a) ε is φ ahead of i because i and R are in phase and i.e., −Z and ε are in phase as ε = ε₀sin wt from diagram i = ε₀ −Zsin(ωt − φ) where, φ = tan⁻¹ XLR
b) i = 1.0A (given)
VR = 160V = iR ⇒ R = 160/1 = 160
VL = 120V = iXL ⇒ XL = 120/1 = 120
Vnet = √(VR² + VL²) = √(160)² + (120)² = √25600 + 14400 = 200: effective value of applied voltage
Z = √(R² + XL²) = √(160)² + (120)² = 200: Impedance
C) When direct current is passed through the circuit then XL will be zero (at ω = 0, inductor will act as a plane wire) and potential drop will only occur at R (i.e., i = ε/R)
For intermediate time E = iR + L(di/dt) where i will vary accordingly