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LAB#3a: FULL-WAVE BRIDGE RECTIFIER CIRCUIT ..., Study notes of Circuit Theory

To construct a full-wave bridge rectifier circuit and analyze its output. 2. To analyze the rectifier output using a capacitor in shunt as a filter. Overview:.

Typology: Study notes

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Uploaded on 09/27/2022

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LAB#3a: FULL-WAVE BRIDGE RECTIFIER CIRCUIT WITHOUT
AND WITH FILTER
Objectives:
1. To construct a full-wave bridge rectifier circuit and analyze its output.
2. To analyze the rectifier output using a capacitor in shunt as a filter.
Overview:
As you have seen already a half-wave rectifier circuit is unsuitable to applications
which need a "steady and smooth" dc supply voltage. One method to improve on this is
to use every half-cycle of the input voltage instead of every other half-cycle. The circuit
which allows us to do this is called a Full-wave Rectifier. Here, unidirectional current
flows in the output for both the cycles of input signal and rectifies it. The rectification can
be done either by a center tap full wave rectifier (using two diodes) or a full wave bridge
rectifier (using four diodes). In this experiment we will study a full wave bridge rectifier.
The Full-wave Bridge Rectifier
Another type of circuit that produces the same
output as a full-wave rectifier is that of the
Bridge Rectifier (Fig. 1). This type of single
phase rectifier uses 4 individual rectifying
diodes connected in a "bridged" configuration to
produce the desired output but 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 in figure. The 4 diodes labeled D1
to D4 are arranged in "series pairs" with only two diodes conducting current during each
half cycle. During the positive half cycle of the supply, diodes D1 and D2 conduct in
Fig. 1: Full-wave Bridge Rectifier
pf3
pf4
pf5

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LAB#3a: FULL-WAVE BRIDGE RECTIFIER CIRCUIT WITHOUT

AND WITH FILTER

Objectives:

  1. To construct a full-wave bridge rectifier circuit and analyze its output.
  2. To analyze the rectifier output using a capacitor in shunt as a filter. Overview: As you have seen already a half-wave rectifier circuit is unsuitable to applications which need a "steady and smooth" dc supply voltage. One method to improve on this is to use every half-cycle of the input voltage instead of every other half-cycle. The circuit which allows us to do this is called a Full-wave Rectifier. Here, unidirectional current flows in the output for both the cycles of input signal and rectifies it. The rectification can be done either by a center tap full wave rectifier (using two diodes) or a full wave bridge rectifier (using four diodes). In this experiment we will study a full wave bridge rectifier. The Full-wave Bridge Rectifier Another type of circuit that produces the same output as a full-wave rectifier is that of the Bridge Rectifier (Fig. 1). This type of single phase rectifier uses 4 individual rectifying diodes connected in a "bridged" configuration to produce the desired output but 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 in figure. The 4 diodes labeled D 1 to D 4 are arranged in "series pairs" with only two diodes conducting current during each half cycle. During the positive half cycle of the supply, diodes D1 and D2 conduct in Fig. 1: Full-wave Bridge Rectifier

series while diodes D3 and D4 are reverse biased and the current flows through the load as shown below (Fig. 2). During the negative half cycle of the supply, diodes D3 and D conduct in series, but diodes D1 and D2 switch of as they are now reverse biased. The current flowing through the load is the same direction as before. Fig. 2: Working of Full-wave bridge rectifier As the current flowing through the load is unidirectional, so the voltage developed across the load is also unidirectional during both the half cycles. Thus, the average dc output voltage across the load resistor is double that of a half-wave rectifier circuit, assuming no losses. max V^2 V^ max^0. 637 V dc    Ripple factor: As mentioned in the previous lab the ripple factor is a measure of purity of the d.c. output of a rectifier and is defined as 1 0. 48

  1. 637

2 2 2 2 2 2    

dc rms dc rms dc dc ac V

V

V

V V

V output V output r In case of a full-wave rectifier Vrms = Vmax/√2 = 0.707Vmax. The ripple frequency is now twice the supply frequency (e.g. 100Hz for a 50Hz supply).

value of the rectifier and its capacitance value, which determines the amount of ripple that will appear superimposed on top of the dc voltage. Apart from rectification efficiency, the main advantages of a full-wave bridge rectifier is that it has a smaller ac ripple value for a given load and a smaller smoothing capacitor than an equivalent half-wave rectifier. The amount of ripple voltage that is superimposed on top of the dc supply voltage by the diodes can be virtually eliminated by adding other improved filters such as a pi-filter. Circuit components/Equipments: (i) A step-down transformer, (ii) 4 junction diodes, (iii) 3 Load resistors, (iv) Capacitor, (v) Oscilloscope, (vi) Multimeters, (vii) Connecting wires, (viii) Breadboard. Circuit Diagram: (As shown in Fig. 1 and 3) Procedure: i) Configure the full-wave rectifier circuit as shown in the circuit diagram. Note down all the values of the components being used. ii) Connect the primary side of the transformer to the a.c. Mains and secondary to the input of the circuit. iii) Measure the input a.c. voltage (Vac) and current (Iac) and the output a.c. (Vac) and d.c. (Vdc) voltages using multimeter for at least 3 values of load resistor (Be careful to choose proper settings of multimeter for ac and dc measurement). iv) Feed the input and output to the oscilloscope (we will use oscilloscope here only to trace the output waveform) and save the data for each measurement. MEASURE THE INPUT AND OUTPUT VOLTAGES SEPARATELY. v) Multiply the Vac at the input by √2 to get the peak value and calculate Vdc Using the formula Vdc = 2Vmax/ π. Compare this value with the measured Vdc at the output.

vi) Calculate the ripple factor and efficiency. vii) Connect the capacitor across the output for each load resistor. Measure the output a.c. and d.c. voltages once again and calculate the ripple factor. Trace the input and output waveforms in oscilloscope and notice the change. (If time permits you could also use different values of capacitors and study the output) Observations:

  1. Code number of diode = ________
  2. Input Voltage: Vac = _________ Volt Table(I): Full-wave rectifier w/o filter Sl. No Load RL (kΩ) Input Current Iac (mA) Output Voltage Ripple Factor r Efficiency η (Vdc^2 /RL)/VacIac (%) Vac (Volt) Vdc (Volt) 2Vmax/ π (Volt) 1 2 3 Table(II): Full-wave rectifier with filter (C = ____ μF) Sl. No Load RL (kΩ) Output Voltage Ripple Factor Vac (Volt) Vdc (Volt) r 1 2 3