Class 12 Physics Chapter 7: Alternating Current

CBSE 2026–27 | NCERT-aligned free notes, diagrams, examples and practice

Alternating current changes magnitude and direction periodically. The chapter develops RMS and average values, AC through resistors, inductors and capacitors, phasors, series LCR circuits, resonance, power and transformers.

1. AC Voltage and Current

A sinusoidal voltage may be written v = Vm sinωt. The angular frequency is ω = 2πf. For a pure resistor, current is in phase with voltage.

Voltage: Vm sinωt
Current in R: Im sinωt
R: V and I in phase

2. RMS Value

For a sinusoidal current, Irms = Im/√2 and Vrms = Vm/√2. RMS values are used for practical AC power calculations.

3. AC Through R, L and C

Component Reactance Phase relation
R R V and I in phase
L XL = ωL Current lags voltage by 90°
C XC = 1/(ωC) Current leads voltage by 90°

4. Series LCR Circuit

Impedance Z = √[R² + (XL − XC)²]. Current Irms = Vrms/Z. The phase angle satisfies tanφ = (XL − XC)/R.

R ── L ── C in series
XL ↑ with frequency   |   XC ↓ with frequency
At resonance: XL = XC

5. Resonance

For a series LCR circuit, resonance occurs at ω0 = 1/√LC. At resonance, impedance is minimum and current is maximum for the ideal series circuit. The circuit behaves as resistive with φ = 0.

6. AC Power

Average power P = VrmsIrmscosφ. The factor cosφ is the power factor. A purely inductive or purely capacitive ideal circuit has zero average power.

7. Transformer

An ideal transformer uses mutual induction to change AC voltage. Vs/Vp = Ns/Np. A step-up transformer has more secondary turns; a step-down transformer has fewer.

AC input → primary coil ║ iron core ║ secondary coil → AC output
Vs/Vp = Ns/Np

Worked Example

For a 230 V RMS supply, peak voltage is Vm = √2×230 ≈ 325 V.

Common Exam Traps

  • Do not confuse peak and RMS values.
  • Inductor: current lags; capacitor: current leads.
  • At series resonance, XL equals XC, not both equal zero.
  • Power factor is cosφ, not φ itself.

Practice Questions

  1. Explain RMS value and derive the relation with peak value.
  2. Compare AC behaviour of R, L and C.
  3. Derive impedance of a series LCR circuit.
  4. Explain resonance and its condition.
  5. Describe transformer operation and voltage ratio.

📌 Concept Diagram: Series LCR Circuit

RLCZ = √[R² + (Xₗ − Xc)²]VVᵣPhasor idea

Real-Life Connection

AC circuits are not only about calculations. The phase relation between voltage and current affects power transfer, motor operation and the efficiency of electrical systems. A low power factor means more current is required for the same useful power.

Application Questions

  1. Why does a capacitor offer lower reactance at higher frequency?
  2. Explain why current becomes maximum at series resonance.
  3. A circuit has Vrms = 100 V, R = 20 Ω and is at resonance. Find the current.
  4. Why cannot an ordinary transformer operate directly with steady DC?

AC Circuit Visuals & Numericals

Series LCR Circuit

AC source → R → L → C → return
Z = √[R² + (XL−XC)²]

Inductive reactance XL=ωL and capacitive reactance XC=1/(ωC). At resonance XL=XC, so the impedance of a series LCR circuit is minimum and current is maximum.

Worked Numerical

If R=10 Ω, XL=8 Ω and XC=4 Ω, Z=√(100+16)=√116≈10.77 Ω.

Transformer

For an ideal transformer, Vs/Vp=Ns/Np. A step-up transformer has more secondary turns; a step-down transformer has fewer.

Power Factor

For an AC circuit, average power is P=VrmsIrmscosφ. Power factor indicates how effectively apparent power is converted into useful average power.

Practice

  1. Calculate rms values.
  2. Find impedance of a series LCR circuit.
  3. Determine resonance frequency.
  4. Solve transformer turns-ratio problems.
  5. Explain the role of power factor.

Common Mistakes to Avoid

  • Confusing rms and peak values.
  • Using resistance instead of impedance in an AC circuit.
  • Forgetting the resonance condition XL=XC.

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