A brief note on Rectifiers, Zener Diodes and Light Devices . Read it before a test. Try each question at the end before you open its answer.
Rectifiers Half-wave, ideal: V d c = V m π V_{dc} = \dfrac{V_m}{\pi} V d c = π V m , V r m s = V m 2 V_{rms} = \dfrac{V_m}{2} V r m s = 2 V m , r = 1.21 r = 1.21 r = 1.21 , η = 40.6 % \eta = 40.6\ \% η = 40.6 % , ripple frequency f f f , PIV = V m = V_m = V m . Full-wave, ideal: V d c = 2 V m π V_{dc} = \dfrac{2V_m}{\pi} V d c = π 2 V m , V r m s = V m 2 V_{rms} = \dfrac{V_m}{\sqrt{2}} V r m s = 2 V m , r = 0.48 r = 0.48 r = 0.48 , η = 81.2 % \eta = 81.2\ \% η = 81.2 % , ripple frequency 2 f 2f 2 f . PIV: V m V_m V m for the bridge, 2 V m 2V_m 2 V m for the centre-tap circuit, and about 2 V m 2V_m 2 V m for a half-wave circuit with a large capacitor. Diode drops: a silicon bridge loses 1.4 1.4 1.4 V, a centre-tap rectifier loses 0.7 0.7 0.7 V. Capacitor filter: Δ V = I f r C \Delta V = \dfrac{I}{f_r C} Δ V = f r C I , V d c ≈ V p − Δ V 2 V_{dc} \approx V_p - \dfrac{\Delta V}{2} V d c ≈ V p − 2 Δ V , r = Δ V 2 3 V d c r = \dfrac{\Delta V}{2\sqrt{3}\, V_{dc}} r = 2 3 V d c Δ V . The Zener regulator Breakdown: a Zener diode works in reverse breakdown at a fixed V z V_z V z . The Zener effect is below about 5 5 5 V and avalanche is above about 7 7 7 V. Currents: I s = V i n − V z R s I_s = \dfrac{V_{in} - V_z}{R_s} I s = R s V in − V z , I L = V z R L I_L = \dfrac{V_z}{R_L} I L = R L V z , I z = I s − I L I_z = I_s - I_L I z = I s − I L . Limits: I z , m i n ≤ I z ≤ I z , m a x = P V z I_{z,min} \le I_z \le I_{z,max} = \dfrac{P}{V_z} I z , min ≤ I z ≤ I z , ma x = V z P . Series resistor: V i n , m a x − V z I z , m a x + I L , m i n ≤ R s ≤ V i n , m i n − V z I z , m i n + I L , m a x \dfrac{V_{in,max} - V_z}{I_{z,max} + I_{L,min}} \le R_s \le \dfrac{V_{in,min} - V_z}{I_{z,min} + I_{L,max}} I z , ma x + I L , min V in , ma x − V z ≤ R s ≤ I z , min + I L , ma x V in , min − V z . Light devices LED: forward biased, λ = 1240 eV nm E g \lambda = \dfrac{1240\ \text{eV nm}}{E_g} λ = E g 1240 eV nm , series resistor R = V s − V f I R = \dfrac{V_s - V_f}{I} R = I V s − V f . Photodiode: reverse biased, the photocurrent follows the intensity, I = η P E I = \eta\,\dfrac{P}{E} I = η E P . Solar cell: no bias, P m a x = F F × V o c I s c P_{max} = FF \times V_{oc} I_{sc} P ma x = F F × V oc I sc , efficiency = P m a x G A = \dfrac{P_{max}}{G A} = G A P ma x . A worked example A 6.8 6.8 6.8 V Zener diode has R s = 100 Ω R_s = 100\ \Omega R s = 100 Ω and a load of 1.0 k Ω 1.0\ \text{k}\Omega 1.0 k Ω . The input is 12 12 12 V. Find I z I_z I z .
The series current. I s = 12 V − 6.8 V 100 Ω = 52 I_s = \dfrac{12\ \text{V} - 6.8\ \text{V}}{100\ \Omega} = 52 I s = 100 Ω 12 V − 6.8 V = 52 mA. The load current. I L = 6.8 V 1000 Ω = 6.8 I_L = \dfrac{6.8\ \text{V}}{1000\ \Omega} = 6.8 I L = 1000 Ω 6.8 V = 6.8 mA. The Zener current. I z = 52 mA − 6.8 mA = 45.2 I_z = 52\ \text{mA} - 6.8\ \text{mA} = 45.2 I z = 52 mA − 6.8 mA = 45.2 mA. Practise with new numbers
Check yourself Why is the PIV of a half-wave circuit with a large capacitor about 2 V m 2V_m 2 V m ? Stuck? Show a hint Show the answerA regulator has no load. Where does the series current go? Stuck? Show a hint Show the answerWhy does a photodiode work in reverse bias, and a solar cell with no bias? Stuck? Show a hint Show the answerSources NCERT Physics Class 12, Semiconductor Electronics: Materials, Devices and Simple Circuits. Horowitz and Hill, The Art of Electronics, third edition.