Inductors store energy in a magnetic field; capacitors store energy in an electric field.

LR circuit time constant: $\tau = L/R$. LC circuit angular frequency: $\omega = \frac{1}{\sqrt{LC}}$

Initially, an inductor acts like an open circuit, while a capacitor acts like a short circuit.

Inductor: $U = \frac{1}{2}LI^2$. Capacitor: $U = \frac{1}{2}CV^2$

LR circuits exhibit exponential current changes; LC circuits exhibit sinusoidal oscillations.

An induced EMF is generated, opposing the change in current.

The current increases exponentially towards a maximum value, determined by the time constant.

The current decreases exponentially to zero, determined by the time constant.

Energy oscillates between the capacitor and inductor, leading to sinusoidal oscillations in charge and current.

The energy stored is quadrupled (since $U = \frac{1}{2}LI^2$).

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: $\omega = \frac{1}{\sqrt{LC}}$.