Air intakes are an integral part of contemporary passenger and military aircraft engines. Their impact on aerodynamic performance across the entire flight envelope is critical to aircraft flight safety, efficiency, and manoeuvrability, especially at high Mach numbers due to shock waves. The high demand for reductions in aircraft weight and size and enhancements in durability, comfort, and thermal and radar signatures compel researchers and engineers to explore new designs and develop efficient air intakes for high-performance aircraft engines. Although a number of studies on air intake have been conducted and reported in the open literature, there is little information available in the public domain on bifurcated twin air intakes using synthetic jet. As a result, the primary goal of this research is to use computational fluid dynamics modelling to investigate the effects of synthetic jets on swirl inflow variable geometry twin air intake aerodynamic performance over a range of Reynolds numbers. Some important parameters (distortion coefficient, non-uniformity index, swirl coefficient, and static and total pressure coefficients) were investigated. Both static and total pressure recovery have been increased at all swirl numbers. A significant decrease in distortion coefficient and swirl coefficient has also been achieved, reaching a 53% reduction in the distortion coefficient and a 62% reduction in the swirl coefficient. The reduction in the non-uniformity index is achieved by 62% for the controlled flow case. The findings show that synthetic jets are effective in controlling the flow separation in the twin air intakes and enhancing aerodynamic performance.
{"title":"Effects of Synthetic Jets on Swirl Inflow in a Variable-Geometry Twin Air-Intake","authors":"Krishna Kumar Rajnath Yadav, Akshoy Ranjan Paul, Anuj Jain, Firoz Alam","doi":"10.1007/s10494-023-00481-8","DOIUrl":"10.1007/s10494-023-00481-8","url":null,"abstract":"<div><p>Air intakes are an integral part of contemporary passenger and military aircraft engines. Their impact on aerodynamic performance across the entire flight envelope is critical to aircraft flight safety, efficiency, and manoeuvrability, especially at high Mach numbers due to shock waves. The high demand for reductions in aircraft weight and size and enhancements in durability, comfort, and thermal and radar signatures compel researchers and engineers to explore new designs and develop efficient air intakes for high-performance aircraft engines. Although a number of studies on air intake have been conducted and reported in the open literature, there is little information available in the public domain on bifurcated twin air intakes using synthetic jet. As a result, the primary goal of this research is to use computational fluid dynamics modelling to investigate the effects of synthetic jets on swirl inflow variable geometry twin air intake aerodynamic performance over a range of Reynolds numbers. Some important parameters (distortion coefficient, non-uniformity index, swirl coefficient, and static and total pressure coefficients) were investigated. Both static and total pressure recovery have been increased at all swirl numbers. A significant decrease in distortion coefficient and swirl coefficient has also been achieved, reaching a 53% reduction in the distortion coefficient and a 62% reduction in the swirl coefficient. The reduction in the non-uniformity index is achieved by 62% for the controlled flow case. The findings show that synthetic jets are effective in controlling the flow separation in the twin air intakes and enhancing aerodynamic performance.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2023-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-023-00481-8.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136309883","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 : 2023-09-20DOI: 10.1007/s10494-023-00490-7
Sergey Golovastov, Grigory Bivol, Fyodor Kuleshov, Artem Elyanov, Victor Golub
This paper presents experimental investigations of the polyurethane foam influence on the combustion dynamics of hydrogen-air flames propagating in a channel with a sudden change in cross-section (i.e. expansion). The channel is open at both ends. Porous media of various lengths and pore size are considered. The porous inserts are placed downstream of the sudden expansion, inside the diagnostic section of dimensions 20 × 40 mm. A Schlieren visualization technique is used to monitor flame shape and propagation dynamics. Various equivalence ratios ranging from 0.3 to 1.0 are tested. The results show that depending on the equivalence ratio, porous length and pore size, the mixture can either propagate throughout the foam or be quenched. In propagating regime, it is found that the output velocity just behind the foam increases linearly with porous matrix length, indicating that the tortuous flow within the foam plays a significant role in the propagation of the flame. These results could be used both to increase the efficiency of gaseous combustion and to ensure the explosion safety of the gas equipment.
{"title":"Flame Front Dynamics in Flow of Hydrogen-Air Mixture in a Channel with Sudden Expansion and Polyurethane Foam","authors":"Sergey Golovastov, Grigory Bivol, Fyodor Kuleshov, Artem Elyanov, Victor Golub","doi":"10.1007/s10494-023-00490-7","DOIUrl":"10.1007/s10494-023-00490-7","url":null,"abstract":"<div><p>This paper presents experimental investigations of the polyurethane foam influence on the combustion dynamics of hydrogen-air flames propagating in a channel with a sudden change in cross-section (i.e. expansion). The channel is open at both ends. Porous media of various lengths and pore size are considered. The porous inserts are placed downstream of the sudden expansion, inside the diagnostic section of dimensions 20 × 40 mm. A Schlieren visualization technique is used to monitor flame shape and propagation dynamics. Various equivalence ratios ranging from 0.3 to 1.0 are tested. The results show that depending on the equivalence ratio, porous length and pore size, the mixture can either propagate throughout the foam or be quenched. In propagating regime, it is found that the output velocity just behind the foam increases linearly with porous matrix length, indicating that the tortuous flow within the foam plays a significant role in the propagation of the flame. These results could be used both to increase the efficiency of gaseous combustion and to ensure the explosion safety of the gas equipment.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2023-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136309334","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 : 2023-09-16DOI: 10.1007/s10494-023-00480-9
Ted Sian Lee, Ean Hin Ooi, Wei Sea Chang, Ji Jinn Foo
The unravelling of multilength-scale insert-generated turbulence, particularly, the induced-forcing plays critical role in the fundamental comprehension of energy formation and decay as a function of grid conformation. This study experimentally investigates the flow mechanical characteristics at ReDh = 4.1 × 104 for a regular-grid (RG), single-square-grid (SSG) and six 2D planar space-filling square-fractal-grids (SFG) of different fractal iterations (N), thickness ratios (tr) and blockage ratios (σ) via piezoelectric thin-film flapping velocimetry (PTFV). Thin-film’s tip-deflection (δrms) and voltage response (Vrms) analysis along the grids’ centreline reveals increasing flow fluctuation strength with increasing σ, tr and decreasing N, owing to higher shedding intensity of lower frequency, larger scale energy-containing vortices from thicker first iteration bar. However, higher: energy dissipation rate, centreline mean velocity decrement rate and local deceleration experienced in the turbulence decay region of larger tr grid, along with additional fractal scales lead to less potent flow-structure-interplay on thin-film undulation. More importantly, SSG-generated turbulence enables the generation of average (Vrms, δrms) and millinewton turbulence forcing Frms that are respectively, 9× and 5× larger than RG of similar σ, and 2× larger than the best performing N = 3 SFG. Our findings disclose the importance of grid geometrical management for effective utilisation of turbulence-generating grids in engineering applications.
{"title":"Realisation of Fractal Grid-Induced Turbulence Strength with PTFV: Effects of Grid Geometry","authors":"Ted Sian Lee, Ean Hin Ooi, Wei Sea Chang, Ji Jinn Foo","doi":"10.1007/s10494-023-00480-9","DOIUrl":"10.1007/s10494-023-00480-9","url":null,"abstract":"<div><p>The unravelling of multilength-scale insert-generated turbulence, particularly, the induced-forcing plays critical role in the fundamental comprehension of energy formation and decay as a function of grid conformation. This study experimentally investigates the flow mechanical characteristics at <i>Re</i><sub><i>Dh</i></sub> = 4.1 × 10<sup>4</sup> for a regular-grid (RG), single-square-grid (SSG) and six 2D planar space-filling square-fractal-grids (SFG) of different fractal iterations (<i>N</i>), thickness ratios (<i>t</i><sub><i>r</i></sub>) and blockage ratios (<i>σ</i>) via piezoelectric thin-film flapping velocimetry (PTFV). Thin-film’s tip-deflection (<i>δ</i><sub><i>rms</i></sub>) and voltage response (<i>V</i><sub><i>rms</i></sub>) analysis along the grids’ centreline reveals increasing flow fluctuation strength with increasing <i>σ</i>, <i>t</i><sub><i>r</i></sub> and decreasing <i>N</i>, owing to higher shedding intensity of lower frequency, larger scale energy-containing vortices from thicker first iteration bar. However, higher: energy dissipation rate, centreline mean velocity decrement rate and local deceleration experienced in the turbulence decay region of larger <i>t</i><sub><i>r</i></sub> grid, along with additional fractal scales lead to less potent flow-structure-interplay on thin-film undulation. More importantly, SSG-generated turbulence enables the generation of average (<i>V</i><sub><i>rms</i></sub>, <i>δ</i><sub><i>rms</i></sub>) and millinewton turbulence forcing <i>F</i><sub><i>rms</i></sub> that are respectively, 9× and 5× larger than RG of similar <i>σ</i>, and 2× larger than the best performing <i>N</i> = 3 SFG. Our findings disclose the importance of grid geometrical management for effective utilisation of turbulence-generating grids in engineering applications.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2023-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-023-00480-9.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135307081","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}
Abstract A direct numerical simulation of a three-dimensional diffuser at Reynolds number Re = 10,000 (based on inlet bulk velocity) has been performed using a low-dissipation finite element code. The geometry chosen for this work is the Stanford diffuser, introduced by Cherry et al. (Int. J. Heat Fluid Flow 29:803–811, 2008). Results have been exhaustively compared with the published data with a quite good agreement. Additionally, further turbulent statistics have been provided such as the Reynolds stresses or the turbulent kinetic energy. A proper orthogonal decomposition and a dynamic mode decomposition analyses of the main flow variables have been performed to identify the main characteristics of the large-scale motions. A combined, self-induced movement of the large-scales has been found to originate in the top-right expansion corner with two clear features. A low-frequency diagonal cross-stream travelling wave first reported by Malm et al. (J. Fluid Mech. 699:320–351, 2012), has been clearly identified in the spatial modes of the stream-wise velocity components and the pressure, associated with the narrow band frequency of $$St in [0.083,0.01]$$ St∈[0.083,0.01] . This movement is caused by the geometrical expansion of the diffuser in the cross-stream direction. A second low-frequency trait has been identified associated with the persisting secondary flows and acting as a back and forth global accelerating-decelerating motion located on the straight area of the diffuser, with associated frequencies of $$St < 0.005$$ St<0.005 . The smallest frequency observed in this work has been $$St = 0.0013$$ St=0.0013 . This low-frequency observed in the Stanford diffuser points out the need for longer simulations in order to obtain further turbulent statistics.
摘要采用低耗散有限元程序对雷诺数Re = 10,000(基于入口体速度)的三维扩散器进行了直接数值模拟。这项工作选择的几何形状是斯坦福扩散器,由Cherry等人介绍。[j] .热流体学报,2008(2)。结果已与已发表的数据进行了详尽的比较,结果相当一致。此外,还提供了进一步的湍流统计,如雷诺应力或湍流动能。通过适当的正交分解和主要流动变量的动态模态分解分析,确定了大尺度运动的主要特征。我们发现,大尺度的联合自生运动起源于右上角的膨胀角,具有两个明显的特征。Malm等人(J. Fluid Mech. 699:320-351, 2012)首次报道了一种低频对角横流行波,该行波在流向速度分量和压力的空间模态中得到了清晰的识别,其窄带频率为$$St in [0.083,0.01]$$ S t∈[0.083,0.01]。这种运动是由扩散器在横流方向上的几何膨胀引起的。第二个低频特征与持续的二次流有关,并作为位于扩散器直线区域的来回全球加减速运动,相关频率为$$St < 0.005$$ S &lt;0.005。在这项工作中观察到的最小频率为$$St = 0.0013$$ S t = 0.0013。在斯坦福扩散器中观察到的这种低频指出,为了获得进一步的湍流统计数据,需要更长的模拟时间。
{"title":"Self-Induced Large-Scale Motions in a Three-Dimensional Diffuser","authors":"Arnau Miró, Benet Eiximeno, Ivette Rodríguez, Oriol Lehmkuhl","doi":"10.1007/s10494-023-00483-6","DOIUrl":"https://doi.org/10.1007/s10494-023-00483-6","url":null,"abstract":"Abstract A direct numerical simulation of a three-dimensional diffuser at Reynolds number Re = 10,000 (based on inlet bulk velocity) has been performed using a low-dissipation finite element code. The geometry chosen for this work is the Stanford diffuser, introduced by Cherry et al. (Int. J. Heat Fluid Flow 29:803–811, 2008). Results have been exhaustively compared with the published data with a quite good agreement. Additionally, further turbulent statistics have been provided such as the Reynolds stresses or the turbulent kinetic energy. A proper orthogonal decomposition and a dynamic mode decomposition analyses of the main flow variables have been performed to identify the main characteristics of the large-scale motions. A combined, self-induced movement of the large-scales has been found to originate in the top-right expansion corner with two clear features. A low-frequency diagonal cross-stream travelling wave first reported by Malm et al. (J. Fluid Mech. 699:320–351, 2012), has been clearly identified in the spatial modes of the stream-wise velocity components and the pressure, associated with the narrow band frequency of $$St in [0.083,0.01]$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:mi>S</mml:mi> <mml:mi>t</mml:mi> <mml:mo>∈</mml:mo> <mml:mo>[</mml:mo> <mml:mn>0.083</mml:mn> <mml:mo>,</mml:mo> <mml:mn>0.01</mml:mn> <mml:mo>]</mml:mo> </mml:mrow> </mml:math> . This movement is caused by the geometrical expansion of the diffuser in the cross-stream direction. A second low-frequency trait has been identified associated with the persisting secondary flows and acting as a back and forth global accelerating-decelerating motion located on the straight area of the diffuser, with associated frequencies of $$St < 0.005$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:mi>S</mml:mi> <mml:mi>t</mml:mi> <mml:mo><</mml:mo> <mml:mn>0.005</mml:mn> </mml:mrow> </mml:math> . The smallest frequency observed in this work has been $$St = 0.0013$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:mi>S</mml:mi> <mml:mi>t</mml:mi> <mml:mo>=</mml:mo> <mml:mn>0.0013</mml:mn> </mml:mrow> </mml:math> . This low-frequency observed in the Stanford diffuser points out the need for longer simulations in order to obtain further turbulent statistics.","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"134912487","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 : 2023-09-12DOI: 10.1007/s10494-023-00487-2
Thomas Lesaffre, Antoine Pestre, Eleonore Riber, Bénédicte Cuenot
{"title":"Correction Methods for Exchange Source Terms in Unstructured Euler-Lagrange Solvers with Point-Source Approximation","authors":"Thomas Lesaffre, Antoine Pestre, Eleonore Riber, Bénédicte Cuenot","doi":"10.1007/s10494-023-00487-2","DOIUrl":"https://doi.org/10.1007/s10494-023-00487-2","url":null,"abstract":"","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135878201","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 : 2023-09-12DOI: 10.1007/s10494-023-00479-2
Nilanjan Chakraborty, Nedunchezian Swaminathan, Salvador Navarro-Martinez
{"title":"Advances in Computational Combustion: The UK Consortium on Turbulent Reacting Flows","authors":"Nilanjan Chakraborty, Nedunchezian Swaminathan, Salvador Navarro-Martinez","doi":"10.1007/s10494-023-00479-2","DOIUrl":"10.1007/s10494-023-00479-2","url":null,"abstract":"","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2023-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"7183960","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 : 2023-09-12DOI: 10.1007/s10494-023-00478-3
Georgios Giamagas, Francesco Zonta, Alessio Roccon, Alfredo Soldati
Abstract We investigate the dynamics of turbulence and interfacial waves in an oil–water channel flow. We consider a stratified configuration, in which a thin layer of oil flows on top of a thick layer of water. The oil–water interface that separates the two layers mutually interacts with the surrounding flow field, and is characterized by the formation and propagation of interfacial waves. We perform direct numerical simulation of the Navier-Stokes equations coupled with a phase field method to describe the interface dynamics. For a given shear Reynolds number, $$Re_tau =300$$ Reτ=300 , and Weber number, $$We=0.5$$ We=0.5 , we consider three different types of oils, characterized by different viscosities, and thus different oil-to-water viscosity ratios $$mu _r=mu _o/mu _w$$ μr=μo/μw (being $$mu _o$$ μo and $$mu _w$$ μw oil and water viscosities). Starting from a matched viscosity case, $$mu _r=1$$ μr=1 , we increase the oil-to-water viscosity ratio up to $$mu _r=100$$ μr=100 . By increasing $$mu _r$$ μr , we observe significant changes both in turbulence and in the dynamics of the oil–water interface. In particular, the large viscosity of oil controls the flow regime in the thin oil layer, as well as the turbulence activity in the thick water layer, with direct consequences on the overall channel flow rate, which decreases when the oil viscosity is increased. Correspondingly, we observe remarkable changes in the dynamics of waves that propagate at the oil–water interface. In particular, increasing the viscosity ratio from $$mu _r=1$$
摘要研究了油水通道流动中的湍流和界面波动力学。我们考虑一个分层结构,其中一层薄薄的油流在一层厚厚的水上面。分隔两层的油水界面与周围流场相互作用,其特征是界面波的形成和传播。本文采用相场法对Navier-Stokes方程进行了直接数值模拟来描述界面动力学。对于给定的剪切雷诺数$$Re_tau =300$$ Re τ = 300和韦伯数$$We=0.5$$ We = 0.5,我们考虑了三种不同类型的油,它们具有不同的粘度,因此油水粘度比$$mu _r=mu _o/mu _w$$ μ R = μ o / μ W(分别为$$mu _o$$ μ o和$$mu _w$$ μ W)。从匹配粘度情况$$mu _r=1$$ μ r = 1开始,我们将油水粘度比提高到$$mu _r=100$$ μ r = 100。通过增大$$mu _r$$ μ r,我们观察到湍流和油水界面动力学的显著变化。特别是,油的大粘度控制了薄油层的流动状态,以及厚水层的湍流活动,直接影响了通道的总流速,当油的粘度增加时,通道的总流速会降低。相应地,我们观察到在油水界面传播的波的动力学发生了显著变化。特别是当黏度比从$$mu _r=1$$ μ r = 1增加到$$mu _r=100$$ μ r = 100时,波从二维的几乎各向同性的模式转变为几乎单色的模式。
{"title":"Turbulence and Interface Waves in Stratified Oil–Water Channel Flow at Large Viscosity Ratio","authors":"Georgios Giamagas, Francesco Zonta, Alessio Roccon, Alfredo Soldati","doi":"10.1007/s10494-023-00478-3","DOIUrl":"https://doi.org/10.1007/s10494-023-00478-3","url":null,"abstract":"Abstract We investigate the dynamics of turbulence and interfacial waves in an oil–water channel flow. We consider a stratified configuration, in which a thin layer of oil flows on top of a thick layer of water. The oil–water interface that separates the two layers mutually interacts with the surrounding flow field, and is characterized by the formation and propagation of interfacial waves. We perform direct numerical simulation of the Navier-Stokes equations coupled with a phase field method to describe the interface dynamics. For a given shear Reynolds number, $$Re_tau =300$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:mi>R</mml:mi> <mml:msub> <mml:mi>e</mml:mi> <mml:mi>τ</mml:mi> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>300</mml:mn> </mml:mrow> </mml:math> , and Weber number, $$We=0.5$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:mi>W</mml:mi> <mml:mi>e</mml:mi> <mml:mo>=</mml:mo> <mml:mn>0.5</mml:mn> </mml:mrow> </mml:math> , we consider three different types of oils, characterized by different viscosities, and thus different oil-to-water viscosity ratios $$mu _r=mu _o/mu _w$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>r</mml:mi> </mml:msub> <mml:mo>=</mml:mo> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>o</mml:mi> </mml:msub> <mml:mo>/</mml:mo> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>w</mml:mi> </mml:msub> </mml:mrow> </mml:math> (being $$mu _o$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>o</mml:mi> </mml:msub> </mml:math> and $$mu _w$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>w</mml:mi> </mml:msub> </mml:math> oil and water viscosities). Starting from a matched viscosity case, $$mu _r=1$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>r</mml:mi> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:math> , we increase the oil-to-water viscosity ratio up to $$mu _r=100$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>r</mml:mi> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>100</mml:mn> </mml:mrow> </mml:math> . By increasing $$mu _r$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:msub> <mml:mi>μ</mml:mi> <mml:mi>r</mml:mi> </mml:msub> </mml:math> , we observe significant changes both in turbulence and in the dynamics of the oil–water interface. In particular, the large viscosity of oil controls the flow regime in the thin oil layer, as well as the turbulence activity in the thick water layer, with direct consequences on the overall channel flow rate, which decreases when the oil viscosity is increased. Correspondingly, we observe remarkable changes in the dynamics of waves that propagate at the oil–water interface. In particular, increasing the viscosity ratio from $$mu _r=1$$ <mml:m","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135826441","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}
Abstract Spatially and temporally resolved velocity measurements in wall-bounded turbulent flows remain a challenge. Contrary to classical laser Doppler velocimetry (LDV) measurements, the laser Doppler velocity profile sensor (LDV-PS) allows the combined measurement of tracer particle position and velocity, which makes it a promising tool. To assess its feasibility a commercial LDV-PS is employed in a turbulent channel flow at $$Re_tau =350$$ Reτ=350 . Additionally, the measurement and signal-processing accuracies of velocity and location are evaluated for various tracer-object sizes and velocities. On this basis, the turbulent channel flow measurements are evaluated and compared to reference data from direct numerical simulations. Thus, potentials of the LDV-PS are investigated for different regions of the flow and various data processing routines as well as the experimental practice are discussed from an application perspective.
在有壁湍流中进行空间和时间分辨速度测量仍然是一个挑战。与传统的激光多普勒测速(LDV)测量相反,激光多普勒速度剖面传感器(LDV- ps)允许对示踪粒子的位置和速度进行组合测量,这使其成为一种很有前途的工具。为了评估其可行性,在$$Re_tau =350$$ R e τ = 350的湍流通道流动中使用了商用LDV-PS。此外,速度和位置的测量和信号处理精度对不同的示踪物体的大小和速度进行了评估。在此基础上,对湍流通道的流量测量结果进行了评价,并与直接数值模拟的参考数据进行了比较。因此,本文研究了LDV-PS在不同流动区域的潜力,并从应用的角度讨论了各种数据处理程序和实验实践。
{"title":"Measurements in a Turbulent Channel Flow by Means of an LDV Profile Sensor","authors":"Saskia Pasch, Robin Leister, Davide Gatti, Ramis Örlü, Bettina Frohnapfel, Jochen Kriegseis","doi":"10.1007/s10494-023-00469-4","DOIUrl":"https://doi.org/10.1007/s10494-023-00469-4","url":null,"abstract":"Abstract Spatially and temporally resolved velocity measurements in wall-bounded turbulent flows remain a challenge. Contrary to classical laser Doppler velocimetry (LDV) measurements, the laser Doppler velocity profile sensor (LDV-PS) allows the combined measurement of tracer particle position and velocity, which makes it a promising tool. To assess its feasibility a commercial LDV-PS is employed in a turbulent channel flow at $$Re_tau =350$$ <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"> <mml:mrow> <mml:mi>R</mml:mi> <mml:msub> <mml:mi>e</mml:mi> <mml:mi>τ</mml:mi> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>350</mml:mn> </mml:mrow> </mml:math> . Additionally, the measurement and signal-processing accuracies of velocity and location are evaluated for various tracer-object sizes and velocities. On this basis, the turbulent channel flow measurements are evaluated and compared to reference data from direct numerical simulations. Thus, potentials of the LDV-PS are investigated for different regions of the flow and various data processing routines as well as the experimental practice are discussed from an application perspective.","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135982589","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}
Compressible vortex rings have been widely investigated for decades under ambient atmospheric conditions, and understanding this transient phenomenon is important for improving the thrust vector and avoiding surface impingement and contamination. However, how the vortex ring behaves in a reduced pressure environment remains unknown. This work provides schlieren imaging and pressure measurement results of the vortex ring when the environmental pressure is lower than 1 atm. The basic structure of the compressible vortex ring in low-pressure environments has been captured. The reduced environmental pressure will degenerate the internal flow structure, including the shock wave, the CRVRs, and the vortices due to the Kelvin–Helmholtz instability, which is consistent with the conclusion of previous numerical work. The vortex ring is confirmed to exist when the environmental pressure is approximately 1.0 kPa.
{"title":"Vortex Ring Formation Following Shock Wave Diffraction in Low-Pressure Environments","authors":"Ziqu Cao, Konstantinos Kontis, Hamid Hosano, Craig White, Ting-Tsung Chang, Muhammed Burak Agir","doi":"10.1007/s10494-023-00486-3","DOIUrl":"10.1007/s10494-023-00486-3","url":null,"abstract":"<div><p>Compressible vortex rings have been widely investigated for decades under ambient atmospheric conditions, and understanding this transient phenomenon is important for improving the thrust vector and avoiding surface impingement and contamination. However, how the vortex ring behaves in a reduced pressure environment remains unknown. This work provides schlieren imaging and pressure measurement results of the vortex ring when the environmental pressure is lower than 1 atm. The basic structure of the compressible vortex ring in low-pressure environments has been captured. The reduced environmental pressure will degenerate the internal flow structure, including the shock wave, the CRVRs, and the vortices due to the Kelvin–Helmholtz instability, which is consistent with the conclusion of previous numerical work. The vortex ring is confirmed to exist when the environmental pressure is approximately 1.0 kPa.</p></div>","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2023-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10494-023-00486-3.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136191867","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 : 2023-09-09DOI: 10.1007/s10494-023-00472-9
Florian R. Menter, Andreas Hüppe, David Flad, Andrey V. Garbaruk, Alexey A. Matyushenko, Andrey S. Stabnikov
{"title":"Large Eddy Simulations for the Ahmed Car at 25° Slant Angle at Different Reynolds Numbers","authors":"Florian R. Menter, Andreas Hüppe, David Flad, Andrey V. Garbaruk, Alexey A. Matyushenko, Andrey S. Stabnikov","doi":"10.1007/s10494-023-00472-9","DOIUrl":"https://doi.org/10.1007/s10494-023-00472-9","url":null,"abstract":"","PeriodicalId":559,"journal":{"name":"Flow, Turbulence and Combustion","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136192200","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}