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Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics and Telecommunications Level: MSc.

Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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Page 1: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

Technical University of Gdansk

Department of Radio Communications

Radio Communication Antennas

by

prof. Ryszard J. Katulski

Field of Study: Electronics and Telecommunications

Level: MSc.

Page 2: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

2

List of the Lecture Topics:

1. Antenna aspects in radio communication link

2. Principles of antenna choice in fixed and mobile link

3. Omnidirectional antennas

4. Sectorized antennas

5. Narrow beam antennas

6. Antenna technique for land mobile communications

7. Microstrip antenna technology

8. Properties of the microstrip antennas

9. Antenna technique for fixed satellite communications

10. Antenna equipment for mobile satellite terminal

11. Base theory of diversity receiving

12. Diversity antenna technique

13. Antenna technique for maritime communications

14. Smart antenna

15. Miniaturization of antenna equipment

Page 3: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

3

1. Antenna aspects in radio communication link – introduction

- Structure of the radio link (transmitter/receiver with wireless part)

- Fixed and mobile link antenna properties

- Omnidirectional and directional properties

- Network structure aspects

- Radio access cellular structure

- Fixed or mobile networks

- Base station and terminal equipment antennas properties

- Sectorized antenna properties

- Adaptive antenna in mobile link (smart conception)

Page 4: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

4

Structure of the radio link (transmitter and receiver with wireless part)

one-directional case

Tr

radiowave propagation medium

Transmitter Antenna

Gt [dB], gt

Receiver Antenna Re

Gr [dB], gr

wireless part of the radio link

Page 5: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

5

Structure of the radio link (transmitter and receiver with wireless part)

two-directional case

Tr/Re

radiowave propagation medium

Tr/Re Antenna

G [dB], g

Tr/Re Antenna

Tr/Rc

G [dB], g

wireless part of the radio link

Page 6: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

6

EMC aspect of antenna properties

- antenna interface:

- desired (main beam),

- undesired pattern (side and back pattern),

- omnidirectional (isotropic),

- sectorized,

- narrow-beam,

- adaptive pattern (smart antenna):

- dynamically adaptation of a Spatial Channel,

- reduction of an Interfernce Field,

- increase of a Network Capacity

Transmitter or Receiver

Radiowave Propagation

Medium

wire part

Antenna Interface

wireless part

Page 7: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

7

Fixed and mobile link antenna properties

- Omnidirectional or directional properties:

- Fixed: directional properties

- Mobile: omnidirectional properties (simple case)

TR/RE

x xTR/RE

x

1v

x

2v

TR/RETR/RE

2º Mobile:

1º Fixed:

Page 8: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

8

Network structure aspect

- multi-station point-to-point network structure:

- multi-station point-to-area cell structure – concept of a base station with terminals

(multi-users wireless access to telecommunication services):

x

TR/RE

x

x

x

TR/RE

TR/RE

TR/RE

TR/RETERMINAL

x

x

x

x

TR/RETERMINAL

xTR/RE

TERMINAL

TR/RETERMINAL

TR/REBASE STATION

Page 9: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

9

point-to-point network structure

- Radio-station antenna properties in fixed network

– directional:

- Radio-station antenna properties in mobile network

- omnidirectional:

x

TR/RE

x

x

x

TR/RE

TR/RE

TR/RE

4v

x

2v

TR/RE

TR/REx

3v

TR/RE

x

x

1v

TR/RE

Page 10: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

10

Cell structure with base station - fixed network case:

- Base radio-station antenna properties

– omni or directional (sector or narrow beamwidth)

- Terminal radio-station antenna properties

– directional (narrow beamwidth)

xx

TR/RETERMINAL

x

x

x

xTR/RE

TERMINAL

TR/RETERMINAL

TR/RETERMINAL

TR/RETERMINAL

TR/REBASE STATION

x

x

x

BASE STATION

x

Page 11: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

11

Cell structure with base station - mobile network case:

- Base radio-station antenna properties

– omnidirectional or sectorized or …?

- Terminal radio-station antenna properties

– omnidirectional (rather) or hemispherical

x

xv

x

v

x

v

x

v

1º) Omni-base

x

2º) Sectorized-base

xv

xv

x v

xv

Page 12: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

12

Adaptive antenna in mobile link (smart conception)

- interference problem (desired and undesired signals):

if for base station omnidirectional pattern

then for base station directional pattern

- antenna array with weight elements and adaptive processor should be applied

- basic conception on example of linear antenna array:

and

pAssp udbeamomni

2

'sec pp beamtor

2

2

K

mmm twtxty

1

min yre

W1

x1

W2

x2

x1·W1

S

x2·W2

Wk

xk

xk·Wk

1 2 k

Adaptive processor

y(t) r

e

Page 13: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

13

Adaptive antenna directivity properties analysis

- 1-D case (equation and scheme):

Km

mmmmmm

K

mmmmm

AAAA

practicein

wtWtwandAx

where

wtjtWAtF

......

:

argexp ,exp

:

argexp,

21

1

W1

x1

W2

x2

x1·W1

S

x2·W2

Wk

xk

xk·Wk

1 2 k

Adaptive processor

y(t) r

e

Page 14: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

14

Adaptive antenna directivity properties analysis

- 2-D case (equation and scheme):

NKnm

nmnmnmnmnmnm

N

n

K

mnmnmnmnm

AAAA

practicein

wtWtwandAx

where

wtjtWAtF

......

:

argexp ,,exp,

:

arg,exp,,

1211

1 1

1 K

2

N

2

Page 15: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

15

Adaptive antenna system

rxxxw

where

jxjwjrje

optimum

T

,,

:1

x

S

Processor Unit

{W}

{X}

y

e

r+

-

Page 16: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

16

Adaptive criterions

- SNIR (maximum of Signal-to-Noise-Interference Ratio):

- MSE (minimum of Mean Square Error):

- correlation method

Iundesired

desired

PP

Pmin

trtyERandtxtxERwhereRRW yrxxyrxx**1

N

ii

i

en

ewhere

eeEyre

1

22

1

min,min

Page 17: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

17

Adaptive procedure – two steps (scheme):

- DOA (Direction of Arrival)

- beamforming

(scheme)

Page 18: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

18

Simple illustration of the DOA (scheme)

Page 19: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

19

DOA algorithms (equations)

Page 20: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

20

Beamforming procedure

- amplitude or phase steering

- phase array

(scheme + equations)

Page 21: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

21

2. Principles of antenna choice in fixed and mobile link

- firstly, the antenna directivity properties should be taken into

account due to the shape and range of the radio system operation area,

- secondly, the antenna gain should be taken into account due to

the energetic bilans od the radio link,

- for fixed link, the antenna equipment with possible small value

of the beamwidth is best solution,

- for mobile link, its depends on the kind of a radio-station:

- for base station the sectorized antenna equipment is prefered,

- for user terminal the short microstrip antenna is prefered

Page 22: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

22

3. Omnidirectional antennas

- omnidirectional is not same as an isotropic property

(isotropic antenna is omnidirectional in each plane – theoretical model)

- omnidirectional antenna is practical case with non-directivity properties

in one plane only

- typical omnidirectional are bellow antennas:

- half-wavelenght dipole in H-plane

- linear antenna (wip antenna) in H-plane

Page 23: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

23

4. Sectorized antenna properties

Antenna array with beamwidth:

- in horizontal plane (depends on users traffic)

- in vertical plane

- with few degrees tillt (non everyone)

(typical pattern with catalog)

00 15 7 tofrom

000 60 90 ,120 or

Page 24: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

24

Sectorized antenna structure

- half-wavelenght dipole or rectangular microstrip radiator array

- vertical polarization (in a base version)

- feeder line

- coupling problem

Page 25: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

25

5. Narrow beam antennas

- narrow beam in each plane (in E-plane and H-plane in practical)

- reflector’s antennas (parabolic form)

- by use rectangular antenna array (high gain)

- in mobile link a main beam position should be steering

Page 26: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

26

6. Antenna technique for land mobile communications

- base radio-station antenna

- omnidirectional in wip form (one cell network with small

traffic)

- sectorized in array form (multi-cell network with big traffic)

- antennas for space and polarization diversity

- terminal antenna

- omnidirectional in wip form

- hemispherical in short microstrip radiator form

Page 27: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

27

7. Microstrip antenna technology

- view of a microstrip radiator:

- main properties of one radiating element:

- integrated and simple construction

- easy technological process

- high energetic effectivness

- small directivity properties

- in wireless systems the radiating element array should be

applied

Page 28: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

28

Microstrip antenna technology – geometry of a microstrip line

ZCT Y G jBS S S

c)

rH

b)

x

z

apertura

l

W m

d)

W m

a)

x

y

Page 29: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

29

Microstrip antenna technology – slot admitance

- slot conductance

- slot susceptance

- slot admitance

where: and

moreover: and

SSS jBGY ˆ

mSS WgG

mSS WbB

mSSmSS WjbgWyY ˆˆ

241

2Hk

Zg

CTdS

CTd

S Z

Hkb

lg2135,3

re

d

0mre

CT W

HZZ

0

Page 30: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

30

Microstrip antenna technology – slot radiation conductance

- slot admitance

- in practice

- in result

conclusion:

to obtain antenna phenomena

with good value of the radiation conductance,

the width of a microstrip line should be greater

radG

surfradS GGG

surfrad GG

mCTd

mSradS WZ

WgGG

Page 31: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

31

Microstrip antenna technology – field distribution in a slot

H

x

z

l

Er

A B

CD

E z

Ea

Page 32: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

32

Microstrip antenna technology

– geometry of a rectangular microstrip radiator

(usefull practical form of the antenna)

L ef+l

E nE r

E tE nE r

E t

F W

L

+ = E t E t+

a)y

x

b)

H

ll

c)

d)

L ef

LL

Page 33: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

33

Design procedure of the microstrip rectangular radiator:

- choice of a dielectric layer

- radiator width

- radiator lenght

where:

and

WandL

LL d 2

dW

813,0258,0

262,03,0

412,0

L

WL

W

HL

re

re

2

1

1212

1

2

1

W

Hrrre

Handr

Page 34: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

34

Microstrip antenna technology – feeding techniques

b)

c)

a) Linia zasilająca

Promiennik

Linia zasilająca

Page 35: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

35

8. Electrical properties of the microstrip antennas

– main analysis techniques

- modelling techniques of the microstrip rectangular radiator

- transmission or cavity equivalence

(schemes of the microstrip lines and cavity without descriptions)

Page 36: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

36

Transmission model of the microstrip rectangular radiator

Y sY s

Z we

L ef

b)

L+ l

F W

L

Z CP

a)

c)

y

x

l l

W ef

LL

Page 37: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

37

Transmission model of the microstrip rectangular radiator

- Electrical (directivity) properties of the antenna

Radiation pattern:

plane z-in x sin2

cos

2

sin2

sinsin

0

0

0

effE

Lk

Hk

Hk

F

plane z-yin cos

2

sin

2

sinsin

0

0

eff

eff

H Wk

Wk

Fz

y

x

L

W

r

P (,,r)

Page 38: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

38

Transmission model of the microstrip rectangular radiator

- Electrical (admitance) properties of the antenna

Resonant input admitance:

deffd

eff

deffdd

eff

deffd

eff

rad

WW

WW

WW

G

2for 120

235,0for 60

1

120

35,0for 90

2

2

2

2

2

Page 39: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

39

Transmission model of the microstrip rectangular radiator

- Electrical (impedance) properties of the antenna

Input impedance vs. frequency:

where:

Resonant frequency:

where:

1

resCP

resin f

ftgjY

ZfZ

W

HZ

YZ

reCPCP

01

effres L

cf

1

2

LLLandsmc eff 2 /103 8

Page 40: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

40

Cavity model of the microstrip rectangular radiator – general description

z

y

x

H

a)

L ef

W ef

Fy 0

x 0

C G

C 10G 10L 10

C mnL mn G mn

TM mn

TM 10

C 10G 10L 10

TM 10

L T

b) c)

y

x

W ef

L ef

l

l

lA 2

A 4

A 3

A 1l

d)

0 0

,),(m n

mnmnz yxAyxE

H

VA mn

mn

effeffmn W

ym

L

xm coscos

00

r

mnmn

k

2

122

effeffmn W

n

L

mk

Page 41: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

41

Cavity model of the microstrip rectangular radiator

- resonant impedance properties for base mode:

where:

LTresin jXRfZ 10

cudirad GGGGR

11

1010

cudirad GGG

% 100

1

in

rad

R

G

Page 42: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

42

Transmission and cavity model of the radiator - comparison

- Radiation pattern in E-plane (x-z plane)

-16

-12

200-20

6040 80

-8

f = 1,6 GHzr = 2,1h = 1,5 mm

-4

0

modeltransmisyjny

pomiar

modelwnękowy

F( )[dB]

z

y

x

L

W

r

P (,,r)

Page 43: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

43

Transmission and cavity model of the radiator - comparison

- Radiation pattern in H-plane (y-z plane)

-16

-12

200-20

6040 80

-8

f = 1,6 GHzr = 2,1h = 1,5 mm

-4

0

modeltransmisyjny

pomiar

modelwnękowy

F()[dB]

z

y

x

L

W

r

P (,,r)

Page 44: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

44

Polarization techniques of the microstrip antenna

- by special radiator feeding

- quasi-kwadrature shape of the radiator:

x

y

L

W

H r

05,1029,1 W

L

Page 45: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

45

Polarization techniques of the microstrip antenna

- by use of the four radiator array

(schemes and desription)

Page 46: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

46

Microstrip radiator – stacked technology

- to increase frequency band due to radio systems application requirements

- especially for modern wide band radio systems

x

y

L

W

H

H

r

r

Page 47: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

47

Hemispherical antenna in short microstrip radiator form

(figure)

Page 48: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

48

Microstrip rectangular array

(scheme)

Page 49: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

49

9. Antenna technique for fixed satellite communications

- for Earth Station application

- high gain with narrow beam of directional properties

- parabolic reflector antennas

- radiation source constructions (polarization aspect)

- linear polarization can be applied but circular is better

- horn antennas (open waveguide) with linear or circular

polarization

- half wavelenght dipole with linear polarization

- crossed dipoles with circular polarization

- for Space Station application

- high gain with narrow beam by use dipole or slot antenna arrra

- or multi-beam antenna array

Page 50: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

50

parabolic reflector antenna construction

- with clasical reflector

Page 51: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

51

parabolic reflector antenna construction

- with offset reflector

Page 52: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

52

parabolic reflector antenna construction

- with dual reflector (Cassegraine Antenna)

Page 53: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

53

Horn antennas (open waveguide)

- a polarization of e-m field in waveguide decides about type of the horn

antenna polarization

Page 54: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

54

Crossed dipoles with circular polarization

- analytical description of the dipoles:

- to obtain circular polarization:

- to obtain required value of the input impedance:

d y

lx d x

ly

Y1Y2

a) b)

2222111121 ˆ ˆ jBGeYYandjBGeYY jj

2 2121

andYY

)50( 21 GG21

1

GGZ in

Page 55: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

55

Antennas for Space Station application

- one- or multi-beam antenna array

Page 56: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

56

10. Antenna equipment for mobile satellite terminal

- satellite antenna techniques for vehicles (on land and sea) with

optional directivity properties depend on kind of

telecommunications services (transmission rate in kbits/s):

- rectangular microstrip radiator and array

- short backfire and helical antenna constructions

- circular polarization should be applied

- crossed dipoles

- antenna equipment for personal satellite terminal

- microstrip radiator with hemispherical pattern

Page 57: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

57

Satellite antenna equipment for vehicles

- relative wide beam should be applied due to permanent change

of antenna position (orientation to satellite)

- optional directivity properties:

- best option with high gain equals more than 20 dB (full

service)

- medium option with gain from 10 to 20 dB (limited service)

- simple option with gain equals few dB (small transmission

rate)

- kind of service:

- full (high transmission rate with the few Mb/s)

- medium (transmission rate with the few kb/s)

- simple (transmission rate is smaller than kb/s)

Page 58: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

58

Idea of the backfire antenna construction

- big and small reflectors with radiation source

x

z

y

D

M

Page 59: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

59

Schemes of the short backfire antenna practical construction

S

S

B

F

B

R

Z

S

a)

b)

,......2,1 ,35,0max nnDB

,......2,1 ,75,0min nnDB

5,0sD

25,021 FF ll

1rl

Page 60: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

60

Short backfire antenna properties – radiation patterns

- one source antenna

- four array

0

-10

dB

-20

-30

0° 30° 60° 120°90° 150° 180°

Modelowanie

Pomiar

F

0

-10

dB

-20

-30

0° 30° 60° 120°90° 150° 180°

Modelowanie

Pomiar

F

Page 61: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

61

Helical antenna constructions

- axis radiation in satellite link application

with circular polarization

- orthogonal to axis radiation -

with linear polarization

(wip antenna eqivalence) in land mobile terminal

- scannig axis in radio-monitoring

- for axis radiation:

and

D

l

S

DCwhere

CS

2,17,0 3,015,0 1412 00

mm l 3

4

4

3

)( Dl

Page 62: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

62

Helical antenna analysis

- radiation properties (pattern for axis radiation):

- radiation properties (polarization)

from axis to ortogonal radiation :

- impednace properties for axis polarization:

cos

2sin

2sin

0 SkwhereN

N

F

)0( 0 )90( 0 cosp

RkZ in 140

y

z

x

P (,,r)

r

R

Page 63: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

63

Reflectors for helical antenna

with

with

D s

Ekran

00 1401102 8,0 mSD

mD 4,0

Page 64: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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Helical antenna properties

Page 65: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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11. Base theory of diversity receiving

Page 66: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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12. Diversity antenna technique

- antenna for space diversity

Page 67: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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antennas for polarization diversity

- with two orthogonal linear polarizations

- +/- 45 degrees

- 0/180 degrees (horizontal/vertical polarizations)

Page 68: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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13. Antenna technique for maritime communications

- wip and mast antenna

a) current distribution

b) radiation pattern

c) omidirectional in horizontal plane

a

b

Page 69: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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analysis method of the wip and mast antenna – thin-wire model

where:

method of moments procedure is applies to determination of the current

distribution as parameter to calculate of radiation pattern with input impedance

and coupling problem analysis of a ship antenna array

l

z

d

x

y

e

l

zEjdzzzGzIkz

4, '''22

2

'

''

,

,exp,

zzR

zzjkRzzG

Page 70: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

70

Antenna technique for maritime communications

- link antennaa) b)

lVlV

hV

lV

hV

h h

lHlH

lZ

lV

Page 71: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

71

Satellite antenna equipment for ship application

- changes of the ship position

- relative wide beam should be applied due to permanent change of antenna

position (orientation to satellite)

- optional directivity properties:

- best option (A standard) with high gain equals more than 20 dB (full

telecommunication service)

- medium option (B standard) with gain from 10 to 20 dB (limited service)

- simple option (C standard) with gain equals few dB (small transmission rate)

- kind of service:

- full (high transmission rate with the few Mb/s)

- medium (transmission rate with the few kb/s)

- simple (transmission rate is smaller than kb/s)

Page 72: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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Antenna technique for underwater communications

- link antenna a)

b)

c)

Page 73: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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14. Smart antenna

Page 74: Technical University of Gdansk Department of Radio Communications Radio Communication Antennas by prof. Ryszard J. Katulski Field of Study: Electronics

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15. Miniaturization of antenna equipment