A Full wave rectifier is a circuit arrangement which makes use of both half cycles of input alternating current (AC) and converts them to direct current (DC). In our tutorial on Half wave rectifiers, we have seen that a half wave rectifier makes use of only onehalf cycle of the input alternating current. Thus a full wave rectifier is much more efficient (double+) than a half wave rectifier. This process of converting both half cycles of the input supply (alternating current) to direct current (DC) is termed full wave rectification.
Full wave rectifier can be constructed in 2 ways. The first method makes use of a centre tapped transformer and 2 diodes. This arrangement is known as Center Tapped Full Wave Rectifier.
The second method uses a normal transformer with 4 diodes arranged as a bridge. This arrangement is known as a Bridge Rectifier.
Full Wave Rectifier Theory
To understand full wave bridgeÂ rectifier theoryÂ perfectly, you need to learn half wave rectifier first. In the tutorial of half wave rectifier, we have clearly explained the basic working of a rectifier. In addition, we have also explained the theory behind a pn junction and the characteristics of a pn junction diode.
Full Wave Rectifier – Working & Operation
The working & operation of a full wave bridge rectifier is pretty simple. Â The circuit diagrams and waveforms we have given below will help you understand the operation of a bridge rectifier perfectly. Â In the circuit diagram, 4 diodes are arranged in the form of a bridge. The transformer secondary is connected to two diametrically opposite points of the bridge at points A & C. Â The load resistance R_{L}Â is connected to bridge through points B and D.
During the first half cycle
During the first half cycle of the input voltage,Â the upper end of the transformer secondary winding is positive with respect to the lower end. Thus during the first half cycle diodes D1 and D_{3} are forward biased and current flows through arm AB, enters the load resistance R_{L}, and returns back flowing through arm DC. During this half of each input cycle, the diodes D_{2} and D_{4 }are reverse biased and current is not allowed to flow in arms AD and BC. The flow of current is indicated by solid arrows in the figure above. We have developed another diagram below to help you understand the current flow quickly. See the diagram below – the green arrows indicate the beginning of current flow from the source (transformer secondary) to the load resistance. The red arrows indicate the return path of current from load resistance to the source, thus completing the circuit. Â Â
During the second half cycle
During the second half cycle of the input voltage,Â the lower end of the transformer secondary winding is positive with respect to the upper end.Â Thus diodes D_{2} and D_{4} become forward biased and current flows through arm CB, enters the load resistance R_{L}, Â and returns back to the source flowing through arm DA. The flow of current has been shown by dotted arrows in the figure. Thus the direction of flow of current through the load resistance R_{L} remains the same during both half cycles of the input supply voltage. Â See the diagram below – the green arrows indicate the beginning of current flow from the source (transformer secondary) to the load resistance. The red arrows indicate the return path of current from load resistance to the source, thus completing the circuit.
Peak Inverse Voltage of a Full wave bridge rectifier:
Let’s analyse peak inverse voltage (PIV) of a full wave bridge rectifier using the circuit diagram. At any instant when the transformer secondary voltage attains positive peak value Vmax, diodes D1 and D3 will be forward biased (conducting) and the diodes D2 and D4 will be reverse biased (non conducting). If we consider ideal diodes in bridge, the forward biased diodes D1 and D3 will have zero resistance. This means voltage drop across the conducting diodes will be zero. This will result in the entire transformer secondary voltage being developed across load resistance RL.
Thus PIV of a bridge rectifier = Vmax (max of secondary voltage)
Bridge Rectifier Circuit Analysis
The only difference in the analysis between full wave and centre tap rectifier is that
 In a bridge rectifier circuit, two diodes conduct during each half cycle and the forward resistance becomes double (2R_{F}).
 In a bridge rectifier circuit, Vsmax is the maximum voltage across the transformer secondary winding whereas in a centre tap rectifier Vsmax represents that maximum voltage across each half of the secondary winding.
The different parameters are explained with equations below:

Peak Current
The instantaneous value of the voltage applied to the rectifier is given as
vs =Â Vsmax Sin wt
Â If the diode is assumed to have a forward resistance of R_{F} ohms and a reverse resistance equal to infinity, the current flowing through the load resistance is given as
i1 = Imax Sin wt and i2 = 0 for the first half cycle
and i1 = 0 and i2 = Imax Sin wt for second half cycle
The total current flowing through the load resistance R_{L}, being the sum of currents i1 and i2 is given as
i = i1 + i2 = Imax Sin wt for the whole cycle.
Where the peak value of the current flowing through the load resistance R_{L} is given as
Imax = Vsmax/(2R_{F} + R_{L})
2. Â Â Output Current
Since the current is the same through the load resistance RL in the two halves of the ac cycle, magnitude od dc current Idc, which is equal to the average value of ac current, can be obtained by integrating the current i1 between 0 and pi or current i2 between pi and 2pi.
3. Â Â DC Output Voltage
Average or dc value of voltage across the load is given as
4. Â Â Root Mean Square (RMS) Value of Current
RMS or effective value of current flowing through the load resistance R_{L }Â is given as
5. Â Â Root Mean Square (RMS) Value of Output Voltage
RMS value of voltage across the load is given as
6. Â Â Rectification Efficiency
Power delivered to load,
7. Â Â Ripple Factor
Form factor of the rectified output voltage of a full wave rectifier is given as
So, ripple factor, Î³ = Â 1.11^{2} â€“ 1) = 0.482
8. Â Â Regulation
The dc output voltage is given as
Merits and Demerits of Fullwave Rectifier Over HalfWave RectifierÂ
Merits – let us talk about the advantages of full wave bridge rectifier over half wave version first. I can think about 4 specific merits at this point.
 Efficiency is double for a full wave bridge rectifier. The reason is that, a half wave rectifier makes use of only one half of the input signal. A bridge rectifier makes use of both halves and hence double efficiency
 The residual ac ripples (before filtering) is very low in the output of a bridge rectifier. The same ripple percentage is very high in half wave rectifier. A simple filter is enough to get a constant dc voltage from the bridge rectifier.
 We know the efficiency of FW bridge is double than HW rectifier. This means higher output voltage, Higher transformer utilization factor (TUF) and higher output power.
Demerits Â Â Fullwave rectifier needs more circuit elements and is costlier.
Merits and Demerits of Bridge Rectifier Over CenterTap Rectifier.
A centre tap rectifier is always a difficult one to implement because of the special transformer involved. A centre tapped transformer is costly as well. One key difference between center tap & bridge rectifier is in the number of diodes involved in construction. A center tap full wave rectifier needs only 2 diodes whereas a bridge rectifier needs 4 diodes. But silicon diodes being cheaper than a center tap transformer, a bridge rectifier is muchpreferred solution in a DC power supply. Â Following are the advantages of bridge rectifier over a center tap rectifier.
 A bridge rectifier can be constructed with or without a transformer. If a transformer is involved, any ordinary step down/step up transformer will do the job. This luxury is not available in a center tap rectifier. Here the design of rectifier is dependent on the center tap transformer, which can not be replaced.
 Bridge rectifier is suited for high voltage applications. The reason is the high peak inverse voltage (PIV) of bridge rectifier when compared to the PIV of a center tap rectifier.
 Transformer utilization factor (TUF) is higher for bridge rectifier.
Demerits of Bridge rectifier over center tap rectifierÂ
Applications of Full wave Bridge rectifier
Full Wave Bridge Rectifier with Capacitor Filter
The output voltage of the full wave rectifier is not constant, it is always pulsating. But this cannot be used in real life applications. In other words, we desire a DC power supply with a constant output voltage. In order to achieve a smooth and constant voltage a filter with a capacitor or an inductor is used. The circuit diagram below shows a half wave rectifier with capacitor filter.
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