Works on Faraday's law of electromagnetic induction and mutual induction.
K = E₂/E₁ = N₂/N₁ = V₂/V₁ = I₁/I₂
Step-up: K > 1 (N₂ > N₁) | Step-down: K < 1 (N₂ < N₁)
Let: N = turns, φm = max flux, f = frequency
Flux varies sinusoidally: φ = φm sin(2πft)
By Faraday's law: e = -N × dφ/dt
dφ/dt = φm × 2πf × cos(2πft)
Maximum dφ/dt = 2πf φm
Maximum EMF: Em = N × 2πf φm
RMS value: E = Em/√2 = (2π/√2) × f × N × φm
EMF Equation:
E₁ = 4.44 f N₁ φm
E₂ = 4.44 f N₂ φm
Efficiency = (Output Power / Input Power) × 100%
η = Output / (Output + Losses) × 100%
η = (V₂I₂ cos φ) / (V₂I₂ cos φ + Pi + Pc) × 100%
At fraction 'x' of full load:
η = (x × VA × cos φ) / (x × VA × cos φ + Pi + x²Pc) × 100%
Max efficiency when: Iron losses = Copper losses (Pi = Pc)
Hysteresis Loss: Due to repeated magnetization/demagnetization
Ph = η × Bm1.6 × f × V → Reduced by silicon steel
Eddy Current Loss: Due to circulating currents in core
Pe = K × Bm² × f² × t² → Reduced by laminated core
Pc = I₁²R₁ + I₂²R₂
Varies with square of load current
| Loss | Nature | Reduction |
|---|---|---|
| Hysteresis | Constant | Silicon steel |
| Eddy current | Constant | Laminated core |
| Copper | Variable (∝I²) | Thick conductors |
| Parameter | Ideal | Practical |
|---|---|---|
| Winding resistance | Zero | Finite |
| Core losses | Zero | Has losses |
| Leakage flux | Zero | Some leakage |
| Magnetizing current | Zero | Required |
| Efficiency | 100% | 95-99% |
| Voltage regulation | Zero | 2-5% |
| Power relation | P₁ = P₂ | P₁ > P₂ |