US2452106A - Radio antenna - Google Patents

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US2452106A
US2452106A US654840A US65484046A US2452106A US 2452106 A US2452106 A US 2452106A US 654840 A US654840 A US 654840A US 65484046 A US65484046 A US 65484046A US 2452106 A US2452106 A US 2452106A
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antenna
transmission line
driven element
section
wavelength
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Gordon H Cotchefer
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q3/00Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
    • H01Q3/12Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system using mechanical relative movement between primary active elements and secondary devices of antennas or antenna systems
    • H01Q3/14Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system using mechanical relative movement between primary active elements and secondary devices of antennas or antenna systems for varying the relative position of primary active element and a refracting or diffracting device

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  • This invention relates to radio reception and transmission, and particularly to an antenna array suitable for both omnidirectional transmission and reception to and from nearby points, and unidirectional transmission and reception to and from distant points.
  • Radio antenna arrays now in common use are designed primarily for transmission and reception to and from distant points and are usually in the form of a series of parallel horizontal or vertical elements of equal length, one being the driven element to which the transmission line leading to the radio receiver or transmitter is attached,
  • the antenna array of this invention comprises a stationary vertical driven element having a height equal to at least two or any higher integral number of half -wavelengths, equipped with one or more parasitic elements of approximately impedance 'half wavelength in height.
  • driven element I has a total height from its top to base insulator 2 of any integral number of half wavelengths greater than i.
  • the length of element l down to point 31s one-half wavelength, and parasitic elements t and 5, located adjacent and parallel to this top sectionoi element l are also of one-
  • Thelength of element lbel'owpoint 3 is equal to any integral number of half wavelengths.
  • Coaxial transmission line 6' is connected to the bottom one-half wavelength section of 'elementl, across insulator l which is located at one-fourth wavelength from base insulator 2.
  • the parasitic elements 4 and 5 are maintained in position by means-of struts 8,
  • center supports 9 which are drilled so as to rotate freely about element l.
  • Supports 9 are supported on fixed thrust bearings H), which may be ball bearings if desired.
  • the lower support 9 is equipped with gear H which is driven by gear [2 attached tosh'aft l3.
  • Shaft I3 is in turn driven by motor it through gears and is supported by brackets l6,
  • Elements l, 4 and 5 are made of metals which are good conductors, but the equipment touching them, except of course the transmission line, should be made of poorly conducting or insulating materials.
  • the antenna is rotated to the desired direction by means of motor i l, which is operated by conventional control means not shown, and the receiver or transmitter is connected to the other end of transmission line ii by conventional means not shown, and the reception or transmission is begun.
  • Transmission line 8 "being connected to the bottom one-half wave section of element l at the one-fourth wavelength point, is matched in impedance by transformer action of element i with a point 6 located at the middle of the top half wave section of element I when the element l is an integral number of half one of the two feed wires is merely insulated from any contact with the antenna and the other is connected to element I at a point near its extreme lower end at which point its impedance is matched by. that of element I.
  • the point of connection of the transmission line is determined by well known principles of radio.
  • the lower portion of element I from base insulator 2 to point 3 radiates omnidirectionally as a simple vertical antenna while the upper portion of element I above point 3, together with the parasitic elements 4 and 5 radiates in a unidirectional manner as a result of the combined reflective action of one of the parasitic elements and the directive action of the other.
  • an antenna suitable for use at a 28.6 megacycle frequency (approximately meters wavelength) A was constructed.
  • Element I was made of Dural tubing assembled in sections of approximately 1% inch diameter, the length of element I from point 2 to insulator I being 8.2 feet and the length of element I above insulator 1 being 41 feet.
  • Elements 4 and 5 were made of inch Dural tubing approximately '15 feet in length. Thus the total length of element I was approximately 1 /2 wavelengths, and the length of elements 4 and 5 was approximately one-half wavelength.
  • Struts 8 were made of hardwood,
  • Transmission line 6 was a coaxial transmission line of approximately 70 ohms impedance. The entire structure was mounted on the ground and supported by guy wires.
  • Reflector element 4 was located approximately 4.8 feet from element I and director ele- .ment 5 was located at approximately 3 feet from element I on the opposite side from element 4, the three elements I, 4 and 5 lying in the same plane. The antenna operated very satisfactorily for both local and distant reception and transmission.
  • the above antenna possesses many advantages over the conventional antennas 1 now in use. For example, it eliminates the necessity of running the feed line to the top of the antenna, which is desirably mounted at a considerable height above ground or building top level. It eliminates the problem of matching the impedance of the transmission line to that of the mid-point of the conventional antenna array, since this is automatically accomplished by the auto-transformer action of elements I, 4 and 5. It eliminates all restrictions on the degree of rotation of the directional array. It eliminates efliciency loss and maintenance problems encoun tered in the use of slip rings and brushes in the conventional rotating beam antenna arrays. It eliminates the necessity of rotating a beam antenna array for transmission or reception of nearby signals.
  • the height of element I may be ill one wavelength or three or more half wavelengths.
  • Director element 5 need not be used, or additional parasitic elements such as an additional reflector element in addition to elements 4 and 5 may be employed, although the three element array shown is preferred.
  • the distance between the elements is readily calculated from known formulas and is generally between about one-tenth and two-tenths of a wavelength.
  • the array may be stationary, but is preferably rotatable. Rotation may be accomplished by any means other than that shown, such as for example by means of a shaft located within element I and coaxial therewith, and leading to a gear at or near the top of element l whereby the parasitic elements are rotated.
  • transmission lines may be used, whether coaxial or dual wire, although coaxial line of about 55 to 75 ohms impedance, connected across an insulator at the lower one-quarter wavelength point as indicated is preferred.
  • the antenna may be designed for other wavelengths than the 10 meter wavelength of the specific example, the system being particularly suitable for wavelengths shorter than about 20 meters, i. e. frequencies greater than about 14 megacycles.
  • Other materials of .construction may be employed although tubing made of light-weight metals of high conductivity, such as Dural, aluminum and the like are preferred for both the driven and the parasitic elements-
  • Other modifications of this invention which would occur to one skilled in the art may be made and these are to be considered within the scope of the invention as defined in the following claims.
  • An antenna array which comprises a straight vertical driven element capable of radiation over a height one-half nL where L is the wave-length and n is an integer greater than 1, a parasitic element of height one-half L adjacent the top one-half L section of the said driven element and a transmission line connected to the bottom onehalf L section of said driven element.
  • An antenna array which comprises a straight vertical driven element capable of radiation over a height one-half nL where L is the Wave-length and n is an integer greater than 1, a parasitic reflector element of height one-half L adjacent the top one-half L section of the said driven element, a parasitic director element of height onchalf L adjacent the top one-half L section of the said driven element and located on the opposite the top one-half L section of the said driven element, and a coaxial transmission line connected to the bottom L section of said driven element across an insulator at point approximately onefourth L from its lower end.
  • An antenna array which comprises a straight vertical driven element capable of radiation over a height one-half 1132 where L is the Wave-length and n is an integer greater than 1, a parasitic reflector element of height one-half L adjacent the top one-half L section of the said driven element, and a two-Wire transmission line connected to the bottom one-half L section of said driven element at a point near its extreme lower end.
  • An antenna array which comprises a stationary straight vertical driven element capable of radiation over a height one-half nL Where L is the Wavelength and n is an integer greater than 1, at least one parasitic element adjacent to and in the plane of the top one-half L section of the said driven element, means for rotating said parasitic element about said driven element as an axis, and a transmission line connected to the bottom one-half L section of said driven element.
  • An antenna array which comprises a stationary straight vertical driven element capable of radiation over a height one-half 'nL where L is the wavelength and n is an integer greater than 1, at least one parasitic element adjacent to and in the plane of the top one-half L section of the said driven element, means for rotating said parasitic element about said driven element as an axis, and a coaxial transmission line connected to the bottom one-half L section of said driven element across an insulator at a point approximately one-fourth L from its lower end.
  • An antenna array which comprises a stationary straight vertical driven element capable of radiation over a height 3/2 L where L is the wavelength, two parasitic elements of height onehalf L located adjacent the top one-half L section of the said driven element on opposite sides thereof and lying in a plane therewith, means for rotating said parasitic elements about said driven element as an axis, and a coaxial transmission line having an impedance between about and '75 ohms connected to said driven element across an insulator at a point approximately one-fourth L from its lower end.
  • a vertical antenna system which comprises a section capable of omnidirectional radiation and a section capable of unidirectional radiation, the driven element of the latter section being directly connected to and in a straight line with the section capable of omnidirectional radiation, and each of said sections being approximately /2 wave length in height.

Description

Oct. 26, 1948.
G. H. COTCHEFER 2,452,106
RADIO ANTENNA Filed March 15, 194s INVENTOR.
' Gordon H. CO/Chfl" T TOIPNEV Patented Oct. 26, 1948 UNITED STATES PATENT OFFICE RADIO ANTENNA Gordon- H. Cotchefer, Long Beach, Calif.
Application March 16, 1946, Serial No. 654,840
12 Claims. 1 This invention relates to radio reception and transmission, and particularly to an antenna array suitable for both omnidirectional transmission and reception to and from nearby points, and unidirectional transmission and reception to and from distant points.
Radio antenna arrays now in common use are designed primarily for transmission and reception to and from distant points and are usually in the form of a series of parallel horizontal or vertical elements of equal length, one being the driven element to which the transmission line leading to the radio receiver or transmitter is attached,
and the others being parasitic or driven elements a double line, attached at two points to the antenna, it is clear that the rotation of the antenna must be confined to relatively narrow limits to avoid twisting the transmission line around the antenna support. This is avoided in some instances by the use of slip rings for making con-' tact between the antenna and the transmission line, but the use of such slip rings involves possible loss of power and faulty operation.
It is an object of this invention to provide an antenna array which permits both omnidirectional transmission and reception to and from local points as well as unidirectional transmission and reception to and from distant points. Further objects are to supply a vertical antenna of simple construction providing for full 360 rotation in either direction without twisting of the transmission line, without the use of slip ring brushes or other moving devices; to avoid the necessity for running the transmission line to the top of the antenna in order to accomplish matching between the array and transmission line supplying energy; to simplify the construction of an efficient unidirectional antenna; and to provide other advantages as will be brought out below.
Briefly the antenna array of this invention comprises a stationary vertical driven element having a height equal to at least two or any higher integral number of half -wavelengths, equipped with one or more parasitic elements of approximately impedance 'half wavelength in height.
element, and a transmission line connected to the bottom half-wavelength section of said driven element. Means are also provided for rotating the parasitic elements about the stationary driven element. I
The invention will become clearer by reference to the attached drawing, in which driven element I has a total height from its top to base insulator 2 of any integral number of half wavelengths greater than i. The length of element l down to point 31s one-half wavelength, and parasitic elements t and 5, located adjacent and parallel to this top sectionoi element l are also of one- Thelength of element lbel'owpoint 3 is equal to any integral number of half wavelengths. Coaxial transmission line 6' is connected to the bottom one-half wavelength section of 'elementl, across insulator l which is located at one-fourth wavelength from base insulator 2. The parasitic elements 4 and 5 are maintained in position by means-of struts 8,
connected to center supports 9 which are drilled so as to rotate freely about element l. Supports 9 are supported on fixed thrust bearings H), which may be ball bearings if desired. The lower support 9 is equipped with gear H which is driven by gear [2 attached tosh'aft l3. Shaft I3 is in turn driven by motor it through gears and is supported by brackets l6, Elements l, 4 and 5 are made of metals which are good conductors, but the equipment touching them, except of course the transmission line, should be made of poorly conducting or insulating materials.
In operation, the antenna is rotated to the desired direction by means of motor i l, which is operated by conventional control means not shown, and the receiver or transmitter is connected to the other end of transmission line ii by conventional means not shown, and the reception or transmission is begun. Transmission line 8, "being connected to the bottom one-half wave section of element l at the one-fourth wavelength point, is matched in impedance by transformer action of element i with a point 6 located at the middle of the top half wave section of element I when the element l is an integral number of half one of the two feed wires is merely insulated from any contact with the antenna and the other is connected to element I at a point near its extreme lower end at which point its impedance is matched by. that of element I. The point of connection of the transmission line is determined by well known principles of radio. The lower portion of element I from base insulator 2 to point 3 radiates omnidirectionally as a simple vertical antenna while the upper portion of element I above point 3, together with the parasitic elements 4 and 5 radiates in a unidirectional manner as a result of the combined reflective action of one of the parasitic elements and the directive action of the other.
As a specific example of an antenna of this invention an antenna suitable for use at a 28.6 megacycle frequency (approximately meters wavelength) A was constructed. Element I was made of Dural tubing assembled in sections of approximately 1% inch diameter, the length of element I from point 2 to insulator I being 8.2 feet and the length of element I above insulator 1 being 41 feet. Elements 4 and 5 were made of inch Dural tubing approximately '15 feet in length. Thus the total length of element I was approximately 1 /2 wavelengths, and the length of elements 4 and 5 was approximately one-half wavelength. Struts 8 were made of hardwood,
-the brackets connecting them to elements I, 4
and 5 were made of insulating materials, and the remainder of the construction was substantially as indicated in the drawing. Transmission line 6 was a coaxial transmission line of approximately 70 ohms impedance. The entire structure was mounted on the ground and supported by guy wires. Reflector element 4 was located approximately 4.8 feet from element I and director ele- .ment 5 was located at approximately 3 feet from element I on the opposite side from element 4, the three elements I, 4 and 5 lying in the same plane. The antenna operated very satisfactorily for both local and distant reception and transmission.
It is apparent that the above antenna possesses many advantages over the conventional antennas 1 now in use. For example, it eliminates the necessity of running the feed line to the top of the antenna, which is desirably mounted at a considerable height above ground or building top level. It eliminates the problem of matching the impedance of the transmission line to that of the mid-point of the conventional antenna array, since this is automatically accomplished by the auto-transformer action of elements I, 4 and 5. It eliminates all restrictions on the degree of rotation of the directional array. It eliminates efliciency loss and maintenance problems encoun tered in the use of slip rings and brushes in the conventional rotating beam antenna arrays. It eliminates the necessity of rotating a beam antenna array for transmission or reception of nearby signals. It eliminates the problem of element misalignment encountered in the use of horizontal antenna arrays due to sagging and other causes. It eliminates the necessity for construction of large and heavy towers now used in horizontal conventional arrays. It eliminates the necessity for using thrust bearings and driving mechanisms heavy enough to support and rotate the conventional horizontal beam antennas.
It simplifies problems of construction and dismantling, and requires relatively small space. It may even be employed in l-ifeboats at sea.
Many modifications of the above equipment may be used. The height of element I may be ill one wavelength or three or more half wavelengths. Director element 5 need not be used, or additional parasitic elements such as an additional reflector element in addition to elements 4 and 5 may be employed, although the three element array shown is preferred. The distance between the elements is readily calculated from known formulas and is generally between about one-tenth and two-tenths of a wavelength. The array may be stationary, but is preferably rotatable. Rotation may be accomplished by any means other than that shown, such as for example by means of a shaft located within element I and coaxial therewith, and leading to a gear at or near the top of element l whereby the parasitic elements are rotated. Other types of transmission lines may be used, whether coaxial or dual wire, although coaxial line of about 55 to 75 ohms impedance, connected across an insulator at the lower one-quarter wavelength point as indicated is preferred. The antenna may be designed for other wavelengths than the 10 meter wavelength of the specific example, the system being particularly suitable for wavelengths shorter than about 20 meters, i. e. frequencies greater than about 14 megacycles. Other materials of .construction may be employed although tubing made of light-weight metals of high conductivity, such as Dural, aluminum and the like are preferred for both the driven and the parasitic elements- Other modifications of this invention which would occur to one skilled in the art may be made and these are to be considered within the scope of the invention as defined in the following claims.
I claim.
1. An antenna array which comprises a straight vertical driven element capable of radiation over a height one-half nL where L is the wave-length and n is an integer greater than 1, a parasitic element of height one-half L adjacent the top one-half L section of the said driven element and a transmission line connected to the bottom onehalf L section of said driven element.
2. An antenna array which comprises a straight vertical driven element capable of radiation over a height one-half nL where L is the Wave-length and n is an integer greater than 1, a parasitic reflector element of height one-half L adjacent the top one-half L section of the said driven element, a parasitic director element of height onchalf L adjacent the top one-half L section of the said driven element and located on the opposite the top one-half L section of the said driven element, and a coaxial transmission line connected to the bottom L section of said driven element across an insulator at point approximately onefourth L from its lower end.
4. An antenna array which comprises a straight vertical driven element capable of radiation over a height one-half 1132 where L is the Wave-length and n is an integer greater than 1, a parasitic reflector element of height one-half L adjacent the top one-half L section of the said driven element, and a two-Wire transmission line connected to the bottom one-half L section of said driven element at a point near its extreme lower end.
5. An antenna array which comprises a stationary straight vertical driven element capable of radiation over a height one-half nL Where L is the Wavelength and n is an integer greater than 1, at least one parasitic element adjacent to and in the plane of the top one-half L section of the said driven element, means for rotating said parasitic element about said driven element as an axis, and a transmission line connected to the bottom one-half L section of said driven element.
6. An antenna array which comprises a stationary straight vertical driven element capable of radiation over a height one-half 'nL where L is the wavelength and n is an integer greater than 1, at least one parasitic element adjacent to and in the plane of the top one-half L section of the said driven element, means for rotating said parasitic element about said driven element as an axis, and a coaxial transmission line connected to the bottom one-half L section of said driven element across an insulator at a point approximately one-fourth L from its lower end.
'7. An antenna array according to claim 6 in which the coaxial transmission line has an impedance between about 55 and 75 ohms, and the inner conductor is connected above the insulator and the shell is connected below the insulator.
8. An antenna array according to claim 6 in which the driven element and the parasitic elements are constructed of light weight metal tubing.
9. An antenna array which comprises a stationary straight vertical driven element capable of radiation over a height 3/2 L where L is the wavelength, two parasitic elements of height onehalf L located adjacent the top one-half L section of the said driven element on opposite sides thereof and lying in a plane therewith, means for rotating said parasitic elements about said driven element as an axis, and a coaxial transmission line having an impedance between about and '75 ohms connected to said driven element across an insulator at a point approximately one-fourth L from its lower end. r
10. An antenna array according to claim 8 in which the wavelength is below about 20 meters.
11. An antenna according to claim 8 in which the wavelength is approximately 10 meters.
12. A vertical antenna system which comprises a section capable of omnidirectional radiation and a section capable of unidirectional radiation, the driven element of the latter section being directly connected to and in a straight line with the section capable of omnidirectional radiation, and each of said sections being approximately /2 wave length in height.
GORDON H. COTCHEFER.
REFERENCES CITED The following references are of record in the file of this patent:
UNITED STATES PATENTS Number Name Date 1,966,491 Ferrell July 17, 1934 2,149,333 Brown Mar. 7, 1939 2,188,389 Cork et al Jan. 30, 1940 2,199,050 Jenkins Apr. 30, 1940 2,243,523 Davis May 27, 1941 2,255,520 Schuster Sept. 9, 1941 OTHER REFERENCES The A. R. R. L. Antenna Book, published by American Radio Relay League, West Hartford, Conn, 1944, pages 128, 129.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2631235A (en) * 1950-10-20 1953-03-10 Sheriff Jack Wavelyn Antenna

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1966491A (en) * 1930-12-01 1934-07-17 Bell Telephone Labor Inc Antenna system
US2149333A (en) * 1937-02-18 1939-03-07 Rca Corp Combined low frequency and turnstile antennas
US2188389A (en) * 1935-11-21 1940-01-30 Emi Ltd Electrical high frequency signaling system
US2199050A (en) * 1937-06-14 1940-04-30 Howard L Jenkins Antenna support
US2243523A (en) * 1938-06-06 1941-05-27 Paul H Davis Method of radio communication
US2255520A (en) * 1939-05-13 1941-09-09 Fernseh Gmbh Directional antenna system

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1966491A (en) * 1930-12-01 1934-07-17 Bell Telephone Labor Inc Antenna system
US2188389A (en) * 1935-11-21 1940-01-30 Emi Ltd Electrical high frequency signaling system
US2149333A (en) * 1937-02-18 1939-03-07 Rca Corp Combined low frequency and turnstile antennas
US2199050A (en) * 1937-06-14 1940-04-30 Howard L Jenkins Antenna support
US2243523A (en) * 1938-06-06 1941-05-27 Paul H Davis Method of radio communication
US2255520A (en) * 1939-05-13 1941-09-09 Fernseh Gmbh Directional antenna system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2631235A (en) * 1950-10-20 1953-03-10 Sheriff Jack Wavelyn Antenna

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