Three Phase Circuits - Third...

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1 ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu Three Phase Circuits 2 ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu Three Phase Circuits Chapter Objectives: Be familiar with different three-phase configurations and how to analyze them. Know the difference between balanced and unbalanced circuits Learn about power in a balanced three-phase system Know how to analyze unbalanced three-phase systems Be able to use PSpice to analyze three-phase circuits Apply what is learnt to three-phase measurement and residential wiring

Transcript of Three Phase Circuits - Third...

1ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Three Phase Circuits

2ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Three Phase Circuits

Chapter Objectives: Be familiar with different three-phase configurations and how

to analyze them.

Know the difference between balanced and unbalanced circuits

Learn about power in a balanced three-phase system

Know how to analyze unbalanced three-phase systems

Be able to use PSpice to analyze three-phase circuits

Apply what is learnt to three-phase measurement and residential wiring

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3ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Three phase Circuits 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 increased 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.

1. Thinner conductors can be used to transmit the same kVA at the same voltage, which

reduces the amount of copper required (typically about 25% less).

2. The lighter lines are easier to install, and the supporting structures 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, most larger motors are three phase because they are essentially self-

starting and do not require a special design or additional starting circuitry.

4ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

a) Single phase systems two-wire typeb) Single phase systems three-wire type.

Allows connection to both 120 V and

240 V.

Two-phase three-wire system. The AC sources

operate at different phases.

Single Phase, Three phase Circuits

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5ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Three-phase Generator The three-phase generator has three induction coils placed 120° apart on the stator.

The three coils have an equal number of turns, the voltage induced across each coil

will have the same peak value, shape and frequency.

6ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Three-phase Voltages

Three-phase four-wire system

Neutral Wire

A Three-phase Generator

Voltages having 120° phase difference

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7ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Three phase Voltages

a) Wye Connected Source b) Delta Connected Source

a) abc or positive sequence b) acb or negative sequence

0

120

240

an p

bn p

cn p

V V

V V

V V

= ∠ °

= ∠ − °

= ∠ − °

0

120

240

an p

bn p

cn p

V V

V V

V V

= ∠ °

= ∠ + °

= ∠ + °

Neutral Wire

8ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Three phase Loads

a) Wye-connected load b) Delta-connected load

1 2 3

Conversion of Delta circuit to Wye or Wye to Delta. Balanced Impedance Conversion:

Y

a b c

Z Z Z Z

Z Z Z Z∆

= = =

= = =

1Z 3 Z

3Y YZ Z

∆ ∆= =

A Balanced load has equal impedances on all the phases

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9ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Three phase Connections

Both the three phase source and the three phase load can be

connected either Wye or DELTA.

We have 4 possible connection types.

• Y-Y connection

• Y-∆ connection

• ∆-∆ connection

• ∆-Y connection

Balanced ∆ connected load is more common.

Y connected sources are more common.

10ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Wye-wye Connection

A balanced Y-Y system, showing the source, line and load impedances.

Source ImpedanceLine Impedance

Load Impedance

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11ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Wye-wye Connection

Phase voltages are: Van, Vbn and Vcn.

The three conductors connected from a to A, b to B and c to C are called LINES.

The voltage from one line to another is called a LINE voltage

Line voltages are: Vab, Vbc and Vca

Magnitude of line voltages is √3 times the magnitude of phase voltages. VL= √3 Vp

Line current In add up to zero.

Neutral current is zero:

In= -(Ia+ Ib+ Ic)= 0

12ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Wye-wye Connection

Magnitude of line voltages is √3 times the magnitude of phase voltages. VL= √3 Vp

3

0 , 120 ,

30

3 90

3 21

120

0

an p bn p cn p

ab an nb an bn

bc bn cn

ca cn an

p

p

an bn p

V

V V V V V V

V V V V V

V V V

V V V

V

V VV

= ∠ ° = ∠ − ° = ∠ + °

= + = − =

= − =

∠ °

∠ − °

= + ∠ −= − = °

Line current In add up to zero.

Neutral current is zero:

In= -(Ia+ Ib+ Ic)= 0

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13ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Wye-wye Connection Phasor diagram of phase and line voltages

= 3 3 3 = 3

L ab bc ca

an bn cn p

p an bn cn

V V V V

V V V V

V V V V

= = =

= =

= = =

14ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Single Phase Equivalent of Balanced Y-Y Connection

Balanced three phase circuits can be analyzed on “per phase “ basis..

We look at one phase, say phase a and analyze the single phase equivalent circuit.

Because the circuıit is balanced, we can easily obtain other phase values using their

phase relationships.

ana

Y

VI

Z=

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15ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

16ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Wye-delta Connection

ABAB

BCBC

CACA

VI

Z

VI

Z

VI

Z

=

=

=

Line currents are obtained from the phase currents IAB, IBC and ICA

3 30

3 30

3 30

a AB CA

b BC AB

c CA BC

AB

BC

CA

I I I

I I I

I

I

I II

I

= − =

= − =

∠ − °

∠ − °

∠− −= = ° 3

L a b c

p AB BC CA

L p

I I I I

I I I I

I I

= = =

= = =

=

Three phase sources are usually Wye connected and three phase loads are Delta

connected.

There is no neutral connection for the Y-∆ system.

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17ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Wye-delta Connection

3

Z∆

Single phase equivalent circuit of the balanced Wye-delta connection

Phasor diagram of phase and line currents

3

L a b c

p AB BC CA

L p

I I I I

I I I I

I I

= = =

= = =

=

18ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Delta-delta Connection

Both the source and load are Delta connected and balanced.

, ,a AB CA b BC AB c CA BC

I I I I I I I I I= − = − = −

, ,BC CAABAB BC CA

V VVI I I

Z Z Z∆ ∆ ∆

= = =

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19ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Balanced Delta-wye Connection

30

3

pV∠− °

Transforming a Delta connected source

to an equivalent Wye connection Single phase equivalent of Delta Wye connection

20ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Power in a Balanced System The total instantaneous power in a balanced three phase system is constant.

2 cos( ) 2 cos( 120 ) 2 cos( 120 )

2 cos( ) 2 cos( 120 ) 2 cos( 120 )

2 cos( )cos( ) cos( 120 ) cos( 120 ) cos( 120 )co

AN p BN p CN p

a p b p b p

a b c AN a BN b CN c

p p

v V t v V t v V t

i I t i I t i I t

p p p p v i v i v i

p V I t t t t t

ω ω ω

ω θ ω θ ω θ

ω ω θ ω ω θ ω

= = − ° = + °

= − = − − ° = − + °

= + + = + +

= − + − ° − − ° + + °[ ]s( 120 )

1cos cos [cos( ) cos( )] Using the identity and simplif

The instantenous power is not function of time.

The total power behav

n2

e

yi g

3 cos p p

t

A B A B A B

p V I

ω θ

θ

− + °

= + + −

=

s similar to DC power.

This result is true whether the load is Y or connected.

The average power per phase .3

cos 3

p p p

p

p

pP I

P

V θ

=

= =

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21ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Power in a Balanced System

The complex power per phase is Sp. The total complex power for all phases is S.

p p

p p p p p

2

p p p p

Complex power for each phas

3 cos

1 1= cos = sin

3 3

S V I

3 3 cos 3 cos

3 3 sin 3 sin

S=3S 3V

e

I 3

p p

p p p p p p p

a b c p p p L L

p p p L L

p

p V I

P p V I Q p V I S V I

P jQ

P P P P P V I V I

Q Q V I V I

I Z

θ

θ θ

θ θ

θ θ

=

= = =

= + =

= + + = = =

= = =

= = =

p L

2

p

p , , and are

Total

all rm

complex powe

s values, is the load impedance angl

3

3

r

eL

p

L L

V

Z

P jQ

I

V

V I

I

V θ

θ

= + = ∠S

22ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Power in a Balanced System

Notice the values of Vp, VL, Ip, IL for different load connections.

2

p2

p p p

p

p

p L, , and are all rms values, is the load impe

To

da

3S=3S 3V I 3

nce

al c

an

3

omplex ower

gle

p

L

p

p

L L

V

VI Z

Z

P

V

V I

I

jQ

I θ

θ

∗= = =

= + = ∠S

VLVL

VL

Vp Vp

VpIp

Ip Ip

VL

Vp

Ip

VL

VL Vp

Vp

Ip

Ip

Y connected load. ∆ connected load.

3L p L p

V V I I= = 3L p L p

V V I I= =

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23ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Power in a Balanced System

24ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Single versus Three phase systems Three phase systems uses lesser amount of wire than single phase systems for the

same line voltage VL and same power delivered.

a) Single phase system b) Three phase system

2 2

'2 '2

Wire Material for Single phase 2( ) 2 2(2) 1.33

Wire Material for Three phase 3( ) 3 3

r l r

r l r

π

π= = = =

If same power loss is tolerated in both system, three-phase system use

only 75% of materials of a single-phase system

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25ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

26ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

VL=840 V (Rms)

Capacitors for pf

Correction

IL

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27ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

7365050.68A

3 3 840

Without Pf Correction

L

L

SI

V= = =

28ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Unbalanced Three Phase Systems An unbalanced system is due to unbalanced voltage sources or unbalanced load.

In a unbalanced system the neutral current is NOT zero.

Unbalanced three phase Y connected load.

Line currents DO NOT add up to zero.

In= -(Ia+ Ib+ Ic) ≠ 0

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29ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

30ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Three Phase Power Measurement

Two-meter method for measuring three-phase power

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31ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Residential Wiring

Single phase three-wire residential wiring

32ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Problem 12.10 Determine the current in the neutral line.

UNBALANCED LOAD

NEUTRAL CURRENT IS NOT

ZERO

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33ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Problem 12.12 Solve for the line currents in the Y-∆∆∆∆ circuit. Take Z∆∆∆∆

=

60∠∠∠∠45°Ω°Ω°Ω°Ω.

SINGLE PHASE EQUIVALENT

CIRCUIT

34ELEC 24409: Circuit Theory 2 Dr. Kalyana Veluvolu

Problem 12.22 Find the line currents Ia, I

b, and I

cin the three-phase network

below. Take Z∆

= 12 - j15Ω, ZY

= 4 + j6 Ω, and Zl

= 2 Ω.

ONE DELTA AND ONE Y

CONNECTED LOAD IS

CONNECTED

TWO Loads are parallel if they are

converted to same type.

Delta connected load is converted to

Y connection.

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