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Antennas

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Antennas Theory, characteristics, and implementations Chris Allen (callen_at_eecs.ku.edu) Course website URL people.eecs.ku.edu/~callen/823/EECS823.htm – PowerPoint PPT presentation

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Title: Antennas


1
Antennas
  • Theory, characteristics, and implementations

Chris Allen (callen_at_eecs.ku.edu) Course website
URL people.eecs.ku.edu/callen/823/EECS823.htm
2
Topics
  • Role of antennas
  • Theory
  • Antenna types
  • Characteristics
  • Radiation pattern beamwidth, pattern solid
    angle
  • Directivity, gain, effective area
  • Bandwidth
  • Friis transmission formula
  • Implementations
  • Dipole, monopole, and ground planes
  • Horn
  • Parabolic reflector
  • Arrays
  • Terminology

3
The role of antennas
  • Antennas serve four primary functions
  • Spatial filter
  • directionally-dependent sensitivity
  • Polarization filter
  • polarization-dependent sensitivity
  • Impedance transformer
  • transition between free space and transmission
    line
  • Propagation mode adapter
  • from free-space fields to guided waves
  • (e.g., transmission line, waveguide)

4
Spatial filter
  • Antennas have the property of being more
    sensitive in one direction than in another which
    provides the ability to spatially filter signals
    from its environment.

Radiation pattern of directive antenna.
Directive antenna.
5
Polarization filter
Antennas have the property of being more
sensitive to one polarization than another which
provides the ability to filter signals based on
its polarization.
In this example, h is the antennas effective
height whose units are expressed in meters.
6
Impedance transformer
  • Intrinsic impedance of free-space, E/H
  • Characteristic impedance of transmission line,
    V/I
  • A typical value for Z0 is 50 ?.
  • Clearly there is an impedance mismatch that must
    be addressed by the antenna.

7
Propagation mode adapter
  • In free space the waves spherically expand
    following Huygens principleeach point of an
    advancingwave front is in fact thecenter of a
    fresh disturbanceand the source of a new train
    of waves.
  • Within the sensor, the waves are guided within a
    transmission line or waveguide that restricts
    propagation to one axis.

8
Propagation mode adapter
  • During both transmission and receive operations
    the antenna must provide the transition between
    these two propagation modes.

9
Antenna types
Antennas come in a wide variety of sizes and
shapes
Horn antenna
Parabolic reflector antenna
Helical antenna
10
Theory
  • Antennas include wire and aperture types.
  • Wire types include dipoles, monopoles, loops,
    rods, stubs, helicies, Yagi-Udas, spirals.
  • Aperture types include horns, reflectors,
    parabolic, lenses.

11
Theory
  • In wire-type antennas the radiation
    characteristics are determined by the current
    distribution which produces the local magnetic
    field.

Yagi-Uda antenna
Helical antenna
12
Theory wire antenna example
Some simplifying approximations can be made to
take advantage the far-field conditions.
13
Theory wire antenna example
Once Eq and Ef are known, the radiation
characteristics can be determined. Defining the
directional function f (q, f) from
14
Theory aperture antennas
  • In aperture-type antennas the radiation
    characteristics are determined by the field
    distribution across the aperture.

Horn antenna
Parabolic reflector antenna
15
Theory aperture antenna example
The far-field radiation pattern can be found from
the Fourier transform of the near-field pattern.
Where Sr is the radial component of the power
density, S0 is the maximum value of Sr, and Fn is
the normalized version of the radiation pattern
F(q, f)
16
Theory
  • Reciprocity
  • If an emf is applied to the terminals of antenna
    A and the current measured at the terminals of
    another antenna B, then an equal current (both in
    amplitude and phase) will be obtained at the
    terminals of antenna A if the same emf is applied
    to the terminals of antenna B.
  • emf electromotive force, i.e., voltage
  • Result the radiation pattern of an antenna is
    the same regardless of whether it is used to
    transmit or receive a signal.

17
Characteristics Radiation pattern
Radiation pattern variation of the field
intensity of an antenna as an angular function
with respect to the axis
Three-dimensional representation of the radiation
pattern of a dipole antenna
18
Characteristics Radiation pattern
Spherical coordinate system
19
Characteristics Radiation pattern
20
Characteristics Radiation pattern
21
Characteristics Radiation pattern
22
Characteristics Radiation pattern
23
Characteristics Radiation pattern
24
Characteristics Beamwidth and beam solid angle
The beam or pattern solid angle, ?p steradians
or sr is defined as where d? is the elemental
solid angle given by
25
Characteristics Directivity, gain, effective
area
Directivity the ratio of the radiation
intensity in a given direction from the antenna
to the radiation intensity averaged over all
directions.
unitless
Maximum directivity, Do, found in the direction
(?, ?) where Fn 1
and
or
Given Do, D can be found
26
Characteristics Directivity, gain, effective
area
Gain ratio of the power at the input of a
loss-free isotropic antenna to the power supplied
to the input of the given antenna to produce, in
a given direction, the same field strength at the
same distance
Of the total power Pt supplied to the antenna, a
part Po is radiated out into space and the
remainder Pl is dissipated as heat in the antenna
structure. The radiation efficiency hl is
defined as the ratio of Po to Pt
Therefore gain, G, is related to directivity, D,
as
And maximum gain, Go, is related to maximum
directivity, Do, as
27
Characteristics Directivity, gain, effective
area
Effective area the functional equivalent area
from which an antenna directed toward the source
of the received signal gathers or absorbs the
energy of an incident electromagnetic wave
It can be shown that the maximum directivity Do
of an antenna is related to an effective area (or
effective aperture) Aeff, by
where Ap is the physical aperture of the antenna
and ha Aeff / Ap is the aperture efficiency (0
ha 1) Consequently
m2
For a rectangular aperture with dimensions lx and
ly in the x- and y-axes, and an aperture
efficiency ha 1, we get
rad
rad
28
Characteristics Directivity, gain, effective
area
  • Therefore the maximum gain and the effective area
    can be used interchangeably by assuming a value
    for the radiation efficiency (e.g., ?l 1)

Example For a 30-cm x 10-cm aperture, f 10
GHz (? 3 cm)?xz ? 0.1 radian or 5.7, ?yz ?
0.3 radian or 17.2G0 ? 419 or 26 dBi (dBi
dB relative to an isotropic radiator)
29
Characteristics Bandwidth
  • The antennas bandwidth is the range of operating
    frequencies over which the antenna meets the
    operational requirements, including
  • Spatial properties (radiation characteristics)
  • Polarization properties
  • Impedance properties
  • Propagation mode properties
  • Most antenna technologies can support operation
    over a frequency range that is 5 to 10 of the
    central frequency
  • (e.g., 100 MHz bandwidth at 2 GHz)
  • To achieve wideband operation requires
    specialized antenna technologies
  • (e.g., Vivaldi, bowtie, spiral)

30
Friis transmission formula
  • At a fixed distance R from the transmitting
    antenna, the power intercepted by the receiving
    antenna with effective aperture Ar is
  • where Sr is the received power density (W/m2),
    and Gt is the peak gain of the transmitting
    antenna.

31
Friis transmission formula
  • If the radiation efficiency of the receiving
    antenna is hr, then the power received at the
    receiving antennas output terminals is
  • Therefore we can write
  • which is known as Friis transmission formula

32
Friis transmission formula
  • as Friis transmission formula can be rewritten
    to explicitly represent the free-space
    transmission loss, LFS
  • which represents the propagation loss experienced
    in transmission between two lossless isotropic
    antennas.With this definition, the Friis formula
    becomes

33
Friis transmission formula
  • Finally, a general form of the Friis
    transmission formula can be written that does not
    assume the antennas are oriented to achieve
    maximum power transfer
  • where (?t, ?t) is the direction of the receiving
    antenna in the transmitting antenna coordinates,
    and vice versa for (?r, ?r).
  • An additional term could be included to represent
    a polarization mismatch between the transmit and
    receive antennas.

34
Implementation
  • Dipole, monopole, and ground planes
  • Horns
  • Parabolic reflectors
  • Arrays

35
Implementation Dipole, monopole, and ground
plane
  • For a center-fed, half-wave dipole oriented
    parallel to the z axis

(V/m)
(W/m2)
Tuned half-wave dipole antenna
36
Dipole antennas
Versions of broadband dipole antennas
37
Dipole antennas
38
Monopole antenna
q
q
Ground plane
Radition pattern of vertical monopole above
ground of (A) perfect and (B) average
conductivity
Mirroring principle creates image of monopole,
transforming it into a dipole
39
Ground plane
  • A ground plane will produce an image of nearby
    currents. The image will have a phase shift of
    180 with respect to the original current.
    Therefore as the current element is placed close
    to the surface, the induced image current will
    effectively cancel the radiating fields from the
    current.
  • The ground plane may be any conducting surface
    including a metal sheet, a water surface, or the
    ground (soil, pavement, rock).

Horizontal current element
Conducting surface(ground plane)
Current element image
40
Implementation Horn antennas
41
Implementation Horn antennas
42
Implementation Parabolic reflector antennas
  • Circular aperture with uniform illumination.
    Aperture radius a.
  • Ap p a 2

where
where
J1( ) is the Bessel function of the first kind,
zero order
43
Implementation Antenna arrays
  • Antenna array composed of several similar
    radiating elements (e.g., dipoles or horns).
  • Element spacing and the relative amplitudes and
    phases of the element excitation determine the
    arrays radiative properties.

Linear array examples
Two-dimensional array of microstrip patch antennas
44
Implementation Antenna arrays
  • The far-field radiation characteristics Sr(?, ?)
    of an N-element array composed of identical
    radiating elements can be expressed as a product
    of two functions
  • Where Fa(?, ?) is the array factor, and Se(?, ?)
    is the power directional pattern of an individual
    element.
  • This relationship is known as the pattern
    multiplication principle.
  • The array factor, Fa(?, ?), is a range-dependent
    function and is therefore determined by the
    arrays geometry.
  • The elemental pattern, Se(?, ?), depends on the
    range-independent far-field radiation pattern of
    the individual element. (Element-to-element
    coupling is ignored here.)

45
Implementation Antenna arrays
  • In the array factor, Ai is the feeding
    coefficient representing the complex excitation
    of each individual element in terms of the
    amplitude, ai, and the phase factor, ?i, as
  • and ri is the range to the distant observation
    point.

46
Implementation Antenna arrays
  • For a linear array with equal spacing d between
    adjacent elements, which approximates to
  • For this case, the array factor becomes
  • Note that the e-jkR term which is common to all
    of the summation terms can be neglected as it
    evaluates to 1.

47
Implementation Antenna arrays
  • By adjusting the amplitude and phase of each
    elements excitation, the beam characteristics can
    be modified.

48
Implementation Antenna arrays
49
Implementation Antenna arrays
50
Implementation Example 2-element
array Isotropic radiators
51
Implementation Example 2-element
array Isotropic radiators
52
Implementation Example 2-element
array Half-wave dipole radiators
53
Implementation Example 2-element array
Half-wave dipole radiators
54
Implementation Example 6-element array
Half-wave dipole radiators
grating lobes
d l produces two grating lobes
55
Antenna arrays Beam steering effects
  • Inter-element separation affects linear array
    gain and grating lobes
  • The broadside array gain is approximatelywhere
    d is the inter-element spacing and N is the
    number of elements in the linear array
  • To avoid grating lobes, the maximum inter-element
    spacing varies with beam steering angle or look
    angle, ?, as

56
Antenna arrays Beamwidth and gain
  • An 2-D planar array with uniform spacing, N x M
    elements in the two dimensions with inter-element
    spacing of ?/2 provides a broadside array gain of
    approximately
  • The beamwidth of a steered beam from a uniform
    N-element array is approximately (for N gt
    5)where b is the window function broadening
    factor (b 1 for uniform window function) andd
    is the inter-element spacing

57
Conclusions
  • Antennas play an important role in microwave
    remote sensing systems.
  • There are both art and science aspects to
    antennas.
  • Antenna arrays enable the radiation
    characteristics to be changed electronically
    (i.e., very rapidly) unlike conventional
    mechanically-steered antennas.
  • Digital beamforming (dedicated transmit or
    receive electronics for each element) enable
    simultaneous realization of multiple antenna
    beams and/or multiple independent signals.

58
Terminology
  • Antenna structure or device used to collect or
    radiate electromagnetic waves
  • Array assembly of antenna elements with
    dimensions, spacing, and illumination sequency
    such that the fields of the individual elements
    combine to produce a maximum intensity in a
    particular direction and minimum intensities in
    other directions
  • Beamwidth the angle between the half-power
    (3-dB) points of the main lobe, when referenced
    to the peak effective radiated power of the main
    lobe
  • Directivity the ratio of the radiation
    intensity in a given direction from the antenna
    to the radiation intensity averaged over all
    directions
  • Effective area the functional equivalent area
    from which an antenna directed toward the source
    of the received signal gathers or absorbs the
    energy of an incident electromagnetic wave
  • Efficiency ratio of the total radiated power to
    the total input power
  • Far field region where wavefront is considered
    planar
  • Gain ratio of the power at the input of a
    loss-free isotropic antenna to the power supplied
    to the input of the given antenna to produce, in
    a given direction, the same field strength at the
    same distance
  • Isotropic radiates equally in all directions
  • Main lobe the lobe containing the maximum power
  • Null a zone in which the effective radiated
    power is at a minimum relative to the maximum
    effective radiation power of the main lobe
  • Radiation pattern variation of the field
    intensity of an antenna as an angular function
    with respect to the axis
  • Radiation resistance resistance that, if
    inserted in place of the antenna, would consume
    that same amount of power that is radiated by the
    antenna
  • Side lobe a lobe in any direction other than
    the main lobe
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