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Publication numberUS3189901 A
Publication typeGrant
Publication dateJun 15, 1965
Filing dateNov 4, 1963
Priority dateDec 15, 1956
Publication numberUS 3189901 A, US 3189901A, US-A-3189901, US3189901 A, US3189901A
InventorsMario Cutolo
Original AssigneeGiovanni Lanza
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Method of producing ionization and luminous emission in a gas or vapor and apparatus for use therein
US 3189901 A
Abstract  available in
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Claims  available in
Description  (OCR text may contain errors)

June 15, 1965 M. CUTOLO 3,189,901

METHOD OF PRODUCING IONIZATION AND LUMINOUS EMISSION IN A GAS OR VAPOR AND APPARATUS FOR USE THEREIN Original Filed Dec. 9, 1957 INVENTOR.

MA RIO CU TQLO ATTORNEY nited States 3,3 21 Claims. (Cl. 343-400) This application is a continuation of US. patent application Serial No. 701,493, filed December 9, 1957, and now abandoned, which application refers to an application filed in Italy on December 15, 1956, which has matured into Italian Patent No. 563,365.

This invention is directed to a method for producing luminous emission in a gas or vapor and more particularly to the production, at great distances, of ionization and/or luminous emission in a gas or vapor by means of magnetic fields and radio waves and apparatus for carrying out the method.

It is well known that an electric field, if sulficiently intense, can cause ionization and electrical discharge in a gaseous medium. The energies required heretofore to produce this phenomenon have been too excessive to be practical and the field voltages, whether A.C. or DC. must of necessity be high. In consequence, it has not proved economical or practical to produce sustained discharges, in a gaseous medium, by means of propagated radio waves at great-distances from the transmitter.

It should be noted that the few solutions to the problem of illumination at considerable distances, through the use of electro-magnetic waves, adopted to date, have all been based on a transmission of electrical energy using radio waves of great power. In spite of that, it has never been possible to reach beyond a few hundreds yards from the transmitter even using transmitting powers of the order of tens or hundreds of kilowatts. The difficulty is explained by the existence of a fundamental law according to which the electro-magnetic field at a given point is directly proportional to the square root of the irradiated power. According to the present invention, the production of ionization and/ or luminescence in a gaseous medium is not dependent on the actual transmission of an electro-magnetic field but rather the luminous electrical discharge is caused at great distance by the combined effect of crossed magnetic and radio-electric fields produced by the radiative component of the transmitted signal rather than, as heretofore, the inductive component.

It is an important object of this invention to provide an improved method of producing ionization and/ or luminous emission by means of propagated radio waves in a gaseous medium located remote of the radio wave transmitter which is economical and practical.

It is a further important object of of the invention to provide an improved method of producing ionization and/or luminous emission in a gaseous medium at great distances from a transmitter which requires a minimum amount of power expenditure.

It is a further important object of the invention to provide apapratus peculiarly adapted to carrying out the method of this invention and which is characterized by its simplicity of construction, high operating efliciency and low cost of maintenance.

In accordance with one embodiment of the present invention, the method comprises applying transmitted radio wave energy to a gaseous medium, under reduced pressure, normal to a magnetic field acting on the gaseous medium, of a frequency of oscillation at about the gyrofrequency of the gaseous medium as determined by the strength of the magnetic field acting thereon, to produce ionization of the gaseous discharge and in certain instances luminous emission.

These and other objects and advantages of the present invention will be better understood from the following detailed description when taken in connection with the accompanying drawings:

FIGURE 1 shows one form of the apparatus of the invention schematically.

FIGURE 2 shows another embodiment of the apparatus according to the invention.

FIGURE 3 illustrates schematically how the method of the invention may be applied to unconfined rarefied gases as in the ionosphere to produce ionization with the earth as the source of the magnetic field.

In the presence of a magnetic field of intensity H, where H is expressed in gauss, a free electron in a gaseous medium will travel in circular or spiral paths around the magnetic lines of force, with a frequency of 2.8 H megacycles per second, the so-called gyrofrequency. It has been found that if a radio wave of a frequency near the gyro value is employed and applied at right angles to the magnetic lines of force, a resonance effect occurs, which enables the electrons, even in a weak A.C. field, to acquire substantial energies. The gaseous medium becomes ionized and luminescence may result. It has been further found that the electrical discharge occurs more easily and at a much lower tension when the radiative rather than the inductive component of an electromagnetic field is made to act on the gas. In fact, the radiative component having extremely low power can be used and consequently the discharge potential acquires a considerably reduced value as compared with that when the inductive component is used.

Referring to FIGURE 1, there is represented, in schematic form, the apparatus of the invention. A container 11 for gas, of any convenient shape, a sphere being shown, is provided having on either side two similar metallic plates 12 and 13, which comprise the plates of a condenser 14, whose dielectric consists of the container 11 and its contents. Plates 12 and 13 may conveniently be positioned within container 11, with electrical connection of a pass-through variety provided in the walls of the container and connected to each of the plates. Plates 15 and 16 are magnetic pole pieces attached to magnet 17, which may conveniently be of the horseshoe or U- shaped type. Usually magnet 17 will be of, the permanent variety, but an electromagnet may be used. Plates 15 and 16 are positioned with respect to condenser plates 12 and 13 such that the magnetic field within container 11 is substantially perpendicular to an electric field to be generated between condenser plates 12 and 13.

Each plate, 12 and 13 of the condenser'is connected to the tuned RF circuit 18 which consists of a sliding wire 19 or bar in shunt with the condenser field. Wire 19 is adjustably positioned to obtain a maximum voltage on condenser plates 12 and 13. Other combinations of inductances may be used to achieve a similar result, but because of its high efficiency this arrangement is to be preferred. The input of the tuned RF circuit 18 is connected by means of a suitable cable 20, of any convenient length, to an antenna 21. This antenna may consist of several elements, to give maximum gain, as generally employed in television, radar and the like. The antenna may be of a tuned variety, such as a yagi, to provide high gain at the gyrofrequency.

The container 11 is filled with air or other gas, and/ or with vapors of such substances as mercury or sodium, under low pressure. Since the container fulfills the primary function of retaining the gas or vapor, under low pressure,

it is immaterial Whether either or both pairs of plates are positioned inside or outside container 11. With this arrangement, when the antenna 21 receives an RF signal substantially at the gyrofrequency and slide wire is adjusted for maximum voltage on plates 12 and 13, the gaseous medium is ionized and luminescence may result depending on the gaseous medium being utilized in container 11. The container 11 is preferably made of a transparent material, such as plastic, and to achieve maximum luminescence, the inside of the transparent eontainer 11 may be coated with appropriate phosphors which fiuoresce on being excited by the ionized gas. For example, a transparent plastic sphere having high insulating properties and approximately one foot in diameter was filled with dry air at a pressure of between 1.2 1() and 2.0 l millimeters of mercury, these pressures being suitable for a sphere not less than 4% inches in diameter. Condenser plates 12 and 13 on the order of one foot in diameter were used and plates 15 and 16 of magnet 17 were about six inches in diameter and concave to conform to the surface of the spherical container 11. Magnet 17 has a field strength H of about 18 gauss. An RF signal was transmitted to antenna 21 of 2.8 H megacycles (about 50 megacycl'es) and slide wire 19 adjusted to tune RF circuit 18 to the transmit-ted frequency. With a transmitted RF signal at about 50 megac'ycles of approximately 70 watts and with a distance of approximately 3000 feet between the transmitting antenna and antenna 21, considerable ionization and luminescence was observed of the gas in container 11.

FIGURE 2 illustrates a somewhat complex but more efiicient arrangement. The container 11, condenser plates 12 and 13, magnetic pole pieces 15 and 16, magnet 17,

tuned circuit 18, cable 20 and antenna 21 are essentially identical with items noted in FIGURE 1. However, a second set of condenser plates 12a and 13a, with tuned circuit 13a, lead in cable 20a and antenna 21a. For a circular polarized beam incident on the antenna, antenna 21 and 21a may be dipoles or equivalent antennas posi- -t-ioned perpendicular to one another. For other polarization, especially linear, it may be necessary to introduce the appropriate delay circuit 22, to provide the necessary phasing of the incoming signals on each antenna, such that and if'the condenser plates are set as nearly as possible perpendicular to the lines of magnetic force.

The terrestrial gyrofrequency will vary with latitude since the strength of the earths magnetic field as wellas inclination thereof varies from the equator to the poles. The intensity H will vary from about 0.7 gauss at the poles to about 0.3 gauss at the equator and will have a strength of 0.57 gauss at Washington, DC. and a gyrofrequency of about 1.6 megacycles at Washington.

If the container 11 is sufiiciently large, considerable inclination is permissible between the lines of force of the magnetic field and the normal to the radio-electric With a large container and sufficiently powerful transmitter, the ionization and luminescence may be achieved by omitting the condenser plates, antennas, and connecting wires, whose primary purpose is to increase the intensity and control the direction of the radio-electric field. If this is done, however, the radio waves must be polarized so that the desired perpendicularity can be achieved between the static magnetic field and the electric vector of the incident radio-electric beam. The field may conveniently have either linear or polar polarization.

An extreme example of the basic principle occurs in the earths ionosphere where the pressure is sufiiciently Cir accompany the phenomenon.

low that the container itself is not necessary and the earth supplies the magnetic field. It has been theoretically proved that when a radio wave of great power and of a frequency almost equal to the local gyrofrequency incides on the ionosphere, due to the elfect to the terrestrial magnetic field, it is able to provoke an electrical discharge and consequently determine a luminous zone at a certain distance from the earths surface. Thus, by employing the general magnetic field of the earth and a high-power radio transmitter on the desired gyrofrequency, with directional antenna designed to emit polarized radio waves whose electric vector incides with the ionosphere near perpendicular to the magnetic field in the ionosphere, a discharge may be produced.

Allowance must be made for ionospheric refraction, which tends to bend the wave-s and change the angle of incidence thereof with respect to the magnetic field. These field lines, except at the North and South poles, are inclined toward the equator. Referring to FIGURE 3, there is a representation of how this may be accomplished schematically. H represents the direction of the magnetic field and T the transmiter and antenna system, generating radio beam B, which intersects the ionosphere II in the neighborhood of A. Note that the transmitter must be on the equator side of A and that the direction of the beam from the antenna should lie in the magnetic meridian, with horizontal or circular polarization.

The enhanced ionization thus produced in the ionosphere has a potential practical use of increasing the range of radio frequencies that the region A can reflect and thus make possible radio communication on a wider frequency range. An increased aurora or airglow may It may be further noted that this procedure enables the control or maintenance of constant ionization in'a region of the ionosphere that otherwise would be subject to marked diurnal variations.

The character of the radio waves may conveniently be of several forms. It is possible to employ a CW transmitter operating on the gyrofrequency, however, much greater efficiency results, for given total power expended, from pulsed transmissions of high peak power.

Alternatively, a basic radio-wave on UHF and VHF may be used, preferably pulsed with high peak power, and modulated by the desired gyrofrequency. This method has the special advantage of permitting the use of narrowly confined beams, and the use of high gain antennas which are easier to achieve on UHF and VHF than on lower frequencies.

To achieve maximum luminescence in the devices of FIGURES 1 and 2, the inside of the transparent container 11 may be coated with a suitable phosphor which phosphoresces when excited by the ionized gas. Thus the device of this invention with suitable antenna may be used to provide illumination in open country without the expense of transmission lines and the like utilizing the radiated power from low frequency radio transmitters,

pulsed to peak power and modulated with the local gyrofrequency. This may be accomplished without interfering with normal broadcasting.

While preferred embodiments of the invention have been disclosed, it is intended that the invention not be limited thereto, but only by the true spirit and scope of the appended claims;

I claim:

1. A method for producing luminosity and ionization locally in the ionosphere which comprises propagating into a portion of the ionosphere a radio wave having a frequency between about 30 and about 3000 megacycles/ sec. and modulated at about the local gyrofrequency.

2. The method of'claim 1 wherein said radio wave is polarized. V

3. The method of claim 1 wherein said radio wave is pulsed.

4. The method of claim 3 wherein said radio wave is polarized circularly.

5. The method of claim 4 wherein said modulation is at about 1.6 megacycles/ sec.

6. The method of claim 5 wherein said radio wave has a frequency between about 30 and about 300 megacycles/ sec.

7. A method for reflecting electromagnetic waves from the ionosphere which comprises (a) producing a zone of locally enhanced ionization in the ionosphere by propagating into a portion thereof a radio Wave having frequencies between about 30 and about 3000 megacycles/sec. and modulated at about the local gyrofrequency, and (b) impinging electro-magnetic waves against said zone of enhanced ionization.

8. The method of claim 7 wherein said radio wave is polarized.

9. The method of claim 8 where said radio wave is pulsed.

10. The method of claim 9 wherein said radio wave is polarized circularly.

11. The method of claim 10 wherein said modulation is at about 1.6 megacycles/sec.

12. The method of claim 10 wherein said radio wave has a frequency between about 30 and about 300 megacycles/sec.

13. A method for controlling changes caused by diurnal variations in the reflectivity of the ionosphere towards electromagnetic waves which comprises producing a zone of locally enhanced ionization in the ionosphere by propagating into a portion thereof a radio wave having a frequency between about 30 and about 3000 megacycles/ sec. and modulated at about the local gyrofrequency, and adjusting the resulting ionization to compensate for diurnal variations.

14. The method of claim 13 wherein said radio wave is pulsed.

15. The method of claim 14 wherein said radio wave is polarized circularly.

16. Apparatus for the production of induced ionization and luminous emission comprising in combination a container adapted to contain a gas under reduced pressure, a magnet having a pair of pole pieces located relative to the container in such a manner that the magnetic lines of force intersect the container, at least one pair of parallel condenser plates located relative to the container in such a manner that a line joining the centers of the condenser plates is normal to the magnetic lines of force, and an antenna adapted to receive the radiative component of radio-electric energy at a predetermined frequency for application across said condenser plates.

17. Apparatus as set forth in claim 16, wherein the magnet is a permanent magnet and the condenser plates are provided with a tuned RF circuit adapted to be tuned to a selected frequency.

18. Apparatus as set forth in claim 17, wherein two pairs of condenser plates, cable means and antennas are provided positioned relative to the container such that lines connecting each center of a pair of plates intersect at an angle normal to the magnetic lines of force and the cable means connecting one pair of condenser plates to its respective antenna includes a delay line such that the radio-electric energy received by one pair of condenser plates is out-of-phase with respect to the energy reaching the other pair.

19. Apparatus for the production of induced ionization and luminous emission comprising in combination a container containing a gas under reduced pressure, magnet means located relative to the container providing magnetic lines of force passing through the gas in the container, condenser means located relative to the container to provide an electric field through said container intersecting the magnetic lines of force within said gas in the container, and antenna means for receiving the radiative component of radio-electric energy at the gyrofrequency of said gas in the magnetic field for application thereof across said condenser means.

20. Apparatus as defined in claim 19 wherein the condenser means includes tuned radio frequency circuit means adapted to be tuned to a selected frequency.

21. Apparatus as set forth in claim 20 wherein the magnet means is a permanent magnet having a pair of pole pieces and the condenser means includes a pair of parallel plates.

References Cited by the Examiner UNITED STATES PATENTS 11/31 Trouant 3240.5

OTHER REFERENCES CHESTER L. JUSTUS, Primary Examiner.

MAYNARD R. WILBUR, Examiner.

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US1832672 *Feb 5, 1929Nov 17, 1931Westinghouse Electric & Mfg CoSystem of television
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US3445844 *Jan 11, 1968May 20, 1969Raytheon CoTrapped electromagnetic radiation communications system
US3518670 *Sep 25, 1967Jun 30, 1970North American RockwellArtificial ion cloud
US4638316 *Oct 30, 1973Jan 20, 1987The United States Of America As Represented By The Secretary Of The NavyRadar reflecting electrolytes
US4843401 *Jan 26, 1988Jun 27, 1989Atlantic RichfieldMethod and apparatus for generating and radiating electromagnetic energy
US4999637 *May 14, 1987Mar 12, 1991Apti, Inc.Creation of artificial ionization clouds above the earth
US5498928 *May 24, 1994Mar 12, 1996Osram Sylvania Inc.Electrodeless high intensity discharge lamp energized by a rotating electric field
US5509032 *Jun 11, 1991Apr 16, 1996The United States Of America As Represented By The Secretary Of The NavyNon-adaptive amplitude-difference interference filter
EP0684629A1 *May 24, 1995Nov 29, 1995Osram Sylvania Inc.Electrodeless high intensity discharge lamp energized by a rotating electric field
EP0840354A2 *Oct 31, 1997May 6, 1998Matsushita Electric Industrial Co., Ltd.High frequency discharge energy supply means and high frequency electrodeless discharge lamp device
Classifications
U.S. Classification342/350, 455/64, 324/304, 398/184, 313/161, 362/263, 375/259, 398/172
International ClassificationH01J65/04, H05H1/00
Cooperative ClassificationH01J65/046, H05H1/00
European ClassificationH01J65/04A2, H05H1/00