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Principles of Electromagnetism and Optics

Electric Potential and Capacitance

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Electric Potential

Potential is the height map of the electric world: charges roll downhill through voltage the way balls roll downhill through altitude. It is a scalar, much easier to compute than the vector field E\vec{E}.

The electric potential VV is the potential energy per unit charge, defined relative to a reference point:

V=refrEdl,E=VV = -\int_{\text{ref}}^{\vec{r}} \vec{E}\cdot d\vec{l}, \qquad \vec{E} = -\nabla V

For a point charge, the potential of a point charge is given by:

V=keQrV = k_e\frac{Q}{r}

ConceptFormula
Potential energyU=qVU = qV
Work by fieldW=q(VAVB)W = q(V_A - V_B)
Equipotential surfacesV=constV = \text{const}, \perp to E\vec{E}

Capacitance & Pitfalls

Capacitance measures how a device stores charge and energy at a given voltage:

C=QV,U=12CV2=Q22CC = \frac{Q}{V}, \qquad U = \frac{1}{2}CV^2 = \frac{Q^2}{2C}

For a parallel-plate capacitor, geometry dictates capacity:

C=ε0AdC = \varepsilon_0\frac{A}{d}

Combine capacitors using these rules:

ConnectionFormula
ParallelCeq=C1+C2C_{\text{eq}} = C_1 + C_2
Series1Ceq=1C1+1C2\dfrac{1}{C_{\text{eq}}} = \dfrac{1}{C_1} + \dfrac{1}{C_2}
Common pitfall: Zero potential does not mean zero field, and zero field does not mean zero potential. The field is the slope of VV; midway between two equal positive charges the field vanishes while the potential remains large.
Placeholder: Electric Potential and Capacitance

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Principles of Electromagnetism and Optics