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N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 102 | P a g e
Space Vector Based Generalized Dpwm Algorithms for Vsi Fed
Induction Motor Drive
N. Praveena1
, G. Satheesh2
, R. Ram Prasad3
1
M.Tech, Department of EEE, G.Pulla Reddy Engineering College, Kurnool, A.P, INDIA
2
Assistant Professor E.E.E Department, G. Pulla Reddy Engineering CollegeKurnool, A.P, INDIA
3
Assistant Professor E. E.E Department, NBKRIST, Vakadu, Nellore, A.P, INDIA
Abstract:
This paper presents Space Vector based Generalized DiscontinuousPulse width modulation (GDPWM)
algorithms for VSI fed Induction motor drive. To avoid the complexity due to angle calculation and sector
identification involved in Conventional space vector pulse width modulation (CSVPWM). The Proposed
algorithms use the concept of Imaginary Switching times and a constant variable µ and modulation phase angle
δ are used to generate modulating waveforms.The proposed algorithms results in reduced current ripple over
CSVPWM. To validate the proposed methods, simulation is carried on V/f controlled Induction Motor drive in
MATLAB/SIMULINK environment and the results are discussed.
Keywords-CSVPWM, GDPWM, Imaginary Switching times, Induction motor, V/f control
I. INTRODUCTION
Improvements in fast switching power
devices have led to an increased interest in voltage
source inverters (VSI) with pulse width modulation
(PWM) control. Out of several approaches, triangular
comparison (TC) approach and space vector (SV)
approach are main implementation techniques. The
space vector approach offers additional degrees of
freedom indesigning PWM techniques over the
triangle-comparison methods. The conventional
SVPWM algorithm employs equal division of zero
voltage vector times within a sampling period or sub
cycle [1, 2]. In this method the reference voltage
vector is synthesized by time averaging two active
states and two zero states in every sampling period
[3]. However, the CSVPWM is known as continuous
PWM (CPWM)method in this switching loss is high.
Hence to reduce the switching losses and to improve
the performance several discontinuous PWM
(DPWM)methods have been reported [3-9]. If the
zero sequence signals are continuous it produces
CPWM scheme and if it is discontinuous it results in
DPWM schemes. A carrier based generalized PWM
method comprising of all DPWM methods is
considered as generalized discontinuous PWM
scheme (GDPWM)[3][4][5].
The conventional space vector pulse width
modulation sector identification and switching
sequences are discussed in [10].CSVPWM suffers
from the drawbacks like computational burden and it
takes more time to execute. Hence the complexity
involved in CSVPWM is more. To reduce the
complexity involved in CSVPWM algorithm, a
simplified approach is developed in [6-9] by using
the concept of imaginary switching times.
This paper presents Space Vector based Generalized
Discontinuous Pulse width modulation (GDPWM)
algorithms for VSI fed Induction motor drive using
the concept of imaginary switching times.
II. PROPOSED SPACE VECTOR
BASED GENERALIZED
DISCONTINUOUS PWM
ALGORITHMS
SVPWM is a continuous PWM (CPWM)
method where Discontinuous SVPWM results when
one of the two zero vector is not used in the
implementation of the SVPWM. One leg of the
inverter does not switch during the whole switching
period and remains tied to either the positive or
negative DC bus .This is known as Discontinuous
SVPWM, since the switching is not continuous. Due
to the manipulation of the Zero Space vector
application in a Switching period one branch of the
inverter remains un-modulated during one Switching
interval. Switching takes place in two branches: one
branch either to the positive DC bus or the negative
DC bus, [when zero voltage [000] is eliminated the
leg voltage is tied to the positive DC bus 0.5Vdc or
when zero voltage [111] is eliminated the leg voltage
is tied to the negative bus voltage 0.5Vdc]. The
number of switching’s thus reduced to two- thirds
compared to the continuous SVPWM and hence
switching losses are reduced significantly. Moreover,
complexity involved in conventional SVPWM is
more. To avoid the complexity due to angle
calculation and sector identification involved in
CSVPWM. The Proposed GDPWM algorithms use
the concept of Imaginary Switching times. The
imaginary switching time periods are proportional to
RESEARCH ARTICLE OPEN ACCESS
N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 103 | P a g e
the instantaneous values of the reference phase
voltages are defined as
(5)
(6)
(7)
Where is the sampling time
is the dc link voltage
are the Phase voltage
To calculate the active vector switching
times, the maximum and minimum values of
imaginary switching times are calculated in every
sampling time
(8)
(9)
To generate the actual gating signals for
inverter, the actual switching times for each inverter
leg can be obtained by the time shifting operation as
follows:
(10)
(11)
(12)
Where
(13)
In the proposed method µ can be defined as
(14)
Where is the angular frequency of the reference
voltage.
‘ is the sign function, where
‘δ’ is the modulation phase angle
When µ=0.5, µ=0 andµ= 1 the CSVPWM,
DPWMMAX and DPWMMIN algorithms can be
obtained. Similarly, the variation of modulation
phase angle δ yields to infinite number of DPWM
methods. If δ = -π/3, π/6, 0, - π/6 then DPWM0,
DPWM1, DPWM2 and DPWM3 can be obtained
respectively. Thus by varying µ and δ the switching
time periods of zero voltage vectors can be changed
and so thatdifferent DPWM sequences can be
obtained.
The modulating waveforms of different
DPWM sequences and CSVPWM are as shown in
Fig 1. DPWM sequences are obtained based on their
clamping sequences. In DPWMMAX method, the
clamping of 120o
takes place at the middle of 0o
-180o
for every 360o
of fundamental voltage. In
DPWMMIN
CSVPWM
DPWMMAX
DPWMMIN
DPWM0
DPWM1
DPWM2
DPWM3
Figure-1Modulating waveforms of different
sequences
method, the clamping of 120 takes place at the
middle of 180o
– 360o
for every 360o
of fundamental
voltage.
In DPWM0 method, the clamping of 60
takes place at the end of 0 for every 180 of
N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 104 | P a g e
fundamental voltage. Another well known method
DPWM1, the clamping of 60 takes place at the
middle 0 180 for every 180 of fundamental
voltage. InDPWM2 method, the clamping of 60
takes place at the start of 90 -180 for every 180 of
fundamental voltage. Another acceptedmethod
DPWM3 clamps every phase during the middle 30
for every 90 of its fundamental voltage.
Block diagram representation of Generalized
DPWM sequences for V/f control induction motor
drive
Figure-2 Block diagram of GDPWM sequences
forV/f control induction motor drive
III. MODELING OF INDUCTION
MOTOR
The most popular method of Speed control
is V/f control method. The Flux and Torque are also
function of frequency and voltage respectively.Speed
is varied by varying the frequency; maintain V/f
constant to avoid saturation of flux. With constant V/f
ratio, motor develops a constant maximum torque.
Among the various reference frames, V/f control
method uses the stationary reference frame. Hence,
the induction motor model is developed in the
stationary reference frame, which is also known as
Stanley reference frame.
The stator and rotor voltage and flux
linkages in the stator reference frame are defined as
(15)
(16)
(17)
(18)
(19)
(20)
(21)
(22)
The electromagnetic torque of the induction motor in
stator reference frame is given by
(23)
The electro-mechanical equation of the induction
motor drive is given by
(24)
IV. SIMULATION RESULTS
To validate Space Vector Based GDPWM
Algorithms for Inverter fed Induction Motor Drive.
Simulation test can be done using Matlab/Simulink
model. The parameters used for simulation and
output results will be given below
The induction motor used in this case study
is a 4 KW, 1470 rpm, 4-pole, 3-phase induction
motor having the following parameters:
Parameter value
Stator Resistance (Rs) 7.83 Ω
Rotor Resistance (Rr) 7.55 Ω
Magnetizing Inductance (Lm) 0.4535 H
Stator Self Inductance (Ls) 0.475 H
Rotor Self Inductance (Lr) 0.475 H
Moment of inertia (J) 0.06 Kg-m2
Table-1 parameters of Induction motor
The total harmonic distortion (THD) of the
no-load current is used as the performance indices for
proposed PWM Techniques. The line current
waveforms at no-load and harmonic spectra for
CSVPWM and some popular DPWM methods for
supply frequency 50Hz are as shown.
4.1 STARTING TRANSIENT RESULTS
The simulation results of starting transients
of proposed drive are shown in Fig 3 (3.1-3.7).The
output voltage waveform is similar to all sequences.
The dc voltage considered for inverter is 600V and
the output voltage obtained at the inverter is
=400V as shown in fig.3.
Initially when the motor is started due to
large inertia in the rotor it posses large amount of
torque so it takes large amount of current which is
observed from Fig 3.
From Fig 3 (3.1-3.7) it can be observed that
upto 0.8sec the starting transients are shown during
this period the speed starts from 0 rpm and reaches
nearly 1500rpm, that means at the time of steady
state it satisfies and before reaches to the steady
state the current waveform gradually reduce and
reaches to the min value of the current less than 4
amps in steady state.
Vdc
GDPWM
Pulses
V/F
Control
Inverter Induction
motor
N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 105 | P a g e
Figure3.1 Starting transients of continuous SVPWM
Figure3.2 Starting transients of DPWMMIN
Figure3.3 Starting transients of DPWMMAX
Figure3.4 Starting transients of DPWM0
N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 106 | P a g e
Figure3.5 Starting transients of DPWM1
Figure3.6 Starting transients of DPWM2
Figure3.7 Starting transients of DPWM3
Figure-3(3.1-3.7) are results of starting transients
of proposed GDPWM drive
4.2 STEADY STATE RESULTS
The simulation results of steady state
transients of proposed drive are shown in Fig 4 (4.1-
4.7). In steady state period the speed reaches
1500rpm. After 0.8 sec the torque reaches zero and
current reaches minimum value this minimum value
current appears because of steady state/no load effect.
Figure4.1 Steady state transients of continuous
SVPWM
N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 107 | P a g e
Figure4.2 Steady state results of DPWMMIN
Figure4.3 Steady state transients of DPWMMAX
Figure4.4 Steady state transients of DPWM0
Figure4.5 Steady state transients of DPWM1
Figure4.6 Steady state transients of DPWM2
Figure4.7 Steady state transients of DPWM3
Figure-4(4.1-4.7) are steady state results of
proposed GDPWM drive
N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 108 | P a g e
4.3 TOTAL HARMONIC DISTORTION OF NO-
LOAD CURRENT FOR INVERTER FED
INDUCTION MOTOR
Figure5.1 THD of Continuous SVPWM
Figure5.2 THD of DPWMMIN
Figure5.3 THD of DPWMMAX
Figure5.4 THD of DPWM0
Figure5.5 THD of DPWM1
Figure5.6 THD of DPWM2
Figure5.7 THD of DPWM3
Figure 5 (5.1-5.7) are the total harmonic distortion
of different sequences
The total harmonic distortion of current in
CSVPWM is more compared to the DPWM
sequences. These THDs are calculated during the
steady state period.
Table-2 comparison of %THD of different PWM
sequences
S.NO SEQUENCES %THD
1 CSVPWM 7.39
2 DPWMMIN 6.08
3 DPWMMAX 6.05
4 DPWM0 6.28
5 DPWM1 6.72
6 DPWM2 6.44
7 DPWM3 5.99
V. CONCLUSIONS
The proposed space vector based
generalized discontinuous PWM algorithms uses the
concept of imaginary switching times.To avoid the
complexity due to angle calculation and sector
identification involved in Conventional
SVPWM.Also the execution time and memory
required is reduced by eliminating the angle and
sector estimation.
From the simulation results ofV/f control of
induction motor drive are discussed here. The total
harmonic distortions of the motor phase current in
Continuous SVPWM are more compared to the
generalized DPWM sequences. The Total THD
values for the proposed GDPWM algorithms are
N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109
www.ijera.com 109 | P a g e
listed. It is observed that there is a gradual decrement
of the %THD in motor phase currents. Hence DPWM
sequences give better performance.The simulation
results show the validity of the proposed algorithm.
REFERENCES
[1] G.Narayanan, “Space vector based hybrid
PWM Techniques for reduced current
ripple,”IEEE, Trans, vol 55, No 4,april
2008.
[2] G.Narayanan and V. T. Ranganathan,
“Analytical evaluation of harmonic
distortion in PWM AC drives using the
notion of stator flux ripple,” IEEE Trans.
Power Electronics., vol. 20, no. 2, pp. 466–
474, Mar. 2005.
[3] K. Sri Gowri,”High-Performance
Generalized ADPWM Algorithm for VSI
Fed IM Drives for Reduced Switching
Losses.”International Journal of Recent
Trends in Engineering, Vol 2, No. 5,
November 2009
[4] AhmetM.hava and Thomas “Simple
Analytical and Graphical Methods for
Carrier- based PWM-VSI Drives”, IEEE
Trans on power electronics vol14 no1 jan
1999
[5] N.Ravisankar Reddy and T. Brahmananda
Reddy “Simplified Space Vector Based
Hybrid PWM Algorithm for Reduced
CurrentRipple”,International Journal of
Recent Trends in Engineering, Vol 2, No. 5,
November 2009
[6] Advanced Bus-Clamping PWM Techniques
Based on Space Vector
Approach.G.Narayanan, Member, IEEE,
Harish K. Krishnamurthy, Di Zhao, and
RajapandianAyyanar, Member, IEEE,2006.
[7] J.Holtz, ―Pulse width modulation for
electronic power conversion, Proc. IEEE,
vol82, no. 8, pp. 1194–1214, Aug. 1994.
[8] K. Sri Gowri, T.Brahmanada Reddy, Ch.
SaiBabu, “Switching Loss Characteristics of
Advanced DPWM Methods Using Space
Vector Based Double Switching Clamping
Sequences,” Proc. ISIEA’09, Kuala Lumpur,
Malaysia, in press.
[9] K. Zhou and D.Wang, “Relationship
between space-vector modulation and three-
phase carrier-based PWM: A comprehensive
analysis,” IEEE Trans Ind. Electron., vol.
49, no. 1, pp. 186–196, Feb. 2002
[10] N.Praveena , G.Satheesh ,
R.Ramprasad“Space Vector Based PWM
Algorithms to ReduceCurrent Ripple for an
Induction Motor Drive ,”International
Journal of Advanced Scientific and
Technical Research, Volume 3, pp 528- 540,
Feb 2013
N.PRAVEENA received B.Tech degree in Electrical
and Electronics Engineeringfrom G.Pullaiah college
of Engineeringand Technology, JNTUA, Anantapur
in the year 2011. She is currently pursuing M.Tech
in G. Pulla- Reddy Engineering College, Kurnool.
Her research interests include Power electronic
controllers, PWM techniques, Electrical Drives.
G.SATHEESH was born in 1979. He graduated
from Bangalore University, Bangalore inthe year
2001. He received M.Tech degree from J.N.T
University, Anantapur, India in the year 2004. He is
presently Assistant Professor in the Electrical and
Electronics EngineeringDepartment, G. Pulla Reddy
Engineering College, Kurnool, India. He is currently
pursuingPh.D. in Electrical Engineering Department,
JNTU, Kakinada.
His areas of interest include Power
electronics, pulse width modulation techniques, AC
Drives and Control.
R.RamPrasad,graduated from Bangalore University,
Bangalore in the year 2002. He received M.Tech
degree from Sri Venkateswara University, Tirupati,
India in the year 2007. He is presently Assistant
Professor in the Electrical and Electronics
Engineering Department, NBKRIST, Vidya Nagar,
Nellore, India.
His areas of interest include Multi Level Inverters,
Harmonic Reduction Techniques Power System
Operation and Control.

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S35102109

  • 1. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 102 | P a g e Space Vector Based Generalized Dpwm Algorithms for Vsi Fed Induction Motor Drive N. Praveena1 , G. Satheesh2 , R. Ram Prasad3 1 M.Tech, Department of EEE, G.Pulla Reddy Engineering College, Kurnool, A.P, INDIA 2 Assistant Professor E.E.E Department, G. Pulla Reddy Engineering CollegeKurnool, A.P, INDIA 3 Assistant Professor E. E.E Department, NBKRIST, Vakadu, Nellore, A.P, INDIA Abstract: This paper presents Space Vector based Generalized DiscontinuousPulse width modulation (GDPWM) algorithms for VSI fed Induction motor drive. To avoid the complexity due to angle calculation and sector identification involved in Conventional space vector pulse width modulation (CSVPWM). The Proposed algorithms use the concept of Imaginary Switching times and a constant variable µ and modulation phase angle δ are used to generate modulating waveforms.The proposed algorithms results in reduced current ripple over CSVPWM. To validate the proposed methods, simulation is carried on V/f controlled Induction Motor drive in MATLAB/SIMULINK environment and the results are discussed. Keywords-CSVPWM, GDPWM, Imaginary Switching times, Induction motor, V/f control I. INTRODUCTION Improvements in fast switching power devices have led to an increased interest in voltage source inverters (VSI) with pulse width modulation (PWM) control. Out of several approaches, triangular comparison (TC) approach and space vector (SV) approach are main implementation techniques. The space vector approach offers additional degrees of freedom indesigning PWM techniques over the triangle-comparison methods. The conventional SVPWM algorithm employs equal division of zero voltage vector times within a sampling period or sub cycle [1, 2]. In this method the reference voltage vector is synthesized by time averaging two active states and two zero states in every sampling period [3]. However, the CSVPWM is known as continuous PWM (CPWM)method in this switching loss is high. Hence to reduce the switching losses and to improve the performance several discontinuous PWM (DPWM)methods have been reported [3-9]. If the zero sequence signals are continuous it produces CPWM scheme and if it is discontinuous it results in DPWM schemes. A carrier based generalized PWM method comprising of all DPWM methods is considered as generalized discontinuous PWM scheme (GDPWM)[3][4][5]. The conventional space vector pulse width modulation sector identification and switching sequences are discussed in [10].CSVPWM suffers from the drawbacks like computational burden and it takes more time to execute. Hence the complexity involved in CSVPWM is more. To reduce the complexity involved in CSVPWM algorithm, a simplified approach is developed in [6-9] by using the concept of imaginary switching times. This paper presents Space Vector based Generalized Discontinuous Pulse width modulation (GDPWM) algorithms for VSI fed Induction motor drive using the concept of imaginary switching times. II. PROPOSED SPACE VECTOR BASED GENERALIZED DISCONTINUOUS PWM ALGORITHMS SVPWM is a continuous PWM (CPWM) method where Discontinuous SVPWM results when one of the two zero vector is not used in the implementation of the SVPWM. One leg of the inverter does not switch during the whole switching period and remains tied to either the positive or negative DC bus .This is known as Discontinuous SVPWM, since the switching is not continuous. Due to the manipulation of the Zero Space vector application in a Switching period one branch of the inverter remains un-modulated during one Switching interval. Switching takes place in two branches: one branch either to the positive DC bus or the negative DC bus, [when zero voltage [000] is eliminated the leg voltage is tied to the positive DC bus 0.5Vdc or when zero voltage [111] is eliminated the leg voltage is tied to the negative bus voltage 0.5Vdc]. The number of switching’s thus reduced to two- thirds compared to the continuous SVPWM and hence switching losses are reduced significantly. Moreover, complexity involved in conventional SVPWM is more. To avoid the complexity due to angle calculation and sector identification involved in CSVPWM. The Proposed GDPWM algorithms use the concept of Imaginary Switching times. The imaginary switching time periods are proportional to RESEARCH ARTICLE OPEN ACCESS
  • 2. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 103 | P a g e the instantaneous values of the reference phase voltages are defined as (5) (6) (7) Where is the sampling time is the dc link voltage are the Phase voltage To calculate the active vector switching times, the maximum and minimum values of imaginary switching times are calculated in every sampling time (8) (9) To generate the actual gating signals for inverter, the actual switching times for each inverter leg can be obtained by the time shifting operation as follows: (10) (11) (12) Where (13) In the proposed method µ can be defined as (14) Where is the angular frequency of the reference voltage. ‘ is the sign function, where ‘δ’ is the modulation phase angle When µ=0.5, µ=0 andµ= 1 the CSVPWM, DPWMMAX and DPWMMIN algorithms can be obtained. Similarly, the variation of modulation phase angle δ yields to infinite number of DPWM methods. If δ = -π/3, π/6, 0, - π/6 then DPWM0, DPWM1, DPWM2 and DPWM3 can be obtained respectively. Thus by varying µ and δ the switching time periods of zero voltage vectors can be changed and so thatdifferent DPWM sequences can be obtained. The modulating waveforms of different DPWM sequences and CSVPWM are as shown in Fig 1. DPWM sequences are obtained based on their clamping sequences. In DPWMMAX method, the clamping of 120o takes place at the middle of 0o -180o for every 360o of fundamental voltage. In DPWMMIN CSVPWM DPWMMAX DPWMMIN DPWM0 DPWM1 DPWM2 DPWM3 Figure-1Modulating waveforms of different sequences method, the clamping of 120 takes place at the middle of 180o – 360o for every 360o of fundamental voltage. In DPWM0 method, the clamping of 60 takes place at the end of 0 for every 180 of
  • 3. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 104 | P a g e fundamental voltage. Another well known method DPWM1, the clamping of 60 takes place at the middle 0 180 for every 180 of fundamental voltage. InDPWM2 method, the clamping of 60 takes place at the start of 90 -180 for every 180 of fundamental voltage. Another acceptedmethod DPWM3 clamps every phase during the middle 30 for every 90 of its fundamental voltage. Block diagram representation of Generalized DPWM sequences for V/f control induction motor drive Figure-2 Block diagram of GDPWM sequences forV/f control induction motor drive III. MODELING OF INDUCTION MOTOR The most popular method of Speed control is V/f control method. The Flux and Torque are also function of frequency and voltage respectively.Speed is varied by varying the frequency; maintain V/f constant to avoid saturation of flux. With constant V/f ratio, motor develops a constant maximum torque. Among the various reference frames, V/f control method uses the stationary reference frame. Hence, the induction motor model is developed in the stationary reference frame, which is also known as Stanley reference frame. The stator and rotor voltage and flux linkages in the stator reference frame are defined as (15) (16) (17) (18) (19) (20) (21) (22) The electromagnetic torque of the induction motor in stator reference frame is given by (23) The electro-mechanical equation of the induction motor drive is given by (24) IV. SIMULATION RESULTS To validate Space Vector Based GDPWM Algorithms for Inverter fed Induction Motor Drive. Simulation test can be done using Matlab/Simulink model. The parameters used for simulation and output results will be given below The induction motor used in this case study is a 4 KW, 1470 rpm, 4-pole, 3-phase induction motor having the following parameters: Parameter value Stator Resistance (Rs) 7.83 Ω Rotor Resistance (Rr) 7.55 Ω Magnetizing Inductance (Lm) 0.4535 H Stator Self Inductance (Ls) 0.475 H Rotor Self Inductance (Lr) 0.475 H Moment of inertia (J) 0.06 Kg-m2 Table-1 parameters of Induction motor The total harmonic distortion (THD) of the no-load current is used as the performance indices for proposed PWM Techniques. The line current waveforms at no-load and harmonic spectra for CSVPWM and some popular DPWM methods for supply frequency 50Hz are as shown. 4.1 STARTING TRANSIENT RESULTS The simulation results of starting transients of proposed drive are shown in Fig 3 (3.1-3.7).The output voltage waveform is similar to all sequences. The dc voltage considered for inverter is 600V and the output voltage obtained at the inverter is =400V as shown in fig.3. Initially when the motor is started due to large inertia in the rotor it posses large amount of torque so it takes large amount of current which is observed from Fig 3. From Fig 3 (3.1-3.7) it can be observed that upto 0.8sec the starting transients are shown during this period the speed starts from 0 rpm and reaches nearly 1500rpm, that means at the time of steady state it satisfies and before reaches to the steady state the current waveform gradually reduce and reaches to the min value of the current less than 4 amps in steady state. Vdc GDPWM Pulses V/F Control Inverter Induction motor
  • 4. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 105 | P a g e Figure3.1 Starting transients of continuous SVPWM Figure3.2 Starting transients of DPWMMIN Figure3.3 Starting transients of DPWMMAX Figure3.4 Starting transients of DPWM0
  • 5. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 106 | P a g e Figure3.5 Starting transients of DPWM1 Figure3.6 Starting transients of DPWM2 Figure3.7 Starting transients of DPWM3 Figure-3(3.1-3.7) are results of starting transients of proposed GDPWM drive 4.2 STEADY STATE RESULTS The simulation results of steady state transients of proposed drive are shown in Fig 4 (4.1- 4.7). In steady state period the speed reaches 1500rpm. After 0.8 sec the torque reaches zero and current reaches minimum value this minimum value current appears because of steady state/no load effect. Figure4.1 Steady state transients of continuous SVPWM
  • 6. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 107 | P a g e Figure4.2 Steady state results of DPWMMIN Figure4.3 Steady state transients of DPWMMAX Figure4.4 Steady state transients of DPWM0 Figure4.5 Steady state transients of DPWM1 Figure4.6 Steady state transients of DPWM2 Figure4.7 Steady state transients of DPWM3 Figure-4(4.1-4.7) are steady state results of proposed GDPWM drive
  • 7. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 108 | P a g e 4.3 TOTAL HARMONIC DISTORTION OF NO- LOAD CURRENT FOR INVERTER FED INDUCTION MOTOR Figure5.1 THD of Continuous SVPWM Figure5.2 THD of DPWMMIN Figure5.3 THD of DPWMMAX Figure5.4 THD of DPWM0 Figure5.5 THD of DPWM1 Figure5.6 THD of DPWM2 Figure5.7 THD of DPWM3 Figure 5 (5.1-5.7) are the total harmonic distortion of different sequences The total harmonic distortion of current in CSVPWM is more compared to the DPWM sequences. These THDs are calculated during the steady state period. Table-2 comparison of %THD of different PWM sequences S.NO SEQUENCES %THD 1 CSVPWM 7.39 2 DPWMMIN 6.08 3 DPWMMAX 6.05 4 DPWM0 6.28 5 DPWM1 6.72 6 DPWM2 6.44 7 DPWM3 5.99 V. CONCLUSIONS The proposed space vector based generalized discontinuous PWM algorithms uses the concept of imaginary switching times.To avoid the complexity due to angle calculation and sector identification involved in Conventional SVPWM.Also the execution time and memory required is reduced by eliminating the angle and sector estimation. From the simulation results ofV/f control of induction motor drive are discussed here. The total harmonic distortions of the motor phase current in Continuous SVPWM are more compared to the generalized DPWM sequences. The Total THD values for the proposed GDPWM algorithms are
  • 8. N. Praveena et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.102-109 www.ijera.com 109 | P a g e listed. It is observed that there is a gradual decrement of the %THD in motor phase currents. Hence DPWM sequences give better performance.The simulation results show the validity of the proposed algorithm. REFERENCES [1] G.Narayanan, “Space vector based hybrid PWM Techniques for reduced current ripple,”IEEE, Trans, vol 55, No 4,april 2008. [2] G.Narayanan and V. T. Ranganathan, “Analytical evaluation of harmonic distortion in PWM AC drives using the notion of stator flux ripple,” IEEE Trans. Power Electronics., vol. 20, no. 2, pp. 466– 474, Mar. 2005. [3] K. Sri Gowri,”High-Performance Generalized ADPWM Algorithm for VSI Fed IM Drives for Reduced Switching Losses.”International Journal of Recent Trends in Engineering, Vol 2, No. 5, November 2009 [4] AhmetM.hava and Thomas “Simple Analytical and Graphical Methods for Carrier- based PWM-VSI Drives”, IEEE Trans on power electronics vol14 no1 jan 1999 [5] N.Ravisankar Reddy and T. Brahmananda Reddy “Simplified Space Vector Based Hybrid PWM Algorithm for Reduced CurrentRipple”,International Journal of Recent Trends in Engineering, Vol 2, No. 5, November 2009 [6] Advanced Bus-Clamping PWM Techniques Based on Space Vector Approach.G.Narayanan, Member, IEEE, Harish K. Krishnamurthy, Di Zhao, and RajapandianAyyanar, Member, IEEE,2006. [7] J.Holtz, ―Pulse width modulation for electronic power conversion, Proc. IEEE, vol82, no. 8, pp. 1194–1214, Aug. 1994. [8] K. Sri Gowri, T.Brahmanada Reddy, Ch. SaiBabu, “Switching Loss Characteristics of Advanced DPWM Methods Using Space Vector Based Double Switching Clamping Sequences,” Proc. ISIEA’09, Kuala Lumpur, Malaysia, in press. [9] K. Zhou and D.Wang, “Relationship between space-vector modulation and three- phase carrier-based PWM: A comprehensive analysis,” IEEE Trans Ind. Electron., vol. 49, no. 1, pp. 186–196, Feb. 2002 [10] N.Praveena , G.Satheesh , R.Ramprasad“Space Vector Based PWM Algorithms to ReduceCurrent Ripple for an Induction Motor Drive ,”International Journal of Advanced Scientific and Technical Research, Volume 3, pp 528- 540, Feb 2013 N.PRAVEENA received B.Tech degree in Electrical and Electronics Engineeringfrom G.Pullaiah college of Engineeringand Technology, JNTUA, Anantapur in the year 2011. She is currently pursuing M.Tech in G. Pulla- Reddy Engineering College, Kurnool. Her research interests include Power electronic controllers, PWM techniques, Electrical Drives. G.SATHEESH was born in 1979. He graduated from Bangalore University, Bangalore inthe year 2001. He received M.Tech degree from J.N.T University, Anantapur, India in the year 2004. He is presently Assistant Professor in the Electrical and Electronics EngineeringDepartment, G. Pulla Reddy Engineering College, Kurnool, India. He is currently pursuingPh.D. in Electrical Engineering Department, JNTU, Kakinada. His areas of interest include Power electronics, pulse width modulation techniques, AC Drives and Control. R.RamPrasad,graduated from Bangalore University, Bangalore in the year 2002. He received M.Tech degree from Sri Venkateswara University, Tirupati, India in the year 2007. He is presently Assistant Professor in the Electrical and Electronics Engineering Department, NBKRIST, Vidya Nagar, Nellore, India. His areas of interest include Multi Level Inverters, Harmonic Reduction Techniques Power System Operation and Control.