1/27
Looks like no tags are added yet.
Mutual inductance M
M = N₂Φ₂₁/I₁ = N₁Φ₁₂/I₂ — coupling between two nearby circuits
Mutually induced emf
ℰ₂ = −M dI₁/dt ; ℰ₁ = −M dI₂/dt
Self-inductance L
Emf induced in a circuit by its own changing current: ℰ = −L dI/dt ; L = NΦ_B / I
Unit of inductance
Henry (H) = 1 V·s/A
Inductor
Circuit element that provides self-inductance; opposes CHANGES in current
Self-inductance of a solenoid
L = μ₀N²A / l
Energy stored in an inductor
U = ½LI²
Energy density of a magnetic field
u_B = B² / (2μ₀)
RL circuit time constant
τ_L = L/R
RL current growth (switch closed)
I(t) = (ℰ/R)(1 − e^(−t/τ_L))
RL current decay
I(t) = I₀ e^(−t/τ_L)
Voltage across inductor while current grows
V_L = ℰ e^(−t/τ_L) (equals ℰ at t = 0, → 0 as t → ∞)
Inductor at t = 0 vs t → ∞ (DC)
t = 0: acts like an open circuit (I = 0); t → ∞: acts like a plain wire
Large vs small τ_L
Large τ_L → current changes slowly; small τ_L → current changes quickly
LC circuit equation
Q/C + L dI/dt = 0
LC charge solution
Q(t) = Q_max cos(ωt + φ)
LC angular frequency
ω = 1/√(LC)
Phase between charge and current in LC
90° out of phase — when Q is max, I = 0 and vice versa
LC energy
Energy sloshes between capacitor (Q²/2C, electric) and inductor (½LI², magnetic); total is conserved
Voltage across inductor in LC at t = 0 (capacitor full)
V_L = Q_max / C
Inductor as a mechanical analogy
Like mass (inertia)/spring — stores energy and gives it back without loss
RLC circuit
Like LC, but resistor dissipates energy → damped oscillations
RLC charge (underdamped)
Q(t) = Q_max e^(−γt) cos(ω′t + φ)
Damping factor γ
γ = R / (2L); how fast oscillations die out
Damped oscillation frequency
ω′² = ω₀² − γ², with ω₀ = 1/√(LC)
Bandwidth (RLC)
Δω = R/L — range of frequencies near resonance where the circuit responds strongly
Quality factor Q
Q = (1/R)√(L/C) = ω₀/Δω — sharpness of the resonance
Applications of LC / RL / RLC circuits
LC: radio tuning, signal generators, filters; RL: metal detectors; RLC: MRI