US2981903A - Gyromagnetic wave transmission devices - Google Patents

Description

April 25, 1961 LE GRAND G. VAN UITERT- 2,981,903 GYROMAGNETIC WAVE TRANSMISSION DEVICES Original Filed Feb. 26, 1954 Q 5 o o L g 20 g m u k d d 6 9 x E Q: E O \l I I 7 o. 02 0. 04 o. 06 0.0a

PARTS Mn /N M m Fe Mn q INVENTO/P L. G. VAN U/TERT A TTORNEV GYROMAGNETIC WAVE TRANSMISSION DEVICES Le Grand G. Van Uitert, Morris Township, Morris County, NJ., assignor to 'Bell Telephone Laboratories, lrfrcorporated, New York, N.Y., a corporation of New ork i Application Aug. 17, 1956, Ser. No. 604,740, which is a continuation of application Ser. No. 412,962, Feb. 26, '1954. Divided and this application Nov. 19, 1957,

. Ser.'No. 697,445

2 Claims. (Cl. 333-24 7 i .os-oa loi-a i-z t in which general formula the maximum amount of manganese present is 10 atomic percent of the amount of iron.

This application is a division of application Serial No. 604,740, filed August 17, 1956 which is, in turn, a continuation of application Serial No. 412,962, filed February 26, 1954, now abandoned and all claims herein contained are based on the description in the latter application.

Since the discovery of the Faraday effect in ferrites at microwave frequencies and the development of the microwave gyrator and associated circuit elements utilizing ferrites, an extensive search has been made for ferrites which are essentially transparent tomicrowave radiation when they are subjected to a magnetic field which is sufficient to take them near to magneticsaturation. In the early stages of this work, several materials showing high Faraday rotation and low loss-for frequencies upwards of 7,000 megacycles were found. However, up to the time of my invention claimed in the said application Serial No. 412,962, no ferrites satisfying these conditions in the frequency range from about 3,000to 7,000 megacycles had been found so that circuits designed for use in this, one of the earliest microwave carrier bands to be allotted for commercial use, had included no ferrite elements.

I have discovered a new series of ferrite materials which show very desirable properties for use in ferrite elements intended for use in this lower microwave region. These materials are magnesium ferrites modified by the substitution of aluminum for part of the iron and in which conductivity losses are further suppressed by the addition of manganese, and in some compositions, additionally, by employing less than stoichiometric amounts of iron so as to produce iron deficient ferrites. This specification contains a complete description of these new materials together with a disclosure of the critical processing conditions which must be adhered to if materials having the properties described are tobe produced. The materials described are of special interest for use in microwave gyrators, polarization circulators and other circuit elements depending for their operation on Faraday rotation at microwave frequencies of from 3,000 megacycles up to 7,000 megacycles, and in other types of apparatus designed for bringing about phase shifting and field shifting such, for example, as the transverse field phase shifter.

The described materials may also find use, for example, in

traveling wave tubes and resonant cavities. A good description of the microwavegyrator, which may be an element in a wave guide, and of some other elements dependent for their operation upon Faraday rotation is to be found in an article by C. L. Hogan in the Bell System 2,981,903 Patented Apr. 25, 1 961.

2 a I Technical Journal, volume 3 1, at page 1 et seq. A more general description of Faraday effect at microwave frequencies by the same author appears in Reviews of Modern Physics, volume 25, pages 253 to 263.

The general formula of the compositions described and included in the devices claimed herein is:

in which general formula the maximum amount of manganese present is 10 atomic percent of the amount of iron.

As an aid in teaching the described invention, two figures are presented as follows:

Fig. 1 is a perspective view of a wave guide containing a ferrite element which may function as a gyrator and is taken from the figure appearing on' page 18 of the Bell System Technical Journal article to which reference is made above; and a Fig. 2 is a plotted curve based on experimental results' designed to indicate the variation in the resistivity of the final ferrite'material with a variation in the amount of manganese used in composition included in the general formula set forth above.

Referring again to Fig. 1 there is depicted a Faraday rotation device comprising a ferrite element 1 composed of any of the materials considered later herein placed in a circular wave guide 2 which is about 12 inches long. Two rectangular wave guides 3 and 4 are com nected with circular wave guide 2 as shown. That portion of circular wave guide 2 containing ferrite element 1' which element is butted to tapered portions 5 and 6 which may consist of a dielectric material such as poly styrene is encompassed by structure 7 comprising electrical winding 8 and cooling coil 9. Electrical winding 8' is energized by an electrical source not shown to produce a horizontal magnetic field in the region of ferrite mag-'f netic element 1, the said field being sufiicient to takeele ment 1 near to magnetic saturation. Radial veins 10 and 11 are inserted for the purpose of absorbing reflections. For the device shown vein 10 is so placed as to absorb horizontally polarized waves while radial vein 11 is so positioned to absorb vertically polarized waves. Tapered transitions 5 and '6 are intended to reduce reflections so absorbed.

"A complete description of the mode of operation of wave guide apparatus such as that depicted in Fig. 1 is beyond the scope of this description. The principle of, operation of such an element may be obtained from the Bell System Technical Journal article to which referenceis made above. i

. f Referring again to Fig. 2, curve 20, on coordinates of logarithm of-D.C. resistivity in ohm-centimetersorr on the? ordinate, which composition falls within the general formula above, indicates the eifectofa variation in. the amount of manganese in an otherwise fixed composia tion on the resistivity of the ferrite. The curve so shown 1 is based on actual experimental observations on materials which were produced in accordance with the procedure outlined in Example 2 herein. Q

The data plotted on this curve is repres'entative'of resistivity characteristics for six compositions in accord-, ance with the formulation set forth on the figure'and containing manganese in the following amounts:

0.02, 0.04 and 0.06 parts of manganese. Current passing r 2,981,803 ll through these samples was, however, too low to be susceptible to accurate measurement on the instrument used. This portion of the curve is considered to be extremely conservative in that from the known accuracy of the instrument the actual resistivity values for these three materials are. well above the values represented by this portion of the curve.

In making up the samples for the resistivity data plotted on. .Fig. 2, the procedures outlined in Example 2 were followed. After the samples were fired, they were in the form of discs of a diameter of approximately one inch. The discs were then machined flat on both circular surfaces to a thickness of 50 mils. One flat area contact covering the entire circular area of the disc was made to each of the two circular areas, a DC. voltage potential of 18 volts was applied across the two area contacts, the current passing through the disc was measured, and the resistivity was calculated.

, The efficiency of a ferrite element for use in microwave apparatus such, for example, as the wave guide structure of Fig. l is generally measured in terms of insertion loss, which is simply the loss in power resulting from the insertion of such an element in such a wave guide structure. Such insertion loss varies inversely with the resistivity of the ferrite so that from Fig. 2 it is seen that adding manganese to the magnesium aluminum ferrite results in decreasing the insertion loss. Although changing the ferrite composition by varying the amount of manganese may result in small changes in the characteristics of the end product other than resistivity, such changes over the composition range indicated are minor and of no consequence when compared with the magnitude of change in the resistivity value indicated.

Providing therefore that the firing conditions and other conditions of treatment of the materials over the range indicated are identical, and provided the conditions of application of the elements constructed of these materials are identical, it is seen that a reduction in insertion loss necessarily results upon the addition of manganese to a magnesium aluminum ferrite.

'A general index of the quality of a ferrite for microwave applications depending upon Faraday rotation is the magnitude of the rotation of the plane of polarization per unit absorption of energy from the transmitted wave. Typical values of this index for the best commercially available ferrites are 400 to 500 degrees rotation per decibel (db) of energy lost in a wave guide at 9,000 megacycles and, until the development described herein, about to 20 degrees per db at 4,000 megacycles. Prior to my work it was thought that the way to increase this index in the microwave frequency range of about 4,000 megacycles was to develop materials having higher intrinsic magnetic saturation moments so that the Faraday rotation per unit volume of ferrite would be increased. My studies, however, have indicated that extension of this principle to the development of materials for use in this frequency range is not justified since an increase in the magnetic moment of such materials results in a corresponding proportionally greater increase in loss so that the resultant index as herein defined is actually lower. In fact, a study of the loss mechanisms at the microwave frequencies hereunder studied has led to the conclusion that the solution to the problem is the production of a ferrite with a much lower intrinsic saturation moment than that of most commercially available ferrites combined, however, with low dielectric loss. These studies have led to the materials herein described which, to date, have given measured figures of merit of greater than 500 degrees per db at 4,000 megacycles.

The next section of this specification is an outline of the procedural steps which are to be followed in carrying out the teachings of this invention. Following this section and accompanying discussion relating to the effect of varying certain conditions of treatment on the final.

characteristics of the material, there are set forth two 4 numbered examples of procedural steps which were followed in preparing several materials falling within the scope of the general formula set forth above.

Outline of manufacturing procedure in which general formula the maximum amount of manganese present is 10 atomic percent of the amount of iron. In setting forth a procedure designed toward obtaining a desired composition within this general formula, compounds which are in themselves, or which will upon calcining yield, oxides of the metallic elements to be contained in the final composition are selected.

The amounts of each of the components are determined in accordance with the composition which is desired. Suitable starting materials include the oxides of all of the elements with the single exception of aluminum oxide,

the desirable properties attributed to the ferrites of this invention being obtainable only by the use of aluminum hydroxide or by the use of compounds which by in situ reaction may be caused to result in aluminum hydroxide. An example of such an in situ reaction is the use of aluminum chloride which in the presence of the basic magnesium mixture results in the formation of aluminum hydroxide.

In connection with the form in which the aluminum addition is made, it is to be expected that the use of the hydroxide will result in a very fine dispersion of aluminum oxide. Since, however, experiments have established that the use of even the finest grade of aluminum oxide obtainable does not result in ferrite materials having the desirable microwave characteristics herein described, the advantage of the hydroxide over the oxide is clearly not entirely attributable to a finer particle size of aluminum being realized by its use.

Magnesium is added in the form of magnesium carbonate or other compoundwhich upon oxidation during calcining results in magnesium oxide a preference existing for the carbonate. Manganese is also added in the form of the carbonate or other material which will yield the oxide upon calcining.

The following tables indicate the amounts of star-ting materials to be used in obtaining the ferrite materials of this invention. Both weight and molar proportions of starting materials are indicated. Table I indicates proportions of suitable starting materials. The proportions of Table II are in terms of oxides.

TABLE I Material Mols The starting materials are mixed in a paste mixer. This I in certain instances to use a non-aqueous solution, such,

for example, as acetone, carbon tetrachloride, or ethanol.

Where a combustible solution is used, mixing is preferfrom about800" C. to about 1200 assume ablycarried out in a ballmill or other enclosed equipinentin'which the fire hazard is minimized- Although the mixing step can be carried out dry, the result will be a cake rather than anintim'ate mixture of powders.

"The mixture is then dried either by filtering if'a water slurry-is used or by evaporation if a non-aqueous solvent is used. Although it is not necessary to remove all of the'liquid from the mixture, if an irritating solvent such as carbon tetrachloride is used it is preferable to dry the mixture completely to protect the operator. The evaporation step may be carried out in air.

The mixture-isthen calcined for about 12 hours in air at a temperature of from 200 C. to'400 'C. below the final firingltemperature. Since, as will be discussed, for most, operationsfirial firing is carried outat from 12,00 C.,to ,1400' C., calcining may generally be carried out at C F a Y The mixture is now broken up in aball mill for a period of about 15 hours in a liquid such as carbon tetrachloride,

ethanol, acetone or water. Some time during this grinding process, either at the start or any time later, a binder suchfas Halowax (chlorinated naphthalene), opal 'wax, or paraffin is added. This binder, which is either dissolved bythe carbon tetrachloride or other grinding medium during the milling step or is added in the form of a solution in a volatile. solvent, acts as a lubricant during the pressing procedure. g

The carbon tetrachloride or other non-aqueous solvent is removed by heating while providing for removal of thevaporous solvent. I Stirring duringthis solvent removal step, for example at from three to four revolutions per second, assures-uniform dispersion. r

The resultant waxy mixture is passed through a screen in order to obtain uniform granules. A 20-mesh screen has been found to be satisfactory for this purpose.

The particles are now put in a vacuum oven so as to remove the last traces of solvent. 7 The oven is maintained at a temperature of from 40 C. to 50 C. or higher, the temperature however being kept below the volatilization point of the wax. Operation of the oven for a period of from 4 to 12 hours is sufiicie'nt to remove virtually all the solvent. Although this solvent removal step can be carried out in any ordinary oven, there must be provision made for the removal of the solvent.

' The mixture is next pressed at a pressure of from 30,000 pounds per square inch to 60,000 pounds per square inch, depending on the desired results. The lower the pressure themore'inhomogeneous the resultant material and, consequently, the less sharp the ferromagnetic resonant'peak. For the general purposes outlined in this diselosur a pressure of 50,000 pounds per square inch has been found to be suitable. The shape into which the materialis pressed is not critical and depends only on the shape desired, the usu ail' barlab, disc or ring forms being used. "Pressingmay be carried' put at room temperature.

i The wax having served its fun '1}; as a lubricant during the pressing process, the pressed pieces are dewaxed in ad oven according to a temperature-time program. If a schedule similar-to the one set forth below is followed homogeneous material results:

Time, hours i Temp erature,

:nwwwuam Since the boilingpoint of thewaxes used in the range of 75 C., most of the wax comes out during the 100 C.

I heatingst ep. Heating to succeeding higher temperatures results in the removal of that portion of the wax that polymerizes as the heating is carried out. Although other heating schedules will work satisfactorily,-there are certain conditions which must be adhered to if most of the wax is to be removed without damage to the pressed bar. For example, bring-ing the body up to -a temperature veny much in excess of the boiling point of the wax quickly will tendto cause cracking and may produce holes in the pressed body.

Heating the body to temperatures in excess of about 500 C. results in the crystallization of a large amount of the material so that the final product after firing will be inhomogeneous and less dense. In connection with the dewaxing step, it is understood that the desired prodnet is homogeneous and has a narrow resonance peak, such material being particularly useful in the microwave range of from 3,000 to 7,000 megacycles. Since, for operation above this range a higher rotation per db may be realized with less dense material, there may be a slight advantage gained by carrying the dewaxing schedule to higher temperatures. I

Final firing is carried out in any conventional furnace which can be heated to the range of from 1300 C. to 1400 C. as for example, in aGlobar, platinum, or gas type furnace. Final firing is carried out in an atmosphere of air or oxygen. For microwave applications not dependent on broad resonance peaks, for example, such as Faraday rotation applications in the 3,000-megacycle to 7,000-megacycle 'band, it is desirable to raise the.tem-: perature of the mix to its ultimate value of at least about 1200 C. and preferably 1300 C. or higher as quickly as possible. 'Such a procedure produces materials having much higher densities than materials brought to the ultimate temperature slowly. Materials so produced may have densities of from 2 to 4 /2 grams per cubic cen-, timeter. TheIdensity of the end product may be further increased by the introduction of water prior to or during the final firing procedure. Although water vapor maybe introduced during firing, it may have a deleterious effect on the heating element of the furnace if an electrical element is used. It is therefore usually found preferable to prehumidify the dewaxed bodies, or to ball mill in water after calcining. a As has been indicated, characteristics of the final product depend on composition and processing conditions. In general, highly'homogeneous materials are to be pre ferred for application in the 3,000-megacycle to 7,000- megacycle band. Homogeneity, in general, increases with density, which may be increased by increasing moisture content during firing, increasing firing temperature and the rate of approach to the firing temperature, and by increasing the iron deficiency. Manganese addition probably has a mineralizing action similar to that of water so that the density of the final material will probably show a slight increase with increasing manganese addition. Since for frequencies above 7,000 megacycles less dense materials are generally preferred, it may be to advantage to utilize lower firing temperatures, to approach these firing temperatures more slowly and to introduce no water prior to or during final firing.

In compositions included in the general formula above, it is important to have an iron deficiency to suppress the formation of divalent metal ions which have the efiect of increasing the conductivty and, therefore, of increasing the eddy current loss of the material. In general, iron deficiencies of from 5 percent to 10 percent have been found to greatly improve the loss characteristics of the final material, although iron deficiencies of as little as 1 percent or less have an ascertainable eifect. Where it is desired to obtain or where there is no objection to producing a heterogeneous material, conductivity loss may be further decreased by increasing the iron deficiency to values as great as 66 percent although, in general, little advantage is gained by going above 25 percent. For the purpose of this description, iron deficiency is given in terms of the amount of metal ion which will have to be added to ionically balance four oxygen atoms, or for the general formula above percent iron deficiency= As has been discussed, in general, although increasing the magnetic saturation moment of the ferrite has the effect of increasing the Faraday rotation for operation in the frequency range of from 3,000 megacycles to 7,000 megacycles, the losses are increased out of proportion to the improvement in Faraday rotation so that the resultant figure of merit is actually less. Reducing the saturation moment of the ferrite has the effect of increasing the figure of merit so that the number of degrees of Faraday rotation per db loss is increased. It should be noted that the critical saturation moment is that of the individual crystallites themselves, the losses not being reduced by virtue of air gap or other dilution elfect which give an apparent lower saturation moment. For. use in the frequency spectrum from 3,000 megacycles up to 7,000 or 8,000 megacycles, the material should have an intrinsic saturation, that is saturation moment of the individual crystallites, of the order of 1,800 gausses or less depending on the exact frequency in which it isintended to use the materials. Since at 4,000 megacycles the initial loss peak is still present in a material having an intrinsic saturation of about 1,800 gausses, ideally, for operation at this frequency, the ferrite should have a saturation moment of less than 1,800 gausses, By use of the processes herein described, ferrites having intrinsic saturation moments of 800 gausses and lower have been produced.

As the frequency of operation goes up it is permissible and generally preferable to use materials having higher saturation moments since at higher frequencies the contributions to loss from the initial loss peak for a given ferrite rod decrease and may be eliminated. Also the higher the saturation of the material the smaller the rod that may be used. However, up to 7,000 or 8,000 megacycles, the number of degrees of Faraday rotation per db loss may still be increased by adding aluminum to lower the saturation. For such uses ferrites produced in accordance with this disclosure in which insertion losses have been minimized by the introduction of small amounts of manganese and iron deficiency are useful.

Ferrites containing .1 atom of aluminum and having intrinsic saturation moments of the order of 1800 gausses show excellent properties in this higher range of frequencies. Above 8,000 megacycles where it is desirable to use materials having still higher saturation moments, the addition of aluminum is disadvantageous.

It should be especially noted that all of the desirable properties attributed to magnesium-manganese-aluminum ferrites produced in accordance with this invention are obtained only by the use of aluminum in the form of the hydroxide. Similar effects may be achieved by creating forms of hydrated alumina by in situ reactions such as by adding aluminum chloride to the basic magnesium mix. The uniform intrinsic low saturation moment materials herein described will not be obtained if the aluminum addition is made in the form of the oxide.

' The following examples are descriptions of the steps followed in producing several compositions within the range of the general formula. In Example 1 the final composition is Mg Al Mn Fe O Example 2 relates to the production of the six compositions on which resistivity measurements were made and plotted to produce the curve of Fig. 2. All but sample A of these six compositions is within the scope of the general formula. Example A, which contains no manganese was produced for the purpose of obtaining a reference point.

EXAMPLE 1 i A mixture of 656 grams of magnesium carbonate, 96.6 grams of aluminum hydroxide, 985 grams of ferric oxide and 85.0 grams of manganese carbonate was prepared by water mixing in a paste mixer. Following this, the slurry was filtered and dried overnight in an oven maintained at a temperature of 110 C. The filter cake was granulated and calcined in air at 900 C. for 15 hours after which the calcined material was ball-milled for 15 hours in carbon tetrachloride during which milling procedure 200 grams of Halowax were added. The material was taken to incipient dryness by stirring in a pastemixer equipped with a heating mantle and an air-blowing ring to evaporate the carbon tetrachloride. The powder was granulated by passage through a 20-mesh screen and was dried in a vacuum oven maintained at 45 C. overnight. The final powder was pressed at 30,000 pounds per square inch into two bar-shaped bodies of dimensions A" x A" x 3 /2". The bars were next dewaxed by placing in a tray covered with asbestos paper ina furnace which was maintained at C. for 6 hours, 150 C. for 3 hours, 200 C. for 3 hours, 250 C. for 3 hours, 300 C. for 3 hours and finally 400 C. for 6 hours. The dewaxed bars were then fired in a Globar-type furnace at 1365 C. in dry air for 10 hours. One of the bars was machined to a cylinder having a diameter of 0.430 inch and a length of 3 inches. When placed in a round 2-inch wave guide section the end product showed a Faraday rotation of 52 degrees for a measured insertion loss of considerably less than 0.1 db at 4,000 megacycles which is equivalent to a figure of merit of greater than 500 degrees per db. This ferrite of composition had a calculated density of 3.8, an iron deficiency of @IMLZLUHJO: 7.5 percent and an intrinsic saturation moment of 1600 gausses.

EXAMPLE 2 A mixture of 843 grams of magnesium carbonate (MgCO 156 grams of aluminum hydroxide (Al(OH)3) 1360 grams of ferric oxide (Fe o and an amount of manganese carbonate(MnCO set forth below was prepared by water mixing in a paste mixer. Following this, the slurry was filtered and dried overnight in an oven maintained at a temperature of C. The filter'cake night. The final powder was pressed at 30,000 pounds per square inch into a disc having a diameter of 1 inch and a thickness of approximately 50 mils. The disc was next dewaxed by placing in a furnace, the temperature of which was gradually raised to 400 C. in a period of 8 hours and was held at this temperature for a period of 4 hours after which the furnace was turned ed and allowed to cool to room temperature. Air was blown through the furnace during the entire heating and cooling cycle. furnace at 1350 C. for 10 hours. During firing. an oxygen fiow was maintained through the furnace. The furnace was then turned ofi and allowed to cool to room temperature, room temperature being attained in about The dewaxed disc was then fired in a Globantypeof the six samples and the resultant compositions of the final products were as follows:

Sample Grams Composition What is claimed is:

1. In a device in whichelectromagnetic waves transmitted therethrough are modified by' the gyromagnetic action of a ferrite body, a ferrite body of the general formula I LOE- OB QQI-1 1-2 4 in which general formula the maximum amount of manganese present is 10 atomic percent of the amount of 0 iron.

2. In a device comprising awave guide for transmitting electromagnetic waves and a ferrite body for modifying lay 'gyromagnetic action electromagnetic waves 10 V transmitted therethrough, a ferrite body of the general formula in which general formula the maximum amount of manganese present is 10 atomic percent of the amount of iron.

References Cited in the file of this patent UNITED STATES PATENTS OTHER REFERENCES Snoek: Physica HI, June 1936, pp. 481-483.,

.Jones et aL: Proceedings Physical Soc. of London, February 1952, pp. 390-391. g

Kordes et al.: Chemical Abstracts, vol. 46, col. 4411, May'25, 1952;

Claims (1)

1. IN A DEVICE IN WHICH ELECTROMAGNETIC WAVES TRANSMITTED THERETHROUGH ARE MODIFIED BY THE GYROMAGNETIC ACTION OF A FERRITE BODY, A FERRITE BODY OF THE GENERAL FORMULA

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