US2604595A - Antenna reflector - Google Patents

Antenna reflector Download PDF

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Publication number
US2604595A
US2604595A US618531A US61853145A US2604595A US 2604595 A US2604595 A US 2604595A US 618531 A US618531 A US 618531A US 61853145 A US61853145 A US 61853145A US 2604595 A US2604595 A US 2604595A
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United States
Prior art keywords
reflector
edges
antenna
horizontal
frequencies
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Expired - Lifetime
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US618531A
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Trevor H Clark
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STC PLC
Federal Telephone and Radio Corp
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Standard Telephone and Cables PLC
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Priority to US618531A priority Critical patent/US2604595A/en
Priority to ES181969A priority patent/ES181969A1/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q19/00Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic
    • H01Q19/10Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using reflecting surfaces

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  • This inventionf relates to radiant energy antenna reflectors and more'particularly to reflectors for use with directional antenna arrange ments in a certain frequency range.
  • the reflector When a directionally sensitive radiation characteristic is desired in an antenna system it is generally necessary to provide one or more reflectors in conjunction with a given antenna.
  • the reflector In order for the reflector to be efflcient, that is to operate with a high reflection coefficient, the reflector should be. designed to. possess high conductivity and for a given frequency should have dimensions such that it is resonant in the onehalf wavelength mode. This characteristic is acceptable when very high frequencies are used. However, if a wide band characteristic is required of-the reflector it should'be of suflicient size as to be substantially non-resonant throughout the operating range.
  • the physical dimensions of the reflector more and more approach a length corresponding to one-half wavelength until'one of the portions of the reflector corresponding to the polarization of the radiation becomes resonant with a respective wavelength. This causes the production of standing Waves along these resonant portions of the reflector with a consequent increase in the back radiation of the reflector.
  • an increase in back radiation that is, sensitivity on both sides of the reflector is a cause for ambiguity of indications.
  • a still further object is to provide a reflector which may be made non-resonant for vertically polarized or for horizontally polarized radiation.
  • Still another object is to provide a reflector which is non-resonant in any of its portions over a wide band of frequencies.
  • I provide a reflector comprised of a rectangular metallic sheet in conjunction with a given antenna the horizontal and/or vertical edges of which approach or may be less than the one-half wavelength for a given low frequency of the band dealt with.
  • the formation of standing waves I provide conductive extensions of the edges of the reflector which correspond to the respective polarization of the radiation to which the antenna is exposed.
  • I provide extensions for the edges as well as for intermediate portions of the reflector parallel to the edges whereby the reflector is effective in avoiding the formation of standing waves on any part of its surface which may be resonant over a broad band of frequencies.
  • Fig. 1 represents a plan view of a reflector in' accordance with my invention designed'for' horizontally polarized radiation;
  • Fig. 2 represents a reflector constructed in accordance with the invention for vertically polarized radiation
  • Figs. 3 and 4 are variations of a reflector designed for a wide frequency band
  • Fig. 5 is a plan view of a reflector, certain edges of which have been lengthened in another way.
  • the reflector of Fig. 1 comprises a rectangular metallic sheet I having a horizontal dimension given by one of the horizontal edges 2 and a vertical dimension which is given by one of its vertical edges 3.
  • the horizontal edges have been provided with horizontal extension bars 4, 5, 6 and 1 which extend the horizontal dimensions to some value In.
  • a dipole antenna 8 designed for operation over a relatively'wide band of frequencies is suitably mounted in front of the reflecting surface I.
  • the antenna is a horizontal dipole, particularly sensitive to waves of a horizontal polarization.
  • the horizontal reflector dimension may be a half wavelength or less.
  • the extensions added thereto are such that In is greater than a half wavelength at the operative frequencies so that resonance effects to horizontal polarized energy will be substantially eliminated.
  • Fig. 2 the reflecting surface I has been provided with vertical extensions 9, H), II and I2 of its vertical edges 3. These extensions are such that Iv is greater than a half Wavelength so that vertical polarized resonance effects will In accordance 3 be substantially reduced or eliminated. It should be clear that if the antenna is designed to operate at both horizontal and vertical polarization, two sets of extensions such as shown in Figs. 1 and 2, may be used on the same reflector.
  • the reflector of Fig. 3 which is intended to operate over a wide band, instead of having individual bar-like extensions of its edges, has been provided with wing-like extensions I3, l4, l and I6, which have their maximum dimension in line with the edges 2 and are reduced to zero in line with the intermediate horizontal portionsof the reflector. This construction will serve further to reduce resonance effects which might occur intermediate the edges of the reflector.
  • a reflector is shown provided with extensions similar in effect to those of Fig..3.
  • individual bars as at I! and I3 are attached to oppositely disposed edges of reflector l parallel to the plane of polarization.
  • the bars I! and l8 progressively assume a smaller size from the outer portions of said edges toward the center portions of said edges of the reflector.
  • FIG. 5 Another system for obtaining an eflective extension of the resonant edges of a reflector has been suggested in Fig. 5 where the horizontal edges have been increased in length by being serrated as at I9 and 20.
  • 'A reflector for use with an antenna adapted to operate on a given band of frequencies and with a predetermined polarization, comprising a member having a plane reflecting surface and a plurality of conductive bar-like extension elements extending from opposite edges of said member in the same plane as said reflecting surface and parallel to the plane of polarization, said elements having divers lengths and spacedly mounted from each other along the opposite edges of said member, whereby said reflector is rendered substantially aperiodic at the operating frequencies in said band.

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  • Aerials With Secondary Devices (AREA)

Description

' Jul 22, 1952 H, CLARK 2,604,595
ANTENNA REFLECTOR Filed Sept. 25, 1945 INVENTOR. TREVOR H. CZ HRK ATTORNEY Patented July 22, 1952 oNiTEostares PATENT orrics "f 7 2,604,595 I ANTENNA REFLECTOR Trevor 'H. ClarkfBoonton, N. J., assignor to Federal -Telephone' and Radio Corporation,
New York, N. Y., a corporation of Delaware Application September 25, 1945, Serial No.618 ,53 1
v I v .1
This inventionfrelates to radiant energy antenna reflectors and more'particularly to reflectors for use with directional antenna arrange ments in a certain frequency range.
When a directionally sensitive radiation characteristic is desired in an antenna system it is generally necessary to provide one or more reflectors in conjunction with a given antenna. In order for the reflector to be efflcient, that is to operate with a high reflection coefficient, the reflector should be. designed to. possess high conductivity and for a given frequency should have dimensions such that it is resonant in the onehalf wavelength mode. This characteristic is acceptable when very high frequencies are used. However, if a wide band characteristic is required of-the reflector it should'be of suflicient size as to be substantially non-resonant throughout the operating range. As the wavelength increases, the physical dimensions of the reflector more and more approach a length corresponding to one-half wavelength until'one of the portions of the reflector corresponding to the polarization of the radiation becomes resonant with a respective wavelength. This causes the production of standing Waves along these resonant portions of the reflector with a consequent increase in the back radiation of the reflector. When a radiation characteristic sensitive in only one direction is desired, an increase in back radiation, that is, sensitivity on both sides of the reflector is a cause for ambiguity of indications.
It is accordingly an object of this invention to reduce back radiation sensitivity of an antenna reflector for comparatively low frequencies in a given band.
It is another object to reduce the formation of standing waves along resonantly dimensioned portions of the reflector.
It is another object to provide a reflector which is non-resonant in any one of its portions with respect to the lowest frequency in a given band.
A still further object is to provide a reflector which may be made non-resonant for vertically polarized or for horizontally polarized radiation.
Still another object is to provide a reflector which is non-resonant in any of its portions over a wide band of frequencies.
In accordance with certain features of the invention, I provide a reflector comprised of a rectangular metallic sheet in conjunction with a given antenna the horizontal and/or vertical edges of which approach or may be less than the one-half wavelength for a given low frequency of the band dealt with. In order to avoid 2 Claims. -(Cl. 250-33135) .1 2 the formation of standing waves I provide conductive extensions of the edges of the reflector which correspond to the respective polarization of the radiation to which the antenna is exposed. In accordance with another feature of the invention I provide extensions for the edges as well as for intermediate portions of the reflector parallel to the edges whereby the reflector is effective in avoiding the formation of standing waves on any part of its surface which may be resonant over a broad band of frequencies. with still another feature of this invention I provide an eifective extension of therespective edges of the reflector Without actually having to introduce a physical extension thereo These and other features and objects of'the invention will become more apparent uponthe consideration of the following detailed description of embodiments to be read in connection with the accompanying drawings in which:
Fig. 1 represents a plan view of a reflector in' accordance with my invention designed'for' horizontally polarized radiation;
Fig. 2 represents a reflector constructed in accordance with the invention for vertically polarized radiation;
Figs. 3 and 4 are variations of a reflector designed for a wide frequency band; and
Fig. 5 is a plan view of a reflector, certain edges of which have been lengthened in another way.
Referring to the drawings, the reflector of Fig. 1 comprises a rectangular metallic sheet I having a horizontal dimension given by one of the horizontal edges 2 and a vertical dimension which is given by one of its vertical edges 3. The horizontal edges have been provided with horizontal extension bars 4, 5, 6 and 1 which extend the horizontal dimensions to some value In. A dipole antenna 8 designed for operation over a relatively'wide band of frequencies is suitably mounted in front of the reflecting surface I. The antenna is a horizontal dipole, particularly sensitive to waves of a horizontal polarization. At the lower frequencies of the wave band the horizontal reflector dimension may be a half wavelength or less. The extensions added thereto are such that In is greater than a half wavelength at the operative frequencies so that resonance effects to horizontal polarized energy will be substantially eliminated.
In Fig. 2 the reflecting surface I has been provided with vertical extensions 9, H), II and I2 of its vertical edges 3. These extensions are such that Iv is greater than a half Wavelength so that vertical polarized resonance effects will In accordance 3 be substantially reduced or eliminated. It should be clear that if the antenna is designed to operate at both horizontal and vertical polarization, two sets of extensions such as shown in Figs. 1 and 2, may be used on the same reflector.
The reflector of Fig. 3, which is intended to operate over a wide band, instead of having individual bar-like extensions of its edges, has been provided with wing-like extensions I3, l4, l and I6, which have their maximum dimension in line with the edges 2 and are reduced to zero in line with the intermediate horizontal portionsof the reflector. This construction will serve further to reduce resonance effects which might occur intermediate the edges of the reflector.
In Fig. 4 a reflector is shown provided with extensions similar in effect to those of Fig..3. However, instead of continuous extension surfaces, individual bars as at I! and I3 are attached to oppositely disposed edges of reflector l parallel to the plane of polarization. The bars I! and l8 progressively assume a smaller size from the outer portions of said edges toward the center portions of said edges of the reflector.
Another system for obtaining an eflective extension of the resonant edges of a reflector has been suggested in Fig. 5 where the horizontal edges have been increased in length by being serrated as at I9 and 20.
While I have shown a few examples of how resonance may be avoided in a reflector for individual and wide band frequencies, it is to be noted that resonance may be eliminated in other ways analogous to the above. 1
While I have described above the principles of my invention in connection withspecific apparatus, it is to be clearly understood that this description-is made only. by way of example and not as a limitation on the scope of my invention as defined in the objects and the accompanyin laims.
;I claimr 1. 'A reflector for use with an antenna adapted to operate on a given band of frequencies and with a predetermined polarization, comprising a member having a plane reflecting surface and a plurality of conductive bar-like extension elements extending from opposite edges of said member in the same plane as said reflecting surface and parallel to the plane of polarization, said elements having divers lengths and spacedly mounted from each other along the opposite edges of said member, whereby said reflector is rendered substantially aperiodic at the operating frequencies in said band.
2. A reflector as claimed in claim 1, wherein said member comprises an element having oppositely disposed edges, each edge having a central portion and outer portions, said extension elements extending from both said edges, the longest of said extension elements attached adjacent the outer portions of said edges and the shortest of said extension elements attached adjacent the central portions of said edges, said extension elements of intermediate lengths being disposed in ascending order from the central portions of said edges in accordance with their length.
TREVOR H. CLARK.
REFERENCES CITED The following references are of record in the file of this patent:
UNITED STATES PATENTS Masters Aug. 30, 1949
US618531A 1945-09-25 1945-09-25 Antenna reflector Expired - Lifetime US2604595A (en)

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ES181969A ES181969A1 (en) 1945-09-25 1948-01-31 IMPROVEMENTS IN ANTENA REFLECTORS

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2644091A (en) * 1953-02-26 1953-06-30 Marvin P Middlemark High-frequency antenna
US2772413A (en) * 1956-03-30 1956-11-27 Trio Mfg Co Composite dipole multi-channel television antenna

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1745342A (en) * 1925-12-29 1930-01-28 Rca Corp Directive-projecting system of electric waves
US2026652A (en) * 1933-01-11 1936-01-07 Csf High frequency transmitter
US2049070A (en) * 1931-09-11 1936-07-28 Rca Corp Aerial system
US2181181A (en) * 1935-03-05 1939-11-28 Telefunken Gmbh Short wave reflector
US2199050A (en) * 1937-06-14 1940-04-30 Howard L Jenkins Antenna support
US2270965A (en) * 1939-06-30 1942-01-27 Rca Corp Ultra high frequency relay system
US2425303A (en) * 1943-05-26 1947-08-12 Rca Corp Antenna system for radio drift indication
US2434893A (en) * 1943-07-09 1948-01-27 Standard Telephones Cables Ltd Unidirectional antenna system
US2480154A (en) * 1945-01-27 1949-08-30 Rca Corp Antenna

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1745342A (en) * 1925-12-29 1930-01-28 Rca Corp Directive-projecting system of electric waves
US2049070A (en) * 1931-09-11 1936-07-28 Rca Corp Aerial system
US2026652A (en) * 1933-01-11 1936-01-07 Csf High frequency transmitter
US2181181A (en) * 1935-03-05 1939-11-28 Telefunken Gmbh Short wave reflector
US2199050A (en) * 1937-06-14 1940-04-30 Howard L Jenkins Antenna support
US2270965A (en) * 1939-06-30 1942-01-27 Rca Corp Ultra high frequency relay system
US2425303A (en) * 1943-05-26 1947-08-12 Rca Corp Antenna system for radio drift indication
US2434893A (en) * 1943-07-09 1948-01-27 Standard Telephones Cables Ltd Unidirectional antenna system
US2480154A (en) * 1945-01-27 1949-08-30 Rca Corp Antenna

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2644091A (en) * 1953-02-26 1953-06-30 Marvin P Middlemark High-frequency antenna
US2772413A (en) * 1956-03-30 1956-11-27 Trio Mfg Co Composite dipole multi-channel television antenna

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