Revisited Example
3.4. We know that
is
differentiable and that
.
Furthermore, the polar coordinate form for
is
.
Use the polar coordinate form of the Cauchy-Riemann equations and
prove that
is
differentiable for all
.
Explore Revisited Solution 3.4.
Solution. It is
easy to verify that polar form of the Cauchy-Riemann
equations (3-22) are indeed
satisfied for all
.
, and
.
Moreover, the partial derivatives
are
continuous for all
.
By Theorem 3.5,
, is
differentiable for all
.
Therefore, using Equation (3-23) and
(3-24), we
have
and
![[Graphics:../Images/CauchyRiemannMod_gr_1069.gif]](../Images/CauchyRiemannMod_gr_1069.gif)
as expected.
You might wonder why we required
.
This happens because equations (3-22) do
not hold at
.
Of course, for the function
, it
is well known that
.
We are done.
Aside. Both
and
can assist us in finding the partial derivatives.
Aside. The Mathematica solution uses the commands.
Mathematica shows that the polar form of the Cauchy-Riemann
equations (3-22) are
satisfied for all
,
, and
.
Aside. The Maple commands are similar.
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Maple shows that the polar form of the Cauchy-Riemann
equations (3-22) are
satisfied for all
,
, and
.
The Cauchy-Riemann
equations hold all points
in
the complex plane,
therefore
is
an analytic function, for all
.
Verify that the derivative can be calculated with either of the
formulas:
(3-23)
, or
(3-24)
.
Aside. The Mathematica solution uses the commands.
Aside. The Maple commands are similar.
>
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>
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>
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>
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>
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Therefore, both Mathematica and Maple have shown that
if
,
then the derivative is
,
as expected.
We are really done.
Aside. Figure R.3.4
a, shows the graphs of
and
.
The partial derivatives of
are
and
,
and the partial derivatives of
are
and
.
They satisfy the
Cauchy-Riemann
equations (3-16) because they
are the real and imaginary parts of an analytic
function.
At the point
, we
have
and
, and
these partial
derivatives appear along the edges of the surfaces
for
at
the points
and
, respectively. Similarly, at
the point
, we
have
and
and
these partial derivatives appear along the edges of the surfaces
for
at
the points
and
, respectively.
.
.
Figure
R.3.4 a
, and
, and
.
.
Figure
R.3.4 b
, and
, and
.
.
Remark.
It is difficult to visualize
because
this partial derivative
is
taken
with respect to changes in the polar angle
, and
so it cannot be visualized as an "ordinary slope."
Figure
R.3.4 c
For
the function
we
see that
, and
.
Figure
R.3.4
We are really really done.
Aside. We can let Mathematica check out the calculations given above.
Remark. In this
book the use of computers is optional.
Hopefully this text will promote their use and understanding.
This solution is complements of the authors.
This material is coordinated with our book Complex Analysis for Mathematics and Engineering.
(c) 2011 John H. Mathews, Russell W. Howell