[1] Reynolds O. An experimental investigation of the circumstances which determine whether the motion of water shall be direct or sinuous, and of the law of resistance in parallel channels [J]. Philosophical Transactions of the Royal Society A, 1883, 174: 935–982.[2] 刘清扬, 雷娟棉, 刘周, 等. 适用于可压缩流动的γ-Ret-fRe转捩模型[J]. 航空学报, 2022, 43(08): 327-337.[3] 孔维萱, 阎超, 赵瑞. 壁面温度条件对边界层转捩预测的影响[J]. 航空学报, 2013, 34(10): 2249-2255. [4] Feldman Y, Gelfgat A Y. Oscillatory instability of a three-dimensional lid-driven flow in a cube [J]. Physics of Fluids, 2010, 22: 093602.[5] Kuhlmann H C, Albensoeder S. Stability of the steady three-dimensional lid-driven flow in a cube and the supercritical flow dynamics [J]. Physics of Fluids, 2014, 26: 024104.[6] Cazemier W, Verstappen R W C P, Veldman A E P. Proper orthogonal decomposition and low-dimensional models for driven cavity flows [J]. Physics of Fluids, 1998, 10: 1685–1699.[7] Auteri F, Parolini N, Quartapelle L. Numerical investigation on the stability of singular driven cavity flow [J]. Journal of Computational Physics, 2002, 183: 1–25.[8] Peng Y F, Shiau Y H, Hwang R R. Transition in a 2-D lid-driven cavity flow [J]. Computers & Fluids, 2003, 32: 337–352.[9] Boppana V B L, Gajjar J S B. Global flow instability in a lid-driven cavity [J]. International Journal for Numerical Methods in Fluids, 2010, 62: 827–853.[10] Brezillon A, Girault G, Cadou J M. A numerical algorithm coupling a bifurcating indicator and a direct method for the computation of Hopf bifurcation points in fluid mechanics [J]. Computers & Fluids, 2010, 39: 1226–1240.[11] Lin L S, Chang H W, Lin C A. Multi relaxation time lattice Boltzmann simulations of transition in deep 2D lid driven cavity using GPU [J]. Computers & Fluids, 2013, 80: 381–387.[12] Gorban A N, Packwood D J. Enhancement of the stability of lattice Boltzmann methods by dissipation control [J]. Physica A, 2014, 414: 285–299.[13] Lestandi L, Bhaumik S, Avatar G R K C, et al. Multiple Hopf bifurcations and flow dynamics inside a 2D singular lid driven cavity [J]. Computers & Fluids, 2018, 166: 86–103.[14] Suman V K, Viknesh S S, Tekriwal M K, et al. Grid sensitivity and role of error in computing a lid-driven cavity problem [J]. Physical Review E, 2019, 99: 013305.[15] Wang T, Liu T. Transition to chaos in lid-driven square cavity flow [J]. Chinese Physics B, 2021, 30(12): 120508.[16] Shen J. Hopf bifurcation of the unsteady regularized driven cavity flow [J]. Journal of Computational Physics, 1991, 95: 228–245.[17] Liberzon A, Feldman Y, Gelfgat A Y. Experimental observation of the steady oscillatory transition in a cubic lid-driven cavity [J]. Physics of Fluids, 2011, 23: 084106.[18] Chang H W, Hong P Y, Lin L S. Simulations of flow instability in three dimensional deep cavities with multi relaxation time lattice Boltzmann method on graphic processing units [J]. Computers & Fluids, 2013, 88: 866-871.[19] Kuhlmann H C, Albensoeder S. Stability of the steady three-dimensional lid-driven flow in a cube and the supercritical flow dynamics [J]. Physics of Fluids, 2014, 26: 024104.[20] Anupindi K, Lai W, Frankel S. Characterization of oscillatory instability in lid driven cavity flows using lattice Boltzmann method [J]. Computers & Fluids, 2014, 92: 7-21. [21] Loiseau J C, Robinet J C, Leriche E. Intermittency and transition to chaos in the cubical lid-driven cavity flow [J]. Fluid Dynamics Research, 2016, 48: 061421.[22] Gelfgat A Y. Linear instability of the lid-driven flow in a cubic cavity [J]. Theoretical and Computational Fluid Dynamics, 2019, 33: 59-82.[23] Zhang J K, Cui M, Zuo Z L, et al. Prediction on steady-oscillatory transition via Hopf bifurcation in a three-dimensional (3D) lid-driven cube [J]. Computers & Fluids, 2021, 229: 105068.[24] Hammami F, Souayeh B, Ben-Cheikh N. Computational analysis of fluid flow due to a two-sided lid driven cavity with a circular cylinder [J]. Computers & Fluids, 2017, 156: 317–328. [25] Zhang J K, Cui M, Li B W, et al. Performance of combined spectral collocation method and artificial compressibility method for 3D incompressible fluid flow and heat transfer [J]. International Journal of Numerical Methods for Heat and Fluid Flow, 2020, 30(12): 5037–5062.[26] Zhang J K, Dong H, Zhou E Z. A combined method for solving 2D incompressible flow and heat transfer by spectral collocation method and artificial compressibility method [J]. International Journal of Heat and Mass Transfer, 2017, 112: 289–299.[27] Chorin A J. A numerical method for solving incompressible viscous flow problems [J]. Journal of Computational Physics, 1967, 2: 12–26.[28] Canuto C, Hussaini M Y, Quarteroni A. Spectral Methods, Fundamentals in Single Domains [M]. New York: Springer-Verlag, 2006: 85–87.[29] Yu P X, Tian Z F. A high-order compact scheme for the pure streamfunction (vector potential) formulation of the 3D steady incompressible Navier-Stokes equations [J]. Journal of Computational Physics, 2019, 382: 65–85.[30] Shu C, Wang L, Chew Y T. Numerical computation of three-dimensional incompressible Navier-Stokes equations in primitive variable form by DQ method [J]. International Journal for Numerical Methods in Fluids, 2003, 43: 345–368.[31] Albensoeder S, Kuhlmann H C. Accurate three-dimensional lid-driven cavity flow [J]. Journal of Computational Physics, 2005, 206: 536–558.[32] Bhaumik S, Sengupta T K. A new velocity vorticity formulation for direct numerical simulation of 3D transitional and turbulent flows [J]. Journal of Computational Physics, 2015, 284: 230–260. |