UNIT-1 Rectifiers & Power Supplies

Rectifier A rectifier is an electrical device that converts alternating current (AC), which periodically reverses direction, to direct current (DC), which is in only one direction, a process known as rectification. Rectifiers have many uses including as components of power supplies and as detectors of radio signals. alternating currentdirect currentpower suppliesdetectorsradio

Types of Rectifier Half Wave Full Wave Bridge

Half-wave rectification In half wave rectification, either the positive or negative half of the AC wave is passed, while the other half is blocked. Because only one half of the input waveform reaches the output, it is very inefficient if used for power transfer. Half- wave rectification can be achieved with a single diode in a one-phase supply, or with three diodes in a three-phase supply.three-phase

The output DC voltage of a half wave rectifier can be calculated with the following two ideal equations: [1] [1]

Full Wave Rectification Like the half wave circuit, a full wave rectifier circuit produces an output voltage or current which is purely DC or has some specified DC component. Full wave rectifiers have some fundamental advantages over their half wave rectifier counterparts. The average (DC) output voltage is higher than for half wave, the output of the full wave rectifier has much less ripple than that of the half wave rectifier producing a smoother output waveform.

In a Full Wave Rectifier circuit two diodes are now used, one for each half of the cycle. A transformer is used whose secondary winding is split equally into two halves with a common centre tapped connection, (C). This configuration results in each diode conducting in turn when its anode terminal is positive with respect to the transformer centre point C producing an output during both half- cycles, twice that for the half wave rectifier so it is 100% efficient as shown below.

The full wave rectifier circuit consists of two power diodes connected to a single load resistance (R L ) with each diode taking it in turn to supply current to the load. When point A of the transformer is positive with respect to point C, diode D 1 conducts in the forward direction as indicated by the arrows. When point B is positive (in the negative half of the cycle) with respect to point C, diode D 2 conducts in the forward direction and the current flowing through resistor R is in the same direction for both half-cycles. As the output voltage across the resistor R is the phasor sum of the two waveforms combined, this type of full wave rectifier circuit is also known as a "bi-phase" circuit.

As the spaces between each half-wave developed by each diode is now being filled in by the other diode the average DC output voltage across the load resistor is now double that of the single half- wave rectifier circuit and is about 0.637V max of the peak voltage, assuming no losses. Where: V MAX is the maximum peak value in one half of the secondary winding and V RMS is the rms value.

Full Wave Bridge Rectifier Another type of circuit that produces the same output waveform as the full wave rectifier circuit above, is that of the Full Wave Bridge Rectifier. This type of single phase rectifier uses four individual rectifying diodes connected in a closed loop "bridge" configuration to produce the desired output. The main advantage of this bridge circuit is that it does not require a special centre tapped transformer, thereby reducing its size and cost. The single secondary winding is connected to one side of the diode bridge network and the load to the other side as shown below.

Circuit Diagram The four diodes labeled D 1 to D 4 are arranged in "series pairs" with only two diodes conducting current during each half cycle.

The Positive Half-cycle During the positive half cycle of the supply, diodes D1 and D2 conduct in series while diodes D3 and D4 are reverse biased and the current flows through the load as shown below.

The Negative Half-cycle During the negative half cycle of the supply, diodes D3 and D4 conduct in series, but diodes D1 and D2 switch "OFF" as they are now reverse biased. The current flowing through the load is the same direction as before.

Voltage Multiplier A voltage multiplier is an electrical circuit that converts AC electrical power from a lower voltage to a higher DC voltage by means of capacitors and diodes combined into a network.electrical circuitvoltagecapacitors diodes Voltage multipliers can be used to generate bias voltages ranging from a few volts for electronic appliances, to millions of volts for purposes such as high-energy physics experiments and lightning safety testing

negative peak (−U s ): The C 1 capacitor is charged through diode D 1 to 0 V (potential difference between left and right plate of the capacitor is U s )Vpotential difference positive peak (+U s ): the potential of C 1 adds with that of the source, thus charging C 2 to 2U s through D 2 negative peak: potential of C 1 drops to 0 V thus allowing C 3 to be charged through D 3 to 2U s. positive peak: potential of C 1 rises to 2U s (analogously to step 2), also charging C 4 to 2U s. The output voltage (the sum of voltages under C 2 and C 4 ) raises till 4U s. In reality more cycles are required for C 4 to reach the full voltage. Each additional stage of two diodes and two capacitors increases the output voltage by twice the peak AC supply voltage.

Zener Diode Voltage Regulator Zener diodes are widely used as voltage references and as shunt regulators to regulate the voltage across small circuits. When connected in parallel with a variable voltage source so that it is reverse biased, a Zener diode conducts when the voltage reaches the diode's reverse breakdown voltage. From that point on, the relatively low impedance of the diode keeps the voltage across the diode at that value.

Circuit Diagram

In this circuit, a typical voltage reference or regulator, an input voltage, U IN, is regulated down to a stable output voltage U OUT. The intrinsic voltage drop of diode D is stable over a wide current range and holds U OUT relatively constant even though the input voltage may fluctuate over a fairly wide range. Because of the low impedance of the diode when operated like this, Resistor R is used to limit current through the circuit. In the case of this simple reference, the current flowing in the diode is determined using Ohms law and the known voltage drop across the resistor R. I Diode = (U IN - U OUT ) / R Ω

The value of R must satisfy two conditions: R must be small enough that the current through D keeps D in reverse breakdown. The value of this current is given in the data sheet for D. For example, the common BZX79C5V6 [2] device, a 5.6 V 0.5 W Zener diode, has a recommended reverse current of 5 mA. If insufficient current exists through D, then U OUT will be unregulated, and less than the nominal breakdown voltage (this differs to voltage regulator tubes where the output voltage will be higher than nominal and could rise as high as U IN ). When calculating R, allowance must be made for any current through the external load, not shown in this diagram, connected across U OUT. [2]voltage regulator tubes R must be large enough that the current through D does not destroy the device. If the current through D is I D, its breakdown voltage V B and its maximum power dissipation P MAX, then I D V B < P MAX.

A load may be placed across the diode in this reference circuit, and as long as the zener stays in reverse breakdown, the diode will provide a stable voltage source to the load. Shunt regulators are simple, but the requirements that the ballast resistor be small enough to avoid excessive voltage drop during worst-case operation (low input voltage concurrent with high load current) tends to leave a lot of current flowing in the diode much of the time, making for a fairly wasteful regulator with high quiescent power dissipation, only suitable for smaller loads.

Switched-mode Power Supply A switched-mode power supply (switching- mode power supply, SMPS, or simply switcher) is an electronic power supply that incorporates a switching regulator in order to be highly efficient in the conversion of electrical power. Like other types of power supplies, an SMPS transfers power from a source like the electrical power grid to a load (e.g., a personal computer) while converting voltage and current characteristics. An SMPS is usually employed to efficiently provide a regulated output voltage, typically at a level different from the input voltage.power supplypower gridvoltagecurrent

Unlike a linear power supply, the pass transistor of a switching mode supply switches very quickly (typically between 50 kHz and 1 MHz) between full-on and full- off states, which minimizes wasted energy. Voltage regulation is provided by varying the ratio of on to off time. In contrast, a linear power supply must dissipate the excess voltage to regulate the output. This higher efficiency is the chief advantage of a switch-mode power supply. Switching regulators are used as replacements for the linear regulators when higher efficiency, smaller size or lighter weight are required. They are, however, more complicated, their switching currents can cause electrical noise problems if not carefully suppressed, and simple designs may have a poor power factor.power factor