The proportionality constant between magnetic flux and current, measured in Henries (H). $\Phi_B = LI$

A coil of wire that resists changes in current and stores energy in a magnetic field.

A measure of the amount of magnetic field lines passing through a given area.

The time it takes for the current in an LR circuit to reach approximately 63.2% of its maximum value. $\tau = L/R$

The rate at which energy oscillates between the capacitor and inductor in an LC circuit. $\omega = \frac{1}{\sqrt{LC}}$

The electromotive force generated in a circuit due to a changing magnetic field. $\varepsilon = -L \frac{dI}{dt}$

A coil of wire that resists changes in current and stores energy in a magnetic field.

The proportionality constant between magnetic flux and current: $\Phi_B = LI$.

Henry (H)

The voltage generated in an inductor due to a changing current, opposing the change: $\varepsilon = -L \frac{dI}{dt}$.

The time it takes for the current in an LR circuit to reach approximately 63.2% of its maximum value: $\tau = \frac{L}{R}$.

The rate at which energy oscillates between the capacitor and inductor in an LC circuit: $\omega = \frac{1}{\sqrt{LC}}$.

Inductor: Stores energy in a magnetic field, resists changes in current. Capacitor: Stores energy in an electric field, resists changes in voltage.

LR Circuit: Contains inductor and resistor, current changes exponentially. LC Circuit: Contains inductor and capacitor, energy oscillates between them sinusoidally.

Inductor: $U = \frac{1}{2}LI^2$ (magnetic field). Capacitor: $U = \frac{1}{2}CV^2$ (electric field).

Inductor: Acts like an open circuit initially. Capacitor: Acts like a short circuit initially.

Inductor: Acts like a wire (short circuit) after a long time. Capacitor: Acts like an open circuit after a long time.