US3405300A - Gas filled coaxial type electric switch with magnetic field cut-off - Google Patents
Gas filled coaxial type electric switch with magnetic field cut-off Download PDFInfo
- Publication number
- US3405300A US3405300A US517345A US51734565A US3405300A US 3405300 A US3405300 A US 3405300A US 517345 A US517345 A US 517345A US 51734565 A US51734565 A US 51734565A US 3405300 A US3405300 A US 3405300A
- Authority
- US
- United States
- Prior art keywords
- magnetic field
- electrodes
- electric switch
- circuit
- current
- 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
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J17/00—Gas-filled discharge tubes with solid cathode
- H01J17/02—Details
- H01J17/14—Magnetic means for controlling the discharge
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01T—SPARK GAPS; OVERVOLTAGE ARRESTERS USING SPARK GAPS; SPARKING PLUGS; CORONA DEVICES; GENERATING IONS TO BE INTRODUCED INTO NON-ENCLOSED GASES
- H01T2/00—Spark gaps comprising auxiliary triggering means
- H01T2/02—Spark gaps comprising auxiliary triggering means comprising a trigger electrode or an auxiliary spark gap
Definitions
- FIG. 1a A first figure.
- ABSTRACT OF THE DISCLOSURE An electric switch of the coaxial cylinder type. It has a pair of cylindrical electrodes which are enclosed in a gas tight envelop, there being an outer cylindrical electrode and an inner cylindrical electrode surrounded at least partially by said outer cylindrical electrode. One of said pair of cylindrical electrodes is a cold cathode and the other of said pair of cylindrical electrodes is an anode.
- the envelope is filled with an ionizable medium at a pressure which is less than k /r r torr, where A is the mean free path of an electron at 1 torr and r and r are the radius of said inner and outer electrode, respectively.
- a magnet means is provided adjacent the outside of said envelope and consists of a permanent magnet and a coil superposing a magnetic field between said electrodes in a direction transverse to the spacing of said electrodes.
- This invention relates to a device for an electric switch which can operate at a high speed, and more particularly to a switch which can be used in a high voltage circuit. Furthermore it relates to such a device which acts as an over-current switch having means controlling the following current therein.
- Ignitrons or thyratrons are representative tubes of the kind now in use as high speed switches in electric circuits.
- the former are essentially diode discharge tubes with control-electrodes and an igniter sealed therein.
- the latter are essentially triode discharge tubes containing a control grid.
- An object of this invention is to eliminate these drawbacks and to provide a novel high speed switch with long life for use in a high voltage circuit.
- Another object of the invention is to provide a high voltage pulse generator with a simple circuit.
- a further object of the invention is to provide an overcurrent circuit breaker which operates at high speed.
- FIGS. 1a and lb are an axial section and transverse section, respectively, of the device of the present invention.
- FIG. 2 is a perspective view of an embodiment of the device of FIGS. la and 1b;
- FIGS. 3 and 4 are graphs illustrating th static characteristics thereof
- FIGS. 5 and 6 are circuit diagrams of modifications of the circuit of the device shown in FIG. 2.
- the device comprises a cylindrical enclosure 2 having sealed into the interior thereof concentric electrodes 3 and 4, a small permanent magnet 5 between the poles of which is positioned the envelope 2, and a coil 6 wrapped around th enclosure 2 concentrically with the electrodes.
- Said electrodes can be of any non-magnetic and conducting material such as copper, aluminum, or carbon. However, it is preferable that they be of a refractory metal such as molybdenum or titanium, or their alloys.
- the enclosure 2 contains an ionizable medium such as hydrogen, neon, nitrogen, argon, miX- ture thereof, or an inert compound gas such as freon gas, etc., at a pressure ranging from l0 to 1 torr.
- the magnet 5 supplies an axial magnetic field.
- a power supply 7 is connected across the electrodes 3 and 4.
- the coil 6 is connected to said power supply 7 or to another supply.
- the current 8 flowing through the coil 6 acts as a driving current and controls the main current flow between electrodes 3 and 4 so that it either flows or does not flow in accordance with a novel means of the present invention.
- This device is essentially a crossed field discharge tube. A perspective sketch of the device is shown in FIG. 2, wherein the reference characters correspond to those in FIG. 1 and the various parts are designated by the same numbers.
- FIG. 3 shows variations in sparking voltage and current relative to the axial magnetic field strength.
- full line and dotted line 112 indicate the sparking voltage and a current characteristics respectively of coaxial electrode tubes in an axial magnetic field.
- Be designates the critical magnetic field strength
- V0 sparking voltages corresponding to magnetic field strengths lower than Be
- V0 sparking voltages corresponding to magnetic field strengths greater than Be.
- the actual magnetic field strength is a combination of the static magnetic field strength Bs of permanent magnet 5 and the magnetic field strength Bx of coil 6.
- the magnetic field strength Bs is selected so that its value is lower than the critical magnetic field strength Be as shown in FIG. 3, while the voltage Va applied across electrodes 3 and 4 is adjusted to have a value between V0 and V0.
- the DC driving current 8 shown in FIG. 2 is not supplied to said coil 6, i.e. Bx is zero, the device will be in open circuit condition. If a driving current 8 is supplied to said coil 6, Bx appears and the field strength increases. When it becomes higher than Be, the device will be in the closed circuit condition and a current, Ic in FIG. 3, flows. Therefore the device can be used as a switch by controlling said driving current 8 in said coil 6.
- the device acts as a switch even when the applied voltage is as high as said voltage V0, i.e. maximum operating voltage is V0.
- FIG. 4 shows typical variations in said V0 in relation to the gas pressure of the ionizable medium.
- the gas pressure P in said enclosure must be lower than M/ (r r where n is a mean free path of an electron at 1 torr and r and r are the radius of the inner and outer electrodes, respectively. He can be expressed as follows:
- inner electrode as the cathode
- inner electrode inner electrode as the anode
- e and m are the charge and the mass of an electron respectively
- Va is the applied voltage.
- the field strength of the magnet should be slightly lower than Bc.
- the inner electrode be used as the anode.
- the electrode materials be refractory metal such as tantalum or molybdenum. When designing the device, the following factors should also be considered. It is necessary to select a suitable material for the aforesaid ionizable medium.
- a light gas such as hydrogen is suitable if a short ignition time is desired, and for a short quenching time a polyatomic gas such as gaseous ethylalcohol is suitable.
- the operable life of the device can be prolonged by employing an outer cylinder which is 20% shorter than the inner cylinder. A longer outer cylinder frequently causes damage of the envelope at its corner.
- the gas pressure and the type of gas therein should be properly selected, various different gases and gas pressures producing various operating voltages.
- a mixture of various kinds of gases requires special attention to the Penning effect which tends to lower the operating voltage, as disclosed in Electrical Breakdown of Gases, Oxford Press 1953, edited by J. M. Meek et al.
- a chemical compound gas such as freon gas is suited for high voltage operation.
- the device isTessentially a cold-cathode discharge tube. Therefore, the constitution thereof is essentially simpler than a hot-cathode tube such as a thyratron. Since the device has no electric contacts therein, no contact failures need be expected during operating periods. This results in an increase in the operable life. Furthermore, since the device operates in a magnetic field, the deionization time is remarkably shorted. Therefore, the quenching time of the ionized medium in the novel device can be shorter than that of a tube such as a thyratron wherein a magnetic field is not used.
- T-ypical specifications for the device are as follows:
- the radii of the inner electrode and outer electrode are 5 mm. and mm., respectively.
- the inner electrode is connected on an anode.
- the ionizable medium is nitrogen at a pressure of 2X10 torr.
- the magnetic field strength of the permanent magnet is 35 gauss.
- the radius of the coil is mm.
- the number of turns is 1000 and the driving current ranges from 20 to ma.
- the maximum controlled current is 50 A.
- the operating voltage ranges from 500 v. to 10 kilovolts and the time response is 10- seconds.
- the operating characteristics of the device can be chosen within the following range: maximum operating voltage is 10 kilovolts or more; the voltage drop between cylindrical electrodes is several hundred volts or less; maximum controlled current is 10 ka.; and the time response is lO 10- seconds.
- the device according to the invention can easily be designed to act as a high speed circuit-breaker.
- the cylindrical electrodes 3 and 4 are connected to a load circuit.
- the device closes any circuit in which it is connected.
- a load current from such a circuit is supplied as a driving current to the coil 6 in a direction to reduce the static magnetic field of the permanent magnet and B is reduced to a value less than Bc, the device opens the circuit.
- the load current supplied as a driving current operates said device to the on or off condition.
- reference character 11 designates a high voltage DC power supply the output voltage of which determines the peak value of a pulse voltage.
- a stabilizing resistor 12 is connected between one side of supply 11 and the device 13 of the present invention, which in turn is driven by an AC current supply 14.
- a small DC voltage supply 15 is connected between device 13 and out-put terminals 16 and controls the level of an out-put pulse.
- the high voltage pulse is generated by following procedure; high voltage Va(Va V0) is applied across the cylindrical electrodes of the device 13 and an AC current is supplied to the coil. During the period of half a cycle of the AC current, the value Bs increases to a value higher than an the value Bo, and accordingly, the device closes the circuit which causes the generation of a high voltage pulse across the out-put terminals -16.
- a DC current controlled device can easily be made.
- a DC power supply 21, load 22, and electrodes 23 and coil 24 of the device 27 according to the present invention are connected in series.
- the DC load current 25 is supplied to the coil 24 in a direction which is the reverse of that of FIG. 2. Therefore, the actual magnetic field strength B decreases with increasing load current.
- the magnetic field strength B is selected so as to have a value slightly larger than Bc, and as a result the device 27 closes the circuit.
- the load current exceeds a predetermined value B is reduced to a value less than Ba, and the device 27 opens the circuit.
- An auxiliary circuit 26 is useful for initiating the discharge between electrodes 23.
- An electric switch of the coaxial cylinder type comprising a gas tight envelope, a pair of cylindrical electrodes enclosed in said gas tight envelope and consisting of an outer cylindrical electrode and an inner cylindrical electrode surrounded at least partially by said outer cylindrical electrode, one of said pair of cylindrical electrodes being a cold cathode and another of said pair of cylindrical electrodes being an anode, an ionizable medium filling said envelope and being at a low pressure less than MH -r torr, where A is the mean free path of an electron at 1 torr and 1' and r are the radius of said inner and outer electrode, respectively, magnet means adjacent the outside of said envelope and consisting of a permanent magnet and a coil superposing a magnetic field between said electrodes in a direction transverse to the direction in which said electrodes are spaced, whereby said electric switch closes an electrical circuit across the space between said electrodes when said superposed magnetic field is more than the electron cut-off field Ba and opens said electrical circuit across the space between said electrodes when said superposed magnetic field is less than said electron cut
Description
GAS FILLED COAXIAL TYPE ELECTRIC SWITCH WITH MAGNETIC FIELD CUT-OFF Filed Dec. 29, 1965 2 Sheets-Sheet ,1
FIG. 1a
INVENTORS KIYOTAKA WASA SHIGERU HAYAKAWA B WVM ATTORNEYS 1968 'KIY(DTAKA WASA ET AL 3,405,300
GAS FILLED COAXIAL.TYPE ELECTRIC SWITCH WITH MAGNETIC FIELD CUT-OFF Filed Dec. 29, 1965 2 Sheets-Sheet 2 H633 F/6Z4 no i V0 2 m o r 35mm Z E10 r? 5mm 0 8 NITROGEN GAS (9 z E a: UJ I Vc 2- o-+--- 8s 80 (Es-+8!) i o 1 l MAGNETIC FIELD 2 I62 lo" I GAS PRESSURE (TORR) |3-- L n E [6 "g LEEBJ INVENTORS K IYOTAKA WASA SHIG ERU HAYAKAWA BYd/M 12 1 M ATTORNEYS United States Patent GAS FILLED COAXIAL TYPE ELECTRIC SWITCH WITH MAGNETIC FIELD CUT-(DEF Kiyotaka Wasa, Osaka-shi, Osaka-fu, and Shigeru Hayakawa, Hirakata-shi, Osaka-fir, Japan, assignors to Matsushita Electric Industrial Co., Ltd., Osaka, Japan Filed Dec. 29, 1965, Ser. No. 517,345 Claims priority, application Japan, July 7, 1965, 40/ 40,663 3 Claims. (Cl. 313-161) ABSTRACT OF THE DISCLOSURE An electric switch of the coaxial cylinder type. It has a pair of cylindrical electrodes which are enclosed in a gas tight envelop, there being an outer cylindrical electrode and an inner cylindrical electrode surrounded at least partially by said outer cylindrical electrode. One of said pair of cylindrical electrodes is a cold cathode and the other of said pair of cylindrical electrodes is an anode. The envelope is filled with an ionizable medium at a pressure which is less than k /r r torr, where A is the mean free path of an electron at 1 torr and r and r are the radius of said inner and outer electrode, respectively. A magnet means is provided adjacent the outside of said envelope and consists of a permanent magnet and a coil superposing a magnetic field between said electrodes in a direction transverse to the spacing of said electrodes. As a result, the electric switch closes an electrical circuit across the space between said electrodes when there is superposed thereon a magnetic field more than an electron cut-olf field Be, and opens said electrical circuit across the space between said electrodes when the superposed magnetic field is less than said electron cutoff fieldBc.
This invention relates to a device for an electric switch which can operate at a high speed, and more particularly to a switch which can be used in a high voltage circuit. Furthermore it relates to such a device which acts as an over-current switch having means controlling the following current therein.
Ignitrons or thyratrons are representative tubes of the kind now in use as high speed switches in electric circuits. The former are essentially diode discharge tubes with control-electrodes and an igniter sealed therein. The latter are essentially triode discharge tubes containing a control grid. These control electrodes are made with special care and moreover they are exposed to a discharge when the tube is in a closed circuit. Therefore, they are easily and often damaged. Thus, considerable caution is required to increase the operable life thereof.
An object of this invention is to eliminate these drawbacks and to provide a novel high speed switch with long life for use in a high voltage circuit.
Another object of the invention is to provide a high voltage pulse generator with a simple circuit.
A further object of the invention is to provide an overcurrent circuit breaker which operates at high speed.
Further features and advantages of the invention will appear from the following description of a presently preferred species thereof.
' In the accompanying drawings:
FIGS. 1a and lb are an axial section and transverse section, respectively, of the device of the present invention;
3,405,300 Patented Oct. 8, 1968 FIG. 2 is a perspective view of an embodiment of the device of FIGS. la and 1b;
FIGS. 3 and 4 are graphs illustrating th static characteristics thereof;
FIGS. 5 and 6 are circuit diagrams of modifications of the circuit of the device shown in FIG. 2.
Referring to FIG. 1, the device comprises a cylindrical enclosure 2 having sealed into the interior thereof concentric electrodes 3 and 4, a small permanent magnet 5 between the poles of which is positioned the envelope 2, and a coil 6 wrapped around th enclosure 2 concentrically with the electrodes. Said electrodes can be of any non-magnetic and conducting material such as copper, aluminum, or carbon. However, it is preferable that they be of a refractory metal such as molybdenum or titanium, or their alloys. The enclosure 2 contains an ionizable medium such as hydrogen, neon, nitrogen, argon, miX- ture thereof, or an inert compound gas such as freon gas, etc., at a pressure ranging from l0 to 1 torr. The magnet 5 supplies an axial magnetic field. A power supply 7 is connected across the electrodes 3 and 4. The coil 6 is connected to said power supply 7 or to another supply. The current 8 flowing through the coil 6 acts as a driving current and controls the main current flow between electrodes 3 and 4 so that it either flows or does not flow in accordance with a novel means of the present invention. This device is essentially a crossed field discharge tube. A perspective sketch of the device is shown in FIG. 2, wherein the reference characters correspond to those in FIG. 1 and the various parts are designated by the same numbers.
For a better understanding of the invention, the static characteristics of the device will be described. FIG. 3 shows variations in sparking voltage and current relative to the axial magnetic field strength. Referring to FIG. 3, full line and dotted line 112 indicate the sparking voltage and a current characteristics respectively of coaxial electrode tubes in an axial magnetic field. It is seen that there is a critical value of magnetic field strength at which the sparking voltage varies abruptly. In FIG. 3, Be designates the critical magnetic field strength, V0 are sparking voltages corresponding to magnetic field strengths lower than Be and V0 are sparking voltages corresponding to magnetic field strengths greater than Be. The actual magnetic field strength is a combination of the static magnetic field strength Bs of permanent magnet 5 and the magnetic field strength Bx of coil 6. The magnetic field strength Bs is selected so that its value is lower than the critical magnetic field strength Be as shown in FIG. 3, while the voltage Va applied across electrodes 3 and 4 is adjusted to have a value between V0 and V0. When the DC driving current 8 shown in FIG. 2 is not supplied to said coil 6, i.e. Bx is zero, the device will be in open circuit condition. If a driving current 8 is supplied to said coil 6, Bx appears and the field strength increases. When it becomes higher than Be, the device will be in the closed circuit condition and a current, Ic in FIG. 3, flows. Therefore the device can be used as a switch by controlling said driving current 8 in said coil 6.
The device acts as a switch even when the applied voltage is as high as said voltage V0, i.e. maximum operating voltage is V0. FIG. 4 shows typical variations in said V0 in relation to the gas pressure of the ionizable medium.
When designing the device, the following essential facts should be considered: For the achievement of a sharp cut-01f characteristic, the gas pressure P in said enclosure must be lower than M/ (r r where n is a mean free path of an electron at 1 torr and r and r are the radius of the inner and outer electrodes, respectively. He can be expressed as follows:
(inner electrode as the cathode) (inner electrode as the anode) where e and m are the charge and the mass of an electron respectively, and Va is the applied voltage. The field strength of the magnet should be slightly lower than Bc. In order to reduce the size of said magnet, it is preferable that the inner electrode be used as the anode. It is also important, in order to increase the operating life, that the electrode materials be refractory metal such as tantalum or molybdenum. When designing the device, the following factors should also be considered. It is necessary to select a suitable material for the aforesaid ionizable medium. A light gas such as hydrogen is suitable if a short ignition time is desired, and for a short quenching time a polyatomic gas such as gaseous ethylalcohol is suitable. The operable life of the device can be prolonged by employing an outer cylinder which is 20% shorter than the inner cylinder. A longer outer cylinder frequently causes damage of the envelope at its corner. In order to make the operating voltage of the device that which is desired, the gas pressure and the type of gas therein should be properly selected, various different gases and gas pressures producing various operating voltages. A mixture of various kinds of gases requires special attention to the Penning effect which tends to lower the operating voltage, as disclosed in Electrical Breakdown of Gases, Oxford Press 1953, edited by J. M. Meek et al. A chemical compound gas such as freon gas is suited for high voltage operation.
The device isTessentially a cold-cathode discharge tube. Therefore, the constitution thereof is essentially simpler than a hot-cathode tube such as a thyratron. Since the device has no electric contacts therein, no contact failures need be expected during operating periods. This results in an increase in the operable life. Furthermore, since the device operates in a magnetic field, the deionization time is remarkably shorted. Therefore, the quenching time of the ionized medium in the novel device can be shorter than that of a tube such as a thyratron wherein a magnetic field is not used.
T-ypical specifications for the device are as follows: The radii of the inner electrode and outer electrode are 5 mm. and mm., respectively. The inner electrode is connected on an anode. The ionizable medium is nitrogen at a pressure of 2X10 torr. The magnetic field strength of the permanent magnet is 35 gauss. The radius of the coil is mm. the number of turns is 1000 and the driving current ranges from 20 to ma. The maximum controlled current is 50 A., the operating voltage ranges from 500 v. to 10 kilovolts and the time response is 10- seconds. The operating characteristics of the device can be chosen within the following range: maximum operating voltage is 10 kilovolts or more; the voltage drop between cylindrical electrodes is several hundred volts or less; maximum controlled current is 10 ka.; and the time response is lO 10- seconds.
The device according to the invention can easily be designed to act as a high speed circuit-breaker. Referring '4 to FIG. 1, the cylindrical electrodes 3 and 4 are connected to a load circuit. When the value Bs of the permanent magnet so as to be is chosen slightly larger than the value Be, the device closes any circuit in which it is connected. When a load current from such a circuit is supplied as a driving current to the coil 6 in a direction to reduce the static magnetic field of the permanent magnet and B is reduced to a value less than Bc, the device opens the circuit. Thus, the load current supplied as a driving current operates said device to the on or off condition.
With the device according to the present invention, a high voltage puulse can easily be generated. Referring to FIG. 5, reference character 11 designates a high voltage DC power supply the output voltage of which determines the peak value of a pulse voltage. A stabilizing resistor 12 is connected between one side of supply 11 and the device 13 of the present invention, which in turn is driven by an AC current supply 14. A small DC voltage supply 15 is connected between device 13 and out-put terminals 16 and controls the level of an out-put pulse. The high voltage pulse is generated by following procedure; high voltage Va(Va V0) is applied across the cylindrical electrodes of the device 13 and an AC current is supplied to the coil. During the period of half a cycle of the AC current, the value Bs increases to a value higher than an the value Bo, and accordingly, the device closes the circuit which causes the generation of a high voltage pulse across the out-put terminals -16.
With the device according to the invention, a DC current controlled device can easily be made. Referring to FIG. 6, a DC power supply 21, load 22, and electrodes 23 and coil 24 of the device 27 according to the present invention are connected in series. The DC load current 25 is supplied to the coil 24 in a direction which is the reverse of that of FIG. 2. Therefore, the actual magnetic field strength B decreases with increasing load current. At the usual operating conditions, the magnetic field strength B is selected so as to have a value slightly larger than Bc, and as a result the device 27 closes the circuit. When the load current exceeds a predetermined value B is reduced to a value less than Ba, and the device 27 opens the circuit. By this means, the device 27 can control the load current. An auxiliary circuit 26 is useful for initiating the discharge between electrodes 23.
It is thought that the invention and its advantages will be understood from the foregoing description and it is apparent that various changes may be made in the form, construction and arrangement of the parts without departing from the spirit and scope of the invention or sacrificing its material advantages, the forms hereinbefore described and illustrated in the drawings being merely preferred embodiments thereof.
We claim:
1. An electric switch of the coaxial cylinder type comprising a gas tight envelope, a pair of cylindrical electrodes enclosed in said gas tight envelope and consisting of an outer cylindrical electrode and an inner cylindrical electrode surrounded at least partially by said outer cylindrical electrode, one of said pair of cylindrical electrodes being a cold cathode and another of said pair of cylindrical electrodes being an anode, an ionizable medium filling said envelope and being at a low pressure less than MH -r torr, where A is the mean free path of an electron at 1 torr and 1' and r are the radius of said inner and outer electrode, respectively, magnet means adjacent the outside of said envelope and consisting of a permanent magnet and a coil superposing a magnetic field between said electrodes in a direction transverse to the direction in which said electrodes are spaced, whereby said electric switch closes an electrical circuit across the space between said electrodes when said superposed magnetic field is more than the electron cut-off field Ba and opens said electrical circuit across the space between said electrodes when said superposed magnetic field is less than said electron cut-off field Bc.
2. An electric switch as claimed in claim 1 wherein the strength of the magnetic field of said permanent magnet is less than the electron cut-01f field Be and said coil superposes a magnetic field in a same direction as that of said permanent magnet to close the electric circuit.
3. An electric switch as claimed in claim 1 wherein the strength of the magnetic field of said permanent magnet is more than the electron cut-off field Be, and said coil superposes a magnetic field in a reverse direction to that of said permanent magnet to open the electric circuit.
References Cited UNITED STATES PATENTS Toulon 315348 X McArthur 315267 Coleman 313158 X Garshelis 313-153 X Boucher et a1 313161 X JAMES W. LAWRENCE, Primary Examiner.
R. JUDD, Assistant Examiner.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4066365 | 1965-07-07 |
Publications (1)
Publication Number | Publication Date |
---|---|
US3405300A true US3405300A (en) | 1968-10-08 |
Family
ID=12586754
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US517345A Expired - Lifetime US3405300A (en) | 1965-07-07 | 1965-12-29 | Gas filled coaxial type electric switch with magnetic field cut-off |
Country Status (1)
Country | Link |
---|---|
US (1) | US3405300A (en) |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3492532A (en) * | 1967-11-17 | 1970-01-27 | Minnesota Mining & Mfg | Overvoltage protection device |
US3641384A (en) * | 1970-03-16 | 1972-02-08 | Hughes Aircraft Co | Switching device |
US3735197A (en) * | 1971-08-13 | 1973-05-22 | V Pakin | Rectifier |
US4071801A (en) * | 1976-12-09 | 1978-01-31 | Hughes Aircraft Company | Crossed-field switch device and method for off-switching |
FR2472830A1 (en) * | 1979-12-26 | 1981-07-03 | Hughes Aircraft Co | DEVICE FOR CONTROLLING ELECTRICAL CONDUCTION IN PLASMA CROSS-CHAMPER MODE |
US4291255A (en) * | 1979-08-17 | 1981-09-22 | Igor Alexeff | Plasma switch |
US5585696A (en) * | 1991-12-06 | 1996-12-17 | Mitsubishi Denki Kabushiki Kaisha | High current density glow discharge switch |
US5597993A (en) * | 1992-11-10 | 1997-01-28 | Mitsubishi Denki Kabushiki Kaisha | Vacuum interrupter |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US1733679A (en) * | 1926-12-13 | 1929-10-29 | Ets Edouard Belin Soc | Arc rectifier |
US2039102A (en) * | 1934-04-28 | 1936-04-28 | Gen Electric | Control system for gaseous discharge devices |
US2615139A (en) * | 1949-05-14 | 1952-10-21 | Rca Corp | Gas rectifier tube employing magnetic field |
US2892145A (en) * | 1956-06-07 | 1959-06-23 | Ivan J Garshelis | Voltage regulators |
US3215893A (en) * | 1959-11-24 | 1965-11-02 | Csf | Cold cathode gaseous rectifier tube |
-
1965
- 1965-12-29 US US517345A patent/US3405300A/en not_active Expired - Lifetime
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US1733679A (en) * | 1926-12-13 | 1929-10-29 | Ets Edouard Belin Soc | Arc rectifier |
US2039102A (en) * | 1934-04-28 | 1936-04-28 | Gen Electric | Control system for gaseous discharge devices |
US2615139A (en) * | 1949-05-14 | 1952-10-21 | Rca Corp | Gas rectifier tube employing magnetic field |
US2892145A (en) * | 1956-06-07 | 1959-06-23 | Ivan J Garshelis | Voltage regulators |
US3215893A (en) * | 1959-11-24 | 1965-11-02 | Csf | Cold cathode gaseous rectifier tube |
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3492532A (en) * | 1967-11-17 | 1970-01-27 | Minnesota Mining & Mfg | Overvoltage protection device |
US3641384A (en) * | 1970-03-16 | 1972-02-08 | Hughes Aircraft Co | Switching device |
US3735197A (en) * | 1971-08-13 | 1973-05-22 | V Pakin | Rectifier |
US4071801A (en) * | 1976-12-09 | 1978-01-31 | Hughes Aircraft Company | Crossed-field switch device and method for off-switching |
US4291255A (en) * | 1979-08-17 | 1981-09-22 | Igor Alexeff | Plasma switch |
FR2472830A1 (en) * | 1979-12-26 | 1981-07-03 | Hughes Aircraft Co | DEVICE FOR CONTROLLING ELECTRICAL CONDUCTION IN PLASMA CROSS-CHAMPER MODE |
US4322661A (en) * | 1979-12-26 | 1982-03-30 | Huges Aircraft Company | Cross-field plasma mode electric conduction control device |
US5585696A (en) * | 1991-12-06 | 1996-12-17 | Mitsubishi Denki Kabushiki Kaisha | High current density glow discharge switch |
US5597993A (en) * | 1992-11-10 | 1997-01-28 | Mitsubishi Denki Kabushiki Kaisha | Vacuum interrupter |
US5646386A (en) * | 1992-11-10 | 1997-07-08 | Mitsubishi Denki Kabushiki Kaisha | Vacuum interrupter |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US3405300A (en) | Gas filled coaxial type electric switch with magnetic field cut-off | |
US4888518A (en) | Gas circulation apparatus for ceramic electron tubes | |
US2141654A (en) | Voltage regulator device | |
US3641384A (en) | Switching device | |
US3714510A (en) | Method and apparatus for ignition of crossed field switching device for use in a hvdc circuit breaker | |
US4291255A (en) | Plasma switch | |
US3612937A (en) | Low-pressure controlled discharge device with trigger electrode within hollow cathode | |
US2504231A (en) | Gaseous discharge device | |
US3558960A (en) | Switching device | |
US3382402A (en) | Multi-stable series connected gaseous discharge devices | |
US3303376A (en) | Triggered vacuum gap device employing gas evolving electrodes | |
US3678289A (en) | Magnetic field control circuit for crossed field switching devices | |
US3405301A (en) | Apparatus for producing quiescent plasma | |
US2184740A (en) | Mercury arc oscillator | |
US3435287A (en) | Deionization of a gas discharge device by varying the tube parameters | |
US2457948A (en) | Electron discharge device | |
US3636407A (en) | Gas-discharge device with magnetic means for extinguishing the discharge | |
US2750555A (en) | Voltage regulating apparatus | |
US3631319A (en) | Triggered spark gap device | |
US2813992A (en) | Gas discharge device utilizing controlled electron trapping | |
US2191595A (en) | Magnetically controlled gaseous discharge device | |
US2116677A (en) | Gaseous electric discharge device and method of operating the same | |
US3604977A (en) | A cross field switching device with a slotted electrode | |
US3519882A (en) | Gas discharge tube with magnetic means for extinguishing the discharge | |
US2124682A (en) | Electrical gaseous discharge device |