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Publication numberUS2939049 A
Publication typeGrant
Publication dateMay 31, 1960
Filing dateMay 29, 1958
Priority dateMay 29, 1958
Publication numberUS 2939049 A, US 2939049A, US-A-2939049, US2939049 A, US2939049A
InventorsBlackman Vernon H
Original AssigneePlasmadyne Corp
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Apparatus for generating high temperatures
US 2939049 A
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Description  (OCR text may contain errors)

ay 31, 1960 v. H. BLACKMAN 2,939,049



APPARATUS FOR GENERATING HIGH TEIVIPERATURES Vernon H. Blackmau, Laguna Beach, Calif., assignor, by mesne assignments, to Plasmadyne Corporation, Santa Ana, Califi, a corporation of California Filed May 29, 1958, Ser. No. 738355 8 Claims. Cl. 315-236 This invention relates to apparatus for generating high temperatures, and high-intensity light. The invention pertains to the general field of discharge-type devices for creating momentarily temperatures measured in millions of degrees.

Discharge-type devices of the class indicated may be divided into those employing'electrodes, and those effecting a discharge in space, Devices employing electrodes present substantial problems of contamination due to the vaporization of electrode material. This produces, particularly in the case of repetitive operation, detrimental effects because of the fact that the radiation capabilities of vapors of impurities are very high. It follows that a large amount of the energy stored in the discharge is dissipated in the form of radiation, thereby reducing the effective temperature of the gas.

With relation to devices which effect discharges in space, that is to say without electrodes, these conventionally consist of a toroidal chamber which produces, in conjunction with magnet means and by virtue of a pinch efiect, a toroidal plasma concentration of filamentlike dimensions. The energy stored in this pinch of plasma, which is at least 100 times as long as it is thick, is readily radiated because of the geometry of the apparatus. For this and other important reasons, such apparatus has been characterized by limitations as to themaximum temperature which may be achieved, it being difficult to supply energy at a rate sufficiently fast to permit the attaining of ultra high temperatures. Other limitations and defects of such toroidal-type plasma devices have included a relative instability of the plasma.

In view of the above factors characteristic of dischargetype devices for obtaining extremely high temperatures, and intense sources of light, it is an object of thepresent invention to provide an improved apparatus for generating a very high temperature, and in a highly efiicient manner.

A further object is to provide an improved apparatus for generating an extremely high temperature in a small volume approximating a point, through the use of a plurality of elements shaped as segments of a hollow spheroid and electrically insulated from each other, such segments each being continuous except for a' single gap or split therein.

These and other objects and advantages of the invention will be more fully set forth in the following specification and claims, considered in connection with the attached drawing to which they relate.

In the drawing:

Figure l is a perspective View illustrating an apparatus constructed in accordance with the present invention;

Figure 2 is a fragmentary perspective view showing a segment of the apparatus of Figure 1;

Figure 3 is a transverse section taken on line 3-3 of Figure 1; and

Figure 4 is aschematic illustration, in fragmentary ate 2,939,949 Patented May 31, 1960 form, of electrical circuit means associated with the apparatus of Figure 1.

.encompassing a cavity having the general shape of a sphere or spheroid. The electrical conductors between the poles of the sphere have been given the reference numeral 11, and the conductors at the poles have been given the reference numeral 12. The cavity, numbered 13, has a generally spherical or spheroidal wall 14 formed by the conductors 11 and 12 and by insulation '15 which separates the conductors. In order to maintain a substantial vacuum in the cavity 13, a spherical envelope 1? is provided and preferably has its outer Wall closely adjacent to cavity wall 14. The envelope is formed of quartz or other insulator.

Each of the conductors 11 and 12 forms part of a single-turn electrical circuit which extends from one side of a single gap or split 18 in each conductor 11 and 12, and thence around the conductor to the other side of the gap or split. In order to conduct current to and from the electrical conductors on opposite sides of the gaps 18, electrical conductor bars 19'are' provided.

Statedmore definitely, the conductors 1'1 and 12 comprise spherical segments of a single hollow sphere or tute the intermediate spherical segments. In the illustrated embodiment, the outer surfaces of the elements 11-, 12' and 15' comprise zones of a first sphere, and the inner surfaces thereof comprise zones of a second sphere having a smaller diameter but a common center. The last-mentioned sphere is the one which comprises the wall 14 of cavity 13.

The bars or conductors 19 are preferably integral with the conductors 11 and I2, and all' are formed of a good electrical conductor such as" copper. Correspondingly, the insulators 16sc'parating the bars 19 are illustrated as being integral with the*insu1ators+1'5 between the conductors 11 and 12.

As previously indicated, each conductor 11 or 12, together with the associated bars 19' on opposite sides of gap 18, comprises a single-turn electrical circuit about the common axis of the spherical segments 11 and 12.

When a very highcurrent is passed substantially simul taneouslythrough each conductor 11 and 12, during a very short period of time, a strong magnetic field is formed to result in acceleration of ionized particles in cavity '13, toward the center portion thereof. This effect, which. may be characterized as a radially-inwardly directed blast or implosion, generates a high temperature in a smallvolume approximating a point. In order to maintain the conductors and insulators in assembled condition despite the strong magnetic forces involved, it is Within thescope of the invention to suitably reinforce the apparatus such as by embedding the same [in a large block of strong insulating; material, which may be jacketed and reinforced at a location remote from the sphere.

Proceeding next to Figure 4, a capacitor means 2 1, of a low-inductance type, is connected by means of leads 22 across the bars 19" for each conductor '11 and 12. The dishcarge of each capacitor 21 is effected by a suitable trigger or switch means 23, under the control of a master control '24. The capacitors 21 are charged from a suit-- able DC. power source, indicated at 26. It is to be understood that a capacitor, trigger, etc. is provided for each pair of bars 19, although some have been omitted in Figure 4 for purposes of simplicity of illustration.

In" the operation of the apparatus, the capacitors 2].-

ments. After the capacitors 21 have been charged, and

after the power source has been disconnected therefrom by suitable means, not shown, the master control 24 is operated to effect closing of the circuits through trigger means 23. Each capacitor 21 thus discharges through a single-turn circuit comprising leads 22, bars 19, and the associated single conductor 11 or 12. The discharges of the capacitors 21 may be simultaneous, or at slightly different times, normally overlapping, within a very short time interval. The discharge currents flow in the same direction about the axis of the sphere.

With the described apparatus, the magnetic fields generated by the electrical currents may be accurately controlled by varying the amount of flow through each conductor 11 and 12, the charges on the respective capacitors 21, the times of discharge, etc. This provides the optimum field strength conditions within the cavity 13. The capacitors may, if desired, be charged from separate sources. It is within the scope of the invention to provide various numbers of conductors, various spacings therebetween, etc. 1

To amplify upon the previously-stated theory relative to the present invention, it is pointed out that the flow of current is in a given direction through the conductor means and circumferentially about the axis of the spheroidal cavity. This results inthe formation of an induced current sheet flowing in the opposite direction and through the gas. The induced current sheet is located within the evacuated cavity and is initially relatively close to the cavity wall formed by the conductor means. Thus, in the situation in which there is an envelope within the cavity, the induced current initially flows through the gas adjacent the inner wall of the envelope, it being remembered that the envelope is formed of non-conductive material.

The sheet of induced current, composed of ions and electrons, acts as a barricade through which the lines of.

' temperature occurs only at a geometrical point.

magnetic force may not pass in quantity. This is particularly true when the rate of change of magnetic field strength is great. This being the case, at least the majority of lines of magnetic force initially pass .(in a spheroidal configuration) between the conductor metal and the current sheet-or largely through the envelope in cases where there is an envelope.

- The generally spheroidal magnetic field acts as a piston to drive (implode) the current sheet, that is to say the ions and electrons, radially inwardly toward the center of the cavity. As the current sheet collapses toward the center, in a shock wave, the lines of magnetic force collapse toward the center (in the above-indicated piston action) to compress the gas, and greatly elevate its temperature because of the speed and collision of the particles. The inward movement continues until the external magnetic pressure is counterbalanced by the in ternal pressure resulting from compression and temperature increase.

Since the lines of magnetic force may not pass through the electrical conductor metal, the conductor is provided with openings (or non-conductors) at the poles of the cavity. The lines of force thus flow through the poles and externally of the spheroid to form continuous loops. As previously indicated, the reinforcing material in which the apparatus is embedded is non-conductive (except possibly in a casing remote from the sphere) and thus does not interfere with the external portions of the lines of force. l

I To aid in the above-described action, the gas within the cavity should be ionized before the capacitors commence to discharge. This may be done in any suitable manner, such as by passing radio-frequency waves through the cavity. For example, electrodes may be located near (but outside) the opening at each pole, and energized by a radio-frequency oscillator.

It is emphasized that the present invention produces a relatively stable concentration of high-temperature plasma near the. center of the cavity. The plasma is stable because the magnetic field is generated by the flow of current through the metal conductor. This is to be contrasted with pinch-type devices, in which the constricting magnetic field results from flow of current through the gas. In such pinch devices, instability resultingfrom variation in current flow is compounded by simultaneous variation in the magnetic field.

The present apparatus may be pulsed, for example at a relatively high frequency, instead, of being employed as a single-operation apparatus. This may be accomplished by rapidly charging and discharging the capacitors.

A feature of the present invention is that all of the lines of magnetic force need not pass through the openings (at the bases of the splits or gaps) in polar conductors 12. Instead, some of the lines of force pass through intermediate layers of insulation 15. This reexternally as segments of spheres. The conductors may be segments of bodies generally shaped as spheroids, such as prolate or oblate spheroids. Throughout this specification and claims, the use of the term spheroid includes not only elements which approach spheres, but also perfect spheres. e

. It is to be understood that the terms poin," approximating a point, etc., do not mean that the high- What is meant is that the highest concentration of plasma is in a small volume, as close to a point as possible. There may, however, be plasma concentrations of lesser density at regions other than the center of the cavity.

Various embodiments, of the present invention, in addition to what has been illustrated and described in detail, may be employed without departing from the scope of the accompanying claims.

1 I claim:

1. Apparatus for generating a very high temperature,

comprising a plurality of continuous hoop-like electrical conductors being electrically separate from each other whereby each defines a single turn of conductive material about said cavity.

. 2. Apparatus for'generating extremely high temperatures and intense light, comprising a plurality of generally parallel electrical conductors having openings shaped to form a spheroidal cavity, each of said conductors being formed with a gap or split at only one point therein to provide single-turn electric circuits around said cavity, and conductor means to conduct current to and from each of said conductors at opposite sides of the gap or split therein.

3. The invention as claimed in claim 2, in which means are provided to insulate said conductors from each other, and to maintain said cavity in a substantially evacuated condition.

- 4. The invention as claimed in claim 2, in which a source of current is connected separately to the conductor means for each of said conductors.

5. The invention as claimed in claim 4, in which said current source comprises a capacitor means connected across the conductor means for each of said conductors, and trigger means to effect discharge of said capacitor means in a single-turn circuit through said conductor means and the associated conductor.

6. Apparatus for creating a very high temperature in a small volume approximating a point, which comprises a plurality of electrical conductors and a plurality of insulators disposed in alternate, parallel relationship and shaped generally as spherical segments of a single hollow sphere, said segments each having a single split or gap therein and creating a single split or gap throughout substantially an entire great semi-circle of said hollow sphere, means to maintain the cavity within said hollow sphere in a substantially evacuated condition, and electrically-conductive bars connected to said segments at points on opposite sides of the splits or gaps therein, said bars extending outwardly from said segments in general- 1y parallel relationship, each of said segments being continuous except at said gap to provide a single-turn electrical circuit around said cavity through which large amounts of current may be passed instantaneously to effect acceleration of ionized particles in said cavity to- 20 2,030,957

ward the center portion thereof.

7. The invention as claimed in claim 6, in which means are provided to supply large amounts of current to each of said segments through the bars therefor and in a substantially instantaneous manner, said means comprising separate capacitor means connected across the bars for each of said conductive segments, trigger means to control discharge of said capacitor means through said segments, control means to operate said trigger means and to time the discharge of the capacitor means, and means to charge said capacitor means.

8. The invention as claimed in claim 7, in which said current supply means is adapted upon discharge of the capacitor means to effect current flow through all of said segments in the same direction about the axis thereof.

References Cited in the file of this patent UNITED STATES PATENTS 966,204 Hewitt Aug. 2, 19.10 1,698,691 Buttolph Jan. 8, 1929 Bethenod et a1. Feb. 18, 1936 2,149,414 Bethenod Mar. 7, 1939

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US966204 *Jul 20, 1904Aug 2, 1910Cooper Hewitt Electric CoInduction-lamp.
US1698691 *Jul 1, 1926Jan 8, 1929Cooper Hewitt Electric CoHigh-intensity induction lamp
US2030957 *Dec 29, 1933Feb 18, 1936Ets Claude Paz & SilvaElectromagnetic apparatus
US2149414 *Oct 14, 1935Mar 7, 1939Ets Claude Paz & SilvaInduction excitation of electric discharge tubes
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US3006835 *Feb 25, 1959Oct 31, 1961William C ElmoreNeutron source using magnetic compression of plasma
US3107211 *Jan 25, 1960Oct 15, 1963Mallinckrodt George ENuclear apparatus
US3361930 *Jun 27, 1966Jan 2, 1968Tobe Deutschmann Lab IncDischarge gap means including a spiral capacitor surrounding opposed electrodes
US3437862 *Jul 19, 1957Apr 8, 1969Zenith Radio CorpMethod and apparatus for producing high temperatures by a magnetic field surrounding an electric arc
US3469144 *Oct 4, 1965Sep 23, 1969Martin Marietta CorpArrangement of electrical components to define a low inductance plasma generating apparatus
US4156832 *Feb 25, 1977May 29, 1979Ultra Centrifuge Nederland N.V.Gas vortex with MHD-drive
US4171503 *Jan 16, 1978Oct 16, 1979Kwon Young DElectrodeless fluorescent lamp
US4240010 *Jun 18, 1979Dec 16, 1980Gte Laboratories IncorporatedElectrodeless fluorescent light source having reduced far field electromagnetic radiation levels
US4254363 *Dec 22, 1978Mar 3, 1981Duro-Test CorporationElectrodeless coupled discharge lamp having reduced spurious electromagnetic radiation
US4365622 *Sep 11, 1980Dec 28, 1982Donald L. Morton & AssociatesMultiple plate resonant electrode
US4374516 *Feb 23, 1981Feb 22, 1983Harrison William HPlanar disc magnetic electrode
US5039903 *Mar 14, 1990Aug 13, 1991General Electric CompanyExcitation coil for an electrodeless high intensity discharge lamp
U.S. Classification315/236, 376/149, 313/161, 315/240, 315/248, 219/780, 315/244, 315/241.00R, 315/173, 376/107
International ClassificationH05H1/02, H05H1/04
Cooperative ClassificationH05H1/04
European ClassificationH05H1/04