Half Wave rectifier Full wave rectifier Mathematical Examples

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Presentation transcript:

Half Wave rectifier Full wave rectifier Mathematical Examples Lecture: 3 Half Wave rectifier Full wave rectifier Mathematical Examples

An a.c. voltage of peak value 20 V is connected in series with a silicon diode and load resistance of 500 Ω. If the forward resistance of diode is 10 Ω, find (i) peak current through diode (ii) peak output voltage What will be these values if the diode is assumed to be ideal ?

Find the current through the diode in the circuit shown in Fig. (i) Find the current through the diode in the circuit shown in Fig. (i). Assume the diode to be ideal.

Determine the current I in the circuit shown in Fig. (i) Determine the current I in the circuit shown in Fig. (i). Assume the diodes to be of silicon and forward resistance of diodes to be zero.

Determine if the diode (ideal) in Fig. 6 Determine if the diode (ideal) in Fig. 6.17 (i) is forward biased or reverse biased.

Important Definition Forward current Peak inverse Voltage Forward current: It is the current flowing through a forward biased diode. Every diode has a maximum value of forward current which it can safely carry. If this value is exceeded, the diode may be destroyed due to excessive heat. For this reason, the manufacturers’ data sheet specifies the maximum forward current that a diode can handle safely. Peak inverse voltage: It is the maximum reverse voltage that a diode can withstand without destroying the junction. Reverse current or leakage current : It is the current that flows through a reverse biased diode. This current is due to the minority carriers. Under normal operating voltages, the reverse current is quite small. Its value is extremely small (< 1µ A) for silicon diodes but it is appreciable (≈100 µA) for germanium diodes. Important Definition Forward current Peak inverse Voltage Reverse current or Leakage voltage

Half Wave Rectifier Circuit details: Fig shows the circuit where a single crystal diode acts as a half-wave rectifier. The a.c. supply to be rectified is applied in series with the diode and load resistance RL Generally, a.c. supply is given through a transformer. The use of transformer permits two advantages. Firstly, it allows us to step up or step down the a.c. input voltage as the situation demands. Secondly, the transformer isolates the rectifier circuit from power line and thus reduces the risk of electric shock.

Half wave Rectifier ( Cont. ) Operation: The a.c. voltage across the secondary winding AB changes polarities after every half-cycle. During the positive half-cycle of input a.c. voltage, end A becomes positive w.r.t. end B. This makes the diode forward biased and hence it conducts current. During the negative half-cycle, end A is negative w.r.t. end B. Under this condition, the diode is reverse biased and it conducts no current. Therefore, current flows through the diode during positive half-cycles of input a.c. voltage only ; it is blocked during the negative half-cycles [See Fig. (ii)]. In this way, current flows through load RL always in the same direction. Hence d.c. output is obtained across RL it may be noted that output across the load is pulsating d.c. Disadvantages : The main disadvantages of a half-wave rectifier are : (i) The pulsating current in the load contains alternating component whose basic frequency is equal to the supply frequency. Therefore, an elaborate filtering is required to produce steady direct current. (ii) The a.c. supply delivers power only half the time. Therefore, the output is low.