Transmitting Antennas Flashcards
What produces EM waves
time varying currents
Isotropic
uniform in all directions
Properties of a real antenna
Input impedance, gain and radiation pattern, polarization
Antenna input impedance
ZA=RA+jXA
Components of resistive antenna input impedance
Rrad (radiation/heat)
Rloss (energy storage)
Gain/Radiation Pattern
Some directions are favored over others
A high gain antenna is
highly directional
Polarization
E-field direction depends on antenna geometry and excitation. What shape does the E-field trace?
conductivity of copper
5.8(10^7)
HPBW
Half power beam-width, bandwidth of signal at -3dB level
SLL
Side Lobe Level, dB level at the first lobe
Assumptions for the Hertzian dipole
filamentary wire, negligible feed gap, dipole lies along z-axis, high conductivity
Antenna directivity
a direction-dependent scaling factor applied to the otherwise isotopically radiated power
Formula to switch to dBi
10log(value)
dBi
dB relative to an isotropic radiator
omnidirectional
there is no dependence in a direction, therefore it is omnidirectional in that direction
Principal Plane Pattern
the radiation patterns plotted in the theta-plane and phi-plane
FBR
Front-to-back ratio, dB level at pi or 180 degrees
FNBW
First Null Beamwidth, bandwidth from the first nulls
Half-wavelength dipole
-Rrad increases faster with length than Rloss
-I(z) becomes sinusoidal
-XA approaches a cross-over at 0 (less capacitive -> inductive)
intrinsic impedance
ratio of E-field and H-field within a medium, the impedance of the medium
Quarter-wavelength monopole theory
We can apply image theory to the half-wavelength dipole antenna: cut the dipole in half (at the
feed-point) and mount the upper arm over a perfectly conductive half-space. Image theory dictates
that the fields above the half-space will be identical to those of a half-wavelength dipole in free
space, while the fields within the half-space go to zero
Quarter-wavelength monopole input impedance
The impedance is reduced by half πA = 36.5 + π21 β¦ for π = π/4, where π
rad =
36.5 β¦. By trimming the length by 4-6%, the reactive component is tuned out,
leaving πA β
π
rad β
35-36.5 β¦
Quarter-wavelength monopole gain and directivity
The directivity (and gain) is double that of a half-wavelength dipole because all the power
is radiated above the boundary and none below it.