In electronics, rectifiers are the circuits which play an important role in converting Alternating current (AC) into direct current (DC). There are different types of rectifiers, but a full wave rectifier stands out as the best in terms of efficiency and precise results. A full wave rectifier utilises positive as well as negative halves of the waveform which is the reason for its successful output. Knowing how a full wave rectifier operates and its benefits is essential to get stable and high-performance power conversion, regardless of whether you're powering a simple gadget or a complex system.
The ability of diodes to allow the current to flow through them in just a single direction is the foundation of the Full Wave Rectifier Principle. Using this characteristic, a full-wave rectifier transforms an AC waveform's positive and negative cycles into a unidirectional current. This can be achieved by arranging diodes to alternately conduct the positive and negative AC input. In other words, a full wave rectifier follows a principle which ensures that the current always follows a single direction.
The full wave rectifier operation can be understood by analysing its working during both the positive and negative cycles of the AC waveform. The full wave rectifier is divided into two common configurations that are:
Four diodes are included in this arrangement, which is a bridge. Two of the diodes conduct during the positive half-cycle, allowing current to flow through the load resistor in a single direction, and the other two conduct during the negative half-cycle, ensuring that the current flows through the load in the same direction.
Positive pulses occur twice each cycle of the AC input, once during each half-cycle, making up the pulsating DC signal that a full wave rectifier produces. As both the positive and negative halves of the input waveform are used, this waveform is smoother than the output of a half-wave rectifier. In the Full Wave Rectifier Graph or waveform, the AC input waveform is plotted on the x-axis; on the other hand, the output voltage is plotted on the y-axis.
Several formulas are associated with a full wave rectifier which is important for understanding as well as solving the problems related to performance and characteristics. These formulas are:
Peak Inverse Voltage (PIV): It is the maximum reverse voltage which a diode experiences during the rectification of AC, which is equal to the peak value of the AC input voltage (VPeak). Mathematically, it can be written as:
DC Output Voltage (VDC): The DC output Voltage is the average output voltage of the rectifier, which can be calculated with the help of the following formula:
Here, Vmax is the peak voltage of the AC input.
RMS Value of Current (IRMS): The RMS or Root Mean Square value of the current is commonly used to calculate the effective current of the circuit. In a full wave rectifier, the RMS value of the output current can be calculated using this formula:
Rectification Efficiency (η): As the name suggests, rectification efficiency is the indicator of the efficiency of the rectifier, which converts AC power into DC power. The formula to find the Rectification Efficiency is as follows:
Here,
PDC = DC power delivered to the load
PAC = AC power supplied by the source
Form Factor (FF): The output voltage's RMS value divided by its average output voltage is known as the form factor. It indicates the waveform's form, including whether it has ripples or is more similar to a clean DC.
Peak Factor (PF): It is the ratio of the peak values of the output voltage to the RMS value of the output voltage. The peak factor of a full wave rectifier can be expressed as:
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