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2 The DFI-Motor Model
The Concordia and Park transformation
s application to the traditional abc DFI-
Motor model allows to write a dynamic model in a d-q synchronous reference frame
as follows
'
d u sd
R s
R s M
dt ¼
L s r u sd þ
L s L r r u rd þ x s u sq þ
u sd
d u sq
dt ¼
R s
R s M
L s r u sq þ
L s L r r u rq x s u sd þ
u sq
ð 1 Þ
d u rd
R r
R r M
dt ¼
L r r u rd þ
L s L r r u sd þ x r u rq þ
u rd
d u rq
dt ¼
R r
R r M
L r r u rq þ
L s L r r u sq x r u rd þ
u rq
Stator and rotor
fl
flux equations are
u sd ¼
L s i sd þ
Mi rd
u sq ¼
L s i sq þ
Mi rq
ð
2
Þ
u rd ¼
L r i rd þ
Mi sd
u rq ¼
L r i rq þ
Mi sq
The mechanical equation is given by
J d
dt ¼ C e C l
k f X
ð
3
Þ
The electromagnetic torque is given by
pM
L s L r r
C e ¼
u sq u rd u sd u rq
ð
4
Þ
where
s, r
Rotor and stator indices
d, q
Synchronous reference frame
α
,
ʲ
Stationary reference frame
R, L, M
Resistance, inductance and mutual in ductance
u, i,
ˆ
Voltage, current and
fl
ux
h s ; h r
Stator and rotor electrical angles
h; X
Rotor mechanical position and speed
d
h s
dt
d
h r
dt
Electrical frequencies of stator, rotor and shaft
d dt
x s ¼
; x r ¼
; x ¼
C l ; C e
Load and electromagnetic torque
J, p
Inertia, number of pole pairs
(M 2 /L s L r )
σ
=1
Leakage coef
cient
In a DFI-Motor, the combined effect of the stator and rotor currents produces a
fundamental flux that is sinusoidally distributed around the air gap and that rotates
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