Synchronous generator

2
SYNCHRONOUS GENERATOR
• Synchronous generator operates on the
principle that when the magnetic flux
linking a conductor changes, an e.m.f. is
induced in the conductor.
• It has an armature winding and a field
winding,
• It is more convenient and advantageous
to place the field winding on the rotor
and armature winding on the stator.
Introduction
Lecture Notes by Dr.R.M.Larik

3
SYNCHRONOUS GENERATOR
• It is easier to insulate stationary winding for higher voltages
because they are not subjected to centrifugal forces and also extra
space is available due to the stationary arrangement of the
armature.
• The stationary 3-phase armature can be directly connected to load
without going through large, unreliable slip rings and brush-gear.
• Since the excitation current is much smaller as compared to load
current, the slip rings and brush gear required are of light
construction.
• Due to simple and robust construction of the rotor, higher speed of
rotating d.c. field is possible.
Advantages of Stationary Armature

4
CONSTRUCTION OF SYNCHRONOUS GENERATOR
• It is the stationary part of the machine and is built up of sheet-steel
laminations having slots on its inner periphery.
• A 3-phase winding is placed in these slots and serves as the
armature winding of the alternator.
• The armature winding is connected in star with neutral grounded.
Stator
Rotor
• The rotor carries a field winding supplied with direct current
through the slip rings by a separate d.c. source.
• This d.c. source (exciter) is generally a small d.c. generator
mounted on the shaft of the alternator.
• Rotor construction is of salient (projected) pole type and non-
salient (cylindrical) pole typeLecture Notes by Dr.R.M.Larik

5
CONSTRUCTION OF SYNCHRONOUS GENERATOR (Contd.)
Rotor (Contd.)
• In this type, salient or projected
poles are mounted on a large
circular steel frame which is
fixed to the shaft of the
alternator.
• The individual field pole
windings are connected in series
such that when the field winding
is energized by the exciter,
adjacent poles have opposite
polarities.
Salient Pole Type

6
Rotor (Contd.)
• Low and medium-speed alternators (120-400 r.p.m.), those driven
by diesel engines or water turbines, have salient pole type rotors
due to the following reasons:
− The salient field poles would cause an excessive windage
loss if driven at high speed and would tend to produce noise.
− Salient-pole construction cannot be made strong enough to
withstand the mechanical stresses to which they may be
subjected at higher speeds.
Salient Pole Type (Contd.)
• For a frequency of 50 Hz, we must use a large number of poles
on the rotor of slow-speed alternators.
• Low-speed rotors possess a large diameter to provide necessary
space for the poles.Lecture Notes by Dr.R.M.Larik

7
Rotor (Contd.)
• Non-salient pole type rotor is made
of smooth solid forged-steel
cylinder having a number of slots
along the outer surface.
• Field windings are embedded in
the slots and are connected in
series to the slip rings through
which they are energized by the
d.c. exciter.
• The regions forming the poles are
left unslotted.
Non-Salient Pole Type

8
Rotor (Contd.)
• High-speed generators (1500 or 3000 r.p.m.), driven by steam
turbines, use non-salient type rotors due to the reasons:
− It gives noiseless operation at high speeds.
− The flux distribution around the periphery is nearly a sine wave
and hence a better e.m.f. waveform is obtained than in the case
of salient-pole type.
• Since steam turbines run at high speed and a frequency of 50 Hz is
required, we need a small number of poles on the rotor.
• We can not use less than 2 poles, hence, the highest possible
speed will be 3000 r.p.m.
Non-Salient Pole Type (Contd.)

9
OPERATION
• The rotor winding is energized from the d.c. exciter and alternate N
and S poles are developed on the rotor.
• When the rotor is rotated in anti-clockwise direction by a prime
mover, the stator or armature conductors are cut by the magnetic
flux of rotor poles.
• Consequently, e.m.f. is induced in the armature conductors due to
electromagnetic induction.
• The induced e.m.f. is alternating since N and S poles of rotor
alternately pass the armature conductors.
• Direction of the induced e.m.f. can be determined by Fleming’s right
hand rule and the frequency is given by;
f = NP/120
where N = speed of rotor in r.p.m.
P = number of rotor polesLecture Notes by Dr.R.M.Larik

10
OPERATION (Contd.)
• Magnitude of the voltage induced in each phase depends upon the
rotor magnetic flux, the number and position of the conductors in the
phase and the speed of the rotor.
• Magnitude of induced e.m.f. depends upon the speed of rotation
and the d.c. exciting current.
• Magnitude of e.m.f. in each phase of stator winding is same,
however, they differ in phase by 120° electrical.

11
FREQUENCY
• Frequency of induced e.m.f. in the stator depends on speed and the
number of poles.
Let N = rotor speed in r.p.m.
P = number of rotor poles
f = frequency of e.m.f. in Hz
• Consider a stator conductor that is successively swept by the N and
S poles of the rotor.
• If a positive voltage is induced when a N-pole sweeps across the
conductor, a similar negative voltage is induced when a S-pole
sweeps.

12
FREQUENCY (Contd.)
• Thus one complete cycle of e.m.f. is generated in the conductor as
a pair of poles passes it.
 No. of cycles/revolution = No. of pairs of poles = P/2
No. of revolutions/second = N/60
 No. of cycles/second = (P/2)(N/60) = N P/120
But number of cycles of e.m.f. per second is its frequency.
 f = NP/120
N is the synchronous speed generally represented by Ns
• For a given alternator, the number of rotor poles is fixed, hence, the
alternator must run at synchronous speed to give the desired
frequency.
• For this reason, an alternator is also called synchronous generator.

13
A.C. ARMATURE WINDINGS
• A.C. armature windings are generally open-circuit type i.e., both ends
are brought out.
• An open-circuit winding is one that does not close on itself i.e., a
closed circuit will not be formed until some external connection is
made to a source or load.
• The following are the general features of a.c. armature windings:
− A.C. armature windings are symmetrically distributed in slots
around the complete circumference of the armature.
− Distributed winding has two principal advantages:
a) Distributed winding generates a voltage in the form of sin wave.
b) Copper is evenly distributed on the armature surface resulting in
uniform heating of winding which can be easily cooled.

14
A.C. ARMATURE WINDINGS (Contd.)
− A.C. armature windings may use full-pitch coils or fractional-pitch
coils
− A coil with a span of 180° electrical is called a full-pitch coil with
two sides of the coil occupyng identical positions under adjacent
opposite poles and the e.m.f. generated in the coil is maximum.
− A coil with a span of less than 180° electrical is called a fractional-
pitch coil (For example, a coil with a span of 150° electrical would
be called a 5/6 pitch coil) and the e.m.f. induced in the coil will be
less than that of a full-pitch coil.
− Most of a.c. machines use double layer armature windings i.e. one
coil side lies in the upper half of one slot while the other coil side
lies in the lower half of another slot spaced about one-pole pitch
from the first one.

15
E.M.F. EQUATION
Let Z = No. of conductors or coil sides in series per phase
 = Flux per pole in webers
P = Number of rotor poles
N = Rotor speed in r.p.m.
In one revolution (60/N second), each stator conductor is cut by P
webers i.e.,
d = P; and dt = 60/N
 Average e.m.f. induced in one stator conductor
=
dϕ
dt
=
Pϕ
Τ60 N
=
PϕN
60
volts
Since there are Z conductors in series per phase,
Average e.m.f. /phase =
PϕN
60
x Z
=
PϕZ
60
x
120 f
P
N =
120 f
P
= 2 f  Z VoltsLecture Notes by Dr.R.M.Larik

16
E.M.F. EQUATION
R.M.S. value of e.m.f./phase = Average value of e.m.f. per phase x
form factor
= 2 f  Z x 1.11 = 2.22 f  Z Volts
 E r.m.s. per phase = 2.22 f  Z volts (i)
If Kp and Kd are the pitch factor and distribution factor of the armature
winding, then,
E r.m.s. per phase = 2.22 Kp Kd f  Z Volts (ii)
Sometimes the turns (T) per phase rather than conductors per phase
are specified, in that case, eq. (ii) becomes:
E r.m.s. per phase = 4.44 Kp Kd f  T Volts (iii)
The line voltage will depend upon whether the winding is star or delta
connected.

17
ARMATURE REACTION
• When an alternator is running at no-load, there will be no current
flowing through the armature winding and magnetic flux produced in
the air-gap will be only due to rotor field.
• When the alternator is loaded, the three-phase currents will produce
an additional magnetic field in the air-gap.
• The effect of armature flux on the flux produced by field ampere-turns
is called armature reaction.
• The armature flux and the flux produced by rotor ampere-turns rotate
at a synchronous speed in the same direction, hence, the two fluxes
are fixed in space relative to each other.
• Modification of flux in the air-gap due to armature flux depends on the
magnitude of stator current and on the power factor of the load.
• Load power factor determines whether the armature flux distorts,
opposes or helps the main flux.

18
ARMATURE REACTION
• When armature is on open-circuit,
there is no stator current and the flux
due to rotor current is distributed
symmetrically in the air-gap
• Since the direction of the rotor is
assumed clockwise, the generated
e.m.f. in phase R1R2 is at its
maximum and is towards the paper
in the conductor R1 and outwards in
conductor R2.
Load at Unity Power Factor
• No armature flux is produced since no current flows in the
armature winding.

19
ARMATURE REACTION (Contd.)
• In case a resistive load (unity p.f.) is
connected across the terminals of
the alternator, according to right-
hand rule, the current is “in” in the
conductors under N-pole and “out” in
the conductors under S-pole.
• Therefore, the armature flux is
clockwise due to currents in the top
conductors and anti-clockwise due to
currents in the bottom conductors.
Load at Unity Power Factor (Contd.)
• The armature flux is at 90° to the main flux (due to rotor
current) and is behind the main flux.

20
• In this case, the flux in the air-gap is distorted but not weakened.
• Therefore, at unity p.f., the effect of armature reaction is merely
to distort the main field; there is no weakening of the main field
and the average flux practically remains the same.
• Since the magnetic flux due to stator currents (i.e., armature
flux) rotate; synchronously with the rotor, the flux distortion
remains the same for all positions of the rotor.
Load at Unity Power Factor (Contd.)

21
• When a pure inductive load
(zero p.f. lagging) is connected
across the terminals of the
alternator, current lags behind
the voltage by 90°.
• This means that current will be
maximum at zero e.m.f. and
vice-versa.
Load at Zero Power Factor Lagging
• Figure shows the condition when the alternator is supplying
resistive load.
• Note that e.m.f. as well as current in phase R1R2 is maximum in this
position.

22
• When the generator is supplying a
pure inductive load, the current in
phase R1R2 will not reach its
maximum value until N-pole
advanced 90° electrical
• Now the armature flux is from right to
left and field flux is from left to right.
Load at Zero Power Factor Lagging (Contd.)
• All the flux produced by armature current (i.e., armature flux)
opposes the field flux and, therefore, weakens it.
• In other words, armature reaction is demagnetizing.

23
• When pure capacitive load (zero p.f.
leading) is connected to the alternator,
the current in armature windings will
lead the induced e.m.f. by 90°.
• Effect of armature reaction will be the
reverse that for pure inductive load.
Load at Zero Power Factor Leading
• Armature flux aids the main flux and generated e.m.f. is increased.
• Figure shows the condition when alternator is supplying resistive load
• The e.m.f. as well as current in phase R1R2 is max in this position
• When alternator is supplying pure capacitive load, the max current in
R1R2 will occur 90° before occurrence of max induced e.m.f.

24
• When the generator is supplying a
pure capacitive load, the maximum
current in R1R2 will occur 90° electrical
before the occurrence of maximum
induced e.m.f.
• Therefore, maximum current in phase
R1R2 will occur if the position of the
rotor remains 90° behind as compared
to its position under resistive load
Load at Zero Power Factor Leading (Contd.)
• It is clear that armature flux is now in the same direction as the field
flux and, therefore, strengthens it.

25
• This causes an increase in the generated voltage.
• Hence at zero p.f. leading, the armature reaction strengthens the
main flux.
• For intermediate values of p.f, the effect of armature reaction is
partly distorting and partly weakening for inductive loads.
• For capacitive loads, the effect of armature reaction is partly
distorting and partly strengthening.
Load at Zero Power Factor Leading (Contd.)

26
ALTERNATOR EQUIVALENT CIRCUIT
• All the quantities are per phase.
E0 = No-load e.m.f.
E = Load induced e.m.f.
• E is induced e.m.f. after
allowing for armature reaction.
• It is equal to phasor difference
of E0 and Ia XAR.
• Terminal voltage V is less than E by the voltage drops in XL and Ra.
 E = V + Ia (Ra + j XL )
and E0 = E + Ia ( j XAR )

27
SYNCHRONOUS REACTANCE (XS)
• Sum of armature leakage
reactance (XL) and reactance of
armature reaction (XAR) is called
synchronous reactance Xs .
Xs = XL + XAR
• It is a fictitious reactance employed to
account for the voltage effects in the
armature circuit produced by the:
− actual armature leakage reactance
− change in the air-gap flux caused by armature reaction.
• The circuit is simplified as shown.
• Synchronous impedance, Zs = Ra + j Xs

28
SYNCHRONOUS REACTANCE (XS) (Contd.)
• Synchronous impedance is the
fictitious impedance employed
to account for the voltage
effects in the armature circuit
produced by the:
− actual armature resistance
− actual armature leakage
reactance
− change in the air-gap flux produced by armature reaction.
• Relationship between generator output voltage and load terminal
voltage is given by:
E0 = V + IaZs
= V + Ia (R + j Xs)

29
PHASOR DIAGRAM OF A LOADED ALTERNATOR
• Consider a Y-connected alternator supplying inductive load, the
load p.f. angle being ϕ.
• In the last slide the figure shows the equivalent circuit of the
alternator per phase i.e. all quantities are per phase.
• Considering the vector diagram:
AC2 = AB2 + BC2
Eo
2 = (AD + BD)2 + (BE + CE)2
Since AD = V cos ϕ, BE = DF = V sin ϕ
BD = I Ra, CE = I Xs
Eo
2 = (V cos ϕ + I Ra)2 + (V sin ϕ + I Xs )2
Eo = V cos ϕ + I Ra
2 V sin ϕ + I Xs
2

30
Problem 1(a): A 3-phase, star-connected alternator supplies a load
of 10 MW at p.f. 0.85 lagging and at 11 kV (terminal voltage). Its
resistance is 0.1 ohm per phase and synchronous reactance 0.66
ohm per phase. Calculate the e.m.f. generated per phase.
Solution:
F.L. output current =
10 x 106
3 x 11000 x 0.85
= 618 A
I Ra drop = 618 x 0.1 = 61.8 V
I XS drop = 618 x 0.66 = 408 V
Terminal voltage/phase = 11,000 / 3
= 6350 V
ϕ = cos -1 (0.85) = 31.8°; sin ϕ = sin 31.8° = 0.527

31
Problem 1(a):
Solution (Contd.):
As seen from the vector diagram I instead
of V has been taken along reference
vector,
E0 = V cos ϕ + I Ro
2 + V sin ϕ + I Xs
2
= 6350 x 0.85 + 61.8 2 + 6350 x 0.527 + 408 2
= 6625 V
Problem 1(b): A 3-phase, synchronous generator is supplying a load of
100 kW at 11 kV (terminal voltage). The p.f. of load is 0.8 lagging. The
armature resistance is 0.3 ohm per phase and synchronous reactance
Xs is 0.5 ohm per phase. Calculate the e.m.f. generated in alternator.
Eo and V are per phase values.

32
VOLTAGE REGULATION
• The voltage regulation of an alternator is defined as the change in
terminal voltage from no-load to full-load (the speed and field
excitation being constant) divided by full-load voltage.
% Voltage regulation =
No load voltage − Full load voltage
Full load voltage
x 100
=
Eo − V
V
x 100
where Eo = Terminal voltage of generator at no load
V = Terminal voltage of generator at full load
• E0 - V is the arithmetic difference and not the phasor difference.
• The factors affecting the voltage regulation of an alternator are:
− i) Ia Ra drop in armature winding
− ii) Ia XL drop in armature winding
− iii) Voltage change due to armature reaction

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