Hostname: page-component-848d4c4894-ttngx Total loading time: 0 Render date: 2024-05-14T15:54:27.433Z Has data issue: false hasContentIssue false

A novel linear stability analysis method for plane Couette flow considering rarefaction effects

Published online by Cambridge University Press:  22 May 2023

Sen Zou
Affiliation:
School of Aeronautics, Northwestern Polytechnical University, Xi'an, Shaanxi 710072, PR China State Key Laboratory of Aerodynamics, China Aerodynamics Research and Development Center, Mianyang 621000, PR China
Lin Bi*
Affiliation:
State Key Laboratory of Aerodynamics, China Aerodynamics Research and Development Center, Mianyang 621000, PR China
Chengwen Zhong*
Affiliation:
School of Aeronautics, Northwestern Polytechnical University, Xi'an, Shaanxi 710072, PR China
Xianxu Yuan
Affiliation:
State Key Laboratory of Aerodynamics, China Aerodynamics Research and Development Center, Mianyang 621000, PR China
Zhigong Tang
Affiliation:
State Key Laboratory of Aerodynamics, China Aerodynamics Research and Development Center, Mianyang 621000, PR China
*
Email addresses for correspondence: bzbaby1010@163.com, zhongcw@nwpu.edu.cn
Email addresses for correspondence: bzbaby1010@163.com, zhongcw@nwpu.edu.cn

Abstract

Following the stability analysis method in classic fluid dynamics, a linear stability equation (LSE) suitable for rarefied flows is derived based on the Bhatnagar–Gross–Krook (BGK) equation. The global method and singular value decomposition method are used for modal and non-modal analysis, respectively. This approach is validated by results obtained from Navier–Stokes (NS) equations. The modal analysis shows that LSEs based on NS equations (NS-LSEs) begin to fail when the Knudsen number ($Kn$) increases past $\sim$0.01, regardless of whether a slip model is used. When $Kn\geq 0.01$, the growth rate of the least stable mode is generally underestimated by the NS-LSEs. Under a fixed wavenumber, the pattern (travelling or standing wave) of the least stable mode changes with $Kn$; when the mode presents the same pattern, the growth rate decreases almost linearly with increasing $Kn$; otherwise, rarefaction effects may not stabilize the flow. The characteristic lengths of the different modes are different, and the single-scale classic stability analysis method cannot predict multiple modes accurately, even when combined with a slip model and even for continuum flow. However, non-modal analysis shows that this error does not affect the transient growth because modes with small growth rates offer little contribution to the transient growth. In rarefied flow, as long as the Mach number ($Ma$) is large enough, transient growth will occur in some wavenumber ranges. The rarefaction effect plays a stabilizing role in transient growth. The NS-LSEs-based method always overestimates the maximum transient growth.

Type
JFM Papers
Copyright
© The Author(s), 2023. Published by Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Bhatnagar, P.L., Gross, E.P. & Krook, M. 1954 A model for collision processes in gases. I. Small amplitude processes in charged and neutral one-component systems. Phys. Rev. 94 (3), 511.CrossRefGoogle Scholar
Bird, G.A. 1994 Molecular Gas Dynamics and the Direct Simulation of Gas Flows. Clarendon.Google Scholar
Bo, Y.T., Wang, P., Guo, Z.L. & Wang, L.P. 2017 DUGKS simulations of three-dimensional Taylor–Green vortex flow and turbulent channel flow. Comput. Fluids 155, 921.CrossRefGoogle Scholar
Broadwell, J.E. 1964 Study of rarefied shear flow by the discrete velocity method. J.Fluid Mech. 19 (3), 401414.CrossRefGoogle Scholar
Cao, B.Y., Sun, J., Chen, M. & Guo, Z.Y. 2009 Molecular momentum transport at fluid–solid interfaces in MEMS/NEMS: a review. Intl J. Mol. Sci. 10 (11), 46384706.CrossRefGoogle ScholarPubMed
Cercignani, C. & Stefanov, S. 1992 Bénard's instability in kinetic theory. Transp. Theory Stat. Phys. 21 (4–6), 371381.CrossRefGoogle Scholar
Chai, C.S. & Song, B.F. 2019 Stability of slip channel flow revisited. Phys. Fluids 31 (8), 084105.Google Scholar
Chen, J.F., Liu, S., Wang, Y. & Zhong, C.W. 2019 A conserved discrete unified gas-kinetic scheme with unstructured discrete velocity space. Phys. Rev. E 100 (4), 43305.CrossRefGoogle ScholarPubMed
Chen, K.W. & Song, B.F. 2021 Linear stability of slip pipe flow. J.Fluid Mech. 910, A35.CrossRefGoogle Scholar
Chen, T., Wen, X., Wang, L.P., Guo, Z.L. & Chen, S.Y. 2020 Simulation of three-dimensional compressible decaying isotropic turbulence using a redesigned discrete unified gas kinetic scheme. Phys. Fluids 32 (12), 125104.CrossRefGoogle Scholar
Chu, A.K.-H. 2003 Stability of slip flows in a peristaltic transport. Europhys. Lett. 64 (4), 435.CrossRefGoogle Scholar
Chu, A.K.-H. 2004 Instability of Navier slip flow of liquids. C. R. Méc 332 (11), 895900.CrossRefGoogle Scholar
Chu, W.K.-H. 2001 Stability of incompressible helium II: a two-fluid system. J.Phys.: Condens. Matter 12 (37), 80658069.Google Scholar
Dongari, N., Agrawal, A. & Agrawala, A. 2007 Analytical solution of gaseous slip flow in long microchannels. Intl J. Heat Mass Transfer 50 (17–18), 34113421.CrossRefGoogle Scholar
Fedorov, A. & Tumin, A. 2011 High-speed boundary-layer instability: old terminology and a new framework. AIAA J. 49 (8), 16471657.CrossRefGoogle Scholar
Galant, D. 1969 Gauss quadrature rules for the evaluation of $2 {\rm \pi}^{-1 / 2} \int _{0}^{\infty } \exp (-x^{2})\,f(x) \,\textrm {d}x$. Math. Comput. 23 (107), 676677.Google Scholar
Gan, C.J. & Wu, Z.N. 2006 Short-wave instability due to wall slip and numerical observation of wall-slip instability for microchannel flows. J.Fluid Mech. 550, 289306.CrossRefGoogle Scholar
Gersting, J. & John, M. 1974 Hydrodynamic stability of plane porous slip flow. Phys. Fluids 17 (11), 21262127.CrossRefGoogle Scholar
Guo, Z.L., Wang, R.J. & Xu, K. 2015 Discrete unified gas kinetic scheme for all Knudsen number flows. II. Thermal compressible case. Phys. Rev. E 91 (3), 033313.CrossRefGoogle ScholarPubMed
Guo, Z.L., Xu, K. & Wang, R.J. 2013 Discrete unified gas kinetic scheme for all Knudsen number flows: low-speed isothermal case. Phys. Rev. E 88 (3), 033305.CrossRefGoogle ScholarPubMed
Guo, Z.Y. & Li, Z.X. 2003 Size effect on microscale single-phase flow and heat transfer. Intl J. Heat Mass Transfer 46 (1), 149159.CrossRefGoogle Scholar
Hanifi, A., Schmid, P.J. & Henningson, D.S. 1996 Transient growth in compressible boundary layer flow. Phys. Fluids 8 (3), 826837.CrossRefGoogle Scholar
He, Q.L. & Wang, X.P. 2008 The effect of the boundary slip on the stability of shear flow. Z. Angew. Math. Mech. 88 (9), 729734.CrossRefGoogle Scholar
Ho, C.M. & Tai, Y.C. 1998 Micro-electro-mechanical-systems (MEMS) and fluid flows. Annu. Rev. Fluid Mech. 30 (1), 579612.CrossRefGoogle Scholar
Huang, J.C., Xu, K. & Yu, P.B. 2012 A unified gas-kinetic scheme for continuum and rarefied flows II: multi-dimensional cases. Commun. Comput. Phys. 12 (3), 662690.CrossRefGoogle Scholar
Lauga, E. & Cossu, C. 2005 A note on the stability of slip channel flows. Phys. Fluids 17 (8), 088106.CrossRefGoogle Scholar
Li, Z.H., Peng, A.P., Zhang, H.X. & Yang, J.Y. 2015 Rarefied gas flow simulations using high-order gas-kinetic unified algorithms for Boltzmann model equations. Prog. Aeronaut. Sci. 74, 81113.CrossRefGoogle Scholar
Li, Z.H. & Zhang, H.X. 2004 Study on gas kinetic unified algorithm for flows from rarefied transition to continuum. J.Comput. Phys. 193 (2), 708738.CrossRefGoogle Scholar
Lin, C.C. 1955 The Theory of Hydrodynamic Stability. Cambridge University Press.Google Scholar
Liu, H.T., Cao, Y., Chen, Q., Kong, M.C. & Zheng, L. 2018 A conserved discrete unified gas kinetic scheme for microchannel gas flows in all flow regimes. Comput. Fluids 167, 313323.CrossRefGoogle Scholar
Liu, S., Bai, J. & Zhong, C.W. 2015 Unified gas-kinetic scheme for microchannel and nanochannel flows. Comput. Maths Applics. 69 (1), 4157.CrossRefGoogle Scholar
Lockerby, D.A., Reese, J.M. & Gallis, M.A. 2005 Capturing the Knudsen layer in continuum-fluid models of nonequilibrium gas flows. AIAA J. 43 (6), 13911393.CrossRefGoogle Scholar
Malik, M., Dey, J. & Alam, M. 2008 Linear stability, transient energy growth, and the role of viscosity stratification in compressible plane Couette flow. Phys. Rev. E 77 (3), 036322.CrossRefGoogle ScholarPubMed
Malik, M.R. 1990 Numerical methods for hypersonic boundary layer stability. J.Comput. Phys. 86 (2), 376413.CrossRefGoogle Scholar
Min, T. & Kim, J. 2005 Effects of hydrophobic surface on stability and transition. Phys. Fluids 17 (10), 108106.CrossRefGoogle Scholar
Ohwada, T., Sone, Y. & Aoki, K. 1989 Numerical analysis of the shear and thermal creep flows of a rarefied gas over a plane wall on the basis of the linearized Boltzmann equation for hard-sphere molecules. Phys. Fluids A 1 (9), 15881599.CrossRefGoogle Scholar
Park, J.H., Bahukudumbi, P. & Beskok, A. 2004 Rarefaction effects on shear driven oscillatory gas flows: a direct simulation Monte Carlo study in the entire Knudsen regime. Phys. Fluids 16 (2), 317330.CrossRefGoogle Scholar
Peng, A.P., Li, Z.H., Wu, J.L. & Jiang, X.Y. 2016 Implicit gas-kinetic unified algorithm based on multi-block docking grid for multi-body reentry flows covering all flow regimes. J.Comput. Phys. 327, 919942.CrossRefGoogle Scholar
Pralits, J.O., Alinovi, E. & Bottaro, A. 2017 Stability of the flow in a plane microchannel with one or two superhydrophobic walls. Phys. Rev. Fluid 2 (1), 013901.CrossRefGoogle Scholar
Průša, V. 2009 On the influence of boundary condition on stability of Hagen–Poiseuille flow. Comput. Maths Applics. 57 (5), 763771.CrossRefGoogle Scholar
Ramachandran, A., Saikia, B., Sinha, K. & Govindarajan, R. 2016 Effect of Prandtl number on the linear stability of compressible Couette flow. Intl J. Heat Fluid Flow 61, 553561.CrossRefGoogle Scholar
Riechelmann, D. & Nanbu, K. 1993 Monte Carlo direct simulation of the Taylor instability in rarefied gas. Phys. Fluids A 5 (11), 25852587.CrossRefGoogle Scholar
Rostami, A.A., Mujumdar, A.S. & Saniei, N. 2002 Flow and heat transfer for gas flowing in microchannels: a review. Heat Mass Transfer 38 (4), 359367.CrossRefGoogle Scholar
Schmid, P.J. 2007 Nonmodal stability theory. Annu. Rev. Fluid Mech. 39 (1), 129162.CrossRefGoogle Scholar
Schmid, P.J. & Henningson, D.S. 1994 Optimal energy density growth in Hagen–Poiseuille flow. J.Fluid Mech. 277, 197225.CrossRefGoogle Scholar
Schmid, P.J. & Henningson, D.S. 2001 Stability and Transition in Shear Flows. Springer.CrossRefGoogle Scholar
Seo, J. & Mani, A. 2016 On the scaling of the slip velocity in turbulent flows over superhydrophobic surfaces. Phys. Fluids 28 (2), 025110.CrossRefGoogle Scholar
Shen, C. 2006 Rarefied Gas Dynamics: Fundamentals, Simulations and Micro Flows. Springer Science & Business Media.Google Scholar
Shizgal, B. 1981 A Gaussian quadrature procedure for use in the solution of the Boltzmann equation and related problems. J.Comput. Phys. 41 (2), 309328.CrossRefGoogle Scholar
Sone, Y. 2007 Molecular Gas Dynamics: Theory, Techniques, and Applications. Springer.CrossRefGoogle Scholar
Sone, Y., Handa, M. & Sugimoto, H. 2002 Bifurcation studies of flows of a gas between rotating coaxial circular cylinders with evaporation and condensation by the Boltzmann system. Transp. Theory Stat. Phys. 31 (4–6), 299332.CrossRefGoogle Scholar
Sone, Y., Takata, S. & Ohwada, T. 1990 Numerical analysis of the plane Couette flow of a rarefied gas on the basis of the linearized Boltzmann equation for hard-sphere molecules. Eur. J. Mech. (B/Fluids) 9 (3), 273288.Google Scholar
Spille, A., Rauh, A. & BüHring, H. 2000 Critical curves of plane Poiseuille flow with slip boundary conditions. Nonlinear Phenom. 3 (2), 171173.Google Scholar
Squires, T.M. & Quake, S.R. 2005 Microfluidics: fluid physics at the nanoliter scale. Rev. Mod. Phys. 77, 9771026.CrossRefGoogle Scholar
Stefanov, S. & Cercignani, C. 1992 Monte Carlo simulation of Bénard's instability in a rarefied gas. Eur. J. Mech. (B/Fluids) 11 (5), 543553.Google Scholar
Stefanov, S. & Cercignani, C. 1993 Monte Carlo simulation of the Taylor–Couette flow of a rarefied gas. J.Fluid Mech. 256, 199213.CrossRefGoogle Scholar
Stefanov, S. & Cercignani, C. 1994 Monte Carlo simulation of a channel flow of a rarefied gas. Eur. J. Mech. (B/Fluids) 13, 9393.Google Scholar
Stefanov, S. & Cercignani, C. 1998 Monte Carlo simulation of the propagation of a disturbance in the channel flow of a rarefied gas. Comput. Maths Applics. 35 (1–2), 4153.CrossRefGoogle Scholar
Straughan, B. & Harfash, A.J. 2013 Instability in Poiseuille flow in a porous medium with slip boundary conditions. Microfluid Nanofluid 15 (1), 109115.CrossRefGoogle Scholar
Vinogradova, O.I. 1999 Slippage of water over hydrophobic surfaces. Intl J. Miner. Process. 56 (1), 3160.CrossRefGoogle Scholar
Wang, P., Su, W., Zhu, L.H. & Zhang, Y.H. 2019 Heat and mass transfer of oscillatory lid-driven cavity flow in the continuum, transition and free molecular flow regimes. Intl J. Heat Mass Transfer 131, 291300.CrossRefGoogle Scholar
Wang, P., Wang, L.P. & Guo, Z. 2016 Comparison of the lattice Boltzmann equation and discrete unified gas-kinetic scheme methods for direct numerical simulation of decaying turbulent flows. Phys. Rev. E 94 (4), 043304.CrossRefGoogle ScholarPubMed
Wu, C., Shi, B.C., Chai, Z.H. & Wang, P. 2016 Discrete unified gas kinetic scheme with a force term for incompressible fluid flows. Comput. Maths Applics. 71 (12), 26082629.CrossRefGoogle Scholar
Xiong, X.M. & Tao, J.J. 2020 Linear stability and energy stability of plane Poiseuille flow with isotropic and anisotropic slip boundary conditions. Phys. Fluids 32 (9), 094104.CrossRefGoogle Scholar
Xu, K. & Huang, J.C. 2010 A unified gas-kinetic scheme for continuum and rarefied flows. J.Comput. Phys. 229 (20), 77477764.CrossRefGoogle Scholar
Yang, L.M., Shu, C., Wu, J. & Wang, Y. 2016 Numerical simulation of flows from free molecular regime to continuum regime by a DVM with streaming and collision processes. J.Comput. Phys. 306, 291310.CrossRefGoogle Scholar
Yang, Z.R., Zhong, C.W. & Zhuo, C.S. 2019 Phase-field method based on discrete unified gas-kinetic scheme for large-density-ratio two-phase flows. Phys. Rev. E 99 (4), 043302.CrossRefGoogle ScholarPubMed
Yoshida, H. & Aoki, K. 2006 Linear stability of the cylindrical Couette flow of a rarefied gas. Phys. Rev. E 73 (2), 021201.CrossRefGoogle ScholarPubMed
Zhang, C., Yan, K. & Guo, Z.L. 2018 A discrete unified gas-kinetic scheme for immiscible two-phase flows. Intl J. Heat Mass Transfer 126, 13261336.CrossRefGoogle Scholar
Zhang, R., Zhong, C.W., Liu, S. & Zhuo, C.S. 2020 Large-eddy simulation of wall-bounded turbulent flow with high-order discrete unified gas-kinetic scheme. Adv. Aerodyn. 2 (1), 27.CrossRefGoogle Scholar
Zhang, W.M., Meng, G. & Wei, X.Y. 2012 A review on slip models for gas microflows. Microfluid Nanofluid 13 (6), 845882.CrossRefGoogle Scholar
Zhu, L.H. & Guo, Z.L. 2017 Numerical study of nonequilibrium gas flow in a microchannel with a ratchet surface. Phys. Rev. E 95 (2), 023113.CrossRefGoogle Scholar