How energy is stored in electric fields and the devices that store charge
In previous chapters, we studied the notion of potential energy and the work-energy theorem. In this chapter, we extend these ideas to electric charges. The concept of electric potential energy and electric potential helps us understand how energy is stored in electric fields and how capacitors work.
The electric potential at a point is the work done per unit positive charge in bringing a test charge from infinity to that point without acceleration:
For an electric dipole with charges ±q separated by distance 2a:
Surfaces where the potential is the same at every point. Key properties:
Capacitance is the ability of a system to store charge per unit potential difference:
The most common capacitor: two parallel conducting plates separated by distance d:
Inserting a dielectric (insulator) between plates increases capacitance by factor κ. The dielectric gets polarized, creating an internal field that opposes the external field, reducing net field and allowing more charge storage.
1/C = 1/C₁ + 1/C₂ + ...
Total capacitance is less than smallest. Same charge on each, voltages add.
C = C₁ + C₂ + ...
Total capacitance is sum of all. Same voltage across each, charges add.
The energy is not stored on the plates but in the electric field between them. The energy density (energy per unit volume) is u = ½ε₀E², showing that stronger fields store more energy.