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US2067966A - Electron discharge device - Google Patents

Electron discharge device Download PDF

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US2067966A
US2067966A US21534A US2153435A US2067966A US 2067966 A US2067966 A US 2067966A US 21534 A US21534 A US 21534A US 2153435 A US2153435 A US 2153435A US 2067966 A US2067966 A US 2067966A
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anode
discharge
anodes
electrodes
pair
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US21534A
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Klemperer Hans
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RCA Corp
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RCA Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J3/00Details of electron-optical or ion-optical arrangements or of ion traps common to two or more basic types of discharge tubes or lamps
    • H01J3/02Electron guns
    • H01J3/025Electron guns using a discharge in a gas or a vapour as electron source
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2893/00Discharge tubes and lamps
    • H01J2893/0061Tubes with discharge used as electron source
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10STECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10S29/00Metal working
    • Y10S29/066Fluid flow to channeled cutter

Definitions

  • My invention relates to electron discharge devices of the gaseous type, more particularly to such devices using an are as a source of electrons.
  • the discharge takes place between a pair of electrodes separate and distinct from the output anode, and a control grid is interposed between the anode and the arc discharge to control the electron flow to the output anode.
  • the conventional tubes of this type have so far been unsatisfactory in oscillating circuits particularly in radio frequency circuits because of the large and variable lag of the controlled electron current behind the controlling voltage.
  • the preferred embodiment of my invention Comprises an envelope containing a pair of electrodes and an ionizable medium at a pressure such that a self-sustaining discharge may be maintained in a path between the electrodes and a pair of output anode members positioned on opposite sides of the discharge path.
  • each of the anodes being completely shielded from the discharge by a shield and a control grid spaced from the anode a distance less than the mean free path of a positive ion in the ionizable medium under operating conditions of the electron discharge device.
  • FIG. 5 1 is a Vertical section of. an electron discharge device shown diagrammatically and embodying one form of my invention
  • Figure 2 is a section of a modification of the oscillation anode used in the electron discharge device shown in Figure 1
  • Figure 3 is a diagrammatic representation of an electron discharge device made in accordance with my invention incorporated in an oscillating circuit.
  • the electron discharge device has an evacuated envelope Ill provided at one end with a press I l.
  • the self-sustaining discharge is maintained between a thermionic cathode l2 in the press and a main anode l3 supported in an arm M at one side of the envelope.
  • the gaseous atmosphere for supporting the self-sustaining discharge between these two electrodes when proper operating voltages are applied. may be any inert gas such as argon and the like, although I prefer a mercury vapor atmosphere supplied by a few drops of mercury IS in the bottom of the tube.
  • the vapor within the tube is ionized and the discharge between the cathode l2 and anode l3 initiated by an auxiliary control electrode Hi. When once established the arc will maintain itself as long as the operating voltage is maintained.
  • I mount on opposite sides of the discharge path between the electrodes l2 and I3 a pair of oscillation anodes I1 and 18 with control grids l9 and 20 interposed between the anodes and the discharge .path.
  • the control grids preferably cover the anodes and may for example be hemispherical as shown in the drawing.
  • the spacing between the anodes l1 and I8 and their control grids l9 and 20 is less than the mean free path of a positive ion in the ionizable medium under operating conditions of the tube to prevent any chances of suflicient ionization to support a self-sustaining 5 discharge in this space.
  • the oscillation anodes and the control grids may be supported in any convenient manner, preferably by mounting the anodes on support leads 2
  • the anode leads and grid conductors may be carried path is not. critical, I have found for best results that the distance between these anodes andthe arc discharge path should be less than one-half but greater than oneequarter of the distance between the cathode l2 and anode l3.
  • M should be less than the distance N but greater than one-half the distance N. If the anodes are spaced too close to the arc discharge, loss of control will result and instead of obtaining a pure electron flow an arc discharge will take place between cathode l2 and the oscillator anodes, thus interfering with the proper operation of the tube at radio frequencies.
  • the electrons available will be insuflicient for proper functioning of the tube and if an attempt is made to increase the number of electrons to the oscillator anodes by raising the voltage on the anodes an arc discharge to these anodes may take place.
  • a screen grid may be placed between the anode and the control grid. This arrangement will decrease the liability of an arc discharge be tween the oscillator anode and the arc discharge path and by reducing the control grid to oscillator anode capacity will increase the upper frequency at which the tube will operate.
  • FIG. 2 I have shown the oscillator anode provided with a screen grid.
  • the anode 39 is supported by means of the support and lead conductor 31 mounted in an extension 32 of an envelope.
  • Surrounding the support is the tubular shield and grid lead 33 supporting the disc member 34 and screen grid 35.
  • Concentric with the tube 33 is the outer shield and grid lead 36 supporting the disc-like member 31 and the control grid 38. Insulating members 39 properly separate the shields 33 and 36 and conductor 3
  • Voltage is applied between the cathode l2 and the main ano'de I3 thru resistor 40 from the voltage supply source.
  • the arc is self-sustaining but can be interrupted by removing the anode voltage.
  • the oscillator anodes l1 and I8 are con nected to opposite sides of an oscillating circuit comprising an inductance 45 and-variable condenser 46 by means of which the frequency of the oscillating circuit can be changed.
  • Voltage is applied to the anodes l1 and I8 thru a choke 41 when switch 48 is closed to complete a circuit to the voltage supply source 49.
  • the control grids I9 and 20 are connected to opposite ends of an inductance 50 coupled to the oscillating circuit to provide oscillations when switch 5! is closed to apply a voltage to the grids from the voltage supply source 52 thru choke 53.
  • This circuit operates in the well-known push-pull fashion. The frequency range can be varied by changing the condenser setting.
  • An electron discharge device having an an velope containing a pair of electrodes and an ionizable medium for supporting a self-sustaindischarge between said pair of electrodes, an anode within said envelope spaced to one side of the discharge path between said pair of electrodes at a distance greater than one fourth the distance between said pair of electrodes, a control electrode over said anode and shielding all parts of the anode from said discharge for controlling the electron current to said anode, the distance between said anode and said control electrode being less than the mean free path of positive ions in the ionizable medium during operation of the electron discharge device.
  • An electron discharge device having an envelopecontaining a pair of electrodes and an ionizable medium for supporting a self-sustaining discharge between said pair of electrodes, a pair of oppositely disposed anodes positioned.- on opposite sides of the path of said discharge between said pair of electrodes and spaced therefrom, and a control electrode over each of said anodes and shielding all parts of the anode from said discharge the distance between said anodes being less than the distance between said pair of electrodes but greater than one-half the distance between said pair of electrodes.
  • An electron discharge device having an envelope containing a pair of electrodes, and an ionizable medium for supporting a self-sustaining discharge between said pair of electrodes, an anode within said envelope spaced to one side of the discharge path between said pair of electrodes a distance less than half but more than a quarter of the distance between said pair of electrodes and having a support rod supported from the wall of said envelope, a shield surrounding said sup- 7;
  • An electron discharge device having an envelope containing a pair of electrodes and an ionizable medium for supporting a self-sustaining discharge between said pair of electrodes, an anode within said envelope spaced to one side of the discharge path between said pair of electrodes and having a support rod supported from the wall of said envelope, a shield surrounding said support rod and provided with a foraminous portion over the anode, a second shield between said sup port rod and said first shield and provided with a foraminous portion between the foraminous portion on said first shield and the surface of said anode.

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  • Electron Sources, Ion Sources (AREA)

Description

Jan. 19, 1937. H. KLEMPERER ELECTRON DISCHARGE DEVICE Filed May 15, 1935 INVENTOR HANS KLEMPERER Patented Jan. 19, 1937 ELECTRON DISCHARGE DEVICE Hans Klcmperer, Summit, N J., assignor, by mesne assignments, to Radio Corporation of America, a corporation of Delaware Application May 15, 1935, Serial No. 21,534
4 Claims.
My invention relates to electron discharge devices of the gaseous type, more particularly to such devices using an are as a source of electrons.
In one form of conventional electron discharge device in which an arc is established in a gaseous atmosphere to provide a source of electrons, the discharge takes place between a pair of electrodes separate and distinct from the output anode, and a control grid is interposed between the anode and the arc discharge to control the electron flow to the output anode. The conventional tubes of this type have so far been unsatisfactory in oscillating circuits particularly in radio frequency circuits because of the large and variable lag of the controlled electron current behind the controlling voltage.
for the generation of high frequency oscillations. and has not been practical for amplification of audio frequencies because of the difficulty of obtaining constant amplification characteristics between zero current and the arc-over point, particularly with low frequency alternating voltages app ied to the control grid. Furthermore, because of the heavy grid current drawn by these tubes the power dissipated in the grid circuit has been very high, making these tubes inefiicient.
It is the principal object of my invention to provide an improved type of gas discharge tube using an arc to provide a source of electrons.
It is a further object of my invention to provide such a tube which is satisfactory at radio frequencies, is efficient in operation, and has a large power output.
The preferred embodiment of my invention Comprises an envelope containing a pair of electrodes and an ionizable medium at a pressure such that a self-sustaining discharge may be maintained in a path between the electrodes and a pair of output anode members positioned on opposite sides of the discharge path. each of the anodes being completely shielded from the discharge by a shield and a control grid spaced from the anode a distance less than the mean free path of a positive ion in the ionizable medium under operating conditions of the electron discharge device. By' properly spacing the'anodes with respect to the arc discharge path I am able to obtain at radio frequencies accurate control similar to that of a high vacuum tube having a thermionic cathode as a source of electrons. The tube is particularly suitable for the generation of high frequency oscillations and has a large power output.
The novel features which I believe to be char- Because of this lag the use of this type of tube has not been feasible acteristic of my invention are set forth with particularity in the appended claims, but the invention itself will best be understood by reference to the following description taken in connection with the accompanying drawing in which Figure 5 1 is a Vertical section of. an electron discharge device shown diagrammatically and embodying one form of my invention; Figure 2 is a section of a modification of the oscillation anode used in the electron discharge device shown in Figure 1; and Figure 3 is a diagrammatic representation of an electron discharge device made in accordance with my invention incorporated in an oscillating circuit.
In Figure 1 the electron discharge device has an evacuated envelope Ill provided at one end witha press I l. The self-sustaining discharge is maintained between a thermionic cathode l2 in the press and a main anode l3 supported in an arm M at one side of the envelope. The gaseous atmosphere for supporting the self-sustaining discharge between these two electrodes when proper operating voltages are applied. may be any inert gas such as argon and the like, although I prefer a mercury vapor atmosphere supplied by a few drops of mercury IS in the bottom of the tube. The vapor within the tube is ionized and the discharge between the cathode l2 and anode l3 initiated by an auxiliary control electrode Hi. When once established the arc will maintain itself as long as the operating voltage is maintained.
In accordance with my invention I mount on opposite sides of the discharge path between the electrodes l2 and I3 a pair of oscillation anodes I1 and 18 with control grids l9 and 20 interposed between the anodes and the discharge .path. The control grids preferably cover the anodes and may for example be hemispherical as shown in the drawing. The spacing between the anodes l1 and I8 and their control grids l9 and 20 is less than the mean free path of a positive ion in the ionizable medium under operating conditions of the tube to prevent any chances of suflicient ionization to support a self-sustaining 5 discharge in this space. The oscillation anodes and the control grids may be supported in any convenient manner, preferably by mounting the anodes on support leads 2| and 22 and the grids on tubular grid leads 23 and 24 surrounding and shielding the anode leads and having on their inner ends disc members 25 and 26 to which the grids are secured and connected at their other ends to grid leading-in wires 21 and 28. The anode leads and grid conductors may be carried path is not. critical, I have found for best results that the distance between these anodes andthe arc discharge path should be less than one-half but greater than oneequarter of the distance between the cathode l2 and anode l3. If the disstance between the cathode l2 and anode I3 is represented by N and the distance between the oppositely disposed oscillator anodes is represented by M, then M should be less than the distance N but greater than one-half the distance N. If the anodes are spaced too close to the arc discharge, loss of control will result and instead of obtaining a pure electron flow an arc discharge will take place between cathode l2 and the oscillator anodes, thus interfering with the proper operation of the tube at radio frequencies. If the anodes are placed too far away from the arc discharge path, the electrons available will be insuflicient for proper functioning of the tube and if an attempt is made to increase the number of electrons to the oscillator anodes by raising the voltage on the anodes an arc discharge to these anodes may take place.
In one example of my'invention making use of mercury vapor and with a voltage of between 2Q and 25 volts applied between the-cathode l2 and anode I3, I have found that with a mesh grid of 10 mil. wire spaced approximately 1 or 2 millimeters apart and with the distance between the anode and the mesh control grid of the order of 2 millimeters a bias voltage of plus 3 volts on the grid will give very good control with oscillator anode voltages between zero and the voltage ap plied between the main anode l3 and the cathode l2.
If it is found desirable to have the oscillator anodes closer to the discharge path or if the capacity between the control grid and .the anode limits the upper frequency at which the tube will operate, a screen grid may be placed between the anode and the control grid. This arrangement will decrease the liability of an arc discharge be tween the oscillator anode and the arc discharge path and by reducing the control grid to oscillator anode capacity will increase the upper frequency at which the tube will operate.
In Figure 2 I have shown the oscillator anode provided with a screen grid. The anode 39 is supported by means of the support and lead conductor 31 mounted in an extension 32 of an envelope. Surrounding the support is the tubular shield and grid lead 33 supporting the disc member 34 and screen grid 35. Concentric with the tube 33 is the outer shield and grid lead 36 supporting the disc-like member 31 and the control grid 38. Insulating members 39 properly separate the shields 33 and 36 and conductor 3|.
While I have shown the grid conductors or anode shields in Figures 1 and 2 as concentric metal tubes, the capacity introduced by these metal tubes can be reduced either by shortening of the extensions 29, 30 and 32 and thus shortening the supports and shields, or I may make these shields of insulating material.
While not limited thereto I prefer to use the electron discharge device embodied in my invention in the type of circuit shown in Figure 3.
Voltage is applied between the cathode l2 and the main ano'de I3 thru resistor 40 from the voltage supply source. The are discharge between the cathode |2 which is energized from a source of voltage 42, and the main anode i3 is initiated when switch 43 is closed to connect the supply voltage source 44 to the auxiliary grid l6. After it is established, the arc is self-sustaining but can be interrupted by removing the anode voltage. The oscillator anodes l1 and I8 are con nected to opposite sides of an oscillating circuit comprising an inductance 45 and-variable condenser 46 by means of which the frequency of the oscillating circuit can be changed. Voltage is applied to the anodes l1 and I8 thru a choke 41 when switch 48 is closed to complete a circuit to the voltage supply source 49. The control grids I9 and 20 are connected to opposite ends of an inductance 50 coupled to the oscillating circuit to provide oscillations when switch 5! is closed to apply a voltage to the grids from the voltage supply source 52 thru choke 53. This circuit operates in the well-known push-pull fashion. The frequency range can be varied by changing the condenser setting.
While I have indicated the preferred embodiment of my invention of which I am now aware and have also indicated only one specific application for which my invention may be employed, it will be apparent that my invention is by no means limited to the exact forms illustrated or the use indicated, but that many variations may be made .in the particular structure used and the purpose for which it is employed without departing from the scope of my invention as set forth in the appended claims.
I claim:
1. An electron discharge device having an an velope containing a pair of electrodes and an ionizable medium for supporting a self-sustaindischarge between said pair of electrodes, an anode within said envelope spaced to one side of the discharge path between said pair of electrodes at a distance greater than one fourth the distance between said pair of electrodes, a control electrode over said anode and shielding all parts of the anode from said discharge for controlling the electron current to said anode, the distance between said anode and said control electrode being less than the mean free path of positive ions in the ionizable medium during operation of the electron discharge device.
2. An electron discharge device having an envelopecontaining a pair of electrodes and an ionizable medium for supporting a self-sustaining discharge between said pair of electrodes, a pair of oppositely disposed anodes positioned.- on opposite sides of the path of said discharge between said pair of electrodes and spaced therefrom, and a control electrode over each of said anodes and shielding all parts of the anode from said discharge the distance between said anodes being less than the distance between said pair of electrodes but greater than one-half the distance between said pair of electrodes.
3. An electron discharge device having an envelope containing a pair of electrodes, and an ionizable medium for supporting a self-sustaining discharge between said pair of electrodes, an anode within said envelope spaced to one side of the discharge path between said pair of electrodes a distance less than half but more than a quarter of the distance between said pair of electrodes and having a support rod supported from the wall of said envelope, a shield surrounding said sup- 7;
port rod and provided with a foraminous port-ion over the anode, the distance between said foraminous portion and said anode being less than the mean free path of positive ions in the ionizable medium during operation of said electron discharge device.
4. An electron discharge device having an envelope containing a pair of electrodes and an ionizable medium for supporting a self-sustaining discharge between said pair of electrodes, an anode within said envelope spaced to one side of the discharge path between said pair of electrodes and having a support rod supported from the wall of said envelope, a shield surrounding said support rod and provided with a foraminous portion over the anode, a second shield between said sup port rod and said first shield and provided with a foraminous portion between the foraminous portion on said first shield and the surface of said anode.
HANS KLEMPERER.
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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2432608A (en) * 1941-03-28 1947-12-16 Ncr Co Multianode, gas-filled discharge device
US2612625A (en) * 1946-11-23 1952-09-30 Ericsson Telefon Ab L M Gaseous discharge tube
US2707771A (en) * 1946-07-05 1955-05-03 Sylvania Electric Prod Electron discharge device of the dynatron oscillator type
US2724786A (en) * 1952-01-26 1955-11-22 Electrons Inc Grid control gaseous discharge rectifier tube
USD521373S1 (en) * 2003-04-07 2006-05-23 Specialty Cereals Pty Limited Box

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2432608A (en) * 1941-03-28 1947-12-16 Ncr Co Multianode, gas-filled discharge device
US2707771A (en) * 1946-07-05 1955-05-03 Sylvania Electric Prod Electron discharge device of the dynatron oscillator type
US2612625A (en) * 1946-11-23 1952-09-30 Ericsson Telefon Ab L M Gaseous discharge tube
US2724786A (en) * 1952-01-26 1955-11-22 Electrons Inc Grid control gaseous discharge rectifier tube
USD521373S1 (en) * 2003-04-07 2006-05-23 Specialty Cereals Pty Limited Box

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