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SATELLITE LINK DESIGN SATELLITE LINK DESIGN

SATELLITE LINK DESIGN - PowerPoint Presentation

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SATELLITE LINK DESIGN - PPT Presentation

By SSadhish Prabhu INTRODUCTION Cost to build and launch a GEO satellite is about 25000 dollars per kg Weight is the most critical factor in any design Dimension of the satellite dia ID: 555862

antenna power satellite gain power antenna gain satellite direction eirp isotropic density flux area distance transmission received receiving ratio

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Slide1

SATELLITE LINK DESIGN

By

S.Sadhish

Prabhu

Slide2

INTRODUCTION

Cost to build and launch a GEO satellite is about 25,000 dollars per kg

Weight is the most critical factor in any design

Dimension of the satellite :

dia

must be less than 3.5m

Antennas are the limiting factor Slide3

Factors influencing system design

Weight of the satellite is driven by two factors

The number and the output power of he transponder on the satellite (requires large power from solar cells which in turn increases the weight )

Weight of the station keeping fuelSlide4

Factors influencing system design

The choice of frequency band

Atmospheric propagation effects

Multiple access techniques Slide5

Performance objective

Bit error rate (BER) in a digital link

Signal-to-noise ratio (S/N) in an analog link

BER or S/N is determined by Carrier - to- noise ration (C/N) at the input of the demodulator in the receiver

C/N > 6 dB

Measured in base band channel Slide6

Basic transmission theory

Objective :

Calculation of the power received by an earth station from satellite transmitter

Two approaches for calculating :

Use of flux density

Link equation (

Friis

transmission equation

)Slide7

Isotropic Radiator

Consider an Isotropic Source radiating Pt Watts uniformly into free space.

At distance R, the area of the spherical shell with center at the source is

4

p

R

2

Flux density at distance R is given by

W/m

2

Equ

4.1Slide8

Isotropic Radiator

W/m

2

Pt

Watts

Distance R

Isotropic Source

Power Flux Density:

Surface Area of sphere =

4

p

R

2

encloses

Pt.Slide9

Antenna Gain

We need directive antennas to get power to go in wanted direction.

Defined as the ratio of power per unit solid angle radiated in a direction to the average power radiated per unit solid angle

P(

) is variation of power with angle.

G(

) is gain at the direction .

P

0

is total power transmitted.

sphere =

4

p

solid radians

(

Eqn

4.2)Slide10

Antenna GainAntenna has gain in every direction!

Usually “Gain” denotes the

maximum

gain of the antenna.

The direction of maximum gain is called “

boresight

”.

Gain is a ratio:

It is usually expressed in

Decibels

(dB) G [dB] = 10 log10 (G ratio)Slide11

Flux density The flux density in the direction of the antenna

boresight

at distance R meter is

W/m

2Slide12

EIRP (Pt*Gt)

An isotropic radiator is an antenna which radiates in all directions equally

Antenna gain is relative to this standard

Antennas are fundamentally passive

No additional power is generated

Gain is realized by focusing power

Similar to the difference between a lantern and a flashlight

Effective Isotropic Radiated Power (EIRP) is the amount of power the transmitter would have to produce if it was radiating to all directions equally

Note that EIRP may vary as a function of direction because of changes in the antenna gain vs. angleSlide13

EIRP

Receiver

Received

power P

t

Incident flux disunity, F

Pt

Watts

Isotropic Source

Receiving antenna area , A gain G

t

R

For an ideal receiving antenna with an aperture area of Am

2

,

P

r

= FASlide14

EIRPA antenna with physical aperture area of A

r

m

2

will not deliver the power

Thus the efficiency is reduced

It is descried by using effective aperture

A

e

A

e = ηAr

(4.5)

Where

η

– aperture efficiency of the antenna

Thus (4.6)

2

P

r

=

Slide15

Fundamental of antenna theory

2

(4.7)

Sub

A

e

in (4.6)

2

This expression is called as the

Friis

transmission equation Slide16

Contd..

In decibel term

Where,

EIRP = 10 log

10

(

P

t

G

t

)

dBW

Gr

= 10 log

10

dB

Lp

– path loss = 20 log

10

dB

2

(4.10)

(4.9)Slide17

In general Pr =

EIRP+G

r

-

L

p

-L

a

-

L

ta-Lra dBW (4.11)

Where

L

a

= attenuation in atmosphere

L

ta

= losses associated with transmitting antenna

L

ra

= losses associated with receiving antenna Slide18

Reference of dBSlide19

Problem # 1 A satellite at a distance of 40,000km from a point on the earth’s surface radiates a power of 10W from an antenna with a gain of 17 dB in the direction of the observer, find the flux density at the receiving point, and the power received by an antenna at this point with an effective area 10m

2Slide20

Problem # 2A satellite operates at a frequency of 11 GHz. The receiving antenna has a gain of 52.3 dB, Find the received power. Slide21

Answer -126dbW

for both

questio

Note:

The received power is commonly called as carrier

power,

C

Because,

Satellites use FM (

Anlog transmission )or PM (digital transmission)In both modulation the carrier is not changed So,

C=P

rSlide22