Abstract:Abstract.The eigenvalue problem for the linear stability of Couette flow between two rotating concentric cylinders to axisymmetric disturbances is considered. It is proved that the principle of exchange of stabilities holds when the cylinders rotate in the same direction and the circulation decreases outwards. The proof is based on the notion of a positive operator which is analogous to a positive matrix. Such operators have a spectral property which implies the principle of exchange of stabilities.
“…This is the principle of exchange of stabilities (PES) which in the early years made it much easier to uncover the instability. As the theory has developed, this is also vital in describing the approach to nonlinear instability as well in the "Rayleigh-unstable" case where μ < η 2 [6]. However, because this work involves an instability primarily associated with slip, we are interested in the case where μ > η 2 , and A < 0 in (2.8), while B > 0 in (2.9); still the Taylor numberT > 0.…”
Section: Exchange Of Stabilitiesmentioning
confidence: 99%
“…Dimensionless parameters. The more recent approach ( [2], [6]) has been to scale the system so that r 1 = η and r 2 = 1, while in [14] Synge scaled the inner radius to unity. The rotation rates are taken as Ω 1 and μΩ 1 , respectively.…”
Viscous Couette flow is derived for flow between two infinitely long concentric rotating cylinders with Navier slip on both. Its axisymmetric linear stability is studied within a regime that would be hydrodynamically stable according to Rayleigh's criterion: opposing gradients of angular velocity and specific angular momentum, based on the rotation rates and radii of the cylinders. Stability conditions are analyzed, by methods based on those of Synge and Chandrasekhar. For sufficiently small slip length on the outer cylinder no instability occurs with arbitrary slip length on the inner cylinder. As a corollary, slip on the inner cylinder is shown to be stabilizing, with no slip on the outer cylinder. Two slip configurations are investigated numerically, first with slip only on the outer cylinder, then second with equal slip on both cylinders. It is found that instability does occur (for large outer slip length), and the principle of exchange of stabilities emerges. The instability disappears for sufficiently large slip length in the second case; Rayleigh's criterion provides an explanation for these phenomena.
“…This is the principle of exchange of stabilities (PES) which in the early years made it much easier to uncover the instability. As the theory has developed, this is also vital in describing the approach to nonlinear instability as well in the "Rayleigh-unstable" case where μ < η 2 [6]. However, because this work involves an instability primarily associated with slip, we are interested in the case where μ > η 2 , and A < 0 in (2.8), while B > 0 in (2.9); still the Taylor numberT > 0.…”
Section: Exchange Of Stabilitiesmentioning
confidence: 99%
“…Dimensionless parameters. The more recent approach ( [2], [6]) has been to scale the system so that r 1 = η and r 2 = 1, while in [14] Synge scaled the inner radius to unity. The rotation rates are taken as Ω 1 and μΩ 1 , respectively.…”
Viscous Couette flow is derived for flow between two infinitely long concentric rotating cylinders with Navier slip on both. Its axisymmetric linear stability is studied within a regime that would be hydrodynamically stable according to Rayleigh's criterion: opposing gradients of angular velocity and specific angular momentum, based on the rotation rates and radii of the cylinders. Stability conditions are analyzed, by methods based on those of Synge and Chandrasekhar. For sufficiently small slip length on the outer cylinder no instability occurs with arbitrary slip length on the inner cylinder. As a corollary, slip on the inner cylinder is shown to be stabilizing, with no slip on the outer cylinder. Two slip configurations are investigated numerically, first with slip only on the outer cylinder, then second with equal slip on both cylinders. It is found that instability does occur (for large outer slip length), and the principle of exchange of stabilities emerges. The instability disappears for sufficiently large slip length in the second case; Rayleigh's criterion provides an explanation for these phenomena.
“…Since that time, it has been developed quite conclusively that for Spiral-Couette flow and for the more general Spiral-Poiseuille flow, that though a complicated competition of modes takes place [10,11], steady helical vortices are observed. In this context, a special problem is treated in this work, as part of a series of studies on mathematical issues arising from the onset of fluid instabilities [5,12,13]. The basic flow under consideration occurs between two infinitely long coaxial cylindrical pipes, with inner and outer radii a and b, respectively.…”
“…That is, we prove that Chandrasekhar's reduced system of equations predict stability when ∂(r 2 Ω) 2 /∂r > 0, at least for insulating magnetic boundary conditions, which are particularly relevant to experiments. Our proof makes use of insights and techniques developed by Herron and Ali ( [11]) (see also [10]). …”
Axisymmetric stability of viscous resistive magnetized Couette flow is re-examined, with emphasis on flows that would be hydrodynamically stable according Rayleigh's criterion: opposing gradients of angular velocity and specific angular momentum. In this regime, magnetorotational instability (MRI) may occur. The governing system in cylindrical coordinates is of tenth order. It is proved, by methods based on those of Synge and Chandrasekhar, that by dropping one term from the system, MRI is suppressed, in fact no instability at all occurs, with insulating boundary conditions. This term is often neglected because it has the magnetic Prandtl number, which is very small, as a factor; nevertheless it is crucially important. (2000). 76E25.
Mathematics Subject Classification
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