Pub Date : 2026-10-23DOI: 10.1007/s10494-026-00801-8
Darish Jeswin Dhas, Cristian Marchioli
We investigate the Lagrangian rotational and deformation dynamics of long flexible fibers in a turbulent channel flow at a shear Reynolds number equal to 300, using one-way coupled Euler-Lagrange direct numerical simulations. The fibers, modeled as chains of sub-Kolmogorov rod elements with prescribed bending stiffness, span more than one order of magnitude in length and are analyzed in three wall-normal slabs covering the near-wall, log-layer and bulk regions. We compute autocorrelations of the tumbling and spinning rates, power spectra of the fiber’s end-to-end vector, and waiting-time distributions of intense tumbling events. Spinning decorrelates on a fixed multiple of the local Kolmogorov time, independent of fiber length, whereas tumbling develops a memory that grows with fiber length by factors of two to five, reversing the ordering of the two timescales between the shortest and longest fibers. Flapping spectra separate into a high-frequency regime in which all fiber lengths carry the same energy in absolute terms and a low-frequency regime in which the energy increases with fiber length. Intense tumbling exhibits approximately exponential, weakly clustered waiting-time statistics whose rescaled form is universal across slabs, fiber lengths and bending rigidities, whereas the event rate depends on both fiber length and rigidity.
{"title":"Lagrangian Statistics of Long Flexible Fibers in Wall-Bounded Turbulence","authors":"Darish Jeswin Dhas, Cristian Marchioli","doi":"10.1007/s10494-026-00801-8","DOIUrl":"10.1007/s10494-026-00801-8","url":null,"abstract":"<div><p>We investigate the Lagrangian rotational and deformation dynamics of long flexible fibers in a turbulent channel flow at a shear Reynolds number equal to 300, using one-way coupled Euler-Lagrange direct numerical simulations. The fibers, modeled as chains of sub-Kolmogorov rod elements with prescribed bending stiffness, span more than one order of magnitude in length and are analyzed in three wall-normal slabs covering the near-wall, log-layer and bulk regions. We compute autocorrelations of the tumbling and spinning rates, power spectra of the fiber’s end-to-end vector, and waiting-time distributions of intense tumbling events. Spinning decorrelates on a fixed multiple of the local Kolmogorov time, independent of fiber length, whereas tumbling develops a memory that grows with fiber length by factors of two to five, reversing the ordering of the two timescales between the shortest and longest fibers. Flapping spectra separate into a high-frequency regime in which all fiber lengths carry the same energy in absolute terms and a low-frequency regime in which the energy increases with fiber length. Intense tumbling exhibits approximately exponential, weakly clustered waiting-time statistics whose rescaled form is universal across slabs, fiber lengths and bending rigidities, whereas the event rate depends on both fiber length and rigidity.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 4","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-10-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-026-00801-8.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149234877","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-23DOI: 10.1007/s10494-026-00804-5
Davide Cavalieri, Davide Schintu, Pietro Paolo Ciottoli, Francesco Creta, Pasquale Eduardo Lapenna
In this study, we investigate the role of phase separation in transcritical oxygen-hydrogen mixing layers under liquid rocket engine-relevant conditions. High-fidelity simulations of a splitter-plate configuration are performed to compare two thermodynamic approaches, a single-phase (SP) model and a multiphase model based on the vapor–liquid equilibrium (VLE) concept. Three operating pressures are considered, spanning near-critical to highly supercritical conditions, with fixed stream Reynolds numbers so that pressure is the only varied parameter. The two models share the same overall flow topology but follow different thermodynamic paths within the two-phase region. The SP model predicts local temperatures below the oxygen injection value, a non-ideal mixing effect absent under VLE, whose mixing path increases monotonically with hydrogen content. Accounting for phase separation results in a thinner thermal mixing layer, reduced temperature fluctuations, a lower growth rate, and modified near-wake dynamics, with a longer recirculation region behind the lip. Conditional statistics of the scalar dissipation rate show that the VLE model predicts more intense molecular mixing at compositions inside the two-phase region, which encompasses the stoichiometric condition most relevant to ignition. The spectral analysis localizes the model effect at the small scales for velocity, while density is affected across all scales. All discrepancies are largest at near-critical pressure and attenuate as the operating pressure moves away from the critical point.
{"title":"Role of Phase Separation in Transcritical Mixing Layers Under Liquid Rocket Engine Conditions","authors":"Davide Cavalieri, Davide Schintu, Pietro Paolo Ciottoli, Francesco Creta, Pasquale Eduardo Lapenna","doi":"10.1007/s10494-026-00804-5","DOIUrl":"10.1007/s10494-026-00804-5","url":null,"abstract":"<div><p>In this study, we investigate the role of phase separation in transcritical oxygen-hydrogen mixing layers under liquid rocket engine-relevant conditions. High-fidelity simulations of a splitter-plate configuration are performed to compare two thermodynamic approaches, a single-phase (SP) model and a multiphase model based on the vapor–liquid equilibrium (VLE) concept. Three operating pressures are considered, spanning near-critical to highly supercritical conditions, with fixed stream Reynolds numbers so that pressure is the only varied parameter. The two models share the same overall flow topology but follow different thermodynamic paths within the two-phase region. The SP model predicts local temperatures below the oxygen injection value, a non-ideal mixing effect absent under VLE, whose mixing path increases monotonically with hydrogen content. Accounting for phase separation results in a thinner thermal mixing layer, reduced temperature fluctuations, a lower growth rate, and modified near-wake dynamics, with a longer recirculation region behind the lip. Conditional statistics of the scalar dissipation rate show that the VLE model predicts more intense molecular mixing at compositions inside the two-phase region, which encompasses the stoichiometric condition most relevant to ignition. The spectral analysis localizes the model effect at the small scales for velocity, while density is affected across all scales. All discrepancies are largest at near-critical pressure and attenuate as the operating pressure moves away from the critical point.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 4","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-10-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149234878","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-16DOI: 10.1007/s10494-026-00796-2
Maximilian Bambauer, Vipin Michael, Markus Klein, Nilanjan Chakraborty
Accurate prediction of Flame-Wall Interactions (FWI) is crucial for the design of compact, high-efficiency combustors but remains a significant challenge for Reynolds-Averaged Navier-Stokes (RANS) simulations. This study presents the development and validation of a lightweight data-driven closure for the mean reaction rate, trained on high-fidelity Direct Numerical Simulation (DNS) data of a V-shaped turbulent premixed flame. To ensure numerical stability and physical consistency, the training methodology incorporates a logarithmic transformation of the reaction rate target and a novel error-function transformation of the wall distance, effectively localizing the model’s sensitivity to the near-wall quenching zone. A-priori validation demonstrates that the neural network accurately captures the mean reaction rate statistics and extrapolates successfully to unseen spatial regions. However, a-posteriori assessment in coupled RANS simulations reveals a critical sensitivity to input feature consistency. The full-feature model (7 input parameters), which includes turbulent kinetic energy and dissipation rate as inputs, fails to predict the correct quenching behavior due to significant discrepancies between the DNS-extracted turbulence quantities used for training and the corresponding quantities obtained from RANS. In contrast, a reduced-feature model (3 input parameters), relying exclusively on the mean progress variable, its gradient, and the transformed wall distance, demonstrates remarkable robustness. By decoupling the prediction from uncertain turbulence quantities, the model with 3 input parameters accurately reproduces the V-flame structure, achieving performance comparable to a manually tuned algebraic closure. Furthermore, the reduced model exhibits strong generalization capabilities, successfully predicting the transient physics of a Head-On Quenching (HOQ) configuration that was not present in the training dataset. These findings highlight that for data-driven RANS closures, selecting input features that remain consistent across fidelity levels, is paramount for achieving predictive stability and generalization.
火墙相互作用(FWI)的准确预测对于设计紧凑、高效的燃烧室至关重要,但对于reynolds - average Navier-Stokes (RANS)模拟来说,这仍然是一个重大挑战。本研究利用v型湍流预混火焰的高保真直接数值模拟(DNS)数据,开发并验证了一种轻量级数据驱动的平均反应速率封闭模型。为了确保数值稳定性和物理一致性,训练方法结合了反应速率目标的对数变换和壁面距离的新颖误差函数变换,有效地将模型的灵敏度定位到近壁面淬火区。先验验证表明,该神经网络能够准确捕获平均反应速率统计数据,并成功地外推到未知的空间区域。然而,在耦合RANS模拟中的后验评估揭示了输入特征一致性的关键敏感性。以湍流动能和耗散率为输入的全特征模型(7个输入参数),由于用于训练的dns提取的湍流量与从RANS中获得的相应量存在显著差异,因此无法预测正确的淬火行为。相比之下,仅依赖于平均进度变量、其梯度和转换后的壁距的减特征模型(3个输入参数)表现出显著的鲁棒性。通过将预测与不确定的湍流量解耦,具有3个输入参数的模型准确地再现了v型火焰结构,实现了与手动调谐代数闭包相当的性能。此外,简化模型显示出强大的泛化能力,成功预测了训练数据集中不存在的迎头淬火(HOQ)配置的瞬态物理。这些发现强调,对于数据驱动的RANS闭包,选择在保真度级别上保持一致的输入特征对于实现预测稳定性和泛化至关重要。
{"title":"Development of A Lightweight Neural Network for Predicting Reaction Rates in RANS Simulations of Flame-Wall Interactions","authors":"Maximilian Bambauer, Vipin Michael, Markus Klein, Nilanjan Chakraborty","doi":"10.1007/s10494-026-00796-2","DOIUrl":"10.1007/s10494-026-00796-2","url":null,"abstract":"<div><p>Accurate prediction of Flame-Wall Interactions (FWI) is crucial for the design of compact, high-efficiency combustors but remains a significant challenge for Reynolds-Averaged Navier-Stokes (RANS) simulations. This study presents the development and validation of a lightweight data-driven closure for the mean reaction rate, trained on high-fidelity Direct Numerical Simulation (DNS) data of a V-shaped turbulent premixed flame. To ensure numerical stability and physical consistency, the training methodology incorporates a logarithmic transformation of the reaction rate target and a novel error-function transformation of the wall distance, effectively localizing the model’s sensitivity to the near-wall quenching zone. A-priori validation demonstrates that the neural network accurately captures the mean reaction rate statistics and extrapolates successfully to unseen spatial regions. However, a-posteriori assessment in coupled RANS simulations reveals a critical sensitivity to input feature consistency. The full-feature model (7 input parameters), which includes turbulent kinetic energy and dissipation rate as inputs, fails to predict the correct quenching behavior due to significant discrepancies between the DNS-extracted turbulence quantities used for training and the corresponding quantities obtained from RANS. In contrast, a reduced-feature model (3 input parameters), relying exclusively on the mean progress variable, its gradient, and the transformed wall distance, demonstrates remarkable robustness. By decoupling the prediction from uncertain turbulence quantities, the model with 3 input parameters accurately reproduces the V-flame structure, achieving performance comparable to a manually tuned algebraic closure. Furthermore, the reduced model exhibits strong generalization capabilities, successfully predicting the transient physics of a Head-On Quenching (HOQ) configuration that was not present in the training dataset. These findings highlight that for data-driven RANS closures, selecting input features that remain consistent across fidelity levels, is paramount for achieving predictive stability and generalization.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 4","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-10-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-026-00796-2.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149189860","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-16DOI: 10.1007/s10494-026-00800-9
Gregory Aranovich
We propose corrections to the diffusion equation providing solutions consistent with nano-scale and multi-scale physics. These corrections can be useful for various applications, including nano-technology, strong-gradient and rarefied transport. The problem is that the classical diffusion equation (which terms are in the core of fluid dynamics models) does not carry information about the structure of the fluid, and fails, for example, at the nano- and multi-scale. As we show here, this information was lost due to the way the original equation was derived. In this paper, we reconsidered Einstein’s derivation of the diffusion equation to eliminate truncation of higher terms. The results give the finite difference equation of mass transport where information about the fluid structure is not lost; this is because the finite-difference length is not a numerical discretization parameter but a mean free path, λ, a fluid property determined by the structure of the fluid and by molecular mechanisms of collision. For this reason, the (λ-discretized) finite difference diffusion equation becomes consistent with nano-scale and multi-scale physics. This is demonstrated by specific examples.
{"title":"Reconsidering Einstein’s Derivation of Diffusion Equation to Provide Solutions Consistent with Nano-Scale and Multi-Scale Physics","authors":"Gregory Aranovich","doi":"10.1007/s10494-026-00800-9","DOIUrl":"10.1007/s10494-026-00800-9","url":null,"abstract":"<div><p>We propose corrections to the diffusion equation providing solutions consistent with nano-scale and multi-scale physics. These corrections can be useful for various applications, including nano-technology, strong-gradient and rarefied transport. The problem is that the classical diffusion equation (which terms are in the core of fluid dynamics models) does not carry information about the structure of the fluid, and fails, for example, at the nano- and multi-scale. As we show here, this information was lost due to the way the original equation was derived. In this paper, we reconsidered Einstein’s derivation of the diffusion equation to eliminate truncation of higher terms. The results give the finite difference equation of mass transport where information about the fluid structure is not lost; this is because the finite-difference length is not a numerical discretization parameter but a mean free path, <i>λ</i>, a fluid property determined by the structure of the fluid and by molecular mechanisms of collision. For this reason, the (<i>λ-</i>discretized) finite difference diffusion equation becomes consistent with nano-scale and multi-scale physics. This is demonstrated by specific examples.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 4","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-10-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149176698","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-06DOI: 10.1007/s10494-026-00799-z
Robin Vivoli, Daniel Pugh, Anthony Giles, Burak Goktepe, Tomas Davies, Steven Morris
Surface roughness has a critical influence on the aerothermal and combustion behavior of gas turbine burners, particularly with the growing use of additively manufactured (AM) components that exhibit inherently rougher surfaces than conventionally machined parts. This study investigates the impact of surface roughness on flow and flame dynamics in a premixed jet burner (PJB) operating under both isothermal-air and reacting hydrogen-fired conditions. Experimental measurements using Laser Doppler Anemometry (LDA) and OH* chemiluminescence were complemented by Computational Fluid Dynamics (CFD) simulations employing Reynolds-Averaged Navier–Stokes (RANS) and Detached Eddy Simulation (DES) frameworks. Building upon existing equivalent sand-grain roughness (kₛ) models, a novel correlation incorporating both measured roughness parameters and bulk flow velocity was developed to improve predictive accuracy for resolved boundary layers (y+ ≈ 1), a regime in which ks+ > y⁺ is common and standard roughness-function formulations lose validity. The new correlation demonstrated strong agreement with experimental data in isothermal simulations. When extended to reacting hydrogen–air flames, RANS simulations successfully reproduced roughness-induced flow redistribution and flame shortening, although DES tended to overpredict bluff-body effects and underperform under lean conditions. Overall, the proposed ks correlation, validated under isothermal conditions, provides a computationally efficient framework for modelling surface-roughness effects, and its extension to reacting hydrogen flames, particularly under RANS, offers a promising basis for future development toward additively manufactured gas turbine components.
表面粗糙度对燃气轮机燃烧器的气动热性能和燃烧性能有着至关重要的影响,特别是随着增材制造(AM)部件的使用越来越多,这些部件的表面比传统的机械加工部件更粗糙。本文研究了在等温空气和反应氢气燃烧条件下,表面粗糙度对预混合燃烧器(PJB)流动和火焰动力学的影响。实验测量采用激光多普勒风速法(LDA)和OH*化学发光,辅以计算流体动力学(CFD)模拟,采用reynolds - average Navier-Stokes (RANS)和分离涡流模拟(DES)框架。在现有等效沙粒粗糙度(kₛ)模型的基础上,开发了一种结合测量粗糙度参数和体流速度的新相关性,以提高分解边界层(y+≈1)的预测精度,在这种情况下,ks + > y+是常见的,标准粗糙度函数公式失去了有效性。新的相关性与等温模拟的实验数据非常吻合。当扩展到反应氢气-空气火焰时,RANS模拟成功地再现了粗糙度诱导的流动再分配和火焰缩短,尽管DES倾向于过度预测崖体效应,并且在稀薄条件下表现不佳。总的来说,在等温条件下验证的ks相关性为模拟表面粗糙度效应提供了一个计算效率高的框架,并将其扩展到反应氢火焰,特别是在RANS下,为未来增材制造燃气轮机部件的发展提供了有希望的基础。补充信息:在线版本包含补充资料,可在https://doi.org/10.1007/s10494-026-00799-z上获得。
{"title":"Novel Low-y⁺ Roughness Correlation for Hydrogen-Fired Jet Burners Validated Under Isothermal and Reacting Conditions","authors":"Robin Vivoli, Daniel Pugh, Anthony Giles, Burak Goktepe, Tomas Davies, Steven Morris","doi":"10.1007/s10494-026-00799-z","DOIUrl":"10.1007/s10494-026-00799-z","url":null,"abstract":"<div><p>Surface roughness has a critical influence on the aerothermal and combustion behavior of gas turbine burners, particularly with the growing use of additively manufactured (AM) components that exhibit inherently rougher surfaces than conventionally machined parts. This study investigates the impact of surface roughness on flow and flame dynamics in a premixed jet burner (PJB) operating under both isothermal-air and reacting hydrogen-fired conditions. Experimental measurements using Laser Doppler Anemometry (LDA) and OH* chemiluminescence were complemented by Computational Fluid Dynamics (CFD) simulations employing Reynolds-Averaged Navier–Stokes (RANS) and Detached Eddy Simulation (DES) frameworks. Building upon existing equivalent sand-grain roughness (kₛ) models, a novel correlation incorporating both measured roughness parameters and bulk flow velocity was developed to improve predictive accuracy for resolved boundary layers (y<sup>+</sup> ≈ 1), a regime in which k<sub>s</sub><sup>+</sup> > y⁺ is common and standard roughness-function formulations lose validity. The new correlation demonstrated strong agreement with experimental data in isothermal simulations. When extended to reacting hydrogen–air flames, RANS simulations successfully reproduced roughness-induced flow redistribution and flame shortening, although DES tended to overpredict bluff-body effects and underperform under lean conditions. Overall, the proposed k<sub>s</sub> correlation, validated under isothermal conditions, provides a computationally efficient framework for modelling surface-roughness effects, and its extension to reacting hydrogen flames, particularly under RANS, offers a promising basis for future development toward additively manufactured gas turbine components.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 3","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-10-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13642420/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149126298","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-05DOI: 10.1007/s10494-026-00790-8
J. M. Duró, E. Mestres, M. Teng, O. Lehmkuhl, I. Rodríguez
Effects of wind direction in realistic urban boundary layers remain difficult to characterize systematically because local flow patterns, and turbulent statistics within a realistic urban canopy may respond differently to changes in the approaching wind. To investigate these multi-scale directional impacts, we conducted high-resolution large-eddy simulations of the atmospheric boundary layer over the Zona Universitària Pedralbes district in Barcelona. The computational meshes employ fourth-order spectral elements, yielding pedestrian-level resolutions below 1 m and resulting in approximately (bf{5.0times 10^8}) degrees of freedom. Sixteen wind directions uniformly distributed over 360({}^circ) are simulated to capture the full directional response of the urban fabric. At pedestrian level, the flow exhibits strong directional sensitivity, with moderate rotations of the incoming wind reorganizing the dominant flow pathways from continuous accelerated corridors, when winds align with major street axes, to fragmented cellular patterns under oblique inflows. These directionally activated channeling corridors govern local ventilation and sheltering. Yet, despite this pronounced local variability, double averaged vertical profiles of mean velocity and turbulence intensity collapse remarkably across all wind directions. Two distinct inflection points are consistently identified in the mean velocity profiles: one located slightly below the average building height, (bf{H_mathrm{avg}}), confirming the persistence of a shear-driven mixing-layer regime even in highly heterogeneous urban morphology, and a second, deeper inflection point near pedestrian level, approximately 0.08–0.10 (bf{H_mathrm{avg}}) above the ground, that marks the transition between recirculating near-ground flow and more connected transport within the urban canopy. Subdomain analysis further shows that this lower inflection point is morphology- and direction-dependent, reflecting changes in the transition between sheltered near-ground recirculation and transport within the urban canopy as preferential flow routes are activated or suppressed by the incoming wind direction. It is shown that urban aerodynamic response is simultaneously robust at the neighbourhood scale, behaving quasi-isotropically in the double-averaged sense, and strongly directional at the local scale, where the activation of preferential ventilation pathways dictates the spatial distribution of momentum and turbulence.
{"title":"Impact of Wind Direction on Flow and Turbulent Statistics Over a Realistic Urban Area: A Large-Eddy Simulation Study","authors":"J. M. Duró, E. Mestres, M. Teng, O. Lehmkuhl, I. Rodríguez","doi":"10.1007/s10494-026-00790-8","DOIUrl":"10.1007/s10494-026-00790-8","url":null,"abstract":"<div><p>Effects of wind direction in realistic urban boundary layers remain difficult to characterize systematically because local flow patterns, and turbulent statistics within a realistic urban canopy may respond differently to changes in the approaching wind. To investigate these multi-scale directional impacts, we conducted high-resolution large-eddy simulations of the atmospheric boundary layer over the Zona Universitària Pedralbes district in Barcelona. The computational meshes employ fourth-order spectral elements, yielding pedestrian-level resolutions below 1 m and resulting in approximately <span>(bf{5.0times 10^8})</span> degrees of freedom. Sixteen wind directions uniformly distributed over 360<span>({}^circ)</span> are simulated to capture the full directional response of the urban fabric. At pedestrian level, the flow exhibits strong directional sensitivity, with moderate rotations of the incoming wind reorganizing the dominant flow pathways from continuous accelerated corridors, when winds align with major street axes, to fragmented cellular patterns under oblique inflows. These directionally activated channeling corridors govern local ventilation and sheltering. Yet, despite this pronounced local variability, double averaged vertical profiles of mean velocity and turbulence intensity collapse remarkably across all wind directions. Two distinct inflection points are consistently identified in the mean velocity profiles: one located slightly below the average building height, <span>(bf{H_mathrm{avg}})</span>, confirming the persistence of a shear-driven mixing-layer regime even in highly heterogeneous urban morphology, and a second, deeper inflection point near pedestrian level, approximately 0.08–0.10 <span>(bf{H_mathrm{avg}})</span> above the ground, that marks the transition between recirculating near-ground flow and more connected transport within the urban canopy. Subdomain analysis further shows that this lower inflection point is morphology- and direction-dependent, reflecting changes in the transition between sheltered near-ground recirculation and transport within the urban canopy as preferential flow routes are activated or suppressed by the incoming wind direction. It is shown that urban aerodynamic response is simultaneously robust at the neighbourhood scale, behaving quasi-isotropically in the double-averaged sense, and strongly directional at the local scale, where the activation of preferential ventilation pathways dictates the spatial distribution of momentum and turbulence.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 3","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-10-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-026-00790-8.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149132301","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-01DOI: 10.1007/s10494-026-00793-5
Maytham M. Abid, Marc Marín-Genescà
<div><p>This study investigates the potential of a novel ducted horizontal-axis wind turbine equipped with an integrated passive flow-control technique (DWT) to enhance wake recovery and power extraction. The PFCT differs from prior mechanisms: unlike brims and flanges (Watanabe et al. 2019; Abe and Ohya 2004; Abe et al. 2005) that rely on radial expansion and brim suction, the PFCT employs three vertically stacked, 40°-inclined sheets generating streamwise vortices that actively entrain ambient fluid into the wake core. Unlike stabilization plates (Watanabe et al. 2019) that suppress vortex shedding, PFCT sheets exploit and organize vortex shedding into coherent streamwise vortices for multi-layer wake mixing. Unlike lobed ejectors (Han et al. 2015) that delay boundary-layer separation in internal flows, PFCT sheets are external ramp-type surfaces interacting with rotor tip vortices in the freestream bypass region. Unlike conventional vortex generators (Nunes et al. 2020; Sullerey et al. 2001; Chong et al. 2008) that energize boundary layers via small tabs, PFCT sheets are large-scale, geometrically integrated wake modifiers operating on global wake structure through pressure-driven entrainment plus vortex-enhanced mixing. Three-dimensional URANS simulations (k–ω SST) were validated against wind tunnel experiments. Validation was performed across three streamwise planes at 1·5D, 2·0D, and 2·5D downstream of the rotor, quantified by mean absolute error (MAE) and root mean square error (RMSE). Grid independence was confirmed through a mesh-sensitivity study. A staged temporal-resolution strategy was adopted for the transient simulations to accurately resolve rotor–wake evolution. Torque convergence remained within 2.3%, and residuals remained below 10<sup>− 7</sup>. Comparative analyses were performed for a bare wind turbine (BWT), a free ducted wind turbine (FDWT), and the proposed DWT. Numerical results indicated that the DWT achieved a peak power coefficient (C<sub>p</sub>) of 43.2%, an 85.4% improvement over the computationally evaluated BWT. The new duct design mitigated wake deficits, yielding an area-averaged wake velocity ratio 4.15× higher than the BWT(1.79× relative to the FDWT) at 1·5D downstream. Near-wake analysis indicated a 21-fold increase in turbulent kinetic energy compared to the BWT, reflecting enhanced local mixing. However, velocity recovery advantages were distance-dependent, with the DWT showing superior performance at 1·5D but reduced area-averaged velocity relative to the FDWT by 2·5D. This reversal reflected the DWT’s higher energy extraction, which depletes wake momentum more severely; the PFCT-induced vortices that accelerated early recovery decayed by 2·5D, leaving a more depleted wake than that of the FDWT’s gentler, sustained recovery. Consequently, the DWT demonstrated improved downstream inflow conditions for the 2D tandem configuration investigated in this study, whereas the single-turbine wake analysis indicated
本研究探讨了一种新型风管水平轴风力机的潜力,该风管水平轴风力机配备了集成的被动流动控制技术(DWT),以提高尾流回收和功率提取。PFCT与之前的机制不同:与边缘和法兰(Watanabe等人,2019;Abe和Ohya 2004; Abe等人,2005)依赖径向膨胀和边缘吸力不同,PFCT采用三片垂直堆叠的40°倾斜片,产生流向涡旋,主动将环境流体夹带到尾流核心。与抑制旋涡脱落的稳定板(Watanabe et al. 2019)不同,PFCT片利用并组织旋涡脱落形成连贯的流向旋涡,用于多层尾迹混合。与在内部流动中延迟边界层分离的叶状喷射器(Han et al. 2015)不同,PFCT片是与自由流旁路区域的转子顶涡相互作用的外部坡道型表面。与传统的旋涡发生器(Nunes et al. 2020; Sullerey et al. 2001; Chong et al. 2008)通过小片片激励边界层不同,PFCT片是大规模的、几何上集成的尾流调节剂,通过压力驱动的夹带和涡流增强的混合作用于全局尾流结构。通过风洞实验验证了三维URANS模拟(k -ω SST)的有效性。在转子下游1.5 d、2.0 d和2.5 d的三个流平面上进行验证,通过平均绝对误差(MAE)和均方根误差(RMSE)进行量化。通过网格敏感性研究确认了网格独立性。采用分段时间分辨策略进行瞬态仿真,以准确分辨旋翼-尾迹演化。扭矩收敛保持在2.3%以内,残差保持在10−7以下。对裸风轮(BWT)、自由风轮(FDWT)和提议的风轮进行了对比分析。数值计算结果表明,DWT的峰值功率系数(Cp)为43.2%,比计算结果提高了85.4%。新的风道设计减轻了尾流缺陷,在下游1.5 d处产生的面积平均尾流速度比BWT高4.15倍(相对于FDWT为1.79倍)。近尾迹分析表明,与BWT相比,湍流动能增加了21倍,反映了局部混合的增强。然而,速度恢复优势与距离有关,DWT在1.5 d时表现出更好的性能,但相对于FDWT,面积平均速度降低了2.5 d。这种逆转反映了DWT更高的能量提取,这更严重地消耗了尾流动量;加速早期恢复的pfct诱导的涡流衰减了2.5 d,留下的尾流比FDWT平缓、持续恢复的尾流更耗尽。因此,在本研究中研究的2D串联结构中,FDWT显示出改善的下游入流条件,而单涡轮尾迹分析表明,FDWT在更大的下游距离上更有效地恢复速度。全面的串接间距调查仍是未来的工作。
{"title":"Numerical Investigation of a New Passive Flow Control Technique to Improve Near-Wake Profiles of a Ducted Wind Turbine","authors":"Maytham M. Abid, Marc Marín-Genescà","doi":"10.1007/s10494-026-00793-5","DOIUrl":"10.1007/s10494-026-00793-5","url":null,"abstract":"<div><p>This study investigates the potential of a novel ducted horizontal-axis wind turbine equipped with an integrated passive flow-control technique (DWT) to enhance wake recovery and power extraction. The PFCT differs from prior mechanisms: unlike brims and flanges (Watanabe et al. 2019; Abe and Ohya 2004; Abe et al. 2005) that rely on radial expansion and brim suction, the PFCT employs three vertically stacked, 40°-inclined sheets generating streamwise vortices that actively entrain ambient fluid into the wake core. Unlike stabilization plates (Watanabe et al. 2019) that suppress vortex shedding, PFCT sheets exploit and organize vortex shedding into coherent streamwise vortices for multi-layer wake mixing. Unlike lobed ejectors (Han et al. 2015) that delay boundary-layer separation in internal flows, PFCT sheets are external ramp-type surfaces interacting with rotor tip vortices in the freestream bypass region. Unlike conventional vortex generators (Nunes et al. 2020; Sullerey et al. 2001; Chong et al. 2008) that energize boundary layers via small tabs, PFCT sheets are large-scale, geometrically integrated wake modifiers operating on global wake structure through pressure-driven entrainment plus vortex-enhanced mixing. Three-dimensional URANS simulations (k–ω SST) were validated against wind tunnel experiments. Validation was performed across three streamwise planes at 1·5D, 2·0D, and 2·5D downstream of the rotor, quantified by mean absolute error (MAE) and root mean square error (RMSE). Grid independence was confirmed through a mesh-sensitivity study. A staged temporal-resolution strategy was adopted for the transient simulations to accurately resolve rotor–wake evolution. Torque convergence remained within 2.3%, and residuals remained below 10<sup>− 7</sup>. Comparative analyses were performed for a bare wind turbine (BWT), a free ducted wind turbine (FDWT), and the proposed DWT. Numerical results indicated that the DWT achieved a peak power coefficient (C<sub>p</sub>) of 43.2%, an 85.4% improvement over the computationally evaluated BWT. The new duct design mitigated wake deficits, yielding an area-averaged wake velocity ratio 4.15× higher than the BWT(1.79× relative to the FDWT) at 1·5D downstream. Near-wake analysis indicated a 21-fold increase in turbulent kinetic energy compared to the BWT, reflecting enhanced local mixing. However, velocity recovery advantages were distance-dependent, with the DWT showing superior performance at 1·5D but reduced area-averaged velocity relative to the FDWT by 2·5D. This reversal reflected the DWT’s higher energy extraction, which depletes wake momentum more severely; the PFCT-induced vortices that accelerated early recovery decayed by 2·5D, leaving a more depleted wake than that of the FDWT’s gentler, sustained recovery. Consequently, the DWT demonstrated improved downstream inflow conditions for the 2D tandem configuration investigated in this study, whereas the single-turbine wake analysis indicated","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 3","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149132463","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-09-29DOI: 10.1007/s10494-026-00797-1
Saber Karimi, Babak Mohammadikalakoo, Paolo Schito
This numerical study, based on steady RANS simulations, investigates the effects of passive, active, and combined flow control techniques on a simplified vehicle model (Ahmed body) under highway-relevant configurations, including platooning and overtaking, at 70 mph (31.3 m/s). The study primarily focuses on an innovative passive flow control method, Rear Linking Tunnels (RLTs), previously introduced by the authors. It also examines the performance of the Single Dielectric Barrier Discharge Actuator (SDBD) as an active flow control strategy and evaluates its combined effects with RLTs on both the target vehicle and surrounding vehicles during platooning and overtaking maneuvers. The results highlight notable variations in drag and lift coefficients, showing that the effectiveness of these flow control methods differs significantly between platooning/overtaking scenarios and single-vehicle cases.
{"title":"Evaluating Flow Control Methods in Vehicle Platooning and Overtaking","authors":"Saber Karimi, Babak Mohammadikalakoo, Paolo Schito","doi":"10.1007/s10494-026-00797-1","DOIUrl":"10.1007/s10494-026-00797-1","url":null,"abstract":"<div><p>This numerical study, based on steady RANS simulations, investigates the effects of passive, active, and combined flow control techniques on a simplified vehicle model (Ahmed body) under highway-relevant configurations, including platooning and overtaking, at 70 mph (31.3 m/s). The study primarily focuses on an innovative passive flow control method, Rear Linking Tunnels (RLTs), previously introduced by the authors. It also examines the performance of the Single Dielectric Barrier Discharge Actuator (SDBD) as an active flow control strategy and evaluates its combined effects with RLTs on both the target vehicle and surrounding vehicles during platooning and overtaking maneuvers. The results highlight notable variations in drag and lift coefficients, showing that the effectiveness of these flow control methods differs significantly between platooning/overtaking scenarios and single-vehicle cases.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 3","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-09-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-026-00797-1.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149133136","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-09-29DOI: 10.1007/s10494-026-00795-3
Maximilian Bambauer, Josef Hasslberger, Finn Ohlendieck, Markus Klein
This study investigates the scale effect in hydrogen-air explosions using high-fidelity 2D and 3D numerical simulations with detailed chemistry. Simulations are conducted in an obstacle-laden channel, varying the geometric scaling factor, hydrogen mole fraction and dimensionality. Results show that flame acceleration increases significantly with geometric scale, primarily due to the enhanced growth of the turbulent flame surface area. Additionally, the local burning rate per unit flame area exhibits a complex dependency on scale and mixture composition, characterized by flame stretch and Markstein numbers, particularly in lean mixtures. It is found that the normalized critical distance to reach a specific velocity decreases as a power-law with increasing scale, confirming that explosions accelerate more effectively over shorter relative distances in larger facilities. While 2D simulations suggest that the corresponding power-law exponents are consistent across a wide range of equivalence ratios, 3D results reveal a critical deviation. The scale effect is significantly more pronounced in 3D than in 2D, where the flame acceleration is found to be significantly stronger and this holds particularly for lean mixtures. The findings are consistent with scale-dependent experimental results obtained in the laboratory-scale MiniRUT and the industrial-scale RUT facilities. They further demonstrate that two-dimensional approximations may substantially underpredict the scale sensitivity of lean hydrogen explosions. In this case, 3D effects are identified as crucial for accurately predicting the severity of hydrogen explosions.
{"title":"Quantifying the Scale Effect in Hydrogen/Air Explosions Using High-Fidelity Simulations with Detailed Chemistry","authors":"Maximilian Bambauer, Josef Hasslberger, Finn Ohlendieck, Markus Klein","doi":"10.1007/s10494-026-00795-3","DOIUrl":"10.1007/s10494-026-00795-3","url":null,"abstract":"<div><p>This study investigates the scale effect in hydrogen-air explosions using high-fidelity 2D and 3D numerical simulations with detailed chemistry. Simulations are conducted in an obstacle-laden channel, varying the geometric scaling factor, hydrogen mole fraction and dimensionality. Results show that flame acceleration increases significantly with geometric scale, primarily due to the enhanced growth of the turbulent flame surface area. Additionally, the local burning rate per unit flame area exhibits a complex dependency on scale and mixture composition, characterized by flame stretch and Markstein numbers, particularly in lean mixtures. It is found that the normalized critical distance to reach a specific velocity decreases as a power-law with increasing scale, confirming that explosions accelerate more effectively over shorter relative distances in larger facilities. While 2D simulations suggest that the corresponding power-law exponents are consistent across a wide range of equivalence ratios, 3D results reveal a critical deviation. The scale effect is significantly more pronounced in 3D than in 2D, where the flame acceleration is found to be significantly stronger and this holds particularly for lean mixtures. The findings are consistent with scale-dependent experimental results obtained in the laboratory-scale MiniRUT and the industrial-scale RUT facilities. They further demonstrate that two-dimensional approximations may substantially underpredict the scale sensitivity of lean hydrogen explosions. In this case, 3D effects are identified as crucial for accurately predicting the severity of hydrogen explosions.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 3","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-09-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-026-00795-3.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149133196","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-09-25DOI: 10.1007/s10494-026-00798-0
Ata Ahmadabadi, Hamed Chehrmonavari, Amirhasan Kakaee
The interaction between spray dynamics, turbulence, and combustion strongly influences the performance of compression-ignition engines operating with alternative fuels. This study employs a validated three-dimensional computational fluid dynamics (CFD) model to investigate the effects of diesel–methanol–ammonia ternary blends on in-cylinder flow, turbulent mixing, combustion characteristics, and emissions in a heavy-duty diesel engine. The simulations show that increasing ammonia content prolongs spray penetration, sustains higher turbulence kinetic energy around top dead center, and delays ignition because of its high latent heat of vaporization and low reactivity. In contrast, methanol enhances atomization, accelerates evaporation, and intensifies premixed combustion, resulting in a 7.9% increase in peak firing pressure relative to diesel. The combined action of methanol and ammonia produces more stable combustion than ammonia-only blends by moderating the pressure-rise rate while maintaining favorable heat-release characteristics. A specifically identified ternary blends improve the conventional NOₓ–soot trade-off, achieving 16.5% lower NOₓ emissions together with 3.5% lower soot emissions than neat diesel, whereas high-ammonia formulations substantially suppress soot because of their carbon-free chemistry but increase CO and unburned hydrocarbon emissions owing to slower oxidation kinetics. These results demonstrate that appropriate diesel–methanol–ammonia blending effectively tailors spray evolution, turbulence development, combustion phasing, and emission characteristics, providing valuable guidance for the design of stable and cleaner low-carbon compression-ignition combustion systems.
{"title":"Spray Evolution, Turbulent Mixing, and Combustion Behavior of Diesel–Ammonia–Methanol Ternary Fuel Blends: A CFD Study","authors":"Ata Ahmadabadi, Hamed Chehrmonavari, Amirhasan Kakaee","doi":"10.1007/s10494-026-00798-0","DOIUrl":"10.1007/s10494-026-00798-0","url":null,"abstract":"<div><p>The interaction between spray dynamics, turbulence, and combustion strongly influences the performance of compression-ignition engines operating with alternative fuels. This study employs a validated three-dimensional computational fluid dynamics (CFD) model to investigate the effects of diesel–methanol–ammonia ternary blends on in-cylinder flow, turbulent mixing, combustion characteristics, and emissions in a heavy-duty diesel engine. The simulations show that increasing ammonia content prolongs spray penetration, sustains higher turbulence kinetic energy around top dead center, and delays ignition because of its high latent heat of vaporization and low reactivity. In contrast, methanol enhances atomization, accelerates evaporation, and intensifies premixed combustion, resulting in a 7.9% increase in peak firing pressure relative to diesel. The combined action of methanol and ammonia produces more stable combustion than ammonia-only blends by moderating the pressure-rise rate while maintaining favorable heat-release characteristics. A specifically identified ternary blends improve the conventional NOₓ–soot trade-off, achieving 16.5% lower NOₓ emissions together with 3.5% lower soot emissions than neat diesel, whereas high-ammonia formulations substantially suppress soot because of their carbon-free chemistry but increase CO and unburned hydrocarbon emissions owing to slower oxidation kinetics. These results demonstrate that appropriate diesel–methanol–ammonia blending effectively tailors spray evolution, turbulence development, combustion phasing, and emission characteristics, providing valuable guidance for the design of stable and cleaner low-carbon compression-ignition combustion systems.</p><h3>Graphical Abstract</h3><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":"117 3","pages":""},"PeriodicalIF":2.2,"publicationDate":"2026-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149035340","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}