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HIGH VOLTAGE ENGINEERING
Prof.P.Swaminathan
Asst.Prof.[SG]/EEE
KARUNYA UNIVERSITY
Overvoltage Phenomenon and
Insulation Coordination
NATURAL CAUSES FOR
OVERVOLTAGES —LIGHTNING
PHENOMENON
Charge Formation in the
Clouds
Cioud model according to
Simpson's theory
Mechanism of Lightning
Strokes
Travelling Waves on
Transmission Lines
Classification of Transmission
Lines
 Transmission lines are usually classified as
 (a) lines with no loss or ideal lines,
 (b) lines without distortion or
distortion less lines,
 (c) lines with small losses, and
 (d) lines with infinite and finite length defined by
all the four parameters.
Reflection and Transmission of
Waves at Transition Points
Successive reflections and
lattice diagrams
 (/) all waves travel downhill, i.e. into the positive time
 (M) the position of the wave at any instant is given by means
of the time scale at the left of the lattice diagram
 (//O the total potential at any instant of time is the
superposition of all the waves which arrive at that point until
that instant of time, displaced in position from each other by
time intervals equal to the time differences of their arrival
 (/v) attenuation is included so that the amount by which a
wave is reduced is taken care of and
 (v) the previous history of the wave, if desired can be easily
traced. If the computation is to be carried out at a point where
the operations cannot be directly placed on the lattice
diagram, the arms can be numbered and the quantity can be
tabulated and computed.
Reflection lattice of a travelling wave
Behaviour of Rectangular Travelling Wave
[Unit Step Function]
at Transition Points—Typical Cases
 Case (i): Open ended transmission line of surge
impedance Z:
 Case (Ii): Short circuited line:
 Case (Hi): Line terminated with a resistance equal
to the surge impedance of the line
 Case (Iv): Line terminated with a capacitor:
 Case (v): Transmission terminated by an
inductance L:
 Case (yi): Line having a series inductor:
 Case (ViI): Line terminated with a transformer
 (taken as an L-C parallel combination):
OVERVOLTAGE DUE TO SWITCHING
SURGES, SYSTEM FAULTS AND
OTHER ABNORMAL CONDITIONS
 Origin of Switching Surges
 The making and breaking of electric circuits with
switchgear may result in abnormal overvoltages in power
systems having large inductances and capacitances.
 The over voltages may go as high as six times the
normal power frequency voltage. In circuit breaking
operation, switching surges with a high rate of rise of
voltage may cause repeated restriking of the arc between
the contacts of a circuit breaker, thereby causing
destruction of the circuit breaker contacts.
 The switching surges may include high natural
frequencies of the system, a damped normal frequency
voltage component, or the restriking and recovery voltage
of the system with successive reflected waves from
Characteristics of Switching
Surges
 (i) De-energizing of transmission lines, cables,
shunt capacitor, banks, etc.
 (ii) Disconnection of unloaded transformers,
reactors, etc.
 (Uf) Energization or reclosing of lines and reactive
loads,
 (i v) Sudden switching off of loads.
 (v) Short circuits and fault clearances.
 (w) Resonance phenomenon like ferro-
resonance, arcing grounds, etc
Switching Overvoltages
In EHV and UHV Systems
 Interruption of low inductive currents (current
chopping) by high speed circuit breakers. This
occurs when the transformers or reactors are
switched off
 Interruption of small capacitive currents, such as
switching off of unloaded lines etc.
 ferro-resonance condition
 This may occur when poles of a circuit breaker do
not close simultaneously
 Energization of long EHV or UHV lines.
Energization of long EHV or UHV
lines
 (a) single pole closing of circuit breaker
 (b) interruption of fault current when the L-G or L-
L fault is cleared
 (c) resistance switching used in circuit breakers
 (d) switching lines terminated by transformers
 (e) series capacitor compensated lines
 (O sparking of the surge diverter located at the
receiving end of the line to limit the lightning over
voltages
Power Frequency Over voltages
in Power Systems
 The power frequency over voltages occur in
large power systems and they are of much
concern in EHV systems, i.e. systems of 400
kV and above. The main causes for power
frequency and its harmonic over voltages are
 (a) sudden loss of loads,
 (b) disconnection of inductive loads or
connection of capacitive loads,
 (c) Ferranti effect, unsymmetrical faults, and
 (d) saturation in transformers, etc.
Control of Over voltages
Due to Switching
 The overvoltages due to switching and
power frequency may be controlled by
 (d) energization of transmission lines in
one or more steps by inserting
resistances
 and withdrawing them afterwards,
 (b) phase controlled closing of circuit
breakers,
 (c) drainage of trapped charges before
reclosing,
Protection of Transmission Lines
against Over voltages
 Protection against Lightning Overvoltages
and Switching Surges of short Duration
 Overvoltages due to lightning strokes can be
avoided or minimized in practice by
 (d) shielding the overhead lines by using ground
wires above the phase wires,
 (b) using ground rods and counter-poise wires,
and
 (c) including protective devices like expulsion
gaps, protector tubes on the lines, and surge
diverters at the line terminations and substations.
Lightning Protection Using
Shielded Wires or Ground Wires
Protective Devices
 (i) Expulsion gaps
 (H) Protector tubes
 (Hi) Rod gaps
 (iv) Surge diverters or lightning arresters
Expulsion gaps
1. External series gap
2. Upper electrode
3. Ground electrode
4. Fibre tube
5. Hollow space
Protector tube mounting
 1 Line conductor on string insulator
 2. Series gap
 3. Protector tube
 4. Ground connection
 5. Cross arm
 6. Tower body
Surge diverters or lightning arresters
Valve Type Lightning Arrestor
PRINCIPLES OF INSULATION COORDINATION ON
HIGH VOLTAGE AND EXTRA HIGH VOLTAGE
POWER SYSTEMS
Basic Impulse Insulation Levels
Surge Protection of Rotating
Machine

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Overvoltage Protection Techniques for Transmission Lines

  • 1. HIGH VOLTAGE ENGINEERING Prof.P.Swaminathan Asst.Prof.[SG]/EEE KARUNYA UNIVERSITY Overvoltage Phenomenon and Insulation Coordination
  • 2. NATURAL CAUSES FOR OVERVOLTAGES —LIGHTNING PHENOMENON
  • 3. Charge Formation in the Clouds
  • 4. Cioud model according to Simpson's theory
  • 6.
  • 8. Classification of Transmission Lines  Transmission lines are usually classified as  (a) lines with no loss or ideal lines,  (b) lines without distortion or distortion less lines,  (c) lines with small losses, and  (d) lines with infinite and finite length defined by all the four parameters.
  • 9. Reflection and Transmission of Waves at Transition Points
  • 10. Successive reflections and lattice diagrams  (/) all waves travel downhill, i.e. into the positive time  (M) the position of the wave at any instant is given by means of the time scale at the left of the lattice diagram  (//O the total potential at any instant of time is the superposition of all the waves which arrive at that point until that instant of time, displaced in position from each other by time intervals equal to the time differences of their arrival  (/v) attenuation is included so that the amount by which a wave is reduced is taken care of and  (v) the previous history of the wave, if desired can be easily traced. If the computation is to be carried out at a point where the operations cannot be directly placed on the lattice diagram, the arms can be numbered and the quantity can be tabulated and computed.
  • 11. Reflection lattice of a travelling wave
  • 12. Behaviour of Rectangular Travelling Wave [Unit Step Function] at Transition Points—Typical Cases  Case (i): Open ended transmission line of surge impedance Z:  Case (Ii): Short circuited line:  Case (Hi): Line terminated with a resistance equal to the surge impedance of the line  Case (Iv): Line terminated with a capacitor:  Case (v): Transmission terminated by an inductance L:  Case (yi): Line having a series inductor:  Case (ViI): Line terminated with a transformer  (taken as an L-C parallel combination):
  • 13. OVERVOLTAGE DUE TO SWITCHING SURGES, SYSTEM FAULTS AND OTHER ABNORMAL CONDITIONS  Origin of Switching Surges  The making and breaking of electric circuits with switchgear may result in abnormal overvoltages in power systems having large inductances and capacitances.  The over voltages may go as high as six times the normal power frequency voltage. In circuit breaking operation, switching surges with a high rate of rise of voltage may cause repeated restriking of the arc between the contacts of a circuit breaker, thereby causing destruction of the circuit breaker contacts.  The switching surges may include high natural frequencies of the system, a damped normal frequency voltage component, or the restriking and recovery voltage of the system with successive reflected waves from
  • 14. Characteristics of Switching Surges  (i) De-energizing of transmission lines, cables, shunt capacitor, banks, etc.  (ii) Disconnection of unloaded transformers, reactors, etc.  (Uf) Energization or reclosing of lines and reactive loads,  (i v) Sudden switching off of loads.  (v) Short circuits and fault clearances.  (w) Resonance phenomenon like ferro- resonance, arcing grounds, etc
  • 15. Switching Overvoltages In EHV and UHV Systems  Interruption of low inductive currents (current chopping) by high speed circuit breakers. This occurs when the transformers or reactors are switched off  Interruption of small capacitive currents, such as switching off of unloaded lines etc.  ferro-resonance condition  This may occur when poles of a circuit breaker do not close simultaneously  Energization of long EHV or UHV lines.
  • 16. Energization of long EHV or UHV lines  (a) single pole closing of circuit breaker  (b) interruption of fault current when the L-G or L- L fault is cleared  (c) resistance switching used in circuit breakers  (d) switching lines terminated by transformers  (e) series capacitor compensated lines  (O sparking of the surge diverter located at the receiving end of the line to limit the lightning over voltages
  • 17. Power Frequency Over voltages in Power Systems  The power frequency over voltages occur in large power systems and they are of much concern in EHV systems, i.e. systems of 400 kV and above. The main causes for power frequency and its harmonic over voltages are  (a) sudden loss of loads,  (b) disconnection of inductive loads or connection of capacitive loads,  (c) Ferranti effect, unsymmetrical faults, and  (d) saturation in transformers, etc.
  • 18. Control of Over voltages Due to Switching  The overvoltages due to switching and power frequency may be controlled by  (d) energization of transmission lines in one or more steps by inserting resistances  and withdrawing them afterwards,  (b) phase controlled closing of circuit breakers,  (c) drainage of trapped charges before reclosing,
  • 19. Protection of Transmission Lines against Over voltages  Protection against Lightning Overvoltages and Switching Surges of short Duration  Overvoltages due to lightning strokes can be avoided or minimized in practice by  (d) shielding the overhead lines by using ground wires above the phase wires,  (b) using ground rods and counter-poise wires, and  (c) including protective devices like expulsion gaps, protector tubes on the lines, and surge diverters at the line terminations and substations.
  • 20. Lightning Protection Using Shielded Wires or Ground Wires
  • 21. Protective Devices  (i) Expulsion gaps  (H) Protector tubes  (Hi) Rod gaps  (iv) Surge diverters or lightning arresters
  • 22. Expulsion gaps 1. External series gap 2. Upper electrode 3. Ground electrode 4. Fibre tube 5. Hollow space
  • 23. Protector tube mounting  1 Line conductor on string insulator  2. Series gap  3. Protector tube  4. Ground connection  5. Cross arm  6. Tower body
  • 24. Surge diverters or lightning arresters
  • 26. PRINCIPLES OF INSULATION COORDINATION ON HIGH VOLTAGE AND EXTRA HIGH VOLTAGE POWER SYSTEMS
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  • 30. Surge Protection of Rotating Machine