A Comparative Study and Experimental Investigation of ...SVPWM, who contributed a lot in PWM methods...

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A Comparative Study and Experimental Investigation of Continuous and Discontinuous PWM algorithms for VSI fed Induction Motor Drive. M.Nayeemuddin 1* Assistant Professor, E.E.E Dept., G. Pulla Reddy Engineering College, Kurnool, AP, e-mail: [email protected] Dr. T. Bramhananda Reddy 2 Professor, E.E.E Department, G. Pulla Reddy Engineering College, Kurnool, AP, India. Dr. M. Vijaya Kumar 3 3 Professor, E.E.E Department, JNTUACOE, Ananthapuramu, Andhra Pradesh, India. AbstractThis paper investigates and compares various continuous and discontinuous Pulse width modulation algorithms for two-level three-phase voltage source Inverter. In SPWM, variable AC output voltage of inverter is produced by comparing a sinusoidal reference signal with triangular signal, where as Conventional SVPWM uses complex voltage vector for PWM control. It is observed that SVPWM algorithm makes it possible to the fundamental output voltage to increase 15.5% as compared with SPWM. More over Conventional SVPWM requires sector information and angle for calculating gating sequence of the inverter, a simplified SVPWM algorithm is also described, which does not require sector and angle calculation. However it is observed that continuous PWM algorithm gives more switching losses and high harmonic distortion at higher modulation index. This paper presents simplified discontinuous Pulse width modulation methods (DPWM) for two-level three-phase voltage source inverters. In the proposed DPWM a zero sequence signal is injected in sinusoidal reference signal to generate different modulators with easier implementation. The simulation and experimental results shows the superiority of this algorithm as compared with conventional PWM algorithms. KeywordsHarmonic distortion, Induction motor, Inverter, Sinusoidal Pulse width modulation (SPWM), Space vector pulse width modulation (SVPWM), Discontinuous PWM (DPWM) Introduction Over the past 60 years major improvements in modern industrial processes can be largely attributed to advancements in AC drives. Prior to the 1950’s most industries were used DC motors because 3-phase induction motors could be operated at only one frequency. Now thanks to advancements in power electronic devices, reliable and cost effective control of induction motor. The increase in the use of induction motors was largely attributed to major industries converting existing diesel engines to run off electricity. The invention of Power Electronic devices changed scenario of industry by the replacement of DC drives with AC drives, for the fact that it has given the choice for developing many strategies for speed control. Due to the improvement of power semiconductor devices accurate Pulse Width Modulation (PWM) algorithms finds drastic growth in motor drive applications, uninterruptible power supply (UPS) and DC to AC and AC to DC power conversion. AC drives require variable voltage supply at variable frequency, for satisfactory operation of the motor drive harmonic distortion of stator current must be low. Due to practical limitations switching frequency cannot be increased beyond its limits, efforts have been made to design precise PWM algorithms [1-10] to reduce harmonic distortion at a given switching frequency. In the literature, a variety of PWM algorithms exist given at [8-9], among those most popular PWM algorithms are sinusoidal PWM (SPWM) and space vector PWM (SVPWM). In the year 1964, SPWM method was introduced by Schonoung [1], in this method variable AC output voltage of inverter is produced by comparing a sinusoidal reference signal (also known as modulating control signal) with triangular signal. Conventional space vector uses complex voltage vector to control the inverter output voltage, this idea is first suggested by Jardan et al. but the conventional space vector PWM technique was first published by Prof. Joachim Holtz in the year 1982[3].Prof. Joachim Holtz is one of the pioneers of SVPWM, who contributed a lot in PWM methods [4-9]. In comparison between SPWM and SVPWM, SVPWM results excellent dc bus utilization and also line stator current harmonics can be minimized. In SVPWM algorithm the zero state voltage vector time is divided equally among the two possible zero state voltage vectors [6-11]. However Conventional SVPWM requires angle and sector information for calculating gating sequence in each sampling time of the inverter, which is very complex and requires longer time for calculation than any other method. Hence to overcome this complexity, a simplified SVPWM algorithm is described, which does not require angle and sector calculation for generating gating sequence. In Simplified algorithm the actual gating signal in each sampling time of the inverter are evaluated from the concept of effective voltages. [11, 13]. However, modification of the modulating signal can be done by utilizing the unequal division of the zero state voltage vectors time, thus various discontinuous PWM algorithms can be generated [16]. These PWM algorithms clamp each phase to either positive or negative dc bus for a total period of 120 o in each fundamental cycle. These PWM algorithms are also known discontinuous PWM (DPWM) algorithms or bus- clamping PWM (BCPWM) algorithms [14-24]. This paper presents a detailed explanation of various continues and discontinuous PWM algorithms by using an injected zero sequence signal to the reference sinusoidal International Journal of Applied Engineering Research ISSN 0973-4562 Volume 12, Number 1 (2017) © Research India Publications. http://www.ripublication.com 272

Transcript of A Comparative Study and Experimental Investigation of ...SVPWM, who contributed a lot in PWM methods...

Page 1: A Comparative Study and Experimental Investigation of ...SVPWM, who contributed a lot in PWM methods [4-9]. In comparison between SPWM and SVPWM, SVPWM results excellent dc bus utilization

A Comparative Study and Experimental Investigation

of Continuous and Discontinuous PWM algorithms

for VSI fed Induction Motor Drive.

M.Nayeemuddin1*

Assistant Professor,

E.E.E Dept., G. Pulla Reddy

Engineering College, Kurnool, AP,

e-mail: [email protected]

Dr. T. Bramhananda Reddy2

Professor, E.E.E Department,

G. Pulla Reddy Engineering College,

Kurnool, AP, India.

Dr. M. Vijaya Kumar3 3Professor, E.E.E Department,

JNTUACOE, Ananthapuramu,

Andhra Pradesh, India.

Abstract— This paper investigates and compares various

continuous and discontinuous Pulse width modulation algorithms

for two-level three-phase voltage source Inverter. In SPWM,

variable AC output voltage of inverter is produced by comparing

a sinusoidal reference signal with triangular signal, where as

Conventional SVPWM uses complex voltage vector for PWM

control. It is observed that SVPWM algorithm makes it possible

to the fundamental output voltage to increase 15.5% as compared

with SPWM. More over Conventional SVPWM requires sector

information and angle for calculating gating sequence of the

inverter, a simplified SVPWM algorithm is also described, which

does not require sector and angle calculation. However it is

observed that continuous PWM algorithm gives more switching

losses and high harmonic distortion at higher modulation index.

This paper presents simplified discontinuous Pulse width

modulation methods (DPWM) for two-level three-phase voltage

source inverters. In the proposed DPWM a zero sequence signal

is injected in sinusoidal reference signal to generate different

modulators with easier implementation. The simulation and

experimental results shows the superiority of this algorithm as

compared with conventional PWM algorithms.

Keywords— Harmonic distortion, Induction motor, Inverter,

Sinusoidal Pulse width modulation (SPWM), Space vector pulse

width modulation (SVPWM), Discontinuous PWM (DPWM)

Introduction

Over the past 60 years major improvements in modern industrial processes can be largely attributed to advancements in AC drives. Prior to the 1950’s most industries were used DC motors because 3-phase induction motors could be operated at only one frequency. Now thanks to advancements in power electronic devices, reliable and cost effective control of induction motor. The increase in the use of induction motors was largely attributed to major industries converting existing diesel engines to run off electricity. The invention of Power Electronic devices changed scenario of industry by the replacement of DC drives with AC drives, for the fact that it has given the choice for developing many strategies for speed control. Due to the improvement of power semiconductor devices accurate Pulse Width Modulation (PWM) algorithms finds drastic growth in motor drive applications, uninterruptible power supply (UPS) and DC to AC and AC to DC power conversion. AC drives require variable voltage supply at variable frequency, for satisfactory operation of the

motor drive harmonic distortion of stator current must be low. Due to practical limitations switching frequency cannot be increased beyond its limits, efforts have been made to design precise PWM algorithms [1-10] to reduce harmonic distortion at a given switching frequency. In the literature, a variety of PWM algorithms exist given at [8-9], among those most popular PWM algorithms are sinusoidal PWM (SPWM) and space vector PWM (SVPWM). In the year 1964, SPWM method was introduced by Schonoung [1], in this method variable AC output voltage of inverter is produced by comparing a sinusoidal reference signal (also known as modulating control signal) with triangular signal. Conventional space vector uses complex voltage vector to control the inverter output voltage, this idea is first suggested by Jardan et al. but the conventional space vector PWM technique was first published by Prof. Joachim Holtz in the year 1982[3].Prof. Joachim Holtz is one of the pioneers of SVPWM, who contributed a lot in PWM methods [4-9].

In comparison between SPWM and SVPWM, SVPWM results excellent dc bus utilization and also line stator current harmonics can be minimized. In SVPWM algorithm the zero state voltage vector time is divided equally among the two possible zero state voltage vectors [6-11]. However Conventional SVPWM requires angle and sector information for calculating gating sequence in each sampling time of the inverter, which is very complex and requires longer time for calculation than any other method. Hence to overcome this complexity, a simplified SVPWM algorithm is described, which does not require angle and sector calculation for generating gating sequence. In Simplified algorithm the actual gating signal in each sampling time of the inverter are evaluated from the concept of effective voltages. [11, 13].

However, modification of the modulating signal can be done by utilizing the unequal division of the zero state voltage vectors time, thus various discontinuous PWM algorithms can be generated [16]. These PWM algorithms clamp each phase to either positive or negative dc bus for a total period of 120o in each fundamental cycle. These PWM algorithms are also known discontinuous PWM (DPWM) algorithms or bus-clamping PWM (BCPWM) algorithms [14-24].

This paper presents a detailed explanation of various continues and discontinuous PWM algorithms by using an injected zero sequence signal to the reference sinusoidal

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modulator [12]. Finally the comparison results with continuous PWM algorithms such as SPWM, conventional SVPWM and Simplified SVPWM with proposed DPWM algorithms are presented. The proposed PWM algorithms have been proved by using laboratory tests and the results are presented. The modulators shown in Fig.1 are divided into two groups (i) Continuous PWM (CPWM. (ii) Discontinuous PWM (DPWM).

In continuous PWM algorithm the modulating signals are within the peak boundaries of the triangular signal, such that for every carrier cycle reference modulator intersects, hence continuous ON and OFF switching occur for each inverter leg switch. In case of DPWM algorithm, the modulator of a phase has clamped to either positive dc bus or negative dc bus for at least 1200, hence such interval corresponds to inverter leg either continuous ON or OFF results discontinuous switching. These modulators which were reported in the literature are discussed in the following section.

Fig1. Modulating Waveforms of different PWM

I. REVIEW OF CONTINUOUS PWM ALGORITHMS

A. Sinusoidal PWM Algorithm

First, confirm that you have the correct template for your paper size. This template has been tailored for output on the A4 paper size. If you are using US letter-sized paper,

Fig. 2 shows a typical two level three phase voltage source Inverter (VSI) which generates AC output power from DC input voltage with desired frequency and amplitude using high frequency PWM Algorithms.

The three phase modulating reference signals are expressed as

)3/π)1-j(2-tw(Sin*V=V epi (1)

))3

π(-)3/π)1-j(2-tw((Cos*V=V epix (2)

Where i=R,Y,B and j=1,2,3 ( i = j )

Vdc

T1 T3

T4 T6

R

T5

T2

YB

OAC

Drive

2

dcV

2

dcV

Fig 2. Three Phase Voltage Source inverter schematic diagram

In this method the PWM Switching pulses are defined by the intersection points of the sinusoidal reference modulator waveform with a high frequency symmetrical triangular signal. Basically there are two methods will come into existence to implement PWM switching sequences. (i) Carrier comparison approach. (ii) Space vector approach.

As shown in Figure 3, in carrier comparison approach modulator wave form is compared with triangular signal and the intersection point gives the switching sequence for corresponding leg switches of the inverter.

Fig 3. SPWM with triangle intersection with phase R

In case of space vector approach using the concept of space vector theory the switching sequence time length is pre calculated for each carrier cycle.

B) Third order Harmonic Injection PWM:

In the literature these modulators have been frequently discussed. The modulating signal is obtained by adding a third order harmonic signal also known as zero sequence component (having magnitude 1/6 or 1/4 of the fundamental peak voltage) with sinusoidal reference signal as expressed in equation (1) and is given as

THIi

*

i V+V=V

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Where )tw3(Sin*V*K=V epTHI

K=1/6 for THIPWM1/6

K=1/4 for THIPWM1/4

Both the above methods are complex to implement because of generating the Sin (3wet) is difficult with hardware implementation. Although when K=1/4, the harmonic distortion is slightly better than conventional SVPWM but DC bus utilization is poor in comparison with SVPWM. On the other hand when K=1/6 it has higher Harmonic distortion but better DC bus utilization compared to that of THI when k=1/4.

C) Space Vector PWM Algorithm:

A Three phase two level inverter has eight switching states, it can be observed that at the same time two switching devices on the same leg cannot be turned on otherwise it will short the DC bus, therefore six symmetrical vectors V1 to V6 can be selected to apply effective voltage. Figure 4(a) represents the active vectors in space vector with stationary d-q reference frame. When V0 and V7 are applied, no power will be transferred from source to load and are known as null vectors or zero vectors.

From the principle of volt second balance expression, the active and zero state voltage vectors times can be calculated as in (3), (4) and (5).[16-18]

sTSin

VrefT

3sin

)3/(1

(3)

( )( ) Tαsin)3/π(Sin

Vref=T s2

(4)

21 TTTT sz (5)

Fig 4(a). Voltage space vectors for SVPWM

However, in the CSVPWM method, the total zero state voltage vector time is equally divided between V0 and V7 (V0=V7) and distributed symmetrically at the start and end of the each sampling time period. Thus, conventional SVPWM

algorithm uses 0127-7210 in sector-I, 0327-7230 in sector-II and so on.

D) Simplified Space Vector PWM

In conventional space vector pwm to calculate the actual gating times, the reference vector is partitioned into active vectors and these active vectors recombine together to generate actual gating pulse. To reduce the complexity involved and calculation effort, simplified PWM is described in which it is possible to generate the actual gating signal exactly same as conventional svpwm by using the instantaneous sampled reference phase voltages only and is not depend on angle & Vref [11,13].

min2max1 ; TTTTTT midmid

Where )T,T,T(∈T BYRmid and is neither minimum nor

maximum imaginary switching time. The effective time ,Teff is defined as the time between Tmax and Tmin and is given by sum of two active vector switching times. The effective time is the time duration in which the effective voltage is supplied from inverter to the motor terminals. Thus, the active and zero states times can be determined without calculating the angle and sector information as shown in fig. 4(b).

Hence by using simplified space vector PWM, actual gate sequence can be generated exactly same as conventional space vector PWM, thus reducing more than 25% execution time & 15% memory size can be minimized.

Fig 4(b). Simplified SVPWM Pulse pattern

II. PROPOSED SIMPLIFIED DPWM ALGORITHM

After careful examination of the continuous PWM algorithms, in Sinusoidal PWM algorithm, modulation index Mi= (πVref)/2Vdc , is defined as the ratio of peak value of the modulator control signal to the peak value of carrier signal, and if its greater than one (Mi>1) causes over modulation along with reduction in number of switching pulses to inverter switches which results loss of its linearity.

It is recognized and proposed that the addition of a zero sequence signal to each of the reference modulating signal makes it possible to utilize the DC bus voltage 15.50% more as compared with conventional SPWM algorithm. It means that it is possible to increase the fundamental output voltage of the inverter by 15.5%. It is viewed that the new modulator

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signal is little bit flattened around its negative peak and positive peak. The new resultant modulator is exactly similar to the modulating reference signal of the conventional SVPWM algorithm.

On the other hand the use of zero sequence signal [12] not only increases the DC bus utilization by 15.5% but also reduces the switching loss of the inverter, it means that number of on and off of the inverter switch is reduced by 33% by clamping each of the pole voltage to either positive bus or negative bus for a period of 120o.

The proposed simplified discontinuous algorithm uses the concept of injected zero sequence signal [18-22] for three phase two level inverter as shown in fig. 5, by using the proposed concept different modulators can generated by adding the zero sequence component to the three phase reference sinusoidal signal, different zero sequence components thus leads to different modulating signals with different properties.

A generalized expression that generates the zero sequence components V0 as a function of VM, Vm and Z0 is given by [21-22]

]*)1(*)*21[( 00 moMo VZVZZV (6)

Where 70

70

TT

TZ

(7)

Zero Sequence

Component (Vo)

Sy

Sr

Sb

Carrier Wave

Vy

Vb

Vr

Fig 5. Block diagram of carrier comparison based PWM employing zero sequence injection principle

By using the zero sequence component various PWM Modulators can be generated, can be expressed in terms of V0 and reference signal as

oV

iV

iV *

; oV

ixV

ixV

*

(8)

T0+T7 = Tz gives the total freewheeling time (Zero state time) of the inverter, VM and Vm are the maximum and minimum values of the three phase modulating reference signal (Vi). By utilizing the concept of unequal division of zero state time, various PWM algorithms can be generated. In the proposed simplified DPWM algorithm, by varying zero sequence component partition parameter ( )

oZ between 0 and

1, various discontinuous PWM algorithms can be generated.

When Z0=0.5, from equation (7) describes the equal division of zero state time, i.e. T0=T7 which results in the conventional space vector PWM algorithm, and the

corresponding zero sequence component is equal to average of VM & Vm , V0= - (VM+Vm )/2.Among various Continuous PWM possibilities, Z0=0.5 is the best choice which have been concluded in the literature.[14,21].

When Z0=0 i.e. T7 =0 and T0=Tz, it means that only the freewheeling state V0 is together with V1 and V2 active vectors as shown in fig.4(a) is applied, the resultant modulating signal is known as DPWMMIN shown in fig. 6(c) in which at any fundamental time instant one of the pole is connected to negative bus for a period of 1200 while the other two are modulating.

When Z0=1 i.e. T0 =0 and T7=Tz, it means that only the freewheeling state V7 is together with V1 and V2 active vectors as shown in fig. 4(a) is applied, the resultant modulating signal is known as DPWMMAX shown in fig. 6(d) in which at any fundamental time instant one of the pole is connected to positive bus for a period of 1200 while the other two are modulating.

Fig 6. (a-d). Showing Various Modulators (a) SPWM (b)Zo=0.5,SVPWM (c) Zo=0 ,DPWMMIN (d)Zo=1,DPWMMAX

Fig 6. (e-h) Showing Various Modulators

(e) DPWM1 (f) DPWM2 (g) DPWM3 (h) DPWM4

Further, four more possibilities for generation of various discontinuous modulators by varying Z0 from zero to one as shown in fig. 6(e) to 6(h) referred as discontinuous PWM1 (DPWM1) to DPWM4. In case DPWM1, change of Z0 from 1

Vr*

Vy*

Vb*

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to 0 coincides with middle of the reference signal. In DPWM2 a phase shift of 300 exists with respect to DPWM1, change of Z0 occurs at the starting of the sector. In case of DPWM3 the reference signal with intermediate signals defines Z0, and DPWM4 is complementary to DPWM2. The performance, in terms of harmonic distortion factor, of above discussed PWM modulators depends on modulation index Mi. When Z0=0.5 i.e. SVPWM modulator will give superior performance in low modulation index region. However at higher modulation index one of the DPWM should be realized.

Direct digital implementation of various DPWM can be done using space vector theory. However for analog implementation shown in fig. 5, the gating pulses for three phase inverter can be generated by comparing modulator wave shown in fig. 6 with triangular signal and the intersection point gives the switching sequence for corresponding leg switches of the inverter. Table 1 shows the generation of various Pulse Width Modulation (PWM) Modulating signals with the variation of zero sequence component (Z0) value.

Table1: Generation of various discontinuous PWM algorithms

S.No. PWM algorithm

Zero sequence Component

oVvalue

1 SPWM Vo=0

2 THIPWM1/6 Vo= (Vp/6) * sin(3wet)

3 THIPWM1/4 Vo= (Vp/4) * sin(3wet)

4 CSVPWM Vo = -(VM+Vm)/2

5 DPWMMIN Vo = -(1+Vm)

6 DPWMMAX Vo = (1-VM)

7 DPWM1 If |Vm|> VM

Vo = -(1+Vm), If

|Vm|< VM Vo = (1-VM)

8 DPWM2 If |Vmx|> VMx

Vo = -(1+Vm), If

|Vmx|< VMx Vo = (1-VM)

9 DPWM3 If |Vm|< VM

Vo = -(1+Vm), If

|Vm| >VM Vo = (1-VM)

10 DPWM4 If |Vmx|< VMx

Vo = -(1+Vm), If

|Vmx| >VMx Vo =(1-VM)

III. IMPLEMENTATION RESULTS

To validate the proposed DPWM algorithm, performance

characteristics have been tested in the laboratory on a constant

volt/frequency ratio 3-HP induction motor drive and also

several numerical simulation studies have been carried out at

different modulation indices by using the Matlab- Simulink.

For the simulation studies and hardware dc link voltage is

taken as 540 V. The simulation and hardware results of

modulating wave, pole voltage and line voltage, steady state

stator current and total harmonic distortion (THD) for various

possible PWM algorithms during low modulation and higher

modulation regions are shown from Fig. 7 to Fig. 54.

A. A) Simulation Results

Fig 7. SPWM algorithm at Mi=0.81

Fig 8. SPWM algorithm at Mi=0.36

Fig 9. SVPWM algorithm at Mi=0.81

Fig 10. SVPWM algorithm at Mi=0.36

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Fig 11. DPWMMIN algorithm at Mi=0.81

Fig 12. DPWMMIN algorithm at Mi=0.81

Fig 13. DPWMMAX algorithm at Mi=0.81

Fig 14. DPWMMAX algorithm at Mi=0.36

Fig 15. DPWM1 algorithm at Mi=0.81

Fig 16. DPWM1 algorithm at Mi=0.36

Fig 17. DPWM2 algorithm at Mi=0.81

Fig 18. DPWM2 algorithm at Mi=0.36

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Fig 19. DPWM3 algorithm at Mi=0.81

Fig 20. DPWM3 algorithm at Mi=0.36

Fig 21. DPWM4 algorithm at Mi=0.81

Fig 22. DPWM4 algorithm at Mi=0.36

B. B) EXPERIMENTAL RESULTS

Fig 23. SPWM algorithm at Mi=0.81: Modulating Signal,

Pulses, Line Voltage and Stator Current

Fig 24. SPWM algorithm at Mi=0.36: Modulating Signal,

Pulses, Line Voltage and Stator Current

Fig. 25 SVPWM algorithm at Mi=0.81: Modulating Signal,

Pulses, Line Voltage and Stator Current

Fig 26. SVPWM algorithm at Mi=0.36: Modulating Signal,

Pulses, Line Voltage and Stator Current

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Fig 27. DMPWMMIN algorithm at Mi=0.81: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 28. DMPWMMIN algorithm at Mi=0.36: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 29. DMPWMMAX algorithm at Mi=0.81: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 30. DMPWMMAX algorithm at Mi=0.36: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 31. DMPWM1 algorithm at Mi=0.81: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 32. DMPWM1 algorithm at Mi=0.36: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 33. DMPWM2 algorithm at Mi=0.81: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 34. DMPWM2 algorithm at Mi=0.36: Modulating

Signal, Pulses, Line Voltage and Stator Current

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Fig 35. DMPWM3 algorithm at Mi=0.81: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 36. DMPWM3 algorithm at Mi=0.36: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 37. DMPWM4 algorithm at Mi=0.81: Modulating

Signal, Pulses, Line Voltage and Stator Current

Fig 38. DMPWM4 algorithm at Mi=0.36: Modulating

Signal, Pulses, Line Voltage and Stator Current

C. Stator Current Harmonic Comparison

Fig 39. SPWM: Harmonic distortion of line current along

with THD at Mi=0.81

Fig 40. SPWM: Harmonic distortion of line current along

with THD at Mi=0.36

Fig 41. SVPWM: Harmonic distortion of line current along

with THD at Mi=0.81

Fig 42. SVPWM: Harmonic distortion of line current along

with THD at Mi=0.36

Fig 43. DPWMMIN: Harmonic distortion of line current

along with THD at Mi=0.81

Fig 44. DPWMMIN: Harmonic distortion of line current

along with THD at Mi=0.36

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Fig 45. DPWMMAX: Harmonic distortion of line current

along with THD at Mi=0.81

Fig 46. DPWMMAX: Harmonic distortion of line current

along with THD at Mi=0.36

Fig 47. DPWM1: Harmonic distortion of line current along

with THD at Mi=0.81

Fig 48. DPWM1: Harmonic distortion of line current along

with THD at Mi=0.36

Fig 49. DPWM2: Harmonic distortion of line current along

with THD at Mi=0.81

Fig 50. DPWM2: Harmonic distortion of line current along

with THD at Mi=0.36

Fig 51. DPWM3: Harmonic distortion of line current along

with THD at Mi=0.81

Fig 52. DPWM3: Harmonic distortion of line current along

with THD at Mi=0.36

Fig 53. DPWM4: Harmonic distortion of line current along

with THD at Mi=0.81

Fig 54. DPWM4: Harmonic distortion of line current along

with THD at Mi=0.36

IV. CONCLUSIONS

This paper reviews the continuous and discontinuous

PWM algorithms, and compares the performance

characteristics of various CPWM and DPWM Algorithms at

different modulation index. The conventional space vector

approach requires the sector information and angle for

calculating gating sequence of the inverter and hence to reduce

the calculation effort involved in the conventional SVPWM

approach, a simplified SVPWM has been presented by using

the concept of imaginary switching times, which gives exactly

the same pulse pattern as the conventional SVPWM. From the

results, the total harmonic distortion (THD) indicate that

conventional SVPWM gives superior performance at lower

modulation index and Discontinuous PWM algorithms gives

superior performance at higher modulation index. The THD

for various PWM algorithms has been presented in table2.

This paper also concludes that continuous PWM algorithm

give continuous pulse pattern which causes in the increment of

switching losses of the inverter, where as discontinuous PWM

algorithms clamp to either negative dc bus or positive dc bus

for a total period of 120o in every fundamental cycle. Hence,

the proposed simplified discontinuous PWM algorithms

reduce the switching losses of the inverter by 33.33%.

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TABLE2: COMPARISON OF LINE CURRENT THD

S.No PWM

Algorithm

THD in Line Current (%)

At

Mi=0.81 At Mi=0.36

1 SPWM 12.39 7.32

2 SVPWM 10.11 7.16

3 DPWMMIN 7.88 8.97

4 DPWMMAX 7.86 9.02

5 DPWM1 8.88 9.19

6 DPWM2 9.42 11.53

7 DPWM3 7.83 9.03

8 DPWM4 9.42 11.23

References

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