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Electricity From the word “ElektronGreek for “amber

20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

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Page 1: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

• Electricity – From the word “Elektron”– Greek for “amber”

Page 2: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Electrical systems have two main objectives:

• To gather, store, process, transportinformation & Energy

• To distribute and convert energy

Page 3: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Electrical Engineering Subdivisions

Communication Computer Systems Control Systems Electromagnetics

Electronics Power Systems Signal Processing

Page 4: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Where do we find electrical circuits?• Communications

– Radio, internet, telephone, television• Data Processing

– Desktop computers, servers• Automobiles

– displays, sensors, motors• Home

– lighting, heating, appliances• Weather Stations

– wind speed, precipitation, temperature• Power Plants

– moving magnets, transformers

Human Body is Polymeric System controlled by Electrical System?

Page 5: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Why Study Electrical Engineeringin SNU MSE ?

• To know the Basic Knowledge of Electronics • So you can understand a little about Electronic

System around you • To Operate and Maintain Electrical Systems• To Communicate with Electrical Engineer • Additionally Good Examination Grade

Page 6: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Basic Definitions

Capacitor dtdVCI = 2

21 CVP =

Power

ResistorRVIorIRV ==

InductordtdILV =

Passive Component

Active ComponentDiode

TransistorOP amp

Passive : No Power Gain (Two terminal)Active : Power Gain : Built-in Power Source

Linear

NonLinear

221 LIP =

RVIRVIP

22

21 ===

Page 7: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Circuit Symbols• Battery or Power Supply• Resistor• Capacitor• Switch

Page 8: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

More Circuit Symbols

• DC Voltage Supply• AC Voltage Supply• Open Circuit• Closed Circuit• Short Circuit • DC Current Supply• AC Current Supply

Page 9: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25
Page 10: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Electrical Current • Current - the rate of flow of charge through a

conductor– Conventional Current

• Direction of flow of positive (+) charges

– Electron Current• Opposite to that of conventional current

• Units for Current– Amperes

• Charge of the Electron– e = -1.603 × 10-19 Coulombs

• 1 A = 1 C/s

Page 11: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Effect of Electric Currents on the Body

• 0.001 A can be felt• 0.005 A is painful• 0.010 A causes involuntary muscle contractions• 0.015 A causes loss of muscle control• 0.070 A can be fatal if the current last for more

than 1 second

Page 12: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Current Equation

tqi∆∆

=

Current in Amperes (A)

Charge inCoulombs (C)

Time in Seconds (s)

dt)t(dqi =Calculus:

Page 13: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Figure 1.4

dttdqti )()( = (1.1)

∫ +=t

ttqdttitq

0

)()()( 0(1.2)

)(tq : Charge

)(ti : Currentt0 : some initial time

at which the chargeis known

Page 14: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Types of Electricity

• Static Electricity - no motion of free charges• Current Electricity - motion of free charges

– Direct Current (DC)– Alternating Current (AC)

Page 15: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Voltage Description

Current Description

Page 16: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

KIRCHHOFF’S CURRENT LAW (KCL)

• The net current entering a node is zero.• Alternatively, the sum of the currents entering a

node equals the sum of the currents leaving a node.

i1 + i2 - i3 = 0 i3 - i4 = 0 i5 + i6 - i7 = 0

Page 17: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Kirchoff Current Law : Σ Ik=0“The sum of current at a node is always zero”

Parallel Circuit : Constant Voltage

∑∑ ===k kk k Z

ZZV

ZVI 1

Resistor ∑=k

kRR /1 Capacitor ∑=k

kCC

ia - ib + ic - id = 0

Σ Ik=0

Current Direction+ : Inward Direction- : Outward Direction

Page 18: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

ia = 4A ib = -2A ic = -8A

ia = ib = ic

Examples of KCL

Page 19: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Voltage • Voltage : A measure of the potential to move electrons.• Sources of Voltage

– Batteries (DC)– Wall Outlets (AC)

V9)t(v =

)t120sin(V110)t(v π=

Unit of voltage : Volts (V) 1V = 1 Joule per coulomb (J/C).

DC

AC

Page 20: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

baab vv −=

Page 21: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

KIRCHHOFF’S VOLTAGE LAW(KVL)

The algebraic sum of the voltages equals zero for any closed path (loop) in an electrical circuit.

Page 22: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Kirchoff Voltage Law : Σ Vk=0“The sum of voltage drop around a loop is always zero”

Serial Circuit : Constant Current

∑∑ ===k

kk

k ZZIZIZV

Resistor ∑=k

kRR Capacitor ∑=k

kCC /1

Same Current for All Elements Same Volatve for All Elements

Page 23: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

A, B C D, E, F

Parallel

Serial

Rearrangement of Circuit

Page 24: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Power and Energy

• Power : the rate of energy conversion• Units : Watts• Equation : p=iv

• Resistors convert electrical energy into heat energy.

p = iv Power delivered by a batteryp = -iv Power dissipated by a resistor

Page 25: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

POWER AND ENERGY

)()()( titvtp =

vip =

2Rip =

Rvp

2

=

∫=1

2

)(t

tdttpw

Power

Energy

Page 26: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Introduction to Circuit Element- Conductor- Voltage Source- Current Source- Resistor

Ideal Element :

Conductor : The voltage between ends of an ideal conductor is zero regardless of the current through the conductor

Short Circuit

Note. Open Circuit

Page 27: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Independent Source

Voltage or Current is specified by itself into Circuit.

Constant Voltage Source Constant Current Source

Battery, Home Power Specially Designed Circuit

Page 28: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Dependent Voltage Source

Voltage or Current is determined by others in Circuits

Τransistor, Amplifier, Electrical Generator

Page 29: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Dependent Current Source

Current through Source is designed as 3vx

if vx = 5V Source : 15A

Many type of real world devices such as Electrical machines Transistor, transformer Amplifierdue to Safety & Economics

Current through Source is designed as 2iy

if iy = 5A Source : 10A

Page 30: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Resistor Equations

• Ohm’s Law: v = iR• Resistance:

ALR ρ

=

Resistivity in Ohms-meters (Ω m)

Cross-sectional AreaIn square meters (m2)

Length inMeters (m)

Resistance inOhms (Ω)

Page 31: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

ALR ρ

=ρ : resistivity

Page 32: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

iRv =R

G 1=Gvi = G : conductance

R : resistance

Ohm’s law

Page 33: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

What is an Insulator?

• A material that does not allow electrons to flow freely• Examples:

– Wood– Plastics– Ceramics– Amber

Page 34: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

What is a conductor?

• A material that allows free electron movement• Examples:

– Aluminum– Gold– Copper– Most Metals

Page 35: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

What is a semiconductor?

• A class of materials whose electron conductivity is between that of a conductor and insulator

• Examples:– Silicon– Germanium

Page 36: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Summary

Page 37: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

> 1021

1 × 1012

1 × 1019

10-8 to 1

2.73 × 10-8

3.5 × 10-5

1.72 × 10-8

2.27 × 10-8

1.12 × 10-6

1.63 × 10-8

5.44 × 10-8

Fused quartzGlass (typical)Teflon

Insulators

Silicon (divice grade)depends on impurity concentration

Semiconductors

AluminumCarbon (amorphous)CopperGoldNichromeSilverTungsten

Conductors Resistivity

Resistivity for Various Material at 300K

Page 38: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Mechanical Strain Gauge(Resistor)

Page 39: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Resistor Color Codes

-2 Silver-1 Gold 0 Black1 Brown2 Red3 Orange4 Yellow5 Green6 Blue7 Violet8 Gray9 White

Tolerance 5% Gold10% Silver20% No 4th band

f

p

n

μ

m

k

M

G

Abbreviation

10-15

10-12

10-9

10-6

10-3

103

106

109

Scale factor

femto-

pico-

nano-

micro-

milli-

kilo-

meg- or mega-

giga-

Prefix

Page 40: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

INTRODUCTION TO CIRCUITS

Page 41: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Kirchoff Current Law : Σ Ik=0“The sum of current at a node is always zero”Parallel Circuit : Constant Voltage

∑∑ ===k kk k Z

ZZV

ZVI 1

Kirchoff Law

Resistor ∑=k

kRR /1 Capacitor ∑=k

kCC

Kirchoff Voltage Law : Σ Vk=0“The sum of voltage drop around a loop is always zero”

Serial Circuit : Constant Current

∑∑ ===k

kk

k ZZIZIZV

Resistor ∑=k

kRR Capacitor ∑=k

kCC /1

Page 42: 20005 - Chapter01 SNUengineering.snu.ac.kr/lecture_pdf/EE/2005 - Chapter01_SNU.pdf · Microsoft PowerPoint - 20005 - Chapter01_SNU Author: professor Created Date: 9/12/2005 2:24:25

Concept Questions

• How can you change the resistance of a resistor?

• How would you determine the resistivity of pencil lead?

• How would you determine the Number of Electrons in Earth?