Page 1 of 12

European Journal of Business &

Social Sciences

Available at https://ejbss.org/

ISSN: 2235-767X

Volume 07 Issue 04

April 2019

Available online: https://ejbss.org/ P a g e | 1947

Direct Torque Control for Matrix Converter-fed

Three phase Induction Motor

VELMURUGAN .S

PG Student

PRIST Deemed to be University, Thanjavur

Abstract— This paper develops a direct torque control

method (DTC) using a matrix converter fed induction motor.

The advantages of matrix converters are combined with the

advantages of the DTC technique; under the constraint of the

unity input power factor, the required voltage vectors are

generated to implement the conventional DTC method of

induction motor. The proposed DTC algorithm is applied to

induction motors and the simulation results are given in

steady-state and transient conditions, while the discussion

about the trend of the DTC method using the MC is also

carried out.

Keywords- Matrix converte; induction motor; direct torque

control method

I. INTRODUCTION

In the past two decades, due to the need to increase

the quality and the efficiency of power supply and usage,

the three phase matrix converter has become a major

modern energy converter and has emerged from the

previously conventional energy conversion modules as

one of the best substitutions [1], [2].

Matrix converter fed motor drive is superior to pulse width

modulation (PWM) inverter drives because it provides

bidirectional power flow, sinusoidal input/output currents,

and adjustable input power factor [3], [4]. Furthermore,

matrix converter allows a compact design due to the lack

of dc-link capacitors for energy storage. However, only a

few of practical matrix converters have been applied to

vector control system of induction motors (IM) for the

reason: Modulation technique and commutation control

are more complicated than conventional PWM inverter

[4].

Since the Direct Torque Control (DTC) method has been

proposed in the mid 1980’s, The Direct Torque Control (DTC)

method for AC machines is prevalently utilized in

Page 2 of 12

European Journal of Business &

Social Sciences

Available at https://ejbss.org/

ISSN: 2235-767X

Volume 07 Issue 04

April 2019

Available online: https://ejbss.org/ P a g e | 1948

√3

when it is comparing with the Field Oriented Control

method. Reducing the torque ripple in conventional

DTC has the cost of small sampling interval that may

lead to high switching frequency [7]. In recent years,

several investigations have been performed with the

aim of improving steady state performance of the

DTC method, e.g., Direct Self Control (DSC) [8],

utilizing Space Vector Modulation (SVM) [9],

utilizing multi level inverters [10],

[16] or Matrix Converter [17] and Predictive Torque

Control [13]-[14].

By combining the advantages of matrix converters

with the advantages of DTC schemes, it is possible to

achieve fast torque and flux responses in a wide speed

range.

In this paper, a new DTC control for matrix converter

is proposed which allows under the constraint of unity

input power factor, the generation of the voltage

vectors required to implement the DTC of three phase

induction motor. Depending on the induction motor

operating point such vectors might be applied and

consequently the electromagnetic torque ripple is reduced.

Simulation results demonstrate the effectiveness of the

proposed control scheme was presented. Both, steady-state

and transient behaviour have been investigated.

II. DTC AND DTC MATRIXCONVERTER

(DTC-MC) STRUCTURES

DTC STRUCTURES

The basic model of DTC induction motor scheme is

shown in Fig. 1. At each sample time, the two stator

currents ica and icb and the DC bus voltage Vdc are

sampled. Using the inverter voltage vector, the α, þ

components of the stator voltage space vector in the

stationary reference frame are calculated as follows.

many variable speed drives, especially in case the torque V = 2 V

(s − cb+cc

)

control is more desired than speed control. The DTC cαref { 3 dc a 2 (1)

method has the dominant advantages such as fast transient

toque response and low calculation burden [6]. However

because of “Bang-Bang”control characteristic and not

using modular regulators, conventional DTC has two

drawbacks. First, the switching frequency is variable and

dependent to the hysteresis bands and speed of the motor.

Second, the torque ripples are considerable especially

Vcþref =

1 Vdc(sb − sc

)

The α, þ components of the stator current space vector

are calculated using

Page 3 of 12

European Journal of Business &

Social Sciences

Available at https://ejbss.org/

ISSN: 2235-767X

Volume 07 Issue 04

April 2019

Available online: https://ejbss.org/ P a g e | 1949

2

Icα = ica (cα = oLcIcα + M (rα

{ Icþ =

ica+2icb

√3

(2) {

Lr

(cþ = oLcIcþ + M (rþ

(3)

The stator flux is a function of the rotor flux which is

provides from the flux observer.

Lr

Then the magnitude of the stator flux is calculated by

|(c| = J(

2 + (

2

(4)

cα cþ

(cref

Tref

Figure. 1. Block diagram of classical DTC

The electromagnetic torque is calculated by

Te =

3 p((cαIcþ–

(cþIcα)

where p is the number of pole pairs.

The torque and flux errors are defined as

{

∆(c = |(cref| — |(c|

∆Te = Tref — Te

(5)

(6) (a) Flux comparator.

Te

(b) Three-level torque comparator.

The inverter switching states are determined by the

torque and flux errors according to the sector determined.

In order to maintain the estimated stator flux

and torque within their boundaries which are determined

by the two hysteresis bandwidths as shown in figure 2a &

2b, at each sampling period, the torque and the stator flux

are estimated and compared with the corresponding

reference values before passing the hysteresis comparator.

The position of the stator flux is detected, and the

most suitable space vector among 8 space

vectors generated by a VSI is selected from the switching

table given in Table 1 to compensate the load torque and the

stator flux.

Vdc

Switching Table

+ -

(c

Sa

Sb

Sc

1

-Th

+ -

T

T

Th

-1

est

(c

Torque and Flux

Estimator

Vdc

Ia

Ic

IM

VSI

Fh

-1

-Fh

1

1

-Fh F

s

h

-1

1

-Th

Th

-1