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Linear Antenna
INFINITESIMAL DIPOLE
• (l >>λ)
• symmetrical at the origin
• Oriented along the z - axis
INFINITESIMAL DIPOLE
• not practical
• used to represent capacitor
plate antennas
• used as building block for
complex geometries
INFINITESIMAL DIPOLE
• (l << λ); (a <<λ)
• I0 is constant.
INFINITESIMAL DIPOLE
• Radiatd Fields
INFINITESIMAL DIPOLE
• Far-field Region
INFINITESIMAL DIPOLE
• Time - Average Radiated Power
and Radiation Resistance
• Directivity and Effective
Aperture
SMALL DIPOLE
• λ/50 < l ≤ λ/10
• symmetrical at the origin
• oriented along the z - axis
SMALL DIPOLE
• current distribution
- triangular
SMALL DIPOLE
• Radiation Resistance
SMALL DIPOLE
• Approximatio of Fields
FINITE LENGTH DIPOLE
• Length > λ/10
• current
-assuming a very thin wire
-I0 - constant
- ceter fed; current vanishes at end
points
FINITE LENGTH DIPOLE
• electric field of a finite lenght
dipole
FINITE LENGTH DIPOLE
• Radiatd Fields
FINITE LENGTH DIPOLE
• Radiation Resistance and Input
Radiation Resistance
• Directivity and Effective
Aperture
HALF - WAVELENGTH DIPOLE
• one of the most commonly used
• radiation resistance - 73 ohms
HALF - WAVELENGTH DIPOLE
• electric and magnetic field
component
HALF - WAVELENGTH DIPOLE
• Radiation Resistance and Input
Impedance
• Directivity and Effective
Aperture
LINEAR ELEMENTS NEAR OR ON INFINITE
PERFECT CONDUCTORS
• antennas radiating into an
unbounded medium
• obstacles introduce alteration of
overall radiation pattern
LINEAR ELEMENTS NEAR OR ON INFINITE
PERFECT CONDUCTORS
• Image Theory - virtual sources
for the refletion
• obstacles introduce alteration of
overall radiation pattern
LINEAR ELEMENTS NEAR OR ON INFINITE
PERFECT CONDUCTORS
LINEAR ELEMENTS NEAR OR ON INFINITE
PERFECT CONDUCTORS
LINEAR ELEMENTS NEAR OR ON INFINITE
PERFECT CONDUCTORS
LINEAR ELEMENTS NEAR OR ON INFINITE
PERFECT CONDUCTORS
LINEAR ELEMENTS NEAR OR ON INFINITE
PERFECT CONDUCTORS
end...

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Linear Antenna

Editor's Notes

  • #2: oldest, simplest, cheapest, versatile
  • #4: - top-hat-loaded antennas ; -end plates are used as capacitive loading(current on dipole nearly uniform) ; negligible radiation- plates ; very small and thin
  • #5: -very small and thin ;
  • #6: -applicable for all region ex. the source; kr<1 nearfieldregion-energy imaginary stored ; kr = 1 radian sphere boundary from imaginary and stored to radiated
  • #7: -applicable for all antenna finite dimension
  • #8: -very small and thin ;
  • #11: radiated power resistance is 1/4 of the infi ; shape sand patterns are the same
  • #12: surrounding boundary ,. phase error max.,., D -largest dimension
  • #14: subdivision of infinitesimal ; elemntfactor- type and direction of flow i ; space factor-current distribution along the space
  • #15: subdivision of infinitesimal ; elemntfactor- type and direction of flow i ; space factor-current distribution along the space
  • #16: subdivision of infinitesimal ; elemntfactor- type and direction of flow i ; space factor-current distribution along the space
  • #17: tx char. imp. - 50 - 75
  • #18: tx char. imp. - 50 - 75
  • #19: tx char. imp. - 50 - 75
  • #20: - practcally there is always an a ground as obstcl
  • #21: for analysis purps - imgnry
  • #22: for analysis purps - imgnry
  • #23: for analysis purps - imgnry
  • #24: image near
  • #25: image near
  • #26: for analysis purps - imgnry