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
8.2 Full 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 full wave rectifier is a circuit arrangement which makes use of both half cycles of an input alternating current (AC) and convert them to direct current (DC).
Full wave rectifier is much more efficient than a half wave rectifier.
This process of converting both half cycles of the input alternating current (AC) to direct current (DC) is termed full wave rectification.
Full wave rectifier is of two types,
1. Center tapped full wave rectifier
2. Bridge full wave rectifier
1. Centre tapped full wave rectifier
In the case of centre-tap full wave rectifier, only two diodes are used, And are connected to the opposite ends of a centre-tapped secondary transformer as shown in the figure below.
- 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, $${I_{rms}} = \frac{{{I_m}}}{{\sqrt 2 }}$$
- DC value of current is, $${I_{DC}} = \frac{{2{I_m}}}{\pi }$$
- Peak inverse voltage is, $$PIV = 2{V_m}$$
- DC value of voltage is, $$\begin{equation} \begin{aligned} {V_{DC}} = {I_{DC}}{R_L} \\ {V_{DC}} = \frac{{2{I_m}}}{\pi }{R_L} \\\end{aligned} \end{equation} $$