U.S. patent number 3,624,658 [Application Number 05/053,563] was granted by the patent office on 1971-11-30 for broadband spiral antenna with provision for mode suppression.
This patent grant is currently assigned to Textron Inc.. Invention is credited to George N. Voronoff.
United States Patent |
3,624,658 |
Voronoff |
November 30, 1971 |
BROADBAND SPIRAL ANTENNA WITH PROVISION FOR MODE SUPPRESSION
Abstract
A six-arm spiral antenna backed by a reflective surface is
energized to activate four arms with the other two arms being
parasitic and Mode 5 radiation is suppressed to achieve broadband
operation.
Inventors: |
Voronoff; George N. (San
Francisco, CA) |
Assignee: |
Textron Inc. (Belmont,
CA)
|
Family
ID: |
21985129 |
Appl.
No.: |
05/053,563 |
Filed: |
July 9, 1970 |
Current U.S.
Class: |
343/805;
343/739 |
Current CPC
Class: |
H01Q
9/27 (20130101); H01Q 1/36 (20130101) |
Current International
Class: |
H01Q
1/36 (20060101); H01Q 9/27 (20060101); H01Q
9/04 (20060101); H01q 001/36 () |
Field of
Search: |
;343/895,739 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Saalbach; Herman Karl
Assistant Examiner: Nussbaum; Marvin
Claims
What is claimed is:
1. An improved spiral antenna comprising six equiangular arms
equally spaced circumferentially apart about a center, first means
electrically connecting together the inner ends of a pair of
adjacent arms, second means connecting together the inner ends of
the pair of arms opposite to the first connected pair of arms,
means applying high-frequency energization between said first and
second means to energize the antenna for producing electromagnetic
radiation therefrom, and suppression means disposed substantially
at a radius of 0.6 wavelength of antenna energization from the
antenna center about the center adjacent each arm for suppressing
electromagnetic radiation at a radius greater than 0.6 wavelength
to thus suppress Mode 5 radiation from the antenna.
2. The antenna of claim 1 further defined by means defining an
electrically conducting ground plane in close proximity to one side
of said antenna adjacent each arm thereof whereby said antenna
radiates away from said plane.
3. The antenna of claim 1 further defined by said suppression means
comprising an annular absorber of a material absorbing
electromagnetic radiation disposed against one side of the antenna
and having an inner diameter in the range of 0.6 to 0.8
wavelength.
4. The antenna of claim 2 further defined by said suppression means
comprising a plurality of resistors connected one between each
antenna arm and said ground plane at a radius in the range of 0.6
to 0.8 wavelength and said arms terminating at such
connections.
5. An improved unidirectional frequency-independent antenna
comprising six equiangular spiral antenna arms disposed in
substantially planar array and spaced equally apart about a center,
means electrically connecting together a first pair of antenna arms
adjacent said center and connecting together the pair of antenna
arms opposite said first pair, means applying high-frequency
electrical energization between said connections to directly
energize said two pairs of arms and parasitically energize the two
remaining unconnected antenna arms whereby said antenna is
energized to radiate in Mode 1 and Mode 5 regions, means defining
an electrically conducting ground plane in close proximity to one
substantially planar side of the antenna, and radiation suppression
means disposed between said antenna and ground plane radially
outward of the Mode 1 radiation region of the antenna and
suppressing Mode 5 radiation whereby substantially only Mode 1
radiation occurs.
6. The antenna of claim 5 further defined by said radiation
suppression means being disposed radially outward of the antenna
from the center thereof substantially 0.6 wavelength of the highest
operating frequency of energization of the antenna.
7. The antenna of claim 6 further defined by said radiation
suppression means comprising a material having a high loss tangent
for high-frequency energization disposed in a ring between said
antenna arms and said ground plane and extending radially outward
from substantially 0.6 wavelength to 0.9 wavelength of the highest
operating frequency of energization of the antenna.
8. The antenna of claim 5 further defined by said suppression means
comprising resistors connected between said antenna arms and said
ground plane and said arms terminating at said resistor
connections.
Description
BACKGROUND OF INVENTION
There have been developed a class of antennas which are oftentimes
termed "frequency-independent antennas" inasmuch as they are
relatively insensitive to frequency variations above some minimum
frequency. Such structures were originally proposed by V. H. Rumsey
and reference in this respect is made to page 33 of the publication
"The Encyclopedia of Electronics," copyright 1962 by Reinhold
Publishing Corporation. Although these types of antennas are
considered to be relatively independent of variations in
energization frequency, it is realized that electrically conducting
bodies disposed in proximity thereto materially varies their
characteristics. In particular, problems oftentimes arise in the
physical mounting of frequency-independent antennas.
One type of frequency-independent antenna is the spiral antenna, as
it is commonly termed. Generally the curvature of the arms of a
spiral antenna may be properly delineated as an Archimedean spiral
or as a logarithmic spiral; however, in the following discussion
the term "spiral" is taken to denominate an antenna having curved
arms of these general types.
In the utilization of spiral antennas many applications require the
mounting of same relatively close to a ground plane or in front of
a shallow cavity and this then creates a frequency dependency which
is generally considered to be highly undesirable. One such
situation in which this type of mounting occurs is the provision of
antennas upon aircraft structures.
There has been carried out a variety of investigations of
frequency-independent antennas including spiral antennas of a
variety of different configurations. For a discussion of at least
one such series of investigations, reference is made to an article
by R. Sivan-Sussman entitled "Various Modes of the Equiangular
Spiral Antenna" and appearing in IEEE Transactions on Antennas and
Propagation, pages 533 to 539, Sept. 1963. Experimental data on a
substantial number of different equiangular spiral antenna
configurations and modes of energization is set forth in the
foregoing article. Such article does not, however, attempt to
propose practical solutions to the problems identified above.
Insofar as practical operating antennas of this general type are
concerned, there have been issued a number of U.S. Pats. such as,
for example, U.S. Pat. Nos. 2,990,548 and 3,131,394 to Wheeler, as
well as others. Conventional prior art spiral antennas do, however,
still suffer from the difficulty of frequency dependency when the
spiral is operated at a close distance from the ground plane and
beam pattern variations with frequency occur.
SUMMARY OF INVENTION
The antenna of the present invention is comprised as a six-arm
spiral comprising a unidirectional radiator backed by a cavity or
ground plane that may be in close proximity to the antenna arms.
The antenna produces a highly desirable radiation pattern which is
stable over a substantial bandwidth or frequency variation.
The six-arm spiral antenna hereof has the first and second arms
thereof electrically connected together and energization applied
between such connection and a connection between the fourth and
fifth arms. The third and sixth arms of the antenna are
parasitically excited to thereby produce only Mode 1 and Mode 5
radiation. The invention furthermore provides for suppression of
Mode 5 radiations either by the utilization of an absorber or
resistive terminations at a predetermined antenna radius. This then
substantially eliminates the variation in radiation pattern with
frequency change caused by the otherwise present Mode 5 radiation.
Other radiation modes are not present so that substantially only
Mode 1 radiation occurs.
DESCRIPTION OF FIGURES
The present invention is illustrated as to particular preferred
embodiments thereof in the accompanying drawings wherein:
FIG. 1 illustrates the patterns of radiation of various harmonics
for a spiral antenna;
FIG. 2 is a schematic illustration in plan view of an antenna in
accordance with the present invention;
FIG. 3 is a central sectional view of one embodiment of the present
invention, such as illustrated in FIG. 2; and
FIG. 4 is a schematic illustration of an alternative embodiment of
the present invention.
DESCRIPTION OF PREFERRED EMBODIMENTS
The present invention comprises a six-arm spiral antenna having a
pair of opposed arms of the antenna parasitically excited and being
backed by a reflecting surface. Investigations of spiral antennas
which, as noted above, are one form of what is generally termed
"frequency-independent antennas," has shown that the radiation
pattern thereof is formed of patterns resulting from the various
independent excitation voltages or currents whose phases are
harmonically related. In this respect, reference is made to FIG. 1
of the drawings of this application wherein there is shown a plot
of radiation patterns as presented in the publication
"Frequency-Independent Antennas" by Victor H. Rumsey, Academic
Press, 1966, page 122. To those knowledgeable in the art, it is
recognized that the first harmonic produces a single-lobe radiation
pattern which is highly advantageous for many applications. The
radiation pattern resulting from a mixture of the various harmonics
may be of theoretical interest but, in general, are detrimental to
the desired result from a frequency stability point of view.
Extensive investigation has been made of this general type of
antenna, as noted above. However, to date, there appears to have
been developed no antenna of this general categorization producing
a stable radiation pattern over an appreciable bandwidth with a
simple feeding arrangement, for example, a bandwidth of 4:1 or
greater.
Particularly under those circumstances wherein a conventional
two-arm spiral antenna is operated over a ground plane at a small
electrical distance therefrom, the beamwidth of the radiation
pattern has been found to fluctuate rapidly with frequency for
frequency bandwidths in excess of 2:1. Investigation of this
phenomenon has indicated that the range of half-power beamwidth
fluctuation is typically in the area of 35.degree. to 110.degree..
It will be appreciated that such fluctuations are intolerable for
many applications.
Careful consideration of the reasons for the above-noted radiation
pattern fluctuations indicates that same are caused by simultaneous
presence of more than one mode of radiation and, in general, it is
the presence of Modes 1 and 3 which pose the problems. It may be
postulated and has, in fact, been established that the Mode 3
radiation is present because of insufficient radiations from the
Mode 1 region of the antenna so that the remainder of the energy to
be radiated by the antenna occurs in the Mode 3 region.
Referring to FIG. 1 of the drawing, there is shown a single lobe of
radiation 11 resulting from the primary or first harmonic and
double-lobes 12 and 13 and 14 which are the result of second, third
and fifth harmonics, respectively. For many applications the
presence of more than one mode of radiation is highly undesirable
as, for example, the presence of Modes 2, 3 or 5 are the cause of
beamwidth fluctuations with frequency variations. The present
invention provides for the suppression of these higher modes of
radiation.
Referring now to FIG. 2 of the drawing, it will be seen to be
schematically illustrated an equiangular spiral antenna 21 having
six spiral arms 22 to 27 extending outwardly from a central
excitation area in numbered order and equal spacing about such
area. The arms of the antenna in themselves may be conventional and
may, for example, be formed by copper plating on very thin
Teflon-impregnated Fiberglas having a copper thickness, for
example, of the order of 0.002 inch.
The present invention provides for particular energization of the
antenna hereof and, referring to FIG. 2, it will be seen that arms
22 and 23 are electrically connected together as by a connection 31
and that arms 25 and 26 are electrically connected together as by a
connection 32. Energization of the antenna is then accomplished by
application of high-frequency energy between the connections 31 and
32, as schematically illustrated by the generator 33. It will be
seen that this then leaves intermediate spiral antenna arms 24 and
27 electrically unconnected and these are thus parasitically
excited by current flowing in the other arms of the antenna. It
will be realized that parasitic excitation of antenna elements is
well known in the art.
It can be established that with the antenna configuration of FIG. 2
and the type of energization employed therein, there will be
radiated from the antenna electromagnetic energy from Modes 1 and 5
with no radiation occurring from Modes 2, 3 or 4. The foregoing can
be established theoretically by a consideration of current vectors
and a determination therefrom that Mode 2, Mode 3 and Mode 4
currents are multiplied by vanishing coefficients with only Mode 1
and Mode 5 excitation currents being multiplied by finite
coefficients. While this is advantageous over conventional spiral
antennas, the present invention proceeds further to suppress Mode 5
radiation, as described below, to then consequently attain
substantially pure Mode 1 radiation to achieve operation over a
frequency band of approximately 4:1.
Mode 5 radiation is herein suppressed by the utilization of
absorbers or resistors particularly located with respect to the
spiral arms. It can be established that Mode 1 radiation occurs
substantially within a central area of the antenna of FIG. 2, as
generally indicated by the dotted line 36 therein. This area has a
circumference of .lambda. which is the wavelength of the highest
operating frequency of the antenna and thus the radius of the
circular area is .lambda./2.pi.. Mode 5 radiation will begin to
occur radially outward from a circular area having a circumference
of approximately 4.lambda. with full development of this mode at a
circumference of 5.lambda.. The present invention thus proceeds,
for example, as illustrated in FIG. 3 to provide an absorber of
high-frequency radiation 41 in engagement with the antenna in the
Mode 5 region thereof. As noted above, the Mode 5 region commences
radially outward from a circular area having a circumference of
approximately 4.lambda. which then is equivalent to a radius of
2.lambda./.pi. or about 0.6.lambda.. Thus the radius of the inner
circumference of the absorber 41 is approximately 0.6.lambda.
wherein again .lambda. is the wavelength at the highest operating
frequency of the antenna.
As a practical matter the radial extent of the absorber 41 may be
as large as desired but, at any rate, it should extend radially
outward sufficiently to encompass the entire Mode 5 region which
extends outwardly to between 0.8.lambda. and 0.9.lambda.. The
actual physical extent of the antenna arms 22 to 27 radially
outward from the center of the antenna may be limited to the
above-noted 0.6.lambda. radius where resistive termination is
provided as set forth below, or, alternatively, the arms may
continue further out from the center. It is noted that the absorber
41 is formed of a material having a high loss tangent such as, for
example, materials sold under the trademark "Eccosorb" such as
"Eccosorb" LS 26, "Eccosorb" AN 72 through AN 79 and "Eccosorb" NZ.
Referring further to FIG. 3, it is noted that the antenna is
mounted above a ground plane 42 which may, for example, be planar
or, if desired, may be formed of a conical shape in accordance with
antenna practices. Antenna energization is herein accomplished by a
conventional balun 43 feeding the antenna from a microwave
generator, in the instance of a transmitting antenna. It is to be
appreciated that the antenna of the present invention may be
operated at a variety of different frequencies but it is
particularly useful in the VHF and UHF region. As an example, an
antenna in accordance with the present invention designed to
operate at a minimum frequency of 100 MHz. would have a diameter of
the order of 3 to 4 feet and might have a ground plane spacing of
only an inch to 11/2 inches rather than the normal .lambda./4
because of space limitations, for example.
As noted above, the present invention proceeds to suppress Mode 5
radiation either by the utilization of an absorber or by resistive
termination of the arms. Referring to FIG. 4 there will be seen to
be schematically illustrated the six-arm antenna of the present
invention having the arms physically terminated at a distance
radially outward from the center of the antenna that is
substantially the above-noted 0.6.lambda.. At the outer end of each
arm there is provided a resistor 46 connected between the end of
the arm and the ground plane 42. This then provides a return path
for Mode 5 current so that same does not reflect from the ends of
the spiral arms, and again this configuration of the present
invention provides a substantially pure Mode 1 radiation. It will
be appreciated that the embodiments of FIGS. 3 and 4 are electrical
equivalents insofar as the objects of the present invention are
concerned.
It has been noted above that, in order to preclude or suppress Mode
5 radiation, there shall be employed either an absorber or
resistors located at an appropriate radius of the antenna. This
radius has been calculated above as a minimum of 0.6.lambda. but it
is to be appreciated that this dimension may be somewhat increased
to increase the antenna bandwidth at the low frequency end, for it
is radially outward of such distance that Mode 5 intensive
radiation occurs. Thus, for example, it is quite practical to place
the resistors 46, for example, at a radial distance outward from
the center of 0.8.lambda.. It is also to be particularly noted that
the presence of the ground plane, even disposed immediately behind
the antenna, is not deleterious to operation of the antenna in the
manner described above. Prior art limitations of radiation pattern
fluctuations for frequency bandwidths in excess of 2:1 are overcome
by the present invention.
* * * * *