Quick Recap — Advanced Electrostatics (Multi-step)

  • Charge sharing / redistribution: common potential V=C1V1+C2V2C1+C2V=\dfrac{C_1V_1+C_2V_2}{C_1+C_2}; heat lost =12C1C2C1+C2(V1V2)2=\dfrac12\dfrac{C_1C_2}{C_1+C_2}(V_1-V_2)^2.
  • Coalescing drops: nn drops (radius rr, potential VV) \to one drop of V=n2/3VV'=n^{2/3}V (since R=n1/3rR=n^{1/3}r, Q=nqQ=nq).
  • Uniformly charged solid sphere: inside E=kQrR3E=\dfrac{kQr}{R^3}, Vcentre=3kQ2R=1.5VsurfaceV_{centre}=\dfrac{3kQ}{2R}=1.5\,V_{surface}; self-energy 3kQ25R\dfrac{3kQ^2}{5R}.
  • Concentric shells (+q+q at aa, q-q at b>ab>a): outside field =0=0; Va=kq ⁣(1a1b)V_a=kq\!\left(\dfrac1a-\dfrac1b\right).
  • Slab of thickness d/2d/2 (full area): C=2KK+1C0C=\dfrac{2K}{K+1}C_0. Touching identical spheres share charge equally: new charges q1+q22\dfrac{q_1+q_2}{2} each.

Worked mini-example. +q+q and 3q-3q attract with force F=kq(3q)r2F=\dfrac{k\,q(3q)}{r^2}. Touched together they share net charge 2q-2q, i.e. q-q each; returned to distance rr the force is kq2r2=F3\dfrac{k\,q^2}{r^2}=\dfrac{F}{3}, now repulsive.