Part of Lecture series on EE321N, Power Electronics-I delivered by me during Fifth Semester of B.Tech. Electrical Engg., 2012
Z H College of Engg. & Technology, Aligarh Muslim University, Aligarh
Please comment and feel free to ask anything related. Thanks!
2. Introduction
• Three terminal single junction latching device*
• Different from either diode (due to 3 terminals)
or the transistor (can’t amplify)
• Wide range of applications like oscillators, trigger
circuits, sawtooth generators, phase control
• Overcomes the limitations of previous trigger
circuits like power dissipation & high
dependability on the SCR chatacteristics
• Other variants include CUJT & PUT
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6. Device Description & Operation
• Consists of a lightly doped n-type Si base to
which heavily doped p-type emitter is
embedded
• At the two ends, there are ohmic contacts
designated as Base 1 & Base 2
• Thus the 3 terminals are: E, B1 & B2
• An interbase resistance RBB = RB1 + RB2|IE = 0
(~5-10 kΩ) exists between the two bases
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7. Contd...
• Equivalent circuit consists of a pn junction
diode and the interbase resistance divided
into two parts RB1 & RB2
• When a voltage VBB is applied between the
bases, the potential of point A w. r. t. B1 is
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1 1
1
1 2
B B
AB BB BB BB
B B BB
R R
V V V V
R R R
8. Contd...
• Where, is known as intrinsic stand off ratio
& ranges from 0.5-0.8
• When VE < V1, the equivalent diode is R. B.
This is the OFF state of the device & is shown
as very low current region on the VE-IE curve
• When VE > V1 + VD, the diode becomes F. B.
this is the ON state of the device
• Vp = V1 + VD = VBB + VD is known as the peak
point voltage
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9. Contd...
• Due to the flow of IE through RB1, number of
charge carriers in RB1 is increased which reduces
its resistance, which in turn decrease V1
• This causes diode to become more & more
F. B. & IE increases further leading to a
regenerative action
• VE decreases with increase in IE & the device is
said to exhibit negative resistance
• Eventually, valley point will be reached after
which there will be no further decrease of RB1
• After valley point, device will reach into
saturation state
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10. UJT Relaxation Oscillator
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R R2
VBB
R1
C
E
B2
B1Ve vo
Ve
Vp
VV
Vo
t
t
Capacitor
charging
1=RC
T
V +VBB
VP
2 1=R C
Capacitor
discharging
Vv
11. Contd...
• The –ve resistance region of the UJT can be
used to advantage in relaxation oscillator
which can provide triggering pulses for SCR
• In the above ckt, R1 & R2 are chosen to be
much smaller than the interbase resistances
• The charging resistance R should be such that
its load line passes through the device
characteristics in the negative resistance
region
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12. Contd...
• When a source voltage VBB is applied to it, C
begins to charge through R exponentially towards
VBB according to the equation
• When vC reaches the peak point voltage, E-B1
junction breaks down & the UJT turns ON. Now C
discharges rapidly through R1
• 2 << 1
• UJT turns OFF when the voltage decays to valley
voltage Vv
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/
1 t RC
C BBv V e
13. Expression for Time Period of
Oscillation
• The time T required for C to charge from initial
voltage Vv to peak-point voltage Vp thru R can
be obtained as:
• Assuming
or
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/
1 t RC
p BB D v BBV V V V V e
/
, 1 t RC
D vV V e
1 1
ln
1
T RC
f
14. Contd...
• If T is taken as the time pd. of the O/P pulse
duration (neglecting small discharge time),
then firing angle is given by
• Design considerations include selection of R1,
R2 & R
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1
ln
1
T RC
16. Further Resources
1. Video lectures on “Basic Electronics & Lab”,
Prof. T. S. Natarajan, Lec-34 UJT
Available on www.nptel.iitm.ac.in,
www.youtube.com/iit
2. Boylestad & Nashelsky, “Electronic Devices &
Circuit Theory”, 7/e, PHI
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