Russell J. Donnelly 5413464226 (Tel) 5413465861 (Fax) 

Taylor Vortex Flow Introduction (Adapted from R. Tagg, Nonlinear Science Today, 4, 1994)The
CouetteTaylor problem concerns flow between independently rotating cylinders.
It is a widely studied example of a system removed from equilibrium, in
which the nonequilibrium condition is achieved by inducing mechanical
stresses on the fluid through motion of the cylinder walls. The system,
originally designed independently by Couette (1888) and Mallock (1888)
for investigation of the viscous behavior of fluids, was the subject of
a landmark work by G. 1. Taylor (1923). In his study, Taylor quantitatively
predicted and experimentally confirmed the existence of a flow instability
when the inner cylinder reaches a critical speed. For low cylinder speeds,
the fluid simply moves azimuthally around the cylinders. Taylor observed
that when this simple flow becomes unstable, it is replaced by a cellular
pattern in which the fluid travels in helical paths around the cylinders
in layers of vorticesnow known as Taylor vortices (figs. 2,3). "TaylorCouette Flow: The Early Days", R. J. Donnelly. Physics Today, November 1991: 3239 (1991), and the progression of instrumentation is described in: "Evolution of Instrumentation for TaylorCouette Flow" R. J. Donnelly. Ordered and Turbulent Patterns in TaylorCouette Flows. C. D. Andereck and F. Hayot, Eds. New York, Plenum Press: 127.(1992). TaylorCouette flow of helium II Taylor Couette flow has many variants. The first problem attempted by the Donnelly group was to see if the linear stability theory for the classical Taylor vortex problem could be made to work for the twofluid theory of helium II. The importance of this problem is that the celebrated Taylor analysis settled the case for the validity of the Navier Stokes equation and the boundary conditions. The first attempt was by Chandrasekhar and Donnelly, but who got it wrong because the form of the equations of motion (called HVBK today) was still up in the air, and they neglected the term in vortex tension. "The Hydrodynamic Stability of Helium II Between Rotating Cylinders, I", S. Chandrasekhar and R. J. Donnelly. Proc. Roy. Soc. A214: 928 (1958) The first experiments on this subject were done by Donnelly in an early PRL: "Experiments on the Hydrodynamic Stability of Helium II Between Rotating Cylinders", R. J. Donnelly. Phys. Rev. Lett. 3: 507508 (1959). The apparatus (at the University of Chicago) is shown below.



The
linking of theory to experiment took many more years. The next main step
was a review article designed to interest the applied mathematics community:
"Flow and Stability of Helium II Between Concentric Cylinders", R. J. Donnelly and M. M. LaMar.J. Fluid. Mech.(1988). The challenge was taken up by C. A. Jones and C. F. Barenghi who produced a very complete set of predictions. We decided to look for their predictions using second sound, and the results formed Chris Swanson’s PhD thesis, and appeared in "Instability of TaylorCouette Flow of Helium II", C. J. Swanson and R. J. Donnelly. Phys. Rev. Lett. 67: 15781581 (1991). This experiment is the first instance of success of a linear instability theory with modern equations of motion for helium II and shows that the equations and boundary conditions used in the analysis are correct. This most recent version of the equations of motion is due to Hills and Roberts. Torque measurements in TaylorCouette flow The apparatus shown above made it easy to do useful experiments in room temperature fluids as well. These were done and summarized in a review article: "An Empirical Torque Relation for
Supercritical Flow Between Rotating Cylinders", R. J. Donnelly and
N. J. Simon. J. Fluid. Mech. 7(Pt. 3): 401418 (1960). Chandrasekhar also worked on the stability of hydromagnetic flows, in particular TaylorCouette flow of a conducting fluid in a magnetic field (see Chandra’s remarkable book Hydrodynamic and Hydromagnetic Stability, Oxford, 1961). Our group undertook to verify these calculations using the hydromagnetic Couette viscometer shown below, with magnetic field furnished by an old cyclotron magnet. The results were published in 1962: "Experiments on the Stability of Flow Between Rotating Cylinders in the Presence of a Magnetic Field", R. J. Donnelly and M. Ozima. Proc. Roy. Soc. A266: 272286 (1962). The
experiment in place is shown below. This cyclotron now sits beside the
entrance drive to Fermilab.



The
ion technique
In the days before techniques such as LDV and PIV were invented, there was no quantitative way to see the Taylor vortices. We therefore devised an electrochemical technique which allowed direct observation of the vortex array: "Experiments on the Stability of Viscous Flow Between Rotating Cylinders IV. The Ion Technique", R. J. Donnelly. Proc. Roy. Soc. A283: 509519 (1965). The principal of obtaining scans of the vortex patterns is shown below:
This
technique allowed Donnelly and Schwarz to verify the “Landau Law”
for the growth of equilibrium amplitude of vortex motion above critical:


Modulated Taylor vortex flow Acting on a suggestion by Fred Reif and Harry Suhl, we began an investigation into the stability of modulated Taylor Vortex flow. In the days before stepping motors we had to use one Graham variable speed drive to modulate the speed control of another:
This problem lasted for many years with various twists and turns, and even was extended to Rayleigh Bénard convection. A review article summarizes the present situation briefly: "Externally
Modulated Hydrodynamic Systems", R. J. Donnelly in. Nonlinear Evolution
of Spatiotemporal Structures in Dissipative Continuous Systems F.
Busse, ed., Streitberg (Bayreuth) Germany,1990. 

Visual Studies of Taylor Couette Flow
Russell Donnelly and Dave Fultz constructed a large rotating cylinder
pair at the University of Chicago. This is shown in the photograph below
taken in 1961, with Sir Geoffrey Taylor and Dave Fultz. Many of the visual
experiments are described in Chandrasekhar’s 1961 stability book.
A photo of Chandra the day the book was received is shown below.


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