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International Journal of Power Electronics and Drive System (IJPEDS)
Vol. 7, No. 1, March 2016, pp. 217~224
ISSN: 2088-8694  217
Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS
Close Loop V/F Control of Voltage Source Inverter using
Sinusoidal PWM, Third Harmonic Injection PWM and Space
Vector PWM Method for Induction Motor
Sandeep Ojha, Ashok Kumar Pandey
Department of Electrical Engineering, Madan Mohan Malaviya University of Technology
Gorakhpur, Uttar Pradesh, India
Article Info ABSTRACT
Article history:
Received Oct 20, 2015
Revised Dec 21, 2015
Accepted Jan 15, 2016
The aim of this paper to presents a comparative analysis of Voltage Source
Inverter using Sinusoidal Pulse Width Modulation Method, Third Harmonic
Injection Pulse Width Modulation Method and Space Vector Pulse Width
Modulation Two level inverter for Induction Motor. In this paper we have
designed the Simulink model of Inverter for different technique. An above
technique is used to reduce the Total Harmonic Distortion (THD) on the AC
side of the Inverter. The Simulink model is close loop. Results are analyzed
using Fast Fourier Transformation (FFT) which is for analysis of the Total
Harmonic Distortion. All simulations are performed in the MATLAB
Simulink / Simulink environment of MATLAB.
Keyword:
Induction motor
Sinusoidal pulse width
modulation
Space vector pulse width
modulation
Third harmonic injection pulse
width modulation
Voltage source inverter
Copyright © 2016 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Sandeep Ojha,
PG Scholar
Department of Electrical Engineering,
Madan Mohan Malaviya University of Technology,
Gorakhpur, Uttar Pradesh, India
Email: ojha.sandeep89@gmail.com
1. INTRODUCTION
A circuit which is used for converting DC power into an AC power at desired output Voltage and
Frequency is known as an Inverter. A phase controlled converter, when it is used in inverter mode, are known
as line-commutated Inverter, only line-commutated inverter requires at the output terminals an existing AC
supply which is used for their commutation it means it required external circuit for commutation. A Force
commutated Inverter gives an independent AC output voltage of adjustable Voltage and Frequency therefore
its application is so vast. In an Inverter we require Forced commutation for thyristor, therefore we can use
other self-commutating device like GTO, MOSFET, and other Transistors to avoiding the commutation
circuit. But for high power application we must use thyristor along with the forced commutation circuit.
There are major four techniques to reduce the Total Harmonic Distortion in Inverter:
1) Sinusoidal Pulse Width Modulation
2) Third Harmonic Injection Method
3) 60° Pulse modulation
4) Space Vector Pulse Width Modulation
 ISSN: 2088-8694
IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224
218
2. TWO LEVEL INVERTER 
In this level 180 degree mode each MOSFET conducts for 180° of a periodic cycle. Each phase has
a pair S1, S4; S3, S6; S5, S2 and each trigger for 180° of time interval. And S1, S3, and S5 conduct at an
interval of 120°. Refer to Figure 1.
0° 60° 120° 180° 240° 300° 360°
S1 S3 S5
S6 S2 S4 S6
Figure 1. Switching period of MOSFET
Specification of each MOSFET 180° mode VSI. Refer to Table 1.
Table 1. For 50 Hz frequency Pulse Generator where amplitude = 230*1.414 and pulse width 50%
S1 Phase Delay = 0 msec
S4 Phase Delay = 10 msec
S3 Phase Delay = 6.667 msec
S6 Phase Delay = 16.667 msec
S5 Phase Delay = 13.33 msec
S2 Phase Delay = 23.33 msec / - 0.0033 sec
3. SINUSOIDAL PULSE WIDTH MODULATION (SPWM)
This technique is very useful for reducing the Total Harmonic Distortion (THD). This technique is
characterized by the constant amplitude pulse. And the width of these pulses is modulated to get Inverter
output Voltage control and to reduce its harmonic content in the voltage. Force commutation is essential for
the pulse width modulation technique. The Switching sequences and topology of the Inverter is same as
normal level of Inverter. In this technique the Gate pulses of each MOSFET is modulated and control the
Switching of MOSFET to get the desired output voltage at desired frequency for input voltage of Induction
motor.
Fourier analysis of the voltage waveform and get the output voltage of an Inverter.
V(t)= A0 + 2* ∑ ∗ ∗ 													 ] (i)
The output voltage wave is odd symmetry. So, A0 and Ak is zero because it has an even symmetry. So,
Bk= (2/π)*[ ∗ sin	 ]
=((4*Vs)/(nπ))*[sin(nπ/2)*sin(nd)] (1)
V0= ∑ ∗ sin ∗ 			sin ∗ sin	, , … ) (2)
nd is made equal to π. So, d= (π/n)
So, the pulse width is made 2d so it is equal to (2d/n).
In the Simulink model sine wave frequency is 50 Hz and the amplitude of the sine wave is 230*1.414 and
carrier frequency is sinusoidal with frequency is 10000 Hz.
For a close loop we take the speed as a feedback and compare to the reference speed and then the speed error
again added with the rotor speed and its output is change into the Gate Pulse of the MOSFET.
4. THIRD HARMONIC INJECTION PULSE WIDTH MODULATION METHOD (THIM)
This method is also a very useful method for eliminating the harmonic in the system which comes
due to the presence of power electronic switches. In this method we inject the third harmonic in the system
IJPEDS ISSN: 2088-8694 
Close Loop V/F control of VSI using SPWM, THIPWM and SVPWMM for IM(Sandeep Ojha)
219
and control the pulse of the each MOSFET to get the harmonic free inverter output voltage. Now to find the
amplitude of the third harmonic of unknown amplitude of the third harmonic component.
So let us take simple sine wave with the third harmonic sine wave of unknown amplitude x.
Y (α) = sin (α) + x*sin (3α) (3)
For finding the maximum value of the function
d/dα (Y (α)) =0
Which gives,
α=cos-1
9 1 / 12 (4)
From equation (3) and (4)
F(x)=Y(α)=[(3x+1)( 3 1 / 12 – 4x 3 1 / 12.
] (5)
For finding the maximum value of equation (5) using formula d/dx (F(x))
So we get x = -0.334, 0.1667
At x = -0.334
d2
/dx2
(F(x)) = 0
At x = 0.1667
d2
/dx2
(F(x)) = 10.3923
Which shows the given function is minimum. At
x = 0.1667 and the value of α is 60°
Now putting the value of α at x = 0.1667
d2
/dx2
(Y (α)) = -2
This shows the function Y (α) is maximum at x = 0.1667 and the value of α is 60°
So this is clear that the third harmonic should be 0.1667 of this amplitude
Now putting the value of x= 0.1667 and α= 60° in equation (4)
Which gives Y (α) =0.866025 which is the peak of resultant waveform with third harmonic. And the
modulation factor of 1/0.866025 is 1.15470053 giving 15.47% more DC utilization.
120°
120°
(6)
Where,
V is Instantaneous maximum Magnitude of fundamental
And
α is instantaneous phase of fundamental
The above results give the information about the amplitude of the output phase voltage is 1.15 times of the
normal output phase voltage. In the Simulink model sine wave frequency is 50 Hz and the amplitude of the
sine wave is 230*1.414 and carrier frequency is sinusoidal with frequency is 10000 Hz. And additional sine
wave is added to add the third harmonic in the Inverter whose sine wave amplitude is 230*1.414/6 and its
frequency is 3 times of rated frequency. For a close loop we take the speed as a feedback and compare to the
reference speed and then the speed error again added with the rotor speed and its output is change into the
Gate Pulse of the MOSFET.
5. SPACE VECTOR PULSE WIDTH MODULATION (SVPWM)
This technique is very useful for reducing the Total Harmonic Distortion. This technique is
characterized by the constant amplitude pulse. And the width of these pulse is modulated to get Inverter
output Voltage control and to reduce its harmonic content. The topology of three leg Voltage Source Inverter
because of the constraint that the input line must never be shored and the output current must be always be
continuous a Voltage Source Inverter can assume only eight distinct sectors. Six out of these eight sectors
produces a non-zero output voltage and are known as non-zero switiching states and the remaining two
sectors produces zero voltage are known as zero switching states.
 ISSN: 2088-8694
IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224
220
The SVPWM can be implemented by using wither sector selection algorithm or by using a carrier based
space vector algorithm.
The types of SVPWM implementations are:
a) Sector selection
b) Reduced switching
c) Carrier based
d) Reduced switching carrier based
 Sector selection of SVPWM : -
Step1. Determine Vd, Vq, Vref, and angle µ
Step2. Determine time duration T1, T2, T0
Step3. Determine the switching time of each
IGBT (S1 to S6)
For Step 1, Refer Figure 2
Figure 2. Vd, Vq, Vref, and µ can determine
Vd=Van–0.5*Vbn-0.5*Vcn (7)
Vq=0+0.866*Vbn–0.866*Vcn (8)
Vref= Vd
2
+ Vq
2
) (9)
µ = tan-1
(Vq/Vd) = wt=2πft (10)
For Step 2, Refer Figure 3 which shows the switching time during a sector1
Figure 3. Reference vector as a combination of adjacent vectors at sector
Switching time duration at sector 1
	 = 1	 + 2	 + 0	 (11)
IJPEDS ISSN: 2088-8694 
Close Loop V/F control of VSI using SPWM, THIPWM and SVPWMM for IM(Sandeep Ojha)
221
Tt*Vref = (T1 *V1 + T2* V2) (12)
Tt* |Vref|* cos (µ) = T1* 2/3*Vdc + V2*2/3 *cos (π/3) (13)
Tt*|Vref|*cos (µ) = V2*0.667*sin(π/3) (14)
Where, (0 <= µ <= 60º)
T1 = Tt*µ*(sin (π/3-µ) / sin (π/3)) (15)
T2 = Tt*µ*(sin (µ) / sin (π/3)) (16)
T0 = Tt – (T1 + T2) (17)
Where, Tt = 1/ft and µ= |Vref| / (0.667*Vdc)
For step 3 refer Table 2
Table 2. Switching Time Calculation at Each sector
Sector Upper Switches (S1, S3, S5) Lower Switches
(S4, S6, S2)
1 S1=T1 + T2 + T0/2
S3= T2 + T0/2
S5= T0/2
S4= T0/2
S6= T1 + T0/2
S2= T1 + T2 + T0/2
2 S1= T1 + T0/2
S3= T1 + T2 + T0/2
S5= T0/2
S4= T2 + T0/2
S6= T0/2
S2= T1 + T2 + T0/2
3 S1= T0/2
S3= T1 + T2 + T0/2
S5= T2 + T0/2
S4= T1 + T2 + T0/2
S6= T0/2
S2= T1 + T0/2
4 S1= T0/2
S3= T1 + T0/2
S5= T1 + T2 + T0/2
S4= T1 + T2 + T0/2
S6= T2 + T0/2
S2= T0/2
5 S1= T2 + T0/2
S3= T0/2
S5= T1 + T2 + T0/2
S4= T1 + T0/2
S6= T1 + T2 + T0/2
S2= T0/2
6 S1= T1 + T2 + T0/2
S3= T0/2
S5= T1 + T0/2
S4= T0/2
S6= T1 + T2 + T0/2
S2= T2 + T0/2
6. SIMULATION MODEL PARAMETER
Specification of model. Refer Table 3.
Table 3. Model parameter and Specification
Inverter Power Supply 400 V DC
Induction Motor parameter
Stator Resistance 1.5ohm
Stator Inductance 0.0354 Henry
Rotor Resistance 0.5 ohm
Rotor Inductance 0.0354 Henry
Mutual Inductance 0.0104 Henry
Nominal Power 5.15 hp
Rated RMS Voltage 330±10 VOLTS
Rated Speed 1500 rpm
Pole 4
Slip 2%
Moment of Inertia 0.0488 Kg*m^2
Load Torque
(Step in Nature)
25 Nm
 ISSN: 2088-8694
IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224
222
7. SIMULINK MODEL AND WAVEFORM
Figure 4 shows the complete Simulink model of Close loop control of Induction Motor with
different different Inverter technique. Figure 5, 7, and 9 shows the Torque and Speed Characterstics with
respect to time and Figure 6, 8, and 10 shows the Stator current of the Induction Motor THD when SPWM,
THIPWM, and SVPWM technique is employed respectively.
Figure 4. Close loop Inverter with IM Load
Figure 5. Two level SPWM INVERTER Torque and
Speed
Figure 8. SPWM Stator current THD
Figure 6. Two level THIPWM INVERTER Torque
and Speed Figure 9. THIPWM Stator current THD
IJPEDS ISSN: 2088-8694 
Close Loop V/F control of VSI using SPWM, THIPWM and SVPWMM for IM(Sandeep Ojha)
223
Figure 7. Two level SVPWM INVERTER Torque
and Speed Figure 10. SVPWM Stator Current THD
8. RESULTS
Table 4 shows the Stator Current of Induction Motor THD with respect there techniques which are
employed. And the result shows the SVPWM technique has better waveform as compre to SPWM and
THIPWM.
Table 4. THD results
LEVEL TECHNIQUE LOAD THD%
TWO
SPWM IM 3.91
THIPWM IM 3.61
SVPWM IM 3.21
9. CONCLUSION
With the help of simulation result we can conclude that SVPWM (Space Vector Pulse Width
Modulation) technique is better than the THIPWM (Third Harmonic Injection Pulse Width Modulation)
technique and SPWM (Sinusoidal Pulse Width Modulation) technique. The THD of Stator current of
SVPWM Inverter is less so its industrial application is better than the THIPM Inverter and SPWM Inverter.
But the rise time of SVPWM Inverter is more as compare to THIPWM and SPWM Inverter that is 1.5 sec,
0.385sec and 0.4 sec simulation time respectively. The system is free from the PID controller. So the
controlling cost of the Induction Motor is cheap. We know that PID controller is 85% efficient. But this
Simulink model is 90-95% efficient.
REFERENCES
[1] Chimezie O. Adiuku, Abdul Rahiman Beig and Saikrishna Kanukollu, “Sensorless Closed Loop V/F control of
medium-Voltage High-Power Induction Motor with Synchronized Space Vector PWM”, IEEE 2015 PP 978-4799.
[2] Vijay Babu Koreboina, Shankar J Magajikondi and A.B. RAJU, “Modeling, Simulation and PC based
Implementation of a Cloed Loop Speed Control of VSI Fed Induction Motor Drive”, IEEE 2011 PP978-4244.
[3] Zulkifilie Bin Ibrahim, Md. Liton, Ismadi Bin Bugis, Nik Munaji Nik Mahadi and Ahmad Shukri, “Simulation
Investigation of SPWM, THIPWM and SVPWM Techniques for Three Phase Voltage Source Inverter”, IJPEDS,
Vol.4 No.2 pp.223-232.
[4] G.K. Dubey and C.R. Kasrabada, “Power Electronics and Drives”, IETE Book Series, Vol. 1, TM HILL P.C. Ltd.,
New Delhi, 1993.
[5] B.K. Bose, “Energy, environment and Advances in Power Electronics”, IEEE Trans. on P.E. Vol.15, No.4 JULY
2000.
[6] P.C. Sen, “thyristorised DC Drive”, New York: Wiley Interscience, 1981.
[7] P. Ramana, B. Santhosh Kumar, K. Alice Maryand M. Suraya Kalavathi, “Comparison of various PWM
Techniques for Field Oriented Control VSI fed PMSM Drive”, IJAREEIE, Vol. 2, Issue. 7, pp. 2928-2936.
[8] R. Kameswara Rao, P. Srinivas, M.V. Suresh Kumar, “Design and analysis of variousInverters using different
PWM Techniques”, IJES, ISSN€: 2319-1813 ISSN, (p): 2319-1805.
 ISSN: 2088-8694
IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224
224
[9] Raja Ram Kumar, Sunil Kumar, Alok Yadav, “Comparison of PWM Techniques and Inverter Performance”, IOSR
Journal of Electrical and Electronics Engineering (IOSR-JEEE), ISSN: 2278-1676, Vol 4, Issue 1 (Jan. – Feb.
2013), PP 18-22.
[10] DUBEY, G.K., Power Semiconductor Controlled Drives. Englewood Cliffs, NJ: Prentice Hall, 1989.
[11] DATTA, S.M. “Power Electronics & Control”. Reston, VA: Reston Publishing Co., Inc., 1985.
[12] Microsemi User Guide, “Field Oriented Control of Permanent Magnet Synchronous Motors (PMSM)”,
www.microsemi.com
[13] N. Mohan, T.M. Undeland, etal. “Power Converters, Applications and Design”, 3rd
edition, Johan Wiley and Sons,
New York, 2003.
[14] Bimal K. Bose, “Modern Power Electronics and AC Drives”, Prentice Hall, 2002.
[15] R. Krishnan, “Electric Motor Drives- Modeling, Analysis, and Control”, Prentice Hall, 2001.
[16] Muhammad H. Rashid, “Power Electronics Circuits, Devices, and Application”, Third Edition.
BIOGRAPHIES OF AUTHORS
Sandeep Ojhareceived the Bachelor of Technology in Electrical Engineering in 2013 from JSS
Academy of Technical Education Noida affiliated to Gautam Buddh Technical University,
Lucknow, Uttar Pradesh, India and currently pursuing Master of Technology in Power
Electronics and Drives from Madan Mohan Malaviya University of Technology, Gorakhpur,
Uttar Pradesh, India.
Ashok Kumar Pandey received the Bachelor of Engineering in Electrical Engineering in 1987
from Madan Mohan Malaviya University of Technology (Madan Mohan Malaviya Engineering
College) Gorakhpur, Uttar Pradesh, India and Master of Technology in Power Electronics,
Electrical Machines and Drives from Indian Institute of Technology Delhi, India in 1995 and
PhD. in Power Electronics, Electrical Machines and Drives from Indian Institute of Technology
Roorkee, India in 2003.

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Close Loop V/F Control of Voltage Source Inverter using Sinusoidal PWM, Third Harmonic Injection PWM and Space Vector PWM Method for Induction Motor

  • 1. International Journal of Power Electronics and Drive System (IJPEDS) Vol. 7, No. 1, March 2016, pp. 217~224 ISSN: 2088-8694  217 Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS Close Loop V/F Control of Voltage Source Inverter using Sinusoidal PWM, Third Harmonic Injection PWM and Space Vector PWM Method for Induction Motor Sandeep Ojha, Ashok Kumar Pandey Department of Electrical Engineering, Madan Mohan Malaviya University of Technology Gorakhpur, Uttar Pradesh, India Article Info ABSTRACT Article history: Received Oct 20, 2015 Revised Dec 21, 2015 Accepted Jan 15, 2016 The aim of this paper to presents a comparative analysis of Voltage Source Inverter using Sinusoidal Pulse Width Modulation Method, Third Harmonic Injection Pulse Width Modulation Method and Space Vector Pulse Width Modulation Two level inverter for Induction Motor. In this paper we have designed the Simulink model of Inverter for different technique. An above technique is used to reduce the Total Harmonic Distortion (THD) on the AC side of the Inverter. The Simulink model is close loop. Results are analyzed using Fast Fourier Transformation (FFT) which is for analysis of the Total Harmonic Distortion. All simulations are performed in the MATLAB Simulink / Simulink environment of MATLAB. Keyword: Induction motor Sinusoidal pulse width modulation Space vector pulse width modulation Third harmonic injection pulse width modulation Voltage source inverter Copyright © 2016 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Sandeep Ojha, PG Scholar Department of Electrical Engineering, Madan Mohan Malaviya University of Technology, Gorakhpur, Uttar Pradesh, India Email: ojha.sandeep89@gmail.com 1. INTRODUCTION A circuit which is used for converting DC power into an AC power at desired output Voltage and Frequency is known as an Inverter. A phase controlled converter, when it is used in inverter mode, are known as line-commutated Inverter, only line-commutated inverter requires at the output terminals an existing AC supply which is used for their commutation it means it required external circuit for commutation. A Force commutated Inverter gives an independent AC output voltage of adjustable Voltage and Frequency therefore its application is so vast. In an Inverter we require Forced commutation for thyristor, therefore we can use other self-commutating device like GTO, MOSFET, and other Transistors to avoiding the commutation circuit. But for high power application we must use thyristor along with the forced commutation circuit. There are major four techniques to reduce the Total Harmonic Distortion in Inverter: 1) Sinusoidal Pulse Width Modulation 2) Third Harmonic Injection Method 3) 60° Pulse modulation 4) Space Vector Pulse Width Modulation
  • 2.  ISSN: 2088-8694 IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224 218 2. TWO LEVEL INVERTER  In this level 180 degree mode each MOSFET conducts for 180° of a periodic cycle. Each phase has a pair S1, S4; S3, S6; S5, S2 and each trigger for 180° of time interval. And S1, S3, and S5 conduct at an interval of 120°. Refer to Figure 1. 0° 60° 120° 180° 240° 300° 360° S1 S3 S5 S6 S2 S4 S6 Figure 1. Switching period of MOSFET Specification of each MOSFET 180° mode VSI. Refer to Table 1. Table 1. For 50 Hz frequency Pulse Generator where amplitude = 230*1.414 and pulse width 50% S1 Phase Delay = 0 msec S4 Phase Delay = 10 msec S3 Phase Delay = 6.667 msec S6 Phase Delay = 16.667 msec S5 Phase Delay = 13.33 msec S2 Phase Delay = 23.33 msec / - 0.0033 sec 3. SINUSOIDAL PULSE WIDTH MODULATION (SPWM) This technique is very useful for reducing the Total Harmonic Distortion (THD). This technique is characterized by the constant amplitude pulse. And the width of these pulses is modulated to get Inverter output Voltage control and to reduce its harmonic content in the voltage. Force commutation is essential for the pulse width modulation technique. The Switching sequences and topology of the Inverter is same as normal level of Inverter. In this technique the Gate pulses of each MOSFET is modulated and control the Switching of MOSFET to get the desired output voltage at desired frequency for input voltage of Induction motor. Fourier analysis of the voltage waveform and get the output voltage of an Inverter. V(t)= A0 + 2* ∑ ∗ ∗ ] (i) The output voltage wave is odd symmetry. So, A0 and Ak is zero because it has an even symmetry. So, Bk= (2/π)*[ ∗ sin ] =((4*Vs)/(nπ))*[sin(nπ/2)*sin(nd)] (1) V0= ∑ ∗ sin ∗ sin ∗ sin , , … ) (2) nd is made equal to π. So, d= (π/n) So, the pulse width is made 2d so it is equal to (2d/n). In the Simulink model sine wave frequency is 50 Hz and the amplitude of the sine wave is 230*1.414 and carrier frequency is sinusoidal with frequency is 10000 Hz. For a close loop we take the speed as a feedback and compare to the reference speed and then the speed error again added with the rotor speed and its output is change into the Gate Pulse of the MOSFET. 4. THIRD HARMONIC INJECTION PULSE WIDTH MODULATION METHOD (THIM) This method is also a very useful method for eliminating the harmonic in the system which comes due to the presence of power electronic switches. In this method we inject the third harmonic in the system
  • 3. IJPEDS ISSN: 2088-8694  Close Loop V/F control of VSI using SPWM, THIPWM and SVPWMM for IM(Sandeep Ojha) 219 and control the pulse of the each MOSFET to get the harmonic free inverter output voltage. Now to find the amplitude of the third harmonic of unknown amplitude of the third harmonic component. So let us take simple sine wave with the third harmonic sine wave of unknown amplitude x. Y (α) = sin (α) + x*sin (3α) (3) For finding the maximum value of the function d/dα (Y (α)) =0 Which gives, α=cos-1 9 1 / 12 (4) From equation (3) and (4) F(x)=Y(α)=[(3x+1)( 3 1 / 12 – 4x 3 1 / 12. ] (5) For finding the maximum value of equation (5) using formula d/dx (F(x)) So we get x = -0.334, 0.1667 At x = -0.334 d2 /dx2 (F(x)) = 0 At x = 0.1667 d2 /dx2 (F(x)) = 10.3923 Which shows the given function is minimum. At x = 0.1667 and the value of α is 60° Now putting the value of α at x = 0.1667 d2 /dx2 (Y (α)) = -2 This shows the function Y (α) is maximum at x = 0.1667 and the value of α is 60° So this is clear that the third harmonic should be 0.1667 of this amplitude Now putting the value of x= 0.1667 and α= 60° in equation (4) Which gives Y (α) =0.866025 which is the peak of resultant waveform with third harmonic. And the modulation factor of 1/0.866025 is 1.15470053 giving 15.47% more DC utilization. 120° 120° (6) Where, V is Instantaneous maximum Magnitude of fundamental And α is instantaneous phase of fundamental The above results give the information about the amplitude of the output phase voltage is 1.15 times of the normal output phase voltage. In the Simulink model sine wave frequency is 50 Hz and the amplitude of the sine wave is 230*1.414 and carrier frequency is sinusoidal with frequency is 10000 Hz. And additional sine wave is added to add the third harmonic in the Inverter whose sine wave amplitude is 230*1.414/6 and its frequency is 3 times of rated frequency. For a close loop we take the speed as a feedback and compare to the reference speed and then the speed error again added with the rotor speed and its output is change into the Gate Pulse of the MOSFET. 5. SPACE VECTOR PULSE WIDTH MODULATION (SVPWM) This technique is very useful for reducing the Total Harmonic Distortion. This technique is characterized by the constant amplitude pulse. And the width of these pulse is modulated to get Inverter output Voltage control and to reduce its harmonic content. The topology of three leg Voltage Source Inverter because of the constraint that the input line must never be shored and the output current must be always be continuous a Voltage Source Inverter can assume only eight distinct sectors. Six out of these eight sectors produces a non-zero output voltage and are known as non-zero switiching states and the remaining two sectors produces zero voltage are known as zero switching states.
  • 4.  ISSN: 2088-8694 IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224 220 The SVPWM can be implemented by using wither sector selection algorithm or by using a carrier based space vector algorithm. The types of SVPWM implementations are: a) Sector selection b) Reduced switching c) Carrier based d) Reduced switching carrier based  Sector selection of SVPWM : - Step1. Determine Vd, Vq, Vref, and angle µ Step2. Determine time duration T1, T2, T0 Step3. Determine the switching time of each IGBT (S1 to S6) For Step 1, Refer Figure 2 Figure 2. Vd, Vq, Vref, and µ can determine Vd=Van–0.5*Vbn-0.5*Vcn (7) Vq=0+0.866*Vbn–0.866*Vcn (8) Vref= Vd 2 + Vq 2 ) (9) µ = tan-1 (Vq/Vd) = wt=2πft (10) For Step 2, Refer Figure 3 which shows the switching time during a sector1 Figure 3. Reference vector as a combination of adjacent vectors at sector Switching time duration at sector 1 = 1 + 2 + 0 (11)
  • 5. IJPEDS ISSN: 2088-8694  Close Loop V/F control of VSI using SPWM, THIPWM and SVPWMM for IM(Sandeep Ojha) 221 Tt*Vref = (T1 *V1 + T2* V2) (12) Tt* |Vref|* cos (µ) = T1* 2/3*Vdc + V2*2/3 *cos (π/3) (13) Tt*|Vref|*cos (µ) = V2*0.667*sin(π/3) (14) Where, (0 <= µ <= 60º) T1 = Tt*µ*(sin (π/3-µ) / sin (π/3)) (15) T2 = Tt*µ*(sin (µ) / sin (π/3)) (16) T0 = Tt – (T1 + T2) (17) Where, Tt = 1/ft and µ= |Vref| / (0.667*Vdc) For step 3 refer Table 2 Table 2. Switching Time Calculation at Each sector Sector Upper Switches (S1, S3, S5) Lower Switches (S4, S6, S2) 1 S1=T1 + T2 + T0/2 S3= T2 + T0/2 S5= T0/2 S4= T0/2 S6= T1 + T0/2 S2= T1 + T2 + T0/2 2 S1= T1 + T0/2 S3= T1 + T2 + T0/2 S5= T0/2 S4= T2 + T0/2 S6= T0/2 S2= T1 + T2 + T0/2 3 S1= T0/2 S3= T1 + T2 + T0/2 S5= T2 + T0/2 S4= T1 + T2 + T0/2 S6= T0/2 S2= T1 + T0/2 4 S1= T0/2 S3= T1 + T0/2 S5= T1 + T2 + T0/2 S4= T1 + T2 + T0/2 S6= T2 + T0/2 S2= T0/2 5 S1= T2 + T0/2 S3= T0/2 S5= T1 + T2 + T0/2 S4= T1 + T0/2 S6= T1 + T2 + T0/2 S2= T0/2 6 S1= T1 + T2 + T0/2 S3= T0/2 S5= T1 + T0/2 S4= T0/2 S6= T1 + T2 + T0/2 S2= T2 + T0/2 6. SIMULATION MODEL PARAMETER Specification of model. Refer Table 3. Table 3. Model parameter and Specification Inverter Power Supply 400 V DC Induction Motor parameter Stator Resistance 1.5ohm Stator Inductance 0.0354 Henry Rotor Resistance 0.5 ohm Rotor Inductance 0.0354 Henry Mutual Inductance 0.0104 Henry Nominal Power 5.15 hp Rated RMS Voltage 330±10 VOLTS Rated Speed 1500 rpm Pole 4 Slip 2% Moment of Inertia 0.0488 Kg*m^2 Load Torque (Step in Nature) 25 Nm
  • 6.  ISSN: 2088-8694 IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224 222 7. SIMULINK MODEL AND WAVEFORM Figure 4 shows the complete Simulink model of Close loop control of Induction Motor with different different Inverter technique. Figure 5, 7, and 9 shows the Torque and Speed Characterstics with respect to time and Figure 6, 8, and 10 shows the Stator current of the Induction Motor THD when SPWM, THIPWM, and SVPWM technique is employed respectively. Figure 4. Close loop Inverter with IM Load Figure 5. Two level SPWM INVERTER Torque and Speed Figure 8. SPWM Stator current THD Figure 6. Two level THIPWM INVERTER Torque and Speed Figure 9. THIPWM Stator current THD
  • 7. IJPEDS ISSN: 2088-8694  Close Loop V/F control of VSI using SPWM, THIPWM and SVPWMM for IM(Sandeep Ojha) 223 Figure 7. Two level SVPWM INVERTER Torque and Speed Figure 10. SVPWM Stator Current THD 8. RESULTS Table 4 shows the Stator Current of Induction Motor THD with respect there techniques which are employed. And the result shows the SVPWM technique has better waveform as compre to SPWM and THIPWM. Table 4. THD results LEVEL TECHNIQUE LOAD THD% TWO SPWM IM 3.91 THIPWM IM 3.61 SVPWM IM 3.21 9. CONCLUSION With the help of simulation result we can conclude that SVPWM (Space Vector Pulse Width Modulation) technique is better than the THIPWM (Third Harmonic Injection Pulse Width Modulation) technique and SPWM (Sinusoidal Pulse Width Modulation) technique. The THD of Stator current of SVPWM Inverter is less so its industrial application is better than the THIPM Inverter and SPWM Inverter. But the rise time of SVPWM Inverter is more as compare to THIPWM and SPWM Inverter that is 1.5 sec, 0.385sec and 0.4 sec simulation time respectively. The system is free from the PID controller. So the controlling cost of the Induction Motor is cheap. We know that PID controller is 85% efficient. But this Simulink model is 90-95% efficient. REFERENCES [1] Chimezie O. Adiuku, Abdul Rahiman Beig and Saikrishna Kanukollu, “Sensorless Closed Loop V/F control of medium-Voltage High-Power Induction Motor with Synchronized Space Vector PWM”, IEEE 2015 PP 978-4799. [2] Vijay Babu Koreboina, Shankar J Magajikondi and A.B. RAJU, “Modeling, Simulation and PC based Implementation of a Cloed Loop Speed Control of VSI Fed Induction Motor Drive”, IEEE 2011 PP978-4244. [3] Zulkifilie Bin Ibrahim, Md. Liton, Ismadi Bin Bugis, Nik Munaji Nik Mahadi and Ahmad Shukri, “Simulation Investigation of SPWM, THIPWM and SVPWM Techniques for Three Phase Voltage Source Inverter”, IJPEDS, Vol.4 No.2 pp.223-232. [4] G.K. Dubey and C.R. Kasrabada, “Power Electronics and Drives”, IETE Book Series, Vol. 1, TM HILL P.C. Ltd., New Delhi, 1993. [5] B.K. Bose, “Energy, environment and Advances in Power Electronics”, IEEE Trans. on P.E. Vol.15, No.4 JULY 2000. [6] P.C. Sen, “thyristorised DC Drive”, New York: Wiley Interscience, 1981. [7] P. Ramana, B. Santhosh Kumar, K. Alice Maryand M. Suraya Kalavathi, “Comparison of various PWM Techniques for Field Oriented Control VSI fed PMSM Drive”, IJAREEIE, Vol. 2, Issue. 7, pp. 2928-2936. [8] R. Kameswara Rao, P. Srinivas, M.V. Suresh Kumar, “Design and analysis of variousInverters using different PWM Techniques”, IJES, ISSN€: 2319-1813 ISSN, (p): 2319-1805.
  • 8.  ISSN: 2088-8694 IJPEDS Vol. 7, No. 1, March 2016 : 217 – 224 224 [9] Raja Ram Kumar, Sunil Kumar, Alok Yadav, “Comparison of PWM Techniques and Inverter Performance”, IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE), ISSN: 2278-1676, Vol 4, Issue 1 (Jan. – Feb. 2013), PP 18-22. [10] DUBEY, G.K., Power Semiconductor Controlled Drives. Englewood Cliffs, NJ: Prentice Hall, 1989. [11] DATTA, S.M. “Power Electronics & Control”. Reston, VA: Reston Publishing Co., Inc., 1985. [12] Microsemi User Guide, “Field Oriented Control of Permanent Magnet Synchronous Motors (PMSM)”, www.microsemi.com [13] N. Mohan, T.M. Undeland, etal. “Power Converters, Applications and Design”, 3rd edition, Johan Wiley and Sons, New York, 2003. [14] Bimal K. Bose, “Modern Power Electronics and AC Drives”, Prentice Hall, 2002. [15] R. Krishnan, “Electric Motor Drives- Modeling, Analysis, and Control”, Prentice Hall, 2001. [16] Muhammad H. Rashid, “Power Electronics Circuits, Devices, and Application”, Third Edition. BIOGRAPHIES OF AUTHORS Sandeep Ojhareceived the Bachelor of Technology in Electrical Engineering in 2013 from JSS Academy of Technical Education Noida affiliated to Gautam Buddh Technical University, Lucknow, Uttar Pradesh, India and currently pursuing Master of Technology in Power Electronics and Drives from Madan Mohan Malaviya University of Technology, Gorakhpur, Uttar Pradesh, India. Ashok Kumar Pandey received the Bachelor of Engineering in Electrical Engineering in 1987 from Madan Mohan Malaviya University of Technology (Madan Mohan Malaviya Engineering College) Gorakhpur, Uttar Pradesh, India and Master of Technology in Power Electronics, Electrical Machines and Drives from Indian Institute of Technology Delhi, India in 1995 and PhD. in Power Electronics, Electrical Machines and Drives from Indian Institute of Technology Roorkee, India in 2003.