Large eddy simulations of a triangular jet and its counterpart through a chamber

doi:10.1088/1674-1056/ab8623

中国物理B ›› 2020, Vol. 29 ›› Issue (6): 64701-064701.doi: 10.1088/1674-1056/ab8623

• ELECTROMAGNETISM, OPTICS, ACOUSTICS, HEAT TRANSFER, CLASSICAL MECHANICS, AND FLUID DYNAMICS • 上一篇下一篇

Large eddy simulations of a triangular jet and its counterpart through a chamber

Xiu Xiao(肖秀), Guo-Chang Wang(王国昌), Min-Yi Xu(徐敏义), Jian-Chun Mi(米建春)

1 Marine Engineering College, Dalian Maritime University, Dalian 116026, China;
2 College of Engineering, Peking University, Beijing 100871, China

收稿日期:2019-12-06 修回日期:2020-01-23 出版日期:2020-06-05 发布日期:2020-06-05
通讯作者: Jian-Chun Mi E-mail:jmi@pku.edu.cn
基金资助:
Project supported by the National Natural Science Foundation of China (Grant Nos. 51879022, 51979045, and 51906029), the Fundamental Research Funds for the Central Universities, China (Grant Nos. 3132019197, 3132020187, and 3132019037), the Projects for Dalian Youth Star of Science and Technology, China (Grant No. 2018RQ12), and the China Postdoctoral Science Foundation (Grant No. 2019M661084).

Large eddy simulations of a triangular jet and its counterpart through a chamber

Xiu Xiao(肖秀)¹, Guo-Chang Wang(王国昌)², Min-Yi Xu(徐敏义)¹, Jian-Chun Mi(米建春)^1,2

1 Marine Engineering College, Dalian Maritime University, Dalian 116026, China;
2 College of Engineering, Peking University, Beijing 100871, China

Received:2019-12-06 Revised:2020-01-23 Online:2020-06-05 Published:2020-06-05
Contact: Jian-Chun Mi E-mail:jmi@pku.edu.cn
Supported by:
Project supported by the National Natural Science Foundation of China (Grant Nos. 51879022, 51979045, and 51906029), the Fundamental Research Funds for the Central Universities, China (Grant Nos. 3132019197, 3132020187, and 3132019037), the Projects for Dalian Youth Star of Science and Technology, China (Grant No. 2018RQ12), and the China Postdoctoral Science Foundation (Grant No. 2019M661084).

摘要/Abstract

摘要： A free triangular jet (TJ1) and its counterpart initially passing a short circular chamber (TJ2) are numerically modeled using large eddy simulation (LES). This paper compares the near-field characteristics of the two jets in detail. To enable some necessary experimental validations, the LES conditions of TJ1 and TJ2 are taken to be identical to those measured by Xu et al. (Sci. China Phys. 56 1176 (2013)) and England et al. (Exp. Fluids. 48 69 (2010)), respectively. The LES predictions are found to agree well with those measurements. It is demonstrated that a strong swirl occurs near the chamber inlet plane for the TJ2 flow. At the center of the swirl, there is a cluster of three sink foci, where each focus is aligned midway between the original triangular apexes. In the vortex skeleton constructed from the time-averaged flow field, the vortices arising from the foci are helically twisted around the core of the jet. As the flow passes through the chamber, the foci merge to form a closed-loop “bifurcation line”, which separates the inward swirling flow and the outward oscillating jet. This global oscillation is regarded as a source node near the centerline of the chamber. If the chamber is removed for a “free” jet, i.e., TJ1, a cluster of three pairs of counter-rotating foci is produced and the net swirl circulation is zero, so the overall oscillation of the jet does not occur.

关键词: turbulent, triangular jet, large eddy simulation

Abstract: A free triangular jet (TJ1) and its counterpart initially passing a short circular chamber (TJ2) are numerically modeled using large eddy simulation (LES). This paper compares the near-field characteristics of the two jets in detail. To enable some necessary experimental validations, the LES conditions of TJ1 and TJ2 are taken to be identical to those measured by Xu et al. (Sci. China Phys. 56 1176 (2013)) and England et al. (Exp. Fluids. 48 69 (2010)), respectively. The LES predictions are found to agree well with those measurements. It is demonstrated that a strong swirl occurs near the chamber inlet plane for the TJ2 flow. At the center of the swirl, there is a cluster of three sink foci, where each focus is aligned midway between the original triangular apexes. In the vortex skeleton constructed from the time-averaged flow field, the vortices arising from the foci are helically twisted around the core of the jet. As the flow passes through the chamber, the foci merge to form a closed-loop “bifurcation line”, which separates the inward swirling flow and the outward oscillating jet. This global oscillation is regarded as a source node near the centerline of the chamber. If the chamber is removed for a “free” jet, i.e., TJ1, a cluster of three pairs of counter-rotating foci is produced and the net swirl circulation is zero, so the overall oscillation of the jet does not occur.

Key words: turbulent, triangular jet, large eddy simulation

中图分类号: (Turbulent jets)

47.27.wg

47.27.-i (Turbulent flows) 47.85.lk (Mixing enhancement)

肖秀, 王国昌, 徐敏义, 米建春. Large eddy simulations of a triangular jet and its counterpart through a chamber[J]. 中国物理B, 2020, 29(6): 64701-064701.

Xiu Xiao(肖秀), Guo-Chang Wang(王国昌), Min-Yi Xu(徐敏义), Jian-Chun Mi(米建春). Large eddy simulations of a triangular jet and its counterpart through a chamber[J]. Chin. Phys. B, 2020, 29(6): 64701-064701.

参考文献 32

[1]	Aleyasin S S, Tachie M F and Koupriyanov M 2017 J. Fluids Eng. 139 101206 doi: 10.1115/1.4036824
[2]	Schadow K C, Gutmark E, Parr D M and Wilson K J 2004 Exp. Fluids 6 129 doi: 10.1007/BF00196464
[3]	Rahman M S, Tay G F K and Tachie M F 2019 Flow Turbul. Combust. 103 797 doi: 10.1007/s10494-019-00047-7
[4]	Hussain F and Husain H S 1989 J. Fluid Mech. 208 257 doi: 10.1017/S0022112089002843
[5]	Li Y, Li B, Qi F and Wang X 2017 Chin. Phys. B 26 024701 doi: 10.1088/1674-1056/26/2/024701
[6]	Grinstein F F, Gutmark E and Parr T 1995 Phys. Fluids 7 1483 doi: 10.1063/1.868534
[7]	Vouros A P, Panidis T, Pollard A and Schwab R R 2015 Int. J. Heat Fluid Flow 51 383 doi: 10.1016/j.ijheatfluidflow.2014.10.002
[8]	Deo R C, Mi J and Nathan G J 2007 Exp. Therm. Fluid Sci. 32 545 doi: 10.1016/j.expthermflusci.2007.06.004
[9]	Xu M, Zhang J, Mi J, Nathan G J and Kalt P A M 2013 Chin. Phys. B 22 034701 doi: 10.1088/1674-1056/22/3/034701
[10]	Shi X D, Feng L H and Wang J J 2019 J. Fluid Mech. 868 66 doi: 10.1017/jfm.2019.162
[11]	Mi J and Nathan G J 2010 Flow Turbul. Combust. 84 583 doi: 10.1007/s10494-009-9240-0
[12]	Iyogun C O and Birouk M 2009 Flow Turbul. Combust. 82 287 doi: 10.1007/s10494-008-9176-9
[13]	Quinn W R 2005 Exp. Fluids 39 111 doi: 10.1007/s00348-005-0988-2
[14]	Ghasemi A, Tuna B A and Li X 2019 J. Fluid Mech. 864 141 doi: 10.1017/jfm.2018.988
[15]	Gutmark E and Grinstein F F 1999 Annu. Rev. Fluid Mech. 31 239 doi: 10.1146/annurev.fluid.31.1.239
[16]	Lindstrom A and Amitay M 2019 AIAA J. 57 2783 doi: 10.2514/1.J058135
[17]	Lee S K 2009 Study of a naturally oscillating triangular-jet flow (PhD Dessertation) (Adelaide: The University of Adelaide)
[18]	Zhang J, Xu M and Mi J 2014 Chin. Phys. B 23 044704 doi: 10.1088/1674-1056/23/4/044704
[19]	Xu M, Mi J and Li P 2012 Flow Turbul. Combust. 88 367 doi: 10.1007/s10494-011-9363-y
[20]	Hinze J O 1975 Turbulence (New York: McGraw-Hill)
[21]	Germano M, Piomelli U, Moin P and Cabot W H 1991 Phys. Fluids A 3 1760 doi: 10.1063/1.857955
[22]	Lilly D K 1992 Phys. Fluids A 4 633 doi: 10.1063/1.858280
[23]	England G, Kalt P A M, Nathan G J and Kelso R M 2010 Exp. Fluids 48 69 doi: 10.1007/s00348-009-0706-6
[24]	Xu M, Zhang J, Mi J, Nathan G J and Kalt P A M 2013 Sci. Chin. Phys. Mech. 56 1176 doi: 10.1007/s11433-013-5099-0
[25]	Mi J, Xu M and Zhou T 2013 Phys. Fluids 25 075101 doi: 10.1063/1.4811403
[26]	Fellouah H and Pollard A 2009 Phys. Fluids 21 115101 doi: 10.1063/1.3258837
[27]	Sadeghi H, Lavoie P and Pollard A 2014 J. Turbul. 15 335 doi: 10.1080/14685248.2014.906810
[28]	Salkhordeh S, Mazumdar S, Jana A and Kimber M L 2019 Flow Turbul. Combust. 102 559 doi: 10.1007/s10494-018-9971-x
[29]	Wong C Y, Nathan G J and Kelso R M 2008 J. Fluid Mech. 606 153 doi: 10.1017/S0022112008001699
[30]	Chakraborty P, Balachandar S and Adrian R J 2005 J. Fluid Mech. 535 189 doi: 10.1017/S0022112005004726
[31]	Jeong J and Hussain F 1995 J. Fluid Mech. 285 69 doi: 10.1017/S0022112095000462
[32]	Green S I 1995 Fluid Vortices (Netherlands: Springer)

Large eddy simulations of a triangular jet and its counterpart through a chamber

Large eddy simulations of a triangular jet and its counterpart through a chamber

RichHTML

PDF (PC)

赞

可视化

摘要/Abstract

引用本文

使用本文

参考文献 32

相关文章 15

Metrics

本文评价

推荐阅读 0

[1]	Jin-Hao Zhang(张津浩), Biao-Hui Li(李彪辉), Yu-Fei Wang(王宇飞), and Nan Jiang(姜楠). Effects of single synthetic jet on turbulent boundary layer[J]. 中国物理B, 2022, 31(7): 74702-074702.
[2]	Biao-Hui Li(李彪辉), Kang-Jun Wang(王康俊), Yu-Fei Wang(王宇飞), and Nan Jiang(姜楠). Experimental investigation on drag reduction in a turbulent boundary layer with a submerged synthetic jet[J]. 中国物理B, 2022, 31(2): 24702-024702.
[3]	Jian-Chao He(何建超), Ming-Wei Fang(方明卫), Zhen-Yuan Gao(高振源), Shi-Di Huang(黄仕迪), and Yun Bao(包芸). Effects of Prandtl number in two-dimensional turbulent convection[J]. 中国物理B, 2021, 30(9): 94701-094701.
[4]	江代文, 张辉, 范宝春, 王安华. Direct numerical simulation on relevance of fluctuating velocities and drag reduction in turbulent channel flow with spanwise space-dependent electromagnetic force[J]. 中国物理B, 2019, 28(5): 54701-054701.
[5]	李晓鹏, 周蕊, 陈小平, 范学军, 谢国山. Shock oscillation in highly underexpanded jets[J]. 中国物理B, 2018, 27(9): 94705-094705.
[6]	白建侠, 姜楠, 郑小波, 唐湛琪, 王康俊, 崔晓通. Active control of wall-bounded turbulence for drag reduction with piezoelectric oscillators[J]. 中国物理B, 2018, 27(7): 74701-074701.
[7]	李山, 姜楠, 杨绍琼, 黄永祥, 吴彦华. Coherent structures over riblets in turbulent boundary layer studied by combining time-resolved particle image velocimetry (TRPIV), proper orthogonal decomposition (POD), and finite-time Lyapunov exponent (FTLE)[J]. 中国物理B, 2018, 27(10): 104701-104701.
[8]	韩洋, 张辉, 范宝春, 李健, 江代文, 赵子杰. Mechanism of controlling turbulent channel flow with the effect of spanwise Lorentz force distribution[J]. 中国物理B, 2017, 26(8): 84704-084704.
[9]	延皓, 王凤聚, 李长春, 黄静. Research on the jet characteristics of the deflector-jet mechanism of the servo valve[J]. 中国物理B, 2017, 26(4): 44701-044701.
[10]	卢浩, 赵文君, 张会强, 王兵, 王希麟. Three-dimensional turbulent flow over cube-obstacles[J]. 中国物理B, 2017, 26(1): 14703-014703.
[11]	闫香, 张鹏飞, 张京会, 乔春红, 范承玉. Quantum polarization fluctuations of partially coherent dark hollow beams in non-Kolmogorov turbulence atmosphere[J]. 中国物理B, 2016, 25(8): 84204-084204.
[12]	F Boufalah, L Dalil-Essakali, H Nebdi, A Belafhal. Effect of turbulent atmosphere on the on-axis average intensity of Pearcey-Gaussian beam[J]. 中国物理B, 2016, 25(6): 64208-064208.
[13]	郑小波, 姜楠, 张浩. Predetermined control of turbulent boundary layer with a piezoelectric oscillator[J]. 中国物理B, 2016, 25(1): 14703-014703.
[14]	阳倦成, 李凤臣, 蔡伟华, 张红娜, 宇波. Direct numerical simulation of viscoelastic-fluid-based nanofluid turbulent channel flow with heat transfer[J]. 中国物理B, 2015, 24(8): 84401-084401.
[15]	李凤臣, 王璐, 蔡伟华. A new mixed subgrid-scale model for large eddy simulation of turbulent drag-reducing flows of viscoelastic fluids[J]. 中国物理B, 2015, 24(7): 74701-074701.