�, ��z
�
F �y (Fourier y )
�* � f(x)\�KT;ÆZ�q1EN� \�p�g2hS�U
∫ +∞
−∞
|f(x)|dx <
+∞, ^�I$
fˆ(λ) =
∫ +∞
−∞
f(x)e−iλxdx
0 f(x)' Fouriery ,f(x)0 fˆ(λ)' Fourier�y ,[X0 fˆ(λ) = F [f(x)], f(x) =
F−1[fˆ(λ)].
�'�� \�#�*9�\ f(x) 'qE*�
f(x) =
1
2pi
∫ +∞
−∞
fˆ(λ)eiλxdλ
0(%/
1. #%
F [c1f1 + c2f2] = c1F [f1] + c2F [f2],
2. �)�%
F [f(x)eiλ0x] = fˆ(λ− λ0)
3. ���! � f(±∞) = f ′(±∞) = · · · = f (n−1)(±∞) = 0, f (n)(x) ' Fourier
P \�^
F [f (n)(x)] = (iλ)nfˆ(λ).
)
(
F [f ′(x)] = iλfˆ(λ), F [f ′′(x)] = −λ2fˆ(λ).
4. ���� � f(x), g(x) \�p�g2hS�-PfSI$
f ∗ g(x) =
∫ +∞
−∞
f(x− ξ)g(ξ)dξ,
^
F [f ∗ g] = fˆ(λ)gˆ(λ).
x.#���~ Fourier -"�+"y
�* f(x)\ [0,+∞)��OT;ÆZ�qVEN� \ [0,+∞)�g2hS�
77
-"y �
fˆs(λ) = Fs[f(x)] ,
∫ +∞
0
f(x) sinλxdx,
+"y �
fˆc(λ) = Fc[f(x)] ,
2
pi
∫ +∞
0
f(x) cos λxdx.
�'��
6e:
P�
f(x) = F−1s [fˆs(λ)] ,
∫ +∞
0
fˆs(λ) sin λxdλ,
6V:
P�
f(x) = F−1c [fˆc(λ)] ,
2
pi
∫ +∞
0
fˆc(λ) cos λxdλ.
L �y Laplace y
�* � f(t) = f(t)h(t), �m h(t) =
{
1, t ≥ 0
0, t < 0
, p 0<$�^�I$
fˆ(p) =
∫ +∞
0
f(t)e−ptdt
0 f(t)' Laplace y ,f(t)0 fˆ(p)' Laplace �y ,[X0 f¯(p) = L[f(t)], f(t) =
L−1[f¯(p)].
�'�� # f(t) \ [0,+∞) ��OT;ÆZq1EN�^0j$_�B�
[f(t)] ≤ keσ0t, σ0 ≥ 0, ^ f¯(p) \ Rep > σ0 �a7�
f(t) =
1
2pii
∫ σ+i∞
σ−i∞
f¯(p)eptdp, σ > σ0.
0(%/
1. #%
L[c1f1 + c2f2] = c1L[f1] + c2L[f2].
2. &|%/
L[f(t− z)] = e−pτL[f(t)], f(t− τ) = f(t− τ)h(t− τ).
3. ���!
L[f (n)(t)] = pnL[f(t)]− pn−1f(+0)− pn−2f ′(+0) · · · − f (n−1)(+0).
78
4. ����
�*
f ∗ g(t) =
∫ t
0
f(t− τ)g(τ)dτ,
^
L[f ∗ g] = L[f ] · L[g].
S:
P5�
a�/:7�'vJnoH75�rH RU5bÆW�'�
/:7�'�i4+��i4+JQL4+�IhMRj
aTbÆW�'QL4
+�
S:
P5.GS:
P�2>
s'/:Z%
0!$Z%��3��/
:7�'4+
0�/:7�'4+
a�uM[oR6
P
�X-a4+'
a�
�`rH(zR Fourier
P (F �y ) J Laplace
P (L �y )
a�/
:7�-a4+�
��{1
1. F℄v
P'
s�2d>-a4+ve
P�&%2fI$'>I$|t
'�/:7�'-a4+�
2.
a�I$|t'�/:7�'-a4+�
3. 2�I$v6
P�
�X�U2fI$�
�$�3
� 3.1 5��=�'��$4+{ ∂u
∂t
= a2
∂2u
∂x2
+ f(t, x), (t > 0,−∞ < x < +∞)
u(0, x) = ϕ(x)
Æ )J��ve
P�
bn −∞ < x < +∞, QF x
sv F �y , X uˆ(t, λ) = F [u(t, x)] =∫ +∞
−∞
u(t, x)e−iλxdx. :
27�J��-℄v F !
P�&�/:7��i4+
{ ∂uˆ
∂t
= −a2λ2uˆ+ fˆ(t, λ)
uˆ(0, λ) = ϕˆ(λ).
)4��
a>I$�
79
7�.a0
uˆ(t, λ) = e−a
2λ2t
[∫ t
0
fˆ(τ, λ)ea
2λ2τdτ + c
]
!���-℄
uˆ(0, λ) = c = ϕˆ(λ)
a&
uˆ(t, λ) = ϕˆ(λ)e−a
2λ2t +
∫ t
0
fˆ(τ, λ)e−a
2λ2(t−τ)dτ
)���v6
P�&
u(t, x) = F−1[ϕˆ(λ)e−a
2λ2t] + F−1
[∫ t
0
fˆ(τ, λ)e−a
2λ2(t−τ)dτ
]
= F−1[ϕˆ(λ)] ∗ F−1[e−a2λ2t] +
∫ t
0
F−1[fˆ(τ, λ)] ∗ F−1[e−a2λ2(t−τ)]dτ
= ϕ(x) ∗ 1
2a
√
pit
e
− x
2
4a2t +
∫ t
0
f(τ, x) ∗ 1
2a
√
pi(t− τ)e
− x
2
4a2(t−τ)dτ
=
1
2a
√
pit
∫ +∞
−∞
ϕ(ξ)e−
(x−ξ)2
4a2t dξ +
1
2a
√
pi
∫ t
0
∫ +∞
−∞
f(τ, ξ)√
t− τ e
−
(x−ξ)2
4a2(t−2) dξdτ,
�m
F−1[e−a
2λ2t] =
1
2pi
∫ +∞
−∞
e−a
2λ2teiλxdλ
=
1
pi
∫ +∞
0
e−a
2λ2t cos λxdλ
=
1
2a
√
pit
e
− x
2
4a2t ,
hRH�sS:Rx$-mW%�R��&�
� 3.2 ���~'
+�4+
∆2u = 0 (−∞ < x < +∞, y > 0)
u(x, 0) = f(x)
lim
x2+y2→+∞
u(x, y) = 0
Æ 2 x v F �y , X uˆ(λ, y) = F [u(x, y)]. &�/:7��i4+{−λ2uˆ+ ∂2uˆ
∂y2
= 0
uˆ|y=0 = fˆ(λ), uˆ|y=+∞ = 0.
7�.a0
uˆ(λ, y) = Aeλy +Be−λy
80
!��-℄
uˆ|y=0 = A+B = fˆ(λ),
uˆ|y=+∞ = 0, & λ > 0 � A = 0; λ < 0 � B = 0,
�3
uˆ(λ, y) = fˆ(λ)[h(−λ)eλy + h(λ)e−λy ] = fˆ(λ)e−|λ|y.
v6
P&
u(x, y) = f(x) ∗ F−1[e−|λ|y]
= f(x) ∗ 1
pi
y
x2 + y2
=
1
pi
∫ +∞
−∞
yf(ξ)
(x− ξ)2 + y2dξ,
�m
F−1[e−|λ|y] =
1
2pi
∫ +∞
−∞
e−|λ|yeiλxdλ
=
1
pi
∫ +∞
−∞
e−λy cos λxdλ
=
1
pi
y
x2 + y2
.
2
�
1. F y9ZMi��qeA��|\�fs�uH8��|��9ZH9lH
O�7�x (−∞,+∞).
2. ^R9Z?SI4m�9�>��;�pC���L�?Twi��QoE
P��oEP�~ÆDj�
� 3.1 Æ} ����
� 3.2 Æ} ����
� 3.3 Æ} ����
� 3.3 J0�y}/Lf'�h<�'��$4+
∂u
∂t
= a2
∂2u
∂x2
, (x > 0, t > 0)
∂u
∂x
∣∣∣∣
x=0
= q
u|t=0 = 0
81
Æ 0*0) II k�-℄�7�mDU x '�$04_�2 x v +"y
uˆ(t, λ) = Fc[u(t, x)] =
∫ +∞
0
u(t, x) cos λxdλ.
� u|x=+∞ = 0, ∂u∂x
∣∣∣
x=+∞
= 0, ^T
Fc
[
∂u
∂t
]
=
∂uˆ
∂t
,
Fc
[
∂2u
∂x2
]
=
∫ +∞
0
∂2u
∂x2
cos λxdx
=
[
∂u
∂x
cos λx+ λu sinλx
]+∞
0
− λ2
∫ +∞
0
u cos λxdx
= −q − λ2uˆ.
C&�I$|t'-a4+ { ∂uˆ
∂t
+ a2λ2 = −a2q
uˆ|t=0 = 0
a&
uˆ(t, λ) =
q
λ2
(e−a
2λ2t − 1).
S +"y '6GA�
u(t, x) =
2
pi
∫ +∞
0
uˆ(t, λ) cos λxdλ
=
2
pi
∫ +∞
0
q
λ2
(e−a
2λ2t − 1) cos λxdλ,
T
∂u
∂t
=
2
pi
∫ +∞
0
−a2qe−a2λ2t cos λxdλ
= − aq√
pit
e
− x
2
4a2t
�3
u(t, x) = u(t, x)− u(0, x) = − aq√
pi
∫ t
0
1√
τ
e
− x
2
4a2τ dτ
v
s!P y = x
2a
√
τ
, &
u(t, x) =
−qx√
pi
∫ +∞
x
2a
√
t
1
y2
e−y
2
dy.
82
2
�
1.5��uH�|
���Yx��9Z�tg�KJH8f}b_P��U
� x HFzdz�
2. ����9ZH�RTwik�R<^RB�
�G��KJH8f}b
(oE�QoEhi) _ +∞ Jr� 0 Hav�
3. qN9Zi�X? F yN9ZW=:�\�
`{^R�
� 3.4 Æ} ����
� 3.4 �h<�'��$4+
∂u
∂t
= a2
∂2u
∂x2
, (x > 0, t > 0)
u|x=0 = f(t), lim
x→+∞
u = 0
u|t=0 = 0
Æ 2�QL4+�h2 xve:
P�Ih2 tv L �y . bn�RMa�
w u¯(p, x) = L[u(t, x)], X4+h
0>I$'�i4+{
pu¯ = a2
∂2u¯
∂x2
u¯|x=0 = f¯(p), u¯|x=+∞ = 0.
7�.a0
u¯(p, x) = Ae
√
p
a
x +Be−
√
p
a
x,
!��b-℄
u¯|x=+∞ = 0, T A = 0;
u¯|x=0 = B = f¯(p),
T
u¯(p, x) = f¯(p)e−
√
p
a
x.
��h&
u(t, x) = L−1[f¯(p)e−
√
p
a
x]
= L−1[f¯(p)] ∗ L−1[e−
√
p
a
x]
= f(t) ∗ x
2a
√
pit3
e
− x
2
4a2t
=
x
2a
√
pi
∫ t
0
f(t− z)√
τ3
e
− x
2
4a2τ dτ.
83
oRr8 3.4 '`F�S,YXm h
&QL4+
∂u
∂t
= a2
∂2u
∂x2
(t > 0, x > 0)
u|x=0 = ϕ(t)
u|t=0 = ψ(x)
'a�
� 3.5 T;ÆZ�:
.7�'QL4+
∂2u
∂t2
= a2
∂2u
∂x2
, (t > 0, 0 < x < l)
u|x=0 = 0, ∂u
∂x
∣∣∣∣
x=l
= A sinωt
u|t=0 = 0, ∂u
∂t
∣∣∣∣
t=0
= 0
Æ b�9���b-℄'QL4+��)a^�b-℄��OMhR:l
s5ag�bn�R L �y
a�
w u¯(p, x) = L[u(t, x)], T
p2u¯ = a2
∂2u¯
∂x2
(0 < x < l)
u¯|x=0 = 0, ∂u¯
∂x
∣∣∣∣
x=p
=
Aω
p2 + ω2
.
ag�h&
u¯ = Aaω
sh
x
a
p
p(p2 + ω2)ch l
a
p
.
S L !
P'6GA�Jx$mz
u(t, x) =
1
2pii
∫ σ+i∞
σ−i∞
u¯(p, x)eptdp
=
∑
k
Res[u¯(p, x)ept, pk],
�m {pk} 0 u¯ept \ p �~�'&TBp�*�
bn u¯eptTh��* p0 = 0,JVT* p˜±1 = ±iω,JVT* p±k = ±i(2k − 1)api2l , k =
1, 2, · · ·.
Res[u¯ept, p0] = 0,
84
Res[u¯ept, p˜1] + Res[u¯e
pt, p˜−1]
=
Aaωsh
(x
a
− p
)
ePt
p(p + iω)ch
(
l
a
p
)
∣∣∣∣∣∣∣∣
p=iω
+
Aaωsh
(x
a
p
)
ePt
p(p− iω)ch
(
l
a
p
)
∣∣∣∣∣∣∣∣
p=−iω
= 2Re
Aaωsh
(x
a
p
)
ePt
p(p+ iω)ch
(
l
a
p
)
∣∣∣∣∣∣∣∣
p=iω
=
Aa
ω cos
ωl
a
sin
ωx
a
sinωt
Res[u¯ept, pk] + Res[u¯e
pt, p−k]
= 2Re
Aaωsh
(x
a
p
)
ePt
p(p2 + ω2)
· 1(
ch
l
a
p
)′
∣∣∣∣∣∣∣∣∣
p=i (2k−1)api
2l
=
(−1)k−116Aaωl2
(2k − 1)pi[4l2ω2 − a2(k − 1)2pi2] sin
(2k − 1)pix
2l
sin
(2k − 1)piat
2l
.
� 3.6 5��:'��
.
∂2u
∂t2
= a2
∂2u
∂x2
+ f(t, x), (t > 0,−∞ < x < +∞)
u|t=0 = 0, ∂u
∂t
∣∣∣∣
t=0
= 0.
Æ X u¯(p, x) = L[u(t, x)], 2��i4+v L �y , &
p2u¯ = a2
∂2u¯
∂x2
+ f¯(p, x), (−∞ < x < +∞)
Æ8� u|x=±∞ = 0, �3 u¯|x=±∞ = 0. b��p�'�/:7��i4+�hM[
R F �y
a�
X
̂¯u(p, λ) = F [u¯(p, x)], T!$7�
p2̂¯u = −a2λ2̂¯u+ ̂¯f(p, λ)
a&
̂¯u(p, λ) = ̂¯f(p, λ)
p2 + a2λ2
,
85
6
P�h&
u = L−1[F−1[̂¯u(p, λ)]]
= F−1
[
L−1
[ ̂¯f(p, λ)
p2 + a2λ2
]]
= F−1
[
L−1
[
1
p2 + a2λ2
]
∗ L−1[̂¯f(p, λ)]]
= F−1
[
sin aλt
aλ
∗ f̂(t, λ)
]
= F−1
[∫ t
0
f̂(t− τ, λ)e
iaλτ − e−iaλτ
2iaλ
dτ
]
=
1
2a
∫ t
0
{
F−1
[
f̂(t− τ, λ)
iλ
eiaλτ
]
− F−1
[
f̂(t− τ, λ)
iλ
e−iaλτ
]}
dτ
=
1
2a
∫ t
0
[∫ x+aτ
0
f(t− τ, ξ)dξ −
∫ x−aτ
0
f(t− τ, ξ)dξ
]
dτ
=
1
2a
∫ t
0
∫ x+aτ
x−aτ
f(t− τ, ξ)dξdτ,
bnR%tA�
F−1
[
f̂(λ)
iλ
]
=
∫ x
0
f(ξ)dξ,
F−1[f̂(λ)eiλx0 ] = f(x+ x0).
2
�
L y9Zi��qeA��|�[V�|�n℄6;�� F y9Z ~�
� 3.7 �1iZm'��$4+{ ∂u
∂t
= a2∆3u = a
2
(
∂2u
∂x2
+
∂2u
∂y2
+
∂2u
∂z2
)
, (t > 0,−∞ < x, y, z < +∞)
u|t=0 = ϕ(x, y, z)
Æ b��iZ'4+�h23l
sv�1 Fourier y , UK�2 x, y, z v
Fourier
P�
w
û(t, λ, µ, ν) = F3[u(t, x, y, z)]
=
∫∫∫ +∞
−∞
u(t, x, y, z)e−i(λx+µy+νz)dλdµdν,
86
^
F3
[
∂2u
∂x2
]
= (iλ)2û, F3
[
∂2u
∂y2
]
= (iµ)2û, F3
[
∂2u
∂z2
]
= (iν)2û.
& û |t'-a4+ { ∂û
∂t
= −a2(λ2 + µ2 + ν2)û
û|t=0 = ϕ̂(λ, µ, ν),
a&
û(t, λ, µ, ν) = ϕ̂(λ, µ, ν)e−a
2(λ2+µ2+ν2)t,
K�2 λ, µ, ν v F !6
P�?efSA�U&
u(t, x, y, z) =
1
(2pi)3
∫∫∫ +∞
−∞
ϕ̂(λ, µ, ν)e−a
2(λ2+µ2+ν2)tei(λx+µy+νz)dλdµdν
= ϕ(x, y, z) ∗ F−1[e−a2λ2t]F−1[e−a2µ2t]F−1[e−a2ν2t]
= ϕ(x, y, z) ∗ 1
(2a
√
pit)3
e
−x
2+y2+z2
4a2t
=
1
(2a
√
pit)3
∫∫∫ +∞
−∞
ϕ(ξ, η, ζ)e−
(x−ξ)2+(y−η)2+(z−ζ)2
4a2t dξdηdζ.
� 3.1 a�i4+{ ∂u
∂t
+ a
∂u
∂x
= f(t, x) (t > 0,−∞ < x < +∞)
u|t=0 = ϕ(x)
Æ} v F �y & { ∂û
∂t
+ iλaû = f̂(t, λ)
û|t=0 = ϕ̂(λ),
a&
û(t, λ) = ϕ̂(λ)e−iλat +
∫ t
0
f̂(τ, λ)e−iλa(t−τ)dτ,
F !6
P&
u(t, x) = ϕ(x− at) +
∫ t
0
f(τ, x− a(t− τ))dτ,
bn
F−1[ϕ̂(λ)e−iλat] =
1
2pi
+∞∫
−∞
ϕ̂(λ)eiλ(x−at)dλ = ϕ(x− at).
����
1. �F7�')a�N
��� f(t, x) = et, N\T)a v(t, x) = et, �;T�
'�["'75
a�
87
2. �;hR L !
P
a�
� 3.2 a�i4+ { ∂u
∂t
= a2
∂2u
∂x2
+ b
∂u
∂x
+ cu
u|t=0 = ϕ(x)
Æ} v F �y & { ∂û
∂t
= (−a2λ2 + ibλ+ c)û
û|t=0 = ϕ̂(λ)
a&
û(t, λ) = ϕ̂(λ)e−(a
2λ2−ibλ−c)t,
�3
u(t, λ) = ϕ(x) ∗ F−1[e−(a2λ2−ibλ−c)t]
= ϕ(x) ∗ 1
2pi
e−ct
∫
−−∞+∞e−a2λ2−ibλ+iλxdλ
=
e−ct
2a
√
pit
∫ +∞
−∞
ϕ(x− ξ)e−
(ξ−b)2
4a2t dξ
���� �;.G2fI$'!P�A�7�m'J_$=�[v F !
P�
� 3.3 a�i4+
∂2u
∂t2
= a2
∂2u
∂x2
, (t > 0,−∞ < x < +∞)
u|t=0 = ϕ(x), ∂u
∂t
∣∣∣∣
t=0
= ψ(x).
Æ} v F �y &
∂2û
∂t2
= −a2λ2û
û|t=0 = ϕ̂(λ), ∂û
∂t
∣∣∣∣
t=0
= ψ̂(λ)
=⇒ û(t, λ) = Aeiaλt +Be−iaλt,
�m
A =
1
2
[
ϕ̂(λ) +
ψ̂(λ)
iaλ
]
, B =
1
2
[
ϕ̂(λ)− ψ̂(λ)
iaλ
]
.
88
=⇒ u(t, x) = 1
2pi
∫ +∞
−∞
[Aeiaλt +Be−iaλt]eiλxdλ
=
1
2
[
1
2pi
∫ +∞
−∞
ϕ̂(λ)eiλ(x+at)dλ+
1
2pi
∫ +∞
−∞
ϕ̂(λ)eiλ(x−at)dλ
]
+
1
2a
[
1
2pi
∫ +∞
−∞
ψ̂(λ)
iλ
eiλ(x+at)dλ− 1
2pi
∫ +∞
−∞
ψ̂(λ)
iλ
eiλ(x−at)dλ
]
=
1
2
[ϕ(x+ at) + ϕ(x− at)] + 1
2a
∫ x+at
x−at
ψ(ξ)dξ,
�m�uMJ�js
1
2pi
∫ +∞
−∞
ψ̂(λ)
iλ
eiλ(x+at)dλ− 1
2pi
∫ +∞
−∞
ψ̂(λ)
iλ
eiλ(x−at)dλ
=
1
2pi
∫ +∞
−∞
∫ x+at
x−at
ψ̂(λ)eiλξdξdλ
=
∫ x+at
x−at
1
2pi
∫ +∞
−∞
ψ̂(λ)eiλξdλdξ
=
∫ x+at
x−at
ψ(ξ)dξ.
����
�F7�m_,9��= f(t, x),�;RS:
P
a� (S,YXm�kD
a ϕ(x) = ψ(x) = 0 '
C�) �\ � 3.6.
� 3.4 a�h<�'4+
∂u
∂t
= a2
∂2u
∂x2
, (t > 0, x > 0)
u|x=0 = 0
u|t=0 = ϕ(x).
Æ} w
û(t, λ) = Fs[u(t, x)] =
∫ +∞
0
u(t, x) sin λxdx,
T
∂û
∂t
= a2
∫ +∞
0
∂2u
∂x2
sinλxdx
= a2
[
∂u
∂x
sinλx− λu cos λx
]+∞
0
− a2λ2
∫ +∞
0
u sinλxdx
= −a2λ2û
û|t=0 = ϕ̂(λ),
&
û = ϕ̂e−a
2λ2t,
89
�3
u =
2
pi
∫ +∞
0
ϕ̂(λ)e−a
2λ2t sinλxdλ
=
2
pi
∫ +∞
0
∫ +∞
0
ϕ(ξ) sin λξdξe−a
2λ2t sinλxdλ
=
1
pi
∫ +∞
0
ϕ(ξ)
∫ +∞
0
e−a
2λ2t[cos λ(x− ξ)− cos λ(x+ ξ)]dλdξ
=
1
2a
√
pit
∫ +∞
0
ϕ(ξ)[e−
(x−ξ)2
4a2t − e− (x+ξ)
2
4a2t ]dξ.
����
1. �F0*M f(t) Z.��Re:
P
a{�
2. �F7�m_Y ∂u
∂x
=��Re:
P
a{�
� 3.5 R Laplace
P
a-a4+{ ∂2u
∂x∂y
= u− e−(x+y), (x > 0, y > 0)
u|x=0 = 0, u|y=0 = xe−x.
Æ} 2 x v L !
P�X u¯(p, y) = L[u(x, y)]. S
L
[
∂2u
∂x∂y
]
= p
∂u¯
∂y
− ∂u
∂y
∣∣∣∣
x=0
= p
∂u¯
∂y
− ∂
∂y
u(0, y) = p
∂u¯
∂y
,
T
p
∂u¯
∂y
= u¯− e
−y
p+ 1
u¯|y = 1
(p+ 1)2
a&
u¯(p, y) =
e−y
(p+ 1)2
,
�3
u(x, y) = xe−(x+y).
����
1. "2 y v L !
P�
2. �;2 x R y ve:
Pja+�
� 3.6 R Laplace
P
aQL4+
∂u
∂t
= a2
∂2u
∂x2
− hu, (x > 0, t > 0), a, h 0e�$
u|x=0 = 0, ∂u
∂x
∣∣∣∣
x=+∞
= 0
u|t=0 = b.
90
Æ} w u¯(p, x) = L[u(t, x)], T
∂2u˜
∂x2
− p+ h
a2
u˜ = − b
a2
u˜|x=0 = 0, ∂u˜
∂x
∣∣∣∣
x=+∞
= 0,
a&
u˜(p, x) =
b
p+ h
(1− e−
q
p+h
a2
x
),
u(t, x) = be−ht − be−htercf
(
x
2a
√
t
)
,
�m
ercf(x) =
2√
pi
∫ +∞
x
e−ξ
2
dξ 0V6�I$.
����
h;R�'75
a�
� 3.7 R�1 F !
P
a�37� ∆3u = −f(x, y, z), 5�Y�0u+
3�
Æ} w û(λ, µ, ν) = F3[u(x, y, z)], &
− (λ2 + µ2 + ν2)û = −f̂(λ, µ, ν),
û =
f̂
ρ2
, ρ2 = λ2 + µ2 + ν2,
u(x, y, z) = F−13
[
f̂
ρ2
]
= f(x, y, z) ∗ F−13
[
1
ρ2
]
,
�m
F−13
[
1
ρ2
]
=
1
(2pi)3
∫∫∫ +∞
−∞
1
ρ2
ei(λx+µy+νz)dλdµdν
v�w�
P�� ν p�\?d r = (x, y, z) 7?�^
λ = ρ sin θ cosϕ, µ = ρ sin θ sinϕ, ν = ρ cos θ,
λx+ µy + νz = ρ · r = ρr cos θ, r2 = x2 + y2 + z2.
T
F−13
[
1
ρ2
]
=
1
(2pi)3
∫ +∞
0
∫ pi
0
∫ 2pi
0
eiρr cos θ sin θdϕdθdρ
=
1
(2pi)2
∫ +∞
0
eiρr cos θ
iρr
∣∣∣∣pi
0
dρ
=
1
2pi2r
∫ +∞
0
sin ρr
ρ
dρ =
1
4pir
.
91
�3
u(x, y, z) =
1
4pi
∫∫∫ +∞
−∞
f(ξ, η, ζ)√
(x− ξ)2 + (y − η)2 + (z − ζ)2 dξdηdζ.
92