prof. girish kumar - gwcet

17
Prof. Girish Kumar Electrical Engineering Department, IIT Bombay [email protected] (022) 2576 7436 Antenna Arrays

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Page 1: Prof. Girish Kumar - GWCET

Prof. Girish KumarElectrical Engineering Department, IIT Bombay

[email protected]

(022) 2576 7436

Antenna Arrays

Page 2: Prof. Girish Kumar - GWCET

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

Page 3: Prof. Girish Kumar - GWCET

1 2j r j ro oE E e E e

2k

cos cos2 2

2 2

d dj j

j ro

j jj r

o

E E e e e

E e e e

2 cos 2 cos cos2

o o

dE E E

2cos cos

2 = dsin sin

dd

d

/ 2d1 2

d

cos2

d

r

1r

2r

P

Array of Two Isotropic Point Sources

1

2

cos2

, 90

cos2

dr r

r dd

r r

>>

Page 4: Prof. Girish Kumar - GWCET

Two Isotropic Point Sources of Same Amplitude and Phase

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

ф 0° 90° 60°

E 0 1

Page 5: Prof. Girish Kumar - GWCET

ORIGIN AT ELEMENT 1

Page 6: Prof. Girish Kumar - GWCET

Two Isotropic Point Sources of Same Amplitude and Opposite Phase

HPBW = 120°

ф 0° 90° 60°

E 0 1

HPBWs = 120° in both orthogonal planes

Page 7: Prof. Girish Kumar - GWCET

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

ф 0° 60° 90° 120° 180°

E 0 1

Page 8: Prof. Girish Kumar - GWCET

Two Isotropic Point Sources of Same Amplitude with 900 Phase Difference at λ/4

HPBW = 180°

Spacing between the sources is reduced to λ/4

ф 0° 90° 120° 150° 180°

E 0 0.924 0.994 1

Page 9: Prof. Girish Kumar - GWCET

Two Isotropic Point Sources Of Same Amplitude withAny Phase Difference

Page 10: Prof. Girish Kumar - GWCET

Dipole AF

Two Same Dipoles and Pattern Multiplication

Dipole Pattern:

Final Pattern

For δ = 0, Array Factor (AF)

will give max. radiation in

Broadside Direction

Page 11: Prof. Girish Kumar - GWCET

PATTERN MULTIPLICATION

Array of two dipole

antennas

Dipole Pattern AF Product of Patterns

Dipole E-Field for Vertical Orientation:

Combined E-Field

Page 12: Prof. Girish Kumar - GWCET

N Isotropic Point Sources of Equal Amplitude and Spacing

where

Enorm

Page 13: Prof. Girish Kumar - GWCET

Radiation Pattern of N Isotropic Elements Array

Radiation Pattern for array of n isotropic radiators of equal

amplitude and spacing.

First SLL

= 20log0.22

= -13.15dB

Arr

ay F

act

or

Page 14: Prof. Girish Kumar - GWCET

Broadside Array (Sources In Phase)

Field pattern of 4 isotropic point sources with the

same amplitude and phase and spacing of /2.

ф Ψ E

0° π 0

90° π/2 0

120° 0 1

Page 15: Prof. Girish Kumar - GWCET

Ordinary Endfire Array

Field pattern of ordinary end-fire array of 4

isotropic point sources of same amplitude.

Spacing is /2 and the phase angle = -.

BWFN=120°

Page 16: Prof. Girish Kumar - GWCET

Increased Directivity Endfire Array (IDEA)

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).

Hansen and Woodyard criteria

Parameter Ordinary end

fire array

Endfire array with

increased Directivity

HPBW 69° 38°

FNBW 106° 74°

Directivity 11 19

Page 17: Prof. Girish Kumar - GWCET

Array with Maximum Field in any Arbitrary Direction

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

For Beam Maxima at ϕ = 60°