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Section 3.2 The Cauchy-Riemann Equations
In Section 3.1 we showed that computing
the derivative of complex functions written in a form such
as
is
a rather simple task. But life isn't always so easy.
Many times we encounter complex functions written
as
. For
example, suppose we had
(3-13)
.
Is there some criterion - perhaps involving the partial derivatives
for u(x,y), and v(x,y) - that
we can use to determine whether f is differentiable, and if so, to
find the value of
?
The answer to this question is yes, thanks to the independent discovery of two important equations by the French mathematician Augustin Louis Cauchy (1789-1857) and the German mathematician Georg Friedrich Bernhard Riemann (1826-1866).
First, let's reconsider the derivative
of
. As
we have stated, the limit given in Equation
(3-1) must not depend on how z
approaches
. We
investigate two such approaches: a horizontal approach and a vertical
approach to
. Recall
from our graphical analysis of
that
the image of a square is a "curvilinear
quadrilateral." For convenience, we let the square have
vertices
,
,
, and
. Then
the image points are
,
,
, and
,
as shown in Figure 3.1.
![[Graphics:Images/CauchyRiemannMod_gr_17.gif]](cauchyriemann/CauchyRiemannMod/Images/CauchyRiemannMod_gr_17.gif)
Figure
3.1 The image of a small square with
vertex
, under
the mapping
.
We know that f is differentiable, so the
limit of the difference quotient
exists
no matter how we approach
.
Thus we can approximate
by
using a horizontal increment in z:
And, we can approximate
by
using a vertical increment in z:
![[Graphics:Images/CauchyRiemannMod_gr_46.gif]](cauchyriemann/CauchyRiemannMod/Images/CauchyRiemannMod_gr_46.gif)
Comparing these two results we see that
which leads us to speculate that
.
These computations lead to the idea of
taking limits along the horizontal and vertical directions. When we
do so, we get
and
We now generalize this idea by taking limits of an arbitrary differentiable complex function and obtain an important result.
Explore Numerical Computations
Theorem 3.3 (Cauchy-Riemann
Equations). Suppose
that
is differentiable at the point
. Then
the partial derivatives
of u and v exist at the
point
,
and
(3-14)
, and
also
(3-15)
.
Equating the real and imaginary parts of Equations
(3-14) and
(3-15) gives
(3-16)
and
.
Derivation of the Cauchy-Riemann Equations with Mathematica.
Exploration for the Cauchy-Riemann Equations.
Note some of the important implications of
this theorem.
(i). If f
is differentiable at
,
then the Cauchy-Riemann Equations (3-16)
will be satisfied at
,
and we can use either either Equation
(3-14) or
(3-15) to evaluate
.
(ii). Taking the
contrapositive, if Equations (3-16) are
not satisfied at
,
then we know automatically that f(z)
is not differentiable at
.
(iii). Even if
Equations (3-16) are satisfied at
,
we cannot necessarily conclude that f is differentiable at
.
We now illustrate each of these points.
Example 3.4. We
know that
is
differentiable and that
. We
also have
.
It is easy to verify that Equations
(3-16) are indeed satisfied:
and
.
Using Equations (3-14) and
(3-15), respectively, to compute
gives
, and
,
as expected.
Example 3.5. Show
that
is
nowhere differentiable.
Solution. We have
, where
and
. Thus,
for any point
,
and
. The
Cauchy-Riemann equations are not
satisfied at any point
,
so we conclude that
is
nowhere differentiable.
Example 3.6. Show
that the function defined by
is not differentiable at the point
even though the Cauchy-Riemann equations are satisfied at
.
Solution. We must use limits to calculate the partial
derivatives at (0,0).
,
,
,
.
Thus we have shown that
,
,
,
![]()
Hence the Cauchy-Riemann equations hold at the point (0,0).
We now show that f
is not differentiable at
. Letting
z approach 0
along the x axis gives
But if we let z approach 0
along the line
given
by the parametric equations
, then
The two limits are distinct, so f is
not differentiable at the origin.
Example 3.6 reiterates that the mere
satisfaction of the Cauchy-Riemann equations is not sufficient to
guarantee the differentiability of a function. The
following theorem, however, gives conditions that guarantee the
differentiability of f at
,
so that which we can use Equation (3-14)
or (3-15) to
compute
. They
are referred to as the Cauchy-Riemann conditions for
differentiability.
Theorem 3.4 (Cauchy-Riemann conditions
for
differentiability). Let
be
a continuous function that is defined in some neighborhood of the
point
.
If all the partial derivatives
are continuous at the point
and if the Cauchy-Riemann equations
and
hold at
,
then f(z) is differentiable
at
and the derivative
can
be computed with either formula (3-14)
or (3-15), i.e.
, or
.
Example 3.7. At the
beginning of this section (Equation
(3-13)) we defined the
function
.
Show that this function is differentiable for all z,
and find its derivative.
Solution. We compute
and
, so
the Cauchy-Riemann Equations (3-16), are
satisfied. Moreover,
are
continuous everywhere. By Theorem 3.4, f
is differentiable everywhere, and, from Equation
(3-14),
Alternatively, from Equation (3-15),
This result isn't surprising because
and
so the function f is really our old
friend
.
Extra Example
1. Given
.
Show that this function is differentiable for all z,
and find its derivative.
Example 3.8. Show
that the function
is
differentiable for all
and find its derivative.
Solution. We first write
and
then compute the partial derivatives.
![]()
, and
.
We note that
are
continuous functions and that the Cauchy-Riemann equations hold for
all values of
. Hence,
using Equation (3-14), we
write
.
Aside. Can you guess
the "complex" form of
?
Extra Example
2. Show that the function
is differentiable for all
and
find its derivative.
The Cauchy-Riemann conditions are particularly useful in determining the set of points for which a function f is differentiable.
Example 3.9. Show
that the function
is
differentiable at points that lie on the x
and y axes but analytic nowhere.
Solution. Recall (Definition 3.1) that when we say a
function is analytic at a point
we mean that the function is differentiable not only at
,
but also at every point in some neighborhood of
. With
this in mind, we proceed to determine where the Cauchy-Riemann
equations are satisfied. We write
and
and
compute the partial derivatives:
,
, and
,
.
Here
are
continuous, and
holds
for all
. But
iff
, which
is equivalent to
. The
Cauchy-Riemann equations hold only when
, and
according to Theorem 3.4, f is
differentiable only at points that lie on the coordinate
axes. But this means that f
is nowhere analytic because any
-neighborhood
about a point on either axis contains points that are not on those
axes.
When polar coordinates
are used to locate points in the plane, we use Expression
(2-2) for a complex function for
convenience; that is,
where
are
real functions of the real variables
. The
polar form of the Cauchy-Riemann equations and a formula for finding
f'(z) in terms of the partial derivatives of U(r,) and V(r,) are
given in Theorem 3.5, which we ask you to prove in Exercise
10. This theorem makes use of the validity of the
Cauchy-Riemann equations for the functions u and v, so the relation
between them and the functions
-
namely,
and
-
is important.
Theorem 3.5 (Polar Form of the
Cauchy-Riemann
equations). Let
be
a continuous function that is defined in some neighborhood of the
point
. If
all the partial derivatives
are
continuous at the point
and if the polar form of the Cauchy-Riemann equations,
(3-22)
and
,
holds, then
is differentiable at
,
and we can compute the derivative
by using either
(3-23)
, or
(3-24) ![]()
.
Example 3.10. Show
that, if f is is the principal square root function given
by
where the domain is restricted to be
, then
the derivative is given by
for every point in the domain
.
Solution. We write
, and
.
Thus,
, and
.
Since
are
continuous at every point in the domain (note the strict inequality
in
),
we use Theorem 3.5 and Equation (3-23)
to get
![[Graphics:Images/CauchyRiemannMod_gr_279.gif]](cauchyriemann/CauchyRiemannMod/Images/CauchyRiemannMod_gr_279.gif)
Note that
is discontinuous on the negative real axis and is undefined at the
origin. Using the terminology of Section 2.4, the negative
real axis is a branch cut, and the origin is a branch point for this
function.
Two important consequences of the Cauchy-Riemann equations close this section.
Theorem
3.6. Let
be
an analytic function on the domain D. Suppose
for all
that
, where
K is a constant. Then
f is constant on D.
Theorem
3.7. Let
be
an analytic function on the domain D. If
for
all
, then
f is constant on D.
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