A.H. van Zuijlen
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61 records found
1
The simulations are performed with the finite-volume solver INCA using an implicit large-eddy simulation approach, a Cartesian adaptive mesh and a cut-cell immersed-boundary method. The Generic Cyclist Model is used throughout the study, allowing the straight-line simulations to be compared with available wind-tunnel Particle Image Velocimetry measurements. The numerical sensitivity to mesh resolution, wall treatment and immersed-boundary mixing is first assessed. The numerical approach is then used to investigate two fixed leg positions, a complete cyclist–bicycle configuration, and yaw angles of +6° and −6°. Finally, a constant rotating reference frame in a rectangular domain is introduced to represent cornering motion.
The straight-line simulations reproduce the main large-scale features of the measured wake. The 12 mm mesh with Werner–Wengle wall-function treatment provides the best compromise between wake resolution and computational cost for the cyclist-only cases, while changing the immersed-boundary mixing threshold has little influence on the time-averaged velocity and vorticity fields. The absolute drag forces remain strongly underestimated, showing that the present near-wall and immersed-boundary treatment is not sufficiently accurate for reliable force prediction.
Changing the fixed leg position alters both the lower-body wake and the larger wake structures behind the hips and torso. The results show that the effect of crank position extends several hundred millimetres downstream and that a more symmetric leg position does not necessarily produce a more symmetric wake. The fine full cyclist–bicycle simulation gives a more detailed representation of the lower wake and shows the influence of the bicycle frame, crankset and other components on the flow between and behind the legs. The corresponding surface results confirm that the simulation remains wall modelled, with relatively high local y+ values on exposed and separated regions.
The yawed-flow simulations show that a fixed yaw angle of 6° already causes a clear lateral displacement and reorganisation of the wake. The upper-body, hip and leg-related structures all change with yaw direction, while the asymmetric crank position causes the positive- and negative-yaw cases to respond differently rather than as exact mirror images.
For the cornering case, the required geometrical configuration was established using a rotating reference frame and a partitioned rectangular domain. However, a stable production simulation was not obtained. The treatment of the outer boundary conditions remains the main issue to address before the cornering setup can be used for aerodynamic analysis.
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The simulations are performed with the finite-volume solver INCA using an implicit large-eddy simulation approach, a Cartesian adaptive mesh and a cut-cell immersed-boundary method. The Generic Cyclist Model is used throughout the study, allowing the straight-line simulations to be compared with available wind-tunnel Particle Image Velocimetry measurements. The numerical sensitivity to mesh resolution, wall treatment and immersed-boundary mixing is first assessed. The numerical approach is then used to investigate two fixed leg positions, a complete cyclist–bicycle configuration, and yaw angles of +6° and −6°. Finally, a constant rotating reference frame in a rectangular domain is introduced to represent cornering motion.
The straight-line simulations reproduce the main large-scale features of the measured wake. The 12 mm mesh with Werner–Wengle wall-function treatment provides the best compromise between wake resolution and computational cost for the cyclist-only cases, while changing the immersed-boundary mixing threshold has little influence on the time-averaged velocity and vorticity fields. The absolute drag forces remain strongly underestimated, showing that the present near-wall and immersed-boundary treatment is not sufficiently accurate for reliable force prediction.
Changing the fixed leg position alters both the lower-body wake and the larger wake structures behind the hips and torso. The results show that the effect of crank position extends several hundred millimetres downstream and that a more symmetric leg position does not necessarily produce a more symmetric wake. The fine full cyclist–bicycle simulation gives a more detailed representation of the lower wake and shows the influence of the bicycle frame, crankset and other components on the flow between and behind the legs. The corresponding surface results confirm that the simulation remains wall modelled, with relatively high local y+ values on exposed and separated regions.
The yawed-flow simulations show that a fixed yaw angle of 6° already causes a clear lateral displacement and reorganisation of the wake. The upper-body, hip and leg-related structures all change with yaw direction, while the asymmetric crank position causes the positive- and negative-yaw cases to respond differently rather than as exact mirror images.
For the cornering case, the required geometrical configuration was established using a rotating reference frame and a partitioned rectangular domain. However, a stable production simulation was not obtained. The treatment of the outer boundary conditions remains the main issue to address before the cornering setup can be used for aerodynamic analysis.
This thesis re-formulates the data-driven framework in the context of resolving passive scalar fluxes. Corrections to the scalar flux vector are regressed for two different frameworks: framework 1 that uses the simple gradient diffusion hypothesis (SGDH) model and framework 2: that additionally introduces transport equations for the scalar variance and dissipation. These models are compared to each other for the Jets in-crossflow (JICF) case for resolving the scalar field where baseline RANS models struggle. Both data-driven frameworks show an improvement in modelling the scalar field and turbulent scalar flux vector than the baseline models. The study also indicates that inclusion of additional transport equations doesn’t necessarily improve regression of the corrective fields. ...
This thesis re-formulates the data-driven framework in the context of resolving passive scalar fluxes. Corrections to the scalar flux vector are regressed for two different frameworks: framework 1 that uses the simple gradient diffusion hypothesis (SGDH) model and framework 2: that additionally introduces transport equations for the scalar variance and dissipation. These models are compared to each other for the Jets in-crossflow (JICF) case for resolving the scalar field where baseline RANS models struggle. Both data-driven frameworks show an improvement in modelling the scalar field and turbulent scalar flux vector than the baseline models. The study also indicates that inclusion of additional transport equations doesn’t necessarily improve regression of the corrective fields.
The Reynolds Number Effect on the Flow Topology on a Flying V Aircraft
A Numerical Investigation
variations in the input data are poorly represented by truncated linear modal bases, leading to non physical oscillations and a loss of physical fidelity in reconstructed fields. This limitation is particularly critical when reconstructing flow fields in multiphase flow simulations, where accurate predictions of
interface dynamics are vital.
This work presents a physics-informed reduced-order model for multiphase flows across geometries parameterised by a scalar quantity d. High-fidelity simulations corresponding to distinct geometrical configurations are mapped onto a common reference domain, enabling the extraction of a shared modal basis.
These modes capture flow features that are common across the dataset and form the foundation for reconstructing flow fields corresponding to previously unseen parameter values. The role of training data distribution is also investigated, revealing that the ROM operates predominantly as a local interpolator
in the parameter space. In particular, predictive accuracy is found to depend strongly on the proximity of training configurations to the target case, suggesting a trade-off between local accuracy and global robustness.
To address the limitations of conventional POD, the solution fields are decomposed into smooth and discontinuous components. For the volume fraction, the interface is explicitly identified using the α = 0.5 contour and regressed across geometries using a Gaussian Process Regression (GPR) model. The full field is subsequently reconstructed from the predicted interface geometry. For the pressure field, the discontinuous capillary jump is analytically modelled using the Young-Laplace relation, ∆p = σκ, where κ represents the curvature of the interface profile. POD is then applied exclusively to the smooth pressure field, after which the discontinuity is reintroduced using the predicted interface curvature.
The performance of this adapted approach is evaluated against a baseline approach involving the direct application of POD to the raw, discontinuous data. Performance is assessed in terms of standard L2-norm based measures such as the root mean squared error, as well as newly defined discontinuity aware error metrics, including interface sharpness, volume fraction phase purity, and localised gradient and laplacian metrics for the pressure. While the direct POD yields lower global RMSE values for the volume fraction, it produces oscillatory and smeared interface representations. In contrast, the adapted approach delivers physically consistent reconstructions, yielding more accurate predictions of meniscus characteristics. For the pressure field, the adapted approach demonstrates superior performance across all metrics within the practical operating range of reduced-order models.
A comparative analysis further shows that removing discontinuities prior to applying POD leads to a more compact and efficient modal basis, with improved energy capture. The results demonstrate that incorporating physical insight into the reduced-order modelling of discontinuous flows significantly enhances both accuracy and computational efficiency. ...
variations in the input data are poorly represented by truncated linear modal bases, leading to non physical oscillations and a loss of physical fidelity in reconstructed fields. This limitation is particularly critical when reconstructing flow fields in multiphase flow simulations, where accurate predictions of
interface dynamics are vital.
This work presents a physics-informed reduced-order model for multiphase flows across geometries parameterised by a scalar quantity d. High-fidelity simulations corresponding to distinct geometrical configurations are mapped onto a common reference domain, enabling the extraction of a shared modal basis.
These modes capture flow features that are common across the dataset and form the foundation for reconstructing flow fields corresponding to previously unseen parameter values. The role of training data distribution is also investigated, revealing that the ROM operates predominantly as a local interpolator
in the parameter space. In particular, predictive accuracy is found to depend strongly on the proximity of training configurations to the target case, suggesting a trade-off between local accuracy and global robustness.
To address the limitations of conventional POD, the solution fields are decomposed into smooth and discontinuous components. For the volume fraction, the interface is explicitly identified using the α = 0.5 contour and regressed across geometries using a Gaussian Process Regression (GPR) model. The full field is subsequently reconstructed from the predicted interface geometry. For the pressure field, the discontinuous capillary jump is analytically modelled using the Young-Laplace relation, ∆p = σκ, where κ represents the curvature of the interface profile. POD is then applied exclusively to the smooth pressure field, after which the discontinuity is reintroduced using the predicted interface curvature.
The performance of this adapted approach is evaluated against a baseline approach involving the direct application of POD to the raw, discontinuous data. Performance is assessed in terms of standard L2-norm based measures such as the root mean squared error, as well as newly defined discontinuity aware error metrics, including interface sharpness, volume fraction phase purity, and localised gradient and laplacian metrics for the pressure. While the direct POD yields lower global RMSE values for the volume fraction, it produces oscillatory and smeared interface representations. In contrast, the adapted approach delivers physically consistent reconstructions, yielding more accurate predictions of meniscus characteristics. For the pressure field, the adapted approach demonstrates superior performance across all metrics within the practical operating range of reduced-order models.
A comparative analysis further shows that removing discontinuities prior to applying POD leads to a more compact and efficient modal basis, with improved energy capture. The results demonstrate that incorporating physical insight into the reduced-order modelling of discontinuous flows significantly enhances both accuracy and computational efficiency.
Neural Operators for Three-Dimensional Turbulent Flows
High-Fidelity Dataset Generation and Surrogate Benchmarking
Experimental Validation of Numerical Flexible Propeller Simulations
Reconstructing Geometric Properties Using Modal Participations
The objective of this report is to study experimental deformations of flexible propellersin terms of their underlying parametric properties. These are compared to simulations using the unsteady Reynolds averaged Navier-Stokes equations for fluid calculations, coupled with a finite element model for the structural calculations.
A custom preprocessor was developed and used to reconstruct the full parametric blade geometry from digital image correlation measurements. The first 10 mode shapes of the undeformed mesh were found using modal decomposition, which was fed as input to a flexible point cloud registration. The participation factors for each mode shape were optimized to minimize an error function, the symmetric chamfer distance. The deformed mesh was processed with a software library, PropArt, to recover the underlying geometry parameters.
It was found that the hydrodynamic pitch β was the best predictor of rake, skew, and camber deformations, with increased inertial forces increasing the magnitude of the deformation. Pitch deformations are largely predicted by the blades' inertial loading, and is mostly independent of β. The blade thickness and chord length deformations were negligible. Simulations tended to over predict the deformations of the propeller, especially at low β, being exacerbated by increased inertial loading. At high β, the deformations were small and well predicted.
The relation between pitch deformation and inertial loading suggests an optimal material stiffness per operating condition exists, to be tuned for an appropriate amount of pitch reduction. The lack of correlation to β also poses a challenge in the design as the wake peak is where the change in pitch is desired. The increase in camber also leads to an increase in thrust at low β, which is contrary to the desired wake peak thrust reduction. These relations should be investigated further, for a broader range of material stiffnesses to see if this holds. Finally, the difference between experimental results and simulations suggests a systematic error due to the error scaling with the inertial forces, which should be further investigated.
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The objective of this report is to study experimental deformations of flexible propellersin terms of their underlying parametric properties. These are compared to simulations using the unsteady Reynolds averaged Navier-Stokes equations for fluid calculations, coupled with a finite element model for the structural calculations.
A custom preprocessor was developed and used to reconstruct the full parametric blade geometry from digital image correlation measurements. The first 10 mode shapes of the undeformed mesh were found using modal decomposition, which was fed as input to a flexible point cloud registration. The participation factors for each mode shape were optimized to minimize an error function, the symmetric chamfer distance. The deformed mesh was processed with a software library, PropArt, to recover the underlying geometry parameters.
It was found that the hydrodynamic pitch β was the best predictor of rake, skew, and camber deformations, with increased inertial forces increasing the magnitude of the deformation. Pitch deformations are largely predicted by the blades' inertial loading, and is mostly independent of β. The blade thickness and chord length deformations were negligible. Simulations tended to over predict the deformations of the propeller, especially at low β, being exacerbated by increased inertial loading. At high β, the deformations were small and well predicted.
The relation between pitch deformation and inertial loading suggests an optimal material stiffness per operating condition exists, to be tuned for an appropriate amount of pitch reduction. The lack of correlation to β also poses a challenge in the design as the wake peak is where the change in pitch is desired. The increase in camber also leads to an increase in thrust at low β, which is contrary to the desired wake peak thrust reduction. These relations should be investigated further, for a broader range of material stiffnesses to see if this holds. Finally, the difference between experimental results and simulations suggests a systematic error due to the error scaling with the inertial forces, which should be further investigated.
Modelling wind farms as forests
Modifying a RANS 𝑘−𝜀 forest canopy model to model wind farms
...
A set of non-dimensional relations is derived through dimensional analysis, with a form of the Cauchy number expressing deformation amplitude. Validation using a Reynolds–Cauchy similarity approach on two geometrically similar propellers of different diameters confirms consistent deformation and less than 5\% difference in thrust and torque coefficients between model and full-scale propeller. The disparities in performance results are attributed to numerical artefacts in the fluid solver, as the results indicate that the $k-\omega$ SST turbulence model is sensitive to near-wall resolution.
Achieving full-scale Reynolds numbers in propeller test facilities is not feasible, yet simulations demonstrate that flexible propellers are sensitive to viscous forces. The study observes disparities in deformation extent across Reynolds numbers. The deformation of flexible propellers improves flow attachment over the blades. The overall Reynolds-number trends remain similar to the rigid results: thrust coefficients increase and torque coefficients decrease as Reynolds numbers increase. The open-water efficiency depends on both coefficients, and larger Reynolds numbers result in higher efficiencies.
The Froude–Cauchy scaling approach proves suitable for model experiments; however, material availability limits practical implementation. This study indicates that the steady-state deformation is primarily governed by stiffness, with negligible impact from the structural-to-fluid density ratio. In contrast, in unsteady conditions, the structural-to-fluid density ratio affects the modal frequencies, which describe the dynamic behaviour of propeller blades. Particularly, propellers with high skew, rake, or with anisotropic material properties are affected by structural-to-fluid density. Furthermore, this analysis observes that the first blade mode of a zero-skew angle propeller is pure bending, and a 30\% variation in structural density does not alter the natural frequency of this blade. However, coupled bend-twist modes are sensitive to the structural density, which therefore affects blade deformation in unsteady conditions.
In conclusion, the extent of propeller deformation can be controlled by a non-dimensional parameter expressing the ratio of elastic to hydrodynamic forces. For steady open-water conditions, deformation is additionally a function of Reynolds number. In unsteady conditions, the structural-to-fluid density ratio becomes relevant, as it alters coupled bend-twist modal frequencies. Thus, the deformation extent in this regime is, in addition to the Reynolds number, a function of fluid damping and the ratio of natural frequency to revolution rate. This study offers a basis for accurate scaling of flexible propellers in both experimental and computational studies. ...
A set of non-dimensional relations is derived through dimensional analysis, with a form of the Cauchy number expressing deformation amplitude. Validation using a Reynolds–Cauchy similarity approach on two geometrically similar propellers of different diameters confirms consistent deformation and less than 5\% difference in thrust and torque coefficients between model and full-scale propeller. The disparities in performance results are attributed to numerical artefacts in the fluid solver, as the results indicate that the $k-\omega$ SST turbulence model is sensitive to near-wall resolution.
Achieving full-scale Reynolds numbers in propeller test facilities is not feasible, yet simulations demonstrate that flexible propellers are sensitive to viscous forces. The study observes disparities in deformation extent across Reynolds numbers. The deformation of flexible propellers improves flow attachment over the blades. The overall Reynolds-number trends remain similar to the rigid results: thrust coefficients increase and torque coefficients decrease as Reynolds numbers increase. The open-water efficiency depends on both coefficients, and larger Reynolds numbers result in higher efficiencies.
The Froude–Cauchy scaling approach proves suitable for model experiments; however, material availability limits practical implementation. This study indicates that the steady-state deformation is primarily governed by stiffness, with negligible impact from the structural-to-fluid density ratio. In contrast, in unsteady conditions, the structural-to-fluid density ratio affects the modal frequencies, which describe the dynamic behaviour of propeller blades. Particularly, propellers with high skew, rake, or with anisotropic material properties are affected by structural-to-fluid density. Furthermore, this analysis observes that the first blade mode of a zero-skew angle propeller is pure bending, and a 30\% variation in structural density does not alter the natural frequency of this blade. However, coupled bend-twist modes are sensitive to the structural density, which therefore affects blade deformation in unsteady conditions.
In conclusion, the extent of propeller deformation can be controlled by a non-dimensional parameter expressing the ratio of elastic to hydrodynamic forces. For steady open-water conditions, deformation is additionally a function of Reynolds number. In unsteady conditions, the structural-to-fluid density ratio becomes relevant, as it alters coupled bend-twist modal frequencies. Thus, the deformation extent in this regime is, in addition to the Reynolds number, a function of fluid damping and the ratio of natural frequency to revolution rate. This study offers a basis for accurate scaling of flexible propellers in both experimental and computational studies.
Gaussian process regression for the prediction of aerodynamic performance
A study of multi-output surrogate modeling with optimal sampling for the development of hypersonic vehicles
This thesis presents a baseline analysis of blade loading and near-wake aerodynamics for a FOWT under prescribed roll motions. A coupled high-fidelity GPU-based Large-Eddy Simulation code GRASP resolved turbulent wake dynamics, while OpenFAST calculated blade loads. Coupling was achieved via the Filtered Actuator Line Method and the AspFAST application programming interface. The IEA 15MW reference turbine was modeled under steady, uniform inflow, with variations in roll amplitude (5° and 10°), roll frequency (0.03Hz and 0.05Hz), and tip-speed ratio (TSR 7 and TSR 9) in a full factorial test set.
Results show that roll motion leads to asymmetric fluctuations across the rotor plane. Normal forces display strong vertical asymmetry, with greater variations in the upper side of the rotor due to its larger distance from the roll center. A kinematic analysis deriving the variation of tangential velocity both azimuthally and over time supported this finding. Tangential forces exhibit lateral variation, with a left-right asymmetry across the rotor plane, though the magnitude of variation is similar on both sides. Both roll amplitude and frequency increase the magnitude of loading fluctuations, while TSR influences their blade spanwise distribution.
Power Spectral Density analysis reveals that roll introduces spectral content at the roll frequency and at 1P sideband frequencies, the latter arising from modulation of the 1P frequency by roll. Higher roll amplitudes, frequencies, and TSRs amplify these load fluctuations. While the prominence of the 1P frequency is negligible at the blade, it is strong in the near wake along with the roll frequency, 3P frequency, and 3P sidebands.
The unsteady blade loads directly shape the near wake. The stable helical vortex system of a bottom-fixed turbine is replaced by an oscillatory corkscrew structure that breaks down earlier and more chaotically. Increased roll amplitude causes stronger lateral oscillations and fragmented vortices, while higher roll frequency produces shorter wavelength perturbations, accelerating vortex pairing. Higher TSR strengthens the initial vortices and accelerates breakdown. Standard deviation of velocity fields in the wake confirms larger fluctuations at the top of the rotor due to its greater distance from the roll axis.
This study establishes a direct link between roll-induced blade loads and near-wake dynamics, providing a foundation for improved FOWT design, control, and wake modeling. Future work should assess far-wake impacts, the persistence of lateral velocities induced by rotational motion, and inertial effects under highly unsteady roll conditions. ...
This thesis presents a baseline analysis of blade loading and near-wake aerodynamics for a FOWT under prescribed roll motions. A coupled high-fidelity GPU-based Large-Eddy Simulation code GRASP resolved turbulent wake dynamics, while OpenFAST calculated blade loads. Coupling was achieved via the Filtered Actuator Line Method and the AspFAST application programming interface. The IEA 15MW reference turbine was modeled under steady, uniform inflow, with variations in roll amplitude (5° and 10°), roll frequency (0.03Hz and 0.05Hz), and tip-speed ratio (TSR 7 and TSR 9) in a full factorial test set.
Results show that roll motion leads to asymmetric fluctuations across the rotor plane. Normal forces display strong vertical asymmetry, with greater variations in the upper side of the rotor due to its larger distance from the roll center. A kinematic analysis deriving the variation of tangential velocity both azimuthally and over time supported this finding. Tangential forces exhibit lateral variation, with a left-right asymmetry across the rotor plane, though the magnitude of variation is similar on both sides. Both roll amplitude and frequency increase the magnitude of loading fluctuations, while TSR influences their blade spanwise distribution.
Power Spectral Density analysis reveals that roll introduces spectral content at the roll frequency and at 1P sideband frequencies, the latter arising from modulation of the 1P frequency by roll. Higher roll amplitudes, frequencies, and TSRs amplify these load fluctuations. While the prominence of the 1P frequency is negligible at the blade, it is strong in the near wake along with the roll frequency, 3P frequency, and 3P sidebands.
The unsteady blade loads directly shape the near wake. The stable helical vortex system of a bottom-fixed turbine is replaced by an oscillatory corkscrew structure that breaks down earlier and more chaotically. Increased roll amplitude causes stronger lateral oscillations and fragmented vortices, while higher roll frequency produces shorter wavelength perturbations, accelerating vortex pairing. Higher TSR strengthens the initial vortices and accelerates breakdown. Standard deviation of velocity fields in the wake confirms larger fluctuations at the top of the rotor due to its greater distance from the roll axis.
This study establishes a direct link between roll-induced blade loads and near-wake dynamics, providing a foundation for improved FOWT design, control, and wake modeling. Future work should assess far-wake impacts, the persistence of lateral velocities induced by rotational motion, and inertial effects under highly unsteady roll conditions.
Wake Modelling of a Floating Offshore Wind Turbine
Tuning of a Large Eddy Simulation with an Actuator Line Method for a FOWT with Sinusoidal Surge and Pitch Motion
Quantifying Unsteady Surface Pressure Fluctuations Induced by a Propeller Slipstream Using a Flexible PCB Measurement Device
Quantification of Propeller Wake-Wing Interactions
With the resurgence of interest in propeller-powered aircraft for short-haul and regional missions, understanding the aerodynamic interaction between propellers and nearby surfaces has become increasingly crucial. While propellers offer superior propulsive efficiency and sustainability benefits, their integration introduces complex unsteady flow phenomena that remain insufficiently explored. Additionally, concepts related to regenerative braking and the negative thrust regime aim to harness the full potential of propellers in the pursuit of sustainable aviation. However, the interactions are more complex in the negative thrust regime and need to be accounted for.
This study investigates the unsteady aerodynamic effects of a pusher-propeller operating upstream of a downstream airfoil, with a focus on both positive and negative thrust regimes. A flexible PCB embedded with microphones and pressure sensors was used to capture unsteady surface pressure fluctuations across different operating conditions. The motivation stems from the limited understanding of unsteady surface pressure fluctuations in negative thrust conditions.
The experimental campaign was conducted in two wind tunnel labs: the M-Tunnel and the Small Low-Turbulence Tunnel in the Low-Speed Wind Tunnel Laboratory of Delft University of Technology, Netherlands. The research was carried out in two experimental phases. In the first phase, the device was validated to verify the response of the microphones and the pressure sensors. A known tonal excitation case, along with a case involving an upstream cylinder, was conducted to assess whether the results aligned with theory and expected trends from the literature. These validation experiments confirmed the device’s capability to capture unsteady flow behaviour. However, certain limitations, such as overshoots in measured pressure data and restricted chordwise and spanwise resolution, were encountered. The second phase was conducted in the Small Low-Turbulence Tunnel featuring a fixed airfoil section downstream of a rotating propeller. The device, comprising the microphones and BMP390 pressure sensors, was wrapped around the leading edge of the airfoil to measure pressure fluctuations across the airfoil surface. Initial validation confirmed the reliability of the device in measuring the flow in the propeller slipstream, with good agreement with results from the literature. Comparative analysis was performed across multiple cases, including nacelle-only baselines and propeller-on conditions at two different advance ratios. In the positive thrust regime, the propeller generated a strong tip vortex trace, which significantly influenced the laminar separation bubble and led to elevated pressure fluctuations and peaks at the tonal harmonic of the blade passage frequency. In contrast, the negative thrust regime featured a weaker tip vortex trace and a broadband-dominated spectrum, with reduced suction observed on the upper surface due to lower dynamic pressure in the slipstream.
The study also highlights that the influence of the propeller slipstream extends well beyond its boundary across the span of the airfoil model. Key limitations included discrepancies in the data measured by two rows of microphones due to surface mounting issues.
Overall, the device proved to be a valuable measurement tool for investigating the unsteady surface pressure fluctuations associated with propeller–wing interaction. The insights gained contribute to a better understanding of surface pressure fluctuations on a body immersed in a propeller slipstream, particularly in energy-harvesting operating regimes. Recommendations for future work include improving sensor mounting fidelity, increasing chordwise resolution, and incorporating time-resolved flow visualisation techniques to complement the surface pressure measurements and provide additional insight into the spatial and temporal evolution of the flow field. ...
With the resurgence of interest in propeller-powered aircraft for short-haul and regional missions, understanding the aerodynamic interaction between propellers and nearby surfaces has become increasingly crucial. While propellers offer superior propulsive efficiency and sustainability benefits, their integration introduces complex unsteady flow phenomena that remain insufficiently explored. Additionally, concepts related to regenerative braking and the negative thrust regime aim to harness the full potential of propellers in the pursuit of sustainable aviation. However, the interactions are more complex in the negative thrust regime and need to be accounted for.
This study investigates the unsteady aerodynamic effects of a pusher-propeller operating upstream of a downstream airfoil, with a focus on both positive and negative thrust regimes. A flexible PCB embedded with microphones and pressure sensors was used to capture unsteady surface pressure fluctuations across different operating conditions. The motivation stems from the limited understanding of unsteady surface pressure fluctuations in negative thrust conditions.
The experimental campaign was conducted in two wind tunnel labs: the M-Tunnel and the Small Low-Turbulence Tunnel in the Low-Speed Wind Tunnel Laboratory of Delft University of Technology, Netherlands. The research was carried out in two experimental phases. In the first phase, the device was validated to verify the response of the microphones and the pressure sensors. A known tonal excitation case, along with a case involving an upstream cylinder, was conducted to assess whether the results aligned with theory and expected trends from the literature. These validation experiments confirmed the device’s capability to capture unsteady flow behaviour. However, certain limitations, such as overshoots in measured pressure data and restricted chordwise and spanwise resolution, were encountered. The second phase was conducted in the Small Low-Turbulence Tunnel featuring a fixed airfoil section downstream of a rotating propeller. The device, comprising the microphones and BMP390 pressure sensors, was wrapped around the leading edge of the airfoil to measure pressure fluctuations across the airfoil surface. Initial validation confirmed the reliability of the device in measuring the flow in the propeller slipstream, with good agreement with results from the literature. Comparative analysis was performed across multiple cases, including nacelle-only baselines and propeller-on conditions at two different advance ratios. In the positive thrust regime, the propeller generated a strong tip vortex trace, which significantly influenced the laminar separation bubble and led to elevated pressure fluctuations and peaks at the tonal harmonic of the blade passage frequency. In contrast, the negative thrust regime featured a weaker tip vortex trace and a broadband-dominated spectrum, with reduced suction observed on the upper surface due to lower dynamic pressure in the slipstream.
The study also highlights that the influence of the propeller slipstream extends well beyond its boundary across the span of the airfoil model. Key limitations included discrepancies in the data measured by two rows of microphones due to surface mounting issues.
Overall, the device proved to be a valuable measurement tool for investigating the unsteady surface pressure fluctuations associated with propeller–wing interaction. The insights gained contribute to a better understanding of surface pressure fluctuations on a body immersed in a propeller slipstream, particularly in energy-harvesting operating regimes. Recommendations for future work include improving sensor mounting fidelity, increasing chordwise resolution, and incorporating time-resolved flow visualisation techniques to complement the surface pressure measurements and provide additional insight into the spatial and temporal evolution of the flow field.
Modelling Blade Loads in Industry-Scale Large-Eddy Simulations of Wind Farms
Using an Analytical Body Force Model
This thesis implements an Analytical Body Force Model (ABFM) that estimates blade load distributions from LES data using limited turbine information. Both one-way and two-way coupling strategies are explored. In the one-way approach, the ABFM supplements the AD model to compute blade forces without influencing the LES. In the two-way approach, the ABFM forces are actively fed back into the LES in a feedback loop, replacing the uniform AD model and improving simulation fidelity. ...
This thesis implements an Analytical Body Force Model (ABFM) that estimates blade load distributions from LES data using limited turbine information. Both one-way and two-way coupling strategies are explored. In the one-way approach, the ABFM supplements the AD model to compute blade forces without influencing the LES. In the two-way approach, the ABFM forces are actively fed back into the LES in a feedback loop, replacing the uniform AD model and improving simulation fidelity.
Aerodynamics of wing-integrated ram-air duct for propeller aircraft
A numerical investigation into wing-integrated duct performance and wing-body junction flow
Simulated six degrees of freedom (6DOF) motion and a power law wind field are inserted in a numerical LiDAR model, in which corrected and uncorrected measurement position, direction and line of sight velocity are constructed. The corrected outputs are validated through reconstructed wind fields and the uncertainty of the correction is quantified. In this study, significant motion-induced bias is identified in the reconstructed wind fields. The dominant motion affecting measurement accuracy was identified as pitch motion, especially when it exhibits a non-zero mean. The relative error of the reconstructed power law wind field parameters is reduced by 3 orders of magnitude. Despite an increase in uncertainties associated with the correction method applied, the correction remains effective in reducing the error in LiDAR measurements induced by FOWT motions. The findings highlight the necessity and feasibility of motion correction for LiDAR measurements, offering substantial improvements in the accuracy and reliability of reconstructed wind fields for floating wind turbine applications. ...
Simulated six degrees of freedom (6DOF) motion and a power law wind field are inserted in a numerical LiDAR model, in which corrected and uncorrected measurement position, direction and line of sight velocity are constructed. The corrected outputs are validated through reconstructed wind fields and the uncertainty of the correction is quantified. In this study, significant motion-induced bias is identified in the reconstructed wind fields. The dominant motion affecting measurement accuracy was identified as pitch motion, especially when it exhibits a non-zero mean. The relative error of the reconstructed power law wind field parameters is reduced by 3 orders of magnitude. Despite an increase in uncertainties associated with the correction method applied, the correction remains effective in reducing the error in LiDAR measurements induced by FOWT motions. The findings highlight the necessity and feasibility of motion correction for LiDAR measurements, offering substantial improvements in the accuracy and reliability of reconstructed wind fields for floating wind turbine applications.
Effect of Large scale Turbulence on Propeller Aerodynamic and Aeroacoustic performance
An Experimental Investigation
characteristics, local windspeed variations, etc.. Unlike the well-documented effects of aerial vehicles flying under steady freestream or small-scale turbulence impingement, research on their performance when subjected to large-scale turbulence representative of an urban airspace is relatively scanty. This experimental work aims to generate large scale turbulence in the order of the rotor diameter and analyze its influence on propeller loading and noise emission.
Bluff body shedding from a cylinder is utilized to generate rotor scale turbulence in the inflow, with a variation in upstream cylinder placement tested to quantify the influence of it’s proximity to the propeller. The presence of an upstream obstruction results in severe penalties to the aerodynamic performance and thrust generation compared to an isolated propeller. An increase in rotor scale fluctuations in the inflow leads to an increased intensity of low-frequency loading fluctuations. The highly turbulent inflow has a severe impact on the noise emissions, with an overall increase in the broadband content and retention of discrete tones emitted at BPF (blade passing frequency) harmonics across all tested advance ratios; contrasting drastically with the emission of the isolated propeller. Further, with the cylinder obstruction placed closer to the propeller, the effect of haystacking is observed in the noise emissions, which dominates the high-frequency range and results in a spectrum comprising of purely broadband content above the 2nd
harmonic of the BPF. The findings highlight a strong influence of large-scale turbulence on propeller performance and noise emissions, while emphasizing the requirement for further investigation which isolates and analyzes each underlying effect to obtain a complete understanding of the identified influence. ...
characteristics, local windspeed variations, etc.. Unlike the well-documented effects of aerial vehicles flying under steady freestream or small-scale turbulence impingement, research on their performance when subjected to large-scale turbulence representative of an urban airspace is relatively scanty. This experimental work aims to generate large scale turbulence in the order of the rotor diameter and analyze its influence on propeller loading and noise emission.
Bluff body shedding from a cylinder is utilized to generate rotor scale turbulence in the inflow, with a variation in upstream cylinder placement tested to quantify the influence of it’s proximity to the propeller. The presence of an upstream obstruction results in severe penalties to the aerodynamic performance and thrust generation compared to an isolated propeller. An increase in rotor scale fluctuations in the inflow leads to an increased intensity of low-frequency loading fluctuations. The highly turbulent inflow has a severe impact on the noise emissions, with an overall increase in the broadband content and retention of discrete tones emitted at BPF (blade passing frequency) harmonics across all tested advance ratios; contrasting drastically with the emission of the isolated propeller. Further, with the cylinder obstruction placed closer to the propeller, the effect of haystacking is observed in the noise emissions, which dominates the high-frequency range and results in a spectrum comprising of purely broadband content above the 2nd
harmonic of the BPF. The findings highlight a strong influence of large-scale turbulence on propeller performance and noise emissions, while emphasizing the requirement for further investigation which isolates and analyzes each underlying effect to obtain a complete understanding of the identified influence.
Aerodynamic analysis of a 2D rigid LEI airfoil
An experimental and numerical study
In this study, the centrifugal compressor of a Pratt & Whitney APS5000, as used in the Boeing 787, was reverse engineered using 3D scans of the impeller and diffuser. These geometries were reconstructed and implemented in a CFD model that was validated against a pass-off test measurement. Through a literature study, it was concluded that the main compressor deterioration effects are increases in impeller tip clearance and impeller and diffuser surface roughness. The impact of these effects on compressor efficiency, pressure ratio, and flow capacity was simulated and incorporated into a Gas turbine Simulation Program (GSP) model to assess the resulting APU performance degradation by evaluating changes in Exhaust Gas Temperature (EGT), fuel flow, and compressor pressure ratio.
The results show that increased surface roughness and tip clearance both lead to reductions in compressor efficiency, pressure ratio and flow capacity, which translate into higher exhaust gas temperatures and increased fuel flow at the APU system level. Plotting the reduction in pressure ratio, increase in EGT and increase in fuel flow as a function of compressor efficiency deterioration and flow capacity deterioration, a compressor deterioration map was made. This map is overlaid with simulated points of varying surface roughness and/or tip clearance serving as a decision tool to aid in root cause determination during APU disassembly.
Although the absolute accuracy of the results is limited by assumptions in geometry reconstruction, turbulence modeling, and validation data, the study provides an indication of the relative reduction in APU system performance and demonstrates a working proof of concept in the form of a deterioration map. Therefore, it is concluded that compressor CFD with gas turbine simulation offers a viable approach to assess compressor deterioration effects and their impact on APU performance, thus enhancing APU condition monitoring and supporting root cause determination in a maintenance environment.
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In this study, the centrifugal compressor of a Pratt & Whitney APS5000, as used in the Boeing 787, was reverse engineered using 3D scans of the impeller and diffuser. These geometries were reconstructed and implemented in a CFD model that was validated against a pass-off test measurement. Through a literature study, it was concluded that the main compressor deterioration effects are increases in impeller tip clearance and impeller and diffuser surface roughness. The impact of these effects on compressor efficiency, pressure ratio, and flow capacity was simulated and incorporated into a Gas turbine Simulation Program (GSP) model to assess the resulting APU performance degradation by evaluating changes in Exhaust Gas Temperature (EGT), fuel flow, and compressor pressure ratio.
The results show that increased surface roughness and tip clearance both lead to reductions in compressor efficiency, pressure ratio and flow capacity, which translate into higher exhaust gas temperatures and increased fuel flow at the APU system level. Plotting the reduction in pressure ratio, increase in EGT and increase in fuel flow as a function of compressor efficiency deterioration and flow capacity deterioration, a compressor deterioration map was made. This map is overlaid with simulated points of varying surface roughness and/or tip clearance serving as a decision tool to aid in root cause determination during APU disassembly.
Although the absolute accuracy of the results is limited by assumptions in geometry reconstruction, turbulence modeling, and validation data, the study provides an indication of the relative reduction in APU system performance and demonstrates a working proof of concept in the form of a deterioration map. Therefore, it is concluded that compressor CFD with gas turbine simulation offers a viable approach to assess compressor deterioration effects and their impact on APU performance, thus enhancing APU condition monitoring and supporting root cause determination in a maintenance environment.