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RECTIFIER
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BED11103; Introduction To Electronic Chapter 2. Page 1Diode Application
RECTIFIER
Diodes are used in circuits called rectifiers that convert ac voltage into dc voltage. Rectifiers in all dc
power supplies that operate from an ac voltage source. In this section, you will study the most basic
type of rectifier, the half-wave rectifier.
After completing this section, you should be able to;
Explain and analyze the operation of half-wave rectifiers
Describe a basic dc power supply and half-wave rectification
Determine the average value of a half-wave rectified voltage
Discuss the effect of barrier potential on a half-wave rectifier output
Define peak inverse voltage (PIV)
Describe the transformer-coupled half-wave rectifier.
Prepared by: HMD UniKL BMI
BED11103; Introduction To Electronic Chapter 2. Page 2Diode ApplicationThe Basic DC Power Supply
1. The dc power supply converts the standard 240V, 60 Hz ac available at wall outlets into a
constant dc voltage.
2. The dc voltage is used to power all types of electronic circuits; television receivers, stereo
systems, VCRs, CD players, and most lab. equipments.
3. Basic block diagrams for a rectifier and complete power supply are shown in Figure below.
4. The rectifier converts the ac input voltage
to a pulsating dc voltage, which is half-
wave rectified as shown in part (a).
5. A block diagram for a complete power
supply is shown in part (b).
6. The filter eliminates the fluctuations in
the rectified voltage and produces a
relatively smooth dc voltage.
7. The regulator is a circuit that maintains a
constant dc voltage for variations in the
input line voltage or in the load.
8. The load is a circuit or device for which
the power supply is producing the dc
voltage and load current.
Prepared by: HMD UniKL BMI
BED11103; Introduction To Electronic Chapter 2. Page 3Diode ApplicationThe Half-Wave Rectifier
1. A diode is connected to an ac source and to a load resistor, RL, forming a half-wave rectifier.
2. During one cycle of the input voltage, when the sinusoidal input voltage (Vin) goes positive,
the diode is forward-biased and conducts current through the load resistor, as shown in part
(a).
3. The current produces
an output voltage across the load RL, which has the same shape as the positive half-cycle of
the input voltage.
4. When the input voltage goes negative during the second half of its cycle, the diode is reverse-
biased.
5. There is no current, so the voltage across the load resistor is 0 V, as shown in Figure (b).
6. The result is only
the positive half-cycles of the ac input voltage appear across the load. Since the output does
not change polarity, it is a pulsating dc voltage with a frequency of 60 Hz, as shown in part
(c).
Prepared by: HMD UniKL BMI
BED11103; Introduction To Electronic Chapter 2. Page 4Diode ApplicationAverage Value of the Half-Wave Output Voltage
The average value of the half-wave rectified output voltage is the value you would measure on a dc
voltmeter. This equation shows that VAVG is approximately 31.8% of VP for a half-wave rectified
voltage.
Effect of the Barrier Potential on the Half-Wave Rectifier Output
During the practical, diode model is used with the barrier potential of 0.7 V taken into account. This
results in a half-wave output with a peak value that is 0.7 V less than the peak value of the input, as
shown in Figure 1.
Prepared by: HMD UniKL BMI
V AVG=V P
π
EXAMPLE What is the average value of the half-wave rectified voltage in Figure below?
Ans: 31.83V
BED11103; Introduction To Electronic Chapter 2. Page 5Diode Application
Peak Inverse Voltage (PIV)
The peak inverse voltage (PIV) equals the peak value of the input voltage. PIV, occurs at the peak of
each negative alternation of the input voltage when the diode is reverse-biased.
FIGURE 2 The PIV occurs at the peak of each half-cycle of the input voltage when the diode is reverse-biased. In
this circuit, the PIV occurs at the peak of each negative half-cycle.
Prepared by: HMD UniKL BMI
Vp(out )=Vp( in )−0 . 7 v
Figure 1: The effect of the barrier potential
on the half-wave rectified output voltage is
to reduce the peak value of the input by
about 0.7 V.
PIV = VP(in)
BED11103; Introduction To Electronic Chapter 2. Page 6Diode Application
Half-Wave Rectifier with Transformer-Coupled Input Voltage
Transformer coupling provides two advantages;
First, it allows the source voltage to be stepped up or stepped down as needed. Second, the ac
source is electrically isolated from the rectifier, thus preventing a shock hazard in the
secondary circuit.
Basic ac circuit’s recall that the secondary voltage of a transformer equals the turns ratio, n, times the
primary voltage. We will define the turns ratio as the ratio of secondary turns, Nsec, to the primary
turns, Npri : n =
N secNpri
Vsec = nVpri
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EXAMPLE: Determine the peak value of the output voltage in the circuit if the turns ratio is 0.5.
Ans: 78V, 77.3V
BED11103; Introduction To Electronic Chapter 2. Page 7Diode ApplicationFULL-WAVE RECTIFIERSIn this section, you will use what you learned about half-wave rectification and expand it to full-wave
rectifiers.
After completing this section, you should be able to
Explain and analyze the operation of full-wave rectifiers
Discuss how full-wave rectification differs from half-wave rectification
Determine the average value of a full-wave rectified voltage
Describe the operation of a center-tapped full-wave rectifier
Explain how the transformer turns ratio affects the rectified output voltage
A full-wave rectifier allows unidirectional (one-way) current through the load during the entire 360°
of the input cycle, whereas a half-wave rectifier allows current through the load only during one-half
of the cycle.
The average value, which is the value measured on a dc voltmeter. VAVG is approximately 63.7% of Vp, for a full-wave rectified voltage.
The Center-Tapped Full-Wave Rectifier
The Center-Tapped Full-Wave Rectifier
Prepared by: HMD UniKL BMI
V AVG=2V P
π
EXAMPLE: Find the average value of the full-wave rectified voltage.
Ans: 9.55V
BED11103; Introduction To Electronic Chapter 2. Page 8Diode Application
1. A center-tapped rectifier is a type of full-wave rectifier that uses two diodes connected to the
secondary of a center-tapped transformer.
2. The input voltage is coupled through the transformer to the center-tapped secondary.
3. Half of the total secondary voltage appears between the center tap and each end of the
secondary winding as shown.
4. For a positive half-cycle of the input voltage, the polarities of the secondary voltages are as
shown in Figure (a). This condition forward-biases diode D1 and reverse-biases diode D2. The
current path is through D1 and the load resistor R1 as indicated.
5. For a negative half-cycle of the input voltage, the voltage polarities on the secondary are as
shown in Figure (b). This condition reverse-biases D1 and forward-biases D2. The current
path is through D1 and R1, as indicated. Because the output current during both the positive
and negative portions of the input cycle is in the same direction through the load, the output
volt- age developed across the load resistor is a full-wave rectified do voltage, as shown.
Prepared by: HMD UniKL BMI
BED11103; Introduction To Electronic Chapter 2. Page 9Diode Application
Effect of the Turns Ratio on the Output Voltage
1. If the transformer's turns ratio is 1, the peak value of the rectified output voltage equals half
the peak value of the primary input voltage.
FIGURE: Center-tapped full-wave rectifier with a transformer turns ratio of 1. Vp(pri) is the peak value of the primary
voltage.
2. In order to obtain an output voltage with a peak equal to the input peak (less the diode drop), a
step-up transformer with a turns ratio of n = 2 must be used, as shown.
Prepared by: HMD UniKL BMI
BED11103; Introduction To Electronic Chapter 2. Page 10Diode Application
FIGURE : Center-tapped full-wave rectifier with a transformer turns ratio of 2.
In any case, the output voltage of a center-tapped full-wave rectifier is always one-half of the total
secondary voltage less the diode drop, no matter what the turn’s ratio.
The Full-Wave Bridge Rectifier
1. The bridge rectifier uses four diodes connected as shown. When the input cycle is positive as
in part (a), diodes D1 and D2 are forward-biased and conduct current in the direction shown.
2. A voltage is developed across R, that looks like the positive half of the input cycle. During this
time, diodes D3 and D4 are reverse-biased.
Prepared by: HMD UniKL BMI
Vout =
V sec2 - 0.7v
BED11103; Introduction To Electronic Chapter 2. Page 11Diode Application
3. When the input cycle is negative as in Figure (b), diodes D3 and D, are forward- bias and
conduct current in the same direction through RL as during the positive half-cycle.
4. During the negative half-cycle, D1 and D2 are reverse-biased. A full-wave rectified output
voltage appears across RL as a result of this action.
Bridge Output Voltage
A bridge rectifier with a transformer-coupled input is shown in Figure a (below). During the positive
half-cycle of the total secondary voltage, diodes D1 and D2 are forward-biased.
The same is true when D3 and D4 are forward-biased during the negative half-cycle.
Prepared by: HMD UniKL BMI
Vp(out) = Vp
BED11103; Introduction To Electronic Chapter 2. Page 12Diode Application
1. As you can see in Figure b (below), two diodes are always in series with the load resistor
during both the positive and negative half-cycles.
2. If these diode drops are taken into account, the output voltage is,
THE DIODE DATA SHEET
A manufacturer's data sheet gives detailed information on a device.
After completing this section, you should be able to
Interpret and use a diode data sheet
Identify maximum voltage and current ratings
Determine the electrical characteristics of a diode
Analyze graphical data
Select an appropriate diode for a given set of specifications
Prepared by: HMD UniKL BMI
Vp(out) = Vp (sec) –
BED11103; Introduction To Electronic Chapter 2. Page 13Diode ApplicationThese are the absolute maximum values under which the diode can be operated without damage to the
device.
An explanation of the parameters from Table 1 follows.
VRRM The maximum peaks reverse voltage that can be applied repetitively across the diode.
Notice that in this case, it is 50 V for the I N4001 and I kV for the 1N4007. This is the
same as PIV rating.
VR The maximum reverse do voltage that can be applied across the diode.
VRSM The maximum peak value of non repetitive reverse voltage that can be applied across
the diode.
Io The maximum average value of a 60 Hz rectified forward current.
IFSM The maximum peak value of non repetitive (one cycle) forward surge current.
TA Ambient temperature (temperature of surrounding air).
Tj The operating junction temperature.
Tstg The storage junction temperature.
Table 1: Maximum rating
RATING SYMBOL 1N4001 1N4002 1N4003 1N4004 1N4005 1N4006 1N4007 UNIT
Peak repetitive
reverse voltage
Working peak
reverse voltage
DC Blocking
voltage
VRRM
VRWM
VR
50 100 200 400 600 800 1000 V
Non repetitive
peak reverse
voltage
VRSM 60 120 240 480 720 1000 1200 V
Prepared by: HMD UniKL BMI
BED11103; Introduction To Electronic Chapter 2. Page 14Diode Application
rms reverse
voltage
VR(rms) 35 70 140 280 420 560 700 V
Average rectified
forward current
(single-
phase,resistive
load, 60Hz,
TA=75C)
Io 1.0 A
Non repetitive
peak surge
current ( surge
applied at rated
load condition )
IFSM 30 (for 1 cycle ) A
Operating and
store junction
temperature range
Tj, Tstg -65 to +175 C
ZENER DIODES
The Zener diode model to be employed for the “on” state will be shown in Figure 1a.
For the “off” state as defined by a voltage less than VZ but greater than 0V with the polarity indicated
in Figure 1b, the Zener equivalent is the open circuit.
Vi and R Fixed
Prepared by: HMD UniKL BMI
FIGURE 1 Zener diode
equivalents for the (a) “on” and (b)
“off” states.
IZ = IR - IL
R
VV Li Where, and
BED11103; Introduction To Electronic Chapter 2. Page 15Diode Application
1. In figure 2, the applied dc voltage is fixed, as is the load resistor. The analysis will be divide in
to 2 steps;
Step 1: Determine the state of the zener diode by removing it from the network and
calculating the voltage across the resulting open circuit.
2. If V ≥ VZ the Zener diode is “on”. ( Refer Figure 1a).
3. If V < VZ the Zener diode is “off”. ( Refer Figure 1b).
Step 2: substitute the appropriate equivalent circuit and solve for the desired unknowns.
4. For the Figure 2(a), the “on” state will equivalent to network Figure 3.
5. The Zener diode current must be determined using KCL.
Prepared by: HMD UniKL BMI
V = VL =
R LViR+R L
VL =
Vz
FIGURE 2 (a) Basic Zener regulator and (b) Determining the state of the Zener diode
BED11103; Introduction To Electronic Chapter 2. Page 16Diode Application
6. The power dissipated by the Zener diode is determined by;
7. Zener diodes are most frequently used in regulator networks or as a reference voltage. Figure
2 (a ) is a simple regulator design to maintain a fixed voltage across the load RL.
~end.
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PZ = VZ IZ