Antenna Arrays - nptel

7 downloads 0 Views 974KB Size Report
d. 1. 2 d cos. 2 d. ϕ θ θ r. 1 r. 2 r. P. Array of Two Isotropic Point Sources. 1. 2 cos ... Point Sources of Same Amplitude and Opposite Phase. HPBW = 120° ф. 0°.
Antenna Arrays

Prof. Girish Kumar Electrical Engineering Department, IIT Bombay

[email protected] (022) 2576 7436

Linear and Planar Arrays Arrays of Two Isotropic Sources Principles of Pattern Multiplication Linear Array of N Elements with Uniform Amplitude  Broadside

 Ordinary Endfire  Increased Directivity Endfire Array (IDEA)  Scanning Array

Linear Arrays with Non-Uniform Amplitude Planar Arrays

Array of Two Isotropic Point Sources E  Eoe j  r1  Eoe j  r2

 k 

d  cos   2  r >> d ,   90   d r2  r  cos    2 

2

P



r1  r 

E  Eo e  j  r  Eo e

 j r

d   j  d cos  j  cos   2 e 2 e     

   j j e 2  e 2  

   

  d  E  2 Eo cos    2 Eo cos  cos    2   

r2 d cos  2

r



r1

 1

d /2

d

   d cos   = dsin 

2 d



2 d



cos 

sin 

2

Two Isotropic Point Sources of Same Amplitude and Phase

ф



90°

E

0

1

60°

HPBWs = 60° in one plane and 360° in another plane

ORIGIN AT ELEMENT 1

Two Isotropic Point Sources of Same Amplitude and Opposite Phase

HPBW = 120° ф



90°

E

0

1

60°

HPBWs = 120° in both orthogonal planes

Two Isotropic Point Sources of Same Amplitude with 900 Phase Difference at λ/2

ф E



60° 0

90°

120° 1

180°

Two Isotropic Point Sources of Same Amplitude with 900 Phase Difference at λ/4 Spacing between the sources is reduced to λ/4

HPBW = 180°

ф



E

0

90°

120°

150°

0.924 0.994

180° 1

Two Isotropic Point Sources Of Same Amplitude with Any Phase Difference

Two Same Dipoles and Pattern Multiplication Dipole Pattern:

For δ = 0, Array Factor (AF) will give max. radiation in Broadside Direction Dipole

AF

Final Pattern

PATTERN MULTIPLICATION Dipole E-Field for Vertical Orientation:

Combined E-Field

Array of two dipole antennas

Dipole Pattern

AF

Product of Patterns

N Isotropic Point Sources of Equal Amplitude and Spacing

where

Enorm

Array Factor

Radiation Pattern of N Isotropic Elements Array

First SLL = 20log0.22 = -13.15dB

Radiation Pattern for array of n isotropic radiators of equal amplitude and spacing.

Broadside Array (Sources In Phase)

ф 0° 90° 120°

Ψ π π/2 0

E 0 0 1 Field pattern of 4 isotropic point sources with the same amplitude and phase and spacing of /2.

Ordinary Endfire Array

BWFN=120°

Field pattern of ordinary end-fire array of 4 isotropic point sources of same amplitude. Spacing is /2 and the phase angle  = -.

Increased Directivity Endfire Array (IDEA)

Hansen and Woodyard criteria

Parameter

Ordinary end fire array

Endfire array with increased Directivity

HPBW

69°

38°

FNBW

106°

74°

Directivity

11

19

Field patterns of end-fire arrays of 10 isotropic point sources of equal amplitude spaced /4 apart. (a) Phase for increased directivity ( = -0.6), (b) Phase of an ordinary end-fire array ( = -0.5).

Array with Maximum Field in any Arbitrary Direction For Beam Maxima at ϕ = 60°

Field pattern of array of 4 isotropic point sources of equal amplitude with phase adjusted to give the maximum at ф = 60° for spacing d = λ/2