Title: Antennas
1Antennas
- Theory, characteristics, and implementations
2Topics
- 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
3The 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)
4Spatial 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.
5Polarization 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.
6Impedance 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.
7Propagation 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.
8Propagation mode adapter
- During both transmission and receive operations
the antenna must provide the transition between
these two propagation modes.
9Antenna types
Antennas come in a wide variety of sizes and
shapes
Horn antenna
Parabolic reflector antenna
Helical antenna
10Theory
- 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.
11Theory
- In wire-type antennas the radiation
characteristics are determined by the current
distribution which produces the local magnetic
field.
Yagi-Uda antenna
Helical antenna
12Theory wire antenna example
Some simplifying approximations can be made to
take advantage the far-field conditions.
13Theory wire antenna example
Once Eq and Ef are known, the radiation
characteristics can be determined. Defining the
directional function f (q, f) from
14Theory aperture antennas
- In aperture-type antennas the radiation
characteristics are determined by the field
distribution across the aperture.
Horn antenna
Parabolic reflector antenna
15Theory 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)
16Theory
- 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.
17Characteristics 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
18Characteristics Radiation pattern
Spherical coordinate system
19Characteristics Radiation pattern
20Characteristics Radiation pattern
21Characteristics Radiation pattern
22Characteristics Radiation pattern
23Characteristics Radiation pattern
24Characteristics 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
25Characteristics 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
26Characteristics 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
27Characteristics 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
28Characteristics 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)
29Characteristics 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)
30Friis 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.
31Friis 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
32Friis 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
33Friis 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.
34Implementation
- Dipole, monopole, and ground planes
- Horns
- Parabolic reflectors
- Arrays
35Implementation 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
36Dipole antennas
Versions of broadband dipole antennas
37Dipole antennas
38Monopole 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
39Ground 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
40Implementation Horn antennas
41Implementation Horn antennas
42Implementation 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
43Implementation 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
44Implementation 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.)
45Implementation 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.
46Implementation 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.
47Implementation Antenna arrays
- By adjusting the amplitude and phase of each
elements excitation, the beam characteristics can
be modified.
48Implementation Antenna arrays
49Implementation Antenna arrays
50Implementation Example 2-element
array Isotropic radiators
51Implementation Example 2-element
array Isotropic radiators
52Implementation Example 2-element
array Half-wave dipole radiators
53Implementation Example 2-element array
Half-wave dipole radiators
54Implementation Example 6-element array
Half-wave dipole radiators
grating lobes
d l produces two grating lobes
55Antenna 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
56Antenna 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
57Conclusions
- 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.
58Terminology
- 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