How to Use This Section

CBSE Board-pattern questions on Alternating Current by mark value, with model answers in examiner-rewarded phrasing — definitions first, phasor diagrams described, derivations stepwise, units carried. The Board regulars: rms derivation, phase relations for pure L and C with diagrams, the LCR impedance derivation, resonance and its applications, power factor/wattless current, and the transformer long answer.

1-Mark Questions (Definitions & Direct)

Q1. Define the rms value of an alternating current. Answer: It is the square root of the mean of i2i^2 over a cycle — equivalently, the steady (DC) current that would produce the same average heating in a given resistor: I=im/2I = i_m/\sqrt 2.

Q2. What is the phase relation between voltage and current in a pure inductor? Answer: The current lags the voltage by π/2\pi/2 (a quarter cycle).

Q3. Define capacitive reactance and give its SI unit. Answer: XC=1/ωCX_C = 1/\omega C, the effective opposition of a capacitor to AC; SI unit: ohm.

Q4. What is wattless current? Answer: The current in a purely inductive or capacitive circuit (ϕ=90\phi = 90 degrees, cosϕ=0\cos\phi = 0): current flows but no average power is dissipated.

Q5. Write the resonance condition for a series LCR circuit and the resonant frequency. Answer: XL=XCX_L = X_C, giving ω0=1/LC\omega_0 = 1/\sqrt{LC} (i.e. ν0=12πLC\nu_0 = \frac{1}{2\pi\sqrt{LC}}).

Q6. On what principle does a transformer work? Answer: Mutual induction — an alternating flux in the shared core induces emfs in both windings in proportion to their turns.

2-Mark Questions (Short Answer)

Q7. Show that the average power consumed by an ideal inductor over a full cycle is zero. Answer: With v=vmsinωtv = v_m\sin\omega t and i=imsin(ωtπ/2)i = i_m\sin(\omega t - \pi/2), the instantaneous power is p=vi=vmim2sin2ωtp = vi = -\frac{v_mi_m}{2}\sin 2\omega t. Since sin2ωt=0\langle\sin 2\omega t\rangle = 0 over a cycle, Pˉ=0\bar P = 0: energy is alternately stored in and returned by the magnetic field.

Q8. The peak value of the 220 V mains is 311 V. Explain the two numbers. Answer: Specified AC voltages are rms values: V=220V = 220 V. The sinusoidal peak is vm=2V=311v_m = \sqrt 2 V = 311 V. The rms value is quoted because it gives DC-equivalent heating (P=V2/RP = V^2/R).

Q9. Distinguish between resistance and reactance. Answer: Resistance opposes current and dissipates energy (ϕ=0\phi = 0); it is frequency-independent. Reactance (XL=ωLX_L = \omega L or XC=1/ωCX_C = 1/\omega C) opposes AC without average dissipation (voltage and current 90 degrees apart) and depends on frequency.

Q10. Why can a capacitor conduct AC but not steady DC? Answer: On DC (ω=0\omega = 0), XC=1/ωCX_C = 1/\omega C \to \infty: once charged, current stops. On AC the capacitor is alternately charged and discharged each half cycle, so charge flows continuously in the circuit, limited by the finite XCX_C.

Q11. A series LCR circuit is at resonance. What are (i) its impedance, (ii) the phase angle, (iii) the power factor? Answer: (i) Z=RZ = R (minimum); (ii) ϕ=0\phi = 0; (iii) cosϕ=1\cos\phi = 1 — maximum power transfer.

3-Mark Questions (Derivations & Numericals)

Q12. Derive the impedance of a series LCR circuit by the phasor method. Answer: The common current is i=imsin(ωt+ϕ)i = i_m\sin(\omega t + \phi). Voltage phasors: VRV_R (=imR= i_mR) along I; VLV_L (=imXL= i_mX_L) ahead of I by 90 degrees; VCV_C (=imXC= i_mX_C) behind by 90 degrees. VLV_L and VCV_C oppose, combining to imXCimXL|i_mX_C - i_mX_L|. Pythagoras on the phasor sum: vm2=(imR)2+(imXCimXL)2v_m^2 = (i_mR)^2 + (i_mX_C - i_mX_L)^2, so im=vm/Zi_m = v_m/Z with Z=R2+(XCXL)2Z = \sqrt{R^2 + (X_C - X_L)^2} and tanϕ=(XCXL)/R\tan\phi = (X_C - X_L)/R.

Q13. A 15 μ\muF capacitor is connected to a 220 V, 50 Hz source. Find the reactance and the rms and peak currents. Answer: XC=12π(50)(15×106)=212 ΩX_C = \frac{1}{2\pi(50)(15\times10^{-6})} = 212\ \Omega; I=220/212=1.04I = 220/212 = 1.04 A; im=2I=1.47i_m = \sqrt2 I = 1.47 A (current leads by 90 degrees).

Q14. State the condition for resonance and show the current is maximum there. Answer: Resonance: XL=XCX_L = X_C, i.e. ω0=1/LC\omega_0 = 1/\sqrt{LC}. Then Z=R2+0=RZ = \sqrt{R^2 + 0} = R, its minimum; hence im=vm/Z=vm/Ri_m = v_m/Z = v_m/R, the maximum possible. VLV_L and VCV_C, equal and opposite, cancel; the whole source voltage sits across R. Resonance requires both L and C — no RL/RC resonance.

Q15. R = 3 Ω\Omega, XL=8 ΩX_L = 8\ \Omega, XC=4 ΩX_C = 4\ \Omega, source 283 V peak at 50 Hz. Find Z, the rms current and the power dissipated. Answer: Z=9+16=5 ΩZ = \sqrt{9 + 16} = 5\ \Omega; I=283/25=40I = \frac{283/\sqrt2}{5} = 40 A; P=I2R=4800P = I^2R = 4800 W (power factor 0.6, current lagging by 53.1 degrees).

5-Mark Questions (Long Answer)

Q16. (a) With a phasor diagram, obtain the average power of a series LCR circuit and define the power factor. (b) Discuss the cases: pure R, pure L or C, and resonance. (c) Why is low power factor undesirable in power supply? Answer:

  1. (a) With v=vmsinωtv = v_m\sin\omega t, i=imsin(ωt+ϕ)i = i_m\sin(\omega t + \phi): p=vi=vmim2[cosϕcos(2ωt+ϕ)]p = vi = \frac{v_mi_m}{2}[\cos\phi - \cos(2\omega t + \phi)]. The oscillating term averages to zero: P=VIcosϕP = VI\cos\phi. The factor cosϕ=R/Z\cos\phi = R/Z is the power factor.
  2. (b) Pure R: ϕ=0\phi = 0, P=VIP = VI (max). Pure L or C: ϕ=90\phi = 90 degrees, P=0P = 0 — wattless current. Resonance: ϕ=0\phi = 0, P=I2RP = I^2R maximum.
  3. (c) For required power P at voltage V, I=P/(Vcosϕ)I = P/(V\cos\phi): small cosϕ\cos\phi forces large current and I2RI^2R line losses grow as its square. Suppliers therefore require pf near 1 (improved by adding capacitors across inductive loads).

Q17. (a) Describe the construction and working of a transformer and derive vs/vp=Ns/Npv_s/v_p = N_s/N_p. (b) List the sources of energy loss and their remedies. (c) A step-down transformer converts 2200 V to 220 V for a 4.4 kW load. Find the turns ratio and the primary and secondary currents (ideal). Answer:

  1. (a) Primary (NpN_p) and secondary (NsN_s) windings, insulated, on a common soft-iron core. AC in the primary creates an alternating core flux ϕ\phi linking both coils. Faraday: vs=Nsdϕ/dtv_s = -N_s\,d\phi/dt and vp=Npdϕ/dtv_p = -N_p\,d\phi/dt (back emf equals applied voltage for negligible primary resistance). Dividing: vs/vp=Ns/Npv_s/v_p = N_s/N_p. With no losses, ipvp=isvsi_pv_p = i_sv_s.
  2. (b) Flux leakage (wind coils one over the other); winding resistance (thick wire); eddy currents (laminated core); hysteresis (low-hysteresis core material).
  3. (c) Ns/Np=220/2200=1/10N_s/N_p = 220/2200 = 1/10; is=4400/220=20i_s = 4400/220 = 20 A; ip=4400/2200=2i_p = 4400/2200 = 2 A.