modul mesin arus bolak-balik
DESCRIPTION
Modul untuk kuliah MACTRANSCRIPT
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MESIN ARUS BOLAK-BALIK
TE 1403
Dr. Dedet C. Riawan, ST., M.Eng
Electrical Engineering Department
Institut Teknologi Sepuluh Nopember Surabaya
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Construction of Synchronous Generator
Stator
Rotor
pole
Shaft
Armature
winding
Field
winding
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Construction of Synchronous Generator
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Excitation of Field Windings
1. Static excitation system fed through slip ring and brushes
2. Rotating excitation system mounted on the shaft brushless
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Excitation System with Slip Ring & Brushes
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Brushless Excitation System
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Interaction of Rotor & Stator Magnetic Fileds
No-load operation
Br induces EA at stator
V = EA
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Interaction of Rotor & Stator Magnetic Fileds
On-load operation
Stator is connected to a load
IA flows in stator producing magnetic field BS BS induces ESTAT at its own stator winding
EA =V + ESTAT
Armature reaction voltage
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Interaction of Rotor & Stator Magnetic Fileds
On-load operation
Br coincide with EA
BS coincides with ESTATThus Bnet will coincide with Vf
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Equivalent Circuit with Armature Reaction
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Armature Reaction & Self-Inductance Voltage
Synchronous Reactance
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Phasor Diagram of Synchronous Generator
Unity power factor
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Phasor Diagram of Synchronous Generator
Lagging power factor
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Phasor Diagram of Synchronous Generator
Leading power factor
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Power & Torque in Synchronous Generator
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Power Angle in Synchronous Generator
If RA
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Parameters of Synchronous Generator
1. Relationship between field current and flux (and therefore between the
field current and EA)
2. The synchronous reactance
3. Armature resistance
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Open-Circuit Test
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Open-Circuit Characteristic
SaturatedUnsaturated
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Short-Circuit Test
V = 0
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Short-Circuit Characteristic
Unsaturated
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Determining the Synchronous Reactance
From OCC
From SCC
For a given field current IF
Given IF
VOC
IA
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Limitation on OCC-SCC method
Note:
EA is obtained from OCC ranging from unsaturated to saturated region
IA is obtained from SCC unsaturated region
Accurate up to unsaturated synchronous reactance
XS,u
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Example of OCC & SCC test results
15.915.214.213.212.811.810.58.76.2Voc
(kV)
300250200162.51501251007550If (A)
Synchronous generator of 10-MVA 13-kV, 3-phase, 50-Hz, Y connected
OCC
SCC
Excitation current of If= 100-A is required to obtain rated IA.
ZPF
Excitation current of If= 290-A is required to obtain rated IA at zero pf
and rated voltage.
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0
100
200
300
400
500
600
700
800
900
1000
0 100 200 300 400If (A)
Isc(A)
0
2
4
6
8
10
12
14
16
18
20
If (A)
Voc(kV)
Example of OCC & SCC test results
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Armature Reaction & Leakage Reactance
Test with Zero Power Factor (ZPF) at IA rated.
Bnet = BR + BS
Bnet ~ ErBR ~ EaBstat ~ -Ear
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Potiers Method
1.Find P from ZPF test
2.Find P from SCC
3.Draw RP = OP
4.Draw RS parallel to initial of OCC slope(OS)
5.Draw SQ perpendicular to RP
Procedure:
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Potiers Method
SQ =IA xl
PQ =BS
Voltage drop due to leakage reactance
Magnetic flux due to armature reaction = Ifar ~ Ear
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Flux and Induced Voltage in Synchronous Generator
Bnet = BR + BS
Er = Ea Ear
Vt = Er - IAXl
where
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Paralleling Synchronous Generators
Purpose of paralleling generator:
1. Meet the demand on loads
2. Increasing reliability
3. Scheduling and maintenance
4. Load sharing for efficient operation
8-MW
8-MW
8-MW
4-MW
4-MW
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Paralleling Synchronous Generators
Requirements:
The rms line voltages of the two generators must be equal.
The two generators must have the same phase sequence.
The phase angles of the two a phases must be equal.
The frequency of the new generator, called the oncoming generator, must beslightly higher than the frequency of the running system.
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Procedure of Paralleling Synchronous Generators
1. Adjust field current until terminal voltage of two generators are equal in
magnitude.
2. Checked phase sequence of two generators. They must be equal.
3. Adjust the frequency of oncoming generator slightly higher.
4. Close the tie breaker
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Paralleling Synchronous Generators
If the rms line voltages of the two generators IS NOT equal
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Paralleling Synchronous Generators
If the two generators DO NOT have the same phase sequence
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Paralleling Synchronous Generators
If the phase angles of the two a phases IS NOT equal
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Paralleling Synchronous Generators
If the frequency of the two generators IS NOT equal
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Paralleling Synchronous Generators
If the frequency and phase sequence of the two generators ARE NOT equal
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Speed Governor in Stand-Alone Operation
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Speed Droop Principle
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Speed Droop Principle
Concept of Speed Droop
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Speed Droop in Stand-alone Operation
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Speed Droop in Stand-alone Operation
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Speed Droop in Stand-alone Operation
Summary:
Active & reactive power supplied by generator will be the amount demanded byload
Governor set point of generator will control the operating frequency (fsys).
Field current regulator will control terminal voltage of the system
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Speed Droop in Parallel Operation with Infinite Grid
S d D i P ll l O i i h I fi i G id
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Speed Droop in Parallel Operation with Infinite Grid
fnl
PG
Pload
Set pointincreased
Pinfbus
S d D i P ll l O ti ith I fi it G id
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Speed Droop in Parallel Operation with Infinite Grid
S d D i P ll l O ti ith I fi it G id
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Speed Droop in Parallel Operation with Infinite Grid
Summary:
Increasing set point of generator will increase generator output power
Frequency of the system is set by infinite bus
Increasing field current will increase reactive power supplied to the grid
Two Same Size Generator in Parallel Operation
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Two Same Size Generator in Parallel Operation
Second generator takes small amount of load
demand during the first moment of
synchronization (PG2)
Two Same Size Generator in Parallel Operation
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Two Same Size Generator in Parallel Operation
Speed of the second generator is increased to
take more load from other.
Two Same Size Generator in Parallel Operation
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Two Same Size Generator in Parallel Operation
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Power Sharing in Parallel Operation
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Power Sharing in Parallel Operation
Power Sharing without shifting system frequency
Power Sharing in Parallel Operation
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S a g a a Op a
Power Sharing without shifting terminal voltage
Synchronous Motor
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y
Three phase winding of stator produces rotating
magnetic field BS
If field winding on rotor is excited with current,
magnetic field BR is produced. This magneticfield will chase BS.
So, rotor will rotate in the same speed as rotating
magnetic field generated by stator synchronous
Synchronous Motor
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y
Synchronous Motor
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From Generating to Motoring Operation
Synchronous Motor
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From Generating to Motoring Operation
Torque-Speed in Synchronous Motor
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Load Changes on Synchronous Motor
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Load Changes on Synchronous Motor
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Load Changes on Synchronous Motor
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Load Changes on Synchronous Motor
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Load Changes on Synchronous Motor
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Load Changes on Synchronous Motor
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Load Changes on Synchronous Motor
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Field Excitation Changes on Synchronous Motor
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Field Excitation Changes on Synchronous Motor
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Under-excited Over-excited
Field Excitation Changes on Synchronous Motor
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Synchronous VAR
Compensator
when P is kept minimum
Field Excitation Changes on Synchronous Motor
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Field Excitation Changes on Synchronous Motor
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Field Excitation Changes on Synchronous Motor
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Field Excitation Changes on Synchronous Motor
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Field Excitation Changes on Synchronous Motor
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Starting Synchronous Motor
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Starting Synchronous Motor
Basic Approach
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Starting Synchronous Motor
Reducing Electrical Frequency
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Low frequency slow rotating magnetic field rotor is capable to
accelerate
Stator frequency is then increased gradually up to nominal value.
Requires variable frequency variable voltage source
Starting Synchronous Motor
External Prime Mover
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Prime mover brings rotor up nominal speedfield excitation is applied
synchronise with grid detach prime mover from rotor shaft
Starting Synchronous Motor
Armotisseur or Damper Winding
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Damper winding
Starting Synchronous Motor
Armotisseur or Damper Winding
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Starting Synchronous Motor
Armotisseur or Damper Winding
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Starting Synchronous Motor
Starting Procedure Using Armotisseur or Damper Winding
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1. Disconnect the field windings from their dc power source and short them
out.
2. Apply a three-phase voltage to the stator of the motor, and let the rotor
accelerate up to near-synchronous speed. The motor should have no load
on its shaft , so that its speed can approach nsync as closely as possible.
3. Connect the dc field circuit to its power source. After this is done, the
motor will lock into step at synchronous speed, and loads may then be
added to its shaft.