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US3193727A - Smoothing circuit for magnetic field generator in series with a.c.-operated magnetron - Google Patents

Smoothing circuit for magnetic field generator in series with a.c.-operated magnetron Download PDF

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US3193727A
US3193727A US234331A US23433162A US3193727A US 3193727 A US3193727 A US 3193727A US 234331 A US234331 A US 234331A US 23433162 A US23433162 A US 23433162A US 3193727 A US3193727 A US 3193727A
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magnetron
magnetic field
inductor
current
anode
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US234331A
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Reftmark Karl Sven-Olof
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US Philips Corp
North American Philips Co Inc
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US Philips Corp
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    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/02—Electrodes; Magnetic control means; Screens
    • H01J23/10—Magnet systems for directing or deflecting the discharge along a desired path, e.g. a spiral path

Definitions

  • the present invention relates to a magnetron circuit in which the magnetic field for the magnetron is produced at least partly by a coil connected in series with the cathode-anode path of the magnetron.
  • the circuit accordingto the invention is in particular adapted to be used witha magnetron fed directly from an alternatingcurrent source or from a power source having an output voltage of which contains a relatively high alternatingcurrent component, such as, for example, a single phase full wave rectifier or a 3-phase half Wave rectifier.
  • a relatively high alternatingcurrent component such as, for example, a single phase full wave rectifier or a 3-phase half Wave rectifier.
  • a device has already been described in which magnetrons fed from a common 3-phase full wave rectifier get all their magnetic field from a coil connected in series with the respective magnetron. Such an arrangement is possible in this case when the level of the output voltage from the 3-phase full wave rectifier is'relatively constant, i.e. when the harmonic content of the outputivoltage is relatively low.
  • the magnetron being operated intermittently with strong current peaks separated by periods during which the magnetron is cut-off, has been found to be undesirable due to the high alternating voltages across the coil and the strong eddy current losses produced thereby.
  • the eddy current losses are produced infthe cylinder of metal, usually copper, surrounding the interaction space of the magnetron, and also in magnetic yokes and pole shoes if present.
  • the cylinder 'forms the anode of the magnetron and at the same time formspart of the vacuum-tight envelope of the magnetron.
  • a method often used for smoothing the magnetic field and decreasing the voltage peaks across a coil connected in a circuit wherein the current varies greatly is to connect a capacitor in parallel with the coil.
  • the capacitor can be connected in series with a resistance.
  • magnetrons such a method has the drawback, however, that the initial current flowing through the magnetron is very high at the instant the magnetron is connected to the Voltage source, due to the fact that the impedance of the magnetron is low when the magnetic field is low.
  • a magnetron which has a magnetic field produced at least partly by a coil connected in series with the cathode-anode path of the magnetron.
  • a shunt circuit including a rectifying element is connected in parallel with the coil.
  • the rectifying element has a polarity such that the shunt circuit is cut-oif when the intensity of the magnetic field produced by the coil is increasing and conductive when the intensity of the magnetic field is decreasing.
  • An additional shunt circuit containing an impedance, in particular a resistance, is preferably connected in parallel with the coil.
  • This resistance is always in parallel with the coil and serves to reduce the high voltage peaks produced across the coil by the current variations during the intervals when the first shunt circuit is cut-off.
  • This impedance which may be a voltage dependent 2 resistor, should have a relatively high resistance value in comparison with the resistance value of the first shunt circuit.
  • a magnetron 1 is energized from an alternating-currentpower supply by way of a supply transformer (not shown).
  • the magnetron itself serves as a single phase half wave rectifier.
  • the magnetic flux of the coil 2 is concentrated by meansnot shown in the drawing within the interaction space of the magnetron. These means may comprise a magnetic yoke of iron which conducts the magnetic flux to two pole shoes situated on either side of the interactionspace of the magnetron.
  • the coil 2 may be: in the shape of a solenoid surrounding the magnetron.
  • the magnetron Due to the fact that the magnetron is energized directly from an alternating-current source, the magnetron operates interrnittently and conducts a high current only during a small fraction of each period, while it is cut-ofi' during the remainder of the period.
  • a magnetic field is built up by the coilZ.
  • the branch containing the rectifier 3 and the resistor 4 is cut-ofiduring these intervals due to the polarity with which the rectifier is connected.
  • the damping resistor 5 has a high resistance value, so that practically all of the anode .current is compelled torflow through the coil 2.
  • the entire anode current is compelledto flow through the coil 2 during the intervals when the magnetron is conducting. Owing to this fact, the great advantage is achieved that a high value of the anode current cannot appear without simultaneously building up a corresponding magnetic field.
  • the initial current is therefore maintained within allowable limits because an increase of the current through the magnetron results in an increase of the magnetic field and therefore in an increase of the impedance of the magnetron, which counteracts the increase of the current.
  • the resistor 5 which can be connected as a further shunt circuit in parallel with the coil 2 has mainly the function of attenuating the voltage peaks over the coil 2 a i g 3 during the intervals when the magnetic field is increasing and the shunt circuit containing the rectifier 3 and the resistor 4 is cut-oft".
  • the resistor 5 is permanently connected in parallel with the coil 2 and its value must therefore be large in comparison with the direct current resistance value of the coilZ, because it would otherwise consume too large an amount of energy and decrease the magnetic field.
  • the value of the resistance 5 is usually also considerably larger than the value of the resistor 4.
  • the circuit can be energized by any supply source, although the advantages of the invention are most apparent when energizing it from a source having relatively strong.
  • variations of the output voltage such as energizing the magnetron directly from an alternating-current power supply, from a single phase full wave rectifier, for example in the form of a bridge rectifier, from a 3'-phase half wave rectifier or the like.
  • the impedance element 6 may be deleted. It is also possible to use the circuit with a magnetron in which only a part of the magnetic field is produced by a coil connected in series with the cathode-anode path of the magnetron. With the circuit according to the invention, it is also possible to energize two or more magnetrons in parallel from a common supply source of the kind mentioned.
  • a magnetron energization circuit comprising a magnetron having an anode and a cathode, means providing a magnetic field for said magnetron comprising an inductor, a source of operating potential having an alternating component, means serially connecting said source of potential and inductor between said anode and cathode, whereby said magnetron conducts current intermittently, and unidirectional current conducting means connected in parallel with said inductor, said unidirectional current conducting means having a polarity to conduct only when the intensity of magnetic field in said inductor is decreasing, whereby fluctuations of intensiy of said magnetic field are reduced.
  • a magnetron energizing circuit comprising a magnetron having an anode and a cathode, means for providing a magnetic field for said magnetron comprising an inductor, a source of alternating potential, means connecting said source and inductor serially between said anode and cathode, whereby said magnetron intermittently conducts current and substantially all of said current flows through said inductor, and means for smoothing fluctuations of intensity of said magnetic field comprising unidirectional current conducting means connected in parallel with said IL inductor, said unidirectional current conducting means having a polarity to conduct current only when the intensity of said magnetic field is decreasing.
  • a magnetron energizing circuit comprising a magnetron having an anode and a cathode, means for provid ing a magnetic field for said magnetron comprising an inductor, a source of alternating potential, means connecting said source and inductor serially between said anode and cathode, whereby said magnetron intermittently conducts current and substantially all of said current flows through said inductor, and means for smoothing fluctuations of intensity of said magnetic field comprising a series circuit of resistor means and unidirectional current conducting means connected in parallel with said inductor, said unidirectional current conductive means having a polarity to conduct current only when the intensity of said magnetic field is decreasing.
  • circuit of claim 3 comprising additional resistor means connected in parallel with said inductor, said additional resistor means having a resistance substantially greater than the direct current resistance of said inductor and greater than the resistance of said first-mentioned resistor means.
  • a magnetron energizing circuit comprising a magnetron having an anode and a cathode, means providing a magnetic field for said magnetron comprising an inductor, means connecting one end of said inductor to said anode, a source of alternating potential, means connecting said source between said cathode and the other end of said inductor whereby said magnetron intermittently conducts current and substantially all of said intermittent current flows through said inductor, and means for smoothing fluctuations of intensity of said magnetic field comprising a series circuit of resistor means and rectifier means connected in parallel with said inductor, said rectifier means being connected in said series circuit with its anode toward said end of said inductor which is connected to said anode of said magnetron.

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Description

y 6, 1965 K. SVEN-OLOF REFTMARK 3,193,727
SMOOTHING' CIRCUIT FOR MAGNETIC FIELD GENERATOR IN SERIES WITH A.C.OPERATED MAGNETRON Filed Oct. 31, 1962 INVENTOR x4 RL svzu- OLOF nsrrmnx BY M Rm United States Patent 3,193,727 SMOGTHING GIRCUTT FOR MAGNETIQ FilELD GENERATOR IN SERHES WlTlli A.C.-0?ERATED MAGNETRON Karl Sven-Clot Reftmarir, Danderyd, Sweden, assignor to North American Philips (Zompany, Inc, New York, N.Y., a corporation of Delaware Filed Oct. 31, 1962, Ser. No. 234,331 Claims priority, application Sweden, Nov. 9, 1961,
6 Claims. (til. SIS-Quit) The present invention relates to a magnetron circuit in which the magnetic field for the magnetron is produced at least partly by a coil connected in series with the cathode-anode path of the magnetron. The circuit accordingto the invention is in particular adapted to be used witha magnetron fed directly from an alternatingcurrent source or from a power source having an output voltage of which contains a relatively high alternatingcurrent component, such as, for example, a single phase full wave rectifier or a 3-phase half Wave rectifier. border to stabilize the working point of a magnetron, circuits have been provided in which the anode current produces a fraction of the magnetic field of the magnetron by means of a coil connected in the anode current circuit. A device has already been described in which magnetrons fed from a common 3-phase full wave rectifier get all their magnetic field from a coil connected in series with the respective magnetron. Such an arrangement is possible in this case when the level of the output voltage from the 3-phase full wave rectifier is'relatively constant, i.e. when the harmonic content of the outputivoltage is relatively low. However, using of thesame circuit with a magnetron fed' for example from a single phase full wave rectifier ordirectly' from the alteriiating-cutrent power supply, the magnetron being operated intermittently with strong current peaks separated by periods during which the magnetron is cut-off, has been found to be undesirable due to the high alternating voltages across the coil and the strong eddy current losses produced thereby. The eddy current losses are produced infthe cylinder of metal, usually copper, surrounding the interaction space of the magnetron, and also in magnetic yokes and pole shoes if present. The cylinder'forms the anode of the magnetron and at the same time formspart of the vacuum-tight envelope of the magnetron.
A method often used for smoothing the magnetic field and decreasing the voltage peaks across a coil connected in a circuit wherein the current varies greatly is to connect a capacitor in parallel with the coil. The capacitor can be connected in series with a resistance. In the special case of magnetrons, such a method has the drawback, however, that the initial current flowing through the magnetron is very high at the instant the magnetron is connected to the Voltage source, due to the fact that the impedance of the magnetron is low when the magnetic field is low.
According to the invention, a magnetron is provided which has a magnetic field produced at least partly by a coil connected in series with the cathode-anode path of the magnetron. A shunt circuit including a rectifying element is connected in parallel with the coil. The rectifying element has a polarity such that the shunt circuit is cut-oif when the intensity of the magnetic field produced by the coil is increasing and conductive when the intensity of the magnetic field is decreasing.
An additional shunt circuit containing an impedance, in particular a resistance, is preferably connected in parallel with the coil. This resistance is always in parallel with the coil and serves to reduce the high voltage peaks produced across the coil by the current variations during the intervals when the first shunt circuit is cut-off. This impedance, which may be a voltage dependent 2 resistor, should have a relatively high resistance value in comparison with the resistance value of the first shunt circuit.
The invention will now be described more fully, by way of example, in reference to the accompanying drawing which shows a schematic diagram of a circuit according to the invention. i Y
In the embodiment shown a magnetron 1 is energized from an alternating-currentpower supply by way of a supply transformer (not shown). The magnetron itself serves as a single phase half wave rectifier. In series with through the magnetron to a certain degree. The magnetic flux of the coil 2 is concentrated by meansnot shown in the drawing within the interaction space of the magnetron. These means may comprise a magnetic yoke of iron which conducts the magnetic flux to two pole shoes situated on either side of the interactionspace of the magnetron. Alternately, the coil 2 may be: in the shape of a solenoid surrounding the magnetron.
The operation of the circuit arrangement is'as follows? Due to the fact that the magnetron is energized directly from an alternating-current source, the magnetron operates interrnittently and conducts a high current only during a small fraction of each period, while it is cut-ofi' during the remainder of the period. During theintervals when the magnetron is conducting, a magnetic field is built up by the coilZ. The branch containing the rectifier 3 and the resistor 4 is cut-ofiduring these intervals due to the polarity with which the rectifier is connected. The damping resistor 5 has a high resistance value, so that practically all of the anode .current is compelled torflow through the coil 2. When the anode current of the cbn-= ducting magnetronrhas' reached amaXimum valueand is beginning to decrease together'with the magneticifield:
produced'by the coil 2,'the decreasing magnetic field gives rise to a counter electromotiveforce having; ax polarity such that the rectifier 3 conducts and the energy contained in the magnetic field discharges through the resistor 4, with slowly decreasing magnetic field. During the succeeding current peak through the magnetron the magnetic field increases again and the process is repeated.
Due to the fact that the energy built up in the magnetic field can discharge through the resistor 4 of relatively low value, the voltage across the coil will attain only permiasible values and the fluctuations of the magnetic field and therefore the eddy current losses decrease While maintaining the magnetic field at a high value.
As previously mentioned practically the entire anode current is compelledto flow through the coil 2 during the intervals when the magnetron is conducting. Owing to this fact, the great advantage is achieved that a high value of the anode current cannot appear without simultaneously building up a corresponding magnetic field. When initially connecting the circuit arrangement to the supply voltage source the initial current is therefore maintained within allowable limits because an increase of the current through the magnetron results in an increase of the magnetic field and therefore in an increase of the impedance of the magnetron, which counteracts the increase of the current.
The resistor 5 which can be connected as a further shunt circuit in parallel with the coil 2 has mainly the function of attenuating the voltage peaks over the coil 2 a i g 3 during the intervals when the magnetic field is increasing and the shunt circuit containing the rectifier 3 and the resistor 4 is cut-oft". The resistor 5 is permanently connected in parallel with the coil 2 and its value must therefore be large in comparison with the direct current resistance value of the coilZ, because it would otherwise consume too large an amount of energy and decrease the magnetic field. The value of the resistance 5 is usually also considerably larger than the value of the resistor 4.
The invention is not limited to the embodiment shown and described. Thus, the circuit can be energized by any supply source, although the advantages of the invention are most apparent when energizing it from a source having relatively strong. variations of the output voltage, such as energizing the magnetron directly from an alternating-current power supply, from a single phase full wave rectifier, for example in the form of a bridge rectifier, from a 3'-phase half wave rectifier or the like. The impedance element 6 may be deleted. It is also possible to use the circuit with a magnetron in which only a part of the magnetic field is produced by a coil connected in series with the cathode-anode path of the magnetron. With the circuit according to the invention, it is also possible to energize two or more magnetrons in parallel from a common supply source of the kind mentioned.
. What is claimed is:
1. A magnetron energization circuit comprising a magnetron having an anode and a cathode, means providing a magnetic field for said magnetron comprising an inductor, a source of operating potential having an alternating component, means serially connecting said source of potential and inductor between said anode and cathode, whereby said magnetron conducts current intermittently, and unidirectional current conducting means connected in parallel with said inductor, said unidirectional current conducting means having a polarity to conduct only when the intensity of magnetic field in said inductor is decreasing, whereby fluctuations of intensiy of said magnetic field are reduced.
2. A magnetron energizing circuit comprising a magnetron having an anode and a cathode, means for providing a magnetic field for said magnetron comprising an inductor, a source of alternating potential, means connecting said source and inductor serially between said anode and cathode, whereby said magnetron intermittently conducts current and substantially all of said current flows through said inductor, and means for smoothing fluctuations of intensity of said magnetic field comprising unidirectional current conducting means connected in parallel with said IL inductor, said unidirectional current conducting means having a polarity to conduct current only when the intensity of said magnetic field is decreasing.
3. A magnetron energizing circuit comprising a magnetron having an anode and a cathode, means for provid ing a magnetic field for said magnetron comprising an inductor, a source of alternating potential, means connecting said source and inductor serially between said anode and cathode, whereby said magnetron intermittently conducts current and substantially all of said current flows through said inductor, and means for smoothing fluctuations of intensity of said magnetic field comprising a series circuit of resistor means and unidirectional current conducting means connected in parallel with said inductor, said unidirectional current conductive means having a polarity to conduct current only when the intensity of said magnetic field is decreasing.
4. The circuit of claim 3, comprising additional resistor means connected in parallel with said inductor, said additional resistor means having a resistance substantially greater than the direct current resistance of said inductor and greater than the resistance of said first-mentioned resistor means.
5. The circuit of claim 4, in which said additional resistor means is a voltage-dependent resistor.
6. A magnetron energizing circuit comprising a magnetron having an anode and a cathode, means providing a magnetic field for said magnetron comprising an inductor, means connecting one end of said inductor to said anode, a source of alternating potential, means connecting said source between said cathode and the other end of said inductor whereby said magnetron intermittently conducts current and substantially all of said intermittent current flows through said inductor, and means for smoothing fluctuations of intensity of said magnetic field comprising a series circuit of resistor means and rectifier means connected in parallel with said inductor, said rectifier means being connected in said series circuit with its anode toward said end of said inductor which is connected to said anode of said magnetron.
References Cited by the Examiner UNITED STATES PATENTS 9/38 Hollmann 328230 7/58 Smith 317-16 X

Claims (1)

1. A MAGNETRON ENERGIZATION CIRCUIT COMPRISING A MAGNETRON HAVING AN ANODE AND A CATHODE, MEANS PROVIDING A MAGNETIC FIELD FOR SAID MAGNETRON COMPRISING AN INDUCTOR, A SOURCE OF OPERATING POTENTIAL HAVING AN ALTERNATING COMPONENT, MEANS SERIALLY CONNECTING SAID SOURCE OF POTENTIAL AND INDUCTOR BETWEEN SAID ANODE AND CATHODE, WHEREBY SAID MAGNETRON CONDUCTS CURRENT INTERMITTENTLY AND UNIDIRECTIONAL CURRENT CONDUCTING MEANS CONNECTED IN PARALLEL WITH SAID INDUCTOR, SAID UNIDIRECTIONAL CURRENT CONDUCTING MEANS HAVING A POLARITY TO CONDUCT ONLY WHEN THE INTENSITY OF MAGNETIC FIELD IN SAIL INDUCTOR IS DECREASING, WHEREBY FLUCTUATIONS OF INTENSITY OF SAID MAGNETIC FIELD ARE REDUCED.
US234331A 1961-11-09 1962-10-31 Smoothing circuit for magnetic field generator in series with a.c.-operated magnetron Expired - Lifetime US3193727A (en)

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SE1116761 1961-11-09

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CN108305763A (en) * 2017-12-27 2018-07-20 中国船舶重工集团公司第七0研究所 A method of reappearing Weak magentic-field in screening arrangement

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2130132A (en) * 1936-07-16 1938-09-13 Telefunken Gmbh Magnetron
US2845580A (en) * 1954-04-30 1958-07-29 Gen Electric Electric protective equipment

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2130132A (en) * 1936-07-16 1938-09-13 Telefunken Gmbh Magnetron
US2845580A (en) * 1954-04-30 1958-07-29 Gen Electric Electric protective equipment

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