Transcript Slide 1

RE1345
KONVERSI TENAGA LISTRIK II
Vita Lystianingrum
1
References
1. Theraja, B. L., ‘Electrical Technology’, S. Chand &
Company Ltd., 1978.
2. Karady, G., ‘Lecture Notes on Synchronous
Generator’,
www.eas.asu.edu/~karady/360_pp.html.
3. Zuhal, ‘Dasar Tenaga Listrik’, ITB Bandung.
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RE1345
KONVERSI TENAGA LISTRIK II
1: Klasifikasi mesin-mesin listrik dan konstruksi
2: Generator sinkron: proses terbangkitnya EMF dan macam-macam
generator sinkron
3: Generator sinkron: berbeban, kerugian tegangan, diagram vektor
untuk pf. lagging, pf. leading
4: Generator sinkron: menentukan voltage regulator dengan metode
EMF dan karakteristik
5: Generator sinkron: kerja paralel
6:
7: Motor sinkron: metode start dan pengaruh perubahan arus eksitasi
8: Motor sinkron: torque dan contoh soal
9 & 10:
UTS
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Review KTL 1:
DC Machines
• Faraday’s Law
-> Dynamically & statically induced.
4
Review: Fleming’s Right-hand Rule
Fleming's right hand rule (for
generators) shows the direction of
induced current flow when a conductor
moves in a magnetic field.
The Thumb represents the direction of
Motion of the conductor.
The First finger represents the direction
of the Field.
The Second finger represents the
direction of the induced or generated
Current
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http://www.walter-fendt.de/ph11e/generator_e.htm
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• Emf generation
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Energy Conversion
B
L
D
B
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Energy Conversion
B
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• Synchronous Generator
• Assumption: rotors are round rotor
-> related to flux distribution
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Voltage generation (Generator)
• A wire loop is rotated in a
magnetic field.
• The magnetic flux through
the loop changes by the
position
B
D
L
B
1
cos wt
2
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Voltage generation (Generator)
• Position 1 all flux links with the
loop
• Position 2 the flux linkage
reduced
1
cos wt
B
2
 t   B D L cos w t 
w  2 n
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Voltage generation (Generator)
• The induced voltage is an ac
voltage
1
B
• The voltage is sinusoidal
Vt   N
2
cos wt
d t 
d cos w t 
 N B DL
 N B D L w sin w t 
dt
dt
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• Stator winding
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1 Winding beginning,
2 Winding end,
3 Voltage,
6 A rotation = one cycle,
7 Coil
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Figure 33 Principle of the two-phase alternating
voltage generator
1 Casing,
2 Stator,
3 Field spider
4 Beginning winding one,
5 End winding one
6 Beginning winding two,
7 End winding two
**Figure 35 Principle of the three-phase
alternating generator
1 1. Winding one beginning
1.2. Winding one end
2.1. Winding two beginning
2.2. Winding two end
3.1. Winding three beginning
3.2. Winding three end
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www.crystal-netbook.info/e148915/e149917/e150166
SYNCHRONOUS MACHINES
•
•
The rotor is supplied by DC current If
that generates a DC flux f.
Operation (two poles)
Flux  f
ns
The rotor is driven by a turbine with
a constant speed of ns.
B-
C+
N
•
The rotating field flux induces a
voltage in the stator winding.
•
The frequency of the induced
voltage depends upon the speed.
A-
A+
S
C-
B+
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•
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**frequency, speed, and poles
• Synchronous generator -> means that electrical
frequency produced is synchronized with the
mechanical rate of rotation of the generator.
• A synchronous generator’s rotor consists of an
electromagnet (DC supplied).
• Rotor’s magnetic field points in whatever
direction the rotor is turned.
• Now, the rate of rotation of the magnetic fields in
the machine is related to the stator electrical
frequency by:
nm P
fe 
120
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•
18
** The frequency - speed relation
nm P
fe 
120
f = electrical frequency, Hz
nm= mechanical speed of magnetic field, rpm
P = number of poles
• Typical rotor speeds are (for 60 Hz)
• 3600 rpm for 2-pole,
• 1800 rpm for 4 pole and
• 450 rpm for 16 poles.
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•
19
• Rotor generated Flux and Induced
Voltage, Round rotor machine
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•
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SYNCHRONOUS MACHINES
Rotor generated Flux and Induced
Voltage, Round rotor machine
•
For the calculation of the induced
voltage, the machine is simplified.
•
On the stator windings of each
phase is represented by one
equivalent coil.
•
•
Similarly on the rotor’s dc winding
is represented by an equivalent
coil.
The rotor coil is supplied by a dc
current I f and has N f turns. This
generates a flux 
Magnetic axis of phase A
Qm= 00
C+
BN

A+
AS
C-
B+
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•
21
SYNCHRONOUS MACHINES
Round Rotor generated flux
Magnetic axis of the rotor
•
Q m= 0o
The rotor generated field is
constant along the gap. The field is
calculated by the Ampere law.
C+
BN
A+
AS
•
The upper part of the rotor the B
lines going out, the lower part
entering into the rotor.
C-
B+
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•
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SYNCHRONOUS MACHINES
Q
• The rotor and with the rotor
the flux rotates with an
angular speed of w
Qm
C+
BN
A+
A-
S
C-
B+
• The flux linkage depend on
the rotor position.
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•
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SYNCHRONOUS MACHINES
All flux links with phase A,
when Q is 00 deg.
Magnetic axis of
phase A
The flux linkage is zero,
when Q is +/-900.
Magnetic axis of
phase A
Qm= 00
C+
B-
Qm= 900
C+
B-
N
N
A+
A-
A+
A-
S
S
C-
B+
C-
B+
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•
24
• Ende..
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•
25
26
•
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27
•
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1 Winding beginning,
2 Winding end,
3 Voltage,
4 A cycle
5 A rotation = two cycles,
6 A rotation = one cycle,
7 Coil
8 Coil connection
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•
28
• Breadth factor, distribution, etc…
• Exciter -> w/ brush; brushless; etc ->
chapman
• Open-circuit characteristic / magnetization
curve of the machine
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•
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