Exercise
3. Let the lines
and
form
the walls of a containing vessel for a fluid flow in the
infinite strip
that
is produced by a single source located at the
point
.
Find the complex potential for the flow in Figure
11.101.
Figure 11.101.
Solution 3.
Answer. Use
the result in Example 11.32.
Both positive and negative y-axes are
streamlines for the complex potential
.
![[Graphics:../Images/SourceSinkModHome_gr_139.gif]](../Images/SourceSinkModHome_gr_139.gif)
Hence, the
positive and negative y-axes could
also be interpreted as walls for a fluid flow in the semi-infinite
strip
.
Therefore, the desired complex potential
is
.
Solution. In
Example 10.13 in Section
10.4, we saw that the
transformation
is a one-to-one conformal mapping of the vertical
strip
onto
the w-plane slit along the
rays
and
.
Also, the point
is
mapped onto
, and
the imaginary axis
in
the z-plane
is mapped onto the imaginary axis
in
the w-plane.
In the complex
w-plane
is
the complex potential for a unit source at the
origin
, and
the positive u-axis and both positive
and negative v-axes are streamlines
in for the complex potential
.
Since
will
map the the infinite strip
onto
the right half-plane
,
the composition
is
the desired complex potential in the infinite
strip
,
where a single source located at the point
and the lines
and
form
the walls of the containing vessel.
We are done.
Aside. We can let Mathematica double check our work.
The velocity potential
is
The stream function
is
We are really done.
We can let Mathematica graph some of the streamlines and velocity potentials.
![[Graphics:../Images/SourceSinkModHome_gr_171.gif]](../Images/SourceSinkModHome_gr_171.gif)
Some
streamlines
for
a fluid flow in the infinite strip
that
is produced by a single source located at the
point
.
![[Graphics:../Images/SourceSinkModHome_gr_175.gif]](../Images/SourceSinkModHome_gr_175.gif)
Some
velocity potentials
for
a fluid flow in the infinite strip
that
is produced by a single source located at the
point
.
![[Graphics:../Images/SourceSinkModHome_gr_179.gif]](../Images/SourceSinkModHome_gr_179.gif)
Streamlines
and velocity potentials for a fluid flow in the infinite
strip
that
is produced by a single source located at the
point
.
We are really really done.
Solving for the
inverse of
we
get
.
We can use Mathematica to check our work and graph the
conformal mapping
.
![[Graphics:../Images/SourceSinkModHome_gr_189.gif]](../Images/SourceSinkModHome_gr_189.gif)
The
conformal mapping
.
We are really really really done.
We can let Mathematica draw some other graphs of the streamlines and velocity potentials.
![[Graphics:../Images/SourceSinkModHome_gr_191.gif]](../Images/SourceSinkModHome_gr_191.gif)
A
density plot of some velocity potentials
for
a fluid flow in the infinite strip
that
is produced by a single source located at the
point
.
![[Graphics:../Images/SourceSinkModHome_gr_195.gif]](../Images/SourceSinkModHome_gr_195.gif)
Some
streamlines
for
a fluid flow in the infinite strip
that
is produced by a single source located at the
point
.
![[Graphics:../Images/SourceSinkModHome_gr_199.gif]](../Images/SourceSinkModHome_gr_199.gif)
Some
velocity potentials
for
a fluid flow in the infinite strip
that
is produced by a single source located at the
point
.
This solution is complements of the authors.
(c) 2008 John H. Mathews, Russell W. Howell