 Open Access
 Total Downloads : 1349
 Authors : L. Sarah Ancelina, I. Gerald Christopher Raj
 Paper ID : IJERTV2IS4829
 Volume & Issue : Volume 02, Issue 04 (April 2013)
 Published (First Online): 04052013
 ISSN (Online) : 22780181
 Publisher Name : IJERT
 License: This work is licensed under a Creative Commons Attribution 4.0 International License
Direct Torque Control for Induction Motor Without Current Sensors
Direct Torque Control for Induction Motor Without Current Sensors
L. Sarah Ancelina M.E.(Power Electronics & Drives)
PSNA college of engineering & Technology, Dindigul.
I. Gerald Christopher Raj M.E(Ph.d..,) Associate Professor
PSNA CET
This project presents a lowcost and simple phasecurrent reconstruction algorithm for threephase induction motor (IM) under direct torque control (DTC) using the information obtained from only one shunt resistor (in series with low side switches in a conventional threephase inverter). The aim is to develop a lowcost highperformance IM drive. The proposed algorithm is robust and very simple. It uses the dc current to reconstruct the stator currents needed to estimate the motor flux and the electromagnetic torque. A theoretical concept is developed, the modified lookup table is presented, and currentaccess tables are designed and used in the phasecurrent reconstruction. The limitations are also studied and presented. Simulation are given to prove the ability of the proposed scheme of reproducing the performances of a traditional DTC IM drive.
DIRECT torque control (DTC) of induction motors has gained popularity in industrial applications mainly due to its simple control structure from its first introduction in 1986 [1]. An electric motor drive controlled with the DTC technique exhibits performance similar to a fieldoriented drive despite a simpler structure [1], [2]. In fact, a DTC scheme achieves the closedloop control of the motor stator flux and the electromagnetic torque without using any current loop or shaft sensor.Many researchers are interested in this control technique because of its wide area applications used with various ac machine types as induction motor [3], PMSM [4], [5], PM Brushless [6], and reluctance motor [7]. The DTC scheme requires information about the stator currents and the dclink voltage, which is used with the inverter switches states, to estimate the values of stator flux and electromagnetic torque. The current feedback for the closedloop control is usually obtained by sensing instantaneous phase currents by current sensors. In general, galvanically isolated current sensors such as Halleffect sensors and current transducers are widely used in many applications [8], [9]. Recently, single current sensor operation has been proposed to reconstruct phase currents from the dclink current sensor [10]. In this way, various approaches have been proposed
in the literature. Some methods adjust the pulsewidth modulation (PWM) signals to ensure that twophase currents can be sampled in each control period [11][15]. Other strategies introduce modifications of the modulation algorithm in order to guarantee the reliability of the measurements from the dclink current sensors under all the operating conditions [16][18]. Other interesting approaches are based on the estimation of the motor phase currents using predictioncorrection algorithms, thus introducing additional computational burden to the drive system [19][22]. Only a few papers deal with the DTC technique for induction motor [23] and PMSM [24]. The algorithm used in these works operates in two stages. First, it predicts the stator currents from a model of the motor and then adjusts the prediction on the basis of the sensed dclink current. This algorithm requires an additional computation burden and the knowledge of the stator transient inductance.In this project, we propose a lowcost single shunt current sensor induction motor (IM) DTC. The stator flux vector and the electromagnetic torque are directly calculated from the voltage and the current derived from a single dclink voltage sensor (simple voltage divider) and a single dclink current sensor (simple shunt resistor). The phase currents are estimated by two dclink current measurement processes. This algorithm does not require additional computation burden or other motor parameter knowledge.
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The key idea of the basic DTC is slip control, which is based on the fact that, under constant stator flux linkage, the change rate of torque is proportional to the instantaneous slip between the stator flux and rotor . Therefore, torque control can be achieved by means of controlling the slip. There will be eight voltage vectors that can be used for torque and flux control as shown in Figure. It is seen that there are 6 nonzero vectors and 2 zero vectors.
Under the basic DTC, the flux and torque control are carried out by means of a switching table, as shown in Figure2.1 the flux plane is divided into 6 sectors. In each sector, there are four nonzero vectors and two zero vectors that are needed to control the flux and torque. Each vector has different effect on the torque and flux linkage. For example, if the flux linkage vector is in sector 1, voltage vector V3 (011) used to increase both the torque and the flux linkage. V4 (100) is used to decrease the both. V2 (010) is used to increase torque
and reduce the amplitude the flux linkage. V5 (101) is used to reduce the both.
If the voltage drop on the stator resistance is neglected, it can be assumed that the flux linkage is always following the direction of the voltage vector. And for each vector, there are two components, one for controlling torque and the other one flux linkage. It is seen that the torque and the flux component are different at different position. It should also be noted that in each border of the 6 sectors, the ability of controlling the flux linkage is very weak sometime, as reported in .
Therefore, if more vectors are used in one sampling interval, maybe a better performance can be expected. And that is the basis of the modified DTC. Under the modified scheme, 3 vectors are used to control flux, such that the amplitude of flux and torque can be controlled.
Figure 2.1Eight voltage space vectors generated by a 3 2 level inverter

The equation for the developed torque of an induction motor may be expressed in terms of the stator and rotor flux space vector as in equation (3.I)
X
Figure 3.1 voltage vectors of 3 PWM inverter
The change of the stator flux vector per switching instant is therefore determined by equation (3.2) and Figure 3.1. The change of the magnitude of stator flux space vector and the change of the torque with varying angle of the stator flux space vector are shown in Figure 3.2, respectively. It may be seen from the figures that the change of stator flux and torque is sinusoidally distributed over the stator flux angle for the non zero voltage vectors V1 to V6 and is constant for the zero vectors V0, and V7. The dc offset of all sinusoids coincides with the line for voltage vectors V0 and V7.
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For example it may be seen, that the application of voltage vector V2, in the centre of section S2 (60 degrees) causes the maximum stator flux increase possible for a given time interval and a given dc link voltage. However, it also causes the developed torque to decrease as shown in Figure 3.2. It has been obtained that the amplitudes, phase shifts and dc levels for the sinusoids in Figure 3.2do not vary with different motor speed and load torque conditions.
The phase shift of the motor torque changes
m
m
T m
sin
(3.1)
increases only marginally (approx. 5 degrees) for high
Xs Xr

X 2 s r
speed, high load torque operation. However, the dc offset of the sinusoid in Figure 3.2 changes considerably with
where , denotes the angle between the stator and the rotor flux space vectors, Xs, Xr, and Xm, represent the stator, rotor and airgap self inductions, respectively. For a constant magnitude of the stator and rotor flux space vectors, the angle may be used to control the torque of the motor. The following expression may be obtained from the stator voltage equation of the induction motor model
motor condition. The zero change line tends to move upwards when the motor speed is increased. Therefore, less positive torque change may be obtained and thus the maximum motor speed is limited.
1 t V dt
s T n 0 s
(3.2)
where Tn, denotes the electrical time constant and Vs, the stator voltage space vector. This expression is valid for a stator fixed reference frame and a stator resistance equal to zero. It can be seen that the stator voltage directly impresses the stator flux. The stator voltage space vector Vs, may assume six different non zero states and two zero states as shown in Figure 3.1
Figure 3.2 Flux and Torque change in 100s
Smilarly, for low speed operation, the zero change line moves towards the negative peaks in Figure 3.4, thus positive torque changes are easily obtained. Since the sequence of the stator flux and torque changes for the voltage vectors V0 to V7 remains unchanged, a selection table as shown in Table 3.1 may be obtained to control the stator flux and torque of an induction motor. The sections of the stator flux space vector are denoted as S1 to S6, according to Figure 3.2. The magnitude error of the stator flux space vector is denoted by . If = 1 then the stator flux level is too low and therefore the voltage vectors V2 or V6 are selected, which cause a positive flux change, as can be seen from Figure 3.2.
Table 3.1 selection table for DTC
The torque error is represented by T and T = 1 denotes that the developed torque is too high and can be decreased by selecting V6 if the angle of the stator flux vector is in section S1 (Table 3.1 and Figure 3.2). Similarly, the torque can be increased by selecting V2 for T = 1. The zero voltage vectors V0 and V7 are selected when the torque error is within the given hysteresis limits.


The basic DTC scheme (see Fig. 1) requires two current sensors at least. The proposed DTC scheme described in this paper uses only one shunt resistor for dclink current measurement as revealed on Fig. 3. For this purpose, a suitable method to reconstruct the phase currents and voltages is devised with a simple modification of the basic DTC scheme using zone shift strategy. Two modifications of the basic DTC are used for estimating the threephase currents from a single dc link current sensor. On the first modification, the control system should be able to generate more voltage vectors. This goal can be
Fig. 4.1 Proposed DTC scheme.
Fig. 4.2 Proposed DTC sectors and inverter voltage
vectors.
approximately by applying, at each cycle period, different voltage vectors for prefixed time intervals, leading to a discrete SVM technique. By using this modulation strategy, new voltage vectors can be
synthesized with respect to those used in the basic DTC technique. It has been verified that subdividing the cycle period in two equal time intervals leads to a substantial reduction of current sensors without the need for too complex switching tables. Using the DSVM technique with two equal time intervals, 12 new voltage vectors can be generated; we use only six active voltage vectors in our proposed DTC scheme as represented in Fig. 4.1. The red vectors represent the synthesized voltage vectors.
As the zone shift strategy, one other modification results in improving the DTC by using a new lookup table and adjusting the six stator flux sectors of the conventional DTC (see Fig. 2). The first sector is taken from 0 to 60 (see Fig. 4.2), instead of 30 to 30. The new operation table of the modified DTC is presented in Table II.
TABLE II
PROPOSED DTC SWITCHING TABLE
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One of the most important purposes for single shunt threephase reconstruction is to reduce the cost. This, in turn, simplifies the sampling circuit to one shunt resistor and some other electronic components. Moreover, the singleshunt algorithm allows the use of power modules that do not provide, for each phase, individual ground connection. Another singleshunt measurement advantage is that the same circuit is being used to sense all three phases. For all measurements, the gains and offset will be the same, which eliminate the software calibration of each phase measurement structure.
Sampling Time
Both dclink current sampling instants must be chosen for the application of the threephasecurrent reconstruction concept. In accordance with Fig. 5
Fig. 5 Recurred sampling time.
the optimal sampling instants should be calculated relatively to the active vector transition instants. For a consistent dclink current value, the signal sampling must take place after an additional delay
Tsample Ton + Tsr + Tss . (9)The sample time includes the total switching device turnon delay time Ton), the dclink current signal rise time (Tsr ), and the signal settling time (Tss ). The Ton parameter includes the dead time, the insulated gate bipolar transistor (IGBT) driver signal processing time, and the worst case switching device (IGBT) ontime delay. The parameter Tss is related to the signal amplifiers and the isolation circuit. Once the sampling is started, the process requires an extra sampleandhold time delay (TADC). The latter can be important, particularly in the case of a lowcost DSC ADC. However, all these delays may be neglected compared to the DTC control period. The sampling instant chosen in the proposed phase current reconstruction is at the end of each half period when the dc current signal is stabilized.
The smallest DTC control period is given by Ts
2 (Ton + Tsr + Tss + TADC) (10) Actually, the sum of all these time delays is about a few microseconds, even with the isolation system, which is far smaller compared to 50 s used in our system. Fig. 5.1
illustrates the example of recurred sampling time when the voltage vector V12is applied.

The control strategy uses the same reference (synchronized sinusoidal signal) as the conventional SPWM while the carrier triangle is a modified one. The control scheme uses an inverted (high frequency) sine carrier that helps to maximize the output voltage for a given modulation index. Enhanced fundamental component demands greater pulse area. The difference in pulse widths (hence area) resulting from triangle wave and inverted sine wave with the low (output) frequency reference sine wave in different sections can be easily understood. In the gating pulse generation of the proposed ISCPWM scheme shown in Fig. 6.1
Fig. 6.1 Inverter sine carrier PWM pulse pattern.
the triangular carrier waveform of SPWM is replaced by an inverter sine waveform. For the ISPWM pulse pattern, the switching angles may be computed as the same way as SPWM scheme. It is worthwhile to note that both in SPWM (considered) and ISCPWM schemes, the number of pulses will be equal to f M and hence the constant
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switching loss is guaranteed. To have conceptual understanding of wider pulse area and hence the dexterous input dc utilization in the ISCPWM, location of switching angles, duty cycle and their dependence on a M and f M are discussed. Fig. 6.2depicts the influence of a M on different switching angles (four angles considered in both cases) at constant f M of 6. From this figure, it is observed that the odd switching instants vary with negative slope and even Inverted Sine Carrier for switching instants have positive slope. Variation of all the switching instants against a M is a straight line and slope f each one is more than its previous one. All the odd switching angles of ISCPWM method happen earlier than similar angles of PWM method, while the situation is reverse in case of even switching angles and hence higher pulse area. Both SPWM and ISCPWM upshots nonlinear relationship in the lower f M range.
Fig. 6.2 Influence of modulation index on switching angles.

A simulation model is established to MATLAB/SIMULINK modelbased on power system toolbox was developed to examine the proposed control algorithm and the phasecurrent reconstructionfeasibility.
Figure 7.Simulation diagram
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Figure 7.1 Current Waveform of Basic
DTC
Figure 7.2 Flux Waveform of Basic DTC
Figure 7.3 Torque Waveform of Basic DTC
FIGURE 7.4 FLUX WAVEFORM OF MODIFIED
DTC
Figure 7.5 Torque Waveform of Modified DTC

CONCLUSION
This project presents a new direct torque and flux control strategy based on two pi controllers and a voltage spacevector modulator. the main conclusions are as follows.

DTCISPWM strategy realizes almost ripplefree operation for the entire speed range. Consequently, the flux, torque, and speed estimation is improved.

The fast response and robustness merits of the basic DTC are entirely preserved.

The switching frequency is constant and controllable. in fact, the better results are due to the increasing of the switching frequency. While for DTC a single voltage vector is applied during one sampling time, for DTC ISPWM a sequence of six vectors is applied during the same time. It can be stated that, using the DTCISPWM topology, the overall system performance is increased



I. Takahashi and T. Noguchi, A new quickresponse and highefficiency control strategy of an induction motor, IEEE Trans. Ind. Appl., vol. IA 22, no. 5, pp. 820827, Sep./Oct. 1986.

S. A. Zaid, O. A. Mahgoub, and K. ElMetwally, Implementation of a new fast direct torque control algorithm for induction motor drives, IETE lectr. Power Appl., vol. 4, no. 5, pp. 305313, May 2010.

C. Patel, R. P. P. A. Day, A. Dey, R. Ramchand, K. K. Gopakumar, and M. P. Kazmierkowski, Fast direct torque control of an openend induction motor drive using 12sided polygonal voltage space vectors, IEEE Trans. Power Electron., vol. 27, no. 1, pp. 400410, Jan. 2012.

Y. Zhang and J. Zhu, Direct torque control of permanent magnet synchronous motor with reduced torque ripple and commutation frequency, IEEE Trans. Power Electron., vol. 26, no. 1, pp. 235248, Jan. 2011

Y. Zhang and J. Zhu, A novel duty cycle control strategy to reduce both torque and flux ripples for DTC of permanent magnet synchronous motor drives with switching frequency reduction, IEEE Trans. Power Electron., vol. 26, no. 10, pp. 30553067, Oct. 2011.

K. D. Hoang, Z. Q. Zhu, andM. P. Foster, Influence and compensation of inverter voltage drop in direct torque controlled fourswitch three phase PM brushless AC drives, IEEE Trans. Power Electron., vol. 26, no. 8, pp. 23432357, Aug. 2011.

S. Bolognani, L. Peretti, and M. Zigliotto, Online MTPA control strategy for DTC synchronous reluctancemotor drives, IEEE Trans. Power Electron., vol. 26, no. 1, pp. 2028, Jan. 2011.
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G. Foo and M. F. Rahman, Direct torque and flux control of an IPM synchronous motor drive using a backstepping approach, IET Elect.Power Appl., vol. 3, no. 5, pp. 413421, Sep. 2009.

M. E. Haque and M. F. Rahman, Incorporating control trajectorieswith the direct torque control scheme of interior permanent magnet synchronous motor drive, IET Elect. Power Appl., vol. 3, no. 2, pp. 93101 Mar. 2009.

T. C. Green and B. W. Williams, Derivation of motor linecurrent waveforms from the dclink current of an inverter, in Proc. IEE Elect. Power Appl., Jul. 1989, vol. 136, no. 4, pt. B, pp. 196204.

W. C. Lee,T. K. Lee, andD. S.Hyun, Comparison of singlesensor current control in the dc link for three phase voltagesource PWM converters, IEEE Trans. Ind. Electron., vol. 48, no. 3, pp. 491505, Jun. 2001.

J. T. Boys, Novel current sensor for PWM AC drives, in Proc Electr. Power Appl., 1988, vol. 135, pt. B, pp. 2732.