New Approach for the Low Speed Operation of PMSM Drives Without Rotational Position Sensors Power Electronics, IEEE Transactions on 512 IEEE TRANSACTIONS ON POWER ELECTRONICS, VOL 11, NO 3, MAY 1996 N[.]
Trang 1New Approach for the Low-Speed Operation of PMSM Drives Without Rotational Position Sensors
Joohn-Sheok IOm, Student, IEEE
Abstract- A new approach to the position sensor elimination
of permanent magnet synchronous machine (PMSM) drives for
low-speed operation is presented in this paper Using the position
sensing characteristics of PMSM itself, the actual rotor position,
as well as the machine speed, can be obtained even in the transient
state Since the essential back-EMF information is obtained from
direct measurement during a special test cycle called MCDI, the
operating speed range of the sensorless drives can be extended
to 10 rpm Moreover, the chronic starting problem of the PMSM
drives can be simply settled by the proposed algorithm In order
to verify the feasibility of the proposed scheme, experimental
results in the low-speed range of about 10 - 100 rpm are also
presented
I INTRODUCTION
P to now, machine drive systems without rotational
position sensors, the so-called sensorless drives, have
gained increased popularity in industrial applications because
of the inherent drawbacks of rotational sensors In general,
the rotational encoder-type sensors are used to obtain speed
or position information of the machine The major drawback
of these sensors is the performance degradation caused by
vibration or humidity Furthermore, these extemal sensors
will result in added cost and increase the size of the drives
[ 11-[6] By these reasons, there has been considerable interest
in developing techniques to achieve the position and speed
information for the sinusoidal back-EMF-type permanent mag-
net synchronous machine (PMSM) without extemal position
sensors The PMSM of this type has widely found its applica-
tion fields on the high-performance machine drive because of
the ripple-free torque characteristics and simple control rule
However, since none of the parameters of the PMSM with
sinusoidal back-EMF varies as a function of the rotor position,
it is very difficult to get the rotor position information without
rotational position sensors in this drives
Basically, most previous studies about the sensorless drives
for the PMSM with sinusoidal back-EMF-type start on the
foundation of the voltage equation of the machine and the
information of the machine terminal quantities, such as line
voltage and phase current Using this information with ma-
chine model, the rotor angle and speed were estimated di-
rectly or indirectly based on the back-EMF information by
various sensorless strategies [ 11-[5] In all cases, however,
since the machine parameters should be well-known for the
proper sensorless operation, the sensitivity to the machine
Manuscript received July 13, 199.5; revised November 30, 199.5
The authors are with the School of Electrical Engineering, Seoul National
Publisher Item Identifier S 088S-S993(96)03SS2-1
University, Seoul 15 1-742, Korea
and Seung-Ki s u l , Member, IEEE
parameter is a major drawback Another important demerit
of the previous studies is the limitation of the controllable speed range, especially in low speed range In the previous studies, the essential back-EMF information was estimated using the terminal quantities, such as currents and voltages But these quantities are very noisy because of the PWM operation of the power stage Especially in the low-speed range, the actual voltage information on the machine terminal can be hardly detected because of the small back-EMF of
the machine and the system noise For instance, when a typical machine with 2000 rpm-rated speed is operated at
50 rpm, the back-EMF is about 1.5 V only Considering the precision of the terminal voltage in PWM fashion and the system noise produced by the nonlinear characteristics of the switching devices [lo], the controllable lower speed range of the conventional sensorless drives is generally limited to the value of around 100 rpm Furthermore, another problem to be considered in the sensorless drives for PMSM is the starting capability At standstill state of the machine, the essential back-EMF information cannot be achieved in the conventional drive algorithm for itself In the literature [6]-[8], some special starting algorithm or initial position detection algorithm were studied for just machine starting However, in the case of sinusoidal back-EMF-type PMSM with symmetrical machine parameters, it is quite difficult to apply these methods to machine drive system
In this paper, new drive technique for the sinusoidal back- EMF-type PMSM drives without rotational position sensor
is presented As described above, the rotor position of the PMSM is related only to the phase of the back-EMF So, the information about the back-EMF of the machine plays the important role of the sensorless drives The back-EMF has a sinusoidal waveform of which magnitude is proportional to the rotor angular speed This means that the PMSM itself has a position sensor characteristic like the resolver-type rotational sensors In the proposed method, the back-EMF information
is obtained by direct measuring at the machine terminal not
by indirect estimation For the purpose of direct back-EMF measurement, a special test cycle, called maximum current decaying interval (MCDI), is introduced Since the back-EMF information is obtained from the direct measurement, the controllable speed range in sensorless drives can be extended
to 10 rpm without parameter dependency Additionally, the chronic starting problem of the PMSM drives without rota- tional sensors or with sensors like the incremental encoder can be solved using the proposed direct-voltage measuring strategy For the successful starting of the general PMSM
0885-8993/96$0.5.00 0 1996 IEEE
Trang 2q r
P
se
(-
vbs
Ld
Fig 1 Space vector diagram for the PMSM
drives, the standstill rotor angle should be known even if a
rotational sensor, such as incremental type encoder, is adopted
for angle detection By detecting the small back-EMF quantity
produced by an initial test current, the initial rotor angle can be
easily determined within several ones [“I in mechanical degree
As a result, the proposed direct back-EMF measuring strat-
egy can be applied to the general sensorless drive system
to increase the controllable lower speed range and to ensure
the initial starting capability To verify the feasibility of the
proposed method, some experimental tests are conducted for
the low speed range (10 N 100rpm)
11 SYSTEM DESCRIPTION
A System Modeling
The general equivalent space vector diagram for the PMSM
is illustrated in Fig 1 It is well-known that none of the
parameters of the PMSM with sinusoidal back-EMF are varied
according to the rotor position [l], [2] Therefore, the ma-
chine model based on the d-q reference frame theory can be
described in simple form as
R, i!pL,]
(Super script s denotes the stationary reference frame.)
As shown in (l), the terminal voltage of the machine con-
sists of the voltage drop terms related to the stator resistance
R, and stator inductance L,, and the back-EMF term including
the rotor speed w, and the back-EMF constant Kp? It is
generally assumed that the back-EMF has the true sinusoidal
waveform related to the rotor position, and its magnitude
is proportional to the rotor speed Therefore, in this aspect,
the PMSM with sinusoidal back-EMF has the positiori sensor
characteristics in itself like the resolver, and the essential in-
formation about rotor angle and speed can be simply obtained
from the back-EMF in the stationary reference frame So the
back-EMF quantity plays an important roll in the machine
drive system without rotational sensor Generally speaking,
this quantity can be obtained using the terminal voltage and
the information about the voltage drop terms In most previous
studies about sensorless drives, the rotor angle and speed are achieved using a specialized estimation algorithm about the back-EMF quantity However, the value of the back-EMF constant is just several 10’s V/krpm in the general commercial PMSM for servo applications Considering the value of K E ,
it is easily surmised that the back-EMF quantity should have
a value about several 1’s V when the machine is operated with 100 rpm mechanical speed Therefore, on the low-speed operating condition, it is quite difficult to obtain the back-EMF information by the conventional estimation method using the machine terminal quantities
B Back-EMF Detection Strategy for Low-Speed Operation
The back-EMF may be detected at the machine terminal through removing the corresponding voltage drops But, since each machine terminal is connected to the center point of the inverter arms in which the pole voltages have two voltage levels, such as zero or dc-link voltage, it is very difficult
to achieve the actual terminal voltage when this voltage is very small In this instance, if the machine terminals are disconnected from the inverter stage, there is one method to detect the small machine voltage at the machine terminal
In this paper, the back-EMF information is obtained by direct measurement of the terminal voltage As previously
mentioned, the back-EMF will appear at the machine terminal when the voltage drop associated with stator resistance and stator inductance is removed A simple way of removing the voltage drops is to hold the machine currents to zero When the machine terminal currents remain zero, the terminal voltage matches the back-EMF And to measure the terminal voltage in analog fashion, the machine terminal should be disconnected from the inverter arms However, it is not easy to actually disconnect the machine and power stage For the purpose of the implementation of disconnection effect, a third state of the inverter pole voltage is introduced in this paper
The states of the inverter pole voltages are always deter- mined by the gating signals Thus, each pole voltage has zero value or DC-link value according to the gating signals When the pole voltages are different from each other, some active voltage is applied to the machine Let’s define this state as the
‘first state’ of inverter In the other case, all the pole voltages have the same value to apply zero voltage to the machine and this condition is defined as the ‘second state’ of inverter In the conventional inverter operation strategy, the machine voltages are generated using these two pole voltage states However, if all the gating signals are removed from the switching devices, the third switching state can be implemented on the inverter side
As shown in Fig 2, when the machine currents flow through
the machine terminals, the phase current would hold its current state because of the inherent characteristics of the stator winding inductance In the normal operation state, the gating signals for upper or lower switching device are always given
by the on state alternately, except during dead time interval
As shown in Fig 2(a), if the gating signal for the lower device
is on, the normal current named, I,,,, flows through the lower switching device, and the current will flow through the upper
Trang 3Fig 2 Current flow at the inverter state of all gating off
diode attached to each switching device in the other case If
the current flows from machine to power stage, the opposite
state takes place, as shown in Fig 2(b) However, if all the
gating signals for switching devices are in the off state, the
machine current named io^ will unconditionally flow through
the upper or lower diode according to its direction, as shown
in Fig 2 Therefore, in this state, the pole voltages of the
inverter are just determined by the machine current direction
This phenomenon has been utilized for establishing the basic
idea of the dead-time compensation strategy also During this
third switching state, the stored energy in the stator inductance
is recovered on the dc-link side effectively For example, as
shown in Fig 2, the machine current is injected to the dc-
link voltage through upper diode or derived from the zero
voltage of the inverter side through the lower diode This
means that the negative largest output voltage is applied to the
machine terminal, and the terminal currents should be decayed
to zero with the maximum rate When the stored energy is
fully recovered and all machine currents reach zero value, the
terminal voltages are determined by the back-EMF because
of the absence of the voltage drop Therefore, the machine
terminals keep the electrically open state as the disconnection
state In this paper, the third state of inverter action is utilized
in the MCDI test cycle to measure the machine back-EMF
Considering the voltage equation of the MCDI test interval
leads that the terminal currents can be reduced to zero within
a few tenths of a microsecond For instance, when a PMSM
with 5-mH winding inductance is operated under 310-V dc-
link voltage condition, 5-A stator current will be reduced to
zero within 13 ps
5[A1 = 13[psec] (2)
ai
?; v d c $ .310 [VI
At the end of this MCDI test cycle, the back-EMF that
appears at the machine terminal can be directly measured
with analog fashion Since the neutral point of the PMSM
is not generally available, the back-EMF should be obtained
from the line-to-line voltage, as shown in Fig 3 The voltage
measurement circuit can be constructed with a laser-trimmed
differential-type isolation amplifier and some additional com-
ponents The maximum measurable line-to-line back-EMF is
clamped to 5 V by the back-to-back-connected zener diodes
and 10 k 0 resistance Therefore, the maximum operation speed
is limited to several hundred rpm In the upper speed range,
the back-EMF quantities can be properly estimated using an
, Inverter,
Fig 3 Back-EMF measurement circuit
T,, = 3.6msec
Y
I
I
I
E,', EA' detect & Speed Control
Fig 4 MCDI test cycle
estimation method [9] Another considerable point is the effect
of the parasitic capacitors on the switching devices Because
of this parasitic capacitor and the leakage inductance of the terminal lines, some resonant phenomenon takes place during the MCDI test cycle and the machine current does not diminish rapidly, as expected in (2) To prevent this resonance, some damping resistors are inserted between the machine terminal
in Y -connection form
With the consideration of the imaginary neutral point of the PMSM, the phase back-EMF can be derived as follows
E: + Et + E," = O
Therefore, the d-q components of the back-EMF on the
stationary frame can be obtained simply as,
E" = (2Ez - E{ - E , " ) / 3
(4)
E: =(E," - El)/&
111 SENSORLESS CONTROL STRATEGY
A Rotor-Angle Detection Strategy
The back-EMF measurement is performed by adding an MCDI test cycle to the current control algorithm, as shown
in Fig 4 In this figure, Test means the sampling interval for MCDI test cycle and for the rotor quantity estimation process At the beginning of the MCDI test cycle, all gating signals for the inverter are blocked When the stator currents reach the zero value, the back-EMF is measured 1; is the
Trang 4Fig
r$
I
I
5 The overall control diagram for low-speed sensorless drive algorithm
torque component current in the synchronous frame fixed to
rotor position After TdlP interval, normal current regulation
process is performed for torque generation Therefore, in the
proposed sensorless algorithm, consequential high-frequency
torque ripple would appear in the case of large viscous friction
load condition However, this ripple can be negligible if a
sufficient inertia is mounted on the machine shaft Considering
the general load pattern that the load quantity would be
increased according to the machine speed, the applicability
of the proposed drive scheme is not damaged Furthermore,
since the ripple frequency determined by the sampling interval
Test is considerably high, this torque ripple is not critical
in the aspect of drive Another choice of the sexisorless
drive for low-speed operation is the usage of the PMSM
with trapezoidal back-EMF In this case, the back-EMF also
can be directly measured at the nonconducting phase [ 2 ]
However, since the torque ripple inherently produced by the
two-phases conducting method is quite severe, it is very
difficult to generate continuously stable electrical torque So
the controllable lower-speed range would be limited about
several hundred rpm in the loaded operating condition
From the measured back-EMF, the actual rotor angle can
be achieved as follows
E: = E -E COS(^,) sin(0,) 1, E = J-.sign(4$)
COS(^,) = E i / E
sin(8,) = - E ; / E
: {
However, when some errors occur at the back-EMF de-
tection instance, the control angle might be influenced by
these errors directly, and this results in the system instability
Therefore, instead of above angle detection method, the rotor
angle is achieved using arc-tangent function and an angle
compensation algorithm is introduced in this paper First, the
rotor angle is achieved as follows
-E: - Kew, sin(0,) sin(0,)
E; Kew, cos(8,) cos(8,)
It is noticeable that the sign of the rotor speed should
be considered at the angle calculation because the speed information is canceled by the division operation of the arc- tangent function When the machine speed has negative value, the rotor angle can be described by
K,w, sin(0,)
= tan(0, - 180')
- sin(0,) - sin(0, - 180')
-
-
-
E; K,w, COS(^,) - COS(^,) COS(^, - 180')
: 8, = t a n 2-'(-E:, E,") + 180' (7)
Therefore, the rotor angle is represented as follows
(8)
The speed direction can be identified using the calculated
0, = 0, + 7r
rotor angle as follows
1 if A&,, > 0
-1 if A0,,,, < 0
To avoid the conflict between (8) and (9), a hysteresis with some bands is added to the rotor speed direction determination process In Fig 5 , the overall rotor angle estimation process
is depicted The lower area enclosed by a dashed box corre- sponds to the speed direction detection process with hysteresis function And the upper area enclosed by another dashed box represents the angle compensation algorithm In this algorithm, the deviation of the calculated rotor angle is limited to some value according to the rotor speed to stabilize the control angle
in the transient state The basic operation concept is that the rotor angle deviation during one estimation step has the same value of the time integral value of the rotor speed Thus, the maximum deviation will be limited by following value
AO,,, = 1.5 x ILF(&)I Test
Trang 5516 MAY 1996
(The L F ( ) function means the low-pass filter.)
If the angle deviation is smaller than these maximum
values, the control angle Bc always follows the rotor angle
6 , calculated from the measured back-EMF However, if the
deviation of the control angle exceeds the maximum value, this
deviation is restricted to the maximum value and the control
angle is more slowly changed than the calculated angle With
the help of this angle compensation algorithm, the control
angle is always maintained to the actual angle with sufficiently
negligible error, even if some measurement errors occur
At the end of the MCDI test cycle, the gating signals are
returned to their original state, and the normal current control
sequence is restarted In this study, the current sampling
interval is chosen to be 60 ps, and the current control algorithm
based on space voltage vector is used for high-performance
current regulation
machine would be slightly rotated to arbitrary direction The rotor angle deviation between the initial point and moved point
is very small, but the angular speed would be sufficiently great to detect the rotor angle Whenever the machine speed
is higher than 10 rpm, the essential back-EMF can be directly measured, and the initial angle detection process can be accomplished through the proposed angle detection strategy Therefore, within several ones ["I deviation of the rotor shaft
in mechanical degree, the initial rotor angle can be easily detected Just after the initial angle determination cycle, a proper starting torque is generated with the information about the electrical initial rotor angle, and the rotor is smoothly rotated according to the direction of the speed command This important feature also can be applied to the general PMSM drives with an incremental encoder type position sensor for smooth machine starting When the incremental encoder is used, the actual rotor position can be achieved
B Speed-Detection Algorithm
From the basic machine equation (I), the back-EMF infor-
mation can be utilized for the accurate rotor angular speed w,
as follows
w, = sign( $) ' d m / K E
when the first zero pulse is encountered Therefore, in most drives, a special type encoder that provides U, V, W pulses
is used for the initial starting However, the rotor position information with just 60" precision is available using this special encoder at the initial starting instance Moreover, in order to measure these pulses, an additional six lines should
be connected between machine and controller for only the initial starting Using the proposed simple voltage measuring minimum area and smallest wiring, the initial position angle
Every MCD1 test cyc1e, the speed can be equipment that can be mounted on the control board with from the back-EMF and speed control algorithm is performed
operating condition, the following remark should be made on
the back-EMF constant
For an accurate determination of w,, it is necessary to
Although the above equation is guaranteed in can be easily detected within reasonable range
IV EXPERIMENTAL RESULTS know the correct back-EMF constant K E This parameter
may be uncertain or may be varying according to the thermal
environment Changing this parameter will cause steady-state
error of the estimated speed This uncertainty can be overcome
by the back-EMF compensation algorithm [9] The basic idea
of this algorithm is that the back-EMF constant slowly varies
according to thermal condition and the long-term average of
the time differentiation value of rotor angle has the same value
of the actual rotor speed With the help of this algorithm,
not only the parameter variation but also the measurement
error of the back-EMF can be compensated easily Because
of the direct rotor position measuring strategy, the back-EMF
constant can be modified to the suitable value to remove the
steady-state error of the estimated speed
C Starting Strategy
Generally, in the PMSM drives, the information about the
standstill rotor angle is required at the initial start-up instant to
produce a proper electrical torque for starting In the case of
the drive system without position sensors, a specially designed
starting algorithm should be included in the drive algorithm
because the back-EMF is not available at the start-up [6]
However, if the proposed direct back-EMF detection strategy
is adopted for the machine drive system, the starting capability
can be given to the drive system in itself
At the start-up instant, a test current with short pulse form
is injected to the machine current By this test current, the
Experimental tests are conducted to evaluate the perfor- mance of the proposed back-EMF detection strategy and the feasibility of the new position sensor elimination technique for low speed operation The overall PMSM drive system for the laboratory prototype test is illustrated in Fig 6 The tested drive system consists of a six-pole Y-connected 0.47 [kW] PMSM and an electric dynamometer load The rating and parameters of the PMSM are presented in Table I The power stage comprises the IGBT inverter with 8.33-kHz switching frequency and 200-V dc link And, high-performance digital signal processor (DSP), TMS320C30 controller specially de- signed for machine drive is used to implement the overall proposed sensorless algorithm, based on C language The whole experimental results including current, machine speed, and angle traces are illustrated by the multichannel oscillo- scope through D/A converter equipped on the main controller Moreover, for monitoring purposes only, an additional incre- mental encoder with 2000 ppr resolution is attached to the machine shaft The actual machine speed and rotor angle are taken from this sensor
The experimental waveforms of the proposed MCDI test cycle are shown in Fig 7 The PMSM is operated with 50 rpm constant speed by the proposed sensorless control algorithm In Fig 7(a), the actual rotor angle in electrical angular degrees is displayed The estimated rotor angle from the proposed angle- estimation strategy is shown in Fig 7 (b), and the detected back-EMF quantity on the stationary q-axis is shown in the
Trang 6i
KE (DC equivalent model)
Iyo+a(DC equivalent model)
._
- -
.- 6.5 [mH]
0.03 [ V/rpm]
.-
l"32OC30
DSP Controller
- > > -
L L : 1
I
(d) v m l ] ? d T L
0
Fig 6 Laboratory experimental setup
TABLE I PMSM RATING AND PARAMETERS
3-phase 6pole Sinusoidal back-EMF PMSM -
Rate Power I 0.47 [kWl ,_
R" I 1.26 r ni
.-
0 rate I 2000.0 [rpm]
T
Fig 7 Experiment waveforms of the MCDI test cycle (a) Actual rotor angle
(elec angle) (b) Estimated rotor angle (elec angle) (c) Detected stationary
q-axis back-EMF (d) Synchronous q-axis current (enlarged time base)
next figure As shown in these figures, using the proposed
MCDI test cycle, the essential back-EMF quantities can be
clearly detected and the new sensor elimination control :scheme
for the low-speed operation has performed very well In the last
figure, Fig 7(d), the torque component current of the machine
is presented in the sampled data fashion To show the MCDI
test interval precisely, the time duration between two anrows in
the other figures is enlarged in this figure At the initial points
of each test cycle, the machine currents are quickly diminished
to zero value to directly measure the back-EMF When the
back-EMF is completely detected, the machine currents are
rapidly stabilized to produce the required electrical torque
Of course, the whole electrical torque is affected by the test
cycle for back-EMF detection, and the maximum conlhuous
output power of the proposed control strategy is limited to
Fig 8 Speed control performance (10 rpm) (a) and (b) Detected syn- chronous q-axis and d-axis back-EMF (c) and (d) Actual and estimated rotor angle (elec angle) (e) and (f) Actual and estimated rotor speed
some value However, this sensor elimination technique can be effectually utilized to some applications in which a continuous full torque operation is not needed and an effective low speed operation is required without position sensors
Fig 8 shows the speed-control performance of the proposed algorithm with 10 rpm speed reference In Fig 8(a) and (b), the traces of the measured back-EMF are shown As shown
in these figures, some low order harmonics are included in the back-EMF waveform These harmonic components appear actually in the machine itself because of the slightly small misalignment of the stator winding or inherent flux distribution
of the permanent magnet However, this harmonic component would be negligible in the higher speed range because the magnitudes of this harmonics are nearly constant irrespective
of the magnitude of the fundamental back-EMF In Fig 8(c)
Trang 7-1001 I t
4
4
Fig 10 50 [rpm]) (a) Initial angle difference E 70°, No load (b) Initial angle difference
5Z -120°, No load (c) Initial angle difference 5Z -40' 1/4 load (d) Initial angle difference -150°, 1/4 load (In each figure, first traces: actual rotor angle (elec.); second traces: estimated rotor angle (elec.); third traces: actual machine speed; last traces: torque component current command on the reference frame fixed to 8est.)
Starting performance of the proposed algorithm (0 i
and (d), the actual rotor angle and the rotor angle calculated
from the back-EMF are shown And, the actual rotor speed
and calculated speed are displayed in Fig 8(e) and (0 The
rotor speed quantities are fluctuated owing to the harmonic
component of the back-EMF If a higher control band width
is selected for speed controller, this speed fluctuation can be
decreased to some degree
In Fig 9, the step response of the proposed sensorless
PMSM control algorithm is depicted when the speed reference
is changed from 20 to 100 rpm and back with 40% rating
load From these experimental results, it can be seen that the
measured back-EMF can be successfully used to obtain the
necessary position and speed information for replacing a shaft
sensor at low speed range (10 - 150 rpm) However, this
proposed sensorless method cannot be applied to the system
that has large viscous friction load at low speed operation
range, because the current decaying operation in the MCDI
test circuit may result in the mechanical resonance when high
current flows to machine In the upper speed range, over 150
rpm, the basic machine-model-based method, such as [9], may
be adopted for the sensorless drives
In Fig 10, the starting performance of the proposed scheme
is presented As described above, since the initial rotor position
can be detected through the injected test current and voltage measurement system, the direct back-EMF measuring strategy gives good starting ability to the control system As shown in the lowest trace of Fig 10(a), the test current for producing arbitrary torque is injected with the initial control angle, which
is always maintained at zero on the stationary reference frame
at the power-up instance During the test current injection cycles, the whole rotor angle estimation process previously mentioned is performed And within a sufficiently short time, the information about the initial rotor angle can be obtained Therefore, at the end of the test cycle, the machine gets
started by the proposed sensor elimination control scheme As shown in Fig 1O(c) and (d), the starting process is successfully applied, even in the same loaded case Considering that the outer load is generally given by the pattern that is proportional
to the machine speed or the square value of the machine speed, the machine starting under a general loaded condition is no more a critical problem
V CONCLUSION
A new approach to the position sensor elimination of the PMSM drives for low-speed operation is presented in this
Trang 8paper It is shown that the actual rotor position, as well as
the machine speed, can be achieved strictly using the: MCDI
test cyc1e and direct measuring the back-EMF with a simp1e
measurement circuit Additionally, a relatively smooth start
[9] J S Kim and S K SUI, “New approach for high performance PMSM
drives without rotational position sensors,’’ APEC Con5 Rec., pp
381-386, 1995
[lo] J S Kim, J W Choi, and S K SUI, “Analysis and compensation
of voltage distortion by zero current clamping in voltage-fed PWM
inverter,”Yokohama ZPEC Conf Rec., pp 265-270, 1995
can be achieved by the injection of a simple test current to
the machine To avoid the steady state-speed estimation error
caused by the parameter variations, the back-EMF constant
compensation algorithm is also proposed The experimental
results show the important features of the new methold in the
low speed region (10-100 [rpm]) with acceptable accuracy
REFERENCES
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Joohn-Sheok Kim (S’92) was born in Korea in
1965 He received the B.S and M.S degrees in electrical engineering from Seoul National Univer- sity, Korea, in 1989 and 1992, respectively, where
he is working toward the Ph.D degree in the area
of power electronics
His major interests are adjustable speed ac drives and static power converter
_ _
120-127, 1992
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3, pp 491497, 1991
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filter estimation of speed and rotor position of a pm synchronous motor,”
ZECON Conf R e c , pp 2097-2102, 1994
[6] R Krishnan and R Ghosh “Starting algorithm and performance of a pm
dc brushless motor drive system with no position sensor,” PLSC Conf
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[7] M Matsui and T Takeshita, “A novel starting method of censorless
salient-pole brushless motor,” ZAS Conf Rec , pp 386-392, 1994
[8] S Kondo, A Takahashi, and T Nishida, “Armature current locus based
estimation method of rotor position of permanent magnet synchronous
motor without mechanical sensor,” ZAS Conf Rec , pp 55-60 1995
Seung-Ki SUI (S’78-M’87) received the B S , M S ,
and P h D degrees in electrical engineering from Seoul National University, Korea, in 1980, 1983, and 1986, respectively
He was with the Department of Electncal and Computer Engineering, University of Wisconsin, Madison, as a Research Associate from 1986 to
1988 He joined Gold-Star Industnal Systems Com- pany as Principal Research Engineer in 1988, where
he remained until 1990 Since 1991 he has been with the Department of Electrical Engineenng, Seoul National University His present research interests are in high-performance electnc machine control using power electronics He is performing vanous research projects for industnal systems and some of the results are applied to the fields of industrial high-power electric machine control