fourier analysis for gps

11
Fourier Analysis for GPS ASEN5190 P. Axelrad October 2003

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Fourier Analysis for GPS. ASEN5190 P. Axelrad October 2003. Periodic Functions. A periodic function of period Tp = 1/fp Can be expressed by a Fourier Trigonometric Series as:. Change of variable. Fourier Coefficients. Examples. a 0. a n. b n. Square Wave. Fourier Transform of a Pulse. - PowerPoint PPT Presentation

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Page 1: Fourier Analysis for GPS

Fourier Analysis for GPS

ASEN5190P. Axelrad

October 2003

Page 2: Fourier Analysis for GPS

Periodic Functions

• A periodic function of period Tp = 1/fp

• Can be expressed by a Fourier Trigonometric Series as:

pf t nT f t

01

cos 2 sin 2n p n pn

f t a a n f t b n f t

Page 3: Fourier Analysis for GPS

Change of variable

01

Let 2 ,

so for , 2

The function is then expressed as:

cos sin

p

p

n nn

x f t

t T x

f

f x a a nx b nx

Page 4: Fourier Analysis for GPS

Fourier Coefficients

01

2

1 cos

1 sin

n

n

a f x dx

a f x nx dx

b f x nx dx

Page 5: Fourier Analysis for GPS

Examples

2

1 1 1Constant ( ) cos 0 sin 02

1 1 1cos cos 0 cos 1 cos sin 02

1 1 1cos ( ) cos 0 cos cos 0 cos sin 02

sin

A Adx A A nx dx f x nx dx

nx nx dx nx dx nx nx dx

mx m n mx dx mx nx dx mx nx dx

n

21 1 1sin 0 sin cos 0 sin 12

x nx dx nx nx dx nx dx

a0 an bn

Page 6: Fourier Analysis for GPS

Square Wave

if - 0

if 0

A xf x

A x

0

00

0

0

0

0

1 2 3 4

1 13 5

1 1 02 2

1 1cos cos 0 for all

1 1 2sin sin 1 cos

4 4 , 0 , , 0 , .3

4so sin sin 3 sin 5 ...

n

n

a Adx Adx

a A nx dx A nx dx n

Ab A nx dx A nx dx nn

A Ab b b b etc

Af x x x x

x2

A

4

Page 7: Fourier Analysis for GPS

Fourier Transform of a Pulse

0

1 1

111

11

0 if 1

1 if 1

( ) ( ) cos ( )sin

( ) ( ) cos ( ) ( ) cos

sin 2sin 2( ) cos sinc

xf x

x

f x A x B x d

A f d B f d

A d

Page 8: Fourier Analysis for GPS

Sinc and Sinc2

-5 -4 -3 -2 -1 0 1 2 3 4 5-0.5

0

0.5

1

-5 -4 -3 -2 -1 0 1 2 3 4 50

0.2

0.4

0.6

0.8

1

Page 9: Fourier Analysis for GPS

Fourier series for a signal that is periodic in P

01

/ 21

0/ 2

/ 21/ 2

/ 2

/ 21/ 2

/ 2

cos 2 sin 2

cos 2

sin 2

n p n pn

P

PP

P

n pPP

P

n pPP

f t a a n f t b n f t

a f t dt

a f t n f t dt

b f t n f t dt

Page 10: Fourier Analysis for GPS

2T

2

/ 2 / 21 1

0/ 2 / 2

/ 2/ 2 / 21 1/ 2 / 2

/ 2 / 2 / 2

0 if NT=P f

A if

sin 2cos 2 cos 2

2 / 2

2 sin 2 sin / 2 sin/

T

PT

P T

P PP T

TP Tp

n p pP PpP T T

pn

tf t Nf

t

AT Aa f t dt AdtP N

A n f ta f t n f t dt A n f t dt

n f P

A n f T A n N Aan N n N N

c nN

x

A

T/2T/2 P=NT

Periodic rectangular pulse

Page 11: Fourier Analysis for GPS

Fourier representation of a periodic rectangular pulse

1

2 sinc cos 2 pn

A A nf t n f tN N N

-2.5 -2 -1.5 -1 -0.5 0 0.5 1 1.5 2 2.5

x 106

-5

0

5

10

15

20x 10

-4

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2

x 104

0

0.5

1

1.5

2x 10

-3

Zoomed in to show lines

Series for 1/T=1.023e6

and fp=1e3