2005•Unpublished venueRequires access

Instability of Plane Couette Flow

Hua-Shu Dou, Boo Cheong Khoo, Nhan Phan-Thien, Koon Seng Yeo

Open publisher page 7 citations

Abstract

The energy gradient theory has been proposed with the aim of better understanding the mechanism of flow transition from laminar flow to turbulent flow. In this theory, it is suggested that the transition to turbulence depends on the relative magnitudes of the energy gradient amplifying the disturbance and the viscous friction damping that disturbance. For a given flow geometry and fluid properties, when the maximum of K (the ratio of the energy gradient in the transverse direction to that in the streamwise direction) in the flow field is larger than a certain critical value, it is expected that instability would occur for some initial disturbances. In this paper, using the energy analysis, the equation for calculating K for plane Couette flow is derived. It is demonstrated that the critical value of K at subcritical transition is about 370 for plane Couette flow. This value is about the same as for plane Poiseuille flow and pipe Poiseuille flow (385-389). Therefore, it is concluded that the critical value of K at subcritical transition is about 370-389 for wall bounded parallel shear flows which include both pressure and shear driven flows.

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What this paper is about

The energy gradient theory has been proposed with the aim of better understanding the mechanism of flow transition from laminar flow to turbulent flow. In this theory, it is suggested that the transition to turbulence depends on the relative magnitudes of the energy gradient amplifying the disturbance and the viscous friction damping that disturbance. For a given flow geometry and fluid properties, when the maximum of K (the ratio of the energy gradient in the transverse direction to that in the streamwise direction) in the flow field is larger than a certain critical value, it is expected that instability would occur for some initial disturbances. In this paper, using the energy analysis, the equation for calculating K for plane Couette flow is derived. It is demonstrated that the critical value of K at subcritical transition is about 370 for plane Couette flow. This value is about the same as for plane Poiseuille flow and pipe Poiseuille flow (385-389). Therefore, it is concluded that the critical value of K at subcritical transition is about 370-389 for wall bounded parallel shear flows which include both pressure and shear driven flows.

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Available abstract

The energy gradient theory has been proposed with the aim of better understanding the mechanism of flow transition from laminar flow to turbulent flow. In this theory, it is suggested that the transition to turbulence depends on the relative magnitudes of the energy gradient amplifying the disturbance and the viscous friction damping that disturbance. For a given flow geometry and fluid properties, when the maximum of K (the ratio of the energy gradient in the transverse direction to that in the streamwise direction) in the flow field is larger than a certain critical value, it is expected that instability would occur for some initial disturbances. In this paper, using the energy analysis, the equation for calculating K for plane Couette flow is derived. It is demonstrated that the critical value of K at subcritical transition is about 370 for plane Couette flow. This value is about the same as for plane Poiseuille flow and pipe Poiseuille flow (385-389). Therefore, it is concluded that the critical value of K at subcritical transition is about 370-389 for wall bounded parallel shear flows which include both pressure and shear driven flows.

Key concepts: Hagen–Poiseuille equation, Couette flow, Turbulence, Mechanics, Laminar flow, Instability, Physics, Isothermal flow

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