motori per trazione
TRANSCRIPT
5-1 Chapter 5 : DC and AC Electric Machines
IIntroduction
Machines used as motors for propulsion and Machines used as motors for propulsion and as generators for braking. as generators for braking.
Can either be DC or AC machinesCan either be DC or AC machines
Instantaneous power rating can be much Instantaneous power rating can be much higher than rated powerhigher than rated power
Capability to provide full torque even at low Capability to provide full torque even at low speedsspeeds
5-2 Chapter 5 : DC and AC Electric Machines
Machine TypesMachine Types
DC: good characteristics but large andDC: good characteristics but large and giving giving maintenance problemsmaintenance problems
AC-induction: complex control, but rugged and widely AC-induction: complex control, but rugged and widely usedused
PM: high energy density, though costly and fault sensitivePM: high energy density, though costly and fault sensitive
EV motors are larger EV motors are larger ⇒⇒ Cost implications are significant Cost implications are significant
HEV motors are smaller HEV motors are smaller ⇒⇒ PM motor performance may PM motor performance may outweigh cost problemoutweigh cost problem
SRM: excellent fault tolerance and ease of construction, SRM: excellent fault tolerance and ease of construction, requires complex controlrequires complex control
5-3 Chapter 5 : DC and AC Electric Machines
Electric Motor and IC Engine Ratings
Power Watts = Torque N −m × Speed rads / s .
HP=Torque ft−lbs ×rpm5252
Comparison Comparison between ICE and between ICE and electric motors:electric motors:
Note:Note:
5-4 Chapter 5 : DC and AC Electric Machines
Electric Motor and IC Engine Ratings
• Rated HP of electric motor is deratedRated HP of electric motor is derated• For short periods, motors can deliver 2 to 3 For short periods, motors can deliver 2 to 3
times rated HPtimes rated HP• Torque can be maximum under stall Torque can be maximum under stall
conditionsconditions• ICE maximum HP is derived under idealized ICE maximum HP is derived under idealized
lab conditionslab conditions• Transmission is essential for ICE to match Transmission is essential for ICE to match
vehicle speedvehicle speed• Electric motor can be directly coupled with Electric motor can be directly coupled with
a single gear.a single gear.
5-5 Chapter 5 : DC and AC Electric Machines
EV/HEV Motor Requirements
Requirements:Requirements:– Flexible drive controlFlexible drive control– Fault tolerance and ruggednessFault tolerance and ruggedness– High efficiencyHigh efficiency– High speedHigh speed– Low acoustic noise and EMILow acoustic noise and EMI– Wide constant power regionWide constant power region– High torque to inertia and power to weight ratiosHigh torque to inertia and power to weight ratios
• Large TLarge Tee/J results in good acceleration /J results in good acceleration
– High peak torque capability (300-400% rated power)High peak torque capability (300-400% rated power)
5-6 Chapter 5 : DC and AC Electric Machines
DC MachinesDC Machines
Characteristics:Characteristics:– Windings at the stator (field) and rotor (armature) Windings at the stator (field) and rotor (armature)
produce two mmf’s in quadrature and generate a Lorentz produce two mmf’s in quadrature and generate a Lorentz forceforce
– Can be operated in different configurations, depending on Can be operated in different configurations, depending on the winding connectionsthe winding connections
– Easy and flexible to control, established manufacturing Easy and flexible to control, established manufacturing technologytechnology
– Low maximum speed, brush maintenance, important EMI Low maximum speed, brush maintenance, important EMI issues and large sizeissues and large size
5-7 Chapter 5 : DC and AC Electric Machines
Separately excited DC machine:Separately excited DC machine:
Independent voltage and field controls are possible in this Independent voltage and field controls are possible in this configurationconfiguration
5-8 Chapter 5 : DC and AC Electric Machines
Electrical ModelingElectrical Modeling
V A=RA iALAA
di A
dte A
e A=K φωm
T e=Kφi A
V F=RF iFLFF
diF
dt
φ= f iF
Armature CircuitArmature Circuit
Field CircuitField Circuit
5-9 Chapter 5 : DC and AC Electric Machines
Magnetic modelingMagnetic modeling
Basic equations:Basic equations: B=μHμ=μ0 μrμ0=4π×10−7
Non linear characteristics with hysteresis effect:Non linear characteristics with hysteresis effect:
ApproximationApproximation
Magnetic CharacteristicsMagnetic Characteristics
5-10 Chapter 5 : DC and AC Electric Machines
Torque-speed characteristicsTorque-speed characteristics
ωm=V A
Kφ−
RA
Kφ 2 T e
Torque-speed equation:Torque-speed equation:
DC Motor CharacteristicsDC Motor Characteristics
• Speed torque characteristics is controlled by varying armature voltage and/or field current
5-11 Chapter 5 : DC and AC Electric Machines
V A=RA I A¿K φω
m¿
⇒V A=RA
KφT ¿K φω
m¿or ω
m¿K 2φ2−V A KφRAT ¿=0
Operating pointOperating point:: VV vs. vs. φφ at operating point at operating point::
Operating PointOperating Point
•For a given (T*,ω*) point, there can several armature voltage or field current
5-12 Chapter 5 : DC and AC Electric Machines
Three-Phase AC MachinesThree-Phase AC Machines
Winding ConfigurationWinding Configuration
3-phase winding:3-phase winding: Sinusoidal distribution:Sinusoidal distribution:
5-13 Chapter 5 : DC and AC Electric Machines
Armature is stationary as opposed to Armature is stationary as opposed to DC machinesDC machines
Rotor circuit generates excitationRotor circuit generates excitation
Can be of two types, induction or Can be of two types, induction or synchronous machinessynchronous machines
No commutator or brushes in the case No commutator or brushes in the case of ac machinesof ac machines
AC MachinesAC Machines
5-14 Chapter 5 : DC and AC Electric Machines
For sinusoidally distributed winding:For sinusoidally distributed winding:
Magnetomotive force:Magnetomotive force:
Winding and MMFWinding and MMF
5-15 Chapter 5 : DC and AC Electric Machines
Phase a winding:Phase a winding: Phase a mmf:Phase a mmf:
4-Pole Machine4-Pole Machine
5-16 Chapter 5 : DC and AC Electric Machines
Vettori di Spazio – sistema di coordinateVettori di Spazio – sistema di coordinate
α=0
ρ
α
ζ
Sia Θ(α,t) la distribuzione della densità angolare di corrente relativa ad un elemento di macchina nel suo riferimento. Dalla teoria delle macchine elettriche, possiamo derivare la Θ(α,t) dalla conoscenza della tensione magnetica Γ(α,t) secondo la legge:
ααα
∂Γ∂=Θ ),(
),(t
t
la Γ(α,t) sarà una distribuzione a gradino. Ciò, indica una distribuzione di densità lineare di corrente lungo la periferia di macchina di tipo impulsivo:
∑=
−=Θm
kkck izpt
2
1
)(),( ααδα
)1()1(2
12 −=−= km
kmk
ππα
5-17 Chapter 5 : DC and AC Electric Machines
Distribuzione di correnteDistribuzione di corrente
kc
m
k
izkm
pt ∑=
−−=Θ
2
1
)1(),(παδα
∑∞
−∞=
Θ=Θh
jphh et αα
.
),(
Applichiamo lo sviluppo in serie di Fourier
Ricordando che il periodo della funzione Θ è T=2p, e quindi che la pulsazione della fondamentale è ω0=p, i coefficienti Θh sono ottenuti come segue:
∑ ∫
∫ ∑∫
=
−
−
=
−
−−=
=
−−==Θ
m
k
jphkc
jphp m
kkc
Tjhp
h
dekm
pizp
deizkm
pp
defT
2
1
2
0
2
0
2
10
)1(2
)1(2
)(1
πα
α
π
α
απαδπ
απαδπ
αα
5-18 Chapter 5 : DC and AC Electric Machines
Vettori di spazioVettori di spazioDalla teoria delle distribuzioni (teorema del campionamento) possiamo calcolare l’integrale precedente: il prodotto della δ di Dirac concentrata nei punti pα-π/p(k-1) per una qualsiasi funzione f(α) è pari alla f(pα- π(k-1)/p) cioè alla funzione originaria campionata nei punti in cui è concentrato l’impulso.Segue quindi: ∑
=
−−=Θ
m
k
km
jh
kch eizp 2
0
)1(
2
π
π
La precedente sommatoria va separata tra correnti uscenti e correnti entranti. Rispetto al riferimento esse saranno sfasate spazialmente di π radianti elettrici (π/p radianti meccanici):
∑∑∑=
−−
=
−−
=
−−=
−+=Θ
m
k
km
jh
kcj
m
k
km
jh
k
m
k
km
jh
kch eizp
eeieizp
1
)1(2
1
)1(2
1
)1(2
22
)(2
ππ
ππ
ππ
5-19 Chapter 5 : DC and AC Electric Machines
Vettori di spazioVettori di spazio
i
c
m
k
km
jp
kc zp
meizp
ππ
π
21
)1(2
1 ==Θ ∑=
−−
∑=
−−=
m
k
km
j
kei1
)1(2
3
2π
i
++=
ππ3
4
33
2
213
2 jjeieiii
( )( )
( )2321
2321
2321
3
23
23
2
aiaii
aa
avavv
++=
++=
++=
i
ψ
v
ψψψ
Dove i è il vettore di spazio associato alla terna di correnti di alimentazione, definito quindi come
5-20 Chapter 5 : DC and AC Electric Machines
Characteristics:Characteristics:
Provides a simple and efficient way of representing Provides a simple and efficient way of representing sinusoidally space distributed variablessinusoidally space distributed variables
Similar to the use of phasorsSimilar to the use of phasors
Gives a compact way of representing machine Gives a compact way of representing machine equationsequations
Facilitates the conversion from a 3-phase system to a Facilitates the conversion from a 3-phase system to a 2-phase system2-phase system
Space Vector RepresentationSpace Vector Representation
5-21 Chapter 5 : DC and AC Electric Machines
Riferimenti di Clarke e di ParkRiferimenti di Clarke e di Park
Riferimento di Clarke: Sistema di assi cartesiani α,β solidali con lo statore
Riferimento cartesiano il cui asse d è ruotato rispetto al riferimento di Clarke di un angolo γ
5-22 Chapter 5 : DC and AC Electric Machines
Trasformazione di Trasformazione di ParkPark
[ ]
⋅=
⋅
−=
−
000 100
0cossin
0sincos
3
2
gg
g
R
gg
g
gg
g
dqq
d
β
α
αββ
αγγγγ
[ ]dqR −αβ [ ]0αβT
Moltiplicando la matrice di rotazione
per quella che rappresenta la trasformazione di Clarke
si ottiene la trasformazione di Park
( ) [ ]
⋅=
+−
−−−
+
−
=
=
⋅
−
−−
⋅
−=
3
2
1
0
3
2
1
0
21
21
21
3
2sin
3
2sinsin
3
2cos
3
2coscos
3
2
21
21
21
23
23
0
21
21
1
100
0cossin
0sincos
32
gg
gT
gg
g
gg
g
dq
q
d
πγπγγ
πγπγγ
γγγγ
5-23 Chapter 5 : DC and AC Electric Machines
Trasformazione inversaTrasformazione inversa
01323211 )(2
3)(
2
1
2
3
3
2iiiijiiiiee −=
−+++−ℜ=ℜ i
02
203
Re
Re
iia
iia
−=
−=
i
i
[ ]
⋅=
⇔
⋅
=
3
2
1
03
2
12
0 2
1
2
1
2
11
3
2
i
i
i
Si
i
i
iaa
i
ii
0032
3iveP iii +ℜ= iv
5-24 Chapter 5 : DC and AC Electric Machines
[ ] [ ] [ ] abcgTg
g
g
g
gg
g
⋅=
⋅
−
−−
=
00
3
2
1
0
2
1
2
1
2
12
3
2
30
2
1
2
11
3
2
αβαβ
β
α
Adoperando la notazione complessa, si può scrivere in maniera equivalente:
g=gα+j gβ = )(2
3)(
2
1
3
232321 ggjggg −++−
,
( )3210 3
1gggg ++=
Trasformazione di ClarkeTrasformazione di Clarke
5-25 Chapter 5 : DC and AC Electric Machines
• Space vector for a balanced set of 3-phase variables has a Space vector for a balanced set of 3-phase variables has a magnitude 3/2 times greater than the magnitude of the magnitude 3/2 times greater than the magnitude of the phase variablesphase variables
• The amplitude of the space vector is constant for a The amplitude of the space vector is constant for a balanced set of variables, but the phase angle is a balanced set of variables, but the phase angle is a function of time.function of time.
• There is a unique set of vectors that would sum up to There is a unique set of vectors that would sum up to give the resultant space vector.give the resultant space vector.
• The multiplication of 2/3 in the previous figure The multiplication of 2/3 in the previous figure represents the relationship between the magnitude of the represents the relationship between the magnitude of the space vector and the peak magnitude of the time varying space vector and the peak magnitude of the time varying phase sinusoid.phase sinusoid.
And the flux-density:And the flux-density:
5-26 Chapter 5 : DC and AC Electric Machines
Types of AC MachinesTypes of AC Machines
Rotor mmf generation technique characterizes an AC machineRotor mmf generation technique characterizes an AC machine
Synchronous machines rotate at synchronous speed; rotor mmf is Synchronous machines rotate at synchronous speed; rotor mmf is produced either by electromagnet (used in utility power generation) or produced either by electromagnet (used in utility power generation) or permanent magnet (can have EV/HEV applications)permanent magnet (can have EV/HEV applications)
Induction machine rotor mmf is induced by the stator currents, and Induction machine rotor mmf is induced by the stator currents, and rotates at a speed close to, but different than the synchronous speedrotates at a speed close to, but different than the synchronous speed
5-27 Chapter 5 : DC and AC Electric Machines
Induction MachinesInduction Machines
Two rotor configurations are possible:Two rotor configurations are possible:Squirrel cage rotors are widely used because of Squirrel cage rotors are widely used because of
their ruggedness and low costtheir ruggedness and low costWound rotors, which can be connected to an Wound rotors, which can be connected to an
external circuitexternal circuit
Squirrel cage Squirrel cage configurationconfiguration
5-28 Chapter 5 : DC and AC Electric Machines
Stator and rotor electrical circuits:Stator and rotor electrical circuits:
Stator and Rotor CircuitsStator and Rotor Circuits
5-29 Chapter 5 : DC and AC Electric Machines
Stator has sinusoidally distributed windingsStator has sinusoidally distributed windings
Balanced sinusoidal currents induce a rotating stator fieldBalanced sinusoidal currents induce a rotating stator field
Currents flow in the short-circuited rotor windings and Currents flow in the short-circuited rotor windings and induce rotor mmf if the difference in speed between stator induce rotor mmf if the difference in speed between stator and rotor is non-zeroand rotor is non-zero
Operation is then comparable to that of a transformerOperation is then comparable to that of a transformer
Interaction of stator and rotor mmf’s produce torqueInteraction of stator and rotor mmf’s produce torque
Induction Machine OperationInduction Machine Operation
5-30 Chapter 5 : DC and AC Electric Machines
Modello in un riferimento qualsiasiModello in un riferimento qualsiasi
=
=
ℑ=
=−
+=
+=
−++=
++=
010
010
'
2
3
)(
rrr
sss
sse
rLe
smrrr
rmsss
rrbr
rrr
sbs
sss
idt
dLv
idt
dLv
mpM
dt
dJMM
LL
LL
jpdt
dR
jpdt
dR
iψ
iiψ
iiψ
ψψ
iv
ψψ
iv
ω
ωω
ω
5-31 Chapter 5 : DC and AC Electric Machines
Motor usually operated at low slip to have a more linear Motor usually operated at low slip to have a more linear characteristic and maximize efficiencycharacteristic and maximize efficiency
Speed-Torque CharacteristicsSpeed-Torque Characteristics
5-32 Chapter 5 : DC and AC Electric Machines
At rated flux:At rated flux:
k M=π rlN S
2
T e=k MBms
Ir′
wherewhere
i r' t =
F r
N S / 2
Ir′=k r
Bms ωslipAnd fromAnd from we getwe get T e=k m k rB
ms2ωslip
Simplified Torque ExpressionSimplified Torque Expression
5-33 Chapter 5 : DC and AC Electric Machines
Two main possibilities:Two main possibilities:
Stator terminal voltage controlStator terminal voltage control
Stator frequency controlStator frequency control
A power electronics converter is usually requiredA power electronics converter is usually required
Speed Control MethodsSpeed Control Methods
5-34 Chapter 5 : DC and AC Electric Machines
Variable stator voltage at fixed frequency:Variable stator voltage at fixed frequency:
Torque-speed profileTorque-speed profile
5-35 Chapter 5 : DC and AC Electric Machines
Variable frequency but constant V/f ratio:Variable frequency but constant V/f ratio:
Torque-speed profileTorque-speed profile
5-36 Chapter 5 : DC and AC Electric Machines
Common mode of operation:Common mode of operation:
Motor driveMotor drive
Torque-speed Torque-speed operating envelopoperating envelop
5-37 Chapter 5 : DC and AC Electric Machines
Regenerating Regenerating BrakingBraking
Feature of electric machines, allows the regeneration of Feature of electric machines, allows the regeneration of kinetic energy back to the electrical form during braking kinetic energy back to the electrical form during braking operationsoperations
Mechanical brakes still required for short transientsMechanical brakes still required for short transients
Extends the range of the vehicle up to 15%Extends the range of the vehicle up to 15%
Induction machine is operated at negative slipInduction machine is operated at negative slip
Part of the four-quadrant operation required by EV/HEVPart of the four-quadrant operation required by EV/HEV
Chapter 5 : DC and AC Electric Machines
Considerazioni di progettoConsiderazioni di progetto
Per le macchine rotanti la Per le macchine rotanti la potenza di dimensionamento è potenza di dimensionamento è sempre una potenza elettrica, sempre una potenza elettrica, assorbita od erogata a seconda assorbita od erogata a seconda che la macchina sia un motore che la macchina sia un motore od un generatore, ed è la od un generatore, ed è la potenza apparente nel caso di potenza apparente nel caso di corrente alternatacorrente alternata
Chapter 5 : DC and AC Electric Machines
Dimensioni principaliDimensioni principaliD: DiametroD: DiametroPasso polarePasso polare
L: lunghezza del pacco lamiereL: lunghezza del pacco lamiereK: Densità di corrente lineareK: Densità di corrente lineare
2
D
p
πτ =
32
N IK
D
ξπ
=
Chapter 5 : DC and AC Electric Machines
DimensionamentoDimensionamentoPotenza di Potenza di dimensionamentodimensionamento
Flusso per poloFlusso per polo
Tensione indottaTensione indotta
3dS EI=
2
2med Max Max
DL DLB L B B
p p
πτπ
Φ = = =
2 4.442
E f N fNπ ξ Φ= = Φ
Chapter 5 : DC and AC Electric Machines
Potenza di dimensionamentoPotenza di dimensionamento
3 22 32
3
d Max
DL DKS fN B
Np
ππ ξξ
= =
=
g
2 fN
p
π ξ2
2 32Max
D L KB
πg Nξ
2n
=
=2 2
60 22Max
D L KB
p
π
22
60 2Maxn B D LK
π
=
=
Chapter 5 : DC and AC Electric Machines
Potenza di dimensionamentoPotenza di dimensionamento
K Densità di corrente lineareK Densità di corrente lineareJ Densità di corrente superficialeJ Densità di corrente superficialehhcc Altezza di cava Altezza di cavawwcc Larghezza di cava Larghezza di cavakkff Fattore di riempimento Fattore di riempimentoppdd passo di dentatura passo di dentaturanncc numero di conduttori in cava numero di conduttori in cava
c f c c dn I k w h J p K= =
Chapter 5 : DC and AC Electric Machines
•Perdita per effetto Joule della cava
•Potenza smaltita
•Con kf=0.4, wc/pd=0.5 hc=0.05 J=4E6 A/m2
Si ha K=40 kA/m
Relazioni utiliRelazioni utilic
f c cd
wK k h J h J
p= ᄉ
2J f c cp k w h Jρ=
J c dp pα ϑ=c
JKρϑ
α=
Chapter 5 : DC and AC Electric Machines
Relazioni utiliRelazioni utiliρρ=0.02E-6 =0.02E-6 ΩΩmmααcc=100 W/(m=100 W/(m22°C)°C)
Si ha Si ha ϑϑ=32°C=32°CCostante di macchina Costante di macchina C=SC=Sdd/(nD/(nD22L)L)(Rapporto fra coppia e volume della (Rapporto fra coppia e volume della macchina)macchina)
Con B=0.8T e K=40kA/m Con B=0.8T e K=40kA/m C=3720 N/mC=3720 N/m33
Chapter 5 : DC and AC Electric Machines
ConclusioniConclusioni
La potenza di traferro SLa potenza di traferro Sdd di una macchina di una macchina elettrica si può esprimere come:elettrica si può esprimere come:
Con Con BBMM valore massimo dell’ induzione valore massimo dell’ induzione magnetica al traferro, magnetica al traferro, KK densità lineare di densità lineare di corrente di armatura, corrente di armatura, D diametro D diametro di di alesaggio, alesaggio, LL lunghezza attiva di macchina. lunghezza attiva di macchina.
22
60 2d MS n B K D L
π=
Chapter 5 : DC and AC Electric Machines
ConclusioniConclusioni
Nelle macchine tradizionali, la Nelle macchine tradizionali, la profondità di cava di eccitazione profondità di cava di eccitazione hhee o di armatura o di armatura hhaa sono limitate dalla sono limitate dalla saturazione dei denti. Una saturazione dei denti. Una macchina che non presenta alcuna macchina che non presenta alcuna dentatura non risente, invece, di dentatura non risente, invece, di questi vincoli.questi vincoli.