Milne-Thomson circle theorem explained

In fluid dynamics the Milne-Thomson circle theorem or the circle theorem is a statement giving a new stream function for a fluid flow when a cylinder is placed into that flow.[1] [2] It was named after the English mathematician L. M. Milne-Thomson.

Let

f(z)

be the complex potential for a fluid flow, where all singularities of

f(z)

lie in

|z|>a

. If a circle

|z|=a

is placed into that flow, the complex potential for the new flow is given by[3]

w=f(z)+\overline{f\left(

a2
\bar{z
} \right)} = f(z) + \overline f\left(\frac \right).

with same singularities as

f(z)

in

|z|>a

and

|z|=a

is a streamline. On the circle

|z|=a

,

z\barz=a2

, therefore

w=f(z)+\overline{f(z)}.

Example

Consider a uniform irrotational flow

f(z)=Uz

with velocity

U

flowing in the positive

x

direction and place an infinitely long cylinder of radius

a

in the flow with the center of the cylinder at the origin. Then
f\left(a2
\barz

\right)=

Ua2
\barz

,  ⇒ \overline{f\left(

a2
\bar{z
} \right)} = \frac, hence using circle theorem,

w(z)=U\left(z+

a2
z

\right)

represents the complex potential of uniform flow over a cylinder.

See also

Notes and References

  1. Book: Batchelor, George Keith. George Batchelor

    . George Batchelor. An Introduction to Fluid Dynamics. 1967. Cambridge University Press. 0-521-66396-2. 422.

  2. Book: Raisinghania, M.D.. Fluid Dynamics. December 2003. 9788121908696.
  3. Tulu. Serdar. Vortex dynamics in domains with boundaries. 2011.