{"title":"周期强迫诱导入流的湍流混合层直接数值模拟","authors":"Y. Kametani, Masayuki Kawagoe, K. Fukagata","doi":"10.1615/tsfp8.2140","DOIUrl":null,"url":null,"abstract":"The direct numerical simulation of the turbulent mixing layer with periodically-forced inflow is performed. The angular frequency Ωc was set as a control parameter. To compare the experimental study of Naka et al. (2010), the angular frequency is set to be Ω = 0.83 (Case A) and 3.85 (Case B). In the present simulation, the momentum thickness shows the Case A achieved the mixing enhancement, while Case B achieves its suppression. Due to the both controls, the Reynolds normal shear stress, especially v′v′ increases behind the periodic forcing. The Reynolds shear stress u′v′ is suppressed in the Case B at downstream. This region is agree with that the mixing suppression is found in the momentum thickness. Furthermore, the anisotropic tensor indicates that two dimensional large coherent structure is generated in the Case B in which mixing was suppressed. Introduction A mixing layer is one of the fundamental free shear flow generated by the velocity gap (Brown & Roshko (2009)). In order to understand the vortex dynamics in shear flows, mixing layers have extensively been studied since Brown & Roshko (1974) experimentally visualized the coherent structure in turbulent mixing layers. Huang & Ho (1990) experimentally studied an acoustically perturbed laminar mixing layer and observed small-scale turbulence created due to interaction of spanwise and streamwise structures after the merging of spanwise vortices. Turbulent mixing layers can be found in various practical applications: e.g., inside combustion chambers and around the exhaust of turbo engines. Techniques for mixing enhancement or suppression are sometimes needed for efficient combustion or noise reduction. Ho (1982) attempted to control the mixing layer by perturbing the flow rates of inflows. They show that the spreading rate of a mixing layer can be manipulated at very low forcing level if the mixing layer is perturbed near a subharmonic of the most-amplified frequency. Naka et al. (2010) studied a mixing layer periodically forced by using a flap-type actuator made of piezoplastic (Polyvinylidene fluoride: PVDF) film aiming at both enhancement and suppression of mixing. They conclude that at some parameters of forcing mixing suppression can also be achieved. In the present study, direct numerical simulation (DNS) of turbulent mixing layers with periodic forcing, which mimics that by the flap-type actuator of Naka et al. (2010), is performed. The forcing by the flap-type actuator is modeled by transversely oscillating the inflow turbulent boundary layers. Direct numerical simulation The governing equations are the incompressible continuity and Navier-Stokes equations as following,","PeriodicalId":206337,"journal":{"name":"Proceeding of Eighth International Symposium on Turbulence and Shear Flow Phenomena","volume":"61 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"DIRECT NUMERICAL SIMULATION OF TURBULENT MIXING LAYERS WITH PERIODIC FORCING INDUCED INFLOW\",\"authors\":\"Y. Kametani, Masayuki Kawagoe, K. Fukagata\",\"doi\":\"10.1615/tsfp8.2140\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The direct numerical simulation of the turbulent mixing layer with periodically-forced inflow is performed. The angular frequency Ωc was set as a control parameter. To compare the experimental study of Naka et al. (2010), the angular frequency is set to be Ω = 0.83 (Case A) and 3.85 (Case B). In the present simulation, the momentum thickness shows the Case A achieved the mixing enhancement, while Case B achieves its suppression. Due to the both controls, the Reynolds normal shear stress, especially v′v′ increases behind the periodic forcing. The Reynolds shear stress u′v′ is suppressed in the Case B at downstream. This region is agree with that the mixing suppression is found in the momentum thickness. Furthermore, the anisotropic tensor indicates that two dimensional large coherent structure is generated in the Case B in which mixing was suppressed. Introduction A mixing layer is one of the fundamental free shear flow generated by the velocity gap (Brown & Roshko (2009)). In order to understand the vortex dynamics in shear flows, mixing layers have extensively been studied since Brown & Roshko (1974) experimentally visualized the coherent structure in turbulent mixing layers. Huang & Ho (1990) experimentally studied an acoustically perturbed laminar mixing layer and observed small-scale turbulence created due to interaction of spanwise and streamwise structures after the merging of spanwise vortices. Turbulent mixing layers can be found in various practical applications: e.g., inside combustion chambers and around the exhaust of turbo engines. Techniques for mixing enhancement or suppression are sometimes needed for efficient combustion or noise reduction. Ho (1982) attempted to control the mixing layer by perturbing the flow rates of inflows. They show that the spreading rate of a mixing layer can be manipulated at very low forcing level if the mixing layer is perturbed near a subharmonic of the most-amplified frequency. Naka et al. (2010) studied a mixing layer periodically forced by using a flap-type actuator made of piezoplastic (Polyvinylidene fluoride: PVDF) film aiming at both enhancement and suppression of mixing. They conclude that at some parameters of forcing mixing suppression can also be achieved. In the present study, direct numerical simulation (DNS) of turbulent mixing layers with periodic forcing, which mimics that by the flap-type actuator of Naka et al. (2010), is performed. The forcing by the flap-type actuator is modeled by transversely oscillating the inflow turbulent boundary layers. 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引用次数: 0
摘要
对具有周期性强迫流入的湍流混合层进行了直接数值模拟。角频率Ωc作为控制参数。为了对比Naka et al.(2010)的实验研究,将角频率设置为Ω = 0.83 (Case A)和3.85 (Case B)。在本仿真中,动量厚度显示Case A实现了混合增强,Case B实现了混合抑制。由于这两种控制,雷诺法向剪应力,特别是v ' v '在周期强迫后增加。工况B下游的雷诺数剪切应力u ' v '被抑制。该区域与动量厚度存在混合抑制的结果一致。此外,各向异性张量表明,在抑制混合的情况B中,产生了二维大相干结构。混合层是由速度间隙产生的基本自由剪切流之一(Brown & Roshko(2009))。为了理解剪切流中的涡旋动力学,自Brown & Roshko(1974)实验可视化湍流混合层中的相干结构以来,对混合层进行了广泛的研究。Huang & Ho(1990)实验研究了声扰动层流混合层,观察到在展向涡旋合并后,展向结构和流向结构相互作用产生的小尺度湍流。湍流混合层可以在各种实际应用中找到:例如,在燃烧室内和涡轮发动机的排气周围。为了有效燃烧或降低噪音,有时需要增强或抑制混合的技术。Ho(1982)试图通过扰动流入的流速来控制混合层。结果表明,如果混合层在放大频率最大的次谐波附近受到扰动,则可以在很低的强迫水平下控制混合层的扩散速率。Naka et al.(2010)利用压电塑料(聚偏氟乙烯:PVDF)薄膜制成的襟翼型致动器,研究了一种周期性强制混合层,目的是增强和抑制混合。他们得出结论,在某些强制混合参数下也可以实现抑制。本研究模拟Naka et al.(2010)的襟翼型执行器,对具有周期强迫的湍流混合层进行直接数值模拟(DNS)。襟翼型作动器的强迫是通过横向振荡流入湍流边界层来模拟的。控制方程为不可压缩连续性方程和Navier-Stokes方程:
DIRECT NUMERICAL SIMULATION OF TURBULENT MIXING LAYERS WITH PERIODIC FORCING INDUCED INFLOW
The direct numerical simulation of the turbulent mixing layer with periodically-forced inflow is performed. The angular frequency Ωc was set as a control parameter. To compare the experimental study of Naka et al. (2010), the angular frequency is set to be Ω = 0.83 (Case A) and 3.85 (Case B). In the present simulation, the momentum thickness shows the Case A achieved the mixing enhancement, while Case B achieves its suppression. Due to the both controls, the Reynolds normal shear stress, especially v′v′ increases behind the periodic forcing. The Reynolds shear stress u′v′ is suppressed in the Case B at downstream. This region is agree with that the mixing suppression is found in the momentum thickness. Furthermore, the anisotropic tensor indicates that two dimensional large coherent structure is generated in the Case B in which mixing was suppressed. Introduction A mixing layer is one of the fundamental free shear flow generated by the velocity gap (Brown & Roshko (2009)). In order to understand the vortex dynamics in shear flows, mixing layers have extensively been studied since Brown & Roshko (1974) experimentally visualized the coherent structure in turbulent mixing layers. Huang & Ho (1990) experimentally studied an acoustically perturbed laminar mixing layer and observed small-scale turbulence created due to interaction of spanwise and streamwise structures after the merging of spanwise vortices. Turbulent mixing layers can be found in various practical applications: e.g., inside combustion chambers and around the exhaust of turbo engines. Techniques for mixing enhancement or suppression are sometimes needed for efficient combustion or noise reduction. Ho (1982) attempted to control the mixing layer by perturbing the flow rates of inflows. They show that the spreading rate of a mixing layer can be manipulated at very low forcing level if the mixing layer is perturbed near a subharmonic of the most-amplified frequency. Naka et al. (2010) studied a mixing layer periodically forced by using a flap-type actuator made of piezoplastic (Polyvinylidene fluoride: PVDF) film aiming at both enhancement and suppression of mixing. They conclude that at some parameters of forcing mixing suppression can also be achieved. In the present study, direct numerical simulation (DNS) of turbulent mixing layers with periodic forcing, which mimics that by the flap-type actuator of Naka et al. (2010), is performed. The forcing by the flap-type actuator is modeled by transversely oscillating the inflow turbulent boundary layers. Direct numerical simulation The governing equations are the incompressible continuity and Navier-Stokes equations as following,