final thesis of control technique for multilevel h-bridge inverter(spwm,svpwm,apod,pod,ipd)

78
1 Control Techniques for Multilevel H – Bridge Inverters Thesis submitted to Visvesvaraya National Institute of Technology, Nagpur In partial fulfilment of requirement for the award of degree of BACHELOR OF TECHNOLOGY (ELECTRICAL AND ELECTRONICS ENGINEERING) Submitted By AMEY PATIL (BT11EEE005) AMEY KHOT (BT11EEE006) CHARUDATT AWAGATHE (BT11EEE018) SRIKANT PILLAI (BT11EEE051) PURUSHOTAM KUMAR (BT11EEE053) Under the guidance of Prof. Dr. M.A. CHAUDHARI Department of Electrical Engineering Visvesvaraya National Institute of Technology Nagpur 440 010 (India) April 2015

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Page 1: Final Thesis of Control Technique For Multilevel H-bridge Inverter(SPWM,SVPWM,APOD,POD,IPD)

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Control Techniques for Multilevel H – Bridge Inverters

Thesis submitted to Visvesvaraya National Institute of Technology,

Nagpur

In partial fulfilment of requirement for the award of degree of

BACHELOR OF TECHNOLOGY

(ELECTRICAL AND ELECTRONICS ENGINEERING)

Submitted By

AMEY PATIL (BT11EEE005)

AMEY KHOT (BT11EEE006)

CHARUDATT AWAGATHE (BT11EEE018)

SRIKANT PILLAI (BT11EEE051)

PURUSHOTAM KUMAR (BT11EEE053)

Under the guidance of

Prof. Dr. M.A. CHAUDHARI Department of Electrical Engineering

Visvesvaraya National Institute of Technology

Nagpur 440 010 (India) April 2015

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Visvesvaraya National Institute of Technology, Nagpur

2014 – 2015

CERTIFICATE

This is to certify that the project work entitled “Control Techniques for

Multilevel H – Bridge Inverters”, is a bonafide work by Mr. Amey Patil, Mr. Amey

Khot, Mr. Charudatt Awagate, Mr. Srikant Pillai and Mr. Purushotam Kumar in

the Department of Electrical Engineering, Visvesvaraya National Institute of

Technology, Nagpur, in partial fulfilment of the requirements of the award of

the degree of Bachelor of Technology in Electrical and Electronics Engineering.

Prof. Dr. S.R. Bhide

Head of Department

Department of Electrical Eng.

VNIT, Nagpur

Prof. Dr. M.A. Chaudhari

Mentor and Coordinator

Assistant Professor

Department of Electrical Eng.

VNIT, Nagpur

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Visvesvaraya National Institute of Technology, Nagpur

2014 – 2015

DECLARATION

This is to declare that the project work entitled “Control Techniques for

Multilevel H – Bridge Inverters”, is a bonafide work performed by us, the below

mentioned students. This project work is being submitted and forwarded in

partial fulfilment of the requirements for the award of the degree of Bachelor

of Technology in Electrical and Electronics Engineering from Visvesvaraya

National Institute of Technology, Nagpur.

To the best of our knowledge this project report has not been submitted

to any other institution or university.

Amey Patil Amey Khot Charudatt Awagate

Srikant Pillai Purushotam Kumar

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Acknowledgement

“The finest task of an Engineer – to survey, to plan, to suggest

resources and material, assemble them for task in hand,

implement and procedure results”

- Visvesvaraya

We take this opportunity to acknowledge with deep sense of gratitude

our project guide Prof. Dr. M.A. Chaudhari, Assistant Professor, Department of

Electrical and Electronics Engineering, VNIT Nagpur for her invaluable guidance,

constant motivation, and continuous support which has led to the successful

completion of this project.

We also take this opportunity to pay our sincere thanks to Dr. S.R. Bhide,

Head of Department, Electrical Engineering, VNIT Nagpur, for providing the

requisite facilities needed to complete the project. We would also like to thank

all the teaching and non-teaching staff for supporting us.

We express our thanks to our parents and all our friends for their

constant support and encouragement, which helped us complete this work.

Amey Patil

Amey Khot

Charudatt Awagate

Srikant Pillai

Purushotam Kumar

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Contents

1 Abstract ...................................................................................................... 8

2 Introduction ............................................................................................... 9

2.1 Inverters ............................................................................................... 9

2.1.1 Voltage Source Inverters (VSI) ...................................................... 10

2.1.2 Current Source Inverters .............................................................. 11

2.2 H-Bridge Inverters .............................................................................. 11

2.2.1 Three phase inverter .................................................................... 13

2.3 Inverter Applications .......................................................................... 14

3 Pulse Width Modulation Schemes ............................................................ 16

3.1 Control techniques for inverter output .............................................. 16

3.2 Internal Pulse Control in inverter ....................................................... 17

3.3 Pulse Width Modulation ..................................................................... 17

3.4 Modulation index ............................................................................... 19

3.5 Types of PWM techniques .................................................................. 20

3.5.1 Single PWM .................................................................................. 20

3.5.2 Multiple PWM .............................................................................. 20

3.5.3 Sine PWM ..................................................................................... 21

3.5.4 Space Vector PWM ....................................................................... 22

3.6 Space Vector PWM ............................................................................. 23

3.6.1 Concept of Space Vectors ............................................................. 23

3.6.2 Space Vector implementation in three phase inverter ................. 26

3.6.3 Main Sectors and Voltage Vector states ....................................... 27

3.6.4 Modulation through Space Vectors .............................................. 28

3.6.5 Conventional Switching Sequence ................................................ 29

3.6.6 Steps in SVPWM implementation ................................................. 31

3.6.7 Switching Time during any sector ................................................. 32

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3.6.8 Sector-wise switching pattern and Switching Timetable .............. 34

3.6.9 Output Voltage of SVPWM ........................................................... 36

4 Multilevel Inverters ................................................................................. 38

4.1 Comparison and advantage of Multilevel Inverters ............................ 39

4.1.1 Advantages of Multilevel Inverter: ............................................... 40

4.2 Types of Multilevel Inverters ............................................................. 41

4.2.1 Diode-clamped Multilevel Inverter ............................................... 41

4.2.2 Flying Capacitor Multilevel Inverter ............................................. 44

4.2.3 Cascaded Multilevel Inverter ........................................................ 46

4.2.4 Comparison of Multilevel Topologies ........................................... 48

4.3 Cascaded Multilevel Inverter .............................................................. 50

4.3.1 Cascaded H-Bridge Inverter with Equal DC voltage ...................... 50

4.3.2 Cascaded H-Bridge Inverter with Unequal DC voltage .................. 52

5 Multilevel Inverter PWM schemes ........................................................... 54

5.1 Level Shifted Sine PWM scheme ......................................................... 55

5.2 Types of Level Shifted Sine PWM ....................................................... 56

5.2.1 In-Phase Disposition IPD ............................................................... 56

5.2.2 Alternative Phase opposite Disposition APOD .............................. 57

5.2.3 Phase Opposite Disposition POD .................................................. 58

5.3 Phase Shifted Sine PWM scheme ...................................................... 59

6 Simulations ............................................................................................... 61

6.1 Simple PWM with Three phase Inverter ............................................. 61

6.2 Space Vector PWM for three phase Inverter ..................................... 62

6.3 Comparison between SPWM and SVPWM ......................................... 65

6.4 Simulation of 5-level Cascaded Inverter ............................................ 67

6.4.1 Multilevel Phase shifted Sine PWM Inverter ................................ 67

6.4.2 Multilevel level shifted Sine PWM Inverter .................................. 69

6.5 Simulation of 7-level Cascaded Inverter by Unequal DC voltages ....... 71

6.6 Comparison between phase shifted and level shifted ........................ 72

6.7 Conclusions ........................................................................................ 74

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7 References................................................................................................ 75

8 Appendices ............................................................................................... 76

8.1 Appendix 1- List of Figures.................................................................. 76

8.2 Appendix 2-List of Tables .................................................................... 78

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1 Abstract

Inverter serves a long variety of applications ranging from simple converting of

battery power to sinusoidal AC to high power HVDC transmission of electricity for a

very long distance. Its irreplaceable need in variable frequency drives which are used

on a very large scale worldwide, makes inverters very invaluable. Still there is much

scope for improvement in the inverting technology and so they have been a well

researching topic across the academics. Inverters have constantly gone over many

technological improvements, starting from the development of the switching gates

technologies, improvements in their max power handling capacities and reduction in

switching losses to improvement in the triggering circuitry. Developing of new pulse

triggering techniques and their specific adjustments as per the demand.

In this thesis, we look upon the various pulse triggering techniques implemented

by inverters and their comparison. We also discuss the methods and benefits of

increasing the level of inverters, including the reducing of Total Harmonic Distortion,

increase bus utilization and other such factors. This thesis has primarily focused on

Sinusoidal Pulse Width Modulation (SPWM), Space Vector concept & transformation,

Conventional Space Vector Pulse Width Modulation (SVPWM) technique,

computations for Space Vector PWM and then on the benefits of increasing the level

of inverter with discussion on different types of multilevel inverters, especially the

cascaded H-Bridge multilevel inverter. Along with the multilevel, we have worked on

the carrier based Sine PWM modes, namely phase shifted pulse width modulation and

level shifted pulse width modulation are can be used in the cascaded H-Bridge

Inverter. Simulations were done using PSIM and MATLAB Simulink for the given PWM

techniques. And it was observed that comparatively Space vector technique utilizes

DC bus voltage more efficiently and generates less harmonic distortion when

compared with Sinusoidal PWM.

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2 Introduction

2.1 Inverters

Inverters are the power electronic circuit, which converts the DC voltage

into AC voltage. The DC source is normally a battery or output of the controlled

rectifier. The output voltage waveform of the inverter can be square wave,

quasi-square wave or low distorted sine wave. The output voltage can be

controlled with the help of drives of the switches. The pulse width modulation

techniques are most commonly used to control the output voltage of inverters.

Such inverters are called as PWM inverters. The output voltage of the inverter

contain harmonics whenever it is not sinusoidal. These harmonics can be

reduced by using proper control schemes.

Inverters can be broadly classified into two types. They are-

Voltage Source Inverter (VSI)

Current Source Inverter (CSI)

When the DC voltage remains constant, then it is called voltage inverter

(VSI) or voltage fed inverter (VFI). When input current is maintained constant,

then it is called current source inverter (CSI) or current fed inverter (CFI).

Sometimes, the DC input voltage to the inverter is controlled to adjust the

output. Such inverters are called variable DC link inverters. The inverters can

have single phase or three-phase output.

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A voltage source inverter is fed by a stiff dc voltage, whereas a current

source inverter is fed by a stiff current source.

A voltage source can be converted to a current source by connecting a

series inductance and then varying the voltage to obtain the desired

current.

A VSI can also be operated in current-controlled mode, and similarly a CSI

can also be operated in the voltage control mode.

The inverters are used in variable frequency ac motor drives, uninterrupted

power supplies, induction heating, static VAR compensators, etc.

The following sections gives us the comparative study between VSI and CSI

2.1.1 Voltage Source Inverters (VSI)

VSI is fed from a DC voltage source having small or negligible impedance.

Input voltage is maintained

constant.

Output voltage does not

dependent on the load.

The waveform of the load

current as well as its magnitude

depends upon the nature of

load impedance.

VSI requires feedback diodes.

The commutation circuit is

complicated.

Power BJT, Power MOSFET, IGBT and GTO with self-commutation can be

used in the circuit.

Figure 2-1: Voltage source inverter

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2.1.2 Current Source Inverters

CSI is fed with adjustable

current from a DC voltage

source of high impedance.

The input current is constant

but adjustable.

The amplitude of output

current is independent of the

load.

The magnitude of output

voltage and its waveform

depends upon the nature of the load impedance.

The CSI does not require any feedback diodes.

Commutation circuit is simple as it contains only capacitors.

2.2 H-Bridge Inverters

As previously mentioned, the purpose of an inverter is to convert DC

power to AC power. Inverters are an integral part of many technologies

including uninterruptable power supplies, induction heating, high-voltage

direct current power transmission, variable frequency drives, electric vehicle

drives, and multiple renewable energy applications. All of these technologies

use inverters to achieve different goals, but all produce AC power from a DC

input. There are many varieties of inverter designs. The most common topology

used is show in the figure 2-3 and is referred to as the H-bridge topology.

Figure 2-2: Current source inverter

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The term H Bridge is derived from the typical graphical representation of such

a circuit. An H bridge is built with four switches (solid-state or mechanical).

When the switches S1 and S4 are closed a positive voltage will be applied across

the motor. By opening S1 and S4 switches and closing S2 and S3 switches, this

voltage is reversed, allowing reverse operation.

Using the nomenclature above, the switches S1 and S2 should never be

closed at the same time, as this would cause a short circuit on the input voltage

source. The same applies to the switches S3 and S4. This condition is known as

shoot-through.

Its basic configuration is shown in figure. This topology is used in

conjunction with either the square wave, or pulse width modulation (PWM)

switching schemes.

The square-wave switching scheme is a method for controlling the

switches (labelled S1 through S4) in order to achieve a square wave AC output

signal. The AC output is achieved by using a control signal with a 50% duty cycle

wired to S1 and S4. An inverted copy of the same signal is also wired to S2 and

Figure 2-3: Current source inverter

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S3. This switching scheme ensures that S1 and S4 are always on when S2 and S3

are off. It should be easily seen how such a switching scheme creates the square

wave output shown in figure. The advantage of using an H-bridge inverter is

that only a single, simple control signal is required to control four transistors.

The disadvantage, however, is that the square wave output is a low quality AC

signal that injects many harmonics into any loads to which it is powering. We

thus aim to reduce the harmonics in the output AC voltage by use of various

modulation techniques.

2.2.1 Three phase inverter

A Basic three phase inverter consist of three legs, each attached to the

phase output line. The upper and lower switching transistor are S1 & S4 for R

phase, S3 & S6 for Y phase and S5 & S2 for B phase respectively.

Figure 2-4: Basic three phase inverter

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2.3 Inverter Applications

DC power source utilization

An inverter converts the DC electricity from sources such

as batteries or fuel cells to AC electricity.

Uninterrupted powers source utilization

An uninterruptible power supply (UPS) uses batteries and an inverter to

supply AC power when main power is not available. When main power is

restored, a rectifier supplies DC power to recharge the batteries.

Electric motor speed control

Inverter circuits designed to produce a variable output voltage range are

often used within motor speed controllers. The DC power for the inverter

section can be derived from a normal AC wall outlet or some other

source. Control and feedback circuitry is used to adjust the final output

of the inverter section which will ultimately determine the speed of the

motor operating under its mechanical load.

Power grid

Grid-tied inverters are designed to feed into the electric power

distribution system. They transfer synchronously with the line and have

as little harmonic content as possible. They also need a means of

detecting the presence of utility power for safety reasons, so as not to

continue to dangerously feed power to the grid during a power outage.

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Solar

A solar inverter is a balance of system (BOS) component of a photovoltaic

system and can be used for both, grid-connected and off-grid systems.

Solar inverters have special functions adapted for use

with photovoltaic arrays, including maximum power point

tracking and anti-islanding protection.

HVDC

With HVDC power transmission, AC power is rectified and high voltage

DC power is transmitted to another location. At the receiving location, an

inverter in a static inverter plant converts the power back to AC. The

inverter must be synchronized with grid frequency and phase and

minimize harmonic generation.

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3 Pulse Width Modulation Schemes

3.1 Control techniques for inverter output

This section examines various methods of output voltage control by means

of inverter gain control. The inverter gain is defined as the ratio of output ac

voltage to input dc voltage. Such gain control is useful in many applications

where the variations of ac output voltage cannot be tolerated due to the

variations in dc input voltage. It is also necessary when volts/Hertz control of

induction motor speeds has to be implemented. The control of motor voltage

is required along with frequency in order to avoid saturation of the motor

magnetic circuit. Various techniques are available for varying the inverter gain.

The most efficient method of controlling the gain and therefore the output

voltage is to incorporate Pulse Width Modulation (PWM) control within the

inverters. In addition to PWM method, there are methods involving external

control of ac output voltage and dc input voltage. To distinguish these methods

from the PWM method, PWM method is referred to as the internal control

method since the output voltage control is realized by means of modifications

in the conduction patterns of the inverter switches. Various methods for the

control of output voltage of inverters can be enumerated as follows:

(1) External control of the AC output voltage

(2) External control of the DC input voltage

(3) Internal control of the inverter output voltage

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In the first two methods, extra circuits for the control of either dc input

or ac output become necessary. The third method, however, does not require

such circuits. This can be clearly understood in the remaining section that

discusses these methods in considerable detail.

The first two methods require the use of peripheral components whereas

the third method requires no external components. Mostly the internal control

of the inverters is dealt, and so the third method of control is discussed in great

detail in the following section.

3.2 Internal Pulse Control in inverter

Inverter output voltage can also be adjusted by exercising a control

within the inverter itself. Pulse width modulation is the most commonly used

technique to control the output voltage of inverter, the various techniques are:

o Single PWM

o Multiple PWM

o Sine PWM

o Space Vector PWM

3.3 Pulse Width Modulation

Pulse-width modulation (PWM) is the basis for control in power

electronics. The theoretically zero rise and fall time of an ideal PWM waveform

represents a preferred way of driving modern semiconductor power devices.

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With the exception of some resonant converters, the vast majority of power

electronic circuits are controlled by PWM signals of various forms. The rapid

rising and falling edges ensure that the semiconductor power devices are

turned on or turned off as fast as practically possible to minimize the switching

transition time and the associated switching losses. Although other

considerations, such as parasitic ringing and electromagnetic interference (EMI)

emission, may impose an upper limit on the turn-on and turn-off speed in

practical situations, the resulting finite rise and fall time can be ignored in the

analysis of PWM signals and processes in most cases. Hence only ideal PWM

signals with zero rise

and fall time will be

considered in this

chapter.

Pulse width

modulation is a

technique in which a

fixed input dc voltage is

given to the inverter

and a controlled ac

output voltage is

obtained by adjusting

the on and off periods

of the inverter

components. This is most popular method of controlling the output voltage and

this method is termed as pulse width modulation technique. PWM is an internal

control method and it gives better result than an external control methods.

Figure 3-1: PWM Duty cycle comparison

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There are number of PWM methods for variable frequency voltage-sourced

inverters. A suitable PWM technique is employed in order to obtain the require

In this method, a fixed dc input voltage is given to the inverter and a

controlled ac output voltage is obtained by adjusting the on and off periods of

the inverter components. Inverters employing PWM principle are called PWM

inverters. PWM techniques are characterized by constant amplitude pulses. The

width of these pulses is modulated to obtain inverter output voltage control

and to reduce its harmonic content. The advantages possessed by PWM

technique are

1. The output voltage control with this method can be obtained without any

additional components.

2. With this method, lower order harmonics can be eliminated or minimized

along with its output voltage control. As higher order harmonics can be

filtered easily, the filtering requirements are minimized.

The main disadvantage of this method is that the SCRs are expensive as they

must possess low turn on and turn off times. This is the most popular method

of controlling the output voltage of an inverter in industrial applications.

Benefits include – Microprocessor control – Efficient use of power –

Tolerance to analog noise – Not susceptible to component drift.

3.4 Modulation index

Modulation index is the ratio of peak magnitudes of the modulating

waveform and the carrier waveform. It relates the inverter's dc-link voltage and

the magnitude of pole voltage (fundamental component) Output by the

inverter. The ratio of the peak magnitudes of modulating wave) and the carrier

wave (VC) is defined as modulation-index.

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𝑀 =𝑉𝑝

𝑉𝑐

3.5 Types of PWM techniques

3.5.1 Single PWM

In single pulse-width modulation control, there is only one pulse per half-

cycle and the width of the pulse is varying to control the output voltage.

Fig.-3-2 shows the generation of gating signals of single pulse width

modulation. The gating signals are generated by the signals of single pulse width

modulation. The single pulse-width modulation converts the reference signal to

the square wave signal. This process is obtained by inter the reference signal to

the zero-crossing circuit witch consider the positive part of the input signal is

positive part of the output signal (square wave) and the negative part of the

input signal is negative part of the output signal.

3.5.2 Multiple PWM

The harmonic content can be reduced by using several pulses in each

half-cycle of output voltage. The generation of gating signals for turning on and

off transistors is shown in Fig. The gating signals are produced by comparing

reference signal with triangular carrier wave. The frequency of the reference

signal sets the output frequency (𝑓O) and carrier frequency (𝑓C) determine the

number of pulses per half cycle.

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3.5.3 Sine PWM

In single-pulse and multiple pulse modulation techniques the width of all

pulses are same but in sinusoidal pulse width modulation the width of each

pulse is varied in proportion to the amplitude of a sine wave. In this technique

the gating signals are generated by comparing a sinusoidal reference signal with

a triangular carrier wave. The gating signal of the inverter is obtained by taking

the repeating sequence (triangular wave) as the control signal and comparing it

Figure 3-2: Bipolar Sine PWM

Figure 3-3: Unipolar Sine PWM

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with the reference wave (sinusoidal wave). In order to detect or eliminate the

zero sequence currents we use zero hold circuit and by comparing them with

the help of greater than or equal to blocks.

A Sinusoidal Pulse Width Modulation technique is also known as the

triangulation, sub oscillation, sub harmonic method is very popular in industrial

applications. In this technique a high frequency triangular carrier wave is

compared with the sinusoidal reference wave determines the switching instant.

It is to be noted that by controlling the modulation index one can control the

amplitude of applied output voltage.

3.5.4 Space Vector PWM

Space Vector modulation technique is another method available for

obtaining output voltage above that of the standard Sine PWM technique. This

is achieved by rotating a reference vector around the state diagram, which is

composed of six basic non zero vectors forming a hexagon. The complete full

circular rotation of the reference vector in the state diagram constitutes unit

pulse time cycle i.e. 20ms for a frequency of 50Hz.

Space Vector technique is further discussed in the immediate section 3.6 along

with its basic principle and conventional implementation.

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3.6 Space Vector PWM

Space Vector Modulation (SVM) was originally developed as vector

approach to Pulse Width Modulation (PWM) for three phase inverters. It is the

more sophisticated technique for generating sine wave that provides a higher

voltage to the motor with lower total harmonic distortion. And it is one of the

most widely used PWM technique for Variable Frequency Drive Applications.

The method is highly computation-intense with dynamic calculations done to

calculate the TON time of every switch within every sampling interval. One of

major advantage of SVPWM is the reduction of Total Harmonic Distortion

(THD), created by the rapid switching created by the PWM algorithm. The main

aim of any modulation technique is to obtain variable output having a maximum

fundamental component with minimum harmonics. Space Vector PWM

(SVPWM) method is an advanced; computation intensive PWM method and

possibly the best techniques for variable frequency drive application.

Also SVPWM has the aptitude for accurate digital implementation which

can be realised through Digital Signal Processor (DSP). This Superior

Performance has enabled it to find wide spread applications in recent years.

3.6.1 Concept of Space Vectors

Space Vector involves a constant amplitude vector rotating at a constant

frequency obtained from their three phase sinusoidal forms. The rotating

vector is rotated in a stationary d-q coordinate frame plane and made to imitate

its equivalent 3 phase rotating vector via 2 phase vectors. This is known as

coordinate transformation.

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For three phase system,

𝑉𝑅𝐸𝐹 = 𝑉𝑅𝑁 + 𝑉𝑌𝑁 + 𝑉𝐵𝑁

Where,

𝑉𝑅𝑁 = 𝑉𝑚 sin(𝜔𝑡)

𝑉𝑌𝑁 = 𝑉𝑚 sin(𝜔𝑡 − (2𝜋3⁄ ))

𝑉𝑌𝑁 = 𝑉𝑚 sin(𝜔𝑡 + (2𝜋3⁄ ))

And with d-q plane,

𝑉𝑅𝐸𝐹 = 𝑉𝑑 + 𝑉𝑞

With this we are able to obtain an equivalent VREF from three phase

directly through 2 vector method as shown in figure 3-4.

We therefore obtain Vd and Vq as follows

𝑉𝑑 = 𝑉𝑅𝑁 + 𝑉𝑌𝑁 cos(2𝜋3⁄ ) + 𝑉𝐵𝑁 cos(4𝜋

3⁄ )

= 𝑉𝑅𝑁 − (12⁄ )𝑉𝑌𝑁 − (1

2⁄ )𝑉𝐵𝑁

= 𝑉𝑅𝑁 + (12⁄ )𝑉𝑅𝑁

= (32⁄ )𝑉𝑅𝑁

𝑉𝑑 = 𝑉𝑅𝑁 + 𝑉𝑌𝑁 cos(2𝜋3⁄ ) + 𝑉𝐵𝑁 cos(4𝜋

3⁄ )

= 𝑉𝑅𝑁 − (12⁄ )𝑉𝑌𝑁 − (1

2⁄ )𝑉𝐵𝑁

= 𝑉𝑅𝑁 + (12⁄ )𝑉𝑅𝑁

= (32⁄ )𝑉𝑅𝑁

Figure 3-4: Coordinate Transformation RYB to d-q

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And in Matrix form as,

⌈𝑉𝑑

𝑉𝑞 ⌉ = [

32⁄ 0 0

0 √32

⁄ − √32

⁄ ] . [

𝑉𝑅𝑁

𝑉𝑌𝑁 𝑉𝐵𝑁

]

𝑉𝑞 = 𝑉𝑅𝑁 cos(3𝜋2⁄ ) + 𝑉𝑌𝑁 cos(𝜋

6⁄ ) + 𝑉𝐵𝑁 cos(5𝜋6⁄ )

= 0 − (√32

⁄ ) 𝑉𝑌𝑁 + (√32

⁄ ) 𝑉𝐵𝑁

= (√32

⁄ ) (𝑉𝑌𝑁 − 𝑉𝐵𝑁)

Figure 3-5: Three phase inverter

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3.6.2 Space Vector implementation in three phase

inverter

The Circuit Model for a typical three phase voltage source PWM inverter

is shown in Fig 3-5. Here, S1 to S6 are the six power switches that shape the

output waveform.

When an upper transistor is switched ON, the corresponding lower

transistor is switched OFF. The ON – OFF states of the upper transistors S1, S3

& S5 determines the Voltage vector state.

Figure 3-6 denotes the VREF

rotation as the switches are

switched ON and OFF. Only the

upper transistor switching is

considered here.

So ‘+ - -‘denotes S1=ON, S3=OFF &

S5=OFF and so on.

Above Figure 3-6 shows Vector space location of every state denoted along

with their corresponding switching states of the upper switches of the circuit.

Figure 3-6: VREF rotating along Voltage Space Vectors

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3.6.3 Main Sectors and Voltage Vector states

Voltage vectors created divides the cycle into 6 sectors as observed in

figure 3-8. Here 6 vector states forms the six corners of a hexagon structure

around which the reference voltage revolves. Other 2 states namely, (111) &

(000) are null vectors as produce no effective output.

The rotating VREF takes the intermediate values between each sector using

the adjacent space vector as d-q plane.

Figure 3-7: Equivalent Switching pattern of the space vectors

Figure 3-8: Space Vector Diagram

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3.6.4 Modulation through Space Vectors

The main factor by which Space Vector Modulation comes out superior

is because of its ability to occupy intermediate values between the space

vectors providing smooth transition for reference voltage VREF as it rotates.

This is achieved by having an average over the sampling period, since the

reference voltage is sampled at regular time interval TS. Within this sampling

period, VREF is synthesized using adjacent vectors and the null vector.

In Figure 3-9, it can be observed that there are 3 averaged values existing

for each sector. The averaging of the VREF is by having one branch of the adjacent

space vector ON for a fraction of the sampling time and then another one so

that overall vector average of both of them yields the desired average vector.

(- - -) or (000) is numbered as state-(0)

(+ - -) or (100) is numbered as state-(1)

(+ + -) or (110) is numbered as state-(2)

(- + -) or (010) is numbered as state-(3)

(- + +) or (011) is numbered as state-(4)

(- - +) or (001) is numbered as state-(5)

(+ - +) or (101) is numbered as state-(6)

(+ + +) or (111) is numbered as state-(7) Figure 3-9: Sector Distribution

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Let us consider Sector 1 for calculation purposes.

If T is the sampling time, then V1 is applied for T1 and V2 is applied for T2

while Zero voltage is applied for the rest of the time period. Here Zero voltage

is TZ, which is the sum of T0 & T7. i.e. T0 + T7 = TZ

𝑇𝑧 = 𝑇 − 𝑇1 − 𝑇2

This way every intermediate value is sampled between adjacent voltage vectors

of each sector and a much smoother reference voltage is obtained as shown in

fig 3-10.

3.6.5 Conventional Switching Sequence

SVPWM is implemented through many different switching sequence

patterns, the most common and widely used is the conventional switching

Figure 3-10: Sector 1 VREF approximation over a sampling time

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sequence, which maintains switching of one transistor at a time to minimise

switching losses.

Conventional Switching

sequence for sector 1 is

presented as shown above figure

3-11. This sequence is followed

for every intermediate VREF value

in this sector.

1. - - -

2. + - -

3. + + -

4. + + +

5. + + +

6. + + -

7. + - -

8. - - -

Conventional

Switching Sequence

In Sector 1

Figure 3-11: Switching Sequence for all VREF pattern in sector (only T1 T2 T0 varies)

Figure 3-12: Graphical switching pattern for different sectors

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It can be easily observed that above sequence implements V1 (+ - -) and

V2 (+ + -) only along with the Zeros V0 (- - -) & V7 (+ + +). The only thing that varies

within a sector is the TON time for both the vectors i.e. T1, T2.

Likewise switching sequence for other sectors can be obtained

implementing their required vectors with appropriate Zero vectors. Figure 3-12

above shows the approximate switching sequence graphically. Note that the

null vectors (or Zero vectors) are used in all the sector sequence (1 to 6).

3.6.6 Steps in SVPWM implementation

Switching times T1 & T2 (for sector 1) or T2 & T3 (for sector 2) is calculated

during each sampling period and implemented accordingly.

Here we demonstrate calculation for Sector 1, which can be similarly

followed for other sectors by substituting their required adjacent voltage space

vectors. T1 T2 T0 & T7 are calculated by Volt-Second integral of VREF for a given

sampling period in the sector.

We have,

𝑉𝑅𝐸𝐹𝑇𝑆 = 𝑉1. 𝑇1 + 𝑉2 . 𝑇2 + 𝑉𝑍. 𝑇𝑍

𝑇𝑆 = 𝑇1 + 𝑇2 + 𝑇𝑍

By Volt-Second integral of VREF

1

𝑇∫ ��𝑅𝐸𝐹 𝑑𝑡

𝑇

0

= 1

𝑇[∫ ��0 𝑑𝑡

𝑇0

0

+ ∫ ��1 𝑑𝑡𝑇1

0

+ ∫ ��2 𝑑𝑡𝑇2

0

+ ∫ ��7 𝑑𝑡𝑇7

0

]

��𝑅𝐸𝐹 . 𝑇 = 𝑉0. 𝑇0 + 𝑉1. 𝑇1 + 𝑉2

. 𝑇2 + 𝑉7. 𝑇7

��𝑅𝐸𝐹 . 𝑇 = 0. 𝑇0 +2

3𝑉1. 𝑇1 +

2

3𝑉𝑑 . (cos 𝜋

3⁄ + 𝑗 𝑠𝑖𝑛 𝜋3⁄ ). 𝑇2 + 0. 𝑇7

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��𝑅𝐸𝐹 . 𝑇 = 2

3𝑉1. 𝑇1 +

2

3𝑉𝑑(cos 𝜋

3⁄ + 𝑗 𝑠𝑖𝑛 𝜋3⁄ )𝑇2

𝑆𝑝𝑙𝑖𝑡𝑖𝑛𝑔 𝑟𝑒𝑎𝑙 𝑎𝑛𝑑 𝑖𝑚𝑎𝑔𝑖𝑛𝑎𝑟𝑦 𝑝𝑎𝑟𝑡𝑠

𝑇 |��𝑅𝐸𝐹| 𝑐𝑜𝑠 𝛼 = 2

3𝑉𝑑𝑇1 +

1

3𝑉𝑑𝑇2 𝑇 |��𝑅𝐸𝐹| 𝑠𝑖𝑛 𝛼 =

1

√3𝑉𝑑𝑇2

Solving for T0, T1, and T2 & T7 gives:

𝑇1 = 3

2𝑚 [(𝑇

√3⁄ ) cos 𝛼 − (𝑇

3⁄ ) sin 𝛼]

𝑇2 = 𝑚𝑇 sin 𝛼

Where,

𝑚 =𝑉𝑅𝐸𝐹

(𝑉𝑑 √3⁄ )⁄

Above Equations are derived for Sector 1, similarly other sector

equations are to be derived for their respective switching time calculations.

3.6.7 Switching Time during any sector

Step 1. Determine Vd, Vq, VREF, and angle (α)

Here, VREF and angle (α) are obtained through Vd & Vq which are

calculated through the following matrix,

⌈𝑉𝑑

𝑉𝑞 ⌉ = [

32⁄ 0 0

0 √32

⁄ − √32

⁄ ] . [

𝑉𝑅𝑁

𝑉𝑌𝑁 𝑉𝐵𝑁

]

And so,

𝛼 = tan−1(𝑉𝑑

𝑉𝑞) |𝑉𝑅𝐸𝐹| = √𝑉𝑑

2 + 𝑉𝑞2

For T0 & T7

TZ = T – T1 – T2

T0 = T7 = 0.5 TZ

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Step 2. Determine time duration T1, T2, T0

Switching time is calculated based on the Volt-Second integral i.e.

𝑉𝑅𝐸𝐹𝑇𝑆 = 𝑉1. 𝑇1 + 𝑉2 . 𝑇2 + 𝑉𝑍. 𝑇𝑍

𝑇𝑆 = 𝑇1 + 𝑇2 + 𝑇𝑍

Giving results as

𝑇1 = 3

2𝑚 [(𝑇

√3⁄ ) cos 𝛼 − (𝑇

3⁄ ) sin 𝛼]

𝑇2 = 𝑚𝑇 sin 𝛼

Where,

𝑚 =𝑉𝑅𝐸𝐹

(𝑉𝑑 √3⁄ )⁄

Step 3. Determine the switching time of each transistor (S1 to S6)

Switching time for every vector state (e.g. T1 or T2 for sector 1) is

calculated and the corresponding switches which defined the state (e.g. state

’+ - -’ or ‘100’ is defined as S1, S6 & S2 as positive while S4, S3 & S5 as closed)

are triggered for the calculated time. This is done for all the required switches.

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3.6.8 Sector-wise switching pattern and Switching

Timetable

Following is the graphical representation of the switching sequence

during each sector. Their values are calculated dynamically as mentioned in the

previous section.

Figure 3-13: Switching plots for all 6 sectors

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And the switching time for each sector can be summarized as shown

below.

Table 3-1: Switching time for each sector 1-6

Sector Upper Switches

(S1, S3, S5) Lower Switches

(S4, S6, S2)

1

S1 = T1 + T2 + T0/2 S4 = T0/2

S3 = T2 + T0/2 S6 = T1 + T0/2

S5 = T0/2 S2 = T1 + T2 + T0/2

2

S1 = T2 + T0/2 S4 = T1 + T0/2

S3 = T1 + T2 + T0/2 S6 = T0/2

S5 = T0/2 S2 = T1 + T2 + T0/2

3

S1 = T0/2 S4 = T1 + T2 + T0/2

S3 = T1 + T2 + T0/2 S6 = T0/2

S5 = T2 + T0/2 S2 = T1 + T0/2

4

S1 = T0/2 S4 = T1 + T2 + T0/2

S3 = T2 + T0/2 S6 = T1 + T0/2

S5 = T1 + T2 + T0/2 S2 = T0/2

5

S1 = T2 + T0/2 S4 = T1 + T0/2

S3 = T0/2 S6 = T1 + T2 + T0/2

S5 = T1 + T2 + T0/2 S2 = T0/2

6

S1 = T1 + T2 + T0/2 S4 = T0/2

S3 = T0/2 S6 = T1 + T2 + T0/2

S5 = T2 + T0/2 S2 = T1 + T0/2

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3.6.9 Output Voltage of SVPWM

The Line to Neutral (phase) voltage obtained [VRN VYN VBN] is obtained

through the following matrix.

[

𝑉𝑅𝑁

𝑉𝑌𝑁

𝑉𝐵𝑁

] = 1

3 𝑉𝐷𝐶 [

2 −1 −1−1 2 −1−1 −1 2

] [����

��

]

The inverter here undergoes through 8 vector states with the following

switching configuration as shown in figure 3-14.

Figure 3-14: Switching states of the inverter

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According to those states following output voltage table is derived for

every input Voltage Vector trigger pulse.

Table 3-2: Output Voltage table

Voltage Vectors

Switching Vectors Line to neutral

Voltage Line to line Voltage

R Y B VAN VBN VCN VRY VYB VBY

V0 0 0 0 0 0 0 0 0 0

V1 1 0 0 23⁄ − 1

3⁄ − 13⁄ 1 0 -1

V2 1 1 0 13⁄ 1

3⁄ − 23⁄ 0 1 -1

V3 0 1 0 − 13⁄ 2

3⁄ − 13⁄ -1 1 0

V4 0 1 1 − 23⁄ 1

3⁄ 13⁄ -1 0 1

V5 0 0 1 − 13⁄ − 1

3⁄ 23⁄ 0 -1 1

V6 1 0 1 13⁄ − 2

3⁄ 13⁄ 1 -1 0

V7 1 1 1 0 0 0 0 0 0

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4 Multilevel Inverters

The Inverter is an electrical device which converts direct current (DC) to

alternate current (AC). The inverter is used for emergency backup power in a

home. The inverter is used in some aircraft systems to convert a portion of the

aircraft DC power to AC. The AC power is used mainly for electrical devices like

lights, radar, radio, motor, and other devices.

Now a day’s many industrial applications have begun to require high

power. Some appliances in the industries however require medium or low

power for their operation. Using a high power source for all industrial loads may

prove beneficial to some motors requiring high power, while it may damage the

other loads. Some medium voltage motor drives and utility applications require

medium voltage. The multi-level inverter has been introduced since 1975 as

alternative in high power and medium voltage situations. The Multi-level

inverter is like an inverter and it is used for industrial applications as alternative

in high power and medium voltage situations.

Multi-level inverters are the modification of basic bridge inverters. They

are normally connected in series to form stacks of level.

Figure 3-1: Typical Inverter Display panel

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The topological structure of multilevel inverter must cope with the

following points-

It should have less switching devices as far as possible.

It should be capable of enduring very high input voltage such as HVDC

transmission for high power applications.

Each switching device should have lower switching frequency owing to

multilevel approach.

4.1 Comparison and advantage of Multilevel

Inverters

Table 4-1: Comparison between Conventional Inverters And Multilevel Inverters

Sr.no Conventional inverter Multilevel inverter

1 Higher THD in output voltage Low THD in output voltage

2 More switching stresses on devices

Reduced switching stresses on devices

3 Not applicable for high voltage applications

Applicable for high voltage applications

4 Higher voltage levels are not produced

Higher voltage levels are produced

5 Since 𝑑𝑣𝑑𝑡⁄ is high, the EMI

from the system is high

Since 𝑑𝑣𝑑𝑡⁄ is low, the EMI from the

system is low

6 Higher switching frequency is used hence switching losses is

high

Lower switching frequency can be used and hence reduction in

switching losses

7 Power bus structure, control schemes are simple

Control scheme is complex as the number of levels increases

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4.1.1 Advantages of Multilevel Inverter:

The multilevel converter has a several advantages such as-

Common Mode Voltage:

The multilevel inverters produce common mode voltage, reducing the stress of

the motor and don’t damage the motor.

Input Current:

Multilevel inverters can draw input current with low distortion.

Switching Frequency:

The multilevel inverter can operate at both fundamental switching frequencies

that are higher switching frequency and lower switching frequency. It

should be noted that the lower switching frequency means lower

switching loss and higher efficiency is achieved.

Reduced harmonic distortion:

Selective harmonic elimination technique along with the multi-level topology

results the total harmonic distortion becomes low in the output waveform

without using any filter circuit.

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4.2 Types of Multilevel Inverters

Multilevel inverters are classified on the basis of the circuit structure and

are of three types

4.2.1 Diode-clamped Multilevel Inverter

The main concept of this inverter is to use diodes and provides the multiple

voltage levels through the different phases to the capacitor banks which are in

series. A diode transfers a limited amount of voltage, thereby reducing the

stress on other electrical devices. The maximum output voltage is half of the

input DC voltage. It is the main drawback of the diode clamped multilevel

inverter. This problem can be solved by increasing the switches, diodes,

capacitors.

Multilevel Inverters

Common DC sources

Diode clamped Inverters

Flying Capacitor Inverters

Separate DC sources

Cascaded Inverters

Figure 4-2: Types of Multilevel Inverter

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Due to the capacitor balancing issues, these are limited to the three levels.

This type of inverters provides the high efficiency because the fundamental

frequency used for all the switching devices and it is a simple method of the

back to back power transfer systems.

Table 4-2: Switching sequence for 5 level Diode Clamped Inverter

Output S1 S2 S3 S4 S1’ S2’ S3’ S4’

VDC 1 1 1 1 0 0 0 0

VDC/2 0 1 1 1 1 0 0 0

0 0 0 1 1 1 1 0 0

-VDC/2 0 0 0 1 1 1 1 0

-VDC 0 0 0 0 1 1 1 1

Figure 4-3: Topology of the diode-clamped inverter (a) three-level inverter, (b) Five -level inverter

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Applications of Diode Clamped Multilevel Inverter:

Static VAR compensation

Variable speed motor drives

High voltage system interconnections

High voltage DC and AC transmission lines

Advantages

When the number of levels is high enough, harmonic content will be low

enough to avoid the need for filters.

Efficiency is high due to all devices which are being switched at the

fundamental frequency.

We are able to control the reactive power flow.

The control method is easy for a back to back intertie system.

Disadvantages

Excessive clamping diodes are being required when the number of levels

get high.

It is hard to do a real power flow control for individual converter.

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4.2.2 Flying Capacitor Multilevel Inverter

The main concept of this inverter is to use capacitors. It is of series

connection of capacitor clamped switching cells. The capacitors transfer the

limited amount of voltage to electrical devices. In this inverter switching states

are like in the diode clamped inverter. Clamping diodes are not required in this

type of multilevel inverters. The output is half of the input DC voltage. It is

drawback of the flying capacitors multi-level inverter. It also has the switching

redundancy within phase to balance the flaying capacitors. It can control both

the active and reactive power flow. But due to the high frequency switching,

switching losses will takes place.

Figure 4-4: Topology of the Flying Capacitor Multilevel inverter (a) three-level inverter, (b) Five -level inverter

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Applications of Flying Capacitors Multilevel Inverter:

Induction motor control using DTC (Direct Torque Control) circuit.

Static VAR generation.

Both AC-DC and DC-AC conversion applications.

Converters with Harmonic distortion capability.

Sinusoidal current rectifiers.

Advantages:

Huge amount of storage capacitors will provide additional ride through

capabilities during power rage.

Switch combination redundancy are provided for balancing different

voltage levels.

When the number of levels is high enough, the harmonic content will be

low enough not to use the filter.

We are able to control both the real and reactive power flow, and making

a possible voltage source converter candidate for high voltage dc

transmission.

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Disadvantages:

When the number of converter levels get high, a huge amount of storage

capacitor is required. Those high level systems are more difficult to

package and those bulky capacitors are expensive.

The switching frequency and switching losses will soar high for real power

transmission and the converter control will get very complicated.

Table 4-3: Switching sequence for 5 level Inverter

4.2.3 Cascaded Multilevel Inverter

A cascade multilevel inverter is a power electronic device built to synthesize

a desired AC voltage from several levels of DC voltages. Such inverters have

been the subject of research in the last several years, where the DC levels were

considered to be identical in that all of them were either batteries, solar cells,

etc. A multilevel converter was presented in which the two separate DC sources

were the secondary of two transformers coupled to the utility AC power. In

contrast, in this paper, only one source is used without the use of transformers.

The interest here is interfacing a single DC power source with a cascade

Output S1 S2 S3 S4 S1’ S2’ S3’ S4’

VDC 1 1 1 1 0 0 0 0

3VDC/4 1 1 1 0 0 0 0 1

VDC/2 1 1 0 0 0 0 1 1

VDC/4 1 0 0 0 0 1 1 1

0 0 0 0 0 1 1 1 1

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multilevel inverter here the other DC sources are capacitors. Currently, each

phase of a cascade multilevel inverter requires ‘n’ DC sources for 2n+1 levels in

applications that involve real power transfer.

Applications of Cascaded Multilevel Inverter:

Motor drives

Active filters

Electric vehicle drives

DC power source utilization

Power factor compensators

Back to back frequency link systems

Interfacing with renewable energy resources.

Figure 4-5: a) Inverter Single Stage b) 5 level Cascaded Inverter c) 7 level Cascaded Inverter

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Advantages:

The modularized structure allows easy packaging and storage.

The quantity of possible voltage levels is more than DC and FC type.

Disadvantages:

Separated DC sources or capacitor are required for each module.

A more complex controller is required due to the amount of capacitors,

which need to be balanced.

4.2.4 Comparison of Multilevel Topologies

Table 4-4: Comparison of multilevel inverter Topologies

Sr. No.

Topology Diode

Clamped Flying

Capacitor Cascaded

1 Power

semiconductor switches

2(m-1) 2(m-1) 2(m-1)

2 Clamping

diodes per phase

(m-1)(m-2) 0 0

3 DC bus

capacitors (m-1) (m-1) (m-1)/2

4 Balancing

capacitors per phase

0 (m-1)(m-

2)/2 0

5 Voltage

unbalancing Average High very small

6 Applications Motor drive

system, STATCOM

Motor drive system,

STATCOM

Motor drive system, PV, fuel cells,

battery system

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The diode clamped inverters particularly the three-level structure have a

wide popularity in motor drive applications besides other multilevel inverter

topologies. However, it would be a limitation of complexity and number of

clamping diodes for the DCMLIs, as the level exceeds. The FCMLIs are based on

balancing capacitors on phase buses and generate multilevel output voltage

waveform clamped by capacitors instead of diodes. The FCMLI topology also

requires balancing capacitors per phase at a number of (m-1)*(m-2)/2 for an

m-level inverter and it will cause to increase the number of required capacitor

in high level inverter topologies and complexity of considering DC-link

balancing. Nowadays, the multilevel inverters have become more attractive for

researchers and manufacturers due to their advantages over conventional

three-level pulse width-modulated (PWM) inverters.

They offer improved output waveforms, smaller filter size, low EMI, lower

total harmonic distortion (THD). Multilevel inverter topology has the least

components for a given number of levels. Cascaded H-Bridge-MLI topology is

based on the series connection of H-bridges with separate DC sources. Since the

output terminals of the H-bridges are connected in series, the DC sources must

be isolated from each other. The need of several sources on the DC side of the

inverter makes multilevel technology attractive for photovoltaic applications.

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4.3 Cascaded Multilevel Inverter

4.3.1 Cascaded H-Bridge Inverter with Equal DC voltage

As the name suggests, the cascaded H-bridge multilevel inverter uses

multiple units of H-bridge power cells connected in a series chain to produce

high ac voltages. A typical configuration of a five-level CHB inverter is shown

in Fig. below, where each phase leg consists of two H-bridge cells powered by

two isolated dc supplies of equal voltage E. The CHB inverter in Fig can

produce a phase voltage with five voltage levels. When switches S11, S21, S12,

and S22 conduct, the output voltage of the H- bridge cells H1 and H2 is VH1 =

VH2 = E, and the resultant inverter phase voltage is VAN = VH1 + VH2 = 2E, which

is the voltage at the inverter terminal A with respect to the inverter neutral

N. Similarly, with S31, S41, S32, and S42 switched on, VAN = –2E. The other three

voltage levels are E, 0, and –E, which correspond to various switching states

Figure 4-6: Cascaded H-Bridge with equal DC Voltage

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summarized in Table. It is worth noting that the inverter phase volt- age VAN

may not necessarily equal the load phase voltage VAO, which is the voltage at

node A with respect to the load neutral O.

It can be observed from Table that some voltage levels can be obtained by

more than one switching state. The voltage level E, for instance, can be

produced by four sets of different (redundant) switching states. The switching

state redundancy is a common phenomenon in multilevel converters. It

provides a great flexibility for switching pattern design, especially for space

vector modulation schemes.

Switching table for 5 level CHB inverter:

Table 4-5: Switching table for 5 level

Equal DC CHB inverter

Output Voltage

VAN

Switching State VH1 VH1 S11 S31 S12 S32

2E 1 0 1 0 E E

E

1 0 1 1 E 0 1 0 0 0 E 0 1 1 1 0 0 E 0 0 1 0 0 E

0

0 0 0 0 0 0 0 0 1 1 0 0 1 1 0 0 0 0 1 1 1 1 0 0 1 0 0 1 E -E 0 1 1 0 -E E

-E

0 1 1 1 -E 0 0 1 0 0 -E 0 1 1 0 1 0 -E 0 0 0 1 0 -E

-2E 0 1 0 1 -E -E

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4.3.2 Cascaded H-Bridge Inverter with Unequal DC voltage

To operate a seven level cascaded

multilevel converter consider two

unequal dc sources, the magnitude of

voltage of first dc source is E and the

second DC source is 2E. With unequal

DC voltages, the number of voltage

levels can be increased without

necessarily increasing the number of

H-bridge cells in cascade. This allows

more voltage steps in the inverter

output voltage waveform for a given

number of power cells. Figure 4-7

shows two inverter topologies,

where the dc voltages for the H- bridge cells are not equal. In the seven-level

topology, the dc voltages for H1H2 are E and 2E, respectively. The two-cell

inverter leg is able to produce seven voltage levels: 3E, 2E, E, 0, –E, –2E, and

–3E. The relationship between the voltage levels and their corresponding

switching states is summarized in Table. In the nine-level topology, the dc

voltage of H2 is three times that of H1. All the nine voltage levels can be

obtained by replacing the H2 output voltage of VH2 = ±2E in Table with VH2 =

±3E and then calculating the inverter phase voltage VAN.

Figure 4-7: One leg with unequal DC voltage

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Switching table for 7 level CHB inverter:

Table 4-6: Switching table for 7 level unequal DC CHB inverter

Output Voltage

VAN

Switching State VH1 VH1

S11 S31 S12 S32

3E 1 0 1 0 E 2E

2E 1 1 1 0 0 2E 0 0 1 0 0 2E

E 1 0 1 1 E 0 1 0 0 0 E 0 0 1 1 0 -E 2E

0 0 0 0 0 0 0 0 0 1 1 0 0 1 1 0 0 0 0 1 1 1 1 0 0

-E 1 0 0 1 E -2E 0 1 1 1 -E 0 0 1 0 0 -E 0

-2E 1 1 0 1 0 -2E 0 0 0 1 0 -2E

-3E 0 1 0 1 -E -2E

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5 Multilevel Inverter PWM schemes

Carrier based PWM schemes:

The carrier-based modulation schemes for multilevel inverters can be

generally classified into two categories: phase-shifted PWM and level-shifted

PWM.

Both modulation schemes can be applied to the CHB inverters.

Figure 5-1: Level-shifted PWM for a Seven-level CHB inverter

(mf = 15, ma = 0.8, fm = 50 Hz and fcr = 900 Hz)

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5.1 Level Shifted Sine PWM scheme

For carriers signals, the time values of each carrier waves are set to [0

1/600 1/300] while the outputs values are set according to the disposition of

carrier waves.

After comparing, the output signals of comparator are transmitted to the

IGBT. It requires (m-1) triangular carriers, all having the same frequency and

amplitude. The frequency modulation index is given by mf = fcr/fm. The

switching frequency of the inverter using the level-shifted modulation is equal

to the carrier frequency, that is, (device switching frequency) fC = fcr. Average

device switching frequency is device switching frequency) fC = fcr/ (m – 1).The

conduction time of the devices is not evenly distributed either.

𝑚𝑎 = ��𝑚

��𝑚(𝑚 − 1) 𝑓𝑜𝑟 0 ≤ 𝑚𝑎 ≤ 1

Where, 𝑉�� is the peak amplitude of the modulating wave 𝑉�� and ��cr is

the peak amplitude of each carrier wave.

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5.2 Types of Level Shifted Sine PWM

5.2.1 In-Phase Disposition IPD

In-Phase Disposition (IPD), where all carriers are in phase.

All the carrier signals are in phase.

Figure 5-2: Switching pattern produced using the IPD carrier-based PWM scheme:

(a) Two triangles and the modulation signal (b) S1RY (c) S2RY (d) S1RN (e) S2RN

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5.2.2 Alternative Phase opposite Disposition APOD

Alternative Phase Opposite Disposition (APOD), where all carriers are

alternatively in opposite disposition.

All the carriers above zero reference are in phase but are in opposition

with those below zero reference.

Figure 5-3: Simulation of carrier-based PWM scheme using APOD for a five-level inverter. (a) Modulation signal and carrier waveforms

(b) Phase “R” output voltage

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5.2.3 Phase Opposite Disposition POD

Phase Opposite Disposition (POD), where all carriers above the zero

reference are in phase but in opposition with those below the zero reference.

The modulating signal of each phase is displaced from each other by 120°.

All the carrier signals have same frequency FC and amplitude AC while the

modulating signal has a frequency of fm and amplitude of Am. The fc should be

in integer the multiples of fm with three-times. This is required for all the

modulating signal of all the three phases see the same carriers, as they are 120°

apart. The carrier waves and the modulating signals are compared and the

output of the comparator defines the output in the positive half cycle the

comparator output will have the value high, if the amplitude of the modulating

Figure 5-4: Simulation of carrier-based PWM scheme using POD.

(a) Modulation signal and phase carrier waveforms (b) Phase “R” output voltage.

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signal is greater than that of the carrier wave and zero otherwise. Similarly for

the negative half cycle, if the modulating signal is lower than the carrier wave

the output of the comparator is high and zero otherwise.

5.3 Phase Shifted Sine PWM scheme

In Phase Shifted Sine PWM all the triangular carriers have the same

Figure 5-5: Phase-shifted PWM for seven-level CHB inverters (mf = 3, ma = 0.8, fm = 50 Hz, and fcr = 180 Hz).

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frequency and same peak-peak amplitude .but there is a phase shift between

any two adjacent carrier waves. For m Voltage levels (m-1) carrier signals are

required and they are phase shifted with an angle of θ= (360°/m-1). The gate

signals are generated with proper comparison of carrier wave and modulating

signal.

In general, a multilevel inverter with m voltage levels requires (m – 1)

triangular carriers In the phase-shifted multicarrier modulation, all the

triangular carriers have the same frequency and the same peak-to-peak

amplitude, but there is a phase shift between any two adjacent carrier waves,

given by PhCR = 360°/(m – 1).

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6 Simulations

Simulations are major here mainly are done through PSIM, except for Space

Vector PWM and their related comparison cases which need computational and

algorithmic calculations which cannot be meet through PSIM. MATLAB Simulink

modelling is done and used for such cases.

Simulations are done to observe the output waveform, calculate the Total

harmonic Distortion THD, perform FFT analysis and observe the dominant

harmonics created and derive conclusions accordingly. Various PWM

techniques are also compared on the basic of their THDs, Data bus utilizations

and other parameters.

6.1 Simple PWM with Three phase Inverter

Figure 6-1: Sinusoidal PWM

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Figure 6-1 shows Gate pulses created by comparator action between the

carrier wave and the reference sinusoidal waves of R, Y and B phases.

Figure 6-2 shows Line voltage, phase voltage and line current for VDC =

540V. Observed voltages are Vph = 230V and VL= 400V for fC = 2 kHz & ma= 1.

6.2 Space Vector PWM for three phase Inverter

Figure 6-2: ma=1 VDC= 540V fC = 2 kHz

Figure 6-3: Simulink model used for Space Vector PWM

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Following SVPWM simulation curves are based on input VDC =500V; ma = 0.8; fC = 2 kHz

Figure 6-4: phase Voltage Vph = 230V

Figure 6-5: line Voltage VL = 400V

Figure 6-6: line current waveform

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Figure 6-8: THD analysis without filter

Figure 6-7: THD analysis with filter

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6.3 Comparison between SPWM and SVPWM

THD analysis of SVPWM and SPWM were compared and tabulated from table

6-1 to 6-3. It was observed that SVPWM generates lesser THD for every

corresponding SPWM for any given ma.

Table 6-1: SVPWM comparison for different modulation index

Table 6-2: SVPWM and SPWM comparison for different modulation index Without filter

Table 6-3: SVPM and SPWM comparison for different modulation index With filter

ma VL RMS VL THD VPH THD IL THD

1 400 52.48 % 52.62 % 1.63 %

0.8 356.8 76.84 % 76.89 % 1.72 %

0.6 308.8 106.06 % 106.07 % 2.07 %

ma SVPWM SPWM

VL THD IL THD VL THD IL THD

1 52.48 % 1.63 % 69.56 % 2.51 %

0.8 76.84 % 1.72 % 91.00 % 2.94 %

0.6 106.06 % 2.07 % 122.00 % 3.59 %

ma SVPWM SPWM

VL THD IL THD VL THD IL THD

1 4.00 % 0.23 % 4.93 % 0.20 %

0.8 4.25 % 0.17 % 5.14 % 0.26 %

0.6 5.12 % 0.17 % 5.82 % 0.29 %

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Figure 6.7 & 6.8 plots the variation of THD voltage as we vary the ma (amplitude

modulation index) for both SVPWM and SPWM.

Fig 6.7 is done without filter addition and while fig 6.8 values represents the

results with the addition of a filter circuit.

1 0.8 0.6

SVPWM 52.51 76.9 106.06

SPWM 69.56 91 122

52.51

76.9

106.06

69.56

91

122

40

50

60

70

80

90

100

110

120

130

140

Lin

e V

olt

age

THD

ma

THD vs ma without filter

1 0.8 0.6

SVPWM 4 4.25 5.12

SPWM 4.93 5.14 5.82

4

4.25

5.12

4.93

5.14

5.82

3.5

3.7

3.9

4.1

4.3

4.5

4.7

4.9

5.1

5.3

5.5

5.7

5.9

6.1

Lin

e V

olt

age

THD

THD vs ma with filter

Figure 6-9: THD vs ma without filter comparison between SVPWM and SPWM

Figure 6-10: THD vs ma with filter comparison between SVPWM and SPWM

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6.4 Simulation of 5-level Cascaded Inverter

The 5 level cascaded Inverter is basically obtained by cascading of 2 H-

Bridges in each phase legs. Pulse triggering is done via 2 methods, Phase shifted

sine PWM and Level shifted Sine PWM. Simulations on both are done as shown

in the next sections.

6.4.1 Multilevel Phase shifted Sine PWM Inverter

The simulation of phase shifted Sine PWM as done as shown in the figure 6-12.

The parameter setting was as below-

VDC-1 = 100V VDC-2 = 100V

ma = 0.8 mf = 15 i.e. fC = 750Hz

Figure 6-12 follows the said parameters.

Figure 6-11: PSIM simulation model for 5 level cascaded H-bridge Inverter

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Accordingly we obtain the following values-

RMS VL = 252.13V RMS Vph= 146.42V

THD Vph = 38 % THD VL = 29 %

Figure 6-12: Phase shifted Sine PWM – a) Phase shifted carrier waves with input phase sine waves

b) Phase voltage VRN c) Line Voltage VRY

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6.4.2 Multilevel level shifted Sine PWM Inverter

Simulation for all three types of Level shifted Sine PWM were performed,

namely IPD, POD and APOD. Which are shown in the subsequent following

diagrams. VDC used is 100V for all thee.

Figure 6-13 IPD gives the following results:

RMS Vph= 120.73V THD Vph= 38.28 %

RMS VL= 200V THD VL= 21.7 %

Figure 6-14 POD gives the following results:

RMS Vph= 120.41V THD Vph= 37.52 %

RMS VL= 207.84V THD VL= 35.17 %

Figure 6-13: IPD (In phase Disposition)

Figure 6-14: POD (Phase opposite Disposition)

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Figure 6-15 APOD gives the following results:

RMS Vph= 121.41V THD Vph= 36.48 %

RMS VL= 204.62V THD VL= 30 %

Comparing all three methods, IPD was observed as the better option,

which has lower VL THD value compared to POD and APOD.

Figure 6-15: APOD (Alternate Phase opposite Disposition)

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6.5 Simulation of 7-level Cascaded Inverter by

Unequal DC voltages

The 7 level simulation of cascaded Inverter by Unequal DC voltage is shown

in figure 6-16.

Parameters set during simulation of 7 level cascaded Inverter by unequal

DC voltages-

VDC-1 = 100V; VDC-2 = 200V; fC = 750Hz; ma = 0.8

Following values were obtain from the simulation-

RMS VL = 311.71V RMS Vph = 185V

THD VL=44.15 % THD Vph = 35.53 %

Figure 6-16: 7 level cascaded inverter with Unequal DC voltage

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THD values obtained for unequal DC voltage source are more than that

for equal voltage source CHB inverter, but the VRMS obtained is greater in this

case.

6.6 Comparison between phase shifted and level

shifted

Table 6-4: Comparison between phase shifted and level shifted

Table 6-5: THD (%) Analysis of Line Voltages of CHB Inverter

Based on Different Schemes

Comparison Phase Shifted Modulation

Level Shifted Modulation (IPD)

Device switching frequency

Same for all devices Different

Device conduction period Same for all devices Different

Rotating of switching patterns

Not required Required

Line to line voltage THD Good Better

Comparison Phase Shifted Modulation

Level Shifted Modulation (IPD)

Device switching frequency

Same for all devices Different

Device conduction period Same for all devices Different

Rotating of switching patterns

Not required Required

Line to line voltage THD Good Better

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Table 6-6: THD (%) Analysis of Line Voltages of CHB Inverter based on Different Schemes at mf=20 VDC=100V

ma Phase shifted IPD 7 level- 2 cell ( unequal DC)

1 25 16.9 27.65

0.8 25 21.73 36.01

0.6 27 25.5 40.72

0.4 68 25.57 79.61

0.2 68.6 25.59 153.55

0.2 0.4 0.6 0.8 1

Phase Shifted PWM 68.6 68 27 25 25

In Phase Disposition 25.59 25.57 25.5 21.73 16.9

7 level 2 Cell 153.55 79.61 40.72 36.01 27.65

68.6 68

27 25 2525.59 25.57 25.5 21.73 16.9

153.55

79.61

40.72 36.0127.65

10

30

50

70

90

110

130

150

Vo

ltag

e TH

D

fs=1kHz (frequency of Switching device) Five Level Inverter

Figure 6-17: THD plot between different PWM schemes

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6.7 Conclusions

Two multicarrier based PWM schemes, the phase- and level-shifted

modulations, are presented. Various aspects associated with the modulation

schemes for the CHB multilevel inverters are discussed, which include gate

signal arrangements, spectrum analyses, and THD profiles. The performance of

the modulation schemes is compared.

PWM strategies viz. SPWM and SVPWM are implemented in

MATLAB/SIMULINK software and its performance is compared with

conventional PWM techniques. Owing to their fixed carrier frequencies fC in

conventional PWM strategies, there are cluster harmonics around the multiples

of carrier frequency. PWM strategies viz. Sinusoidal PWM and SVPWM utilize a

changing carrier frequency to spread the harmonics continuously to a wideband

area so that the peak harmonics are reduced greatly.

In this project first comparative analysis of Space Vector PWM with

conventional SPWM for a two level Inverter is carried out. The Simulation study

reveals that SVPWM gives 15% enhanced fundamental output with better

quality i.e. lesser THD compared to SPWM.

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7 References

1. W. A. Hill and C. D. Harbourt, “Performance of Medium Voltage Multilevel Inverters”,

IEEE Industry Applications Society (IAS) Conference, Vol. 2, pp. 1186–1192, 1999.

2. P. W. Hammond, “A New Approach to Enhance Power Quality for Medium Voltage AC

Drives”, IEEE Transactions on Industry Applications, Vol. 33, No. 1, pp. 202–208, 1997.

3. P.S. Bhimbra, “Power Electronics”, 2 ed., New Delhi, Khanna Publications, 2004.

4. G. Narayanan, IISc(Bangalore), Lectures on “Pulse width Modulation for Power

Electronic converters’” NTPEL

5. Muhammad H. Rashid, “Power Electronics Circuits, devices, and Applications”,

Prentice-Hall of India Private Limited, Third Edition, 2004.

6. N. Mohan, T. M. Undeland, et al, “Power Electronics - Converters, Applications and

Design”, 3rd edition, John Wiley & Sons, New York, 2003.

7. Hong Hee Lee, Phan Quoc Dzung, Le Dinh Khoa, Le Minh Phuong & Huynh Tan Thanh,

“The adaptive space vector PWM for four switch three phase inverter fed induction

motor with DC – Link Voltage Imbalance” in Hong School of Electrical Engineering,

University of Ulsan, Korea, 2008, IEEE, DOI: 10.1109/TENCON.2008.4766516

8. Kapil Jain, Pradyumn Chaturvedi, “MATlab -based Simulation & Analysis of Three -

level SPWM Inverter”, International Journal of Soft Computing and Engineering

(IJSCE), March 2012, Volume-2, Issue-1.

9. Moin Sheik, “Multilevel Inverter topologies and control scheme” [Online],

Available:https://www.academia.edu/6742849/Multilevel_Inverter_3-

level_topologies_Diode_and_capacitor_clamped_and_controlscheme_spwm

10. Hind Djeghloud and Hocine Benalla, “Space Vector Pulse Width Modulation Applied

to Three-Level Voltage Inverter”, 5th International Conference on Technology and

Automation ICTA’05, Thessaloniki, Greece, Oct 2010.

11. Jae Hyeong Seo, Chang Ho Choi, Dong Seok Hyun, “A New Simplified space-Vector

PWM Method for Three-Level Inverters”, IEEE Transactions on Power Electronics,

Volume 16, Issue 4, July 2010, Pages 545 – 550.

12. Dong-Myung Lee, Jin-Woo Jung, and Sang-Shin Kwak, “Simple Space Vector PWM

Scheme for 3-level NPC Inverters Including the Over modulation Region”, Journal of

Power Electronics, Vol. 11, No. 5, September 2011.

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8 Appendices

8.1 Appendix 1- List of Figures

Figure 2-1: Voltage source inverter................................................................. 10

Figure 2-2: Current source inverter................................................................. 11

Figure 2-3: Current source inverter................................................................. 12

Figure 2-4: Basic three phase inverter ............................................................ 13

Figure 3-1: PWM Duty cycle comparison ........................................................ 18

Figure 3-2: Bipolar Sine PWM ......................................................................... 21

Figure 3-3: Unipolar Sine PWM ....................................................................... 21

Figure 3-4: Coordinate Transformation RYB to d-q ......................................... 24

Figure 3-5: Three phase inverter ..................................................................... 25

Figure 3-6: VREF rotating along Voltage Space Vectors..................................... 26

Figure 3-7: Equivalent Switching pattern of the space vectors ....................... 27

Figure 3-8: Space Vector Diagram ................................................................... 27

Figure 3-9: Sector Distribution ........................................................................ 28

Figure 3-10: Sector 1 VREF approximation over a sampling time .................... 29

Figure 3-11: Switching Sequence for all VREF pattern in sector (only T1 T2 T0

varies) ............................................................................................................. 30

Figure 3-12: Graphical switching pattern for different sectors ....................... 30

Figure 3-13: Switching plots for all 6 sectors................................................... 34

Figure 3-14: Switching states of the inverter .................................................. 36

Figure 3-1: Typical Inverter Display panel ....................................................... 38

Figure 4-2: Types of Multilevel Inverter .......................................................... 41

Figure 4-3: Topology of the diode-clamped inverter (a) three-level inverter, . 42

Figure 4-4: Topology of the Flying Capacitor Multilevel inverter .................... 44

Figure 4-5: a) Inverter Single Stage b) 5 level Cascaded Inverter .................... 47

Figure 4-6: CHB with equal DC voltage ................Error! Bookmark not defined.

Figure 4-7: One leg with unequal DC voltage .......Error! Bookmark not defined.

Figure 5-1: Level-shifted PWM for a ............................................................... 54

Figure 5-2: Switching pattern produced.......................................................... 56

Figure 5-3: Simulation of carrier-based PWM scheme using APOD for a five-level

inverter. (a) Modulation signal and carrier waveforms ................................... 57

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Figure 5-4: Simulation of carrier-based PWM scheme .................................... 58

Figure 5-5: Phase-shifted PWM for seven-level CHB inverters ........................ 59

Figure 6-1: Sinusoidal PWM ............................................................................ 61

Figure 6-2: ma=1 VDC= 540V fC = 2 kHz ............................................................. 62

Figure 6-3: Simulink model used for Space Vector PWM ................................ 62

Figure 6-4: phase Voltage Vph = 230V .............................................................. 63

Figure 6-5: line Voltage VL = 400V ................................................................... 63

Figure 6-6: line current waveform .................................................................. 63

Figure 6-7: THD analysis with filter ................................................................. 64

Figure 6-8: THD analysis without filter ............................................................ 64

Figure 6-9: THD vs ma without filter comparison between SVPWM and SPWM

....................................................................................................................... 66

Figure 6-10: THD vs ma with filter comparison between SVPWM and SPWM . 66

Figure 6-11: PSIM simulation model for 5 level cascaded H-bridge Inverter ... 67

Figure 6-12: Phase shifted Sine PWM – .......................................................... 68

Figure 6-13: IPD (In phase Disposition) ........................................................... 69

Figure 6-14: POD (Phase opposite Disposition) ............................................... 69

Figure 6-15: APOD (Alternate Phase opposite Disposition) ............................. 70

Figure 6-16: 7 level cascaded inverter with Unequal DC voltage .................... 71

Figure 6-17: THD plot between different PWM schemes ................................ 73

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8.2 Appendix 2-List of Tables

Table 3-1: Switching time for each sector 1-6 ................................................. 35

Table 3-2: Output Voltage table ..................................................................... 37

Table 4-1: Comparison between Conventional Inverters ................................ 39

Table 4-2: Switching sequence for 5 level Diode Clamped Inverter ................ 42

Table 4-3: Switching sequence for 5 level Inverter ......................................... 46

Table 4-4: Comparison of multilevel inverter Topologies ............................... 48

Table 4-5: Switching table for 5 level .............................................................. 51

Table 4-6: Switching table for 7 level unequal DC CHB inverter ...................... 53

Table 6-1: SVPWM comparison for different modulation index ..................... 65

Table 6-2: SVPWM and SPWM comparison for different modulation index ... 65

Table 6-3: SVPM and SPWM comparison for different modulation index....... 65

Table 6-4: Comparison between phase shifted and level shifted .................... 72

Table 6-5: THD (%) Analysis of Line Voltages of CHB Inverter ......................... 72

Table 6-6: THD (%) Analysis of Line Voltages of CHB Inverter based on Different

Schemes at mf=20 VDC=100V ........................................................................... 73