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US1799345A - Electron tube - Google Patents

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Publication number
US1799345A
US1799345A US723694A US72369424A US1799345A US 1799345 A US1799345 A US 1799345A US 723694 A US723694 A US 723694A US 72369424 A US72369424 A US 72369424A US 1799345 A US1799345 A US 1799345A
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United States
Prior art keywords
mercury
electron
electrode
electron emission
electron tube
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Expired - Lifetime
Application number
US723694A
Inventor
Wilford J Winninghoff
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
General Electric Vapor Lamp Co
Original Assignee
General Electric Vapor Lamp Co
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
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Publication date
Application filed by General Electric Vapor Lamp Co filed Critical General Electric Vapor Lamp Co
Priority to US723694A priority Critical patent/US1799345A/en
Application granted granted Critical
Publication of US1799345A publication Critical patent/US1799345A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J19/00Details of vacuum tubes of the types covered by group H01J21/00
    • H01J19/82Circuit arrangements not adapted to a particular application of the tube and not otherwise provided for

Definitions

  • My present invention relates to electron emission methods and devices such as are used for radio communication and for use in the arts generally and particularly to such a device in which electron emission is caused by condenser effect between parts of the device one of which is capable of giving off electrons when under an electrostatic strain.
  • Electron discharge by this method I find is achieved with minimum energy consumpt on and is adapted to close control and regulation of the quantity of electrons caused to flow.
  • thiselectronflow is achieved with less consumption of energy and greater adaptability of control than such a flow secured from a glowing filament which is heated by electric current flow because in the lat ter case the greater part of the energy consumed is used in the heating of the filament to incandescence and because close or flexible control of electron emissions is trammeled by the short range of filament temperatures between which maximum and minimum electron emission occurs.
  • An electron flow source of this kind is free from certain disadvantages of the Cooper Hewitt mercury arc rectifier such for example, as those attending critical vapor pressures, the heating of the mercury necessary for starting electron emission, and the comparatively great mass or inertia of the mercury molecule. These disadvantages are not metwith herebecause electron emission is produced in the device of my invention by electrostatic difierence of potential between the mercury and another electrode connected at a difference of potential in an electric circuit.
  • An object of my invention is therefore to provide an electron emission devlce suitable for the control and regulation of electrical and electro-magnetic circuits in' which elec- 1924. Serial No. 723,694.
  • Another object of my invention is to pro- Vide an electron emission device in which great flexibility of control of the quantity of elgptrons down to very small quantities is poss1 e.
  • Fig. 1 is an elevation view of an embodiment of my invention in the form of a three element electron tube suitable for use in radio communication, and
  • Fig. 2 is a diagram of a conventional radio receiving circuit of which the device of Fig. 1 is a part.
  • the sealed envelope 1 has sealed through the bottom of the chamber 2 formed at the bottom thereof the electrode 3 which terminates below the surface of the body of mercury 4 contained in said envelope.
  • the band 5 of conducting material is formed thereon a terminal 6.
  • the plate electrode 7 which is supported by the lead 8 sealed into the envelope through the reentrant tube 9 which extends downwardly from the top of said envelope.
  • Another lead 10 sealed through said reentrant tube 9 and extending parallel with said lead 8 and passing through an opening 11 in said plate 7 supports and-acts as a lead for the grid electrode 12 positioned between said plate 7 and the body of mercury 4 and parallel therewith.
  • the electrode 2 is connected to the negative terminal of a source of electric current 16 and the band 5 is connected through the terminal 6 to the positive terminal of said source. Connection is also made from said electrode 2 to the negative terminal of a second source of electric current 17 the other terminal (positive) of which is connected through telephone receivers 18, variometer 19 to said lead 8. Connection is made from lead 10 through the grid leak and condenser 20 and 21 in parallel through the secondary coil 22 to the said electrode 2.
  • pnmary 0011 23 cooperatmg wlth sald 0011 22 is connected to a suitable aerial 24 and to ground 25.
  • the variable condenser 26 connected across coil 22 serves for tuning the secondary circuit.
  • the electrostatic field produced between band 5 and mercury body 4 by the difference of potential therebetween in the circuit of direct current source 16 results in an electron emission from said body of mercury which completes the circuit between said body 4 and said plate electrode 7 whereby current flows through the telephones 18.
  • the electron stream also serves as a conductive path between grid electrode 12 and mercury 4 whereby any potential difference induced in secondary 22 will cause current to flow between said body 4 and said grid whereby the current flow in the telephone circuit is varied with the resulting signal reproduction in said telephones.
  • the temperature electron emission characteristic of the liquid cathode may be varied for difierent uses as by using mercury with sodium, copper, calcium, cadmium, bismuth, boron, thorium, thoria, or other metal or metalloid or oxides thereof.
  • solid sodium, potassium, or other metals or oxides thereof which are serviceable as electron emitters is used instead of the mercury electrode as described in the specification.
  • the method of energizing a sealed tube having electrodes mounted therein and an OK- terior terminal insulated from said internal electrodes which consists in applying potential difference to the internal electrodes of said device and continually applying electrostatic force to the exterior terminal to cause one of said interior electrodes to emit electrons to establish and maintain current fioW in the path between said internal electrodes and applying potential variations from another source of current to vary the current flow between the main electrodes.

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Description

April 7, 1931.
W. J. WINNI'NGHOFF ELECTRON TUBE Filed July 2, 1924 INVENTOR Patented Apr. 7, 1931 UNITED STATES PATENT OFFICE WILFORD J. WINNINGHOIEF, OF EAST ORANGE, NEW JERSEY, ASSIGNOR TO GENERAL ELECTRIC VAPOR LAMP COMPANY, OF HOBOKEN, NEW JERSEX', A CORPORATION OF NEW JERSEY ELECTRON TUBE Application filed July 2,
My present invention relates to electron emission methods and devices such as are used for radio communication and for use in the arts generally and particularly to such a device in which electron emission is caused by condenser effect between parts of the device one of which is capable of giving off electrons when under an electrostatic strain.
I have discovered that an effective electron fiow suitable for use in devices of the kind and nature of audion tubes and the like can be obtained by creating a potential difference between a pool of electrically conducting liquid and another conducting body pos tioned in close proximity thereto but electrically insulated therefrom as by a thin sheet of glass used for the separation thereof. Electron discharge by this method I find is achieved with minimum energy consumpt on and is adapted to close control and regulation of the quantity of electrons caused to flow. Andforexample,thiselectronflow is achieved with less consumption of energy and greater adaptability of control than such a flow secured from a glowing filament which is heated by electric current flow because in the lat ter case the greater part of the energy consumed is used in the heating of the filament to incandescence and because close or flexible control of electron emissions is trammeled by the short range of filament temperatures between which maximum and minimum electron emission occurs.
An electron flow source of this kind is free from certain disadvantages of the Cooper Hewitt mercury arc rectifier such for example, as those attending critical vapor pressures, the heating of the mercury necessary for starting electron emission, and the comparatively great mass or inertia of the mercury molecule. These disadvantages are not metwith herebecause electron emission is produced in the device of my invention by electrostatic difierence of potential between the mercury and another electrode connected at a difference of potential in an electric circuit.
An object of my invention is therefore to provide an electron emission devlce suitable for the control and regulation of electrical and electro-magnetic circuits in' which elec- 1924. Serial No. 723,694.
tron emission or flow is produced with a minimum of energy consumption.
Another object of my invention is to pro- Vide an electron emission device in which great flexibility of control of the quantity of elgptrons down to very small quantities is poss1 e.
Other objects of my invention will appear from the specification and from the drawings in which:
Fig. 1 is an elevation view of an embodiment of my invention in the form of a three element electron tube suitable for use in radio communication, and
Fig. 2 is a diagram of a conventional radio receiving circuit of which the device of Fig. 1 is a part.
In the drawings the sealed envelope 1 has sealed through the bottom of the chamber 2 formed at the bottom thereof the electrode 3 which terminates below the surface of the body of mercury 4 contained in said envelope. About said envelope in the vicinity of said mercury body is formed the band 5 of conducting material having formed thereon a terminal 6.
Within the envelope and substantially parallel to the surface of the body 4 is mounted the plate electrode 7 which is supported by the lead 8 sealed into the envelope through the reentrant tube 9 which extends downwardly from the top of said envelope. Another lead 10 sealed through said reentrant tube 9 and extending parallel with said lead 8 and passing through an opening 11 in said plate 7 supports and-acts as a lead for the grid electrode 12 positioned between said plate 7 and the body of mercury 4 and parallel therewith.
In Fig. 2 the electrode 2 is connected to the negative terminal of a source of electric current 16 and the band 5 is connected through the terminal 6 to the positive terminal of said source. Connection is also made from said electrode 2 to the negative terminal of a second source of electric current 17 the other terminal (positive) of which is connected through telephone receivers 18, variometer 19 to said lead 8. Connection is made from lead 10 through the grid leak and condenser 20 and 21 in parallel through the secondary coil 22 to the said electrode 2. The
pnmary 0011 23 cooperatmg wlth sald 0011 22 is connected to a suitable aerial 24 and to ground 25. The variable condenser 26 connected across coil 22 serves for tuning the secondary circuit.
In the operation of the device of my invention as appliedto the circuit shown in Fig. 2 the electrostatic field produced between band 5 and mercury body 4 by the difference of potential therebetween in the circuit of direct current source 16 results in an electron emission from said body of mercury which completes the circuit between said body 4 and said plate electrode 7 whereby current flows through the telephones 18. The electron stream also serves as a conductive path between grid electrode 12 and mercury 4 whereby any potential difference induced in secondary 22 will cause current to flow between said body 4 and said grid whereby the current flow in the telephone circuit is varied with the resulting signal reproduction in said telephones.
The temperature electron emission characteristic of the liquid cathode may be varied for difierent uses as by using mercury with sodium, copper, calcium, cadmium, bismuth, boron, thorium, thoria, or other metal or metalloid or oxides thereof. In some cases solid sodium, potassium, or other metals or oxides thereof which are serviceable as electron emitters is used instead of the mercury electrode as described in the specification.
I claim:
The method of energizing a sealed tube having electrodes mounted therein and an OK- terior terminal insulated from said internal electrodes which consists in applying potential difference to the internal electrodes of said device and continually applying electrostatic force to the exterior terminal to cause one of said interior electrodes to emit electrons to establish and maintain current fioW in the path between said internal electrodes and applying potential variations from another source of current to vary the current flow between the main electrodes.
Signed at Hoboken, in the county of Hudson and State of New Jersey, this first day of July, A. D. 1924.
IVILFORD J. VIN N IN GHOFF.
US723694A 1924-07-02 1924-07-02 Electron tube Expired - Lifetime US1799345A (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2478901A (en) * 1933-08-16 1949-08-16 Harold E Edgerton Electric system
US2532188A (en) * 1943-07-15 1950-11-28 Hartford Nat Bank & Trust Co Ion discharge tube for high voltages

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2478901A (en) * 1933-08-16 1949-08-16 Harold E Edgerton Electric system
US2532188A (en) * 1943-07-15 1950-11-28 Hartford Nat Bank & Trust Co Ion discharge tube for high voltages

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