Physics > Semi-conductor Devices and Electronics > 8.0 Rectifier
Semi-conductor Devices and Electronics
1.0 Introduction
1.1 Classification of solids on the basis of their conductivity
1.2 Band theory of solids
1.3 Classification of solids on the basis of band theory
2.0 Types of semiconductor
3.0 Mass action law
4.0 Electrical conductivity in semiconductor
5.0 $p-n$ junction
5.1 Depletion region
5.2 Forward biasing of a $p-n$ junction
5.3 Reverse biasing of a $p-n$ junction
6.0 Breakdown voltage
7.0 $I-V$ characteristics of a $p-n$ junction
8.0 Rectifier
8.1 Half wave rectifier
8.2 Full wave rectifier
8.3 Ripple frequency
8.4 Ripple factor
8.5 Ripple efficiency $\left( \eta \right)$
8.6 Form factor
9.0 Light emitting diode (LED)
10.0 Zener diode
11.0 Transistor
12.0 Boolean identities
13.0 Logic gates
14.0 De Morgan's theorem
8.1 Half wave rectifier
1.2 Band theory of solids
1.3 Classification of solids on the basis of band theory
5.2 Forward biasing of a $p-n$ junction
5.3 Reverse biasing of a $p-n$ junction
8.2 Full wave rectifier
8.3 Ripple frequency
8.4 Ripple factor
8.5 Ripple efficiency $\left( \eta \right)$
8.6 Form factor
A half wave rectifier is a single $p-n$ junction diode connected in series to the load resistor.
Alternating input voltage is given to a step-down transformer and the resulting reduced output voltage of a transformer is given to the diode $D$ and load resistance $R_L$.
The DC output voltage is measured across the load resistor $R_L$.
The half wave rectifier converts only one-half cycle of the input alternating current (AC) to a direct current (DC).
- Peak value of current is, $${I_m} = \frac{{{V_m}}}{{{r_f} + {R_L}}}$$
where,
$r_f$: Forward diode resistance
$R_L$: Load resistance
$V_m$: Peak value of the alternating voltage
- $rms$ value of current is, $${I_{rms}} = \frac{{{I_m}}}{2}$$
- DC value of current is, $${I_{DC}} = \frac{{{I_m}}}{\pi }$$
- Peak inverse voltage is, $$PIV = {V_m}$$
- DC value of voltage is, $$\begin{equation} \begin{aligned}
{V_{DC}} = {I_{DC}}{R_L} \\
{V_{DC}} = \frac{{{I_m}}}{\pi }{R_L} \\\end{aligned} \end{equation} $$