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UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
RADIATION PATTERN
Hanyang University
5/40 Antennas & RF Devices Lab.
- Definition : A mathematical function or a graphical representation of the radiation properties of the
antenna as a function of space coordinates.
- Field pattern : E & H fields’
magnitude (Linear scale. Angular
Space)
- Power pattern : Square of
magnitude’s of E&H fields (Linear
scale. Angular Space)
- Power pattern : Magnitude of E &
H fields (dB scale)
RADIATION PATTERN
Hanyang University
6/40 Antennas & RF Devices Lab.
- Dividing a field component by its maximum value, we obtain a normalized sphere field pattern which is a
dimensionless number with maximum value of unity. Thus the normalized field pattern for the component
of the electric field is given by
• Patterns may also be expressed in terms of the power per unit area or Poynting vector as S (θ,Φ) at a
certain distance from the antenna. Normalizing this power with respect to its maximum value yields a
normalized power pattern as a function of angle which is a dimensionless number with a maximum
value of unity
RADIATION PATTERN
UNIT 3.1 new.pptx(Transmission lines and antennas)
Antennas & RF Devices Lab.
• Major lobe (main beam) : The radiation lobe containing the direction of
maximum radiation.
• Minor lobe : any lobe except a major lobe.
• Side lobe : The radiation lobe in any direction other than the intended
lobe.
(Usually a side lobe is adjacent to the main lobe and occupies the hemisphere
in the direction of the main beam.)
• Back lobe : The radiation lobe whose axis makes an angle of
approximately 180◦ with respect to the beam of an antenna. Usually it
refers to a minor lobe that occupies the hemisphere in a direction opposite
to that of the major(main) lobe.
• Minor lobes usually represent radiation in undesired directions, and they
should be minimized.
• Side lobes are normally the largest of the minor lobes.
• The level of minor lobes is usually expressed as a ratio of the power
density in the lobe in question to that of the major lobe. This ratio is often
termed the side lobe ratio or side lobe level. It is an indication of
directivity of antenna.
Hanyang University
9/40
- Radiation Pattern Lobes
(a) Radiation lobes and beamwidths of an antenna pattern.
(b) Linear plot of power pattern and its associated lobes and beamwidths
Antennas & RF Devices Lab.
Isotropic antenna pattern
Directional antenna pattern
- Having the property of radiating or receiving
electro-magnetic wave more effectively in
some directions than in others.
- This term usually applied to an antenna
whose maximum directivity is significantly
greater than that of a half-wave dipole
Omnidirectional antenna pattern
- Having an essentially non directional pattern in a given plane
- Having a directional pattern in any orthogonal plane. Radiation pattern
may be in XY,YZ, XZ plane
- A Special type of a directional pattern.
2.2.2 Isotropic, Directional, and Omnidirectional Patterns
Isotropic antenna pattern
- A hypothetical lossless antenna pattern having
equal radiation in all directions.
- Ideal, not physically realizable.
- Often taken as a reference for expressing the
directive properties of actual antennas.
Hanyang University
11/40 Antennas & RF Devices Lab.
Radian and Steradian
Radian measures plane
angles (2D), while steradian
measures solid angles (3D).
Steradian: solid angle
subtended at the center
of a sphere by an area of
its surface equal to the
square of the radius of
the sphere
Hanyang University
12/40 Antennas & RF Devices Lab.
Radiation Power Density
Poynting Vector
• The quantity used to describe the power associated with an electromagnetic wave is the instantaneous
Poynting vector defined as
• The total power crossing a closed surface
Average Power Density
• For applications of time-varying fields, it is desirable to find the average power density.
• The average power density is obtained by integrating the instantaneous Poynting vector over
one period and dividing by the period.
Hanyang University
13/40 Antennas & RF Devices Lab.
Radiation Power Density
Average Radiated Power
• The power density associated with the electromagnetic fields of an antenna in its far-field region is
predominately real and will be referred to as radiation density.
• The average power radiated by an antenna (radiated power) can be written as
Power Pattern Versus Average Radiated Power
• The power pattern of the antenna is the average power density radiated by the antenna as a function of
the direction.
• The observations are usually made on a large sphere of constant radius extending into the far field.
14
It is the power radiated from an antenna per unit solid angle(that is it is the power
per steradian)
• We have Sr =
• = (watts/Sr),
• It can be also obtained by simply multiplying the radiation density by thesquare
of the distance
• Total Radiated Power Using Radiation Intensity: The total power is obtained by
integrating the radiation intensity over the entire solid angle of 4π.
Radiation Intensity
 Beamwidth - The angular separation between two identical points on opposite side the
pattern maximum.
 The beamwidth of an antenna is a very important figure of merit and often is used as a
trade-off between it and the side lobe level; that is, as the beamwidth decreases, the side
lobe increases and vice versa.
 The beamwidth of the antenna is also used to describe the resolution capabilities of the
antenna to distinguish between two adjacent radiating sources or radar targets.
 Half-Power Beam Width (HPBW). In a plane containing the direction of the maximum of a
beam, the angle between the two directions in which the radiation intensity is one-half
value of the beam.
 First-Null Beamwidth (FNBW ). Angular separation between the first nulls of the pattern.
Beamwidth
Beamwidth
 Beam solid angle is defined as a solid angle at which the total power is radiated or received
by an antenna.
 Unit of Beam solid angle is Steradians (Sr)
BEAM AREA (or BEAM SOLID ANGLE)
ϴ φ
Beam efficiency
Hanyang University
19/40 Antennas & RF Devices Lab.
The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity
averaged over all directions.
Directivity D
Hanyang University
20/40 Antennas & RF Devices Lab.
The beam solid angle ΩA is defined as the solid angle through which all the power of the antenna would
flow if its radiation intensity is constant (and equal to the maximum value of U) for all angles within ΩA.
Directivity D
 The ability of an antenna or antenna system to concentrate the
radiated power in a given direction .
 The ratio of the gain to the directivity is the antenna efficiency factor.
G= k D
Where k= efficiency factor
Gain G
Antenna Apertures
• The concept of aperture is most simply introduced by considering a receiving antenna, to describe the
power capturing characteristics of the antenna when a wave imposes on it.
• Suppose that the antenna is an electromagnetic horn immersed in the field of a uniform plane as
suggested in Fig.
• Let the Poynting vector, or power density, of the plane wave be S watts per square meter and the area
of the mouth of the horn be A square meters.
• If the horn extracts all the power from the wave over its
entire area A , then the total power P absorbed from the
wave is
• Thus, the electromagnetic horn may be regarded as a aperture, the total power it extracts from a
passing wave being proportional to the aperture or area of its mouth
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
Effective Height
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
Friis transmission formula
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)
UNIT 3.1 new.pptx(Transmission lines and antennas)

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UNIT 3.1 new.pptx(Transmission lines and antennas)

  • 5. Hanyang University 5/40 Antennas & RF Devices Lab. - Definition : A mathematical function or a graphical representation of the radiation properties of the antenna as a function of space coordinates. - Field pattern : E & H fields’ magnitude (Linear scale. Angular Space) - Power pattern : Square of magnitude’s of E&H fields (Linear scale. Angular Space) - Power pattern : Magnitude of E & H fields (dB scale) RADIATION PATTERN
  • 6. Hanyang University 6/40 Antennas & RF Devices Lab. - Dividing a field component by its maximum value, we obtain a normalized sphere field pattern which is a dimensionless number with maximum value of unity. Thus the normalized field pattern for the component of the electric field is given by • Patterns may also be expressed in terms of the power per unit area or Poynting vector as S (θ,Φ) at a certain distance from the antenna. Normalizing this power with respect to its maximum value yields a normalized power pattern as a function of angle which is a dimensionless number with a maximum value of unity RADIATION PATTERN
  • 8. Antennas & RF Devices Lab. • Major lobe (main beam) : The radiation lobe containing the direction of maximum radiation. • Minor lobe : any lobe except a major lobe. • Side lobe : The radiation lobe in any direction other than the intended lobe. (Usually a side lobe is adjacent to the main lobe and occupies the hemisphere in the direction of the main beam.) • Back lobe : The radiation lobe whose axis makes an angle of approximately 180◦ with respect to the beam of an antenna. Usually it refers to a minor lobe that occupies the hemisphere in a direction opposite to that of the major(main) lobe. • Minor lobes usually represent radiation in undesired directions, and they should be minimized. • Side lobes are normally the largest of the minor lobes. • The level of minor lobes is usually expressed as a ratio of the power density in the lobe in question to that of the major lobe. This ratio is often termed the side lobe ratio or side lobe level. It is an indication of directivity of antenna.
  • 9. Hanyang University 9/40 - Radiation Pattern Lobes (a) Radiation lobes and beamwidths of an antenna pattern. (b) Linear plot of power pattern and its associated lobes and beamwidths
  • 10. Antennas & RF Devices Lab. Isotropic antenna pattern Directional antenna pattern - Having the property of radiating or receiving electro-magnetic wave more effectively in some directions than in others. - This term usually applied to an antenna whose maximum directivity is significantly greater than that of a half-wave dipole Omnidirectional antenna pattern - Having an essentially non directional pattern in a given plane - Having a directional pattern in any orthogonal plane. Radiation pattern may be in XY,YZ, XZ plane - A Special type of a directional pattern. 2.2.2 Isotropic, Directional, and Omnidirectional Patterns Isotropic antenna pattern - A hypothetical lossless antenna pattern having equal radiation in all directions. - Ideal, not physically realizable. - Often taken as a reference for expressing the directive properties of actual antennas.
  • 11. Hanyang University 11/40 Antennas & RF Devices Lab. Radian and Steradian Radian measures plane angles (2D), while steradian measures solid angles (3D). Steradian: solid angle subtended at the center of a sphere by an area of its surface equal to the square of the radius of the sphere
  • 12. Hanyang University 12/40 Antennas & RF Devices Lab. Radiation Power Density Poynting Vector • The quantity used to describe the power associated with an electromagnetic wave is the instantaneous Poynting vector defined as • The total power crossing a closed surface Average Power Density • For applications of time-varying fields, it is desirable to find the average power density. • The average power density is obtained by integrating the instantaneous Poynting vector over one period and dividing by the period.
  • 13. Hanyang University 13/40 Antennas & RF Devices Lab. Radiation Power Density Average Radiated Power • The power density associated with the electromagnetic fields of an antenna in its far-field region is predominately real and will be referred to as radiation density. • The average power radiated by an antenna (radiated power) can be written as Power Pattern Versus Average Radiated Power • The power pattern of the antenna is the average power density radiated by the antenna as a function of the direction. • The observations are usually made on a large sphere of constant radius extending into the far field.
  • 14. 14 It is the power radiated from an antenna per unit solid angle(that is it is the power per steradian) • We have Sr = • = (watts/Sr), • It can be also obtained by simply multiplying the radiation density by thesquare of the distance • Total Radiated Power Using Radiation Intensity: The total power is obtained by integrating the radiation intensity over the entire solid angle of 4π. Radiation Intensity
  • 15.  Beamwidth - The angular separation between two identical points on opposite side the pattern maximum.  The beamwidth of an antenna is a very important figure of merit and often is used as a trade-off between it and the side lobe level; that is, as the beamwidth decreases, the side lobe increases and vice versa.  The beamwidth of the antenna is also used to describe the resolution capabilities of the antenna to distinguish between two adjacent radiating sources or radar targets.  Half-Power Beam Width (HPBW). In a plane containing the direction of the maximum of a beam, the angle between the two directions in which the radiation intensity is one-half value of the beam.  First-Null Beamwidth (FNBW ). Angular separation between the first nulls of the pattern. Beamwidth
  • 17.  Beam solid angle is defined as a solid angle at which the total power is radiated or received by an antenna.  Unit of Beam solid angle is Steradians (Sr) BEAM AREA (or BEAM SOLID ANGLE) ϴ φ
  • 19. Hanyang University 19/40 Antennas & RF Devices Lab. The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions. Directivity D
  • 20. Hanyang University 20/40 Antennas & RF Devices Lab. The beam solid angle ΩA is defined as the solid angle through which all the power of the antenna would flow if its radiation intensity is constant (and equal to the maximum value of U) for all angles within ΩA. Directivity D
  • 21.  The ability of an antenna or antenna system to concentrate the radiated power in a given direction .  The ratio of the gain to the directivity is the antenna efficiency factor. G= k D Where k= efficiency factor Gain G
  • 22. Antenna Apertures • The concept of aperture is most simply introduced by considering a receiving antenna, to describe the power capturing characteristics of the antenna when a wave imposes on it. • Suppose that the antenna is an electromagnetic horn immersed in the field of a uniform plane as suggested in Fig. • Let the Poynting vector, or power density, of the plane wave be S watts per square meter and the area of the mouth of the horn be A square meters. • If the horn extracts all the power from the wave over its entire area A , then the total power P absorbed from the wave is • Thus, the electromagnetic horn may be regarded as a aperture, the total power it extracts from a passing wave being proportional to the aperture or area of its mouth