Transmitting Antennas Flashcards

1
Q

What produces EM waves

A

time varying currents

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2
Q

Isotropic

A

uniform in all directions

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3
Q

Properties of a real antenna

A

Input impedance, gain and radiation pattern, polarization

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4
Q

Antenna input impedance

A

ZA=RA+jXA

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5
Q

Components of resistive antenna input impedance

A

Rrad (radiation/heat)
Rloss (energy storage)

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6
Q

Gain/Radiation Pattern

A

Some directions are favored over others

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7
Q

A high gain antenna is

A

highly directional

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8
Q

Polarization

A

E-field direction depends on antenna geometry and excitation. What shape does the E-field trace?

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9
Q

conductivity of copper

A

5.8(10^7)

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10
Q

HPBW

A

Half power beam-width, bandwidth of signal at -3dB level

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11
Q

SLL

A

Side Lobe Level, dB level at the first lobe

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12
Q

Assumptions for the Hertzian dipole

A

filamentary wire, negligible feed gap, dipole lies along z-axis, high conductivity

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13
Q

Antenna directivity

A

a direction-dependent scaling factor applied to the otherwise isotopically radiated power

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14
Q

Formula to switch to dBi

A

10log(value)

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15
Q

dBi

A

dB relative to an isotropic radiator

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16
Q

omnidirectional

A

there is no dependence in a direction, therefore it is omnidirectional in that direction

17
Q

Principal Plane Pattern

A

the radiation patterns plotted in the theta-plane and phi-plane

18
Q

FBR

A

Front-to-back ratio, dB level at pi or 180 degrees

19
Q

FNBW

A

First Null Beamwidth, bandwidth from the first nulls

20
Q

Half-wavelength dipole

A

-Rrad increases faster with length than Rloss
-I(z) becomes sinusoidal
-XA approaches a cross-over at 0 (less capacitive -> inductive)

21
Q

intrinsic impedance

A

ratio of E-field and H-field within a medium, the impedance of the medium

22
Q

Quarter-wavelength monopole theory

A

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

23
Q

Quarter-wavelength monopole input impedance

A

The impedance is reduced by half 𝑍A = 36.5 + 𝑗21 Ω for 𝑙 = πœ†/4, where 𝑅rad =
36.5 Ω. By trimming the length by 4-6%, the reactive component is tuned out,
leaving 𝑍A β‰… 𝑅rad β‰… 35-36.5 Ω

24
Q

Quarter-wavelength monopole gain and directivity

A

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.

25
Q

Broadside

A

a type of radiation pattern for a linear array antenna where the axis of the main lobe is perpendicular to the axis of the array

26
Q

900 MHz ISM band

A

902-928 MHz

27
Q

ISM band

A

The ISM radio bands are portions of the radio spectrum reserved internationally for industrial, scientific, and medical (ISM) purposes, excluding applications in telecommunications.[1]

28
Q

End fire array

A

An endfire array is a linear array in which the direction of radiation is along the line of the antennas

29
Q

Skin effect

A

If the radius of the conductor is much less than the skin depth, we can assume that the current is uniform to one skin depth