Scanning antenna including a dielectric waveguide and a rotatable cylinder coupled thereto

Information

  • Patent Grant
  • 6211836
  • Patent Number
    6,211,836
  • Date Filed
    Friday, July 30, 1999
    25 years ago
  • Date Issued
    Tuesday, April 3, 2001
    23 years ago
Abstract
A scanning antenna includes a cylinder coupled to a dielectric waveguide into which an electromagnetic wave is launched. The cylinder includes rows of features such as recesses or stubs of differing vertical dimensions and periods. The cylinder when rotated directs the coupled radiation over a range determined by the periods of features in the rows and the rotation of the cylinder. Both transmitters and receivers are described. Benefits are described in connection with different cross section geometries to the waveguide. Also, both linear and circular polarization operations are described.
Description




FIELD OF THE INVENTION




This invention relates to scanning antennas and more particularly to such antennas which steer electromagnetic radiation from a dielectric waveguide in directions determined by the geometry of a rotatable cylinder (or drum) coupled to it.




BACKGROUND OF THE INVENTION




U.S. Pat. No. 5,572,228 issued Nov. 5, 1996 and U.S. Pat. No. 5,815,124 issued Sep. 29, 1998 describe evanescent coupling antennas which employ rotatable cylinders placed in close proximity to a dielectric rod waveguide and operative to radiate the coupled energy in directions determined by the period of features on the surface of the cylinder. By defining rows of features where the features of each row have a different period, the radiation can be directed in a plane over a range determined by the different periods and by rotating the cylinder about an axis parallel to the axis of the waveguide.




The features on the cylinder surface, of each of the antennas disclosed in the above-noted patents, comprise conductor strips of like thickness and at a given and different spacing in each row about the cylinder. The operation of such an antenna as well as the advantages in such applications as vehicle collision avoidance systems for automobiles and aircraft and the like are described in the above-noted patents which are incorporated herein by reference.




BRIEF DESCRIPTION OF THE INVENTION




It has been discovered that by including features which vary in vertical dimension as well as in period from row to row, greater control over the transmitted (or received) waveform, arbitrary polarization, and increased gain are achieved. Accordingly, generic features of embodiments of this invention include a dielectric rod waveguide (DRW) with an electromagnetic wave launched therein and a rotatable cylinder including rows of generally circular recesses of different depths or generally circular stubs of different heights where the period in each row varies in a prescribed manner. The cylinder is rotated to scan that electromagnetic radiation over a lateral space determined by the varying feature periods and by the rotation of the cylinder.











BRIEF DESCRIPTION OF THE DRAWING





FIG. 1

is a schematic representation of a beam steering antenna including a dielectric waveguide and a spinning drum in accordance with the principles of this invention;





FIGS. 2 and 3

are schematic representations of a dielectric rod waveguide and a coupled row of the drum of

FIG. 1

including recesses and stubs in the drum surface respectively;





FIGS. 4



a


,


4




b


,


4




c


,


4




d


,


4




e


,


4




f


,


4




g


,


4




h


,


4




i


,


4




j


and


5




a


,


5




b


,


5




c


,


5




d


,


5




e


,


5




f


,


5




g


and


5




h


are charts of stub and recess profiles and of waveguide profiles for the drum and waveguide of

FIG. 1

, respectively;





FIGS. 6



a


,


6




b


,


6




c


,


6




d


,


6




e


and


6




f


are charts of feature configurations and gap variations for the drum of

FIG. 1

in accordance with the principles of this invention;





FIGS. 7



a


and


7




b


are graphs of different wave patterns for different gap profiles between the waveguide and drum of

FIG. 1

;





FIG. 8

is a schematic representation of an antenna as in

FIG. 1

also including a parabolic reflector;





FIG. 9

is a graph of the beam profile radiated by the antenna of

FIG. 8

;





FIGS. 10 and 12

are schematic representations of the antenna of

FIG. 1

with a parabolic reflector and a moving planar reflector and of a duplex system using such reflectors in both a transmitting mode and a receiving mode;





FIG. 11

is a schematic representation of the antenna of

FIG. 1

with an additional planar, leaky dielectric waveguide; and





FIG. 13

is a schematic representation of a beam steering antenna with a switching mechanism.











DETAILED DESCRIPTION OF AN ILLUSTRATIVE EMBODIMENT OF THIS INVENTION





FIG. 1

shows a dielectric rod waveguide


11


placed in close proximity to a cylinder or drum


12


. Drum


12


includes rows of recesses or holes where the holes of each row have a different period. A periodic set of holes in a representative row is shown in the figure as PSH line


14


. It can be seen from the figure that the features have similar X and Y dimensions.




In operation, a signal is launched into waveguide


11


by signal generator


16


and drum


12


is rotated about an axis


17


by drum driver


18


. The drum is made of metallic material and is coupled to the evanescent field generated by the signals in the waveguide in a manner fully described in the above-noted patents. Signal generator


16


and driver


18


are controlled by controller


19


in a well understood manner.




The apparatus of

FIG. 1

is operative to radiate signals in lateral directions dictated by the period of the features (recesses) in each row of drum


12


as that row comes into alignment with the waveguide. As the drum spins, the direction of the (beam) radiation changes. By choosing the periods of the features in the rows carefully and by spinning the drum, the lateral space over which the beam is broadcast is determined. The direction of the beam radiated as the waveguide is in alignment with each of the consecutive rows of features is determined by the equation:




Coupling angle (for both transmitting and receiving):






φ=arcsin (


C/V




ph




−λ/A


)






where C is the velocity of light, V


ph


is the phase velocity of the electromagnetic wave in the waveguide. λ is the wavelength of the electromagnetic wave in free space and Λ is the period of the features in the row. The direction of the radiated beam is indicated in

FIG. 1

by the solid arrow


20


and the broken arrows φ


1


and φ


2


which indicate the plane of the beam.





FIG. 2

shows an illustrative section


21


of drum


12


of

FIG. 1

with a row of holes aligned with waveguide


11


. The radiated beam is indicated by arrow


22


and the plane of radiation is indicated by curved arrow


23


.

FIG. 3

shows an arrangement analogous to that shown in

FIG. 2

except that the features of the illustrative section of the drum comprise stubs rather than holes.




The features of the various rows of the apparatus of

FIG. 1

may comprise holes, recesses or stubs.

FIG. 4



a


demonstrates a cross section through an illustrative feature as indicated by plane


25


. FIGS


4




b


through


4




j


illustrate nine alternative cross sections arranged in three rows. The top row as viewed shows illustrative stub profiles


27


,


28


, and


29


. The middle row shows recesses


30


,


31


, and


32


. The bottom row shows holes


33


,


34


, and


35


.




Not only may the feature profile be different, the waveguide cross section also may be different.

FIGS. 5



a


through


5




h


show illustrative cross sections for the waveguide. It is clear from the figures that the waveguide cross section may be disk-shaped (


51


), donut-shaped (


52


), square-shaped (


53


), diamond-shaped (


55


) (viz. square-shaped but rotated 90 degrees with respect to the coupled drum). The cross section also may be oval (


56


), T-shaped (


57


) or rectangular (


58


). The drum material may comprise quartz, Teflon™ polyethylene, polystyrene, sapphire, or microwave ceramic and may be embedded in foam or other material with a small dielectric constant and loss.





FIGS. 6



a


through


6




f


show an illustrative set of waveguide (


11


) and drum (


12


) variations. The gap between the drum and the waveguide may vary as shown at


60


and


61


in the

FIGS. 6



a


and


6




b


, the representation at


60


illustrating the apparatus with recesses


62


. The representation at


61


illustrates the apparatus with stubs


63


. Further, the recess depth may vary as shown at


65


or the stub height may vary as shown at


66


as shown in

FIGS. 6



c


and


6




d


. Also, the recess or stub diameter may vary as shown at


67


and


68


, respectively as shown in

FIGS. 6



e


and


6




f


.





FIG. 7



a


is a graph of gap δ in mm versus X, the position along the waveguide of

FIG. 6



a


at


60


.

FIG. 7



b


is a graph of power db versus the angle of the radiated beam. Curves in

FIG. 7



b


correspond to the different gap arrangements of

FIG. 7



a.


For a constant gap represented by horizontal line


70


in

FIG. 7



a,


the power curve is as represented by curve


71


in

FIG. 7



b.


For a straight line variation of about three millimeters at the end of the drum to about one millimeter at a six inch position as represented by line


74


in

FIG. 7



a,


the power curve is as represented by curve


72


in

FIG. 7



b.


A gap of from five millimeters at the end of the drum to one millimeter at the six inch position varying as represented by the curve


75


in

FIG. 7



a,


produces a power curve represented by curve


73


in

FIG. 7



b.






Parabolic reflectors are conveniently used with the scanning antenna of

FIG. 1

in accordance with the principles of this invention for directing the beam from the antenna in elevation planes that are at angles to the azimuth X-Y plane.

FIG. 8

shows one such apparatus with an oval-shaped waveguide


80


and a drum


81


with rows of recesses. The parabolic reflector is designated


82


.

FIG. 9

is a graph of power (dB) versus azimuth in degrees showing the far-field beam pattern. The power is −49 at an azimuth at −35 degrees, −45 at −10 degrees, and zero at the reference X-Y plane.




Two-dimensional beam steering can be achieved with the apparatus of

FIG. 1

by employing a parabolic reflector which is in a fixed position and a planar reflector which moves.

FIG. 10

illustrates such an arrangement. Specifically,

FIG. 10

illustrates apparatus comprising a waveguide


90


having an illustrative oval cross section. The apparatus also includes a (spinning) drum


91


and a parabolic reflector


92


. A planar reflector


93


rotates back and forth from a position in the plane of the axis of the drum as shown through an angle O to a position parallel to that axis. The directions of the beam are dictated by the positions of reflector


93


. The solid arrows


94


,


95


, and


96


indicated the beam path from waveguide


90


to reflector


92


to reflector


93


in one position of reflector


93


; the broken arrows


97


,


98


, and


99


indicate the beam path for a second position of reflector


93


.





FIG. 11

illustrates a waveguide


100


and an adjacent spinning drum


101


with rows of recesses. The apparatus also includes a planar, “leaky”, dielectric waveguide


102


which has a printed circuit dipole grating formed on it. The grating is represented by dashed lines


103


,


104


,


105


, and


106


. Waveguide


102


is positioned in the path of the beam radiated from drum


101


as shown. The plane in which radiation is directed from waveguide


102


is represented at


107


. This embodiment of the invention is particularly attractive when space is limited.




The apparatus represented in

FIG. 1

is described in terms of a transmitting antenna. The apparatus also is useful as a receiving antenna.

FIG. 12

illustrates one transmitting and receiving embodiment, both the transmitting antenna and the receiving antenna employing parabolic reflectors and a moving planar reflector. Specifically, the transmitting antenna of

FIG. 12

includes a waveguide


11


and a spinning drum


112


with rows of recesses as shown. Antenna


112


also includes a parabolic reflector


113


and a moving planar reflector


114


. The receiving antenna includes a waveguide


116


, a spinning antenna


117


, a parabolic reflector


118


, and a moving planar reflector


119


. An electromagnetic wave launched into waveguide


111


as indicated by arrow


120


is directed as indicated by the arrows


121


and


122


and received by the receiving antenna as indicated by solid arrows


126


and


127


to generate an electromagnetic wave as indicated by arrow


128


.




Duplex beam steering can also be achieved without the two moving planar reflectors


114


and


119


of

FIG. 12

with a shared spinning drum using two dielectric waveguides each with an associated parabolic mirror instead.




A problem might appear when an antenna in accordance with the principles of the invention is designed to operate at relatively large scanning angles. The problem is overcome by using a switch to feed the antenna from opposite ends of the dielectric rod waveguides (DRW). Such an arrangement is illustrated in

FIG. 13

where a switch


130


is operative to feed signals alternatively to end


131


and end


132


of the waveguide


133


as illustrated in the figure.




The number of beam positions in a lateral plane is determined by the number of rows of features on a drum. The number of rows on a drum determines the resolution. Antennas in accordance with the invention have a drum length of four to twenty inches with the spacing between rows of one wavelength. A drum may have twenty to eighty rows of features with the spacing between features of two to five millimeters. The drum typically is rotated at from one revolution per minute to twenty revolutions per second.




The use of stubs, recesses, or holes on the drum provides for increased efficiency per unit length, arbitrary polarization and for an increased coupling efficiency. Specifically, it has been found that when both, the waveguide and features have cross-section with rotating symmetry of 4


th


order (square, round, octagonal etc.) the antenna can operate with arbitrary polarization, i.e. the main lobe of the antenna pattern for each fixed drum position is the same for any polarization. This includes such fundamental polarizations as horizontal and vertical polarizations, and right-hand and left-hand circular polarizations.



Claims
  • 1. A scanning antenna comprising a rotatable cylinder having an outer surface and a first axis, an elongated dielectric waveguide having a second axis, said cylinder and said waveguide being located in positions closely spaced from one another such that electromagnetic signals in said waveguide are coupled to said cylinder, said cylinder comprising metallic material and including at said outer surface thereof a plurality of parallel rows of surface features, each surface feature in each of said plurality of rows having like X and Y dimensions, each of said surface features in a row having a first range of X and Y dimensions different from the range of said dimensions in every other one of said rows.
  • 2. A scanning antenna as in claim 1 wherein the features of each of said plurality of rows are of vertical dimensions to change the distances between said cylinder and said waveguide over the length of said waveguide.
  • 3. An antenna as in claim 1 wherein each of said surface features comprises a stub.
  • 4. An antenna as in claim 3 wherein each of said stubs in a row has a different height.
  • 5. An antenna as in claim 1 wherein each of said surface features comprises a recess in said outer surface.
  • 6. An antenna as in claim 5 wherein each of said recesses in a row has a different depth.
  • 7. An antenna as in claim 1 also including means for rotating said cylinder about said first axis.
  • 8. An antenna as in claim 7 wherein said first and second axes are parallel to one another and said outer surface and said second axis also are parallel to one another.
  • 9. An antenna as in claim 7 wherein said outer surface and said second axis define a varying gap therebetween.
  • 10. An antenna as in claim 1 wherein said first and second axis are parallel to one another.
  • 11. An antenna as. in claim 1 wherein said waveguide has a circular cross section.
  • 12. An antenna as in claim 1 including means for introducing electromagnetic signals to said waveguide.
  • 13. An antenna as in claim 12 wherein said means comprises a switch for introducing said signals from either end of said waveguide controllably.
  • 14. An antenna as in claim 1 wherein all of said surface features in a row have the same X and Y dimensions.
  • 15. An antenna as in claim 14 wherein the surface features of each row of said plurality of rows have circular cross sections.
  • 16. An antenna as in claim 1 also including a reflector of a material and in a fixed position to reflect a beam emanating from said cylinder.
  • 17. An antenna as in claim 16 wherein said reflector comprises a parabolic reflector.
  • 18. An antenna as in claim 17 also including a second reflector.
US Referenced Citations (5)
Number Name Date Kind
2993205 Cooper Jul 1961
4001835 Dover et al. Jan 1977
5014069 Seiler et al. May 1991
5572228 Manasson et al. Nov 1996
5815124 Manasson et al. Sep 1998