If U =U(x, y ) is converted to polar coordinates to become U =U(r, θ) one can
treat r=r(x, y )and θ=θ(x, y )to calculate the following derivatives of Uwith respect
xand y
∂U
∂x
=∂U
∂r
∂r
∂x
+∂U
∂θ
∂θ
∂x
∂^2 U
∂x^2 =
∂U
∂r
∂^2 r
∂x^2 +
∂r
∂x
[
∂^2 U
∂r^2
∂r
∂x +
∂^2 U
∂r ∂θ
∂θ
∂x
]
+
∂U
∂θ
∂^2 θ
∂x^2 +
∂θ
∂x
[
∂^2 U
∂θ ∂r
∂r
∂x +
∂^2 U
∂θ^2
∂θ
∂x
]
(12 .57)
and
∂U
∂y
=∂U
∂r
∂r
∂y
+∂U
∂θ
∂θ
∂y
∂^2 U
∂y^2 =
∂U
∂r
∂^2 r
∂y^2 +
∂r
∂x
[
∂^2 U
∂r^2
∂r
∂y +
∂^2 U
∂r ∂θ
∂θ
∂y
]
+
∂U
∂θ
∂^2 θ
∂y^2 +
∂θ
∂y
[
∂^2 U
∂θ ∂r
∂r
∂y +
∂^2 U
∂θ^2
∂θ
∂y
]
(12 .58)
The transformation equations from rectangular to polar coordinates is performed
using the transformation equations
x=rcos θ and y=rsin θ (12 .59)
One can solve for rand θin terms of xand y to obtain
r^2 =x^2 +y^2 and tan θ=
y
x
(12 .60)
Differentiate the equations (12.60) with respect to xand show
2 r
∂r
∂x = 2x and sec
(^2) θ∂θ
∂x =−
y
x^2 (12 .61)
which simplifies using the transformation equations (12.59) to the values
∂r
∂x
= cos θ and ∂θ
∂x
=−sin θ
r
(12 .62)
Differentiate the the equations (12.60) with respect to yand show
2 r∂r
∂y
= 2y and sec^2 θ∂θ
∂y
=^1
x
(12 .63)
Use the transformation equations (12.59) and simplify the equations (12.63) and
show
∂r
∂y = sin θ and
∂θ
∂y =
cos θ
r (12 .64)