U.S. patent number 3,832,717 [Application Number 05/231,673] was granted by the patent office on 1974-08-27 for dish reflector for a high gain antenna.
Invention is credited to Robert B. Taggart, Jr..
United States Patent |
3,832,717 |
Taggart, Jr. |
August 27, 1974 |
DISH REFLECTOR FOR A HIGH GAIN ANTENNA
Abstract
A dish reflector for a high antenna formed by a plurality of
generally triangular petals joined edgewise to form a
quasi-paraboloid configuration.
Inventors: |
Taggart, Jr.; Robert B.
(Mountain View, CA) |
Family
ID: |
22870213 |
Appl.
No.: |
05/231,673 |
Filed: |
March 3, 1972 |
Current U.S.
Class: |
343/840;
343/915 |
Current CPC
Class: |
H01Q
15/162 (20130101) |
Current International
Class: |
H01Q
15/14 (20060101); H01Q 15/16 (20060101); H01q
015/20 () |
Field of
Search: |
;343/840,912,915 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lieberman; Eli
Attorney, Agent or Firm: Fihe; Paul B.
Claims
What is claimed is:
1. A dish reflector for a high-gain antenna which comprises
a plurality of generally triangular reflective petals and
means connecting said petals in edgewise overlapping relation to
form a quasi-paraboloid with a line extending centrally outward
through each petal being of generally parabolic form and a
transverse line being substantially rectilinear,
said connecting means including a plurality of connecting members
joining the overlapping edges of said petals through registered
holes therein at predetermined dispositions which define the
ultimate assembled quasi-paraboloid conformation of the
reflector.
2. A dish reflector according to claim 1 wherein
the generally parabolic curvature of each petal outwardly is such
that the phase errors of reflected electromagnetic energy at the
focus of the quasi-paraboloid are minimized.
3. A dish reflector according to claim 1 which comprises
a rigid rim connected to the exterior edges of said petals to
provide structural rigidity.
4. A dish reflector according to claim 3 wherein
said rim includes a plurality of rim segments slotted to receive
the outer edges of said petals and joined at the extremities by
angular corner brackets.
5. A dish reflector according to claim 1 wherein
said petals, prior to connection by said connecting means, are in
the form of flat sheets of flexible material.
6. A dish reflector according to claim 1 wherein
said petals are formed of flexible material.
Description
FIELD OF THE INVENTION
The present invention relates generally to antennas, and more
particularly, to a dish reflector for a high-gain antenna.
The invention described herein was made in the performance of work
under a NASA contract and is subject to the provisions of Section
305 of the National Aeronautics and Space Act of 1958, Public Law
85-568 (72 Stat. 435/ 42 U.S.C. 2457).
BACKGROUND OF THE INVENTION
A high-gain antenna is an obvious necessity to provide an
intelligible signal when the received electromagnetic energy is at
a relatively low power level. For example, an ordinary television
antenna having relatively low-gain characteristics is perfectly
satisfactory to produce intelligible sound and a clear television
picture when located within line of sight of a conventional
television transmitting station. On the other hand, a television or
other communication signal transmitted from a satellite in orbit
obviously arrives at an intercepting antenna with a relatively low
power level of electromagnetic energy wherefore the use of a
high-gain antenna is imperative. Commonly, such a high-gain antenna
takes the form of a relatively large size paraboloid reflector
which receives the radiated electromagnetic energy over its entire
surface and in accordance with the general reflective
characteristic of a paraboloid, reflects such energy to a collector
located at its focal point.
Recently, proposals for the wide dissemination of educational
information to remote areas have included the provision of a
plurality of television receivers arranged in such remote areas to
receive the television signal emanating from a satellite. The
number and remote locations of these plural receiving stations
present practical problems in the shipping, local installation and
cost. More particularly, both the size and shape of a true
paraboloid do not lend themselves readily to mass production
techniques; thus the cost is high. If a unitary structure, shipping
and handling are a problem; if composed of a plurality of compound
curvature sections, yet added cost and assembly complexity
appear.
SUMMARY OF THE PRESENT INVENTION
Accordingly, it is the general objective of the present invention
to provide a high-gain antenna which incorporates a dish reflector
formed from a number of parts capable of fabrication by mass
production techniques wherefore the costs are minimized and the
elements can readily be shipped in their disassembled form in a
relatively compact light weight package but subsequently assembled
and installed in operating condition quickly, easily, and with
assurance of high-gain performance.
Generally, the dish reflector is formed by the assembly of a
plurality of generally triangular reflector petals in substantially
edgewise, abutting relationship to form a dish in the form of a
quasi-paraboloid. Generally the term, "quasi-paraboloid," refers to
a dish reflector structure wherein a section line extending
outwardly from the center of the antenna through the center of one
of the petals has an approximate parabolic configuration whereas a
section line transverse to such outwardly extending line remains
substantially rectilinear. More particularly, the generally
paraboloid curvature of each individual petal outwardly from the
center of the reflector dish is determined by the precise positions
of connection of adjoining petals and is designed to minimize the
phase errors resultant from the departure of the reflector
conformation from that of a true paraboloid.
In order to simplify and reduce manufacturing costs of the dish
reflector, each of the petals is initially formed, in one case, by
a simple blanking operation, in a flat, generally triangular form
from sheet aluminum, steel, or other material having a highly
reflective surface and in particular being capable of bending
during assembly to form the ultimate quasi-paraboloid shape. During
the blanking operation, holes are formed along the edges of the
petals in predetermined calculated disposition so that upon
subsequent assembly of the petals in edgewise abutting relation
through the use of nuts and bolts, pop rivets, or other connecting
means, the desired quasi-paraboloid conformation will automatically
be achieved thus eliminating the need for any skill or technical
know-how on the part of the person assembling the structure.
Preferably, rim segments are arranged to receive the outer edges of
the triangular petals during installation and adjacent rim segments
are in turn joined by the simple bolted connection of angular
corner brackets thereto so as to function as assembly jigs during
the assembly operation and to subsequently function as a rigid
exterior rim structure for the dish reflector enabling it to
withstand mechanical shock and also enabling appropriate mounting
of the dish reflector in the desired disposition for optimum
reception of the electromagnetic radiation.
Obviously, the disassembled petals, rim segments, and corner
brackets can be shipped in a rather compact package even though the
ultimate size of the assembled dish reflector is relatively large,
yet upon arrival, use of but simple tools by a relatively unskilled
person enables erection of the dish reflector in a period of less
than two hours. Because of the pre-established petal dimensions and
the holes therein which control the configuration of the assembled
reflector, the desired high-gain is assured.
The quasi-paraboloid configuration can obviously be obtained in
other specific fashions, one example being the edgewise connection
of a plurality of generally triangular reflective petals to
preformed, rigid ribs projecting radially in a generally parabolic
configuration, enabling the elimination of the exterior rim
segments.
BRIEF DESCRIPTION OF THE DRAWINGS
The stated objective of the invention and the manner in which it is
achieved as summarized hereinabove will become more readily
apparent from a perusal of the following detailed description of
exemplary embodiments of the invention illustrated in the
accompanying drawings wherein:
FIG. 1 is a perspective view of a microwave antenna incorporating a
dish reflector in accordance with the present invention,
FIG. 2 is an enlarged, fragmentary, sectional view taken along line
2--2 of FIG. 1 illustrating certain structural details of the dish
reflector,
FIG. 3 is another enlarged, fragmentary, sectional view taken along
line 3--3 of FIG. 1 illustrating yet further structural
details,
FIG. 4 is an exploded view of the parts indicating the manner of
assembly of the dish reflector of FIG. 1,
FIG. 5 is a three-axis diagram explanatory of the manner in which
gain of the reflector is maximized, and
FIG. 6 is an exploded, perspective view similar to FIG. 4 of the
parts of a modified dish reflector embodying the invention.
DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS OF THE
INVENTION
With initial reference to FIG. 1, a high-gain antenna is
illustrated and includes in accordance with the present invention,
a dish reflector 10 whose interior surface is formed from highly
reflective material, and specifically has the conformation of a
quasi-paraboloid which conformation will be more precisely defined
hereinafter. Three supporting legs 12 project upwardly from a rigid
base 14 to engage and support the rim of the dish reflector 10 in
proper orientation so that the Z axis of the quasi-paraboloid, as
indicated in FIG. 1, is directed towards a satellite or other
source of radiation which is to be reflected by the reflector
towards a suitable collector 16 supported by suitable arms 18
projecting upwardly and inwardly from spaced points on the rim of
the reflector so that such collector will reside also on the Z axis
and more particularly at the focal point of the quasi-paraboloid so
that, as will be explained in greater detail hereinafter, and as in
the case of true paraboloid reflectors, the reflected
electromagnetic energy will be focused at such collector 16 whose
output in turn after appropriate electronic processing is fed
through a feed line indicated at 20 to a conventional television
set (not shown). It will be obvious that the collected energy can
alternatively provide an input signal to a sound receiver or other
form of electronic equipment and such receiving equipment forms no
part of the present invention, in and of itself. Furthermore, as
will be apparent, a simple electronic reversal enables delivery of
energy to the antenna dish for transmission rather than reception
of electromagnetic energy.
As specifically illustrated in FIG. 1, the dish reflector 10 is
formed by ten petals 22 of highly reflective material, each petal
subtending an angle of 36.degree. at its central apex and curving
outwardly so that in central section through its altitude defines
substantially a parabola, as shown in FIG. 2. A section line at
right angles or transverse to the altitude of each triangular petal
22 on the other hand is rectilinear as shown in FIG. 3 so that
slight deviations from a true paraboloid result. The described and
illustrated conformation of all of the reflector petals 22 is the
same and the totality of the conformation of the 10 petals is
encompassed by the mentioned term, "quasi-paraboloid."
Preferably, the individual petals 22 are formed from rather thin
and flexible aluminum sheet (e.g., 0.040 inch) and to add
structural rigidity to the arrangement, the outer edge or base of
each triangular petal is supported in a slot 24 at one side of a
boxlike rim segment 26 which is preferably formed as an extruded
aluminum section (see FIG. 4) and the closely abutting ends of
adjoining rim segments 26 are in turn joined rigidly by angular
corner brackets 28 which encompass the adjacent rim segments and
are joined to the rim segments and the outer corners of the petals
22 by suitable nuts and bolts indicated at 30. In turn, the
adjoining edges of the petals 22 have a plurality of holes 32 at
spaced intervals therealong and are arranged in overlapping
relation as shown in FIG. 3 so that they can be joined by the
application of pop rivets 34, as shown, or alternatively by any
other form of connecting means such as a simple nut and bolt
arrangement.
Preferably, as illustrated in FIG. 4, each of the individual,
generally triangular petals 22 is initially formed by blanking in
essentially a flat configuration, but since it is formed from
slightly flexible material such as the thin aluminum mentioned
hereinabove, each petal is capable of being bent in single
curvature so that the altitude of the assembled triangular petal
will approximate the parabolic configuration described hereinabove
and shown in FIG. 2, while retaining a rectilinear disposition in
the transverse direction as shown and described in connection with
FIG. 3. The desired configuration is obtained in accordance with
the present invention by precisely positioning the holes along the
adjacent edges of the petal sections so that when the pop rivets 34
are applied thereto, the individual petals 22 are bent to the
desired singly curved conformation.
The assembly operation is extremely simple once the petals 22 have
been so formed with the required exterior dimensions and the
desired hole dispositions. Initially, two of the rim segments 26
are assembled with the angular corner bracket 28 and two adjacent
petals 22 are then slipped into the adjoining rim segments so as to
lie in edgewise overlapping relationship. The bolts 30 are manually
applied to the bracket segments and other corners of the petals.
The first pop rivet 34 is then applied to the outermost,
overlapping holes 32 of the two petals, the desired registration of
the holes being readily attained by a slight bending of the
adjacent petals. Thereafter, additional pop rivets 34 or other
connecting means are applied in succession to the registering holes
32 in the adjacent petals 22 and upon completion of the riveting
operation, the desired quasi-paraboloid configuration is attained.
It is to be particularly noted that the bracket 28 and rim segments
26 function, during such assembly operation, as assembly jigs to
facilitate ease and rapidity in the assembly of the dish
reflector.
When the assembly is completed, even though the petals 22
themselves are relatively thin material, the rim segments 26 and
brackets 28 joined thereto form a mechanically rigid structure so
that the assembled dish reflector 10 will retain its shape
regardless of weather conditions or mechanical shock.
In view of the fact that the assembled dish reflector 10 is a
quasi-paraboloid, the path lengths of radiation from a plane wave
front reflected at different points to the focus will have regular
variations in comparison to the corresponding path lengths
utilizing a true paraboloid. Such differences in path lengths will
in turn result in slight phase errors of the reflected
electromagnetic energy, but by suitable design criteria to be
described in detail hereinafter, these phase errors are minimized
so that the realizable gain of the ten petal antenna as
specifically described hereinabove is reduced by no more than a
fraction of a decibel below that achievable by a perfect
paraboloid.
More particularly, and with reference to the diagrammatic showing
of FIG. 5, the distance traveled bu an electromagnetic wave from an
XY plane 36 through the focal point 38 of the quasi-paraboloid will
initially travel a distance [F - Z (y)] to a point 40 on the
reflective petal 22 and will thereafter travel from this point 40
to the focal point 38 a distance, L = ([F - Z (y)].sup.2 + x.sup.2
+ y.sup.2).sup.1/2, the total distance, d, being equal to the sum,
[F - Z(y)] + ([F - Z(y)].sup.2 + x.sup.2 + y.sup.2).sup.1/2. It
being known that the distance from a plane through the focus to a
perfect paraboloid and thence to the focal point is equal to 2F (F
being the focal distance as indicated) in accordance with the
general definition of a paraboloid, the difference in distance
which we will refer to as the phase error distance will be (2F -
d). In order to minimize the phase error as desired, it is merely
necessary then to determine the amount of bending of the petal 22
to provide a dimension Z.sub.min (y) such that the quantity,
##SPC1## is a minimum, r.sub.o being the radius of the antenna, and
w(y) the half-width of a single petal.
Knowing the value Z.sub.min (y), it is then but a simple geometric
transformation to find the precise shape of a petal 22 and the hole
dispositions to produce the requisite amount of bending to provide
Z.sub.min (y) and the consequent minimized phase error. By way of
example, in one particular dish reflector designed for operation at
2.62 GHz with a reflector diameter of approximately 7 feet, the
individual petals 22 as stamped in their flat triangular form had
an altitude of 43.5 inches and the precise X and Y dimensions of
the individual petal holes, as indicated in FIG. 4, were as follows
measured from the center or apex of the triangular petal
outwardly:
X Y 0.487 0.500 1.462 3.504 2.437 6.516 3.412 9.546 4.386 12.598
5.361 15.677 6.255 18.531 7.229 21.680 8.123 24.606 9.017 27.575
9.910 30.589 10.804 33.655 11.697 36.768 12.509 39.656 13.322
42.587
the mechanical tolerances in the hole dispositions was maintained
at 0.005 inch which is well within the capability of standard mass
production blanking techniques and with this particular reflector
configuration, an antenna gain of 32 dB was attained which is but
0.9 dB below that of a perfect paraboloid. It will be apparent that
if the dish reflector is made with an increased number of sections,
yet higher gain can be realized, but in view of the close
approximation to that of a perfect paraboloid with use of but 10
petals the described structure was considered entirely adequate and
of course enables the assembly operation to proceed quite rapidly,
and as previously mentioned, such assembly can be achieved by an
unskilled laborer in less than 2 hours, and the resultant reflector
dish has excellent gain.
The number of petals can accordingly be changed without departing
from the spirit of the invention and other changes such as
integrating the rim segments with the petals will similarly suggest
themselves. Additionally, the petals and supports therefor can be
considerably modified while retaining the quasi-paraboloid
conformation. By way of example, in FIG. 6, petals 42 formed of
expanded metal which is flexible and highly reflective are joined
at their edges by machine screws 44 to radially extending parabolic
ribs 46 formed from rigid metal straps with suitable threaded holes
therein. A radial section through each petal 42 is substantially
parabolic but a transverse section is substantially rectilinear as
in the first embodiment so that the simple structural but excellent
gain characteristics are again achieved.
Additional modifications and/or alterations can obviously be made
without departing from the spirit of the invention. Accordingly,
the foregoing description of but two embodiments of the invention
is to be considered as purely exemplary and not in a limiting
sense, and the actual scope of the invention is to be indicated
only be reference to the appended claims.
* * * * *