$\Delta V = V_B - V_A = -\int_A^B \vec{E}\cdot d\vec{l}$
$V_{pt} = \frac{k q}{r}, \quad U_{pt} = \frac{k q_1 q_2}{r}$
$\Delta U = q \Delta V, \quad W_{\text{field}} = -\Delta U$
$\vec{E} = -\vec{\nabla} V = -\left(\frac{\partial V}{\partial x}\hat{i} + \frac{\partial V}{\partial y}\hat{j} + \frac{\partial V}{\partial z}\hat{k}\right)$
$V(x) = k \int \frac{dq}{r}$
$C = \frac{Q}{V}, \quad C_0 = \frac{\varepsilon_0 A}{d}, \quad C = \kappa C_0$
$C_{\text{parallel}} = \sum C_i, \quad \frac{1}{C_{\text{series}}} = \sum \frac{1}{C_i}$
$U_C = \frac{1}{2} C V^2 = \frac{Q^2}{2C} = \frac{1}{2} Q V$
$u_E = \frac{1}{2}\varepsilon_0 E^2, \quad E = \frac{E_0}{\kappa}$
$\varepsilon_0 = 8.854 \times 10^{-12}\text{ C}^2/(\text{N}\cdot\text{m}^2)$
$I = \frac{dQ}{dt} = n q v_d A, \quad \vec{J} = \sigma \vec{E} = \frac{\vec{E}}{\rho}$
$R = \frac{\rho L}{A}, \quad V = IR, \quad P = IV = I^2 R = \frac{V^2}{R}$
$\sum I_{\text{in}} = \sum I_{\text{out}}, \quad \sum \Delta V = 0$
$R_{\text{series}} = \sum R_i, \quad \frac{1}{R_{\text{parallel}}} = \sum \frac{1}{R_i}$
RC Charge: $q(t) = C\mathcal{E}(1 - e^{-t/\tau}), \quad \tau = RC$
RC Discharge: $q(t) = Q_0 e^{-t/\tau}, \quad I(t) = -\frac{Q_0}{\tau}e^{-t/\tau}$