U.S. patent number 3,747,116 [Application Number 05/248,706] was granted by the patent office on 1973-07-17 for radiating cone antenna.
Invention is credited to Robert A. Milam.
United States Patent |
3,747,116 |
Milam |
July 17, 1973 |
RADIATING CONE ANTENNA
Abstract
A radiating cone antenna having a conical reflecting surface and
a parabolic reflecting surface in spacial relationship and
surrounding said conical reflecting surface. A linear directive
radiator is positioned at the focus of the parabolic reflecting
surface and energy from the radiator is reflected from the
parabolic reflecting surface to the conical reflecting surface
which, in turn, reflects the energy in a constant phase front.
Inventors: |
Milam; Robert A. (Indianapolis,
IN) |
Family
ID: |
22940317 |
Appl.
No.: |
05/248,706 |
Filed: |
April 28, 1972 |
Current U.S.
Class: |
343/837; 343/840;
343/872 |
Current CPC
Class: |
H01Q
19/18 (20130101) |
Current International
Class: |
H01Q
19/10 (20060101); H01Q 19/18 (20060101); H01q
019/10 () |
Field of
Search: |
;343/837,838,840,914,872
;240/41.1,41.35C,41.37,41.35R,41.35,44.25 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lieberman; Eli
Claims
I claim:
1. A parabolic reflector antenna comprising:
a conical reflector,
an annular parabolic reflector surrounding said conical reflector
with the focal axis of said parabolic reflector being perpendicular
to the altitude of said conical reflector, and
an antenna feed positioned at the focus of said parabolic reflector
whereby energy radiating from said antenna feed is reflected from
said parabolic reflector to said conical reflector which reflects
energy along a line of constant phase.
2. A parabolic reflector antenna as set forth in claim 1 wherein
the configuration of said conical reflector is a right angle
cone.
3. A parabolic reflector antenna as set forth in claim 1 wherein
the apex of said conical reflector is located on the focal axis of
said parabolic reflector.
4. A parabolic reflector antenna as set forth in claim 1 wherein
the forward edge of said parabolic antenna extends beyond said
antenna feed.
5. A parabolic reflector antenna as set forth in claim 4 wherein
the forward edge of said parabolic antenna is covered with a flat
radome.
Description
STATEMENT OF GOVERNMENT INTEREST
The invention described herein may be manufactured and used by or
for the Government of the United States of America for governmental
purposes without the payment of any royalties thereon or
therefor.
BACKGROUND OF THE INVENTION
The present invention relates to a radio frequency antenna and more
particularly to an antenna having first and second reflecting
surfaces for transmitting energy in a constant phase front.
Antennas having parabolic reflectors are widely used for directing
beams of radio frequency energy. Generally, a beam of energy from a
radiator is projected at a small angle to the axis of a parabolic
reflector and the radiator is located on the axis at substantially
the focal point of the reflector. The radiating system including
the parabolic reflector is arranged to be oriented both in
elevation and in azimuth by suitable mechanical means so that the
axis of the paraboloid can be directed at a target. One such
antenna system is shown and described in U.S. Pat. No. 2,541,806,
entitled, "Beam Antenna System," which issued Feb. 13, 1951, to
Burton P. Brown, Jr. In this patented device, the antenna member is
a dipole which is located at or near the focus of a paraboloid
reflector and the axis of the reflector passes through the dipole
at or near the midpoint thereof. A source of signal energy is
provided for exciting the dipole and this source produces pulses of
oscillations of high frequency energy. Means is provided for
shifting the antenna beam pattern from coincidence with the axis of
the reflector and for rotating the antenna assembly so that a
rotating beam will be projected.
SUMMARY OF THE INVENTION
The present invention relates to a radio frequency antenna for
reflecting energy along a constant phase front. A conical
reflecting surface is provided and a parabolic reflecting surface
is spaced from and surrounds the conical reflecting surface. A feed
mechanism is positioned at the focus of the parabolic reflector and
energy from the feed mechanism is reflected from the parabolic
reflector to the conical reflector. The conical reflector, in turn,
reflects energy along a line of constant phase, which is the basic
criteria for maximum antenna gain.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a diagrammatic view illustrating the use of a parabolic
antenna of the prior art;
FIG. 2 is a diagrammatic view illustrating the use of a parabolic
antenna of the present invention;
FIG. 3 is a side view showing a parabolic antenna of the present
invention in an annular configuration;
FIG. 4 is a top view of the parabolic antenna shown in FIG. 3 of
the drawing; and
FIG. 5 is a sectional view of a preferred embodiment of the present
invention.
DESCRIPTION OF THE PREFERRED EMBODIMENT
Referring first to FIG. 1 of the drawing which illustrates a prior
art configuration of a parabolic reflector, the point of feed, A,
is located at the focus of the parabolic curve 11 and waves which
are reflected from the parabola parallel with the focal axis arrive
at line C with equal phase. The path lengths of AB.sub.1 C.sub.1,
AB.sub.2 C.sub.2, AB.sub.3 C.sub.3, and AB.sub.4 C.sub.4 are equal.
The use of parabolic reflectors in the antenna art is more fully
described on pages 336-350 of the text, "Antennas," by John D.
Kraus, McGraw-Hill Book Company, Inc. (1950).
Referring now to FIG. 2 of the drawing, the present invention
utilizes a parabolic reflector wherein the reflector is positioned
so that its focal axis is parallel to the line C, which represents
a constant phase front. Electromagnetic energy emitted from point
source A, which is located at the focus of the parabolic curve 11,
is reflected from a reflector represented by curve 11 to a second
reflector represented by straight line 12. In FIG. 2 of the
drawing, the path lengths of AB.sub.1 B'.sub.1 C.sub.1, AB.sub.2
B'.sub.2 C.sub.2, and AB.sub.3 B'.sub.3 C.sub.3 are equal.
By rotation of curve 11 and line 12 about axis D, parabolic surface
13 is generated which has point A as a radiating feed point, as
shown in FIGS. 3 and 4 of the drawing. Feed point A is located as
the focus of surface 13. Surface 14, which is generated by the
rotation of line 12, is a cone. By way of example, angle .theta.
might be 90.degree., and surface 14 would be a right angle cone. It
can be seen that the altitude of the cone is perpendicular to the
focal axis of parabolic surface 13.
Referring now to FIG. 5 of the drawing, there is shown a feed
element 15 which is energized from circular waveguide 16. It is
desirable to locate the feed point at the apex of the cone surface
14, with the apex also being the focus for parabolic surface 13.
Feed element 15 might be any conventional rear feed primary antenna
and, by way of example, might be crossed dipoles, spirals, horns,
or reflectors fed by waveguides.
Numerous advantages can be obtained by using the antenna system of
the present invention. In many feeds, the rays of electromagnetic
energy which are more rearwardly directed are at greater field
strength. For example, referring to FIG. 5 of the drawing, ray F
would have a greater field strength than ray G. When ray F is
reflected from conical surface 14, however, it will be further from
feed 15 than ray G. Thus, rays reflecting from surface 14 will be
at a lower intensity as the feed is approached. This permits larger
feed structures to be used without having the usual severe
shadowing which results in lower gain and also pattern distortion
is conventional parabolic reflector antennas. Also the impedance
mismatch resulting from energy reflecting back into the feed is
minimized, or eliminated and, therefore, larger RF bandwidths can
be achieved.
The conical shape of surface 14 provides a convenient mechanical
support of large feed structure and either all or part of a
transmitting and receiving RF system can be packaged in the inner
cone space. The advantages to be gained from this arrangement are
the elimination of RF rotary couplings, and shortening of transmit
and receiver RF lines thereby resulting in minimum energy loss and
improved noise figure. If desired, the outer surface of reflector
17 can be made spherical and positioned in a socket type of gimbal
for direction purposes.
As shown in FIG. 5 of the drawings, the forward edge of reflector
17 can extend beyond the end of feed mechanism 15. Thus reflector
17 prevents unwanted electromagnetic radiation from either being
transmitted or received to the side of the antenna. The ordinary
"spillover" effect common to a conventional parabolic antenna is
avoided thereby providing a very "low noise" antenna having high
efficiency. Additionally, a flat sheet of dielectric material 18
can be fitted to the front of reflector 17 to serve as a radome and
to permit a simple means of pressurization, if desired.
The embodiment shown in FIGS. 3, 4, and 5 of the drawing can be
elliptical in shape or of other configuration without departing
from the scope of the invention. Also this invention could apply
equally well to a visible spectrum and to other RF spectrums which
use a parabolic reflector in receiving or transmitting energy. By
way of example, the present invention could be used with a
carbon-arc search light whereby energy would not be redirected back
to the lamp thereby providing for cooler operation.
It can thus be seen that the present invention provides an improved
parabolic reflector antenna which does not have many of the
inherent disadvantages common to presently used reflector
antennas.
* * * * *