Salam Academy
Paper 4 · Module

Electric fields

3 subtopics≈ 110 min in total
  1. Electric fields and uniform fields

    An electric field is a region where a charge experiences a force. Field strength is the force per unit positive charge: E=FqE=\dfrac Fq (N C⁻¹ or V m⁻¹). Between parallel plates with p.d. VV and separation dd, the field is uniform: E=VdE=\dfrac Vd. A charged particle in a uniform field feels a constant force qEqE, so it accelerates uniformly and, if it enters at right angles, follows a parabola like a projectile.

    ≈ 35 min
  2. Coulomb's law

    Two point charges exert forces on each other proportional to the product of the charges and inversely proportional to the square of their separation: F=Q1Q24πε0r2F=\dfrac{Q_1Q_2}{4\pi\varepsilon_0r^2}, with ε0=8.85×10−12\varepsilon_0=8.85\times10^{-12} F m⁻¹. Like charges repel; unlike attract. A point charge (or charged sphere, from outside) creates a radial field E=Q4πε0r2E=\dfrac Q{4\pi\varepsilon_0r^2}. Fields from several charges add as vectors.

    ≈ 35 min
  3. Electric potential

    Electric potential at a point is the work done per unit positive charge bringing a small test charge from infinity: V=Q4πε0rV=\dfrac Q{4\pi\varepsilon_0r}. Unlike gravitational potential, it can be positive (near a positive charge) or negative. A charge qq at that point has potential energy EP=qV=Qq4πε0rE_P=qV=\dfrac{Qq}{4\pi\varepsilon_0r}. Field strength is minus the potential gradient, E=−ΔVΔrE=-\dfrac{\Delta V}{\Delta r}, so field lines cross equipotentials at right angles.

    ≈ 40 min