Lesson 8: Transformer Theory and Operation Notes/Lesso… · Ideal Transformer Calculations Lesson...

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2/4/2016 1 LESSON 8: IDEAL TRANSFORMER THEORY AND OPERATION ET 332b Ac Motors, Generators and Power Systems 1 Lesson 8_et332b.pptx Learning Objectives Lesson 8_et332b.pptx 2 After this presentation you will be able to: Explain how an ideal transformer operates Find the voltages and currents on both sides of an ideal transformer using the turns ration Reflect impedances through a transformer Identify and compute the no-load currents that flow in a non-ideal transformer Draw the no-load circuit model of a non-ideal transformer.

Transcript of Lesson 8: Transformer Theory and Operation Notes/Lesso… · Ideal Transformer Calculations Lesson...

Page 1: Lesson 8: Transformer Theory and Operation Notes/Lesso… · Ideal Transformer Calculations Lesson 8_et332b.pptx 14 Example 8-2: 300 kVA 2400-120, 60 Hz single phase transformer operates

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LESSON 8: IDEAL

TRANSFORMER THEORY AND

OPERATION

ET 332b Ac Motors, Generators and Power Systems

1 Lesson 8_et332b.pptx

Learning Objectives

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After this presentation you will be able to:

Explain how an ideal transformer operates

Find the voltages and currents on both sides of an ideal

transformer using the turns ration

Reflect impedances through a transformer

Identify and compute the no-load currents that flow in a

non-ideal transformer

Draw the no-load circuit model of a non-ideal transformer.

Page 2: Lesson 8: Transformer Theory and Operation Notes/Lesso… · Ideal Transformer Calculations Lesson 8_et332b.pptx 14 Example 8-2: 300 kVA 2400-120, 60 Hz single phase transformer operates

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Ideal Transformer Action

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Principle: Stationary coils, time varying flux due to ac current flow. Flux

produced by one coil must link to other coil to induce voltage

Lentz's Law

dt

dNe m

11

dt

dNe m

22

Induced voltage

has opposite

polarity from

source

Ideal Transformer Action

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For sinusoidal sources

maxpp fN44.4E

maxss fN44.4E

maxs

maxp

s

p

fN44.4

fN44.4

E

E

s

p

s

p

N

N

E

E

Dividing the above equations gives:

Voltage relationship

for Ideal transformer

Voltage ratio equals

the turns ratio Where: E’p = voltage induced in the primary (V)

E’s = voltage induced in the secondary (V)

Np = turns in the primary coil

Ns = turns in the secondary coil

Primary Secondary

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Assumptions for Ideal Transformer

Operation

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1) All flux produced in the primary coil links to the secondary coil

2) no core losses due to hysteresis or eddy currents

3) no power losses

4) permeability is infinite (no saturation no magnetizing )

5) windings have zero resistance

6) no current required to magnetize the iron core

For ideal transformer

s

p

s

p

s

p

V

V

N

N

E

Ea

Where: a = turns ratio

Vp = nameplate rated primary voltage (higher V)

Vs = nameplate rated secondary voltage (lower V)

E’p = induced primary voltage

E’s = induced secondary voltage

Ideal Transformer Equations

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sp

s

p

s

p

EaE

N

N

E

Ea

Voltage Ratio

The turns ratio is a

scalar. Introduces no

phase shift

Apparent Power balance

sp

sspp

SS

IEIE

No power losses in

idea transformer

Current Ratio Current ratio is the

inverse of the voltage

ratio a

1

I

I

s

p

sp Ia

1I

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Ideal Transformer Equations-

Impedance Transforms

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Impedances Reflected Through Ideal Transformers

Load impedance as

seen from primary

side of transformer Zin

p

p

inI

EZ

By Ohm’s Law

Zload

s

sload

I

EZ

Write Es and Is in terms of primary values ps

p

s IaI a

EE

2

p

p

p

p

p

p

s

s

a

1

I

E

Ia

1

a

E

Ia

a

E

I

E

in

2

load2inload ZaZ a

1ZZ

Load impedance is

increased when

viewed from primary

side

Ideal Transformer Equations-

Impedance Transforms

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Derive equation when impedances are connected to the primary side and

viewed from the secondary side.

p

p

loadI

EZ

Zin Zload a

II EaE s

psp

s

sin

I

EZ

Write primary values in terms of

secondary and substitute in the

Zload equation.

s

s2

s

ss

s

p

p

loadI

Ea

I

aEa

a

I

Ea

I

EZ

in2

load2

inload Za

Z aZZ

Generally : Moving impedance from secondary

to primary multiply by a2. Moving from

primary to secondary, divide by a2.

s2

p2

sp Za

Z aZZ

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Ideal Transformer Calculations

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Example 8-1: A 25 kVA, 7200 - 240/120 center-tap single phase

transformer operates at rated voltage. It supplies a single phase load that has

an equivalent impedance of 7.2 +36.9o ohms. Assume Ideal operation and

find:

a.) turns ratio

b.) secondary current

c.) primary current

d.) load Z as seen from primary side

e.) PT, ST, QT, and Fp

240 V

120 V

120 V

7200 V

Example 8-1 Solution (1)

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a) For ideal transformers

Ans

b) Secondary current Use Ohm’s law to find Is

Ans

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Example 8-1 Solution (2)

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c) Find the primary current

Ans

d) Find the input impedance as seen from the primary side

Ans

Example 8-1 Solution (3)

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e) Find the power and the power factor of the load

Using secondary side quantities

Ans

Using primary side quantities

Ans

Power equal on both sides of ideal transformer

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Example 8-1 Solution (4)

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Now find the power factor and the active and reactive powers

Ans Ans

Ans

Ideal Transformer Calculations

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Example 8-2: 300 kVA 2400-120, 60 Hz single phase

transformer operates at 2300 volts on the primary side. It supplies

115 kVA to a load that has a power factor of 0.723 lagging.

Assume idea operation and find:

a.) secondary voltage at operating voltage

b.) secondary current

c.) impedance of the load as seen on the secondary side

d.) impedance of the load as seen on the primary side

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Example 8-2 Solution (1)

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a) Find secondary voltage at operating voltage

Use rated values to find turns ratio

Ans

b) Find secondary current at operating voltage

Power is equal on both

sides of ideal transformers Ans

Example 8-2 Solution (2)

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c) Find load impedance seen on secondary side

Angle between V and I.

Change sign for

impedance angle

Ans

Next find impedance angle

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Example 8-2 Solution (3)

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d) Find load impedance seen on primary side of transformer

Reflecting impedance from secondary to primary-multiply by a2.

Ans

Non-Ideal Operation-No-load

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Practical transformers draw current with no load connected to secondary winding.

Current caused by two non-ideal conditions: power losses and core magnetization

Control hysteresis losses - use alloy steels designed

for magnetic circuits

Control eddy current losses - laminate core,

insulate laminates

Active power losses Hysteresis losses - power losses due to

repeated change in magnetic polarity. It takes

more mmf (NI) to demagnetize core in one

direction than the other.

Eddy currents - ac currents induced in iron core

due to changing magnetic field

Active power loss

Control

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Non-Ideal Operation-No-load

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A finite amount of current is necessary to drive mutual flux between coils.

Permeability is finite so reluctance is finite Some NI = F needed.

Al

R m = mutual flux R = reluctance R

INm

R

2NL In terms of inductance so core has inductance with associated

inductive reactance

Define above as the magnetizing inductance with associated magnetizing

reactance Xm

No-Load Circuit Model

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VT = the primary voltage I0 = exciting current

Ife = core-loss component IM = magnetizing component

Rfe = resistance that represents the core losses

Xm = inductive reactance that represents the core magnetizing L

VT

Io

Rfe XM

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No-Load Circuit Model

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Model equation using phasors

fe

Tfe

R

VI

M

TM

jX

VI

Mfeo III

Mfeo IjII Add current magnitudes at 90 degrees

No-load apparent power oTM IVS

fe

2

Tfe

fe

2

Tfe

P

VR

R

VP

M

TM

I

VX Model parameter formulas

Core loss resistance Magnetizing reactance

No-Load Transformer Example

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Example 8-3: Computing the values of magnetizing reactance

and core loss resistance. A 50 kVA 7200-240 V, 60 Hz single

phase transformer is operating with no load. With the primary

connected to a 7200 V system, it draws 248 W and has a

power factor of 0.187 lagging. Find:

a) the exciting current and its components

b) the magnitudes of magnetizing reactance, XM and core loss R

c) Repeat parts a and b if the transformer is energized from

the secondary (low voltage) side.

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Example 8-3 Solution (1)

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a) Find current Io

SM = magnetizing apparent power

Ans

Example 8-3 Solution (2)

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b) Find the value of core loss resistance and magnetizing reactance

Ans

Ans

Ans

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Example 8-3 Solution (3)

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c) Find same parameters on secondary side

Power constant through transformer

Ans

Example 8-3 Solution (4)

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q

Compute Rfe and XM

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Example 8-3 Solution (5)

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Ans

Compare using turns ratio transfer

209,032 on primary 39,801 on primary

End Lesson 8: Ideal Transformer Theory and

Operation

ET 332b Ac Motors, Generators and Power Systems

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Lesson 8_et332b.pptx