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Zero–speed sensorless drive capability offractional–slot inset
PM machine
Adriano Faggion Nicola Bianchi Silverio BolognaniEmanuele
Fornasiero
Electric Drives LaboratoryDepartment of Industrial
EngineeringUniversity of Padova
PEMD 2012Power Electronics, Machines and Drives Conference
Bristol, 27-29 March 2012
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
This presentation refers to the paper:
Adriano Faggion, Nicola Bianchi, Silverio Bolognani andEmanuele
Fornasiero
”Zero–speed sensorless drive capability offractional–slot inset
PM machine”
IEEE – PEMD 2012Power Electronics, Machines and Drives
Conference
Bristol (UK), 27-29 March 2012.
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fractional–slot inset PM machine 2
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Outline
1 Introduction
2 Self sensing rotor position detection
3 Inset 12–slot 8–pole PM machine
4 Finite element simulations
5 Experimental results
6 Conclusions
PEMD 2012 Zero–speed sensorless drive capability of
fractional–slot inset PM machine 3
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Introduction
Sensorless control purpose
For the sensorless control purpose, three different
rotorconfigurations are studied in a previous paper:(a)
Interior,(b) Ringed–pole and (c) Inset Permanent Magnet
(PM)Rotor.
(a) Interior PM motor (b) Ringed pole PMMotor
(c) Inset PM motor
PEMD 2012 Zero–speed sensorless drive capability of
fractional–slot inset PM machine 4
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Introduction
Sensorless control purpose
For the sensorless control purpose, three different
rotorconfigurations are studied in a previous paper:(a)
Interior,(b) Ringed–pole and (c) Inset Permanent Magnet
(PM)Rotor.
⇒ Among these the inset PM machine results to have agood
performance as far as the sensorless rotor positiondetection is
concerned.Then in the paper a 12–slot 8–pole inset PMconfiguration
is deeply studied.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Sensorless technique1 The detection of the rotor position by
means of a high
frequency (HF) signal injection is a common sensorlessdetection
technique.
2 It consists on the injection of a HF voltages in the
statorwindings, which causes a HF currents.
3 HF current vector draws a figure that containsinformation of
the rotor position.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Rotation due to thecross-saturation effect
Rotating HF voltage vector⇓
Ellipse HF current vectortrajectory⇓
HF saliency can bedefined as:
ξHF =∆Imax∆Imin
⇓mutual inductance Ldqh
causes the ellipseinclination �
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fractional–slot inset PM machine 7
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
HF rotating voltage, injected in a general rotating
referenceframe dxqx , of the type:
uxdh = Uhcos(ωht)uxqh = Uhsin(ωht)
is adopted.It is assumed that the machine is standstill
(electrical speedequal to zero).
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
The magnetic model of the machine can be described bymeans of
the matrix of differential HF inductances in eachoperating point,
expressed by:
L =[
Ldh LdqhLqdh Lqh
] Lavg = Lqh + Ldh2Ldif =
Lqh − Ldh2
Ldh is the HF d–axis inductanceLqh is the HF q–axis
inductanceLdqh is the HF cross saturation inductanceLavg is the HF
average inductanceLdif is the HF difference inductance.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
High Frequency current vector results of two components:
īdqh = īcw + īccw
with
īcw = −Λh∆
Lavgej(ωht+π2 )
īccw = −Λh∆
√L2dif + L
2dqh
e−j(2(∆θ−�)+ωht+π2 )
where � is the displacement due to the presence
ofcross-saturation between the d– and q–axis. It can becomputed
as:
� =12
arctan(−
LdqhLdif
)and ∆ = LdhLqh − L2dqh ,∆θ = θ̃me − θme.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
HF voltage vector injection in the actual dq ⇒ ∆θ = 0
andthen:
īdqh = −Λh∆
Lavgej(ωht+π2 )︸ ︷︷ ︸
īcw
− Λh∆
√L2dif + L
2dqh
e−j(−2�+ωht+π2 )︸ ︷︷ ︸
īccw
ī cwī ccw
(d)
ī cw
ī ccw
(e)
ξHF =∆Imax∆Imin
=Lavg +
√L2dif + L
2dqh
Lavg −√
L2dif + L2dqh
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
The HF current vector īdqh is used to recognize themaximum axis
direction of the ellipse. This should coincidewith the d–axis.
x
x
(f) Ideal case Ldqh = 0
xx
(g) Real case Ldqh 6= 0
However, because of the cross–saturation the actual d–axisis not
correctly recognized but an axis displaced of theangle error � with
respect to the d–axis is found.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Figure: Sensorless rotor position estimation scheme
Output of the estimation scheme is:
idemf = −Λh∆
√L2dif + L
2dqh
sin(2∆θ − 2�)
This quantity is manipulated in order to zeroing the term∆θ − �.
The result is:
∆θ − � = 0 ⇒ θ̃me = θme + �
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Particular case ]1If the motor does not exhibit a
cross–saturation between thed– and q–axis, the angle error �
becomes equal to zero.The direction of maximum axis is along the
d–axis.
⇒ Correct estimation of the rotor position.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Particular case ]1No cross–saturation between the d– and q–axis.
Angleerror � becomes zero.
ξHF =Lavg +
√L2dif + L
2dqh
Lavg −√
L2dif + L2dqh
⇒ ξHF =Lavg + LdifLavg − Ldif
=LqhLdh
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Particular case ]2If the d– and q–axis inductances are equal,
the currentvariation on the d– and q–axis becomes equal.Anyway, the
HF saliency remains, due to thecross-saturation.
⇒ Rotor position estimation with 45◦ angle error.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Particular case ]2d– and q–axis inductances equal. HF saliency
remains, duethe presence of the cross-saturation.
ξHF =Lavg +
√L2dif + L
2dqh
Lavg −√
L2dif + L2dqh
⇒ ξHF =Lavg + LdqhLavg − Ldqh
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Particular case ]3In case of:• No cross–saturation between the
two axes• d– and q–axis HF inductances equalthen the current
ellipse degenerates into a circle.
⇒ Rotor position detection not allowable.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Self sensing rotor position detection
Particular case ]3No cross–saturation and d– and q–axis
inductances equal.The current ellipse degenerates in a
circumference.
ξHF =Lavg +
√L2dif + L
2dqh
Lavg −√
L2dif + L2dqh
⇒ ξHF =LavgLavg
= 1
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Inset 12–slot 8–pole PM machine
Geometry of 12–slot 8–pole inset PM motor
(a) (b)
In red the coil of phase a. The stator exhibits afractional–slot
non–overlapped coil winding.
Variable Dimension measure unity
Stack length 90 (mm)External stator diameter 133.6 (mm)Inner
stator diameter 71.5 (mm)PM thickness 4.95 (mm)PM width 16 (mm)
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Inset 12–slot 8–pole PM machine
Geometry of 12–slot 8–pole inset PM motor
Id = 0 and Iq = 0.Without the current the flux due to the PMs
practicallydoesn’t flow through the tooth.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Inset 12–slot 8–pole PM machine
Geometry of 12–slot 8–pole inset PM motor
(c) Id = I and Iq = 0 (d) Id = 0 and Iq = I
FE simulation have been done excluding the effect of
themagnet.In the case of Fig.(d) there is a more density of the
flux lines.Then the Lq inductance results greater than the Ld
one.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Finite element simulations
FE Simulations
The FE simulations have been carried out with the aimof
determining the main characteristics of the motor.Some simulations
have been done for different (Id , Iq)currents, to cover a wide
range of operating points.Nominal current is IN = 10 A.The current
limits are −20 A ≤ Id ≤ 20 A and0 A ≤ Iq ≤ 20 A.The differential
inductances are computed and themagnetic saliency of the motor is
derived.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Finite element simulations
Map of the magnetic saliency ξHF
• It is worth noticing that the saliency is sufficientlyhigh in
the whole second half plane. It remains aroundξHF = 1.6.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Finite element simulations
Map of the ratio Ldif /Lavg .
• The difference inductance Ldif is greater than zero inthe
whole Id–Iq plane.⇒ The rotor position is detected even under
overload.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Finite element simulations
Map of the ratio Ldqh/Lavg
• The cross–saturation inductance Ldqh is negligiblealong the
MTPA trajectory.⇒ The angle error � is very low.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Finite element simulations
Map of the error |�| due to cross–coupling (deg)
• � remains lower than 1 el .deg. up to the nominalcurrent.• �
increases for higher currents, however remaininglower than 10 el
.deg. along the MTPA trajectory.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Finite element simulations
Inset 12–slot 8–pole rotor configuration
Summary of the motor characteristicsX A difference inductance
Ldif is always greater
than zero in a whole plane, since Lqh > Ldh.X The mutual
differential inductance is negligible,
since it is quite similar to that on a SPM motor.X The angle
error due to the cross–saturation is
very low, especially along the MTPA trajectory.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Experimental results
Test bench setup
Some experimental tests have been carried out in order toverify
the self–sensing motor capability in all the dq currentplane.
INVERTER
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Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Experimental results
Experimental setup
• The machine under test is coupled to a master drive.• The
master drive can be speed– or torque–controlled byan industrial
inverter.• The inset PM machine is controlled by a
laboratoryinverter monitored by an acquisition system.• A rotating
voltage vector, with amplitude Uh equal to 20 V ,is added to the
reference power voltages u∗d and u
∗q given by
the current regulators.• The injection frequency is set to 500
Hz.• The tests have been carried out locking the inset PMmachine by
the master one.
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Conclusions
Experimental results
High frequency currents at two different working pointsalong the
MTPA trajectory
time (s)
i d(A
)
0 0.002 0.004 0.006 0.008 0.01−2
0
2
time (s)
i q(A
)
0 0.002 0.004 0.006 0.008 0.01−2
0
2
(e) id = 0 and iq = 0
0 0.002 0.004 0.006 0.008 0.018
10
12
0 0.002 0.004 0.006 0.008 0.01−4
−2
0
time (s)
i d(A
)
time (s)
i q(A
)
(f) id = −2 and iq = 10
X Each current is given by the sum of a constant value anda
sinusoidal signal due to the HF voltage injection.X The amplitude
of the iq current oscillation is lower thanthat of the id current,
being Lqh > Ldh .
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Experimental results
High frequency ellipses in the id –iq plane
−8 −6 −4 −2 0 2 4 6 8 10 12 14−8
−6
−4
−2
0
2
4
6
8
10
12
14MTPAHF Ellipse
Rotation due to thecross-saturation effect
X The HF saliency is obtained applying: ξhf = ∆Imax/∆Imin.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Experimental results
HF Saliency
−8 −6 −4 −2 0 2 4 6 8 10 12 14−8
−6
−4
−2
0
2
4
6
8
10
12
14MTPAHF Ellipse
X ξHF for each ellipse are slightly lower to those estimatedby
FE simulation.X ξHF remains equal to 1.6 in all the left dq
half–plane.X FE simulations highlight that the saliency remains
also inoverload conditions.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Experimental results
Angle error �
−8 −6 −4 −2 0 2 4 6 8 10 12 14−8
−6
−4
−2
0
2
4
6
8
10
12
14MTPAHF Ellipse
X All the ellipses have the maximum axis practically parallelto
the d–axis.X This means that the error � is very low.X With |̄i | ≤
IN the � remains lower than 1 el .deg..X A low error confirms the
low cross–saturation effect.X This confirms the results given by
the FE simulation.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Conclusions
Conclusions
X The 12–slot 8–pole inset PM motor results to be verysuitable
for the sensorless rotor position detection, based onthe HF voltage
injection.X The iron tooth introduced between each couple of
PMsyields a proper HF rotor saliency.X This magnetic behaviour
results to be slightly affected byiron saturation and
cross–saturation phenomena.X This characteristics remain also under
overloadoperations.
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Conclusions
Related Papers by the Authors
S. Bolognani, S. Calligaro, R. Petrella, and M.
Tursini,”Sensorless control of ipm motors in the low–speedrange and
at stand–still by hf–injection and dftprocessing.”,In in IEEE
International Electric Machines and DrivesConference, 2009. IEMDC
’09., May 2009, pp.1557–1564.
N. Bianchi, S. Bolognani, J.–H. Jang, and S.–K. Sul,”Advantages
of inset pm machines for zero–speedsensorless position
detection”,IEEE Trans. on Industry Applications, vol. 44, no. 4,
pp.1190 –1198, 2008.
PEMD 2012 Zero–speed sensorless drive capability of
fractional–slot inset PM machine 36
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Conclusions
Related Papers by the Authors (cont.)
N. Bianchi, S. Bolognani, and A. Faggion,”Predicted and measured
errors in estimating rotorposition by signal injection for
salient-pole pmsynchronous motors”,in IEEE International Electric
Machines and DrivesConference, 2009. IEMDC ’09., May 2009,
pp.1565–1572.
A. Faggion, S. Bolognani, and N. Bianchi,”Ringed–pole permanent
magnet synchronous motor forposition sensorless drives”,in IEEE
Energy Conversion Congress and Exposition,2009. ECCE 2009., 2009,
pp. 3837 –3844.
PEMD 2012 Zero–speed sensorless drive capability of
fractional–slot inset PM machine 37
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Introduction
Self sensingrotor positiondetection
Inset 12–slot8–pole PMmachine
Finite elementsimulations
Experimentalresults
Conclusions
Conclusions
Related Papers by the Authors (cont.)
A. Faggion, N. Bianchi, and S. Bolognani,”A ringed–pole spm
motor for sensorless drives –electromagnetic analysis, prototyping
and tests”,in IEEE International Symposium on
IndustrialElectronics, ISIE 2010, Bari, IT, Jul. 4–7, 2010.
A. Faggion, E. Fornasiero, N. Bianchi and S.
Bolognani,”Sensorless capability of fractional-slot
surface-mountedPM motors”,in Electric Machines Drives Conference
(IEMDC), 2011IEEE International, 2011, pp. 593 –598
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Self sensingrotor positiondetection
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Finite elementsimulations
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Conclusions
Conclusions
Thank you for the attention.
PEMD 2012 Zero–speed sensorless drive capability of
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IntroductionSelf sensing rotor position detectionInset 12–slot
8–pole PM machineFinite element simulationsExperimental
resultsConclusions