{"title":"Implicit large eddy simulations with a high-order TENO scheme","authors":"Lin Fu, Xiangyu Y. Hu, N. Adams","doi":"10.1615/tsfp10.570","DOIUrl":"https://doi.org/10.1615/tsfp10.570","url":null,"abstract":"Although TENO schemes, proposed by Fu et al. (2016), show promising results for turbulence reproduction, they are unsuitable to function as a reliable subgrid LES model by generating excessive dissipation. Meanwhile, the state-ofthe-art implicit LES models, e.g. the localized artificial diffusivity scheme by Kawai et al. (2010), typically depend on shock sensors, which are case-dependent and fail to retain the monotonicity near discontinuities. The difficulty locates on scale-separating the low-wavenumber smooth regions, high-wavenumber fluctuations and discontinuities sufficiently and incorporating adequate dissipation into numerical schemes correspondingly. In this paper, we propose a new 8-point 6th-order TENO8-A scheme, which is motivated for gas dynamics and physics-consistent for incompressible and compressible turbulence modeling. While the low-wavenumber smooth region is handled by the optimized linear scheme, with the measurement of local flow scales, the high-wavenumber fluctuations and discontinuities are predicted with adaptive nonlinear dissipation. The new scheme is Galilean invariant and free from physics-based sensors rendering its high generality. Benchmark simulations demonstrate that, while the TENO8-A scheme exhibits exceptional performance in gas dynamics, it faithfully reproduces the kinetic energy evolution for incompressible turbulence and predicts the vorticity, entropy and acoustic modes as good as the physics-motivated ILES models for compressible turbulence decay. REFERENCES Fu, Lin, Hu, Xiangyu Y & Adams, Nikolaus A 2016 A family of high-order targeted eno schemes for compressible-fluid simulations. Journal of Computational Physics 305, 333–359. Kawai, Soshi, Shankar, Santhosh K & Lele, Sanjiva K 2010 Assessment of localized artificial diffusivity scheme for large-eddy simulation of compressible turbulent flows. Journal of Computational Physics 229 (5), 1739–1762.","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"126 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115463205","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"INFLUENCE OF LARGE-SCALE LOW- AND HIGH-SPEED STRUCTURES ON A TURBULENT BOUNDARY LAYER","authors":"Jinyul Hwang, H. Sung","doi":"10.1615/tsfp10.250","DOIUrl":"https://doi.org/10.1615/tsfp10.250","url":null,"abstract":"Direct numerical simulation data of a turbulent boundary layer (Reτ ≈ 1000) are used to explore the influences of large-scale structures on the near-wall vortical motions. The large-scale streamwise velocity fluctuations (ul) are extracted by employing a spanwise wavelength filter (λz/δ > 0.5). The r.m.s. of the streamwise swirling strength (λx) is conditionally sampled as a function of the strength of ul. The streamwise swirling strength is attenuated or amplified under the negativeor positive-ul events in the nearwall region, respectively. The asymmetric influence of the large scales on the near-wall region is due to the associated spanwise motions within the footprints of ul, i.e., the congregative and dispersive motions induced by the outer large-scale low(ul < 0) and high-speed structures, respectively (Hwang et al. 2016). The dispersive motions are more intense than the congregative motions because the positive-ul motions toward the wall (sweep) lead to an enhancement of the spanwise momentum. Conditionally averaged velocity fields associated with the vortical structures under the footprints show that the modulated swirling motions lie within the congregative and dispersive motions. The intense dispersive motions under the positive-ul event strengthen the smallscale spanwise velocity fluctuations (ws) close to the wall compared to ws associated with the attenuated vortical motions under the congregative motion. In addition, the wall-normal velocity components around the near-wall swirling motions are attenuated or amplified, which is attributed to the modulation of λx on the large scales. We quantify the contribution of the modulated vortical motions to the skin friction by employing the decomposition method of Yoon et al. (2016). The velocity-vorticity correlation","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"66 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"131366462","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"On the scaling of turbulent asymptotic suction boundary layers","authors":"Marco Ferro, B. Fallenius, J. Fransson","doi":"10.1615/tsfp10.1070","DOIUrl":"https://doi.org/10.1615/tsfp10.1070","url":null,"abstract":"An analysis of turbulent suction boundary layers is carried out on the basis of new experimental data. The streamwise extent of the suction region of the present experimental apparatus is significa ...","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"155 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"127338811","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"COMPUTATION OF WALL PRESSURE SPECTRA FROM CFD RANS SOLUTIONS INDUCED BY INCOMPRESSIBLE TURBULENT BOUNDARY LAYERS","authors":"M. Slama, C. Leblond, P. Sagaut","doi":"10.1615/tsfp10.680","DOIUrl":"https://doi.org/10.1615/tsfp10.680","url":null,"abstract":"A method is developed to compute the wall pressure spectrum under a turbulent boundary layer based on RANS solutions. HighReynolds number flows, such as the ones encountered in naval architecture studies, are considered. The model solves a specific equation for the wall pressure, based on the integral solution of a Poisson equation. A new model is proposed, the Extended Anisotropic Model (EAM), for the space-time velocity correlations which are necessary in order to close the equation. The method is applied to a turbulent boundary layer flow over a flat plate and satisfying results are obtained for the frequency pressure spectrum.","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"27 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"126559569","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
F. Stylianou, S. Angeli, S. Kassinos, Mårten Svensson
{"title":"THE EFFECT OF FLOW RATE, HEAD POSITION, AND INHALER ORIENTATION ON THE AIRFLOW AND PARTICLE DEPOSITION IN AN MRI-BASED MOUTH-THROAT GEOMETRY","authors":"F. Stylianou, S. Angeli, S. Kassinos, Mårten Svensson","doi":"10.1615/tsfp10.390","DOIUrl":"https://doi.org/10.1615/tsfp10.390","url":null,"abstract":"","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"51 3 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"117346633","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Direct numerical simulation of a turbulent curved pipe flow with a 90° bend","authors":"Yongmann M. Chung, Zhixin Wang","doi":"10.1615/tsfp10.920","DOIUrl":"https://doi.org/10.1615/tsfp10.920","url":null,"abstract":"Direct numerical simulations (DNS) have been performed for a turbulent curved pipe flow going through a 90◦ bend at Reynolds number ReD = 5300 (or Reτ = 180). The swirl switching phenomenon downstream of the bend is investigated. Mean turbulence statistics in both upstream and downstream of the bend are compared with available DNS and experimental data, and very good agreements have been achieved. Two significant force oscillations in the downstream of the bend are observed: spatial oscillation along the flow direction and temporal oscillation at pipe cross-sections. It is found that the quasi-periodic force oscillation is closely associated with the unsteady motions of Dean vortices. Conditional-averaged flow fields based on positive and negative forces show mirror states of the Dean vortices with one of them being suppressed. It is also observed that the mean flow oscillation is strongly linked with the swirl switching phenomenon.","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"212 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123387934","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Inferring the structural properties of eddies in the log layer from spectral statistics","authors":"L. Agostini, M. Leschziner","doi":"10.1615/tsfp10.1110","DOIUrl":"https://doi.org/10.1615/tsfp10.1110","url":null,"abstract":"The structure of near-wall layers has been the subject of much research over many years, with conceptual descriptions of the Attached Eddy Hypothesis (AEH, henceforth) by Townsend (1980) and Perry & Chong (1982) being key historical fix points. The fact that major efforts have continued unabated over the past two to three decades reflects the exceptional structural complexity of near-wall layers awaiting insight, as well as new opportunities to investigate open questions as a consequence of outstandingly high-quality experimental and DNS data emerging over the past decade (Marusic et al. (2013); Smits et al. (2011); Hultmark et al. (2013); Rosenberg et al. (2013); Jiménez & Hoyas (2008); Lee & Moser (2015)). In particular, the availability of massive amounts of spatially and temporally fully-resolved raw DNS data for fairly high Reynolds numbers has opened new routes to investigating many statistical and structural properties of near-wall layers, with the objective of unravelling a variety of scale-interaction processes.","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"04 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"128990453","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Direct Numerical Simulation of Shock-Induced Drop Breakup with a Sharp-Interface-Method","authors":"J. Kaiser, S. Adami, N. Adams","doi":"10.1615/tsfp10.490","DOIUrl":"https://doi.org/10.1615/tsfp10.490","url":null,"abstract":"We present twoand three-dimensional numerical results of the shock-induced breakup of a liquid droplet in air. We apply a conservative interface interaction model for sharp-interface representation and a block-based multi-resolution scheme to adaptively refine our mesh. Numerical modeling effects, such as the flux reconstruction scheme and the use of a scale separation model, that treats non-resolved interface segments, are investigated. Similarly as a previous study (Meng, 2016), we identify two dominant mechanisms of droplet breakup at certain Mach numbers flattening of the droplet and sheet stripping occurring simultaneously and influencing each other in our simulations. Three-dimensional simulations show the flattening mechanism and the mushroom-like deformation of the droplet. They also explain the occurrence of a recirculation zone in the droplet wake. The two-dimensional simulations already exhibit the sheet stripping mechanism, which occurs during and after droplet flattening. Small sheets emerge from both the upstream and the downstream side of the water column, while the main sheet develops at the droplet equator.","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"21 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124636121","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Reappraisal of the asymptotic state of a zero pressure gradient turbulent boundary layer","authors":"L. Djenidi, K. Talluru, R. Antonia","doi":"10.1615/tsfp10.260","DOIUrl":"https://doi.org/10.1615/tsfp10.260","url":null,"abstract":"","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"10 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"121807175","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Volume 2The Structure Of Turbulent Flows In Wind Farms","authors":"C. Meneveau","doi":"10.1615/tsfp10.630","DOIUrl":"https://doi.org/10.1615/tsfp10.630","url":null,"abstract":"In this presentation we provide an overview of our current understanding of the flow structure and turbulence in the wind turbine array boundary layer (WTABL). This particular type of shear flow develops when the atmospheric boundary layer interacts with an array of large wind turbines (Calaf et al. 2010, Cal et al. 2010, Stevens & Meneveau 2017). We distinguish between developing and fully developed WTABL and perform a series of Large Eddy Simulations that represent the turbines as actuator disks (see Figure 1 below). Salient LES results are synthesized in order to develop simplified analytical models needed for wind farm design and optimization. There one encounters the dichotomy of modeling individual turbine wakes or to model the wind farm flow as a boundary layer over a roughened surface whose properties depend upon the wind farm array. The coupled wake boundary layer model (Stevens et al. 2016a) attempts to match these two approaches iteratively. Ultimately, such models can lead to improved estimation of optimal wind turbine spacing including costs associated with covered surface, cabling and operation & maintenance (Stevens et al. 2016b). We also present new results on the temporal variability of wind power as measured in a wind tunnel experiment (Bossuyt et al. 2017) and its relationship to the spatio-temporal properties of turbulent boundary layers (Wilzcek et al. 2015). It turns out that as a first approximation, for situations without thermal stratification effects, one may consider the sum of turbine power to be a discrete sampling of the wavenumber-frequency spectrum of turbulent boundary layers. This model thus enables us to connect wind farm design parameters (turbine spacing, positioning, etc.) to fundamental properties of turbulent boundary layers.","PeriodicalId":266791,"journal":{"name":"Proceeding of Tenth International Symposium on Turbulence and Shear Flow Phenomena","volume":"23 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115821351","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}