Über die Stabilität freier Grenzschichten zwischen leitenden und isolierenden Fluiden im transversalen Magnetfeld bei endlichen Werten der magnetischen Reynoldszahl

Übersicht Es wurde eine theoretische Untersuchung der Stabilität einer freien leitenden Grenzschicht im transversalen Magnetfeld unter Berücksichtigung des Einflusses der magnetischen Reynoldszahl durchgeführt. Für den Spezialfall einer Isolator-Leiter-Sprungschicht wird unter Beschränkung auf ebene Störungen gezeigt, daß im Falle des Leerlaufbetriebes sowie für kleine Abweichungen von diesem der Einfluß der magnetischen Reynoldszahl sowie der der Hartmannzahl relativ unbedeutend ist, während der Wechselwirkungsparameter der wesentlichste MHD-Parameter des Problems ist.

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Summary A theoretical study of the stability of free conducting shear layers in a transverse, magnetic field in the range of finite magnetic Reynolds numbers was performed. In the special case of a layer between insulating and conducting fluids and with restriction to plane disturbances it was shown that, in the idling motion case as well as in the case of small deviations from it, the influence of the magnetic Reynolds number and the one of the Hartmann number is comparatively small and the interaction parameter is the most important MHD-parameter of the problem.

     

High Péclet number heat exchange between cocurrent streams

Summary  This paper concentrates on the analysis of the heat transfer between two cocurrent laminar flows in parallel channels. For high values of the Péclet number Pe, a boundary layer arises near the wall separating the streams. Matched asymptotic expansions (MAE) are used to obtain approximate solutions. We consider arbitrary inlet temperatures and derive higher-order corrections of the boundary problem. The separating wall is supposed to be sufficiently thin to neglect the heat conduction in it. Analyticity and adiabatic conditions at the outer walls impose restrictions on the inlet temperatures. It turns out, however, that only the inlet temperatures at the wall separating the two fluids enter the leading-order problem. The Nusselt numbers thus calculated are in the leading order proportional to (Pe/x)^1/3, where x is the stream-wise coordinate. An estimate of the thickness of the separating wall to validate the MAE approach is obtained. It is also demonstrated that the MAE analysis is unable to describe the heat exchange of counterflowing fluids. Received 9 June 1999; accepted for publication 17 November 1999     

Hopf Bifurcations and Hysteresis in Flow-induced Vibrations of Cylinders

Flow-induced oscillations of rigid cylinders exposed to fully developed flow can be described by a fourth order autonomous system of ordinary differential equations. Its rest solution is the only equilibrium point which is unstable in the entire regime of parameters. It turns out that Hopf bifurcations from the trivial solution occur in regions of comparatively low damping. We found that a wind speed parameter, Ω, controls the bifurcations while the other parameters have been arranged into discrete sets. In the case of two bifurcating solutions with branches of amplitudes tending towards each other, hysteresis occurred. The bifurcating solutions are unstable close to their respective bifurcation points. The branch tending to the left-hand side changes its stability and exhibits high-level amplitudes of synchronized oscillations. This type of solution can also be analysed by means of asymptotic methods. Near the location of the bifurcation, the predictions of bifurcation theory, the multiple scales approach, and numerics are in quite good agreement. As opposed to this, the branch tending to the right-hand side represents synchronized oscillations of somewhat smaller period but much smaller cylinder amplitudes, and these vibrations remain unstable in the entire regime of parameters. This means that keeping the cylinder fixed, starting the wind tunnel, and releasing the cylinder at low wind speeds would lead to a jump of its displacement amplitude from the low, unstable to the comparatively high-stable values. It is shown that the theoretical predictions are in fairly good agreement with the experimental trends of flow-induced synchronized cylinder oscillations.     

Deterministic and Stochastic Oscillations of a Flexible Cylinder in Arrays of Static Tubes

This study concentrates on vortex-induced vibrations of one flexiblecylinder in an array of fixed tubes. To describe approximately thedynamics of this system we generalize a previously developed linearsemi-empirical model that includes memory effects. We choose a cubicdamping term to model adequately vortex-induced oscillations and weobtain thus a nonlinear integro-differential equation governing thedisplacement of the cylinder. We use a two-variable expansion to derivecriteria for the appearance of stable, periodic, nonlinear oscillations.This approach predicts the appearance of a limit cycle and gives acriterion for the stability of the oscillations. In a stochasticoscillation model we apply additive white noise to the otherwisedeterministic oscillator model. For small values of the noise intensitywe can approximately solve the Fokker–Planck equation. A comparison ofthis approximation with numerical simulations shows a satisfactorydegree of agreement.     

The transition of flow-induced cylinder vibrations to chaos

Flow-induced oscillations of rigid cylinders exposed to fully developed turbulent flow can be described by a fourth order autonomous system. Among the pertinent constants, the mass ratio is the control parameter governing the transition from limit cycle oscillations to chaotic vibrations. Particular attention is paid to the stability of the limit cycles: it has been found that they lose their stability at the point of appearance of quasi-periodic motion. The documentation of this transition is performed in terms of Lyapunov exponents, phase plots, Fourier spectra, bifurcation diagrams, and Poincaré maps. As opposed to the calculation of the Lyapunov exponents where remarkable numerical difficulties were encountered, the investigation of the remaining quantities shows clearly the passage of cylinder motions from limit cycle oscillations to more and more irregular vibrations, leading finally to chaos.