### Abstract

Original language | English |
---|---|

Pages (from-to) | 687-714 |

Number of pages | 28 |

Journal | Journal of Fluid Mechanics |

Volume | 851 |

Early online date | 31 Jul 2018 |

DOIs | |

Publication status | Published - 25 Sep 2018 |

### Fingerprint

### Keywords

- bifurcation
- vortex instability
- wakes

### Cite this

*Journal of Fluid Mechanics*,

*851*, 687-714. https://doi.org/10.1017/jfm.2018.526

}

*Journal of Fluid Mechanics*, vol. 851, pp. 687-714. https://doi.org/10.1017/jfm.2018.526

**Flow around an inclined circular disk.** / Gao, Song; Tao, Longbin; Tian, Xinliang; Yang, Jianmin.

Research output: Contribution to journal › Article

TY - JOUR

T1 - Flow around an inclined circular disk

AU - Gao, Song

AU - Tao, Longbin

AU - Tian, Xinliang

AU - Yang, Jianmin

PY - 2018/9/25

Y1 - 2018/9/25

N2 - Direct numerical simulations are performed for the uniform flow around an inclined circular disk. The diameter–thickness aspect ratio ( X=D/td) of the disk is 50 and the inclination angle (\alpha) is considered over the range of 0<6<80 deg, where \alpha=0 deg refers to the condition where the flow is normal to the disk. The Reynolds number (Re), based on the short axis of projection in the streamwise direction, is defined as Re=U_\inf D cos \alpha /\mu, where U_\inf is the velocity of the flow and \mu is the kinematic viscosity. Re is investigated over the range of 50 < Re < 300. In the considered Re–\alpha parametric space, five states are observed and denoted as: (I) steady state (SS); (II) periodic state (PS); (III) periodic state with a low frequency modulation (PSL); (IV) quasi-periodic state (QP) and (V) chaotic state (CS). Both Re and \alpha affect the bifurcation mechanism. The bifurcating sequence occurring at \alpha=0 deg is generally observed over the whole Re–\alpha space, although it is advanced at small \alpha and delayed at large \alpha. The advancement of thresholds for different states is due to the effects introduced by inclination, which tend to select the plane of symmetry for the wake in order to regulate the wake and intensify some flow features. Nevertheless, the bifurcations are still in the dominant position when leading a state without stable symmetry, i.e. the planar symmetry could not be recovered by small \alpha. These phenomena are further discussed with respect to the vortex shedding patterns behind the disk. Furthermore, for any fixed disk, the wake behaviour is only associated with that found in the steady vertical state of a freely falling disk. The fully coupled fluid–body system is fundamentally different from the fixed cases.

AB - Direct numerical simulations are performed for the uniform flow around an inclined circular disk. The diameter–thickness aspect ratio ( X=D/td) of the disk is 50 and the inclination angle (\alpha) is considered over the range of 0<6<80 deg, where \alpha=0 deg refers to the condition where the flow is normal to the disk. The Reynolds number (Re), based on the short axis of projection in the streamwise direction, is defined as Re=U_\inf D cos \alpha /\mu, where U_\inf is the velocity of the flow and \mu is the kinematic viscosity. Re is investigated over the range of 50 < Re < 300. In the considered Re–\alpha parametric space, five states are observed and denoted as: (I) steady state (SS); (II) periodic state (PS); (III) periodic state with a low frequency modulation (PSL); (IV) quasi-periodic state (QP) and (V) chaotic state (CS). Both Re and \alpha affect the bifurcation mechanism. The bifurcating sequence occurring at \alpha=0 deg is generally observed over the whole Re–\alpha space, although it is advanced at small \alpha and delayed at large \alpha. The advancement of thresholds for different states is due to the effects introduced by inclination, which tend to select the plane of symmetry for the wake in order to regulate the wake and intensify some flow features. Nevertheless, the bifurcations are still in the dominant position when leading a state without stable symmetry, i.e. the planar symmetry could not be recovered by small \alpha. These phenomena are further discussed with respect to the vortex shedding patterns behind the disk. Furthermore, for any fixed disk, the wake behaviour is only associated with that found in the steady vertical state of a freely falling disk. The fully coupled fluid–body system is fundamentally different from the fixed cases.

KW - bifurcation

KW - vortex instability

KW - wakes

U2 - 10.1017/jfm.2018.526

DO - 10.1017/jfm.2018.526

M3 - Article

VL - 851

SP - 687

EP - 714

JO - Journal of Fluid Mechanics

JF - Journal of Fluid Mechanics

SN - 0022-1120

ER -