12.1 the dirichlet conditions:

13
12.1 The Dirichlet conditions: Chapter 12 Fourier series Advantages: (1)describes functions that are not everywhere continuous and/or differentiable. (2)represent the response of a system to a period input and depend on the frequency of the input (3)using in string vibration, light scattering, input signal transmission in electronic circuit (1) The function must be periodic. (2) It must be single-valued and continuous, except possibly at a finite number of finite discontinuities. (3) It must have only a finite number of maxima and minima within one period. (4) The integral over one period of a function must converge.

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Chapter 12 Fourier series. Advantages: describes functions that are not everywhere continuous and/or differentiable. represent the response of a system to a period input and depend on the frequency of the input - PowerPoint PPT Presentation

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Page 1: 12.1 The Dirichlet conditions:

12.1 The Dirichlet conditions:

Chapter 12 Fourier series

Advantages:(1) describes functions that are not everywhere continuous

and/or differentiable.(2) represent the response of a system to a period input and

depend on the frequency of the input (3) using in string vibration, light scattering, input signal

transmission in electronic circuit

(1) The function must be periodic.

(2) It must be single-valued and continuous, except possibly at a finite number of finite discontinuities.

(3) It must have only a finite number of maxima and minima within one period.

(4) The integral over one period of a function must converge.

Page 2: 12.1 The Dirichlet conditions:

all functions may be written as the sum of an odd and an even part

Chapter 12 Fourier series

:)(

:)(

)()()]()([2

1)]()([

2

1)(

xf

xf

xfxfxfxfxfxfxf

odd

even

oddeven

chosen as the sum of a cosine series

chosen as the sum of a sine series orthogonal properties:

the length of a period is L: )/)(2cos()/2cos(

)/)(2sin()/2sin(

00

00

LLxrLrx

LLxrLrx

pr

prL

prdxL

px

L

rx

pr

prL

prLdxL

px

L

rx

prdxL

px

L

rx

Lx

x

Lx

x

Lx

x

for 0

0for 2/

0for 0)2

sin()2

sin(

for 0

0for 2/

0for )2

cos()2

cos(

and allfor 0)2

cos()2

sin(

0

0

0

0

0

0

Page 3: 12.1 The Dirichlet conditions:

Fourier series expansion of the function f(x) is

Chapter 12 Fourier series

0for )2

sin()(2

0for )2

cos()(2

obtain to )2

sin()( and )2

cos()( using Similarly,

)(2

2)]}

2cos()

)(2[cos(

)]2

sin())(2

[sin({2

2

)]2

sin()2

cos([2

)(

properties orthogonal by obtained ts,coefficienFourier called are , ,

)]2

sin()2

cos([2

)(

0

0

0

0

0

0

0

0

0

0

0

0

0

0

0

0

x

x

0

000

00

10

1

0

0

1

0

rdxL

rxxf

Lb

rdxL

rxxf

La

dxL

rxxfdx

L

rxxf

dxxfL

a

aL

L

rx

L

Lxrb

L

rxx

L

Lxra

L

ra

L

dxL

rxb

L

rxadx

adxxf

baa

L

rxb

L

rxa

axf

Lx

xr

Lx

xr

Lx

x

L

Lx

x

r

rr

rr

Lx

x r

Lx

x

Lx

x

rr

rr

r

Page 4: 12.1 The Dirichlet conditions:

Ex: Express the square-wave function as a Fourier series

Chapter 12 Fourier series

2/0for 1

02/for 1)(

Tt

tTtf

f(t) is an odd function, so only the sine term survives

T

ttttf

r

rrr

rr

T

rt

r

T

Tdt

T

rt

T

dtT

rttf

Tb

r

TT

T

Tr

2for ........)

5

5sin

3

3sin(sin

4)(

even for 0

odd for 4

])1(1[2

)1(cos2

|)2

cos()2

(4

)2

sin(4

)2

sin()(2

2/0

2/

0

2/

2/

Page 5: 12.1 The Dirichlet conditions:

(1) At a point of finite discontinuity, , the Fourier series converges to

(2) At a discontinuity, the Fourier series representation of the function will overshoot

its value. It never disappears even in the limit of an infinite number of terms.

This behavior is known as Gibb’s phenomenon.

Chapter 12 Fourier series

dx

)]()([lim2

10

dd xfxf

1 term 2 terms

3 terms

20 terms

overshooting

12.4 Discontinuous functions

Page 6: 12.1 The Dirichlet conditions:

Chapter 12 Fourier series

12.5 Non-periodic functions:

period=L, no particular symmetry

period=2L, antisymmetry; odd fun

period=2L, symmetry; even fun

Page 7: 12.1 The Dirichlet conditions:

Ex. : Find the Fourier series of 20 ,)( 2 x xxf

46

16

3

4116

3

42

20for )2

cos()1(

163

4

3

8

4

20

1for )1(16

cos16

)2

cos(8

|)2

cos(8

)2

sin(4

|)2

sin(2

)2

cos()4

2cos(

4

2

0 ,22 ,4L period function even an is )(

),()4( and )()(

2

21

222

122

2

2

0

22

2

20

2222

2

0222022

2

0

20

2

2

0

22

2

2

r

r

r

r

r

r

rxx

xrx

rx

dxxdxxar

rr

rr

dxrx

r

rxx

r

dxrx

xr

rxxr

dxrx

xdxrx

xa

bxxf

Ikxfkxfxfxf

Chapter 12 Fourier series

(1) make the function periodic and symmetric

Page 8: 12.1 The Dirichlet conditions:

(2) make the function periodic and antisymmetric

Chapter 12 Fourier series

4not zero to converges seriesFourier the 2at

)2

sin()]1)1(()(

2)1(

1[8

)1)1(()(

16)1(

8|)

2cos()

2(

8)1(

8

])2

sin(2

|)2

sin(2

[4

)1(8

)2

cos(22

|)2

cos(2

)2

sin(

))(2

sin())((2

1)

2sin(

2

1

)4

2sin()(

4

2)

4

2sin(

4

2

0 ,4 ;)()4( and )()(

31

2

32022

2

0

20

2

0

20

22

0

2

0

2

22

0

2

0

2

22

0

2

x

rx

rrx

rr

rx

rrr

dxrx

r

rxxrrr

dxrx

xr

rxx

rdx

rxx

dxrx

xdxrx

x

dxrx

xdxrx

xb

aLxfxfxfxf

rr

r

rrr

r

r

r

Page 9: 12.1 The Dirichlet conditions:

Integration and differentiation (1) The Fourier series of f(x) is integrated term by term then the resulting Fourier series converges to the integral of f(x). (2) f(x) is a continuous function of x and is periodic then the Fourier series that results from differentiating term by term converges to f(x).

)2()2

sin()1(

323

4)

2sin()

1(

)1(32

3

4

3 133

122

3

Crx

rxC

rx

rrx

x

r

r

r

r

Chapter 12 Fourier series

Ex: Find the Fourier series of 20 ,)( 3 x xxf

Sol: from the previous example

integrate (1) term by term

)1()2

cos()1(

163

4

122

2

rx

rx

r

r

integrate (1) term by term

put (3) into (2)

)3()2

sin()1(

821

rx

rx

r

r

00)0(for

)2

sin()1(

96)2

sin()1(

161

331

3

Cf

Crx

r

rx

rx

r

r

r

r

Page 10: 12.1 The Dirichlet conditions:

12.7 Complex Fourier series

rxirxirx sincos)exp(

* ,)(2

1 ,)(

2

1

is and to relations the has

for 0

for )2

exp()2

exp(

:ityorthogonal the using

)2

exp()(1

)2

exp()(

0

0

0

0

rrrrrrrr

rrr

Lx

x

Lx

xrr

r

ccibacibac

bac

pr

prLdxL

irx

L

irx

dxL

irxxf

Lc

L

irxcxf

Complex Fourier series expansion is:

Chapter 12 Fourier series

Page 11: 12.1 The Dirichlet conditions:

Chapter 12 Fourier series

Ex: Find a complex Fourier series for in the range xxf )( 22 x

)2

exp()1(2

)1(2

sin2

cos2

|)2

exp(1

)]exp()[exp(1

)2

exp(2

1|)

2exp(

2)

2exp(

4

1

0 (2)

04

1

0 (1)

,0

22

2222

2

2

22

2

2

2

20

irx

r

ix

r

ir

r

ir

r

i

irx

ririr

irx

dxirx

ir

irx

ir

xdx

irxxc

r

xdxc

r

rr

r

r

r

Page 12: 12.1 The Dirichlet conditions:

general proof:

Chapter 12 Fourier series

12.8 Parseval’s theorem:

)(2

1)

2

1(|||)(|

1 2

1

220

220

0r

rr

rr

Lx

xbaacdxxf

L

22

**

**

**

|||)(|1

)()(set we if

])2

exp()(1

[

)2

exp()()()(1

)2

exp()()()(

)2

exp()( ),2

exp()(

0

0

0

0

0

0

0

0

rr

Lx

x

rr

r

Lx

xr

r

Lx

xr

rLx

x

rr

rr

rr

cdxxfL

xfxg

cdxL

irxxg

Lc

dxL

irxxg

L

cdxxgxf

L

L

irxxgcxgxf

L

irxxg

L

irxcxf

Page 13: 12.1 The Dirichlet conditions:

Ex: Using Parseval’s theorem and the Fourier series for

evaluate the sum

Chapter 12 Fourier series

22 ,)( 2 x-xxf

1

4

r

r

90256)

9

16

5

16(

1

5

1616

2

1)

3

4()(

2

1)

2

1(

)2

cos()1(

163

4 using and

5

16

4

1

44

14

144

222

1

220

122

22

2

4

r

rr

rr

r

r

r

rbaa

rx

rxdxx