· The circuit diagram of a bridge rectifer is shown above. It uses four diodes and a transformer.
· During the +ve half-cycle, end A is +ve and end B is –ve thus diodes D1 and D3 are forward bias while diodes D2 and D4 are reverse biased thus a current flows through diode D1, load RL ( C to D) and diode D3.
· During the –ve half-cycle, end B is +ve and end A is –ve thus diodes D2 and D4 are forward biased while the diodes D1 and D3 are reverse biased. Now the flow of current is through diode D4 load RL ( D to C) and diode D2. Thus, the waveform is same as in the case of center-tapped full wave rectifier.
Advantages
- The need for center-taped transformer is eliminated.
- The output is twice when compared to center-tapped full wave rectifier.
for the same secondary voltage.
- The peak inverse voltage is one-half(1/2) compared to center-tapped full wave rectifier.
- Can be used where large amount of power is required.
Disadvantages
· It requires four diodes.
· The use of two extra diodes cause an additional voltage drop thereby reducing the output voltage.
2.5.6 Efficiency of Full-wave rectifier
Let V = Vmsinθ be the voltage across the secondary winding
I = Imsinθ be the current flowing in secondary circuit
rf = diode resistance
RL = load resistance
dc power output
input ac power
Squaring both sides we get
The efficiency will be maximum if rf is negligible as compared to RL.
Maximum efficiency = 81.2 %
This is the double the efficiency due to half wave rectifier. Therefore a Full-wave rectifier is twice as effective as a half-wave rectifier.
Particulars | Half wave rectifier | Centre-tapped Full wave rectifier | Bridge rectifier |
1. No. of diodes 2. Idc 3. Vdc 4.Irms 5.Efficiency 6.PIV 7.Ripple factor | 1 Im / Π Vm / Π Im / 2 40.6 % Vm 1.21 | 2 2Im /Π 2Vm / Π Im /√ 2 81.2 % 2Vm 0.48 | 4 2Im /Π 2Vm / Π Im /√ 2 81.2 % Vm 0.48 |
Note:
- The relation between turns ratio and voltages of primary and secondary of the transformer is given by
- N1 / N2 = Vp / Vs
- RMS value of voltage and Max. value of voltage is related by the equation.
- Vrms = Vm / √2 ( for full-cycle of ac)
- If the type of diode is not specified then assume the diode to be of silicon type.
- For an ideal diode, forward resistance rf = 0 and cut-in voltage , Vγ = 0.
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