US3811099A - Means of securing ferrimagnetic core in a microwave phaser - Google Patents

Means of securing ferrimagnetic core in a microwave phaser Download PDF

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US3811099A
US3811099A US00397199A US39719973A US3811099A US 3811099 A US3811099 A US 3811099A US 00397199 A US00397199 A US 00397199A US 39719973 A US39719973 A US 39719973A US 3811099 A US3811099 A US 3811099A
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core
waveguide
ferrimagnetic
heat
conducting elements
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US00397199A
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R Mason
L Lavedan
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US Department of Navy
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/18Phase-shifters
    • H01P1/19Phase-shifters using a ferromagnetic device
    • H01P1/195Phase-shifters using a ferromagnetic device having a toroidal shape

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  • ABSTRACT A mounting assembly for mounting a rectangular ferrimagnetic core longitudinally within a rectangular waveguide of a high-power-mode phase shifter comprising:
  • the present invention relates generally to microwave phase shifters and more particularly to antenna phase shifters utilizing ferrite materials.
  • the phase shift caused by the ferrite rod can be varied.
  • phase shifter used to illustrate the present invention a hollow rectangular ferrimagnetic core is.
  • the phase is varied by sending a current pulse through the wire which acts to induce a magnetic flux in the toroid.
  • the current pulse has dissipated and thus H 0, there will still be some remanent magnetic flux density B in the toroid due to hysteresis effects.
  • the remanent flux density change will cause a change in the propagation constants in the toroid.
  • the microwave signal will pass through the ferrimagnetic toroid either faster or slower depending on whether the flux density is increased or decreased from its last level. This change in the electrical length of the toroid will cause the phase shift in the microwave signal.
  • the flux density is proportional to the size of the current pulse through the wire.
  • the phase shift can be varied by varying the size of the current pulse.
  • This invention concerns itself with mounting the toroid of ferrimagnetic material in the longitudinal center of a rectangular waveguide.
  • Ferrimagnetic core materials are generally fragile and magnetostrictive and therefore must be attached to, and supported in, the waveguide in a movement-restricting manner; yet the stresses on the ferrimagnetic materials resulting from the differential thermal expansions of thedifferent materials in the phase shifter must be limited to an acceptable level.
  • the invention comprises a mounting designed to properly restrict the movement of the ferrimagnetic core of a high-power-rnode phase shifter,- while allowing space for the thermal and magnetostrictive expansion of the ferrite material of the core.
  • An object of the present invention is to mount a ferrimagnetic core in a waveguide such thatmovement of this core will properly be. restricted while still allowing space for thermal and magnetostrictive expansion.
  • a further object is to provide the ferrimagnetic core from slipping out of its mountings in a waveguide.
  • FIGURE of the drawing is an embodiment of the present invention.
  • the drawing shows the basic ferrimagnetic-core phaseshifter that will be used to illustrate the present invention.
  • Thewalls of the rectangular waveguide 26 are made of metal.
  • the rectangular, ferrim'agnetic, toroid core 24 is positioned in the longitudinal center of the waveguide 26.
  • This core consists of a bonded stack of one or more ferrimagnetic toroids.
  • This wire 14 is fed into the toroid core by the feedline l2.
  • toroid core 24 On either side of toroid core 24 are heat-conducting elements 20 in the shape of Es.;Since the toroid core 24 dissipates large amounts of heat in a high-power mode, the optimum design for the heat-conducting element for optimum thermal conduction would be to completely surround the toroid core with the element. The problem is that the more material is placed around the toroid core 24, the poorer becomes the toroid cores electrical performance. Taking these two factors into consideration, it has been found that the optimum design is-in the shape of an E. This design will provide a small surface against the toroid core, while providing a large surface (back of the E) to transfer thermal energy to the waveguide wall where it can be dissipated.
  • a transformer is bonded to each end of the ferrite toroid core.
  • This transformer is' a dielectric, impedance-matching' transformer which acts to match the high impedance of the empty waveguide to the very low impedance of the ferrimagnetic toroid (dielectric constant E 16).
  • Multi-step transformers have been found best suited to perform this matching function.
  • the transformer may take any shape, the only requirement being that it completely cover the end of the toroid core and partially overlap the heat-conducting elements. The purpose of this overlap is to restrict the longitudinal movement of the toroid core with respect to the heat-conducting elements.
  • Dielectric keys 22 are inserted in keyholes positioned partially in the waveguide wall and partially in the heat conducting surface. These keys act to restrict the longitudinal movement of the heat conducting elements with respect to the waveguide walls 26.
  • the keys may be made of a dielectric material since if any highly conductive material such as a metal is used, the key appears to be an electrical bump in the waveguide. This electrical bump tends to disrupt the waveguide field and affect the V.S.W.R.
  • dielectric pins or pegs are used as the keys. There is no real limitation as to what shape the key may take so long as it rests partially in the heatconducting element and partially in the waveguide.
  • a thin metallic sheet 18, for example of aluminum, extends completely from one sidewall of the waveguide to the other sidewall and acts as the top and the bottom of the waveguide over the toroid.
  • the toroid core is made slightly higher than the adjacent heat-conducting elements.
  • the toroid will push-up on the metallic sheet while an aluminum cover 28 pushes down on the sheet thus giving a very tight contact between the waveguide metallic sheet 18 and the toroid core 24.
  • the toroid core 24 is (l) restricted by the heatconducting elements 20 from lateral movement, (2) restricted by the top and bottom of the'waveguide from vertical movement, (3) restricted by the transformer 10 from longitudinal movement with respect to the heat-conducting elements 20.
  • the longitudinal movement of the heat-conducting elements 20 with respect Obviously, many modifications and variations of the present invention are possible in light of the above teachings. It is therefore to be understood that, within the scope of the appended claims, the invention may be practiced otherwise than as specifically described.
  • a mounting assembly for mounting a core of ferrimagnetic material in a waveguide of a high-power microwave phase-shifter comprising:
  • a ferrimagnetic core mounted longitudinally within said waveguide
  • said ferrimagnetic core being restrained from motion in the sidewise direction by the heat-conducting elements, said ferrimagnetic core being restrained in the vertical direction by the top and bottom walls of said rectangular waveguide.
  • thermoelectric element is formed in the shape of an E, the long backside of the E being positioned against said waveguide and the three legs being positioned to face said ferrimagnetic core.
  • top and bottom walls of said waveguide are formed by a thin metallic sheet, and further, wherein said ferrimagnetic core has a higher height dimension than said heat-conducting elements such that said ferrimagnetic core pushes up on said thin metallic sheet thus making a tight contact between the top and bottom of said ferrimagnetic core and said waveguide.

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Abstract

A mounting assembly for mounting a rectangular ferrimagnetic core longitudinally within a rectangular waveguide of a highpower-mode phase shifter comprising: A. HEAT CONDUCTING ELEMENTS ON TWO OPPOSITE SIDES OF THE FERRIMAGNETIC CORE EXTENDING LONGITUDINALLY ALONG THE CORE; B. DIELECTRIC TRANSFORMERS AT EACH END OF THE CORE SO AS TO PARTIALLY OVERLAP THE ENDS OF THE HEAT-CONDUCTING ELEMENTS THEREBY RESTRICTING MOTION OF THE CORE WITH RESPECT TO THE WAVEGUIDE; C. DIELECTRIC PINS INSERTED INTO PIN-HOLES POSITIONED PARTIALLY IN THE WAVEGUIDE AND PARTIALLY IN THE HEAT-CONDUCTING ELEMENTS TO RESTRICT LONGITUDINAL MOTION OF THE HEAT-CONDUCTING ELEMENTS WITH RESPECT TO THE WAVEGUIDE.

Description

[4 1 May 14, 1974 United States Patent [191 Mason et al.
Primary Examiner-Paul L. Gensler CORE IN A MICROWAVE PHASER AlmrneLAgem, 0r Firm-R. S. Sciascia; P; Schneider;
E. LaRoche MEANS OF SECURING FERRIMAGNETIC [75] Inventors: Robert J. Mason, Medford, NJ.;
' Louis J. Lavedan, Jr., Springfield,
ABSTRACT A mounting assembly for mounting a rectangular ferrimagnetic core longitudinally within a rectangular waveguide of a high-power-mode phase shifter comprising:
a. heat conducting elements on two opposite sides of the ferrimagnetic core extending longitudinally along the core; 7 b. dielectric transformers at each end of the core so 8 h t d a CV. m A e D MS n 8 .h m m y 3 fibmw e mw U Q B v M. hw e TrN S e n .m d S e S H A F N .4 7 2 I... .l.
21 App]. No.: 397,199
as to partially overlap the ends of the heat-conducting elements thereby restricting motion of the core with respect to the waveguide;
Int Cl Field of Search.................
c. dielectric pins inserted into pin-holes positioned 2 M N 9. awe 3 4 ,H2 J u M M N P 3 3 3 3 partially in the waveguide and partially in the heat-conducting elements to restrict longitudinal 333/24.l 333/241 motion of the heat-conducting elements with Hem respect to the waveguide.
sm m N.m Mm sm SEC mTm m rT .mSA e D RE3 WW NH U9 5 4 N m w w 3,758,883 9/1973 Cox et al. 3,408,597 lO/l968 6 Claims, 1 Drawing Figure MEANS OF SECURING FERRIMAGNETIC CORE IN A MICROWAVE PHASER FIELD OF THE INVENTION The present invention relates generally to microwave phase shifters and more particularly to antenna phase shifters utilizing ferrite materials.
DESCRIPTION OF Tl-IE PRIOR ART producing a magnetic field surrounding the material.
By varying the strength of the magnetic field, the phase shift caused by the ferrite rod can be varied.
In the phase shifter used to illustrate the present invention a hollow rectangular ferrimagnetic core is.
mounted longitudinally within a rectangular waveguide. A wire mounted in a dielectric slab is inserted in the space within the hollow ferrimagnetic core. The phase is varied by sending a current pulse through the wire which acts to induce a magnetic flux in the toroid. When the current pulse has dissipated and thus H 0, there will still be some remanent magnetic flux density B in the toroid due to hysteresis effects. The remanent flux density change will cause a change in the propagation constants in the toroid. Thus the microwave signal will pass through the ferrimagnetic toroid either faster or slower depending on whether the flux density is increased or decreased from its last level. This change in the electrical length of the toroid will cause the phase shift in the microwave signal. The flux density is proportional to the size of the current pulse through the wire. Thus the phase shift can be varied by varying the size of the current pulse.
This invention concerns itself with mounting the toroid of ferrimagnetic material in the longitudinal center of a rectangular waveguide. Ferrimagnetic core materials are generally fragile and magnetostrictive and therefore must be attached to, and supported in, the waveguide in a movement-restricting manner; yet the stresses on the ferrimagnetic materials resulting from the differential thermal expansions of thedifferent materials in the phase shifter must be limited to an acceptable level.
The prime problem in such phase. shifters results from the face that the thermal expansion of the metal of the waveguide is much greater than the thermal expansion of the ferrimagnetic core. Thus during highpower-mode operation, when the ferrimagnetic core dissipates large amounts of heat, the waveguide will expand much more than the core, and thus the core will have a tendency to slip out of its mounting within the metal waveguide. A mounting that allows sufficient clearances for thermal and magnetostrictive expansion and yet restricts the movement of this core is therefore desirable.
SUMMARY OF THE INVENTION 1 Briefly, the invention comprises a mounting designed to properly restrict the movement of the ferrimagnetic core of a high-power-rnode phase shifter,- while allowing space for the thermal and magnetostrictive expansion of the ferrite material of the core.
Thus in a phase shifter where a toroid core of ferrimagnetic material is mounted longitudinally in a waveguide, movement of this toroid core is restricted by a. positioning heat-conducting elements on the sides of the-core between it and the waveguide so as to extend longitudinally along the core and restrict lateral movement; I
b. positioning dielectric transformers at each end of the core to completely cover the ends of the core and partially overlap the ends of the heat-conducting elements in order to restrict longitudinal motion of the core with respect to the heat-conducting elements;
c. placing a plurality of dielectric keys into a plurality of keyways, the keyways being positioned partially in the waveguide wall and partially in the heat-conducting elements and acting to restrict longitudinal motion of the heat-conducting element with respect to the waveguide;
d. restraining movement of the core top and bottom walls-of the waveguide.
OBJECTS OF THE INVENTION An object of the present invention is to mount a ferrimagnetic core in a waveguide such thatmovement of this core will properly be. restricted while still allowing space for thermal and magnetostrictive expansion.
A further object is to provide the ferrimagnetic core from slipping out of its mountings in a waveguide.
BRIEF DESCRIPTION OF THE DRAWING The single FIGURE of the drawing is an embodiment of the present invention.
DETAILED DESCRIPTION OF THE INVENTION The drawing shows the basic ferrimagnetic-core phaseshifter that will be used to illustrate the present invention. Thewalls of the rectangular waveguide 26 are made of metal. The rectangular, ferrim'agnetic, toroid core 24 is positioned in the longitudinal center of the waveguide 26. This core consists of a bonded stack of one or more ferrimagnetic toroids. The wire 14, embedded in a coaxial dielectric insert 16 in the center of I the toroid core, acts to conduct the pulse of current which will change theremanent flux density B, and thus roid appear electricallyshorteror longer to the microwave energy. This wire 14 is fed into the toroid core by the feedline l2.
On either side of toroid core 24 are heat-conducting elements 20 in the shape of Es.;Since the toroid core 24 dissipates large amounts of heat in a high-power mode, the optimum design for the heat-conducting element for optimum thermal conduction would be to completely surround the toroid core with the element. The problem is that the more material is placed around the toroid core 24, the poorer becomes the toroid cores electrical performance. Taking these two factors into consideration, it has been found that the optimum design is-in the shape of an E. This design will provide a small surface against the toroid core, while providing a large surface (back of the E) to transfer thermal energy to the waveguide wall where it can be dissipated.
Appropriate clearances are provided between the ferrimagnetic core 24 and the heat-conducting elements 20 to allow for thermal and magnetostrictive expansion. Thus, since the core is free to move within these clearances, the stresses inthe ferrite core due to expansion are limited to an acceptable value,
A transformer is bonded to each end of the ferrite toroid core. This transformer is' a dielectric, impedance-matching' transformer which acts to match the high impedance of the empty waveguide to the very low impedance of the ferrimagnetic toroid (dielectric constant E 16).
Multi-step transformers have been found best suited to perform this matching function. Themore steps used to provide intermediate steps between the two ex tremes, the better the broad-band matching characteristics.
In this particular case a two-step impedancematching transformer is used, though the invention is by no means limited to a two-step transformer,'and any number of steps are possible.
The transformer may take any shape, the only requirement being that it completely cover the end of the toroid core and partially overlap the heat-conducting elements. The purpose of this overlap is to restrict the longitudinal movement of the toroid core with respect to the heat-conducting elements.
Dielectric keys 22 are inserted in keyholes positioned partially in the waveguide wall and partially in the heat conducting surface. These keys act to restrict the longitudinal movement of the heat conducting elements with respect to the waveguide walls 26. The keys may be made of a dielectric material since if any highly conductive material such as a metal is used, the key appears to be an electrical bump in the waveguide. This electrical bump tends to disrupt the waveguide field and affect the V.S.W.R.
In the drawing, dielectric pins or pegs are used as the keys. There is no real limitation as to what shape the key may take so long as it rests partially in the heatconducting element and partially in the waveguide.
Due to the very high dielectric constant E of the ferrite material, if there is a low dielectric-constant gap between the ferrite toroidand the waveguide ceiling a number of unwanted modes are set up in the waveguide. Furthermore, there are unwanted absorptions and resonances such that the guide cannot work over a proper bandwidth. Thus a very tight fit between the waveguide and the toroid is desired. Inorder to accomplish this a thin metallic sheet 18, for example of aluminum, extends completely from one sidewall of the waveguide to the other sidewall and acts as the top and the bottom of the waveguide over the toroid.
The toroid core is made slightly higher than the adjacent heat-conducting elements. Thus, when the thin metallic sheet is placed over the toroid 24 and the heatconducting elements 20, the toroid will push-up on the metallic sheet while an aluminum cover 28 pushes down on the sheet thus giving a very tight contact between the waveguide metallic sheet 18 and the toroid core 24.
Thus the toroid core 24 is (l) restricted by the heatconducting elements 20 from lateral movement, (2) restricted by the top and bottom of the'waveguide from vertical movement, (3) restricted by the transformer 10 from longitudinal movement with respect to the heat-conducting elements 20. The longitudinal movement of the heat-conducting elements 20 with respect Obviously, many modifications and variations of the present invention are possible in light of the above teachings. It is therefore to be understood that, within the scope of the appended claims, the invention may be practiced otherwise than as specifically described.
What is claimed is:
1. A mounting assembly for mounting a core of ferrimagnetic material in a waveguide of a high-power microwave phase-shifter comprising:
a waveguide;
a ferrimagnetic core mounted longitudinally within said waveguide;
a plurality of heat-conducting elements positioned on two opposite sidesof said ferrimagnetic core and extending longitudinally along said ferrimagnetic core with a predetermined clearance between said ferrimagnetic core and said heat conducting elements to allow for thermal expansion;
a plurality of dielectric transformers, one bonded to each end of said ferrimagnetic core, completely covering the ends of said core and partially covering the ends of said heat-conducting elements thereby limiting the longitudinal motion of said core with respect to said heat-conducting elements;
a plurality of dielectric keys inserted into a plurality of keyways, said keyways being positioned partially in said waveguide wall and partially in said heatconducting elements and acting to restrict longitudinal motion of said heat-conducting elements with respect to said waveguide;
said ferrimagnetic core being restrained from motion in the sidewise direction by the heat-conducting elements, said ferrimagnetic core being restrained in the vertical direction by the top and bottom walls of said rectangular waveguide.
2. A mounting assembly as in claim 1, wherein. said heat-conducting element is formed in the shape of an E, the long backside of the E being positioned against said waveguide and the three legs being positioned to face said ferrimagnetic core.
3. A mounting assembly as in claim l, wherein said ferrimagnetic core is formed in the shape of a rectangular toroid.
4. A mounting assembly as in claim 1, wherein said dielectric keys are formed in the shape of pins.
5. A mounting assembly as in claim 1, wherein said vtransformers are two-step, microwave, impedancematching, dielectric transformers;
6. A mounting assembly as in claim 1, wherein the top and bottom walls of said waveguide are formed by a thin metallic sheet, and further, wherein said ferrimagnetic core has a higher height dimension than said heat-conducting elements such that said ferrimagnetic core pushes up on said thin metallic sheet thus making a tight contact between the top and bottom of said ferrimagnetic core and said waveguide.

Claims (6)

1. A mounting assembly for mounting a core of ferrimagnetic material in a waveguide of a high-power microwave phase-shifter comprising: a waveguide; a ferrimagnetic core mounted longitudinally within said waveguide; a plurality of heat-conducting elements positioned on two opposite sides of said ferrimagnetic core and extending longitudinally along said ferrimagnetic core with a predetermined clearance between said ferrimagnetic core and said heat conducting elements to allow for thermal expansion; a plurality of dielectric transformers, one bonded to each end of said ferrimagnetic core, completely covering the ends of said core and partially covering the ends of said heatconducting elements thereby limiting the longitudinal motion of said core with respect to said heat-conduCting elements; a plurality of dielectric keys inserted into a plurality of keyways, said keyways being positioned partially in said waveguide wall and partially in said heat-conducting elements and acting to restrict longitudinal motion of said heatconducting elements with respect to said waveguide; said ferrimagnetic core being restrained from motion in the sidewise direction by the heat-conducting elements, said ferrimagnetic core being restrained in the vertical direction by the top and bottom walls of said rectangular waveguide.
2. A mounting assembly as in claim 1, wherein said heat-conducting element is formed in the shape of an ''''E'''', the long backside of the ''''E'''' being positioned against said waveguide and the three legs being positioned to face said ferrimagnetic core.
3. A mounting assembly as in claim 1, wherein said ferrimagnetic core is formed in the shape of a rectangular toroid.
4. A mounting assembly as in claim 1, wherein said dielectric keys are formed in the shape of pins.
5. A mounting assembly as in claim 1, wherein said transformers are two-step, microwave, impedance-matching, dielectric transformers.
6. A mounting assembly as in claim 1, wherein the top and bottom walls of said waveguide are formed by a thin metallic sheet, and further, wherein said ferrimagnetic core has a higher height dimension than said heat-conducting elements such that said ferrimagnetic core pushes up on said thin metallic sheet thus making a tight contact between the top and bottom of said ferrimagnetic core and said waveguide.
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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3849746A (en) * 1973-10-18 1974-11-19 Us Navy Mounting assembly for ferrimagnetic core in waveguide phase shifter
US4445098A (en) * 1982-02-19 1984-04-24 Electromagnetic Sciences, Inc. Method and apparatus for fast-switching dual-toroid microwave phase shifter
EP0139800A1 (en) * 1983-11-01 1985-05-08 Electromagnetic Sciences, Inc. Method and apparatus for fast-switching dual-toroid microwave phase shifter
US5610562A (en) * 1992-11-12 1997-03-11 Ant Nachrichtentechnik Gmbh Waveguide absorber
EP2720312A1 (en) * 2012-10-12 2014-04-16 Honeywell International Inc. Systems and methods for injection molded phase shifter

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3408597A (en) * 1966-05-11 1968-10-29 Bell Telephone Labor Inc Nonreciprocal gyromagnetic waveguide device with heat transfer means forming a unitary structure
US3758883A (en) * 1972-05-15 1973-09-11 Bendix Corp Copper foil ferrite phase shifter
US3761845A (en) * 1972-07-27 1973-09-25 Hughes Aircraft Co Fabrication method and apparatus using ferrite for shifting phase of an electromagnetic wave

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3408597A (en) * 1966-05-11 1968-10-29 Bell Telephone Labor Inc Nonreciprocal gyromagnetic waveguide device with heat transfer means forming a unitary structure
US3758883A (en) * 1972-05-15 1973-09-11 Bendix Corp Copper foil ferrite phase shifter
US3761845A (en) * 1972-07-27 1973-09-25 Hughes Aircraft Co Fabrication method and apparatus using ferrite for shifting phase of an electromagnetic wave

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3849746A (en) * 1973-10-18 1974-11-19 Us Navy Mounting assembly for ferrimagnetic core in waveguide phase shifter
US4445098A (en) * 1982-02-19 1984-04-24 Electromagnetic Sciences, Inc. Method and apparatus for fast-switching dual-toroid microwave phase shifter
EP0139800A1 (en) * 1983-11-01 1985-05-08 Electromagnetic Sciences, Inc. Method and apparatus for fast-switching dual-toroid microwave phase shifter
US5610562A (en) * 1992-11-12 1997-03-11 Ant Nachrichtentechnik Gmbh Waveguide absorber
EP2720312A1 (en) * 2012-10-12 2014-04-16 Honeywell International Inc. Systems and methods for injection molded phase shifter
US8988304B2 (en) 2012-10-12 2015-03-24 Honeywell International Inc. Systems and methods for injection molded phase shifter

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