• Champ électrique total (d. volumique)

    \[ \iiint_{P\in\mathcal{v}} \frac{\rho_c(P)\mathrm{d} \mathcal{v}(P)\vec{PM}}{4\pi\epsilon_0 \norm{PM}^3}\]

  • Potentiel total (d. volumique)

    \[ \iiint_{P\in \mv} \frac{\rho_c \dd \mv(P)}{4\pi\epsilon_0 \norm{PM}}\]

  • Champ électrique total (d. surfacique)

    \[\\iint_{P\in S} \frac{\sigma(P)\dd S(P)\vec{PM}}{4\pi\epsilon_0 \norm{PM}^3}\]

  • Potentiel total (d. surfacique)

    \[ \iint_{P\in S} \frac{\sigma \dd S(P)}{4\pi\epsilon_0 \norm{PM}}\]

  • Champ électrique total (d. linéique)

    \[\int_{P\in C} \frac{\lambda(P)\dd S(P)\vec{PM}}{4\pi\epsilon_0 \norm{PM}^3}\]

  • Potentiel total (d. linéique)

    \[ \int_{P\in C} \frac{\lambda \dd S(P)}{4\pi\epsilon_0 \norm{PM}}\]