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1 Electronic Devices and 
Circuits (2131006) 
Transistor 
as 
A VOLTAGE REGULATOR
Index 
1.Voltage Regulation 
2.Zener follower 
3.Two transistor regulator 
2
What is ”Voltage Regulation” ? 
Besides being use in buffer circuits and 
impedance , the emitter follower is widely 
use in voltage regulators. 
In conjunction with a zener diode ,the 
emitter follower can produce regulated 
output voltages with much larger output 
currents. 
3
Zener Follower 
In fig. shows a zener 
follower, a circuit that 
combines a zener 
regulator and emitter 
follower. 
4
How its works? 
 The zener voltage is the input to the base of the 
emitter follower. 
 The d.c output voltage of the emitter follower is 
VOUT = VZ – VBE 
 This output voltage is fixed so that it is equal to the 
zener voltage minus the VBE drop of the transistor . 
5
 If the supply voltage changes , the zener voltage remains approximately constant , and so 
does the output voltage. 
 In other word the circuit acts like a voltage regulator because the output voltage is always 
one VBE drop less than the zener voltage. 
 The zener follower has two advantages over an ordinary zener regulator: first zener diode 
of in fig. has to produce a load current of only 
IB=IOUT / βdc 
 Since this base current is much smaller than the output current , we can use a much 
smaller zener diode . 
 For instance , if you are trying to supply several amperes to a load resistor , and ordinary 
zener regulator requires a zener diode capable of handling several amperes . 
6
 The second advantage of a zener follower is it low output impedance. In an ordinary 
zener regulator , the load resistor sees and output impedance approximately Rz, The 
zener impedance. 
 But in the zener follower the output impedance is 
Zout = r’e + Rz / βdc 
 In the fig(b) shows the equivalent output circuit. Because zout is usually very small 
compared to RL , an emitter follower can hold the D.C. output voltage almost constant 
because the source looks stiff . 
 In summary , the zener follower provides the regulation of a zener diode with the 
increased current handaling capability of an emitter follower. 
7
Two-Transistor Regulator 
In fig. shows two transistor 
regulator 
8
9 
The d.c. input voltage vin comes from a 
unregulated power supply such as a bridge 
rectifier with a capacitor input filter. 
Vin has a peak-to-peak ripple of about 10 
percent of the d.c. voltage. 
The final output voltage Vout has almost no 
ripple and is almost constant in value , 
even though the input voltage and load 
current may vary over a large range
How its works? 
 Any attempted changes output voltage produce an amplified feedback voltage 
that opposes the original change . 
 For instants , suppose the output voltage is increases. then , the voltage appearing at 
the based of Q1 will increase . 
 Since Q1 and R2 form a CE amplifier , the collector voltage of Q1 will decrease 
because of the voltage gain. 
 Since the collector voltage of Q1 has decreased the voltage of Q2 decreases . 
 Because Q2 is an emitter follower the output voltage will decrease. 
 In the other words we have negative feedback . 
 The original increase in output voltage produces an opposing decrease in output 
voltage. 
10
 The overall effect is that the output voltage will increase only slightly , much less then 
it would without the negative feedback . 
 Conversely , if the output voltage tries to decrease less voltage appears at the Q1 
base more voltage appears at the Q1 collector , and more voltage appears at the 
Q2 emitter . 
 We have a returning voltage that opposes the original changes in the output 
voltage. 
 Therefore , the output voltage decrease only a little far less than without the negative 
feedback. 
 Because of the zener diode , the Q1 emitter voltage equals Vz. The Q1 base 
voltage is one VBE drop higher. 
11
 Therefore, The voltage across R4 is : 
V4=VZ+VBE 
 With ohm’s law , the current through R4 is : 
I4=(Vz+VBE)/R4 
 Since , This current flow through R3 in series with R4, The output voltage is: 
Vout = I4(R3+R4) 
 After expanding; 
Vout=((R3+R4)(VZ+VBE))/R4 
12
THANK YOU 
13

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Transistor as a voltage regulation

  • 1. 1 Electronic Devices and Circuits (2131006) Transistor as A VOLTAGE REGULATOR
  • 2. Index 1.Voltage Regulation 2.Zener follower 3.Two transistor regulator 2
  • 3. What is ”Voltage Regulation” ? Besides being use in buffer circuits and impedance , the emitter follower is widely use in voltage regulators. In conjunction with a zener diode ,the emitter follower can produce regulated output voltages with much larger output currents. 3
  • 4. Zener Follower In fig. shows a zener follower, a circuit that combines a zener regulator and emitter follower. 4
  • 5. How its works?  The zener voltage is the input to the base of the emitter follower.  The d.c output voltage of the emitter follower is VOUT = VZ – VBE  This output voltage is fixed so that it is equal to the zener voltage minus the VBE drop of the transistor . 5
  • 6.  If the supply voltage changes , the zener voltage remains approximately constant , and so does the output voltage.  In other word the circuit acts like a voltage regulator because the output voltage is always one VBE drop less than the zener voltage.  The zener follower has two advantages over an ordinary zener regulator: first zener diode of in fig. has to produce a load current of only IB=IOUT / βdc  Since this base current is much smaller than the output current , we can use a much smaller zener diode .  For instance , if you are trying to supply several amperes to a load resistor , and ordinary zener regulator requires a zener diode capable of handling several amperes . 6
  • 7.  The second advantage of a zener follower is it low output impedance. In an ordinary zener regulator , the load resistor sees and output impedance approximately Rz, The zener impedance.  But in the zener follower the output impedance is Zout = r’e + Rz / βdc  In the fig(b) shows the equivalent output circuit. Because zout is usually very small compared to RL , an emitter follower can hold the D.C. output voltage almost constant because the source looks stiff .  In summary , the zener follower provides the regulation of a zener diode with the increased current handaling capability of an emitter follower. 7
  • 8. Two-Transistor Regulator In fig. shows two transistor regulator 8
  • 9. 9 The d.c. input voltage vin comes from a unregulated power supply such as a bridge rectifier with a capacitor input filter. Vin has a peak-to-peak ripple of about 10 percent of the d.c. voltage. The final output voltage Vout has almost no ripple and is almost constant in value , even though the input voltage and load current may vary over a large range
  • 10. How its works?  Any attempted changes output voltage produce an amplified feedback voltage that opposes the original change .  For instants , suppose the output voltage is increases. then , the voltage appearing at the based of Q1 will increase .  Since Q1 and R2 form a CE amplifier , the collector voltage of Q1 will decrease because of the voltage gain.  Since the collector voltage of Q1 has decreased the voltage of Q2 decreases .  Because Q2 is an emitter follower the output voltage will decrease.  In the other words we have negative feedback .  The original increase in output voltage produces an opposing decrease in output voltage. 10
  • 11.  The overall effect is that the output voltage will increase only slightly , much less then it would without the negative feedback .  Conversely , if the output voltage tries to decrease less voltage appears at the Q1 base more voltage appears at the Q1 collector , and more voltage appears at the Q2 emitter .  We have a returning voltage that opposes the original changes in the output voltage.  Therefore , the output voltage decrease only a little far less than without the negative feedback.  Because of the zener diode , the Q1 emitter voltage equals Vz. The Q1 base voltage is one VBE drop higher. 11
  • 12.  Therefore, The voltage across R4 is : V4=VZ+VBE  With ohm’s law , the current through R4 is : I4=(Vz+VBE)/R4  Since , This current flow through R3 in series with R4, The output voltage is: Vout = I4(R3+R4)  After expanding; Vout=((R3+R4)(VZ+VBE))/R4 12