The lid-driven right-angled isosceles triangular cavity flow

被引:16
|
作者
An, B. [1 ]
Bergada, J. M. [1 ]
Mellibovsky, F. [2 ]
机构
[1] Univ Politecn Cataluna, Dept Fluid Mech, Barcelona 08034, Spain
[2] Univ Politecn Cataluna, Dept Phys, Aerosp Engn Div, Barcelona 08034, Spain
关键词
bifurcation; chaos; NAVIER-STOKES EQUATIONS; STEADY VISCOUS-FLOW; LINEAR-STABILITY ANALYSIS; LATTICE BOLTZMANN METHOD; BOUNDARY-CONDITIONS; INCOMPRESSIBLE-FLOW; EXTRAPOLATION METHOD; NUMERICAL-SOLUTION; HOPF-BIFURCATION; FLUID-FLOW;
D O I
10.1017/jfm.2019.512
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
We employ lattice Boltzmann simulation to numerically investigate the two-dimensional incompressible flow inside a right-angled isosceles triangular enclosure driven by the tangential motion of its hypotenuse. While the base flow, directly evolved from creeping flow at vanishing Reynolds number, remains stationary and stable for flow regimes beyond R-e greater than or similar to 13 400, chaotic motion is nevertheless observed from as low as R-e similar or equal to 10 600. Chaotic dynamics is shown to arise from the destabilisation, following a variant of the classic Ruelle-Takens route, of a secondary solution branch that emerges at a relatively low R-e similar or equal to 4908 and appears to bear no connection to the base state. We analyse the bifurcation sequence that takes the flow from steady to periodic and then quasi-periodic and show that the invariant torus is finally destroyed in a period-doubling cascade of a phase-locked limit cycle. As a result, a strange attractor arises that induces chaotic dynamics.
引用
收藏
页码:476 / 519
页数:44
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