# Power Electronics - Introduction

Power Electronics refers to the process of controlling the flow of current and voltage and converting it to a form that is suitable for user loads. The most desirable power electronic system is one whose efficiency and reliability is 100%.

Take a look at the following block diagram. It shows the components of a Power Electronic system and how they are interlinked.

A power electronic system converts electrical energy from one form to another and ensures the following is achieved −

• Maximum efficiency
• Maximum reliability
• Maximum availability
• Minimum cost
• Least weight
• Small size

Applications of Power Electronics are classified into two types − Static Applications and Drive Applications.

## Static Applications

This utilizes moving and/or rotating mechanical parts such as welding, heating, cooling, and electro-plating and DC power.

## Drive Applications

Drive applications have rotating parts such as motors. Examples include compressors, pumps, conveyer belts and air conditioning systems.

### Air Conditioning System

Power electronics is extensively used in air conditioners to control elements such as compressors. A schematic diagram that shows how power electronics is used in air conditioners is shown below.

# Power Electronics - Switching Devices

A power electronic switching device is a combination of active switchable power semiconductor drivers that have been integrated into one. The main characteristics of the switch are determined by internal correlation of functions and interactions of its integrated system. The figure given below shows how a power electronic switch system works.

The external circuit of the above diagram is usually held at a high potential relative to the control unit. Inductive transmitters are used to support the required potential difference between the two interfaces.

Power switching devices are normally selected based on the rating at which they handle power, that is, the product of their current and voltage rating instead of their power dissipation rate. Consequently, the major attractive feature in a power electronic switch is its capability to dissipate low or almost no power. As a result, the electronic switch able to achieve a low and continuous surge of power.

# Power Electronics - Linear Circuit Elements

Linear circuit elements refer to the components in an electrical circuit that exhibit a linear relationship between the current input and the voltage output. Examples of elements with linear circuits include −

• Resistors
• Capacitors
• Inductors
• Transformers

To get a better understanding of linear circuit elements, an analysis of resistor elements is necessary.

## Resistors

A resistor is a device in which the flow of an electric current is restricted resulting in an energy conversion. For example, when electricity flows through a light bulb, the electricity is converted into a different form of energy such as heat and/or light. The resistance of an element is measured in ohms (Ω).

The measure of resistance in a given circuit is given by −

$$R=\rho \frac{L}{A}$$

Where R − resistance; ρ − resistivity; L − length of wire; and A − cross-sectional area of wire

### Symbol of Various Resistors

 Resistor A variable resistor A potentiometer

## Capacitors

A capacitor refers to an electrical device that has two conducting materials (also known as plates) separated by an insulator known as a dielectric. It uses electric field to store electric energy. The electric field is developed when the capacitor is connected to a battery, thus making positive electric charges accumulate on one plate and negative electric charges on the other plate.

When energy is stored in the electrical field of a capacitor, the process is called charging, and when energy is removed, the process is called discharging. The level of electrical energy stored in a capacitor is called capacitance and is measured in farads (F). One farad is the same as one coulomb per unit volt given by 1 C/V.

The difference between a capacitor and a battery is that a capacitor stores electrical energy while a battery stores chemical energy and releases the energy at a slow rate.

### Symbol of Various Capacitors

The various symbols of a capacitor are given in the table below.

 Fixed Capacitor Variable Capacitor Polarized Capacitor

## Inductors

Inductors are electronic devices that use magnetic field to store electric energy. The simplest form of an inductor is a coil or a wire in loop form where the inductance is directly proportional to the number of loops in the wire. In addition, the inductance depends on the type of material in the wire and the radius of the loop.

Given a certain number of turns and radius size, only the air core can result in the least inductance. The dielectric materials, which serve the same purpose as air include wood, glass, and plastic. These materials help in the process of winding the inductor. The shape of the windings (donut shape) as well as ferromagnetic substances, for example, iron increase the total inductance.

The amount of energy that an inductor can store is known as inductance. It is measured in Henry (H).

### Symbol of Various Inductors

 Fixed inductor Variable inductor

## Transformers

This refers to a device that alters energy from one level to another through a process known as electromagnetic induction. It is usually used to raise or lower AC voltages in applications utilizing electric power.

When the current on the primary side of the transformer is varied, a varied magnetic flux is created on its core, which spreads out to the secondary windings of the transformer in form of magnetic fields.

The operation principle of a transformer relies on Faraday’s law of electromagnetic induction. The law states that the rate of change of the flux linking with respect to time is directly related to the EMF induced in a conductor.

A transformer has three main parts −

• Primary winding
• Magnetic core
• Secondary winding

### Electromagnetic Devices

The concept of electromagnetism is widely used in technology and it is applied in motors, generators and electric bells. For example, in a doorbell, the electromagnetic component attracts a clapper that hits the bell and causes it to ring.

### Controllers

Controllers are devices that receive electronic signals transferred from a measured variable in a process and compare the value obtained with a set point of control. It utilizes digital algorithms to correlate and compare functions.

### Sensors

Sensors are used to determine current, which constantly varies to provide feedback for purposes of control. Sensing current makes it possible to achieve a smooth and accurate converter function. Current sensors are critical in converters such that the information in parallel or multiphase converters is easily shared.

### Filters

Electronic filters are also used to carry out processing of signals to remove undesired frequencies. They are analog circuits and exist in either active or passive state.

# Silicon Controlled Rectifier

A silicon controlled rectifier or semiconductor-controlled rectifier is a four-layer solidstate current-controlling device. The name "silicon controlled rectifier" is General Electric's trade name for a type of thyristor.

SCRs are mainly used in electronic devices that require control of high voltage and power. This makes them applicable in medium and high AC power operations such as motor control function.

An SCR conducts when a gate pulse is applied to it, just like a diode. It has four layers of semiconductors that form two structures namely; NPNP or PNPN. In addition, it has three junctions labeled as J1, J2 and J3 and three terminals(anode, cathode and a gate). An SCR is diagramatically represented as shown below.

The anode connects to the P-type, cathode to the N-type and the gate to the P-type as shown below.

In an SCR, the intrinsic semiconductor is silicon to which the required dopants are infused. However, doping a PNPN junction is dependent on the SCR application.

## Modes of Operation in SCR

• OFF state (forward blocking mode) − Here the anode is assigned a positive voltage, the gate is assigned a zero voltage (disconnected) and the cathode is assigned a negative voltage. As a result, Junctions J1 and J3 are in forward bias while J2 is in reverse bias. J2 reaches its breakdown avalanche value and starts to conduct. Below this value, the resistance of J1 is significantly high and is thus said to be in the off state.

• ON state (conducting mode) − An SCR is brought to this state either by increasing the potential difference between the anode and cathode above the avalanche voltage or by applying a positive signal at the gate. Immediately the SCR starts to conduct, gate voltage is no longer needed to maintain the ON state and is, therefore, switched off by −

• Decreasing the current flow through it to the lowest value called holding current

• Using a transistor placed across the junction.

• Reverse blocking − This compensates the drop in forward voltage. This is due to the fact that a low doped region in P1 is needed. It is important to note that the voltage ratings of forward and reverse blocking are equal.

# Power Electronics - TRIAC

The acronym TRIAC stands for Triode for Alternating Current. A TRIAC is a semiconductor device with three terminals that control the flow of current, thus the name Triac. Unlike SCR, TRIAC is bi-directional while SCR is bi-directional. It is ideal for operation utilizing AC power for switching purposes since it can control current flow for both halves in an alternating current cycle. This explained clearly in the diagram below.

## TRIAC Symbol

The circuit diagram for a TRIAC is shown below. It resembles two thyristors placed back to back.

## TRIAC Structure

The TRIAC Structure is regarded as a DIAC having an extra gate contact incorporated to ensure device control. Similar to other power devices, the TRIAC is manufactured from silicon. Consequently, the process of fabricating the silicon leads to the production of cheaper devices. As indicated below, the TRIAC has a six areas namely; four N-type regions and two P-type regions.

## TRIAC Operation

The operation of the TRIAC is based on the thyristor. It facilitates the switching function in AC electrical components and systems. They are widely used in light dimmers because they allow both halves of the AC cycle to be utilized. As a result, this makes them more efficient in power usage. As much as it is possible to use thyristors to function as TRIAC, it is not cost efficient for operations that require low power. It is possible to view a TRIAC in terms of two thyristors.

TRIACs are normally used in applications that do not require very high power because they exhibit non-symmetrical switching in their operation. This is disadvantageous for applications utilizing high power as it causes electromagnetic interference. As a result, TRIACs are used in motor controls, light residential light dimmers and small electric fans to control speed.

# Power Electronics - BJT

A Bipolar Junction Transistor (BJT) is a transistor whose operation depends on the contact made by two semicondutors. It can act as a switch, amplifier or oscillator. It is known as a bipolar transistor since its operation requires two types of charge carriers (holes and electrons). Holes constitute the dominant charge carriers in P-type semiconductors while electrons are the main charge bearers in N-type semiconductors.

## Structure of a BJT

A BJT has two P-N junctions connected back to back and sharing a common region B (base). This ensures contacts are made in all the regions that are base, collector and emitter. The structure of a PNP bipolar transistor is shown below.

The BJT shown above consists of two diodes connected back to back, resulting in the depletion of the regions called quasi-neutral. The width of quasi-neutral of the emitter, base and collector are indicated above as WE’, WB’ and WC’. They are obtained as follows −

$$W_{E}^{'}=W_{E}-X_{n,BE}$$ $$W_{B}^{'}=W_{B}-X_{p,BE}-X_{p,BC}$$ $$W_{C}^{'}=W_{C}-X_{n,BC}$$

The conventional signs of the currents for the emitter, base and collector are denoted by IE, IB and IC respectively. Therefore, the collector and base current are positive when a positive current meets the collector or base contact. In addition, the emitter current is positive when current leaves the emitter contact. Thus,

$$I_{E}=I_{B}+I_{C}$$

When a positive voltage is applied to the base contact relative to the collector and emitter, the base-collector voltage as well as base-emitter voltage becomes positive.

For simplicity, VCE is assumed to be zero.

Diffusion of electrons occur from the emitter to the base while diffusion of holes originates from the base to the emitter. Once the electrons reach the base-collector depleted region, they are swept through the region by an electric field. These electrons form the collector current.

When a BJT is biased in the forward active mode, the total emitter current is obtained by adding the electron diffusion current (IE,n), the hole diffusion current (IE, p) and the baseemitter current.

$$I_{E}=I_{E,n}+I_{E,p}+I_{r,d}$$

The total collector current is given by the electron diffusion current (IE,n), less the base recombination current(Ir,B).

$$I_{C}=I_{E,n}-I_{r,B}$$

The sum of the base current IB is obtained by adding the hole diffusion current (IE, p), base recombination current (Ir,B) and the base-emitter recombination current of the depletion layer (Ir,d).

$$I_{B}=I_{E,p}+I_{r,B}+I_{r,d}$$

## Transport Factor

This is given by the ratio of the collector current and the emitter current.

$$\alpha =\frac{I_{C}}{I_{E}}$$

Applying the Kirchhoff’s current law, it is found that the base current is given by the difference between the emitter current and the collector current.

## Current Gain

This is given by the ratio of the collector current to the base current.

$$\beta =\frac{I_{C}}{I_{B}}=\frac{\alpha }{1-\alpha }$$

The above explains how a BJT can produce current amplification. The transport factor (α) approaches one if the collector current is almost equivalent to the emitter current. The current gain (β) thus becomes greater than one.

For further analysis, the transport factor (α) is rewritten as a product of the emitter efficiency (γE) the base transport factor (αT) and the recombination factor of the depletion layer (δr). It is rewritten as follows −

$$\alpha =\gamma _{E}\times \alpha _{T}\times \delta _{r}$$

The following is a summary of the discussed emitter efficiency, base transport factor and depletion layer recombination factor.

## Emitter Efficiency

$$\gamma _{E}=\frac{I_{E,n}}{I_{E,p}+I_{E,P}}$$

## Base Transport Factor

$$\alpha _{T}=\frac{I_{E,n}-I_{r,b}}{I_{E,n}}$$

## Depletion Layer Recombination Factor

$$\delta _{r}=\frac{I_{E}-I_{r,d}}{I_{E,n}}$$

# Power Electronics - IGBT

The insulated gate bipolar transistor (IGBT) is a semiconductor device with three terminals and is used mainly as an electronic switch. It is characterized by fast switching and high efficiency, which makes it a necessary component in modern appliances such as lamp ballasts, electric cars and variable frequency drives (VFDs).

Its ability to turn on and off, rapidly, makes it applicable in amplifiers to process complex wave-patterns with pulse width modulation. IGBT combines the characteristics of MOSFETs and BJTs to attain high current and low saturation voltage capacity respectively. It integrates an isolated gate using FET (Field effect transistor) to obtain a control input.

## IGBT Symbol

The amplification of an IGBT is computed by the ratio of its output signal to its input signal. In conventional BJTs, the degree of gain (β) is equal to the ratio of its output current to the input current.

IGBT has a very low value of ON state resistance (RON) than a MOSFET. This implies that the voltage drop (I2R) across the bipolar for a particular switching operation is very low. The forward blocking action of the IGBT is similar to that of a MOSFET.

When an IGBT is used as controlled switch in a static state, its current and voltage ratings equal to that of BJT. On the contrary, the isolated gate in IGBT makes it easier to drive BJT charges and hence less power is required.

IGBT is switched ON or OFF based on whether its gate terminal has been activated or deactivated. A constant positive potential difference across the gate and the emitter maintains the IGBT in the ON state. When the input signal is removed, the IGBT is turned OFF.

## IGBT Principle of Operation

IGBT requires only a small voltage to maintain conduction in the device unlike in BJT. The IGBT is a unidirectional device, that is, it can only switch ON in the forward direction. This means current flows from the collector to the emitter unlike in MOSFETs, which are bi-directional.

## Applications of IGBT

The IGBT is used in medium to ultra-high power applications, for example traction motor. In large IGBT, it is possible to handle high current in the range of hundred amperes and blocking voltages of up to 6kv.

IGBTs are also used in power electronic devices such as converters, inverters and other appliances where the need for solid state switching is necessary. Bipolars are available with high current and voltage. However, their switching speeds are low. On the contrary, MOSFETs have high switching speeds although they are expensive.

# Power Electronics - MOSFET

Metal Oxide Semiconductor Field Effect Transistor (MOSFET) is a type of transistor used to switch electronic signals. It has four terminals namely; source (S), Drain (D), Gate (G) and Body (B).The MOSFET’s body is normally connected to the terminal of the source(S), which results in three-terminal device similar to other field effect transistors (FET). Since these two main terminals are usually interconnected via short circuit, only three terminals are visible in electrical diagrams.

It is the most common device in circuits that are both digital and analogue. Compared to the regular transistor, a MOSFET needs low current (less than one mill-ampere) to switch ON. At the same time, it delivers a high current load of more than 50 Amperes.

## Operation of a MOSFET

MOSFET has a thin layer of silicon dioxide, which acts as the plate of a capacitor. The isolation of the controlling gate raises the resistance of the MOSFET to extremely high levels (almost infinite).

The gate terminal is barred from the primary current pathway; thus, no current leaks into the gate.

MOSFETs exist in two main forms −

• Depletion state − This requires the gate-source voltage (VGB) to switch the component OFF. When the gate is at zero (VGB) the device is usually ON, therefore, it functions as a load resistor for given logic circuits. For loading devices with N-type depletion, 3V is the threshold voltage where the device is switched OFF by switching the gate at negative 3V.

• Enhancement state − The gate-source voltage (VGB) is required in this state to switch the component ON. When the gate is at zero (VGB) the device is usually OFF and can be switched ON by ensuring the gate voltage is higher than the source voltage.

## Symbol and Basic Construction

Where, D − Drain; G − Gate; S − Source; and Sub − Substrate

# Power Semiconductor Devices Solved Ex

A (BJT) emits a current of 1mA, and has emitter efficiency of 0.99. The base transport factor is 0.994 and a depletion layer recombination factor is 0.997. For the BJT calculate the following −

## The transport factor

The rewritten transport factor is given by −

$$\alpha =\gamma _{E}\times \alpha _{T}\times \delta _{r}$$

Substituting the values, we get

$$\alpha =0.99\times 0.994\times 0.997=0.981$$

## The current gain

Current gain is given by −

$$\beta =\frac{I_{C}}{I_{B}}=\frac{\alpha }{1-\alpha }$$

Substituting the values, we get

$$\beta =\frac{0.981}{1-0.981}=51.6$$

## The collector current

$$I_{C}=\alpha \times I_{E}=0.981\times 1=0.981mA$$

## The base current

$$I_{B}=I_{E}-I_{C}=1-0.981=19\mu A$$

# Power Electronics - Pulse Converters

## Phase Controlled Converter

A phase controlled converter converts AC to DC energy (line commutated). In other words, it is used in the conversion of fixed-frequency and fixed-voltage AC power into variable DC voltage output. It is expressed as

• Fixed Input − Voltage, frequency and AC power

• Variable output − DC voltage output

The AC input voltage that goes into a converter is normally at fixed RMS (root mean square) and fixed frequency. The inclusion of phase-controlled thyristors in the converter ensures that a variable DC output voltage is obtained. This is made possible by altering the phase angle at which the thyristors are triggered. As a result, a pulsating waveform of the load current is obtained.

During the input supply half cycle, the thyristor is in forward bias and is switched ON via the application of sufficient gate pulse (trigger). Current starts to flow once the thyristor has been switched ON, that is, at a point ωt=α to point ωt=β. The moment the load current drops to zero, the thyristor switches OFF as a result of line (natural) commutation.

There are a number of power converters that utilize natural commutation. These include −

• AC to DC converters
• AC to AC converters
• AC voltage controllers
• Cycloconverters

The above power converters will be explained in the next chapters in this tutorial.

## 2- Pulse Converter

A 2-phase pulse converter, also known as a level 2 pulse width modulator (PWM) generator, is used to generate pulses for pulse width modulation converters that are carrier based. It does this by utilizing level-two topology. This block controls switching devices for control purposes like IGBTs and FETs that exist in three types of converters namely −

• 1 arm (single phase half bridge)
• 2 arms (single phase full bridge)
• 3 arms ( three phase bridge)

The reference input signal in a 2-pulse converter is compared to a carrier. If the reference input signal is more than the carrier, the pulse equals to 1 for the upper device and 0 for the lower device.

In order to control a device with a single-phase full bridge (2 arms), it is necessary to apply unipolar or bipolar pulse width modulation. In unipolar modulation each of the two arms is independently controlled. A second reference input signal is generated internally through a shift in initial reference point by 180°

When the bipolar PWM is applied, the state of the lower switching device in the second single phase full bridge is similar to the upper switch in the first single phase full bridge device. Using a unipolar modulation leads to smooth AC waveforms while the bipolar modulation results in less varying voltage.

## 3-Pulse Converter

Consider a three-phase 3-pulse converter, where each of the thyristor is in conduction mode during the third of the supply cycle. The earliest time a thyristor is triggered into conduction is at 30° in reference to the phase voltage.

Its operation is explained using three thyristors and three diodes. When the thyristors T1, T2 and T3 are replaced by diodes D1, D2 and D3, conduction will begin at angle 30° in respect to the phase voltages uan, ubn and ucn respectively. Therefore, the firing angle α is measured initially at 30° in reference to the phase voltage corresponding to it.

The current can only flow in one direction through the thyristor, which is similar to inverter mode of functioning where power flows from the DC side to the AC side. In addition, the voltage in the thyristors is controlled by controlling the firing angle. This is achieved when α = 0(possible in a rectifier). Thus, the 3-pulse converter acts as an inverter and a rectifier.

## 6-Pulse Converter

The figure below shows a six-pulse bridge controlled converter connected to a three-phase source. In this converter, the number of pulses is twice that of phases, that is p = 2m. Using the same converter configuration, it is possible to combine two bridges of the six-pulse to obtain a twelve or more pulses converter.

When commutation is not available, two diodes will conduct at any particular time. Furthermore, to obtain a voltage drop across the load, two diodes must be at positioned at opposite legs of the bridge. For example, diodes 3 and 6 cannot be ON at the same time. Therefore, the voltage drop across the DC load is a combination of line voltage VL from the three-phase source.

It is important to note that more the number of pulses, the greater the utilization of the converter. In addition, the fewer the number of pulses the lesser the utilization of the converter.

# Effect of Source Inductance

The analysis of most converters is usually simplified under ideal conditions (no source impedance). However, this assumption is not justified since source impedance is normally inductive with a negligible resistive element.

Source inductance has a significant impact on the converter performance because its presence alters the output voltage of the converter. As a result, the output voltage reduces as the load current reduces. In addition, the input current and output voltage waveforms change significantly.

Source inductance effect on a converter is analyzed in the following two ways.

## Effect on Single Phase

Assuming that the converter operates in conduction mode and the ripple from the load current is negligible, the open circuit voltage becomes equal to average DC output at a firing angle of α.The diagram below shows a fully controlled converter with source in single phase. The thyristors T3 and T4 are assumed to be in conduction mode when t = 0. On the other hand, T1 and T2 fire when ωt = α

Where −

• Vi = input voltage
• Ii = input current
• Vo = output voltage
• Io = output voltage

When there is no source inductance, commutation will occur at T3 and T4. Immediately thyristors T1 and T2 are switched ON. This will lead the input polarity to change instantaneously. In the presence of source inductance, change of polarity and commutation does not occur instantaneously. Thus, T3 and T4 do not commutate as soon as T1 and T2 are switched ON.

At some interval, all the four thyristors will be conducting. This conducting interval is called the overlap interval (μ).

The overlap during commutation reduces the DC output voltage and the angle of extinction γ resulting in failed commutation when αis close to 180°. This is shown by the waveform below.

## Effect on Three Phase

Just like the single-phase converter, there are no instantaneous commutations due to the presence of the source inductances. Taking the source inductances into consideration, the effects (qualitative) on the converter performance is the same as in a single phase converter. This is shown in the diagram below.

# Power Electronics - Performance Parameters

It is important to determine the performance parameters for different converters whose topologies can be single phase or multi-phase.

## Assumptions

• The devices used are ideal, that is, they do not have any losses
• The devices have resistive loads

$$V_{DC}=\frac{1}{T} \int_{0}^{T}V_{L}\left ( t \right )dt$$

$$V_{L}=\sqrt{\frac{1}{T}}\int_{0}^{T}V_{L}^{2}\left ( t \right )dt$$

### Form Factor

$$FF=\frac{V_{L}}{V_{DC}}$$

### Ripple Factor

$$RF=\frac{\sqrt{V_{L}^{2}-V_{DC}^{2}}}{V_{DC}}=\sqrt{FF^{2}-1}$$

### Efficiency(Rectification Factor)

$$\eta =\frac{P_{DC}}{P_{L}+P_{D}}$$

Where the above are defined as −

$P_{DC}=V_{DC}\times I_{DC}$

$P_{L}=V_{L}\times I_{L}$

$P_{D}=R_{D}\times I_{L}^{2}$($P_{D}$ is the rectifier losses and $R_{D}$ the resistance)

$$\eta =\frac{V_{DC}I_{DC}}{\left ( V_{L}I_{L} \right )+\left ( R_{D}I_{L}^{2} \right )}=\frac{V_{DC}^{2}}{V_{L}^{2}}\times \frac{1}{1+\frac{R_{D}}{R_{L}}}$$

But $R_{D}=0$

Therefore,

$$\eta =\left ( \frac{V_{DC}}{V_{L}} \right )^{2}=\left ( \frac{1}{FF}\right )^{2}$$

### Transformer Utilization Factor

$$TUF=\frac{P_{DC}}{VA \:Rating \:of \:the \:Transformer }=\frac{P_{DC}}{\frac{VA_{p}+VA_{s}}{2}}$$

VAp and VAs are the primary and secondary power ratings of the transformer.

# Reactive Power Control of Converters

In high voltage direct current (HVDC) converters, the stations are line commutated. This implies that the initial current of the valve can only be delayed in reference a zero value of the converter bus voltage in AC form. Consequently, for better control of voltage, the converter bus is connected to a reactive power source.

Reactive power sources are used to vary capacitors in static systems. The response of the reactive power system is dictated by voltage control in dynamic conditions.

When operating unstable AC systems, problems tend to arise because of unstable voltage and overvoltage surges. A better coordination of reactive power sources is required to simplify the control of the firing angles. As a result, this feature of the reactive power converter is increasingly being applied in modern converters using HVDC.

## Reactive Power Control in Steady State

The equations expressing reactive power as a function of active power are given in terms of unit quantities.

Base converter voltage is given by −

$$V_{db}=3\sqrt{\frac{2}{\pi }}\times V_{L}$$

Where VL = Line to line voltage (on winding side)

Base DC Current (Idb ) = Rated DC Current (Idr)

Base DC Power (Pdc) = nb × Vdb × Idb, where nb = number of bridges in series

BaseBase AC voltage (Vb) = (Va)

Base AC Power = Base DC Power

$$\sqrt{\frac{18}{\pi }}\times V_{a}\times I_{db}\times n_{b}$$

# Power Electronics - Dual Converters

Dual converters are mainly found in variable speed drives (VFDs). In a dual converter, two converters are linked together back to back. The operation of a dual converter is explained using the diagram below. It is assumed that −

• A dual converter is an ideal one (gives pure DC output) at its terminals.

• Each two-quadrant converter is a controlled DC source in series with a diode.

• Diodes D1 and D2 show the unidirectional flow of current.

Considering a dual converter operating without circulating current, the AC current is barred from flowing by controlled firing pulses. This ensures that the converter carrying the load current conducts while the other converter is blocked. This means that a reactor between the converters is not needed.

## Battery Charger

A battery charger also known as a recharger utilizes electric current to store energy in a secondary cell. The charging process is determined by the type and size of the battery. Different types of batteries have different tolerance levels to overcharging. The recharging process may be achieved by connecting it to a constant voltage or constant current source.

### Charging Rate (C)

The charging rate is defined as the rate of charging or discharging a battery and is equal to the battery capacity in one hour.

A battery charger is specified in terms of its charging rate C. For example, a battery charger with a rating of C/10 would give a charging capacity in 10 hours while one rated 3C would charge a battery in 20 minutes.

## Types of Battery Chargers

There are many types of battery chargers. In this tutorial, we will consider the five main types.

• Simple chargers − Operates by supplying a constant DC power source into the battery being charged.

• Fast chargers − Uses control circuitry to charger the battery rapidly and in the process prevent the battery cells from damage.

• Inductive chargers − Uses electromagnetic induction to charge the battery.

• Intelligent chargers − Used to charge a battery that contains a chip that communicates with the smart charger.

• Motion powered charger − Makes use of human motion to charge a battery. A magnet placed between two springs is moved up and down by human motion thus charging the battery.

# Phase Controlled Converters Solved Example

A separately excited DC motor has the following parameters: 220V, 100A and 1450 rpm. Its armature has a resistance of 0.1 Ω. In addition, it is supplied from a 3 phase fullycontrolled converter connected to a 3-phase AC source with a frequency of 50 Hz and inductive reactance of 0.5 Ω and 50Hz. At α = 0, the motor operation is at rated torque and speed. Assume the motor brakes re-generatively using the reverse direction at its rated speed. Calculate the maximum current under which commutation is not affected.

Solution

We know that,

$$V_{db}=3\sqrt{\frac{2}{\pi }}\times V_{L}-\frac{3}{\pi }\times R_{b}\times I_{db}$$

Substituting the values, we get,

$220=3\sqrt{\frac{2}{\pi }}\times V_{L}-\frac{3}{\pi }\times 0.5\times 100$

Therefore,

$V_{L}=198V$

Voltage at rated speed = $220-\left ( 100\times 0.1 \right )=210V$

At the rated speed, the regenerative braking in the reverse direction,

$=3\sqrt{\frac{2}{\pi }}\times 198\cos \alpha -\left ( \frac{3}{\pi }\times 0.5+0.1\right )\times I_{db}=-210V$

But $\cos \alpha -\cos \left ( \mu +\alpha \right )=\frac{\sqrt{2}}{198}\times 0.5I_{db}$

For commutation to fail, the following limiting condition should be satisfied.

$\mu +\alpha \approx 180^{\circ}$

Therefore, $\quad \cos \alpha =\frac{I_{db}}{198\sqrt{2}}-1$

Also,

$\frac{3}{\pi }I_{db}-\frac{3\sqrt{2}}{\pi }\times 198-\left ( \frac{3}{\pi }\times 0.5+0.1 \right )I_{db}=-210$

This gives, $\quad 0.3771I_{db}=57.4$

Therefore, $\quad I_{db}=152.2A$

# Power Electronics - Choppers

A chopper uses high speed to connect and disconnect from a source load. A fixed DC voltage is applied intermittently to the source load by continuously triggering the power switch ON/OFF. The period of time for which the power switch stays ON or OFF is referred to as the chopper’s ON and OFF state times, respectively.

Choppers are mostly applied in electric cars, conversion of wind and solar energy, and DC motor regulators.

### Classification of Choppers

Depending on the voltage output, choppers are classified as −

• Step Up chopper (boost converter)
• Step Down Chopper(Buck converter)
• Step Up/Down Chopper (Buck-boost converter)

## Step Up Chopper

The average voltage output (Vo) in a step up chopper is greater than the voltage input (Vs). The figure below shows a configuration of a step up chopper.

### Current and Voltage Waveforms

V0 (average voltage output) is positive when chopper is switched ON and negative when the chopper is OFF as shown in the waveform below.

Where

TON – time interval when chopper is ON

TOFF – time interval when chopper is OFF

Vs – Source voltage

T – Chopping time period = TON + TOFF

Vo is given by −

$$V_{0}=\frac{1}{T}\int_{0}^{T_{ON}}V_{S}dt$$

When the chopper (CH) is switched ON, the load is short circuited and, therefore, the voltage output for the period TON is zero. In addition, the inductor is charged during this time. This gives VS = VL

$L\frac{di}{dt}=V_{S},$ $\frac{\Delta i}{T_{ON}}=\frac{V_{S}}{L}$

Hence,$\Delta i=\frac{V_{S}}{L}T_{ON}$

Δi = is the inductor peak to peak current. When the chopper (CH) is OFF, discharge occurs through the inductor L. Therefore, the summation of the Vs and VL is given as follows −

$V_{0}=V_{S}+V_{L},\quad V_{L}=V_{0}-V_{S}$

But $L\frac{di}{dt}=V_{0}-V_{S}$

Thus,$L\frac{\Delta i}{T_{OFF}}=V_{0}-V_{S}$

This gives,$\Delta i=\frac{V_{0}-V_{S}}{L}T_{OFF}$

Equating Δi from ON state to Δi from OFF state gives −

$\frac{V_{S}}{L}T_{ON}=\frac{V_{0}-V_{S}}{L}T_{OFF}$, $V_{S}\left ( T_{ON}+T_{OFF} \right )=V_{0}T_{OFF}$

$V_{0}=\frac{TV_{S}}{T_{OFF}}=\frac{V_{S}}{\frac{\left ( T+T_{ON} \right )}{T}}$

This give the average voltage output as,

$$V_{0}=\frac{V_{S}}{1-D}$$

The above equation shows that Vo can be varied from VS to infinity. It proves that the output voltage will always be more than the voltage input and hence, it boosts up or increases the voltage level.

## Step Down Chopper

This is also known as a buck converter. In this chopper, the average voltage output VO is less than the input voltage VS. When the chopper is ON, VO = VS and when the chopper is off, VO = 0

When the chopper is ON −

$V_{S}=\left ( V_{L}+V_{0} \right ),\quad V_{L}=V_{S}-V_{0},\quad L\frac{di}{dt}=V_{S}-V_{0},\quad L\frac{\Delta i}{T_{ON}}=V_{s}+V_{0}$

Thus, peak-to-peak current load is given by,

$\Delta i=\frac{V_{s}-V_{0}}{L}T_{ON}$

### Circuit Diagram

Where FD is free-wheel diode.

When the chopper is OFF, polarity reversal and discharging occurs at the inductor. The current passes through the free-wheel diode and the inductor to the load. This gives,

$$L\frac{di}{dt}=V_{0}........................................\left ( i \right )$$

Rewritten as −$\quad L\frac{\Delta i}{T_{OFF}}=V_{0}$

$$\Delta i=V_{0}\frac{T_{OFF}}{L}...................................\left ( ii \right )$$

Equating equations (i) and (ii) gives;

$\frac{V_{S}-V_{0}}{L}T_{ON}=\frac{V_{0}}{L}T_{OFF}$

$\frac{V_{S}-V_{0}}{V_{0}}=\frac{T_{OFF}}{T_{ON}}$

$\frac{V_{S}}{V_{0}}=\frac{T_{ON}-T_{OFF}}{T_{ON}}$

The above equation gives;

$$V_{0}=\frac{T_{ON}}{T}V_{S}=DV_{S}$$

Equation (i) gives −

$\Delta i=\frac{V_{S}-DV_{S}}{L}DT$, from $D=\frac{T_{ON}}{T}$

$=\frac{V_{S}-\left ( 1-D \right )D}{Lf}$

$f=\frac{1}{T}=$chopping frequency

### Current and Voltage Waveforms

The current and voltage waveforms are given below −

For a step down chopper the voltage output is always less than the voltage input. This is shown by the waveform below.

## Step Up/ Step Down Chopper

This is also known as a buck-boost converter. It makes it possible to increase or reduce the voltage input level. The diagram below shows a buck-boost chopper.

When the chopper is switched ON, the inductor L becomes charged by the source voltage Vs. Therefore, Vs = VL.

$$L\frac{di}{dt}=V_{S}$$ $$\Delta i=\frac{V_{S}}{L}T_{ON}=\frac{V_{S}}{L}T\frac{T_{ON}}{T}=\frac{DV_{S}}{Lf}$$

Because −

$D=\frac{T_{ON}}{T}$ and $f=\frac{1}{T} .............................................. \left ( iii \right )$

When the chopper is switched OFF, the inductor’s polarity reverses and this causes it to discharge through the diode and the load.

Hence,

$$V_{0}=-V_{L}$$ $$L\frac{di}{dt}=-V_{0}$$

$L\frac{\Delta i}{T_{OFF}}=-V_{0}$, thus $\Delta i=-\frac{V_{0}}{L}T_{OFF}................................\left ( iv \right )$

Evaluating equation (iii) and (iv) gives −

$\frac{DV_{S}}{Lf}=-\frac{V_{0}}{L}T_{OFF}$, $DV_{S}=-DV_{S}=-V_{0}T_{OFF}f$

$DV_{S}=-V_{0}\frac{T-T_{ON}}{T}=-V_{0}\left ( 1-\frac{T_{ON}}{T} \right )$, $V_{0}=-\frac{DV_{S}}{1-D}$

Because $D=\frac{T_{ON}}{T}=\frac{T-T_{OFF}}{1-D}$

This gives,

$V_{0}=\frac{DV_{S}}{1-D}$

D can be varied from 0 to 1. When, D = 0; VO = 0

When D = 0.5, VO = VS

When, D = 1, VO = ∞.

Hence, in the interval 0 ≤ D ≤ 0.5, output voltage varies in the range 0 ≤ VO < VS and we get step down or Buck operation. Whereas, in the interval 0.5 ≤ D ≤ 1, output voltage varies in the range VS ≤ VO ≤ ∞ and we get step up or Boost operation.

# Power Electronics - Control Methods

In a converter, there are two basic methods of control used to vary the output voltage. These are −

• Time ratio control
• Current limit control

## Time Ratio Control

In time ratio control, a constant k given by $\frac{T_{ON}}{T}$ is varied. The constant k is called duty ratio. Time ratio control can be achieved in two ways −

### Constant Frequency

In this control method, the frequency (f = 1/T0N) is kept constant while the ON time T is varied. This is referred to as pulse width modulation (PWM).

### Variable Frequency

In variable frequency technique, the frequency (f = 1/T) is varied while the ON time T is kept constant. This is referred to as the frequency modulation control.

## Current Limit Control

In a DC to DC converter, the value of the current varies between the maximum as well as the minimum level for continuous voltage. In this technique, the chopper (switch in a DC to DC converter) is switched ON and then OFF to ensure that current is kept constant between the upper and lower limits. When the current goes beyond the maximum point, the chopper goes OFF.

While the switch is at its OFF state, current freewheels via the diode and drops in an exponential manner. The chopper is switched ON when the current reaches the minimum level. This method can be used either when the ON time T is constant or when the frequency (f=1/T).

# Power Electronics - Resonant Switching

Resonant switch converters refers to converters that have inductor and capacitor (L-C) networks and whose current and voltage waveforms vary in a sinusoidal manner during each period of switching. There are various resonant switch converters −

• Resonant DC to DC converters
• DC to AC inverters
• Resonant AC inverters to DC converters

In this tutorial, we will focus on Resonant DC to DC converters

## Resonant DC to DC Converters

The concept of switch mode power supply (SMPS) is explained below using a DC to DC converter. The load is given a constant voltage supply (VOUT) that is obtained from a primary source of voltage supply VIN. The value of VOUT is regulated by varying resistor in series (RS) or the current source connected in shunt (IS). By controlling VOUT through varying IS and ensuring RS is kept constant, a considerable amount of power is lost in the converter.

## Switched Mode Power Supply (SMPS)

An SMPS (switched mode power supply) refers to an electronic device that uses a switching regulator for the purpose of converting electrical power in an efficient manner. SMPS takes power from the main power lines and transfers it to a load. For example, a computer while ensuring the voltage and current characteristics are converted.

The difference between an SMPS and a linear supply of power is that the former keeps switching ON and OFF during low dissipation and uses less time during high dissipation regions. This ensures less energy is wasted. Actually, an SMPS does not dissipate any power.

The size of an SMPS is smaller and very light, compared to a normal linear supply power device of the same size and shape.

The figure below shows the circuit diagram for an SMPS. When the switching frequency is varied, the stored energy can be varied for each cycle and hence the voltage output is varied.

The waveforms below are for a half bridge converter also known as a push-pull. It is used in applications utilizing high power. The input voltage is halved as indicated in the waveform.

# DC to DC Converters Solved Example

A step up chopper has an input voltage of 150V. The voltage output needed is 450V. Given, that the thyristor has a conducting time of 150μseconds. Calculate the chopping frequency.

Solution −

The chopping frequency (f)

$f=\frac{1}{T}$

Where T – Chopping time period = $T_{ON}+T_{OFF}$