D. Ragni
Please Note
52 records found
1
1. How does turbulence distortion affect noise generation and prediction?
2. How can turbulence-distortion effects be included in Amiet’s model?
3. How does this apply to rotors?
...
1. How does turbulence distortion affect noise generation and prediction?
2. How can turbulence-distortion effects be included in Amiet’s model?
3. How does this apply to rotors?
Aeroacoustic Investigation of Propellers Operating at Low-Reynolds Numbers
Study of conventional and unconventional configurations
Undoubtedly, the noise generated by their unique propeller-driven propulsion systems poses a significant public health concern. Operating at low altitudes throughout their missions and producing an acoustic signature characterized by strong tonal noise and prominent high-frequency components, these vehicles are expected to have a greater impact on communities than traditional aircraft.... ...
Undoubtedly, the noise generated by their unique propeller-driven propulsion systems poses a significant public health concern. Operating at low altitudes throughout their missions and producing an acoustic signature characterized by strong tonal noise and prominent high-frequency components, these vehicles are expected to have a greater impact on communities than traditional aircraft....
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.
The framework integrates established analytical and semi-empirical aeroacoustic models with aerodynamic data based on derived geometry and detailed flight information. It models all major noise sources from the airborne components, such as the Leading Edge Inflatable (LEI) kite, bridle lines, tether, and onboard ram-air turbine. The most significant contributions to the overall noise signature were found to be turbulent boundary layer trailing edge (TBL-TE) noise from airfoils, modeled using the Brooks–Pope–Marcolini (BPM) approach, vortex-shedding noise from cylindrical structures such as the tether and bridle lines, and tonal harmonics produced by the rotating turbine blades, captured through Hanson’s helicoidal surface theory.
To generate aerodynamic input, spanwise airfoil profiles were automatically extracted from 3D CAD models and analyzed through XFOIL. Real-time flight data was provided by an onboard sensor suite and processed through an Extended Kalman Filter (EKF), allowing dynamic simulation of flight conditions. Audio recordings were collected during test flights using GoPro cameras, enabling experimental validation of the acoustic predictions despite the absence of calibrated SPL measurements.
Validation showed strong agreement between predicted and measured spectra up to 5 kHz, particularly for turbine harmonics and general spectral shape. Deviations in the lower tonal harmonics were primarily attributed to acoustic shielding caused by the turbine’s duct structure. Additionally, the use of GoPro cameras introduced limitations due to their lack of calibration data and the presence of internal low-pass filtering above 5 kHz. Despite these constraints, the model successfully predicted tonal peaks, including the blade passing frequency and higher-order harmonics, aligning well with the experimental observations.
Additionally, the framework investigates the influence of the propagation effects, such as atmospheric absorption and geometric spreading, and integrates them to produce realistic observer-based predictions. Despite using non-professional audio hardware, the predictions captured key features including harmonic roll-off and broadband trends, affirming the framework's validity for early-stage design and evaluation.
This work demonstrates that low-order, physics-based models paired with aerodynamic inputs and synchronized flight data can yield meaningful acoustic predictions for AWES. The framework offers modularity, computational efficiency, and adaptability for future upgrades, such as the use of calibrated microphones or high-fidelity CFD data. It serves as a foundation for future extensions in auralization, psychoacoustic testing, and component-level noise reduction strategies.
Ultimately, the thesis bridges theoretical modeling with field-based validation, supporting the responsible integration of AWES technologies into noise-sensitive environments. ...
The framework integrates established analytical and semi-empirical aeroacoustic models with aerodynamic data based on derived geometry and detailed flight information. It models all major noise sources from the airborne components, such as the Leading Edge Inflatable (LEI) kite, bridle lines, tether, and onboard ram-air turbine. The most significant contributions to the overall noise signature were found to be turbulent boundary layer trailing edge (TBL-TE) noise from airfoils, modeled using the Brooks–Pope–Marcolini (BPM) approach, vortex-shedding noise from cylindrical structures such as the tether and bridle lines, and tonal harmonics produced by the rotating turbine blades, captured through Hanson’s helicoidal surface theory.
To generate aerodynamic input, spanwise airfoil profiles were automatically extracted from 3D CAD models and analyzed through XFOIL. Real-time flight data was provided by an onboard sensor suite and processed through an Extended Kalman Filter (EKF), allowing dynamic simulation of flight conditions. Audio recordings were collected during test flights using GoPro cameras, enabling experimental validation of the acoustic predictions despite the absence of calibrated SPL measurements.
Validation showed strong agreement between predicted and measured spectra up to 5 kHz, particularly for turbine harmonics and general spectral shape. Deviations in the lower tonal harmonics were primarily attributed to acoustic shielding caused by the turbine’s duct structure. Additionally, the use of GoPro cameras introduced limitations due to their lack of calibration data and the presence of internal low-pass filtering above 5 kHz. Despite these constraints, the model successfully predicted tonal peaks, including the blade passing frequency and higher-order harmonics, aligning well with the experimental observations.
Additionally, the framework investigates the influence of the propagation effects, such as atmospheric absorption and geometric spreading, and integrates them to produce realistic observer-based predictions. Despite using non-professional audio hardware, the predictions captured key features including harmonic roll-off and broadband trends, affirming the framework's validity for early-stage design and evaluation.
This work demonstrates that low-order, physics-based models paired with aerodynamic inputs and synchronized flight data can yield meaningful acoustic predictions for AWES. The framework offers modularity, computational efficiency, and adaptability for future upgrades, such as the use of calibrated microphones or high-fidelity CFD data. It serves as a foundation for future extensions in auralization, psychoacoustic testing, and component-level noise reduction strategies.
Ultimately, the thesis bridges theoretical modeling with field-based validation, supporting the responsible integration of AWES technologies into noise-sensitive environments.
Aeroacoustic testing in acoustically disturbed environments
Improvements to closed test section wind tunnel experiments
The investigation of wall cavities for microphone placement was done with Computational Fluid Dynamics simulations, which in turn were validated experimentally. Cavities covered with a mesh cover were investigated, since previous literature shows that these reduce hydrodynamic noise while allowing for the transmission of waves to the microphones. The numerical simulations show that covering microphone cavities with a mesh cover results in a stagnant flow inside the cavities. As consequence, the only source of pressure fluctuations at the cavity bottoms are acoustic waves. The hydrodynamic pressure fluctuations from the wall’s boundary layer still propagate acoustically to the cavity bottoms. The findings show that increasing cavity size, by increasing the cavity opening diameter with respect to the length of the eddies in the turbulent boundary layer, leads to a lower propagation of spurious pressure fluctuations to the cavity bottoms. This in turn leads to an increased signal to noise ratio of acoustic measurements recorded at closed test section wind tunnels.
Wind tunnel wall liners have been characterized based on their viscous resistivity, inertial resistivity and roughness. Several porous liners have been tested experimentally. The aim was to analyze their impact on the aerodynamic properties of the wind tunnel boundary layer, on the generation of spurious noise, and on the absorption of acoustic reflections. The results show that the ideal choice of liner consists of a liner: with high viscous resistivity, which leads to high acoustic absorption; with low roughness, to reduce the impact on the wind tunnel wall’s boundary layer; and with low inertial resistivity, to reduce the generation of spurious noise. The best lining material tested was melamine foam.
The acoustic propagation and acoustic interference in a closed wind tunnel test section were predicted with a FEM acoustic solver. The propagation was modelled on a baseline test section, with fully reflective walls, and on test sections with lined walls. The numerical results were found to give a very accurate prediction of the acoustic experimental tests. It was possible to use the numerical results to improve the post—processing of experimental data. The Green’s function used to process experimental microphone data with beamforming was corrected, using the numerical results. Beamforming with the Green’s function corrected for the acoustically disturbed environment led to a higher beamforming spatial resolution. In addition, the estimated noise levels are more accurate when the correction is used. This improved approach was shown to work for post—processing experimental measurements of a monopole sound source placed at the center of the test section, with and without free—stream flow.
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The investigation of wall cavities for microphone placement was done with Computational Fluid Dynamics simulations, which in turn were validated experimentally. Cavities covered with a mesh cover were investigated, since previous literature shows that these reduce hydrodynamic noise while allowing for the transmission of waves to the microphones. The numerical simulations show that covering microphone cavities with a mesh cover results in a stagnant flow inside the cavities. As consequence, the only source of pressure fluctuations at the cavity bottoms are acoustic waves. The hydrodynamic pressure fluctuations from the wall’s boundary layer still propagate acoustically to the cavity bottoms. The findings show that increasing cavity size, by increasing the cavity opening diameter with respect to the length of the eddies in the turbulent boundary layer, leads to a lower propagation of spurious pressure fluctuations to the cavity bottoms. This in turn leads to an increased signal to noise ratio of acoustic measurements recorded at closed test section wind tunnels.
Wind tunnel wall liners have been characterized based on their viscous resistivity, inertial resistivity and roughness. Several porous liners have been tested experimentally. The aim was to analyze their impact on the aerodynamic properties of the wind tunnel boundary layer, on the generation of spurious noise, and on the absorption of acoustic reflections. The results show that the ideal choice of liner consists of a liner: with high viscous resistivity, which leads to high acoustic absorption; with low roughness, to reduce the impact on the wind tunnel wall’s boundary layer; and with low inertial resistivity, to reduce the generation of spurious noise. The best lining material tested was melamine foam.
The acoustic propagation and acoustic interference in a closed wind tunnel test section were predicted with a FEM acoustic solver. The propagation was modelled on a baseline test section, with fully reflective walls, and on test sections with lined walls. The numerical results were found to give a very accurate prediction of the acoustic experimental tests. It was possible to use the numerical results to improve the post—processing of experimental data. The Green’s function used to process experimental microphone data with beamforming was corrected, using the numerical results. Beamforming with the Green’s function corrected for the acoustically disturbed environment led to a higher beamforming spatial resolution. In addition, the estimated noise levels are more accurate when the correction is used. This improved approach was shown to work for post—processing experimental measurements of a monopole sound source placed at the center of the test section, with and without free—stream flow.
Aerodynamics and Aeroacoustics of Propeller Operation at Negative Thrust
A Computational Study
Despite these potential advantages, the aerodynamic and aeroacoustic characteristics of propellers operating in negative thrust mode remain largely unexplored. This dissertation addresses this knowledge gap through computational analysis, comparing the performance of isolated propeller configurations in negative thrust mode with the well-understood positive thrust mode. The results reveal that the distinct aeroacoustic characteristics of propellers operating in negative thrust conditions, compared to conventional positive thrust conditions, offer a promising avenue for reducing community noise, not only through the possibility of steeper descents but also through changes in the noise emissions from the propeller itself.
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Despite these potential advantages, the aerodynamic and aeroacoustic characteristics of propellers operating in negative thrust mode remain largely unexplored. This dissertation addresses this knowledge gap through computational analysis, comparing the performance of isolated propeller configurations in negative thrust mode with the well-understood positive thrust mode. The results reveal that the distinct aeroacoustic characteristics of propellers operating in negative thrust conditions, compared to conventional positive thrust conditions, offer a promising avenue for reducing community noise, not only through the possibility of steeper descents but also through changes in the noise emissions from the propeller itself.
Interactions of Multi-Rotors with Surfaces
Aerodynamic Characterization and Performance Modelling
The high power-to-weight ratio and efficiency of electric motors provide an excellent platform to explore disruptive propulsion system configurations. An observable design trend here is the tight integration of distributed, fixed-pitched rotors with aerodynamic surfaces, aimed at generating beneficial aerodynamic coupling effects to increase the aircraft’s efficiency and reduce acoustic emissions.
An auspicious integrated tilt-wing propulsion system layout is known as Over-The-Wing propulsion, which promises favorable aerodynamic effects by the rotor-induced flow and reduced noise signature during fly-over by shielding. However, during the operation of Over-The-Wing propulsion in eVTOL flight conditions, several multi-rotor-surface interactions are encountered, resulting in unexplored aerodynamic and aeroacoustic effects. As a consequence, design guidelines to maximize aerodynamic performance and minimize noise signature for Over-The-Wing propulsion for eVTOL flight conditions are missing in the public domain. This thesis focuses on enabling Over-The-Wing propulsion for vertical flight through experimentation and low-order modeling of the fundamental aerodynamic interactions between distributed rotors and surfaces. ...
The high power-to-weight ratio and efficiency of electric motors provide an excellent platform to explore disruptive propulsion system configurations. An observable design trend here is the tight integration of distributed, fixed-pitched rotors with aerodynamic surfaces, aimed at generating beneficial aerodynamic coupling effects to increase the aircraft’s efficiency and reduce acoustic emissions.
An auspicious integrated tilt-wing propulsion system layout is known as Over-The-Wing propulsion, which promises favorable aerodynamic effects by the rotor-induced flow and reduced noise signature during fly-over by shielding. However, during the operation of Over-The-Wing propulsion in eVTOL flight conditions, several multi-rotor-surface interactions are encountered, resulting in unexplored aerodynamic and aeroacoustic effects. As a consequence, design guidelines to maximize aerodynamic performance and minimize noise signature for Over-The-Wing propulsion for eVTOL flight conditions are missing in the public domain. This thesis focuses on enabling Over-The-Wing propulsion for vertical flight through experimentation and low-order modeling of the fundamental aerodynamic interactions between distributed rotors and surfaces.
Design of Synthetic Jet Actuators for Jet Noise Control
Towards Aircraft Noise Reduction
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The research set-up was designed for open-jet numerical simulations using the commercial Lattice Boltzmann Method (LBM) based CFD solver PowerFLOW, with future compatibility for experimental open-jet wind tunnel validation studies at the TU Delft's Anechoic wind tunnel. Three variations of a two-sideplate research set-up were created based on a slat-and-main-wing modified 30P30N airfoil cross-section. A `No Gap' (NG) geometry that connects the slat to both sideplates; a `No Horn & Step Stump' (NH) geometry that has a simplified slat side-edge and slat stump, a feature that blends the main wing with the fuselage; and a `Horn & Smooth Stump' (H) geometry, which incorporates a slat horn on the slat side-edge and a slat stump modelled after the Airbus A320. For all three variations, the relative positions of the slat track, slat side-edge and other junction surfaces were modelled after the Airbus A320 as well. All model variants were analysed based on their far-field noise radiation and the near-field behaviour of aerodynamic turbulent structures.
The results of the simulated scaled models were compared to literature. The noise radiation of the `H' model was scaled in power and frequency (Strouhal-based), and compared to beamforming integration flyover data of a junction of an Airbus A320. The model shows good spectral resemblance for higher frequencies, with larger discrepancies at lower frequencies. The low-frequency discrepancies were attributed to beamforming limitations stemming from Rayleigh's criterion, as well as a likely over-prediction of lower frequency noise by the scaled `H' set-up. Comparison to full-scale Reynolds number tests on a model Airbus A320 revealed the slope of the scaled noise spectrum resembled the slope of the slat noise of the Airbus A320 at full Reynolds number both at low and high frequencies.
Contrary to earlier research, the set-up without a sideplate-slat gap, `NG', produced excess noise compared to the `Gap'-models, `NH' and `H'. The excess noise is attributed to a larger spanwise extent of the slat narrow-band peak noise mechanism. The narrow-band peaks stem from a slat-cusp-to-slat-trailing-edge flow-acoustic resonance. The introduction of a side-edge (for the `NH' and `H' models) increases the spanwise velocity in the slat cove and creates a slat cove wake that gets accelerated over the slat track. This study showed that the altered slat cove wake shape prevents the canonical slat-cusp-to-slat-trailing-edge flow impingement from occurring on part of the slat, thus limiting the extent of the resonance mechanism. This phenomenon was portrayed by visualising the slat cove wake through total pressure isosurfaces and visualising the narrow-band peak noise source regions through a Ffowcs-Williams and Hawkings (FWH)-based source visualisation technique. A lack of loading on the slat (which is a property of the non-modified 30P30N cross-section as well) is hypothesised as the reason why the introduction of a slat side-edge does not increase the noise radiation for the models with a slat side-edge (`NH', and `H'). ...
The research set-up was designed for open-jet numerical simulations using the commercial Lattice Boltzmann Method (LBM) based CFD solver PowerFLOW, with future compatibility for experimental open-jet wind tunnel validation studies at the TU Delft's Anechoic wind tunnel. Three variations of a two-sideplate research set-up were created based on a slat-and-main-wing modified 30P30N airfoil cross-section. A `No Gap' (NG) geometry that connects the slat to both sideplates; a `No Horn & Step Stump' (NH) geometry that has a simplified slat side-edge and slat stump, a feature that blends the main wing with the fuselage; and a `Horn & Smooth Stump' (H) geometry, which incorporates a slat horn on the slat side-edge and a slat stump modelled after the Airbus A320. For all three variations, the relative positions of the slat track, slat side-edge and other junction surfaces were modelled after the Airbus A320 as well. All model variants were analysed based on their far-field noise radiation and the near-field behaviour of aerodynamic turbulent structures.
The results of the simulated scaled models were compared to literature. The noise radiation of the `H' model was scaled in power and frequency (Strouhal-based), and compared to beamforming integration flyover data of a junction of an Airbus A320. The model shows good spectral resemblance for higher frequencies, with larger discrepancies at lower frequencies. The low-frequency discrepancies were attributed to beamforming limitations stemming from Rayleigh's criterion, as well as a likely over-prediction of lower frequency noise by the scaled `H' set-up. Comparison to full-scale Reynolds number tests on a model Airbus A320 revealed the slope of the scaled noise spectrum resembled the slope of the slat noise of the Airbus A320 at full Reynolds number both at low and high frequencies.
Contrary to earlier research, the set-up without a sideplate-slat gap, `NG', produced excess noise compared to the `Gap'-models, `NH' and `H'. The excess noise is attributed to a larger spanwise extent of the slat narrow-band peak noise mechanism. The narrow-band peaks stem from a slat-cusp-to-slat-trailing-edge flow-acoustic resonance. The introduction of a side-edge (for the `NH' and `H' models) increases the spanwise velocity in the slat cove and creates a slat cove wake that gets accelerated over the slat track. This study showed that the altered slat cove wake shape prevents the canonical slat-cusp-to-slat-trailing-edge flow impingement from occurring on part of the slat, thus limiting the extent of the resonance mechanism. This phenomenon was portrayed by visualising the slat cove wake through total pressure isosurfaces and visualising the narrow-band peak noise source regions through a Ffowcs-Williams and Hawkings (FWH)-based source visualisation technique. A lack of loading on the slat (which is a property of the non-modified 30P30N cross-section as well) is hypothesised as the reason why the introduction of a slat side-edge does not increase the noise radiation for the models with a slat side-edge (`NH', and `H').
The electrification of passenger vehicles comes with benefits like a smoother driving experience, requiring less maintenance, and has led to an overall noise decrease. However, annoying noises that were previously masked by loud engines are now audible. Automotive cooling fan noise is such an example. The tonal character of the fan is annoying to pedestrians and residents, especially during car charging. The batteries reach high temperatures while charging, increasing the cooling demand from the fan module compared to conventional cars. In this situation, no inflow is generated from driving and the fan is operating at high rotational velocities and pressure requirements.
When the (axial) inflow to the fan is non-uniform, (the velocity changes over the circumference), a varying force is generated on the fan blade, when it rotates. When this non-uniformity is stationary (constant in time), these force fluctuations are periodic, and this is the main cause of the tonal noise. The non-uniformities in fan modules arise from inflow distortions, like for example heat exchanger, duct bends, or the shape of the shroud.
In current fan modules, unequal blade spacing is used to reduce the annoyance of these tones. This reduces the noise at the Blade Pass Frequency, but introduces tones at other harmonics of the rotational frequency, overall mainly leading to a reduction in noise annoyance.
Flow obstructions have been shown an effective means of reducing noise in equally spaced axial fans with low Mach number, while minimizing aerodynamic losses. They introduce a secondary non-uniformity in the inflow, which creates a secondary aeroacoustic source on the fan blade. When placed at the correct circumferential angle, cancellation between the primary and secondary source is possible. This research investigates if such flow obstructions can still yield adequate noise reduction on unequally spaced fans, and if (multiple) upstream heat exchangers prohibit the working mechanism of flow obstructions.
It was found that flow obstructions can indeed significantly reduce tonal noise at the fan BPF, by up to 13 dB on the fan axis, and 6dB at an angle 45\degree from the axis. The upstream radiator and condenser did not compromise this reduction, and the obstruction still reduces noise when the fan operates at a lower rotational velocity. Using a superposition of obstructions (creating a multi-modal obstruction) could also control multiple tones. However, with the large number of tones to be controlled in an unequally spaced fan, the overall sound pressure attenuation and annoyance reduction are insignificant.
Furthermore, the low-fidelity analytical tool developed in the thesis was an effective means of rapid obstruction design and optimization. Although information on the fan's primary noise is needed, as well as some parameters to define the obstruction wake (which can be obtained with cheaper, RANS simulations), the model correlated well with simulation data obtained in PowerFLOW. ...
The electrification of passenger vehicles comes with benefits like a smoother driving experience, requiring less maintenance, and has led to an overall noise decrease. However, annoying noises that were previously masked by loud engines are now audible. Automotive cooling fan noise is such an example. The tonal character of the fan is annoying to pedestrians and residents, especially during car charging. The batteries reach high temperatures while charging, increasing the cooling demand from the fan module compared to conventional cars. In this situation, no inflow is generated from driving and the fan is operating at high rotational velocities and pressure requirements.
When the (axial) inflow to the fan is non-uniform, (the velocity changes over the circumference), a varying force is generated on the fan blade, when it rotates. When this non-uniformity is stationary (constant in time), these force fluctuations are periodic, and this is the main cause of the tonal noise. The non-uniformities in fan modules arise from inflow distortions, like for example heat exchanger, duct bends, or the shape of the shroud.
In current fan modules, unequal blade spacing is used to reduce the annoyance of these tones. This reduces the noise at the Blade Pass Frequency, but introduces tones at other harmonics of the rotational frequency, overall mainly leading to a reduction in noise annoyance.
Flow obstructions have been shown an effective means of reducing noise in equally spaced axial fans with low Mach number, while minimizing aerodynamic losses. They introduce a secondary non-uniformity in the inflow, which creates a secondary aeroacoustic source on the fan blade. When placed at the correct circumferential angle, cancellation between the primary and secondary source is possible. This research investigates if such flow obstructions can still yield adequate noise reduction on unequally spaced fans, and if (multiple) upstream heat exchangers prohibit the working mechanism of flow obstructions.
It was found that flow obstructions can indeed significantly reduce tonal noise at the fan BPF, by up to 13 dB on the fan axis, and 6dB at an angle 45\degree from the axis. The upstream radiator and condenser did not compromise this reduction, and the obstruction still reduces noise when the fan operates at a lower rotational velocity. Using a superposition of obstructions (creating a multi-modal obstruction) could also control multiple tones. However, with the large number of tones to be controlled in an unequally spaced fan, the overall sound pressure attenuation and annoyance reduction are insignificant.
Furthermore, the low-fidelity analytical tool developed in the thesis was an effective means of rapid obstruction design and optimization. Although information on the fan's primary noise is needed, as well as some parameters to define the obstruction wake (which can be obtained with cheaper, RANS simulations), the model correlated well with simulation data obtained in PowerFLOW.
Turbulent boundary layer trailing edge noise reduction by using a perforated add-on
A Lattice bolzmann approach
Turbulent boundary layer trailing edge noise is becoming an increasingly important problem in wind turbine applications. The wind turbine rotor diameter is expected to keep growing bigger in the future and trailing edge noise is known to scale with the relative rotor tip velocity to the power 5-6. One effective and yet relatively novel method to reduce this type of noise is the addition of perforated add-on devices to the rear end of the rotor blades. The perforated add-ons have been extensively tested experimentally in recent years. The experimental studies have been instrumental in developing design rules but currently, the precise mechanisms behind this noise reduction are not yet fully understood. The project objective is to obtain insights into the aero-acoustic flow physics responsible for the far-field noise reduction for perforated add-on trailing edge noise problems. To accomplish this, the first high-fidelity numerical LBM study in which the geometry of the per- forations is fully resolved is performed. The simulation is performed with the commercial Lattice Boltzmann method-based solver, PowerFLOW. A scaled 2.5D airfoil simulation is performed with an inflow of 20 [m/s] in lifting conditions. Three different airfoil add-on configurations are simulated. One baseline, one with a homogenous perforation spacing, and one geometry where this spacing is decreasing in the downstream direction. The simulation results are validated against experiments and a noise reduction of about 3 − 4 [dB] is found for in the lower frequency range Stc < 10. A distribution of sound sources was found over the add-on for all frequencies. The frequencies up to Stc = 10 show signs of destructive acoustic interference contributing to the observed noise reduction. Besides this phenomenon, two additional mechanisms were identified as contributing to the observed noise reduction. The second is the milder ∆p jump at the trailing edge caused by communicating boundary layers on both sides of the add-on. A good indication of this milder pressure jump is the correlation coefficient Rpp between two points on opposite sides of the add-on close to the edge. No development or growth of the zone of the correlation coefficient was found over the add-on except for the vicinity close to the trailing edge. A mean vertical upward flow is observed, flowing out of and extending above the perforations. This is believed to be relevant for the achieved noise reduction. The effect possibly has simultaneous positive and negative conflicting contributions to noise reduction. Lastly, it was concluded that the spectra of the homogeneous and linear perforated geometries showed too much similarity, therefore it was difficult to couple discrepancies in the near-field between the two cases to observations of the far-field spectra. ...
Turbulent boundary layer trailing edge noise is becoming an increasingly important problem in wind turbine applications. The wind turbine rotor diameter is expected to keep growing bigger in the future and trailing edge noise is known to scale with the relative rotor tip velocity to the power 5-6. One effective and yet relatively novel method to reduce this type of noise is the addition of perforated add-on devices to the rear end of the rotor blades. The perforated add-ons have been extensively tested experimentally in recent years. The experimental studies have been instrumental in developing design rules but currently, the precise mechanisms behind this noise reduction are not yet fully understood. The project objective is to obtain insights into the aero-acoustic flow physics responsible for the far-field noise reduction for perforated add-on trailing edge noise problems. To accomplish this, the first high-fidelity numerical LBM study in which the geometry of the per- forations is fully resolved is performed. The simulation is performed with the commercial Lattice Boltzmann method-based solver, PowerFLOW. A scaled 2.5D airfoil simulation is performed with an inflow of 20 [m/s] in lifting conditions. Three different airfoil add-on configurations are simulated. One baseline, one with a homogenous perforation spacing, and one geometry where this spacing is decreasing in the downstream direction. The simulation results are validated against experiments and a noise reduction of about 3 − 4 [dB] is found for in the lower frequency range Stc < 10. A distribution of sound sources was found over the add-on for all frequencies. The frequencies up to Stc = 10 show signs of destructive acoustic interference contributing to the observed noise reduction. Besides this phenomenon, two additional mechanisms were identified as contributing to the observed noise reduction. The second is the milder ∆p jump at the trailing edge caused by communicating boundary layers on both sides of the add-on. A good indication of this milder pressure jump is the correlation coefficient Rpp between two points on opposite sides of the add-on close to the edge. No development or growth of the zone of the correlation coefficient was found over the add-on except for the vicinity close to the trailing edge. A mean vertical upward flow is observed, flowing out of and extending above the perforations. This is believed to be relevant for the achieved noise reduction. The effect possibly has simultaneous positive and negative conflicting contributions to noise reduction. Lastly, it was concluded that the spectra of the homogeneous and linear perforated geometries showed too much similarity, therefore it was difficult to couple discrepancies in the near-field between the two cases to observations of the far-field spectra.
The performance of established dynamic stall models such as the one developed by Pierce and the current General Electric dynamic stall model (GE2021) was assessed in reverse flow conditions. In addition, improvements to the GE2021 model were proposed to enhance its performance, including a delay in the effective angle of attack as a function of the reduced frequency and the addition of vortex effects in the load calculation. Three options for the inclusion of vortex effects were explored. The first used the formulation of vortex effects developed by Pierce, which, being very similar to those proposed in the original Beddoes-Leishman model, allows assessment of the performance of the latter for reverse flow dynamic stall. The second focused on the interpretation proposed by Sheng, Galbraith, and Coton of the vortex effects calculation formulated by Beddoes. The last consisted of a simplification of the sinusoidal vortex effects computation of the second approach. In addition, study and tuning of the variables and coefficients involved in this calculation were developed in order to provide a versatile model with the ability to provide reliable results in both forward and reverse flow conditions.
This project aims to be a first step in the study of reverse flow modelling and to improve our understanding of its modelling requirements. ...
The performance of established dynamic stall models such as the one developed by Pierce and the current General Electric dynamic stall model (GE2021) was assessed in reverse flow conditions. In addition, improvements to the GE2021 model were proposed to enhance its performance, including a delay in the effective angle of attack as a function of the reduced frequency and the addition of vortex effects in the load calculation. Three options for the inclusion of vortex effects were explored. The first used the formulation of vortex effects developed by Pierce, which, being very similar to those proposed in the original Beddoes-Leishman model, allows assessment of the performance of the latter for reverse flow dynamic stall. The second focused on the interpretation proposed by Sheng, Galbraith, and Coton of the vortex effects calculation formulated by Beddoes. The last consisted of a simplification of the sinusoidal vortex effects computation of the second approach. In addition, study and tuning of the variables and coefficients involved in this calculation were developed in order to provide a versatile model with the ability to provide reliable results in both forward and reverse flow conditions.
This project aims to be a first step in the study of reverse flow modelling and to improve our understanding of its modelling requirements.
The analysis of the fixed-wing kite revealed prominent peaks around 1500 Hz and 2000 Hz in the noise spectra, with the higher frequency peak observed at higher kite velocities. Analytical predictions indicated laminar boundary layer vortex shedding and tether vortex shedding as the main noise sources. The study also investigated the directivity of the turbulent boundary layer trailing edge noise, which revealed dipoles that exhibited slight deformations at higher frequencies.
For the LEI kite, noise analysis identified peaks in the sound pressure level around 300-400 Hz and 1000-2000 Hz. Analytical predictions highlighted turbulent boundary layer trailing edge noise and vortex shedding from the tether and bridle lines as the dominant noise sources.
By considering the implications of these findings, the noise impact of airborne wind energy systems can be minimized, fostering their sustainable deployment and acceptance. ...
The analysis of the fixed-wing kite revealed prominent peaks around 1500 Hz and 2000 Hz in the noise spectra, with the higher frequency peak observed at higher kite velocities. Analytical predictions indicated laminar boundary layer vortex shedding and tether vortex shedding as the main noise sources. The study also investigated the directivity of the turbulent boundary layer trailing edge noise, which revealed dipoles that exhibited slight deformations at higher frequencies.
For the LEI kite, noise analysis identified peaks in the sound pressure level around 300-400 Hz and 1000-2000 Hz. Analytical predictions highlighted turbulent boundary layer trailing edge noise and vortex shedding from the tether and bridle lines as the dominant noise sources.
By considering the implications of these findings, the noise impact of airborne wind energy systems can be minimized, fostering their sustainable deployment and acceptance.
Study of high aspect-ratio dual intersecting jets and the installation effect on control authority
An experimental and numerical investigation
The intersecting twin jet has recently captured significant attention from the Aerothermal team for several reasons. Firstly, it provides the ability to actively control the flow angle from the HVAC unit into the vehicle cabin without requiring direct interaction with the vent. Additionally, it facilitates the flushing of the vent outlets with the A-class surfaces in the vehicle interior, helps achieve a simple and minimalist design for the instrument panel and other interior surfaces that align with Tesla's design language
The objective pursued in this thesis is to investigate the physics represented by the bulk flow characteristics of intersecting twin jets, and to scrutinize the installation effect on the merging jet, focusing on the influence of the installation surface offset height. This objective is achieved by characterizing the evolution of large-scale flow structures in High AR intersecting twin jets at moderate Reynolds numbers experimentally using planar Particle Image Velocimetry (PIV) in both installed and uninstalled conditions. Once accomplished, the experimental results are then used to help select, validate, and calibrate the appropriate RANS turbulence model.
The experimental results show that the intersecting jets converge before merging and forming a single jet. This jet behaves like a single jet emanating from a more recessed origin. The variation of the flow ratio between the two nozzle outlets results in varying the jet angle. The study reveals that the placement of the surface impacts the jet angle and velocity and introduces a circulation zone that affects the jet's behavior and direction. The surface's impact depends on the offset distance, length, and profile of the surface. The results also suggest that accurate computational prediction of the jet characteristics requires high mesh resolution and an appropriate selection of turbulence intensity. Among the four turbulence models assessed, the k-omega SST model is found to be adequate for the application, although it exhibits some numerical hysteresis. Overall, the findings provide insights into the dynamics of jet-surface interactions and can guide the design of systems involving such flows.
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The intersecting twin jet has recently captured significant attention from the Aerothermal team for several reasons. Firstly, it provides the ability to actively control the flow angle from the HVAC unit into the vehicle cabin without requiring direct interaction with the vent. Additionally, it facilitates the flushing of the vent outlets with the A-class surfaces in the vehicle interior, helps achieve a simple and minimalist design for the instrument panel and other interior surfaces that align with Tesla's design language
The objective pursued in this thesis is to investigate the physics represented by the bulk flow characteristics of intersecting twin jets, and to scrutinize the installation effect on the merging jet, focusing on the influence of the installation surface offset height. This objective is achieved by characterizing the evolution of large-scale flow structures in High AR intersecting twin jets at moderate Reynolds numbers experimentally using planar Particle Image Velocimetry (PIV) in both installed and uninstalled conditions. Once accomplished, the experimental results are then used to help select, validate, and calibrate the appropriate RANS turbulence model.
The experimental results show that the intersecting jets converge before merging and forming a single jet. This jet behaves like a single jet emanating from a more recessed origin. The variation of the flow ratio between the two nozzle outlets results in varying the jet angle. The study reveals that the placement of the surface impacts the jet angle and velocity and introduces a circulation zone that affects the jet's behavior and direction. The surface's impact depends on the offset distance, length, and profile of the surface. The results also suggest that accurate computational prediction of the jet characteristics requires high mesh resolution and an appropriate selection of turbulence intensity. Among the four turbulence models assessed, the k-omega SST model is found to be adequate for the application, although it exhibits some numerical hysteresis. Overall, the findings provide insights into the dynamics of jet-surface interactions and can guide the design of systems involving such flows.
Airline collaboration and Environmental impact
Airline Collaborative Network Planning to mitigate Environmental Impact