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Pin(ac) = [(Ip)/(2)]² x [RD + RL]

Mathematics

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Pin(ac)=[Ip2]2×[RD+RL]P_{in(ac)} = \left[\frac{I_p}{2}\right]^2 \times [R_D + R_L] Efficiency=dc power outputpower in input signal\text{Efficiency} = \frac{\text{dc power output}}{\text{power in input signal}} =[Ipπ]2×RL[Ip2]2×[RD+RL]= \frac{\left[\frac{I_p}{\pi}\right]^2 \times R_L}{\left[\frac{I_p}{2}\right]^2 \times [R_D + R_L]} =Ip2π2×RL÷Ip24×1[RD+RL]= \frac{I_p^2}{\pi^2} \times R_L \div \frac{I_p^2}{4} \times \frac{1}{[R_D + R_L]} =Ip2π2×RL×4Ip2×1[RD+RL]= \frac{I_p^2}{\pi^2} \times R_L \times \frac{4}{I_p^2} \times \frac{1}{[R_D + R_L]} =4RLπ2[RD+RL]= \frac{4 R_L}{\pi^2 [R_D + R_L]} =4RLπ2(RD+RL)= \frac{4 R_L}{\pi^2 (R_D + R_L)} =4RLRLπ2(RD+RL)RL= \frac{\frac{4 R_L}{R_L}}{\pi^2 \frac{(R_D + R_L)}{R_L}} =4π2(1+RDRL)= \frac{4}{\pi^2 \left(1 + \frac{R_D}{R_L}\right)} =0.4061+RDRL(4.11)= \frac{0.406}{1 + \frac{R_D}{R_L}} \quad (4.11)

If resistance of diode RDR_D is far less than resistance of RLR_L,

RDRL≈0\frac{R_D}{R_L} \approx 0

Therefore, Efficiency of a half wave rectifier circuit is about 0.406 or 40.6%.

This means that a half wave rectifier circuit can only rectify about 40.6% of a full cycle of an input signal. Note that 50% (half cycle) of the input signal is not rectified but blocked by the diode. This means, about 9.4% of the input signal is lost during the process of rectification.

4.4. PEAK INVERSE VOLTAGE (PIV) OF DIODE IN HALF WAVE RECTIFIER CIRCUIT
During the negative half cycle of the input signal, the diode in a half wave rectifier circuit does not allow electric current to flow through it. See Figure 4.4. If electric current do not flow through the diode, it means that the voltage across the
Electronics for Beginners

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