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Radiation Pattern
Abdullah Al Mehedi
ID- 150105
Section- A
1
Radiation Pattern
◦ Beamwidth
◦ Pattern Solid Angle
◦ Directivity
◦ Efficiency
◦ Gain
Radiation pattern
Directional Radiation
2
Beamwidth
Antenna Beam width is the angle between
the half-power of an antenna pattern or
beam over which the relative power is at or
above 50% of the peak power.
 Known as half-power.
Beamwidth = 70λ / D
where,
λ = Wavelength
D = Diameter
3
Beamwidth
3D Radiation Pattern.
Polar Radiation Pattern
4
Antenna Pattern Solid Angle
sin .d d d   
A differential solid angle,
d, in sr, is defined as
2
0 0
sin 4 ( ).d d sr
 
 
   
 
   
For a sphere, the solid angle is found by
integrating
An antenna’s pattern solid angle,
 ,p n
P d   
All of the radiation emitted by the antenna is
concentrated in a cone of solid angle p over
which the radiation is constant and equal to the
antenna’s maximum radiation value. 5
DIRECTIVITY
 Fundamental antenna parameter.
 Measurement of radiation pattern
 Equally in all directions would have
effectively zero directionality,
 Directivity of equally directional
antenna would be 1.
6
DIRECTIVITY
7
Directivity
Normalized radiation pattern can be written
as a function in spherical coordinates:
Efficiency
Power is fed to an antenna through a T-Line and
the antenna appears as a complex impedance
.ant ant antZ R jX 
ant rad dis
R R R 
radiation
dissipativeFor the antenna is driven by phasor current j
o sI I e 

Power dissipated by ohmic losses is 21
2
diss o diss
P I R
rad rad
rad diss rad diss
P R
e
P P R R
 
 
8
Gain
   , ,G eD   
The power gain, G, of an antenna is very
much like its directive gain, but also takes
into account efficiency
The maximum power gain max maxG eD
The maximum power gain is often
expressed in dB.
   max max10
10logG GdB 
9
?
10

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Radiation pattern mcre 13 november 2016

  • 1. Radiation Pattern Abdullah Al Mehedi ID- 150105 Section- A 1
  • 2. Radiation Pattern ◦ Beamwidth ◦ Pattern Solid Angle ◦ Directivity ◦ Efficiency ◦ Gain Radiation pattern Directional Radiation 2
  • 3. Beamwidth Antenna Beam width is the angle between the half-power of an antenna pattern or beam over which the relative power is at or above 50% of the peak power.  Known as half-power. Beamwidth = 70λ / D where, λ = Wavelength D = Diameter 3
  • 5. Antenna Pattern Solid Angle sin .d d d    A differential solid angle, d, in sr, is defined as 2 0 0 sin 4 ( ).d d sr               For a sphere, the solid angle is found by integrating An antenna’s pattern solid angle,  ,p n P d    All of the radiation emitted by the antenna is concentrated in a cone of solid angle p over which the radiation is constant and equal to the antenna’s maximum radiation value. 5
  • 6. DIRECTIVITY  Fundamental antenna parameter.  Measurement of radiation pattern  Equally in all directions would have effectively zero directionality,  Directivity of equally directional antenna would be 1. 6
  • 7. DIRECTIVITY 7 Directivity Normalized radiation pattern can be written as a function in spherical coordinates:
  • 8. Efficiency Power is fed to an antenna through a T-Line and the antenna appears as a complex impedance .ant ant antZ R jX  ant rad dis R R R  radiation dissipativeFor the antenna is driven by phasor current j o sI I e   Power dissipated by ohmic losses is 21 2 diss o diss P I R rad rad rad diss rad diss P R e P P R R     8
  • 9. Gain    , ,G eD    The power gain, G, of an antenna is very much like its directive gain, but also takes into account efficiency The maximum power gain max maxG eD The maximum power gain is often expressed in dB.    max max10 10logG GdB  9
  • 10. ? 10

Hinweis der Redaktion

  1. The Antenna Radiation Pattern is a graphical representation of the antennas radiated electrical performance. This wave of energy (electromagnetic in origin) emitted from the antenna that propagates through space is measured at a defined Angle, Amplitude, and Frequency. The measurement of this performance is commonly presented in a graphical format.
  2. Beamwidth : Antenna Beam width is the angle between the half-power of an antenna pattern or beam over which the relative power is at or above 50% of the peak power. *Antenna beam width is also known as the half-power. Formula : Beamwidth = 70λ / D where, λ = Wavelength D = Diameter
  3. The main beam is the region around the direction of maximum radiation (usually the region that is within 3 dB of the peak of the main beam). The main beam in Figure 2 is centered at 90 degrees. The sidelobes are smaller beams that are away from the main beam. These sidelobes are usually radiation in undesired directions which can never be completely eliminated. The sidelobes in Figure 2 occur at roughly 45 and 135 degrees. The Half Power Beamwidth (HPBW) is the angular separation in which the magnitude of the radiation pattern decrease by 50% (or -3 dB) from the peak of the main beam. From Figure 2, the pattern decreases to -3 dB at 77.7 and 102.3 degrees. Hence the HPBW is 102.3-77.7 = 24.6 degrees. Another commonly quoted beamwidth is the Null to Null Beamwidth. This is the angular separation from which the magnitude of the radiation pattern decreases to zero (negative infinity dB) away from the main beam. From Figure 2, the pattern goes to zero (or minus infinity) at 60 degrees and 120 degrees. Hence, the Null-Null Beamwidth is 120-60=60 degrees. Finally, the Sidelobe Level is another important parameter used to characterize radiation patterns. The sidelobe level is the maximum value of the sidelobes (away from the main beam). From Figure 2, the Sidelobe Level (SLL) is -14.5 dB.
  4. A radian is defined with the aid of Figure a). It is the angle subtended by an arc along the perimeter of the circle with length equal to the radius. A steradian may be defined using Figure (b). Here, one steradian (sr) is subtended by an area r2 at the surface of a sphere of radius r.
  5. Directivity is a fundamental antenna parameter. It is a measure of how 'directional' an antenna's radiation pattern is. An antenna that radiates equally in all directions would have effectively zero directionality, and the directivity of this type of antenna would be 1 (or 0 dB).
  6. An antenna's normalized radiation pattern can be written as a function in spherical coordinates: F(O,Q) A normalized radiation pattern is the same as a radiation pattern; it is just scaled in magnitude such that the peak (maximum value) of the magnitude of the radiation pattern (F in equation [1]) is equal to 1. Mathematically, the formula for directivity (D) is written as: D = 1/(1/4pi………) This equation for directivity might look complicated, but the numerator is the maximum value of F, and the denominator just represents the "average power radiated over all directions". This equation then is just a measure of the peak value of radiated power divided by the average, which gives the directivity of the antenna.
  7. An antenna efficiency e can be defined as the ratio of the radiated power to the total power fed to the antenna.