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Modeling of DC Machines By Dr. Ungku Anisa Ungku Amirulddin Department of Electrical Power Engineering College of Engineering Dr. Ungku Anisa, July 2008 1 EEEB443 - Control & Drives

Modeling of DC Machines By Dr. Ungku Anisa Ungku Amirulddin Department of Electrical Power Engineering College of Engineering Dr. Ungku Anisa, July 20081EEEB443

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Modeling of DC MachinesByDr. Ungku Anisa Ungku AmirulddinDepartment of Electrical Power EngineeringCollege of Engineering

Dr. Ungku Anisa, July 2008 1EEEB443 - Control & Drives

OutlineIntroductionTheory of OperationField ExcitationSeparately Excited DC MotorState-Space ModelingBlock Diagrams and Transfer FunctionsMeasurement of Motor ConstantsReferences

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 2

IntroductionDC motor in service for more than a centuryDominated variable speed applications before

Power Electronics were introducedAdvantage:

Precise torque and speed control without sophisticated electronics

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 3

IntroductionSome limitations:

High maintenance (commutators & brushes)ExpensiveSpeed limitationsSparking

Commonly used DC motorsSeparately excitedSeries (mostly for traction applications)

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 4

DC Machine – Theory of Operation Field winding - on stator pole

if produces f

Armature winding –on rotor ia produces a

f and a mutually perpendicularmaximum torque

Rotor rotates clockwiseFor unidirectional torque and

rotation ia must be same polarity under

each field poleachieved using commutators

and brushes

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 5

DC Machine – Field ExcitationDepends on connections of field winding relative to

armature windingTypes of DC machines:

Separately ExcitedShunt ExcitedSeries ExcitedCompoundedPermanent Magnet

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 6

DC Machine – Field ExcitationSeparately Excited

Field winding separated from armature winding Independent control of if (f ) and ia (T)

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 7

DC Machine – Field ExcitationShunt Excited

Field winding parallel to armature winding

Variable-voltage operation complex Coupling of f (if ) and T (ia)

productionT vs characteristic almost

constant AR = armature reaction (as T , ia , armature flux

weakens main flux f , )

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 8

DC Machine – Field ExcitationSeries Excited

Field winding in series with armature winding

Variable-voltage operation complex Coupling of f (if ) and T (ia)

productionT ia

2 since if = ia

High starting torqueNo load operation must be

avoided (T = 0, )

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 9

DC Machine – Field ExcitationCompounded

Combines best feature of series and shunt Series – high starting torque Shunt – no load operation

Cumulative compounding shunt and series field

strengthens each other. Differential compounding

shunt and series field opposes each other.

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 10

Long-shunt connection

Short-shunt connection

DC Machine – Field ExcitationPermanent Magnet

Field provided by magnetsLess heat

No field winding resistive losses

Compact Armature similar to

separately excited machine

Disadvantages: Can’t increase flux Risk of demagnetisation

due to armature reaction

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 11

Lf Rf

if

aa

aaaa edt

diLiRv

+

ea

_

LaRa

ia+

vt

_

+

vf

_

Separately Excited DC Machine

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 12

dt

diLiRv fffff

abae iKiKT Electromagnetic torque

ba KKe Armature back e.m.f.

Armaturecircuit

Fieldcircuit

Separately Excited DC MotorMotor is connected to a

load.Therefore,

whereTL= load torque

J = load inertia (kg/m2)

B = viscous friction coefficient (Nm/rad/s)

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 13

Le TBdt

dJT

DC Machine - State-Space ModelingDC motor dynamic equations:

Therefore,

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 14

aa

aaaa edt

diLiRv

Le TBdt

dJT

a

ba

aa

a

aa

L

Kv

Li

L

R

dt

di

1

Lab T

JJ

Bi

J

K

dt

d 1

abae iKiKT

ba KKe (1) (2)

(3) (4)

(5)

(6)

DC Machine - State-Space ModelingFrom (5) and (6), the dynamic equations in state-space

form:

where s = differential operator with respect to time This can be written compactly as:

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 15

L

aa

a

b

a

b

a

aa

T

v

J

Li

JB

JK

LK

LR

s

si

10

01

BUAXX

(7)

(8)

DC Machine - State-Space ModelingComparing (7) and (8):

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 16

JB

JK

LK

LR

b

a

b

a

a

A

vector variable state ----- Tai X

vector input ----- TLa TvU

J

La10

01B

DC Machine - State-Space ModelingThe roots of the system are the eigenvalues of matrix A

1 and 2 always have negative real part, i.e. motor is stable on open-loop operation.

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 17

JB

JK

LK

LR

b

a

b

a

a

A

a

b

a

a

a

a

a

a

JL

K

JL

BR

J

B

L

R

J

B

L

R 22

21 42

1

2

1, (9)

DC Machine – Block Diagrams and Transfer FunctionsTaking Laplace transform of (1) and (3) and neglecting initial

conditions:

These relationships can be represented in the following block diagram

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 18

aa

b

LR

K

s

sωsVsI a

a

JB

Kbs

sTsIsω La

(10) (11)

aa LR s

1

JB s

1

Kb

TL(s)

Te(s)Ia(s)

Va(s)

Kb

(s)++

-

-

DC Machine – Block Diagrams and Transfer FunctionsFrom the block diagram, the following transfer functions can be derived:

Since the motor is a linear system, the speed response due to simultaneous Va input and TL disturbance is:

The Laplace inverse of (14) gives the speed time response (t).

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 19

22a

ωVsssV

sωsG

a

baaaa

b

KBRJRBLJL

K

(12)

(13)

22

LωT

ss

s

sT

sωsG

L

baaaa

aa

KBRJRBLJL

LR

sTsGsVsGsω LωTaωV La (14)

DC Machine – Measurement of Motor ConstantsTo analyse DC motors we need values for Ra, La and Kb

Armature Resistance Ra

DC voltage applied at armature terminals such that rated ia

flows

This gives the dc value for Ra

Need to also correct for temperature at which motor is expected to operate at steady state

Similar procedure can be applied to find Rf of field circuitDr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 20

rated ,

resistance contact

a

brushdca i

VVVR

DC Machine – Measurement of Motor ConstantsArmature Inductance La

Apply low AC voltage through variac at armature terminals

Measure ia Motor must be at standstill

(i.e. = 0 and e = 0)

f = supply frequency in HzRa = ac armature resistanceSimilar procedure can be

applied to find Lf of field circuit

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 21

f

RI

V

La

a

a

a 2

2

2

(variac)

DC Machine – Measurement of Motor ConstantsEMF Constant Kb = K

Rated field voltage applied and kept constant

Shaft rotated by another dc motor up to rated speed

Voltmeter connected to armature terminals gives value of Ea

Get values of ea at different speeds

Plot Ea vs. Slope of curve = Kb Units of Kb = [V/rads-1]

Dr. Ungku Anisa, July 2008 EEEB443 - Control & Drives 22

Ea (V)

(rad/s)

ReferencesKrishnan, R., Electric Motor Drives: Modeling, Analysis and

Control, Prentice-Hall, New Jersey, 2001.Chapman, S. J., Electric Machinery Fundamentals, McGraw

Hill, New York, 2005.Nik Idris, N. R., Short Course Notes on Electrical Drives,

UNITEN/UTM, 2008.Ahmad Azli, N., Short Course Notes on Electrical Drives,

UNITEN/UTM, 2008.

Dr. Ungku Anisa, July 2008 23EEEB443 - Control & Drives