{"title":"用流体速度轮廓动力学方法分析稳态涡环","authors":"Yoon-Rak Choi","doi":"10.26748/ksoe.2021.070","DOIUrl":null,"url":null,"abstract":"A water-jet can be used as one of the propulsion systems for ships and marine life. When a jet is injected to obtain thrust, a vortex ring is formed at a nozzle and then propagated downstream (Krueger et al., 2008). Furthermore, a vortex ring is generated due to volcanic eruption or nuclear explosion (Akhmetov, 2009). The flow of a vortex ring is formulated with the Helmholtz vorticity equation in inviscid and incompressible fluids (Batchelor, 1967). A steady vortex ring was first reported by Helmholtz (1867) who examined a vortex ring of an small circular cross section, while a spherical vortex was first analyzed by Hill (1894). Norbury (1973) analyzed a vortex ring in a steady state for general circumstances, which is referred to as the Norbury–Fraenkel family (N-F family) of vortex rings. A dynamic analysis is required for analyzing the instability due to the disturbance or interaction between vortex rings. A contour dynamics (CD) method for fluid velocity is used for analyzing the complex evolution of the contour of a vortex core. The CD method is a two-dimensional or axisymmetric flow analysis method due to the isolated vorticity in an inviscid, incompressible, and irrotational flow field (Pullin, 1992; Smith et al., 2018). The CD method can drastically reduce the burden of computations because the computation is performed in the form of line integrals on the boundary contour of the vorticity region. The fluid velocity on the contour is calculated using the CD method and then applied with time integrals to estimate the dynamic changes in the shape of the vortex core. Zabusky et al. (1979) introduced the CD method in dynamic analysis of two-dimensional vortex patches. Various examples of dynamic analysis for threedimensional axisymmetric vortex rings are provided in the study by Shariff et al. (1989). In this study, the CD method was applied to the analysis of the N-F family of vortex rings which are flows in steady state. Choi (2020) combined the CD method for a stream function (Shariff et al., 1989) and the direct shape-calculation method, and thus obtained results that were superior that those reported by Norbury (1973) wherein surface integrals and Fourier analysis were used. As a follow-up study to Choi (2020), in this study, we analyzed the N-F family of vortex rings using the CD method for fluid velocity examined in studies by Shariff et al. (1989) and Shariff et al. (2008). A stream function has been mostly used for analyzing a vortex ring in a steady state (Batchelor, 1967; Fraenkel, 1970; Fraenkel, 1972; Norbury 1973). In this study, we examined whether the CD method for fluid velocity, which is used in dynamic analysis, can also be applied to the analysis of a vortex ring in Journal of Ocean Engineering and Technology [ARTICLE IN PRESS] https://doi.org/10.26748/KSOE.2021.070 pISSN 1225-0767 eISSN 2287-6715","PeriodicalId":315103,"journal":{"name":"Journal of Ocean Engineering and Technology","volume":"26 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2022-03-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Analysis of Steady Vortex Rings Using Contour Dynamics Method for Fluid Velocity\",\"authors\":\"Yoon-Rak Choi\",\"doi\":\"10.26748/ksoe.2021.070\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A water-jet can be used as one of the propulsion systems for ships and marine life. When a jet is injected to obtain thrust, a vortex ring is formed at a nozzle and then propagated downstream (Krueger et al., 2008). Furthermore, a vortex ring is generated due to volcanic eruption or nuclear explosion (Akhmetov, 2009). The flow of a vortex ring is formulated with the Helmholtz vorticity equation in inviscid and incompressible fluids (Batchelor, 1967). A steady vortex ring was first reported by Helmholtz (1867) who examined a vortex ring of an small circular cross section, while a spherical vortex was first analyzed by Hill (1894). Norbury (1973) analyzed a vortex ring in a steady state for general circumstances, which is referred to as the Norbury–Fraenkel family (N-F family) of vortex rings. A dynamic analysis is required for analyzing the instability due to the disturbance or interaction between vortex rings. A contour dynamics (CD) method for fluid velocity is used for analyzing the complex evolution of the contour of a vortex core. The CD method is a two-dimensional or axisymmetric flow analysis method due to the isolated vorticity in an inviscid, incompressible, and irrotational flow field (Pullin, 1992; Smith et al., 2018). The CD method can drastically reduce the burden of computations because the computation is performed in the form of line integrals on the boundary contour of the vorticity region. The fluid velocity on the contour is calculated using the CD method and then applied with time integrals to estimate the dynamic changes in the shape of the vortex core. Zabusky et al. (1979) introduced the CD method in dynamic analysis of two-dimensional vortex patches. Various examples of dynamic analysis for threedimensional axisymmetric vortex rings are provided in the study by Shariff et al. (1989). In this study, the CD method was applied to the analysis of the N-F family of vortex rings which are flows in steady state. Choi (2020) combined the CD method for a stream function (Shariff et al., 1989) and the direct shape-calculation method, and thus obtained results that were superior that those reported by Norbury (1973) wherein surface integrals and Fourier analysis were used. As a follow-up study to Choi (2020), in this study, we analyzed the N-F family of vortex rings using the CD method for fluid velocity examined in studies by Shariff et al. (1989) and Shariff et al. (2008). A stream function has been mostly used for analyzing a vortex ring in a steady state (Batchelor, 1967; Fraenkel, 1970; Fraenkel, 1972; Norbury 1973). 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引用次数: 0
摘要
水射流可用作船舶和海洋生物的推进系统之一。当射流注入以获得推力时,在喷嘴处形成旋涡环并向下游传播(Krueger et al., 2008)。此外,火山喷发或核爆炸也会产生漩涡环(Akhmetov, 2009)。用亥姆霍兹涡度方程(Batchelor, 1967)表示了无粘性和不可压缩流体中的涡环流动。Helmholtz(1867)首先报道了稳定涡环,他研究了一个小圆形截面的涡环,而Hill(1894)首先分析了球形涡环。Norbury(1973)分析了一般情况下稳态下的涡环,称之为涡环的Norbury - fraenkel族(N-F族)。由于涡旋环之间的干扰或相互作用而引起的不稳定性需要进行动力学分析。采用流体速度的轮廓动力学方法分析了涡核轮廓的复杂演化过程。CD方法是一种二维或轴对称流动分析方法,由于在无粘、不可压缩和无旋转的流场中存在孤立的涡量(Pullin, 1992;Smith et al., 2018)。CD方法以线积分的形式在涡度区边界轮廓上进行计算,大大减少了计算量。采用CD法计算轮廓上的流体速度,并结合时间积分估计涡核形状的动态变化。Zabusky et al.(1979)将CD方法引入二维涡旋斑块的动态分析。Shariff et al.(1989)的研究提供了三维轴对称涡环动力分析的各种实例。本文将CD方法应用于稳态流动的N-F族涡环的分析。Choi(2020)结合了流函数的CD方法(Shariff et al., 1989)和直接形状计算方法,从而获得了优于Norbury(1973)报告的结果,其中使用了表面积分和傅里叶分析。作为Choi(2020)的后续研究,在本研究中,我们使用Shariff et al.(1989)和Shariff et al.(2008)研究中检验的流体速度的CD方法分析了N-F族涡环。流函数主要用于分析稳定状态下的涡环(Batchelor, 1967;Fraenkel, 1970;Fraenkel, 1972;Norbury 1973)。在这项研究中,我们研究了用于动力分析的流体速度的CD方法是否也可以应用于涡环的分析,海洋工程与技术杂志[ARTICLE In PRESS] https://doi.org/10.26748/KSOE.2021.070 pISSN 1225-0767 eISSN 2287-6715
Analysis of Steady Vortex Rings Using Contour Dynamics Method for Fluid Velocity
A water-jet can be used as one of the propulsion systems for ships and marine life. When a jet is injected to obtain thrust, a vortex ring is formed at a nozzle and then propagated downstream (Krueger et al., 2008). Furthermore, a vortex ring is generated due to volcanic eruption or nuclear explosion (Akhmetov, 2009). The flow of a vortex ring is formulated with the Helmholtz vorticity equation in inviscid and incompressible fluids (Batchelor, 1967). A steady vortex ring was first reported by Helmholtz (1867) who examined a vortex ring of an small circular cross section, while a spherical vortex was first analyzed by Hill (1894). Norbury (1973) analyzed a vortex ring in a steady state for general circumstances, which is referred to as the Norbury–Fraenkel family (N-F family) of vortex rings. A dynamic analysis is required for analyzing the instability due to the disturbance or interaction between vortex rings. A contour dynamics (CD) method for fluid velocity is used for analyzing the complex evolution of the contour of a vortex core. The CD method is a two-dimensional or axisymmetric flow analysis method due to the isolated vorticity in an inviscid, incompressible, and irrotational flow field (Pullin, 1992; Smith et al., 2018). The CD method can drastically reduce the burden of computations because the computation is performed in the form of line integrals on the boundary contour of the vorticity region. The fluid velocity on the contour is calculated using the CD method and then applied with time integrals to estimate the dynamic changes in the shape of the vortex core. Zabusky et al. (1979) introduced the CD method in dynamic analysis of two-dimensional vortex patches. Various examples of dynamic analysis for threedimensional axisymmetric vortex rings are provided in the study by Shariff et al. (1989). In this study, the CD method was applied to the analysis of the N-F family of vortex rings which are flows in steady state. Choi (2020) combined the CD method for a stream function (Shariff et al., 1989) and the direct shape-calculation method, and thus obtained results that were superior that those reported by Norbury (1973) wherein surface integrals and Fourier analysis were used. As a follow-up study to Choi (2020), in this study, we analyzed the N-F family of vortex rings using the CD method for fluid velocity examined in studies by Shariff et al. (1989) and Shariff et al. (2008). A stream function has been mostly used for analyzing a vortex ring in a steady state (Batchelor, 1967; Fraenkel, 1970; Fraenkel, 1972; Norbury 1973). In this study, we examined whether the CD method for fluid velocity, which is used in dynamic analysis, can also be applied to the analysis of a vortex ring in Journal of Ocean Engineering and Technology [ARTICLE IN PRESS] https://doi.org/10.26748/KSOE.2021.070 pISSN 1225-0767 eISSN 2287-6715