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NCU Math, Spring 2014: Complex Analysis Homework Solution 2
Text Book: An Introduction to Complex Analysis
Problem. 7.3
Sol:
(a)
f(z) = u(x, y) + iv(x, y) where we dene u(x, y) = x and v(x, y) = −y2
. It is easy to see that u and v are
smooth. So we have
∂u
∂x = 1, ∂u
∂y = 0,
∂v
∂x = 0, ∂v
∂y = −2y.
Since ∂u
∂y = −∂v
∂x = 0 and ∂u
∂x = ∂v
∂y = 1 i y = −1
2 , we can get that f(z) is dierentiable only at y = −1
2 and is
not dierentiable at z = −1
2 by virtue of Theorem 6.4 and 6.5. Moreover, f (z) = ∂u
∂x (0, −1
2 ) + i∂v
∂x (0, −1
2 ) = 1 for
z = −1
2 by Theorem 6.5.
(b)
f(z) = u(x, y)+iv(x, y) where we dene u(x, y) = x2
and v(x, y) = y2
. It is easy to see that u and v are smooth.
So we have
∂u
∂x = 2x, ∂u
∂y = 0,
∂v
∂x = 0, ∂v
∂y = 2y.
Since ∂u
∂y = −∂v
∂x = 0 and ∂u
∂x = ∂v
∂y = 2x = 2y i x = y, we can get that f(z) is dierentiable only at x = y and is not
dierentiable at z ∈ {x + iy|x = y} by virtue of Theorem 6.4 and 6.5. Moreover, f (z) = ∂u
∂x (x, x) + i∂v
∂x (x, x) = 2x
for z = x + ix and x ∈ R by Theorem 6.5.
(c)
f(z) = u(x, y)+iv(x, y) where we dene u(x, y) = yx and v(x, y) = y2
. It is easy to see that u and v are smooth.
So we have
∂u
∂x = y, ∂u
∂y = x,
∂v
∂x = 0, ∂v
∂y = 2y.
Since ∂u
∂x = ∂v
∂y and ∂u
∂y = −∂v
∂x i x = y = 0, we can get that f(z) is dierentiable only at x = y = 0 and
is not dierentiable at z ∈ {x + iy|x = 0 or y = 0} by virtue of Theorem 6.4 and 6.5. Moreover, f (z) =
∂u
∂x (0, 0) + i∂v
∂x (0, 0) = 0 for z = 0 by Theorem 6.5.
(d)
1
f(z) = u(x, y) + iv(x, y) where we dene u(x, y) = x3
and v(x, y) = (1 − y)3
. It is easy to see that u and v are
smooth. So we have
∂u
∂x = 3x2
, ∂u
∂y = 0,
∂v
∂x = 0, ∂v
∂y = −3(1 − y)2
.
Since ∂u
∂y = −∂v
∂x = 0 and ∂u
∂x = ∂v
∂y = 3x2
= −3(1−y)2
= 0 i x = 0 and y = 1, we can get that f(z) is dierentiable
only at x = 0, y = 1 and is not dierentiable at z ∈ {x + iy|x = 0 or y = 1} by virtue of Theorem 6.4 and 6.5.
Moreover, f (z) = ∂u
∂x (0, 1) + i∂v
∂x (0, 1) = 0 for z = i by Theorem 6.5.
Problem. 7.4
Sol:
(a)
We dene u(x, y) = x3
+ 3xy2
− 3x and v(x, y) = y3
+ 3x2
y − 3y. So f(z) = u + iv. It is easy to see that u and
v are smooth. So we have
∂u
∂x = 3x2
+ 3y2
− 3, ∂u
∂y = 6xy,
∂v
∂x = 6xy, ∂v
∂y = 3y2
+ 3x2
− 3.
Since ∂u
∂x = ∂v
∂y = 3x2
+ 3y2
− 3 and ∂u
∂y = −∂v
∂x i xy = 0 , we can get that f(z) is dierentiable only at xy = 0 and
is not dierentiable at z ∈ {x + iy|xy = 0} by virtue of Theorem 6.4 and 6.5. Thus f is not analytic everywhere.
Moreover, f (z) = ∂u
∂x (x, y) + i∂v
∂x (x, y) = 3x2
− 3 or 3y2
− 3 for z = x or iy by Theorem 6.5.
(b)
From some computations,
f(z) = 6(x2
− y2
− 2xyi) − 2(x − yi) − 4i(x2
+ y2
)
= (6x2
− 6y2
− 2x) + i(−4x2
− 4y2
− 12xy + 2y).
We dene u(x, y) = 6x2
− 6y2
− 2x and v(x, y) = −4x2
− 4y2
− 12xy + 2y. So f(z) = u + iv. It is easy to see that
u and v are smooth. So we have
∂u
∂x = 12x − 2, ∂u
∂y = −12y,
∂v
∂x = −8x − 12y, ∂v
∂y = −8y − 12x + 2.
Then
∂u
∂x
=
∂v
∂y
⇔ 6x + 2y = 1,
∂u
∂y
= −
∂v
∂x
⇔ x + 3y = 0.
This implies that ∂u
∂x = ∂v
∂y and ∂u
∂y = −∂v
∂x i z = 3
16 − 1
16 i. Thus we can get that f(z) is dierentiable only at
z = 3
16 − 1
16 i and is not dierentiable at z ∈ C − { 3
16 − 1
16 i} by virtue of Theorem 6.4 and 6.5. Therefore f is not
analytic everywhere. Moreover, f ( 3
16 − 1
16 i) = ∂u
∂x ( 3
16 , − 1
16 ) + i∂v
∂x ( 3
16 , − 1
16 ) = 1
4 − 3
4 i by Theorem 6.5.
2
(c)
We dene u(x, y) = 3x2
+ 2x − 3y2
− 1 and v(x, y) = 6xy + 2y. So f(z) = u + iv. It is easy to see that u and v
are smooth. So we have
∂u
∂x = 6x + 2, ∂u
∂y = −6y,
∂v
∂x = 6y, ∂v
∂y = 6x + 2.
Since ∂u
∂x = ∂v
∂y = 6x + 2 and ∂u
∂y = −∂v
∂x = −6y for all z ∈ C , we can get that f(z) is dierentiable for all z ∈ C by
virtue of Theorem 6.4 and 6.5. Thus f is analytic in C. Moreover, f (z) = ∂u
∂x (x, y)+i∂v
∂x (x, y) = 6x+2+6yi = 6z+2
for z ∈ C by Theorem 6.5.
(d)
Since f doesn't dene in z = 0, ±2i, we only consider z ∈ C − {0, ±2i}. By virtue of Theorem 6.1, we have
f(z) = 2z2
+6
z(z2+4) is dierentiable for all z ∈ C − {0, ±2i}. f is not analytic in C but is analytic in C − {0, ±2i}. When
we use Theorem 6.1 again, we can get that
f (z) =
4z(z(z2
+ 4)) − (2z2
+ 6)(3z2
+ 4)
(z(z2 + 4))
2
=
−2(z4
+ 5z2
+ 12)
z2(z2 + 4)2
.
for all z ∈ C − {0, ±2i}.
(e)
It is easy to see that
f(z) = ey2
−x2
e−2xyi
= e−(x2
+2xyi−y2
)
= e−z2
.
Since −z2
, ez
are dierentiable in C and Theorem 6.1, we can get that f(z) = e−z2
is dierentiable in C. So f is
analytic in C. Moreover,
f (z) = e−z2
· (−2z)
= −2ze−z2
by virtue of Theorem 6.1 and Example 7.1.
Problem. 7.5
Sol:
3
Since
w(z) = (ay3
+ ix3
) + xy(bx + icy)
= (ay3
+ bx2
y) + i(x3
+ cxy2
),
we dene u(x, y) = ay3
+ bx2
y and v(x, y) = x3
+ cxy2
. It is easy to see that u and v are smooth and
∂u
∂x = 2bxy, ∂u
∂y = 3ay2
+ bx2
,
∂v
∂x = 3x2
+ cy2
, ∂v
∂y = 2cxy.
So w is analytic i
∂u
∂x = ∂v
∂y ,
∂u
∂y = −∂v
∂x ,
⇔
2bxy = 2cxy,
3ay2
+ bx2
= −(3x2
+ cy2
),
from Theorem 6.4 and 6.5. This implies that w is analytic i a = 1 and b = c = −3. Moreover, we have
∂w
∂z
=
∂u
∂x
+ i
∂v
∂x
= −6xy + i(3x2
− 3y2
)
= 3i(x2
+ 2ixy − y2
)
= 3i · z2
by Theorem 6.5.
Problem. 7.8
Sol:
(a)
It is easy to see that
f(z) =
z2
z if z = 0,
0 if z = 0,
=
z3
|z|2 if z = 0,
0 if z = 0,
=
x3
−3xy2
x2+y2 + i−3x2
y+y3
x2+y2 if z = 0,
0 if z = 0,
= u(x, y) + iv(x, y)
4
where we dene
u(x, y) =
0 if x = y = 0
x3
−3xy2
x2+y2 o.w.
and v(x, y) =
0 if x = y = 0
−3x2
y+y3
x2+y2 o.w.
So
∂u
∂x
(0, 0) = lim
h→0
h3
−3h·02
h2+02 − 0
h
= lim
h→0
h
h
= 1,
∂u
∂y
(0, 0) = lim
k→0
03
−3·0·k2
02+k2 − 0
k
= lim
h→0
0
k
= 0,
∂v
∂x
(0, 0) = lim
h→0
−3h2
·0+03
h2+02 − 0
h
= lim
h→0
0
h
= 0,
∂v
∂y
(0, 0) = lim
k→0
−3·02
k+k3
02+k2 − 0
k
= lim
h→0
k
h
= 1.
This implies that ∂u
∂x (0, 0) = ∂v
∂y (0, 0) = 1 and ∂u
∂y (0, 0) = −∂v
∂x (0, 0) = 0. Thus f satises Cauchy-Riemann equations
at z = 0.
(b)
From some computations, we have for z = 0
f(z) − f(0)
z
=
z2
z
z
=
z
z
2
.
It suces to show that limz→0
z
z
2
doesn't exist. It is easy to see that
lim
z=x,x→0
z
z
2
= lim
z=x→0
x
x
2
= 1.
Also
lim
z=x+ix,x→0
z
z
2
= lim
z=x+ix,x→0
x − ix
x + ix
2
= lim
z=x+ix,x→0
1 − i
1 + i
2
=
1 − i
1 + i
2
=
(1 − i)4
4
.
Since 1 = (1−i)4
4 , we can get that limz→0
z
z
2
doesn't exist.
5
Problem. 7.10
Sol:
Since x = r cos θ and y = r sin θ, we can get that
∂x
∂r
= cos θ,
∂x
∂θ
= −r sin θ,
∂y
∂r
= sin θ,
∂y
∂θ
= r cos θ.
By chain rule, we have
∂u
∂r
=
∂u
∂x
·
∂x
∂r
+
∂u
∂y
·
∂y
∂r
=
∂u
∂x
cos θ +
∂u
∂y
sin θ,
∂u
∂θ
=
∂u
∂x
·
∂x
∂θ
+
∂u
∂y
·
∂y
∂θ
= r(−
∂u
∂x
sin θ +
∂u
∂y
cos θ),
∂v
∂r
=
∂v
∂x
·
∂x
∂r
+
∂v
∂y
·
∂y
∂r
=
∂v
∂x
cos θ +
∂v
∂y
sin θ,
∂v
∂θ
=
∂v
∂x
·
∂x
∂θ
+
∂v
∂y
·
∂y
∂θ
= r(−
∂v
∂x
sin θ +
∂v
∂y
cos θ).
So
∂u
∂r
=
∂v
∂y
cos θ −
∂v
∂x
sin θ =
1
r
∂v
∂θ
,
∂u
∂θ
= r(−
∂v
∂y
sin θ −
∂v
∂x
cos θ) = −r
∂v
∂r
.
by virtue of Cauchy-Riemann conditions.
Conversely, we have
∂r
∂x
=
x
r
,
∂r
∂y
=
y
r
,
∂θ
∂x
=
−y
r2
,
∂θ
∂y
=
x
r2
,
6
from r2
= x2
+ y2
and θ = tan−1
(y
x ). Since chain rule, we can get that
∂u
∂x
=
∂u
∂r
·
∂r
∂x
+
∂u
∂θ
·
∂θ
∂x
=
∂u
∂r
x
r
−
∂u
∂θ
y
r2
,
∂u
∂y
=
∂u
∂r
·
∂r
∂y
+
∂u
∂θ
·
∂θ
∂y
=
∂u
∂r
y
r
+
∂u
∂θ
x
r2
,
∂v
∂x
=
∂v
∂r
·
∂r
∂x
+
∂v
∂θ
·
∂θ
∂x
=
∂v
∂r
x
r
−
∂v
∂θ
y
r2
,
∂v
∂y
=
∂v
∂r
·
∂r
∂y
+
∂v
∂θ
·
∂θ
∂y
=
∂v
∂r
y
r
+
∂v
∂θ
x
r2
.
Thus
∂u
∂x
=
∂v
∂θ
x
r2
+
∂v
∂r
y
r
=
∂v
∂y
,
∂u
∂y
=
∂v
∂θ
y
r2
−
∂v
∂r
x
r
= −
∂v
∂x
,
by (7.7).
Moreover,
f (z) =
∂u
∂x
+ i
∂v
∂x
= (
∂u
∂r
x
r
−
∂u
∂θ
y
r2
) + i(
∂v
∂r
x
r
−
∂v
∂θ
y
r2
)
= (
∂u
∂r
x
r
+
∂v
∂r
y
r
) + i(
∂v
∂r
x
r
−
∂u
∂r
y
r
)
= (cos θ − i sin θ)ur + (sin θ + i cos θ)vr
= e−iθ
ur + ie−iθ
vr
= e−iθ
(ur + ivr).
from above, Theorem 6.5, and (7.7).
We dene u(r, θ) =
√
r cos θ
2 and v(r, θ) =
√
r sin θ
2 . Then f(z) =
√
re−iθ/2
=
√
r cos θ
2 + i
√
r sin θ
2 = u(r, θ) +
iv(r, θ). Obviously, u and v are smooth in C − {0}. Also,
∂u
∂r = 1
2
√
r
cos θ
2 , ∂u
∂θ = −
√
r
2 sin θ
2 ,
∂v
∂r = 1
2
√
r
sin θ
2 , ∂v
∂θ =
√
r
2 cos θ
2 ,
for all z ∈ C − {0}. So
∂u
∂r
=
1
2
√
r
cos
θ
2
=
1
r
∂v
∂θ
,
∂u
∂θ
=
−
√
r
2
sin
θ
2
= −r
∂v
∂r
.
7
Thus we can apply Theorem 6.5 to get that f(z) is dierentiable at all z except z = 0. Moreover, we have
f (z) = e−iθ
(ur + ivr)
= e−iθ
(
1
2
√
r
cos
θ
2
+ i
1
2
√
r
sin
θ
2
)
=
1
2
√
r
e−iθ
e
iθ
2
=
1
2
√
r
e− iθ
2 .
Problem. 7.18
Sol:
(a)
Since ∂2
u
∂x2 = e−x
sin y and ∂2
u
∂y2 = −e−x
sin y are both smooth, we have ∂2
u
∂x2 + ∂2
u
∂y2 = 0. So u is harmonic.
Let v(x, y) satises that ∂v
∂y = ∂u
∂x = −e−x
sin y and ∂v
∂x = −∂u
∂y = −e−x
cos y. Then v = e−x
cos y +h(x) for some
real-valued function h by ∂v
∂y = −e−x
sin y. But ∂v
∂x = −e−x
cos y. So h (x) = 0. This implies that v = e−x
cos y + C
for some real constant C. Thus the corresponding analytic function is e−x
sin y + ie−x
cos y + iC for some real
constant C.
(b)
Since ∂2
v
∂x2 = − cos x cosh y and ∂2
u
∂y2 = cos x cosh y are both smooth, we have ∂2
u
∂x2 + ∂2
u
∂y2 = 0. So u is harmonic.
Let u(x, y) satises that ∂u
∂x = ∂v
∂y = cos x sinh y and ∂u
∂y = −∂v
∂x = sin x cosh y. Then u = sin x sinh y + h(y)
for some real-valued function h by ∂u
∂x = cos x sinh y. But ∂u
∂y = sin x cosh y. So h (y) = 0. This implies that u =
sin x sinh y +C for some real constant C. Thus the corresponding analytic function is sin x sinh y +C +i cos x cosh y
for some real constant C.
Problem. 7.24
Sol:
For convenience, we dene C = {(x, y)|u(x, y) = c} and D = {(x, y)|v(x, y) = d}. Let (a, b) ∈ C ∩ D with
f (a+ib) = 0. Since (a, b) ∈ C and f (a+ib) = 0, the tangent vector to C at (a, b) is parallel to (uy(a, b), −ux(a, b)) =
0. Similarly, we have the tangent vector to D at (a, b) is parallel to (vy(a, b), −vx(a, b)) = 0. It suces to show that
(uy(a, b), −ux(a, b)) · (vy(a, b), −vx(a, b)) = 0. Because of Cauchy-Riemann equations, we can get that
(uy(a, b), −ux(a, b)) · (vy(a, b), −vx(a, b))
=uy(a, b)vy(a, b) + ux(a, b) · vx(a, b)
= − vx(a, b)ux(a, b) + ux(a, b) · vx(a, b)
=0.
8
Now, we consider the case f(z) = z2
= (x2
− y2
) + 2xyi. So C = {(x, y)|x2
− y2
= c} and D = {(x, y)|2xy = d}.
Let (a, b) ∈ C ∩ D with f (a + ib) = 0. Thus a2
= b2
and ab = 0. The tangent vector to C at (a, b) is parallel to
(b, a) = 0. Similarly, The tangent vector to D at (a, b) is parallel to (a, −b) = 0. Then C and D are orthogonal by
(b.a) · (a, −b) = 0.
9

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Hw2sol

  • 1. NCU Math, Spring 2014: Complex Analysis Homework Solution 2 Text Book: An Introduction to Complex Analysis Problem. 7.3 Sol: (a) f(z) = u(x, y) + iv(x, y) where we dene u(x, y) = x and v(x, y) = −y2 . It is easy to see that u and v are smooth. So we have ∂u ∂x = 1, ∂u ∂y = 0, ∂v ∂x = 0, ∂v ∂y = −2y. Since ∂u ∂y = −∂v ∂x = 0 and ∂u ∂x = ∂v ∂y = 1 i y = −1 2 , we can get that f(z) is dierentiable only at y = −1 2 and is not dierentiable at z = −1 2 by virtue of Theorem 6.4 and 6.5. Moreover, f (z) = ∂u ∂x (0, −1 2 ) + i∂v ∂x (0, −1 2 ) = 1 for z = −1 2 by Theorem 6.5. (b) f(z) = u(x, y)+iv(x, y) where we dene u(x, y) = x2 and v(x, y) = y2 . It is easy to see that u and v are smooth. So we have ∂u ∂x = 2x, ∂u ∂y = 0, ∂v ∂x = 0, ∂v ∂y = 2y. Since ∂u ∂y = −∂v ∂x = 0 and ∂u ∂x = ∂v ∂y = 2x = 2y i x = y, we can get that f(z) is dierentiable only at x = y and is not dierentiable at z ∈ {x + iy|x = y} by virtue of Theorem 6.4 and 6.5. Moreover, f (z) = ∂u ∂x (x, x) + i∂v ∂x (x, x) = 2x for z = x + ix and x ∈ R by Theorem 6.5. (c) f(z) = u(x, y)+iv(x, y) where we dene u(x, y) = yx and v(x, y) = y2 . It is easy to see that u and v are smooth. So we have ∂u ∂x = y, ∂u ∂y = x, ∂v ∂x = 0, ∂v ∂y = 2y. Since ∂u ∂x = ∂v ∂y and ∂u ∂y = −∂v ∂x i x = y = 0, we can get that f(z) is dierentiable only at x = y = 0 and is not dierentiable at z ∈ {x + iy|x = 0 or y = 0} by virtue of Theorem 6.4 and 6.5. Moreover, f (z) = ∂u ∂x (0, 0) + i∂v ∂x (0, 0) = 0 for z = 0 by Theorem 6.5. (d) 1
  • 2. f(z) = u(x, y) + iv(x, y) where we dene u(x, y) = x3 and v(x, y) = (1 − y)3 . It is easy to see that u and v are smooth. So we have ∂u ∂x = 3x2 , ∂u ∂y = 0, ∂v ∂x = 0, ∂v ∂y = −3(1 − y)2 . Since ∂u ∂y = −∂v ∂x = 0 and ∂u ∂x = ∂v ∂y = 3x2 = −3(1−y)2 = 0 i x = 0 and y = 1, we can get that f(z) is dierentiable only at x = 0, y = 1 and is not dierentiable at z ∈ {x + iy|x = 0 or y = 1} by virtue of Theorem 6.4 and 6.5. Moreover, f (z) = ∂u ∂x (0, 1) + i∂v ∂x (0, 1) = 0 for z = i by Theorem 6.5. Problem. 7.4 Sol: (a) We dene u(x, y) = x3 + 3xy2 − 3x and v(x, y) = y3 + 3x2 y − 3y. So f(z) = u + iv. It is easy to see that u and v are smooth. So we have ∂u ∂x = 3x2 + 3y2 − 3, ∂u ∂y = 6xy, ∂v ∂x = 6xy, ∂v ∂y = 3y2 + 3x2 − 3. Since ∂u ∂x = ∂v ∂y = 3x2 + 3y2 − 3 and ∂u ∂y = −∂v ∂x i xy = 0 , we can get that f(z) is dierentiable only at xy = 0 and is not dierentiable at z ∈ {x + iy|xy = 0} by virtue of Theorem 6.4 and 6.5. Thus f is not analytic everywhere. Moreover, f (z) = ∂u ∂x (x, y) + i∂v ∂x (x, y) = 3x2 − 3 or 3y2 − 3 for z = x or iy by Theorem 6.5. (b) From some computations, f(z) = 6(x2 − y2 − 2xyi) − 2(x − yi) − 4i(x2 + y2 ) = (6x2 − 6y2 − 2x) + i(−4x2 − 4y2 − 12xy + 2y). We dene u(x, y) = 6x2 − 6y2 − 2x and v(x, y) = −4x2 − 4y2 − 12xy + 2y. So f(z) = u + iv. It is easy to see that u and v are smooth. So we have ∂u ∂x = 12x − 2, ∂u ∂y = −12y, ∂v ∂x = −8x − 12y, ∂v ∂y = −8y − 12x + 2. Then ∂u ∂x = ∂v ∂y ⇔ 6x + 2y = 1, ∂u ∂y = − ∂v ∂x ⇔ x + 3y = 0. This implies that ∂u ∂x = ∂v ∂y and ∂u ∂y = −∂v ∂x i z = 3 16 − 1 16 i. Thus we can get that f(z) is dierentiable only at z = 3 16 − 1 16 i and is not dierentiable at z ∈ C − { 3 16 − 1 16 i} by virtue of Theorem 6.4 and 6.5. Therefore f is not analytic everywhere. Moreover, f ( 3 16 − 1 16 i) = ∂u ∂x ( 3 16 , − 1 16 ) + i∂v ∂x ( 3 16 , − 1 16 ) = 1 4 − 3 4 i by Theorem 6.5. 2
  • 3. (c) We dene u(x, y) = 3x2 + 2x − 3y2 − 1 and v(x, y) = 6xy + 2y. So f(z) = u + iv. It is easy to see that u and v are smooth. So we have ∂u ∂x = 6x + 2, ∂u ∂y = −6y, ∂v ∂x = 6y, ∂v ∂y = 6x + 2. Since ∂u ∂x = ∂v ∂y = 6x + 2 and ∂u ∂y = −∂v ∂x = −6y for all z ∈ C , we can get that f(z) is dierentiable for all z ∈ C by virtue of Theorem 6.4 and 6.5. Thus f is analytic in C. Moreover, f (z) = ∂u ∂x (x, y)+i∂v ∂x (x, y) = 6x+2+6yi = 6z+2 for z ∈ C by Theorem 6.5. (d) Since f doesn't dene in z = 0, ±2i, we only consider z ∈ C − {0, ±2i}. By virtue of Theorem 6.1, we have f(z) = 2z2 +6 z(z2+4) is dierentiable for all z ∈ C − {0, ±2i}. f is not analytic in C but is analytic in C − {0, ±2i}. When we use Theorem 6.1 again, we can get that f (z) = 4z(z(z2 + 4)) − (2z2 + 6)(3z2 + 4) (z(z2 + 4)) 2 = −2(z4 + 5z2 + 12) z2(z2 + 4)2 . for all z ∈ C − {0, ±2i}. (e) It is easy to see that f(z) = ey2 −x2 e−2xyi = e−(x2 +2xyi−y2 ) = e−z2 . Since −z2 , ez are dierentiable in C and Theorem 6.1, we can get that f(z) = e−z2 is dierentiable in C. So f is analytic in C. Moreover, f (z) = e−z2 · (−2z) = −2ze−z2 by virtue of Theorem 6.1 and Example 7.1. Problem. 7.5 Sol: 3
  • 4. Since w(z) = (ay3 + ix3 ) + xy(bx + icy) = (ay3 + bx2 y) + i(x3 + cxy2 ), we dene u(x, y) = ay3 + bx2 y and v(x, y) = x3 + cxy2 . It is easy to see that u and v are smooth and ∂u ∂x = 2bxy, ∂u ∂y = 3ay2 + bx2 , ∂v ∂x = 3x2 + cy2 , ∂v ∂y = 2cxy. So w is analytic i ∂u ∂x = ∂v ∂y , ∂u ∂y = −∂v ∂x , ⇔ 2bxy = 2cxy, 3ay2 + bx2 = −(3x2 + cy2 ), from Theorem 6.4 and 6.5. This implies that w is analytic i a = 1 and b = c = −3. Moreover, we have ∂w ∂z = ∂u ∂x + i ∂v ∂x = −6xy + i(3x2 − 3y2 ) = 3i(x2 + 2ixy − y2 ) = 3i · z2 by Theorem 6.5. Problem. 7.8 Sol: (a) It is easy to see that f(z) = z2 z if z = 0, 0 if z = 0, = z3 |z|2 if z = 0, 0 if z = 0, = x3 −3xy2 x2+y2 + i−3x2 y+y3 x2+y2 if z = 0, 0 if z = 0, = u(x, y) + iv(x, y) 4
  • 5. where we dene u(x, y) = 0 if x = y = 0 x3 −3xy2 x2+y2 o.w. and v(x, y) = 0 if x = y = 0 −3x2 y+y3 x2+y2 o.w. So ∂u ∂x (0, 0) = lim h→0 h3 −3h·02 h2+02 − 0 h = lim h→0 h h = 1, ∂u ∂y (0, 0) = lim k→0 03 −3·0·k2 02+k2 − 0 k = lim h→0 0 k = 0, ∂v ∂x (0, 0) = lim h→0 −3h2 ·0+03 h2+02 − 0 h = lim h→0 0 h = 0, ∂v ∂y (0, 0) = lim k→0 −3·02 k+k3 02+k2 − 0 k = lim h→0 k h = 1. This implies that ∂u ∂x (0, 0) = ∂v ∂y (0, 0) = 1 and ∂u ∂y (0, 0) = −∂v ∂x (0, 0) = 0. Thus f satises Cauchy-Riemann equations at z = 0. (b) From some computations, we have for z = 0 f(z) − f(0) z = z2 z z = z z 2 . It suces to show that limz→0 z z 2 doesn't exist. It is easy to see that lim z=x,x→0 z z 2 = lim z=x→0 x x 2 = 1. Also lim z=x+ix,x→0 z z 2 = lim z=x+ix,x→0 x − ix x + ix 2 = lim z=x+ix,x→0 1 − i 1 + i 2 = 1 − i 1 + i 2 = (1 − i)4 4 . Since 1 = (1−i)4 4 , we can get that limz→0 z z 2 doesn't exist. 5
  • 6. Problem. 7.10 Sol: Since x = r cos θ and y = r sin θ, we can get that ∂x ∂r = cos θ, ∂x ∂θ = −r sin θ, ∂y ∂r = sin θ, ∂y ∂θ = r cos θ. By chain rule, we have ∂u ∂r = ∂u ∂x · ∂x ∂r + ∂u ∂y · ∂y ∂r = ∂u ∂x cos θ + ∂u ∂y sin θ, ∂u ∂θ = ∂u ∂x · ∂x ∂θ + ∂u ∂y · ∂y ∂θ = r(− ∂u ∂x sin θ + ∂u ∂y cos θ), ∂v ∂r = ∂v ∂x · ∂x ∂r + ∂v ∂y · ∂y ∂r = ∂v ∂x cos θ + ∂v ∂y sin θ, ∂v ∂θ = ∂v ∂x · ∂x ∂θ + ∂v ∂y · ∂y ∂θ = r(− ∂v ∂x sin θ + ∂v ∂y cos θ). So ∂u ∂r = ∂v ∂y cos θ − ∂v ∂x sin θ = 1 r ∂v ∂θ , ∂u ∂θ = r(− ∂v ∂y sin θ − ∂v ∂x cos θ) = −r ∂v ∂r . by virtue of Cauchy-Riemann conditions. Conversely, we have ∂r ∂x = x r , ∂r ∂y = y r , ∂θ ∂x = −y r2 , ∂θ ∂y = x r2 , 6
  • 7. from r2 = x2 + y2 and θ = tan−1 (y x ). Since chain rule, we can get that ∂u ∂x = ∂u ∂r · ∂r ∂x + ∂u ∂θ · ∂θ ∂x = ∂u ∂r x r − ∂u ∂θ y r2 , ∂u ∂y = ∂u ∂r · ∂r ∂y + ∂u ∂θ · ∂θ ∂y = ∂u ∂r y r + ∂u ∂θ x r2 , ∂v ∂x = ∂v ∂r · ∂r ∂x + ∂v ∂θ · ∂θ ∂x = ∂v ∂r x r − ∂v ∂θ y r2 , ∂v ∂y = ∂v ∂r · ∂r ∂y + ∂v ∂θ · ∂θ ∂y = ∂v ∂r y r + ∂v ∂θ x r2 . Thus ∂u ∂x = ∂v ∂θ x r2 + ∂v ∂r y r = ∂v ∂y , ∂u ∂y = ∂v ∂θ y r2 − ∂v ∂r x r = − ∂v ∂x , by (7.7). Moreover, f (z) = ∂u ∂x + i ∂v ∂x = ( ∂u ∂r x r − ∂u ∂θ y r2 ) + i( ∂v ∂r x r − ∂v ∂θ y r2 ) = ( ∂u ∂r x r + ∂v ∂r y r ) + i( ∂v ∂r x r − ∂u ∂r y r ) = (cos θ − i sin θ)ur + (sin θ + i cos θ)vr = e−iθ ur + ie−iθ vr = e−iθ (ur + ivr). from above, Theorem 6.5, and (7.7). We dene u(r, θ) = √ r cos θ 2 and v(r, θ) = √ r sin θ 2 . Then f(z) = √ re−iθ/2 = √ r cos θ 2 + i √ r sin θ 2 = u(r, θ) + iv(r, θ). Obviously, u and v are smooth in C − {0}. Also, ∂u ∂r = 1 2 √ r cos θ 2 , ∂u ∂θ = − √ r 2 sin θ 2 , ∂v ∂r = 1 2 √ r sin θ 2 , ∂v ∂θ = √ r 2 cos θ 2 , for all z ∈ C − {0}. So ∂u ∂r = 1 2 √ r cos θ 2 = 1 r ∂v ∂θ , ∂u ∂θ = − √ r 2 sin θ 2 = −r ∂v ∂r . 7
  • 8. Thus we can apply Theorem 6.5 to get that f(z) is dierentiable at all z except z = 0. Moreover, we have f (z) = e−iθ (ur + ivr) = e−iθ ( 1 2 √ r cos θ 2 + i 1 2 √ r sin θ 2 ) = 1 2 √ r e−iθ e iθ 2 = 1 2 √ r e− iθ 2 . Problem. 7.18 Sol: (a) Since ∂2 u ∂x2 = e−x sin y and ∂2 u ∂y2 = −e−x sin y are both smooth, we have ∂2 u ∂x2 + ∂2 u ∂y2 = 0. So u is harmonic. Let v(x, y) satises that ∂v ∂y = ∂u ∂x = −e−x sin y and ∂v ∂x = −∂u ∂y = −e−x cos y. Then v = e−x cos y +h(x) for some real-valued function h by ∂v ∂y = −e−x sin y. But ∂v ∂x = −e−x cos y. So h (x) = 0. This implies that v = e−x cos y + C for some real constant C. Thus the corresponding analytic function is e−x sin y + ie−x cos y + iC for some real constant C. (b) Since ∂2 v ∂x2 = − cos x cosh y and ∂2 u ∂y2 = cos x cosh y are both smooth, we have ∂2 u ∂x2 + ∂2 u ∂y2 = 0. So u is harmonic. Let u(x, y) satises that ∂u ∂x = ∂v ∂y = cos x sinh y and ∂u ∂y = −∂v ∂x = sin x cosh y. Then u = sin x sinh y + h(y) for some real-valued function h by ∂u ∂x = cos x sinh y. But ∂u ∂y = sin x cosh y. So h (y) = 0. This implies that u = sin x sinh y +C for some real constant C. Thus the corresponding analytic function is sin x sinh y +C +i cos x cosh y for some real constant C. Problem. 7.24 Sol: For convenience, we dene C = {(x, y)|u(x, y) = c} and D = {(x, y)|v(x, y) = d}. Let (a, b) ∈ C ∩ D with f (a+ib) = 0. Since (a, b) ∈ C and f (a+ib) = 0, the tangent vector to C at (a, b) is parallel to (uy(a, b), −ux(a, b)) = 0. Similarly, we have the tangent vector to D at (a, b) is parallel to (vy(a, b), −vx(a, b)) = 0. It suces to show that (uy(a, b), −ux(a, b)) · (vy(a, b), −vx(a, b)) = 0. Because of Cauchy-Riemann equations, we can get that (uy(a, b), −ux(a, b)) · (vy(a, b), −vx(a, b)) =uy(a, b)vy(a, b) + ux(a, b) · vx(a, b) = − vx(a, b)ux(a, b) + ux(a, b) · vx(a, b) =0. 8
  • 9. Now, we consider the case f(z) = z2 = (x2 − y2 ) + 2xyi. So C = {(x, y)|x2 − y2 = c} and D = {(x, y)|2xy = d}. Let (a, b) ∈ C ∩ D with f (a + ib) = 0. Thus a2 = b2 and ab = 0. The tangent vector to C at (a, b) is parallel to (b, a) = 0. Similarly, The tangent vector to D at (a, b) is parallel to (a, −b) = 0. Then C and D are orthogonal by (b.a) · (a, −b) = 0. 9