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US2805337A - Magnetron oscillators and their associated output circuits - Google Patents

Magnetron oscillators and their associated output circuits Download PDF

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Publication number
US2805337A
US2805337A US570240A US57024056A US2805337A US 2805337 A US2805337 A US 2805337A US 570240 A US570240 A US 570240A US 57024056 A US57024056 A US 57024056A US 2805337 A US2805337 A US 2805337A
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magnetron
output
factor
associated output
waveguide
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Expired - Lifetime
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US570240A
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Dunsmuir Robert
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British Thomson Houston Co Ltd
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British Thomson Houston Co Ltd
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/36Coupling devices having distributed capacitance and inductance, structurally associated with the tube, for introducing or removing wave energy

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  • This invention relates to magnetron oscillators and their associated output circuits, and in particular to such oscillators utilised in the generation of very short pulses.
  • the build-up time of the magnetron should be kept as short as possible so that it occupies a minimum number of cycles of the R. F. oscillation.
  • the build-up time is governed by the Q factor of the loaded magnetron and will be a minimum when the Q factor is at a maxi mum. This unfortunately means that little power is coupled out of the magnetron.
  • the Q factor may be deiined as the ratio of resonator reactance to output resistance.
  • the present invention comprises the combination of a magnetron and an associated output circuit arranged so that on the commencement of a train of oscillations it presents the magnetron with a high output Q factor and thus allows a rapid build-up of R. F. oscillations in the magnetron, and wherein the output circuit has a suitably positioned reflector such that a fraction of the initial R. F. output will return to the magnetron and reduce the Q factor of the output circuit when the build-up of R. l". voltage has been substantially completed, so that substantial R. F. power may then be extracted from the magnetron.
  • the high external Q factor may be obtained by loosely coupling a waveguide to the magnetron.
  • a reflector in the form of an inductive post may be mounted in the waveguide at a suitable position to achieve the desired result.
  • Fig. 1 is a sectional View showing a magnetron connected to a waveguide output circuit.
  • Fig. 2 is a view along the line A-A of Fig. 1, and
  • Fig. 3 is an equivalent electrical circuit of the output of the magnetron shown in Fig. 1.
  • Magnetron i coupled to an associated output circuit formed by a rectangular waveguide feeder 7.
  • Magnetron l contains cathode 2 and an anode consisting of a number of vane segments.
  • the output resonator 3 of the anode is coupled by a tapered slot transformer 4 to the output waveguide 7.
  • This transformer is so arranged as to present a small resistance in series with the self-inductance of output resonator 3 when the waveguide is matched. If the output resonator is represented by an equivalent circuit of Fig. 3 which contains inductance L and capacitance C, then the resistance looking into slot 4 from the resoifr- Patented Sept. 3, 1957 nator 3 will be represented by R, where R is a small resistance.
  • slot 4 and the coupling to resonator 3 is so adjusted as to provide a high external Q factor for the system, for example 300.
  • Slot 4 tapers gradually so that a wave entering the narrow portion of the slot at 8 from the magnetron travels outwards along the waveguide 7 without appreciable reflection.
  • a metal post 6 is inserted across the waveguide to reflect the outgoing wave.
  • Post 6 is arranged as an inductive post and is positioned parallel to the shorter dimension of rectangular waveguide '7.
  • the wave reiiected from post 6 combines with the outgoing wave from the magnetron to present a resistance at the output resonator 3 which is considerably greater than the resistance which would occur at the same point in the absence of post 6.
  • the distance from resonator 3 to post 6 should correspond to an integral number (n) of half wavelengths plus an amount which is less than a quarter wavelength.
  • the value of n may be four times the number of cycles of oscillation required for buildup.
  • a reflectionless output window S may be mounted across the waveguide to provide a vacuum seal for the magnetron on whichever side of post 6 is convenient. To reduce the chance of breakdown of window 5 it is desirable to position this window at a point of minimum voltage for the standing wave pattern produced by the combination of outgoing and reliected waves.
  • a magnetron arranged to present the magnetron with a high output Q factor and thus allow a rapid build-up of radio frequency oscillation in the magnetron, and a reflector positioned in said oumut circuit by a distance from the magnetron equal to an integral number of half wavelengths of the oscillations plus a distance which is less than an eighth wavelength so that a fraction of the initial radio frequency output will return to the magnetron and reduce the Q factor of the output circuit when the build-up of radio frequency voltage has been substantially completed, whereby substantial radio frequency power may be then extracted from the magnetron.

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Description

R. DUNSMUIR 2,805,337 MACNETRON CSCILLATCRS AND THEIR ASSOCIATED OUTPUT CIRCUITS Filed March 8, 1956.
Sept. 3, 1957 ed Sata NIAGNETRUN OSSHLLATORS AND THE ASSCATED (BUTPUT CRCUITS This invention relates to magnetron oscillators and their associated output circuits, and in particular to such oscillators utilised in the generation of very short pulses.
It is important that in magnetron oscillators required to generate very short pulses (e. g. pulses of the order of 0.1 micro-second and containing about 300 oscillatory cycles) the build-up time of the magnetron should be kept as short as possible so that it occupies a minimum number of cycles of the R. F. oscillation. The build-up time is governed by the Q factor of the loaded magnetron and will be a minimum when the Q factor is at a maxi mum. This unfortunately means that little power is coupled out of the magnetron. The Q factor may be deiined as the ratio of resonator reactance to output resistance.
It is the object of the present invention to obtain a quick build-up combined with a high power output.
The present invention comprises the combination of a magnetron and an associated output circuit arranged so that on the commencement of a train of oscillations it presents the magnetron with a high output Q factor and thus allows a rapid build-up of R. F. oscillations in the magnetron, and wherein the output circuit has a suitably positioned reflector such that a fraction of the initial R. F. output will return to the magnetron and reduce the Q factor of the output circuit when the build-up of R. l". voltage has been substantially completed, so that substantial R. F. power may then be extracted from the magnetron.
The high external Q factor may be obtained by loosely coupling a waveguide to the magnetron. A reflector in the form of an inductive post may be mounted in the waveguide at a suitable position to achieve the desired result.
in order that the invention may be more fully understood reference will now be made to the accomparr drawing, in which:
Fig. 1 is a sectional View showing a magnetron connected to a waveguide output circuit.
Fig. 2 is a view along the line A-A of Fig. 1, and
Fig. 3 is an equivalent electrical circuit of the output of the magnetron shown in Fig. 1.
Referring now to Figs. l and 2, in which like parts have like references, there is shown a magnetron i coupled to an associated output circuit formed by a rectangular waveguide feeder 7. Magnetron l contains cathode 2 and an anode consisting of a number of vane segments. The output resonator 3 of the anode is coupled by a tapered slot transformer 4 to the output waveguide 7. This transformer is so arranged as to present a small resistance in series with the self-inductance of output resonator 3 when the waveguide is matched. If the output resonator is represented by an equivalent circuit of Fig. 3 which contains inductance L and capacitance C, then the resistance looking into slot 4 from the resoifr- Patented Sept. 3, 1957 nator 3 will be represented by R, where R is a small resistance.
In calculating the Q factor of this circuit, i. e. the ratio of reactance to resistance, account must be taken of the inductance and capacitance of the other resonators which are effectively connected across BB in Fig. 3. If N is the number of anode resonators in the magnetron and L is the inductance per resonator, then it can be shown that the eiective Q factor of the system (that is the Q factor which takes account of the power dissipation in the load only) is approximately given by where w is Zar times the frequency.
The width of slot 4 and the coupling to resonator 3 is so adjusted as to provide a high external Q factor for the system, for example 300. Slot 4 tapers gradually so that a wave entering the narrow portion of the slot at 8 from the magnetron travels outwards along the waveguide 7 without appreciable reflection. In accordance with the invention a metal post 6 is inserted across the waveguide to reflect the outgoing wave. Post 6 is arranged as an inductive post and is positioned parallel to the shorter dimension of rectangular waveguide '7.
The wave reiiected from post 6 combines with the outgoing wave from the magnetron to present a resistance at the output resonator 3 which is considerably greater than the resistance which would occur at the same point in the absence of post 6. For this condition to be satised the distance from resonator 3 to post 6 should correspond to an integral number (n) of half wavelengths plus an amount which is less than a quarter wavelength. The value of n may be four times the number of cycles of oscillation required for buildup. A reflectionless output window S may be mounted across the waveguide to provide a vacuum seal for the magnetron on whichever side of post 6 is convenient. To reduce the chance of breakdown of window 5 it is desirable to position this window at a point of minimum voltage for the standing wave pattern produced by the combination of outgoing and reliected waves.
While the invention has been described with reference to a particular embodiment employing a vane type magnetron and a waveguide output feeder it will be appreciated that other types of magnetron and other types of feeder, such as co-axial lines, can be used without departing from the invention.
What I claim is:
ln combination, a magnetron, an associated output circuit arranged to present the magnetron with a high output Q factor and thus allow a rapid build-up of radio frequency oscillation in the magnetron, and a reflector positioned in said oumut circuit by a distance from the magnetron equal to an integral number of half wavelengths of the oscillations plus a distance which is less than an eighth wavelength so that a fraction of the initial radio frequency output will return to the magnetron and reduce the Q factor of the output circuit when the build-up of radio frequency voltage has been substantially completed, whereby substantial radio frequency power may be then extracted from the magnetron.
References Cited in the le of this patent UNITED STATES PATENTS
US570240A 1955-03-16 1956-03-08 Magnetron oscillators and their associated output circuits Expired - Lifetime US2805337A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB7701/55A GB791735A (en) 1955-03-16 1955-03-16 Improvements relating to magnetron oscillators and their associated output circuits

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FR (1) FR1149225A (en)
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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3003118A (en) * 1958-03-31 1961-10-03 Sanders Associates Inc Synchronized regenerative amplifier
US3309558A (en) * 1963-10-07 1967-03-14 Varian Associates Electromagnetic wave transmission systems including a dielectric window for transmitting high-frequency highpower electromagnetic energy to a load from a source of suchenergy such as a resonant cavity of a klystron
US3364383A (en) * 1962-10-19 1968-01-16 English Electric Valve Co Ltd Waveguide impedance transformers
US3510720A (en) * 1967-07-03 1970-05-05 Varian Associates Traveling wave tubes having frequency dependent attenuative gain equalizers
US4356430A (en) * 1980-09-05 1982-10-26 Varian Associates, Inc. Gyrotron cavity resonator with an improved value of Q

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2630533A (en) * 1945-10-10 1953-03-03 Melvin A Herlin Magnetron frequency stabilization apparatus
US2765423A (en) * 1950-12-18 1956-10-02 Litton Industries Inc Magnetron output coupler

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2630533A (en) * 1945-10-10 1953-03-03 Melvin A Herlin Magnetron frequency stabilization apparatus
US2765423A (en) * 1950-12-18 1956-10-02 Litton Industries Inc Magnetron output coupler

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3003118A (en) * 1958-03-31 1961-10-03 Sanders Associates Inc Synchronized regenerative amplifier
US3364383A (en) * 1962-10-19 1968-01-16 English Electric Valve Co Ltd Waveguide impedance transformers
US3309558A (en) * 1963-10-07 1967-03-14 Varian Associates Electromagnetic wave transmission systems including a dielectric window for transmitting high-frequency highpower electromagnetic energy to a load from a source of suchenergy such as a resonant cavity of a klystron
US3510720A (en) * 1967-07-03 1970-05-05 Varian Associates Traveling wave tubes having frequency dependent attenuative gain equalizers
US4356430A (en) * 1980-09-05 1982-10-26 Varian Associates, Inc. Gyrotron cavity resonator with an improved value of Q

Also Published As

Publication number Publication date
GB791735A (en) 1958-03-12
FR1149225A (en) 1957-12-23

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