US1799345A - Electron tube - Google Patents
Electron tube Download PDFInfo
- 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
- Authority
- US
- United States
- Prior art keywords
- mercury
- electron
- electrode
- electron emission
- electron tube
- Prior art date
- Legal status (The legal status 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 status listed.)
- Expired - Lifetime
Links
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 12
- 229910052753 mercury Inorganic materials 0.000 description 12
- 238000000034 method Methods 0.000 description 3
- DGAQECJNVWCQMB-PUAWFVPOSA-M Ilexoside XXIX Chemical compound C[C@@H]1CC[C@@]2(CC[C@@]3(C(=CC[C@H]4[C@]3(CC[C@@H]5[C@@]4(CC[C@@H](C5(C)C)OS(=O)(=O)[O-])C)C)[C@@H]2[C@]1(C)O)C)C(=O)O[C@H]6[C@@H]([C@H]([C@@H]([C@H](O6)CO)O)O)O.[Na+] DGAQECJNVWCQMB-PUAWFVPOSA-M 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 229910052708 sodium Inorganic materials 0.000 description 2
- 239000011734 sodium Substances 0.000 description 2
- ZSLUVFAKFWKJRC-IGMARMGPSA-N 232Th Chemical compound [232Th] ZSLUVFAKFWKJRC-IGMARMGPSA-N 0.000 description 1
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- OYPRJOBELJOOCE-UHFFFAOYSA-N Calcium Chemical compound [Ca] OYPRJOBELJOOCE-UHFFFAOYSA-N 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- ZLMJMSJWJFRBEC-UHFFFAOYSA-N Potassium Chemical compound [K] ZLMJMSJWJFRBEC-UHFFFAOYSA-N 0.000 description 1
- 229910052776 Thorium Inorganic materials 0.000 description 1
- 229910052797 bismuth Inorganic materials 0.000 description 1
- JCXGWMGPZLAOME-UHFFFAOYSA-N bismuth atom Chemical compound [Bi] JCXGWMGPZLAOME-UHFFFAOYSA-N 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 229910052793 cadmium Inorganic materials 0.000 description 1
- BDOSMKKIYDKNTQ-UHFFFAOYSA-N cadmium atom Chemical compound [Cd] BDOSMKKIYDKNTQ-UHFFFAOYSA-N 0.000 description 1
- 229910052791 calcium Inorganic materials 0.000 description 1
- 239000011575 calcium Substances 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000005686 electrostatic field Effects 0.000 description 1
- 238000005265 energy consumption Methods 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229910052752 metalloid Inorganic materials 0.000 description 1
- 150000002738 metalloids Chemical class 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 229910052700 potassium Inorganic materials 0.000 description 1
- 239000011591 potassium Substances 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- ZCUFMDLYAMJYST-UHFFFAOYSA-N thorium dioxide Chemical compound O=[Th]=O ZCUFMDLYAMJYST-UHFFFAOYSA-N 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J19/00—Details of vacuum tubes of the types covered by group H01J21/00
- H01J19/82—Circuit 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.
Landscapes
- Cold Cathode And The Manufacture (AREA)
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.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US723694A US1799345A (en) | 1924-07-02 | 1924-07-02 | Electron tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US723694A US1799345A (en) | 1924-07-02 | 1924-07-02 | Electron tube |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US1799345A true US1799345A (en) | 1931-04-07 |
Family
ID=24907294
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US723694A Expired - Lifetime US1799345A (en) | 1924-07-02 | 1924-07-02 | Electron tube |
Country Status (1)
| Country | Link |
|---|---|
| US (1) | US1799345A (en) |
Cited By (2)
| 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 |
-
1924
- 1924-07-02 US US723694A patent/US1799345A/en not_active Expired - Lifetime
Cited By (2)
| 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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