lecture 9 intro to power electronics ece 370 machines and power 1

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LECTURE 9 LECTURE 9 INTRO TO POWER INTRO TO POWER ELECTRONICS ELECTRONICS ECE 370 ECE 370 Machines and Power Machines and Power 1

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Page 1: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

LECTURE 9LECTURE 9INTRO TO POWER INTRO TO POWER

ELECTRONICSELECTRONICS

ECE 370ECE 370

Machines and PowerMachines and Power

1

Page 2: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

INVERTERSINVERTERS

2

Perhaps the most rapidly growing area in modern power electronics is static frequency conversion

This is conversion of ac power at one frequency to ac power at another frequency by means of solid-state electronics

Page 3: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

INVERTERSINVERTERS

3

Traditionally there have been two approaches to static ac frequency conversion:

1. Cycloconverter

2. Rectifier-inverter

Page 4: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

INVERTERSINVERTERS

4

The cycloconverter is a device for directly converting ac power at one frequency to ac power at another frequency

The rectifier-inverter first converts ac power to dc power and then converts the dc power to ac power again at a different frequency

Page 5: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

INVERTERSINVERTERS

5

A rectifier-inverter is divided into two parts:

1. A rectifier to produce dc power

2. An inverter to produce ac power from the dc power

Page 6: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

6

The basic rectifier circuits for converting ac power to dc power was covered previously

These circuits have one problem from a motor-control point of view

Output voltage is fixed for a given input voltage

This problem can be overcome by replacing diodes in these circuits with SCRs

Page 7: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

7

The figure below shows a three-phase full-wave rectifier circuit with the diodes in the circuits replaced by SCRs

Page 8: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

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Page 9: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

The average output voltage is found from:The average output voltage is found from:

9

cos

33)(

3 2/

6/

m

abdc

VtdvV

Page 10: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

10

The average dc output voltage from this circuit depends on when the SCRs are triggered during their positive half-cycles

If they are triggered at the beginning of the half-cycle, this circuit will be the same as that of a three-phase full-wave rectifier with diodes

Page 11: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

11

If the SCRs are never triggered, the output voltage will be 0 V

For any other firing angle between 0˚ and 90˚ on the waveform, the dc output voltage will be somewhere between the maximum value and 0 V

Page 12: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

12

When SCRs are used instead of diodes in the rectifier circuit to get control of the dc voltage output, this output voltage will have more harmonic content than a simple rectifier would, and some form of filtering on its output is needed

The following figure shows an inductor and capacitor filter placed at the output of the rectifier to help smooth the dc output

Page 13: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

RECTIFIERSRECTIFIERS

13

Page 14: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

INVERTERSINVERTERS

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Inverters are classified into two basic types by the utilized commutation technique:

External Commutation

Self Commutation

Page 15: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

EXTERNAL COMMUTATION EXTERNAL COMMUTATION INVERTERSINVERTERS

15

External commutation inverters are inverters in which the energy required to turn off the SCRs is provided by an external motor or power supply

Page 16: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

EXTERNAL COMMUTATION EXTERNAL COMMUTATION INVERTERSINVERTERS

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An example of an external commutation is shown below

Page 17: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

EXTERNAL COMMUTATION EXTERNAL COMMUTATION INVERTERSINVERTERS

17

The inverter is connected to a three-phase synchronous motor, which provides the countervoltage necessary to turn off one SCR when its companion is fired

The SCRs in this circuit are triggered in the following order:

SCR1, SCR6, SCR2, SCR4, SCR3, SCR5

Page 18: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

EXTERNAL COMMUTATION EXTERNAL COMMUTATION INVERTERSINVERTERS

18

When SCR1 fires, the internal generated voltage in the synchronous motor provides the voltage necessary to turn off SCR3

Note that if the load is not connected to the inverter, the SCRs would never be tuned off and after ½ cycle a short circuit would develop through SCR1 and SCR4

This inverter is also called a load-commutated inverter

Page 19: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

19

If it is not possible to guarantee that a load will always provide the proper countervoltage for commutation, then a self-commutation inverter must be used

Self-commutation inverters can be

designed using GTOs, IGBTs, or power transistors

Page 20: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

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There are three major types of self-commutation inverters:

1. Current source inverters (SCI)

2. Voltage source inverters (VSI)

3. Pulse-width modulation inverters (PWM)

Page 21: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

21

Pulse-width modulation is the process of modifying the width of the pulses in a pulse train in direct proportion to a small control signal

Page 22: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

The principle of single-phase inverter The principle of single-phase inverter operation can be explained with the operation can be explained with the following figurefollowing figure

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Page 23: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

23

The figure shown is a three-phase inverter using power transistors as active devices

Page 24: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

24

Since power transistor are self-commutating, no special commutation components are included in this circuit

In this circuit, the transistors are made to conduct in the following order: T1, T6, T2, T4, T3, T5

The output phase and line voltage from this circuit are shown on the next slide

Page 25: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

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Page 26: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

A three-phase output can be obtained A three-phase output can be obtained from a configuration of six transistors and from a configuration of six transistors and six diodessix diodes

26

Page 27: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

Two types of control signals can be Two types of control signals can be applied to the transistors: 180applied to the transistors: 180oo conduction conduction or 120or 120oo conduction conduction

27

Page 28: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

For 180 degrees operation, each device For 180 degrees operation, each device conducts 180 degreesconducts 180 degrees

   The sequence of firing is: 123, 234, 345, The sequence of firing is: 123, 234, 345,

456, 561, 612456, 561, 612

The gating signals are shifted from each The gating signals are shifted from each other by 60 degreesother by 60 degrees

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Page 29: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

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Page 30: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

For 120 degrees operation, each transistor For 120 degrees operation, each transistor conducts for 120 degreesconducts for 120 degrees

The sequence of firing is: 61, 12, 23, 34, The sequence of firing is: 61, 12, 23, 34, 45, 56, 6145, 56, 61

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SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

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SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

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Current source inverters and voltage source inverters are different from PWM inverters and have been used for a long time

PWM inverters require more complex control circuitry and faster switching components than CSI and VSI

Page 33: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

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Page 34: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATION SELF-COMMUTATION INVERTERSINVERTERS

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In the current source inverter, a rectifier is connected to an inverter through a large series inductor LS

The inductance of LS is sufficiently large that the dc current I constrained to be almost constant

Page 35: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SELF-COMMUTATIION SELF-COMMUTATIION INVERTERSINVERTERS

35

The SCR current output waveform will be roughly a square wave since IS is constrained to be nearly constant

The line-to-line voltage will be triangular

It is easy to limit overcurrent conditions in this design, but the output voltage can swing widely in response to changes in load

Page 36: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SINGLE-PHASE CURRENT SINGLE-PHASE CURRENT SOURCE INVERTERSOURCE INVERTER

36

A single-phase CSI circuit with capacitor commutation is shown below

Page 37: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SINGLE-PHASE VOLTAGE SINGLE-PHASE VOLTAGE SOURCE INVERTERSOURCE INVERTER

37

In the voltage source inverter, a rectifier is connected to an inverter through a series inductor LS and a parallel capacitor C

The capacitance of C is sufficiently large that the voltage is constrained to be almost constant

Page 38: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SINGLE-PHASE VOLTAGE SINGLE-PHASE VOLTAGE SOURCE INVERTERSOURCE INVERTER

38

The SCR line-to-line voltage output waveform will be roughly a square wave, since the voltage Vc is constrained to be nearly constant

The output current flow will be approximately triangular

Page 39: LECTURE 9 INTRO TO POWER ELECTRONICS ECE 370 Machines and Power 1

SINGLE-PHASE VOLTAGE SINGLE-PHASE VOLTAGE SOURCE INVERTERSOURCE INVERTER

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Voltage variations are small in this circuit, but currents can vary wildly with variations in load, and overcurrent protection is difficult to implement

The frequency of both current and voltage source inverters can be easily changed by changing the firing pulses on the gates of the SCRs, so both inverters can be used to drive ac motors at variable speeds