A New Cascaded Multilevel Inverter withReduced Number of Switches

Abstract—

This paper proposes a new topology for cascaded multilevel inverters. This structure

consists of series connection of proposed basic unit blocks which are built with both

unidirectional and bidirectional switches. The proposed structure has some advantages including:

reduction in the number of switches and driver circuits, cost and installation area. Three

algorithms for determination of dc voltage sources' magnitudes have also been proposed. The

algorithms can produce all odd and even levels at the output voltage. The proposed structure also

has fewer dc voltage sources variety and less maximum blocking voltage of switches compared

to conventional inverters. The capability of proposed structure in producing all odd and even

output voltage levels is proved by simulation result for a 21-level inverter.

1. INTRODUCTION

Nowadays, multilevel inverters have become more attractive for their use in high-voltage

and high-power applications. In multilevel inverters, the desired output voltage is achieved by

suitable combination of multiple low dc voltage sources used at the input side. As the number of

dc sources is increased, the output voltage becomes closer to a pure sinusoidal waveform. The

required dc voltage can be chosen from different sources such as batteries, photovoltaic, fuel

cells, capacitors, the rectified output voltage of wind turbines, and other similar dc voltage

sources [1-3]. Some advantages of multilevel inverters are good power quality, low switching

losses and electromagnetic compatibility due to the low dv/dt transitions [4].

Some of the fundamental multilevel topologies include the cascaded H-bridge structures

[5], flying capacitor [6], and diode-clamped converter [7]. Other proposed configurations for

multilevel converters are mainly derived from these three basic topologies [2], [4], [8-9]. Among

these three topologies, cascaded multilevel converter has got more attention in literatures [10-

11]. This paper particularly focuses on Cascaded multilevel converters. This topology is divided

into two symmetrical and asymmetrical structures. If all dc voltage sources are equal, the inverter

is then known as symmetrical multilevel inverter, otherwise it is known as asymmetrical

multilevel inverter. In asymmetrical multilevel inverters, the number of produced output voltage

levels is high when compared to symmetrical multilevel inverter with the same number of dc

voltage sources and switches [12]. One of the main challenges in multilevel inverters is to reduce

the number of power electronic switches while considering operational conditions. Although low

voltage rate switches can be utilized in a multilevel inverter, each switch requires related deriver

circuits. This may cause the overall circuit to be more expensive and complex. So in practical

implementation reducing the number of switches and gate deriver circuits are very important.

In recent years, many configurations are presented in order to reduce the number of

overall switches used in cascaded multilevel inverters. Some of these structures are in references

[4] and [13]. The presented structures aim in reducing the number of switches while having the

availability to produce all odd and even levels at the output voltage. The structures presented in

these literatures have significant reduction in the number of switches and consequently reduction

in installation area. However in the structures of [8] and [13], the implemented switches are

bidirectional (consisting of two IGBTs and two anti-parallel diodes). So the total number of

IGBTs is high which increases cost. Nevertheless, because of using one deriver circuit for each

switch, the overall numbers of deriver circuits needed for the recommended topologies are fewer

compared to conventional multilevel inverter.

This paper proposes a new topology for cascaded multilevel inverters which uses a

combination of bidirectional and unidirectional switches. It should be considered that by suitable

combination of bidirectional and unidirectional switches, fewer deriver circuits and IGBTs can

be achieved. Moreover, to produce all odd and even levels at the output voltage, three procedures

for determination of dc voltage sources' magnitudes have also been proposed. The capability of

proposed structure in producing all odd and even output voltage levels is proved by simulation

result for a 21-level inverter.

MULTILEVEL INVERTER

An inverter is an electrical device that converts direct current (DC) to alternating current (AC);

the converted AC can be at any required voltage and frequency with the use of appropriate

transformers, switching, and control circuits. Static inverters have no moving parts and are used

in a wide range of applications, from small switching power supplies in computers, to large

electric utility high-voltage direct current applications that transport bulk power. Inverters are

commonly used to supply AC power from DC sources such as solar panels or batteries.

The electrical inverter is a high-power electronic oscillator. It is so named because early

mechanical AC to DC converters were made to work in reverse, and thus were "inverted", to

convert DC to AC. The inverter performs the opposite function of a rectifier

Cascaded H-Bridges inverter

A single-phase structure of an m-level cascaded inverter is illustrated in Figure 31.1. Each

separate dc source (SDCS) is connected to a single-phase full-bridge, or H-bridge, inverter. Each

inverter level can generate three different voltage outputs, +Vdc, 0, and –Vdc by connecting the dc

source to the ac output by different combinations of the four switches, S1, S2, S3, and S4. To

obtain +Vdc, switches S1 and S4 are turned on, whereas –Vdc can be obtained by turning on

switches S2 and S3. By turning on S1 and S2 or S3 and S4, the output voltage is 0. The ac outputs of

each of the different full-bridge inverter levels are connected in series such that the synthesized

voltage waveform is the sum of the inverter outputs. The number of output phase voltage levels

m in a cascade inverter is defined by m = 2s+1, where s is the number of separate dc sources. An

example phase voltage waveform for an 11-level cascaded H-bridge inverter with 5 SDCSs and 5

full bridges is shown in Figure 31.2. The phase voltage van = va1 + va2 + va3 + va4 + va5.

For a stepped waveform such as the one depicted in Figure 31.2 with s steps, the Fourier

Transform for this waveform follows

Single-phase structure of a multilevel cascaded H-bridges inverter

Output phase voltage waveform of an 11-level cascade inverter with 5 separate dc sources.

The magnitudes of the Fourier coefficients when normalized with respect to Vdc are as

follows:

The conducting angles, θ1, θ2, ..., θs, can be chosen such that the voltage total harmonic

distortion is a minimum. Generally, these angles are chosen so that predominant lower frequency

harmonics, 5th, 7th, 11th, and 13th, harmonics are eliminated [25]. More detail on harmonic

elimination techniques will be presented in the next section.

Multilevel cascaded inverters have been proposed for such applications as static var

generation, an interface with renewable energy sources, and for battery-based applications.

Three-phase cascaded inverters can be connected in wye, as shown in Figure 31.3, or in delta.

Peng has demonstrated a prototype multilevel cascaded static var generator connected in parallel

with the electrical system that could supply or draw reactive current from an electrical system

[20-23]. The inverter could be controlled to either regulate the power factor of the current drawn

from the source or the bus voltage of the electrical system where the inverter was connected.

Peng [20] and Joos [24] have also shown that a cascade inverter can be directly connected in

series with the electrical system for static var compensation. Cascaded inverters are ideal for

connecting renewable energy sources with an ac grid, because of the need for separate dc

sources, which is the case in applications such as photovoltaic’s or fuel cells.

Cascaded inverters have also been proposed for use as the main traction drive in electric

vehicles, where several batteries or ultracapacitors are well suited to serve as SDCSs [19, 26].

The cascaded inverter could also serve as a rectifier/charger for the batteries of an electric

vehicle while the vehicle was connected to an ac supply as shown in Figure 31.3. Additionally,

the cascade inverter can act as a rectifier in a vehicle that uses regenerative braking.

Three-phase wye-connection structure for electric vehicle motor drive and battery charging.

The main advantages and disadvantages of multilevel cascaded H-bridge converters are

as follows

Advantages:

The number of possible output voltage levels is more than twice the number of dc sources

(m = 2s + 1).

The series of H-bridges makes for modularized layout and packaging. This will enable

the manufacturing process to be done more quickly and cheaply.

Disadvantages:

Separate dc sources are required for each of the H-bridges. This will limit its application

to products that already have multiple SDCSs readily available.

Diode-Clamped Multilevel Inverter

The neutral point converter proposed by Nabae, Takahashi, and Akagi in 1981 was

essentially a three-level diode-clamped inverter [5]. In the 1990s several researchers published

articles that have reported experimental results for four-, five-, and six-level diode-clamped

converters for such uses as static var compensation, variable speed motor drives, and high-

voltage system interconnections [18-31]. A three-phase six-level diode-clamped inverter is

shown in Figure 31.5. Each of the three phases of the inverter shares a common dc bus, which

has been subdivided by five capacitors into six levels. The voltage across each capacitor is V dc,

and the voltage stress across each switching device is limited to Vdc through the clamping diodes.

Table 31.1 lists the output voltage levels possible for one phase of the inverter with the negative

dc rail voltage V0 as a reference. State condition 1 means the switch is on, and 0 means the

switch is off. Each phase has five complementary switch pairs such that turning on one of the

switches of the pair requires that the other complementary switch be turned off. The

complementary switch pairs for phase leg a are (Sa1, Sa’1), (Sa2, Sa’2), (Sa3, Sa’3), (Sa4, Sa’4), and (Sa5,

Sa’5). Table 31.1 also shows that in a diode-clamped inverter, the switches that are on for a

particular phase leg are always adjacent and in series. For a six-level inverter, a set of five

switches is on at any given time.

Three-phase six-level structure of a diode-clamped inverter.

Diode-clamped six-level inverter voltage levels and corresponding switch states.

Advantages:

All of the phases share a common dc bus, which minimizes the capacitance requirements

of theconverter. For this reason, a back-to-back topology is not only possible but also

practical for uses such as a high-voltage back-to-back inter-connection or an adjustable

speed drive.

The capacitors can be pre-charged as a group.

Efficiency is high for fundamental frequency switching.

Disadvantages:

Real power flow is difficult for a single inverter because the intermediate dc levels will

tend to overcharge or discharge without precise monitoring and control.

The number of clamping diodes required is quadratically related to the number of levels,

which can be cumbersome for units with a high number of levels.

Flying Capacitor Multilevel Inverter

Meynard and Foch introduced a flying-capacitor-based inverter in 1992 [32]. The structure of

this inverter is similar to that of the diode-clamped inverter except that instead of using clamping

diodes, the inverter uses capacitors in their place. The circuit topology of the flying capacitor

multilevel inverter is shown in Figure 31.7. This topology has a ladder structure of dc side

capacitors, where the voltage on each capacitor differs from that of the next capacitor. The

voltage increment between two adjacent capacitor legs gives the size of the voltage steps in the

output waveform.

Three-phase six-level structure of a flying capacitor inverter.

One advantage of the flying-capacitor-based inverter is that it has redundancies for inner

voltage levels; in other words, two or more valid switch combinations can synthesize an output

voltage. Table 31.2 shows a list of all the combinations of phase voltage levels that are possible

for the six-level circuit shown in Figure 31.7. Unlike the diode-clamped inverter, the flying-

capacitor inverter does not require all of the switches that are on (conducting) be in a consecutive

series. Moreover, the flying-capacitor inverter has phase redundancies, whereas the diode-

clamped inverter has only line-line redundancies [2, 3, 33]. These redundancies allow a choice of

charging/discharging specific capacitors and can be incorporated in the control system for

balancing the voltages across the various levels.

In addition to the (m-1) dc link capacitors, the m-level flying-capacitor multilevel inverter will

require (m-1) × (m-2)/2 auxiliary capacitors per phase if the voltage rating of the capacitors is

identical to that of the main switches. One application proposed in the literature for the

multilevel flying capacitor is static var generation [2, 3]. The main advantages and disadvantages

of multilevel flying capacitor converters are as follows [2, 3].

Advantages:

Phase redundancies are available for balancing the voltage levels of the capacitors.

Real and reactive power flow can be controlled.

The large number of capacitors enables the inverter to ride through short duration outages

and deep voltage sags.

Disadvantages:

Control is complicated to track the voltage levels for all of the capacitors. Also,

precharging all of the capacitors to the same voltage level and startup are complex.

Switching utilization and efficiency are poor for real power transmission.

The large numbers of capacitors are both more expensive and bulky than clamping diodes

in multilevel diode-clamped converters. Packaging is also more difficult in inverters with

a high number of levels.

Flying-capacitor six-level inverter redundant voltage levels and corresponding switch states

Other Multilevel Inverter Structures

Besides the three basic multilevel inverter topologies previously discussed, other

multilevel converter topologies have been proposed; however, most of these are “hybrid” circuits

that are combinations of two of the basic multilevel topologies or slight variations to them.

Additionally, the combination of multilevel power converters can be designed to match with a

specific application based on the basic topologies. In the interest of completeness, some of these

will be identified and briefly described.

A. Generalized Multilevel Topology

Existing multilevel converters such as diode-clamped and capacitor-clamped multilevel

converters can be derived from the generalized converter topology called P2 topology proposed

by Peng [34] as illustrated in Figure 31.8. The generalized multilevel converter topology can

balance each voltage level by itself regardless of load characteristics, active or reactive power

conversion and without any assistance from other circuits at any number of levels automatically.

Thus, the topology provides a complete multilevel topology that embraces the existing multilevel

converters in principle.

Figure 31.8 shows the P2 multilevel converter structure per phase leg. Each switching device,

diode, or capacitor’s voltage is 1Vdc, for instance, 1/ (m-1) of the DC-link voltage. Any converter

with any number of levels, including the conventional bi-level converter can be obtained using

this generalized topology [1, 34].

Generalized P2 multilevel converter topology for one phase leg.

B. Mixed-Level Hybrid Multilevel Converter

To reduce the number of separate DC sources for high-voltage, high-power applications

with multilevel converters, diode-clamped or capacitor-clamped converters could be used to

replace the full-bridge cell in a cascaded converter [35]. An example is shown in Figure 31.9.

The nine-level cascade converter incorporates a three-level diode-clamped converter as the cell.

The original cascaded H-bridge multilevel converter requires four separate DC sources for one

phase leg and twelve for a three-phase converter. If a five-level converter replaces the full-bridge

cell, the voltage level is effectively doubled for each cell. Thus, to achieve the same nine voltage

levels for each phase, only two separate DC sources are needed for one phase leg and six for a

three-phase converter. The configuration has mixed-level hybrid multilevel units because it

embeds multilevel cells as the building block of the cascade converter. The advantage of the

topology is it needs less separate DC sources. The disadvantage for the topology is its control

will be complicated due to its hybrid structure.

Mixed-level hybrid unit configuration using the three-level diode-clamped converter as the

cascaded converter cell to increase the voltage levels.

Zero-voltage switching capacitor-clamped inverter circuit.

C. Soft-Switched Multilevel Converter

Some soft-switching methods can be implemented for different multilevel converters to

reduce the switching loss and to increase efficiency. For the cascaded converter, because each

converter cell is a bi-level circuit, the implementation of soft switching is not at all different from

that of conventional bi-level converters. For capacitor-clamped or diode-clamped converters,

soft-switching circuits have been proposed with different circuit combinations. One of soft-

switching circuits is a zero-voltage-switching type which includes auxiliary resonant

commutated pole (ARCP), coupled inductor with zero-voltage transition (ZVT), and their

combinations [1, 36] as shown in Figure 31.10.

D. Back-to-Back Diode-Clamped Converter

Two multilevel converters can be connected in a back-to-back arrangement and then the

combination can be connected to the electrical system in a series-parallel arrangement as shown

in Figure 31.11. Both the current demanded from the utility and the voltage delivered to the load

can be controlled at the same time. This series-parallel active power filter has been referred to as

a universal power conditioner [37-43] when used on electrical distribution systems and as a

universal power flow controller [44-48] when applied at the transmission level. Previously, Lai

and Peng [30] proposed the back-to-back diode-clamped topology shown in Figure 31.12 for use

as a high-voltage dc inter connection between two asynchronous ac systems or as a

rectifier/inverter for an adjustable speed drive for high-voltage motors. The diode-clamped

inverter has been chosen over the other two basic multilevel circuit topologies for use in a

universal power conditioner for the following reasons:

All six phases (three on each inverter) can share a common dc link. Conversely, the

cascade inverter requires that each dc level be separate, and this is not conducive to a

back-to-back arrangement.

The multilevel flying-capacitor converter also shares a common dc link; however,

each phase leg requires several additional auxiliary capacitors. These extra capacitors

would add substantially to the cost and the size of the conditioner.

Because a diode-clamped converter acting as a universal power conditioner will be expected to

compensate for harmonics and/or operate in low amplitude modulation index regions, a more

sophisticated, higher-frequency switch control than the fundamental frequency switching method

will be needed. For this reason, multilevel space vector and carrier-based PWM approaches are

compared in the next section, as well as novel carrier-based PWM methodologies.

Multilevel Converter PWM Modulation Strategies

Pulse width modulation (PWM) strategies used in a conventional inverter can be

modified to use in multilevel converters. The advent of the multilevel converter PWM

modulation methodologies can be classified according to switching frequency as illustrated in

Figure 31.13. The three multilevel PWM methods most discussed in the literature have been

multilevel carrier-based PWM, selective harmonic elimination, and multilevel space vector

PWM; all are extensions of traditional two-level PWM strategies to several levels. Other

multilevel PWM methods have been used to a much lesser extent by researchers; therefore, only

the three major techniques will be discussed in this chapter.

Series-parallel connection to electrical system of two back-to-back inverters.

Six-level diode-clamped back-to-back converter structure.

Classification of PWM multilevel converter modulation strategies

Multilevel converter design example

Number of levels and voltage rating of active devices

In a multilevel inverter, determining the number of levels will be one of the most

important factors because this affects many of the other sizing factors and control techniques.

Tradeoffs in specifying the number of levels that the power conditioner will need and the

advantages and complexity of having multiple voltage levels available are the primary

differences that set a multilevel filter apart from a single level filter.

As a starting point, known is the nominal RMS voltage rating, Vnom, of the electrical system to

which the diode clamped power conditioner will be connected. The dc link voltage must be at

least as high as the amplitude of the nominal line-neutral voltage at the point of connection,

or2⋅Vnom.

The parallel inverter must be able to inject currents by imposing a voltage across the parallel

inductors, LPI, that is the difference between the load voltage VL and parallel inverter output

voltage VPI. The most difficult time to impose a voltage across the inductors is when the load

voltage waveform is at its maximum or minimum. Simulation results have shown that the

amplitude of the desired load voltage Vnom should not be more than 70 percent of the overall dc

link voltage for the parallel inverter to have sufficient margin to inject appropriate compensation

currents. Without this margin, complete compensation of reactive currents may not be possible.

This margin can be incorporated into a design factor for the inverter. Because the dc link voltage

and the voltage at the connection point can both vary, the design factor used in the rating

selection process incorporates these elements as well as the small voltage drops that occur in the

inverters during active device conduction.

The product of the number of the active devices in series (m-1) and the voltage rating of the

devices Vdev must then be such that

The minimum number of levels and the voltage rating of the active devices (IGBTs, GTOs,

power MOSFETs, etc.) are inversely related to each other. More levels in the inverter will lower

the required voltage device rating of individual devices; or looking at it another way, a higher

voltage rating of the devices will enable a fewer minimum number of levels to be used.

Electrical system connection of multilevel diode-clamped power conditioner.

Increasing the number of levels does not affect the total voltage blocking capability of the active

devices in each phase leg because lower device ratings can be used. Some of the benefits of

using more than the minimum required number of levels in a diode clamped inverter are as

follows:

1. Voltage stress across each device is lower. Both active devices and dc link capacitors could be

used that have lower voltage ratings (which sometimes are much cheaper and have greater

availability).

2. The inverter will have a lower EMI because the dV/dt during each switching will be lower.

3. The output of the waveform will have more steps, or degrees of freedom, which enables the

output waveform to more closely track a reference waveform.

4. Lower individual device switching frequency will achieve the same results as an inverter with

a fewer number of levels and higher device switching frequency. Or the switching frequency can

be kept the same as that in an inverter with a fewer number of levels to achieve a better

waveform.

The drawbacks of using more than the required minimum number of levels are as follows:

1. Six active device control signals (one for each phase of the parallel inverter and the series

inverter) are needed for each hardware level of the inverter – i.e., 6⋅(m-1) control signals.

Additional levels require more computational resources and add complexity to the control.

2. If the blocking diodes used in the inverter have the same rating as the active devices, their

number increases dramatically because 6⋅(m-2)⋅(m-1) diodes would be required for the back-to-

back structure.

Considering the trade-offs between the number of levels and the voltage rating of the devices

will generally lead the designer to choose an appropriate value for each.

Fault diagnosis in multilevel converters

Since a multilevel converter is normally used in medium to high power applications, the

reliability of the multilevel converter system is very important. For instance industrial drive

applications in manufacturing plants are dependent upon induction motors and their inverter

systems for process control. Generally, the conventional protection systems are passive devices

such as fuses, overload relays, and circuit breakers to protect the inverter systems and the

induction motors. The protection devices will disconnect the power sources from the multilevel

inverter system whenever a fault occurs, stopping the operated process. Downtime of

manufacturing equipment can add up to be thousands or hundreds of thousands of dollars per

hour, therefore fault detection and diagnosis is vital to a company’s bottom line. In order to

maintain continuous operation for a multilevel inverter system, knowledge of fault behaviors,

fault prediction, and fault diagnosis are necessary. Faults should be detected as soon as possible

after they occur, because if a motor drive runs continuously under abnormal conditions, the drive

or motor may quickly fail.

The possible structure for a fault diagnosis system is illustrated in Figure 31.33. The

system is composed of four major states: feature extraction, neural network classification, fault

diagnosis, and switching pattern calculation with gate signal output. The feature extraction

performs the voltage input signal transformation, with rated signal values as important features,

and the output of the transformed signal is transferred to the neural network classification. The

networks are trained with both normal and abnormal data for the MLID; thus, the output of this

network is nearly 0 and 1 as binary code. The binary code is sent to the fault diagnosis to decode

the fault type and its location. Then, the switching pattern is calculated to reconfigure the

multilevel inverter.

Switching patterns and the modulation index of other active switches can be adjusted to

maintain voltage and current in a balanced condition after reconfiguration recovers from a fault.

The MLID can continuously operate in a balanced condition; of course, the MLID will not be

able to operate at its rated power. Therefore, the MLID can operate in balanced condition at

reduced power after the fault occurs until the operator locates and replaces the damaged switch

Structure of fault diagnosis system of a multilevel cascaded H-bridges inverter.

Applications:

DC power source utilization

Inverter designed to provide 115 VAC from the 12 VDC source provided in an

automobile. The unit shown provides up to 1.2 amperes of alternating current, or enough to

power two sixty watt light bulbs.

An inverter converts the DC electricity from sources such as batteries, solar panels, or

fuel cells to AC electricity. The electricity can be at any required voltage; in particular it can

operate AC equipment designed for mains operation, or rectified to produce DC at any desired

voltage.

Grid tie inverters can feed energy back into the distribution network because they

produce alternating current with the same wave shape and frequency as supplied by the

distribution system. They can also switch off automatically in the event of a blackout.

Micro-inverters convert direct current from individual solar panels into alternating

current for the electric grid.[1]

Uninterruptible power supplies

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 is used to

supply DC power to recharge the batteries.

Induction heating

Inverters convert low frequency main AC power to a higher frequency for use in

induction heating. To do this, AC power is first rectified to provide DC power. The inverter then

changes the DC power to high frequency AC power.

HVDC power transmission

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.

Variable-frequency drives

A variable-frequency drive controls the operating speed of an AC motor by controlling

the frequency and voltage of the power supplied to the motor. An inverter provides the controlled

power. In most cases, the variable-frequency drive includes a rectifier so that DC power for the

inverter can be provided from main AC power. Since an inverter is the key component, variable-

frequency drives are sometimes called inverter drives or just inverters.

Electric vehicle drives

Adjustable speed motor control inverters are currently used to power the traction motors

in some electric and diesel-electric rail vehicles as well as some battery electric vehicles and

hybrid electric highway vehicles such as the Toyota Prius. Various improvements in inverter

technology are being developed specifically for electric vehicle applications.[2] In vehicles with

regenerative braking, the inverter also takes power from the motor (now acting as a generator)

and stores it in the batteries.

Air conditioning

An air conditioner bearing the inverter tag uses a variable-frequency drive to control the

speed of the motor and thus the compressor.

The general case

A transformer allows AC power to be converted to any desired voltage, but at the same

frequency. Inverters, plus rectifiers for DC, can be designed to convert from any voltage, AC or

DC, to any other voltage, also AC or DC, at any desired frequency. The output power can never

exceed the input power, but efficiencies can be high, with a small proportion of the power

dissipated as waste heat.

PULSE WIDTH MODULATION

What is PWM?

Pulse Width Modulation (PWM) is the most effective means to achieve constant

voltage battery charging by switching the solar system controller’s power devices. When in

PWM regulation, the current from the solar array tapers according to the battery’s condition and

recharging needs Consider a waveform such as this: it is a voltage switching between 0v and

12v. It is fairly obvious that, since the voltage is at 12v for exactly as long as it is at 0v, then a

'suitable device' connected to its output will see the average voltage and think it is being fed 6v -

exactly half of 12v. So by varying the width of the positive pulse - we can vary the 'average'

voltage.

Similarly, if the switches keep the voltage at 12 for 3 times as long as at 0v, the average

will be 3/4 of 12v - or 9v, as shown below.

and if the output pulse of 12v lasts only 25% of the overall time, then the average is

By varying - or 'modulating' - the time that the output is at 12v (i.e. the width of the

positive pulse) we can alter the average voltage. So we are doing 'pulse width modulation'. I said

earlier that the output had to feed 'a suitable device'. A radio would not work from this: the radio

would see 12v then 0v, and would probably not work properly. However a device such as a

motor will respond to the average, so PWM is a natural for motor control.

Pulse Width modulator

So, how do we generate a PWM waveform? It's actually very easy, there are circuits

available in the TEC site. First you generate a triangle waveform as shown in the diagram below.

You compare this with a d.c voltage, which you adjust to control the ratio of on to off time that

you require. When the triangle is above the 'demand' voltage, the output goes high. When the

triangle is below the demand voltage, the

When the demand speed it in the middle (A) you get a 50:50 output, as in black. Half the

time the output is high and half the time it is low. Fortunately, there is an IC (Integrated circuit)

called a comparator: these come usually 4 sections in a single package. One can be used as the

oscillator to produce the triangular waveform and another to do the comparing, so a complete

oscillator and modulator can be done with half an IC and maybe 7 other bits.

The triangle waveform, which has approximately equal rise and fall slopes, is one of the

commonest used, but you can use a saw tooth (where the voltage falls quickly and rinses slowly).

You could use other waveforms and the exact linearity (how good the rise and fall are) is not too

important.

Traditional solenoid driver electronics rely on linear control, which is the application of a

constant voltage across a resistance to produce an output current that is directly proportional to

the voltage. Feedback can be used to achieve an output that matches exactly the control signal.

However, this scheme dissipates a lot of power as heat, and it is therefore very inefficient.

A more efficient technique employs pulse width modulation (PWM) to produce the

constant current through the coil. A PWM signal is not constant. Rather, the signal is on for part

of its period, and off for the rest. The duty cycle, D, refers to the percentage of the period for

which the signal is on. The duty cycle can be anywhere

from 0, the signal is always off, to 1, where the signal is constantly on. A 50% D results in a

perfect square wave. (Figure 1)

A solenoid is a length of wire wound in a coil. Because of this configuration, the solenoid

has, in addition to its resistance, R, a certain inductance, L. When a voltage, V, is applied across

an inductive element, the current, I, produced in that element does not jump up to its constant

value, but gradually rises to its maximum over a period of time called the rise time (Figure 2).

Conversely, I does not disappear instantaneously, even if V is removed abruptly, but decreases

back to zero in the same amount of time as

the rise time.

Therefore, when a low frequency PWM voltage is applied across a solenoid, the current

through it will be increasing and decreasing as V turns on and off. If D is shorter than the rise

time, I will never achieve its maximum value, and will be discontinuous since it will go back to

zero during V’s off period (Figure 3).* In contrast, if D is larger than the rise time, I will never

fall back to zero, so it will be continuous, and have a DC average value. The current will not be

constant, however, but will have a ripple (Figure 4).

At high frequencies, V turns on and off very quickly, regardless of D, such that the

current does not have time to decrease very far before the voltage is turned back on. The

resulting current through the solenoid is therefore considered to be constant. By adjusting the D,

the amount of output current can be controlled. With a small D, the current will not have much

time to rise before the high frequency PWM voltage takes effect and the current stays constant.

With a large D, the current will be able to rise higher before it becomes constant. (Figure 5)

Dither

Static friction, stiction, and hysteresis can cause the control of a hydraulic valve to be

erratic and unpredictable. Stiction can prevent the valve spool from moving with small input

changes, and hysteresis can cause the shift to be different for the same input signal. In order to

counteract the effects of stiction and hysteresis, small vibrations about the desired position are

created in the spool. This constantly breaks the static friction ensuring that it will move even

with small input changes, and the effects of hysteresis are average out.

Dither is a small ripple in the solenoid current that causes the desired vibration and there

by increases the linearity of the valve. The amplitude and frequency of the dither must be

carefully chosen. The amplitude must be large enough and the frequency slow enough that the

spool will respond, yet they must also be small and fast enough not to result in a pulsating

output.

The optimum dither must be chosen such that the problems of stiction and hysteresis are

overcome without new problems being created. Dither in the output current is a byproduct of low

frequency PWM, as seen above. However, the frequency and amplitude of the dither will be a

function of the duty cycle, which is also used to set the output current level. This means that low

frequency dither is not independent of current magnitude. The advantage of using high frequency

PWM is that dither can be generated separately, and then superimposed on top of the output

current.

This allows the user to independently set the current magnitude (by adjusting the D), as

well as the dither frequency and amplitude. The optimum dither, as set by the user, will therefore

be constant at all current levels.

Why the PWM frequency is important:

The PWM is a large amplitude digital signal that swings from one voltage extreme to the

other. And, this wide voltage swing takes a lot of filtering to smooth out. When the PWM

frequency is close to the frequency of the waveform that you are generating, then any PWM

filter will also smooth out your generated waveform and drastically reduce its amplitude. So, a

good rule of thumb is to keep the PWM frequency much higher than the frequency of any

waveform you generate.

Finally, filtering pulses is not just about the pulse frequency but about the duty cycle and

how much energy is in the pulse. The same filter will do better on a low or high duty cycle pulse

compared to a 50% duty cycle pulse. Because the wider pulse has more time to integrate to a

stable filter voltage and the smaller pulse has less time to disturb it the inspiration was a request

to control the speed of a large positive displacement fuel pump. The pump was sized to allow full

power of a boosted engine in excess of 600 Hp.

At idle or highway cruise, this same engine needs far less fuel yet the pump still normally

supplies the same amount of fuel. As a result the fuel gets recycled back to the fuel tank,

unnecessarily heating the fuel. This PWM controller circuit is intended to run the pump at a low

speed setting during low power and allow full pump speed when needed at high engine power

levels.

Motor Speed Control (Power Control)

Typically when most of us think about controlling the speed of a DC motor we think of

varying the voltage to the motor. This is normally done with a variable resistor and provides a

limited useful range of operation. The operational range is limited for most applications

primarily because torque drops off faster than the voltage drops.

Most DC motors cannot effectively operate with a very low voltage. This method also

causes overheating of the coils and eventual failure of the motor if operated too slowly. Of

course, DC motors have had speed controllers based on varying voltage for years, but the range

of low speed operation had to stay above the failure zone described above.

Additionally, the controlling resistors are large and dissipate a large percentage of energy

in the form of heat. With the advent of solid state electronics in the 1950’s and 1960’s and this

technology becoming very affordable in the 1970’s & 80’s the use of pulse width modulation

(PWM) became much more practical. The basic concept is to keep the voltage at the full value

and simply vary the amount of time the voltage is applied to the motor windings. Most PWM

circuits use large transistors to simply allow power On & Off, like a very fast switch.

This sends a steady frequency of pulses into the motor windings. When full power is

needed one pulse ends just as the next pulse begins, 100% modulation. At lower power settings

the pulses are of shorter duration. When the pulse is On as long as it is Off, the motor is

operating at 50% modulation. Several advantages of PWM are efficiency, wider operational

range and longer lived motors. All of these advantages result from keeping the voltage at full

scale resulting in current being limited to a safe limit for the windings.

PWM allows a very linear response in motor torque even down to low PWM% without

causing damage to the motor. Most motor manufacturers recommend PWM control rather than

the older voltage control method. PWM controllers can be operated at a wide range of

frequencies. In theory very high frequencies (greater than 20 kHz) will be less efficient than

lower frequencies (as low as 100 Hz) because of switching losses.

The large transistors used for this On/Off activity have resistance when flowing current, a

loss that exists at any frequency. These transistors also have a loss every time they “turn on” and

every time they “turn off”. So at very high frequencies, the “turn on/off” losses become much

more significant. For our purposes the circuit as designed is running at 526 Hz. Somewhat of an

arbitrary frequency, it works fine.

Depending on the motor used, there can be a hum from the motor at lower PWM%. If

objectionable the frequency can be changed to a much higher frequency above our normal

hearing level (>20,000Hz) .

PWM Controller Features:

This controller offers a basic “Hi Speed” and “Low Speed” setting and has the option to

use a “Progressive” increase between Low and Hi speed. Low Speed is set with a trim pot inside

the controller box. Normally when installing the controller, this speed will be set depending on

the minimum speed/load needed for the motor. Normally the controller keeps the motor at this

Lo Speed except when Progressive is used and when Hi Speed is commanded (see below). Low

Speed can vary anywhere from 0% PWM to 100%.

Progressive control is commanded by a 0-5 volt input signal. This starts to increase PWM

% from the low speed setting as the 0-5 volt signal climbs. This signal can be generated from a

throttle position sensor, a Mass Air Flow sensor, a Manifold Absolute Pressure sensor or any

other way the user wants to create a 0-5 volt signal. This function could be set to increase fuel

pump power as turbo boost starts to climb (MAP sensor). Or, if controlling a water injection

pump, Low Speed could be set at zero PWM% and as the TPS signal climbs it could increase

PWM%, effectively increasing water flow to the engine as engine load increases. This controller

could even be used as a secondary injector driver (several injectors could be driven in a batch

mode, hi impedance only), with Progressive control (0-100%) you could control their output for

fuel or water with the 0-5 volt signal.

Progressive control adds enormous flexibility to the use of this controller. Hi Speed is

that same as hard wiring the motor to a steady 12 volt DC source. The controller is providing

100% PWM, steady 12 volt DC power. Hi Speed is selected three different ways on this

controller: 1) Hi Speed is automatically selected for about one second when power goes on. This

gives the motor full torque at the start. If needed this time can be increased ( the value of C1

would need to be increased). 2) High Speed can also be selected by applying 12 volts to the High

Speed signal wire. This gives Hi Speed regardless of the Progressive signal.

When the Progressive signal gets to approximately 4.5 volts, the circuit achieves 100%

PWM – Hi Speed.

How does this technology help ?:

The benefits noted above are technology driven. The more important question is how the PWM

technology Jumping from a 1970’s technology into the new millennium offers:

• Longer battery life:

– reducing the costs of the solar system

– reducing battery disposal problems

• More battery reserve capacity:

– increasing the reliability of the solar system

– reducing load disconnects

– opportunity to reduce battery size to lower

the system cost

• Greater user satisfaction:

– get more power when you need it for less

money!!

SPACE VECTOR PWM

The Space Vector PWM generation module accepts modulation index commands and

generates the appropriate gate drive waveforms for each PWM cycle. This section describes the

operation and configuration of the SVPWM module.

A three-phase 2-level inverter with dc link configuration can have eight possible

switching states, which generates output voltage of the inverter. Each inverter switching state

generates a voltage Space Vector (V1 to V6 active vectors, V7 and V8 zero voltage vectors) in

the Space Vector plane (Figure: space vector diagram). The magnitude of each active vector

(V1to V6) is 2/3 Vdc (dc bus voltage).

The Space Vector PWM (SVPWM) module inputs modulation index commands

(U_Alpha and U_Beta) which are orthogonal signals (Alpha and Beta) as shown in Figure. The

gain characteristic of the SVPWM module is given in Figure . The vertical axis of Figure

represents the normalized peak motor phase voltage (V/Vdc) and the horizontal axis represents

the normalized modulation index (M).

The inverter fundamental line-to-line Rms output voltage (Vline) can be approximated (linear

range) by the following equation:

………….. (1)

Where dc bus voltage (Vdc) is in volts

Space Vector Diagram

This document is the property of International Rectifier and may not be copied or

distributed without expressed consent

Transfer Characteristics

The maximum achievable modulation (Umag_L) in the linear operating range is given

by:

………….. (2)

Over modulation occurs when modulation Umag > Umag_L. This corresponds to the

condition where the voltage vector in (Figure: voltage vector rescaling)increases beyond the

hexagon boundary. Under such circumstance, the Space Vector PWM algorithm will rescale the

magnitude of the voltage vector to fit within the Hexagon limit. The magnitude of the voltage

vector is restricted within the Hexagon; however, the phase angle (θ) is always preserved. The

transfer gain (Figure :transfer characteristics) of the PWM modulator reduces and becomes non-

linear in the over modulation region.

Voltage Vector Rescaling

This document is the property of International Rectifier and may not be copied or

distributed without expressed consent.

PWM Operation

Upon receiving the modulation index commands (UAlpha and UBeta) the sub-module

SVPW M_Tm starts its calculations at the rising edge of the PWM Load signal. The SVPWM

_Tm module implements an algorithm that selects (based on sector determination) the active

space vectors (V1 to V6) being used and calculates the appropriate time duration (w.r.t. one

PWM cycle) for each active vector. The appropriated zero vectors are also being selected. The

SVPWM _Tm module consumes 11 clock cycles typically and 35 clock cycles (worst case Tr) in

over modulation cases. At the falling edge of nSYNC, a new set of Space Vector times and

vectors are readily available for actual PWM generation (PhaseU, PhaseV, PhaseW) by sub

module Pwm Generation. It is crucial to trigger PwmLoad at least 35 clock cycles prior to the

falling edge of nSYNC signal; otherwise new modulation commands will not be implemented at

the earliest PWM cycle.

The above Figures voltage vector rescaling illustrates the PWM waveforms for a voltage

vector locates in sector I of the Space Vector plane (shown in Figure). The gating pattern outputs

(PWMUH … PWMWL) include dead time insertion

3-phase Space Vector PWM

2-phase (6-step PWM) Space Vector PWM

PWM Carrier Period:

Input variable PwmCval controls the duration of a PWM cycle. It should be populated

by the system clock frequency (Clk) and Pwm frequency (PwmFreq) selection. The variable

should be calculated as:

……….. (3)

The input resolution of the Space Vector PWM modulator signals U_Alpha and U_Beta

is 16-bit signed integer. However, the actual PWM resolution (PwmCval) is limited by the

system clock frequency.

Dead time Insertion Logic Dead time is inserted at the output of the PWM Generation

Module. The resolution is 1 clock cycle or 30nsec at a 33.3 MHz clock and is the same as those

of the voltage command registers and the PWM carrier frequency register.

The dead time insertion logic chops off the high side commanded volt*seconds by the

amount of dead time and adds the same amount of volt*seconds to the low side signal. Thus, it

eliminates the complete high side turn on pulse if the commanded volt*seconds is less than the

programmed dead time.

Dead time Insertion

The dead time insertion logic inserts the programmed dead time between two high and

low side of the gate signals within a phase. The dead time register is also double buffered to

allow “on the fly” dead time change and control while PWM logic is inactive.

Symmetrical and Asymmetrical Mode Operation

There are two modes of operation available for PWM waveform generation, namely the

Center Aligned Symmetrical PWM (Figure) and the Center Aligned Asymmetrical PWM

(Figure)The volt-sec can be changed every half a PWM cycle (Tpwm) since Pwm Load occurs

every half a PWM cycle (compare Figure :symmetrical pwm and Figure :asymmetrical PWM).

With Symmetrical PWM mode, the inverter voltage Config = 0), the inverter voltage can be

changed at two times the rate of the switching frequency. This will provide an increase in voltage

control bandwidth, however, at the expense of increased current harmonic

Asymmetrical PWM Mode

Three-Phase and Two-Phase Modulation

Three-phase and two-phase Space Vector PWM modulation options are provided for the

IRMCx203. The Volt-sec generated by the two PWM strategies are identical; however with 2-

phase modulation the switching losses can be reduced significantly, especially when high

switching frequency (>10Khz) is employed. Figure: three-phase and two phase modulation

shows the switching pattern for one PWM cycle when the voltage vector is inside sector 1

Three Phase and Two Phase Modulation

The field Two Phase PWM of the PWM Config write register group provides selection of

three-phase or two-phase modulation. The default setting is three-phase modulation. Successful

operation of two-phase modulation in the entire speed operating range will depend on hardware

configuration. If the gate driver employs a bootstrap power supply strategy, disoperation will

occur at low motor fundamental frequencies (< 2Hz) under two-phase modulation control.

Sinusoidal Pulse Width Modulation

In many industrial applications, Sinusoidal Pulse Width Modulation (SPWM), also called

Sine coded Pulse Width Modulation, is used to control the inverter output voltage. SPWM

maintains good performance of the drive in the entire range of operation between zero and 78

percent of the value that would be reached by square-wave operation. If the modulation index

exceeds this value, linear relationship between modulation index and output voltage is not

maintained and the over-modulation methods are required

Space Vector Pulse Width Modulation

A different approach to SPWM is based on the space vector representation of voltages in

the d, q plane. The d, q components are found by Park transform, where the total power, as well

as the impedance, remains unchanged.

Fig: space vector shows 8 space vectors in according to 8 switching positions of inverter,

V* is the phase-to-center voltage which is obtained by proper selection of adjacent vectors V1

and V2.

Inverter output voltage space vector

Determination of Switching times

The reference space vector V* is given by Equation (1), where T1, T2 are the intervals of

application of vector V1 and V2 respectively, and zero vectors V0 and V7 are selected for T0.

V* Tz = V1 *T1 + V2 *T2 + V0 *(T0/2) + V7 *(T0/2)……….(4)

Space Vector Pulse Width Modulation (continued)

Fig. below shows that the inverter switching state for the period T1 for vector V1 and for

vector V2, resulting switching patterns of each phase of inverter are shown in Fig. pulse pattern

of space vector PWM.

Inverter switching state for (a)V1, (b) V2

Pulse pattern of Space vector PWM

Comparison

In Fig:- comparison, U is the phase to- center voltage containing the triple order

harmonics that are generated by space vector PWM, and U1 is the sinusoidal reference voltage.

But the triple order harmonics are not appeared in the phase-to-phase voltage as well. This leads

to the higher modulation index compared to the SPWM.

Comparison of SPWM and Space Vector PWM

As mentioned above, SPWM only reaches to 78 percent of square wave operation, but the

amplitude of maximum possible voltage is 90 percent of square-wave in the case of space vector

PWM. The maximum phase-to-center voltage by sinusoidal and space vector

PWM are respectively

Vmax = Vdc/2 : Sinusoidal PWM

Vmax = Vdc/√3 : Space Vector PWM

Where, Vdc is DC-Link voltage.

This means that Space Vector PWM can produce about 15 percent higher than

Sinusoidal PWM in output voltage.

SVM PWM Technique

The Pulse Width modulation technique permits to obtain three phase system voltages,

which can be applied to the controlled output. Space Vector Modulation (SVM) principle differs

from other PWM processes in the fact that all three drive signals for the inverter will be created

simultaneously. The implementation of SVM process in digital systems necessitates less

operation time and also less program memory.

The SVM algorithm is based on the principle of the space vector u*, which describes all

three output voltages ua, ub and uc :

u* = 2/3 . ( ua + a . ub + a2 . uc ) ………(5)

Where a = -1/2 + j . v3/2 We can distinguish six sectors limited by eight discrete vectors

u0…u7 (fig:- inverter output voltage space vector), which correspond to the 23 = 8 possible

switching states of the power switches of the inverter.

Space vector Modulation

The amplitude of u0 and u7 equals 0. The other vectors u1…u6 have the same amplitude

and are 60 degrees shifted.

By varying the relative on-switching time Tc of the different vectors, the space vector u*

and also the output voltages ua, ub and uc can be varied and is defined as:

ua = Re ( u* )

ub = Re ( u* . a-1)

uc = Re ( u* . a-2) …………(6)

During a switching period Tc and considering for example the first sector, the vectors u0,

u1 and u2 will be switched on alternatively.

Definition of the Space vector

Depending on the switching times t0, t1 and t2 the space vector u* is defined as:

u* = 1/Tc . ( t0 . u0 + t1 . u1 + t2 . u2 )

u* = t0 . u0 + t1 . u1 + t2 . u2

u* = t1 . u1 + t2 . u2 ………….. (7)

Where

t0 + t1 + t2 = Tc and

t0 + t1 + t2 = 1

t0, t1 and t2 are the relative values of the on switching times.

They are defined as: t1 = m . cos ( a + p/6)

t2 = m . sin a

t0 = 1 - t1 - t2

Their values are implemented in a table for a modulation factor m = 1. Then it will be

easy to calculate the space vector u* and the output voltages ua, ub and uc. The voltage vector

u* can be provided directly by the optimal vector control laws w1, vsa and vsb. In order to

generate the phase voltages ua, ub and uc corresponding to the desired voltage vector u* the

following SVM strategy is proposed.

Total harmonic distortion:

The total harmonic distortion, or THD, of a signal is a measurement of the harmonic

distortion present and is defined as the ratio of the sum of the powers of all harmonic

components to the power of the fundamental frequency. Lesser THD allows the components in a

loudspeaker, amplifier or microphone or other equipment to produce a more accurate

reproduction by reducing harmonics added by electronics and audio media. A THD rating < 1%

is considered to be in high-fidelity and inaudible to the human ear

To understand a system with an input and an output, such as an audio amplifier, we start with an

ideal system where the transfer function is linear and time-invariant. When a signal passes

through a non-ideal, non-linear device, additional content is added at the harmonics of the

original frequencies. THD is a measurement of the extent of that distortion.

When the input is a pure sine wave, the measurement is most commonly the ratio of the sum of

the powers of all higher harmonic frequencies to the power at the first harmonic, or fundamental,

frequency:

According to Wikipedia, the online encyclopedia for all things defined, “Total Harmonic

Distortion of a signal is a measurement of the harmonic distortion present and is defined as the

ratio of the sum of the powers of all harmonic components to the power of the fundamental

frequency.” Lesser THD, for example, allows the components in a loudspeaker, amplifier or

microphone or other equipment to make a violin sound like a violin when played back and not a

cello or simply a distorted noise. (1)

As a musician, I typically have learned about harmonics in terms of chords, distortion and

found them useful in tuning guitars at various frets across the neck of the guitar.

For those of us in the lighting and electrical world, THD refers to the Harmonic Distortion

present with most electrical equipment, and more specifically now, the distortion present with

electronic ballasts. THD is the measurement of the distortion created from the equipment’s

current draw. True resistive loads, such as an incandescent light bulb, do not have THD.

Equipment containing coils and capacitors, such as motors, drives, fluorescent lighting and HID

lighting, have some measure of THD.

In the true engineering sense; only fundamental frequency current can provide real power.

Systems with Power Factor correction capacitors and motors are considered to be “linear loads”

with acceptable (negligible) distortion levels. However, solid-state electronic devices have been

shown to be the largest contributor to distortion due to the switching of diode bridges producing

a discontinuous current, which then causes a distorted sine wave. (2)

In four wire WYE systems such as 120/208 and 277/480-volt systems; harmonics may cause a

problem with overheating of the neutral wire. The phase wires should also be designed for the

increased harmonic current, but since the “triplens” are additive, the problem is especially

critical on the neutral. The third harmonic and other “triplens” (9th, 15th, etc.) Are additive.

Total Harmonic Distortion is the percentage of all of these additive values in relation to the total

load. The sum of triplen harmonics greater than 33 percent will result in neutral current greater

than individual line currents. The resultant current exceeds the neutral conductor’s rating and

causes overheating of the neutral and/or transformer.

It is a common misconception that electronic ballasts increase THD. Currently available

electronic ballasts actually decrease the THD on an electrical system compared to a system

applying magnetic ballasts. ANSI C82.11 requires that the maximum THD of electronic ballasts

not exceed 32 percent and the maximum triplens not exceed 30 percent. Electronic ballasts today

are rated at less than 20 percent, 15 percent, or less than 10 percent THD. The magnetic ballast is

rated in the 20 to 28 percent range.

Electronic ballasts reduce THD in two ways.

1. The electronic ballast has a lower THD percentage than the magnetic ballast.

2. The biggest reduction comes from the fact that electronic ballasts reduce the total load.

BASICS OF TWO-LEVEL A ND MULTILEVEL INVERTERS

Two-Level Inverters

This is the most widely used topology in various lowand medium-power applications.

The full-bridge configuration of the three-phase voltage source inverter is shown in Figure 1.

The witching logic to obtain output voltage for a 1200 mode of operation is shown in Table 1.

This topology can be used at a very high switching frequency to obtain low THD by using PWM

techniques. Power devices are to be connected in series–parallel to achieve a large power

capability. They suffer from static and dynamic voltage sharing problems in series and parallel

connection of power devices, high rate of change of voltage due to synchronous commutation of

Series devices and inclusion of high switching frequency harmonic contents in inverter output

voltage [3].

Multilevel Inverters

Multilevel inverters have grown as better counterparts to conventional two-level

inverters. Commonly employed multilevel inverter topologies are Diode Clamped, Capacitor

Clamped and Cascaded Multilevel inverters. In all these topologies, the output voltage is

synthesized from several levels of input voltages obtained from several capacitors connected

across the dc bus. In a capacitor clamped inverter, both real and reactive power can be

controlled, but it suffers from higher switching losses due to real power transfer thus reducing

the efficiency of power conversion. Also, it requires a large number of storage capacitors at

higher levels. The cascaded inverter uses a large number of separate dc sources for each of the

bridges. However, in the diode clamped topology, all devices are switched at the fundamental

frequency resulting in low switching losses and high efficiency. Other main features of this

topology are controlled reactive power flow between source and load, much better dynamic

voltage sharing among switching devices and

Simple topological structure. Therefore, diode clamped inverter topology is considered here for

study. The control logic is simple, especially for back-to-back inter-tie connections of two

systems. However, it requires a large number of clamping diodes for a large number of output

Voltage levels. To produce an m-level output phase voltage, (m-1) switches are required for each

half phase leg, a total of (m-1) dc link capacitors for energy storage and (m-1)*(m-2) clamping

diodes for each phase leg [1-2].

Three-Level Diode Clamped Multilevel Inverter (DCMLI)

Three-phase diode clamped three-level inverter (neutral point clamped) topology is

shown in Figure 2. The circuit consists of two dc link capacitors, 12 power switches and six

clamping diodes. The middle point of the dc bus capacitor is known as neutral point ‘n’. The

main feature

Of this topology is clamping diodes that clamp the switch voltage to half of the dc bus voltage,

reducing the voltage stress of the switching device. The output voltage has three different states:

+, 0 and – and the corresponding output phase voltages are +Vdc/2, 0 and -Vdc/2. Switching

States to synthesize the output voltages for phase ‘A’ are defined in Table 2. A similar logic can

be applied for the other two phases.

Five-Level DCMLI

The circuit diagram of the five-level DCMLI topology is shown in Figure 3. It consists of

24 power switches and 36 clamping diodes. The DC bus has four capacitors for a DC bus voltage

Vdc. The voltage across each capacitor

Figure Three-phase two-level inverter.

Is Vdc/4; thus, the voltage stress across each device will

Be limited to Vdc/4 through the clamping diode. Table

3 shows the switching combinations and corresponding

Output phase voltage levels where switching state

‘1’ represents the switch is in ‘on’ condition and state

‘0’ indicates the switch is in ‘off’ condition. When the

Number of levels is high enough in the DCMLI, harmonic contents in the output voltage and

current get reduced to avoid the need for filters.

3. Switching Loss Calculations:

Consider a single MOSFET switch connected across a dc voltage of value Vdc. Current through

switch during ‘on’ time is considered as Idc. Figure 4 shows the waveforms of the voltage

across and the current through the switch when it is operated at a switching frequency of Fs =

1/Ts, where Ts is the switching period. To simplify the expressions, the switching waveforms are

represented by linear approximations. In the figure, vm and im are the voltage across and the

current through the MOSFET [3, 5]. Switching losses can be calculated from the turn-on and

Turn-off characteristics of the devices. Instantaneous voltage and current during turn on time

tc(on) are

Instantaneous power during the interval tc(on) is

And energy dissipated during this interval is tc(on),

And during turn-off transition, of t c(off), the current falls fr om Idc to zero and the Von rises

linearly to Vdc.

The instantaneous voltage and current during this period are

The instantaneous power dissipated during the interval

Hence, the energy dissipated can be found as tc(off),tc(off) is

With a switching frequency of Fs, the average switching loss in the switch during each transition

of turn on and

Turn off can be found as

Hence, the average switching loss Psw in the switch is

Eqn. (11) shows that the switching power loss in a semiconductor switch varies linearly with the

switching frequency and switching times. Therefore, with the devices having short switching

times, it is possible to operate them at a higher switching frequency thus avoiding excessive

switching power losses in the device [8-10].

4. Modulation Technique

Modulation techniques for voltage source inverters may be carrier based or carrier-less

and open loop or Closed loop. These modulation or control techniques for multilevel voltage

source inverters are classified in Figure 5. Simulation investigation of different multilevel control

techniques have been presented in [11]. The SPWM technique is considered for study in this

paper. It is the simple technique to be implemented. In the SPWM technique, a triangular carrier

wave at a high switching frequency is compared with the sinusoidal Reference wave at a

fundamental output frequency. The SPWM technique is again divided into Alternate Phase

Opposition Disposition, Phase Opposition Disposition and In Phase (PH) [12]. Figure 6 shows

the generation of switching pulses for power device S1 of the two-level inverter shown in Figure

1. One triangular carrier wave is compared with a sinusoidal reference wave to generate

switching pulses. For power device S4, the complementary of this pulse is to be given. The

control principle of the SPWM is to use several triangular carrier signals keeping only one

modulating sinusoidal signal. If an m-level inverter is employed, (m-1) level shifted carriers will

be needed.

Two and four triangular carrier signals are needed for three- and five-level inverters,

respectively. The carriers Have the same frequency fc and the same peak-to-peak amplitude Ac.

The zero reference is placed in the middle Of the carrier set. The modulating signal is a sinusoid

of frequency fm and amplitude Am. At every instant, each Carrier is compared with the

modulating signal. Each comparison switches the switch ‘on’ if the modulating Signal is greater

than the triangular carrier assigned to that switch. Obviously, the actual driving signals for The

power devices can be derived from the results of the modulating–carrier comparison by means of

a control Logic circuit. Figure 7 shows the generation of switching pulses for power devices Sa1

and Sa2 of the three-level inverter shown in Figure 2. Pulses for the lower two devices Sa1 ’ and

Sa2 ’ are complementary to these pulses,

Respectively. Figure 8 shows the generation of switching pulses for power devices Sa1, Sa2, Sa3

and Sa4 of the fivelevel Inverter shown in Figure 3. Pulses for the lower four devices Sa1 ’, Sa2

’, Sa3 ’ and Sa4 are complementary to these pulses, respectively. Vr is the reference sin wave

and Vt1, Vt2, Vt3, Vt4 are four carrier signals

Structure of 21-level based on proposed multilevel inverter:

SWITCHING PATTERN TO PRODUCE DIFFERENT OUTPUT VOLTAGE LEVELS

CHAPTER

MATLAB

Matlab is a high-performance language for technical computing. It integrates computation,

visualization, and programming in an easy-to-use environment where problems and solutions are

expressed in familiar mathematical notation. Typical uses include Math and computation

Algorithm development Data acquisition Modeling, simulation, and prototyping Data analysis,

exploration, and visualization Scientific and engineering graphics Application development,

including graphical user interface building.

Matlab is an interactive system whose basic data element is an array that does not require

dimensioning. This allows you to solve many technical computing problems, especially those

with matrix and vector formulations, in a fraction of the time it would take to write a program in

a scalar no interactive language such as C or Fortran.

The name matlab stands for matrix laboratory. Matlab was originally written to provide easy

access to matrix software developed by the linpack and eispack projects. Today, matlab engines

incorporate the lapack and blas libraries, embedding the state of the art in software for matrix

computation.

Matlab has evolved over a period of years with input from many users. In university

environments, it is the standard instructional tool for introductory and advanced courses in

mathematics, engineering, and science. In industry, matlab is the tool of choice for high-

productivity research, development, and analysis.

Matlab features a family of add-on application-specific solutions called toolboxes. Very

important to most users of matlab, toolboxes allow you to learn and apply specialized

technology. Toolboxes are comprehensive collections of matlab functions (M-files) that extend

the matlab environment to solve particular classes of problems. Areas in which toolboxes are

available include signal processing, control systems, neural networks, fuzzy logic, wavelets,

simulation, and many others.

The matlab system consists of five main parts:

Development Environment. This is the set of tools and facilities that help you use matlab

functions and files. Many of these tools are graphical user interfaces. It includes the matlab

desktop and Command Window, a command history, an editor and debugger, and browsers for

viewing help, the workspace, files, and the search path.

The matlab Mathematical Function Library. This is a vast collection of computational

algorithms ranging from elementary functions, like sum, sine, cosine, and complex arithmetic, to

more sophisticated functions like matrix inverse, matrix eigenvalues, Bessel functions, and fast

Fourier transforms.

The matlab Language. This is a high-level matrix/array language with control flow

statements, functions, data structures, input/output, and object-oriented programming features. It

allows both "programming in the small" to rapidly create quick and dirty throw-away programs,

and "programming in the large" to create large and complex application programs.

Matlab has extensive facilities for displaying vectors and matrices as graphs, as well as

annotating and printing these graphs. It includes high-level functions for two-dimensional and

three-dimensional data visualization, image processing, animation, and presentation graphics. It

also includes low-level functions that allow you to fully customize the appearance of graphics as

well as to build complete graphical user interfaces on your matlab applications.

The matlab Application Program Interface (API). This is a library that allows you to write C

and Fortran programs that interact with matlab. It includes facilities for calling routines from

matlab (dynamic linking), calling matlab as a computational engine, and for reading and writing

MAT-files.

SIMULINK:

Introduction:

Simulink is a software add-on to matlab which is a mathematical tool developed by The

Math works,(http://www.mathworks.com) a company based in Natick. Matlab is powered by

extensive numerical analysis capability. Simulink is a tool used to visually program a dynamic

system (those governed by Differential equations) and look at results. Any logic circuit, or

control system for a dynamic system can be built by using standard building blocks available in

Simulink Libraries. Various toolboxes for different techniques, such as Fuzzy Logic, Neural

Networks, dsp, Statistics etc. are available with Simulink, which enhance the processing power

of the tool. The main advantage is the availability of templates / building blocks, which avoid the

necessity of typing code for small mathematical processes.

Concept of signal and logic flow:

In Simulink, data/information from various blocks are sent to another block by lines

connecting the relevant blocks. Signals can be generated and fed into blocks dynamic /

static).Data can be fed into functions. Data can then be dumped into sinks, which could be

scopes, displays or could be saved to a file. Data can be connected from one block to another,

can be branched, multiplexed etc. In simulation, data is processed and transferred only at

Discrete times, since all computers are discrete systems. Thus, a simulation time step (otherwise

called an integration time step) is essential, and the selection of that step is determined by the

fastest dynamics in the simulated system.

Fig Simulink library browser

Connecting blocks:

fig Connectung blocks

To connect blocks, left-click and drag the mouse from the output of one block to the input of

another block.

Sources and sinks:

The sources library contains the sources of data/signals that one would use in a dynamic

system simulation. One may want to use a constant input, a sinusoidal wave, a step, a repeating

sequence such as a pulse train, a ramp etc. One may want to test disturbance effects, and can use

the random signal generator to simulate noise. The clock may be used to create a time index for

plotting purposes. The ground could be used to connect to any unused port, to avoid warning

messages indicating unconnected ports.

The sinks are blocks where signals are terminated or ultimately used. In most cases, we would

want to store the resulting data in a file, or a matrix of variables. The data could be displayed or

even stored to a file. the stop block could be used to stop the simulation if the input to that block

(the signal being sunk) is non-zero. Figure 3 shows the available blocks in the sources and sinks

libraries. Unused signals must be terminated, to prevent warnings about unconnected signals.

fig Sources and sinks

Continuous and discrete systems:

All dynamic systems can be analyzed as continuous or discrete time systems. Simulink

allows you to represent these systems using transfer functions, integration blocks, delay blocks

etc.

fig continous and descrete systems

Non-linear operators:

A main advantage of using tools such as Simulink is the ability to simulate non-linear

systems and arrive at results without having to solve analytically. It is very difficult to arrive at

an analytical solution for a system having non-linearities such as saturation, signup function,

limited slew rates etc. In Simulation, since systems are analyzed using iterations, non-linearities

are not a hindrance. One such could be a saturation block, to indicate a physical limitation on a

parameter, such as a voltage signal to a motor etc. Manual switches are useful when trying

simulations with different cases. Switches are the logical equivalent of if-then statements in

programming.

fig simulink blocks

Mathematical operations:

Mathematical operators such as products, sum, logical operations such as and, or,

etc. .can be programmed along with the signal flow. Matrix multiplication becomes easy with the

matrix gain block. Trigonometric functions such as sin or tan inverse (at an) are also available.

Relational operators such as ‘equal to’, ‘greater than’ etc. can also be used in logic circuits

fig Simulink math blocks

SIGNALS & DATA TRANSFER:

In complicated block diagrams, there may arise the need to transfer data from one portion

to another portion of the block. They may be in different subsystems. That signal could be

dumped into a goto block, which is used to send signals from one subsystem to another.

Multiplexing helps us remove clutter due to excessive connectors, and makes

matrix(column/row) visualization easier.

fig signals and systems

Making subsystems

Drag a subsystem from the Simulink Library Browser and place it in the parent block

where you would like to hide the code. The type of subsystem depends on the purpose of the

block. In general one will use the standard subsystem but other subsystems can be chosen. For

instance, the subsystem can be a triggered block, which is enabled only when a trigger signal is

received.

Open (double click) the subsystem and create input / output PORTS, which transfer signals into

and out of the subsystem. The input and output ports are created by dragging them from the

Sources and Sinks directories respectively. When ports are created in the subsystem, they

automatically create ports on the external (parent) block. This allows for connecting the

appropriate signals from the parent block to the subsystem.

Setting simulation parameters:

Running a simulation in the computer always requires a numerical technique to solve a

differential equation. The system can be simulated as a continuous system or a discrete system

based on the blocks inside. The simulation start and stop time can be specified. In case of

variable step size, the smallest and largest step size can be specified. A Fixed step size is

recommended and it allows for indexing time to a precise number of points, thus controlling the

size of the data vector. Simulation step size must be decided based on the dynamics of the

system. A thermal process may warrant a step size of a few seconds, but a DC motor in the

system may be quite fast and may require a step size of a few milliseconds.

SIMULATION RE SULTS:-

COMPARISON OF THE PROPOSED S TRUCTURE WITH CONVENTIONAL

CASCADED MULTILEVEL INVERTER

The main purpose of this paper is reduction of the components of the cascaded multilevel

inverters. As mentioned in previous section, the proposed structure is a combination of

bidirectional and unidirectional switches. Since each switch needs only one deriver circuit, the

overall number of deriver circuits is equal to the number of switches (N drive,) . In Table III,

different parameters of proposed structure concerning the number of voltage steps in the three

algorithms are summarized.

To examine the performance of proposed multilevel inverter in generation of a desired

output voltage waveform, a 21-level inverter based on proposed topology as shown in Fig. 6 is

simulated in MA TLABSIMULINK environment. It should be mentioned that the magnitude of

structure in Fig. 6 is chosen based on second algorithm. This inverter can generate staircase

output voltage waveform with maximum of 200V. The load is a series R-L with magnitudes R =

70Q and L = 55mH , respectively. There are several modulation strategies [8, 13]. In this work,

the fundamental frequency switching technique has been used. Table IV shows the switching

pattern of structure in Fig. 6 to produce different output voltage levels. Fig. 7 shows the control

block diagram of inverter. The main idea in control strategy is to deliver the load a voltage that

minimizes the error with respect to reference voltage.

For highlighting sufficiency of proposed structure, different parameters of recommended

structure for the same conditions are compared to that presented in [4] (Fig. 4(a», [13] (Fig. 4(b»

and conventional cascaded multilevel converters (FigA(c». It is noteworthy that switches used in

reference [13] are bidirectional. Although, two IGBTs are used in bidirectional switches, in case

of using common emitter configuration, one circuit deriver can be used for them [2]. The dc

voltage source magnitudes of [4] and [13] and conventional cascade converter must be selected

in a way which all odd and even voltage steps can be produced. For this purpose, for the

structure offered in [4], two method including symmetrical (all dc voltage sources are equal) and

binary (in which the magnitude of dc sources are selected as a power of 2) is used. Likewise, for

the structure offered in [13], only one state can be considered in which all dc voltage sources are

set to be equal. Also for the conventional cascaded multilevel inverter three algorithms

(symmetrical, binary and trinary) can be considered.

The results of comparison for the recommended configuration and pre-mentioned structures are

investigated. Fig. 5 compares the recommended configuration with the structures recommended

in [4] and [13] and conventional cascaded multilevel inverter concerning the number of switches,

number of IGBTs, number of deriver circuits, number of dc voltage sources, variety of sources

and maximum standing voltage for symmetrical and asymmetrical structures. Figures 8 -11

shows the output voltage of different parts in structure. As these figures clearly show, the output

voltage of each unit can only produce zero or positive values. By adding H-bridge inverter at the

output terminal of circuit shown in Fig. 2, it's possible to produce negative value of output

voltage. For the simulated 21-level inverter, the voltage waveforms of load voltage and current

are shown in Figs. 12 and 13. From Fig. 13, it's clear that the proposed structure can produce

both positive and negative values of output voltage.

MATLAB DESIGN OF CASE STUDY & RESULTS:

Simulation Results:-

CONCLUSION

In this paper, a new topology has been introduced for cascaded multilevel inverters. The

proposed structure is a compound of both bidirectional and unidirectional switches which has the

advantage of using fewer IGBTs and deriver circuits. Therefore the proposed topology results in

reduction of installation area and cost. Also three procedures have been presented for the

determination of dc voltage sources' magnitude. Using these algorithms, both symmetrical and

asymmetrical configuration has been made for sources of studied structures and by concerning

different points of view including the number of IGBTs, deriver circuit, the variety of dc voltage

magnitudes, a comparison has been made between the proposed topology and other referred

three structures. The results of the simulation for proposed 2I-level inverter demonstrate that the

proposed configuration has prominent feature compared to other cascaded multilevel inverters.

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