KTUNOTES.IN Module II Performance of an alternator

64
Module II Performance of an alternator KTUNOTES.IN To get more study materails visit www.ktunotes.in

Transcript of KTUNOTES.IN Module II Performance of an alternator

Page 1: KTUNOTES.IN Module II Performance of an alternator

Module II

Performance of an alternator KTUNOTES.IN

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Page 2: KTUNOTES.IN Module II Performance of an alternator

Rotating Magnetic Field

Performance of an alternator

When balanced 3-phase currents flow in balanced 3-phase windings, a rotating magnetic field is produced.

2-pole 3-phase stator winding

Three windings are displaced by 120o along the air-gap periphery.

Each phase spread over 60o

(called phase-spread σ=60o)

Coil aa′ represents phase a winding

Positive currents are to be flowing as indicated by crosses in coil-sides a′ , b′ , c′

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Page 3: KTUNOTES.IN Module II Performance of an alternator

Performance of an alternator

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Page 4: KTUNOTES.IN Module II Performance of an alternator

Space phasor representation

Performance of an alternator

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Page 5: KTUNOTES.IN Module II Performance of an alternator

Space phasor representation

Performance of an alternator

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Page 6: KTUNOTES.IN Module II Performance of an alternator

Space phasor representation

A constant-amplitude rotating m.m.f. or rotating field is produced in the air-gap of a three-phase machines at synchronous speed

Performance of an alternator

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Page 7: KTUNOTES.IN Module II Performance of an alternator

Armature Resistance

Armature reaction

Armature leakage reactance

Synchronous reactance

Causes of voltage drop in alternators

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Page 8: KTUNOTES.IN Module II Performance of an alternator

Electrical machine works based on Faraday's law.

Machine requires a magnetic field and armature

Faraday's law - an emf induced in the armature.

Load connected with armature, current flowing in the

armature

As soon as current starts flowing through the armature

conductor there is one reverse effect of this current on the

main field flux of the alternator

This reverse effect is referred as armature reaction in

So, the effect of armature (stator) flux on the flux produced

by the rotor field poles is called armature reaction.

Armature reaction in alternators

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Page 9: KTUNOTES.IN Module II Performance of an alternator

It is the interaction between field pole and the

armature pole

The armature reaction in synchronous machine

affects the main field flux and vary differently for

different power factors.

Armature reaction

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Page 10: KTUNOTES.IN Module II Performance of an alternator

Armature reaction is discussed three conditions

unity power factor

zero power factor lagging

zero power factor leading.

Unity power factor

Armature current and induced emf - same phase.

EMF induced in the armature - due to changing

main field flux, linked with the armature

Armature reaction

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Page 11: KTUNOTES.IN Module II Performance of an alternator

Field is excited by DC- the main field flux is constant

in respect to field magnets

it would be alternating in respect of armature

main field flux of the alternator

emf E across the armature is proportional to

Armature flux φa is proportional to armature current

Armature reaction - Unity power factor

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Page 12: KTUNOTES.IN Module II Performance of an alternator

Armature flux φa is proportional to armature current

Armature flux φa is in phase with armature current I.

At unity power factor I and E are in same phase.

Φa is phase with E.

Φa is in phase with E and Φf is in quadrature with E

φa is in quadrature with main field flux φf

two fluxes are perpendicular to each other,

The armature reaction of alternator at unity power

factor is purely distorting or cross-magnetizing type.

Armature reaction - Unity power factor

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Page 13: KTUNOTES.IN Module II Performance of an alternator

Hence, at ωt = 0, E is maximum and φf is zero.

At ωt = 90°, E is zero and φf has maximum value.

At ωt = 180°, E is maximum and φf zero.

At ωt = 270°, E is zero and φf has negative maximum

value.

Armature reaction - at Lagging Zero Power Factor

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Page 14: KTUNOTES.IN Module II Performance of an alternator

Here, φf got maximum value 90° before E.

Hence φf leads E by 90°.

Now, armature current I is proportional to armature

flux φa, and I lags E by 90°.

Hence, φa lags E by 90°.

φa and φf act directly opposite to each other.

Thus, armature reaction of alternator at lagging zero

power factor is purely demagnetizing type. That

means, armature flux directly weakens main field

flux.

Armature reaction - at Lagging Zero Power Factor

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Page 15: KTUNOTES.IN Module II Performance of an alternator

At leading pf, Ia leads emf E by an angle 90°.

φf leads, emf E by 90°, φa is proportional to Ia.

Hence, φa is in phase with Ia.

φa also leads E, by 90° as Ia leads E by 90°.

As in this case both armature flux and field flux lead

induced emf E by 90°

Armature reaction - at Leading Zero Power factor

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Page 16: KTUNOTES.IN Module II Performance of an alternator

φf and φa are in same direction.

Hence, the resultant flux is simply arithmetic sum of

field flux and armature flux.

Hence, at last it can be said that, armature reaction

of alternator due to a purely leading electrical power

factor is totally magnetizing type.

Armature reaction - at Leading Zero Power factor

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Page 17: KTUNOTES.IN Module II Performance of an alternator

Armature reaction flux is constant in magnitude and

rotates at synchronous speed.

The armature reaction is cross magnetizing when the

generator supplies a load at unity power factor.

When the generator supplies a load at leading

power factor the armature reaction is partly de

magnetizing & partly cross-magnetizing.

Nature of Armature reaction

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Page 18: KTUNOTES.IN Module II Performance of an alternator

When the load current flows through the armature

winding, it build up the local flux, which cuts the

winding and counter emf is generated. This effect

produces armature reactance which is equal to 2πfL,

where L is in H. This armature reactance is called

leakage reactance

Synchronous Reactance and Impedance

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Page 19: KTUNOTES.IN Module II Performance of an alternator

The combination of leakage reactance with armature

reactance is synchronous reactance

Synchronous Impedance

Synchronous Reactance and Impedance

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Page 20: KTUNOTES.IN Module II Performance of an alternator

Equivalent circuit of syn. Generator is

Phasor Diagram

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Page 21: KTUNOTES.IN Module II Performance of an alternator

Phasor Diagram

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Page 22: KTUNOTES.IN Module II Performance of an alternator

Phasor Diagram

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Page 23: KTUNOTES.IN Module II Performance of an alternator

Phasor Diagram

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Page 24: KTUNOTES.IN Module II Performance of an alternator

The per phase model of a synchronous machine

Open and short circuit test data can be used to

determine synchronous reactance

In short circuit condition

Determination of synchronous reactance

Armature resistance is often neglected,

stf JXVE

0V , t scA II

0V when , t sc

f

sI

EX

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Page 25: KTUNOTES.IN Module II Performance of an alternator

The voltage regulation of an alternator is defined as the change in its terminal voltage when full load is removed, keeping field excitation and speed constant, divided by the rated terminal voltage.

So if Vph = Rated terminal voltage

Eph = No load induced e.m.f.

the voltage regulation is defined as,

Voltage regulation

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Page 26: KTUNOTES.IN Module II Performance of an alternator

The Open-Circuit Test

1. Generator is rotated at the rated speed.

2. Field current is increased from 0 to maximum.

Voltage regulation - EMF

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Voltage regulation-EMF method

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Voltage regulation- EMF method

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Page 29: KTUNOTES.IN Module II Performance of an alternator

Voltage regulation- EMF method

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Page 30: KTUNOTES.IN Module II Performance of an alternator

The Open-Circuit Test

Voltage regulation - EMF method

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Voltage regulation EMF method

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Page 32: KTUNOTES.IN Module II Performance of an alternator

MMF method (Ampere turns method)

Tests: Conduct tests

OCC (upto 125% of rated voltage)

SCC (for rated current)

Voltage regulation

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Page 33: KTUNOTES.IN Module II Performance of an alternator

MMF method (Ampere turns method)

Voltage regulation- MMF method

1. By suitable tests plot OCC and SCC 2. From the OCC find the field current If1 to produce rated voltage, V. KTUNOTES.IN

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Page 34: KTUNOTES.IN Module II Performance of an alternator

3. From SCC find the magnitude of field current If2 to

produce the required armature current.

4. Draw If2 at angle (90+Φ) from If1, where Φ is the

phase angle of current from voltage. If current is

leading, take the angle of If2 as (90-Φ).

5. Find the resultant field current, If and mark its

magnitude on the field current axis.

6. From OCC. find the voltage corresponding to If, which

will be E0.

Voltage regulation - MMF method

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Voltage regulation - MMF method

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Page 36: KTUNOTES.IN Module II Performance of an alternator

Tests:

Conduct tests to find

1. OCC (upto 125% of rated voltage)

2. SCC (for rated current)

3. ZPF (for rated current and rated voltage)

4. Armature Resistance (if required)

Voltage regulation- ZPF method

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Page 37: KTUNOTES.IN Module II Performance of an alternator

Voltage regulation- ZPF method

1. plot OCC and SCC

2. Draw tangent to OCC (air gap line)

3. Conduct ZPF test (using purely

inductive load at rated current and

rated voltage) at full load for

rated voltage and fix the point B.

4. Draw the line BH with length equal

to field current required to produce

full load current at short circuit.

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Page 38: KTUNOTES.IN Module II Performance of an alternator

5. Draw HD parallel to the air gap line so as to touch the OCC.

6. Draw DE parallel to voltage axis. Now, DE represents

voltage drop IXL and BE represents the field current

required to overcome the effect of armature reaction.

Triangle BDE is called Potier triangle and XL is the

Potier reactance

7. Find E from V, IXL and Φ. Consider Ra also if required.

The expression to use is

8. Find field current corresponding to E.

Voltage regulation- ZPF method

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Page 39: KTUNOTES.IN Module II Performance of an alternator

8. Find field current corresponding to E.

9. Draw FG with magnitude equal to BE at angle (90+Ψ)

from field current axis, where Ψ is the phase angle

of current from voltage vector E (internal phase

angle).

10. The resultant field current is given by OG. Mark this

length on field current axis.

11. From OCC find the corresponding E0.

Voltage regulation- ZPF method

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Page 40: KTUNOTES.IN Module II Performance of an alternator

ASA method

Tests: Conduct tests to find

1. OCC (upto 125% of rated voltage)

2. SCC (for rated current)

3. ZPF (for rated current and rated voltage)

4. Armature Resistance (if required)

Voltage regulation- ASA method

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Page 41: KTUNOTES.IN Module II Performance of an alternator

Voltage regulation- ASA method Steps:

1. Follow steps 1 to 7 as in ZPF method.

2. Find If1 corresponding to terminal

voltage V using air gap line (OF1 in

figure).

3. Draw If2 with length equal to field

current required to circulate rated current

during short circuit condition at an angle

(90+Φ) from If1. The resultant of If1 and

If2 gives If (OF2 in figure).

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4. Extend OF2 upto F so that F2F accounts for the

additional field current accounting for the effect of

saturation. F2F is found for voltage E as shown.

5. Project total field current OF to the field current axis

and find corresponding voltage E0 using OCC.

Voltage regulation- ASA method

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Page 43: KTUNOTES.IN Module II Performance of an alternator

Load Characteristics of Synchronous Generator

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Page 44: KTUNOTES.IN Module II Performance of an alternator

Load Characteristics of Synchronous Generator

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Page 45: KTUNOTES.IN Module II Performance of an alternator

Load Characteristics of Synchronous Generator

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Page 46: KTUNOTES.IN Module II Performance of an alternator

Load Characteristics of Synchronous Generator

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Page 47: KTUNOTES.IN Module II Performance of an alternator

While If and N constant, V changes with IL in the

armature and the relationship between the Vand IL of

an alternator is known as its load characteristics.

Load Characteristics of Synchronous Generator

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Page 48: KTUNOTES.IN Module II Performance of an alternator

In salient pole machines the air gap is not uniform

Minimum along the polar axis and maximum along the inter

polar axis.

So, in a salient-pole machine, the two mmfs do not act on the

same magnetic circuit.

Consequently the methods for finding out the regulation of

cylindrical rotor machines when applied to salient pole

machines give incorrect results .

In case of salient pole machines regulation is found out by

applying Blondel’s two reaction theory.

REGULATION OF SALIENT POLE SYNCHRONOUS MACHINE

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Page 49: KTUNOTES.IN Module II Performance of an alternator

According to this theory two axes are recognized in the

machine theory

1. Along the polar axis called the direct axis or d-axis

2. Component acting at right angles to the pole axis called the

quadrature axis or q-axis

BLONDELS TWO REACTION THEORY

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Page 50: KTUNOTES.IN Module II Performance of an alternator

The direct axis component is magnetising or demagnetising.

Quadrature component axis is cross magnetising.

Fig shows the stator m.m.f. wave and the flux distribution in

the air gap along direct axis and quadrature axis of the pole.

BLONDELS TWO REACTION THEORY

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Page 51: KTUNOTES.IN Module II Performance of an alternator

The field winding wound on salient poles produces the m.m.f.

wave (Ff) which is nearly sinusoidal and it always acts along

the direct axis.

m.m.f. Ff always acts along the direct axis.

Due to this m.m.f, emf (Ef ) is produced and it lags Ff by 90o .

Armature carries current Ia, produces its own m.m.f. wave FAR.

This Ia and FAR resolved in two components, one acting along

d-axis and other along quadrature axis.

These components are denoted as, Fd & Fq and Id & Iq

BLONDELS TWO REACTION THEORY

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Page 52: KTUNOTES.IN Module II Performance of an alternator

The positions of FAR, Fd and Fq in space are shown in the Fig.

The instant chosen to show these positions is such that the

current in phase R is maximum positive and is lagging Ff by

angle Ψ.

BLONDELS TWO REACTION THEORY

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Page 53: KTUNOTES.IN Module II Performance of an alternator

The phasor diagram corresponding to the positions considered is shown in the Fig. The Ia lags Ef by angle Ψ.

BLONDELS TWO REACTION THEORY

• Fd is produced by Id which is at 90o to Ef

• Fq is produced by Iq in phase with Ef .

• Flux components of ΦAR are Φd and Φq

• It can be seen that the reactance offered to

flux along direct axis is less than the

reactance offered to flux along quadrature

axis.

• Due to this, the flux ΦAR is no longer along

FAR or Ia.

• Depending upon the reluctances offered

along the direct and quadrature axis, the

flux ΦAR lags behind Ia.

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Page 54: KTUNOTES.IN Module II Performance of an alternator

Φd = Pd Fd where Pd = permeance along the direct axis

Permeance is the reciprocal of reluctance

But Fd = m.m.f. = Kar Id in phase with Id

The m.m.f. is always proportional to current. While Kar is the

armature reaction coefficient.

... Φd = Pd Kar Id

Similarly Φq = Pq Kar Iq

As the reluctance along direct axis is less than that along

quadrature axis, the permeance Pd along direct axis is more than

that along quadrature axis, (Pd Pq ).

The phasor diagram corresponding to the positions considered is shown in the Fig. 3. The Ia lags Ef by angle Ψ.

BLONDELS TWO REACTION THEORY

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Page 55: KTUNOTES.IN Module II Performance of an alternator

Let Ed and Eq be the induced e.m.f.s due to the fluxes Φd and Φq

Ed lags Φd by 90o while Eq lags Φq by 90o .

where Ke = e.m.f. constant of armature winding

The resultant e.m.f. is the phasor sum of Ef, Ed and Eq.

The phasor diagram corresponding to the positions considered is shown in the Fig. 3. The Ia lags Ef by angle Ψ.

BLONDELS TWO REACTION THEORY

Substituting expressions for Φd and Φq

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Page 56: KTUNOTES.IN Module II Performance of an alternator

Now Xard = Equivalent reactance corresponding to the d-axis

component of armature reaction = Ke Pd Kar

Xarq = Equivalent reactance corresponding to the q-axis

component of armature reaction = Ke Pq Kar

For a realistic alternator we know that the voltage equation is,

where Vt = terminal voltage

XL = leakage reactance

BLONDELS TWO REACTION THEORY

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Page 57: KTUNOTES.IN Module II Performance of an alternator

Substituting in expression for ĒR ,

Xd = d-axis synchronous reactance

= XL +Xard

Xq = q-axis synchronous reactance

= XL + Xarq

BLONDELS TWO REACTION THEORY

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Page 58: KTUNOTES.IN Module II Performance of an alternator

In the phasor diagram shown in Fig. the angles Ψ and δ are not

known, through Vt, Ia and Φ values are known. Hence the

location of Ef is also unknown.

Determination of Ψ

BLONDELS TWO REACTION THEORY

Id = Ia sinΨ

Iq = Ia cosΨ

cosΨ = Iq/Ia

Ia Ra has two components

Id Rd = drop due to Ra in phase with Id

Iq Ra = drop due to Ra in phase with Iq

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Page 59: KTUNOTES.IN Module II Performance of an alternator

Detail phasor diagram

The Id Xd and Iq Ra can be drawn leading Id and Iq by 90o

respectively.

BLONDELS TWO REACTION THEORY

Id = Ia sinΨ

Iq = Ia cosΨ

cosΨ = Iq/Ia

Ia Ra has two components

Id Ra = drop due to Ra in phase with Id

Iq Ra = drop due to Ra in phase with Iq

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Page 60: KTUNOTES.IN Module II Performance of an alternator

cosΨ = Iq/Ia

Thus point C can be located. Hence the direction of Ef is also known.

Now triangle ODC is also right angle triangle,

BLONDELS TWO REACTION THEORY

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Page 61: KTUNOTES.IN Module II Performance of an alternator

Now triangle ODC is also right angle triangle,

δ = Ψ - Φ for lagging p.f.

BLONDELS TWO REACTION THEORY

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Slip Test

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Page 63: KTUNOTES.IN Module II Performance of an alternator

PROCEDURE:

1. Connections are made as per the circuit diagram.

2. Initially set field regulator, 3-ɸ variac at minimum position and TPST switch open.

3. The DC motor is started slowly by sliding starter handle and it is run at a speed slightly less than the synchronous speed of the alternator.

4. Close the TPST switch.

5. With field winding left open, a positive sequence balanced voltages of reduced magnitude (around 25% of rated Value) and of rated frequency are impressed across the armature terminals.

Slip Test

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Page 64: KTUNOTES.IN Module II Performance of an alternator

6. The prime mover (DC motor) speed is adjusted till ammeter and voltmeters pointers swing slowly between maximum and minimum positions.

7. Under this condition , readings of maximum and minimum values of both ammeter and voltmeter are recorded

Slip Test

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