A full-wave rectifier is an electronic device that is used for rectifying the AC, into direct current DC. While the half-wave rectifier utilizes only one-half of the AC waveform, this is useful for most electronic devices that require a constant DC supply of power. In this article, we will discuss the full-wave rectifier along with its workings, advantages, and applications in detail.
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A full-wave rectifier is an electric circuit that is used to convert an Alternating current into Direct current. It uses both, the positive and the negative halves of the AC input signal hence it is more effective than the half-wave rectifier that just uses the positive half of the wave. Full-wave rectifiers are common in power supplies by converting AC voltage from the mains into DC voltage. It requires two junction diodes such that one diode rectifies one half and the second diode rectifies the second half of the input.
A full-wave rectifier converts both halves of the alternating current into direct current. It can be designed using two configurations:
Let's discuss how these configurations work in detail.
In this connection, a center-tapped transformer is used where the transformer has the secondary winding connected to a center-tapped. The center-tap is grounded and two diodes are used. Each diode conducts during different half cycles of the AC input.
Positive Half Cycle: During the positive half cycle one diode allows the current to flow through load resistor in single direction.
Negative Half Cycle: During the negative half cycle second diode will conduct and allows the current to flow through load resistor in same direction as positive half cycle.
In a bridge rectifier, four diodes are arranged to form a bridge, Hence, this arrangement does not require center-tapped transformer making it more efficient. During the positive half cycle, first two diodes will conduct and in the negative half cycle, the other two diodes will conduct. this results in current flowing through the load resistor in the same direction.
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A full-wave rectifier produces an output waveform which is a pulsating DC. Ideally, the output in full-wave rectification would be a straight line DC but instead of this, the output will contain ripples. To minimize the ripple filtering techniques can be used.
Without filtering: The output will have a series of pulses, but the frequency of these pulses will be twice the input frequency (since both halves are utilised).
With filtering: A filter capacitor on the other hand regulates these pulses and comes up with a steady DC voltage.
Full-wave rectifier is composed of different components, which helps it to function properly. These components are duscussed below:
The following formulas are used in constructing a Full-wave rectifier; These formulas consists are discussed below:
1. Average Output Voltage (DC Voltage)
The average output voltage ( $V_{D C}$ ) is given by:
$$
V_{D C}=\frac{2 V_m}{\pi}
$$
Where:$V_m$ is the peak voltage across the secondary winding of the transformer.
2. RMS Value of the Output Voltage
The root mean square (RMS) value of the output voltage ( $V_{R M S}$ ) for a full-wave rectifier is given by:
$$
V_{R M S}=\frac{V_m}{\sqrt{2}}
$$
3. Efficiency
The efficiency $(\eta)$ of a full-wave rectifier is a measure of how much of the AC power is converted into $D C$ power. It is calculated as:
$$
\eta=\frac{P_{D C}}{P_{A C}}=\frac{V_{D C}^2}{V_{R M S}^2}=\frac{0.81}{1}=81.2 \%
$$
Where:
$P_{D C}$ is the DC power delivered to the load,
$\quad P_{A C}$ is the AC power supplied by the transformer.
4. Ripple Factor
The ripple factor $(\gamma)$ is a measure of the amount of $A C$ ripple present in the DC output. For a fullwave rectifier, it is calculated as:
$$
\gamma=\frac{I_{A C}}{I_{D C}}=\frac{1}{\sqrt{f}}
$$
5. Peak Inverse Voltage (PIV)
For a center-tapped full-wave rectifier, the peak inverse voltage (PIV) across each diode is equal to the peak voltage of the transformer secondary winding, $V_m$.
$$
P I V=V_m
$$
6. DC Output Power
The DC output power delivered to the load resistor $R_L$ is given by:
$$
P_{D C}=V_{D C} \times I_{D C}
$$
Where:
$I_{D C}$ is the average DC current, calculated as:
$$
I_{D C}=\frac{V_{D C}}{R_L}
$$
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Full-wave rectifiers can be used in the power supply circuits of most electronic devices because they deliver more power in DC form than half-wave rectifiers. Some common applications include:
There are two types of rectifier
Half wave rectifier
Full-wave rectifier
A device that converts the dc into ac.
Centered tapped rectifier
Bridge full-wave rectifier.
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