US3295062A - High frequency electrical oscillation generators - Google Patents

High frequency electrical oscillation generators Download PDF

Info

Publication number
US3295062A
US3295062A US342002A US34200264A US3295062A US 3295062 A US3295062 A US 3295062A US 342002 A US342002 A US 342002A US 34200264 A US34200264 A US 34200264A US 3295062 A US3295062 A US 3295062A
Authority
US
United States
Prior art keywords
arc
electrode
electrodes
waveguide
input
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
US342002A
Other languages
English (en)
Inventor
Froome Keith Davy
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.)
National Research Development Corp UK
Original Assignee
Nat Res Dev
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 Nat Res Dev filed Critical Nat Res Dev
Application granted granted Critical
Publication of US3295062A publication Critical patent/US3295062A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • H—ELECTRICITY
    • H03—ELECTRONIC CIRCUITRY
    • H03B—GENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
    • H03B11/00—Generation of oscillations using a shock-excited tuned circuit
    • H03B11/04—Generation of oscillations using a shock-excited tuned circuit excited by interrupter
    • H03B11/08—Generation of oscillations using a shock-excited tuned circuit excited by interrupter interrupter being discharge tube
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
    • H01J25/005—Gas-filled transit-time tubes
    • H—ELECTRICITY
    • H03—ELECTRONIC CIRCUITRY
    • H03B—GENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
    • H03B19/00—Generation of oscillations by non-regenerative frequency multiplication or division of a signal from a separate source

Definitions

  • This invention relates to high frequency electrical oscillation generators and is more particularly concerned with the generation of energy at -microwave frequencies by arrangements resembliny those already described in prior U.K. patent specification No. 944,983 and in which a very short high intensity cold cathode arc discharge is coupled to and maintained by energy from a microwave power source and which includes an output circuit, e.g., a suitable waveguide, designed to extract and transmit output power at harmonic frequencies of the input microwave energy.
  • an output circuit e.g., a suitable waveguide
  • Objects of the invention include the improvement of the operating efficiency of such generators and the reduction or elimination of unwanted harmonic frequencies in the output energy.
  • each of the said first and second arc electrodes is of metal rod or wire form and means are provided for operating said arc discharge in an inert gas at a high pressure of between 1,000 and 4,000 lbs./ sq. inch in order to provide a dense plasma region between and joining said arc electrodes.
  • the gas filling is mainly of argon with a small percentage, say, 4% to 15% of hydrogen to inhibit plasma diffusion.
  • the arc discharge is located within a cavity or waveguide forming part of the power output cincuit and the coupling of the input microwave power to the are is effected by the disposition of one arc electrode across a rectangular section waveguide carrying the input microwave energy.
  • the invention also includes a method of operating a generator as referred to above and in which one arc electrode is of smaller cross section than the oth-er in order to first obtain and thereafter maintain the optimum arc dimension for deriving a chosen harmonic output frequency.
  • the are is initially driven 'by the combined action of the input microwave energy and a D.C. voltage across the arc electrodes to cause transport of electrode metal from the smaller cross section electrode to the larger cross section electrode whereby the arc dimension is progressively changed towards a value at which it becomes resonant at the required harmonic frequency.
  • the initial D.C. energisation is replaced by an A.C.
  • energisation preferably of square waveform, at a suitable frequency, preferably but not essentially within the range of MiO-5,000 c.p.s., whereby the optimum arc dimension is thereafter maintained by successive transfer of electrode material backwards and forwards lfrom one electrode to the other.
  • FIGURE l is a perspective view, with parts broken away, of an ultra-high frequency electrical oscillation generator constructed in accordance with the invention
  • ⁇ while FGURE 2 is a cross sectional view of the central arc discharge region of the device of FIG. l drawn to an enlarged scale.
  • the embodiment illustrated comprises a rectangular shaped base block 1t) of metal, eg., brass, having three borings therethrough extending respectively between the approximate centre points of its three pairs of opposite side walls.
  • One of the horizontal bores is formed at its central region as a rectangular section input waveguide 11 while the other horizontal bore is provided at its central region with an inserted circular section metal tube 40, e.g. of phosphor bronze, to form a circular section output waveguide 12.
  • the longitudinal axes of the two waveguides 11, 12 are disposed at right angles to one another and are so positioned that the outer surface of the tube 4G just breaks into the input waveguide 11 so that such tube surface is parallel and coincident with the lower wider surface of the input waveguide as may be seen more clearly in FiG. 2.
  • the bore defining the input waveguide 11 is formed at one end with a suitable screw threaded counterboring 41 to accommodate an input coupling connector 13 for the attachment of a further waveguide 42 by which input energy at a suitable Q-band frequency may be supplied t-o the input waveguide 11 through a cylindrical quartz window 14 which is secured by the coupling connector and serves hermetically to seal such input end of the guide.
  • the opposite end of the same bore is also counterbored and screw threaded at 43 to receive a plug 44 forming part of input matching control means which includes a screw threaded spindle 45 terminating at its outer end in a matching control knob 15 and at its inner end in a rectangular tuning piston 15 which is slidabie along the longitudinal axis of the rectangular waveguide 11.
  • the plug 44 forms part of sealing means by which this end of the waveguide 11 is also hermetically sealed.
  • the position of the piston 16 is adjustable along the guide by means of the knob 15.
  • the bore defining the output ⁇ waveguide 12 is similarly counterbored and screw threaded at one end to accommodate a screwed plug containing a threaded spindle to the outer end of which is attached a matching control knob 19 and to the inner end of which is secured a circular tuning piston 20 which is slida'ble along the axis of the circular waveguide 12 to a position controlled by the knob 19.
  • This piston is adjustable with an inner limit such that it can just touch a part of the cathode arc electrode as will be described later.
  • the plug accommodating this matching control means likewise forms part of means for hermetically sealing the related end of the waveguide 12 'while at the opposite end the same bore continues the waveguide surface defined by the inner surface of the tube 4G and terminates in an output coupling connector 17 which also includes a cylindrical quartz window 18 to effect hermetic sealing of this end of the waveguide 12.
  • the third bore in the block 11i is disposed so as to be perpendicular to each of the waveguides 11, 12 and is at a position where its axis intersects each of the longitudinal axes of such guides.
  • the lower cathode electrode 22 is constituted by a very thin platinum wire, e.g. of 0.008 inch diameter. This wire is secured to the upper end of a rod 46 which can be adjusted axially as described later. As seen more clearly in FIG. 2 ⁇ the upper end of the cathode wire 22 is embraced by and is slidable within the bore of a cylindrical cathode sheath 23, conveniently formed of annealed molybdenum. This sheath is itself secured in the upper end of a sleeve 24 which is also adjustable axially as described later. The lower end of the said third bore is counterbored and screw threaded at 47 to receive a sealing plug 48 forming part of a sealing gland Which includes the sealing elements 25 (FIG.
  • the sealing plug just referred to is itself bored internally and screw threaded to receive a threaded external region Of the sleeve 24, the latter terminating outwardly in an enlarged head 49 to which is attached a cathode plunger adjustment control member 26.
  • Such enlarged head 49 of the sleeve 24 is itself counterbored and screw threaded to receive the plug 50 of a further sealing gland surrounding the rod 46 carrying the cathode wire 22.
  • Such rod 46 is screw threaded at its outer end and this region is received within a threaded bore of the plug 50 and terminates at its Outward end in a cathode arc adjusting knob 27.
  • the inner, reduced diameter, end of the sheath 23 extends through a snug fitting aperture 51 in the output guide tube 40 to a chosen position just inside the inner guide surface, such choice of position being under the control of the cathode plunger adjusting member 26.
  • the cathode wire 22 itself extends still further inwards :beyond the inner end of the sheath 23 towards the centre ofthe output waveguide to a position which is accurately controllable by the arc adjusting knob 27.
  • the various sealing glands provide for hermetic sealing of this end of the third bore.
  • the opposing upper or anode electrode of the arc assembly 21 comprises a platinum wire 28 of substantially greater diameter and therefore cross sectional area .than the cathode wire 22, e.g. of 0.020 inch diameter.
  • This anode wire projects through a clearance aperture 30 in the tube 4) of the output waveguide, the clearance between the anode wire and the edge of the aperture being not more than 0.004 inch.
  • the lowermost end of the anode wire 28 which immediately faces the upper end of the cathode wire 22 is of pointed or conical shape.
  • the an-ode wire is adjustable axially by means described later and is slidable within a cylindrical tuning plunger 31 made of copper or other similar metal and itself adjustable in the same axial direction by control means to be described later.
  • Such tuning plunger 31 is slidable within the bore of a surrounding metal sleeve 33 made of copper or similar metal.
  • This sleeve is provided at its lower end with an enlarged diameter ange 34 the upper surface of which opposes the upper surface of the adjoining region of the input waveguide 12 formed in the block 10 but is separated and insulated therefrom by an interposed mica sheet 35 so as t-o -provide a capacitive coupling between the anode electrode 28 and the metal base block 10.
  • the sleeve 33 isV secured in position within an accommodating counterbore 452 of the said third bore by means of a screwed collar 36 made of insulating material and having an annular recess for accommodating a resilient sealing washer 53.
  • Such counterbore 52 is itself sealed through the intermediary of packing elements 54 by a sealing plug 55 inserted in an internally threaded counterbore at the upper end of the said third bore.
  • the said plug 55 is bored axially to accommodate a tubular member 56 the lower end of this is screw threaded for engagement with a threaded element of the packing elements S4 and carries the tuning plunger 31.
  • the upper end of such tubular member has an enlarged head to which is secured an anode plunger control member 32 whereby the axial position of the aforesaid tuning plunger 31 may be controlled from outside Q .the 19.10.03 2,0.
  • the said tubular member 56 is itself bored axially to accommodate a screw threaded member 57 whose lower end is connected to the anode wire 28 and whose upper end, after emerging through a packing gland 58, has secured .thereon the anode arc control knob 29 whereby the precise position of the lower end of the anode wire can be controlled from the exterior of the block 10.
  • the sealing glands provided ensure the hermetic sealing of the upper end of the third bore whereby the arc chamber and the inter communica-ting regions of the waveguides 11, 12 are hermetically'sealed and can be filled with a suitable inert gas under high pressure provided by way of communicating conduit 59 and external connector 60 to a gas supply source shown schematically at 61.
  • the gas supply preferably is of argon with the addition of a small amount of between 4% and 15% of hydrogen and the operating pressures, preferably controllable, lie between 1,000 and 4,000 pounds per square inch.
  • the input waveguide 11 is shown symbolically connected to an input oscillation generator 62 such as a C.W. klystron type generator operating at a frequency in the Q-band, e.g. 35 gc./s.
  • the output connector 17 is shown as supplying output energy to any desired load 63 by way of power monitoring means 64.
  • the upper or anode arc electrode 28, which is insulated from the metal block 10, is shown connected by way of a change-over switch 65 either to one terminal of a direct current supply source 66 or to one terminal of an alternating current supply source v67.
  • the opposite terminals of the two supply sources are connected to earth as is also the metal block 10 and the lower cathode arc electrode 22.
  • Variable resistances 63 and 69 are included in the respective D.C. and A.C. supply leads to control the amplitude of the currents supplied to the arc electrodes.
  • the D.C. source 66 is one capable of providing a current of the order of l -ampere at 200 Volts while the A.C. source 67 is one capable of providing a square wave output of 200 volts peak-to-peak and a current amplitude of up to 1 ampere.
  • the frequency of this source is conveniently within the range ZOO-5,000 cycles per second.
  • the input microwave power source 62 is arranged to-supply input energy to the waveguide 11 and appropriate matching adjustments are made by the knob 15 serving to control the position of the tuning piston 16 in the input waveguide 11.
  • the switch means 65 is positioned to supply direct current to the arc electrodes 22, 28 from the ydirect current source 66 and this is adjusted to a value of between 300 and 600 ma. by adjustment of the series resistance 68.
  • the input power from the oscillation generator 62 may be about l0 watts of microwave energy at the commencement of operation of the device.
  • the applied gas pressure from the source 61 is conveniently adjusted to be of the order of 2,400 lb./sq. inch.
  • the microwave input tuning is not approximately correct diiiiculty may be experienced in starting with the described direct current supply to the arc electrodes if the gas pressure is at the above quoted normal operating value of 2,400 p.s.i. In this case the gas pressure may be raised temporarily to 4,000 p.s.i. while adjustments are made and then lowered again.
  • the polarity of the applied direct current from the source 66 is such as to cause operation with the upper arc electrode 28 as ⁇ an anode and as a result of this there is a transport of platinum from the lower and thinner cathode wir'e 22 to the lower tip of the upper anode wire 28 and this transport of metal may be used to form a small ball of molten platinum on the anode which is allowed to grow in size until it is of such dimension that it becomes resonant at a desired one of the harmonic frequencies of the input Q-band energy supplied by the source 62. Such resonance point may be observed by the monitoring means 64 and when it is reached, the
  • the arc current from the A.C. supply is preferably limited to a value comparable with that obtained under the initial D.C. operation by adjustment of the second, noninductive, resistance 69 in series with the A.C. supply.
  • the change from D.C. to A.C. energisation of the arc inhibits further change in the mean size of the now-resonant arc and the molten ball end of the upper electrode 28 by reason of the alternate transport of electrode material from one arc electrode to the other.
  • Initial setting of the arc electrodes relative to one another is effected Iby means of the control knobs 27 and 29.
  • Efficient energisation of the arc by the input microwave source 62 arising from the pick-up constituted by the lower end of the anode rod 28 traversing the centre of the rectangular input guide 11 is facilitated by the provision of the matching control knob 15 and its attached tuning piston 16 and by positioning of the anode tuning plunger 31 through the intermediary of its control member 32.
  • Selection of the required harmonic output frequency and the attainment of maximum output at such frequency is effected by adjustment of the tuning piston 20 through the intermediary of the matching control knob 19 and by adjustment of position of the cathode sheath 23 relative to the arc electrode wire 22 through the intermediary of the adjusting member 26.
  • the platinum arc electrodes should be adjusted as describe-d -above to operate in a molten state under the action of the heat of the arc, such arc is still believed to be of the cold cathode type in that the electron emission is throught not to be predominantly of thermionic origin but most probably to be thermionically enhanced field emission caused by a region of the positive ion space-charge at the boundary between the plasma and the negative electrode.
  • the very dense plasma joining the anode electrode to the cathode electrode behaves like a wire and conducts the microwave drive into the space-charge regions.
  • a high frequency oscillation generator comprising a body having a sealed chamber therein, a first arc electrode of rod form projecting into said chamber, a second arc electrode of thin wire form also projecting into said chamber opposite said first electrode to define an arc gap between the ends of said arc electrodes, electric power supply means connected to said electrodes for establishing an arc discharge between said first and second are electrodes, microwave power input means for coupling input energy from a microwave power source to one of said arc electrodes, microwave power output means for extracting from said arc discharge output energy at a harmonic frequency of said input energy, and a gaseous filling of inert gas at a pressure of at least 1000 pounds per square inch in said chamber to provide a dense plasma region between and joining the opposing ends of said first and second arc electrodes.
  • said microwave power input means comprise a first waveguide in said body
  • said microwave power output means -comprise a second waveguide in said body, said first arc electrode extending across said iirst waveguide into said second waveguide and the arc gap between ⁇ said arc electrodes being in said second waveguide.
  • a generator according to claim 2 in which said first and second arc electrodes lie in a common axial line which is normal to each of two spaced planes which respectively contain the longitudinal axes of said first and second waveguides.
  • a generator according to claim 3 in which the longitudinal axes of said first and second waveguides are at right angles.
  • a generator according to claim 2 in which said first waveguide is a rectangular section waveguide, said first arc electrode extending thereacross in a median plane parallel to the lesser side walls of said first waveguide and in which said second waveguide is a circular section waveguide, said arc gap being substantially coincident with the axis of said second waveguide.
  • a generator according to claim 1 in which said first arc electrode is of much greater cross section than said second arc electrode and is of pointed shape at its arc discharge end.
  • a generator according to claim 1 in which said inert gas comprises a major part of argon.
  • a generator according to claim 1 in which at least one of said arc electrodes is embraced adjacent the arc discharge end thereof by a surrounding conductive sheath of substantially greater cross section, said sheath being adjustable in the axial direction of the arc electrode to form a tuning plunger.
  • a generator according to claim 1 which includes means for supplying alternating current to said arc electrodes during operation of the generator.
  • a generator according to claim 13 in which said alternating current supply means are arranged to provide current having an alternation frequency in the range ZOO-5,000 cycles per second.
  • a generator according to claim 14 which also includes means for supplying direct current and switching means for ⁇ connecting either said direct current supply or said alternating current supply to said arc electrodes.

Landscapes

  • Plasma Technology (AREA)
US342002A 1963-02-08 1964-02-03 High frequency electrical oscillation generators Expired - Lifetime US3295062A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB5279/63A GB1034645A (en) 1963-02-08 1963-02-08 Improvements in high frequency electrical oscillation generators

Publications (1)

Publication Number Publication Date
US3295062A true US3295062A (en) 1966-12-27

Family

ID=9793117

Family Applications (1)

Application Number Title Priority Date Filing Date
US342002A Expired - Lifetime US3295062A (en) 1963-02-08 1964-02-03 High frequency electrical oscillation generators

Country Status (4)

Country Link
US (1) US3295062A (en))
BE (1) BE643492A (en))
FR (1) FR1453230A (en))
GB (1) GB1034645A (en))

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3521121A (en) * 1968-07-05 1970-07-21 Ikor Inc Oxygen containing,superatmospheric envelope used as a pulse generator
CN102395244A (zh) * 2011-10-21 2012-03-28 无锡绿波新能源设备有限公司 微波发生天线

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2817045A (en) * 1952-02-05 1957-12-17 Itt Electromagnetic wave generator
US2848649A (en) * 1952-01-24 1958-08-19 Itt Electromagnetic wave generator
US3058028A (en) * 1948-05-24 1962-10-09 Wilkes Gilbert Thermionic type detector for microwave signals
US3069634A (en) * 1958-01-13 1962-12-18 Gen Electric Co Ltd Microwave arc-type modulator
US3099768A (en) * 1959-03-25 1963-07-30 Gen Electric Low noise electron beam plasma amplifier

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3058028A (en) * 1948-05-24 1962-10-09 Wilkes Gilbert Thermionic type detector for microwave signals
US2848649A (en) * 1952-01-24 1958-08-19 Itt Electromagnetic wave generator
US2817045A (en) * 1952-02-05 1957-12-17 Itt Electromagnetic wave generator
US3069634A (en) * 1958-01-13 1962-12-18 Gen Electric Co Ltd Microwave arc-type modulator
US3099768A (en) * 1959-03-25 1963-07-30 Gen Electric Low noise electron beam plasma amplifier

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3521121A (en) * 1968-07-05 1970-07-21 Ikor Inc Oxygen containing,superatmospheric envelope used as a pulse generator
CN102395244A (zh) * 2011-10-21 2012-03-28 无锡绿波新能源设备有限公司 微波发生天线

Also Published As

Publication number Publication date
FR1453230A (fr) 1966-06-03
GB1034645A (en) 1966-06-29
BE643492A (en)) 1964-05-29

Similar Documents

Publication Publication Date Title
US2439401A (en) Magnetron oscillator of the resonant cavity type
GB555825A (en) Improvements in high frequency apparatus embodying electron discharge tubes
US4751429A (en) High power microwave generator
US2427752A (en) Concentric line lamp for measuring high-frequency power
US2364732A (en) Ultra high frequency generator
US2428622A (en) Tuning and coupling means for highfrequency systems
US3295062A (en) High frequency electrical oscillation generators
US2428193A (en) Magnetron
US2513933A (en) Cold cathode magnetron
US5552672A (en) Magnetron construction particularly useful as a relativistic magnetron
US2096817A (en) High frequency oscillator
US2252118A (en) Electron tube
US3392308A (en) Crossed field tube having a pair of permanent magnets of different magn etomotive force
US2184740A (en) Mercury arc oscillator
US3325740A (en) High frequency oscillation generators
US3636407A (en) Gas-discharge device with magnetic means for extinguishing the discharge
US2428609A (en) High-frequency electric discharge device
US3013180A (en) Magnetron device and system
US2953714A (en) High frequency electric discharge devices
US2928987A (en) Magnetron device and system
US2519826A (en) Electron discharge device
US2797324A (en) Space resonant system
US2582202A (en) Electrical breakdown device
US2846618A (en) Magnetron
US2514925A (en) High-frequency electric discharge device and system therefor