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POWER ELECTRONICS
AND
CONVERTERS
Southern School of Engineering and Technology
DEPARTMENT OF ELECTRICAL ENGINEERING
Dr. Muhammad Abrar
Power Semiconductor Devices
Power Semiconductor Diodes
 Diode is a simple Semiconductor
device which is used for many
purposes in electronic applications.
 Diode consists of two doped
semiconductors, one of a P-type and
other of N-type.
Review of Basic p-n Diode
 When Tetravalent semiconductor is doped with
pentavalent impurities , then electrons are the
majority carriers and N-type semiconductor is
formed.
 Secondly, P-type with holes as the majority carriers
is formed, when trivalent impurities are added to
the tetravalent semiconductor material.
 After that, P-type semiconductor and N-type
Semiconductor are diffused together.
Review of Basic p-n Diode
 By Diffusion, electrons from N-type region flow to
P-type region and holes flow from P-type to the N-
type region leaving behind negatively charged ions.
 In this process, electric field is created with
opposite polarities to the respective (n-type or p-
type) regions which blocks the further transfer of
both carriers and as a result, a potential barrier is
formed in between the semiconductors which is
called Depletion region.
Review of Basic p-n Diode
 The PN junction can be used according to the need and
in a controlled manner.
 It can be used in three modes, Zero bias , Forward Bias
and Reverse Bias.
 In Zero Bias mode, it remains at its neutral behaviour.
 In Forward Bias mode, a potential difference is applied
to the junction where P-type material is connected with
the positive terminal and N-type is connected with the
negative terminal of the Source.
Forward Bias mode
When this arrangement is made , opposite
polarity potential (w.r.t depletion region) breaks
the potential barrier(inside) and flow of charges
is started from both ends and as a result the
current is observed.
Reverse Bias Mode
 In Reverse Bias, P-type is connected
with negative terminal and N-type is
connected with the positive terminal of
the source.
Reverse Bias Mode
 This arrangement keeps the majority
carriers of both materials away from
breaking the depletion region and
source potential(outside) attracts the
majority carriers which results in
increment of depletion region and a
large voltage is observed.
10
The Diode Characteristic I-V
Curve
Power Diode
 Diodes are used in almost every
electronic device both on small and large
scales.
 However, diode needs some modification
in high power applications.
 Diode undergoes some problems such
as ability to conduct high current in
forward bias and to hold high voltage
and avoid breakdown in reverse bias.
 To overcome these problems, concept of
Power diodes is introduced.
Power Diode
 Power diode is built with vertical
orientation to provide extra cross-
sectional area which is required to
handle large amount of current.
 The other problem of controlling
breakdown voltage in reverse bias is
overcome by controlling the relative
factors.
Power Diode
 Breakdown occurs due to the high
electric field in potential barrier.
 Electric field and depletion width has
inverse relation (E=V/d), so to control
the break down at very high voltage,
depletion width has to be altered, and
to alter the depletion width, Doping of
the material has to be changed.
Power Diode
An extra layer of N-type material is introduced. Here, N-type in the middle
region is less doped and the other P-type and N-type materials are
normally doped.
When the diode comes in reverse bias mode, it sees a large potential
barrier across the lightly doped N-type region, which makes it able to
withstand more voltage than normal. Extra layer used here, has to
provide required majority carriers to maintain the current without
reduction during the forward bias mode.
Reverse bias i-v
characteristics of a power
Diode.
Forward bias i-v
characteristics of a power
Diode.
Difference Between Normal and
Power Diode
1- Design
Simple diodes consist of a simple PN junction. They are smaller
in size and lighter in weight, while power diodes are in modified
form and they are larger and heavier normally. Power diodes are
usually available in metal form.
2- Voltage Rating
Simple diodes are used in normal low power components so
they have a relatively low voltage ratings as compared to power
diodes. Power diodes can have very high voltage ratings usually
in thousands of volts.
Difference Between Normal and
Power Diode
 3- Current Rating
Power diodes have a high hand in Current ratings
over normal diodes , that can be in several hundred
amperes.
 4-Temperature
Major probelm in handling high power applications is
the generation of heat and temperature. Power diodes
have the accessiblity of operation at higher temperature
whereas normal diodes do not need this feature in high
priority.
 5- Cost
Power Diodes are costly as compared to the simple
diodes due to the additional components and features.
Summary
 A p-n junction diode is a minority carrier, unidirectional,
uncontrolled switching device.
 A power diode incorporates a lightly doped drift region
between two heavily doped p type and n type regions.
 Maximum reverse voltage withstanding capability of a power
diode depends on the width and the doping level of the drift
region.
 A power diode should never be subjected to a reverse
voltage greater than the reverse break down voltage.
 The i-v characteristics of a forward biased power diode is
comparatively more linear due to the voltage drop in the drift
region.
Summary
 The forward voltage drop across a
conducting power diode depends on the
width of the drift region but not affected
significantly by its doping density.
 For continuous forward biased operation the
RMS value of the diode forward current
should always be less than its rated RMS
current at a given case temperature.
 Surge forward current through a diode should
be less than the applicable surge current
rating.
Summary
 During “Turn On” the instantaneous
forward voltage drop across a diode may
reach a level considerably higher than its
steady state voltage drop for the given
forward current. This is called forward
recovery voltage.
 During “Turn Off” the diode current goes
negative first before reducing to zero.
This is called reverse recovery of a
diode.
Summary
 The peak negative current flowing through a diode
during Turn Off is called the “reverse recovery current”
of the diode.
 The total time for which the diode current remains
negative during Turn Off is called “the reverse recovery
time” of the diode.
 A diode can not block reverse voltage till the reverse
current through the diode reaches its peak value.
 Both the “reverse recovery current” and the “reverse
recovery time” of a diode depends on the forward
current during Turn Off, rate of decrease of the forward
current and the type of the diode.
Summary
 Normal or slow recovery diodes have smaller
reverse recovery current but longer reverse
recovery time. They are suitable for line
frequency rectifier operation.
 Fast recovery diodes have faster switching
times but comparatively lower break down
voltages. They are suitable for high frequency
rectifier or inverter free- wheeling operation.
 Fast recovery diodes need to be protected
against voltage transients during Turn Off”
using R-C snubber circuit.

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Lecture-2.pptx

  • 1. POWER ELECTRONICS AND CONVERTERS Southern School of Engineering and Technology DEPARTMENT OF ELECTRICAL ENGINEERING Dr. Muhammad Abrar
  • 3. Power Semiconductor Diodes  Diode is a simple Semiconductor device which is used for many purposes in electronic applications.  Diode consists of two doped semiconductors, one of a P-type and other of N-type.
  • 4. Review of Basic p-n Diode  When Tetravalent semiconductor is doped with pentavalent impurities , then electrons are the majority carriers and N-type semiconductor is formed.  Secondly, P-type with holes as the majority carriers is formed, when trivalent impurities are added to the tetravalent semiconductor material.  After that, P-type semiconductor and N-type Semiconductor are diffused together.
  • 5. Review of Basic p-n Diode  By Diffusion, electrons from N-type region flow to P-type region and holes flow from P-type to the N- type region leaving behind negatively charged ions.  In this process, electric field is created with opposite polarities to the respective (n-type or p- type) regions which blocks the further transfer of both carriers and as a result, a potential barrier is formed in between the semiconductors which is called Depletion region.
  • 6. Review of Basic p-n Diode  The PN junction can be used according to the need and in a controlled manner.  It can be used in three modes, Zero bias , Forward Bias and Reverse Bias.  In Zero Bias mode, it remains at its neutral behaviour.  In Forward Bias mode, a potential difference is applied to the junction where P-type material is connected with the positive terminal and N-type is connected with the negative terminal of the Source.
  • 7. Forward Bias mode When this arrangement is made , opposite polarity potential (w.r.t depletion region) breaks the potential barrier(inside) and flow of charges is started from both ends and as a result the current is observed.
  • 8. Reverse Bias Mode  In Reverse Bias, P-type is connected with negative terminal and N-type is connected with the positive terminal of the source.
  • 9. Reverse Bias Mode  This arrangement keeps the majority carriers of both materials away from breaking the depletion region and source potential(outside) attracts the majority carriers which results in increment of depletion region and a large voltage is observed.
  • 11. Power Diode  Diodes are used in almost every electronic device both on small and large scales.  However, diode needs some modification in high power applications.  Diode undergoes some problems such as ability to conduct high current in forward bias and to hold high voltage and avoid breakdown in reverse bias.  To overcome these problems, concept of Power diodes is introduced.
  • 12. Power Diode  Power diode is built with vertical orientation to provide extra cross- sectional area which is required to handle large amount of current.  The other problem of controlling breakdown voltage in reverse bias is overcome by controlling the relative factors.
  • 13. Power Diode  Breakdown occurs due to the high electric field in potential barrier.  Electric field and depletion width has inverse relation (E=V/d), so to control the break down at very high voltage, depletion width has to be altered, and to alter the depletion width, Doping of the material has to be changed.
  • 14. Power Diode An extra layer of N-type material is introduced. Here, N-type in the middle region is less doped and the other P-type and N-type materials are normally doped. When the diode comes in reverse bias mode, it sees a large potential barrier across the lightly doped N-type region, which makes it able to withstand more voltage than normal. Extra layer used here, has to provide required majority carriers to maintain the current without reduction during the forward bias mode.
  • 15. Reverse bias i-v characteristics of a power Diode.
  • 16. Forward bias i-v characteristics of a power Diode.
  • 17. Difference Between Normal and Power Diode 1- Design Simple diodes consist of a simple PN junction. They are smaller in size and lighter in weight, while power diodes are in modified form and they are larger and heavier normally. Power diodes are usually available in metal form. 2- Voltage Rating Simple diodes are used in normal low power components so they have a relatively low voltage ratings as compared to power diodes. Power diodes can have very high voltage ratings usually in thousands of volts.
  • 18. Difference Between Normal and Power Diode  3- Current Rating Power diodes have a high hand in Current ratings over normal diodes , that can be in several hundred amperes.  4-Temperature Major probelm in handling high power applications is the generation of heat and temperature. Power diodes have the accessiblity of operation at higher temperature whereas normal diodes do not need this feature in high priority.  5- Cost Power Diodes are costly as compared to the simple diodes due to the additional components and features.
  • 19. Summary  A p-n junction diode is a minority carrier, unidirectional, uncontrolled switching device.  A power diode incorporates a lightly doped drift region between two heavily doped p type and n type regions.  Maximum reverse voltage withstanding capability of a power diode depends on the width and the doping level of the drift region.  A power diode should never be subjected to a reverse voltage greater than the reverse break down voltage.  The i-v characteristics of a forward biased power diode is comparatively more linear due to the voltage drop in the drift region.
  • 20. Summary  The forward voltage drop across a conducting power diode depends on the width of the drift region but not affected significantly by its doping density.  For continuous forward biased operation the RMS value of the diode forward current should always be less than its rated RMS current at a given case temperature.  Surge forward current through a diode should be less than the applicable surge current rating.
  • 21. Summary  During “Turn On” the instantaneous forward voltage drop across a diode may reach a level considerably higher than its steady state voltage drop for the given forward current. This is called forward recovery voltage.  During “Turn Off” the diode current goes negative first before reducing to zero. This is called reverse recovery of a diode.
  • 22. Summary  The peak negative current flowing through a diode during Turn Off is called the “reverse recovery current” of the diode.  The total time for which the diode current remains negative during Turn Off is called “the reverse recovery time” of the diode.  A diode can not block reverse voltage till the reverse current through the diode reaches its peak value.  Both the “reverse recovery current” and the “reverse recovery time” of a diode depends on the forward current during Turn Off, rate of decrease of the forward current and the type of the diode.
  • 23. Summary  Normal or slow recovery diodes have smaller reverse recovery current but longer reverse recovery time. They are suitable for line frequency rectifier operation.  Fast recovery diodes have faster switching times but comparatively lower break down voltages. They are suitable for high frequency rectifier or inverter free- wheeling operation.  Fast recovery diodes need to be protected against voltage transients during Turn Off” using R-C snubber circuit.