Exercise
8. Let
denote
the branch of the inverse of
that
is a
one-to-one mapping of the
-plane
slit along the segment
onto
the domain
.
Use the complex potential
, in
the
-plane
to show that the complex potential
,
determines the ideal fluid flow around the
segment
,
where the velocity at points distant from the origin is given
by
, (as
shown in Figure
11.58).
Solution 8.
Use the result of Exercise 2
where we see that the complex potential
determines
the ideal fluid flow
around the unit circle
, where
the velocity at points distant from the origin is given approximately
by
;
that is, the direction of the flow for large values of
is inclined at an angle
with the
axis. The complex potential in the
plane is
Now use the trigonometric
identities
and
.
This produces the desired complex potential in the z-plane
.
We are done.
Aside. For
illustration we can make a plot of the stream function
using
.
![[Graphics:../Images/FluidFlowModHome_gr_317.gif]](../Images/FluidFlowModHome_gr_317.gif)
Flow around a plate at a 45o angle.
The
complex potential is
.
We are really done.
The inverse
of
is
.
![[Graphics:../Images/FluidFlowModHome_gr_322.gif]](../Images/FluidFlowModHome_gr_322.gif)
A
conformal branch of the mapping
.
This solution is complements of the authors.
(c) 2008 John H. Mathews, Russell W. Howell