lecture 14 second-order circuits (2) hung-yi lee

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Lecture 14 Second-order Circuits (2) Hung-yi Lee

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Page 1: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Lecture 14Second-order Circuits (2)

Hung-yi Lee

Page 2: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Second-Order CircuitsSolving by differential

equation

Page 3: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Second-order Circuits

• Steps for solving by differential equation• 1. List the differential equation (Chapter 9.3)• 2. Find natural response (Chapter 9.3)• There are some unknown variables in the natural

response.• 3. Find forced response (Chapter 9.4)• 4. Find initial conditions (Chapter 9.4)• 5. Complete response = natural response + forced

response (Chapter 9.4)• Find the unknown variables in the natural response

by the initial conditions

Page 4: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Review Step 1: List Differential Equations

sCCC vL

vLC

vL

Rv

C

11 sLL i

LCi

LCii

11

RC

1L

Page 5: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Review Step 2: Natural Response

λ1, λ2 is

21

21

Overdamped

Critical damped

Complex0

0

Underdamped

Undamped

20

2 20

2

20

2

Real

02 N20NN tytyty 2

02

21,

Page 6: Lecture 14 Second-order Circuits (2) Hung-yi Lee

α=0Undamped

Fix ω0, decrease αThe position of the two roots λ1 and λ2.

20

221,

Page 7: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.11

0 V0

0 V30)(

F640

1 ,5 H,1.0

t

ttv

CRL

s

Natural response iN(t):

01

NNN iLC

iL

Ri

0? ttiL

0640050 NNN iii

tei AN 06400502 ttt AeAeAe

06400502

2

640045050,

2

21

j7625

sCCC vL

vLC

vL

Rv

C

11

sLLL vL

iLC

iL

Ri

11

Page 8: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.11

0 V0

0 V30)(

F640

1 ,5 H,1.0

t

ttv

CRL

s

Natural response iN(t): 0? ttiL

j7625, 21

dj 21,

tbtaety ddt

N sincos

tbtaeti tN 76sin76cos25

Forced response iF(t)=0 tbtaetiti t 76sin76cos25

NL Complete response iL(t):

Two unknown variables, so two initial conditions.

sCCC vL

vLC

vL

Rv

C

11

sLLL vL

iLC

iL

Ri

11

Page 9: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.11

Initial condition

30V

short

open

00 Li

300 Cv

00 Li

300 Cv

00 Ci 00

CvC

300 Lv 300

LiL

0 V0

0 V30)(

F640

1 ,5 H,1.0

t

ttv

CRL

s

0? ttiL

0t

Page 10: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.11

tbtaeti t 76sin76cos25L 00

Li

300 LiL 3000

Li

aiL 0 0 tbeti t 76sin25L

tetebti tt 76cos7676sin25 2525L

760L bi 300 95.3b

teti tL 76sin295.3 25

Page 11: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.11

teti tL 76sin295.3 25

)9076cos(95.3)( 25 teti tLTextbook:

Page 12: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

0 V30

0 V0)(

F640

1 ,? H,1.0

t

ttv

CRL

s

Natural response vN(t): 0?C ttv

tev AN

06400102 ttt AeAeRAe 06400102 R

2

640041010,

2

21

RR

sCCC vL

vLC

vL

Rv

C

11

306400640010 CCC vvRv

0640010 NNN vvRv

Forced response vF(t):

ssv YF 306400640010 FFF vvRv 30

Page 13: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

Initial condition:

0V

short

open

00 Li

00 Cv

00 Li

00 Cv

00 Ci 00

CvC

0 V30

0 V0)(

F640

1 ,? H,1.0

t

ttv

CRL

s

0?C ttv

Page 14: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

tvtvtv F NC

tt eetv 2121N AA

2

640041010,

2

21

RR

30F tv

Different R gives different response

R16R160 R

0R 16R

?0R

00 Cv 00

CvC

Initial condition:

Page 15: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

16R 34ROverdamped:

2

64004341010,

2

21

R 320,20

ttC eAeAtv 320

220

130)(

ttC eAeAtv 320

220

1 32020)(

3021 AA

032020 21 AA

2,32 21 AA

tvtvtv F NC

tt eetv 2121N AA

2

640041010,

2

21

RR

30F tv

00 Cv 00

CvC

Initial condition:

Page 16: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

16RCritical damped:

tvtvtv F NC

tt eetv 2121N AA

2

640041010,

2

21

RR

30F tv

80, 21 )( 802

801N

tt teAeAtv

30)( 802

801

ttC teAeAtv

808030)( 80802

80 tttC teeAetv

030)0( 1 AvC 301 A

3030 802

80 tt teAe

08030)0( 2 AvC 24002 A

00 Cv 00

CvC

Initial condition:

Page 17: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

tvtvtv F NC

tt eetv 2121N AA

2

640041010,

2

21

RR

30F tv

j7625, 21 16RUnderdamped: 5R

tbtaetv t 76sin76cos25N

tbtaetv t 76sin76cos30 25C

0300 avC30a

tbtae

tbtaetvt

tc

76cos7676sin76

76sin76cos2525

25

076250 bavC

87.9b

00 Cv 00

CvC

Initial condition:

Page 18: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

tbtaetv t 76sin76cos30 25C

t

ba

bt

ba

aebatv t

C 76sin76cos302222

2522

30a 87.9b

31.58cos x sin x

)76cos(58.3130)( 25 xtetv tC 8.161x

Page 19: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 9.12

)8.16176cos(58.3130)( 25 tetv tC

24003030)( 8080C

tt teetv

ttC eetv 32020 23230)(

Page 20: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Non-constant Input

• Find vc(t) for t > 0 when vC(0) = 1 and iL(0) = 0

Li12

1cv

sv

cc vi 12

1

LL iv 5.0

LcLs iivv

cc vi dtviiviv cccccs 2

cccccs vvvvvv

12

12

12

1

12

1

sccc vvvv 6712

dtvii ccL 2

Page 21: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Non-constant Input

4,3, 21 0712 NNN vvv

tKtKvF cossin 21

t

tKtKtKtKtKtK

sin30

cossinsincos7cossin12 212121

30127 121 KKK 30711 21 KK

0127 212 KKK 0117 21 KK 17

331 K

17

212 K

sccc vvvv 6712

Natural response vN(t):

Forced response vF(t):

tt eAeAtv 42

31N

tvvvv sFFF sin566712

tvs cos5

Page 22: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Non-constant Input

Li12

1cv

sv

10 Cv 00 Li

20 Ci 200 CC vCi

240 Cv

Initial Condition:

Page 23: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Non-constant Input

tvtvtv FN C

tKtKvF cossin 21 17

331 K

17

212 K

tt eAeAtv 42

31N

tteAeAtv tt cos17

21sin

17

3342

31C

10 Cv 240 Cv

117

2121 AA

tteAeAtv tt sin17

21cos

17

3343 4

23

1C

2417

3343 21 AA

251 A

17

4292 A

Page 24: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Second-Order CircuitsZero Input + Zero State

& Superposition

Page 25: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Review: Zero Input + Zero State

y(t) = general solution + special solution

= natural response + forced response

y(t) = state response (zero input) + input response (zero state)

= =

y(t): voltage of capacitor or current of inductor

If input = input 1 + input 2 + ……

= state response (zero input) + input 1 response + input 2 response ……

Set sources to be zeroSet state vc, iL to be zero

Page 26: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1

30015)(

F2

1 ,

4

5 H,

8

1

ttv

CRL

s

Vv 30C AiL 00

State response (Zero input):Find vC(t) for t>0

01

statestatestate vLC

vL

Rv 01610 statestatestate vvv

016102 8,2

ttstate eAeAtv 8

22

1

sCCC vL

vLC

vL

Rv

C

11

(pulse)

Page 27: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1

ttstate eAeAtv 8

22

1

Vv 30state

00state vC

321 AA

082 21 AA1,4 21 AA

ttstate eetv 824

State response (Zero input):

30015)(

F2

1 ,

4

5 H,

8

1

ttv

CRL

s

Vv 30C AiL 00

Find vC(t) for t>0

sCCC vL

vLC

vL

Rv

C

11

(pulse)

Page 28: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1

00C v 00C v

=

0

-15

)(1 tvs

…30

15

tsv

15

0

)(2 tvs3030

Input response (Zero State):

30015)(

F2

1 ,

4

5 H,

8

1

ttv

CRL

s

Vv 30C AiL 00

Find vC(t) for t>0

(pulse)

(set state to be zero)

Page 29: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1 sCCC vL

vLC

vL

Rv

C

11

0

15

)(1 tvs

…30

00C v 00C v

15161610 111 inputinputinput vvv

ttinput eAeAtv 8

22

11 15 015 21 AA

082 21 AA 52 A

201 Att ee 82 52015

15

0

)(2 tvs30

3083022 52015 tt

input eetv

30002 ttvinput

30t

Page 30: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1

=

0

-15

)(1 tvs

…30

15

tsv

15

0

)(2 tvs3030

Input response (Zero State):

02 tvinput

tt

input

ee

tv82

1

52015

tt

inputinput

ee

tvtv82

1

52015

300 t

Page 31: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1

=

0

-15

)(1 tvs

…30

15

tsv

15

0

)(2 tvs3030

Input response (Zero State): 30t

tvtvtv inputinputinput 21

3088

3022

5

20

tt

tt

ee

ee

308

302

2

5

2015

t

t

input

e

e

tv

t

t

input

e

e

tv

8

2

1

5

2015

Page 32: Lecture 14 Second-order Circuits (2) Hung-yi Lee

30t300 t

Example 1

ttstate eetv 824

tt

input

ee

tv82 52015

Input response (Zero State)

State response (Zero input)

3088

3022

5

20

tt

tt

input

ee

ee

tv

300 t

30t

tt eetvtvtv 82inputstateC 62415

308302inputstateC 520 ttetvtvtv

Page 33: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1 – Differential Equation

15 tsv

30

30015)(

F2

1 ,

4

5 H,

8

1

ttv

CRL

s

Vv 30C AiL 00

Find vC(t) for t>0

(pulse)

Vv 30C 00 Cv

0t

30t Vv 1530C

Assume 30s is large enough

030 Li

30t Vv 1530C 030

Cv

Page 34: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1 – Differential Equation

Vv 30C

00 Cv

Vv 1530C

030 Cv

t0t 30t

15vs t 0vs t

1516

1610 CCC

vvv

0

1610 CCC

vvv

tt eAeAtv 82

21C 15

6

24

2

1

A

A:300 t

Page 35: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 1 – Differential Equation

Vv 30C

00 Cv

Vv 1530C

030 Cv

t0t 30t

15vs t 0vs t

0

1610 CCC

vvv

tt eAeAtv 82

21C

2402

601 5,20 eAeA

1530 3082

3021C eAeAv

08230 3082

3021C eAeAv

308302C 520 tt eetv

1516

1610 CCC

vvv

Page 36: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2

0)(

F2

1 ,

4

5 H,

8

1

tttv

CRL

s

Vv 30C AiL 00

State response (Zero input):

Find vC(t) for t>0

sCCC vL

vLC

vL

Rv

C

11

ttstate eetv 824 Changing the input will not

change the state (zero input) response.

Page 37: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2

0)(

F2

1 ,

4

5 H,

8

1

tttv

CRL

s

Vv 30C AiL 00

Input response (Zero state):

Find vC(t) for t>0

sCCC vL

vLC

vL

Rv

C

11

00input v 00input v

(set state to be zero)Input

What is the response? 4 methods

Page 38: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 1 for Zero State

sCCC vL

vLC

vL

Rv

C

11

tvvv 161610 inputinputinput

Natural Response:

01610 NNN vvv

21 KtKtvF tKtKK 161610 211

ttN eAeAtv 8

22

1

Forced Response:

tvvv 161610 FFF

8

5,1 21 KK

8

5ttvF

00input v 00input v

ttFNinput eAeAttvtvtv 8

22

18

5

Page 39: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 1 for Zero State

ttinput eAeAttv 8

22

18

5 00input v 00input v

08

50 21 AAvinput

ttinput eAeAtv 8

22

1 821

08210 21 AAvinput24

13

2

2

1

A

A

ttinput eettv 82

24

1

3

2

8

5

Page 40: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 2 for Zero State

Find the response of each small pulse

Then sum them together

Page 41: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 2 for Zero State

=

0

-1

…1 1

0

…t t

tt eetv 82

3

1

3

41 tttt eetv 82

3

1

3

41

tttt eeeetv 8822 13

11

3

4

tetetv tt 83

12

3

4 82 tee tt 82

3

8

Page 42: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 2 for Zero State

teetv tt 820 3

8

1

t

1t

teetv ttttt 11

1

82

3

8

Consider a point avalue of the pulse at t1 is

att 1

tee

av

tata

t

11

1

82

3

8

Page 43: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 2 for Zero State

at

t

tatainput dteettv

0

82

3

8

at

t

taat

t

ta dtteedttee0

88

0

22

3

8

3

8 1

2 at

a

edtte

atat

Consider a point avalue of the pulse at t1 is teeav tata

t 11

1

82

3

8

Page 44: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 2 for Zero State

1

64

118

643

81

4

112

43

8 88

22 a

eea

ee

aa

aa

aa eaea 82

64

118

64

1

3

8

4

112

4

1

3

8

aa eea 82

24

1-

3

2

8

5

at

t

taat

t

tainput dtteedtteeav

0

88

0

22

3

8

3

8

12

ata

edtte

atat

18

643

812

43

8 88

22 t

eet

ee

ta

ta

0t

at

We can always replace “a” with “t”.

Page 45: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 3 for Zero State

att

0

t …

teetv tt

82

3

1

3

41

dtee

avat

t

tata

input

0

82

3

1

3

41

…………

The value at time point a

Page 46: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 3 for Zero State

at

t

tatainput dteeav

0

82

3

1

3

41

at

t

at

t

taat

t

ta dtedtedt0 0

8

0

2

3

1

3

41

18

1

3

11

2

1

3

4 8822 aaaa eeeea

aa eea 82 124

11

3

2 aa eea 82

24

1-

3

2

8

5

at

t

at

t

taat

t

ta dteedteedt0 0

88

0

22

3

1

3

41

Page 47: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 4 for Zero State

0

1 …

ttxslope )(

?)(slope ty

Source Input:

Input (Zero State) Response

)()( tutxstep Source Input:

Input (Zero State) Response

ttstep eety 82

3

1

3

41

Page 48: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Method 4 for Zero State

txtytyty slope161610 slopeslopeslope

txtytyty step161610 stepstepstep

ttxslope )( ?)(slope ty

)()( tutxstep ttstep eety 82

3

1

3

41

txtxtytyty stepslope 16161610 slopeslopeslope

tyty stepslope tt ee 82

3

1

3

41

A24

1

3

2 82slope tt eetty

8

5A

Page 49: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2

at

t

tatainput dteeav

0

82

3

1

3

41

at

t

tatainput dteetav

0

82

3

8Method 2:

Method 3:

Method 4: tvinput tt ee 82

3

1

3

41

Page 50: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2

ttC eettv 82

24

23

3

10

8

5

ttvs

0)(

F2

1 ,

4

5 H,

8

1

tttv

CRL

s

tvtvtv inputstateC

Page 51: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 2 – Checked by Differential Equation

0)(

F2

1 ,

4

5 H,

8

1

tttv

CRL

s

Vv 30C AiL 00

Find vC(t) for t>0

ttC eAeAttv 8

22

18

5

ttN eAeAtv 8

22

1

sCCC vL

vLC

vL

Rv

C

11

8

5ttvF 30C v 00

Li

00C vC 30L iL

38

521 AA

0821 21 AA24

23,

3

1021 AA

Page 52: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 F2

1 ,

4

5 H,

8

1 CRL

Vv 30C AiL 00

Find vC(t) for t>0

30

300

0

30

0

s

t

t

t

V

ttv

How to solve it?I will show how to solve the problem by

Method 1: Differential equationMethod 2: Integrating Step ResponsesMethod 3: Differentiate the sources

Page 53: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 – Method 1: Differential Equation

Vv 30C AiL 00

Find vC(t) for t>0

30

300

0

30

0

s

t

t

t

V

ttv

ttC eettv 82

24

23

3

10

8

5

300 t

24060

24

23

3

10

8

5303030 eevv CC

ttC eetv 82

3

23

3

201 24060

3

23

3

2013030 eevv CC

Page 54: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 – Method 1: Differential Equation

tt eAeAtv 82

21C 30

24060

24

23

3

10

8

53030 eevC 24060

3

23

3

20130 eevC

tt eAeAtv 82

21C 82

2402

601C 3030 eAeAv

24

23

24

1A,

3

10

3

2A 240

260

1 ee

2402

601C 8230 eAeAv

30830282C 24

1

3

2

24

23

3

1030 tttt eeeetv

30t

Page 55: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 – Method 2: Integrating Step Responses

att

0

t …

teetv tt

82

3

1

3

41

dtee

avt

t

tata

input

30

0

82

3

1

3

41

…………

The value at time point a

If a > 30 a

If a < 30

If a > 30Integrating from 0 to a

Integrating from 0 to 30

Page 56: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 – Method 2: Integrating Step Responses

30

0

82

3

1

3

41

t

t

tatainput dteeav

30

0

30

0

830

0

2

3

1

3

41

t

t

t

t

tat

t

ta dtedtedt

18

1

3

11

2

1

3

430 2408602 eeee aa

ttstate eetv 824

30

0

30

0

8830

0

22

3

1

3

41

t

t

t

t

tat

t

ta dteedteedt

30830282input 24

1

3

2

24

1

3

230 tttt eeeetv

Page 57: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 – Method 3: Differentiate the sources

30

300

0

30

0

s

t

t

t

V

ttv

30

300

0

0

1

0

s

t

t

t

tv

1

30

tvtv pulseinput

?tvinputResponse: tvpulseResponse:

Page 58: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 – Method 3: Differentiate the sources

30

300

0

0

1

0

s

t

t

t

tv

1

30

tvpulseResponse:

30t tt

pulse eetv 82

3

1

3

41

tvtv pulseinput

Aeettv ttinput 82

24

1

3

2

024

1

3

20 Avinput 8

5A

8

5

24

1

3

2 82 ttinput eettv

8

5

24

1

3

23030 24060 eevinput

Page 59: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Example 3 – Method 3: Differentiate the sources

30

300

0

0

1

0

s

t

t

t

tv

1

30

tvpulseResponse:

300 t tvtv pulseinput 2408602 1

3

11

3

4eeeetv tt

pulse

8

5

24

1

3

23030 24060 eevinput

Aeeeetv ttinput 2408602 1

24

11

3

2

............30 inputv 30A

308302

82input

24

1

3

224

1

3

230

tt

tt

ee

eetv

Page 60: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Announcement

• 11/12 ( 三 ) 第二次小考• Ch5. Dynamic Circuit (5.3)• Ch9. Transient response (9.1, 9.3, 9.4)

• 助教時間:週一到週五 PM6:30~7:30

Page 61: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Homework

• 9.58• 9.60

Page 62: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Homework

• Find v(t) for t>0 in the following circuit. Assume that v(0+)=4V and i(0+)=2A.

Page 63: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Homework

• Determine v(t) for t>0 in the following circuit

Page 64: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Thank You!

Page 65: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Homework

• 9.58

• 9.60

3.1624cos2512 7C tetv t

tt teeti 55L 2086

Page 66: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Homework

• Find v(t) for t>0 in the following circuit. Assume that v(0+)=4V and i(0+)=2A.

Page 67: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Homework

• Determine v(t) for t>0 in the following circuit

1675.075.6 364C tt eetv

Page 68: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Appendix

Page 69: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Higher order?

• All higher order circuits (3rd, 4th, etc) have the same types of responses as seen in 1st-order and 2nd-order circuits

Page 70: Lecture 14 Second-order Circuits (2) Hung-yi Lee

Acknowledgement

• 感謝不願具名的同學 • 指出投影片中 Equation 的錯誤

• 感謝 吳東運 (b02)• 指出投影片中 Equation 的錯誤

• 感謝 林裕洲 (b02)• 發現課程網站的投影片無法開啟