I. Langella
Please Note
21 records found
1
As with any technology, challenges remain. Whilst combustion modelling using Computational Fluid Dynamics (CFD) is not a solved problem to begin with, hydrogen combustion is made more complex by differential diffusion. This occurs when different species do not diffuse at the same rate. Hydrogen tends to diffuse faster than other species, causing local changes in mixture fraction, in addition to super-adiabatic temperatures and super-equilibrium product concentrations. This effect is stronger in strained or curved flames. Flame strain and curvature also influences the local reaction rate. These phenomena occur on a very small length and time scale. To simulate this directly, very fine meshes and very precise transport equations for each species are required. This can be prohibitively expensive for large scale designs or for design iteration.
In cases where simulating this behaviour directly is not possible, an alternative model is required. In this paper, five variants of such a model are assessed. These models are based on the assumption that the flame can be approximated as an ensemble of 1-dimensional flamelets. These flamelets can be analysed before the CFD simulations are performed. The results are then parametrized by a number of control variables, using a presumed filtered probability density function which aims to include sub-grid scale effects. By changing the flamelet conditions and control variable definition, different manifolds can be generated. In this paper, a number of these Flamelet-Generated Manifolds (FGMs) are compared to a higher fidelity model (using an Eulerian Stochastic Fields (ESF) approach). These FGMs use the mixture fraction, the progress variable and their sub-grid variances as control variables. Five different FGMs are tested, characterized by the progress variable definition (water vs hydrogen mass fraction) and flamelet strain rate (0 (unstrained) vs 3000 vs 6000 vs 13000 s^-1.
The performance of these models is assessed by means of a Large Eddy Simulation (LES) of a combustor with a bluff-body, using the open source CFD software OpenFOAM. The bluff-body causes a recirculation zone in its wake. Additionally, it causes a strain on the flame front, where differential diffusion is expected to cause super-adiabatic temperatures and super-equilibrium mixture fractions.
The results show that the FGMs give a good prediction of the conditionally averaged reaction rates. They are also capable of qualitatively predicting the increase in mixture fraction, super-adiabatic temperature and super-equilibrium product mass fractions. They can therefore be used in a strained combustor setting with lean, premixed hydrogen. However, there are challenges regarding the prediction of temperature, especially for FGMs using a hydrogen based progress variable. This should be investigated in the future. Furthermore, the FGMs predict the reaction rate well despite over-predicting the local effects of strain and differential diffusion. ...
As with any technology, challenges remain. Whilst combustion modelling using Computational Fluid Dynamics (CFD) is not a solved problem to begin with, hydrogen combustion is made more complex by differential diffusion. This occurs when different species do not diffuse at the same rate. Hydrogen tends to diffuse faster than other species, causing local changes in mixture fraction, in addition to super-adiabatic temperatures and super-equilibrium product concentrations. This effect is stronger in strained or curved flames. Flame strain and curvature also influences the local reaction rate. These phenomena occur on a very small length and time scale. To simulate this directly, very fine meshes and very precise transport equations for each species are required. This can be prohibitively expensive for large scale designs or for design iteration.
In cases where simulating this behaviour directly is not possible, an alternative model is required. In this paper, five variants of such a model are assessed. These models are based on the assumption that the flame can be approximated as an ensemble of 1-dimensional flamelets. These flamelets can be analysed before the CFD simulations are performed. The results are then parametrized by a number of control variables, using a presumed filtered probability density function which aims to include sub-grid scale effects. By changing the flamelet conditions and control variable definition, different manifolds can be generated. In this paper, a number of these Flamelet-Generated Manifolds (FGMs) are compared to a higher fidelity model (using an Eulerian Stochastic Fields (ESF) approach). These FGMs use the mixture fraction, the progress variable and their sub-grid variances as control variables. Five different FGMs are tested, characterized by the progress variable definition (water vs hydrogen mass fraction) and flamelet strain rate (0 (unstrained) vs 3000 vs 6000 vs 13000 s^-1.
The performance of these models is assessed by means of a Large Eddy Simulation (LES) of a combustor with a bluff-body, using the open source CFD software OpenFOAM. The bluff-body causes a recirculation zone in its wake. Additionally, it causes a strain on the flame front, where differential diffusion is expected to cause super-adiabatic temperatures and super-equilibrium mixture fractions.
The results show that the FGMs give a good prediction of the conditionally averaged reaction rates. They are also capable of qualitatively predicting the increase in mixture fraction, super-adiabatic temperature and super-equilibrium product mass fractions. They can therefore be used in a strained combustor setting with lean, premixed hydrogen. However, there are challenges regarding the prediction of temperature, especially for FGMs using a hydrogen based progress variable. This should be investigated in the future. Furthermore, the FGMs predict the reaction rate well despite over-predicting the local effects of strain and differential diffusion.
Highly Strained Lean Premixed Hydrogen Flames
Emissions, Stability and Modelling
This thesis aims to contribute to the development of more accurate and affordable CFD tabulated-chemistry large eddy simulation (LES) models of lean premixed hydrogen flames subjected to intensive strain, thereby advancing the capabilities to optimally design hydrogen combustor leveraging strained regimes. First, the fundamental hydrogen flame response to strain is investigated extensively from the point of view of emissions, flame structure, and flame stability through high-fidelity detailed chemistry simulations in simplified laminar settings. Hence, with the help of the insights gathered in the previous phase, novel tabulated chemistry modelling approaches are proposed for LES of strained and turbulent hydrogen flames. The proposed models are tested a priori at unfiltered and filtered grids in a turbulent counterflow setup, where strain is established both by shear-driven turbulence and by the configuration.... ...
This thesis aims to contribute to the development of more accurate and affordable CFD tabulated-chemistry large eddy simulation (LES) models of lean premixed hydrogen flames subjected to intensive strain, thereby advancing the capabilities to optimally design hydrogen combustor leveraging strained regimes. First, the fundamental hydrogen flame response to strain is investigated extensively from the point of view of emissions, flame structure, and flame stability through high-fidelity detailed chemistry simulations in simplified laminar settings. Hence, with the help of the insights gathered in the previous phase, novel tabulated chemistry modelling approaches are proposed for LES of strained and turbulent hydrogen flames. The proposed models are tested a priori at unfiltered and filtered grids in a turbulent counterflow setup, where strain is established both by shear-driven turbulence and by the configuration....
Large eddy simulation of hydrogen combustion
Development of models and applications for sustainable power generation
Hydrogen is considered a promising alternative fuel because it produces no carbon emissions during combustion and can be generated from renewable energy sources. However, hydrogen combustion introduces significant challenges due to the complex behaviour of turbulent flames. Accurately predicting these behaviours requires advanced numerical methods, such as Large Eddy Simulations (LES), which capture unsteady flow dynamics at relatively affordable computational cost. Flamelet-based LES models are particularly attractive because they simplify combustion chemistry by representing turbulent flames as collections of laminar flame structures. While effective for hydrocarbon fuels, applying these models to hydrogen requires additional considerations, especially regarding differential diffusion effects that strongly influence flame stability and structure.
This thesis advances the modelling of turbulent hydrogen combustion by developing and validating flamelet-based LES approaches. It introduces improved modelling techniques, including dynamic closures and methods to account for non-unity Lewis number effects, which are essential for capturing hydrogen-specific behaviour. The models are tested across various flame configurations and subsequently applied to a hydrogen-capable combustor developed at TU Delft. Through simulation, the research provides insights into fuel-air mixing, flame stabilization, and nitrogen oxide (NOx) formation during the transition from methane to hydrogen operation. Overall, the work contributes to the development of reliable simulation tools that support the design of cleaner combustion systems and facilitate the integration of hydrogen into future energy and aviation applications. ...
Hydrogen is considered a promising alternative fuel because it produces no carbon emissions during combustion and can be generated from renewable energy sources. However, hydrogen combustion introduces significant challenges due to the complex behaviour of turbulent flames. Accurately predicting these behaviours requires advanced numerical methods, such as Large Eddy Simulations (LES), which capture unsteady flow dynamics at relatively affordable computational cost. Flamelet-based LES models are particularly attractive because they simplify combustion chemistry by representing turbulent flames as collections of laminar flame structures. While effective for hydrocarbon fuels, applying these models to hydrogen requires additional considerations, especially regarding differential diffusion effects that strongly influence flame stability and structure.
This thesis advances the modelling of turbulent hydrogen combustion by developing and validating flamelet-based LES approaches. It introduces improved modelling techniques, including dynamic closures and methods to account for non-unity Lewis number effects, which are essential for capturing hydrogen-specific behaviour. The models are tested across various flame configurations and subsequently applied to a hydrogen-capable combustor developed at TU Delft. Through simulation, the research provides insights into fuel-air mixing, flame stabilization, and nitrogen oxide (NOx) formation during the transition from methane to hydrogen operation. Overall, the work contributes to the development of reliable simulation tools that support the design of cleaner combustion systems and facilitate the integration of hydrogen into future energy and aviation applications.
Fourteen thermodynamic, velocity, and species mass fraction signals were reduced via autoencoders with 2–4 latent variables; the three-latent representation emerged as optimal, isolating transition sharpness and mid-frequency modes. Clustering of this space with a modularity-based algorithm consistently identified precursors with maximum lead times of ~42 μs and virtually no false positives. In one case, a flashback was successfully predicted and suppressed. Robustness analyses confirmed generalization across locations and noise levels, demonstrating that wall-based latent clustering advances predictive flashback control toward real-world deployment. ...
Fourteen thermodynamic, velocity, and species mass fraction signals were reduced via autoencoders with 2–4 latent variables; the three-latent representation emerged as optimal, isolating transition sharpness and mid-frequency modes. Clustering of this space with a modularity-based algorithm consistently identified precursors with maximum lead times of ~42 μs and virtually no false positives. In one case, a flashback was successfully predicted and suppressed. Robustness analyses confirmed generalization across locations and noise levels, demonstrating that wall-based latent clustering advances predictive flashback control toward real-world deployment.
Magnetic Stabilisation of Strained Hydrogen Flames
Exploring active control strategies via magnetic fields to stabilise thermodiffusive instabilities in lean-premixed hydrogen flames
anisms. These mechanisms involve magnetically induced alterations to the bulk flow field, which subsequently couple with differential diffusion effects to influence the distribution of reactants, affecting mixture fraction and the temperature field. Key findings demonstrate that the representative thermal thickness of the flame remains effectively unchanged, with a kernel-density (KDE) mode shift of 0.16 %. Crucially, total kinematic stretch is reduced by approximately 5-13 % near the axis, driven primarily by the curvature-induced contribution. Tangential strain exhibits a distinct two-regime response, decreasing by about 5-8 % in the preheat zone but increasing by 6-8 % in the reaction zone. Furthermore, a two-regime velocity-field redistribution is observed, where the axial component broadly weakens, while the radial velocity decreases for low progress variable (C) near the axis and strengthens for C ≳ 0.5. This research clarifies that direct magnetic effects are intrinsically weak and negligible
for practical control, with effective manipulation relying on these indirect pathways. The study also highlights that the efficacy of magnetic control diminishes with increasing strain rates and richer equivalence ratios. This work provides novel insights into the fundamental mechanisms governing magnetic control in premixed hydrogen flames, offering a framework for advancing sustainable combustion technologies. ...
anisms. These mechanisms involve magnetically induced alterations to the bulk flow field, which subsequently couple with differential diffusion effects to influence the distribution of reactants, affecting mixture fraction and the temperature field. Key findings demonstrate that the representative thermal thickness of the flame remains effectively unchanged, with a kernel-density (KDE) mode shift of 0.16 %. Crucially, total kinematic stretch is reduced by approximately 5-13 % near the axis, driven primarily by the curvature-induced contribution. Tangential strain exhibits a distinct two-regime response, decreasing by about 5-8 % in the preheat zone but increasing by 6-8 % in the reaction zone. Furthermore, a two-regime velocity-field redistribution is observed, where the axial component broadly weakens, while the radial velocity decreases for low progress variable (C) near the axis and strengthens for C ≳ 0.5. This research clarifies that direct magnetic effects are intrinsically weak and negligible
for practical control, with effective manipulation relying on these indirect pathways. The study also highlights that the efficacy of magnetic control diminishes with increasing strain rates and richer equivalence ratios. This work provides novel insights into the fundamental mechanisms governing magnetic control in premixed hydrogen flames, offering a framework for advancing sustainable combustion technologies.
SHTARWaRS
Scaled-up Hybrid-electric Turboprop AiRcraft with Water Recovery System
A Numerical Analysis of a Hydrogen-Fueled Trapped Vortex Combustor for RQL Applications
Using Large-Eddy Simulations
Injector-coupled RDC Operating Effects
Characterization of Wave Modes and Stagnation Pressure-gain in a Rotating Detonation Combustor with a Novel Injector Configuration
This thesis, conducted at the TU Berlin Hermann-Föttinger Institute for Fluid Dynamics, examines the influence of the injector design on RDC operation. First, a comparative study evaluates a novel low-pressure-loss Twin-Co-Axial injector against a well-documented Radial-Inward-Slot baseline, assessing reduced injector pressure losses and improved mixing quality. Second, the effect of injector pressure-balance is investigated, a parameter governing post-wave recovery and impacting the balance between mixture stratification and parasitic burning. Together, these studies advance the understanding of injector-driven wave behaviour and performance. ...
This thesis, conducted at the TU Berlin Hermann-Föttinger Institute for Fluid Dynamics, examines the influence of the injector design on RDC operation. First, a comparative study evaluates a novel low-pressure-loss Twin-Co-Axial injector against a well-documented Radial-Inward-Slot baseline, assessing reduced injector pressure losses and improved mixing quality. Second, the effect of injector pressure-balance is investigated, a parameter governing post-wave recovery and impacting the balance between mixture stratification and parasitic burning. Together, these studies advance the understanding of injector-driven wave behaviour and performance.
A CFD-based methodology was developed to reconstruct injection profiles from apparent heat release rate (aHRR) data and to apply nozzle flow theory for approximating injector behavior, validated through experimental comparison. The findings indicate that classical convergent-nozzle theory fails to capture the observed injection trends. While convergent nozzle theory predicts variable, pressure-dependent mass flow rates, the reconstructed mass flow profiles exhibit nearly constant injection rates when the needle is open, consistent with convergent–divergent nozzle theory predictions. However, the observed variation in maximum injection rates across different cases suggests these deviations may arise not only from geometric constraints but also from aerodynamic phenomena such as boundary layer separation or recirculation within the injector. Such flow features can induce pressure-dependent effects that limit injector performance beyond what nozzle geometry and convergent-nozzle theory alone would predict.
Regarding combustion, the study reveals that hydrogen ignition, triggered by a small diesel pilot, is dominated by localized high-temperature regions produced by the diesel flame. This accelerated autoignition contrasts with alternative hypotheses involving radical transport or direct flame interaction.
Overall, these results advance the understanding of injection and ignition phenomena in hydrogen HPDI engines, providing valuable insights for refining CFD models and supporting the development of efficient hydrogen-powered heavy-duty engines. ...
A CFD-based methodology was developed to reconstruct injection profiles from apparent heat release rate (aHRR) data and to apply nozzle flow theory for approximating injector behavior, validated through experimental comparison. The findings indicate that classical convergent-nozzle theory fails to capture the observed injection trends. While convergent nozzle theory predicts variable, pressure-dependent mass flow rates, the reconstructed mass flow profiles exhibit nearly constant injection rates when the needle is open, consistent with convergent–divergent nozzle theory predictions. However, the observed variation in maximum injection rates across different cases suggests these deviations may arise not only from geometric constraints but also from aerodynamic phenomena such as boundary layer separation or recirculation within the injector. Such flow features can induce pressure-dependent effects that limit injector performance beyond what nozzle geometry and convergent-nozzle theory alone would predict.
Regarding combustion, the study reveals that hydrogen ignition, triggered by a small diesel pilot, is dominated by localized high-temperature regions produced by the diesel flame. This accelerated autoignition contrasts with alternative hypotheses involving radical transport or direct flame interaction.
Overall, these results advance the understanding of injection and ignition phenomena in hydrogen HPDI engines, providing valuable insights for refining CFD models and supporting the development of efficient hydrogen-powered heavy-duty engines.
Modelling and Design Guidelines for Ram Air Ducts Using the Meredith Effect
Applied to an Organic Rankine Cycle Waste Heat Recovery System
The study uses the IMOTHEP Distributed fans Research Aircraft with electric Generators by ONERA (DRAGON) concept, a hybrid electric aircraft with two tail-mounted turbogenerators. The research proceeds in several stages. Initially, a multipass-condenser's potential to reduce pressure drop was examined by adjusting the heat exchanger blockage factor per pass, but results showed no reduction in pressure drop.
Next, a lumped parameter model was developed to analyze drag, pressure drop, temperature increase, and ram air duct length. This model evaluated the sensitivity of duct geometrical parameters on the drag recovery factor—a dimensionless number indicating net thrust. Findings revealed that inclining the heat exchanger efficiently increases the drag recovery factor, while the diffuser area ratio has a similar effect but is less space-efficient. The mass flow rate ratio showed less sensitivity, and fin height or pitch had the smallest effect on drag recovery.
Using the lumped parameter model, an optimal preliminary ram air duct design was identified for different spatial constraints. The study found that inline plain tube bundle and flat tube offset strip fin heat exchangers provided more compact solutions with higher drag recovery factors. For large diffuser-blocked area fractions, optimal duct geometry remained independent of heat exchanger type, characterized by a 70-degree maximum inclination angle, a 0.7 mass flow rate ratio, and maximized diffuser area ratio within spatial constraints.
A verification study of the lumped parameter model was conducted using a two-dimensional Reynolds Averaging Navier Stokes (RANS) computational fluid dynamics (CFD) analysis with k-ω SST turbulence and a porous zone to mimic the heat exchanger. The CFD analysis confirmed the lumped parameter model's predictions, with a 0.8% difference in drag recovery factor for optimal duct geometry. Across various geometries, the mean absolute difference in drag recovery factor between models was 1.082%, with a standard deviation of 0.584%.
In conclusion, integrating the condenser in the propulsion unit within spatial constraints results in positive thrust, thus supporting Meredith's 1935[2] claim. This integration reduces net drag and improves overall efficiency, contributing to significant emission reductions in line with ACARE's targets. ...
The study uses the IMOTHEP Distributed fans Research Aircraft with electric Generators by ONERA (DRAGON) concept, a hybrid electric aircraft with two tail-mounted turbogenerators. The research proceeds in several stages. Initially, a multipass-condenser's potential to reduce pressure drop was examined by adjusting the heat exchanger blockage factor per pass, but results showed no reduction in pressure drop.
Next, a lumped parameter model was developed to analyze drag, pressure drop, temperature increase, and ram air duct length. This model evaluated the sensitivity of duct geometrical parameters on the drag recovery factor—a dimensionless number indicating net thrust. Findings revealed that inclining the heat exchanger efficiently increases the drag recovery factor, while the diffuser area ratio has a similar effect but is less space-efficient. The mass flow rate ratio showed less sensitivity, and fin height or pitch had the smallest effect on drag recovery.
Using the lumped parameter model, an optimal preliminary ram air duct design was identified for different spatial constraints. The study found that inline plain tube bundle and flat tube offset strip fin heat exchangers provided more compact solutions with higher drag recovery factors. For large diffuser-blocked area fractions, optimal duct geometry remained independent of heat exchanger type, characterized by a 70-degree maximum inclination angle, a 0.7 mass flow rate ratio, and maximized diffuser area ratio within spatial constraints.
A verification study of the lumped parameter model was conducted using a two-dimensional Reynolds Averaging Navier Stokes (RANS) computational fluid dynamics (CFD) analysis with k-ω SST turbulence and a porous zone to mimic the heat exchanger. The CFD analysis confirmed the lumped parameter model's predictions, with a 0.8% difference in drag recovery factor for optimal duct geometry. Across various geometries, the mean absolute difference in drag recovery factor between models was 1.082%, with a standard deviation of 0.584%.
In conclusion, integrating the condenser in the propulsion unit within spatial constraints results in positive thrust, thus supporting Meredith's 1935[2] claim. This integration reduces net drag and improves overall efficiency, contributing to significant emission reductions in line with ACARE's targets.
Eulerian Stochastic Field method with FGM tabulation
For Partially Premixed Hydrogen Flames
Direct Numerical Simulations were performed to study the behaviour of sinusoidal perturbations imposed on the flame front, focusing on the growth rates of these perturbations under two different strain rates (2000 1/s and 4000 1/s). The results indicated that the tangential strain improved the stability of the flame front, as the strain rate led to a reduction in both the maximum observed growth rate and the growth rate after the perturbation reached its peak. The growth rates observed were in the non-linear regime, characterised by continual variation over time. At higher strain rates, the flame front stabilised more quickly, suggesting a strong correlation between strain rate and perturbation growth dynamics. The strain-induced velocity gradients displaced the flame front, reducing its effective curvature and wavelength, further contributing to the stabilisation process.
In addition to the strain rate, the study investigated the effects of varying the amplitude and wavelength of initial perturbations. It was found that the amplitude of the initial perturbation had little impact on the maximum growth rate, but variations in the initial wavelength significantly influenced both the growth dynamics and the maximum growth rate of the perturbations.
Overall, the results provided a comprehensive understanding of how tangential strain affected flame stability and highlighted the importance of wavelength variations in determining perturbation growth rates. These findings provide insights into potential strategies to improve flame stability in practical combustion systems aimed at reducing emissions, such as in lean hydrogen combustion. ...
Direct Numerical Simulations were performed to study the behaviour of sinusoidal perturbations imposed on the flame front, focusing on the growth rates of these perturbations under two different strain rates (2000 1/s and 4000 1/s). The results indicated that the tangential strain improved the stability of the flame front, as the strain rate led to a reduction in both the maximum observed growth rate and the growth rate after the perturbation reached its peak. The growth rates observed were in the non-linear regime, characterised by continual variation over time. At higher strain rates, the flame front stabilised more quickly, suggesting a strong correlation between strain rate and perturbation growth dynamics. The strain-induced velocity gradients displaced the flame front, reducing its effective curvature and wavelength, further contributing to the stabilisation process.
In addition to the strain rate, the study investigated the effects of varying the amplitude and wavelength of initial perturbations. It was found that the amplitude of the initial perturbation had little impact on the maximum growth rate, but variations in the initial wavelength significantly influenced both the growth dynamics and the maximum growth rate of the perturbations.
Overall, the results provided a comprehensive understanding of how tangential strain affected flame stability and highlighted the importance of wavelength variations in determining perturbation growth rates. These findings provide insights into potential strategies to improve flame stability in practical combustion systems aimed at reducing emissions, such as in lean hydrogen combustion.
Motivated by the importance of understanding how the interaction between the developing flow and the vibrating nozzle walls has an effect on supersonic noise generation and propagation, this work has studied the effect that wall compliancy has on the vibroacoustic loading of TOP contoured nozzles. This is demonstrated by means of cold flow tests carried out in the High Speed Laboratories of the Delft University of Technology on a stiff-walled aluminum nozzle, which serves as a baseline test case, and on a urethane-based compliant walled nozzle. Tests are conducted under comparable flow conditions and test parameters are measured by means of acoustic and optical techniques. Simultaneous recordings are performed and include the nozzle-wall deformation, by means of stereoscopic tracking of tracers on the nozzle lip, the imprint of the near-field acoustic signature, by means of arrays of pressure-microphones, and Schlieren imaging of the jet plume.
Measurement data allows for a Fourier decomposition of the nozzle lip displacement and of the acoustic pressure field in azimuth. Reconstruction of the instantaneous plume development enables the identification of the main flow structures responsible for noise generation.
Comparison of results between the two test articles highlights a different spectral content and directivity pattern. Correlation between the structural displacements and the acoustic signal, together with the use of DMD, quantitatively aids the investigation of how FSI has an impact on the generation of an aeroelastic tone at 180 Hz. Findings suggest that its production is the result of the periodic thickening and thinning of the shear layer owing to the heightened flapping motion of the nozzle lip preceding RSS transition, driven by an intensified shock foot instability. ...
Motivated by the importance of understanding how the interaction between the developing flow and the vibrating nozzle walls has an effect on supersonic noise generation and propagation, this work has studied the effect that wall compliancy has on the vibroacoustic loading of TOP contoured nozzles. This is demonstrated by means of cold flow tests carried out in the High Speed Laboratories of the Delft University of Technology on a stiff-walled aluminum nozzle, which serves as a baseline test case, and on a urethane-based compliant walled nozzle. Tests are conducted under comparable flow conditions and test parameters are measured by means of acoustic and optical techniques. Simultaneous recordings are performed and include the nozzle-wall deformation, by means of stereoscopic tracking of tracers on the nozzle lip, the imprint of the near-field acoustic signature, by means of arrays of pressure-microphones, and Schlieren imaging of the jet plume.
Measurement data allows for a Fourier decomposition of the nozzle lip displacement and of the acoustic pressure field in azimuth. Reconstruction of the instantaneous plume development enables the identification of the main flow structures responsible for noise generation.
Comparison of results between the two test articles highlights a different spectral content and directivity pattern. Correlation between the structural displacements and the acoustic signal, together with the use of DMD, quantitatively aids the investigation of how FSI has an impact on the generation of an aeroelastic tone at 180 Hz. Findings suggest that its production is the result of the periodic thickening and thinning of the shear layer owing to the heightened flapping motion of the nozzle lip preceding RSS transition, driven by an intensified shock foot instability.
Unsteady SpaRTA
Data-driven turbulence modelling for unsteady applications
Despite promising results for steady RANS simulations, little has yet been investigated in URANS applications. In this dissertation, this lack of research will be addressed. The main ideas are then, first, to see how the available information in URANS simulations can be used to improve the anisotropic Reynolds stress tensor prediction, and second if and how this can be done by using a sparse regression technique, whose framework is known as SpaRTA. A procedure involving the triple decomposition of High-Fidelity velocity fields is applied, aiming at finding a model exclusively for the stochastic component of the anisotropy. The test case which is considered is the flow around a cylinder at Re=3900. The High-Fidelity data was collected by running Large Eddy Simulations in OpenFOAM, after which the velocity was split into its different components through Proper Orthogonal Decomposition.
A priori results have shown good performance of the trained models, outperforming the Boussinesq assumption both in the prediction of turbulence componentiality and also on the values of the single anisotropy components. ...
Despite promising results for steady RANS simulations, little has yet been investigated in URANS applications. In this dissertation, this lack of research will be addressed. The main ideas are then, first, to see how the available information in URANS simulations can be used to improve the anisotropic Reynolds stress tensor prediction, and second if and how this can be done by using a sparse regression technique, whose framework is known as SpaRTA. A procedure involving the triple decomposition of High-Fidelity velocity fields is applied, aiming at finding a model exclusively for the stochastic component of the anisotropy. The test case which is considered is the flow around a cylinder at Re=3900. The High-Fidelity data was collected by running Large Eddy Simulations in OpenFOAM, after which the velocity was split into its different components through Proper Orthogonal Decomposition.
A priori results have shown good performance of the trained models, outperforming the Boussinesq assumption both in the prediction of turbulence componentiality and also on the values of the single anisotropy components.