Alternating Current is Chapter 7 of CBSE Class 12 Physics. This chapter covers AC circuits containing resistors, inductors, and capacitors (RLC circuits), the concept of impedance, resonance, power in AC circuits, and transformers. Understanding AC is essential since household electricity in India is AC at 220 V, 50 Hz.
This chapter carries 5–7 marks. LCR circuit analysis, resonance, transformer problems, and power factor are commonly tested.
Key Concepts
1. Alternating Current Basics
An alternating current changes direction periodically. It is described as:
I = I₀ sin ωt and V = V₀ sin ωt
where I₀, V₀ are peak values and ω = 2πf (angular frequency).
RMS (Root Mean Square) Values
The effective or DC-equivalent values used for AC calculations:
Irms = I₀/√2 ≈ 0.707 I₀
Vrms = V₀/√2 ≈ 0.707 V₀
Household AC: Vrms = 220 V → V₀ = 220√2 ≈ 311 V
2. AC Through Pure Components
| Component | Impedance | Phase Relation |
|---|---|---|
| Resistor (R) | R | V and I are in phase |
| Inductor (L) | XL = ωL = 2πfL | V leads I by 90° (π/2) |
| Capacitor (C) | XC = 1/(ωC) = 1/(2πfC) | I leads V by 90° (π/2) |
XL = inductive reactance; XC = capacitive reactance (both in Ω)
3. Series LCR Circuit
Impedance: Z = √[R² + (XL − XC)²]
Current: I = V/Z
Phase angle: tan φ = (XL − XC)/R
- If XL > XC: circuit is inductive (V leads I)
- If XC > XL: circuit is capacitive (I leads V)
- If XL = XC: resonance (purely resistive)
Resonance
At resonance: XL = XC → ωL = 1/(ωC)
Resonant frequency: f₀ = 1/(2π√LC)
At resonance: Z = R (minimum impedance), I = V/R (maximum current)
Quality Factor (Q)
Q = ωL/R = 1/(ωCR) = (1/R)√(L/C)
Higher Q → sharper resonance peak → more selective tuning
4. Power in AC Circuits
P = VrmsIrms cos φ
where cos φ is the power factor.
| Circuit | Power Factor | Power |
|---|---|---|
| Pure R | cos φ = 1 | P = VI (maximum) |
| Pure L or C | cos φ = 0 | P = 0 (wattless current) |
| LCR at resonance | cos φ = 1 | P = V²/R (maximum) |
5. Transformer
A device that changes AC voltage from one level to another using mutual induction.
Vs/Vp = Ns/Np = Ip/Is (for ideal transformer)
- Step-up: Ns > Np → voltage increases, current decreases
- Step-down: Ns < Np → voltage decreases, current increases
- Efficiency: η = (output power)/(input power) × 100%. Ideal transformer: η = 100%
Energy Losses in Transformer
- Copper loss: I²R heating in coils → use thick copper wires
- Iron/core loss: Eddy currents in core → use laminated core
- Hysteresis loss: Energy to magnetise/demagnetise core each cycle → use soft iron
- Flux leakage: Not all flux links both coils → use close winding
Solved Examples
Example 1
A series LCR circuit has R = 100 Ω, L = 0.5 H, C = 10 μF connected to 200 V, 50 Hz. Find impedance and current.
Answer: XL = 2π × 50 × 0.5 = 157 Ω. XC = 1/(2π × 50 × 10⁻⁵) = 318 Ω.
Z = √[100² + (157 − 318)²] = √[10000 + 25921] = √35921 = 189.5 Ω
I = V/Z = 200/189.5 = 1.06 A
Example 2
Find the resonant frequency for L = 0.1 H and C = 100 μF.
Answer: f₀ = 1/(2π√LC) = 1/(2π√(0.1 × 10⁻⁴)) = 1/(2π × 3.16 × 10⁻³) = 50.3 Hz
Example 3
A transformer with 500 primary turns and 50 secondary turns is connected to 220 V AC. Find the output voltage.
Answer: Vs = Vp × Ns/Np = 220 × 50/500 = 22 V (step-down)
Important Questions for Board Exams
1-Mark
- What is the power factor of a pure inductor?
- What is resonance in an LCR circuit?
3-Mark
- Derive the expression for impedance of a series LCR circuit.
- What is a transformer? Explain its working with a diagram.
- What is resonance? Derive the condition and resonant frequency for a series LCR circuit.
5-Mark
- Explain the working of a series LCR circuit. Derive expressions for impedance and resonant frequency. What is the Q factor?
Quick Revision Points
- AC: I = I₀ sin ωt; Irms = I₀/√2; Vrms = V₀/√2
- XL = ωL (V leads I by 90°); XC = 1/(ωC) (I leads V by 90°)
- LCR: Z = √[R² + (XL − XC)²]; tan φ = (XL − XC)/R
- Resonance: XL = XC; f₀ = 1/(2π√LC); Z = R (min); I = max
- Power: P = VIcos φ; pure L or C → P = 0 (wattless)
- Transformer: Vs/Vp = Ns/Np; losses: copper, iron, hysteresis, flux leakage
Previous: Ch 6 — Electromagnetic Induction
Next: Ch 8 — Electromagnetic Waves
Chapter Navigation
Previous: Electromagnetic Induction Class 12 Notes
Next: Electromagnetic Waves Class 12 Notes
Related Chapters in Class 12 Physics
- Electromagnetic Induction Class 12 Notes
- Moving Charges and Magnetism Class 12 Notes
- Electromagnetic Waves Class 12 Notes
Practice What You Learned
Test yourself with our JEE Main Mock Test Set 1 to see how well you’ve mastered the concepts.