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[PDF] The Finite Fourier Transforms

Sn sin(n?x/L) This transform should be used with Dirichlet boundary conditions that specify the value of u at x = 0 and x = L



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The finite Fourier sine transform of F (x)0 < x < l is defined as fs (p) = l ? 0 F (x)sin p?x l dx;p ? I Similarly the finite Fourier cosine 



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transform Fourier transform of derivatives convolution The function has finite number of discontinuities in Fourier Sine and Cosine transform



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When Kernel is sine or cosine or Bessel's function the transformation is called Fourier sine or which is called inverse finite Fourier sine transform



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A periodic function of time f(t) of period T can be represented by a Fourier transform F(n) = 1 T ZT/2 ?T/2 f(t)e?jn?0tdt f(t) = X? n=?? F(n)e+jn?0t where F(n) is the corresponding Fourier series where F(n) =1 2 (Cn? iSn) F(?n) =1 2 (Cn+ iSn) and F(0) = C0



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The Finite Fourier Transform and the Fast Fourier Transform Algorithm 1 Introduction: Fourier Series Early in the Nineteenth Century Fourier in studying sound and oscillatory motion conceived of the idea of representing periodic functions by their coefficients in an expansion as a sum of sines and cosines rather than their values

Page 1

SATHYABAMA UNIVERSITY UNIT III SMT1201 ENGINEERING MATHEMATICS III The infinite Fourier transform - Sine and Cosine transform - Properties - Inversion theorem - Convolution theorem - Parseval's identity - Finite Fourier sine and cosine transform.

FOURIER TRANSFORMS

Complex Fourier Transform (Infinite)

-LULv-wise continuous in each finite partial interval then the complex Fourier transform of f(x) is defined by

à L(:O; L5

Inverse Fourier Transform

B:T; L5

Properties of Fourier Transform

. Linear Property F{af(x) + bg(x)} = a F{f(x)} + b F{g(x)} where F is the Fourier transform

2. Shifting Theorem

If à

L(:O;PDAJà F=;=

LAÜaeÔ(:O;

3. Change of Scale property

à

L(:O;PDAJà L5

Ô(@ae

ÔASDANA=

Mr

4. Modulation Theorem

à

L(:O;PDAJà L5 6>(:O F=; E(:O E=;?

Convolution Theorem

The convolution of two functions f(x) and g(x) is defined as

B:T;ÛC:T;

Ls

¾tè

±B:P;C:T

FP;@P Fourier Transform Page 2SATHYABAMA UNIVERSITY UNIT III SMT1201 ENGINEERING MATHEMATICS III

Fourier Transform of Convolution of two functions

Fourier Transform of Convolution of f(x) and g(x) is the product of their Fourier

Transform

B:T;ÛC:T;

Infinite Fourier Cosine Transform

àÖ L §6 4

Inverse Fourier Cosine Transform

B:T; L §6 4

Infinite Fourier Sine Transform

àae L §6 4

Inverse Fourier Sine Transform

B:T; L §6 4

Properties of Fourier Sine and Cosine Transforms

1 Linear Property

àÖ<=B:T;

G>C:T;=

L=àÖ

G>àÖ

àae<=B:T;

G>C:T;=

L=àae

G>àae

Page 3

SATHYABAMA UNIVERSITY UNIT III SMT1201 ENGINEERING MATHEMATICS III

WOEsÀo[ Identity

ìB:T;

2 Modulation Property

5 Identities

If FC (s) and Gc(s) are the Fourier cosine transforms and Fs(s) and Gs(s) are the transforms of f(x) and g(x) respectively then i) ׬ ii) ׬ iii) ׬ 4׬ 4׬

4 Page 4SATHYABAMA UNIVERSITY UNIT III SMT1201 ENGINEERING MATHEMATICS III

Problem1Ift heFour iertransformoff xisF sthen,wha tisFouri ertr ansformof f ax?

Solution:

Fouriertransf ormoff xis

is1 2 xF sF fx fx edx f is1 2 xF fax fax edx f

Putt ax

dta dx is/ 1 2 t adtF fax ft ea f is/ 1 1.2 t af te dta f

1. .sF fax Fa a

Problem2Findthe Fouri ersinetransformof 3xe.

Solution:

0

2sinsF fx fx sxdx

3 3 0

2sinx x

sF ee sxdx 3 2 0

23sincos9

xesxs xs @2 22 2sinsi ncos9 ax axs ee bxdx abx bbx s ab Problem3Findthe Fourie rsinetransformofaxf xe ,0a. Hencededuce that 2 0 sin 1 2 x xdx ex

Solution:

0

2sinsF fx fx sxdx

0

2sinaxa x

sF ee sxdx 2 22s s a

Byi nverseSinetra nsform,we get

0

2sinsf xF ssx ds

2 2 0

2 2sinssx dss a

PROBLEMSPage 5SATHYABAMA UNIVERSITY UNIT III SMT1201 ENGINEERING MATHEMATICS III 2 2 0

2 sins sxf x dss a

2 2 0 sin 2 s sxf x dss a 2 2 0 sin 2 axs sxe dss a

Put1,ax

2 0 sin 2 1 s sxe dss

Replace 's' by 'x'

2 0 sin.1 2 s sxdx ex

Problem4Prove that1cos2C C CF f x ax F s a F s a.

Solution:

0

2cosc cF s F f x f x sx dx

0

2cos cos coscF f x ax f x ax sxdx

0 cos cos2 2 a s x a s xf x dx 0 0

1 2 1 2cos cos2 2f x s a xdx f x s a xdx

1.2c cF s a F s a

Problem5Find the Fourier cosine transform ofcos , 0 0, x x af xx a

Solution:

0 0

2 2cos cos cos

a cF f x f x sxdx x sxdx 0 cos 1 cos 12 2 as x s xdx 0 sin 1 sin 11 1 12 as x s x s s sin 1 sin 11 1 12 s a s a s s , provided1, 1.S S

Problem6Findax

CF xeandax

SF xe.

Solution:

ax c sdF xe F f xds ax ax c sdF xe F eds 0

2sinaxde sxdxds

Page 6SATHYABAMA UNIVERSITY UNIT III SMT1201 ENGINEERING MATHEMATICS III 2 2

22 22 2

2 2.d s a s

ds s as a ax ax s c s cd dF xe F e F xf x F f xds ds 0

2cosaxde sxdxds

22 22 2

2 2 2.d a as

ds s as a Problem7IfF sis the Fourier transform off x, then prove that the Fourier transform of axe f xisF s a.

Solution:

is1 2 xF s F f x f x e dx is1 2 iax iax xF e f x e f x e dx 1 2 i a s xe f x dx .F s a Problem8Find the Fourier cosine transform of23x xe e.

Solution:

Let23x xf x e e

0

2coscF f x f x sx dx

2 2 0 0

23 cos 3 cosx x x x

cF e e e sxdx e sxdx

2 22 2 3.4 1s s

Problem9State convolution theorem.

Solution:

If F(s) and G(s) are Fourier transform off xandg xrespectively, Then the Fourier transform of the convolutions ofandf x g xis the product of their Fourier transforms. i.e.*F f x g x F f x F g x Problem 10Derive the relation between Fourier transform and Laplace transform.

Solution:

Consider, 010 , 0

xte g t tf tt

The Fourier transform off xis given by

is1 2 tF f t f t e dt is1 2 xt te g t e dt Page 7SATHYABAMA UNIVERSITY UNIT III SMT1201 ENGINEERING MATHEMATICS III is1 2 x te g t dt 1 2 pte g t dt wherep xis 0 1 2 stL g t L f t e f t dt

Fourier transform of1

2f tLaplace transform of g(t) where g(t) is defined by (1).

Problem 11Find the Fourier sine transform of1

x.

Solution:

0

2sinsF f x f x sx dx

0

1 2 1sinsF sx dxx x

Letsxquotesdbs_dbs11.pdfusesText_17

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