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The Diac
II PHYSICS – 07.04.2022
Dr.R.Hepzi Pramila Devamani,
Assistant Professor of Physics,
V.V.Vanniaperumal College for Women,
Virudhunagar.
The Diac
• A Diac is a two-terminal, three
layered bidirectional device which
can be switched from its OFF state
to ON state for either polarity of
applied voltage.
• The Diac can be constructed in
either npn or pnp form.
• Fig(1) shows the basic structure of a
Diac in pnp form.
• Fig.(2) shows the symbol of a diac.
• The two leads are connected to p-
regions of silicon separated by an n-
region.
• The structure of diac is similar to
that of transistor.
The Diac
The differences are
• There is no terminal attached to the base
layer.
• The three regions are nearly identical in
size.
• The doping concentrations are identical
to give the device symmetrical properties.
Operation
• When a positive or negative voltage is applied across the
terminals of a diac, only a small leakage current IBO will flow
through the device.
• As the applied voltage s increased, the leakage current will
continue to flow until the voltage reaches the breakover
voltage VBO.
• At this point avalanche breakdown of the reverse biased
junction occurs and the device exhibits negative resistance i.e
the current through the device increases with the decreasing
values of applied voltage.
• The voltage across the device then drops to breakback voltage
VW.
V-I Characteristics of Diac
• Fig shows the V-I
characteristics of a diac.
• For applied positive voltage
less than – VBO, a small
leakage current flows through
the device.
• Under such conditions, the
diac blocks the flow of current
and behaves as an open circuit.
• The voltages + VBO and – VBO
are the breakdown voltages
and have a range of 30 to 50 V.
V-I Characteristics of Diac
• When the positive or negative voltage is equal to or greater
than the breakdown voltage, diac begins to conduct and the
voltage drop across it becomes a few volts.
• Conduction then continues until the device current drops
below its holding current.
• The breakover voltage and holding current values are identical
for the forward and reverse regions of the operation.
• Diacs are used for triggering of triacs in adjustable phase
control of a.c. mains power.
• Some of the applications of diac are (i) light dimming (ii) heat
control and (iii) universal motor speed control.
Applications of Diac
• Although a triac may be fired into the conducting state by a simple resistive
triggering circuit, more reliable and faster turn-on may be had if a
switching device is used in series with the gate. One of the switching
devices that can trigger a triac is the diac.
• (i) Lamp dimmer
• Fig shows a typical circuit that may be used for smooth control of a.c.
power fed to a lamp.
• This permits to control the light output from the lamp.
• The basic control is by an RC variable gate voltage arrangement.
• The series R4 – C1 circuit across the triac is designed to limit the rte of
voltage rise across the device during switch off.
Lamp dimmer - Working
• As the input voltage increases positively or
negatively, C1 and C2 charge at a rate
determined by R2
• When the voltage across C3 exceeds the
breakover voltage of the diac, the diac is fired
into the conducting state.
• The capacitor C3 discharges through the
conducting diac into the gate of the triac.
• Hence the triac is turned on to pass the a.c.
power to the lamp.
• By adjusting the value of R2, the rate of
charge of capacitors and hence the point at
which triac will trigger on the positive or
negative half cycle of input voltage can be
controlled.
• Fig shows the waveforms of supply voltage
and load voltage in the diac-triac control
circuit.
• The firing of triac can be controlled upto a
maximum of 1800.
• Thus we can provide a continuous control of
load voltage from zero to full r.m.s value.
Heat Control
• Fig shows a typical diac-triac
circuit that is used for the smooth
control of a.c. power in a heater.
• The capacitor C3 in series with a
choke L across the triac helps to
slow-up th voltage rise across the
device during switch-off.
• The resistor R4 in parallel wih the
diac ensures smooth control at all
positions of variable resistance R2.
Heat Control - Working
• As the input voltage increases positively or negatively, C1
and C2 charge at a rate determined by R2
• When the voltage across C3 exceeds the breakover voltage
of the diac, the diac conducts.
• The capacitor C3 discharges through the conducting diac
into the gate of the triac.
• Hence the triac is turned on to pass the a.c. power to the
heater.
• By adjusting the value of R2, any portion of positive or
negative half cycles of the supply voltage can be passed
through the heater.
• This permits a smooth control of the heat from the heater.
THANK YOU

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Diac.pptx

  • 1. The Diac II PHYSICS – 07.04.2022 Dr.R.Hepzi Pramila Devamani, Assistant Professor of Physics, V.V.Vanniaperumal College for Women, Virudhunagar.
  • 2. The Diac • A Diac is a two-terminal, three layered bidirectional device which can be switched from its OFF state to ON state for either polarity of applied voltage. • The Diac can be constructed in either npn or pnp form. • Fig(1) shows the basic structure of a Diac in pnp form. • Fig.(2) shows the symbol of a diac. • The two leads are connected to p- regions of silicon separated by an n- region. • The structure of diac is similar to that of transistor.
  • 3. The Diac The differences are • There is no terminal attached to the base layer. • The three regions are nearly identical in size. • The doping concentrations are identical to give the device symmetrical properties.
  • 4. Operation • When a positive or negative voltage is applied across the terminals of a diac, only a small leakage current IBO will flow through the device. • As the applied voltage s increased, the leakage current will continue to flow until the voltage reaches the breakover voltage VBO. • At this point avalanche breakdown of the reverse biased junction occurs and the device exhibits negative resistance i.e the current through the device increases with the decreasing values of applied voltage. • The voltage across the device then drops to breakback voltage VW.
  • 5. V-I Characteristics of Diac • Fig shows the V-I characteristics of a diac. • For applied positive voltage less than – VBO, a small leakage current flows through the device. • Under such conditions, the diac blocks the flow of current and behaves as an open circuit. • The voltages + VBO and – VBO are the breakdown voltages and have a range of 30 to 50 V.
  • 6. V-I Characteristics of Diac • When the positive or negative voltage is equal to or greater than the breakdown voltage, diac begins to conduct and the voltage drop across it becomes a few volts. • Conduction then continues until the device current drops below its holding current. • The breakover voltage and holding current values are identical for the forward and reverse regions of the operation. • Diacs are used for triggering of triacs in adjustable phase control of a.c. mains power. • Some of the applications of diac are (i) light dimming (ii) heat control and (iii) universal motor speed control.
  • 7. Applications of Diac • Although a triac may be fired into the conducting state by a simple resistive triggering circuit, more reliable and faster turn-on may be had if a switching device is used in series with the gate. One of the switching devices that can trigger a triac is the diac. • (i) Lamp dimmer • Fig shows a typical circuit that may be used for smooth control of a.c. power fed to a lamp. • This permits to control the light output from the lamp. • The basic control is by an RC variable gate voltage arrangement. • The series R4 – C1 circuit across the triac is designed to limit the rte of voltage rise across the device during switch off.
  • 8. Lamp dimmer - Working • As the input voltage increases positively or negatively, C1 and C2 charge at a rate determined by R2 • When the voltage across C3 exceeds the breakover voltage of the diac, the diac is fired into the conducting state. • The capacitor C3 discharges through the conducting diac into the gate of the triac. • Hence the triac is turned on to pass the a.c. power to the lamp. • By adjusting the value of R2, the rate of charge of capacitors and hence the point at which triac will trigger on the positive or negative half cycle of input voltage can be controlled. • Fig shows the waveforms of supply voltage and load voltage in the diac-triac control circuit. • The firing of triac can be controlled upto a maximum of 1800. • Thus we can provide a continuous control of load voltage from zero to full r.m.s value.
  • 9. Heat Control • Fig shows a typical diac-triac circuit that is used for the smooth control of a.c. power in a heater. • The capacitor C3 in series with a choke L across the triac helps to slow-up th voltage rise across the device during switch-off. • The resistor R4 in parallel wih the diac ensures smooth control at all positions of variable resistance R2.
  • 10. Heat Control - Working • As the input voltage increases positively or negatively, C1 and C2 charge at a rate determined by R2 • When the voltage across C3 exceeds the breakover voltage of the diac, the diac conducts. • The capacitor C3 discharges through the conducting diac into the gate of the triac. • Hence the triac is turned on to pass the a.c. power to the heater. • By adjusting the value of R2, any portion of positive or negative half cycles of the supply voltage can be passed through the heater. • This permits a smooth control of the heat from the heater.