Site icon DCAClab Blog

Full Wave Bridge Rectifier Circuit

The full-wave bridge rectifier is a circuit consisting of four diodes arranged in a bridge-type structured figure as shown. This circuit gives full-wave rectification and is cost-effective as well, thus used in many applications.


Construction Of Full Wave Rectifier

Full Wave Bridge Rectifier

Four diodes are used in the bridge rectifier. All the four diodes are connected in the form of a diamond-shape to the transformer and the load as in the shown circuit diagram.

Working of Full Wave Rectifier

The working of the full-wave rectifier is simple. The primary winding of the transformer is supplied with a sinusoidal supply. Whereas, the secondary of the transformer is diametrically connected to the two diametrically opposite points. The load Rload is connected to the remaining two points of the bridge.

Now when the AC input is given, during the first half cycle, the upper part of the transformer becomes positive when compared to the lower half of the same. Thus during the first half diodes, D4 and D1 are in forward biased. The currents follow the path 1-2 and enter the load. While returning, the path is 4-3. Similarly, diodes D2 and D3 are reverse biased. Thus, no current flows through the path 2-3 and 1-4.

During the negative half-cycle, i.e. in the next cycle, the upper portion of the transformer becomes negative when compared with the lower portion of the same. Thus diodes D2 & D3 are forward biased and the currents follow the path as 3-2-4-1. The other two, i.e., D1 & D4 are reversed biased for this cycle. So no current flows through the path 1-2 and 3-4. Hence negative cycle is rectified as it appears across the load.

The waveform of the rectified input will look like



Maximum of secondary Voltage = Peak Inverse Voltage (PIV) of the bridge rectifier

Thus in the bridge rectifier circuit, two diodes out of four conduct during one half-cycle and henceforward resistance becomes double that is 2RF.

Peak Current in Full Wave Rectifier

The value of the instantaneous applied voltage to the rectifier is given as

Vs = Vsmaxsin wt

Let us suppose that the diode has a forward resistance of Rf ohms and the reverse resistance equals to infinity, hence current through the RL load can be given as :

The sum of currents I1 and I2 flows through the load resistance RL which is given as:

I = I1 + I2 = Imax Sin wt for complete cycle

The peak value of load current flowing through the load resistance RL is :

Imax = Vsmax/(2RF + RL)

Output Current of Full Wave Rectifier

The current through the load RL is the sum of the two halves of the ac cycles. The magnitude of the direct current Idc is equal to the average value of the ac current and is obtained by integrating the current I1 between 0 & Π or current I2 between Π & 2Π.

Idc = 1 / Π ∫ ∫0Π  I1 d(wt)

= 1/Π ∫ ∫0Π  Imax sin wt d(wt)

= 2Imax / Π

DC Output voltage

DC or average value of voltage across the load is given by

Vdc = Idc RL = 2/ (Π ImaxRL)

Root Mean Square (RMS) Value of Current

Effective or RMS value of the current flowing through the load resistance RL can be given as:

I2RMS = 1/ Π ∫ ∫0Π I1 d (wt) = I2max / 2

IRMS   = Imax / √2

Rectification Efficiency of Full Wave Rectifier

Now the amount of power delivered to the load

Pdc = I2dc RL = 2Im/Π =RLoad

= (4/Π2)I2RL

Alternating (AC) power input to the transformer = power dissipated at the diode + power dissipated from load resistance RL

I2RMSRf + I2RMSRLoad = (I2m/2) (Rf + RLoad)

Rectification efficiency,

n = Pdc / Pac = ((4/Π2)I2m RLoad) / ((I2m/2) (Rf + RLoad)

=0.812(1+Rf / RLoad)

Ripple Factor of Full Wave Rectifier

Rectified output voltage, form factor is given as:

Kf = IRMS/ Iavg = (Im/√2) / (2Im/ Π) = 1.11

Thus ripple factor, γ = √(1.112 – 1) = 0.482

Regulation of Full Wave Rectifier

The DC output voltage is given as

Vdc = Idc RL= 2/(ImRL)

= (2VsmRL / (Rf + RLoad))

= (2Vsm / Π) – (IdcRf)

Applications of Full Wave Rectifier

Conversion of AC Power to DC Power

In many of the electronics applications, regulated DC Power supply is used. One of the most convenient and reliable ways is to convert the AC supply to DC supply. The said conversion is done through a rectifier which uses a system of diodes arranged in a particular way.

Now if two the diodes are used then the arrangement made is a half-wave rectifier which rectifies only half of the AC signal. Whereas, when four diodes are arranged in a particular way then the circuit is the Full Wave Rectifier which rectifies both the cycles of the AC signal. Also with the help of a center-tapped transformer and with two diodes, we can have a full-wave rectifier.

Here the bridge rectifier is used for the application. The arrangement consists of 4 diodes arranged in a way that the anodes of the two adjacent diodes are connected together to give the positive supply to output and the cathodes of the other two are connected together to give the negative supply to the output. The cathode and anode of two adjacent diodes are connected together at the positive of AC supply whereas cathode and anode of another two diodes are connected at the negative of the AC supply. Hence, the four diodes are arranged in a bridge-type configuration such that in each half-cycle two alternate diodes conduct producing a DC voltage with some repels.

Uses of Rectifier while Soldering

Half-wave rectifiers are used in soldering iron type of circuit and are also used in mosquito repellent to drive the lead for the fumes. In electric welding, the bridge rectifier circuit is used to supply polarized and steady DC voltage.

In AM Radio

A half-wave rectifier is used in AM radio as a detector because the output consists of an audio signal. Due to the less intensity of the current, it is if very less use to more complex rectifiers.

For Modulation

For demodulating amplitude of a modulated signal, a half-wave rectifier is used. In a radio signal, for detecting the amplitude of a modulating signal, a full-wave bridge rectifier is used.

Also, a half-wave rectifier is used for the purpose of voltage multiplier.

Other applications are as follows:

Full Wave Bridge Rectifier with Capacitor Filter

As we know, the output voltage of the full-wave rectifier is not constant, it is always pulsating and thus can’t be used in real-life applications. In other words, we require a DC supply with a constant output voltage. This need can be fulfilled by using an adequate filter with an inductor or a capacitor to make the output voltage smooth and constant.

Here capacitor is connected in parallel to the load resistance in a linear power supply. The capacitor is used to increase the DC voltage and to reduce the ripple voltage components of the output obtained. This capacitor is also called a reservoir or smoothing capacitor. Generally, this is followed by a voltage regulator which eliminates the remaining ripples so that the required output can be achieved.

Till the time, the rectifier conducts and the potential is higher than the charge across the capacitor, the capacitor would store the energy from the transformer. But when the output of the rectifier falls below the charge across the capacitor, the capacitor would discharge its energy into the circuit. As the rectifier conducts current only in the forward direction, all the energy discharged by the capacitor will flow into the load. This makes the output a sawtooth wave which is a convenient linear approximation to the actual waveform as shown below:

Advantages of Full Wave Bridge Rectifier

Disadvantages of Full Wave Bridge Rectifier


Ajay Dheeraj

(Technical Content Developer)

Exit mobile version