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Government College of Engineering, Aurangabad
Department of Electrical Engineering
Presentation on
Inductive Power Transfer
PRESENTED BY
Sukanya Jadhav
(ME16F12F012)
M. E. (EPS)
GUIDEDED BY
Prof.
M.R.Bachawad
2016-17
Contents
 Introduction
 IPT Power supplies
 Functions of an IPT
 IPT equations
 Application
 Conclusion
Inductive power transfer
What is Inductive Power Transfer
The Basic principle
 IPT finds application in factory
automation, for lighting applications, for
instrumentation and electronic systems.
 IPT is also used for powering electric
vehicles(EV).
 These are hands-free charging systems
that are unaffected by dirt, chemicals, or
the weather
 Can be extended to dynamic charging systems
where a vehicle may be charged while it is in
motion on an instrumented lane along the road.
 Such systems offer convenience and reliability
and surprisingly may well be the lowest cost of
all private transportation options including
conventional vehicles.
 But in achieving these features there are some
significant difficulties that must be overcome.
IPT POWER SUPPLIES
 At the present time, IPT power supplies typically
operate from a three-phase utility to produce a current in
the track at the desired frequency.
 This track current is commonly a constant current so that
all pickups on the track have the same magnetic
excitation.
 The track frequency may typically be anywhere in the
range 5–140 kHz, although in lower power levels even
higher frequencies may be used.
 The power supply either operates at a fixed frequency or
a variable frequency.
Functions of an IPT System
Fig: General arrangement for an IPT
system.
 A power supply takes power from a utility and
energizes a primary loop or track to which pickup
coils may be magnetically attached.
 In its most basic form, an IPT pickup consists of a
coil of wire in close proximity to the track wires
positioned to capture magnetic flux around the
track conductor.
 A voltage is induced in this coil as described by
Ampere’s and Faraday’s laws.
 Conceptually, this is very similar to a
transformer, though with a much lower magnetic
coupling.
The Basic IPT Equation
The performance of an IPT pickup is primarily determined
from two parameter:
 the open circuit voltage induced in the pickup coil at
frequency (ὠ)due to the primary track current(I1),
Voc= jὠMI1
 And its short circuit current Isc= MI1/L2
Where M is mutual inductance between the track and
pick up coil
And ὠL2 is the pickup coil inductance.
 The product of these two parameters
results in the uncompensated VA of
the pickup Su
 So the equation for IPT is
 Without compensation, the maximum
power that can be drawn from a pickup is
Su/2
 In order to improve the available power,
the pickup inductor is compensated with
capacitors.
 Normally, the compensation capacitor C2
is applied either directly in series or in
parallel, although parallel tuned pickups
are more common due to their inherent
current limiting capabilities
 The output power equation after tuning becomes,
 Where Q is the tuned quality factor, which is
determined by the output load or controller by
controlling the output voltage/current
Applications
Primary coil of a Monorail
 Energy has been coupled from a primary to a
secondary across an air gap of significant but small
proportions that stays relatively constant, even in
the presence of movement.
 The primary coil on a monorail has the form of an
elongated loop that is loosely coupled to a pickup
coil on a vehicle and may transfer 1–10 kW of
power across a 4–10-mm gap.
 With an Automatic Guided Vehicles (AGV), the air
gap may be 10–20 mm, and there may be a
possible misalignment of similar magnitude (10–20
mm).
 Now a days, efforts are taken for improvement of
tolerance to misalignment
Car Charging
Concept of Wireless Charging
Factory Automation Material handling
Tunnel Lighting
Conclusion
 In conclusion, it is clear that inductive
coupling power transmission would be
extremely beneficial to society if it were
implemented in homes and home
electronics.
 It is also highly beneficial to industries
and conventional transportation.
 Huge changes can be done after research
in this field
References
“Inductive Power Transfer” By Grant A.
Covic, Senior member IEEE, and John
T. Boys.
“Inductive Power Transfer, Powering
our future” By Grant A. Covic
www.conductix.in
www.electronicdesign.com

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Inductive power transfer

  • 1. Government College of Engineering, Aurangabad Department of Electrical Engineering Presentation on Inductive Power Transfer PRESENTED BY Sukanya Jadhav (ME16F12F012) M. E. (EPS) GUIDEDED BY Prof. M.R.Bachawad 2016-17
  • 2. Contents  Introduction  IPT Power supplies  Functions of an IPT  IPT equations  Application  Conclusion
  • 4. What is Inductive Power Transfer
  • 6.  IPT finds application in factory automation, for lighting applications, for instrumentation and electronic systems.  IPT is also used for powering electric vehicles(EV).  These are hands-free charging systems that are unaffected by dirt, chemicals, or the weather
  • 7.  Can be extended to dynamic charging systems where a vehicle may be charged while it is in motion on an instrumented lane along the road.  Such systems offer convenience and reliability and surprisingly may well be the lowest cost of all private transportation options including conventional vehicles.  But in achieving these features there are some significant difficulties that must be overcome.
  • 8. IPT POWER SUPPLIES  At the present time, IPT power supplies typically operate from a three-phase utility to produce a current in the track at the desired frequency.  This track current is commonly a constant current so that all pickups on the track have the same magnetic excitation.  The track frequency may typically be anywhere in the range 5–140 kHz, although in lower power levels even higher frequencies may be used.  The power supply either operates at a fixed frequency or a variable frequency.
  • 9. Functions of an IPT System Fig: General arrangement for an IPT system.
  • 10.  A power supply takes power from a utility and energizes a primary loop or track to which pickup coils may be magnetically attached.  In its most basic form, an IPT pickup consists of a coil of wire in close proximity to the track wires positioned to capture magnetic flux around the track conductor.  A voltage is induced in this coil as described by Ampere’s and Faraday’s laws.  Conceptually, this is very similar to a transformer, though with a much lower magnetic coupling.
  • 11. The Basic IPT Equation The performance of an IPT pickup is primarily determined from two parameter:  the open circuit voltage induced in the pickup coil at frequency (ὠ)due to the primary track current(I1), Voc= jὠMI1  And its short circuit current Isc= MI1/L2 Where M is mutual inductance between the track and pick up coil And ὠL2 is the pickup coil inductance.
  • 12.  The product of these two parameters results in the uncompensated VA of the pickup Su  So the equation for IPT is
  • 13.  Without compensation, the maximum power that can be drawn from a pickup is Su/2  In order to improve the available power, the pickup inductor is compensated with capacitors.  Normally, the compensation capacitor C2 is applied either directly in series or in parallel, although parallel tuned pickups are more common due to their inherent current limiting capabilities
  • 14.  The output power equation after tuning becomes,  Where Q is the tuned quality factor, which is determined by the output load or controller by controlling the output voltage/current
  • 16. Primary coil of a Monorail
  • 17.  Energy has been coupled from a primary to a secondary across an air gap of significant but small proportions that stays relatively constant, even in the presence of movement.  The primary coil on a monorail has the form of an elongated loop that is loosely coupled to a pickup coil on a vehicle and may transfer 1–10 kW of power across a 4–10-mm gap.  With an Automatic Guided Vehicles (AGV), the air gap may be 10–20 mm, and there may be a possible misalignment of similar magnitude (10–20 mm).  Now a days, efforts are taken for improvement of tolerance to misalignment
  • 22. Conclusion  In conclusion, it is clear that inductive coupling power transmission would be extremely beneficial to society if it were implemented in homes and home electronics.  It is also highly beneficial to industries and conventional transportation.  Huge changes can be done after research in this field
  • 23. References “Inductive Power Transfer” By Grant A. Covic, Senior member IEEE, and John T. Boys. “Inductive Power Transfer, Powering our future” By Grant A. Covic www.conductix.in www.electronicdesign.com