U.S. patent number 3,805,268 [Application Number 05/116,691] was granted by the patent office on 1974-04-16 for antenna-polarization means.
This patent grant is currently assigned to General Electric Company. Invention is credited to Pope Patterson Britt.
United States Patent |
3,805,268 |
Britt |
April 16, 1974 |
ANTENNA-POLARIZATION MEANS
Abstract
A polarization sensitive phase shifter is applied to selected
portions of the aperture of a reflecting antenna so as to produce
similar primary and cross-polarized radiation phase patterns.
Inventors: |
Britt; Pope Patterson (Utica,
NY) |
Assignee: |
General Electric Company
(Utica, NY)
|
Family
ID: |
22368652 |
Appl.
No.: |
05/116,691 |
Filed: |
December 31, 1970 |
Current U.S.
Class: |
343/756; 342/188;
343/909; 342/153; 343/840 |
Current CPC
Class: |
H01Q
15/22 (20130101); H01Q 25/001 (20130101); H01Q
19/028 (20130101) |
Current International
Class: |
H01Q
19/02 (20060101); H01Q 15/22 (20060101); H01Q
19/00 (20060101); H01Q 25/00 (20060101); H01Q
15/14 (20060101); H01q 019/06 (); H01q
015/22 () |
Field of
Search: |
;343/753,756,909,840 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Tubbesing; T. H.
Claims
What is claimed as new and desired to be secured by Letters Patent
of the
1. In a radar antenna, a polarization selective antenna
illumination phase shifter comprising:
polarization modifying means having portions placed in registration
with portions of an antenna in which a principal polarization
vector representation of antenna illuminating differs from a
cross-polarization
2. In a parabolic reflector antenna, means for eliminating
cross-polarized return comprising:
selective phase-shifting means for shifting the phase of one
component of returned radiation 180.degree., said phase-shifting
means including portions in registration with first and second
opposite quadrants of said
3. The arrangement of claim 2 in which said phase shifting means
is
4. The arrangement of claim 3 in which said phase-shifting means is
of parabolic contour and spaced one-quarter wavelength from said
reflector.
5. The arrangement of claim 2 in which said phase-shifting means is
planar, disposed substantially perpendicularly to the boresight of
said antenna, and on the opposite side of the feed of said antenna
from said reflector.
6. An antenna comprising, in combination:
a. a feed for receiving radiation;
b. a reflector for focusing radiation on said feed; and
c. selective phase shifting means for converting the phase
distribution of one component of antenna illumination, said
selective phase shifting means including a portion in registration
with a portion of said reflector in which a principal polarization
vector representation of antenna illumination differs from a
cross-polarized vector representation of
7. An antenna according to claim 6 in which said selective phase
shifting
8. An antenna according to claim 6 in which said selective phase
shifting means is disposed on the opposite side of said feed from
said reflector.
9. An antenna comprising in combination:
a. a surface for illumination by radiation; and
b. selective phase shifting means for converting the phase
distribution of one component of antenna illumination, said
selective phase shifting means including a portion in registration
with a portion of said surface in which a principal polarization
vector representation of antenna illumination differs from a
cross-polarization vector representation of antenna illumination.
Description
BACKGROUND OF THE INVENTION
This invention relates to antennas in reflected wave object
detection systems and more particularly to antennas including means
for manipulating the polarization of radiation incident
thereupon.
In radar systems such as monopulse radar, pulses are transmitted,
and echo pulses which bounce off an object in the radar field of
view are received by a system's antenna. One form of typical
antenna comprises a reflector and an element upon which reflected
radiation is focused, commonly called a feed. Information is
derived from the echo pulse to determine such information as the
object's angular position with respect to the boresight of the
radar system. A common form of radar tracking comprises the
comparison of a sum signal of the system to a defference signal.
These signals are derived from the well-known sum and difference
radiation patterns of a radar antenna, and may be referred to as
the principal patterns. Where a curved reflecting antenna is used,
cross-polarization of reflected signals is produced in response to
reflection from a curved surface. The feed thus responds to
cross-polarized patterns as well as the principal patterns. The
linearity of tracking of an object by a monopulse radar system is
adversely affected by cross-polarization. If the magnitude of the
cross-polarized phase patterns are great enough with respect to the
magnitude of the principal patterns, the radar system may even be
totally deceived as to the position of the object it is tracking.
Various techniques for reducing the adverse effects of
cross-polarized returns have been utilized. One such approach is
the use of an antenna having as long a focal length as possible,
thus reducing the curvature of the antenna over the portion from
which returned signals are reflected. Another approach is the use
of a polarization screen. Both of these techniques reduce the
amplitude of the cross-polarized radiation. Neither technique,
however, eliminates the effects of cross-polarization. More
specifically, neither technique converts the pattern of the
cross-polarized returns to that of the principal return. In
addition, cross-polarization may occur due to reflection from the
object. No prior technique exists for providing similar primary and
cross-polarized phase patterns in response to reflections from an
object.
SUMMARY OF THE INVENTION
It is, therefore, an object of the present invention to provide a
means in a monopulse radar system to eliminate the effects of
cross-polarization and provide for smoother and more accurate angle
tracking by a monopulse radar system.
It is a more specific object of the present invention to provide a
means for converting the cross-polarized portion of the return to a
feed in a monopulse antenna into the same pattern as the principal
return.
It is a specific object of the present invention to eliminate the
effects of cross-polarization due to curvature of a radar antenna
reflector.
It is also an object of the present invention to eliminate the
effect of cross-polarization due to reflection of radar pulses from
an object or active cross-polarization deception jamming.
Briefly stated, in accordance with the present invention, there is
provided an antenna for use in a radar system in which a
polarization sensitive phase shifter is applied to selected
portions of the aperture of the reflecting antenna so as to produce
similar principal and cross-polarized radiation phase patterns.
BRIEF DESCRIPTION OF THE DRAWINGS
The foregoing objects and features of novelty are embodied in the
invention which is pointed out with particularity in the claims
forming the concluding portion of the specification. The invention
both as to its organization and manner of operation, may be further
understood by reference to the following description taken in
connection with the following drawings.
FIG. 1 is a pictorial representation of a use of the present
invention;
FIGS. 2a, 2b and 2c are representations of the principal
polarization phase, cross-polarization phase, and their resulting
composite pattern for an antenna, respectively;
FIG. 3 is a diagram illustrating a typical antenna aperture field
distribution, resolved into principal and cross-polarized
components.
FIG. 4 is a further representations of components of radiation
illustrated in FIG. 3;
FIGS. 5 and 6 are illustrative embodiments of the present
invention; and
FIG. 7 is a chart useful in understanding the operation of the
present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Basic Theory
In FIG. 1, an object 1 is tracked by a radar system 2 having an
antenna 3 including a feed 4 and a reflector 5. The radar system 2
sights along a boresight 6. For purposes of illustration, the size
of the object 1 is greatly exaggerated with respect to the
reflector 5. The return from the object 1 in actuality subtends a
small portion of the curvature of the reflector 5, and in return is
indicated by the reference numeral 7 in FIG. 1.
The angular response to the sum and difference patterns in a system
in which there are only principal radiation patterns is illustrated
in FIG. 2a. In FIG. 2b, the angular response of a system to a
cross-polarized radiation is illustrated. FIG. 2c illustrates total
response of an antenna. Magnitude of response is plotted against
arbitrary units, the waveforms of FIGS. 2a-2c being nominal
patterns. The magnitude of the waveforms in FIG. 2b compared to
those of FIG. 2a varies with the degree of cross-polarization.
Where the magnitude of the cross-polarized pattern is small with
respect to the principal pattern, conventional tracking by
comparing the sum signal to the difference signal may be
accomplished. As the magnitude of the cross-polarized pattern
increases, such tracking may become impossible. Cross-polarization
produced by reflection from an antenna reflector is illustrated in
FIGS. 3 and 4. FIG. 3 illustrates a typical antenna aperture field
distribution. The principal components are the vertical vectors and
the cross-polarization components are the horizontal vectors. The
theory of the aperture-field distribution is explained at Section
12.3 of Silver, Microwave Antenna Theory and Design (McGraw-Hill
Book Company, New York, 1949). In order to transform the
illustration of FIG. 3 into a more workable form, the illustrations
of FIG. 4 and the following convention are used.
The vectors of FIG. 3 are lumped into quadrants. If the phase of
the vector in the vertical illumination, i.e., the principal
polarization points upward, a plus sign is used. In the case of the
cross-polarized, or horizontal component, a plus is used if the
vector points to the right, and a minus is used if the vector
points to the left. Thus, the representation in illustration a of
FIG. 4 represents the principal polarization sum pattern, each
quadrant containing a plus sign. In addition, using the
above-described convention, the representation illustration b of
FIG. 4 is obtained for the cross-polarization sum pattern in which
plus signs are in the upper left and lower right quadrants, and
minus signs are in the upper right and lower left quadrants.
Construction of the Preferred Embodiments
In accordance with the present invention, a polarization sensitive
phase shifter is applied to selected portions of the aperture of
the reflecting antenna 3 to produce similar response from the
principal and cross-polarized radiation phase patterns. A first
embodiment is illustrated in FIG. 5 in which illustration a is a
section taken along the line I--I of the elevation of illustration
b. The same reference numerals are used to denote elements
corresponding to those of FIG. 1.
In the embodiment of FIG. 5 a filter 10 comprising a polarization
sensitive phase shifter is interposed between the feed 4 which is a
means for receiving radiation and the reflector 5. The filter 10
may take any well-known form, for example, a wire grid, dielectric
grid, or any other well-known form. The filter 10 is oriented to
affect only the cross-polarized components of the radiation
incident upon the reflector 5. The dimensions are chosen such that
the phase shift provided will convert the radiation pattern a of
FIG. 4 to that of pattern b. This may be accomplished using
well-known electro magnetic radiation theory. For example, in the
specific embodiment of FIG. 5, a wire grid is used, and the wires
are substantially horizontally disposed to match the polarization
of incident radiation. The distance between the grid wires is less
than one-quarter wave-length and more than one-eighth wavelength of
the reflected radiation. The grid 10 is spaced one-quarter
wavelength from the reflector 5 and conforms to its contour. The
grid 10 reflects radiation. In the present embodiment, the desired
phase shift may be achieved over a bandwidth equal to 10 percent of
the operating frequency of the radar system 2. A transmissive
filter could also be placed between the feed 4 and reflector 5.
In the embodiment of FIG. 6, a filter 11 which transmits radiation
comprising first and second pairs of wire grids 12 and 13 is
provided on the opposite side of the feed 4 from the reflector 5.
In this particular embodiment, the wires within a grid are spaced
by three-eighths of a wavelength, and the first and second grid
pairs 12 and 13 have their facing sides spaced by one-quarter
wavelength. Two pairs of grid wires are used since this arrangement
is more convenient for achieving 180.degree. phase shift. Here,
again, the frequency bandwidth over which the phase shift filter 11
is effective is approximately 10 percent.
It should be noted that the present invention may be applied to
other forms of antennas. The shape of a filter such as the filter
10 or 11, i.e., the portions which must be in registration with
corresponding portions of an antenna reflector, is dictated by
antenna geometry. Well-known theory may be used to calculate the
primary and the cross-polarized patterns. The shape of a filter
necessary to convert the cross-polarized radiation to a pattern
similar to the primary radiation is a shape including filter
portions in registration with portions of an antenna in which
vector representations of the primary cross-polarized patterns of
the antenna illumination differ. Well-known electromagnetic
radiation theory may be used to provide any number of different
sorts of planar or other filters to provide the necessary phase
shift. Thus while two pairs of planar grids are provided in the
specific embodiment of FIG. 6, other numbers of differently shaped
grids could be employed.
The filter comprises polarization modifying means in the form of
selective phase shifting means. The filter is selective in that it
only affects one of the two components of returned radiation. In
the embodiments illustrated, only the cross-polarized component is
phase shifted.
Of course, while the filters 10 or 11 are oriented to convert the
cross-polarized radiation pattern to the primary pattern, they may
be oriented to do the opposite. In either case, a smooth response
such is that of FIG. 2a is provided, rather than that of FIG.
2c.
OPERATION
In FIG. 7, desired distributions of a two lobe antenna system are
illustrated in column a, columns b and c illustrate the radiation
phase distribution for vertical and horizontal components of
radiation; and columns d and e represent the radiation phase
distribution of the vertical and horizontal components for a
corrected antenna using the embodiment of FIGS. 5 or 6. The symbol
for the well-known pattern to which each representation in FIG. 7
corresponds is marked next to the representation. The azimuth
difference pattern is denoted .DELTA.Az and the elevation
difference pattern is denoted .DELTA.E1. It will be noted that the
corrected antenna patterns agree with the desired distribution
patterns. A convention similar to that of FIG. 4 is used. Upward
pointing vectors of the vertical component correspond to a plus,
and downward pointing vectors correspond to a minus for the
vertical component. For the horizontal component, arrows pointing
to the left correspond to a plus, to the right correspond to a plus
and the arrows pointing to the left correspond to a minus.
In order to illustrate the operation of the present embodiment, the
response to the sum signal as illustrated in FIG. 6 is examined.
Note that the horizontal component representation, the upper right
and lower lefthand vectors, point to the left, corresponding to
phase shifting means. For example, filter 10 of FIG. 5 or filter 11
of FIG. 6 operates only on these portions of the antenna to change
the cross-polarized component orientation by 180.degree. to provide
the uncorrected horizontal representation to the corrected
horizontal representation. The invention operates similarly on the
other representations derived from the returned signal.
The present invention is especially useful in situations in which
the cross-polarization is produced by the object 1 (FIG. 1). Where
a reflected signal is cross-polarized due to reflection from an
object on the boresight 6, for example, the return will be the same
as the primary return of an object which is off boresight. Thus a
radar system tracking a target producing cross-polarized reflection
would respond as though the target were off boresight.
Consequently, a tracking radar would be deceived into scanning a
portion of the sky other than where the object 1 is. The present
invention eliminates this problem.
In addition, the invention provides for smoother monopulse tracking
even where the cross-polarization is due only to the geometry of
the antenna reflector. As seen in FIG. 2a, a smoother sum to
difference ratio is obtained than for the representation of FIG.
2c.
The present invention is not limited to the standard lobe radar,
but may also be incorporated in conical scan-lobe on receive only
(LORO) and conical scan radar systems. The invention may also be
practiced in accordance with the above teachings on non-reflective
antennas such as aperture and lens antennas and various types of
arrays.
* * * * *