(a) Show that when Laplace’s equation ∂ 2 u ∂ x 2 + ∂ 2 u ∂ y 2 + ∂ 2 u ∂ z 2 = 0 is written in cylindrical coordinates, it becomes ∂ 2 u ∂ r 2 + 1 r ∂ u ∂ r + 1 r 2 ∂ 2 u ∂ θ 2 + ∂ 2 u ∂ z 2 = 0 (b) Show that when Laplace’s equation is written in spherical coordinates, it becomes ∂ 2 u ∂ ρ 2 + 2 ρ ∂ u ∂ ρ + cot ϕ ρ 2 ∂ u ∂ ϕ + 1 ρ 2 sin 2 ϕ ∂ 2 u ∂ θ 2 = 0
(a) Show that when Laplace’s equation ∂ 2 u ∂ x 2 + ∂ 2 u ∂ y 2 + ∂ 2 u ∂ z 2 = 0 is written in cylindrical coordinates, it becomes ∂ 2 u ∂ r 2 + 1 r ∂ u ∂ r + 1 r 2 ∂ 2 u ∂ θ 2 + ∂ 2 u ∂ z 2 = 0 (b) Show that when Laplace’s equation is written in spherical coordinates, it becomes ∂ 2 u ∂ ρ 2 + 2 ρ ∂ u ∂ ρ + cot ϕ ρ 2 ∂ u ∂ ϕ + 1 ρ 2 sin 2 ϕ ∂ 2 u ∂ θ 2 = 0
Solution Summary: The author explains the Laplace equation in cylindrical coordinates. The spherical coordinate is (r,theta,z).
(a) Show that when Laplace’s equation
∂
2
u
∂
x
2
+
∂
2
u
∂
y
2
+
∂
2
u
∂
z
2
=
0
is written in cylindrical coordinates, it becomes
∂
2
u
∂
r
2
+
1
r
∂
u
∂
r
+
1
r
2
∂
2
u
∂
θ
2
+
∂
2
u
∂
z
2
=
0
(b) Show that when Laplace’s equation is written in spherical coordinates, it becomes
∂
2
u
∂
ρ
2
+
2
ρ
∂
u
∂
ρ
+
cot
ϕ
ρ
2
∂
u
∂
ϕ
+
1
ρ
2
sin
2
ϕ
∂
2
u
∂
θ
2
=
0
4. Use method of separation of variable to solve the following wave equation
მłu
J²u
subject to
u(0,t) =0, for t> 0,
u(л,t) = 0, for t> 0,
=
t> 0,
at²
ax²'
u(x, 0) = 0,
0.01 x,
ut(x, 0) =
Π
0.01 (π-x),
0
Solve the following heat equation by method of separation variables:
ди
=
at
subject to
u(0,t) =0, for
-16024
ძx2 •
t>0, 0 0,
ux (4,t) = 0, for
t> 0,
u(x, 0) =
(x-3,
\-1,
0 < x ≤2
2≤ x ≤ 4.
ex
5.
important aspects.
Graph f(x)=lnx. Be sure to make your graph big enough to easily read (use the space given.) Label all
6
33
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