Exercise
6. The complex
potential
determines
an electrostatic field that is referred to as a dipole.
6 (b). Show
that the lines of flux of a dipole are circles that pass through the
origin,
as shown in Figure
11.104.
Figure 11.104.
Solution 6 (b) .
Consider Example 11.30 where a source is located
at
and sink is located at
. The
streamlines were shown to be circles that satisfy the
equation
,
If the strength is changed to
. The
velocity potential and stream function are
, and
,
respectively. Solving for the
streamline
, we
start with
Then get the equation
which can be written as
.
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![]()
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which is the equation of a circle with center
at
that
passes through the points
.
If we let
in the last equation, and observe that
and
then
we obtain
which is the equation of a circle with center
at
and
radius
.
We are done.
Aside. We can let Mathematica double check our work.
![[Graphics:../Images/SourceSinkModHome_gr_384.gif]](../Images/SourceSinkModHome_gr_384.gif)
Graphs
of some circles
.
We are really done.
Aside. We can let Mathematica graph some of the equipotential curves and flux lines.
The velocity potential
is
The stream function
is
![[Graphics:../Images/SourceSinkModHome_gr_395.gif]](../Images/SourceSinkModHome_gr_395.gif)
Some
equipotential curves
.
![[Graphics:../Images/SourceSinkModHome_gr_397.gif]](../Images/SourceSinkModHome_gr_397.gif)
A
density plot for
the equipotentials
.
![[Graphics:../Images/SourceSinkModHome_gr_399.gif]](../Images/SourceSinkModHome_gr_399.gif)
Some
flux lines
.
This solution is complements of the authors.
(c) 2008 John H. Mathews, Russell W. Howell