1. By: Dr Rosemizi Abd Rahim
EKT 103
CHAPTER 4
AC Machine
By: Dr Rosemizi Abd Rahim

2. AC Machine
Alternating current (ac) is the primary source of electrical energy.
It is less expensive to produce and transmit alternating current (ac) than direct current (dc).
For this reason, and because ac voltage is induced into the armature of all generators, ac machines are generally more practical.
It is very easy to step up or step down the voltage for AC electricity through the use of transformers. It is not very straight forward to step up or step down the voltage for DC electricity- for power loads, it is typically done through inversion to AC- stepping up/down using a transformer- and rectification back to DC.
May function as a generator (mechanical to electrical) or a motor (electrical to mechanical)

3. DC Machine & AC machine
AC motor - no need rectification, so don't need split rings.
DC motor - ends of the coil connect to a split ring to 'rectify' the emf produced

4. AC Motor As in the DC motor case,
a current is passed through the coil, generating a torque on the coil.
Since the current is alternating, the motor will run smoothly only at the frequency of the sine wave.

5. AC Generator
This process can be described in terms of Faraday's law when you see that the rotation of the coil continually changes the magnetic flux through the coil and therefore generates a voltage

6. Generator and Motor

7. How Does an Electric Generator Work?

8. Classification of AC Machines
Two major classes of machines;
i) Synchronous Machines:
• Synchronous Generators: A primary source of electrical energy.
• Synchronous Motors: Used as motors as well as power factor compensators (synchronous condensers).
ii) Asynchronous (Induction) Machines:
• Induction Motors: Most widely used electrical motors in both domestic and industrial applications.
• Induction Generators: Due to lack of a separate field excitation, these machines are rarely used as generators.

9. Synchronous Machine

10. Synchronous Machine Origin of name: syn = equal, chronos = time
Synchronous machines are called ‘synchronous’ because their mechanical shaft speed is directly related to the power system’s line frequency.
the rotating air gap field and the rotor rotate at the same speed, called the synchronous speed.
Synchronous machines are ac machine that have a field circuit supplied by an external dc source.
DC field winding on the rotor,
AC armature winding on the stator

11. Synchronous Machine
Synchronous machines are used primarily as generators of electrical power, called synchronous generators or alternators.
They are usually large machines generating electrical power at hydro, nuclear, or thermal power stations.
Synchronous motors are built in large units compare to induction motors (Induction motors are cheaper for smaller ratings) and used for constant speed industrial drives
Application as a motor: pumps in generating stations, electric clocks, timers, and so forth where constant speed is desired.

12. Synchronous Machine fe is the power line frequency.
The frequency of the induced voltage is related to the rotor speed by:
where P is the number of magnetic poles
fe is the power line frequency.
Typical machines have two-poles, four-poles, and six-poles

13. Synchronous Machine Construction Energy is stored in the inductance
As the rotor moves, there is a change in the energy stored
Either energy is extracted from the magnetic field (and becomes mechanical energy – motor)
Or energy is stored in the magnetic field and eventually flows into the electrical circuit that powers the stator – generator

14. Synchronous Machine
Construction
DC field windings are mounted on the (rotating) rotor - which is thus a rotating electromagnet
AC windings are mounted on the (stationary) stator resulting in three-phase AC stator voltages and currents
The main part in the synchronous machines are
i) Rotor
ii) Stator

15. Synchronous Machine Rotor
There are two types of rotors used in synchronous machines:
i) cylindrical (or round) rotors
ii) salient pole rotors
Machines with cylindrical rotors are typically found in higher speed higher power applications such as turbogenerators. Using 2 or 4 poles, these machines rotate at 3600 or 1800 rpm (with 60hz systems). 
Salient pole machines are typically found in large (many MW), low mechanical speed applications, including hydrogenerators, or smaller higher speed machines (up to 1-2 MW).
Salient pole rotors are less expensive than round rotors.

16. Synchronous Machine – Cylindrical rotor
Turbine
D » 1 m
L » 10 m
Steam
d-axis
q-axis
Stator winding
    High speed
3600 r/min Þ 2-pole
1800 r/min Þ 4-pole
î    Direct-conductor cooling (using hydrogen or water as coolant)
î   Rating up to 2000 MVA N
Uniform air-gap
Stator
Rotor winding
Rotor S
Turbogenerator

17. Synchronous Machine – Cylindrical rotor
Stator
Cylindrical rotor

18. Synchronous Machine – Salient Pole
Most hydraulic turbines have to turn at low speeds (between 50 and 300 r/min)
A large number of poles are required on the rotor
Turbine
Hydro (water)
D » 10 m
Non-uniform air-gap N S
d-axis
q-axis
Hydrogenerator

19. Synchronous Machine – Salient Pole
Stator
Salient-pole rotor

20. Synchronous machine rotors are simply rotating electromagnets built to have as many poles as are produced by the stator windings.
Dc currents flowing in the field coils surrounding each pole magnetize the rotor poles.
The magnetic field produced by the rotor poles locks in with a rotating stator field, so that the shaft and the stator field rotate in synchronism.
Salient poles are too weak mechanically and develop too much wind resistance and noise to be used in large, high-speed generators driven by steam or gas turbines. For these big machines, the rotor must be a solid, cylindrical steel forging to provide the necessary strength.

21. Axial slots are cut in the surface of the cylinder to accommodate the field windings.
Since the rotor poles have constant polarity they must be supplied with direct current.
This current may be provided by an external dc generator or by a rectifier.
In this case the leads from the field winding are connected to insulated rings mounted concentrically on the shaft.
Stationary contacts called brushes ride on these slip rings to carry current to the rotating field windings from the dc supply.
The brushes are made of a carbon compound to provide a good contact with low mechanical friction.
An external dc generator used to provide current is called a “ brushless exciter “.

22. Synchronous Machine Stator
The stator of a synchronous machine carries the armature or load winding which is a three-phase winding.
The armature winding is formed by interconnecting various conductors in slots spread over the periphery of the machine’s stator. Often, more than one independent three phase winding is on the stator. An arrangement of a three-phase stator winding is shown in Figure below. Notice that the windings of the three-phases are displaced from each other in space.

23. Synchronous Machine
Construction
Stator

24. Synchronous Machine
Magnetomotive Forces (MMF’s) and Fluxes Due to Armature and Field Windings
Flux produced by a stator winding

25. Synchronous Machine
Magnetomotive Forces (MMF’s) and Fluxes Due to Armature and Field Windings

26. Synchronous Machine
Magnetomotive Forces (MMF’s) and Fluxes Due to Armature and Field Windings
Two Cycles of mmf around the Stator

27. Synchronous Generator
Equivalent circuit model – synchronous generator

28. If the generator operates at a terminal voltage VT while supplying a load corresponding to an armature current Ia, then;
In an actual synchronous machine, the reactance is much greater than the armature resistance, in which case;
Among the steady-state characteristics of a synchronous generator, its voltage regulation and power-angle characteristics are the most important ones. As for transformers, the voltage regulation of a synchronous generator is defined at a given load as;

29. Synchronous Generator
Phasor diagram of a synchronous generator
The phasor diagram is to shows the relationship among the voltages within a phase (Eφ,Vφ, jXSIA and RAIA) and the current IA in the phase.
Unity P.F (1.0)

30. Synchronous Generator
Lagging P.F
Leading P.F.

31. Synchronous Generator
Power and Torque
In generators, not all the mechanical power going into a synchronous generator becomes electric power out of the machine
The power losses in generator are represented by difference between output power and input power shown in power flow diagram below

32. Synchronous Generator
Losses
Rotor
- resistance; iron parts moving in a magnetic field causing
currents to be generated in the rotor body
- resistance of connections to the rotor (slip rings)
Stator
- resistance; magnetic losses (e.g., hysteresis)
Mechanical
- friction at bearings, friction at slip rings
Stray load losses
- due to non-uniform current distribution

33. Synchronous Generator
The input mechanical power is the shaft power in the generator given by equation:
The power converted from mechanical to electrical form internally is given by
The real electric output power of the synchronous generator can be expressed in line and phase quantities as
and reactive output power

34. Synchronous Generator
In real synchronous machines of any size, the armature resistance RA is more than 10 times smaller than the synchronous reactance XS (Xs >> RA). Therefore, RA can be ignored

35. Synchronous Motor

36. Synchronous Motor
Power Flow

37. Example : Synchronous Generator.
A three-phase, wye-connected 2500 kVA and 6.6 kV generator operates at full-load. The per-phase armature resistance Ra and the synchronous reactance, Xd, are (0.07+j10.4).
Calculate the percent voltage regulation at
0.8 power-factor lagging, and
0.8 power-factor leading.

38. Solution.

39. Induction Machine
The machines are called induction machines because of the rotor voltage which produces the rotor current and
the rotor magnetic field is induced in the rotor windings.
Induction generator has many disadvantages and low efficiency. Therefore induction machines are usually referred to as induction motors.

40. Induction Machine
Three-phase induction motors are the most common and frequently encountered machines in industry
simple design, rugged, low-price, easy maintenance
wide range of power ratings: fractional horsepower to 10 MW
run essentially as constant speed from no-load to full load
Its speed depends on the frequency of the power source
not easy to have variable speed control
requires a variable-frequency power-electronic drive for optimal speed control

41. Construction Slip rings
Cutaway in a typical wound-rotor IM. Notice the brushes and the slip rings
Brushes

42. Construction An induction motor has two main parts
i) a stationary stator
consisting of a steel frame that supports a hollow, cylindrical core
core, constructed from stacked laminations (why?),
having a number of evenly spaced slots, providing the space for the stator winding
Stator of IM

43. Construction ii) a revolving rotor
composed of punched laminations, stacked to create a series of rotor slots, providing space for the rotor winding
conventional 3-phase windings made of insulated wire (wound-rotor) » similar to the winding on the stator
aluminum bus bars shorted together at the ends by two aluminum rings, forming a squirrel-cage shaped circuit (squirrel-cage)

44. Construction Two basic design types depending on the rotor design
squirrel-cage: conducting bars laid into slots and shorted at both ends by shorting rings.
wound-rotor: complete set of three-phase windings exactly as the stator. Usually Y-connected, the ends of the three rotor wires are connected to 3 slip rings on the rotor shaft. In this way, the rotor circuit is accessible.

45. Construction
1. Squirrel cage – the conductors would look like one of the exercise wheels that squirrel or hamsters run on.

46. Construction
2. Wound rotor – have a brushes and slip ring at the end of rotor
Notice the slip rings

47. Rotating Magnetic Field
Balanced three phase windings, i.e. mechanically displaced 120 degrees form each other, fed by balanced three phase source
A rotating magnetic field with constant magnitude is produced, rotating with a speed
Where fe is the supply frequency and
P is the no. of poles and nsync is called
the synchronous speed in rpm
(revolutions per minute)

48. Synchronous speed P 50 Hz 60 Hz 2 3000 3600 4 1500 1800 6 1000 1200 8
750
900 10
600
720 12
500

49. Principle of operation
This rotating magnetic field cuts the rotor windings and produces an induced voltage in the rotor windings
Due to the fact that the rotor windings are short circuited, for both squirrel cage and wound-rotor, and induced current flows in the rotor windings
The rotor current produces another magnetic field
A torque is produced as a result of the interaction of those two magnetic fields
Where ind is the induced torque and BR and BS are the
magnetic flux densities of the rotor and the stator respectively

50. Induction motor speed At what speed will the IM run?
Can the IM run at the synchronous speed, why?
If rotor runs at the synchronous speed, which is the same speed of the rotating magnetic field, then the rotor will appear stationary to the rotating magnetic field and the rotating magnetic field will not cut the rotor. So, no induced current will flow in the rotor and no rotor magnetic flux will be produced so no torque is generated and the rotor speed will fall below the synchronous speed
When the speed falls, the rotating magnetic field will cut the rotor windings and a torque is produced

51. Induction motor speed
So, the IM will always run at a speed lower than the synchronous speed
The difference between the motor speed and the synchronous speed is called the Slip (s)
Where nslip= slip speed
nsync= speed of the magnetic field
nm = mechanical shaft speed of the motor

52. The Slip Where s is the slip
Notice that : if the rotor runs at synchronous speed
s = 0
if the rotor is stationary
s = 1
Slip may be expressed as a percentage by multiplying the above eq. by 100, notice that the slip is a ratio and doesn’t have units

53. Induction Motors and Transformers
Both IM and transformer works on the principle of induced voltage
Transformer: voltage applied to the primary windings produce an induced voltage in the secondary windings
Induction motor: voltage applied to the stator windings produce an induced voltage in the rotor windings
The difference is that, in the case of the induction motor, the secondary windings can move
Due to the rotation of the rotor (the secondary winding of the IM), the induced voltage in it does not have the same frequency of the stator (the primary) voltage

54. Frequency
The frequency of the voltage induced in the rotor is given by
Where fr = the rotor frequency (Hz)
P = number of stator poles
n = slip speed (rpm)

55. Frequency
What would be the frequency of the rotor’s induced voltage at any speed nm?
When the rotor is blocked (s=1) , the frequency of the induced voltage is equal to the supply frequency
On the other hand, if the rotor runs at synchronous speed (s = 0), the frequency will be zero

56. Torque
While the input to the induction motor is electrical power, its output is mechanical power and for that we should know some terms and quantities related to mechanical power
Any mechanical load applied to the motor shaft will introduce a Torque on the motor shaft. This torque is related to the motor output power and the rotor speed
and

57. Horse power
Another unit used to measure mechanical power is the horse power
It is used to refer to the mechanical output power of the motor
Since we, as an electrical engineers, deal with watts as a unit to measure electrical power, there is a relation between horse power and watts

58. Example
A 208-V, 10hp, four pole, 60 Hz, Y-connected induction motor has a full-load slip of 5 percent
What is the synchronous speed of this motor?
What is the rotor speed of this motor at rated load?
What is the rotor frequency of this motor at rated load?
What is the shaft torque of this motor at rated load?

59. Solution

60. Equivalent Circuit
The induction motor is similar to the transformer with the exception that its secondary windings are free to rotate
As we noticed in the transformer, it is easier if we can combine these two circuits in one circuit but there are some difficulties

61. Equivalent Circuit
When the rotor is locked (or blocked), i.e. s =1, the largest voltage and rotor frequency are induced in the rotor.
On the other side, if the rotor rotates at synchronous speed, i.e. s = 0, the induced voltage and frequency in the rotor will be equal to zero.
Where ER0 is the largest value of the rotor’s induced voltage obtained at s = 1(locked rotor)

62. Equivalent Circuit The same is true for the frequency, i.e.
It is known that
So, as the frequency of the induced voltage in the rotor changes, the reactance of the rotor circuit also changes
Where Xr0 is the rotor reactance
at the supply frequency
(at blocked rotor)

63. Equivalent Circuit
Then, we can draw the rotor equivalent circuit as follows
Where ER is the induced voltage in the rotor and RR is the rotor resistance

64. Equivalent Circuit Now we can calculate the rotor current as
Dividing both the numerator and denominator by s so nothing changes we get
Where ER0 is the induced voltage and XR0 is the rotor reactance at blocked rotor condition (s = 1)

65. Equivalent Circuit
Now we can have the rotor equivalent circuit

66. Equivalent Circuit
Now as we managed to solve the induced voltage and different frequency problems, we can combine the stator and rotor circuits in one equivalent circuit
Where

67. Power losses in Induction machines
Copper losses
Copper loss in the stator (PSCL) = I12R1
Copper loss in the rotor (PRCL) = I22R2
Core loss (Pcore)
Mechanical power loss due to friction and windage
How this power flow in the motor?

68. Power flow in induction motor

69. Power relations

70. Equivalent Circuit We can rearrange the equivalent circuit as follows
Resistance equivalent to mechanical load
Actual rotor resistance

71. Power relations

72. Power relations 1 s
1-s

73. Example A 480-V, 60 Hz, 50-hp, three phase induction motor is
drawing 60A at 0.85 PF lagging. The stator copper losses
are 2 kW, and the rotor copper losses are 700 W. The
friction and windage losses are 600 W, the core losses are
1800 W, and the stray losses are negligible. Find the
following quantities:
The air-gap power PAG.
The power converted Pconv.
The output power Pout.
The efficiency of the motor.

74. Solution

75. Solution

76. Example
A 460-V, 25-hp, 60 Hz, four-pole, Y-connected induction motor has the
following impedances in ohms per phase referred to the stator circuit:
R1= 0.641 R2= 0.332
X1=  X2=  XM= 26.3 
The total rotational losses are 1100 W and are assumed to be constant.
The core loss is lumped in with the rotational losses. For a rotor slip of
2.2 percent at the rated voltage and rated frequency, find the motor’s
Speed
Stator current
Power factor
Pconv and Pout
ind and load
Efficiency

77. Solution

78. Solution

79. Solution

80. Induction Motor – Power and Torque
The output power can be found as
Pout = Pconv – PF&W – Pmisc
The induced torque or developed torque:

81. Example A two-pole, 50-Hz induction motor supplies 15kW to a
load at a speed of 2950 rpm.
What is the motor’s slip?
What is the induced torque in the motor in N.m under these conditions?
What will be the operating speed of the motor if its torque is doubled?
How much power will be supplied by the motor when the torque is doubled?

82. Solution

83. Solution
In the low-slip region, the torque-speed curve is linear and the induced torque is direct proportional to slip. So, if the torque is doubled the new slip will be 3.33% and the motor speed will be