-section alters the delivered flux through the exit area it presents to the thruster. The beam extraction requirement of the ion optics fixes both parameters that govern that flux. ...
The framework is first validated against the non-gridded conical intake and applied to four passive baseline configurations combining two intake profiles with two discharge-chamber geometries. The intake profile produces sub-percent differences at the throat and discharge-exit planes, as expected because diffuse re-emission removes the directional memory the profile would otherwise carry. The chamber geometry produces a measurable effect on the throat measurement, indicating that the throat responds to the downstream boundary at the level of a passive chamber wall alone.
The framework is then applied to the SITAEL split-ring architecture, scaled to a 16U CubeSat platform and coupled to the RIT-µ3 ion optics at 215 km. The interface is modelled as an absorbing-diffuse boundary at the neutral transparency τn = 0.25, with the central blank resolved as a physical surface. Resolving the interface changes the reported performance. The chamber density is 1.67× the fully absorbing-boundary prediction, the delivered flux is 0.43× it, and the residence time is 4.05× it. These corrections exceed the differences between the intake geometries reported in the literature.
The study then examines three geometric parameters at the exit face against the resolved interface: the blank surface profile, the intake capture area, and the discharge-chamber cross-section. The blank surface profile redirects the returned population within the chamber without altering the flux delivered to the thruster. The intake capture area enters the reported collection efficiency through its normalization alone and leaves the delivered flux unchanged at fixed exit geometry. Only the discharge-chamber cross-section alters the delivered flux through the exit area it presents to the thruster. The beam extraction requirement of the ion optics fixes both parameters that govern that flux.
The objective of the present work is to develop a robust set up to simulate an RDE employing the DLR TAU code to obtain physical solutions to investigate the flow field within the engine and its performance. The impact of different modeling decisions and their influence on the flow physics shall be addressed.
First, a set of 1D shock tube simulations have been conducted to evaluate the best solver parameters to capture detonation dynamics. Later, results of 2D simulations based on a test case from literature were performed and the modeling decisions were re-evaluated for this more realistic case. Lastly, two different 3D simulations have been performed and compared with the respective experimental results.
The results showed that a resolution of 200 microns was enough in 2D simulations to capture the main flow features. Moreover, the chosen chemical reaction mechanism was from Ó Conaire et al. 2004, and the upwind flux that performed the best was the AUSMDV (Wada et al. 1994) solver. Moreover, the time step employed was of the order of ten to the power of minus eight seconds. Different inlet boundary conditions were studied, finding the Dirichlet type more suitable to uncouple injection and detonation dynamics. In addition, different ignition strategies were evaluated, proving that the strategies were successful and achieved a stable mode of operation.
This work presents a robust set up to perform 2D and 3D RDE simulations employing the DLR TAU code. It also provides many insights into the impact of different modeling decisions on the flow field and evolution of the engine performance.
...
The objective of the present work is to develop a robust set up to simulate an RDE employing the DLR TAU code to obtain physical solutions to investigate the flow field within the engine and its performance. The impact of different modeling decisions and their influence on the flow physics shall be addressed.
First, a set of 1D shock tube simulations have been conducted to evaluate the best solver parameters to capture detonation dynamics. Later, results of 2D simulations based on a test case from literature were performed and the modeling decisions were re-evaluated for this more realistic case. Lastly, two different 3D simulations have been performed and compared with the respective experimental results.
The results showed that a resolution of 200 microns was enough in 2D simulations to capture the main flow features. Moreover, the chosen chemical reaction mechanism was from Ó Conaire et al. 2004, and the upwind flux that performed the best was the AUSMDV (Wada et al. 1994) solver. Moreover, the time step employed was of the order of ten to the power of minus eight seconds. Different inlet boundary conditions were studied, finding the Dirichlet type more suitable to uncouple injection and detonation dynamics. In addition, different ignition strategies were evaluated, proving that the strategies were successful and achieved a stable mode of operation.
This work presents a robust set up to perform 2D and 3D RDE simulations employing the DLR TAU code. It also provides many insights into the impact of different modeling decisions on the flow field and evolution of the engine performance.
Results show that compressibility strongly influences the mean flow field and aerodynamic loads of the FFA-W3-211 airfoil. Trends toward transonic flow and unsteady shock waves were identified with increasing absolute angle of attack and freestream Mach number. The results at α = -6° display a 30% reduction in the negative lift coefficient from cl = -0.43 to -0.31 and a 190% increase in drag coefficient from cd = -0.026 to -0.075, with increasing Mach number from M∞ = 0.5 to 0.65. For the same Mach number range, the lift coefficient results at α = -10° display a plateau around cl ≈ -0.65 to -0.67, and a 100% increase in drag coefficient, from cd = -0.085 to -0.174. At moderate angles of attack, the increased mean drag was influenced by the growth of trailing edge separation. Beyond M∞ = 0.6, the emergence of shock waves plays a greater role in inducing earlier separation and less efficient pressure recovery. The growth of the separation region decreases the mean negative lift for α ≤ -6°. For α ≥ -8°, conversely, the emergence of supersonic flow and lower pressures over the trailing edge counteract the effects of increased separation. For the phase-averaged analysis of the transonic buffet cycle at α = -10° and M∞ = 0.65, the phase-averaged lift coefficient varies periodically in a range of approximately ~22% of the time-averaged lift coefficient, while the phase-averaged drag coefficient varies up to ~80% of the time-averaged drag coefficient.
This work is part of the foundation for understanding the effects of compressibility in wind turbine airfoils and wind turbines. It identifies the complex interplay of shock waves, separation, and shock wave–boundary layer interaction (SWBLI) in the transonic regime. The results highlight and challenge current assumptions of incompressible flow for the design and operation of modern and future large-scale wind turbines that rely on incompressible aerodynamic polars.
...
Results show that compressibility strongly influences the mean flow field and aerodynamic loads of the FFA-W3-211 airfoil. Trends toward transonic flow and unsteady shock waves were identified with increasing absolute angle of attack and freestream Mach number. The results at α = -6° display a 30% reduction in the negative lift coefficient from cl = -0.43 to -0.31 and a 190% increase in drag coefficient from cd = -0.026 to -0.075, with increasing Mach number from M∞ = 0.5 to 0.65. For the same Mach number range, the lift coefficient results at α = -10° display a plateau around cl ≈ -0.65 to -0.67, and a 100% increase in drag coefficient, from cd = -0.085 to -0.174. At moderate angles of attack, the increased mean drag was influenced by the growth of trailing edge separation. Beyond M∞ = 0.6, the emergence of shock waves plays a greater role in inducing earlier separation and less efficient pressure recovery. The growth of the separation region decreases the mean negative lift for α ≤ -6°. For α ≥ -8°, conversely, the emergence of supersonic flow and lower pressures over the trailing edge counteract the effects of increased separation. For the phase-averaged analysis of the transonic buffet cycle at α = -10° and M∞ = 0.65, the phase-averaged lift coefficient varies periodically in a range of approximately ~22% of the time-averaged lift coefficient, while the phase-averaged drag coefficient varies up to ~80% of the time-averaged drag coefficient.
This work is part of the foundation for understanding the effects of compressibility in wind turbine airfoils and wind turbines. It identifies the complex interplay of shock waves, separation, and shock wave–boundary layer interaction (SWBLI) in the transonic regime. The results highlight and challenge current assumptions of incompressible flow for the design and operation of modern and future large-scale wind turbines that rely on incompressible aerodynamic polars.
Preliminary Design of a Turbine Test Facility for Rocket Engine Applications
Enhancing rapid and agile development of rocket engines
A three-phase methodology is adopted. First, top-level requirements are derived for turbines representative of 1 MN-class engines, and a scaling strategy is defined. The selected approach fixes Baljé specific speed and specific diameter, together with the inlet spouting Mach number, to preserve the main thermal and aero-mechanical phenomena while reducing power to a feasible range. Applying this methodology to a dataset of hydrogen–oxygen turbines yields a test envelope of roughly 3 M W shaft power at 30–50 krpm and defines the corresponding pressure, temperature, and mass-flow ranges for the facility.
In the second phase, several power-dissipation concepts are surveyed and modelled using zero- and one-dimensional analyses. A Pareto-based Analytic Hierarchy Process is then used to structure the trade-off. A self-designed, directly driven water pump with inducer and impeller stages is down-selected as the preferred concept, capable of absorbing 3 M W of power at 100 kg/s with a total pressure rise of 210 bar while avoiding cavitation through appropriate inlet pressurization.
The third phase focuses on the shaft support subsystem. A parametric rotordynamic model of the coupled turbine–pump shaft and pillow block is developed to derive stiffness, damping, load, and lubrication requirements for angular-contact ball bearings operating in the 30–50 krpm range. Results show that, with bearing stiffness in the 107–108 N/m range and moderate external damping, critical speeds can be placed outside the operating window, resonance crossings remain within acceptable displacement limits, and bearing loads and losses lie within achievable catalog values.
Overall, the work demonstrates the feasibility of a multi-MW turbine test facility that combines a high level of representativeness with broad flexibility, and provides ceiling requirements and subsystem concepts that form a concrete baseline for subsequent detailed design and eventual construction. ...
A three-phase methodology is adopted. First, top-level requirements are derived for turbines representative of 1 MN-class engines, and a scaling strategy is defined. The selected approach fixes Baljé specific speed and specific diameter, together with the inlet spouting Mach number, to preserve the main thermal and aero-mechanical phenomena while reducing power to a feasible range. Applying this methodology to a dataset of hydrogen–oxygen turbines yields a test envelope of roughly 3 M W shaft power at 30–50 krpm and defines the corresponding pressure, temperature, and mass-flow ranges for the facility.
In the second phase, several power-dissipation concepts are surveyed and modelled using zero- and one-dimensional analyses. A Pareto-based Analytic Hierarchy Process is then used to structure the trade-off. A self-designed, directly driven water pump with inducer and impeller stages is down-selected as the preferred concept, capable of absorbing 3 M W of power at 100 kg/s with a total pressure rise of 210 bar while avoiding cavitation through appropriate inlet pressurization.
The third phase focuses on the shaft support subsystem. A parametric rotordynamic model of the coupled turbine–pump shaft and pillow block is developed to derive stiffness, damping, load, and lubrication requirements for angular-contact ball bearings operating in the 30–50 krpm range. Results show that, with bearing stiffness in the 107–108 N/m range and moderate external damping, critical speeds can be placed outside the operating window, resonance crossings remain within acceptable displacement limits, and bearing loads and losses lie within achievable catalog values.
Overall, the work demonstrates the feasibility of a multi-MW turbine test facility that combines a high level of representativeness with broad flexibility, and provides ceiling requirements and subsystem concepts that form a concrete baseline for subsequent detailed design and eventual construction.
Swing eVTOL
Final report
It is shown that the varying geometry of the channel imposes constraints on the maximum expansion angle before flow separation occurs, the sonic point location and the length/width combination in order to achieve a certain vent Mach number and mass flow rate, although this is also decided by the reservoir and ambient conditions. However, besides the physical properties of the model, there is evidence that the flow properties are dominated by the thermal processes occurring inside the setup. Condensation occurs only in the reservoir, releasing latent heat and making the isentropic flow assumption invalid by definition. It is demonstrated that it is likely that the thermal radiation from the test section of the HTFD onto the model is sufficient to thermally choke the flow. It is unlikely that the flows become choked due to the effects of friction alone. Cooling the models by 10-15°C did not result in significant changes in flow properties, and to have noticeable effects on the flow, the models would have to be cooled to much lower temperatures so that condensation occurs in the channel instead of the reservoir. Although the vapor remains unsaturated in the channels, there are signs of local temperature spikes in the ex- panding sections of the channels, near the vent, when either no or low heating power is supplied to the reservoir water and the pressure in the channel is reduced. This implies that either the temperature at the center of the channel is lower than what could be expected from the temperature measurements and heat is thus released by the deposition of the vapor, or the particles that condensed in the reser- voir partially evaporate after the throat of the channel, after which the evaporative cooling freezes the remainder of the particles, with the accompanying latent heat release. It is also not expected that a pressurized reservoir is necessary to create the plumes on Enceladus, nor is the presence of a geomet- rical throat, due to the combined effects of friction and condensing vapor. The results of one physical model are compared to a computational fluid dynamics model using the same geometry, and the main difference between the physical and numerical model is that the vent pressure of the numerical model is approximately half the vent pressure of the physical model, and the temperature of the numerical model dropped to about -50°C at the expanding section of the channel where the temperature only increased throughout the channel for the physical model. This, and the small heat spike near the vent under low-power conditions, has questioned the accuracy of the temperature measurement method and further research would be required to improve this accuracy. ...
It is shown that the varying geometry of the channel imposes constraints on the maximum expansion angle before flow separation occurs, the sonic point location and the length/width combination in order to achieve a certain vent Mach number and mass flow rate, although this is also decided by the reservoir and ambient conditions. However, besides the physical properties of the model, there is evidence that the flow properties are dominated by the thermal processes occurring inside the setup. Condensation occurs only in the reservoir, releasing latent heat and making the isentropic flow assumption invalid by definition. It is demonstrated that it is likely that the thermal radiation from the test section of the HTFD onto the model is sufficient to thermally choke the flow. It is unlikely that the flows become choked due to the effects of friction alone. Cooling the models by 10-15°C did not result in significant changes in flow properties, and to have noticeable effects on the flow, the models would have to be cooled to much lower temperatures so that condensation occurs in the channel instead of the reservoir. Although the vapor remains unsaturated in the channels, there are signs of local temperature spikes in the ex- panding sections of the channels, near the vent, when either no or low heating power is supplied to the reservoir water and the pressure in the channel is reduced. This implies that either the temperature at the center of the channel is lower than what could be expected from the temperature measurements and heat is thus released by the deposition of the vapor, or the particles that condensed in the reser- voir partially evaporate after the throat of the channel, after which the evaporative cooling freezes the remainder of the particles, with the accompanying latent heat release. It is also not expected that a pressurized reservoir is necessary to create the plumes on Enceladus, nor is the presence of a geomet- rical throat, due to the combined effects of friction and condensing vapor. The results of one physical model are compared to a computational fluid dynamics model using the same geometry, and the main difference between the physical and numerical model is that the vent pressure of the numerical model is approximately half the vent pressure of the physical model, and the temperature of the numerical model dropped to about -50°C at the expanding section of the channel where the temperature only increased throughout the channel for the physical model. This, and the small heat spike near the vent under low-power conditions, has questioned the accuracy of the temperature measurement method and further research would be required to improve this accuracy.
This thesis aims to improve the physical understanding of the interaction between the ocean, icy crust, and the plumes of Enceladus, by experimentally simulating such a plume in the wind tunnel laboratories of TU Delft, and monitoring and analyzing the dynamic physical processes taking place across the experimental setup. A physical analog, separated into regions simulating the ocean, crevasse, and vent of the plume mechanism, is monitored with pressure and temperature sensors, while plume particles are detected with optical tracing
techniques. These observations lead to estimations of the vapor mass flow rate, the outflow Mach number, and the fraction of the plume mass that is condensed. It is found that the ocean conditions can be easily controlled through an adjustable heating power supply. The vapor flow generated by the boiling ocean becomes choked in the crevasse and can attain supersonic velocities. The thermodynamic conditions at the vent of the plume exhibit a greatly varying behavior suggesting that the combined effect of the crevasse geometry and the
nucleation of vapor into liquid and icy particles results in considerable diversity in the plume characteristics. Thus, an isentropic description of the plume flow is found to be inadequate, while a Rayleigh flow is found to be feasible. Heat exchange phenomena appear to dominate locally the plume flow, as strong evidence of thermal choking in the crevasse is found. Particles with speeds of up to 426 ± 5 m/s are detected being ejected from the vent of the crevasse, and the maximum fraction of condensed plume mass is found to be 2.94% ± 0.15%. Finally, the possibility of a supersonic plume generated on Enceladus by a crevasse of constant cross-sectional area and cold walls is examined and found to be feasible. ...
This thesis aims to improve the physical understanding of the interaction between the ocean, icy crust, and the plumes of Enceladus, by experimentally simulating such a plume in the wind tunnel laboratories of TU Delft, and monitoring and analyzing the dynamic physical processes taking place across the experimental setup. A physical analog, separated into regions simulating the ocean, crevasse, and vent of the plume mechanism, is monitored with pressure and temperature sensors, while plume particles are detected with optical tracing
techniques. These observations lead to estimations of the vapor mass flow rate, the outflow Mach number, and the fraction of the plume mass that is condensed. It is found that the ocean conditions can be easily controlled through an adjustable heating power supply. The vapor flow generated by the boiling ocean becomes choked in the crevasse and can attain supersonic velocities. The thermodynamic conditions at the vent of the plume exhibit a greatly varying behavior suggesting that the combined effect of the crevasse geometry and the
nucleation of vapor into liquid and icy particles results in considerable diversity in the plume characteristics. Thus, an isentropic description of the plume flow is found to be inadequate, while a Rayleigh flow is found to be feasible. Heat exchange phenomena appear to dominate locally the plume flow, as strong evidence of thermal choking in the crevasse is found. Particles with speeds of up to 426 ± 5 m/s are detected being ejected from the vent of the crevasse, and the maximum fraction of condensed plume mass is found to be 2.94% ± 0.15%. Finally, the possibility of a supersonic plume generated on Enceladus by a crevasse of constant cross-sectional area and cold walls is examined and found to be feasible.
Transonic Dimples
An experimental study of the flow structures formed at transonic speeds over dimpled surfaces
A transonic flow was reproduced experimentally using an asymmetric nozzle. Then, the performance of five dimple designs was evaluated against the criteria adopted for transonic bumps. Measurements included Schlieren, surface pressure and PIV. Results reveal that small spherical dents seem to produce spanwise excitations that subdue the detrimental effects of expansion fans formed at their edges, and ultimately allow for a higher momentum retention across the interaction. ...
A transonic flow was reproduced experimentally using an asymmetric nozzle. Then, the performance of five dimple designs was evaluated against the criteria adopted for transonic bumps. Measurements included Schlieren, surface pressure and PIV. Results reveal that small spherical dents seem to produce spanwise excitations that subdue the detrimental effects of expansion fans formed at their edges, and ultimately allow for a higher momentum retention across the interaction.
Dimpled channel flows
An experimental investigation into the drag performance of dimpled surfaces in turbulent channel flows
The present thesis focuses on an attempt to manipulate particles without the use of any real channels or external field. Although such manipulation is desired in the micro-scale, a top down approach is preferred and hence, the manipulation is carried out in a scaled up model. First, a Hele-Shaw flow cell is designed with sources and sinks in the millimeter scale to deviate streamlines in the same range. Thereafter, four different velocity fields are studied under different combination of sources and sinks, which are then compared to the computational ones. The property of a Hele-Shaw cell that the averaged velocity over the height of the channel is irrotational, makes it possible to compute velocity fields by the use of potential flow theory. The same velocity fields are hence, computed using a discrete source based Panel Method. A good agreement is found between computation and experiment, making PIV measurements not a necessary option for evaluation of velocity fields under these sources and sinks. Finally, individual particle is inserted into the Hele-Shaw cell and manipulated using unsteady fields. The manipulation includes tasks such as diverting particles having same initial position to different end locations; trapping particle for different instances of time and then releasing them into different directions; flipping positions of two particles; and deflecting a particle by ninety degrees. The individual particle trajectory for the above manipulation activities are tracked down using a particle tracking code and then compared with the ones generated using the Panel Method. This, however, excludes the activities where particles need to be trapped because of particle fluctuation near stagnation point. Overall, the Panel Method serves well in predicting particle path-lines and can be used as a tool for manipulating particles. ...
The present thesis focuses on an attempt to manipulate particles without the use of any real channels or external field. Although such manipulation is desired in the micro-scale, a top down approach is preferred and hence, the manipulation is carried out in a scaled up model. First, a Hele-Shaw flow cell is designed with sources and sinks in the millimeter scale to deviate streamlines in the same range. Thereafter, four different velocity fields are studied under different combination of sources and sinks, which are then compared to the computational ones. The property of a Hele-Shaw cell that the averaged velocity over the height of the channel is irrotational, makes it possible to compute velocity fields by the use of potential flow theory. The same velocity fields are hence, computed using a discrete source based Panel Method. A good agreement is found between computation and experiment, making PIV measurements not a necessary option for evaluation of velocity fields under these sources and sinks. Finally, individual particle is inserted into the Hele-Shaw cell and manipulated using unsteady fields. The manipulation includes tasks such as diverting particles having same initial position to different end locations; trapping particle for different instances of time and then releasing them into different directions; flipping positions of two particles; and deflecting a particle by ninety degrees. The individual particle trajectory for the above manipulation activities are tracked down using a particle tracking code and then compared with the ones generated using the Panel Method. This, however, excludes the activities where particles need to be trapped because of particle fluctuation near stagnation point. Overall, the Panel Method serves well in predicting particle path-lines and can be used as a tool for manipulating particles.
expanding gas jet. Low-temperatures can give brittle fracture of the material in the piping downstream of the choke. Models are needed to verify whether the material temperature remains above the lower-design temperature. For the model validation, Imperial College in London (on request by Shell) has carried out lab experiments with argon gas that expands through an orifice from 120 bara to 1 bara. Awaiting the results of the lab experiments, detailed simulations were carried out in the present study using the Fluent CFD programme.
The 3D, steady, compressible Reynolds-Averaged Navier-Stokes equations were solved with the SST k −ω model for the turbulence. The considered configuration is the same as in the lab. It consists of an upstream chamber with argon at 120 bara, that expands through a 5 mm long orifice with 1.55 mm diameter, into a square outlet section with 50 mm sides and 500 mm length. The inlet temperature is -17 oC and the outlet pressure is 1 bara. The supersonic flow leaving the orifice reaches a maximum Mach number of about 9, just before a shock to subsonic flow is found. The jet reaches very low temperatures due to isentropic expansion, and reaches the isenthalpic expansion temperature of 196 K (or -77 oC) downstream of the shock. The jet reaches the sides of the outlet at a distance of about 100 mm.
The maximum Mach number of about 9 predicted by Fluent is higher than the value of about 6 found in a previous simulation study that used the STAR-CCM+ CFD programme. To verify the Fluent results, the distributions of grid cells was varied and the number of grid cells was increased. Also, a MATLAB programme was written that solved the inviscid compressible equations (Euler equations) for an axisymmetric jet.
This confirmed the Fluent results. In addition to the 3D square outlet section, also 3D and 2D Fluent simulations were carried out for a cylindrical outlet (using a hydraulic diameter of 50 mm). The maximum Mach number and the jet structure (velocity, temperature) are not affected by the side walls. This is because the side walls are sufficiently far from the jet.
Furthermore, the temperature and the heat transfer at the walls of the outlet section were investigated. Thereto both adiabatic and non-adiabatic walls were considered. The ambient temperature is 20 oC. Thermal boundary layers are formed along the side walls, that are exposed to a temperature of 196 K (the isenthalpic expansion temperature) in the centre of the pipe, up to a distance of about 1.5 m, where the outer edge of the boundary layer reaches the centre of the pipe. Thereafter the centre line temperature increases due to heat inflow from the ambient. ...
expanding gas jet. Low-temperatures can give brittle fracture of the material in the piping downstream of the choke. Models are needed to verify whether the material temperature remains above the lower-design temperature. For the model validation, Imperial College in London (on request by Shell) has carried out lab experiments with argon gas that expands through an orifice from 120 bara to 1 bara. Awaiting the results of the lab experiments, detailed simulations were carried out in the present study using the Fluent CFD programme.
The 3D, steady, compressible Reynolds-Averaged Navier-Stokes equations were solved with the SST k −ω model for the turbulence. The considered configuration is the same as in the lab. It consists of an upstream chamber with argon at 120 bara, that expands through a 5 mm long orifice with 1.55 mm diameter, into a square outlet section with 50 mm sides and 500 mm length. The inlet temperature is -17 oC and the outlet pressure is 1 bara. The supersonic flow leaving the orifice reaches a maximum Mach number of about 9, just before a shock to subsonic flow is found. The jet reaches very low temperatures due to isentropic expansion, and reaches the isenthalpic expansion temperature of 196 K (or -77 oC) downstream of the shock. The jet reaches the sides of the outlet at a distance of about 100 mm.
The maximum Mach number of about 9 predicted by Fluent is higher than the value of about 6 found in a previous simulation study that used the STAR-CCM+ CFD programme. To verify the Fluent results, the distributions of grid cells was varied and the number of grid cells was increased. Also, a MATLAB programme was written that solved the inviscid compressible equations (Euler equations) for an axisymmetric jet.
This confirmed the Fluent results. In addition to the 3D square outlet section, also 3D and 2D Fluent simulations were carried out for a cylindrical outlet (using a hydraulic diameter of 50 mm). The maximum Mach number and the jet structure (velocity, temperature) are not affected by the side walls. This is because the side walls are sufficiently far from the jet.
Furthermore, the temperature and the heat transfer at the walls of the outlet section were investigated. Thereto both adiabatic and non-adiabatic walls were considered. The ambient temperature is 20 oC. Thermal boundary layers are formed along the side walls, that are exposed to a temperature of 196 K (the isenthalpic expansion temperature) in the centre of the pipe, up to a distance of about 1.5 m, where the outer edge of the boundary layer reaches the centre of the pipe. Thereafter the centre line temperature increases due to heat inflow from the ambient.