U.S. patent number 3,641,579 [Application Number 04/807,603] was granted by the patent office on 1972-02-08 for frequency-independent icr antenna.
This patent grant is currently assigned to Textron Inc.. Invention is credited to George N. Voronoff.
United States Patent |
3,641,579 |
Voronoff |
February 8, 1972 |
FREQUENCY-INDEPENDENT IcR ANTENNA
Abstract
The invention provides interrupted coaxial-line radiators upon a
ground plane and arranged in a frequency-independent manner for
broadband radiation from a flush-mounted structure. The radiators
may be arranged in a log-periodic array or in a spiral array for
frequency-independent operation.
Inventors: |
Voronoff; George N. (San
Francisco, CA) |
Assignee: |
Textron Inc. (Belmont,
CA)
|
Family
ID: |
25196770 |
Appl.
No.: |
04/807,603 |
Filed: |
March 17, 1969 |
Current U.S.
Class: |
343/792.5;
343/846; 343/895 |
Current CPC
Class: |
H01Q
9/27 (20130101); H01Q 11/10 (20130101) |
Current International
Class: |
H01Q
9/27 (20060101); H01Q 11/10 (20060101); H01Q
11/00 (20060101); H01Q 9/04 (20060101); H01q
011/10 (); H01q 001/36 () |
Field of
Search: |
;343/767,771,792.5,895,908 |
References Cited
[Referenced By]
U.S. Patent Documents
|
|
|
3480961 |
November 1969 |
Copeland et al. |
|
Primary Examiner: Lieberman; Eli
Claims
I claim:
1. An improved antenna comprising an electrically conducting ground
plane, a plurality of interrupted coaxial-line radiators disposed
on said ground plane with the exterior of each radiator
electrically contacting said ground plane, said radiators being
disposed in frequency-independent array, and a pair of coaxial
cables disposed in adjacent parallel relation on said ground plane
and connected to separate radiators extending as stub branches from
said cables in log-periodic array on said ground plane for
supplying electrical energization to said radiators whereby
electromagnetic energy is unidirectionally radiated into space from
said radiators.
2. The antenna of claim 1 further defined by said cables carrying
electrical energization of opposite phase for supply to said
radiators.
3. The antenna of claim 1 further defined by each of said cables
having said stub branches extending from both sides thereof and
alternate branches of each extending across the adjacent cable as a
coaxial cable with the interrupted coaxial line commencing on the
opposite side of the cable crossed.
4. The antenna of claim 1 further defined by said antenna having
two mirror image portions with each including one of said cables
and each having branches extending alternately from opposite cable
sides, said branches comprising said interrupted coaxial line
radiators, and said portions being disposed with the cables thereof
in adjacent parallel relation so alternate branches from the
combination of portions extend outwardly on each side thereof from
different cables.
5. An improved antenna comprising an electrically conducting ground
plane, a plurality of interrupted coaxial-line radiators disposed
upon said ground plane in equiangular spirals with the exterior of
each radiator electrically contacting said ground plane, said
radiators being disposed in frequency-independent array, a pair of
coaxial cables connected to separate radiators at the center of
said spirals for supplying electrical energization thereto whereby
electromagnetic energy is unidirectionally radiated into space from
said radiators.
6. The antenna of claim 5 further defined by there being two spiral
arms of radiators and said arms being energized with signals of
like phase by said cables.
7. The antenna of claim 5 further defined by there being two spiral
arms of radiators and said arms being energized with signals of
180.degree. phase relationship by said cables.
Description
BACKGROUND OF INVENTION
Requirements for broadband radiation from antennas has led to the
development of what are generally termed "frequency-independent"
antennas. In general, characteristics of an antenna of a given
shape are dependent upon antenna dimensions measured in
wavelengths; thus antennas with several characteristic dimensions
are normally limited to operation within a fairly narrow band of
frequencies. In order to overcome this limitation, it is possible
to formulate antenna shapes described by angles rather than linear
dimensions, and, in practical applications, these antennas are
essentially independent of frequency for all frequencies above a
certain lower limit. This general class of antennas is herein
termed "frequency independent," and it is noted that this type of
antenna may be defined in terms of polar coordinates with input
terminals at the origin thereof wherein the antenna is bounded by
curves which are equiangular spirals. The form of the bounding
surfaces of such an antenna is fixed by the requirement that a
change in scale should be equivalent to a rotation in azimuth
angle, and this applies both to planar configuration and
three-dimensional shapes.
An alternative frequency-independent antenna configuration
comprises plane shapes that are essentially cross sections of the
general three-dimensional shape identified above. Although the
electrical properties of such antennas are not strictly frequency
independent, they do repeat periodically with the logarithm of the
frequency; consequently are generally termed "log-periodic"
antennas. For this type of antenna the frequencies for which the
structure has the same electrical properties are arranged in
geometrical progression. Many different log-periodic antenna shapes
are known, and various different log-periodic dipole arrays and
log-periodic slot arrays have been developed. Reference is made,
for example, to U.S. Pat. No. 2,989,749 setting forth one type of
antenna in accordance with this general proposition.
Further with regard to frequency-independent antennas, it is noted
that log-periodic structures formed as dipole arrays are basically
free-space antennas so as to be incapable of operation efficiently
against a ground plane. Log-periodic slot antennas, on the other
hand, require cavity backing, as set forth, for example, in U.S.
Pat. No. 3,218,644. While this general classification of antennas
will be seen to be highly advantageous, it is yet limited insofar
as low-profile or flush-mounted antenna structures are concerned.
The present invention does employ the principles of
frequency-independent antennas which may incorporate log-periodic
configuration but without the limitations noted above.
Further with regard to the propagation of electromagnetic waves,
there has been developed a class of radiators commonly denominated
as interrupted coaxial-line radiators or slotted TEM-line
radiators. In this respect, it is noted that the term "IcR" is
oftentimes employed as an identification of this type of radiator.
A slotted TEM-line antenna is basically a series-fed array of
electrically small radiating loop elements, and in practice this is
normally embodied as a coaxial line having the sheath thereof
transversely slotted along the length of the line to form the
radiating elements. The length of transmission line between slots
or radiating loops, as they may be termed, provides the requisite
phase delay between elements of the antenna. Characteristics of
this type of antenna have been developed by prior workers in the
field, and a brief description thereof is to be found, for example,
in IEEE transactions on antennas and propagation, Mar., 1969, page
260, as written by Mr. John R. Copeland. Radiation from this type
of antenna may occur from the slot and/or from the center conductor
at the slot but for convenience such is herein termed slot
radiation.
The present invention combines interrupted coaxial-line radiators
in frequency-independent antenna configuration to achieve results
unavailable with either alone. Although various antenna
configurations employed in the present invention are actually
approximations of two frequency independent shapes they are herein
denominated as frequency independent for convenience of
nomenclature.
SUMMARY OF INVENTION
In brief, the present invention provides a plurality of interrupted
coaxial-line radiators upon a ground plane and energized from input
coaxial lines with the radiators being oriented in
frequency-independent array upon the ground plane. Inasmuch as the
ground plane is an integral part of the IcR, it is not necessary to
back the structure with cavities; consequently, there is achieved a
low-profile frequency-independent antenna, particularly suited for
utilization upon aircraft, spacecraft and the like. In accordance
with one embodiment of the present invention, the radiators of this
antenna are arranged in a log-periodic fashion in two sections
energized with like voltages of opposite polarity to produce a
linear principle polarization action of electromagnetic radiation
in space. Another embodiment of this invention provides interrupted
coaxial-line radiators disposed in an equiangular or logarithmic
spiral or an Archimedean spiral with arms being energized at the
center of the spiral with like voltages of either the same or
opposite phase relationship to produce a conical circularly
polarized beam with a null along a central axis normal to the
ground plane, or a broad circularly polarized beam with a peak
along such axis.
The present invention is particularly directed to the provision of
a frequency-independent antenna structure of low-profile requiring
no cavity backing for unidirectional radiation. The invention is
applicable for mounting upon metallic nonplanar surfaces, such as
those of aircraft, missiles, and the antenna structure is
particularly useful in the VHF region.
DESCRIPTION OF FIGURES
The present invention is illustrated as to particular preferred
embodiments thereof in the accompanying drawings, wherein:
FIG. 1 is a partial side elevational view of an interrupted
coaxial-line radiator;
FIG. 2 is a transverse sectional view of an interrupted
coaxial-line radiator taken in the plane 2--2 of FIG. 1;
FIG. 3 is a plan view of a log-periodic antenna in accordance with
the present invention;
FIG. 4 is a schematic illustration of one section of the antenna of
FIG. 3; and
FIG. 5 is a perspective view of an Archimedean spiral antenna in
accordance with the present invention.
DESCRIPTION OF PREFERRED EMBODIMENTS
Considering first the general aspects of an interrupted
coaxial-line radiator, reference is made to FIGS. 1 and 2 of the
drawings. There is illustrated in these figures a conventional
coaxial transmission line 11 having a central conductor 12, and a
coaxial electrically conducting sheath 13. Many coaxial lines
employ a solid dielectric 14 between the central and outer
conductors thereof, and this may, for example, comprise solid
polyethylene dielectric. In accordance with the present invention,
the transmission line 11 has spaced slots 16 formed transversely
through the outer sheath of conductor 13, with the central
conductor 12 being continuous throughout the line. In addition to
the transmission line, as briefly described above, there is
provided an electrically conducting ground plane 21, upon which the
line is disposed, in electrical contact therewith. The slots 16 and
the center conductor 12 at these slots act as radiating elements,
and the slots may extend partially or entirely about the outer
conductor 13. In the illustrated embodiment, the slots are shown to
extend about an angle which is somewhat less than the entire
circumference of the outer conductor. Radiation from the line is,
in part, dependent upon the circumferential extent of the slots
therein, and, in addition, by forming the line as illustrated, it
is possible to readily attach the line to the ground plane, as by
solder or welds 22, because a part of the sheath extends
continuously along the ground plane.
Electrical energization is provided to the transmission line 11,
and electromagnetic radiation emanates from the slots 16 therealong
and from the center conductor exposed at these slots. A plurality
of factors are involved in the characteristics of such radiation,
as for example, the radii of the conductors, the slot width and
circumferential extent, as well as the voltage existing across the
slots and the distance between slots. Without entering into a
detailed discussion of this type of radiator, it is noted that the
radiation characteristics thereof are known in the art, and for
particular physical configuration can be calculated by conventional
theory. The slotted transmission line 11 is termed a slotted
TEM-line or an interrupted coaxial line radiator (IcR).
Referring now to FIGS. 3 and 4 of the drawing, there is illustrated
one preferred embodiment of the present invention, wherein
interrupted coaxial line radiators are employed, in accordance with
the present invention, as radiators in a log-periodic antenna
structure. The antenna is formed of two portions 31 and 32, with
these being fed by coaxial lines 33 and 34, respectively. The
coaxial lines 33 and 34 are mounted upon an electrically conducting
ground plane 36, and are fed or energized by signals of equal
amplitude but with 180.degree. phase relationship. Energization of
the coaxial lines may be accomplished from an appropriate
transmitter, or the like, 37, including means such as a hybrid
circuit for achieving the above-noted opposite phase relationship
of signals applied to the separate lines. The lines 33 and 34 are
appropriately terminated as by a matched load therebetween.
Each of the coaxial feedlines 31 and 32 is provided with
branch-slotted TEM lines. It is to be appreciated that inasmuch as
each portion may have a substantial number of branches, the
illustration of FIG. 3 is broken, so that only initial and terminal
branches are illustrated for compactness of illustration.
Referring to FIG. 4, there will be seen to be schematically
illustrated the orientation of branches of a single portion 31 of
the antenna. No attempt is made in FIG. 4 to show details of
structure, but instead, the line diagram thereof is intended only
to clarify the relative location and extent of the branches of the
section. In accordance with established theory of log-periodic
antennas, the portion 31 illustrated in FIG. 4 will be seen to have
a number of branches 41, 42, 43, 44, etc., extending from one side
of the feedline 34, and a number of intermediate branches 51, 52,
53, etc., extending from the other side of the feedline 34. Energy
is fed into the coaxial line 34 at the left thereof in the drawing
and propagates along the line as well as out the branch lines noted
above. As this energy passes through the branch lines,
electromagnetic energy thereof is radiated into space through the
gaps in the lines as described above.
The embodiment of the present invention illustrated in FIG. 3 has
the two portions 31 and 32 thereof formed as mirror images so that
the first branch lines of each extend in opposite directions from
each other and the second branch lines extend toward and across
each other. It is particularly noted that the branch lines of each
section alternate in their direction of extension from the central
feedline or coaxial cable thereof. It is also to be noted that in
accordance with the theory of log-periodic antennas the length of
successive branch lines 41 to 44, for example, increases
successfully from the feed end of the section, in somewhat the
manner as illustrated in FIG. 4. In certain respects this may be
likened to a log-periodic dipole array except that interrupted
coaxial radiators are employed in place of dipoles. Furthermore,
the sections 31 and 32 of the present invention are mounted upon a
conducting ground plane 36 in marked distinction to log-periodic
dipole antennas which operate as free-space antennas. In
circumstances where the antenna is not operated at too high a
frequency the crossing branches may be slightly offset to both pass
over the other coaxial line.
The theory of "frequency independency" of log-periodic antennas is
applicable to the present invention and consequently the
relationship of the branch lines of radiators of the present
invention is not further developed herein. It is, however, noted
that the nature of the radiation patterns and the radiation
intensity from individual branch lines depend upon the termination
of the end of the lines and the parameters of the gaps in the
radiators. The branches may be terminated as short circuits, as
illustrated, or alternatively may be open circuited or loaded. It
is also to be appreciated that the center conductor of the
interrupted coaxial line radiator need not be straight at the gaps
therein. The conductor may in fact be formed as a single or
multiple loop if desired in order to achieve additional control of
radiation properties. With regard to radiation pattern it is noted
that the principal polarization of the antenna of FIG. 3 is linear
and the direction thereof in space is parallel to the branches or
radiator lines. The orientation of principle polarization of the
antenna may be changed by changing the orientation of lines and in
this respect, it is noted that these lines or branches need not be
straight but may take other forms such as, for example, T-shaped or
L-shaped. It will be appreciated that once the desired radiation
characteristics of individual branches or radiator lines have been
established the overall antenna pattern may be synthesized by
well-known methods.
An alternative embodiment of the present invention is illustrated
in FIG. 5 wherein there is shown what may be termed an IcR
Archimedean spiral antenna. The antenna comprises a pair of
parallel spiral coaxial lines or radiators 61 and 62 disposed upon
a ground plane 63 in the form of an Archimedean spiral. The lines
61 and 62 are fed at the center of the spiral as by means of input
coaxial cables 64 and 66 from a suitable transmitter unit, not
shown. The two arms 61 and 62 of this spiral are formed as
interrupted coaxial line radiators, as indicated, with the input
portions 67 and 68 comprising impedance-matching sections. The arms
are energized from the center of the spiral, with energy then being
propagated outwardly along the two arms 61 and 62 to the outer ends
of the arms where they are appropriately terminated at a desired
impedance to to prevent reflection. The maximum spiral diameter is
limited, in accordance with established theory to the free-space
wavelength at lowest operating frequency divided by twice the
relative dielectric constant in the loaded coaxial lines. It will
be appreciated that Archimedean spirals are essentially frequency
independent and it is noted that while these types of antennas are
known in the art they have previously required cavity backing for
unidirectional radiation.
The two arms of the antenna of FIG. 5 may be fed with input signals
of the same or opposite phases depending upon the desired radiation
pattern from the antenna. Desired signal amplitude and phase
relationships may be achieved by utilization of a hybrid circuit at
the input, for example. In the instance wherein the two spiral arms
61 and 62 are fed in 180.degree. phase relationship the antenna
radiates a broad circularly polarized beam with its peak directed
along the axis normal to the ground plane. Alternatively, when the
two spiral arms 61 and 62 are energized with signals of the same
phase relationship the antenna radiates a conical circularly
polarized beam with a null thereof directed along the axis normal
to the ground plane.
In common with the embodiment of the invention illustrated in FIG.
4 and described above, the radiation patterns of the antenna of
FIG. 5 are essentially independent of frequency provided that the
gaps in the interrupted coaxial radiators radiate a proper amount
of power, as discussed above. This embodiment of the present
invention does provide unidirectional radiation through the use of
interrupted coaxial line radiators in a frequency-independent
array. In common with the above-described embodiment of the present
invention the present embodiment has the advantages of a low
profile and ability to conform to nonplanar surfaces and is
suitable for application in the VHF region.
* * * * *