Chapter 1 DC Drives Part1

download Chapter 1 DC Drives Part1

of 46

Transcript of Chapter 1 DC Drives Part1

  • 8/9/2019 Chapter 1 DC Drives Part1

    1/46

    DC DrivesDC Drives

  • 8/9/2019 Chapter 1 DC Drives Part1

    2/46

    Learning Objectives

    At the end of this Chapter, you should be able to :

    Analyze the operation and characteristics of

    various types of DC motors

    Analyze the operation and characteristics of DC

    motor in four quadrants

  • 8/9/2019 Chapter 1 DC Drives Part1

    3/46

    3

    Review of D.C. motors: operation, characteristics and

    modes of control

    Degree of Control applied: quadrants of control,

    implications on power electronic requirements

    Converters: principles, single and three phase bridge

    configurations, controllability and protection,

    implications on a.c. supply power factor and

    harmonics!

    "ulse #idth $odulated Chopper amplifiers:

    principles, single%four quadrant bridge configurations,

    losses, controllability and protection, supply

    implications capacitor, cho&e, regeneration!

  • 8/9/2019 Chapter 1 DC Drives Part1

    4/46

    4

    'ypes of (lectric $otors'ypes of (lectric $otors

    $otors are categori)ed on the basis of input

    supply, construction and operation principles

    Classification of $otors

    (lectric $otors

    *lternating Current

    *C! $otors

    Direct Current DC!

    $otors

    +ynchronous nduction

    'hree%"hase+ingle%"hase

    +elf (-cited+eparately

    (-cited

    +eries +huntCompound

  • 8/9/2019 Chapter 1 DC Drives Part1

    5/46

    5

    DC $otorsDC $otors

    ield pole /orth pole and south pole

    Receive electricity to formmagnetic field

    *rmature Cylinder between the poles

    (lectromagnet when current goes through

    0in&ed to drive shaft to drive the load

    Commutator

    1verturns current direction in armature

    DC $otors 2 Components

    (Direct Industry, 1!"

  • 8/9/2019 Chapter 1 DC Drives Part1

    6/46

    6

    DC $otorsDC $otors

    +peed control without impact of

    power supply quality

    Changing armature voltage

    Changing field current

    Restricted use

    ew low3medium speed applications

    Clean, non%ha)ardous areas

    (-pensive compared to *C motors

  • 8/9/2019 Chapter 1 DC Drives Part1

    7/467

    ield winding parallel

    with armature winding 0ine Current 4 field

    current 5 armature

    current

    +peed constant

    independent of load

    up to certain torque

    +peed control:

    insert resistance

    in armature or

    field circuit

    DC motors

    Self-excited DC motor: shunt motor

    ia

    Ra

    La

    ea

    n

    Ka

    if

    vf

    Va

    Field current supplied from aseparate source

    Separately-excited DC motor:

  • 8/9/2019 Chapter 1 DC Drives Part1

    8/468

    +elf%e-cited DC motor: series motor

    DC motors

    ield winding in serieswith armature winding

    ield current 4

    armature current

    +peed restricted to6777 R"$

    *void running with

    no load: speed

    uncontrolled

    +uitable for

    high startingtorque: cranes,

    hoists

  • 8/9/2019 Chapter 1 DC Drives Part1

    9/469

    Electric drives are used for a

    wide range of different loads.

    Some common load

    characteristics are shown along

    with their associated equations.

    It is desirable that the load

    torque and the motor torque

    characteristics are orthogonalor

    nearly so. his will improve

    speed regulation.

    S!eed" #

    orque" L

    L

    $ %&

    ' %(#

    Eg." )oist

  • 8/9/2019 Chapter 1 DC Drives Part1

    10/46

    10

    m#$torque,Developed%m,#$torque,&oad%

    sradspeed,'

    tcoefficien(riction),m*+Inertia,ofoment-

    %')dt

    d'-%

    &

    1.

    /

    &

    ==

    =

    ==

    ++=

    Dynamic torque equation for a motor

    Dynamic voltage equation for a DC motor

    aa

    aaaa edt

    di&0iv ++=

  • 8/9/2019 Chapter 1 DC Drives Part1

    11/46

    11

    Relationship between speed, field

    flu- and armature voltage

    Ea= Z!"#$%&' Define (a= Z!"#$%&'

    DC motors

    Back electromotive force: Ea= KaN Volts

    !ere Ka= Volts"r#m

    $f s#ee% is eresse% as = ' N"60 ra%(sec)1

    Back electromotive force: Ea= Ka1

    !ere Ka1

    = Volts" ra%(sec)1= Kv

    = ZP/(2 A)

    Ea= Kv Volts* !ere emf co+sta+t Kv= Volts" ra%(sec)1

    (a4 electromotive force developed at armature terminals volts!

    4 field flu- which is directly proportional to field current

    / 4 speed in R"$ revolutions per minute!

    = speed inradians"sec

  • 8/9/2019 Chapter 1 DC Drives Part1

    12/46

    1'

    !o)er developed* !a= Ea+a ,atts

    orque developed = !a" Nm

    orque: , = Ea$a" Nm

    DC motors

    8asic equations for average ($ and

    average 'orque developed by motor

    *verage ($, Ea= (a. = (v/olts

    = (a. +a m Define (a.= Z!"#0 &'

    &verage orque* = (+a m*

    +a= armature current

    = speed* rad1 sec-.

    (v= /olts"rad1 sec-.* E2F constant

    (= m"&* torque constant

  • 8/9/2019 Chapter 1 DC Drives Part1

    13/46

    13

    ia

    Ra

    La

    ea

    n

    Ka

    if

    vf

    Va

    aa i2% =

    1

    A3

    %v

    a

    v

    a

    v

    aa

    v

    a

    v

    aaa

    %A3a

    1

    v

    aaa

    vaaaaaa

    a%aa1A3

    va1aa

    secrad%22

    0

    2

    3

    20I

    23

    20I3

    24%Ias

    torque,ofin terms56pressin+

    secrad2

    0I3

    20I50I3

    constantisflu6ifspeed,Avera+e

    I2I2%

    developed%orqueAvera+e

    22or$25

    =

    ==

    =

    =

    +=+=

    ==

    ==

    n12e aa =

    aa

    aaaa edt

    di&0iv ++=

    7eparately.e6cited motor:

    Avera+e induced volta+e:

    Dynamic 3olta+e and torque equations

  • 8/9/2019 Chapter 1 DC Drives Part1

    14/46

    14

    1

    A3

    %v

    a

    v

    a

    v

    aa

    v

    a

    v

    aaa

    %A3a

    1

    v

    aaa

    vaaaaaa

    a%aa1A3

    va1aa

    secrad%

    22

    0

    2

    3

    2

    0I

    2

    3

    2

    0I324%Ias

    torque,ofin terms56pressin+

    secrad2

    0I320I50I3

    constantisflu6ifspeed,Avera+e

    I2I2%

    developed%orqueAvera+e22or$25

    =

    =

    =

    =

    =

    +=+=

    ==

    ==

    1

    A3

    %v

    a

    v

    a

    1

    v

    aaa

    a%A3

    va

    secrad%22

    0

    2

    3

    secrad2

    0I3

    constantisflu6ifspeed,Avera+e

    I2%

    developed%orqueAvera+e

    25

    volta+earmatureAvear+e

    =

    =

    =

    =

    Self-excited Shunt Motor:

    Avera+e induced volta+e:

  • 8/9/2019 Chapter 1 DC Drives Part1

    15/46

    15

    Ra'Rf

    La

    ea

    n

    Ka

    Va L

    f

    if$ i

    a

    /afaA3

    afaa

    I22%

    developed%orqueAvera+e$I225

    =

    =

    /afaaa

    afaa

    f

    aa

    i22i12%

    developed%orque

    ni22e

    i21

    n12e

    equationsDynamic

    a

    ==

    =

    =

    =

    aI22

    "0(0I3$

    $,7peedAvera+e

    5"0(0I3

    edt

    di

    "&(&"0(0iv

    fa

    faaa

    afaaa

    a

    a

    fafaaa

    +=

    ++=++++=

    Series Excited Motor:

    Avera+e induced volta+e

    Dynamic 3olta+e equations

  • 8/9/2019 Chapter 1 DC Drives Part1

    16/46

    16

    320I3 += aaa

    aI2% %=

    $m4A"(2"sec3olts4rad(2constant,isIIf

    secrad7peed,8

    Acurrent,ArmatureI

    33olta+e,Applied3

    $m4Aconstant,%orque2

    sec3olts4radconstant,f#m#e)ac*29here

    %

    1

    3f

    1.

    a

    a

    %

    1

    3

    =

    ==

    =

    =

    =

    =

  • 8/9/2019 Chapter 1 DC Drives Part1

    17/46

    17*current"+ield+ullI

    ,required-*current"+ieldI

    secradS!eed"

    *current"*rmatureI

    VVoltage"*!!lied V

    #m/*constant"orqueK

    secVolts/radconstant"f.m.e0ac%Kwhere

    fo

    f

    (1

    a

    a

    (V

    =

    +=

    ;f

    f

    %

    ;f

    f

    3

    I

    I2I%

    I

    I20I3

    a

    aaa

  • 8/9/2019 Chapter 1 DC Drives Part1

    18/46

    18

    1.

    foao

    fa

    a

    %

    1

    3

    secrad7peed,8

    Acurrent,ieldullIAcurrent,ArmatureullI

    (required"Acurrent,ieldIAcurrent,ArmatureI

    33olta+e,Applied3

    $m4Aconstant,%orque2

    sec3olts4radconstant,f#m#e)ac*29here

    ==

    ===

    ===

    =

    =

    =

    =

    +=

    ;

    %

    ;

    3

    I

    I2I%

    I

    I20I3

    a

    a

    a

    a

    a

    aaa

  • 8/9/2019 Chapter 1 DC Drives Part1

    19/46

    19

    Acurrent,ieldullI

    (required"Acurrent,ieldI

    secrad7peed,8

    Acurrent,ArmatureI

    33olta+e,Applied3

    $m4Aconstant,%orque2

    sec3olts4radconstant,f#m#e)ac*29here

    fo

    f

    1.

    a

    a

    %

    1

    3

    =

    =

    ==

    =

    =

    =

    =

    =

    +=

    ;f

    f%

    ;f

    f3

    I

    I2I%

    I

    I20I3

    a

    aaa

  • 8/9/2019 Chapter 1 DC Drives Part1

    20/46

    !ro3lem:.

    - fi&e% fiel% ./ motor %rives a com#ressor a+%!as t!e folloi+ c!aracteristics:

    Back emf co+sta+t 0(17' V"r#m

    ,or2e co+sta+t 1(64 N(m"--rmat2re resista+ce 0('5

    +%er t!e most severe co+%itio+s* t!e com#ressor+ee%s to e %rive+ at 8'5 r#m it! a tor2e of 50Nm( .etermi+e t!e ma&im2m c2rre+t a+% voltaere2ire% for t!e motor(

  • 8/9/2019 Chapter 1 DC Drives Part1

    21/46

    31

  • 8/9/2019 Chapter 1 DC Drives Part1

    22/46

    - ./ tractio+ motor !as t!e folloi+c!aracteristics:

    Back emf co+sta+t ' V"ra%(s)1 2ll

    fl2&e%,or2e co+sta+t 3 Nm"- 2ll fl2&e%-rmat2re fiel% resista+ces 0(3 -rmat2re i+%2cta+ce ' m;

    ,!e motor is to #rovi%e a ma&im2m tor2e of 600N(m at a s#ee% of 1500 r#m(

    .etermi+e t!e armat2re voltae* V%(

    !ro3lem:0

  • 8/9/2019 Chapter 1 DC Drives Part1

    23/46

    2otor s!eed $1;@#1!@

    =;

    1!;;/

    =;

    / === rads

    N

    3?@

  • 8/9/2019 Chapter 1 DC Drives Part1

    24/46

    '4

    The

    -T plane with motor's shaft cross sectional area is shown.

    ElectricalElectrical 2ech2ech

    For)ardFor)ard

    2otoring2otoring4ve4ve

    4ve4ve

    2ech2ech ElectricalElectrical

    For)ardFor)ard

    5ra6ing5ra6ing -ve-ve

    4ve4ve

    ElectricalElectrical 2ech2ech

    7everse7everse

    2otoring2otoring -ve-ve -ve-ve

    7everse7everse

    5ra6ing5ra6ing4ve4ve -ve-ve

    2ech2ech ElectricalElectrical

    2otor2otorElectricalElectrical 2echanical2echanical

    ! = +/! = +/ ! =! =

    ,hen accelerating,hen accelerating

    8enerator8enerator

    ElectricalElectrical

    ! = +/! = +/ ! =! =

    ,hen 3ra6ing,hen 3ra6ing

    2echanical2echanical

  • 8/9/2019 Chapter 1 DC Drives Part1

    25/46

    '5

    The positive orforward speed isarbitrarily chosen

    The positivepositivetorquetorqueis in thedirection that will

    produceproduceacceleration inacceleration inforward speedforward speed,as shown above.

    For)ard

    7everse

    < $< $$

    < $$$ < $V

  • 8/9/2019 Chapter 1 DC Drives Part1

    26/46

    '6

    Both torque and speed are positivetorque and speed are positive- themotor rotates in forward directionforward direction, which is in

    the same direction as the motor torquethe same direction as the motor torque.

    The power of the motor is the product of the

    speed and torque ! " T#, therefore the

    power of the motor is positive.

    $nergy$nergyis converted from electrical form toelectrical form tomechanical formmechanical form, which is used to rotate theused to rotate the

    motormotor.

    The mode of operation is %nown as forwardforward

    motorin.motorin.

    Ea #ositive

    $a #ositive

  • 8/9/2019 Chapter 1 DC Drives Part1

    27/46

    '7

    The speed is in forward directionspeed is in forward directionbut the motormotortorque is in oppositetorque is in oppositedirection or negative value.

    The torque producedtorque producedby the motor is used to &bra%eused to &bra%e&the forward rotationthe forward rotationof the motor.

    The mechanical energy during the bra%ing, ismechanical energy during the bra%ing, isconverted to electrical energyconverted to electrical energy- thus the 'ow ofenergy is from the mechanical system to theelectrical system.

    The product of the torque and speed is negativeproduct of the torque and speed is negativethusthe power is negative, implying that the motorimplying that the motoroperates in bra%ing modeoperates in bra%ing mode.

    The mode of operation is %nown as forwardforward!ra"in.!ra"in.

    Ea #ositive

    $a +eative

  • 8/9/2019 Chapter 1 DC Drives Part1

    28/46

    '8

    The speed and the torque of the motor are inspeed and the torque of the motor are inthe same direction but are both negativethe same direction but are both negative.

    The reverse electrical torque is used to rotatereverse electrical torque is used to rotate

    the motor in reverse directionthe motor in reverse direction. The power, i.e. the product of the torque andproduct of the torque and

    speed, is positive implying that the motorspeed, is positive implying that the motoroperates in motoring modeoperates in motoring mode.

    The energy is converted fromelectrical formelectrical form

    to mechanical formto mechanical form. This mode of operation is %nown as reversereverse

    motorinmotorin.

    Ea +eative

    $a +eative

  • 8/9/2019 Chapter 1 DC Drives Part1

    29/46

    '9

    The speed is in reverse direction but the torque ispositive.

    The motor torque is used to &bra%e& the reversemotor torque is used to &bra%e& the reverse

    rotation of the motorrotation of the motor. The mechanical energy gained during the bra%ing ismechanical energy gained during the bra%ing is

    converted to electrical formconverted to electrical form- thus power 'ow fromthe mechanical system to the electrical system.

    The product of the speed and torque is negativeproduct of the speed and torque is negative

    implying that the motor operates in bra%ing modeimplying that the motor operates in bra%ing mode. This mode of operation is %nown as reversereverse

    !ra"in.!ra"in.

    Ea +eative

    $a #ositive

  • 8/9/2019 Chapter 1 DC Drives Part1

    30/46

    30

    ,or2e"s#ee% c!aracteristics of variale s#ee% %rive

    ,!e o#eratio+ of a %rive ofte+ e&te+%s o2tsi%e o+e 2a%ra+ta+% are ofte+ eresse% as a four-quadrant torque/speedra#!( ,!e 2se of 2a%ra+t c!arts to re#rese+t commo+state c!a+es are as s!o+(

    ypically motor control systems )ill operate in either +* ++or +/ of thesee quadrants1

    Note:9uadrant ++ and +/ have the potential forregeneration1

    S!eed" #

    orque"

    III

    III IV

    e.g." Locomotive

    S!eed" #

    orque"

    III

    III IV

    e.g." Electric carS!eed" #

    orque"

    III

    III IV

    e.g." 3rane

  • 8/9/2019 Chapter 1 DC Drives Part1

    31/46

    - oo%s> elevator is to e 2se% to lift !eav loa%s etee+floors i+ a ma+2fact2ri+ com#le& as s!o+ i+ F+87E .($t is to e #oere% a ./ motor it! co+sta+t e&citatio+(

    ,!e %etails elo %efi+e t!e c!aracteristics for t!e motor:?otor: ,or2e co+sta+t 0(8 Nm"-

    Back emf co+sta+t 0(8 V"ra% s)1-rmat2re resista+ce 0(03

    a ,!e elevator is to carr loa%s it! ma&im2m ei!t of 800k( ,!e ei!t of t!e lift is 300 k( ,!e 2il%i+ !as 5 floorsa+% t!e averae !ei!t of eac! floor is 8 m( ,!e mi+im2mtime for t!e elevator to move from ro2+% floor to to# floor is

    33 s( se t!e acceleratio+ %2e to ravit at sea level* g= 9(81ms)'( /alc2late i t!e mi+im2m #oer re2ireme+t for t!emotor a+% ii t!e tor2e !e+ t!e motor is r2++i+ at as#ee% of 900 r#m( .etermi+e t!e motor armat2re c2rre+t a+% t!e armat2revoltae(

    !ro3lem:;

  • 8/9/2019 Chapter 1 DC Drives Part1

    32/46

    4 metres

    +loor (

    o! +loor

    DC motor

    u!

    down

    5nd +loor

    F+87E .

  • 8/9/2019 Chapter 1 DC Drives Part1

    33/46

    33

    ) metres

    +loor (

    o! +loor

    DC motor

    u!

    down

    5nd +loor

    ,otal mass* m = @ A = 1100 k

    ,otal !ei!t of floors = ; & = 40 mVelocit of t!e lift* v = ; & " = 1(' m"sorce to lift t!e loa%* = m a = m & 9(81 = 10791 k(m"s'Coer re2ire%* C = , = v = 13057 @atts

    D = 94('5 ra%"s,or2e %evelo#e%* , = C" = 138(54 N(m

    ei!t of loa% = @ k(ei!t of t!e lift = k(!ei!t of eac! floor = ; mNo( of floors = ,ime take+ = sec

    a

    ol2tio+:

  • 8/9/2019 Chapter 1 DC Drives Part1

    34/46

    Torque constant " (.)*m+

    Bac% emf constant " (.)+rad s-

    rmature resistance " (.(/

    3=#>;;#;?61@?#1@3

    A1@#1@?>#;

    !

    I2%%orque,

    20I3

    a%

    3

    =+=

    ==

    =

    +=

    a

    a

    aaa

    I

  • 8/9/2019 Chapter 1 DC Drives Part1

    35/46

    - a+tr cra+e is to e #oere% a ./ motorit! co+sta+t e&citatio+( ,!e ./ motor is toraise a+% loer a loa% it! ma&im2m ei!t of1500 k( -s s!o+ i+ F+87E 0* t!e motorit! t!e #arameters liste% elo* is ei+ 2se%it! a 50:1 re%2ctio+ earo& a+% a %r2m of%iameter 0(3 m( ,!e %etails elo %efi+e t!ec!aracteristics for t!e motor a+% %c)%cco+verter(

    ?otor: ,or2e co+sta+t = 0(6 Nm"- Back emf co+sta+t =0(6 V"ra% s)1

    -rmat2re resista+ce = 0('

    !ro3lem:pen-loop control:

    #ee% co+trol of motors is carrie% o2t i+ eit!er o#e+

    or close% loo#(

  • 8/9/2019 Chapter 1 DC Drives Part1

    46/46

    ?@=ER

    3@#R@LLER2@@R L@*A

    ?ower

    InRequireds!eed

    acho

    *ctuals!eed

    $+ close% loo# s#ee% co+trol sstem* t!e o2t#2t s#ee%is com#are% it! t!e re2ire% s#ee% to %etermi+e t!e

    error(,!e i+#2t #oer is t!e+ a%F2ste% to re%2ce t!e error(,!e close% loo# a##roac! !as ma+ a%va+taes* 2tt!e e&tra ee+se a+% com#le&it is +ot F2stifie% ifs#ee% re2latio+ is 2+im#orta+t(

    Closed-loop control: