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Dr.R.Hepzi Pramila Devamani,
Assistant Professor of Physics,
V.V.Vanniaperumal College for Women,
Virudhunagar.
 UJT is a three terminal silicon diode.
 UJT has only one PN junction.
 UJT differs from ordinary diode in that it has
three leads
 UJT differs from FET in that it has no ability
to amplify.
 UJT has the ability to control a large ac power
with a small signal.
 UJT exhibits a negative resistance
characteristic which makes it useful as an
oscillator.

 UJT consists of a lightly doped
silicon bar with a heavily doped
P type material alloyed to its one
side for producing single P-N
junction.
 As in figure, there are terminals,
one emitter, E and two bases B1
and B2, at the top and bottom of
the silicon bar.
 The emitter leg is drawn at an
angle to the vertical and arrow
points in the direction of
conventional current when UJT
is in the conduction state.
 Interbase resistance is
the resistance between
B1 and B2.
 It is the total resistance
of the silicon bar from
one end to the other with
emitter terminal open.
 RBB = RB2 + RB1
 RB2 > RB1
 RB1 = 60 % of RBB
 When a battery of 30V is applied across B2 B1, there is a
progressive fall of voltage over RBB provided E is open.
 The emitter acts as a voltage divider.
 With emitter open, I1 = I2 , the interbase current is given by ohm’s
law.
 I = I2 = VBB / RBB
 A part of VBB is dropped over RB2 and part on RB1.
 VA is the voltage drop across RB1. Using simple voltage divider
relationship
 VA = VBB RB1/ RB1 + RB2
 The voltage division factor is given by ⴄ, the intrinsic stand-off
ratio
 ⴄ = RB1 / RB1 + RB2
 VA = ⴄ VBB, ⴄ = 0.5 to 0.85
 Junction, When VBB is switched on, VA is
developed and reverse- biases the junction.
 If VB is the barrier voltage of the P-N junction,
then total reverse bias voltage is =
 VA + VB = ⴄ VBB + VB
 VB = 0.7 V.
 The emitter junction will not become forward-biased
unless its applied voltage VB exceeds (ⴄ VBB + VB).
 The value of VE is called peak-point voltage Vp. When
Ve = Vp emitter current Ip starts to flow through RB1 to
ground.
 The UJT is then said to have been fired or turned
ON.
 Due to flow of IE through RB1, number of charge
carriers in RB1 is increased which reduces its
resistance.
 As ⴄ depends on RB1, its value is also
decreased.
 When VE and IE , increases, RB1 decreases,
 ⴄ decreases and VA decreases.
 This decreases in VA causes more emitter current to
flow which causes a further reduction in RB, ⴄ and VA.
 The process is regenerative.
 VA and VB quickly drop as IE increases.
 Since VE decrease when IE increases, the UJT
possesses negative resistance.
 The terminals E and B1 are active terminals
whereas B2 is the bias terminal i.e., it is meant only
for applying external voltage across the UJT.
 UJT is triggered into conduction by applying a
suitable positive pulse at its emitter.
 It can be brought back to OFF state by applying a
negative trigger pulse.
 The unique property of UJT is that it can be triggered by any one
of its three terminals.
 Once triggered, the emitter current IE of the UJT increases
regeneratively till it reaches a limiting value determined by the
external power supply.
 Because of this particular behaviour, UJT is used in a variety of
circuit applications such as
 Phase control
 switching
 Pulse generation
 Sine wave generator
 Sawtooth generator
 Timing Circuits
 Voltage or current regulated supplies.

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Unijunction transistor

  • 1. Dr.R.Hepzi Pramila Devamani, Assistant Professor of Physics, V.V.Vanniaperumal College for Women, Virudhunagar.
  • 2.  UJT is a three terminal silicon diode.  UJT has only one PN junction.  UJT differs from ordinary diode in that it has three leads  UJT differs from FET in that it has no ability to amplify.  UJT has the ability to control a large ac power with a small signal.  UJT exhibits a negative resistance characteristic which makes it useful as an oscillator. 
  • 3.  UJT consists of a lightly doped silicon bar with a heavily doped P type material alloyed to its one side for producing single P-N junction.  As in figure, there are terminals, one emitter, E and two bases B1 and B2, at the top and bottom of the silicon bar.  The emitter leg is drawn at an angle to the vertical and arrow points in the direction of conventional current when UJT is in the conduction state.
  • 4.  Interbase resistance is the resistance between B1 and B2.  It is the total resistance of the silicon bar from one end to the other with emitter terminal open.  RBB = RB2 + RB1  RB2 > RB1  RB1 = 60 % of RBB
  • 5.  When a battery of 30V is applied across B2 B1, there is a progressive fall of voltage over RBB provided E is open.  The emitter acts as a voltage divider.  With emitter open, I1 = I2 , the interbase current is given by ohm’s law.  I = I2 = VBB / RBB  A part of VBB is dropped over RB2 and part on RB1.  VA is the voltage drop across RB1. Using simple voltage divider relationship  VA = VBB RB1/ RB1 + RB2  The voltage division factor is given by ⴄ, the intrinsic stand-off ratio  ⴄ = RB1 / RB1 + RB2  VA = ⴄ VBB, ⴄ = 0.5 to 0.85
  • 6.  Junction, When VBB is switched on, VA is developed and reverse- biases the junction.  If VB is the barrier voltage of the P-N junction, then total reverse bias voltage is =  VA + VB = ⴄ VBB + VB  VB = 0.7 V.  The emitter junction will not become forward-biased unless its applied voltage VB exceeds (ⴄ VBB + VB).  The value of VE is called peak-point voltage Vp. When Ve = Vp emitter current Ip starts to flow through RB1 to ground.
  • 7.  The UJT is then said to have been fired or turned ON.  Due to flow of IE through RB1, number of charge carriers in RB1 is increased which reduces its resistance.  As ⴄ depends on RB1, its value is also decreased.  When VE and IE , increases, RB1 decreases,  ⴄ decreases and VA decreases.  This decreases in VA causes more emitter current to flow which causes a further reduction in RB, ⴄ and VA.
  • 8.  The process is regenerative.  VA and VB quickly drop as IE increases.  Since VE decrease when IE increases, the UJT possesses negative resistance.  The terminals E and B1 are active terminals whereas B2 is the bias terminal i.e., it is meant only for applying external voltage across the UJT.  UJT is triggered into conduction by applying a suitable positive pulse at its emitter.  It can be brought back to OFF state by applying a negative trigger pulse.
  • 9.  The unique property of UJT is that it can be triggered by any one of its three terminals.  Once triggered, the emitter current IE of the UJT increases regeneratively till it reaches a limiting value determined by the external power supply.  Because of this particular behaviour, UJT is used in a variety of circuit applications such as  Phase control  switching  Pulse generation  Sine wave generator  Sawtooth generator  Timing Circuits  Voltage or current regulated supplies.