Summary of electromagnetism formulae (ch. 13–15, 17–19). Derivations and limits of validity are in the respective chapters.

Coulomb’s law F=kq1q2r2F = k\,\frac{q_1 q_2}{r^2}

Field and potential (point charge) E=kQr2V=kQrE = k\,\frac{Q}{r^2} \qquad V = k\,\frac{Q}{r}

Capacitor C=QVC=ε0Ad (piano)EC=12CV2C = \frac{Q}{V} \qquad C = \frac{\varepsilon_0 A}{d}\ \text{(piano)} \qquad E_C = \tfrac12 C V^2

Ohm’s law and power V=RiP=ViV = Ri \qquad P = Vi

Resistors in series and parallel Rs=R1+R21Rp=1R1+1R2R_s = R_1 + R_2 \qquad \frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2}

Lorentz force F=qv×B\pq{F} = q\,\pq{v}\times\pq{B}

Magnetic field of sources B=μ0i2πr (filo)B=μ0iN (solenoide)B = \frac{\mu_0 i}{2\pi r}\ \text{(filo)} \qquad B = \frac{\mu_0 i N}{\ell}\ \text{(solenoide)}

Faraday-Neumann-Lenz law

ΓE=ddtΦB\Gamma_E = -\ddt{\Phi_B}

Maxwell’s equations in integral form: see the formula sheet in ch. 19.

Topics: Electrostatics · Electric circuits · Magnetism · Electromagnetic induction

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