US2404093A - Antenna - Google Patents

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Publication number
US2404093A
US2404093A US400195A US40019541A US2404093A US 2404093 A US2404093 A US 2404093A US 400195 A US400195 A US 400195A US 40019541 A US40019541 A US 40019541A US 2404093 A US2404093 A US 2404093A
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Prior art keywords
circuit
exterior
resonant
coupling
systems
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Expired - Lifetime
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US400195A
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Walter Van B Roberts
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RCA Corp
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RCA Corp
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    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H2/00Networks using elements or techniques not provided for in groups H03H3/00 - H03H21/00
    • H03H2/005Coupling circuits between transmission lines or antennas and transmitters, receivers or amplifiers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/27Adaptation for use in or on movable bodies
    • H01Q1/28Adaptation for use in or on aircraft, missiles, satellites, or balloons

Definitions

  • the present invention relates to an arrangementfor using the outer sur-face of anraircraft or other 'ungrounded I conductively 'cased vehicle as an antenna.
  • An object of the present invention is. toutilize the relatively greatdimensions of the plane itself as the antenna either for-transmitting:orreceiv-- ing and thus do away with the necessity. for anyprojecting structure of any considerabledimensions.
  • 'Another object of the'present invention is to provide a mean for coupling aresonant'system entirely contained within a body which also is a resonant system tothe containing resonant'systern.
  • the present invention maybe applied not. only to-airplanes but,-also, to dirigibles or any kind of aircraft made largely of metal soas to form an electrically resonant system. It maybe applied even to' metal bodied motor Vehicles'insulated from the ground'by rubber tires.
  • '13 indicates an elongated conducting body insulated from earth such as, forexample, the fuselage of a metal'covered-airplane.
  • the body B considered as a resonant system isvery broadly resonant and will respond to a relatively large range offrequencies.
  • the interior resonant system may 'be coupled to the 'exteriorresonant system, asi shown in" Figure 1, by providing *a magnetic link circuit which is magnetically coupled to the interior tuned circuit C. It is passed through a pairof holes'h, h in B so that the conductor'wireof' the link encloses-some of the magnetic flux surrounding B. 'Holes 72., h are preferably located alonga line of current "flowing on the outside of B. The amount of coupling increases with the distance between" the holes and withthe separation between the external part of thelink circuit K and the surface of B.
  • transducer T may comprise radio receiving equipment, while if it i to be used'for transmitting, the transducer -may comprise a "generator of intelligence :bearing high frequency energy coupled to the tuned circuit C.
  • FIG. 2 shows a modified formoftheinvention wherein coupling between the interior'and exterior systems is electrostatic innature.
  • B is, as before, assumed to be of a length the order of one-half. the wavelength of the operating frequency.
  • Within the pipe is aconductive rod R connected to the pipe by asliding piston S.
  • the rod is .alsoslidable in the piston.
  • This current may be small but a small current fed in at one end of a dipole will excite a relatively large amount of current in the middle of the dipole, thus obtaining the desired coupling.
  • the interior system may be sharply tuned to a desired frequency while by sliding S (together with R as a unit) inside P, the coupling between the interior and exterior systems may be adjusted.
  • the in terior system may be fed with energy from an oscillator or amplifier in the usual fashion for transmission purposes while for reception, the receiving set will obtain voltage from the interior system.
  • the interior system need not be of the concentric line type but may be a tuned circuit C as shown in Figure 3.
  • the projecting rod shown in Figure 2 may be replaced by a small streamlined cap D fitting over the end of the body B and insulated therefrom.
  • the coupling between the systems may be adjusted by moving the tap X indicated on the tuned circuit C.
  • this wavelength range includes the range at present as signed to frequency modulation broadcasting
  • a pair of resonant systems the first of said systems having appreciable radiation resistance, the second of said systems being enclosed within said first system, and means for coupling said systems, said means comprising a member coupled with said second system and having a portion extending to the exterior of said first system, said member having associated therewith an electromagnetic field of the same nature as the electromagnetic field at the exterior of said first system at the position where said member extends, said extending portion being at a position where the exterior field is a maximum.
  • a pair of resonant systems the first of said systems having appreciable radiation resistance, the second of said systems being enclosed within said first system, and means for coupling said systems, said means comprising a member coupled with said second system and having a portion extending to the exterior of said first system, said member having associated therewith an electromagnetic field of the same nature as the electromagnetic field at the exterior of said first system at the position where said member extends, said extending portion being at a position where the exterior field is a maximum, said second system being tuned to the resonance frequency of said first system.
  • a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of 'said system, a resonant circuit within said body and'means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending to the exterior of said body, said member having associated therewith an electromagnetic field of the same nature as the electromagnetic field at the exterior of said body at its point of extension.
  • a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending to the exterior of said body at a point of maximum magnetic field, said member being arranged to encircle a portion of said magnetic field.
  • a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending to the exterior of said body at a point of maximum electric 6.
  • a vehicle having an electrically conductive exterior forming a hollow resonant body, said vehicle having a length of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a conductor linked to said circuit and passing through apertures in said body arranged along the length thereof and spaced from said body to encircle some of the magnetic field surrounding said body.
  • an aircraft comprising a hollow electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a conductor linked to said circuit and passing through apertures in said body arranged along the length thereof at opposite sides of the region of maximum field surrounding said body and spaced from said body to encircle some of said magnetic field.
  • a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending at one end of said body.
  • a hollow electrically conductive body having a length of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a conductive cap at one end of said body and connected to 6 body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending from said body at a position where the electromagnetic field is 5 a maximum.

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Astronomy & Astrophysics (AREA)
  • Aviation & Aerospace Engineering (AREA)
  • General Physics & Mathematics (AREA)
  • Remote Sensing (AREA)
  • Control Of Motors That Do Not Use Commutators (AREA)

Description

July 16, 1946. w. VAN B. ROBERTS ANTENNA Filed June 28, 1941 '70 TRANSDl/Cfl? INVENTOR WALTER VAN .ROBERTS BY MW ATTORNEY Patented July 16, 1946 Walter van B. Roberts, Princeton, N. J assignor to Radio Corporation of America, a; corporation .of Delaware Application J une 28, 1941, Serial No. 400,195
The present invention. relates to an arrangementfor using the outer sur-face of anraircraft or other 'ungrounded I conductively 'cased vehicle as an antenna.
It has been customarygboth for receivingiand transmitting, to provide aircraft with a conventional type of antenna, such as,'a loopiantenna,
an open wire antenna trailing: behind the. plane or strung fixedly on support projecting from the plane, or a self supportingrod' antenna.
An object of the present invention is. toutilize the relatively greatdimensions of the plane itself as the antenna either for-transmitting:orreceiv-- ing and thus do away with the necessity. for anyprojecting structure of any considerabledimensions.
'Another object of the'present invention is to provide a mean for coupling aresonant'system entirely contained within a body which also is a resonant system tothe containing resonant'systern.
' The present invention maybe applied not. only to-airplanes but,-also, to dirigibles or any kind of aircraft made largely of metal soas to form an electrically resonant system. It maybe applied even to' metal bodied motor Vehicles'insulated from the ground'by rubber tires.
"The invention will be more fully understood by reference to i a full detailed description which is accompanied by'a drawing in which Figure 1 illustrates' schematically anembodiment of the invention, Figure 1a. illustrates a modification of Figure 1, and'Figures 2 and 3; further modifications thereof.
In Figure 1, '13 indicates an elongated conducting body insulated from earth such as, forexample, the fuselage of a metal'covered-airplane.
Structural details of the planesuch as wings,
motors, landinggear,'etc., which are not'pertinent to the present invention -have not been shown. Such a bodyconstitutes' a dipole with a relatively large radiation resistance but relatively small reactance 'forfrequenciespther than its natural frequency. This is because- 0f the-large ratio of maximum diameter-to'itslength as compared with the usual wire -o tubing dipole. As a result of the small ratio of length-to cross-section, the body B considered as a resonant system isvery broadly resonant and will respond to a relatively large range offrequencies. Let us suppose,thereforeythathorizontally polarized radio waves impinge upon horizontal body B with a frequency of the order of the natural frequency of the body. As a result,- oscillating current news along the-surface of B, which current pro- I 10 Claims. (Cl: 250- 33) ducesamagnetic field around the bodyiland an electric field along the-body. Theiproduced' magnetic' field is'greate'st at the middleof the body,
and the electrostatic field is greatest at the 'ends.
Inside the enclosed body is another resonantJciricuit Ctuned to the desired frequency. Due'. to 'the'shielding action of B, no voltage can betpicked up by the interior tuned circuit by anyconnection that'can be made Within Bat any. position therewithin.
The interior resonant system may 'be coupled to the 'exteriorresonant system, asi shown in" Figure 1, by providing *a magnetic link circuit which is magnetically coupled to the interior tuned circuit C. It is passed through a pairof holes'h, h in B so that the conductor'wireof' the link encloses-some of the magnetic flux surrounding B. 'Holes 72., h are preferably located alonga line of current "flowing on the outside of B. The amount of coupling increases with the distance between" the holes and withthe separation between the external part of thelink circuit K and the surface of B. It will be appreciated that in place of an independent link circuit a portion of the interior resonant circuit C may be brought'out through the aforesaid holes h, h, as shown in Figure Id, at K, so as to provide direct mutual inductance between the interior and exterior systems.
If the present system is to be used for receiving signals, transducer T may comprise radio receiving equipment, while if it i to be used'for transmitting, the transducer -may comprise a "generator of intelligence :bearing high frequency energy coupled to the tuned circuit C.
Figure 2 shows a modified formoftheinvention wherein coupling between the interior'and exterior systems is electrostatic innature. In Figure 2, B is, as before, assumed to be of a length the order of one-half. the wavelength of the operating frequency. Re-entrantly connected .to one end of B, where the electrostatic field is the greatest, is a metal pipe P of somewhatgreater lengththan a quarter of the operating wavelength. Within the pipe is aconductive rod R connected to the pipe by asliding piston S. The rod is .alsoslidable in the piston. When the right end of the rod is. entirely inside the pipe, the concentric line formed by R and P will be resonant and entirely decoupled from the dipole formed by the outer surface of B. However, if S and Rbe moved to .the rightso that the rod R projects slightly beyond the end of the pipe, electrostatic linesof force willbe set up as shown atL between the end ofthe rod and. the end of the outer-surface of B. These lines of force interact with the lines of force emanating from the ends of B due to oscillations on the outside of B and hence constitute a capacity coupling between the two systems. The coupling may also be considered from a diiferent point of view as follows: Since the current in the rod is not zero at the point where the rod leaves the pipe, there must be an equal and opposite current flowing from the end of the pipe into the end of dipole body B. This current may be small but a small current fed in at one end of a dipole will excite a relatively large amount of current in the middle of the dipole, thus obtaining the desired coupling. By means of relative adjustment between R and S, the interior system may be sharply tuned to a desired frequency while by sliding S (together with R as a unit) inside P, the coupling between the interior and exterior systems may be adjusted. The in terior system may be fed with energy from an oscillator or amplifier in the usual fashion for transmission purposes while for reception, the receiving set will obtain voltage from the interior system.
Since the coupling between the interior and exterior systems has been demonstrated to be due to the capacity between a high voltage point of the interior system and a high voltage point of the exterior system, the interior system need not be of the concentric line type but may be a tuned circuit C as shown in Figure 3. Furthermore, if desired, the projecting rod shown in Figure 2 may be replaced by a small streamlined cap D fitting over the end of the body B and insulated therefrom. In this case, the coupling between the systems may be adjusted by moving the tap X indicated on the tuned circuit C.
It should be noted that the system is applicable to automobiles or other land vehicles having metal bodies for the reception of wavelengths approximating twice the length of the vehicle. In the case of cars of ordinary dimensions, this wavelength range includes the range at present as signed to frequency modulation broadcasting,
While I have shown and particularly described several embodiments of my invention, it is to DB distinctly understood that my invention is not limited thereto but that modifications within the scope of my invention may be made.
I claim:
1. In combination, a pair of resonant systems, the first of said systems having appreciable radiation resistance, the second of said systems being enclosed within said first system, and means for coupling said systems, said means comprising a member coupled with said second system and having a portion extending to the exterior of said first system, said member having associated therewith an electromagnetic field of the same nature as the electromagnetic field at the exterior of said first system at the position where said member extends, said extending portion being at a position where the exterior field is a maximum.
2. In combination, a pair of resonant systems, the first of said systems having appreciable radiation resistance, the second of said systems being enclosed within said first system, and means for coupling said systems, said means comprising a member coupled with said second system and having a portion extending to the exterior of said first system, said member having associated therewith an electromagnetic field of the same nature as the electromagnetic field at the exterior of said first system at the position where said member extends, said extending portion being at a position where the exterior field is a maximum, said second system being tuned to the resonance frequency of said first system.
3. In a radiant energy system, a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of 'said system, a resonant circuit within said body and'means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending to the exterior of said body, said member having associated therewith an electromagnetic field of the same nature as the electromagnetic field at the exterior of said body at its point of extension.
4. In a radiant energy system, a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending to the exterior of said body at a point of maximum magnetic field, said member being arranged to encircle a portion of said magnetic field.
5. In a radiant energy system, a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending to the exterior of said body at a point of maximum electric 6. In a radiant energy system, a vehicle having an electrically conductive exterior forming a hollow resonant body, said vehicle having a length of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a conductor linked to said circuit and passing through apertures in said body arranged along the length thereof and spaced from said body to encircle some of the magnetic field surrounding said body.
'7. In a radiant energy system, an aircraft comprising a hollow electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a conductor linked to said circuit and passing through apertures in said body arranged along the length thereof at opposite sides of the region of maximum field surrounding said body and spaced from said body to encircle some of said magnetic field.
8. In a radiant energy system, a vehicle having an electrically conductive surface forming a hollow resonant body whose length is of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending at one end of said body. 7
9. In a radiant energy system, a hollow electrically conductive body having a length of the order of a half wavelength at the operating frequency of said system, a resonant circuit within said body and means for coupling said circuit to the exterior of said body, including a conductive cap at one end of said body and connected to 6 body and means for coupling said circuit to the exterior of said body, including a member coupled with said circuit and extending from said body at a position where the electromagnetic field is 5 a maximum.
WALTER VAN B. ROBERTS.
US400195A 1941-06-28 1941-06-28 Antenna Expired - Lifetime US2404093A (en)

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Cited By (30)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2449562A (en) * 1944-10-03 1948-09-21 Us Sec War Antenna
US2510698A (en) * 1946-01-28 1950-06-06 Johnson William Arthur Radio aerial, particularly for aircraft and other vehicles
US2520986A (en) * 1947-10-22 1950-09-05 Motorola Inc Vehicular antenna system
US2520987A (en) * 1947-10-22 1950-09-05 Motorola Inc Vehicle body antenna
US2527609A (en) * 1945-08-10 1950-10-31 Int Standard Electric Corp Arrangement for coupling to an electric antenna
US2607894A (en) * 1948-02-24 1952-08-19 Johnson William Arthur Aerial system
US2618747A (en) * 1949-02-15 1952-11-18 Rca Corp Aircraft antenna system
US2652492A (en) * 1949-03-05 1953-09-15 Collins Radio Co Dipole antenna and feed arrangement therefor
US2707750A (en) * 1948-06-08 1955-05-03 Sylvania Electric Prod Ultra high frequency translator
US2968037A (en) * 1957-04-08 1961-01-10 Thomas F Thompson High frequency receiving antenna
US3488657A (en) * 1965-10-18 1970-01-06 Bendix Corp Low profile antenna
US3500426A (en) * 1965-10-22 1970-03-10 Scott & Fetzer Co Magnetically driven antenna array
US3936834A (en) * 1972-06-21 1976-02-03 The United States Of America As Represented By The Secretary Of The Navy High powered ferrite loaded helicopter antenna
DE1591161C1 (en) * 1967-06-05 1977-11-10 Hagenuk Neufeldt Kuhnke Gmbh Method and device for emitting electric streamlines into the water from on board a ship made of metal, the conductive hull acting as an electric dipole
US4317121A (en) * 1980-02-15 1982-02-23 Lockheed Corporation Conformal HF loop antenna
EP0196209A2 (en) * 1985-03-27 1986-10-01 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
EP0223398A1 (en) * 1985-10-29 1987-05-27 Toyota Jidosha Kabushiki Kaisha Vehicle antenna system
US4717922A (en) * 1984-11-06 1988-01-05 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4717921A (en) * 1984-11-15 1988-01-05 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4723127A (en) * 1984-12-12 1988-02-02 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4754284A (en) * 1984-11-15 1988-06-28 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4789866A (en) * 1984-11-08 1988-12-06 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4794397A (en) * 1984-10-13 1988-12-27 Toyota Jidosha Kabushiki Kaisha Automobile antenna
US4804966A (en) * 1984-10-29 1989-02-14 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4804968A (en) * 1985-08-09 1989-02-14 Toyota Jidosha Kabushiki Kaisha Vehicle antenna system
US4806942A (en) * 1985-06-10 1989-02-21 Toyota Jidosha Kabushiki Kaisha Automobile TV antenna system
US4816837A (en) * 1985-08-01 1989-03-28 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4821042A (en) * 1985-06-28 1989-04-11 Toyota Jidosha Kabushiki Kaisha Vehicle antenna system
US4823142A (en) * 1985-06-21 1989-04-18 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4845505A (en) * 1987-02-13 1989-07-04 Toyota Jidosha Kabushiki Kaisha Automobile antenna system for diversity reception

Cited By (33)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2449562A (en) * 1944-10-03 1948-09-21 Us Sec War Antenna
US2527609A (en) * 1945-08-10 1950-10-31 Int Standard Electric Corp Arrangement for coupling to an electric antenna
US2510698A (en) * 1946-01-28 1950-06-06 Johnson William Arthur Radio aerial, particularly for aircraft and other vehicles
US2520986A (en) * 1947-10-22 1950-09-05 Motorola Inc Vehicular antenna system
US2520987A (en) * 1947-10-22 1950-09-05 Motorola Inc Vehicle body antenna
US2607894A (en) * 1948-02-24 1952-08-19 Johnson William Arthur Aerial system
US2707750A (en) * 1948-06-08 1955-05-03 Sylvania Electric Prod Ultra high frequency translator
US2618747A (en) * 1949-02-15 1952-11-18 Rca Corp Aircraft antenna system
US2652492A (en) * 1949-03-05 1953-09-15 Collins Radio Co Dipole antenna and feed arrangement therefor
US2968037A (en) * 1957-04-08 1961-01-10 Thomas F Thompson High frequency receiving antenna
US3488657A (en) * 1965-10-18 1970-01-06 Bendix Corp Low profile antenna
US3500426A (en) * 1965-10-22 1970-03-10 Scott & Fetzer Co Magnetically driven antenna array
DE1591161C1 (en) * 1967-06-05 1977-11-10 Hagenuk Neufeldt Kuhnke Gmbh Method and device for emitting electric streamlines into the water from on board a ship made of metal, the conductive hull acting as an electric dipole
US3936834A (en) * 1972-06-21 1976-02-03 The United States Of America As Represented By The Secretary Of The Navy High powered ferrite loaded helicopter antenna
US4317121A (en) * 1980-02-15 1982-02-23 Lockheed Corporation Conformal HF loop antenna
US4794397A (en) * 1984-10-13 1988-12-27 Toyota Jidosha Kabushiki Kaisha Automobile antenna
US4804966A (en) * 1984-10-29 1989-02-14 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4717922A (en) * 1984-11-06 1988-01-05 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4789866A (en) * 1984-11-08 1988-12-06 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4717921A (en) * 1984-11-15 1988-01-05 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4754284A (en) * 1984-11-15 1988-06-28 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4723127A (en) * 1984-12-12 1988-02-02 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
EP0196209A2 (en) * 1985-03-27 1986-10-01 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4792807A (en) * 1985-03-27 1988-12-20 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
EP0196209A3 (en) * 1985-03-27 1988-06-01 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4806942A (en) * 1985-06-10 1989-02-21 Toyota Jidosha Kabushiki Kaisha Automobile TV antenna system
US4823142A (en) * 1985-06-21 1989-04-18 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4821042A (en) * 1985-06-28 1989-04-11 Toyota Jidosha Kabushiki Kaisha Vehicle antenna system
US4816837A (en) * 1985-08-01 1989-03-28 Toyota Jidosha Kabushiki Kaisha Automobile antenna system
US4804968A (en) * 1985-08-09 1989-02-14 Toyota Jidosha Kabushiki Kaisha Vehicle antenna system
EP0223398A1 (en) * 1985-10-29 1987-05-27 Toyota Jidosha Kabushiki Kaisha Vehicle antenna system
US4804967A (en) * 1985-10-29 1989-02-14 Toyota Jidosha Kabushiki Kaisha Vehicle antenna system
US4845505A (en) * 1987-02-13 1989-07-04 Toyota Jidosha Kabushiki Kaisha Automobile antenna system for diversity reception

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