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International Journal of Power Electronics and Drive System (IJPEDS)
Vol. 8, No. 3, September 2017, pp. 1147~1159
ISSN: 2088-8694, DOI: 10.11591/ijpeds.v8i3.pp1147-1159  1147
Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS
Indirect Pulse-vector Control of Wound Rotor Induction Motor
Drive in ANSYS Electromagnetics Suite
Tatiana Andreevna Funk, Yuriy Semenovich Usynin, Evgeny Viktorovich Belousov
Department of Electric Drive, South Ural State University, Chelyabinsk, Russian Federation
Article Info ABSTRACT
Article history:
Received Jun 26, 2017
Revised Aug 5, 2017
Accepted Aug 20, 2017
This paper deals with the problem of estimation of rotor angular position for
the indirect pulse-vector control of wound rotor induction motor drive. The
paper considers issues of thematic justification and expanding of the field of
using sensorless motor drives. With a view to improve energy consumption
readings during design and modernization of motor drives of massive
mechanisms with moderate standards for accuracy of velocity control,
requiring long-term velocity decrease during load reduction (according to
technological process conditions), using the system of the pulse-vector
control of wound rotor induction motor is suggested. The paper provides the
solution for the problem of developing math models of this motor drive
system both for the motor-mounted sensor, and for indirect angular position
sensing. The models were developed in ANSYS Electromagnetics Suite
using the finite element method for studying electromagnetic processes.
Based on the models, the investigation of transition and steady states of a
motor drive was carried out, process quality parameters were obtained,
namely: max and root-mean-square currents, torques; velocity control errors
caused by pulse operation mode. From that simulation, the result illustrates
the effectiveness of the proposed approach.
Keyword:
Finite element method
Indirect control system
No motor-mounted sensor
motor drive
Wound rotor induction motor
pulse-vector control
Copyright © 2017 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Tatiana Andreevna Funk,
Department of Electric Drive,
South Ural State University,
76 Lenin prospect, Chelyabinsk, Russian Federation, 454080.
Email: kozinata@susu.ru
1. INTRODUCTION
In the recent years, indirect determination of variable coordinates of a no motor-mounted sensor
motor drive, or so-called sensorless methods are coming into wider use for various mechanisms and motor
drive control systems [1]-[9]. Sensorless systems enable to improve regulation characteristics of control
objects with no mounting of the direct measurement device onto the motor shaft required [1],[2]. Moreover,
in some cases, mounting a sensor onto the shaft can be either economically or technically unfeasible [3], or
crucially impossible due to technological process conditions – for instance, because of vibration, radiation,
emissions, extreme temperatures, powered motions, and isolated location of a unit from the control system.
In the general context, application of indirect methods for velocity and position determination is
most relevant within the design and modernization of massive mechanism motor drives with moderate
standards for accuracy of velocity control: lift-and-carry mechanisms, industrial fans, band conveyors,
hydraulic pumps, compressors, air blowers, smoke and air exhausters, etc. [10].
Among them, mechanisms requiring velocity decrease during long-term load reduction or removal.
For instance, fans built in industrial facilities, air exhausters in oxygen converter plants. This group may also
include motor drives of band conveyors (provided that they are idle at night shifts), but in order to prevent
freeze-up of bearing greasing, it is reasonable to switch them to lower rotation in no-load conditions.
 ISSN: 2088-8694
IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159
1148
In the quality of power motors in above mechanisms, induction motors with short-circuit or wound
rotors are used. The motor velocity either remains non-adjustable, or is adjusted inserting ballast resistors to
stator’s or rotor’s circuits. No adjustment or using relay-contactor circuits is accompanied by higher energy
consumption. Rise in prices of electric energy and other power resources results in need for modernization of
considered motor drives [6],[11].
Using two-section frequency changer in such mechanisms is not always feasible due to high cost,
complicated operation, and heavy requirements for personnel qualification. There was a range of studies
dedicated to the pulse-vector control (hereinafter – PVC) of wound rotor induction motor drive (hereinafter –
WRIM) [12],[13]. The purpose of those systems is to create the current in the rotor with the frequency same
to stators, i.e. to prevent sliding. They fairly suit the above mechanisms because of moderate cost and having
no excessive adjustment capabilities, as well as show low energy consumption under low-velocity modes.
Control in such system is carried out depending on the rotor angular position – thus, it is essential either to
mount the position sensor onto the shaft, or to use the method for indirect rotor position determination.
Previous studies and papers on the PVC of motor drives suggested the PVC of WRIM with the rotor
position sensor [12], described the developed principle and algorithm for indirect determination of the initial
angular position, established differential equations and functional relationships between state variables and
rotor turning angle, giving the brief explanation of the system modeling through using the finite element
method [13]. The present paper sets the problem of developing an exhaustive math model and studying the
PVC of WRIM, aimed at further use of the system to improve the technological process quality and enhance
resource and energy consumption readings of massive mechanisms.
2. RESEARCH METHOD
2.1. The Method of the PVC of WRIM
The considered PVC [12] contains the three-phase WRIM and three-phase thyristor bridge rectifier.
Shall we denote stator windings by AX, BY, CZ, and phases of three-phase powering voltage by A, B, C.
The electromagnetic moment will be formed by sequential series connection of two stator phases through
corresponding thyristors to two rotor windings. The magnetomotive force (hereinafter-MMF) vector of stator
windings performs discrete motion with a 60-degree step. Switching is made depending on the rotor position,
thereby providing the orientation of MMF vectors of stator and rotor windings to correspond to the motor
torque. Either stator winding is left off the line during operation of two other ones. The tertiary rotor winding
is being off the line during the whole operation cycle.
2.2. Specifics of Modeling the PVC of WRIM and Indirect Position Determination (IPD)
The considered PVC system constitutes the multi-phase, pulse, non-linear, unsymmetrical system,
thus, examination of its operation in steady and transition modes by using the analytic methods for analyzing
electromagnetic processes – for instance, applying differential equations of the multi-phase circuit is inclined
to excessive complicating and extension of calculation conditions included as a compound of the math
model. It may be reasonable to take advantage of using the progressive numerical methods for analyzing the
electromagnetic system, and calculate the motor drive through using the finite element method [14].
Application of this method enables to take specifics of the motor drive system into account and
significantly simplify processing and analysis of the modeling results. ANSYS Electromagnetics suite was
used as it enables to: create a WRIM state space model, calculate the motor drive through using the finite
element method; carry out analysis of electromagnetic processes in close relation to the powered motions and
control system; analyze changes of circuit currents, electromagnetic torque, and voltages on motor windings,
depending on the relative position of the stator and the rotor. In solving the problem of mathematical
analysis, the experience of modeling motor drive systems using the finite element method, described in [15],
was taken into account.
Modeling of the PVC system with indirect determination of the rotor angular position in ANSYS
Electromagnetics Suite was divided into three stages: сreating the WRIM model as a control system unit, and
analysis of its operation in steady and transition modes through using the finite element method; engineering
the model of the PVC system using the rotor position sensor, and analysis of motor drive operation as a
control system prototype, with indirect determination of the rotor angular position; developing the model of
the PVC of the induction motor with indirect determination of the rotor angular position; analysis of this
motor drive system in steady and transition modes.
2.3. Architecting and Analyzing the WRIM Model
As a prototype for modeling, the crane-metallurgy wound rotor motor MTF111-6 was chosen.
Nameplate data of the motor are given in Table 1.
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1149
Table 1. MTF 111-6 Motor Nameplate Data
Parameter Unit Value
Nominal Stator Voltage V 380
Nameplate Angular Velocity rpm 895
Nameplate Power kW 3.5
Cos ϕ - 0.73
Energy Conversion Efficiency % 70
Nameplate Stator Current A 10.4
Nameplate Rotor Current A 15
Nameplate Electromotive Force on Rotor Rings V 176
Crippling Torque N∙m 85
Pole Pairs pcs 3
Created based on key geometric dimensions, parameters of gaps and motor windings [16], the 2D
motor model is given in Figure 1(a), considering the number of pole pairs. Stator and rotor cores are made of
electric steel No. 1212, induction-permeability of which was set as the non-linear property based on 24
points [17]. Motor windings are made of copper.
During architecting the model, the rotation area was created and included the rotor and motor shaft,
ground potential boundaries were determined; three-phase stator and rotor windings were distributed over
slots; the number of coil windings were considered; the external disturbance of windings allowing to energize
winding by any electromotive force sources, was set. The grid to break the model into finite elements was
selected, having higher density in the air gap and motor slots Figure 1(a), the calculation of the
electromagnetic torque was set, the time step enabling to obtain correct results for shortest possible terms was
determined.
Parameters obtained based on the model are as follows (values in brackets): stator (I1n = 10.5 А) and
rotor (I2n = 15 А) currents, nameplate motor electromagnetic torque (Tn = 38 N∙m), motor crippling torque
(Tc = 91 N∙m), nameplate sliding (sn = 0.1), angular velocity (ωn = 895 rpm), power coefficient (cosφ = 0.73),
energy conversion efficiency (η = 0.7). All the parameters match to directory and empirical readings for this
motor given in Table 1.
2.4. Modeling the PVC with Rotor Position Sensor
The principle of motor drive system operation [12] required untraditional completion of the pulse-
phase control unit (PPCU) with 6 sync channels, and creation of the specific sector evaluation unit (SEU).
The functional diagram of the PVC system implemented in ANSYS Electromagnetics Suite is given in
Figure 1(b). Here is USET – set voltage, UFB – feedback voltage proportional to circuit current, CR – current
regulator, UCR – current regulator output voltage, PPCU – pulse-phase control unit, UC – set current voltage,
TBR – thyristor bridge rectifier, IM – induction motor, RPS – rotor position sensor, CS – current sensor,
SEU – sector evaluation unit, αFB – rotor angular position.
Figure 1. Segment of 2D motor model with finite element breakdown (a) and functional diagram of PPCU
with rotor angular position sensor (b)
The diagram on Figure 1(b) implements the closed current control circuit. The UFB feedback
waveform is compared to the USET waveform, and depending on the result of comparing δ, the PPCU forms
the thyristor enabling lag waveform and UC current set waveform. If δ reaches the maximum, the lag
waveform equals zero, and enabling pulses are given to thyristors at the zero crossing of the power voltage,
i.e. the whole positive half-wave of power voltage is applied to rotor windings. If δ decreases, the thyristor
enabling lag increases, and the reduced positive half-wave of power voltage is applied to rotor windings.
In the considered PVC system, pulse-phase control problems differ from traditional to some extent,
as according to the diagram operation principles, 6 positive half-waves of linear power voltages are
USET
UFB
–
CR PPCU TBR IM RPS
CS
SEU
Sector No.
UCR UC
αFB
δ
 ISSN: 2088-8694
IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159
1150
alternatively applied to motor windings: UAC, UBC, UBA, UCA, UCB, UAB, being out of phase against each
other. The designed functional diagram of the 6-sync-channel PPCU is given in Figure 2.
Figure 2. PPCU functional diagram
Six power voltages and current regulator (UCR) output waveform are inputted to the PPCU. Output
waveforms of the PPCU are six current-set waveforms: UC1, UC2, UC3, UC4, UC5, UC6, which, together with
SEU output waveforms, form the thyristor enabling pulses. The PPCU functional diagram includes 6
comparators – corresponding to the number of sync channels. The current regulator output UCR passes
through the degree limitation unit DLU and is inputted to six adders. To the second input of each adder, the
saw-tooth waveform is given from reference voltage generators (RVG1 – RVG6), having the phase same to
that of the power voltage. Adder’s output value is given to the comparator, taking a value of “1” in case of
positive input waveform. In fiure 3 φ is phase shift between power voltage and reference voltage, C1 – C12
–
DLU
U
UCR
UC1
0
1
0
1
UАС
– UC2
0
1
0
1
UВС
– UC3
0
1
0
1
UВА
– UC4
0
1
0
1
UСА
– UC5
0
1
0
1
UСВ
–
UC6
0
1
0
1
UАВ
φ = π/6
φ = π/2
φ = 5π/6
φ = 7π/6
φ = 3π/2
φ = 11π/6
UACcom
UВСcom
UВАcom
UСАcom
UСВcom
UАВcom
UST1
UST2
UST3
UST4
UST5
UST6
U1
U2
U3
U4
U5
U6
RVG1
RVG2
RVG3
RVG4
RVG5
RVG6
C1
C2
C3
C4
C5
C6
C7
C8
C9
C10
C11
C12
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are comparators. This way, the thyristor enabling lag waveform is formed, depending on UCR current values.
Figure 3(a) shows time graphs depicting the principle of the PPCU operation, through the example of the
UC1 output waveform formation.
The UAC power voltage is phase-shifted by φ = π/6. The comparator C1 acts as a syncing device, and
the UACcom output waveform takes the value of “1”, if the power voltage is > 0. Through using the adder, the
comparison of UCR and the waveform from the linearly decreasing saw-tooth voltage generator UST1 (phase-
shifted as the power voltage), is carried out. If UCR > UST1, then a “1”- waveform emerges on the C2 output.
UC1 current set waveform is formed on the product unit output (UACcom given to the first input, UC2 output is
given to the second input).
The SEU functional diagram is showed in Figure 3(b). The waveform from the RPS is given to the
SEU input, which corresponds to the rotor turning angle (in geometric degrees). The proportional unit
(K = 3) transforms geometric degrees into electric degrees. The rotor turning angle (α) waveform (in electric
degrees) passes through the Degree Reset Device (DRD) in case of 360-degree rotor turn. The Device
includes the Sampling Unit (SU) transforming the continuous waveform αFB waveform into the staircase
waveform αSU with sampling level 360. The adder compares αFB and αSU, and forms the saw-tooth waveform.
For instance, if αFB waveform continuously increases with time in Figure 4(a), then waveforms αSU and α will
look like it is showed in Figure 4(a) and (b).
(a) (b)
Figure 3. PPCU time graphs (a) and sector evaluation unit (SEU) functional diagram (b)
Figure 4. Degree reset device (DRD) waveforms: output SU waveform αSU (a) and output DRD waveform (b)
Further, waveform α equal to the rotor turning angle (0-360 el. degrees), comes to the comparison
unit (CU), where 6 conditions enable to determine the thyristor pair to set enabling pulses to. For instance, if
the rotor turning angle α lies within 0 ≤ α < 60 electric degrees, then in case of current set waveform UC1,
enabling pulses are given to the first thyristor pair. A current path emerges as follows: power network
UACcom
t
t
UAC
t
UCR
UC1
φ = π/6
t
U1
UST1
C
α, el.
degrees
SU
–
+
0 ≤ α < 60
60 ≤ α <120
120 ≤ α < 180
180 ≤ α < 240
240 ≤ α < 300
300 ≤ α < 360
α, geom.
degrees
VD1
VD2
VD3
VD4
VD5
VD6
α
αFB
αSU
UC1
UC2
UC3
UC4
UC5
UC6
DRD
CU Thyristors
t
α
360
b)
t
a)
360
720
1080
1440
αFB
αSU
α
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IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159
1152
A-phase-stator winding AX-thyristor VD1-two rotor windings-thyristor VD2-stator winding BY-power
network B-phase. The motor obtains the electromagnetic torque. The rotor turns clockwise. Degree α
increases and reaches the value equal to or exceeding 60 electric degrees, power circuit current falls down to
zero, the first thyristor pair is turned off, while enabling pulses are given to the next thyristor pair. Stator
winding flux linkage vector performs a discrete motion by 60 electric degrees, etc.
By way of example, Figures 5-8 show the model-based transition processes of the pulse-vector
motor drive launch with a mounted sensor. Figure 5(a) shows the dependence of the rotor turning angle α
(electric degrees) on time. With such change of α, waveforms from the comparison unit, corresponding to the
sector number; time graphs of thyristor currents will look like as depicted in Figures 5(b), (c).
(a)
(b) (c)
Figure 5. Rotor turning angle (a), comparison unit waveforms corresponding to sector number (b) and
thyristor currents time graphs (c)
At a nominal waveform in the PVC, power circuit current has the pulse nature with the max of 18 A
(Figure 6). The motor obtains the electromagnetic torque as shown in Figure 7, affected by which, the motor
accelerates up to 80 rad/s for 1 second as shown in Figure 8. The diagram has two types of pulse-nature,
caused by thyristor commutator operation, and the torque formation principle.
Figure 6. Transition process of power circuit current at motor start
t, ms
α, el. degrees
0.00 0.20 0.40 0.60 0.80 1.00
Time [s]
0.00
10.00
20.00
AM1.I
[A]
Curve Info
AM1.I
TR
IJPEDS ISSN: 2088-8694 
Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk)
1153
Figure 7. Transition process of motor electromagnetic torque at motor start
Figure 8. Transition process of motor angular velocity at motor start
2.5. Development of the PVC of WRIM with Indirect Rotor Position Determination
The indirect determination system, as well as the system with the rotor position sensor, contains the
wound rotor induction motor (IM), current regulator (CR), pulse-phase control unit (PPCU), thyristor bridge
rectifier (TBR), and current sensor (CS); the indirect rotor position determination unit (IRDPU) exercises the
function of the rotor position sensor and sector evaluation unit as shown in Figure 9.
The IRDPU includes the initial angular position (α0) computer (for reference on the operation
procedure-see [13]), and the current angular position (αC) computer, allowing to timely switch thyristors in
transition and steady modes of the system.
Figure 9. Functional diagram of the PVC with indirect rotor position determination
During motor operation in transition and steady modes, determination of current angular position αC
through comparing current voltages on motor winding (as it was done to determine α0), does not seem
possible. Calculation of αC based on instantaneous voltages is also difficult due to presence of points having
ambiguous values – for instance, zero crossing points. That is why indirect calculation of αC was performed
based on root-mean-square rotor winding voltages, in 3 steps. For convenient operation, stator windings
voltages UAX, UBY, UCZ were used as accessible for direct measurement of electric parameters within indirect
calculation of αC.
The indirect αC computer includes three voltage sensors (VS) measuring stator windings voltages -
VSAX, VSBY, VSCZ, and root-mean-square voltages units – RMSAX, RMSBY, RMSCZ. The functional diagram
of the IRPDU (αC) is given in Figure 10. To the input of the unit, instant voltages on stator windings – uAX,
uBY, uCZ – are given; thyristor control waveforms are the output. The IRPDU contains 6 sector determination
channels, by the number of sectors. Channels alternatively form the thyristor control pulses in case if the
corresponding condition is met when comparing voltages on stator windings.
Let us consider the principle of IRPDU (αC) operation through the example of the first sector
determination channel (Channel 1). The Channel 1 Functional Diagram within Interaction with other
Channels is given in Figure 11. During operation, thyristors VD2 and VD5 are enabled in the first sector, and
the current goes through stator windings AX and CZ, while stator winding BY remains unenergized.
Maximum positive motor electromagnetic torque is reached at UCZ > UAX. It is essential to feed
enabling pulses to thyristors VD2 and VD5 when UCZ > UAX condition is met. Verification of meeting the
condition goes as follows. Root-mean-square voltages UCZ and UAX come to the adder S11 (the subscript
indicates a channel an element belongs to); if the adder output waveform δ1 > 0, then on the output of the
0.00 0.20 0.40 0.60 0.80 1.00
Time [s]
-12.50
37.50
87.50
FEA1.TORQUE
Curve Info
FEA1.TORQUE
TR
0.00 0.20 0.40 0.60 0.80 1.00
Time [s]
0.00
40.00
80.00
VM_ROTB2.OMEGA
[rad_per_sec]
Curve Info
VM_ROTB2.OMEGA
TR
USET
UFB
–
CR PVC TBR IM IRPDU
CS
UCR UC
α
δ
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IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159
1154
voltage comparing unit VCU1, the waveform UVCU1 is formed, bearing the “1”-value; if δ1 < 0, then
UVCU1 = 0.
Figure 10. IRDPU αc Functional Diagram
The waveform UVCU1 is fed to the first waveform-inverting comparator IC11. The waveform UVCU1
is fed to the first waveform-inverting comparator IC11. Then, from the comparator, the waveform comes to
the integrator I1 with the time constant T = 0.001 and single saturation zone. Thus, as long as the integrator
input waveform equals zero, the waveform UI1 = 0 is formed on the integrator output, which is fed to the
second inverting comparator IC21, forming the “1”-value on the output. If at this very moment, there is a
waveform from the previous-channel comparator, which reports on finishing operation and it is time for
enabling the next thyristor pair, thyristors VD2 and VD5 receive enabling pulses. Once UCZ becomes lower
than UAX, δ1 ≤ 0, and UVCU1 equals zero, then the integrator input (after the inverting comparator IC11),
receives the “1”-value, output integrator waveform reaches the “1”-value for t = 0.001 s, IC21 acts, and
enabling pulse feeding to thyristors VD2 and VD5 is halted. On the output of the third inverting comparator
IC31, the waveform permitting enabling second-sector thyristors is formed.
Figure 11. Channel 1 functional diagram within interaction with other channels
The integrator I1 will not leave the saturation zone until it receives the “-1”-value waveform on the
input. The reset waveform will come to the integrator after the rotor comes all 6 sectors and turns 360
degrees. Then, all the processes repeat. This pulse is formed by the integrator reset unit IRU1, which contains
Channel 1 (UCZ>UAX)
Channel 2 (UBY>UCZ)
Channel 3 (UAX>UBY)
Channel 4 (UCZ>UAX)
Channel 5 (UBY>UCZ)
Channel 6 (UAX>UBY)
VD2
VD5
VD4
VD1
VD6
VD3
UC1
UC2
UC3
UC4
UC5
UC6
UAX
UBY
UCZ
RMSAX
RMSBY
RMSCZ
uAX
uBY
uCZ
VSAX
VSBY
VSCZ
IRPDU αc
δ1
VCU1
UVCU1
0
1
–UAX
+UC
Z
IC11 I1
0
1
IC21
0
1
IC31
VD2
VD5
UC1
δ6
VCU 6
UVCU6
0
1
+UA
X
–UBY
IC16 I6
0
1
IC26
0
1
IC36
… …
S11
0
1
IC46
e-Tt
S16
S21
…
Channel 1
Channel 6
…
IRU1
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1155
the pure delay element, product element, inverting comparator IC41, and adder S21. Presence of integrators
with the saturated zone in the IRPDU provides protection from false acts. Other sector determination
channels operate the similar way.
By way of example, Figures 12-15 show the transition processes of the no-load launch of the PVC
with the indirect determination of rotor angular position. Figure 12 depicts the dependence of the rotor
turning angle α (electric radians) from time (t = 800 ms). At such change of α, IRPDU-originated waveforms
corresponding to the sector number, and time graphs of thyristor currents, will look like as showed in
Figures 13, 14.
(a)
(b)
(c)
Figure 12. Rotor turning angle (radians) (a), IRPDU waveforms corresponding to sector number (b) and
thyristor currents time graphs (c)
In case of half-waveform in the PVC, power circuit current has the pulse nature with the maximum
of 10 A as shown in Figure 13. The motor obtains the electromagnetic torque as shown in Figure14, affected
by which, the motor accelerates up to 20 rad/s for 0.8 seconds as shown in Figure 15.
Figure 13. Power circuit current at motor start
Figure 14. Motor electromagnetic torque at motor start
0.00 100.00 200.00 300.00 400.00 500.00 600.00 700.00 800.00
Time [ms]
-2.00
3.00
8.00
12.45
AM1.I
[A]
Curve Info
AM1.I
TR
0.00 100.00 200.00 300.00 400.00 500.00 600.00 700.00 800.00
Time [ms]
-2.50
2.50
7.50
12.50
17.50
FEA1.TORQUE
Curve Info
FEA1.TORQUE
TR
0.00 200.00 400.00 600.00 800.00
0.00
2.00
4.00
6.00
Curve Info
TR
α, rad
t, ms
 ISSN: 2088-8694
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Figure 15. Motor angular velocity at motor start
Figure 16 depicts the fragment of forming thyristor-enabling pulses based on 3-step-averaged
voltages (UAX, UBY, UCZ). Within the time range t1-t2, UAX ≥ UBY, on the output of the Channel 6, the “1”-
value is formed, enabling pulses are fed to thyristors VD3 and VD2. At t2, voltage UAX becomes lower than
UBY, the waveform U6 disappears, Channel 1 starts operating. Within the time range t2-t3, the condition UСZ ≥
UAX is met, and the waveform U1 = 1 is formed on the Channel 1 output, while enabling impulses are fed to
thyristors VD2 and VD5.
Figure 16. Fragment of Forming Enabling Pulses Based on Averaged Voltages
3. RESULTS AND ANALYSIS
3.1. Process Quality Paramters for the PVC of WRIM with Rotor Position Sensor and with Indirect
Rotor Angular Position Determination
Mechanisms that the PVC is positioned to, require ensuring auxiliary low-velocity low-static-torque
modes. That is why it makes sense to analyze process quality parameters obtained on the ANSYS-based math
model, for low angular velocities. In this context, let us consider the following process quality parameters:
the ratio of maximum and root-mean-square power circuit currents of the nameplate stator current Imax/I1N
and IRMS/I1N; the ratio of maximum and average motor electromagnetic torques of the nameplate torque
Tmax/TN and TAV/TN; the ration of velocity fluctuation of the nameplate synchronous velocity ∆ω/ω0N, caused
by the pulse-nature operation mode. Control process quality parameters obtained in ANSYS
Electromagnetics Suite for the PVC of WRIM bouth with rotor position sensor and with indirect rotor
angular position determination, are given in aggregate in Table 2. for absolute and relative values. For
explanation, Figure 17 depicts the determination of quality parameters for the 0.2 ratio between the angular
velocity and the nameplate synchronous velocity ω0N.
Table 2. Process Quality Parameters
Parameter for the PVC of WRIM with RPS for the PVC of WRIM with RPD
TAV/ T N 0 0.1 0.2 0.3 0.4 0.5 0 0.1 0.2 0.3 0.4 0.5
T AV, N.
m 0 3.7 7.4 11.1 14.8 18.5 0.0 3.7 7.4 11.1 14.8 18.5
T max/ T N 0.2 0.6 1.8 2.8 3.2 4.1 0.2 0.3 0.7 1.8 3.0 3.3
T max, N.
m 8.6 23.5 65.7 102.0 118.0 150.0 9.2 9.8 24.9 68.2 110 123
IRMS/I1N 0.2 0.3 0.3 0.5 0.6 0.8 0.2 0.2 0.3 0.3 0.5 0.6
IRMS, A 2.5 2.7 3.6 5.0 6.2 8.0 2.4 2.5 2.7 3.6 5 6.2
Imax/I1N 0.4 0.6 1.3 1.8 2.2 3.3 0.4 0.6 1.3 1.7 2.2 2.5
Imax, A 4.1 6.3 14.0 18.5 22.5 33.9 4.2 6.2 13.8 18.1 23 26
ωav/ω0N 0.9 0.8 0.5 0.3 0.2 0.1 0.9 0.8 0.5 0.3 0.2 0.2
ωav, rad/s 96.4 85.0 50.0 26.8 21.0 9.6 98 88 52 29 25 20
∆ω/ω0N 0.02 0.03 0.04 0.07 0.11 0.11 0.02 0.03 0.04 0.07 0.11 0.12
0.00 100.00 200.00 300.00 400.00 500.00 600.00 700.00 800.00
Time [ms]
0.00
10.00
20.00
VM_ROTB2.OMEGA
[rad_per_sec]
Curve Info
VM_ROTB2.OMEGA
TR
50
t
UAX UBY
UСZ
100
U, V
t1 t2 t3
UAX ≥ UBY
U6 = 1; U1, U2…U5 = 0
Conductive thyristors VD3 and VD2
UAX < UBY, UCZ ≥ UBY
U1 = 1; U2, U3…U6 = 0
Conductive thyristors VD2 and VD5
IJPEDS ISSN: 2088-8694 
Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk)
1157
At a glance, current and torque ratios Imax/I1N < Tmax/TN and IRMS/I1N < TAV/TN, may prompt
questions, as in most cases the current grows faster than the torque, but in the considered diagram, stator and
rotor windings form the series circuit – here emerges the effect typical for series-excitation motors, when the
differential torque runs ahead the differential current.
3.2. Comparing indirect determination and rotor position sensor systems
Examination of the PVC of WRIM in ANSYS Electromagnetics Suite figured their efficiency when
used as control systems of massive mechanism motor drives with moderate standards for accuracy of velocity
control, requiring velocity decrease during long-term load reduction or removal. Based on quality parameters
considered in Paragraph 3.1, comparison of the model of motor drive with indirect determination rotor
angular position determination and the pulse-vector control with rotor position sensor, revealed the indirect-
determination system shows fair results as well. The rotor angular position computer implemented in ANSYS
Electromagnetics Suite, possesses the relatively plain structure and requires 3 voltage sensors on stator
windings to measure the current rotor position, and the programmed controller possessing minor computing
powers as compared with famous methods for indirect determination of the state vector [2]. With that,
position computer provides for correct rotor angular position determination accurate within a sector, meeting
the necessary and sufficient criterion of successful PVC operation. In cases when rotor position
determination accuracy must be enhanced, further voltage analysis of the stator unenergized winding can be
carried out.
Figure 17. Fragment of ANSYS calculation curves of motor drive velocity control mode: a) velocity ω;
b) electromagnetic torque T; c) circuit current ic
4. CONCLUSION
The models of the pulse-vector control of wound rotor induction motor drive with the rotor position
sensor and indirect position determination were developed by means of ANSYS Electromagnetics Suite.
Implementation of the untraditional pulse-phase control unit syncing thyristor-enabling pulses with the
network in the pulse-vector control system, ensured meeting required motor torque values in the half-wave
detection circuit.
Examinations carried out in ANSYS Electromagnetics Suite figures that the method of indirect rotor
angular position is appropriate. The pulse-vector control with indirect rotor angular position determination is
operable, having quality parameters being highly competitive with those of the sensor-mounted system.
a)
c)
ω, rad/s
T, N.
m
ic, A
t, s
t, с
t, s
Imax = 21,5 A
T max = 122 N.
m
ω max = 27 rad/s ω max = 14 rad/s
ω av = 20 rad/s
T av = 18.5 N.
m
I RMS = 6.2 A
b)
t, s
 ISSN: 2088-8694
IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159
1158
Properties of the PVC with indirect determination and process quality parameters enable to infer that the
problems stated in the introduction were successfully solved.
Application of the developed PVC with indirect determination will allow carrying out
modernization of massive mechanisms with moderate standards for accuracy of velocity control, velocity
decrease during load reduction or removal, with as low economic costs as possible – both during
modernization itself, and during further operation.
ACKNOWLEDGEMENTS
The work was supported by Act 211 Government of the Russian Federation, contract
№ 02.A03.21.0011
REFERENCES
[1] I. M. Alsofyani and N. R. N. Idris, “A Review on Sensorless Techniques for Sustainable Reliablity and Efficient
Variable Frequency Drives of Induction Motors,” Renewable and Sustainable Energy Reviews, vol. 24, pp. 111-
121, 2013.
[2] J. Holtz, “Sensorless Control of Induction Motor Drives,” Proceedings of the IEEE, vol/issue: 90(8), pp. 1359–
1394, 2002.
[3] J. C. Gamazo-Real, et al., “Position and Speed Control of Brushless DC Motors Using Sensorless Techniques and
Application Trends,” Sensors, vol/issue: 10(7), pp. 6901-6947, 2010.
[4] C. M. Verrelli, et al., “Nonlinear Tracking Control for Sensorless Permanent Magnet Synchronous Motors with
Uncertainties,” Control Engineering Practice, vol. 60, pp. 157-170, 2017.
[5] Z. Qiao, et al., “New Sliding-mode Observer for Position Sensorless Control of Permanent-magnet Synchronous
Motor,” IEEE Transactions on Industrial Electronics, vol/issue: 60(2), pp. 710-719, 2013.
[6] D. A. Dominic and T. R. Chelliah, “Analysis of Field-oriented Controlled Induction Motor Drives under Sensor
Faults and an Overview of Sensorless Schemes,” ISA Transactions, vol/issue: 53(5), pp. 1680-1694, 2015.
[7] M. H. Holakooie, et al., “Full-order Luenberger Observer Based on Fuzzy-logic Control for Sensorless Field-
oriented Control of a Single-sided Linear Induction Motor,” ISA Transactions, vol. 60, pp. 96-108, 2016.
[8] M. Beschi, et al., “Sensorless Model-based Object-detection Applied on an Underactuated Adaptive Hand Enabling
an Impedance Behavior,” Robotics and Computer-Integrated Manufacturing, vol. 46, pp. 38-47, 2017.
[9] S. Derammelaere, et. al., “Sensorless load angle control for two-phase hybrid stepper motors,” Mechatronics, vol.
43, pp. 6-17, 2017.
[10] M. Montanari, et. al., “Speed Sensorless Control of Induction Motors Based on a Reduced-Order Adaptive
Observer,” IEEE Transactions on Control Systems Technology, vol/issue: 15(6), pp. 1049-1064, 2007.
[11] P. Shinde, et al., “Speed Control of Induction Motor by Using Variable Frequency Drive,” Rupali Burungale et al
Int. Journal of Engineering Research and Applications, vol/issue: 4(4), pp. 35-37, 2014.
[12] Y. S. Usynin, et al., “Asynchronous Electric Drive with Pulse-vector Control,” Russian Electrical Engineering,
vol/issue: 82(3), pp. 134-137, 2011.
[13] Y. S. Usynin, et al., “Pulse-vector Control with Indirect Determination of Rotor Angular Position,” Russian
electrical engineering, vol/issue: 84(10), pp. 566-571, 2013.
[14] M. A. Iqbal and V. Agarwal, “Investigation & Analysis of Three Phase Induction Motor Using Finite Element
Method for Power Quality Improvement,” International Journal of Electronic and Electrical Engineering,
vol/issue: 7(9), pp. 901-908, 2014.
[15] Y. S. Usynin, et al., “Synthesis of Control System by Electrical Drive with Synchronous Reluctance Independent
Excitation Machine,” Bulletin of South Ural State University. Series: Power Engineering, vol/issue: 18(37), pp.
38-41, 2012.
[16] Y. V. Alekseev, et al., “Crane Electrical Equipment: Reference Book,” Moscow, Energiya Publishing House, pp.
240, 1979.
[17] I. P. Kopylov, “Handbook of electrical machines: 2 tons,” Moscow, Energoatomizdat Publishing House, pp. 688,
1989.
BIOGRAPHIES OF AUTHORS
Tatiana Andreevna Funk received the PhD degree from South Ural State University, Chelyabinsk,
Russian Federation, in 2012. She is currently an Associate Professor in the Department of Electric
Drive, South Ural State University, Chelyabinsk, Russian Federation. Her research interests
include motor drive control systems with motor-mounted sensor and indirect control systems.
IJPEDS ISSN: 2088-8694 
Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk)
1159
Yuriy Semenovich Usynin received the PhD degree from Moscow Power Engineering Institute,
Moscow, Russian Federation in 1994. He is currently a Professor in the Department of Electric
Drive, South Ural State University, Chelyabinsk, Russian Federation. His research interests
include motor drive control systems and the electric drive with the field regulated reluctance
machine.
Evreniy Viktorovich Belousov received the PhD degree from South Ural State University,
Chelyabinsk, Russian Federation, in 2014. He is currently an Associate Professor in the
Department of Electric Drive, South Ural State University, Chelyabinsk, Russian Federation. His
research interests include the electric drive with the field regulated reluctance machine and electric
transport.

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Indirect Pulse-vector Control of Wound Rotor Induction Motor Drive in ANSYS Electromagnetics Suite

  • 1. International Journal of Power Electronics and Drive System (IJPEDS) Vol. 8, No. 3, September 2017, pp. 1147~1159 ISSN: 2088-8694, DOI: 10.11591/ijpeds.v8i3.pp1147-1159  1147 Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS Indirect Pulse-vector Control of Wound Rotor Induction Motor Drive in ANSYS Electromagnetics Suite Tatiana Andreevna Funk, Yuriy Semenovich Usynin, Evgeny Viktorovich Belousov Department of Electric Drive, South Ural State University, Chelyabinsk, Russian Federation Article Info ABSTRACT Article history: Received Jun 26, 2017 Revised Aug 5, 2017 Accepted Aug 20, 2017 This paper deals with the problem of estimation of rotor angular position for the indirect pulse-vector control of wound rotor induction motor drive. The paper considers issues of thematic justification and expanding of the field of using sensorless motor drives. With a view to improve energy consumption readings during design and modernization of motor drives of massive mechanisms with moderate standards for accuracy of velocity control, requiring long-term velocity decrease during load reduction (according to technological process conditions), using the system of the pulse-vector control of wound rotor induction motor is suggested. The paper provides the solution for the problem of developing math models of this motor drive system both for the motor-mounted sensor, and for indirect angular position sensing. The models were developed in ANSYS Electromagnetics Suite using the finite element method for studying electromagnetic processes. Based on the models, the investigation of transition and steady states of a motor drive was carried out, process quality parameters were obtained, namely: max and root-mean-square currents, torques; velocity control errors caused by pulse operation mode. From that simulation, the result illustrates the effectiveness of the proposed approach. Keyword: Finite element method Indirect control system No motor-mounted sensor motor drive Wound rotor induction motor pulse-vector control Copyright © 2017 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Tatiana Andreevna Funk, Department of Electric Drive, South Ural State University, 76 Lenin prospect, Chelyabinsk, Russian Federation, 454080. Email: kozinata@susu.ru 1. INTRODUCTION In the recent years, indirect determination of variable coordinates of a no motor-mounted sensor motor drive, or so-called sensorless methods are coming into wider use for various mechanisms and motor drive control systems [1]-[9]. Sensorless systems enable to improve regulation characteristics of control objects with no mounting of the direct measurement device onto the motor shaft required [1],[2]. Moreover, in some cases, mounting a sensor onto the shaft can be either economically or technically unfeasible [3], or crucially impossible due to technological process conditions – for instance, because of vibration, radiation, emissions, extreme temperatures, powered motions, and isolated location of a unit from the control system. In the general context, application of indirect methods for velocity and position determination is most relevant within the design and modernization of massive mechanism motor drives with moderate standards for accuracy of velocity control: lift-and-carry mechanisms, industrial fans, band conveyors, hydraulic pumps, compressors, air blowers, smoke and air exhausters, etc. [10]. Among them, mechanisms requiring velocity decrease during long-term load reduction or removal. For instance, fans built in industrial facilities, air exhausters in oxygen converter plants. This group may also include motor drives of band conveyors (provided that they are idle at night shifts), but in order to prevent freeze-up of bearing greasing, it is reasonable to switch them to lower rotation in no-load conditions.
  • 2.  ISSN: 2088-8694 IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159 1148 In the quality of power motors in above mechanisms, induction motors with short-circuit or wound rotors are used. The motor velocity either remains non-adjustable, or is adjusted inserting ballast resistors to stator’s or rotor’s circuits. No adjustment or using relay-contactor circuits is accompanied by higher energy consumption. Rise in prices of electric energy and other power resources results in need for modernization of considered motor drives [6],[11]. Using two-section frequency changer in such mechanisms is not always feasible due to high cost, complicated operation, and heavy requirements for personnel qualification. There was a range of studies dedicated to the pulse-vector control (hereinafter – PVC) of wound rotor induction motor drive (hereinafter – WRIM) [12],[13]. The purpose of those systems is to create the current in the rotor with the frequency same to stators, i.e. to prevent sliding. They fairly suit the above mechanisms because of moderate cost and having no excessive adjustment capabilities, as well as show low energy consumption under low-velocity modes. Control in such system is carried out depending on the rotor angular position – thus, it is essential either to mount the position sensor onto the shaft, or to use the method for indirect rotor position determination. Previous studies and papers on the PVC of motor drives suggested the PVC of WRIM with the rotor position sensor [12], described the developed principle and algorithm for indirect determination of the initial angular position, established differential equations and functional relationships between state variables and rotor turning angle, giving the brief explanation of the system modeling through using the finite element method [13]. The present paper sets the problem of developing an exhaustive math model and studying the PVC of WRIM, aimed at further use of the system to improve the technological process quality and enhance resource and energy consumption readings of massive mechanisms. 2. RESEARCH METHOD 2.1. The Method of the PVC of WRIM The considered PVC [12] contains the three-phase WRIM and three-phase thyristor bridge rectifier. Shall we denote stator windings by AX, BY, CZ, and phases of three-phase powering voltage by A, B, C. The electromagnetic moment will be formed by sequential series connection of two stator phases through corresponding thyristors to two rotor windings. The magnetomotive force (hereinafter-MMF) vector of stator windings performs discrete motion with a 60-degree step. Switching is made depending on the rotor position, thereby providing the orientation of MMF vectors of stator and rotor windings to correspond to the motor torque. Either stator winding is left off the line during operation of two other ones. The tertiary rotor winding is being off the line during the whole operation cycle. 2.2. Specifics of Modeling the PVC of WRIM and Indirect Position Determination (IPD) The considered PVC system constitutes the multi-phase, pulse, non-linear, unsymmetrical system, thus, examination of its operation in steady and transition modes by using the analytic methods for analyzing electromagnetic processes – for instance, applying differential equations of the multi-phase circuit is inclined to excessive complicating and extension of calculation conditions included as a compound of the math model. It may be reasonable to take advantage of using the progressive numerical methods for analyzing the electromagnetic system, and calculate the motor drive through using the finite element method [14]. Application of this method enables to take specifics of the motor drive system into account and significantly simplify processing and analysis of the modeling results. ANSYS Electromagnetics suite was used as it enables to: create a WRIM state space model, calculate the motor drive through using the finite element method; carry out analysis of electromagnetic processes in close relation to the powered motions and control system; analyze changes of circuit currents, electromagnetic torque, and voltages on motor windings, depending on the relative position of the stator and the rotor. In solving the problem of mathematical analysis, the experience of modeling motor drive systems using the finite element method, described in [15], was taken into account. Modeling of the PVC system with indirect determination of the rotor angular position in ANSYS Electromagnetics Suite was divided into three stages: сreating the WRIM model as a control system unit, and analysis of its operation in steady and transition modes through using the finite element method; engineering the model of the PVC system using the rotor position sensor, and analysis of motor drive operation as a control system prototype, with indirect determination of the rotor angular position; developing the model of the PVC of the induction motor with indirect determination of the rotor angular position; analysis of this motor drive system in steady and transition modes. 2.3. Architecting and Analyzing the WRIM Model As a prototype for modeling, the crane-metallurgy wound rotor motor MTF111-6 was chosen. Nameplate data of the motor are given in Table 1.
  • 3. IJPEDS ISSN: 2088-8694  Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk) 1149 Table 1. MTF 111-6 Motor Nameplate Data Parameter Unit Value Nominal Stator Voltage V 380 Nameplate Angular Velocity rpm 895 Nameplate Power kW 3.5 Cos ϕ - 0.73 Energy Conversion Efficiency % 70 Nameplate Stator Current A 10.4 Nameplate Rotor Current A 15 Nameplate Electromotive Force on Rotor Rings V 176 Crippling Torque N∙m 85 Pole Pairs pcs 3 Created based on key geometric dimensions, parameters of gaps and motor windings [16], the 2D motor model is given in Figure 1(a), considering the number of pole pairs. Stator and rotor cores are made of electric steel No. 1212, induction-permeability of which was set as the non-linear property based on 24 points [17]. Motor windings are made of copper. During architecting the model, the rotation area was created and included the rotor and motor shaft, ground potential boundaries were determined; three-phase stator and rotor windings were distributed over slots; the number of coil windings were considered; the external disturbance of windings allowing to energize winding by any electromotive force sources, was set. The grid to break the model into finite elements was selected, having higher density in the air gap and motor slots Figure 1(a), the calculation of the electromagnetic torque was set, the time step enabling to obtain correct results for shortest possible terms was determined. Parameters obtained based on the model are as follows (values in brackets): stator (I1n = 10.5 А) and rotor (I2n = 15 А) currents, nameplate motor electromagnetic torque (Tn = 38 N∙m), motor crippling torque (Tc = 91 N∙m), nameplate sliding (sn = 0.1), angular velocity (ωn = 895 rpm), power coefficient (cosφ = 0.73), energy conversion efficiency (η = 0.7). All the parameters match to directory and empirical readings for this motor given in Table 1. 2.4. Modeling the PVC with Rotor Position Sensor The principle of motor drive system operation [12] required untraditional completion of the pulse- phase control unit (PPCU) with 6 sync channels, and creation of the specific sector evaluation unit (SEU). The functional diagram of the PVC system implemented in ANSYS Electromagnetics Suite is given in Figure 1(b). Here is USET – set voltage, UFB – feedback voltage proportional to circuit current, CR – current regulator, UCR – current regulator output voltage, PPCU – pulse-phase control unit, UC – set current voltage, TBR – thyristor bridge rectifier, IM – induction motor, RPS – rotor position sensor, CS – current sensor, SEU – sector evaluation unit, αFB – rotor angular position. Figure 1. Segment of 2D motor model with finite element breakdown (a) and functional diagram of PPCU with rotor angular position sensor (b) The diagram on Figure 1(b) implements the closed current control circuit. The UFB feedback waveform is compared to the USET waveform, and depending on the result of comparing δ, the PPCU forms the thyristor enabling lag waveform and UC current set waveform. If δ reaches the maximum, the lag waveform equals zero, and enabling pulses are given to thyristors at the zero crossing of the power voltage, i.e. the whole positive half-wave of power voltage is applied to rotor windings. If δ decreases, the thyristor enabling lag increases, and the reduced positive half-wave of power voltage is applied to rotor windings. In the considered PVC system, pulse-phase control problems differ from traditional to some extent, as according to the diagram operation principles, 6 positive half-waves of linear power voltages are USET UFB – CR PPCU TBR IM RPS CS SEU Sector No. UCR UC αFB δ
  • 4.  ISSN: 2088-8694 IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159 1150 alternatively applied to motor windings: UAC, UBC, UBA, UCA, UCB, UAB, being out of phase against each other. The designed functional diagram of the 6-sync-channel PPCU is given in Figure 2. Figure 2. PPCU functional diagram Six power voltages and current regulator (UCR) output waveform are inputted to the PPCU. Output waveforms of the PPCU are six current-set waveforms: UC1, UC2, UC3, UC4, UC5, UC6, which, together with SEU output waveforms, form the thyristor enabling pulses. The PPCU functional diagram includes 6 comparators – corresponding to the number of sync channels. The current regulator output UCR passes through the degree limitation unit DLU and is inputted to six adders. To the second input of each adder, the saw-tooth waveform is given from reference voltage generators (RVG1 – RVG6), having the phase same to that of the power voltage. Adder’s output value is given to the comparator, taking a value of “1” in case of positive input waveform. In fiure 3 φ is phase shift between power voltage and reference voltage, C1 – C12 – DLU U UCR UC1 0 1 0 1 UАС – UC2 0 1 0 1 UВС – UC3 0 1 0 1 UВА – UC4 0 1 0 1 UСА – UC5 0 1 0 1 UСВ – UC6 0 1 0 1 UАВ φ = π/6 φ = π/2 φ = 5π/6 φ = 7π/6 φ = 3π/2 φ = 11π/6 UACcom UВСcom UВАcom UСАcom UСВcom UАВcom UST1 UST2 UST3 UST4 UST5 UST6 U1 U2 U3 U4 U5 U6 RVG1 RVG2 RVG3 RVG4 RVG5 RVG6 C1 C2 C3 C4 C5 C6 C7 C8 C9 C10 C11 C12
  • 5. IJPEDS ISSN: 2088-8694  Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk) 1151 are comparators. This way, the thyristor enabling lag waveform is formed, depending on UCR current values. Figure 3(a) shows time graphs depicting the principle of the PPCU operation, through the example of the UC1 output waveform formation. The UAC power voltage is phase-shifted by φ = π/6. The comparator C1 acts as a syncing device, and the UACcom output waveform takes the value of “1”, if the power voltage is > 0. Through using the adder, the comparison of UCR and the waveform from the linearly decreasing saw-tooth voltage generator UST1 (phase- shifted as the power voltage), is carried out. If UCR > UST1, then a “1”- waveform emerges on the C2 output. UC1 current set waveform is formed on the product unit output (UACcom given to the first input, UC2 output is given to the second input). The SEU functional diagram is showed in Figure 3(b). The waveform from the RPS is given to the SEU input, which corresponds to the rotor turning angle (in geometric degrees). The proportional unit (K = 3) transforms geometric degrees into electric degrees. The rotor turning angle (α) waveform (in electric degrees) passes through the Degree Reset Device (DRD) in case of 360-degree rotor turn. The Device includes the Sampling Unit (SU) transforming the continuous waveform αFB waveform into the staircase waveform αSU with sampling level 360. The adder compares αFB and αSU, and forms the saw-tooth waveform. For instance, if αFB waveform continuously increases with time in Figure 4(a), then waveforms αSU and α will look like it is showed in Figure 4(a) and (b). (a) (b) Figure 3. PPCU time graphs (a) and sector evaluation unit (SEU) functional diagram (b) Figure 4. Degree reset device (DRD) waveforms: output SU waveform αSU (a) and output DRD waveform (b) Further, waveform α equal to the rotor turning angle (0-360 el. degrees), comes to the comparison unit (CU), where 6 conditions enable to determine the thyristor pair to set enabling pulses to. For instance, if the rotor turning angle α lies within 0 ≤ α < 60 electric degrees, then in case of current set waveform UC1, enabling pulses are given to the first thyristor pair. A current path emerges as follows: power network UACcom t t UAC t UCR UC1 φ = π/6 t U1 UST1 C α, el. degrees SU – + 0 ≤ α < 60 60 ≤ α <120 120 ≤ α < 180 180 ≤ α < 240 240 ≤ α < 300 300 ≤ α < 360 α, geom. degrees VD1 VD2 VD3 VD4 VD5 VD6 α αFB αSU UC1 UC2 UC3 UC4 UC5 UC6 DRD CU Thyristors t α 360 b) t a) 360 720 1080 1440 αFB αSU α
  • 6.  ISSN: 2088-8694 IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159 1152 A-phase-stator winding AX-thyristor VD1-two rotor windings-thyristor VD2-stator winding BY-power network B-phase. The motor obtains the electromagnetic torque. The rotor turns clockwise. Degree α increases and reaches the value equal to or exceeding 60 electric degrees, power circuit current falls down to zero, the first thyristor pair is turned off, while enabling pulses are given to the next thyristor pair. Stator winding flux linkage vector performs a discrete motion by 60 electric degrees, etc. By way of example, Figures 5-8 show the model-based transition processes of the pulse-vector motor drive launch with a mounted sensor. Figure 5(a) shows the dependence of the rotor turning angle α (electric degrees) on time. With such change of α, waveforms from the comparison unit, corresponding to the sector number; time graphs of thyristor currents will look like as depicted in Figures 5(b), (c). (a) (b) (c) Figure 5. Rotor turning angle (a), comparison unit waveforms corresponding to sector number (b) and thyristor currents time graphs (c) At a nominal waveform in the PVC, power circuit current has the pulse nature with the max of 18 A (Figure 6). The motor obtains the electromagnetic torque as shown in Figure 7, affected by which, the motor accelerates up to 80 rad/s for 1 second as shown in Figure 8. The diagram has two types of pulse-nature, caused by thyristor commutator operation, and the torque formation principle. Figure 6. Transition process of power circuit current at motor start t, ms α, el. degrees 0.00 0.20 0.40 0.60 0.80 1.00 Time [s] 0.00 10.00 20.00 AM1.I [A] Curve Info AM1.I TR
  • 7. IJPEDS ISSN: 2088-8694  Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk) 1153 Figure 7. Transition process of motor electromagnetic torque at motor start Figure 8. Transition process of motor angular velocity at motor start 2.5. Development of the PVC of WRIM with Indirect Rotor Position Determination The indirect determination system, as well as the system with the rotor position sensor, contains the wound rotor induction motor (IM), current regulator (CR), pulse-phase control unit (PPCU), thyristor bridge rectifier (TBR), and current sensor (CS); the indirect rotor position determination unit (IRDPU) exercises the function of the rotor position sensor and sector evaluation unit as shown in Figure 9. The IRDPU includes the initial angular position (α0) computer (for reference on the operation procedure-see [13]), and the current angular position (αC) computer, allowing to timely switch thyristors in transition and steady modes of the system. Figure 9. Functional diagram of the PVC with indirect rotor position determination During motor operation in transition and steady modes, determination of current angular position αC through comparing current voltages on motor winding (as it was done to determine α0), does not seem possible. Calculation of αC based on instantaneous voltages is also difficult due to presence of points having ambiguous values – for instance, zero crossing points. That is why indirect calculation of αC was performed based on root-mean-square rotor winding voltages, in 3 steps. For convenient operation, stator windings voltages UAX, UBY, UCZ were used as accessible for direct measurement of electric parameters within indirect calculation of αC. The indirect αC computer includes three voltage sensors (VS) measuring stator windings voltages - VSAX, VSBY, VSCZ, and root-mean-square voltages units – RMSAX, RMSBY, RMSCZ. The functional diagram of the IRPDU (αC) is given in Figure 10. To the input of the unit, instant voltages on stator windings – uAX, uBY, uCZ – are given; thyristor control waveforms are the output. The IRPDU contains 6 sector determination channels, by the number of sectors. Channels alternatively form the thyristor control pulses in case if the corresponding condition is met when comparing voltages on stator windings. Let us consider the principle of IRPDU (αC) operation through the example of the first sector determination channel (Channel 1). The Channel 1 Functional Diagram within Interaction with other Channels is given in Figure 11. During operation, thyristors VD2 and VD5 are enabled in the first sector, and the current goes through stator windings AX and CZ, while stator winding BY remains unenergized. Maximum positive motor electromagnetic torque is reached at UCZ > UAX. It is essential to feed enabling pulses to thyristors VD2 and VD5 when UCZ > UAX condition is met. Verification of meeting the condition goes as follows. Root-mean-square voltages UCZ and UAX come to the adder S11 (the subscript indicates a channel an element belongs to); if the adder output waveform δ1 > 0, then on the output of the 0.00 0.20 0.40 0.60 0.80 1.00 Time [s] -12.50 37.50 87.50 FEA1.TORQUE Curve Info FEA1.TORQUE TR 0.00 0.20 0.40 0.60 0.80 1.00 Time [s] 0.00 40.00 80.00 VM_ROTB2.OMEGA [rad_per_sec] Curve Info VM_ROTB2.OMEGA TR USET UFB – CR PVC TBR IM IRPDU CS UCR UC α δ
  • 8.  ISSN: 2088-8694 IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159 1154 voltage comparing unit VCU1, the waveform UVCU1 is formed, bearing the “1”-value; if δ1 < 0, then UVCU1 = 0. Figure 10. IRDPU αc Functional Diagram The waveform UVCU1 is fed to the first waveform-inverting comparator IC11. The waveform UVCU1 is fed to the first waveform-inverting comparator IC11. Then, from the comparator, the waveform comes to the integrator I1 with the time constant T = 0.001 and single saturation zone. Thus, as long as the integrator input waveform equals zero, the waveform UI1 = 0 is formed on the integrator output, which is fed to the second inverting comparator IC21, forming the “1”-value on the output. If at this very moment, there is a waveform from the previous-channel comparator, which reports on finishing operation and it is time for enabling the next thyristor pair, thyristors VD2 and VD5 receive enabling pulses. Once UCZ becomes lower than UAX, δ1 ≤ 0, and UVCU1 equals zero, then the integrator input (after the inverting comparator IC11), receives the “1”-value, output integrator waveform reaches the “1”-value for t = 0.001 s, IC21 acts, and enabling pulse feeding to thyristors VD2 and VD5 is halted. On the output of the third inverting comparator IC31, the waveform permitting enabling second-sector thyristors is formed. Figure 11. Channel 1 functional diagram within interaction with other channels The integrator I1 will not leave the saturation zone until it receives the “-1”-value waveform on the input. The reset waveform will come to the integrator after the rotor comes all 6 sectors and turns 360 degrees. Then, all the processes repeat. This pulse is formed by the integrator reset unit IRU1, which contains Channel 1 (UCZ>UAX) Channel 2 (UBY>UCZ) Channel 3 (UAX>UBY) Channel 4 (UCZ>UAX) Channel 5 (UBY>UCZ) Channel 6 (UAX>UBY) VD2 VD5 VD4 VD1 VD6 VD3 UC1 UC2 UC3 UC4 UC5 UC6 UAX UBY UCZ RMSAX RMSBY RMSCZ uAX uBY uCZ VSAX VSBY VSCZ IRPDU αc δ1 VCU1 UVCU1 0 1 –UAX +UC Z IC11 I1 0 1 IC21 0 1 IC31 VD2 VD5 UC1 δ6 VCU 6 UVCU6 0 1 +UA X –UBY IC16 I6 0 1 IC26 0 1 IC36 … … S11 0 1 IC46 e-Tt S16 S21 … Channel 1 Channel 6 … IRU1
  • 9. IJPEDS ISSN: 2088-8694  Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk) 1155 the pure delay element, product element, inverting comparator IC41, and adder S21. Presence of integrators with the saturated zone in the IRPDU provides protection from false acts. Other sector determination channels operate the similar way. By way of example, Figures 12-15 show the transition processes of the no-load launch of the PVC with the indirect determination of rotor angular position. Figure 12 depicts the dependence of the rotor turning angle α (electric radians) from time (t = 800 ms). At such change of α, IRPDU-originated waveforms corresponding to the sector number, and time graphs of thyristor currents, will look like as showed in Figures 13, 14. (a) (b) (c) Figure 12. Rotor turning angle (radians) (a), IRPDU waveforms corresponding to sector number (b) and thyristor currents time graphs (c) In case of half-waveform in the PVC, power circuit current has the pulse nature with the maximum of 10 A as shown in Figure 13. The motor obtains the electromagnetic torque as shown in Figure14, affected by which, the motor accelerates up to 20 rad/s for 0.8 seconds as shown in Figure 15. Figure 13. Power circuit current at motor start Figure 14. Motor electromagnetic torque at motor start 0.00 100.00 200.00 300.00 400.00 500.00 600.00 700.00 800.00 Time [ms] -2.00 3.00 8.00 12.45 AM1.I [A] Curve Info AM1.I TR 0.00 100.00 200.00 300.00 400.00 500.00 600.00 700.00 800.00 Time [ms] -2.50 2.50 7.50 12.50 17.50 FEA1.TORQUE Curve Info FEA1.TORQUE TR 0.00 200.00 400.00 600.00 800.00 0.00 2.00 4.00 6.00 Curve Info TR α, rad t, ms
  • 10.  ISSN: 2088-8694 IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159 1156 Figure 15. Motor angular velocity at motor start Figure 16 depicts the fragment of forming thyristor-enabling pulses based on 3-step-averaged voltages (UAX, UBY, UCZ). Within the time range t1-t2, UAX ≥ UBY, on the output of the Channel 6, the “1”- value is formed, enabling pulses are fed to thyristors VD3 and VD2. At t2, voltage UAX becomes lower than UBY, the waveform U6 disappears, Channel 1 starts operating. Within the time range t2-t3, the condition UСZ ≥ UAX is met, and the waveform U1 = 1 is formed on the Channel 1 output, while enabling impulses are fed to thyristors VD2 and VD5. Figure 16. Fragment of Forming Enabling Pulses Based on Averaged Voltages 3. RESULTS AND ANALYSIS 3.1. Process Quality Paramters for the PVC of WRIM with Rotor Position Sensor and with Indirect Rotor Angular Position Determination Mechanisms that the PVC is positioned to, require ensuring auxiliary low-velocity low-static-torque modes. That is why it makes sense to analyze process quality parameters obtained on the ANSYS-based math model, for low angular velocities. In this context, let us consider the following process quality parameters: the ratio of maximum and root-mean-square power circuit currents of the nameplate stator current Imax/I1N and IRMS/I1N; the ratio of maximum and average motor electromagnetic torques of the nameplate torque Tmax/TN and TAV/TN; the ration of velocity fluctuation of the nameplate synchronous velocity ∆ω/ω0N, caused by the pulse-nature operation mode. Control process quality parameters obtained in ANSYS Electromagnetics Suite for the PVC of WRIM bouth with rotor position sensor and with indirect rotor angular position determination, are given in aggregate in Table 2. for absolute and relative values. For explanation, Figure 17 depicts the determination of quality parameters for the 0.2 ratio between the angular velocity and the nameplate synchronous velocity ω0N. Table 2. Process Quality Parameters Parameter for the PVC of WRIM with RPS for the PVC of WRIM with RPD TAV/ T N 0 0.1 0.2 0.3 0.4 0.5 0 0.1 0.2 0.3 0.4 0.5 T AV, N. m 0 3.7 7.4 11.1 14.8 18.5 0.0 3.7 7.4 11.1 14.8 18.5 T max/ T N 0.2 0.6 1.8 2.8 3.2 4.1 0.2 0.3 0.7 1.8 3.0 3.3 T max, N. m 8.6 23.5 65.7 102.0 118.0 150.0 9.2 9.8 24.9 68.2 110 123 IRMS/I1N 0.2 0.3 0.3 0.5 0.6 0.8 0.2 0.2 0.3 0.3 0.5 0.6 IRMS, A 2.5 2.7 3.6 5.0 6.2 8.0 2.4 2.5 2.7 3.6 5 6.2 Imax/I1N 0.4 0.6 1.3 1.8 2.2 3.3 0.4 0.6 1.3 1.7 2.2 2.5 Imax, A 4.1 6.3 14.0 18.5 22.5 33.9 4.2 6.2 13.8 18.1 23 26 ωav/ω0N 0.9 0.8 0.5 0.3 0.2 0.1 0.9 0.8 0.5 0.3 0.2 0.2 ωav, rad/s 96.4 85.0 50.0 26.8 21.0 9.6 98 88 52 29 25 20 ∆ω/ω0N 0.02 0.03 0.04 0.07 0.11 0.11 0.02 0.03 0.04 0.07 0.11 0.12 0.00 100.00 200.00 300.00 400.00 500.00 600.00 700.00 800.00 Time [ms] 0.00 10.00 20.00 VM_ROTB2.OMEGA [rad_per_sec] Curve Info VM_ROTB2.OMEGA TR 50 t UAX UBY UСZ 100 U, V t1 t2 t3 UAX ≥ UBY U6 = 1; U1, U2…U5 = 0 Conductive thyristors VD3 and VD2 UAX < UBY, UCZ ≥ UBY U1 = 1; U2, U3…U6 = 0 Conductive thyristors VD2 and VD5
  • 11. IJPEDS ISSN: 2088-8694  Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk) 1157 At a glance, current and torque ratios Imax/I1N < Tmax/TN and IRMS/I1N < TAV/TN, may prompt questions, as in most cases the current grows faster than the torque, but in the considered diagram, stator and rotor windings form the series circuit – here emerges the effect typical for series-excitation motors, when the differential torque runs ahead the differential current. 3.2. Comparing indirect determination and rotor position sensor systems Examination of the PVC of WRIM in ANSYS Electromagnetics Suite figured their efficiency when used as control systems of massive mechanism motor drives with moderate standards for accuracy of velocity control, requiring velocity decrease during long-term load reduction or removal. Based on quality parameters considered in Paragraph 3.1, comparison of the model of motor drive with indirect determination rotor angular position determination and the pulse-vector control with rotor position sensor, revealed the indirect- determination system shows fair results as well. The rotor angular position computer implemented in ANSYS Electromagnetics Suite, possesses the relatively plain structure and requires 3 voltage sensors on stator windings to measure the current rotor position, and the programmed controller possessing minor computing powers as compared with famous methods for indirect determination of the state vector [2]. With that, position computer provides for correct rotor angular position determination accurate within a sector, meeting the necessary and sufficient criterion of successful PVC operation. In cases when rotor position determination accuracy must be enhanced, further voltage analysis of the stator unenergized winding can be carried out. Figure 17. Fragment of ANSYS calculation curves of motor drive velocity control mode: a) velocity ω; b) electromagnetic torque T; c) circuit current ic 4. CONCLUSION The models of the pulse-vector control of wound rotor induction motor drive with the rotor position sensor and indirect position determination were developed by means of ANSYS Electromagnetics Suite. Implementation of the untraditional pulse-phase control unit syncing thyristor-enabling pulses with the network in the pulse-vector control system, ensured meeting required motor torque values in the half-wave detection circuit. Examinations carried out in ANSYS Electromagnetics Suite figures that the method of indirect rotor angular position is appropriate. The pulse-vector control with indirect rotor angular position determination is operable, having quality parameters being highly competitive with those of the sensor-mounted system. a) c) ω, rad/s T, N. m ic, A t, s t, с t, s Imax = 21,5 A T max = 122 N. m ω max = 27 rad/s ω max = 14 rad/s ω av = 20 rad/s T av = 18.5 N. m I RMS = 6.2 A b) t, s
  • 12.  ISSN: 2088-8694 IJPEDS Vol. 8, No. 3, September 2017 : 1147 – 1159 1158 Properties of the PVC with indirect determination and process quality parameters enable to infer that the problems stated in the introduction were successfully solved. Application of the developed PVC with indirect determination will allow carrying out modernization of massive mechanisms with moderate standards for accuracy of velocity control, velocity decrease during load reduction or removal, with as low economic costs as possible – both during modernization itself, and during further operation. ACKNOWLEDGEMENTS The work was supported by Act 211 Government of the Russian Federation, contract № 02.A03.21.0011 REFERENCES [1] I. M. Alsofyani and N. R. N. Idris, “A Review on Sensorless Techniques for Sustainable Reliablity and Efficient Variable Frequency Drives of Induction Motors,” Renewable and Sustainable Energy Reviews, vol. 24, pp. 111- 121, 2013. [2] J. Holtz, “Sensorless Control of Induction Motor Drives,” Proceedings of the IEEE, vol/issue: 90(8), pp. 1359– 1394, 2002. [3] J. C. Gamazo-Real, et al., “Position and Speed Control of Brushless DC Motors Using Sensorless Techniques and Application Trends,” Sensors, vol/issue: 10(7), pp. 6901-6947, 2010. [4] C. M. Verrelli, et al., “Nonlinear Tracking Control for Sensorless Permanent Magnet Synchronous Motors with Uncertainties,” Control Engineering Practice, vol. 60, pp. 157-170, 2017. [5] Z. Qiao, et al., “New Sliding-mode Observer for Position Sensorless Control of Permanent-magnet Synchronous Motor,” IEEE Transactions on Industrial Electronics, vol/issue: 60(2), pp. 710-719, 2013. [6] D. A. Dominic and T. R. Chelliah, “Analysis of Field-oriented Controlled Induction Motor Drives under Sensor Faults and an Overview of Sensorless Schemes,” ISA Transactions, vol/issue: 53(5), pp. 1680-1694, 2015. [7] M. H. Holakooie, et al., “Full-order Luenberger Observer Based on Fuzzy-logic Control for Sensorless Field- oriented Control of a Single-sided Linear Induction Motor,” ISA Transactions, vol. 60, pp. 96-108, 2016. [8] M. Beschi, et al., “Sensorless Model-based Object-detection Applied on an Underactuated Adaptive Hand Enabling an Impedance Behavior,” Robotics and Computer-Integrated Manufacturing, vol. 46, pp. 38-47, 2017. [9] S. Derammelaere, et. al., “Sensorless load angle control for two-phase hybrid stepper motors,” Mechatronics, vol. 43, pp. 6-17, 2017. [10] M. Montanari, et. al., “Speed Sensorless Control of Induction Motors Based on a Reduced-Order Adaptive Observer,” IEEE Transactions on Control Systems Technology, vol/issue: 15(6), pp. 1049-1064, 2007. [11] P. Shinde, et al., “Speed Control of Induction Motor by Using Variable Frequency Drive,” Rupali Burungale et al Int. Journal of Engineering Research and Applications, vol/issue: 4(4), pp. 35-37, 2014. [12] Y. S. Usynin, et al., “Asynchronous Electric Drive with Pulse-vector Control,” Russian Electrical Engineering, vol/issue: 82(3), pp. 134-137, 2011. [13] Y. S. Usynin, et al., “Pulse-vector Control with Indirect Determination of Rotor Angular Position,” Russian electrical engineering, vol/issue: 84(10), pp. 566-571, 2013. [14] M. A. Iqbal and V. Agarwal, “Investigation & Analysis of Three Phase Induction Motor Using Finite Element Method for Power Quality Improvement,” International Journal of Electronic and Electrical Engineering, vol/issue: 7(9), pp. 901-908, 2014. [15] Y. S. Usynin, et al., “Synthesis of Control System by Electrical Drive with Synchronous Reluctance Independent Excitation Machine,” Bulletin of South Ural State University. Series: Power Engineering, vol/issue: 18(37), pp. 38-41, 2012. [16] Y. V. Alekseev, et al., “Crane Electrical Equipment: Reference Book,” Moscow, Energiya Publishing House, pp. 240, 1979. [17] I. P. Kopylov, “Handbook of electrical machines: 2 tons,” Moscow, Energoatomizdat Publishing House, pp. 688, 1989. BIOGRAPHIES OF AUTHORS Tatiana Andreevna Funk received the PhD degree from South Ural State University, Chelyabinsk, Russian Federation, in 2012. She is currently an Associate Professor in the Department of Electric Drive, South Ural State University, Chelyabinsk, Russian Federation. Her research interests include motor drive control systems with motor-mounted sensor and indirect control systems.
  • 13. IJPEDS ISSN: 2088-8694  Inderect Pulse-Vector Control of Wound Rotor Induction Motor Drive in .... (Tatiana Andreevna Funk) 1159 Yuriy Semenovich Usynin received the PhD degree from Moscow Power Engineering Institute, Moscow, Russian Federation in 1994. He is currently a Professor in the Department of Electric Drive, South Ural State University, Chelyabinsk, Russian Federation. His research interests include motor drive control systems and the electric drive with the field regulated reluctance machine. Evreniy Viktorovich Belousov received the PhD degree from South Ural State University, Chelyabinsk, Russian Federation, in 2014. He is currently an Associate Professor in the Department of Electric Drive, South Ural State University, Chelyabinsk, Russian Federation. His research interests include the electric drive with the field regulated reluctance machine and electric transport.