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2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical and Computer Engineering Lecture 2 and Lecture 4.1 Introduction to Electric Circuit Analysis Prof. Klaus Yung-Jane Hsu 徐永珍

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Page 1: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2003/2/20 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

EE110300 Practice of Electrical and Computer Engineering

Lecture 2 and Lecture 4.1

Introductionto

Electric Circuit Analysis

Prof. Klaus Yung-Jane Hsu徐永珍

Page 2: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

What Is An Electric Circuit?

• Electrical Systems– Information, Power, Control, etc.

• Behavioral Model• An electric circuit is a mathematical

model which approximates the behavior of an actual electrical system.

Page 3: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

What Is Electric Circuit Theory?

• A Special Case of Electromagnetic Field Theory

• The Study of Static and Moving Electric Charges

• 學習分析電荷的交通問題

Page 4: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

5 Basic Model Elements in Electric Circuit Theory

• Active Components– Voltage Source– Current Source

• Passive Components– Resistor– Capacitor– Inductor

Page 5: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Atomic TheoryAtomic Theory

K L M NN ucleus

Simplified representation of the atom

Nucleus normally consists of neutrons and protons (positively charged)

Electrons orbit the nucleus in discrete orbits called shells (K, L, M, N, etc.)

Atom is electrically neutral since No. of protons = No. of electrons

The outer most shell is called the valence shell and electrons in this shell

are called valence electrons

Page 6: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Different Types of Material

• Conductors are materials (e.g. copper, aluminum, gold) that have large numbers of free electrons.

• Insulators do not conduct (e.g. plastic, rubber, porcelain) because they have full or nearly full valence shells.

• Semiconductors have half-filled valence shells (e.g. silicon, germanium).

Page 7: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

What Is Electric Charge?

• A body is said to be charged when it has an excess or deficiency of electrons.

• The unit of electrical charge is the coulomb (C) = 6.24 x 1018 electrons.

• Coulomb’s Law: F = kQ1Q2 / r2 where k = 9 x 109, Q1 and Q2 are charges in coulombs, and r in m.

Page 8: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Current

• 電流,即電荷的流量• 1 A of current is 1 C of charge passing a

given point in 1 s, i.e.

I = Q / t or Q = I x t.

Page 9: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Direction of Current

• Electrons flow from negative terminal to positive terminal but conventional current flows in the opposite direction.

E+- I

Lamp

Direction of conventional current

Page 10: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Voltage

• 電壓,即電位差• When charges are transferred from one body

to another, a potential difference or voltageresults between them.

• The voltage between two points is 1 V if it requires 1 J of energy to move 1 C of charge from one point to the other; i.e. V = W / Q.

• Symbol for DC Voltage Sources:

Page 11: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Practical DC Voltage Source -Battery

• Primary batteries are not rechargeable;Secondary batteries are rechargeable.

• Batteries come in different shapes (e.g button), sizes (e.g. AAA, AA, C, D), types ( e.g. alkaline, carbon-zinc, lithium, NiCad, lead acid) and ratings.

• Battery capacity (Ah) = current drain x expected life.

Page 12: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Other DC Voltage Sources

• Electronic power supplies rectify ac to dc for use in equipment or labs.

• Solar/photovoltaic cells convert sunlight to electrical energy for remote areas or space applications.

• DC generators convert mechanical energy to electrical energy by rotating a coil of wire through a magnetic field.

Page 13: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Practical DC Current Sources

• Usually, a combination of DC voltage sources and other electrical devices (e.g. transistors, resistors, etc.) is required.

• Symbol of a DC Current Source:

Page 14: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Resistor

• A resistor is defined as a component whose terminal voltage is proportional to the current flowing through. That is, a resistor is a device that obeys the Ohm’s Law.

• Ohm’s Law: V=IR• The constant R is called the resistance (Ω) of

the resistor.• Symbol:

Page 15: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Resistor Color Code

Band

1 2 3 4 5

3

33

1

33

5

5533 5

4

2, Significant Figures

MultiplierTolerance

Reliability

Colour: Bk, Br, R, O, Y, Gn, Bl, V, Gr, W, Gl , S , No ColourBand 1: 1 2 3 4 5 6 7 8 9 Band 2: 0 1 2 3 4 5 6 7 8 9Band 3: 1 10 102 103 104 105 106 107 .1 .01 Band 4: 5% 10% 20%

Page 16: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

CapacitanceCapacitance

n A capacitor consists of two metal plates separated by an insulator(dielectric) which may be air, oil, mica, plastic, ceramic, etc.

n When a dc source is applied across the capacitor, one of the platesbecomes positive and the other negative.

n The amount of charge stored by a capacitor is: Q = CV (C)

MetalPlates

Lead Dielectric

Lead

Parallel-plate capacitor

EC

Circuit symbol

E

C

ψ

Electric fieldof capacitor

Page 17: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Capacitance (contCapacitance (cont’’d)d)

n Capacitance of a parallel-plate capacitor is: C = ε A / d (F), where ε is the permittivity of the

dielectric, A is the area of each plate and d is theseparation of the plates. Further,ε = εr εo where εr is the relative permittivity or dielectricconstant of the dielectric and εo = 8.85 x 10-12 F/m isthe permittivity of air.

n Energy stored between the plates is given by W = 1/2CV2 (J)

Page 18: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Induced Voltage & InductionInduced Voltage & Induction

dtdΦ

= Ne

8FaradayÕs Law: voltage is induced in a circuit whenever the flux linking the circuit is changing and the magnitude of the voltage is proportional to the rate of change of flux linkages:

(volts)

8LenzÕs Law: the polarity of the induced voltage (known as the counter emf or back emf) is such as to oppose the cause producing it.

Page 19: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Self-InductanceSelf-Inductance

L vL= L d i

d t

+

-

I

Voltage acrossinductor

l

dA

Inductor Coil

dtdi

Lv L =

4Induced voltage across the coil is:

(V)

4Approximate inductance of coil (when l /d > 10) is:

lAN

orl

ANL or

22 µµµ=

: = permeability

(H)

Page 20: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Power

• The Rate of Doing Work:

where W is the work (or energy) in joulesand t is in seconds.

• P=V I

tW

=P (watts, W)

Page 21: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Series Circuits & KVLSeries Circuits & KVL

E R

+-

+

-+

-VR

R

+ -V

V

1

2

3

2

3

1

E

1

2+-

I

n KirchhoffÕs Voltage Law states that for a closed loop:ΣV = 0, or Σ Vrises = Σ Vdrops

n The total resistance of n resistors in series is:RT = R1 + R2 + . . . + Rn

n The total power is: PT = P1 + P2 + . . . + Pn

Page 22: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Voltage Divider RuleVoltage Divider Rule

The voltage applied to a series circuit will bedropped across all the resistors in proportionto the magnitude of the individual resistors.

Vx = (Rx / RT) E

E R

+-

+

-+

-V

R

R

+ -V

V

1

2

3

2

3

1

I

Page 23: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Parallel CircuitParallel Circuit

n Elements/branches are said to be parallel when they have only2 nodes in common. The voltage across all parallel elements ina circuit will be the same.

n Voltage sources of different potentials should never beconnected in parallel.

IT

E+

I1 I2

R1 R2 I3R3

RT

Ix = E / Rx; KCL: IT = I1 + I2 + I3 = E / RT

Page 24: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Parallel Circuits & KCLParallel Circuits & KCL

n KirchhoffÕs Current Law: ΣI = 0, or Σ Iin = Σ Iout

n Overall conductance: GT=G1 + G2 + . . + Gn =1/RT

i.e. Total resistance, RT = 1/(1/R1 + 1/R2 + . . . + 1/Rn)n For 2 resistors in parallel: RT= R1R2 / (R1 + R2)n For n equal resistors in parallel: RT = R/n where R is the

resistance of each resistor.

n Current divider rule: Ix = (RT/Rx)ITn Total power dissipated: PT = P1 + P2 + . . . + Pn

where P1 = E2/R1 or EI1; . . . . ; Pn = E2/Rn or EIn

Page 25: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Capacitor ChargingCapacitor Charging

vc= E(1-e-t/τ) i = (E/R)e-t/τ

τ = RC

vR = Ee-t/τ

E C

a

b

R

+

- cTransientInterval

SteadyState

t

vc

v

E

t

i

0

0

ER

i

Page 26: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Current Buildup Transient in InductorCurrent Buildup Transient in Inductor

vR = E(1-e-t/τ)

vL = Ee-t/τ

i = (E/R)(1-e-t/τ) τ = L/R

E+

-

TransientInterval

SteadyState

t

v

E

t

i

0

0

ER

i

R

L vL

L

Page 27: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2/20/2003 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

What Will You Get in Learning Electric Circuit Theory?

• Being equipped with basic common sense, language, and analysis skill for studying the hardware of any electrical systems

• Extensive examples will be encountered in the courses of Microelectronics, Power Electronics, and Power Systems

Page 28: Introduction to Electric Circuit Analysis · 2005. 9. 12. · 2003/2/20 Advanced Silicon Device and Material Laboratory NTHU, HsinChu, Taiwan, 30013 EE110300 Practice of Electrical

2003/2/20 Advanced Silicon Device and Material Laboratory

NTHU, HsinChu, Taiwan, 30013

Bon Voyage!旅途愉快!