US2117246A - Electron discharge device - Google Patents

Electron discharge device Download PDF

Info

Publication number
US2117246A
US2117246A US589939A US58993932A US2117246A US 2117246 A US2117246 A US 2117246A US 589939 A US589939 A US 589939A US 58993932 A US58993932 A US 58993932A US 2117246 A US2117246 A US 2117246A
Authority
US
United States
Prior art keywords
grid
positive
volts
negative
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
Application number
US589939A
Inventor
Hakon H Haglund
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.)
Western Union Telegraph Co
Original Assignee
Western Union Telegraph 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.)
Filing date
Publication date
Application filed by Western Union Telegraph Co filed Critical Western Union Telegraph Co
Priority to US589939A priority Critical patent/US2117246A/en
Application granted granted Critical
Publication of US2117246A publication Critical patent/US2117246A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J17/00Gas-filled discharge tubes with solid cathode
    • H01J17/50Thermionic-cathode tubes
    • H01J17/52Thermionic-cathode tubes with one cathode and one anode
    • H01J17/54Thermionic-cathode tubes with one cathode and one anode having one or more control electrodes
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J17/00Gas-filled discharge tubes with solid cathode
    • H01J17/02Details
    • H01J17/04Electrodes; Screens

Definitions

  • This invention relates to the construction ⁇ and operation of electron discharge devices and particularly to devices which are suitable foruse as relays which may be started instantly by the r, application of a predetermined positive voltage to the grid and may be stopped suddenly the instant a certain critical negative potential is applied to the grid.
  • Thermionic devices which have the characteristic of starting into operation when a certain positive potential is applied to the grid and continuing to operate thereafter unaffected by the grid potential have now become well known and are in commercial use.
  • the object of my l5 present invention is to provide a thermionic current controlling device in which the plate current may not only be started instantly with substantially the maximum value and will continue to flow unalected by fluctuations in the positive potential applied to the grid but which may be stopped suddenly by the application of a ⁇ critical negative potential to the grid.
  • a thermionic tube having these characteristics isapplicable to conditions which cannot be fulfilled byprior devices.
  • FIG. 1 is a diagram of a circuit arrangement in which my device may be utilized to advantage.
  • the device shown in Fig. 1 comprises an envelope l consisting' of glass, quartz 'or the like,
  • the grid is constructed oi ilnewire mesh and forms a closed cage completely enveloping the cathode lilament 2, so
  • the current continues toY flow in the plate circuit unaffected by fluctuation ⁇ in positive grid potential.
  • the grid is made neg- 20 ative by a certain critical value, positive ions collect and form a sheath of positive ions about the grid wires. This sheath acts like a layer of insulation. At the critical negative potential this sheath is made sufficiently thick to overlap between the small apertures of the grid and effectively block the ionic path through the grid. Since the cathode is completely enclosed or enveloped by the grid structure, the arc is stopped or extinguished and cle-ionization takes place. 39
  • the value of the critical negative voltage will depend, of course, upon the size of the apertures between the grid mesh wires.
  • the coarser the mesh the higher will be the critical negative voltage required.
  • the thickness of the sheath 3,-" of positive ions is a function of the negative grid voltage and also of the positive ion current. Hence a higher critical negative voltage will be required for a larger plate circuit current.
  • the thermionic tube or device of my invention may therefore be characterized as a gaseous controlled rectifier wherein the grid so completely encloses or envelopes either the cathode or the anode and is composed of a wire mesh of such dimensions that an arc can be startedby applying positive potential to the grid and can likewise be extinguished by applying a 'critical negative potential thereto.
  • I have indicated at B, the output of an amplier or magnifier of a telegraph receiving or repeating apparatus connected by conductor 'l with the continuous ring of a rotary repeater RR of the usual well-known construction.
  • the segments a, b1, c, etc. are connected alternately to the grids of two thermionic tubes T1, T2 of the construction described in which the cathodes are completely enclosed or enveloped by the fine mesh grids.
  • the cathodes are connected in parallel to the other conductor 8 of the amplifier output through a conductor 9 and resistance R1.
  • the plates or anodes of the tubes are connected respectively through the actuating coils of the sending-on relays SR1 and SR2, through ythe conductor HJ and battery BA to the amplier output conductor 8.
  • the relay armatures t1 and t2 are normally biased to their left hand or negative polarity contacts by the biasing coils bc.
  • the received signaling impulses have a maximum of ten volts positive and a minimum of ten volts negative and that the amplier output is normally biased to five volts positive so that there will be an available positive voltage of fifteen volts and an available minimum voltage of ten volts at the terminals of the arnpliiler. Also assume that there is a voltage drop of five volts across the resistance R1 when current flows through one tube and a drop of ten volts when current iiows through both tubes. y
  • the illustration of the transmitted signal with square topped waves is of course, not attained in actual practice.
  • the diagram of received signals shows that there is a lag between the transmission and the reception and also that the dots or impulses of unit length are too weak to be recorded.
  • the diagram of repeated signals indicates that the regenerated signals repeated into the outgoing line or cable include the missing dot impulses and constitute a faithful reproduction of the original transmitted signals.
  • the repeated signal impulse transmitted to the outgoing line changes from maximum positive to minimum negative, as indicated by the diagram.
  • the received signal is at a minimum l volts negative which is reduced by the volts positive bias to 5 volts negative at the terminals of the amplifier. Since the tube T2 is still operating, there is a drop of 5 volts across the resistance R1 giving a resultant of volts negative to be applied to the grid of tube T2. This stops tube T2 and causes the tongue t2 of sending-on relay SR2 to move over to its left hand contact under the control of its biasing coil. Accordingly as the sending-on brush B2 engages segment d the negative impulse being transmitted to line is continued from tongue t2.
  • the amplier output has dropped to its no signal value, due to the fact that a series of single impulses are coming in and the attenuation of the cable is assumed to be so great that these signals are almost completely lost in transmission.
  • the voltage at the amplifier output is 5 volts positive due to the positive bias. Since neither tube is operating, there is no drop at the resistance R1 and hence the 5 volts positive is applied to the grid of tube T1 which starts it into operation, thereby energizing the relay SR1 and moving its tongue t1 over to its right hand contact.
  • the sending-on brush B2 engages the contact e', the repeated signal impulse shifts from negative to positive as indicated.
  • a thermionic device comprising an electronemitting cathode, an anode, a grid element and an enclosing envelope, a gaseous medium within said envelope, said grid element consisting of a ne mesh wire structure completely enclosing said cathode, the apertures of said grid element having an area of such size that they are completely closed to the passage of electrons by a sheath of positive ions upon the application of a critical negative voltage to the grid element.
  • An electronic control switch comprising a receptacle having an ionizable medium therein, a solid electron emitting cathode and an anode element disposed in said receptacle and a .control grid completely enclosing said cathode, comprising in its entirety a metallic member provided with uniformly distributed small perforations of uniform size.
  • An electron dischargedevice comprising a 5 receptacle having an ionizable medium therein,

Landscapes

  • Particle Accelerators (AREA)

Description

May 10, 1938. H. H. HAGLUND ELECTRON DISCHARGE DEVICE RNNNQ A|IT WENN .W ,I M
NNN
Filed Jan. 30, 1932 jjfagiund Elmo/ww Patented May 10, 1938 UNITED STATE-s PATENT F-FCE ELECTRON DISCHARGEv DEVICE Application January 30, 1932, Serial No. 589,939
5 Claims.
This invention relates to the construction `and operation of electron discharge devices and particularly to devices which are suitable foruse as relays which may be started instantly by the r, application of a predetermined positive voltage to the grid and may be stopped suddenly the instant a certain critical negative potential is applied to the grid.
Thermionic devices which have the characteristic of starting into operation when a certain positive potential is applied to the grid and continuing to operate thereafter unaffected by the grid potential have now become well known and are in commercial use. The object of my l5 present invention is to provide a thermionic current controlling device in which the plate current may not only be started instantly with substantially the maximum value and will continue to flow unalected by fluctuations in the positive potential applied to the grid but which may be stopped suddenly by the application of a `critical negative potential to the grid. A thermionic tube having these characteristics isapplicable to conditions which cannot be fulfilled byprior devices.
The novel features which I believe to `be characteristic of my invention are set forth with particularity in the appended claims. The-invention itself, however, both as to its construction and mode of operation will best be understood by reference to the following description taken in connection with the accompanying drawing `in which Figure 1 is a longitudinal sectional view of a device embodying my invention;
- and Figure 2 is a diagram of a circuit arrangement in which my device may be utilized to advantage.
The device shown in Fig. 1 comprises an envelope l consisting' of glass, quartz 'or the like,
4.0 and containing a rare inert gas, a body of easily vaporizable monatomic metal 4, 'suchwas mercury or a mixture of them. The grid?, is constructed oi ilnewire mesh and forms a closed cage completely enveloping the cathode lilament 2, so
4:5 that no electrons can pass from the cathode `to the anode plate 3 without passing through the grid. It is in this feature' that myinvention is distinguished from prior devices. in corta-n prior thermionic devices in `which the grid `50 completely surrounds the cathode, as for instance in the thyratron type, after starting, the plate current attains its maximum value instantly and the grid has no further control, either to modulate, limit or extinguish it. The a device of my present invention operates in the apertures in the grid to the anode.
(Cl. Z50-27.5)
same manner in regard to the instantaneous starting and continuous maximum flow in the plate circuit irrespective of fluctuations in grid potential so long as it remains positive, but itl diiers from the thyratron in that the plate cure5 rent may also be stopped instantly by applying a critical value of negative potential to the grid. Herein lies the fundamental difference between the thyratron type and my present device. 11') The operation of my thermionic device having a grid-enclosed cathode is probably as follows: When the grid is made positive, there'is a flow of electrons from the cathode through the small These elecd'5 trons collide with the atoms of the gas, causing ionization and thereby starting the arc. As previously stated, the current continues toY flow in the plate circuit unaffected by fluctuation `in positive grid potential. If the grid is made neg- 20 ative by a certain critical value, positive ions collect and form a sheath of positive ions about the grid wires. This sheath acts like a layer of insulation. At the critical negative potential this sheath is made sufficiently thick to overlap between the small apertures of the grid and effectively block the ionic path through the grid. Since the cathode is completely enclosed or enveloped by the grid structure, the arc is stopped or extinguished and cle-ionization takes place. 39 The value of the critical negative voltage will depend, of course, upon the size of the apertures between the grid mesh wires. The coarser the mesh, the higher will be the critical negative voltage required. The thickness of the sheath 3,-", of positive ions is a function of the negative grid voltage and also of the positive ion current. Hence a higher critical negative voltage will be required for a larger plate circuit current. :in
The thermionic tube or device of my invention may therefore be characterized as a gaseous controlled rectifier wherein the grid so completely encloses or envelopes either the cathode or the anode and is composed of a wire mesh of such dimensions that an arc can be startedby applying positive potential to the grid and can likewise be extinguished by applying a 'critical negative potential thereto.
I have illustrated in Fig. 2, an example of a circuit arrangement particularly adapted for use with the thermionic tube of the present invention, this arrangement being claimed in my copending application, Serial No. 509,798, now Patent No. 1,944,888, Jan. 30, 1934. '55
I have indicated at B, the output of an amplier or magnifier of a telegraph receiving or repeating apparatus connected by conductor 'l with the continuous ring of a rotary repeater RR of the usual well-known construction. The segments a, b1, c, etc. are connected alternately to the grids of two thermionic tubes T1, T2 of the construction described in which the cathodes are completely enclosed or enveloped by the fine mesh grids. The cathodes are connected in parallel to the other conductor 8 of the amplifier output through a conductor 9 and resistance R1. The plates or anodes of the tubes are connected respectively through the actuating coils of the sending-on relays SR1 and SR2, through ythe conductor HJ and battery BA to the amplier output conductor 8. The relay armatures t1 and t2 are normally biased to their left hand or negative polarity contacts by the biasing coils bc.
Let us assume that the received signaling impulses have a maximum of ten volts positive and a minimum of ten volts negative and that the amplier output is normally biased to five volts positive so that there will be an available positive voltage of fifteen volts and an available minimum voltage of ten volts at the terminals of the arnpliiler. Also assume that there is a voltage drop of five volts across the resistance R1 when current flows through one tube and a drop of ten volts when current iiows through both tubes. y The illustration of the transmitted signal with square topped waves is of course, not attained in actual practice. The diagram of received signals shows that there is a lag between the transmission and the reception and also that the dots or impulses of unit length are too weak to be recorded. The diagram of repeated signals indicates that the regenerated signals repeated into the outgoing line or cable include the missing dot impulses and constitute a faithful reproduction of the original transmitted signals.
Let us examine the operation more in detail. When the brush B1 is on the segment b, the received signal is at a maximum and hence there is a voltage of 15 positive at the terminals of the amplifier. At this instant current has been flowing through both tubes thereby causing a drop of 10 volts across resistance R, thus leaving 5 volts positive to be applied to the grid oi tube T2. This tube, therefore, continues to operate and holds its tongue or armature t2 against its right hand contact. Consequently the tube T2 will continue to operate and as the sending brush B2 engages the segment b', the repeated signal will continue as a maximum positive impulse from the tongue t2.
When the brush B'1 engages the segment c, the received signal is at zero and the voltage at the amplifier output is 5 volts positive bias. Both tubes are still in operation and hence there is a drop of 10 volts across resistance R1 to be subtracted, leaving a resultant of 5 volts negative which is applied to the grid of tube T1. This stops the tube and the tongue t1 of relay SR1 is moved by its biasing coil to the left hand contact.
As the sending brush now engages the segment c', the repeated signal impulse transmitted to the outgoing line changes from maximum positive to minimum negative, as indicated by the diagram.
When the brush B1 moves onto the segment d, the received signal is at a minimum l volts negative which is reduced by the volts positive bias to 5 volts negative at the terminals of the amplifier. Since the tube T2 is still operating, there is a drop of 5 volts across the resistance R1 giving a resultant of volts negative to be applied to the grid of tube T2. This stops tube T2 and causes the tongue t2 of sending-on relay SR2 to move over to its left hand contact under the control of its biasing coil. Accordingly as the sending-on brush B2 engages segment d the negative impulse being transmitted to line is continued from tongue t2.
When the brush B1 has reached the pick-up segment e, the amplier output has dropped to its no signal value, due to the fact that a series of single impulses are coming in and the attenuation of the cable is assumed to be so great that these signals are almost completely lost in transmission. The voltage at the amplifier output is 5 volts positive due to the positive bias. Since neither tube is operating, there is no drop at the resistance R1 and hence the 5 volts positive is applied to the grid of tube T1 which starts it into operation, thereby energizing the relay SR1 and moving its tongue t1 over to its right hand contact. As the sending-on brush B2 engages the contact e', the repeated signal impulse shifts from negative to positive as indicated.
'Ihis will suice to explain the operation. It will be observed that the tubes are started and are also stopped by the received signal impulses, whereas when the thyratron tubes are employed, as in my prior applications, Ser. Nos. 335,963 and 343,109, now Patent No. 1,901,296, March 14, 1933, it is necessary to provide a special rotary distributor to stop the operation of the tubes. My present invention, therefore, greatly simplies the apparatus required and consequently enhances the elicency and permits of greater speed.
It will be obvious to engineers that my invention is applicable to the control of various arrangements of circuits and apparatus and that the application above described is merely illus-' trative for the purpose of making a. clear and complete disclosure of the invention.
I claim:
1. The method of controlling the duration of an arc discharge in a gas which consists in rendering conductive the arc path between two electrodes, establishing in the arc path a negative electric field which completely envelopes one electrode and having a potential high enough to form a closed sheath. of positive ions to thereby extinguish the arc.
2. The method of controlling the duration of an arc discharge in a gas which consists in rendering conductive the arc path between two electrodes, setting up in the arc path a negative electrostatic eld which completely envelopes one electrode and is so disposed that at a critical value the resulting sheath of positive ions extinguishes the arc.
3. A thermionic device comprising an electronemitting cathode, an anode, a grid element and an enclosing envelope, a gaseous medium within said envelope, said grid element consisting of a ne mesh wire structure completely enclosing said cathode, the apertures of said grid element having an area of such size that they are completely closed to the passage of electrons by a sheath of positive ions upon the application of a critical negative voltage to the grid element.
4. An electronic control switch comprising a receptacle having an ionizable medium therein, a solid electron emitting cathode and an anode element disposed in said receptacle and a .control grid completely enclosing said cathode, comprising in its entirety a metallic member provided with uniformly distributed small perforations of uniform size.
5. An electron dischargedevice, comprising a 5 receptacle having an ionizable medium therein,
a solid electron emitting cathode and an anode element disposed in said receptacle and a control grid completely enclosing said cathode, said grid being metallic throughout and having a plurality of small openings of uniform size.
HAKON H. HAGLUND.
US589939A 1932-01-30 1932-01-30 Electron discharge device Expired - Lifetime US2117246A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US589939A US2117246A (en) 1932-01-30 1932-01-30 Electron discharge device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US589939A US2117246A (en) 1932-01-30 1932-01-30 Electron discharge device

Publications (1)

Publication Number Publication Date
US2117246A true US2117246A (en) 1938-05-10

Family

ID=24360198

Family Applications (1)

Application Number Title Priority Date Filing Date
US589939A Expired - Lifetime US2117246A (en) 1932-01-30 1932-01-30 Electron discharge device

Country Status (1)

Country Link
US (1) US2117246A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2457948A (en) * 1945-02-16 1949-01-04 Albert G Thomas Electron discharge device
US2795726A (en) * 1950-01-16 1957-06-11 Siemens Ag Screen-mesh electrode for electrical discharge tubes
US5150018A (en) * 1991-08-12 1992-09-22 North American Philips Corporation Gas discharge lamp with grid and control circuits therefor
US5274299A (en) * 1990-12-27 1993-12-28 North American Philips Corporation Grid controlled gas discharge lamp

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2457948A (en) * 1945-02-16 1949-01-04 Albert G Thomas Electron discharge device
US2795726A (en) * 1950-01-16 1957-06-11 Siemens Ag Screen-mesh electrode for electrical discharge tubes
US5274299A (en) * 1990-12-27 1993-12-28 North American Philips Corporation Grid controlled gas discharge lamp
US5150018A (en) * 1991-08-12 1992-09-22 North American Philips Corporation Gas discharge lamp with grid and control circuits therefor

Similar Documents

Publication Publication Date Title
GB694034A (en) Electrical devices utilizing semiconductor materials for the translation of electriccurrents
US2293177A (en) Electron discharge device circuits
US2117246A (en) Electron discharge device
Townsend et al. Cold cathode tubes for transmission of audio frequency signals
US2092861A (en) Oscillation generating circuits including gas-filled tube
US2100195A (en) Electric discharge apparatus
US2416355A (en) Impulse generator circuits
US2479846A (en) Gas-filled electric discharge device
US1334150A (en) Electrical discharge-tube
GB370967A (en) Improvements in and relating to electric discharge devices for the control of energyin electrical circuits
US2813992A (en) Gas discharge device utilizing controlled electron trapping
US1965589A (en) Gaseous electric discharge device and method of making the same
US2459199A (en) Arc discharge device
US1190412A (en) Electrode for devices for varying electrical resistance.
US2474224A (en) Electronic switch
US2657309A (en) Storage device utilizing semiconductor
US2025912A (en) Signaling system employing glow discharges
US2068040A (en) Thermionic discharge relay system
US2607021A (en) Gas filled discharge device
US1464104A (en) Selective apparatus for signaling circuits
US1387984A (en) Negative resistance
US1426801A (en) Repeater for ttndtjlatory currents
US2402188A (en) Electronic device and circuits
US1871537A (en) Electron discharge device
US1038910A (en) Relay for undulatory currents.