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Electrostatic Energy and Energy Density in Capacitor Geometries, Provas de Física

The solution to problem 1.8 from dr. Christopher s. Baird's university of massachusetts lowell course, which involves calculating the total electrostatic energy and energy density for three different capacitor geometries: parallel plates, concentric spheres, and concentric cylinders. The equations for potential difference, electric field, and energy density.

Tipologia: Provas

2016

Compartilhado em 28/04/2016

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Jackson 1.8 Homework Problem Solution
Dr. Christopher S. Baird
University of Massachusetts Lowell
PROBLEM:
(a) For the three capacitor geometries in Problem 1.6 calculate the total electrostatic energy and express
it alternatively in terms of the equal and opposite charges Q and -Q placed on the conductors and the
potential difference between them.
(b) Sketch the energy density of the electrostatic field in each case as a function of the appropriate
linear coordinate.
SOLUTION:
(a) For a simple capacitor, the total energy is given by W = ½QV. In problem 1.6, we found the
following results.
Parallel plates capacitor:
V=Q d
Aϵ0
and
E=Q
Aϵ0
Concentric spheres capacitor:
V=Q
4π ϵ0
(
1
a1
b
)
and
E=1
4πϵ0
Q
r2
Concentric cylinders capacitor:
V=Q
2πϵ0Lln
(
b
a
)
and
E=Q
2πrϵ0L
It is straight-forward to substitute these equations into the energy equation and find the following:
Parallel plates capacitor:
W=Q2d
2Aϵ0
and
W=V2Aϵ0
2d
Concentric spheres capacitor:
and
W=V22πϵ0a b
ba
Concentric cylinders capacitor:
W=Q2
4π ϵ0Lln
(
b
a
)
and
W=V2π ϵ0L
ln
(
b/a
)
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Jackson 1.8 Homework Problem Solution

Dr. Christopher S. Baird University of Massachusetts Lowell PROBLEM: (a) For the three capacitor geometries in Problem 1.6 calculate the total electrostatic energy and express it alternatively in terms of the equal and opposite charges Q and - Q placed on the conductors and the potential difference between them. (b) Sketch the energy density of the electrostatic field in each case as a function of the appropriate linear coordinate. SOLUTION: (a) For a simple capacitor, the total energy is given by W = ½ QV. In problem 1.6, we found the following results. Parallel plates capacitor: V^ =^ Q d A ϵ 0 and E =^

Q

A ϵ 0 Concentric spheres capacitor: V^ =^

Q

a

b )^

and E =^

4 π ϵ 0

Q

r 2 Concentric cylinders capacitor: V^ =^

Q

2 π ϵ 0 L ln

b

a )^

and E =^

Q

2 π r ϵ 0 L It is straight-forward to substitute these equations into the energy equation and find the following: Parallel plates capacitor: W =

Q

2 d 2 A ϵ 0 and (^) W =

V

2 A ϵ 0 2 d Concentric spheres capacitor: W =

Q

2

a

b )^

and (^) W =

V

2 2 π ϵ 0 a b ba Concentric cylinders capacitor: W^ =^

Q

2 4 π ϵ 0 L

ln(

b

a )^

and W =

V

2 π ϵ 0 L

ln ( b / a )

(b) The energy density is defined as w =^ ϵ 0 2 E (^2). A simple substitution of the fields found in problem 1. reveals: Parallel plates capacitor: w =

Q

2 2 ϵ 0 A 2 Concentric spheres capacitor: w =

Q

2 32 π 2 ϵ 0 r − 4 Concentric cylinders capacitor: w =

Q

2 8 π 2 ϵ 0 L 2 r − 2

z

w

d

Q

2

0

A

2

z

w

0 a

Q

2

2

0

a

4

b

Q

2

2

0

b

4

z

w

a

Q

2

2

ε 0 L

2

a

2

b

Q

2

2

0

L

2

b

2