Von Kármán swirling flow is a flow created by a uniformly rotating infinitely long plane disk, named after Theodore von Kármán who solved the problem in 1921. The rotating disk acts as a fluid pump and is used as a model for centrifugal fans or compressors. This flow is classified under the category of steady flows in which vorticity generated at a solid surface is prevented from diffusing far away by an opposing convection, the other examples being the Blasius boundary layer with suction, stagnation point flow etc.

Flow description 
Consider a planar disk of infinite radius rotating at a constant angular velocity  in fluid which is initially at rest everywhere. Near to the surface, the fluid is being turned by the disk, due to friction, which then causes centrifugal forces which move the fluid outwards. This outward radial motion of the fluid near the disk must be accompanied by an inward axial motion of the fluid towards the disk to conserve mass. Theodore von Kármán noticed that the governing equations and the boundary conditions allow a solution such that  and  are functions of  only, where  are the velocity components in cylindrical  coordinate with  being the axis of rotation and  represents the plane disk. Due to symmetry, pressure of the fluid can depend only on radial and axial coordinate .
Then the continuity equation and the incompressible Navier–Stokes equations reduce to

where  is the kinematic viscosity.

No rotation at infinity  

Since there is no rotation at large ,  becomes independent of  resulting in . Hence  and .

Here the boundary conditions for the fluid  are

Self-similar solution is obtained by introducing following transformation,  

where  is the fluid density.

The self-similar equations are

 

with boundary conditions for the fluid  are

The coupled ordinary differential equations need to be solved numerically and an accurate solution is given by Cochran(1934). The inflow axial velocity at infinity obtained from the numerical integration is , so the total outflowing volume flux across a cylindrical surface of radius  is . The tangential stress on the disk is . Neglecting edge effects, the torque exerted by the fluid on the disk with large () but finite radius  is

The factor  is added to account for both sides of the disk. From numerical solution, torque is given by . The torque predicted by the theory is in excellent agreement with the experiment on large disks  up to the Reynolds number of about , the flow becomes turbulent at high Reynolds number.

Rigid body rotation at infinity  
This problem was addressed by George Keith Batchelor(1951). Let  be the angular velocity at infinity. Now the pressure at  is . Hence  and .
Then the boundary conditions for the fluid  are

Self-similar solution is obtained by introducing following transformation,

The self-similar equations are

 

with boundary conditions for the fluid  is

The solution is easy to obtain only for  i.e., the fluid at infinity rotates in the same sense as the plate. For , the solution is more complex, in the sense that many-solution branches occur. Evans(1969) obtained solution for the range . Zandbergen and Dijkstra showed that the solution exhibits a square root singularity as  and found a second-solution branch merging with the solution found for . The solution of the second branch is continued till , at which point, a third-solution branch is found to emerge. They also discovered an infinity of solution branches around the point . Bodoyni(1975) calculated solutions for large negative , showed that the solution breaks down at . If the rotating plate is allowed to have uniform suction velocity at the plate, then meaningful solution can be obtained for . 

For  ( represents solid body rotation, the whole fluid rotates at the same speed) the solution reaches the solid body rotation at infinity in an oscillating manner from the plate. The axial velocity is negative  for  and positive  for . There is an explicit solution when .

Nearly rotating at the same speed,  
Since both boundary conditions for  are almost equal to one, one would expect the solution for  to slightly deviate from unity. The corresponding scales for  and  can be derived from the self-similar equations. Therefore, 

To the first order approximation(neglecting ), the self-similar equation  becomes

 

with exact solutions

These solution are similar to an Ekman layer solution.

Non-Axisymmetric solutions 
The flow accepts a non-axisymmetric solution with axisymmetric boundary conditions discovered by Hewitt, Duck and Foster. Defining

and the governing equations are

with boundary conditions

The solution is found to exist from numerical integration for .

Bödewadt flow
Bödewadt flow describes the flow when a stationary disk is placed in a rotating fluid.

Two rotating coaxial disks  
This problem was addressed by George Keith Batchelor(1951), Keith Stewartson(1952) and many other researchers. Here the solution is not simple, because of the additional length scale imposed in the problem i.e., the distance  between the two disks. In addition, the uniqueness and existence of a steady solution are also depend on the corresponding Reynolds number .
Then the boundary conditions for the fluid  are

In terms of , the upper wall location is simply . Thus, instead of the scalings 

used before, it is convenient to introduce following transformation,

so that the governing equations become

with six boundary conditions

and the pressure is given by

Here boundary conditions are six because pressure is not known either at the top or bottom wall;  is to be obtained as part of solution. For large Reynolds number , Batchelor argued that the fluid in the core would rotate at a constant velocity, flanked by two boundary layers at each disk for  and there would be two uniform counter-rotating flow of thickness  for . However, Stewartson predicted that for  the fluid in the core would not rotate at , but just left with two boundary layers at each disk. It turns out, Stewartson predictions were correct (see Stewartson layer).

There is also an exact solution if the two disks are rotating about different axes but for .

Applications 

Von Kármán swirling flow finds its applications in wide range of fields, which includes rotating machines, filtering systems, computer storage devices, heat transfer and mass transfer applications, combustion-related problems, planetary formations, geophysical applications etc.

References

Bibliography

 

Fluid dynamics
Flow regimes