Changing magnetic flux Φ_B through a circuit induces emf according to Faraday’s law ε = −dΦ_B/dt; the minus sign (Lenz’s law) ensures the induced current opposes the change. Motional emf ε = Bℓv arises when a conductor moves in a field. Self-inductance L and mutual inductance M relate flux and current (ε = −L dI/dt, ε₂ = −M dI₁/dt). In AC, inductors and capacitors introduce reactances X_L = ωL and X_C = 1/(ωC), while LR/LC circuits have characteristic time and frequency scales τ_L = L/R and ω = 1/√(LC).
Induction & AC calculators
Faraday/flux, motional emf, inductance, AC reactance, LR/LC
📈 EMI & AC graph
Faraday’s law, flux & motional emf
| Concept | Formula | Notes |
|---|---|---|
| Magnetic flux | Φ_B = B A cos θ | Wb (weber), θ angle between B and normal |
| Faraday’s law | ε = − dΦ_B/dt, ε = −N dΦ_B/dt | Induced emf; minus sign = Lenz’s law |
| Motional emf (rod) | ε = B ℓ v | v ⊥ B, ℓ length in field |
| Rotating rod/disk | ε = ½ B ω L² (rod), ε = ½ B ω R² (disk) | Between center and rim |
Inductance, AC reactance, LR & LC
| Concept | Formula | Notes |
|---|---|---|
| Self-inductance | L = Φ/I, ε = −L dI/dt | U = ½ L I² |
| Solenoid inductance | L = μ₀ n² A l | n = turns per unit length |
| Mutual inductance | M = Φ₂₁/I₁, ε₂ = −M dI₁/dt, M = k√(L₁L₂) | 0 ≤ k ≤ 1 (coupling) |
| AC reactance | X_L = 2πfL, X_C = 1/(2πfC) | Inductive: V leads I; capacitive: I leads V |
| RLC impedance | |Z| = √(R² + (X_L − X_C)²) | Series RLC |
| LR time constant | τ_L = L / R | I(t) growth: I = (ε/R)(1 − e^{−t/τ_L}) |
| LC oscillator | ω = 1/√(LC), T = 2π√(LC) | Energy oscillates between L and C |
About this induction & AC tool
This page brings together the core electromagnetic induction formulas needed for school physics, JEE, and NEET: Faraday’s law and flux, motional emf for rods and rotating systems, self and mutual inductance, AC reactance for R–L–C elements, and LR/LC transients. Each calculator is paired with a step-by-step derivation so you can connect the equations to the physical picture.