Suppose that the equation z = f x , y is expressed in the polar form z = g r , θ by making the substitution x = r cos θ and y = r sin θ . (a) View r and θ as functions of x and y and use implicit differentiation to show that ∂ r ∂ x = cos θ and ∂ θ ∂ x = − sin θ r (b) View r and θ as functions of x and y and use implicit differentiation to show that ∂ r ∂ y = sin θ and ∂ θ ∂ y = cos θ r (c) Use the results in parts (a) and (b) to show that ∂ z ∂ x = ∂ z ∂ r cos θ − 1 r ∂ z ∂ θ = sin θ ∂ z ∂ y = ∂ z ∂ r sin θ + 1 r ∂ z ∂ θ = cos θ (d) Use the result in part (c) to show that ∂ z ∂ x 2 + ∂ z ∂ y 2 = ∂ z ∂ r 2 + 1 r 2 ∂ z ∂ θ 2 (e) Use the result in part (c) to show that if z = f x , y satisfies Laplace’s equation ∂ 2 z ∂ x 2 + ∂ 2 z ∂ y 2 = 0 then z = g r , θ satisfies the equation ∂ 2 z ∂ r 2 + 1 r 2 ∂ 2 z ∂ θ 2 + 1 r ∂ z ∂ r = 0 and conversely. The latter equation is called the polar form of Laplace’s equation.
Suppose that the equation z = f x , y is expressed in the polar form z = g r , θ by making the substitution x = r cos θ and y = r sin θ . (a) View r and θ as functions of x and y and use implicit differentiation to show that ∂ r ∂ x = cos θ and ∂ θ ∂ x = − sin θ r (b) View r and θ as functions of x and y and use implicit differentiation to show that ∂ r ∂ y = sin θ and ∂ θ ∂ y = cos θ r (c) Use the results in parts (a) and (b) to show that ∂ z ∂ x = ∂ z ∂ r cos θ − 1 r ∂ z ∂ θ = sin θ ∂ z ∂ y = ∂ z ∂ r sin θ + 1 r ∂ z ∂ θ = cos θ (d) Use the result in part (c) to show that ∂ z ∂ x 2 + ∂ z ∂ y 2 = ∂ z ∂ r 2 + 1 r 2 ∂ z ∂ θ 2 (e) Use the result in part (c) to show that if z = f x , y satisfies Laplace’s equation ∂ 2 z ∂ x 2 + ∂ 2 z ∂ y 2 = 0 then z = g r , θ satisfies the equation ∂ 2 z ∂ r 2 + 1 r 2 ∂ 2 z ∂ θ 2 + 1 r ∂ z ∂ r = 0 and conversely. The latter equation is called the polar form of Laplace’s equation.
Suppose that the equation
z
=
f
x
,
y
is expressed in the polar form
z
=
g
r
,
θ
by making the substitution
x
=
r
cos
θ
and
y
=
r
sin
θ
.
(a) View r and
θ
as functions of x and y and use implicit differentiation to show that
∂
r
∂
x
=
cos
θ
and
∂
θ
∂
x
=
−
sin
θ
r
(b) View r and
θ
as functions of x and y and use implicit differentiation to show that
∂
r
∂
y
=
sin
θ
and
∂
θ
∂
y
=
cos
θ
r
(c) Use the results in parts (a) and (b) to show that
∂
z
∂
x
=
∂
z
∂
r
cos
θ
−
1
r
∂
z
∂
θ
=
sin
θ
∂
z
∂
y
=
∂
z
∂
r
sin
θ
+
1
r
∂
z
∂
θ
=
cos
θ
(d) Use the result in part (c) to show that
∂
z
∂
x
2
+
∂
z
∂
y
2
=
∂
z
∂
r
2
+
1
r
2
∂
z
∂
θ
2
(e) Use the result in part (c) to show that if
z
=
f
x
,
y
satisfies Laplace’s equation
∂
2
z
∂
x
2
+
∂
2
z
∂
y
2
=
0
then
z
=
g
r
,
θ
satisfies the equation
∂
2
z
∂
r
2
+
1
r
2
∂
2
z
∂
θ
2
+
1
r
∂
z
∂
r
=
0
and conversely. The latter equation is called the polar form of Laplace’s equation.
With integration, one of the major concepts of calculus. Differentiation is the derivative or rate of change of a function with respect to the independent variable.
Need a deep-dive on the concept behind this application? Look no further. Learn more about this topic, calculus and related others by exploring similar questions and additional content below.