Polyphase Systems-Power Electronics-Handout, Exercises of Power Electronics

This lecture handout is for Power Electronics course by Prof. Azhar Raza at Bengal Engineering and Science University. It includes: Polyphase, Systems, Ac, Generator, Conductor, Construction, Maintenance, Costs, Phase, Sequence

Typology: Exercises

2011/2012

Uploaded on 07/23/2012

gangadarr
gangadarr 🇮🇳

5

(1)

25 documents

1 / 32

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Polyphase Systems
Introduction
An ac generator designed to develop a single sinusoidal voltage for each rotation of the shaft
(rotor) is referred to as a single-phase ac generator. If the number of coils on the rotor is
increase in a specified manner, the result is a Polyphase ac generator, which develops more
than one ac phase voltage per rotation of the rotor.
In general, three-phase systems are preferred over single-phase systems for the transmission of
power for many reasons, including the following:
1. Thinner conductor can be used to transmit the same kVA at the same voltage, which
reduces the amount of copper required (typically about 25% less) and in turn reduces
construction maintenance costs.
2. The lighter lines are easier to install, and the supporting structure can be less massive and
farther apart.
3. Three-phase equipment and motors have preferred running and starting characteristics
compared to single-phase systems because of a more even flow of power to the
transducer than can be delivered with a single-phase supply.
4. In general, larger motors are three phase because they are essentially self-starting and do
not require a special design or additional starting circuitry.
docsity.com
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe
pff
pf12
pf13
pf14
pf15
pf16
pf17
pf18
pf19
pf1a
pf1b
pf1c
pf1d
pf1e
pf1f
pf20

Partial preview of the text

Download Polyphase Systems-Power Electronics-Handout and more Exercises Power Electronics in PDF only on Docsity!

Polyphase Systems

Introduction

An ac generator designed to develop a single sinusoidal voltage for each rotation of the shaft (rotor) is referred to as a single-phase ac generator. If the number of coils on the rotor is

increase in a specified manner, the result is a Polyphase ac generator, which develops more

than one ac phase voltage per rotation of the rotor.

In general, three-phase systems are preferred over single-phase systems for the transmission of

power for many reasons, including the following:

  1. Thinner conductor can be used to transmit the same kVA at the same voltage, which reduces the amount of copper required (typically about 25% less) and in turn reduces construction maintenance costs.
  2. The lighter lines are easier to install, and the supporting structure can be less massive and farther apart.
  3. Three-phase equipment and motors have preferred running and starting characteristics compared to single-phase systems because of a more even flow of power to the transducer than can be delivered with a single-phase supply.
  4. In general, larger motors are three phase because they are essentially self-starting and do not require a special design or additional starting circuitry.

e AN  Em ( AN )sin  t

sin ( 120 )

0 e (^) BNEm ( BN )  t

sin ( 240 )

0

eCN  Em ( CN )  t 

0 EANErms ( AN ) 0

0 EBNErms ( BN ) 120

0 ECNErms ( CN ) 240

 EAN  EBN  ECN  0

cos( 30 )

2 0  AN

AB

E

E

2

3

2

 

AN

AB

E

E

E (^) AB  3 E AN

E (^) AB  3 Erms ( AN )(  j

0 0 ( )

0  EAB  3 Erms ( AN ) 30  EAB  3 Erms AN  0  30

………………………………………………………………………………………………

EBC  ECN  E BN

 E BC  EBN  E CN

0 0  EBCErms ( BN ) 120  Erms ( CN ) 240

(cos 120 sin 120 ) (cos 240 sin 240 )

0 0 ( )

0 0  E (^) BCErms ( BN )  jErmsCNj

( )(^ ( )

E (^) BCErmsBN   jErmsCN   j

( )(^ ( )

E (^) BCErmsBN   jErmsBN   j

[ Erms (^) ( BN )  Erms ( CN ) ]

E (^) BCErms ( BN )( j

E (^) BC  3 Erms ( BN )( j )

0  EBC  3 Erms ( BN ) 90

0 0 ( )

0  EBC  3 Erms ( BN ) 90  EBC  3 ErmsBN  120  30

………………………………………………………………………………………………

ECA  EAN  E CN

 ECA  ECN  E AN

0 0  ECAErms ( CN ) 240  Erms ( AN ) 0

0 ( )

0 0  ECAErms ( CN )(cos 240  j sin 240 ) Erms AN  0

( ) ) ( ) 2

3

2

1 ECA ErmsCN ( jErms AN

    

) 2

3

2

3  E (^) CAErms ( CN )(  j

[ Erms (^) ( AN )  Erms ( CN ) ]

) 2

1

2

3  E (^) CA  3 Erms ( CN )(  j

0 0 ( )

0  ECA  3 Erms ( CN ) 210  ECA  3 ErmsCN  240  30

………………………………………………………………………………………………

0 EAB  3 Erms ( AN ) 30

0  EABErms ( AB ) 30

Erms (^) ( AB )  3 Erms ( AN )

2 sin( 30 ) sin( 30 )

0 ( )

0  e (^) ABErms ( AB )  t   EmABt

………………………………………………………………………………………………

0 EBC  3 Erms ( BN ) 90

0  EBCErms ( BC ) 90

Erms (^) ( BC )  3 Erms ( BN )

2 sin( 90 ) sin( 90 )

0 ( )

0  e (^) BCErms ( BC )  t   EmBCt

………………………………………………………………………………………………

0 ECA  3 Erms ( CN ) 210

0  ECAErms ( CA ) 210

E (^) rms ( CA )  3 Erms ( CN )

2 sin( 210 ) sin( 210 )

0 ( )

0  e (^) CAErms ( CA )  t   EmCAt

……………………………………………………………………………………………....

Line Voltages (ABC Sequence)

0 ( )

0 E (^) ABErms ( AB ) reference

0 EBCErms ( BC ) 120

0 ECAErms ( CA ) 240

Determining the phase sequence from the line voltages of a three-phase generator

ACB Phase Sequence (Y-Connected Generator)

Phase Voltages (ACB Sequence)

0 ( )

0 E (^) ANErms ( AN ) reference

0 ECNErms ( CN ) 120

0 EBNErms ( BN ) 240

Determining the phase sequence from the phase voltages of a three-phase generator

Line Voltages (ACB Sequence)

0 ( )

0 E (^) ABErms ( AB ) reference

0 ECAErms ( CA ) 120

0 EBCErms ( BC ) 240

The ^ -Connected Generator

Phase Sequence ABC

E AB  EAN and eAN  2 EAN sin  t

2 sin( 120 )

0

E BC  EBN and eBN  EBN  t 

2 sin( 240 )

0

E CA  ECN and eCN  ECN  t 

ELEg

I (^) BAIAaI AC

I (^) AaIBAI AC

0 0  IAaIrms ( BA ) 0  Irms ( AC ) 240

(cos 240 sin 240 )

0 0  I (^) AaIrms ( BA ) Irms ( AC )  j

I (^) AaIrms BAIrms AC   j

I (^) AaIrms ( BA ) Irms ( BA )(  j

[ I (^) rms ( BA )  Irms ( AC ) ]

I (^) AaIrms ( BA )(  j

I (^) Aa  3 Irms ( BA )(  j

0 0 ( )

0  IAa  3 Erms ( BA ) 30  IAa  3 IrmsBA  0  30

………………………………………………………………………………………………

I (^) CBIBbI BA

I (^) BbICBI BA

0 0  IBbIrms ( CB ) 120  Irms ( BA ) 0

( )

0 0  I (^) BbIrms ( CB )(cos 120  j sin 120 ) IrmsBA

I (^) BbIrmsCB (   jIrmsBA

I (^) BbIrmsCB (   jIrmsCB

[ I (^) rms ( CB )  Irms ( BA ) ]

I (^) BbIrms ( CB )(  j

I (^) Bb  3 Irms ( CB )(  j

0 0 ( )

0  IBb  3 Irms ( CB ) 150  IBb  3 IrmsCb  120  30

………………………………………………………………………………………………

I (^) ACICcI CB

I (^) CcIACI CB

0 ICc  3 Irms ( AC ) 270

0  ICcIrms ( Cc ) 270

I (^) rms ( Cc )  3 Irms ( AC )

2 sin( 270 ) sin( 270 )

0 ( )

0  i (^) CcIrms ( Cc )  t   ImCct

…………………………………………………………………………………………....

cos( 30 ) 2 0  BA

Aa

I

I

2

3

2

  BA

Aa

I

I

I (^) Aa  3 I BA

0 0 ( )

0  EAB  3 Erms ( AN ) 30  EAB  3 Erms AN  0  30

…………………………………………………………………………………………………….

EBC  ECN  E BN

 E BC  EBN  E CN

0 0  EBCErms ( BN ) 240  Erms ( CN ) 120

(cos 240 sin 240 ) (cos 120 sin 120 )

0 0 ( )

0 0  E (^) BCErms ( BN )  jErmsCNj

E (^) BC Erms ( BN )( jErms ( CN )   j

E (^) BC Erms ( BN )( jErms ( BN )   j

[ Erms (^) ( BN )  Erms ( CN ) ]

E (^) BCErms ( BN )( j

E (^) BC  3 Erms ( BN )( j )

0  EBC  3 Erms ( BN ) 270

0 0 ( )

0  EBC  3 Erms ( BN ) 270  EBC  3 ErmsBN  240  30

………………………………………………………………………………………………

ECAEANE CN

 ECA  ECN  E AN

0 0  ECAErms ( CN ) 120  Erms ( AN ) 0

0 ( )

0 0  ECAErms ( CN )(cos 120  j sin 120 ) Erms AN  0

( ) ) ( ) 2

3

2

1  E (^) CAErmsCN (   jErms AN

) 2

3

2

3  E (^) CAErms ( CN )(  j

[ Erms (^) ( AN )  Erms ( CN ) ]

) 2

1

2

3  E (^) CA  3 Erms ( CN )(  j

0 0 ( )

0  ECA  3 Erms ( CN ) 150  ECA  3 ErmsCN  120  30

………………………………………………………………………………………………

ACB Phase sequence

I (^) BAIAaI AC

I (^) AaIBAI AC

0 0  IAaIrms ( BA ) 0  Irms ( AC ) 120

(cos 120 sin 120 )

0 0  I (^) AaIrms ( BA ) Irms ( AC )  j

I (^) AaIrms ( BA ) Irms ( AC )(  j

I (^) AaIrms ( BA ) Irms ( BA )(  j

[ I (^) rms ( BA )  Irms ( AC ) ]

I (^) AaIrms ( BA )(  j

I (^) Aa  3 Irms ( BA )(  j

0 0 ( )

0  IAa  3 Erms ( BA ) 30  IAa  3 IrmsBA  0  30

………………………………………………………………………………………………