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37
CHAPTER THREE Basic Transcendental Functions of Complex Variables
§3-1 The Exponential Function
1. If iyxz += , the complex exponential ez is given by
(cos sin )
z x iy x iy
xe e e e
e y i y
+= =
= +
上述之定義中,使用到 Euler's Formula: θθθ sincos ie i += , R∈θ
在此須先證明 e i y 是否亦符合 Euler's Formula,使得 yiyeiy sincos += ------ (1)
所以,底下我們將先舉出在實變函數中 Exponential 函數的性質,而後再證明之。 * 在實變微積分中,若定義
axexf =)( 則其有下列之性質
i) 2121 xxxx eee =+ ii) 1)0( =f
iii) )()( xafaexf ax ==′ Using the above mentioned properties, we want to prove that the Equation (1) holds for any real number y.
yiyeiy sincos +=
Let iyeyf =)( )()( yhiyg +=
where both g(y ) and h (y) are real functions and satisfy the properties mentioned above, i.e., )()( yfiyf =′
1)0( =f Thus, when
)()()( yhiygyf ′+′=′ ( )
[ ( ) ( )]( ) ( )
i f yi g y i h yi g y h y
== += −
We know that when the equality holds any y, there must have Real part = Real part and Im = Im
So, we obtain the following equations: ( ) ( ) (2)( ) ( ) (3)
g y h yh y g y′ = − − − − − − −⎧
⎨ ′ = − − − − − −⎩
Differentiating equation (2) with respect to y, gives )()()( ygyhyg −=′−=′′
⇒ 0)()( =+′′ ygyg ⇒ )4(sincos)( 21 −−−−−−+= ycycyg From equation (2), we know that
1 2
( ) ( )sin cos (5)
h y g yc y c y
′= −= − − − − − − −
And then we use the property 1)0( =f : ⇒ 1)0()0()0( =+= higf This implies that
38
(0) 1(0) 0
gh
=⎧⎨ =⎩
⇒ 12
10
cc=⎧
⎨ =⎩
⇒ ( ) cos( ) sin
g y yh y y
=⎧⎨ =⎩
⇒ )()()( yhiygyfeiy +== yiy sincos +=
♣ Some basic properties of the exponential function are discussed as below.
2. If, 111 yixz += and 222 yixz += are two complex numbers, then 221 zzzz zeee +=
)()( 2121121 yixyixzz eeee ++=
[ ] [ ][ ][ ]
1 2
1 2
1 2
1 2 1 2
1 2 1 2
1 2
1 1 2 2
1 2 1 2 1 2 2 1
1 2 1 2( ) ( )
( ) ( )
cos sin cos sin
(cos cos sin sin ) (sin cos sin cos )
cos( ) sin( )
x x
x x
x x
x x i y y
x x i y y
z z
e y i y e y i y
e y y y y i y y y y
e y y i y y
e eee
+
+
+ +
+ + +
+
= + ⋅ +
= − + +
= + + +
=
=
=
3. If ]sin[cos)( yiyezf x += is analytic in the entire complex plane, then zezf =′ )(
* 為了證明上述結果,我們必須先了解下列的性質。 If ),(),()( yxviyxuzf += ,且其
yv
xu
∂∂
=∂∂
, yu
xv
∂∂
−=∂∂
而且 xu∂∂
,yv
∂
∂,
xv
∂∂
,yu
∂∂ 均為連續 ⇔ )(zf is analytic
Since ]sin[cos)( yiyezf x +=
⇒ yeyxu x cos),( =
yeyxv x sin),( = It is easily seen that
yexu x cos=∂∂
yeyv x cos=
∂∂
⇒ yv
xu
∂∂
=∂∂ -------- (1)
And yexv x sin=
∂∂
, yeyu x sin−=
∂∂
⇒ yu
xv
∂∂
−=∂∂ -------- (2)
Furthermore, xu∂∂
,yu
∂∂
,xv
∂∂ and
yv
∂
∂ are continuous everywhere in the xy-plane, and
satisfy the Cauchy-Riemann conditions for all finite values of z everywhere in this plane. ⇒ )(zf is analytic for all z and is therefore an entire function.
39
The derivative ( )f z′ is easily found as
xvi
xuzf
∂∂
+∂∂
=′ )(
cos sin[cos sin ]
x x
x
z
e y i e ye y i ye
= +
= +
=
♣ Chain Rule: If ( )g z is also an analytic function, we have ( ) ( )( ) ( ) ( )g z g zd e e g zdz
′= .
4. zx ee 和 之比較如下表所示:
xe ze
1) 0>xe ze 沒有大小
2) 0≠xe )1(0 0 ==⋅≠ − eeee zzz
3) xexf =)( is one-to-one function *** zezf =)( is a periodic function.
Its period is 2πi *** ]sin[cos yiyee xz +=
( 2 )
2
2
[cos( 2 ) sin( 2 )]
,
x
x i y n
x i y n i
z n i
e y n i y ne eee n I
π
π
π
π π+
+ +
+
= + + +
=
=
= ∈
iT π2= (imaginary period),故知 ze 為週期函數。 ♣ MATLAB Commands for plotting ze , ( )Re ze , and ( )Im ze :
% Magnitude of exp(z) x=[-1:0.05:1]; y=[-6:0.05:6]; [X,Y]=meshgrid(x,y); Z=X+i*Y; w=exp(Z); wm=abs(w); meshz(X,Y,wm);hold on title('Magnitude of exp(z)') % Real part of exp(z) x=[-1:0.05:1]; y=[-6:0.05:6]; [X,Y]=meshgrid(x,y); Z=X+i*Y; w=exp(Z); wm=real(w); meshz(X,Y,wm);hold on surf(X,Y,wm) title('Real Part of exp(z)') % Imaginary part of exp(z) x=[-1:0.05:1]; y=[-6:0.05:6]; [X,Y]=meshgrid(x,y); Z=X+i*Y;
40
w=exp(Z); wm=imag(w); meshz(X,Y,wm);hold on title('Imaginary Part of exp(z)')
41
5. For iyxz += , we have
1) 0≠ze
2) 1=yie and xz ee = (The magnitude of ze is determined by the real part of z.)
3) If ikze z π21 =⇔= , k = constant.
4) If ikzzee zz π22121 =−⇔= where k is an integer.
1) From 0 1z ze e e−⋅ = = , since the product is never zero, neither factor can be zero. Therefore, Cze z ∈∀≠ 0 .
2) 1sincos 22 =+= yye yi
Since ]sin[cos yiyee xz += ,
then yiyee xz sincos +=
1xx
ee
= ⋅
=
3) Let 1]sin[cos =+= yiyee xz
thus cos 1
sin 0
x
x
e y
e y
⎧ =⎪⎨
=⎪⎩
Since Rxe x ∈∀≠ 0 , we see that 0sin =y . Hence Inny ∈= ,π
Because ( )不合11cos0 −=⇒> ye x ⇒ Ikky ∈= ,2 π Thus, we seek that kn 2= . If we take 01 =⇒= xe x 因此, iyxz +=
02
ink i
ππ
= += ←此為必要條件
現在,尚須證明其充分條件亦成立,故 Suppose that ikz π2= , where k I∈ . Then, we obtain that
2
cos2 sin 21
z k ie ek i k
π
π π== +=
4) Since 21 zz ee = 121 =⇔ −zze Hence from the property 3), we have ikzz π221 =− , where k I∈ . The theorem is thus established. Since Cze z ∈∀≠ 0 , and 1=− zzee We have that
zz
ee 1=−
6. Let us show that z ze e=
z x i y x i ye e e+ −= =
(cos sin )
x i y
xe ee y i y
−=
= −
42
(cos sin ) (cos sin )z x xe e y i y e y i y= + = −
Thus, we see that z ze e= ♣ Some useful identities:
1) 0 / 2 3 / 2 / 21, , 1,i i i i ie e i e e i eπ π π π−= = = − = − =
2) 1 0ie π + =
3) DeMoivre’s Theorem: (cos sin ) cos sinni n i nθ θ θ θ+ = + or ( )ni ine eθ θ= . 4) Complex functions of a real variable: ( ) ( ) ( )f t u t iv t= + , where ( )u t and ( )v t are real.
⇒ ( ) ( ) ( )f t u t iv t′ ′ ′= +
Example 1 Find 7 2
7
cos(2 )td e t
dt
⎡ ⎤⎣ ⎦ .
1. Direct differentiation ⇒ laborious ! 2. Note that ( )2 2(1 )cos(2 ) Ret i te t e += .
Let 2(1 )( ) i tf t e += . Then, we have (7) 7 7 2(1 ) 7 2(1 )( ) 2 (1 ) 2 ( 8 )(1 )i t i tf t i e i i e+ += + = × − +
Thus,
( ) ( ){ }7 2
7 2(1 ) 10 27
10 2
cos(2 )Re 2 ( 8 )(1 ) Re 2 sin 2 cos2 sin 2 cos2
2 (sin 2 cos2 )
ti t t
t
d e ti i e e t t i t t
dte t t
+⎡ ⎤⎣ ⎦ ⎡ ⎤= × − + = + + −⎡ ⎤⎣ ⎦⎣ ⎦
= +
H.W. 1 (a) Suppose we want the n-th derivative, with respect to t, of ( )2( ) / 1f t t t= + . Notice that
1( ) Ref tt i
⎛ ⎞= ⎜ ⎟−⎝ ⎠ and that the n-th derivative of the function in the brackets is exactly taken. Using
the method of Example 1, as well as the binomial theorem (which perhaps should be reviewed), show that
( 1) / 2 1 2( )
2 10
( 1) !( 1)! ( 1)( )(2 )!( 1 2 )!( 1)
n k n kn
nk
n n tf tk n kt
+ + −
+=
− + −=
+ −+∑ , for n odd,
1 2/ 2( )
2 10
!( 1)! ( 1)( )(2 )!( 1 2 )!( 1)
k n knn
nk
n n tf tk n kt
+ −
+=
+ −=
+ −+∑ , for n even.
(b) Using the method of part (a), find similar expressions for the nth derivative of ( )2( ) 1/ 1f t t= + . Note that this function is identical to ( )Im 1/( )t i− .
【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3.1, Problem 24, Pearson Education, Inc., 2005.】 H.W. 2 The absolute magnitude of the expression
12 ( 1)
01
Ni i i N in
nP e e e eψ ψ ψ ψ
−−
== + + + + = ∑
is of interest in many problems involving radiation from N identical physical elements (e.g., antennas, loudspeakers). Here ψ is a real quantity that depends on the separation of the elements and the position of an observer of the radiation. P can tell us the strength of the radiation observed. (a) Using the formula for the sum of a finite geometric series (see H.W. 8 in page 6, lecture note of
ch_01), show that
43
sin / 2( )sin / 2
NP ψψψ
=
(b) Find 0lim ( )Pψ ψ→ .
(c) Use a calculator or a simple computer program to plot ( )P ψ for 0 2ψ π≤ ≤ when N = 3. 【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3.1, Problem 25, Pearson Education, Inc., 2005.】
(a) Let iz e ψ= , then 1 1
2 1 1 111 1
N NN z zP z z z
z z
− +− − −= + + + + = =
− −.
⇒ ( ) ( )( ) ( )
/ 2 / 2 / 2
/ 2 / 2 / 2
/ 2
/ 2
/ 2
/ 2
1 1( )1 1
cos( / 2) sin( / 2) cos( / 2) sin( / 2)cos( / 2) sin( / 2) cos( / 2) sin( / 2)
2 sin( / 2)2 sin(
iN iN iN iN iN
i i i i i
iN
i
iN
i
e e e e ePe e e e e
N i N N i Nei ie
e i Nie
ψ ψ ψ ψ ψ
ψ ψ ψ ψ ψ
ψ
ψ
ψ
ψ
ψ
ψ ψ ψ ψψ ψ ψ ψ
ψψ
−
−
⎡ ⎤− − −= = = ⎢ ⎥
− − −⎢ ⎥⎣ ⎦⎡ ⎤+ − −
= ⎢ ⎥+ − +⎣ ⎦
=/ 2)
Thus, we have / 2
/ 22 sin( / 2) sin( / 2)( )2 sin( / 2) sin( / 2)
iN
ie i N NP
ie
ψ
ψψ ψψψ ψ
= = ------------ Q.E.D.
(b) Consider
0
sin( / 2) / 2 cos( / 2)limsin( / 2) 1/ 2 cos( / 2)
N N N Nψ
ψ ψψ ψ→
= =
Thus, we have
0lim ( )P Nψ
ψ→
=
(c) MATLAB commands: % H.W.1 part (c) N=3; phi=[0:0.1:2*pi]; y=sin(N*phi)./sin(phi); Y=abs(y); plot(phi,Y)
0 1 2 3 4 5 6 70
0.5
1
1.5
2
2.5
3
44
§3-2 The Trigonometric Function
1. Since xixe xi sincos +=
xixe xi sincos −=− then we see that
sin2
cos2
i x i x
i x i x
e exi
e ex
−
−
⎧ −=⎪⎪
⎨+⎪ =⎪⎩
⇒ 屬於實數
and sinh
2
cosh2
x x
x x
e ex
e ex
−
−
⎧ −=⎪⎪
⎨+⎪ =⎪⎩
⇒ 屬於實數
1) Given any complex number z , we define
sin2
cos2
i z i z
i z i z
e ezi
e ez
−
−
−=
+=
2) The functions zsin and zcos are analytic for all values of z. Moreover,
sin2
2cos
i z i z
i z i z
d i e i ezdz i
e e
z
−
−
+=
+=
=
cos2
( )2
sin
i z i z
i z i z
d i e i ezdz
e ei
z
−
−
−=
− −=
= −
2. 底下是一些三角函數和 Hyperbolic Function 的性質:
1) 1sincos 22 =+ xx , 1sinhcosh 22 =− xx
2) cxdxx
+=−
−∫ 12 sin11 ,
cxdxx
+=+
−∫ 12 sinh11
3) ℒ 2 2{sin }t sωωω
=+
,
ℒ 2 2{sinh }t sωωω
=−
4) ℒ 2 2{cos }st
sω
ω=
+,
ℒ 2 2{cosh }st
sω
ω=
−
3. If iyxz += , then
1) yxiyxz sinhcoscoshsinsin += 2) yxiyxz sinhsincoshcoscos −=
45
1) ieez
zizi
2sin
−−=
( ) ( )
2
2[cos sin ] [cos sin ]
2cos ( ) sin ( )
2
cos sin2 2
sin cosh cos sinh
i x i y i x i y
y i x y i x
y y
y y y y
y y y y
e ei
e ei
e x i x e x i xi
x e e i x e ei
e e e ei x
x y i x y
+ − +
− + − −
− −
− −
−=
−=
+ − −=
− + +=
− += +
= +
2) 同理可證。在此另舉一證法: 由 Taylor's Series,知
3 5 2 1
03 5 2 1
0
( 1)sin3! 5! (2 1)!
sinh3! 5! (2 1)!
n n
nn
n
z z zz zn
z z zz zn
+∞
=+∞
=
⎧ −= − + − + =⎪
+⎪⎨⎪ = + + + =⎪ +⎩
∑
∑
比較上列二式可得 sinh sinsin sinh
iz i ziz i z
=⎧⎨ =⎩
同樣地,由下二式 2 4 2
02 4 2
0
( 1)cos 12! 4! (2 )!
cosh2! 4! (2 )!
n n
nn
n
z z zzn
z z zz zn
∞
=∞
=
⎧ −= − + − + =⎪
⎪⎨⎪ = + + + =⎪⎩
∑
∑
比較可得 cosh coscos cosh
iz ziz z
=⎧⎨ =⎩
由上述結果我們便可證明 2) 之結果: Since )cos(cos yixz +=
cos cos sin sincos cosh sin sinh
x i y x i yx y i x y
= −= −
4. 1sin ≤x ,在實變函數中成立;但在複變函數中, 1sin ≤z ,不一定成立。
Since yxiyxz sinhcoscoshsinsin += ,
thus yxyxz 22222 sinhcoscoshsinsin +=
yx
yxyx22
2222
sinhsin
sinh)sin1()sinh1(sin
+=
−++=
If we take 2π
=x , 1=y ,then obtain
1sin 2 =x , 0sinh 2 >y
⇒ 1sin 2 >z ⇒ 1sin ≤z ,不一定成立
5. If Innzz ∈=⇒= ,π0sin .
46
From 02
sin =−=−
ieez
zizi
⇒ 12 =⇒= − zizzi eee i
⇒ 1)22( =+ yixie ⇒ 1]2sin2[cos2 =+− xixe y ⇒ 02sin =x Since 02 >ye ,when 02sin =x , we know 12cos ±=x But in this case we must take 12cos +=x (如此 02 >ye 才能配合題意之要求). ⇒ πnx 22 = ⇒ πnx = 而因 12cos =x ,故取 12 =− ye 故知 0=y ⇒ iyxz +=
0,
n in n Iππ
= += ∈
6. If 1cos 02
z z n n Iπ⎛ ⎞= ⇒ = + ∈⎜ ⎟⎝ ⎠
, .
From 02
cos =+=− zizi eez , we see that zzi ee i−= .
⇒ 12 −=zie ⇒ 1]2sin2[cos2 −=+− xixe y Then, we have sin 2 0x = + .
Since 02 >− ye ,when 02sin =x , we know that 12cos ±=x . But in this case we must take 12cos −=x (such that they satisfy 02 >− ye , 12cos2 −=− xe y ). ⇒ π)12(2 += nx
⇒ 12
x n π⎛ ⎞= +⎜ ⎟⎝ ⎠
又因 12cos −=x ,故取 12 =− ye 。 ⇒ 02 =− y ⇒ 0=y 故 iyxz +=
1 0212
n i
n
π
π
⎛ ⎞= + +⎜ ⎟⎝ ⎠⎛ ⎞= +⎜ ⎟⎝ ⎠
7. Given the complex number z , we define
1) sin 1tancos 2
zz z nz
π⎛ ⎞= ≠ +⎜ ⎟⎝ ⎠
,
2) coscotsin
zz z nz
π= ≠,
3) 1seccos 2
z z nz
π π= ≠ +,
4) 1cscsin
z z nz
π= ≠,
where In∈ in all above cases. 5) ztan and zcot both have a fundamental period of π. 6) zsec and zcsc both have a fundamental period of 2π.
8. ztan , zcot , zsec and zcsc are analytic functions of z except for the above mentioned
y
x 0 π 2π 3π -3π -2π -π
y
x0
π2
3− π
2
1− π
2
1π
2
3 π
2
5
47
limiting values. We can define that
1) ππ nzzzdzd
+≠=2
sec)(tan 2 ,
2) πnzzzdzd
≠−= ,2csc)(cot
3) ππ nzzzzdzd
+≠=2
tansec)(sec ,
4) πnzzzzdzd
≠−= ,cotcsc)(csc
where in all cases , In∈ .
9. If iyxz += , then
1) sin sinz z= , cos cosz z=
sin sin( ) sin( )z x i y x i y= + = −
yxiyxyixyix
sinhcoscoshsinsincoscossin
−=−=
⇒ sin sinz z= yxiyxz sinhcoscoshsinsin +=
sin sin cosh cos sinhz x y i x y= −
同理 cos cosz z=
2) yxz 222 sinhsin|sin| +=
3) yxz 222 sinhcos|cos| +=
4) 1cossin 22 =+ zz 5) 212121 sincoscossin)sin( zzzzzz ±=± 6) 212121 sinsincoscos)cos( zzzzzz ∓=±
7) sin cos2
z zπ⎛ ⎞− =⎜ ⎟⎝ ⎠
8) zzz cossin22sin = 9) zzz 22 sincos2cos −=
以上各式之證明均非常簡單,留待給讀者證明。
10. Let us show that
21
2121 tantan1
tantan)tan(zzzzzz
−+
=+
where 1 212
z z n π⎛ ⎞+ ≠ +⎜ ⎟⎝ ⎠
, In∈ .
)cos()sin()tan(
21
2121 zz
zzzz++
=+
21
21
2121
2121
tantan1tantan
sinsincoscossincoscossin
zzzz
zzzzzzzz
−+
=
−+
=
♣ MATLAB Commands for plotting cos( )z :
% Magnitude of cos(z) x=[-6:0.05:6]; y=[-1:0.05:1]; [X,Y]=meshgrid(x,y); Z=X+i*Y; w=cos(Z);
48
wm=abs(w); meshz(X,Y,wm);hold on title('Magnitude of cos(z)')
H.W.1 Let ( ) sin(1/ )f z z= .
(a) Express this function in the form ( , ) ( , )u x y iv x y+ . Where in the complex plane is this function analytic?
(b) What is the derivative of ( )f z ? Where in the complex plane ( )f z′ is analytic? 【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3.2, Problem 22, Pearson Education, Inc., 2005.】 (a) Since ( ) sin(1/ )f z z= , where 1/ z is analytic except for z = 0. But, sinz is analytic for all z. Therefore,
we have sin(1/ )z is analytic for all 0z ≠ . Since z x iy= + , we have
2 2 2 2 2 2
2 2 2 2 2 2 2 2
sin(1/ ) sin sin
sin cosh cos sinh
x iy x yz ix y x y x y
x y x yix y x y x y x y
⎛ ⎞ ⎛ ⎞−= = −⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟+ + +⎝ ⎠ ⎝ ⎠
⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞= −⎜ ⎟ ⎜ ⎟ ⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟ ⎜ ⎟ ⎜ ⎟+ + + +⎝ ⎠ ⎝ ⎠ ⎝ ⎠ ⎝ ⎠
where
2 2 2 2( , ) sin coshx yu x y
x y x y
⎛ ⎞ ⎛ ⎞= ⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟+ +⎝ ⎠ ⎝ ⎠
and 2 2 2 2( , ) cos sinhx yv x y
x y x y
⎛ ⎞ ⎛ ⎞= ⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟+ +⎝ ⎠ ⎝ ⎠
(b) 21sin(1/ ) cos(1/ )d z z
dz z⎛ ⎞= −⎜ ⎟⎝ ⎠
----------- analytic for all 0z ≠ .
H.W. 2 Show that sin(2 ) sinh(2 )tancos(2 ) cosh(2 )
x i yzx y+
=+
【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3.2, Problem 28, Pearson Education, Inc., 2005.】
Since
2 2 2 2
sin sin cosh cos sinhtancos cos cosh sin sinh(sin cosh cos sinh )(cos cosh sin sinh )
cos cosh sin sinh
z x y i x yzz x y i x yx y i x y x y i x y N
Dx y x y
+= =
−+ −
= ≡+
Consider the denominator D:
49
( ) ( )
[ ]
2 2 2 2 2 2 2 2
2 2
cos cosh sin sinh cosh 1 sin sin cosh 1
cosh sin(1 cosh 2 ) [1 cos(2 )]
21 cosh(2 ) cos(2 )2
x y x y y x x y
y xy x
y x D
+ = − + −
= −+ − −
=
= + =
Now, consider the numerator N: The real part of N is
( )2 2
2 2
cosh sin cos sinh sin cos1sin cos cosh sinh sin cos sin(2 )2
y x x y x x
x x y y x x x
−
= − = =
Then, consider the imaginary part of numerator:
( )2 2
2 2
cos cosh sinh sin cosh sinh1sinh cosh cos sin sinh cosh sinh(2 )2
x y y x y y
y y x x y y y
+
= + = =
Thus, we have
( )
1 12 2
12
sin(2 ) sinh(2 )
cosh 2 cos2
x i yND y x
+=
+
This implies that sin(2 ) sinh(2 )tancos(2 ) cosh(2 )
x i yzx y+
=+
---------- Q.E.D.
H.W. 3 (a) Since yxiyxz sinhcoscoshsinsin += and sinh coshy y≤ , show that
sinh sin coshy z y≤ ≤ .
(b) Derive a comparable double inequality for cos z . 【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3.2, Problem 30, Pearson Education, Inc., 2005.】 (a) Since yxiyxz sinhcoscoshsinsin += , we have
( )
2 2 2 2
2 2 2 2
2 2 2
2
sin sin cosh cos sinh
sin cosh cos sinh
sin cosh cos cosh sinh cosh
cosh sin cos
cosh cosh cosh (since cosh is positive!)
z x y i x y
x y x y
x y x y y y
y x x
y y y y
= +
= +
≤ + ≤
= +
= = =
∵
∴ sin coshz y≤ ----------- (1) On the other hand, we have
( )
2 2 2 2
2 2 2 2
2 2 2
2
sin sin cosh cos sinh
sin sinh cos sinh sinh cosh
sinh sin cos
sinh sinh
z x y x y
x y x y y y
y x x
y y
= +
≥ + ≤
= +
= =
∵
⇒ sinh siny z≤ ------------ (2) From Eqs.(1) and (2), we conclude that
sinh sin coshy z y≤ ≤ ------------ Q.E.D. (b) Since cos cos cosh sin sinhz x y i x y= − , we have
50
( )
2 2 2 2
2 2 2 2
2 2 2
2
cos cos cosh sin sinh
cos cosh sin sinh
cos cosh sin cosh sinh cosh
cosh sin cos
cosh cosh cosh (since cosh is positive!)
z x y i x y
x y x y
x y x y y y
y x x
y y y y
= −
= +
≤ + ≤
= +
= = =
∵
∴ cos coshz y≤ ----------- (3) Similarly, we have
( )
2 2 2 2
2 2 2 2
2 2 2
2
cos cos cosh sin sinh
sin sinh cos sinh sinh cosh
sinh sin cos
sinh sinh
z x y x y
x y x y y y
y x x
y y
= +
≥ + ≤
= +
= =
∵
⇒ sinh cosy z≤ ------------ (4) From Eqs.(3) and (4), we conclude that
sinh cos coshy z y≤ ≤ ------------ Q.E.D. H.W. 4 Find all roots of the equation sin cosh 4z = .
( )2 2 4 , 0, 1, 2,z n i nπ π= + ± = ± ± 【本題摘自:James Ward Brown and Ruel V. Churchill, Complex Variables and Applications, 6rd ed., Exercise 24, Problem 16, McGraw-Hill, Inc., 2005.】 H.W. 5 Find all roots of the equation cos 2z = . ( )12 cosh 2 or 2 ln 2 3 , 0, 1, 2,z n i n i nπ π−= + ± + = ± ± 【本題摘自:James Ward Brown and Ruel V. Churchill, Complex Variables and Applications, 6rd ed., Exercise 24, Problem 17, McGraw-Hill, Inc., 2005.】
51
§3-3 The Hyperbolic Functions
1. Recall that when we study in the real variable, the hyperbolic functions have been defined as following:
2sinh
xx eex−−
= , its graph is as shown in Fig. (a).
and 2
coshxx eex
−+= , its graph is as shown in Fig. (b).
2. Given any complex number z , we define
2
sinhzz eez
−−= ,
ieez
zizi
2sin
−−=
2
coshzz eez
−+= ,
2cos
zizi eez−+
=
1) 若取 z 為實數,則上述定義與實變函數中的雙曲線函數之定義可相符合。 2) zsinh and zcosh both have a fundamental period of 2π i . 3) zz sinh)sinh( −=−
zz cosh)cosh( =−
4) 1sinhcosh 22 =− zz
5) sinh2
z zd d e ezdz dz
−⎛ ⎞−= ⎜ ⎟
⎝ ⎠
zeezz
cosh2
)(=
−−=
−
)2
(coshzz ee
dzdz
dzd −+
=
zeezz
sinh2
=−
=−
6) If Ininzz ∈=⇒= ,0sinh π . Since 0sinh =z
⇒ 02
z ze e−⎛ ⎞−=⎜ ⎟⎜ ⎟
⎝ ⎠
⇒ zz ee −= Then, we have
122 =+ yixe This means that
y
x 0
3π i
2π i
π i
−2π i
−π i
2sinh
xx eexy−−
==
-5
-60
-40
-20
20
40
60
y
0 5x
Fig. (a)
2cosh
xx eexy−+
==
-5
-60
-40
-20
20
40
60
y
0 5x
Fig. (b)
52
1)2sin2(cos2 =+ yiye x 利用實部=實部,虛部=虛部,我們可得知 02sin =y ----------
and 12cos2 =⋅ ye x ----------
Since 02 >xe ⇒ 12cos =y ( 1− 不合) From , we can obtain that πny 22 = ⇒ πny = Again, we need
12 =xe ⇒ 0=x So, if sinh 0z = , we conclude that
iyxz += inin ππ =+= 0
7) If 1cosh 0 ,2
z z n i n Iπ⎛ ⎞= ⇒ = + ∈⎜ ⎟⎝ ⎠
Since 02
cosh =+=− zz eez ,
⇒ zz ee −−= ⇒ 12 −=ze ⇒ 1]2sin2[cos2 −=+− yiye x ⇒ 02sin =y
Since 02 >xe ⇒ 12cos −=y ⇒ π)12(2 += ny
故 1 ,2
y n n Iπ⎛ ⎞= + ∈⎜ ⎟⎝ ⎠
.
Again we need 12 −=xe ⇒ 0=x So, if sinh 0z = , we conclude that
iyxz += 12
n iπ⎛ ⎞= +⎜ ⎟⎝ ⎠
* 由(6)及(7)知,只有純虛數才能使 sinh z 和 cosh z 等於 0。
3. Given the complex number z, we define the other hyperbolic functions as followings:
1) sinh 1tanhcosh 2
zz z n iz
π⎛ ⎞= ≠ +⎜ ⎟⎝ ⎠
, .
2) coshcothsinh
zz z n iz
π= ≠, .
3) 1 1seccosh 2
h z z n iz
π⎛ ⎞= ≠ +⎜ ⎟⎝ ⎠
, .
4) 1cscsinh
h z z n iz
π= ≠, .
where In∈ in all cases. 5) Both ztanh and zcoth have a fundamental period of π i . 6) Both zhsec and zhcsc have a fundamental period of 2π i .
4. ztanh , zcoth , zhsec and zhcsc are analytic functions of z,其中 z 值不可為上述重點 3
所限制的各不允許值,則
1) 2 1(tanh ) sech2
d z z z n idz
π⎛ ⎞= ≠ +⎜ ⎟⎝ ⎠
,
2) 2(coth ) cschd z z z n idz
π= − ≠,
y
x0
3π i
2π i
π i
−π i
−2π i
iπ23
−
iπ21
−
iπ21
iπ23
iπ25
53
3) 1(sech ) sech tanh2
d z z z z n idz
π⎛ ⎞= ≠ +⎜ ⎟⎝ ⎠
,
4) (csch ) csch cothd z z z z n idz
π= − ≠,
where In∈ in all cases.
5. If iyxz += , then 1) xyixyz coshsinsinhcossinh += 2) xyiyyz sinhsincoshcoscosh +=
1) 2
sinhzz eez
−−=
( ) ( )
21 [ (cos sin ) (cos sin )]2
cos sin2 2
cos sinh sin cosh
x i y x i y
x x
x x x x
e e
e x i y e y i y
e e e ey i y
y x i y x
+ − +
−
− −
−=
= + − −
− += +
= +
2) zcosh 同理可證,亦可仿 §3-2 3.之 2) 證之。
6. If iyxz += , then a) zizi sin)(sinh = , zizi sinh)(sin = b) zzi cos)(cosh = , zzi cosh)(cos =
c) sinh sinhz z= , cosh coshz z=
d) xyz 222 sinhsin|sinh| +=
xyz 222 sinhcos|cosh| += H.W. 1 (a) Where on the line x y= is the equation sin sinh 0z i z+ = satisfied?
(b) Using MATLAB, obtain a three-dimensional plot of sin sinhz i z+ and verify that the surface obtained has zero height at points in Part (a). Include 0z = and at least one other solution, on the line, of the given equation.
【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3.3, Problem 20, Pearson Education, Inc., 2005.】 (a) Since sin sinh 0z i z+ = , we have
sin cosh cos sinh [sinh cos cosh sin ] 0x y i x y i x y i x y+ + + = ---------- (A) Using Re = Re and Im =Im, gives
sin cosh cosh sin 0x y x y− = Put x y= in the preceding equation, yields
sin cosh cosh sinx x x x= ---------- satisfied! Equating the imaginary part in Eq.(A), gives
cos sinh sinh cos 0x y x y+ = Put x y= in the preceding equation, yields
2sinh cos 0x x =
⇒ 0x = or 2
, 0, 1, 2, 3,x n nππ⎡ ⎤= ± + =⎢ ⎥⎣ ⎦. Also, y x= in this case.
(b) MATLAB commands:
x=[0:0.05:2]; y=[0:0.05:2] ; [X,Y]=meshgrid(x,y); Z=X+i*Y;
54
w=sin(Z)+i*sinh(Z); wm=abs(w); meshz(X,Y,wm);view(150,70)
H.W. 2 Find all roots of the equation (a) 1
2cosh z = , (b) sinh z i= , and (c) cosh 2z = − .
【本題摘自:James Ward Brown and Ruel V. Churchill, Complex Variables and Applications, 6rd ed., Exercise 25, Problem 14, Pearson Education, Inc., 2005.】
(a) ( )132 , 0, 1, 2,n i nπ± = ± ± (b) ( )122 , 0, 1, 2,n i nπ+ = ± ± (c) ( )ln 2 3 (2 1) , 0, 1, 2,n i nπ± + + + = ± ±
55
§3-4 The Logarithmic Function
1. For any complex number 0≠z , there exists complex numbers w such that 0≠= zew . In particular, one of such w’s is the complex number as shown below:
θizw += ||ln
Let θierz = , where rz =|| . Hence, we have
ln| |
ln
ln
w z i
r i
r i
i
e eee er ez
θ
θ
θ
θ
+
+=
=
= ⋅
==
Thus, we can define that
zizizzarg||ln
||lnln+=+= θ
1) Define πθπθ ≤
56
2 2 2 2
2 21
#
x yix y x yx i y z
z z zx y
= −+ +−
= = =⋅+
ii) Polar coordinate method: Let )(zfw = and (cos sin )z x iy r iθ θ= + = + , then
⎩⎨⎧
==
θθ
sincos
ryrx
In Chapter 2, we have derived the formula as shown below:
rwi
zdwd
∂∂
−= )sin(cos θθ
Note that θizzzfw +=== ||lnLn)(
θir += ln
⇒ rwi
zdwd
∂∂
−= )sin(cos θθ
1(cos sin )
1(cos sin )
1
ir
r i
z
θ θ
θ θ
= − ⋅
=⋅ +
=
----------- Q.E.D.
2. In the real variable analysis, we know that if 01 >x and 02 >x , then
2121 lnlnln xxxx +=⋅ However, in the complex variable analysis, the following 2121 LnLnLn zzzz +=⋅ may be not true. For example: Let iziz +−== 1, 21 then izz −−=⋅ 121 First, we have
iz LnLn 1 =
ln | |2
2
i i
i
π
π
= +
=
and )1Ln(Ln 2 iz +−= 3ln | 1 |4
3ln 24
i i
i
π
π
= − + +
= +
But 1 2Ln( ) Ln ( 1 )z z i⋅ = − − 3ln | 1 | ( )4
3ln 24
i i
i
π
π
= − − + −
= −
Hence, iizz ππ432ln
2LnLn 21 ++=+
iπ452ln +=
57
1 2Ln( ) #z z≠ ⋅
♣ But, the following theorems are still satisfied.
3. If the complex numbers 1z , 2z , 3z are different from zero, then the principal values of the arguments and logarithms of the product, quotient, and powers among these complex numbers are given by
1) )(),(2argarg)(Arg 2111121 azznzzzz -π++=⋅ )(),(2LnLn)(Log 2112121 bzznizzzz -π++=⋅
where 1n is assumed to be the values of 1, 0, 1− as following:
⎪⎪⎩
⎪⎪⎨
⎧
−≤+
58
where 2n is assumed to be the values of 1, 0, 1− as followings:
⎪⎪⎩
⎪⎪⎨
⎧
−≤−
59
Example 3 Find )22(Ln i+ .
Ln ( 2 2)ln | 2 2 | arg( 2 2)
ln 24
ii i i
i π
+= + + +
= +
Example 4 Find the principal value of i
ieπ3
)31(2 ⎥⎦
⎤⎢⎣⎡ −− .
3
3
33
1 3 1 33 ln arg2 2
( 1 3)2
1 3( )2
1 32
[cos3 sin 3 ]
i
i
ii
i ii i
e i
ie
ie
i e
π
π
ππ
ππ π
⎡ ⎤⎛ ⎞− − − −+⎢ ⎥⎜ ⎟
⎢ ⎥⎝ ⎠⎣ ⎦
⎡ ⎤− −⎢ ⎥⎣ ⎦
⎡ ⎤− −= ⎢ ⎥⎣ ⎦
⎛ ⎞− −= ⎜ ⎟
⎝ ⎠
= +
2
23 ln13
233
2
( 1)i i
i i
e
e
e
ππ
ππ
π
⎡ ⎤⎛ ⎞+ −⎜ ⎟⎢ ⎥⎝ ⎠⎣ ⎦
⎛ ⎞−⎜ ⎟⎝ ⎠
= − ⋅
= −
= −
5. If 0≠z , w and λ are any complex number,
then kizwz w π2Ln)(Ln += ----------- (1)
kiww ezz λπλλ 2)( ⋅= ----------- (2) where k is the integer given by bracket function
⎥⎦⎤
⎢⎣⎡ +−=
π2Arg)Re(||ln)Im(
21 zwzwk
Denote wz by α , zarg by θ , and let viuw += , then
zww ez Ln==α
]||ln[||ln
]||][ln[
θθ
θ
uzvivzu
izviu
ee
e
+−
++
⋅=
=
Thus,
⎪⎩
⎪⎨⎧
++=
= −
kuzvz
e vzu
πθ
α θ
2||lnarg
|| ||ln ------------ (3)
where k is the integer such that ππθπ ≤++
60
⎥⎦⎤
⎢⎣⎡ +−=
⎥⎦⎤
⎢⎣⎡ +−=+=
π
πθ
2arg)Re(||Ln)Im(
21
2||Ln
21]1[
zwzw
uzvtk
Now, using Eq. (3), we see that
kizw
kiizviu
kuzvivzu
kuzvie
i
z
vzu
w
π
πθ
πθθ
πθ
αα
α
θ
2Ln
2)||)(ln(
]2||ln[||ln
]2||ln[][Ln
arg||ln
Ln)(Ln
||ln
+=
+++=
+++−=
+++=
+=
=
−
故(1)式已被證得。 同理,可證得(2)式。
H.W. 1 Consider the identity ln lnnz n z= , where n is an integer, which is valid for appropriate choice of
the logarithms on each side of the equation. Let 1z i= + and 5n = . (a) Find the values of ln nz and ln z that satisfy ln lnnz n z= . (b) For the given z and n, is ln lnnz n z= satisfied? (c) Suppose n = 2 and z is unchanged. Is ln lnnz n z= then satisfied?
【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3.4, Problem 26, Pearson Education, Inc., 2005.】
(a) 54
5ln ln 5 Ln 2z z i π⎡ ⎤= = +⎢ ⎥⎣ ⎦
(b) No. (c) Yes.
6. Definition (Branch):
A branch of a multivalued function is a single-valued function analytic in some domain. At every point of the domain, the single-valued function must assume exactly one of the various possible values that the multivalued function can assume.
Definition (Branch cut) A line used to create a domain of analyticity is called a branch line or branch cut.
Definition (Branch point) Any point that must lie on a branch cut ⎯ no matter what branch used ⎯ is called a branch point of a multivalued function.
Ex. (1) Ln z ≡ principal value of ln z, which is defined for all z except z = 0. (2) Ln z is also used to denote the principal branch of the logarithm function, which is defined for all
z except z = 0 and values of z on the negative real axis. (3) ( ) Lnf z r iθ= + , where 3 / 2 / 2π θ π− < ≤ .
⇒ It is discontinuous at the origin and at all points on the positive imaginary axis. (4) ( ) Lnf z r iθ= + , where 3 / 2 2 / 2 2 , 0, 1, 2,k k kπ π θ π π− + < ≤ + = ± ± , are, for each k,
analytic branches, provided z is confined to the domain D1. Example 5 (a) Find the largest domain of analyticity of ( ) Ln[ (3 4 )]f z z i= − + .
(b) Find the numerical value of (0)f .
(a) For the given function, the non-analytic points are located at:
61
Im 0, Re 0w w= ≤
If (3 4 )w z i= − + , these two conditions can be rewritten as
[ ]Im ( ) (3 4 ) 0 4x iy i y+ − + = ⇒ = [ ]Re ( ) (3 4 ) 0 3x iy i x+ − + ≤ ⇒ ≤
So, the full domain of analyticity is shown in the following Fig. (a).
(b) (0) Ln( 3 4 ) Ln(5) arg( 3 4 )f i i i= − − = + − − , where arg( 3 4 )iπ π− < − − < .
⇒ (0) Ln(5) 2.214f i= − ⇒ Fig. (b).
H.W. 2 (a) Show that ( )Ln Ln( )z is analytic in the domain consisting of the z-plane with a branch cut along
the line 0, 1y x= ≤ . (See below) (b) Find ( )Ln Ln( )d z dz within the domain of analyticity found in part (a). (c) What branch cut should be used to create the maximum domain of analyticity for
( )Ln Ln Ln( )z⎡ ⎤⎣ ⎦ ? 【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3-5, Problem 15, Pearson Education, Inc., 2005.】
H.W. 3 The complex electrostatic potential ( , ) Ln(1/ )x y i zφ ψΦ = + = , where 0z ≠ , can be created by an
electric line charge located at 0z = and lying perpendicular to the xy-plane. (a) Sketch the streamlines for this potential. (b) Sketch the equipotentials for 1, 0, 1, 2φ = − .
jy
x
− 4i
− 3
− 2.214 (approx.)
jy
x
Branch cut y = 4, x ≤ 3
3 + 4i
Fig. (a)Fig. (b)
jy
x.
Domain of analytic of Ln z (shaded)
jy
x
Branch cut Domain D1
jy
x
Branch cut
1
Fig. HW-2
62
(c) Find the components of the electric field at an arbitrary point (x, y). 【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3-5, Problem 16,
Pearson Education, Inc., 2005.】 (a) Since ( , ) Ln(1/ ) Lnx y i z zφ ψΦ = + = = −
⇒ 2 2( , ) Lnx y x yφ ⎛ ⎞= − +⎜ ⎟⎝ ⎠
, ( )1( , ) tan yxx yψ −= − , where ψ ’s are ramp emanating from origin. (b) Since 2 21 Ln 1x y φ⎛ ⎞− = − + = = −⎜ ⎟
⎝ ⎠, therefore
2 2x y e+ = if 1φ = −
Also, when 2 20 Ln 0x y φ⎛ ⎞= − + = =⎜ ⎟⎝ ⎠
, therefore
2 2 1x y+ = if 0φ =
When 2 21 Ln 1x y φ⎛ ⎞= − + = =⎜ ⎟⎝ ⎠
, therefore
2 2 1/x y e+ = if 1φ = The electric field is
x ydE iEdzΦ⎛ ⎞+ = −⎜ ⎟
⎝ ⎠
⇒ 2 2xxE
x y=
+ and 2 2y
yEx y
=+
(c) MATLAB commands:
% HW (c) x=[-2.5:0.02+0.001:2.5]; y=x; [X,Y]=meshgrid(x,y); Z=X+i*Y; w=log(Z-1-1*i); %wm=real(w); % for real part wm=imag(w); % for imag part Meshz(X,Y,wm); % for imag part and real View(45,45);
H.W. 4 Let
3( )( ) 10 zf z = . This function is evaluated such that ( )f z′ is real when 1z = . Find (1 )f i′ + . Where in the complex plane is ( )f z analytic?
【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3-6, Problem 24, Pearson Education, Inc., 2005.】
ψ = π/4
ψ = −π/4
ψ = −3π/4
x
y
x
yφ = 1
φ = 0
φ = − 1
63
(1 ) 0.137 0.0148f i i′ + = − ; ( )f z is an entire function.
(a) real part
(b) imaginary part
H.W. 5 Let ( )( ) 10
zef z = . This function is evaluated such that 2( / 2)f i e ππ −= . Find ( )f z′ and ( / 2)f iπ′ .
【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3-6, Problem 24, Pearson Education, Inc., 2005.】
[ ][Ln(10) 2 ]( ) Ln(10) 2zi e zf z e i eπ π+′ = + and ( / 2) 0.00464 0.01f i iπ′ = −
64
§3-5 Inverse Trigonometric and Hyperbolic Functions
1. 1) Let sinz w= , then ( )1/ 21 2sin ln 1z i zi z− ⎡ ⎤= − + −⎢ ⎥⎣ ⎦
Since 2
iw iwe ezi
−−= , assume that iwp e= and 1/ iwp e−= , then we have
1/2
p pzi
−=
⇒ 22 1izp p= −
⇒ 2 2 1 0p izp− − = Solve this equation for p:
( )1/ 221p zi z= + − or ( )1/ 221iwe zi z= + − ⇒ ( )1/ 221 ln 1w zi zi
⎡ ⎤= + −⎢ ⎥⎣ ⎦
Since 1sinw z−= , we have
( )1/ 21 21sin ln 1z zi zi− ⎡ ⎤= + −⎢ ⎥⎣ ⎦
2) Other inverse trigonometric functions:
( )1/ 21 21cos ln 1z z zi− ⎡ ⎤= + −⎢ ⎥⎣ ⎦
1tan ln2i i zz
i z− +⎛ ⎞= ⎜ ⎟−⎝ ⎠
2. Inverse of Hyperbolic function
1) ( )1/ 21 2sinh ln 1z z z− ⎡ ⎤= + +⎢ ⎥⎣ ⎦
2) ( )1/ 21 2cosh ln 1z z z− ⎡ ⎤= + −⎢ ⎥⎣ ⎦
3) 1 1 1tanh ln2 1
zzz
− +⎛ ⎞= ⎜ ⎟−⎝ ⎠
3. Derivative of inverse trigonometric functions:
1) ( )( )
1/ 21 21/ 22
1 1sin ln 11
d dz zi zdz dz i z
− ⎧ ⎫⎡ ⎤= + − =⎨ ⎬⎢ ⎥⎣ ⎦⎩ ⎭ −
2) ( )
11/ 22
1cos1
d zdz z
− −=−
3) ( )
12
1tan1
d zdz z
− =+
4. Derivative of inverse hyperbolic functions:
1) ( )
11/ 22
1sinh1
d zdz z
− =+
2) ( )
11/ 22
1cosh1
d zdz z
− =−
65
3) ( )
12
1tanh1
d zdz z
− =−
Example 1 Find 1sin (1/ 2)− .
1/ 21 1 3sin (1/ 2) ln
2 4i
i− ⎡ ⎤⎛ ⎞= +⎢ ⎥⎜ ⎟
⎝ ⎠⎢ ⎥⎣ ⎦
Taking ( )1/ 23/ 4 3 / 2= , the above expression becomes
( )1 1 3sin (1/ 2) ln ln 1 ( / 6) 2 , 0, 1, 2,2 2 6i i k k
iππ π−
⎡ ⎤= + = − ∠ = + = ± ±⎢ ⎥
⎣ ⎦
Taking ( )1/ 23/ 4 3 / 2= − , the above expression becomes
( )1 1 3 5sin (1/ 2) ln ln 1 (5 / 6) 2 , 0, 1, 2,2 2 6i i k k
iππ π−
⎡ ⎤= − = − ∠ = + = ± ±⎢ ⎥
⎣ ⎦
Example 2 Find all the numbers whose sine is 2.
This question is to solve sin 2z = . Thus, we have
( )1/ 21 1sin (2) ln 2 3ii
− ⎡ ⎤= + −⎢ ⎥⎣ ⎦
Taking ( )1/ 23 3i− = + , the above expression becomes
( ) ( )( )
12
2
1sin (2) ln 2 3 Ln 2 3 2
2 1.317, 0, 1, 2,
i i i i ki
k i k
π
π
π
π
− ⎡ ⎤⎡ ⎤= + = − + + +⎣ ⎦ ⎢ ⎥⎣ ⎦
= + − = ± ±
Taking ( )1/ 23 3i− = − , the above expression becomes
( ) ( )( )
12
2
1sin (2) ln 2 3 Ln 2 3 2
2 1.317, 0, 1, 2,
i i i i ki
k i k
π
π
π
π
− ⎡ ⎤⎡ ⎤= − = − − + +⎣ ⎦ ⎢ ⎥⎣ ⎦
= + + = ± ±
Example 3 Find all the numbers whose sine is i.
This question is to solve sin z i= . Thus, we have
( )1/ 21 21sin ( ) ln 2 ln(1 2)i i ii
− ⎡ ⎤= + = − ±⎢ ⎥⎣ ⎦
Taking ( )1/ 23 3i− = + , the above expression becomes
( ) ( )( ) ( ) ( )
1Ln 2 1 2 2 Ln 2 1
sin ( ) ln 1 2Ln 2 1 2 2 Ln 2 1
i i k k ii i
i i k k i
π π
π π π π−
⎧ ⎡ ⎤− − + = − −⎪ ⎣ ⎦⎡ ⎤= − − ± = ⎨⎣ ⎦ ⎡ ⎤− + + + = + − +⎪ ⎣ ⎦⎩
where 0, 1, 2,k = ± ± . H.W. 1 Show that ( )1 1sin ( ) ( 1) ln 1 2ni n iπ− += + − + . 【本題摘自:James Ward Brown and Ruel V. Churchill, Complex Variables and Applications, 6rd ed., Section 29, Example 1, McGraw-Hill, Inc., 2005.】 H.W. 2 Show that ( ) ( )1tanh (1/ 2) ln cot / 2ie iθ θ− = ⎡ ⎤⎣ ⎦ . 【本題摘自:A. David Wunsch, Complex Variable with Applications, 3rd ed., Exercise 3-7, Problem 16,
66
Pearson Education, Inc., 2005.】
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