US2163740A - Phase wave ion gun - Google Patents
Phase wave ion gun Download PDFInfo
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- US2163740A US2163740A US51580A US5158035A US2163740A US 2163740 A US2163740 A US 2163740A US 51580 A US51580 A US 51580A US 5158035 A US5158035 A US 5158035A US 2163740 A US2163740 A US 2163740A
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- charged particles
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- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H5/00—Direct voltage accelerators; Accelerators using single pulses
Definitions
- This invention relates to the acceleration of charged particles by electrostatic impulses.
- I disclose a method of utilizing the piezo-electric differences of potential appearing 5 periodically on the faces of a series of piezo crystals under oscillatory pressure in such a way as to successively accelerate through said differences of potential groups of ions passing along this series.
- my method attains its 10 objects by allowing for the decreasing time intervals subtended by successive equidistant points along the path of an accelerating particle through the use of phase difierences of the oscillating electrostatic generators, whether they be 15 piezo-electric or otherwise, so adjusted that the field of any given generator will attain a maximum potential difierence at a time corresponding to the' arrival of the accelerating charged particle within the locus of said field.
- the several objects in this invention is that it is desirable to attain ions or charged particles of high kinetic energy for purposes of transmutation, and for the induction of radioactivity.
- My invention allows a potential drop on the order of 25 10,000 voltssuch as that appearing on piezo crystals under relatively small displacements to be successively applied to the accelerating ion or charged particle until it has attained an energy equivalent corresponding to as many 30 times a multiple of this incremental piezo drop as there are composite sections in the apparatus.
- the apparatus satisfying the former object be compact and of light weight.
- This invention is unique in size and weight as compared to other electrostatic accelerators.
- a further object is to obviate the necessity of using excessive input potentials to the accelerating apparatus.
- FIG. 50 The figure shows a broken section in side elevation of the assembly of the cylindrical chamber of the"gun which illustrates my invention and with the external parts of the associated electrical system shown in schematic diagram.
- the cylindrical aluminum casing I is sealed at the one end by an insulating disk I I and gasket I'l secured thereto by cap screws l and at the other end by the plate l4, gasket I3 and cap screws I6, altogether forming with exhaust tube I a chamber capable of sup- 5 porting a high vacuum when the source of, ions used so permits.
- a coated filament 9 has been chosen for simplicity as a source of ions. This filament has its leads brought through the insulating sup- 10 port lI within gromets I2 forming with them a soldered and crimped seal.
- the annular plate I and control grid 8 are similarly supported, and together with the filament 9 form a source of low velocity ions axially collimated down the casing I and capable of modulation by potentials impressed on control grid 8.
- a series of rigid insulating annuli 6 which centralize and axially space a series of rigid steel annuli 2, thus forming a series of insulated annular partitions incapable of longitudinal displacement of any moment.
- the multiple nature of these partitions is illustrated by the broken casing and circuit'at I8.
- a piezo crystal 3 of Rochelle salt for instance, in annular form, and subject to the axial pressure which may result from a magneto strictive longitudinal extension of the nickel alloy ring 5, positioned to bear upon said crystal 3.
- each ring, 5 Concentrically surrounding each ring, 5, is an energizing field winding, t, capable of inducing and maintaining magneto-strictive oscillation in these rings, especially at the natural mechanical resonant frequency.
- the electrical leads for each field winding pass through conduits I9 to enter into the series transmission circuit comprising the coupling inductance L3, parallel condensers Cl, C2, C3, C4, C5 and C6, spanning one side of the line and the series field elements 4.
- any wave form of electric displacement induced in L3 will travel down the lineto supply oscillatory energy to the inductances Q in turn, and if sustained in periodic succession each magneto-striction ring 5 will respond at the frequency induced in L3.
- phase of this response relative to the preceding one in any given field coil 4 will be a function of its position in the artificial transmission line and of the capacitance of the parallel condenser preceding 5 it. In that the characteristics of this line are adjustable, the phase of each section may be made to lag behind or to advance ahead any fraction of its period beyond its preceding section in the series.
- the oscillator E3 is coupled 5 to La and In by the inductance L1.
- the inductance La is made to impress the oscillations of L1, 011 a control grid circuit comprising bias resistor R and grid condenser C1.
- E: and E supply the filament and plate with potentials suitable to maintain their ionic beam.
- a quantum of ions leaves the plate 1 and is projected into the axial space between the faces 01' the first piezo crystal.
- the antinodal maximum which released said quantum from the space cloud of ions near the filament is arranged by the relative'phasing efi'ected by C1 to bring pressure on said crystal only at a time calculated to allow for ,the arrival of said quantum within the electrodes oi the first 01. said electrostatic generators. Consequently, although there has been no appreciable retarding of the approaching charged group-oi particles, this quantum suddenly finds itself in a region of high potential gradient through which it proceeds to fall with an attendant gain in kinetic energy.
- a device to electrostatically accelerate charged particles comprising a source of charged particles, a plurality of electrostatic generators sequentially aligned to form a-path of acceleration for said particles, said generators having relative phase of potential means to form an accelerating region of maximum potential gradient to accelerate said charged particles along'said 6 path.
- a device to electrostatically accelerate charged particles comprising a source oi charged in said generators, and means thereby to maintain an accelerating maximum gradient of potential along said path to accell6 erate said charged particles.
- a device to electrostatically accelerate charged particles comprising a source 01' charged particles, a plurality of electrostatic generators,
- a plurality oi aligned electrodes connected there- 20 charged particles comprising a source oi. charged particles, a plurality of piezo electric crystal generators, an alignment of electrically impress said generators thereon, said alignment forming a path for said particles, and relative phase means of compression on said crystals to produce an accelerating region of maximum potential gradient on said path to acll celerate said particles therealong.
- the combination in a systemto produce electrostatic acceleration of charged particles comprising a source of charged particles, 9. plurality of oscillatory electrostatic generators, eleco trodes for said generators aligned to form a path for said particles, means to impress the oscillatory potentials of said generators sequentially on said electrodes to produce a maximum of potential gradient to move along said path and effective to accelerate the motion of said particles thereon.
- a device to electrostatically accelerate charged particles comprising a source of said charged particles, a plate for collimating said charged particles, a grid for controlling the fiow of said charged particles, an alignment of electrodes to form a path for said particles, a plurality of piezo electric generators, means for impressing the potentials of said generators on said electrodes, a magnetostriction element for exciting each piezo electric generator, electromagnetic means for exciting said magnetostriction elements, and means for adjusting the relative phases of said electromagnetic meansto produce 5 a maximum of potential gradient to move along said path to accelerate said particles.
Description
June 27, 1939. N. B. WALES, JR
PHASE WAVE ION GUN Original Filed NOV. 26, 1935 INVENTOR m Q t vim w as ssms Patented June 27, 1939 PHASE WAVE ION GUN Nathaniel B. Wales, Jr., New York, N. Y.
Application November 26, 1935, Serial No. 51,580 Renewed January 9, 1939 6 Claims.
This invention relates to the acceleration of charged particles by electrostatic impulses. In particular, I disclose a method of utilizing the piezo-electric differences of potential appearing 5 periodically on the faces of a series of piezo crystals under oscillatory pressure in such a way as to successively accelerate through said differences of potential groups of ions passing along this series. Specifically, my method attains its 10 objects by allowing for the decreasing time intervals subtended by successive equidistant points along the path of an accelerating particle through the use of phase difierences of the oscillating electrostatic generators, whether they be 15 piezo-electric or otherwise, so adjusted that the field of any given generator will attain a maximum potential difierence at a time corresponding to the' arrival of the accelerating charged particle within the locus of said field. Among 20 the several objects in this invention is that it is desirable to attain ions or charged particles of high kinetic energy for purposes of transmutation, and for the induction of radioactivity. My invention allows a potential drop on the order of 25 10,000 voltssuch as that appearing on piezo crystals under relatively small displacements to be successively applied to the accelerating ion or charged particle until it has attained an energy equivalent corresponding to as many 30 times a multiple of this incremental piezo drop as there are composite sections in the apparatus.
It is also desirable that the apparatus satisfying the former object be compact and of light weight. This invention is unique in size and weight as compared to other electrostatic accelerators.
A further object is to obviate the necessity of using excessive input potentials to the accelerating apparatus.
40 In the following specification, I shall disclose a clear and complete exposition of the construction and operation of my invention. It is understood that the method, as well as the specific structure involved in this invention,
4 comprises its novelty. Considering now the drawing as illustrative of one exemplification of my invention where in like numerals in the specification and drawing refer to corresponding parts.
50 The figure shows a broken section in side elevation of the assembly of the cylindrical chamber of the"gun which illustrates my invention and with the external parts of the associated electrical system shown in schematic diagram.
.5 Referring to the figure, the cylindrical aluminum casing I is sealed at the one end by an insulating disk I I and gasket I'l secured thereto by cap screws l and at the other end by the plate l4, gasket I3 and cap screws I6, altogether forming with exhaust tube I a chamber capable of sup- 5 porting a high vacuum when the source of, ions used so permits. In this examplification of my principle a coated filament 9 has been chosen for simplicity as a source of ions. This filament has its leads brought through the insulating sup- 10 port lI within gromets I2 forming with them a soldered and crimped seal. The annular plate I and control grid 8 are similarly supported, and together with the filament 9 form a source of low velocity ions axially collimated down the casing I and capable of modulation by potentials impressed on control grid 8. Within the casing I are enclosed a series of rigid insulating annuli 6 which centralize and axially space a series of rigid steel annuli 2, thus forming a series of insulated annular partitions incapable of longitudinal displacement of any moment. The multiple nature of these partitions is illustrated by the broken casing and circuit'at I8. Within each partition, there is arranged a piezo crystal 3 of Rochelle salt, for instance, in annular form, and subject to the axial pressure which may result from a magneto strictive longitudinal extension of the nickel alloy ring 5, positioned to bear upon said crystal 3.
Concentrically surrounding each ring, 5, is an energizing field winding, t, capable of inducing and maintaining magneto-strictive oscillation in these rings, especially at the natural mechanical resonant frequency. The electrical leads for each field winding pass through conduits I9 to enter into the series transmission circuit comprising the coupling inductance L3, parallel condensers Cl, C2, C3, C4, C5 and C6, spanning one side of the line and the series field elements 4. Evidently any wave form of electric displacement induced in L3 will travel down the lineto supply oscillatory energy to the inductances Q in turn, and if sustained in periodic succession each magneto-striction ring 5 will respond at the frequency induced in L3. However, the phase of this response relative to the preceding one in any given field coil 4 will be a function of its position in the artificial transmission line and of the capacitance of the parallel condenser preceding 5 it. In that the characteristics of this line are adjustable, the phase of each section may be made to lag behind or to advance ahead any fraction of its period beyond its preceding section in the series. The oscillator E3 is coupled 5 to La and In by the inductance L1. The inductance La is made to impress the oscillations of L1, 011 a control grid circuit comprising bias resistor R and grid condenser C1. E: and E, supply the filament and plate with potentials suitable to maintain their ionic beam.
The operation of my invention is as follows: A quantum of ions leaves the plate 1 and is projected into the axial space between the faces 01' the first piezo crystal. The antinodal maximum which released said quantum from the space cloud of ions near the filament is arranged by the relative'phasing efi'ected by C1 to bring pressure on said crystal only at a time calculated to allow for ,the arrival of said quantum within the electrodes oi the first 01. said electrostatic generators. Consequently, although there has been no appreciable retarding of the approaching charged group-oi particles, this quantum suddenly finds itself in a region of high potential gradient through which it proceeds to fall with an attendant gain in kinetic energy. At the'region of departure from this electrostatic locus, the ordinary retarding force which would obtain with the recession of a charged particle from an op positely charged plane is absent due to the disappearance of the piezo field with the recession of the compressive antinode, and only a negligible image field remains to retard the increased velocity of this accelerated group of particles. This cycle of operations is continued with a phase difference for successive sections calculated to correspond to the decreasing periods of transit attendant upon the passage of equidistant points by an accelerating point. The theoretical limit tothe velocities so attained is determined by the frequency at which the period, is equal to the period of transit for the first of the series of piezo fields. Practically the limit is determined by the natural period associated with magnetostriction elements oi structural convenience.
It is desired to emphasize that the novel principle involved, together with the novel means used to incorporate it, is in brief the use of discrete electrostatic generators of oscillatory po-' tential so phased as to cause a gradient of potential to obtain at points so disposed and at such times as to coincide with the path of an accelerating particle. The particular structure here disclosed may also be paralleled in its satisfaction of the principle by an annular column of electrets controlled in phase by an oscillatory neutralization of their fields under scansion 0! their associated electrodes by a cathode beam. Or similarly, the principle of discrete generators may be satisfied by the photoelectric charges oscillatorily deposed on an annular column of electrodes scanned as above by a phasing cathode or ultra violet beam.
What I claimand desire to secure by United States Letters Patent is:
1. A device to electrostatically accelerate charged particles, comprising a source of charged particles, a plurality of electrostatic generators sequentially aligned to form a-path of acceleration for said particles, said generators having relative phase of potential means to form an accelerating region of maximum potential gradient to accelerate said charged particles along'said 6 path.
2. A device to electrostatically accelerate charged particles, comprising a source oi charged in said generators, and means thereby to maintain an accelerating maximum gradient of potential along said path to accell6 erate said charged particles.
3. A device to electrostatically accelerate charged particles, comprising a source 01' charged particles, a plurality of electrostatic generators,
a plurality oi aligned electrodes connected there- 20 charged particles, comprising a source oi. charged particles, a plurality of piezo electric crystal generators, an alignment of electrically impress said generators thereon, said alignment forming a path for said particles, and relative phase means of compression on said crystals to produce an accelerating region of maximum potential gradient on said path to acll celerate said particles therealong.
5. The combination in a systemto produce electrostatic acceleration of charged particles, comprising a source of charged particles, 9. plurality of oscillatory electrostatic generators, eleco trodes for said generators aligned to form a path for said particles, means to impress the oscillatory potentials of said generators sequentially on said electrodes to produce a maximum of potential gradient to move along said path and effective to accelerate the motion of said particles thereon.
6. A device to electrostatically accelerate charged particles, comprising a source of said charged particles, a plate for collimating said charged particles, a grid for controlling the fiow of said charged particles, an alignment of electrodes to form a path for said particles, a plurality of piezo electric generators, means for impressing the potentials of said generators on said electrodes, a magnetostriction element for exciting each piezo electric generator, electromagnetic means for exciting said magnetostriction elements, and means for adjusting the relative phases of said electromagnetic meansto produce 5 a maximum of potential gradient to move along said path to accelerate said particles.
NATHANIEL B. WALES, JR.
said path and to-accelerate l3 electrodes, means to U
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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US51580A US2163740A (en) | 1935-11-26 | 1935-11-26 | Phase wave ion gun |
Applications Claiming Priority (1)
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US51580A US2163740A (en) | 1935-11-26 | 1935-11-26 | Phase wave ion gun |
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US2163740A true US2163740A (en) | 1939-06-27 |
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US51580A Expired - Lifetime US2163740A (en) | 1935-11-26 | 1935-11-26 | Phase wave ion gun |
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Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2420514A (en) * | 1944-05-25 | 1947-05-13 | Gen Electric | Electron lens structure |
US2460109A (en) * | 1941-03-25 | 1949-01-25 | Bell Telephone Labor Inc | Electrical translating device |
US2489082A (en) * | 1944-07-01 | 1949-11-22 | Forest Lee De | High-voltage generator |
US2545595A (en) * | 1947-05-26 | 1951-03-20 | Luis W Alvarez | Linear accelerator |
US2570124A (en) * | 1949-10-20 | 1951-10-02 | Rca Corp | Positive ion beam gun |
US2740913A (en) * | 1951-11-01 | 1956-04-03 | Itt | Electron gun |
US2988642A (en) * | 1958-06-30 | 1961-06-13 | Schlumberger Well Surv Corp | Particle accelerating system |
US3085189A (en) * | 1951-08-10 | 1963-04-09 | Thonemann Peter Clive | Energy-transfer systems |
US3086385A (en) * | 1958-10-15 | 1963-04-23 | Saint Gobain | Furnace adapted for use in dilatometry |
US3184632A (en) * | 1961-02-28 | 1965-05-18 | Gen Telephone & Elect | Wave generator with time-variant electric potential distribution |
-
1935
- 1935-11-26 US US51580A patent/US2163740A/en not_active Expired - Lifetime
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2460109A (en) * | 1941-03-25 | 1949-01-25 | Bell Telephone Labor Inc | Electrical translating device |
US2420514A (en) * | 1944-05-25 | 1947-05-13 | Gen Electric | Electron lens structure |
US2489082A (en) * | 1944-07-01 | 1949-11-22 | Forest Lee De | High-voltage generator |
US2545595A (en) * | 1947-05-26 | 1951-03-20 | Luis W Alvarez | Linear accelerator |
US2570124A (en) * | 1949-10-20 | 1951-10-02 | Rca Corp | Positive ion beam gun |
US3085189A (en) * | 1951-08-10 | 1963-04-09 | Thonemann Peter Clive | Energy-transfer systems |
US2740913A (en) * | 1951-11-01 | 1956-04-03 | Itt | Electron gun |
US2988642A (en) * | 1958-06-30 | 1961-06-13 | Schlumberger Well Surv Corp | Particle accelerating system |
US3086385A (en) * | 1958-10-15 | 1963-04-23 | Saint Gobain | Furnace adapted for use in dilatometry |
US3184632A (en) * | 1961-02-28 | 1965-05-18 | Gen Telephone & Elect | Wave generator with time-variant electric potential distribution |
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