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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.
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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 =^
A ϵ 0 Concentric spheres capacitor: V^ =^
a
and E =^
4 π ϵ 0
r 2 Concentric cylinders capacitor: V^ =^
2 π ϵ 0 L ln
b
and E =^
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 =
2 d 2 A ϵ 0 and (^) W =
2 A ϵ 0 2 d Concentric spheres capacitor: W =
2
a
and (^) W =
2 2 π ϵ 0 a b b − a Concentric cylinders capacitor: W^ =^
2 4 π ϵ 0 L
b
and W =
2 π ϵ 0 L
(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 =
2 2 ϵ 0 A 2 Concentric spheres capacitor: w =
2 32 π 2 ϵ 0 r − 4 Concentric cylinders capacitor: w =
2 8 π 2 ϵ 0 L 2 r − 2
2
0
2
2
2
0
4
2
2
0
4
2
2
2
2
2
2
0
2
2