SCIENTIFIC ABSTRACT M.I. CHECHELNITSKIY -

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December 31, 1967
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SCIENTIFIC ABSTRACT
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DUBITSKIY, L.G.; GRITSEVICH, G.V., inzh., retsenzent; CRECHELINITSKlY. M.I., inzb.p retsenzent; KOLETINAp A.V.# insh., re GORDEYEVAp L.P.9 tekbn. red. [Radio methods of production control] Radiotekhnicheakie Metody kontrolia izdelii. Iad.2., perer. i dop. Moskva, Mashgiz# 1963. 350 p. (MIRA 17:3) CHECHELINITSKIY) 0. (Checholinyte.2kyis Oolp inzhe The sea produces current. Nauka i zhyttia U no.12,.22-24 D 16:L, (MIM15:2) (Tidal power) s/114/60/000/007/007/009 Z194/E455 AUTHOR: Chechellnitskiy, Ya_I_ TITLE: Improvements In Turbine Blade Manufacture at the Leningrad Kirov Works PERIODICAL: Znergomashinostroyeniye, 196o, No-7, PP-31-34 TEXT: Steam turbine blades manufactured in the Leningrad Kirov Works are grouped into three classes according to difficulty of manufacture. The first group includes those easiest to make; they are those of constant section and are usually cold-rolled. The second class includes wholly or partially milled blades, with thickened-root and constant blad1e profile in the working section. The manufacture of these blades calls for a great deal of machining and special fixtures, cutters and gauges. The third group, the most difficult to manufacture, includes fu.Ily-machined blades with complicated roots, such as skew-milled: and screw blades, whose profiles vary over the working length. Manufacture of these blades requires a great deal of machining~, agaim with special and complicated accessories. From the standpoint of Improving manufacturing procedure the third class of blades is the most Interesting, an it requires the most labour. Card 1/4 s/114/60/000/007/007/009 z194/z455 Improvements in Turbine Blade Manufacture at the Lenl!ngrad Kirov Works The working part of these blades to formed by profiles of curvo- linear surfaces of variable cross-section over the entire length of the blade and there is no plane of symmetry. The cross- aections of the working parts of the blades are at an angle to the radial surfaces of the root. The blade contour is such that they must be machined with reference to certain predetermined reference surfaces and lines. The most accurate reference surf ce-/ would be the plane of the axial direction of the steam inlet edg:' and the Inner profile of the working part of the blade. However, from the manufacturing point of view, it is preferable to make the reference surfaces not the inner profile of the working part of the blade but the plane of the root fromthe side of the external proft-le. When this method in used the tolerances between operations becomes very close-aind it is necessary to introduce an additional reference basis, such as the skew faces of the working parts of the blades. Blade mantifacture is made more difficult and expensive because of the manufacturing Card 2/4 s/ii4/60/000/007/007/009 C194/E455 Improvements in Turbine Blade Manufacture at the Leningrad Kirov Works tolerances between operations with reference to the first edge of the face relative to theFroot. Instability of the reference base when milling the first skew edge made it necessary to refrain from machining two components simultaneously and to machine each part separately. Difficulties arose because the reference base wandbred during machining. This is particularly important in making screw blades. The introduction of an additional manufacturing reference point in the form of a dowel overcame the difficulties and made it possible to use-a constant reference point when milling skew edges of the internal and part of the external surface of the working part of the blade. The method of milling that in &4opted now that the manufacturing reference point Is available is described. It was also possible to simplify the design of the milling fittings. A further important point is to reduce the amount of labour required in manufacturing blades. Analysis of existing methods of machining blades shows that individual machining did not meet the Card' 3/ 4 s/114/60/000/007/007/009 9194/9455 Improvements in Turbine Blade Manufacture at the Leningrad Kirov Works requirements. This is particularly tr-ue of milling work. Objections can be raised to multiple machining of parts to finished dimensions where it in necessary to maintain strict tolerances and good finish. Such objections, however, cannot be raised to preliminary rough milling and there are many such operations in the manufacture of blading. They include the mi-IlIng of the inlet edges of skew and screw blades. for which up to 16 blades may be machined at once on a horizontal milling. machine and 8 on a vertical willing machine. A silmilar situation arises when milling the roots of skew and screw blades. Considerations that arise in multiple machining of parts are discussed and it is argued that simultaneous milling of two similar right and left handed blades in better than milling either separately. Improved methods of machining skew blades gave a mean improvement in labour productivity of 36%, whilst the mean labour-content of the blades was reduced by 24%, the corresponding ftgursa for screw blades being 48 and 32% respectively. There are 5 figures and I table. Card 4/4 YAL-1- TP offialoW of the desIV a stem - turbiiws do"loped'.tw tba- nrew Plknt. Pmergam"Mno-troen" 7 no.9: 32-350 161. (KM 14:9) two turbime) ,CHECHFL M- V~.'I - -- Selecting an economically expedient technologicLl process for machining the parts of marine engines. Sudostroenit- no.S.- 46-50 Ag 165. (~MIRA 18:9) CHECHEIISKA, B. 1'111~bafi*l T.,t15;vchelska B. PvcParatlon on LaborsIory Scale of Ergo- - - *erol fron Dii e eHIMM AsOerfillsu Niger. .10ft%Ymy"ale ergostirolu % grzybnl AsPerg-Mus Niger w skali labo- t*toryJnej".jPcRce GI. Wt.. PrZein. Roln. I Spoi N, S) _Wr=,w,,, 1952. PV~T. 4 v,%. I tab. Ths cdmftnt~ of ergosterol in Azpergillus Niger taken frcin a citric add factory -was determinod. Two prLicipal methods ~.of extraction of WgMt -ml were uEed. - 1) 0Xtrattlon of Eats and sterots and the hydro- Polish Technical Abet* Wis of fats, followed by the Isolation of ergo&terol from ~ the ~ nonhy- NO.. 1' 1954. drolized portion, 2) hYdrolYsis of the whole material with potassium - - Chemistry and C hemical Technology. in hy&at---d alcoho! and the extnetlen of th e unhyd.-OIL~Vd hYdroxide Pclllcn ivith a sulta.Wie solvent The evapDration of the scivent left the residue of ergcsterol. In order to find the most convenient p3rameters. a Aumbdr Of experiments, in MOdIfIcation of both methods w~are =rIed out: the quantity of potassium hydroxide. the time of hydrolysis and, extraction, the kind and the quality of solvent. The most suitable me- 910d vas found, to.W* hydrolising the fungus with KOH In hydrated 39COW, ILSIV9 30*10 Of KOH - talculated ort the basis of the dry* fungus MIXInt with Witter, -filtering the precipitate and extracting the zolu- tim three tlrnes-wlth`~ benzene. Then the fungus was extracted three tUM with alcoh4land the solution was Mtered hot. The precipitate, ft. n benzene-d alcoholic extract was xeCrYSW [zed -several U.-nes', frm the rabvhir~ -of alcohol a-ad benme (4 : 1) or dichloroathane. Dif- terMt fdndd-Qf4" y1eldeo VaAaW quantibles of argosterol;.1j.Ls pas- ANO AhW "-.-?-ykld domds on the conditbw of fermentation (medi U.M. AMkitioul.and,eUthe age of fungL The content of the crude ergosterol After varification, it decreased to As WWM-%W0-.'-,-_Zuhod on 11"MtOVY scale Le. with small quanWW i at. *M, ibe -Scion waii vskovoly #mL [77 chvmlstry of pyri'dino. IV. Peacdolls of unideA 61 Hal is filt(ltd A-, Od l"Nill. N.,11cot I'Pts. 1.0 g. II, AIRO likofinic. and Isonic-olinle acids wjUrftfurrme. prtpd.-. R trrraft!. in. 224-0'. and IIHC ,1, m. 267~-V. hydo and rinines. Roz-nnit Chtchelska sold TagLU. in the saint: inanner, RINItCH1011 (M), M. 2 in, 202-4*), and (W.10INCal (IV), Ch ~j tall, 27, R'NIICII..YAfe,jICI (V) in. 1~ this abstr. l1re obtained. ni-w P., PIC011110YI, -aid R, IiallictitiIII)yl.) prel"I. (MI,' with .2.1 r. Mc,1,111- q) by millivIng.4 r.. W. )i arid HCI and2. K.37 C11, in 10 nit. nollyd. EtOlf ford hh~; -amide (24A g. Ill 90 ml. 1-1101-1,21 g. KC0,, 7k V m 100-2 . Ill (1.7 g.) tind 1 ~7 g. 2-11 ,ht~ol F, 37~-, CIIOare heated on a ILOWth for I hr., tirrald crote'la.140-22, telluxed in 20 mi. EtOH, r 116, qr axe also prcpd. hr., the EtOff is distd., and the residue a1lowed to ttwld a- LFC1, -n. abrive 120' (decompli i 2f P,"IF 1` 2-14-0', is made by siowly adding 2.4 for several months, giN-ing the 2- CoRO CH, IVHP 1, ra, 17C-7 V. ~J Jh,,11cid auiid~ to 11.5 ill]. 85% HiSO, ind 1.9 g. 37% 7.5*. By the mttliods descrititd, R*NHCH.-OH (VI), ln.', C;f f) , 145-7% (R'.IVHhClfl (VM), in. 32IR-8* VI m-! i~t 20-10*. warnied at 40' for I hr., andholding at np. for 1,%g. product ppts.-.aIrttr treats-- -8* (decompli.)i VII picnak, in. 2 7', VJXHCR,-~ ?,il*,' :q1:CQs, Simffn;-ly 1.5 j. I treated with _11 ISOO jVAfj!j.HCl (VITI), m. ane YM piacte, in. JSS-,LI.' 0.1*.S g. of 11. Nicotinic acid nitifle (3.5 S.). art prep4. V and VIJI sbow a -At,%t bnctfAmWk action 21. 1 g ~ ,.7 1;/0 C I f)t) a ii El 2 5 in Oro agminst Afyc,.!,ar*riutr. swrpnais wid M"yeo-hac. ml. 8517,, ll-SC)i 11CM(d at 330' fw, 2 lirs.j poured into ice' Whim 2-19, C,!t~Lt~~ Practk r. vnrl XavCO, added it) syl 111. the pl3fd. starling rwifN ~V- URBAMIO Tadouss: NALIWAKI, StanislAw-, SMOMA4MWIjFOVl, marwam; VocallAxi Bosennal DAMOVSKA, HoUna; FALICIrl, Jerzy; GtM, j , szek; SZOW, storan.- UKUMKA. Iron&: VINULTM, Jan; JAKDfMKA. Krystyna; URBAN=. Alloje, Search for now antitubormlous agents. Gruslica 22 no,10:681-6" oct, 54. 1. Z Oddslalu 8yatesy Lokov lust7tUft Gruslicy; klormmik prof, dre T.Urtmmokts dywaktor: proro d%,Jjnslovlcs. (CHMMMAPY, In varl d1seasom tlAorowl prov.) (rmwmmis, therew antitubera. sionto, research) CHECHELSK~, Bozenna Bozenna. Chechelska: "On Reactions of Amides of Nitrobenzoig Acids with Formaldehyde and Amines.,11 Roczniki Che:aii, Vol 30, No 1. Warsaw, 1956. Published from the Chair of Organic Technology., II, Warsaw Polytechnic, and the Tuberculosis Institute, Warsaw, 28 Mar 55 - IMBANSK, Tadouas; BBI&INKI. Czeslaw. C Bozena; CHYLDISXk, Barbara; MLSWWSXI, Halina; PAIMKI, 1~,; HAISKI, leezek; -;a; ZYIDWSKI, Jerzy; SIOPM NkLINOVSKI, Stanislaw; MAMMA, ;;;w Stefan; NAMMSEk, Irena; V3UUIW. Jan; JANXIM. Xieczyslaw; JAKD(OWSEA, Hrystyna; URBAW)KA, Alicja; EMMIGOV, Anatol Searching for now anti-tuberculosis drugs. Qmzlica 26 no.11:889-917 XOT 58. 1, 1 Zakladm Syntesy rAkm Instytutu Gruslicy Kierownik Zakladu: prof. dr T. Urbauski . Vyrektor . Instytutu*. prof. dr J. Kis iewicz Pracownia Synt. Lekow Przectwgrmlicych. Warszawa. ul. KDszykowa 75. (TMIROMMU, therapy, imentigation of 300 cpda. for anti-tubere. eff. (Pol)) XMIRBOVp A9I9, lush,; ICI_ pja,,Z,, insh. Nwh1me for manipulating large-size places. Izdbr. v 3312 3 no.Z-.16 P 158. (MIRA 11:3) (Nachine-shop practice) AnNA31YET, 0.0. [Afenasliev 0.0 .1; OCRTITS, S.M. [Horvits, S.K.1; IGRATOVA, L.P. [Itma;ovaf L.P.]; KOTOTO K.P.; NOVIK, o0B. [Novyk, H.B.); OF= I.T-INTSAX Lj~.; ROZINKAN, G.S. (Rozenman, B.S.]; ii;TMRNOY, V.A.; TSITRIN, L.I.; CHECKIWO H.I. [Choc6niev. K9-1.1; WOOTAX, S.I.; HAZARRNKO, -N-o*. GOILATEMKO, L..[Horksjenko, Lj, takhn.red. ELight industry ofthe Ukraine] Lehis pronyaloviat' Ukrainy. Kylv. DsrzkTyd_vo-tskhn.lit-ry URSR. 1160. 117 PjKIRA 14:4) (Ukraine--Industries) CHECHINEV, M. 1. CHECHENEV, N. 1. -- "CHArjar or THE PROPEPTIC5 Or THE SURFACE or FRO-,T GELATIN AFTEP TANN I IIG. "SUE) I JUL 52, 14oscow TccllNOLOQICAL Wy or Licia INDt)5TPY mcul L. P. KAOANOVIcif (Dl:,:SE0TATION FOn T"C DCORCE OF CANOIDATC in Tw4NICAL Scirricr) 3(): VECHERNAYA 1403KVA, JANUARY-DECEMBER iQ52 smuRANm, I.T., kand.tekhn.nauk; KMV. M.P., prof.; CHECHEIMY. N-I-i kand,tekhn,nauk- MIKHANOSHA' YO-S-* Inzh. Making high-viscous gelatins of chrome-tanned shaviW. Izv. Tys. uchebe zave; tekh.leg, pros. to.2:40-46 156. (KIRA 11:6) l.Kiyevokly tekhnologichookly Institut legkby proWshlennosti. (Gelatin) WWOMIN A Overcoming the difficulties of the Arctic. Zhil.-tom. khos. 8 no. 8:5-8 158. (KIRA 11:8) 1. Predesdatell Ispolkom lkrwmskogo gorodskogo S*veta depatatov tradyashchikhoya. (Karmansk-Municipal servioes) CHECHaTIN, M. G., Cand Med Sci -- (diss) "Healing of skin-muscle wounds of the tibia and reactivity changes in the sciatic nerve after application on a limb of torniquet stanching of blood-flow." Rostov-. na-Don, 1960 15 pp;.(Ministry of Public Health RSFSR, Rostov-na-Don. State Medicai Inst); 300 copies; price not given; (KL, 17-60, 173) ~I-E6 "Is m RUSAKOV, V. I., kand. - ind. -naukt CYWMIN, M. G. Rare form of anoma2y causing aspbyzia in a.--nevborn infant. Akush. i gin. no.2:97-98 162. (MIRA 15:6) 1. Is kliniki fakul't*txk*yA&lrurjii (sav. - prof. B. Z. Outnftov) Hostovakogo-na-Danu meditsins)wgo institute, (dir. - prof. P. P. Kovalenko) (AS A) (RESPIRATOHr WAWS-~UNMWIXS AND DEFORUTIES) t 1 Ti f L nd 3) i i ll I d C,11-,,V, do'l sa-~ lnoori,-, 14 CHSCEMNIN, H.Te.. kand. tekhu. nauk Us.Ing asbestos-cement plpes.for p1piplines In Cxechoslovakla, and Hunpry Strol. mat. 5 no.6:39-40 J6 159. (MIRA 12:8) iCzechoolovakia-P%pe, Asbestos-coment) CHECHININ, Ms.. kand.takhn.nauk -Basic requirements concerning quality Indexes of asbestos- cewant p1pes. Strolomt. 5 00-11:13-16 N 159. (KIPA 130) (Pipe. Asbestos-cament-Testing) ,MZCHXITIN. M.Te., kand.tekhn.nauk ftsic properties of asbestos-cement pipes for gas pipelines. Stroi. truboprov.*5 no.3:12-15 Mr 160* Oak 13:9) (Gas, Natural-Pipelines) (Pipe, Asbestos-ce Ment) I CHSCHMIll, M.Te., kand.takhnniLldc =-------- :.- Mking and usW asbestos-cement gas plpe�9 Strolo mate 6 uo97: 7-1o ii ,6o. (KIRA 13:7) (0" pipe@) (Pipe. Asbestos-cement) ALIFERENKOV, A.D., inzh.; CHECHENIN, M.Ye., kand. teklin. nauk ~ t.--- " - ~'' Study of tho deformability of asbestos-cement pipes under repeated loads. Trudy NIIAsbesttsementa no.18:2a-27 164. (MIRA 17:11) LOMANKIN, ~ M.To. Problem of the study of gas flow through the walls of asbestos- oement, pipes. Trudy.XIIAsbeetteesenta no.19s:56-61 165a (MIRA 1.9$q) 0141 Wr ACC NRs AP5027352 SOURCE CODE: UR/0250/65/00/01010659/0663- AUTHOR: Chekalinakayal, YU IT[ Chechenina, YLe. P. PRG: Physics Institute, AN BSSR (Institut fiiiki ANBSSR) TITLE: Amplification of a flux ifian-inhomogeneous layer when fionlineirity istaken, into account SOURCE:. AN BSSR. Doklady, v.:9 no*~10,1965,_659-663 TOPIC TAGS: solid state laser' laser optics, light reflection, light ieflec~- tion coefficient, light t.ransmission,.solid state amplifier ABSTRACT: The properties of an amplifying Inhomogeneous plane-parallel layer with arbitrary reflection coefficients,on the end-fac 8- es were investigated. Harmfullosse in.the active substance were taken into account, and the dependence of the amplifi- cation coefficient on the radiation density'was considered in the calculations. It wasshown that the use of an active layer with the reflection coefficients r1 and r2:' on theend f 8 as an amplifier is limited by the oscillation threshold. The condi-~~ tion X < 1/~_rff! must be fulfilled if the systimis to operate in the amplification 1 2 mode (X is the single pass gain). The tDaximum. possible value for X for extremely small fluxes W - 0) is Xjim - el(ko-pA (k 'is the initial gain of the active sub- stance, p is thelloss.coefficient inside the active layer, and t is the thickness of the Ii~yer). Because of nonlinear.effects, there is a limiting flux So S0 0 is Card 112 z7t?.~/ go_qo 9. L 4962-66 ACC NN AP5027352 "A perpendicularly incildent.flux-on the layer surface) at which X 1. When,So.< S6Aj. the incident flux is,amplified;when So~> So* -it is attenuated, ie. part of the- incident flux is lost inside the layer. The limiting.Value.for flux at.whi& the am-, plification changes into attenuation does not depend on the length of the amplifying, layer. The value of X obtained at very.large incident fluxes (aSo 4 w) is equal to CP'-. In this casethe coefficient oflexternal losses In X/jt is negative and equals, -p, i.e., the incident flux is attenuated.by.losses. To investigate the effect of the layer arameters (ko, pq L. r1, r2),.calculations were performed for.the output p emission, gain, and the yield of useful energy by a volume unit of the amplifying layer at incident radiation smaller that the limiting radiation. Due to.the nonlinear. effects, gaina n and n-r(n = TIT + n and nR are transmission and reflec- R) (where nT tion gains, Tespectivel~)_esse_ntially depend on the-magnitude of the incident flux'So. Even small incident fluxes cause a decrease in n and nT in comparison with the maximum possible gains no and 0, When.S Idecreases, n and nT increase (the-'dloser ko is thresh Ti to ko the greater the increase). At, large light fluxes, i.e., ten to.a. hundred.-. times smaller than the limiting one,-total. gains are:close to unity and are indepen- dent of k0. The dependence of n and nT,on the reflection.c7aefficient r1 of the input end-f ace, of the amplifying layer for rjr2 - constant, shows that 1nT teaches a maximum in the region where rl.is approximately equal to r2- 'qhen r, increases n and np de crease to a value equal totj. Orig. art. has: Al formiilas, 2 figures: and 2 tables. [JAI SUB CODE: Ogte/SUBM DATE:- 07Ju,165/ ORIG REF: 009/., OTH REF: 001/: ATD.PRESS:. Card :7ACC NR, --'-AP7'003'279 SOURCE CODE: UA-/0250/66/010/012/0929/0932 AUTHOR: Chechenina. Ye P.; Katseva., I. R. ORG: Institute of Physics, AN BSSR (Institut fiziki AN BSSR) TITLE: Bmission from a generator-amplifier system SOURCE: AN BSSR. Doklady, v. 10, no. 12, 1966, 929~~932 TOPIC TAGS: laser emission, nolecular amplifier, feedback amplifier, laser optic mat.prial, laser cavity ABSTRACT: Making use of a procedure developed in an earlier paper (DAN BSSR v. 9, 10, 1965). the authors calculate the emission produced by a generator-amplifier Vs- tem with allowance for their mutual influence (i.e., the feedback between the generator and the amplifier)o for different parameters of the active medium and of the resonator. The properties of such a system are compared with those of a system in which*the quantum generator and the quantum amplifier are considered separately, so as to determine the region of parameters in which.the feedback must be taken into account. The calculation is based'on energy relations with allowance for the depend- ence of the gain of the active medium on the radiation density. A computer (Minsk-1) was used for the calculations. The results are presented in the form of plots of the emission flux against the relative reflection coefficients and of the emitted energy on the relative reflection coefficient. The investigation shows that the mutual influence of the generator and the amplifier in such a compound system must Card 1/2 ACC NR: AP7003279 be taken into account if the amplifier length is shorter tbam or equal to the length of the driver generator, or when the amplifying section is long but the reflection I coefficients are close to the threshold values.. This report was presented by Academician AN BSSR B. I. Stepanov. Orig. art. has: 2 figures. SUB CODE: 20 / MM DA72; -IOJun66/ ORIG PJW; 0031 07H MW: OD6 Card 2/2 CHECHELINITSKIY, Ya.l., inzh. Economic basis tor using "cial-equipment.in the iftachini of ng components in turbine manufacture. Ene'rgamashinostroenie 11 no.704-39 Jl 165. 180) .00 I I I & 00 '3 00 a 0043 s0- 00 C1000106Y -of the -tab ad'heAmmor f". Pedam. J. r". WAS.R.) 14, 1741-U(IM).-TU add conga. of the (BUY portions of the river Pereb (Pecs Anwifis) was studied, ematially by broug"jam of 11W Sue"d. adds fradinamim of the brommes, awl detirombut" L;i Weatification of the maim fractims. Click mW tah Primt! the Maim Ifedima at fbe Niel. own W%; t1h more y mantd. A" IOWA VA": ad, MR.%) with 5 double boDde (about V15.1W."Wd &.0 ftm C.1111.0I with 4 double bomb (about 3% Limalmic and hoolemic adds war " found. rob" "mm Interest- tell remit was The ixtalion froof the oft of bromaldes a. 71-53% fir. vh" do itof -, to any knoym unotd. add, ap1mrsuly belonons to,a new yerin of Calf(S. - 001. The tissues were treated in the cold with 93-5% RiOll. followed by tatz. with MOD; the multing ad (50-S. lot) vm saponified by 300 cc. S air. KOH at room temp. for 2 Itts., after which the ZtOH wax thstd.. the *WtA at.. taken up In UO cc. hot H&O and scidified after cooling with IOU cc. 6 N liblvAl, The acids weir estd. witb Et.0. washed with IIA), and dried at If I 'hVI I L I Tdl-r,* at to- Is Mtn. The acid vidat. usi biiiinimiiid to Hif..'~ Rt P %01o. at -to to - 15' aud allowed to Stamat in the tkAd &%%,I dark for wvrnd lim, after wWb It- twomitles, otte filtered all. washett free of Of with CR;l' and treated with W C4114 (295 cc. / 1.). The beftafte- jumA, Imonsidr.. weighed after ittyins. reprmat the octa.- brandde no. of LeIrkmitch. Thebenneftext~amemoling whileevaltu.tave the III ;on. 711c M10 mother liquor. after mmOV11 at ex ce" or. wa_~ e'rapd. and the rr%iduc treated with 70 cc. hot pett. ether to )ivld the IV fr"on of hgormitles: the Pett. ether-ituol. lWart on cry~tu. (rout hot MR gave the V ftect*I=-. SimitaIr treatment of the mother liquo" gave a I , we fmctiom to Vill. The operations Were IV Ord until %tifficient accumulation of fractions wu done rar the ourcreding operatiom. The bromides from frjw- tim I fmn th~ tody, brad. rae. internal orpm of the Perch cormpontit4l to the! d"twomide of clupan"mic " (70-75'.'j. firl; the liver and llie Iwain gave A InInt. what lower fir rotarnt (OKI XV, 0' which cmT-Iftm& to the aM The ittilt. gave the twomile cmiate. 71.W-V fir, AU (A (lie. Macke" ouil do not alai 10 -A Ala - - _k 66 ia-11', 4,1111961W UWAM0110 Imm tl"SIA" ____ IBM 000AW off Z I son*" -4 SNIGNQ NA# dog #01 assail me Ong III -1 0 a 0 '0 "1w A S a ad 0 a a 0 0 0 40 0 0 sees 0 e 0 ~.2' 00000 ;Tea d h eseelessee a to 0 10 001s;901::::::0&oo00sG* sees& fee ZOO me* 900 goo woo 4111116 goo M.N. cof 7 oZ I Coa*~WWM *left fteo 1~__ I VpIA". -The P11-wilve (4 hishiv 111-41.1, 6 1,70k.41 of MN f"1111 fic-A-watef fish. The VINC111 toil% (4,21 cl,".Iv 11,1t.1tv Almotsi the usne io wom VA444A 441111 ('11610V 1111141VIII M It 1114t,11ev PROKCPIYNVA, H.S.; PILYUSHIROK, S.V.; NIKOIAYEVA, R.I.; CHIRCHMOVA M V. 1-1. .11. ! MIKHAYLOVA, A.L.; STMUOVA9 A.V.; IOPUKUP li.ye;-r 9 VOINOV, K.F.9 red.; UMEBA, N.9 takhn. red. [Econaw of Pskov Province; statistical collection) Narodnos kho- siaistwo Pokovskoioblasti; statistlebeekii abornik. Leningrad Goestatisdatp 1960. 175 pe (MIU 14261 1. hke-T (Province) Statiotlohesko!ye upravleniye.2* Robot- niki btatiatiahmakaga. ftkavakoy oblasti (for all. A=apt Kogloy, T6120y, 3. -SaWallmUStatiatimbselen o uprarlemiya Pskovskoy oblasti (for Kozlov). 4. Zamestitell nachall- nika, Statisticheskogo upravleniya Pskovakqr o~lasti (for Voinov) (Pskov Provine"tatisticaj #0 ek) lei '19 It I# 1 0 x I C r. N ,A A ji. I t j Oe A '00 00 -A Bill" a neg. t"t. "t. 6~ns a MI CMl_ pin when 3 drain 2 N Cd(.N(h)I. :., drap,4 lee N's nitn) 00 a j. IdivilIGNOM of P140111 01001ift 64-0 IN OWOM a" 10 1-idt 111142,141134" 1111-11,01w (10' O'Ite W'jh , ,:Is@" " s~ twelbeft. L. M. 09 a I few dro" of tem u4n. aml %hALen: it,,, trt,j call hr aude :;KvI'" Stitt N. 1. lIWjWVW'ftv 111 -A v%.t. Toidentily the I.AtInitillgrat 101"Iell cl 00 in kallare. a few to . of finciv shAved IrAthet is likilel with and their heavy metal Sell fortnallitta MC basis. drop tests 0.3 ad. 1110 1 mL . and the eat. is tnted. The vittd. I-60 0* a ~ i dmtdy a no. of individual tyfles. As a t"Mins give the follarwing COW tests: Oak: I orange pl.t., .'.cm dewrlowd to i .00 00 & rule more than one test isareded few identification. Tivul-. U filk-yellow spal. M deep lilac ", IV no change. V 'Z see fatgin 1% 11150,gi"calond cianplexes with POIYPbtDOll ppeari slowly a ng yellow spot with violet baides. VI dark 1 an a plate (I) at Ital-IT (U -finlyphel"s gisse -Iorvd spot with . eel ish border, VII rapidly applAng lilac. ft. a 00 Muplex" with Mohr a as (60/0 sq. wiln.); The Color red border, Vill hlark-vWlet %IKA, I yrlk~vr SW - Pitte - varift with pit; hence 2 Variants an Us 000 cl~ III arg.. IV sk~ derp.lilac spot. V arit., Go 0 IM (U1) and Its treat t with 10% V1 dark sW with lilac border, VII slowly,apscadocLtv. ago ASCII is reduced by Sam willing (arcrigrated by lig and 00,3 vicift b(irder, vinnel.. IX yellow s Inv Ag seliV; Use vanations ad the leat an: 111011* 4M tW boom not: so"liv a aran law, tit ppt.. W.41 A Zoe 00' i) with Im- AuCjs (V), aftertroated with 2 NHg(NOv)eM),F dmdy tit lilac t' rv Mi-lilac .Ilir, Orblack I r djoe eel iatiff"rated with silet tea with Hg- border,";Mblack ventra'T"'Pot. V11 Mack banter sirmad L are* 0'= (No0s, NIWII. (VM). and AWY the dark Wat, VM yt1low-orange spot, 11 lilac Color in center, The seduction X red-brown sWt. i fast created with Miv AuCh (IX)-. coWlesicenter; m obalan: lorarge Y, drop CA 10-0- if AX.T.O. by write tannins is, also useful: Mt.. U yellow 9W, ill slowly appearing pale lilac Vat. -0, 1. follmsed by the leg Main by NH.OH W- IT brW-pink calm. V blue border, VI large. almost black ej Ag% I hen ~!' %-ilb 11 valmia cit. gives an arance-reif ame oft the spot. VU rapidly appearing black-lilac CoMr. VIU no Zoe 0" fairest. giftmirelkweakv at the inivismied lip d tM P1IPWP chaw. 11 deep-red center. X large, almost black 1611,01; By I oak eat. giv" an OfSAW-yellow &PER 1111111t; P11w 031114 Varbratho., I red ppt.. 11 red ~txn. III brawn-sted v14. hoe calork -a crater. IV no change, V it VI AV-spot critter. VU filw-black border. Vill neg., X G. M, kla'dapff Coe ~v Oft %.not* ---I vXA 0 AV 60 U 7;j Is 19 0 4 0 0 0 q 0 0 * 0 0 : * 0 a a 0 0 0 0 go 600000 0 00 CHECHENTSEV, V.N.; FIRSANOVA, L.A.; FEDORC1111K, O.E. Thermodymnic Investigat-ion of the reqction Si -0 SiCl --->2S'~-12- Izv. vys. ixcheb. zav.; tsvet. met. 8 no.4:97-102 0 165. 4;~-- (MIRA 18-`~) 1. Kafedra proizvodstva chistyldi metallov -4. poluprovodnikovykh materialov Moskovskogo instituta stali 4- splavov. ACC NRt AP5028979 SOURCE CODE: UR/0149/65/000/0-"/0097/6102 AUTHOR: 'Chechentsev., V. N Firsanav% L. A.,; Fedorcbuk, 0. K. ORG: Moscow Institute of Steel and Alloys,- Production of Pure Metals and Semicon- Aucting Haterlais Dept_(Moakovskiy instituL stali i aplavov, Kafedra proizvodstva -i-h-istykh metallov i po uprovodnikovykh materialov TITLX-. -Thermodimamic study of the reaction Si sici z! 2 SiCl 4 2 SOURCE: IVUZ. Tsvetnaya setallurgiyal no. 4, 1965, 97-102. TOPIC TAGS: silicon, chlorine coMmund, equilibrium constant, thermodynamic calculation, chemical kinetics ABSTRACT! In view of discrepancies in the findings of Schaefer and Nickl (Z. anorg, und allgem. Chem., B. 274, 250, 1953) on the equilibrium of the reaction. -S1+S1C'4,2S1C12 669.782, Card J/3 t 13532-66 ACC NR, AP502.8979 and considering that reliable.knowledge of the values rmodynamic functions will facilitate the selection of the optimal conditions fo ~Irefting Si by the transport restigated this equilibrium in the temperature range: reaction method, the authors.in% of 1200-1300*C on employing the~llcurrentll method (Fig. 1) where a current of Sicl is passed (by means of argon) over a Si- .containing boat at a given temperature. Ehra- polation of the obtained values of a (mole fractionof SiCl nvert d t MY to ~zero flow rate of'.SiCl gives the equilibrium position. On thcio basies.thoe temperature um constant C was determined and hence alto the values of dependence of the.equi ibri the isobaric-isothermal potential.,& Z' o? the reaction were calculated: A V varies linearly from +6790 cal/mole SiCl 4 at 1200*C to -1395 cal/mole SiCl 4 at 1300*C. The temperature at which the reaction components, taken in standard states, are in an equilibrium, was found to be 1283*C by graphic means for log C - 0. The kinetics of the formation of SiCl is found to be such that the rate of formation of SiCI in- 2 creases with increasing temperature and, to a lesser extent, with incteasing how rate of Sicl The thermal effect of thereaction is calculated at 127,000 cal/mole for the 124,13006C temperature,range, and hence the reaction is governed by chemical ki- netics, i.e the reaction rate is determined by the rate of chemical interaction. Orig. art. ;as: 5 figures, 2 tables, I formulae SUB 'CODE: 07, l1/ SUEM DATE: lOJul64/ ORIC REP: 001/ O!M REF: .002 Card U/ L 46039-66 '-767 ACC NRs AT0022714 s6uRcE Com- uR/2848/66/boo/ba/b280289 AUTHORS: Chechentsea.V*..14; Firsanova, L. A.; Zayt8ey - -fatylyeriko, Le Fe _1 V. N.; I OWs Nosaw Imstitate for Ited od AUWas ftWtnW fW Xmfaotwe'of Pure "Is Wd Vrolow tra abletIft nstsuev I Wjkh x1sterls"T) TITLE: Obtaining high purity silicon by distillation for the lower chloride SOURMi Moscow, Institut zZI I a Tove Sba m1kv no. 41, 1966. Fixicheaknya khimiya metallurgiaheakikh protsessov I sistem (Physical chemistry of metallurgical processes and systems), 281-289 TOPIC TAGS: silicon, silicon compound,, vacuum distillation ABSTRAGTt The kinetics and thermoctTmdes of the silicon purification by vacuum distilln lon from SiC12 was studied, The standard free energy calculations for a number of reactions of' StC14 with various elements vere carried out by the method of A. N. Krestovnikov i. dr. (Spravochnik po raschatan astallurgicheskikh r'eaktsiyp Metanurgizdat, 1963). The results of the calculations are presented graphically (see Fig,- 1). These calculations shoved the feasibility of obtaining high purity silicon according to the reaction Si + SiCla MCI$. 1/3 AT6022714 Fig, 1, Dependence of the free energy on the too per ature for a mmber of reactions betmeen SiCl and different slownts* 4 I - 4Cu + SiCt. am 4CwC + Si. + a. As + SiC2. we 3 4- 1. Sb + SIC14 SbM + SI: 3 -Sl+3"W& - 4 nx:~ - B.+ SIC3. + 78 :: 24 FA al ++ SSIRM Z 4 &~ C ~ +S IS: L + SICIG + Sk 9w22ftk+ SIC16 +31 The above reaction was studied in vacuum over the temperature interval of 3.150 to 1300C at an average workiM Pressure Of SiCl of 0.2--0.4 atm. A schemtic of 4 the experimutal ingta3lation is presented, and the experinental results are pro- sentedgraphicaUl (see Fig, 2), It was found that the optJz= conditions for the purification of silicon by the above nothod aret reaction temperature - 128M; rate of SiC14 flow - 20 if/hour; duration of process - 3 hours. 2/3 AT6022714 Figs 2* Dependence of the amount of transported silicon on the rate of. supply of SiC14 at 1250CO Orig. art. has: 1 tableg 3 graphs, and I equation. SUB COI)E: 3.11 SUBM DATEs none/ ORIG YdW: 001/ OTH M7z 005 Or, Wri 'o flov rates-SiO g7h VOLOBUYEV, V.I.; FILIPPOV9 I.N.; RYZHWO, D.M.;-CHAL~GHMINjDA.-S SAMURA, I.N.; GfWDSKIY,, le.B., red.; Ai-'D REYEV, tekhn. red. [Work experience of innovators in a vire rod mill] Opyt raboty novatorov provolochnogo stana. Kharlkov. Metal- lurlsdat, 1954. 89 p. (MIFli 16s$) Rolliag idna-Technological innovations) SOV/IZ4-58-2-1759 Translation from- Referativnyy zhurnal, Mekhanika, 1958, Nr 2, p 38 (USSR) AUTHORS: Ruzin, 1. 1. , Faynshtevn, AC-M. , Checherinda, Ye. T. TITLE: Design Calculation of Burners According to the_UKF1N-_(Khar'kov Coal-chemical Scientific Research Institute)method [Raschet gorelok po metodu UKh1N1 PERIODICAL: Soobshch. Gos. soyuzn. in-ta po proyektir, predpriyatiy koksokhim. prom-sti, 1955, Nr 15, pp I and 88-95. ABSTRACT: Bibliographic entry Card 1/1 C C HE 16 /V / Ac/ 0 V1, V" USSR/Physics - Magnetostriction Card 1/1 i:vb. 146-11/a FD- Author : Volkov, D. I. and Chechernikov, V,. I. Title : Temperature dependence of magnetostriction of ferromagnetic alloys periodical : Zhur. eksp. i teor. fiz., 27, 208-214, Aug 1954 Abstract : Study the temperature dependence of magnetostriction of saturated ferromagnetic alloys on nickel basis (Ni-Cu, Ni4la, Ni-Fe). The results of measurements were insatisfactory agreement with theory. Fourteen references including 5 foreign. Institution : Moscow State University Submitted : October 26, 1953 CHEU71EPIUKOV, V. I. CHECHERNINV3, V. I.: "The temperature dependence of paramagnet-Je. sus- /Jo ~,! ~- --cept)-lility of nickel alloys-" Moscow state U imeni I.I. V. Lomono- sov. 'Moscow, 1956 GISSUITATION For the Degree of Candidate in PHYSICOPMHFJ,IRTI " SCILNGE.) So: Knixha5-a letopis', No. 24, 1956 USSR / Magnetism. Ferrmagnetim F - Abs Jour :Ref Zhur - Fizika, No 4, 1957, No 9525 Author :Volkov, D.I., Chechernikov, V.I., Tseytlin, V.B. Inst : Not given Title :Temperature Dependence of 11agnetostriction of Ferromague- tic Alloys. Orig Pub :Vestin. Mosk. un-ta, 1956, No 2, 21-28 Abstract :An experimental study vas made of the temperature dependen- ce of the magaetostriction of saturation)k3of ferromagnetic alloys with a nickel base (Ni-Cu, Ni-Co., Ni-Ma and a Ni-Fe alloy with 45% nickel) in the tmperature region close to- the Curie point. It vas established that in this tempera- ture region the variation of X,$with T is linear in charac- ter, and this is in accordance with the theory of the tem- perature dependence of even Akulov effects. For Ni-Co al- Card 1/3 USSR / Magnetism..Ferromagnetism Abs Jour : Ref Zhur - Fizika, No 4., 1957., No 9525 4 Abstract : loys (2.4 and 6% Co) and the Ni-Fe alloy (45% Ni) this li- near dependence of ~5 on T is observed in a greater range of temperatures than for Bi-Cu and fii-Mn. It is noted that on the h., (T) curves of the Ni-Cu and Ni-Mn alloys (3-7 aid 8.5 atomic percent of manganese), in the direct vicinity of the Curie point (19), there appear clearly pronounced a- symptotic "tails" which vanish at Tk>90. For the case of Ni-Cu alloys, the authors establish the dependence of Tk on the composition of the alloy. 7he authors propose that such "tails" on thehs(T) curves are due to micro-irregulari- ties in the ccmposition and to the appearance of magnetic oil dering at close distance. A study of the temperature depen- dence of X_sfor Ni-Co alloys (29 and 30.5% NO which have an allotropic transformation, has shown that at the transfor- Card 2/3 USSR / Magnetism . Ferrmagnetim F - 4 Abs Jour : Ref Zhur - Fizika, No 4, 1937, No 9525 Abstract -. mation. temperature jumps appear in saturation magnetostric- tion, the ks (T) curves have considerable hysteresis, and the hysteresis loop remains 'unclosed at room temperatures. Card : 3/3 V, x, 137-58-1-1550 Translation from: Referativnyy zhurnal, Metallurgiya, 1958, Nr 1,, p 207 (USSR) AUTHORS: Chechernikov, V. TITLE: Paramagnetic Susceptibility of Nickel-base Ferromagnetic Alloys (Paramagnitnaya vospriimchivost' ferromagnitnykh splavov na osnove nikelya) PERIODICAL: Vestn. Mosk. un-ta Ser. matem., mekhan., - astron., fiz., khimii, 1957, Nr 1. pp 47-52 ABSTRACT: The Faraday- Sucks mith method (the elastic bring method) was used to investigate the paramagnetic susceptibility (PS) of fer- romagnetic alloys (Ni-Cu, Ni-Al, Ni-Si, Ni-Sn, Ni-Cr, Ni-Mn) ) in a at temperatures above the Curie point (1200 > T >, 0 vacuum of appx. 10-3mm Hg. k The samples investigated, pre- pared in the form of balls of 2 mm diameter, were subjected to annealing for 8 hours before measurement. The measure- ments were made in a nor-uniform magnetic field produced by means of shaped conical electromagnetic pole shoes. It is shown that for the Ni-Al and Ni-Si alloys the negative PS is inversely proportional to the temperature over a broad interval of temp- Card 1/2 eratures, the magnitude of the interval being dependent upon 137-58-1-1550 Paramagnetic Susceptibility of (cont.) the non-ferrot-nagnetic element contents. The PS of Ni alloys in the high temperature range may be represented in the form of the expression ;~ = Xk +X T where )(k is the PS that is independent of the temperature, and Xt is the PS varying in accordance with the Curie-Weiss law. in the case of Ni-Cu alloys, /Yk undergoes virtually linear diminution as the Cu content rises, while in the case of other alloys, Xk increases with the proportion of the non-ferromagnetic component and is highly dependent upon the valence of the latter. The magnetic moments and the Curie-Weiss con- stant diminish as the non-ferromagnetic element increases. Obviously, a portion of the s-electrons of the non-ferromagnetic element participates in the paramagnetism described by the Curie-Weiss law, while another part is involved in a paramagnetism analogous to that of Pauli. The results obtained are in good agreement with the literature data and the theory of s-d exchange interaction. V.R. 1. Ferronapnotic 2. Ferromagnetic xtaterials--Para- tragne'Lic Card 2/2 AUTHORS: Volkov, D. I. and Chechernikov__V, i. 126-1-27/40 TITLE: On the temperature dependence of the paramagnetic susceptibility of ferromagnetic alloys. ~O temperaturnoy zavisimosti paramapitnoy vospriimchivosti ferro- magnitnykh splavov). PERIODICAL: Fizika Metallov i Metallovedeniye, 1957, Vol-51 NO-1, pp. 168-169 (USSR) ABSTRACT: The temperature dependence of the paramagnetic suscept- ibility of ferromagnetic alloys was investigated in the tempgrature range from the ferromagnetic Curie point to 1200 C in vacuum by means of the Faraday-Sacksmith method for the binary alloys N_'-Cu. Ni-Al. Ni-Si. Wi-Sn, Ni-Cr and Ni-Mo in which the concentration of the non- ferromagnetic component was varied within wide limits. The investigations have shown that in the high temperature range the paramagnetic susceptibility of the studied alloys can be satisfactorily described by the relation: 't = 'Xk + '4 (1) The results are graphed in Fig,l and discussed in the text. Card 1/2 There are 1 figure and 1 Slavic reference. 126-1-27/40 On the temperature dependence of the paramagnetic susceptibility of ferromagnetic alloys. SUBMITTED: September 29, 1956. ASSOCIATION: Moscow State University imeni M. V. Lomonosov. (Moskovskiy Gosudarstvennyy Universitet imeni M. V. Lomonosova). AVAILABLE: Library of Congress. Card 2/2 ;,--, ~ 01 1 11-1, // '~! ~ ' XONOVALOV. V.V.; CAECEILTON. V.1.- D.V.; FIRM, 1.Yp-. MUMMA Preliminary heat treatment of glass batches. Stek,! ker. 14 n-).7:1-6 J3. '57. O-u-j~ lo: 2) (Glass manu-Pacture) C_~ K~le /~ Oil/ AUTHORS: Volkov, D. I., ChechernikoT, V. I. 48-8-2t0/?5 TITLE: Temperature Dependence of the Paramagnetic Susceptibility of Alloys on a Nickel- basis (Temperaturuaya zavisimostl paramagnitnoy vospriisohivosti splavov na o9nove n1kelys.). PERIODICAL: Izvestlya Al SSSR Seriya Fizicheakaya, 1957, Vol* 21, Nr 8, PP* 1111-1115 (USSR) ABSTRACT: As an introductory remark it is maintained here that this field of research has not been fully explored. From a theoretical point of view it is generally assumed, that the paramagnetic susceptibility of ferro- magnetic metals in the range of temperatures above the ferromagnetic Curie-point T to Of is caused by the Inner electrons. Whereas the role of the outer electrone is not touched at all. TJnder certain circumstances, how- ever, the consideration of the effect of a-electrons might be of great Importance in the range of temperatures above the Curie-potnt, because here the peculiarities of the temperature dependence of the paramagnetic CARD 1/3 susceptibility of alloys containing non-ferromagnetic Temperature Dependence of the Paramagnetic Aa-8-W;25 Susceptibility of Alloys on a Niokelbasis elements with differing valence must be taken Into consideration. This problem was investigated in this paper. Taperim*ntal research was executed on pure nickel and Its alloys with non-ferromagnetic components: NI-Cu, NI-Znt Ni-Al, Ni-Si, Ri-Mo and Ni-Cr in the temperature range from the Curiepoint up to 12000C. The method by 7araday-Sucksmith was employed for the measurement of the paramagnetic auseeptibilltyt the investigations being conducted in vacuum up to 12000C. The conclusions drawn here are such, that the paramagnetic susceptibility of ferro- magnetic alloys does not follow the law by Curie- Weiss, at high temperatures, but the generall law X - X~, + TC9 , C denoting the Curie-Weiss constant, aP the parametric Curie point, Xk a X independent of temperature. Further research furnished, that the CARD 2/3 paramagnetic susceptibility is largely dependent on the Temperature Dependence of the Paramagnetic 48-8-3-0/25 Susceptibility of Alloys on a Nickelbasis strength of the magnetic field at temperatures near the Curie point, and that with an increase of the concentration of the non-ferromagnetic components in the nickel alloy the values of the coefficients dependent upon temperature and the composition of the alloy decrease. Bear the Curie point the parameter varies with a linear relation and drops to zero at the Curie point. There are 8 figures and 7 references, I of which is 31avic. ASSOCIATION: Deptwut oV-1hysids, of the Moscow State University imeni M. V. Lomonosow (Fizicheakiy fakulket Moskovskogo gos. universitets. im. M. T. Lomonosova) AVAILABLE: Library of Congress CARD 3/3 If L I ~j 1v,2- '\ Cv V01MVP D. I.P KOfiDMMp E. Lp ERINCEJX, G. S., A. P.J9 RCLEJ, V. E.Jq CRZCMNIKOV, V. I., and GOFMAN, U. J MIRYASOV, N. A.p PARSANOV, ~ ~Moscov) *Besults of Studies of Certain Hepatic and Magoeto-Optical Properties of Ferro-ftpetics:" :1 'Saturation Magrotization of CuNj Alloys at 1,0v Tqm1mratures.w %"NsPetic PPepertles of NhB System." 5E *TOWeratun Dependence of Paramgnstic Susceptibility of Farriteg." 5~"Mh9wtO-OPt1c&1 ROSOURMS, In 1ferromagmetics."k (Krinchik) report presented at Colloqulm on Magnetism, Grenoble, France, 2-5 Jul 58. Rval: B - 3,111,755 3 SOP 58. 24(3) AUTHORS: Volkov,D.I.,and Chechernikov, V.I. SOV/155-58-2-44/47 -TITLEt The Temperature Depondence of the Paramtgnetic Receptivity of 't omo Farrites (Tempers,turnaya savisimost, param&gnitnoy .vospriimehivosti n*kotorykh forritov) PnioDiCALs Nauchnyye doklady vysahey shkoly. lisiko-matematicheakiye nauki, 1958, Nr 2, pp 208-213 (USSR) ABSTRACT: The present paper is a report on the experimental investigation of the temperature dependence of the paramagnetic receptivity of several ferrit (nickel-, cobalt-, manganese-, magnesium-, lithium ferrit::).-It was stateds in the immediate neighborhood of the ferromagnetic Curie-point the receptivity is a function of the temperature and the field. for higher temperatures the depedence on the field suspends, but not always It follows the law of Reel ,[hef 111 9.g..~.the behavior of the manganese ferrite in the interval from 6T30K to 9000 K deviates essentially from Neel without depend- ing on the field. For 136001 the receptivity of the lithium ferrite changes desultorily. There ore 5 figures, and 4 referenoes, 2 of which are Soviet, and .2 Americiane Card 112 The lemperature Dependence of the Paramagnetic Receptivity of some Ferritea SOV/155-58-2-44/47 ,LSSOCILTIONsMoskovskiy gosudarstvennyy uni,**rsitet imeni X.V.Lomonosova (Moscow State 'Univirsity imeni V.V.Lomonoaov) SUBMITTEDs January 17, 1956 Card 2/2 240) AUTHOR: TITLE: PERIODICAL: ABSTRACT: 14 Chechernikov,V.I. 3011/55-58-4-10'/31 -------------- On Paramagnetic Susceptibility of the Alloys Ni-Ag and Ni-W (0 paramagnitnoy vospriimchivosti splavov Ni-Ag Ni-W) Vestnik Moskovskogo universiteta, Seriyzn mif., flzrtkij, J~~Ilv1i,, ;958, Nr 4. PP 145-146 (USSR The author investigated the temperature dependenoe of the paramag3etic susceptibility from the Curie-point to 1200 0-C for 10- mm Hg. It was stated that 1 1 is no straight 'Line but a curve concave with respect to the T-axis. The author confirmed the formula k + T p where p is the paramagnet-.a Curizt-roint, c is the Curie-We-13 const'ant. k is the magnetic susceptibility; (1) is valid for T ~s the ferromagnetic Carie-point f~,r Ni-Cn. Nz-Zn, Ni-Al, Ni-Sn, NI-Cr, Ni-Mo. There are 2 figures, I table, and 2 So-iriet references. ASSOCIATION%Kafedra magnetizma (Chair of Magnetiom) SUBMITTED: 00tober 149 1957 Card 1/1 24(3) AUTHORS: Chechernikovq V, I., Volkov, Yu, D. SoV/56-35-4-6/52 TITLE: The Temperature Dependence of Paramagnetic Susceptibility in Nickel-Zinc Ferrites (Temperaturnaya zavisimost, paramagnitn,ly vospriimchivosti nikelt-tsinkovykh ferritov) PERIODICALz Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1958, vol 35, Nr 4? pp 875-B79 (USSR) ABSTRACT: Whereas for ferromagnetic metals and alloys the paramagnetic susceptibility 7(obeys the Curie-Weiss (Kyuri-Veyss) law at -high temperatures (T*9Curie)t this is not the case with the temperature dependence of X in ferrites. The first theoretical investigation of these regularities was carried out by Neel (Refl); the results he obtained are describecl in short. They agree well with experimental results* In the case of alloys a considerable degree of dependence of C_ and19-values on composition (C - Curie-Weiss constant, 9 - Curie point) was found. Already in a previous paper the authors carried out an experimental investigation of the temperature dependence of'X Card 1/3 the experimental system is described by reference 4- The Temperature Dependence of Paramagnetic SOV/56-35-4-6/52 Susceptibility in Nickel-Zinc Ferrites The present paper gives the results obtained by numerous measurements. Figure I shows the dependence of 1/X on T within the range of 300-15000K for 10 different ferrites. Whereas for Fe203,ZnO I/X increases' practioally linearly with Tj the vther curves are more or less curved towards the T-axis, especially that for Fe203-NiO. Figures 2 and 3 show the dependence of the constants 8 t CH q d and 1/)~on the percentage of the ZnO content in ferrite. Figure 4, on the other hand, shows the dependence of I/it on T, viz. experimental curves together with those calculated according to Neel's law. It is shown that, within the range of about 850-15001K, the theoretical and experimental curves coincide. The authors further investigated the magnetization curves fo F 00.5 NiO*0.5 ZnO (Fig 6) at. 5 different temperatures (range 5 7-5560K). It was found that with increasing T the specific magnetization 6 decreases; the course of the curves d(H)(range 0-5000 Oe) more and more develops into a straight line. For H(6) near E) Curie the Card 2/3 The Temperature Dependence of Paramagnetic V/56-35-4-6/52 Susceptibility in Nickel-Zine-Ferrites formula H - ai% + b63 is given. The authors thank Professor Ye 1. Kondorskiy and D. I. Volkov for discussing the results. Th;re are 6 figures and 5 references, 2 of which are Soviet. ASSOCIATION: Noskovskiy gosudarstvennvy universitet (Moscow State University), SUBMITTED: May 5, 1958 Card 3/3 CHSCHIRNIKOV. T.I.;VOIZDV. Yu.D. StudF of nickel size ferates in the transitional region, Test Moak. ung Sero mt. g m9kh. . astron. , f Is. , khim. 14 no.2:101-105 159 (min 13:3) 1. Kafedra, viagnetizza Moskovskogo gosuniversitsta. (NICINI ilue fairstes) J 00 68044 AUTHOR. Chachernikov, V. I. BOV/55-59-3-12/32 The-Temperature-dependencelof TITLE: PERIODICAL: ABSTRACT: Card 113 the Paramagnetic Susoeptibilit of Nickel - Magnesium an Nickel - Manganese Perrites Vestnik.1doskovskogo univa:-aitata. Seriya matematikiy,mekhaniki, astronomii, fiiiii, 96 (UgSR) 1, 1959, Nr 3, pp 93 - I In the present paper nickel-magnesium and nickel-manganese fer- ritos of the composition Fe,.O 3N-160 1-z 902are investigated within the wide temperature interval ranging from the ferromagnetic Cu-rie point 0f to - 15000K. In the above formula M.den'otes the bivalent metal manganese or magnesium. The five sampl. es investi- gated of the nickel-manganese ferrite system eorresponded to the following values of z: 0, 0.2, 0.4, 0A., and 1. From the system of nickel-magnesium ferrites 6 samples with the following values of a were investigated.- 09 0.2, 0-39~0-5, 0."59 and i. Moreover, 'nick6l-manganese.samples with z - Op 0.2, 0.4, 0.6, and I were investigated. No phase transformations occur in the samples used in this case within the temperature interval under investigation,,*** 68044 The Temperature-dependenoe of the Paramagnetic Susceptibi- SOV/55-59-3-12/32 lity of Niokel - Magne sium and Nickel - Manganese Ferrites Two diagrama show the temperature dependence of the inverse molar susceptibility for all fferrites investigated within the temperature interval of from 650 to - 15000K. Two other dia- grams show the coefficients C, 6, 1 40 and 0, which are con- tained in NeelPs law I - 1 +1 - as functions of the ~ T 0 percentage of MgO and KnO in the ferrite. These constants de- crease for nickel manganese ferrites with an increase in the KnO-content. In niokel-mWesium ferrites this decrease Is lose distinctly marked, and.1 P40 even increases slightly with an in- emease in the XgO-content in the ferrite. The decrease of C (which apparently characterizes the paramagnetic moment), ia due to the tact that the manganese- and magnesium atoms lose elec- trona, thus reducing tbe non-oompeneated electron spin* of the nickel- or ixon ions. The variation of the parameter 1 40 is essentially correlated with the variation of the constant n of the molecular field. The dearease of 6 with increasing z-may be Card 2 explaired by the fact that P. decreases with an.increase of th 68044 The.Temperature-dependence of the Paramagnetic Susoeptibi- SOV/55-59-3-12/32 Xity.of Nickel - Magnesiumand Nickel - Manganese Ferrites wamber of magnesium- and manganese ions. The decrease of 0 with increasing z is explained mainly by the decrease of n and C and the exchange interaction of the ions in the various sublattices. The theoretical oli-rWes for C, do.1a,.and 0 are,in practical agreement with experimental curves. Neel's law applies to all ferrites in a wide temperature interval of about 850 - 15000X- It would be of interest to investigate*these ferrites in the immediate vicinity of the feTromagnetic Curie point in order to study the.range of farromagnetio transition. The author thanks D. 1. Volkor.for some useful advioe.,There are 4 figures and 5 references, 2 of which are Soviet ASSOCIATION: Kafedra magnetizma (Chair for Magnetism) SUBMITTED.: Doe-amber 29, 1958 Card 3/.3 S/18 60/000/03/05/008 BO19YI1056 AUTHORSs -Chechernikovi.L..L., Uchaykina, R. P. TITIZ: The Temperature Dependence of the Magnetic Susceptibility of Ferrite-garnets of Yttrium and lirlium 1A PERIODICAL: Vestnik Moskovskogo universiteta. Seriya 3, fizika, astronomiya, 1960, ho. 5, PP- 57 - 41 TEXT: The garnets investigated here have the formulas 5Fe 20 3' 3Y203and 5Fe2O 3* 3Gd 20 31 the samples were of spherical shape and had a diameter of I - 1.5 mm. The measurements were carried out at field strengths 0of from 1,500 to 20,000 oersteds and at temperatures of from 500 to 1350 K. rom the temperature dependence of the reciprocal of molar susceptibility near Curie point it may be seen that susceptibility changes slowly with tempera- ture. Within this range, susceptibility is a function of field strength, whereas at higher temperatures it depends only on temperature. Formula (1) is given, which describes the dependence of the intensity of magnetization d on the magnetic field in the neighborhood of the Curie temperature: vl~ Card 1/2 The Temperature Dependence of the Magnetic S/188/60/000/03/05/008 Susceptibility of Ferrite-garnets of Yttrium and B019/BO56 Gadolinium H - ad + P(13 (a and A are temperature-dependent coefficients). Fig. 2 shows that with rising temperature and fixed magnetic field strength, magnetization rapidly decreases. This diagram further shows that the isothermal lines of magnetization are nonlinear only in the ferromagnetic region, while in the paramagnetic region they may be approximated by a straight line; in this case, susceptibility depends only on H. In Fig- 5 experimental results concerning the dependence of reciprocal molar susoeptibility on absolute temperature within the range of from 640 to 13500K are compared with the theoretical results calculated according to Neel (Ref. 6). There are 5 figures, 1 table, and 7 references: 2 Soviet, 4 French, and 1 German. ASSOCILTIONs Kafedra magnetizma (Chair of Magnetism) 11~s SUBMITTEDs October 14, 1959 Card 2/2 82328 C S/139/60/000/03/oo6/o45 AUTHORS: Chechernikov, V.I. and Uc a n . R,F. _r~ TITLE: Temperature Dependence of the Paramagnetic Susceptibilitv~ of Nickel-cadmium Ferrites PERIODICAL- Izvestiya vysshikh uchebnykh zavedeniy, Fizika, 1960, Nr 3, pp 39 - 42 (USSR) ABSTRACT: The paramagnetic susceptibility was measured by an apparatus based on the Faraday-Sucksmith method. The susceptibility was measured in a -,r-acuum inthe temperature interval between 300 and about 1 400 0K. The high temperatures.were obta3-ned with the aid of a furnace made of a quartz tube and heated by platinum wire. The tempera- ture of the furnace was measured by a platinum-platinum rhodium thermocouple. 20-40 mg specimens were investigated in fields between 900 and 20 000 Oe. The specimens were mixed ATi-Cd ferrites~5descrlbed by the formula Fe 20 U - z)NIO-zCdO, where z was varied between 0 and 1. The lerrites were obtained from the oxides Fe2o 3! Nio and CdO, which were mixed and compressed under a pressure of 3 t/cm 2. and then heated at 1 250 OC for three hours. Cardl/3 82328 5/139/60/000/03/oo6/045 Temperature Dependence of the ParamEa0gaMPAusceptibility of Nickel-cadmium Ferrites Figure I plots the reciprocal of the molar susceptibility as a function of temperature for the specimens indicated. As the CdO concentration increases, the dependence of 1/x on T gradually becomes linear. According to the Neel theory the reciprocal of the susceptibility as a function of temperature is given by Eq (1). Using experimental values for the constants in this expression, one can calculate the theoretical dependence of the reciprocal susceptibility on temperature, Figure 2 gives this dependence. The dotted curves are theoretical and the continuous curves are experimental. The two curves coincide in a wide temperature interval. The area of agreement increases with increasing cadmium-oxide conc entration. The curves do not agree near the ferro- magnetic Curie point. Measurements were also carried out of the magnetic susceptibility near the ferromagnetic *' 01, '. -t - - - - - Curie -polnt~.- -1-t-was found that near Q., .. here is a V Card2/3 temperature region where the susceptibility is weakly 82328 S/JL39/60/000/03/Oo6/o45 Temperature Dependence of the ParaEmoain2efi'c"Sxxsceptibility of Nickel-cadmium Perrites dependent on T but is a function of the magnetic field H The dependence of the specific magnetisation H Is described by anexpression of the form given by Eq (2), which holds between 1 000 and 10 000 Oe. The coefficients a and 0 depend on temperature and con- centrat�on. The c efficient a varies linearly with temperature neax---&.;,- but vanishes at f T The coefficient varies nonlinearly with temperature. These facts were used to determine the ferromagnetic Curie points for ferrites with z = 0 , 0.1, 0-2, 0.3, 0.4. 0.5 and 0.6. for which the Curie points were 843 750, 710, 6351 580, 540 and 480 OK, respectively. Thus, thse ferro- magnetic Curie point is a practicalVlinear function of the cadmium-oxide content of the ferrite. There are 4 figures and 4 references, 3 of which are Vrench and 1 is Soviet. ASSOCIATION: Moskovskiy gosunivert-titst imeni M.V. Lomonosova (Moscow State UniverzFlty imeni M.V. Lomonosev) SUBMITTED. March 9, 1959 Card3/3 CIMHIRNIKOT. V.I.; UCWKINA, R.G. Investigating ferrates In Ittrium and gadolinium garnets in the vicinity of the ferromagnstle Curie point. Mz.m9tA metalloved. 9 n0-3:456-458 * 160- (MM 13:6) 1. moskovekly sudaretvenW universitst 126 MeTeLomonomovae FIFFOrrates) (Curie point) 85962 hL11-1, 24'Zo, AUTHOR: Chechernikov'_V.1. TITLE: --Te-UTAVM-t~~~Ce-;f the Ferromaxnetic SuseeptibilitMtof Iron Nickel Alloys I -A - V - - PERIODICAL: Fizika wetallov i metallovedeniye, 1960, Vol.10, No-5, pp.672-675 TEXT: It is known that the paramagnetic susceptibility of nickel alloys at temperatures very much greater than the ferromagnetic Curie temperature may be represented as a sum of two terms, namely 5/126/60/010/005/006/030 2032/2414 % = Xk + %T The magnetic susceptibility %T %T = C/T - Op (1) follows the Curie- Weiss law where C is the Curie -Weiss constant and Op is the paramagnetic Curie temperature. The quantity Xk is not temperature dependent and is, in fact, a susceptibility of the Card 1/4 85962 S/126/60/01o/oo5/006/030 E032/z414 Temperature Dependence of the Ferromaxnetle Susceptibility of iron Nickel Alloys Paull type. It has been shown experimentally by the present author and Volkov (Ref.1) that 'Xk strongly depends on the concentration of the non-ferromaXnetic component in the alloy. It increases with this concentration, and the rate of increase is greater for greater valencies of the non-ferromagnetic component. In the present paper, the author reports a study of iron-nickel alloys which has not so far been carried out from the above point of view. Alloys containing 89.6, 80.3, 77.69 75.1, 69.o, 58-81 48.5 and 38.8 at.% Ni were Investigated. The paramagnetic susceptibility was measured using an apparatus described by the present author In Ref-3. This apparatus is based on the Faraday -Sucksmith method. All the measurements were . carried out in an argon atmosphere. FIg.1 shows the reciprocal of the paramagnetic susceptibility as a function of temperature In the range 400 to 12000C. The curve marked l- refers to pure nickel and the remaining numbers refer to the above eight nickel concentrations respectively. In most cases the dependence is Card 2/4 85962 S/126/60/010/005/Oo6/030 2032/E414 Temperature Dependence of the Ferromagnetic Susceptibility of Iron Nickel Alloys practically linear. Only in the 89.6 and 80.3% alloys can one detect a small departure from linearity. In the-st two cases the curve bends towards the temperature axis. In the first of these two alloys this departure begins at about 10000C and in the second at about 11000C. In other words, the linear parts of the plot of reciprocal susceptibility versus temperature become longer for lower concentrations of nickel, and below 77% Ni all the plots are linear in the above temperature interval, i.e. these alloys obey the Curie- Weiss law. The dotted lines in Fig.1 represent a plot of III - = f(T) - %k for the above two alloys. This relation is linear. Pig.2 shown a plot Of %k as a function of the atomic concentration of iron in the alloys. As can be seen, the temperature independent Card 3/4 85962 S/126/60/010/005/006/030 3032/9414 Temperature Dependence of the Ferromagnetic Susceptibility of Iron Nickel Alloys susceptibility Xk decreases with iron concentration and in practically zero at a nickel concentration of about 75%. Beyond this value 'Xk remains unaltered. The results obtained by the present author suggest that Xk depends not only on the paramagnetism of the conduction electrons and the a- d exchange interaction, but also on the diamagnetic properties of the metal. It follows that in studying ferromagnetic metals and alloys in the paramagnetic region, both paramagnetic and diamagnetic properties of these materials should.be taken into account. There are 3 figures and 9 references: 5 Soviet and 4 Non-Soviet (one of which is translatedlinto Russian). ASSOCIATION: Moskovskiy gosudarstvannyy universitet Im. H.V.Lomonomova (Moscow State Univeratty im. M.V.Lomonosov) SUBMITTED: February 2, 1960 Card 4/4 21210 #7, IQ, S/188/61/000/001/005/009 210M) 11", 11~01" B108/H09 AUTHORSs Chechernikov, V. I., Kollchenko, V. G. I ~.. TITLE: Temperature dependence of the paramagnetic susceptibility of copper-cadmium ferrites PERIODICALt Vestnik Moskovskogo universiteta. Seriya 3, fizika, astronomiya, no. 1, 1961, 36-39 TEXTs In order to check the correctness of Neel's hyperbolic law of the temperature dependence of the paramagnetic susceptibility for high temperature, the authors studied copper-cadmium ferrites containing cadmium ferrite of normal spinel structure. The ferrites were prepared from Fe 20V CuO, and CdO powders which were mixed with ethyl alcohol for 44 hr. Subsequently, the mixture was driedg siftvd, and mixed with poly- vinyl alcohol. Samples were pressed at 3 tons/GMZ, annealed at 10500C for 3 hr, and slowly cooled to room temperature., The cylindrical samples (1-5 mm high) were examined between 300 and 1400 K, using the Faraday- Sucksmith method (Ref- 4: Sucksmith W. Proc. Roy. Soc., AjJO, 5519 1939). Fig. 1 shows the temperature dependence of the reciprocal molar para- Card 1/4, 21210 3/188/61/000/001/005/009 Temperature dependence of the... B108/.B209 magnetic susceptibility of various copper-cadmium ferrites between their respective ferromagnetic Curie points and 1400 0K- It is seen that with rising CdO content in the ferrite, the curves are gradually straightened. On the basis of experimental data, the authors determined the constants in Neel's law. Fig. 2 shows a comparison of the theoretical curves, as calculated with these constants and Neel's law, and the experimental ones. Finally, the authors studied the dependence of the constants 0, 1/10 ~,C) in Neel's law (Ref. 3: Neel L. Ann. Phys., 1, 137, 1948) on the percentual content of cadmium ferrite (CdO-Fe 20 3) iu the composite ferrite. They found that all the constants decrease with increasing con- tent of cadmium oxide. The results show that the paramagnetic suscepti- bility of the ferrites under discussion follows Neel's law in the range of high temperatuxes. LAbstracter's note: In the original legends to the figures, the symbol Gd should read Cd]. There are 4 figures and 5 references. 3 Soviet-bloc and 2 non-Soviet-bloc. ASSOCIATION; Kafedra magnetizma, (Department-of Magnetism) SUBMITTED: July 27, 1960 Card 2/4 Temperature dependence of the... B108/B209 Ix vL &W 40 AT Fig. 1 &V IM rly Legend to Fig. lt (1) Fe 20 3' CUO; (2) Fe203' O-qCuO-O-lGdO; (3) Fe203* 0-f3CUO-0-2GdO; (4) Fe203' O-6CuO-0-4GdO; (5) Fe 2 03*0-5CUO-0-5GdO; (6) Fe203* 0-4cuO-O.6GdO; (7) Fe203' 0,.-3CuO-0-7GdO; (8) Fe203* GdO. Card 5/4 S/188/61/000/001/005/009 Temperature dependence of the... 1211V 1 Fig. 2 alI J, 41V MW T*lf xm Legend to Fig. 2: (1) Fe 2 0 3* 0-7GdO-0-3CuO; (2) Fe 2 0 3'0-5GdO-0-5CUO; (3) Fe 2 0 3* O-2GdO-O-8CuO; W-Fe 20 3' CUO. Card 4/4 210 S/188 61T000/001/005/009 B108/B209 30076 2y'W" S/048/61/025/011/022/031 I,- 117/B102 AUTHOR: Cheche- TITLE: Temperature dependence of the paramagnetic susceptibility of mixed ferrites PERIODICAL: Akademiya nauk MR. Izvestiya. Seriya fizicheskaya. v. 25, no. 11, 1961, 1399-1402 TEXT: The constants CN, 9, 1/1., and a contained in the law 1/X - 1/Xo + T/Ca - a/(T - 9), (1), first established by Neel for ferrites were studied between ferromagnetic Curie point and 15000K as functions of ferrite composition. The following ferrite systems were examined: Fe 203(1 - z)NiO-zIAO and Fe203(1 - z)CdO--.PO. M stands for Zn, Cd, Mg, Mn, and P for Cu and Li. The allantity z varied between 0 and 1. The numerical values of the above constants were determined from -Derimental data. Applying the values thus found, the theoretical I/Y = f(T) can be calculated from (1). 9, Xo. and a depend on Temperature dependence of S~0076 1 048 61/025/011/022/01 B117/B102 the constants of the molecular field, on the number of magnetical1y active iron ions, and on their atomic constant C V. . A satisfactory agreement between theoretical and experimental values only at high temperatures. It was found in all examined the character of the curves 11Xf(T) differs most widely. base ferrites, CN dropped nonlinearly with rising component, The same was also observed to hold for A particularly strong change of the constants is observed ferrites, It was shown that mixed ferrites, like metals, possess a transition region in which Y depends also on H. The width of this region, which depends between experimental and theoretical results, can by heat treatment (10 hr at 12000K and chilling in Chechernikov. V. 1. ~ Volkovj Yu. D. , Vestn. Llosk. but cannot be elim.'Mated. Systematic studies of a ferrites have shown that the constants CTJ 05 1 h /X. can be observed cases, although In all nickel- content of the second the other constants. in mixed simple ferrites and not only on T but on. the diver-ence be narrowed by 5o-60 water) (Ref- 3; un,-ta ` 2, 1011 (1959))~' large -group of mixed and a deDend on the -4+e composition in a specific manner and that the magnetic structure be determined fr~- -!/X f(T) In the paramagnetic region. 30076 B/048/61/025/011/022/031 Temperature dependence of ... B117/B102 In the case of a linear dependence (Curie - Weiss law) a magnetic structure of normal ferromagnetics is observed if 9 p> 0, while the structure of compensated antiferromagnetics can be observed if 9 p< 0. Ferrimagnetizs are subjected to Neel's law in the paramagnetic region. There are 5 figures and 3 references: 2 Soviet and I non-Soviet, The referen~-e to the English-language*publication reads as follows: Ref. 1: Neel L, A-in. Phys., )) 137 (1948). ASSOCIATION- Kafedra magnetizma fizicheskogo fakullteta Moskovskogo gosudarstvennogo universiteta im. M. V. Lomonosova (Department of Magnetism of the Physics Division of Moscow State University imeni M. V. Lomonosov) Card 3/3 22121 S/056J61/040/003/001/031 B111IB202 AUTHORSs Cheohernikov, V,1.1 Kolichenko, V*Q* TITLZs Antiferromagnetic properties of cobaltous oxide PERIODICAU Zhurnal okeparimentallnoy i teoratioheakoy fizikip vo 40# no* 3* 19619 721 - 724 TEXTs The authors studied the magnetic susceptibility of CoO between 100 - 70001r. The temperature dependence showed a sharp peak at 292 0Ko Purthermoreq the authors determined the dependence of susceptibility on the magnetic field in antiferromagnetic state and in the region of the an- tiferromagnetic Curie point. The authors determined the dependence of the magnetic susceptibility on the magnetic field strength H in CoO because the dependence mentioned in the references (J.Phys. et Radium, 12, 765, 19511 ZUTF9 Z 1119, 19571 J. do Phys., j_2# 170P 1951) was different in other substances* This fact has hitherto not been fully explained* Magnetic susceptibility was determined by measuring the force acting upon a sample which has been brought into an inhomogeneous magnetic fielde The Card 1 /7- ~ 22121 3/056J61/040/003/001/031 Antiferromagnetic properties B111/B202 force vas measured by determining the defbrmation of an elastical circular ring consisting of beryl2lum bronze. For a mass of 10 - 25 mg of the sample the point of the scale denotes a value of - 10-7. The low tempe- ratures of about 10001 'were produced by evaporating liquid nitrogen. By means of quartz threads the sample was freely suspended in a double-vall glass tube. The individual chambers were filled with nitrogen vapor in order to keep the temperatures as constant as possible. The temperature vas measured by means of a copper-constantan thermocouple. The studies were made with magnetic field strengths of up to 18,000 oe* The antifer- romagnetic Curie point (2920K) is independent of the external magnetic field* If the curve in Fig. I is extrapolated until the absolute zero is attained a magnetic susceptibility of - 55*10-6 is obtained. Above 470 0K the curve shown in Pig. 2 obeys the Curie-Weise law. The authors ob- tained C = 3.05 for the Curie-Weies constant, P a 4-97 for the atomic P magnetic momentp and 0 -2700K for the paramagnetic Curie point* L.D. Undau is mentioned. There are 4 figures-and 11 referenoess 2 Soviet- SIG5 61/040/003/001/031 Antiferromagnetic properties ... B111%202 bloc and 9 nourBoviet-bloc* The 2 most recent references to English lan- CwLge Publicationa read as followes J. R. Singer, Phys. Rev.p IM, 929, 19561 We Sucksmithp Proo. Royp Soc.9 A 170, 551P 1939- ASSOCTATIONt Moskovskiy gosuderetvennyy universitet (Moscov State University) SUBMITTEDr January 29, 1960 initially) October 319 1960 rafter revision) low 37h18 3/188/62/000/002/003/013 ~i;- 9900 B104/B102 AUTHOR: Chechernikov, V. 1. TITLE: A,study of nickel-cadmium ferrites in the transition range PERIODICAL: Moscow. Universitet. Vestnik. Seriya III. Fizikap astronomiya, no. 2, 1962, 20-23 TEXT: The investigation of nickel-cadmium ferrites near the ferromagnetic Curie point was based on an experimental arrangement described previously (V. I. Chechernikov, I'Vesbu Mosk. un-ta"j ser. matem., mekbansp astron.1 fiz., khimiit no. 1, 1957). The ferrites were obtained from Fe 0 Nio 2 3* and CdO powder by pressing and sintering. In the transition range above the ferromagnetic Curie point the magnetic susceptibility varies slowly with the temperature in the beginning and decreases rapidly with increas- ing temperature afterwards. In the transition range the magnetic susceptibility depends on the magnetic field strength. Only at high temperatures does it depend on the temperature alone and obeys the Neel law. The magnetization curve in the transition range can be described by S/188/62/000/002/003/013 A study of nickel-cadmium ... B104/B102 0Cd + 363 . H, where m and 0 are coefficients depending on temperature and concentration. In fields of 1000-1500 oersteds the second term of this equation is of importance at temperatures near the Curie point. At higher temperatures the value of this term decreases and magnetization becomes a linear function of the magnetic field strength. - and 3 are positive in the temperature range investigated. o6 is a linear function of temper- ature and tends toward zero for T - 0 . ~ is no linear function of f temperature; at 8 it.pos sesses a minimum. lost ferrites.have similar f ch characteristics. Th,' re 4 fi ASSOCIATION: Kafedra, etizma. Re'arti~ea of Magnetism) magn SUBMITTED: MaY 3t 1961 Card 2/2 38878 0 S/188/62/000/003/003/012, B111/B112 AUTFOR: Chechernikov, V. 1. TITLE: Some magnetic properties of a Europium ferrite garnet PERIODICAL: Moscow. Universitet. Vestnik. Seriya III. Fizika, astronomiya, no. 3, 1962, 27-29 TE7XT: The author studied the ferrite garnet 3Eu 203* 5Fe203 near the ferroma[netic Curie point Q f - 2800 using the ponderomotive method (V. 1. Chechernikov, R. P. Uchaykina, "Vestn. Mosk. un-ta", ser. fiz., astronomii, no. 3, 1960). For T Of, ~Krapidly decrea:ses. Near the Curie point, ad + PCF3 - H (1) states the dependence of the specific magnetization a on the field strength H where a, 0 are tempqrature and pressure dependent coefficients. (1) holds only for pure magnetization. The nonlinearity of (1) gradually decreases as the temperature increases and stops at T = 2890. The 0 f canbe exactly evaluated after determining the Card.1/2 S/16 62/000/003/003/012 Some magnetic properties of*.. BI I I YBI 12 functions a(T), P(T) experimentally; this is of special theoretical importance. Finallyit is established that the region in which (1) holds where X depends only on T and not on H, is much narrower (8-100) for ferrite garnets than for other ferromagnetics. There are 3 figures. ASSOCIATION: Kafedra magnetizma (Department of Magnetism) SUBMITTED: June 4, 1961 Soo two'** W. 250- so Fig. 3 Card' 2/2 200 00,0's W T. 340 ::00 258- so 11W S/126/62/013/001/008f'018 E032/L314 AUTHOPZ-, and Galeyev, G.S. TITLE: A study of iron-base alloys in the paramagnetic region PERIODICAL, Fizika metallov i metallovedeniye, v6 13, no. 1, 1962, 93 - 96 TEXT: The authors report a study of ordered Fe-Al and Fe-MO alloys, whose magnetic properties in the paramagnetic region have not as yet been investigated. The paramagnetic susceptib- ility was measured in the range 750 - 1 200 0C with the aid of the Sucksmith balance; the particular alloys examined were. as follows: 4.06; 5.98; 12.70; 19-57; 21.60; 24.70 and 28-3 at-'D Al and 0.95; 2.49; 5.6 and 6.1 ate% Mo. It was found that for the Fe-Al alloys the susceptibility was inversely proportional. to the temperature. The paramagnetic Curie point of the Fe-Al alloys was a linear function of the concentration up to 22 at.O,'D Al. Thereafter, even a small change in the~concentration of Al gave rise to a more rapid reduction in the paramagnetic Card 1/3 s/i26/62/oi3/001/00/018 A.study of iron-base ... ~E032/E314 Curie point and for an alloy with 24'7 at.0c Al in an unordered 0 state ep = 236 C. It was found from the relation between the paramagnetic Curie point- '_--i and the percentage concentration p of Al that the Curie point for pure Fe should be 828 OC and this is. in good agreement. with published data. In the case of Fe-Mo a 1 1 0 Y 5 t h e law relation between the recipro .1, c of the susceptibility and the absolute-temperature is again linear for 6.1 and 5.6 at.% Mo but at 0.95 at.05, Mo and 2.119 at Mo there is a discontinuity at 930 0C. This is ascribed to an a y transition. Below this point the Curie-Weiss law is found to hold. The paramagnetic Curie point of Fe-Mo alloys decreases with concentration of Mo less rapidly than in the case of Fc-Al alloys. The general conclusion is that the above alloys follow the linear Curie-Weiss law at high temperatures and the susceptibility due to conduction electrons is zero. The magnetic properties of ordered alloys in the paramagnetic region are very dependent on.the degree of order.~.Thus-, for example, the paramngnetic Curie point of an alloy with 24,.7 at 50' Card 2/3 s/i26/62/013/001/008/018 A study of iron-base .... E032/E314 Al increases from 236 deg for the unordered state to 364 do_z for the ordered state. There is also an appreciable change in the Curie-Weiss constant and the mean number of Bohr magnetons per atom of the alloy. There are 4 figures and 1 table. ASSOCIATION: Moslzovskiy gosuniversitet im. MvV* Lomonosova (Moscow State University'im. M.V. Lomonosov) SUBMIlT ED: Allril 23, 1961