CHAPTER 3
INDUCTION MACHINE
3.1 INTRODUCTION
·
Induction motor is the common type of AC motor.
·
Induction motor was invented by Nicola Tesla
(1856-1943) in 1888.
·
Also known as asynchronous motor.
·
It has a stator and a rotor mounted on bearings
and separated from the stator by an air
gap.
·
It requires no
electrical connection to the rotating member.
·
Such motor are classified induction machines
because the rotor voltage (which
produce the
rotor current and the rotor magnetic field) is induced in the rotor winding
rather than being physically connected by wires.
·
The transfer of energy from the stationary
member to the rotating member is by
means of
electromagnetic induction.
·
This motor is widely used by the industries
because:
- Rugged. -
Simple construction.
- Robust. -
Reliable.
- High
efficiency. -
Good power factor.
- Require less
maintenance -
Easy to start.
- Rotates
itself without external assistant.
- Less
expensive than direct current motor of equal power and speed.
·
The weaknesses of this machine are:
- Low starting
torque if compared to dc shunt motor.
- Speed will be
reduced when load increased.
- Speed can’t
be changed without reducing efficiency.
·
Small single phase induction motors (in
fractional horsepower rating) are used in
many household
appliances such as:
- Blenders
- Lawn mowers
- Juice mixers
- Washing machines
- Refrigerators
·
Two phase induction motors are used primarily as
servomotor in control system.
·
Large three phase induction motors (in ten or hundreds
of horsepower) are used in:
- Pumps -
Fans
- Compressors -
Paper mills
- Textile mills,
and so forth.
3.2 INDUCTION MOTOR CONSTRUCTION
·
Unlike dc machine, induction machine have a
uniform air gap.
·
Composed by two main parts:
- Stator
- Rotor
·
Figure 4.1 and 4.2 show the inside of induction
machine.
Figure 3.1
Figure 3.2
Stator
ConstructionThe stator and the rotor are electrical circuits that perform as electromagnets. The stator is the stationary electrical part of the motor. The stator core of a NEMA motor is made up of several hundred thin laminations.
Figure 3.3:Stator core
Stator
WindingsStator laminations are stacked together forming a hollow cylinder. Coils of insulated wire are inserted into slots of the stator core.
Figure 3.4:Stator winding
Each grouping of coils, together with the
steel core it surrounds, form an electromagnet. Electromagnetism is the
principle behind motor operation. The stator windings are connected directly to
the power source.Rotor Construction
·
The rotor also consists of laminated
ferromagnetic material, with slot cuts on the
outer surface.
·
The rotor are of two basic types :
- Squirrel cage
- Wound rotor
Squirrel cage rotor
·
It consist of a series of a conducting bars laid
into slots carved in the face of the rotor
and shorted at
either ends by large shorting ring.
·
This design is referred to as squirrel cage
rotor because the conductors would look like one of the exercise wheels that
squirrel or hamsters run on.
·
Small squirrel cage rotors use a slotted core of laminated steel into
which molten aluminums cast to form the conductor, end rings and fan blades.
·
Larger squirrel cage rotors use brass bars and brass end rings that are brazed
together
to form the
squirrel cage.
·
Skewing the rotor slots help to:
- Avoid
crawling (locking in at sub-synchronous speeds)
- Reduce
vibration
·
Squirrel cage rotor is better than wound rotor
because it is:
- Simpler
- More rugged
- More economical
- Require less
maintenance
Figure 3.5:Squirrel cage Rotor
Figure 3.6 : Rotor core
Figure 3.7
Wound rotor
·
Has a complete set of three phase insulated
windings that are mirror images of the
winding on
stator.
·
Its three phase winding are usually wye
connected and ends of three rotor wires are
tied to a slip
rings on the rotor shaft.
·
The rotor winding are shorted through carbon
brushes riding on the slip rings.
·
The existence of rheostat enable user to modify
the torque speed characteristic of the
motor. It is
used to adjust the starting torque and running speed.
·
The three phase rheostat is composed of three
rheostat connected in wye with a
common lever.
·
Lever is used to simultaneously adjust all the
three rheostat arms. Eg: Moving
rheostat to the
zero resistance position shorts the
resistor and simulates a squirrel cage motor.
·
Are rarely used because:
- More
expensive than squirrel cage induction motor.
- Larger than
squirrel cage induction motor with similar power.
- Require
frequent maintenance due to wear associates to brushes and slip ring.
Figure 3.8 Wound
rotor induction motor showing rheostat connections
Figure 3.9:Wound rotor
3.3 ROTATING
MAGNETIC FIELD
·
When a three phase stator winding is connected
to a three-phase voltage supply,
three-phase currents will flow in
the winding which induce three-phase flux in the stator.
·
These flux will rotate at a speed called as Synchronous
Speed, ns.
·
The flux is called as rotating magnetic field.
·
The equation is:- where f = supply
frequency , p = no. of poles
·
Rotating magnetic field will cause the rotor to
rotate the same direction as the stator
flux.
·
Torque direction is always the same as the flux
rotation.
·
At the time of starting the motor, rotor speed
is 0.
·
The rotating magnetic field will cause the rotor
to rotate from 0 speed to a speed that
is lower than the synchronous
speed.
·
If the rotor speed is equal to the
synchronous speed, there will be no cutting of flux
and rotor current equals zero.
Therefore, it is not possible for the rotor to rotate at ns.
3.4 SLIP AND ROTOR
SPEED
·
Slip is defined as :
where ns = synchronous speed in rpm
n = rotor speed in rpm
·
Slip can also represented in percent.
·
The frequency of the rotor, fr is:
where s = slip
f
= supply frequency
Example 1
Calculate the synchronous speed of a 3-phase induction
motor having 20 poles when it is
connected to a 50 Hz source.
Solution
Example 2
A 0.5 hp, 6-pole induction motor is excited by a 3 –phase,
60 Hz source. If the full-load speed is 1140 rpm, calculate the slip.
Solution
Example 3
The 6-pole,wound-rotor induction motor is excited by a
3-phase, 60 Hz source. Calculate the frequency of the rotor current under the
following conditions:
(i) at standstill
(ii) motor turning at 500 rpm in the same direction as the
revolving field
(iii) motor turning at 500 rpm in the opposite direction to
the revolving field
(iv) motor turning at 2000 rpm in the same direction as the
revolving field
Solution
ns = 120f / p = 120(60/6) = 1200 rpm
(i) n=0
=
fr = sf =
1 x 60 = 60Hz
(ii) n = +500
=
fr = sf =
0.583 x 60 = 35 Hz
(iii) n = -500
= (s>1 motor is
operating as a brake)
fr = sf =
1.417 x 60 = 85 Hz
(iv)n = +2000
=
fr = sf =
-0.667 x 60 = -40 Hz (-ve means that the
phase sequence of the voltages induced in the rotor winding is reversed)
Example 4
A 3-phase, 4 pair of poles, 400kW,400V,60Hz induction motor is 780 rpm full-load speed.
Determine the frequency of the rotor current under full load condition.
Solution
f rotor = sf
n s =
=
3.5 PER-PHASE EQUIVALENT CIRCUIT OF THREE-PHASE INDUCTION MOTOR
The per-phase equivalent circuit
of a three-phase induction motor is just like a single –phase transformer
equivalent circuit.
The difference is only that the secondary
winding is short-circuited unlike in the
transformer it is open-circuited as a load is to be connected later.
Complete Equivalent Circuit
For Induction Machine Referred To The
Stator Circuit
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Figure 3.10
The subscript ‘1’ is refering to the stator side while ‘2’ is referring
to the rotor side
R1, X1, R2,
Rm , Xm are value perphase
Input Power, Pin = 3V1I1cosθ
Stator copper loss, Pscl = 3I12R1
Core Loss, Pcl = 3V12/Rm
(always neglected because
too small)
Power across the air-gap, Pag
=
3I22R2 /s
= Pin - Pscl - Pcl
Rotor copper loss, Prcl = 3I22R2
Mechanical power/gross output
power/converted power,
P mech = Pag – Prcl
= 3I22R2
/s - 3I22R2
=
Pag (1-s)
Net power output, Poutput
= P mech – P friction & windage loss
For Torque:
Maximum Slip:
3.6 POWER FLOW OF AN INDUCTION MOTOR
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Figure 3.11
Example 5
A 10 poles, 50 Hz, Y connection 3-phase induction motor having a rating of 60kW and 415V. The slip of the motor is 5% at 0.6 power factor lagging. If the full load
efficiency is 90%, calculate:
(i) Input power
(ii) Line current and phase current
(iii) Speed of the rotor (rpm)
(iv) Frequency of the rotor
(v) Torque developed by the motor (if friction and windage
losses is 0)
Solution
(i) η =
(ii) Y connection, IΦ = IL, VΦ=
P in =3VΦIΦcos=
IL=
IΦ = IL=154.59A
(iii) n s =
n = n s (1-s)
= 600 (1-0.05) = 570 rpm
(iv) fr =
sf = 0.05(50) = 2.5Hz
(v) T =
Or
ws=
wm = ws(1-s)
= 62.83(1-0.05) = 59.69 rad/s
Example 6
A 3-phase, delta connection, 4 pole, 440V, 60 Hz induction motor having a rotor speed 1200rpm
and 50kW input power at 0.8 power factor lagging. The copper losses and iron
losses in the stator amount to 2kW and the windage and friction losses are 3kW. Determine:
(i) Net output power
(ii) Efficiency
(iii) Input current
Solution
(i) ns =
120f/p = 120(60)/4 = 1800 rpm
=
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P net output = 29kW
(ii) η =
(iii)Δ connection
Example 7
A 3-phase induction motor, delta connection,5 pair of poles,
60 Hz is connected to a 440V source.The slip is 3% and the windage and friction losses are 3kW. The equivalent circuit perphase referred
to the stator circuit is:-
R1 = Stator resistance = 0.4Ω
X1 = Stator leakage inductance = 1.4Ω
R2’ = Rotor resistance = 0.6Ω
X2’ = Rotor leakage inductance = 2Ω
Rm = no-load loses resistance = 150Ω
Xm = magnetizing reactance = 20Ω
Calculate:
(i) Input power
(ii) Speed of the
rotor
(iii) Mechanical power
(iv) Developed torque
(v) Efficiency
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(i) P in
=3VIcosθ
V = 440V
Z total =
Pin =
3(440)(29.64)cos(-50.460) = 24907.5W
(ii)
,
n = ns(1-s) , n
= 720(1-0.03) = 698.4 rpm
(iii) Pm = 3(I22R2/s
– I22R2)
V2 = 440 – I1Z1
= 440 – (18.87-22.86j)(0.4+j1.4)
= 400.45-17.27j V
I2 = A
Pm = 3
[19.942 - 19.942(0.6)] = 23140.5W
(iv) T dev
=
Pag = 3I22R2/s = 3(19.94)2(0.6)/(0.03)
= 23856.2W
ws =
T =
(v)
Example 8
A 3-phase
induction motor, wye connection, 60 Hz is connected to a 220V source.The
slip is 5% and
rotor speed is 855 rpm. The equivalent
circuit perphase is:-
R1 = Stator resistance = 0.4Ω
X1 = Stator leakage inductance = 1Ω
R2’ = Rotor resistance = 0.8Ω
X2’ = Rotor leakage inductance = 3.5Ω
Rm = no-load loses resistance = 150Ω
Xm = magnetizing reactance = 10Ω
Calculate:
(i) Number of poles
(ii) Input power
(iii) Mechanical power
(iv) Developed torque
(v) Efficiency
Solution
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(i) n = 855rpm
s = 0.05
ns = 120f/p
, sns =
ns – n , n = ns –
sns
= ns(1-s)
ns
=
=
ns = 120f/p
p =
(ii) Pin
=
Z total =Ω
Pin =
(iii) Pm = 3(I22R2/s
– I22R2)
V2 = – I1Z1
= – (6.53-j12.73)(0.4+j1)
= 111.68-1.438j V
I2 = A
Pm = 3
[6.82 - 6.82(0.8)] = 2108.54W
(iv) T dev =
Pag = 3I22R2/s
ws =
T = (3I22R2/s)
/ ws =[3(6.8)2(0.8)/(0.05)] / 94.25 = 23.55Nm
(v)
3.7 TORQUE SPEED CHARACTERISTICS
Figure 3.12
There are 3 regions involve in a
3-phase induction motor:-
(i) Braking/Plugging
Braking process
occurs at s>0(positive slip). In this case the motor acts as a brake where
it rotates in opposite direction respect to the rotor.(2<slip<1).
(ii) Motoring
Motoring is the
region where induction motor acts as a motor. Slip is reducing from 1 into 0.
Slip equals to 0 at synchronous speed,ns.(1<slip<0).
(iii) Generating
Generating
region is a region where motor acts as a generator. During this time the slip
is negative. At this time, the motor acts as a generator.(slip<0)
3.8 DETERMINATION OF CIRCUIT MODEL PARAMETER
The parameter of the equivalent
circuit can be determined from the results of a:
- No load test
- Blocked rotor test
-.DC test
The blocked rotor test:
- To determine X1 and
X2
- When combines with DC test, it
also determines R2
- Test is performed by blocking
the rotor so that it cannot turn and measuring the line
voltage, line current and three phase power input to the stator
- Connection for the test is
shown in Figure 4.13
Figure
3.13 Basic circuit for blocked rotor
test and no load test
The no load test:
- To determine magnetizing
reactance, Xm, and the combined core, friction and windage
losses (these losses are essentially constant for all load condition)
- The connection for the no load
test are identical to those shown in Figure 12
- However, the rotor is unblocked
and allowed to run unloaded at rated voltage and rated
frequency
DC test:
- To determine R1
- Accomplished by connecting any
two stator leads to a variable voltage DC source as
shown in Figure 4.14.
- The DC source is adjusted to
provide approximately rated stator current, and the
resistance between two stator leads is determined from voltmeter and
ammeter reading
Figure
3.14 Basic circuit for DC test
Example 9
The following test data were taken on a 7.5hp, four pole,
208 V, 60 Hz Y connected design A induction motor having a rated current of
28A.
DC test : Vdc
= 13.6V Idc = 28 A
No-load test: Vt = 208 V f = 60 Hz
Ia
= 8.12 A P in
= 420 W
Ib
= 8.2 A
Ic
= 8.18 A
Locked rotor test: Vt = 25 V f = 15 Hz
Ia
= 28.1 A P in
= 920 W
Ib
= 28 A
Ic
= 27.6 A
Sketch the per-phase equivalent circuit for this motor.
Solution
From the DC
test,
From the no-load test,
Pscl = 3I12R1 =
3(8.17A)2(0.243Ω) = 48.7W
Pag = Pin
–Pscl = 420W- 48.7W = 371.3W
From the locked-rotor test,
θ = cos-1
R1 + R2 = 0.517(cos 40.4°) = 0.394Ω
DC test, R1 = 0.243Ω, R2 = 0.394Ω – 0.243Ω = 0.151Ω
At 15 Hz, X = 0.517(sin 40.4°)=0.335Ω
At 60 Hz, X = = X1 + X2
For class A induction motor, this reactance is assumed to be
divided equally between the rotor and stator,
X1 = X2 = 0.67 Ω
Xm
= 14.7 -0.67 = 14.03Ω
3.9 STARTING OF INDUCTION
MOTOR
(i) Direct On Line
Starter(DOL)
- A widely-used starting method of electric
motors.
- The simplest motor starter.
- A DOL starter connects the motor terminals directly to the power supply.
- Hence, the motor is subjected to the full voltage of the power supply.
- Consequently, high starting current flows through the motor.
-This type of starting is suitable for small motors below 5 hp
(3.75 kW).
- Most motors are reversible or, in other words, they can be run clockwise
and anti-
clockwise.
- A reversing starter is an electrical or electronic circuit that reverses
the direction of a
motor automatically.
- Logically, the circuit is composed of two DOL circuits; one for clockwise
operation and
the other for anti-clockwise
operation.
- It takes a starting current 6(six) times the
full load current.
- For large
motor the high starting current causes voltage drop in the power system which
may trip other motors in the systems.
(ii)Star-Delta Starter
- For
star-delta connection the motor windings are connected in star during starting.
- The
connection is changed to delta when the motor starts running.
- The
starting current and starting torque of DOL started and start-delta connected
motors are as follows:
Example:
DOL -6I and 2T
Star-delta - 2I and 2T/3
DOL -6I and 2T
Star-delta - 2I and 2T/3
- Thus it can be seen that the starting current and starting torque are both reduced.
- The motor
should be capable to start at such reduced torque with load.
- The Star Delta starter can only be used with a motor
which is rated for connection in
delta operation at
the required line voltage
(iii)Autotransformer starter
- An Auto transformer starter
uses an auto transformer to reduce the voltage applied to a
motor during start.
- The auto transformer may
have a number of output taps and be set-up to provide a single stage starter,
or a multistage starter.
- Typically, the auto
transformer would have taps at 50%, 65% and 80% voltage,
enabling the motor to be started at one or
more of these settings.
- As the motor approaches full
speed, the auto transformer is switched out of the circuit
Tutorial 3
1. A 3 phase
induction machine 373kW, 6 poles is connected to a 440V, 50 Hz, has a full load
speed of 950 rpm. If the machine is comprised of 6 poles, calculate the
frequency of the rotor current during full load.
2. Determine the
synchronous speed of a six pole 460V 60 Hz induction motor if the frequency is
reduced to 85 % of its rated value.
3. A 4 pole induction machine is supplied
by 60 Hz source and having 4% of full load slip. Calculate the rotor frequency
during:
(i) Starting
(ii) Full load
4. A 3-phase induction motor, delta/star
connection, 2 poles, 50 Hz is connected to a 410V
source .The rotor
speed is 2880 rpm and the windage and friction losses are 600 W. The
equivalent
circuit perphase referred to the stator circuit is:-
R1 = 0.4Ω X2 = 2 Ω
X1 = 2 Ω Rm = 150Ω
R2 = 2 Ω Xm = 20Ω
Calculate:
(i) Input power
(ii) Air-gap power
(iii) Mechanical power
(iv) Developed torque/torque induced
(v) Efficiency
5. A 440V, 50Hz, 10 pole, delta/Y
connected induction motor is rated at 100kW. The
equivalent
parameter for the motor are:
At full load condition , the friction and windage losses are
400W, the miscellaneous losses are 100W and the core losses are 1000W. The slip
of the motor is 0.04.
(i) Calculate
the input power
(ii) Calculate
the stator copper loss
(iii) Calculate the air
gap power
(iv) Calculate
the converted power
(v) Calculate
the torque induced by the motor
(vi) Calculate the
load torque
(vii) Calculate
the starting torque
(viii) Calculate
the maximum torque and slip
(ix) Calculate
the efficiency of the motor
6. Squirrel cage and wound rotors are the two common types of rotor
used in
induction machines. Give four(4)
advantages of squirrel cage rotor.
7. A 4 pole induction machine is
supplied by 50 Hz source and having 4% of full load
slip. Find the
rotor frequency during:
(i) Starting
(ii) Full load
8. A 3-phase, Y-connected,
50 Hz, 4 pair of poles,
induction motor having 720 rpm full
load speed. The motor is
connected to a 415 V supply. The machine has the following
impedances in ohms per phase
referred to the stator circuit:
R1 = 0.2
Ω X1 = 2.0
Ω
R2 = 0.9
Ω X2 = 4.0
Ω
Xm = 60 Ω
If
the total friction and windage losses are 200 W,
(i)
Find the slip, s.
(ii) Find the input power, Pin.
(iii) Find
the air gap power, Pag.
(iv) Find
the mechanical power, Pm.
(v)
Find the torque induced by the motor, τ ind.
(vi) Find
the efficiency of the motor.
9. Induction machine is a common type
of AC machine. State three weaknesses of the
induction
machine.
10. A 3-phase, delta-connected,
50 Hz, 2 pair of poles,
induction motor having 1455
rpm full load speed. The motor
is connected to a 415 V supply. The machine has the
following impedances in ohms
per phase referred to the stator circuit:
R1
= 0.2 Ω X1 = 0.6
Ω
R2 = 0.9 X2 = 0.4
Ω
Xm = 20 Ω
If the total friction and windage losses are 1000 W,
calculate:
(i) Slip
(ii) Input
power, Pin
(iii)Air
gap power, Pag
(iv) Mechanical
power, Pconv
(v) Torque
induced by the motor, τ ind
(vi)Efficiency
of the motor
11. A 3-phase,
Y-connected, 6 poles, 415 V, 50 Hz induction motor having a rotor speed 950
rpm. The input power is 100 kW at 0.85 power factor lagging. The copper
and iron losses in the stator are 4 kW and the windage and friction
losses are 4 kW. Determine the output power
of the motor.