alternating current machines 10&11

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L/O 10 & 11 jh 3/05 1 3 Phase Synchronous Machines Learning 10 & 11

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Page 1: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 1

3 Phase Synchronous Machines

Learning 10 & 11

Page 2: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 2

A cage type induction motor will travel at a speed slightly slower than synchronous speed due to slip.

If there were no slip the motor would travel at synchronous speed…..a cage motor can not deliver torque at synchronous speed.

A SYNCHRONOUS MOTOR has special DC windings which latch onto the rotating magnetic field.

The RMF drags the rotor around at synchronous speed.

Page 3: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 3

In simple terms….

A motor can generate and a generator can be made to motor.

A synchronous motor and an alternator are one and the same machine.

Page 4: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 4

DC field

AC output on rotor

Page 5: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 5

Page 6: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 6

An alternator can motor and under bad circumstances drive the diesel engine like a compressor !

Page 7: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 7www.tecowestinghouse.com

Synchronous motor rotor

Rotor & amortisseur windings (bars)

Page 8: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 8

www.panasia.com

Salient poles on rotor

Synchronous Motors

Stator

Pony motor Excitation gear AC/stator windings

Page 9: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 9

Synchronous motor rotor with DC excitation unit. AC is induced into rotor of exciter and rectified to smooth DC for the DC fields which are embedded in the laminations. 4 pole ??

Page 10: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 10

Construction details.

• Large diameter rotors for slow moving machines. Often salient pole type.

• Small rotors for faster machines eg; 6,4,2 pole machines

• Stators are essentially the same for all speeds

Page 11: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 11

Frequency and speed.

f = ------------ Hz.n x p

120

n = RPM

f = frequency in hertz

P = number of poles

120 = 60 x 2

Minutes to seconds

Pairs of poles eg 1 x N & 1 x S

P 251 L/O 10.2

Page 12: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 12

For an ALTERNATOR.

What do we need to produce an EMF ????

Page 13: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 12

For an ALTERNATOR.

What do we need to produce an EMF ????

1. Conducting path

Page 14: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 12

For an ALTERNATOR.

What do we need to produce an EMF ????

1. Conducting path

2. Magnetic field

Page 15: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 12

For an ALTERNATOR.

What do we need to produce an EMF ????

1. Conducting path

2. Magnetic field

3. Relative motion between the 2

Page 16: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 13

Consider this equation

Vg = 4.44 x Ø x f x N x kd x kp

This is for explanation only

Not in the exam.

4.44 = 4 x 1.11 (form factor)

Ø = flux per pole

f = frequency (speed of cutting)

N = number of turns in coil

Kd & Kp = winding type and style

Page 17: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 14

Different shapes of sine waves

Page 18: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 15

Shows how each conductor/coil contributes to the sine wave within the alternator.

For interest only.

Page 19: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 16

Voltage regulation.

L/O 11.2 p 254

Page 20: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 17

No load volts Full load No load

100% load @ .8pf Vert = 20V/div Horiz = 1s/div

Voltage regulator catches load.

750kVA Alternator

Page 21: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 18

Alt

Alternator

Page 22: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 18

Alt

Load

Alternator

Page 23: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 18

Alt

LoadR

XLInternal

Impedance

Alternator

Page 24: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 19

As an alternator goes on load, the internal losses cause the output voltage to drop.

The powerfactor of the load affects the output voltage.

Jenneson p 254

Page 25: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 20Jenneson p 254

Drop to internal losses.

Page 26: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 21

Voltage regulation

Read carefully the example 11.3 p 254

Important….you need to know this !!

Page 27: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 22

Frequency .. No load to 100% FLC

Horiz = 1sec/div

Page 28: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 23

Nameplate data

L/O 10.4 etcNRG turbine set

Page 29: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 24NRG Turbine set ExciterbearingMain Altnr.

Page 30: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 25NRG gas turbine

Page 31: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 26

Page 32: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 27

SlipringsTo take DC to the rotor

Page 33: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 28

The effects of change in excitation of an alternator.

Read carefully 11.3.4 this is difficult stuff.

Page 34: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 29L/O 11.1 p 255

Page 35: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 29

A stand alone alternator is one which delivers power to its own isolated load away from the power grid.

L/O 11.1 p 255

Page 36: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 29

A stand alone alternator is one which delivers power to its own isolated load away from the power grid.

Paralled machines are either supplying load to a grid system or they could be supplying a common load along with one or more alternators.

L/O 11.1 p 255

Page 37: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 29

A stand alone alternator is one which delivers power to its own isolated load away from the power grid.

Paralled machines are either supplying load to a grid system or they could be supplying a common load along with one or more alternators.

A machine could be

•“tied to the grid”

•Separate from the grid

•Paralled to one or more machines

L/O 11.1 p 255

Page 38: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 30

Parallel operation

1. Waveforms the same

2. Same phase sequence

3. Same voltages

4. Voltages in phase

5. Same frequency

These are usually ”user changeable”

Jenneson p 255

Page 39: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 31

The frequencies must be the same.

Page 40: Alternating Current Machines 10&11

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Phase sequence need to be the same

The voltages and sequence need to be identical between the mains and the incoming machine.

Page 41: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 33

Alternator at Gladstone Base Hospital (one of 3 sets throughout the hospital.)

Page 42: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 34

3 phase Dunlite machine

Page 43: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 35

Small 1 phase portable 5kVA unit

750W portable unit

Page 44: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 36

Synchronous motors

In simple terms….

A DC field in the rotor “locks into” the rotating magnetic field of the stator and the rotor gets dragged around at synchronous speed.

Jenneson p 259 L/O 11Ref. to Ralph’s pp

Page 45: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 37Dragline machinesThe square grey machines are sync. motors

Page 46: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 38Transportable sub-station to power dragline.

Page 47: Alternating Current Machines 10&11

L/O 10 & 11 jh 3/05 39