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XVIII International Conference on Electrical Machines ���ICEM 2008
New Theoretical Approach to the Synchronous Reluctance Machine (SynRM) Behavior and Performance
Conclusions� A new operating diagram for the SynRM is introduced
based on the machine vector model in the rotor reference frame.
�The main machine performance can be explainedand evaluated by this diagram that demonstrates the machine flux, current, torque, and power factor for all possible machine operating points below and above base speeds.
�The saturation effect on torque, IPF, current and flux is discussed with this diagram by FEM calculations.
� An online parameter estimator based on the machine terminal values and power factor is presented.
Main Performance (Ideal & Saturation Effect)
SynRM Operating DiagramA new operating diagram for the SynRM demonstrates the machine flux,
current, torque, and power factor for all possible machine operating points in just one diagram, by combining the torque vs. current angle
graphs at constant current, constant flux and power factor.
Parameter Estimator
Reza R. Moghaddam ‡†, Freddy Magnussen †, Chandur Sadarangani ‡†, Heinz Lendenmann †
‡ Royal institute of Technology, KTH, School of Electrical Engineering, Department of Electrical Machines and Power Electronics , Stockholm, Sweden. † ABB Corporate Research, Västerås, Sweden.
0
5
10
15
20
25
30
0 10 20 30 40 50 60 70 80 90Current Angle (elec. Deg.)
Sal
ienc
y R
atio
(Zea
ta)
IPF=0,9IPF=0,85IPF=0,8IPF=0,7IPF=0,6IPF=0,5
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
0 10 20 30 40 50 60 70 80 90Current Angle (elec. deg.)
IPF
zetha=200zetha=12zetha=8zetha=4
θ
T
ctefEEEE
=>>> 4321
4f
cteEffff
=<<< 4321
4I
1tan =θξδ /1tan =ξθ =tan
1tan =δ
4321 IIII >>>
4λ
4321 λλλλ >>>
3λ2λ
1λ
3f
2f
1f
4E
3E
2E
1E
T
θ
3I
2I
1I
( ) ( )θ2sin22
3 2ILLp
T qdag ⋅−=
���
����
����
����
�⋅���
����
�⋅��
�
�
��
�
�−= −
ξθ
ωtan
tan2sin11
223 1
2E
LLp
Tdq
ag
( )( ) .sincottancos 1 θθξθ <⋅+−= −IPF
( )( )IPF1costantan −+⋅−= θθξ
0121
1 TTB
���
����
� +=
ξξ
A
B
C
D
G
1tan =θξδ /1tan =
ξθ =tanξδ /1tan =
ξθ =tan1tan =δ
θ
IPFT
., cteIIT C ==
., cteIIT A ==
., cteT A == λλ
., cteT G == λλ
., cteT B == λλ
.,
cteT
D
C
====
λλλ
IPF11
, +−=
ξξ
GDIPF
���
����
� +
���
����
�−
=
=
ξξ
ξξ
121
121
,,,, EBCFAIPF
0
0
121
112
T
TTD
���
����
�+
=
=+
=
ξξ
ξξ
0TTTT GCA === IPF
IPF
1
., cteIIT G ==
900
., cteIIT C ==
0.20.20.2
0.40.4
0.4 0.6
0.6
0.6
0.6
0.8
0.8
0.8
0.8
1
1
1
1
1
1.2
1.2
1.2
1.2
1.2
1.4
1.4
1.4
1.4
1.4
1.4
1.6
1.6
1.6
1.8
2
Current angle ϑ [d]
Tor
que
T ag [
pu]
10 20 30 40 50 60 70 80
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
0.20.40.40.4
0.60.60.6
0.80.80.80.8
11
11
1.2
1.2
1.2
1.2
1.4
1.4
1.4
1.4
1.4
1.6
1.61.6
1.6
1.6
1.8
1.8
1.8
1.8
1.8
2
2
2
2.2
Current angle ϑ [d]
Tor
que
T ag [
pu]
10 20 30 40 50 60 70 80
1
2
3
4
5
6
7
8
0.4
0.4
0.6
0.6
0.6
0.8
0.8
0.8
0.8
1
1
1
1
1.2
1.2
1.2
1.4
1.4
1.6
1.6
1.8
Current angle ϑ [d]
IPF
[*]
20 30 40 50 60 70 80
0.2
0.3
0.4
0.5
0.6
0.7
0 0.5 1 1.50
0.5
1
1.5
Time [s]
| i s
|
[pu]
| i s |
0 0.5 1 1.50
2
4
6
8
10
Time [s]
Sal
ienc
y R
atio
ζ
Actual ζEstimated ζ
0 0.5 1 1.50
10
20
30
40
50
Time [s]
L d [mH
]
Actual L dEstimated L d
0 0.5 1 1.50
2
4
6
8
10
Time [s]
L q [m
H]
Actual L qEstimated L q
( ) ( )( )( )IPF
ii iqd
1costantan
tantan,−+⋅−=
=+⋅−=
θθ
ϕθθξ
( )
( )
( )( )θ
θω
θϕθ
ω
θδ
ωθδλλ
sincoscos
sincos
sinsin
sinsin
,
1 IPFIE
IE
IE
iiiiL
i
q
qqdq
−+−⋅=
=+−⋅=
=⋅=⋅==
Torque at Constant Stator CurrentThe maximum torque per ampere (MTPA) is when
for certain current the torque is maximized
Under Saturation FEM
Ideal
Torque at Constant Stator Flux The maximum torque per volt (MTPV) is
when for certain flux the torque is maximized
IdealUnder Saturation FEM
Internal Power Factor (IPF) at Constant Stator Current
The maximum torque per kilo volt-ampere (MTPkVA) is when for certain current the power factor is maximized
IdealUnder Saturation FEM
Saliency Ratio at Constant Internal Power Factor (IPF)
Stator Current (p.u.) as parameter
Stator Current (p.u.) as parameterStator Flux (p.u.) as parameter
Machine Model
J. K. Kostko rotor 1923
d
λ
i
e
vqv
dvdλ
qλ
di
qi
si
q
ssiR
�
�
�
i�
�
( )( )
�e�cosIPF
�cosPF
RR
i
s-cr-c
⊥=
=
→
∆
∆ci
MOGHADDAMRREZA .
β
d
q
( ) θξλ
λδ
ϕθtan
1tan
tan1 ====+
−
dd
d
q
i iL
iL
100
100
100
100
200
200
200
200
300
300
300
300
400
400
400
400
500
500
500
500
600
600
600
600
700
700
700
70050
50
50
50
100
100
100
150
150
150
200
200
200
250
250
250
250
300
300
300
300
350
350
350
350
400
400
400
400
dq-axis Current idm & iqm [A Peak]
dq-a
xis
flux
λ d & λ
q [Vs
Pea
k]
λd & λq [Vs Peak] as function of d- and q-axis current
50 100 150 200 250 300 350 400
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
d-axis flux
(iq Parameter)
q-axis flux
(id Parameter)
Ldt
d�
�j�
cR
si isR
v e
ci
MOGHADDAMRREZA .
Saliency Ratio Estimator based on Power Factor
Inductances Estimator based on Terminal Values
SynRM
Internal Power Factor (IPF) at Constant
Saliency Ratio
angleload
angletorque
anglecurrent
::
:
δβ
δβθ +=The SynRM used for FEM and calculations
Simulated Machine Performance at Start Up and Nominal Load in Matlab-Simulink Including Saturation
IMSynRM
SynRM = Reluctance Concept + Rotating Sinusoidal Magneto Motive Force – the same as in IMIn this paper a simpler method to describe the SynRM behavior is discussed.
SynRM Capabilities vs. IMo Higher Efficiency;Eff1,+0.5-4%-unit.o Higher Torque density at same dT-rise; ~+25%.o Higher Overload Capacity. o Easier Production; no Cage.o Adaptability:
o Same Production Line.o Same enclosure.o ~ Same Inverter.
o Lower maintenance. o Higher Reliability.o ~ Same Field-Weakening.o Easier Sensor-less Control.o Braking at Standstill.
Constant torque
hyperbolae
Constant current circles
Constant voltage ellipses
di
qi
A
B
� Possible operating points of SynRM: points “A – G”. � Different control strategies: dashed vertical lines:
� MTPA (�=45°), MTPkVA (tan�=��) and MTPV (tan�=�)
� Delivering T0 with different control strategies:� Points “A”, “G” and “C” represent MTPA, MTPkVA and
MTPV respectively. Running the machine in all these conditions produces same torque T0.
� Field-weakening: If MTPA is followed for below base speed operation, point “A”, then in one strategy the machine current trajectory above base speed and in constant power region starts from “A” and moves to “D”, and for another method it passes point “D” and moves to “B”.
� Traditional Circle Diagram for machine operation demonstration