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Troubleshooting, Maintenance & 
Protection of AC Electrical 
Motors and Drives 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Industrial Electricity 
Industrial electricity is all about Single-phase 
and Three-phase transformers, AC and DC 
machines - their construction, design, testing, 
operation and maintenance. 
For troubleshooting Electrical equipment and 
control circuits, it is important to know the 
basic principals on which the electrical 
equipment works. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Principle of a transformer 
A transformer works on the principle of 
electromagnetic induction - an e.m.f. is 
induced in a coil if it links a changing flux. 
Transformers are designed to change the 
voltage of electrical power supply from one 
value to another. They are widely used in 
power systems. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
e.m.f. Induced 
f = fmax sinwt 
fmax –the maximum value of the flux in webers, 
w = 2pf 
f – frequency in cycles per secs. 
The e.m.f. induced in the winding is given by Faraday’s Law and 
the direction of induced e.m.f. is given by Lenz’s Law. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Faraday’s Law 
When the flux linking with the circuit changes, an e.m.f. is induced in 
the circuit proportional to the rate of change of flux. The instantaneous 
value of the e.m.f. induced in the primary winding is given by : 
e1 = – N1 df 
dt 
The maximum e.m.f. is given by : 
E1max = – 2 p fmax f N1 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Lenz’s Law 
The polarity of the induced e.m.f. is given by the Lenz’s Law. 
The direction of the induced e.m.f. is such that the current induced by it 
tends to stop the change producing it. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Ideal Transformer 
• Winding resistances are negligible 
• All flux produced is confined to core of transformer and links fully both 
windings 
• The permeability of the core is high enough so magnetizing current 
required to produce flux and establish it in the core is negligible. 
• Eddy current and hysteresis losses are negligible 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
V = -E1 
E2 
E1 
I0 
I1 
V = -E 1 1 
I (Negligible) 0 
E = V I 2 2 2 
E1 
(a) No Load (b) On Load 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
I1 
2 
(N /N ) 1 2 
I2 I2 
I1 I1 
Z2 
N1 N1 N2 N2 Z2 
Z2 
V1 V1 
V1 
2 
(N /N ) 1 2 
(A) (B) ( C ) 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Testing Transformers 
• Measurement of winding resistance 
• Measurement of Voltage ratio 
• Test Phasor voltage relationship 
• Measurement of impedance voltage, short circuit 
• impedance and load loss. 
• Measurement of no load loss and no load current. 
• Measurement of insulation resistance. 
• Dielectric test 
• Temperature rise 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Electromechanical Energy Conversion 
• The electromechanical energy conversion device is a link 
between electrical and mechanical systems. 
• When the mechanical system delivers energy through the 
device to the electrical system, the device is called a generator. 
• When electrical system delivers energy through device to 
the mechanical system, the device is called a motor. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
For a Generator 
Tm = Te + Tf 
and, e and i are in same direction. 
where, 
Tm – is Mechanical Torque 
Te – is Electrical Torque 
Tf – is Torque lost due to friction 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Right-hand Rule 
Hold the conductor in right hand with fingers closed 
around conductor and thumb pointing towards 
the direction of the current. The fingers will point towards the 
direction of the magnetic lines of the flux produced around the 
conductor. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Cork Screw Rule 
The direction and the travel in which it has to be 
rotated are related to each other the same way as the 
direction of the current in the conductor and the 
direction of the field that would be produced due to the 
current. The magnetic field exists in the plane 
perpendicular to the conductor. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Flux produced by Current 
Carrying Coil 
Flux can be produced by causing the current to flow through a 
coil instead of a conductor. 
The direction of the magnetic flux in the coil is given by the 
Right-hand rule. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
E.m.f induced due to Rotation of a Conductor in a 
Magnetic Field 
The e.m.f. induced due to rotation of a conductor or a coil 
in a magnetic field is given as: 
e.m.f. (e) = B L v 
where: 
B – is flux density of magnetic field (wb/m2) 
L – length of the conductor perpendicular to magnetic 
field (meters) 
v – velocity of conductor (m/sec) 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Fleming’s Right Hand Rule for Determining the Direction 
of e.m.f. Induced 
Fleming’s right hand rule states that if the forefinger of the 
right hand points in the direction of the field and the thumb 
towards the motion, then the middle finger points towards the 
direction of e.m.f. induced. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Fleming’s Left Hand Rule 
Gives the relationship between the direction of the current, the 
direction of field and the direction of the motion. If the 
forefinger of the left hand points towards the field, the middle 
finger points towards the direction of the current and the 
thumb points towards the direction of motion. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Force on a Conductor in a Magnetic Field 
If a conductor carries current in a magnetic field, then a 
mechanical force is exerted on it. The force exerted on the 
conductor is given as : 
F = B L I 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Torque on a Conductor in a Magnetic Field 
If the conductor on a rotor has a radius of r, then the torque produced on 
the conductor is given as : 
T = F r 
or 
T = B L I r 
For a coil with two sides, the electromagnetic torque will be double. 
The Power is given as : 
Power = T wr 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
A Generator or a Motor Action 
e.m.f. is induced enough to overcome the drop of volts in 
resistance of the winding and supply the load at the required 
voltage. 
The electromagnetic torque produced by current-carrying 
conductors is counter torque, opposing the rotation. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Motor Armature 
The rotational or speed e.m.f is produced in opposition to the 
applied voltage. This is known as counter or back e.m.f. 
Mechanical torque is produced as required by the load driven 
by the motor. For more torque and mechanical power output, 
there must be more input to the motor from the mains. The 
motor draws current according to the requirement of the load. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Basic Characteristics of Electrical Machines 
• The voltages are induced in the windings, the load currents 
and the terminals voltages under different loading conditions. 
• The speed at which the machine works under different 
loading conditions, frequency. 
• The power input or the output received from the machine. 
• The torque produced under different loading conditions. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Single Phase Power System 
W= V I cosf 
here, 
W– is the power (watts) 
V – is R.M.S. Voltage 
I – is R.M.S. Current 
cosf – is Power Factor [ =W/ V I ] 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Three-Phase Power Systems 
For Delta-connected system : 
Line Voltage = Phase Voltage 
Line Current = 1.732 * Phase Current 
For Star-connected system : 
Line Voltage = 1.732 * Phase Voltage 
Line Current = Phase Current 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Clamp-on Meter 
When an AC circuit is to be tested, a Clip-around or clamp-on 
meter is quite useful. The clamp-on meter has a probe in the 
form of iron or ferrite core which can be opened to allow it to 
be clamped-on or clipped over the current carrying conductor. 
When the clip is closed, it forms the magnetic core of a 
transformer. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Megohmmeter 
High resistance measurements of the order of megaohms are 
required in electrical equipment testing and troubleshooting. 
Megohmmeter based on megaohm Bridge method is used for 
high resistance measurements. 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Harmonics 
• Fundamental frequency of AC power distribution system 
is 50Hz or 60 Hz 
• Harmonic frequency - Any sinusoidal frequency, which is 
a multiple of the fundamental frequency 
• Can be even or odd multiples of the sinusoidal 
fundamental frequency 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Linear and Non Linear Loads 
• Linear electric load - Draws purely sinusoidal current 
when connected to sinusoidal voltage source – 
Resistors, capacitors, inductors 
• Non Linear electric load – Draws non-sinusoidal 
current when connected to sinusoidal voltage source – 
diode bridge, thyristor bridge, variable speed drives, 
rectifiers 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Fundamental wave with 3rd Harmonic 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
Harmonic Order 
• The Multiple, that the harmonic frequency is of the 
fundamental frequency 
Harmonic frequencies of 50 Hz fundamental are: 
Even Harmonics Odd Harmonics 
2nd harmonic -100 Hz 3rd harmonic - 150 Hz 
4th harmonic - 200 Hz 5th harmonic - 250 Hz 
6th harmonic -300 Hz 7th harmonic - 350 Hz 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
DO YOU WANT TO KNOW MORE? 
If you are interested in further training or information, 
please visit: 
http://idc-online.com/slideshare 
www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss

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Troubleshooting, Maintenance and Protection of AC Electrical Motors and Drives

  • 1. Troubleshooting, Maintenance & Protection of AC Electrical Motors and Drives www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 2. Industrial Electricity Industrial electricity is all about Single-phase and Three-phase transformers, AC and DC machines - their construction, design, testing, operation and maintenance. For troubleshooting Electrical equipment and control circuits, it is important to know the basic principals on which the electrical equipment works. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 3. Principle of a transformer A transformer works on the principle of electromagnetic induction - an e.m.f. is induced in a coil if it links a changing flux. Transformers are designed to change the voltage of electrical power supply from one value to another. They are widely used in power systems. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 4. e.m.f. Induced f = fmax sinwt fmax –the maximum value of the flux in webers, w = 2pf f – frequency in cycles per secs. The e.m.f. induced in the winding is given by Faraday’s Law and the direction of induced e.m.f. is given by Lenz’s Law. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 5. Faraday’s Law When the flux linking with the circuit changes, an e.m.f. is induced in the circuit proportional to the rate of change of flux. The instantaneous value of the e.m.f. induced in the primary winding is given by : e1 = – N1 df dt The maximum e.m.f. is given by : E1max = – 2 p fmax f N1 www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 6. Lenz’s Law The polarity of the induced e.m.f. is given by the Lenz’s Law. The direction of the induced e.m.f. is such that the current induced by it tends to stop the change producing it. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 7. Ideal Transformer • Winding resistances are negligible • All flux produced is confined to core of transformer and links fully both windings • The permeability of the core is high enough so magnetizing current required to produce flux and establish it in the core is negligible. • Eddy current and hysteresis losses are negligible www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 8. V = -E1 E2 E1 I0 I1 V = -E 1 1 I (Negligible) 0 E = V I 2 2 2 E1 (a) No Load (b) On Load www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 9. I1 2 (N /N ) 1 2 I2 I2 I1 I1 Z2 N1 N1 N2 N2 Z2 Z2 V1 V1 V1 2 (N /N ) 1 2 (A) (B) ( C ) www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 10. Testing Transformers • Measurement of winding resistance • Measurement of Voltage ratio • Test Phasor voltage relationship • Measurement of impedance voltage, short circuit • impedance and load loss. • Measurement of no load loss and no load current. • Measurement of insulation resistance. • Dielectric test • Temperature rise www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 11. Electromechanical Energy Conversion • The electromechanical energy conversion device is a link between electrical and mechanical systems. • When the mechanical system delivers energy through the device to the electrical system, the device is called a generator. • When electrical system delivers energy through device to the mechanical system, the device is called a motor. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 12. For a Generator Tm = Te + Tf and, e and i are in same direction. where, Tm – is Mechanical Torque Te – is Electrical Torque Tf – is Torque lost due to friction www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 13. Right-hand Rule Hold the conductor in right hand with fingers closed around conductor and thumb pointing towards the direction of the current. The fingers will point towards the direction of the magnetic lines of the flux produced around the conductor. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 14. Cork Screw Rule The direction and the travel in which it has to be rotated are related to each other the same way as the direction of the current in the conductor and the direction of the field that would be produced due to the current. The magnetic field exists in the plane perpendicular to the conductor. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 15. Flux produced by Current Carrying Coil Flux can be produced by causing the current to flow through a coil instead of a conductor. The direction of the magnetic flux in the coil is given by the Right-hand rule. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 16. E.m.f induced due to Rotation of a Conductor in a Magnetic Field The e.m.f. induced due to rotation of a conductor or a coil in a magnetic field is given as: e.m.f. (e) = B L v where: B – is flux density of magnetic field (wb/m2) L – length of the conductor perpendicular to magnetic field (meters) v – velocity of conductor (m/sec) www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 17. Fleming’s Right Hand Rule for Determining the Direction of e.m.f. Induced Fleming’s right hand rule states that if the forefinger of the right hand points in the direction of the field and the thumb towards the motion, then the middle finger points towards the direction of e.m.f. induced. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 18. Fleming’s Left Hand Rule Gives the relationship between the direction of the current, the direction of field and the direction of the motion. If the forefinger of the left hand points towards the field, the middle finger points towards the direction of the current and the thumb points towards the direction of motion. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 19. Force on a Conductor in a Magnetic Field If a conductor carries current in a magnetic field, then a mechanical force is exerted on it. The force exerted on the conductor is given as : F = B L I www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 20. Torque on a Conductor in a Magnetic Field If the conductor on a rotor has a radius of r, then the torque produced on the conductor is given as : T = F r or T = B L I r For a coil with two sides, the electromagnetic torque will be double. The Power is given as : Power = T wr www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 21. A Generator or a Motor Action e.m.f. is induced enough to overcome the drop of volts in resistance of the winding and supply the load at the required voltage. The electromagnetic torque produced by current-carrying conductors is counter torque, opposing the rotation. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 22. Motor Armature The rotational or speed e.m.f is produced in opposition to the applied voltage. This is known as counter or back e.m.f. Mechanical torque is produced as required by the load driven by the motor. For more torque and mechanical power output, there must be more input to the motor from the mains. The motor draws current according to the requirement of the load. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 23. Basic Characteristics of Electrical Machines • The voltages are induced in the windings, the load currents and the terminals voltages under different loading conditions. • The speed at which the machine works under different loading conditions, frequency. • The power input or the output received from the machine. • The torque produced under different loading conditions. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 24. Single Phase Power System W= V I cosf here, W– is the power (watts) V – is R.M.S. Voltage I – is R.M.S. Current cosf – is Power Factor [ =W/ V I ] www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 25. Three-Phase Power Systems For Delta-connected system : Line Voltage = Phase Voltage Line Current = 1.732 * Phase Current For Star-connected system : Line Voltage = 1.732 * Phase Voltage Line Current = Phase Current www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 26. Clamp-on Meter When an AC circuit is to be tested, a Clip-around or clamp-on meter is quite useful. The clamp-on meter has a probe in the form of iron or ferrite core which can be opened to allow it to be clamped-on or clipped over the current carrying conductor. When the clip is closed, it forms the magnetic core of a transformer. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 27. Megohmmeter High resistance measurements of the order of megaohms are required in electrical equipment testing and troubleshooting. Megohmmeter based on megaohm Bridge method is used for high resistance measurements. www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 28. Harmonics • Fundamental frequency of AC power distribution system is 50Hz or 60 Hz • Harmonic frequency - Any sinusoidal frequency, which is a multiple of the fundamental frequency • Can be even or odd multiples of the sinusoidal fundamental frequency www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 29. Linear and Non Linear Loads • Linear electric load - Draws purely sinusoidal current when connected to sinusoidal voltage source – Resistors, capacitors, inductors • Non Linear electric load – Draws non-sinusoidal current when connected to sinusoidal voltage source – diode bridge, thyristor bridge, variable speed drives, rectifiers www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 30. Fundamental wave with 3rd Harmonic www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 31. Harmonic Order • The Multiple, that the harmonic frequency is of the fundamental frequency Harmonic frequencies of 50 Hz fundamental are: Even Harmonics Odd Harmonics 2nd harmonic -100 Hz 3rd harmonic - 150 Hz 4th harmonic - 200 Hz 5th harmonic - 250 Hz 6th harmonic -300 Hz 7th harmonic - 350 Hz www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss
  • 32. DO YOU WANT TO KNOW MORE? If you are interested in further training or information, please visit: http://idc-online.com/slideshare www.idc-online.com/slideshare TTeecchhnnoollooggyy TTrraaiinniinngg tthhaatt Wwoorrkkss