Transitions to chaos in the spherical couette flow due to periodic variations in the rotation velocity of one of the boundaries

The results of an experimental investigation of unsteady viscous incompressible flows in a spherical gap, when the rotation velocity of one sphere varies in accordance with the harmonic law, while that of the other sphere remains constant, are presented. The modulation amplitudes and frequencies are small compared with the mean rotation velocities of the spheres. Transition to chaos is studied in a layer, whose thickness is equal to the inner sphere radius, in the case of counter rotation of the spherical boundaries. A periodic flow generated as a result of the mutual synchronization of the frequencies of a three-frequency regime preceding that under study at lower Reynolds numbers is taken as the original state. It is shown that certain properties of turbulent flows near the threshold of their formation essentially depend on the modulation frequency.     

Two-phase couette flow

A study is made of plane laminar Couette flow, in which foreign particles are injected through the upper boundary. The effect of the particles on friction and heat transfer is analyzed on the basis of the equations of two-fluid theory. A two-phase boundary layer on a plate has been considered in [1, 2] with the effect of the particles on the gas flow field neglected. A solution has been obtained in [3] for a laminar boundary layer on a plate with allowance for the dynamic and thermal effects of the particles on the gas parameters. There are also solutions for the case of the impulsive motion of a plate in a two-phase medium [4–6], and local rotation of the particles is taken into account in [5, 6]. The simplest model accounting for the effect of the particles on friction and heat transfer for the general case, when the particles are not in equilibrium with the gas at the outer edge of the boundary layer, is Couette flow. This type of flow with particle injection and a fixed surface has been considered in [7] under the assumptions of constant gas viscosity and the simplest drag and heat-transfer law. A solution for an accelerated Couette flow without particle injection and with a wall has been obtained in [6]. In the present paper fairly general assumptions are used to obtain a numerical solution of the problem of two-phase Couette flow with particle injection, and simple formulas useful for estimating the effect of the particles on friction and heat transfer are also obtained.Translated from Izvestiya Akademii Nauk SSSR, Mekhanika Zhidkosti i Gaza, No. 3, pp. 42–46, May–June, 1976.     

Stability of nonisothermal couette flow

A study is made of the loss of stability of the stationary flow of a viscous fluid between two heated rotating cylinders. The linearized stability problem is studied in the Boussinesq approximation. The perturbations are assumed to be periodic in the time, and also in the axial and azimuthal directions. The neutral curves are calculated numerically. The ranges of variation of the parameters of the problem are found, and in them the most dangerous perturbations (in the class of spatially periodic perturbations) are those without rotational symmetry.Translated from Izvestiya Akademii Nauk SSSR, Mekhanika Zhidkosti i Gaza, No. 1, pp. 167–170, January–February, 1980.I thank V. I. Yudovich for constant interest in the work.     

Secondary regimes in couette flow

We consider the asymptotic solutions of secondary steady flows in a fluid contained between cylinders rotating in the same direction for large Reynolds numbers.The existence of secondary axisymmetric steady flows in a fluid contained between cylinders rotating in the same direction was shown in [1, 2]. In the following we present the asymptotic behavior of such solutions for the case of large Reynolds numbers. The construction follows the scheme suggested in [3].     

Asymptotic investigation of two-phase couette flow

We consider plane and cylindrical Couette flow for a two-phase medium. The motion of the medium is described by the equations obtained in [1]. Collisions between the particles are disregarded, and their motion, in addition to the inertial forces, is determined by the pressure gradient of the carrying phase and the forces of viscous interaction between the carrying phase and the particles. We obtain simple asymptotic solutions of the indicated problems for small and large values of the dimensionless determining parameters. In a number of cases the solution has the nature of a boundary layer on solid walls.Translated from Izvestiya Akademii Nauk SSSR, Mekhanika Zhidkosti i Gaza, No. 4, pp. 67–73, July–August, 1978.     

Natural convection in unsteady MHD couette flow

 The combined effect of natural convection and uniform transverse magnetic field on the couette flow of an electrically conducting fluid between two parallel plates for impulsive motion of one of the plates in discussed. Under the assumption of negligible induced magnetic field and applied magnetic field being fixed relative to the fluid or plate, the governing equations have been solved exactly, and the expressions for velocity and temperature field have been presented for two different cases. A comparative study is made between the velocity field for magnetic field fixed with respect to plate and magnetic field fixed with respect to fluid. Received on 12 July 1999     

Numerical analysis of the stability of nonisothermal couette flow

The stability of convective motion of a liquid between two rotating heated cylinders is investigated in the absence of external forces. The mathematical model for describing the convection is obtained from the general equations [1, 2] on the assumption that the density of the liquid, the thermal conductivity, the specific heat and the viscosity coefficients depend only on temperature, and that the work done by the pressure forces and the viscous dissipation are negligibly small. The thermal expansion coefficient of the liquid is not assumed to be small, which distinguishes the models in question from the classical Oberbeck-Boussinesq model [1, 3, 4]. Rostov-on-Don. Translated from Izvestiya Akademii Nauk SSSR, Mekhanika Zhidkosti i Gaza, No. 5, pp. 70–76, September–October, 1988.     

Characteristics of a viscoplastic material in the couette flow

A model governing a steady flow of a viscoplastic material between coaxial cylinders is proposed. Nonlinear velocity sensitivity typical of superplastic materials is taken into account. An algorithm of calculating the characteristics of the material is developed. The algorithm is based on the experimental data on moments and angular velocities of the rotating coaxial cylinders. The stability of the algorithm to errors in the initial data is estimated.     

Unsteady-state development of plane couette flow for viscoelastic fluids

Unsteady-state development of plane Couette flow for viscoelastic fluids is analyzed using a constitutive equation that can be obtained from molecular theory, in which the molecules are regarded as finitely extensible dumbbells. Typical features of the flow situation are as follows: (i) For a fluid with moderate elasticity, not only stress overshoot but also velocity overshoot are predicted. (ii) For suitable combinations of elasticity and gap width, and for some time intervals stress propagation and reflection phenomena are predicted. (iii) After a sufficient time has elapsed, the stress state behaves similarly to that corresponding to the start-up of a steady simple shear flow.     

Numerical simulation of instabilities and secondary regimes in spherical couette flow

In all previous numerical investigations of spherical Couette flow only axisymmetric regimes were considered. At the same time, in experiments [1–4] it was found that when both spheres rotate and the layer is thin centrifugal instability of the main flow leads to the appearance of nonaxisymmetric secondary flows of the azimuthal traveling wave type. The results of an initial numerical investigation of these flows are presented below. Solving the linear problem of the stability of the main flow and simulating the secondary flows on the basis of the complete nonlinear Navier-Stokes equations has made it possible to supplement and explain many of the results obtained experimentally. The type of bifurcation and the structure of the disturbances whose growth leads to the appearance of three-dimensional nonstationary flows are determined, and the transitions between different secondary regimes in the region of weak supercriticality are described.Moscow. Translated from Izvestiya Rossiiskoi Akademii Nauk, Mekhanika Zhidkosti i Gaza, No. 1, pp. 3–15, January–February, 1995.     

Mass transport for couette flow in a flat conduit

The mass transport is determined in a two-dimensional channel due to pure shear-Couette flow. Local concentration, mean concentration and flux at the walls of the conduit are determined analytically for arbitrary wall velocity ratios. The special case of a fixed lower wall and a moving upper wall of the channel has been numerically evaluated. In addition the case of linear homogeneous chemical reaction has been treated for shear flow of the liquid in the conduit.

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Stofftransport bei Couette-Strömung im Kanal

Zusammenfassung Es wird der Stofftransport in einem Kanal mit reiner Scher-Couette-Strömung analytisch bestimmt. Dabei wird die lokale Konzentration, die mittlere Konzentration, sowie der Konzentrationsflu\ über die WÄnde bei beliebigem GeschwindigkeitsverhÄltnis der WÄnde bestimmt. Die numerische Auswertung der analytischen Ergebnisse beschrÄnkte sich auf den Fall des Stofftransportes in einem Kanal, dessen untere Wand sich in Ruhe befindet, wÄhrend die obere Wand sich mit konstanter Geschwindigkeit bewegt. Es wird au\erdem die Konzentration bei linearer homogener chemischer Reaktion bei Scherströmung angegeben.

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Nomenclature c concentration - c _w wall concentration aty=0,h - c _i initial concentration atx = 0 - ¯ c (x) mean concentration - D diffusion coefficient - h width of the channel - k ^* homogeneous chemical reaction coefficient - u ₁ velocity of lower channel wally=0 - u ₂ velocity of upper channel wally=h - x axial coordinate - y coordinate perpendicular to channel (y ^*=y/h) - _n, _n Eigenvalues - J _±1/3 Besselfunction of ±1/3 order     

Stability of the inviscid plane couette flow in bubbly fluids

The aim of this article is to study the stability of shear flows in bubbly fluids. A mathematical model of bubbly fluids is presented. The stability of shear flows is studied by two methods: by using a spectral approach and by solving the initial-value problem. It is proved that the linear velocity profile is stable in the long wave approximation. Communicated by R. Grimshaw     

Effect of nonuniform accommodation coefficient distribution on the couette flow

The Couette flow is considered for surfaces with nonuniformly distributed energy accommodation coefficients α. It is shown that at Knudsen numbers greater or of the order of unity heat fluxes and viscous stresses can be considerably optimized by varying the surface distribution of α at a fixed integral value. At the same time, for Kn ≪ 1 the flows with nonuniformly distributed α are similar with the flow with a constant accommodation coefficient equal to its mean value.