SCIENTIFIC ABSTRACT NIKOLSKIY, V. N. - NIKOLSKIY, V. V.

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SCIENTIFIC ABSTRACT
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NIKOLISKIY. V.V.# Cand Med Jci - (dius) 05tate of phftocyto actIvIty cf PI"d leucocytes in patients with CIOS-oq "m blood circulation Nos 1958t 12 pp (First Vos 6rder of 6nin kd In5t in I.V. SechenoV, 200 copies Ms 32-58, 112) - 77 - Mwgoqttc activity of laukoertoo In circulatory 4 isord*rs of tho brain Lwttb stmory in Franchj * Zbqr*rAvre L pett 1* 58 no.I:Z9-34 1580 (MMA 11:2) Is Kefi*4.ro vArvtWkb IdesaW (tow* - prof e ToeltAK P (does&&"D I Nookovskago ordeam, Imalm m4itshakora tastitul i twat Sachenove. (MAIN, blood supply, also, off. an phocacytooto Me)) (MQMrf*SLS, in var. Us. brain Was Use Ous)) NIMISKItt V.L; AMMUs M.A. Mialml characteristLes of enasowllUs *WervW a Lmi~arsk, zhwo IWILO I PGM. 61 no,6c865-466 161. (milpi 15c2) 1. urodm nervrqkh bolemey ("pobtyarnhahly aby saamsti san- duywhctwgo - dotsout S.A.Kellnikav) I Mookovskoac ordem toaLna mditatnskogo lmtltuta, (ENCEPHALITIS) V.*;l 6. VcF, Virus. in -:w :ya .4 -- ~~ i I-I- -- f_- RIKOLISK11 0 V.P. Sverkhzvukovye techentia v diffuzore tsentrobectmgo, nal7mtatelia. i-bskva, Oborongits 1942# 3 P- (TSIAM. 11ridy, no. W4) Title tr.s Supersonic flow In a centrifu4al superchareer diffuser. TWOLAI M2 no.U SO: Aeronautical Sciences and Aviation in the 4oviet Union# [Abrary of Coneress, 1955 SUMALINIKOYF KeustanUa Tedorovicku KIKOLISKIT Y~~ UM.~ tokbn. ' 'Q remk,, retsowwntj YAKIXM=, -I~kbn. mmk, red.; SATILITEVI, ro.Ya.j, M, ixd-ma; IMOCKLI, 'r.r,,, t*kba. red, EgftdMphical mathads of deteiminine the air ptrmaters of the centrifugal stap of a comprwasorl GrardanalftlebaWds q)&. soby opredeleniia parmotroy yozdukha v toentrobashnoi stupoul kompiessora. MoGkya, Vashgis, 1961-a 227 p. (Kim 15:2) (Compressors) Rafto Vaves Oct "fte Electronics of a Mana Comb," V. X. Immkh-'r. "!A V. S. Rikolskly "Miur Tekh Fit" Vol 22) 'No 10, PP 1599-i6o5 LVestigate "~Aio-wave properties of Plamr e016 pierced by dlectrcm currents, taking ibto &ccmmt tbe scatter of Uhe electrons according to Ve- locity. Give general method of solvin$ ymblen for arbitrary stationary function fo(v) of distribution of the electr=s in the currents &&cording to velocity. Indebted to Prof S. 1). Gvozdover. Cite related vorks of L. W, Losh*Aw *49), A. 1. Akhiyezer, amd Ya. D. Yaynberg 1951). 1 MMLIKIr, T. S,g USILIMS 9. I.And U)PtWHIW,,, T. M~ wrom of Uw glamitim Squtlem In the ?beery or AmplUlors of ContimsWU ftfte Wavew Iv a poper gives at tlw AU-0niveroltr Sclostifle Conferame IlLoomommew zesteresol, feet. Week. Ok-a U-Se 1953 Wabelation W1695s 1 war 56 VASELITIT, ro.t.; UNIM, I.M.; NIKOLISKIT. T.S. Theavy of travollug-wave tube@ with a cowputatlom o0 therma a*tion of elealraw In flow. R no.5t45-52 W 153. (KW& 6:8) 1, I!,stabukty fftrtst Noskavskage gotn4antvanage univeraltsta, ,;. W- (a atronice) ,- O~y V (:4 SZ7,r 6e. c 4", dele-C V- ) - -C~~ I & lm(f);~ I, I I " 0/ L 1.5ta. VD M.~ --AP5CM438 110m,'WAYWI, A I R. 2 -Gi -(Engiro-mr.) Bv-I,:*us Yu.- V-. t4rintter),. q. ';it, - S. (EnFi - I - M:$:Lzelor); shvarzab ya bear) TVM'~t IEf6ct.or the technological protems of tremling mt-Im "-v. -1964i -254 504A!'11"N! '-St4l 75 (7 q'wPo'.1 r, 41: f 6rro&II,3:r, chromium rcintalnint -nlloy, alumistum cont-On'Ing alloy, c;>i~r*.qion mietant alloy/91-626 &)ftoy -xmt~=I liz--AV -MB"tablut?- Of A-T ,Olilt alIV)clixted wIth tlie reducLicin, rracenm. -,w,. CI" ionn which fom. during coating or tim ~d r-- p r1or to dviving djecr"um the At&bI 11ty of U1,41- INI't4l of tile heaters Vigaacmn c-m-rosior, In tic --mirim of service, NII sh- inzt tur ILho wire in ita fiwl size in v=7 affec-tim. CrIlIc. art. han 1 table. .-.41 -IMM; 'Y", L r-y. ;'iQl R,'g !K)V; 001 Xlup X"I ;Awd .111 ACCM1011 Mks APWAM' AMOFfis ftkollakLys V, S-00movs, TITLZI Molting nickol-chrcatim alloys in an are fUMOO Vith MW supply" SOUSCII 3"119 no* 2# l9as 137-139 TOPIC TAGSt nickel chrmium alloys 1101tings -01799A blow$ Kh2CM80 nickel chrmium alloy, Kh15X60 nickel chrcnium alloys titanium resmalp silicon content, in, nichrme, nichrome strength, nichrme plasticity# Kh2Cb8M3 alloy, U20NOM alloy ARSTRACTo Experimental results obtained in, molting XL-Cr alloys in an are furnace with blown-in. oxygen are presented. Tho procedure was developed for obtaining, metal with a low C content, and free of' titanium (despite the us* of'Ti-containing: waste products such as (WCWT3, WGNOMO and. others), The relatioa of Cr/G to temperature was studied in order to determine optimal content of' chromium, k schamsitic: drawing of the molting "sembly used in these experiments. is, sham in F21 . I of the Snclosures It consists of a 50-kg induction oven. with the crucibla (&I mad f ~neslua-chramium, a floating tungstsn-rhoni= therviomple with an I I( ) cowacted to the potentiometer (b) and W the oxygen tank alundust tip passed frm the tank throu& the motor Into the quarta tube VA" ACMSICK Of, APWUM According to the tests of several melts in. the tu*mtwv Ijaterml. Cr/r. relation was Cii 30 W L + r (CI The authors conclude that this m1ting procedure resulted in an effective decarbanization of the metals# in the rmoval of Tis and an in a greater content of Si which, increased the strength and plastic properties of the alloys. Orig. art'. hast 4 figures and 2, foroLlass AMOCrATICKt nme SQWTMi 00 DATZ AMt 039&rdk MCLI OL 390 COD& HL sour I", an am 11101.1 SKIT V 7.3. 1 G(ll ~ (IV, I N . K&klr.g nickel-phro-rito kllr)yi Jrj An 21 - flir,~lr.F9 Wlth txj~.--n r.~F'--Otrp, of aie bath. .33tall 24 ? flckA 1,119) UILM, Kolo, professor: XAMIMITF I.R., im-henen. NIKOWSM T Oct. rodaktor,o SUROTA, T.A., rodaktor; AXDIXW. G.G. pim- 9 0 wxn=F-nnzw, rodaktaro [CMJ*x It= stWiy In mol olue od pjW] Zompj*kvWj khror4mWestj as mollieft thafttakh I larleral&. Kookva. Uglatektdc4at, 1954., M P. (Km 8t5) (Tim attdy) im sur t 4sr h; GRIBIN, G.P., otv*tsty*wqT red.; Z mIaMTA, ~V.A.~,rod=txdatellstvs; AL&WTA,,T*.t.. tokha.red.; =WT. A.P., takhm.red. (Organization of labor and wages In coal altos. a handbook for mine workers] Organ1satelta truda I sarebotoalm iplgta an vVlltWkh shakhtakh: spravochnoo iposoble d1la rabotalkav-shakhty. Moskva, Ugletakhtsdat. 1957. 258 P. (NIXA 10:12) (Cool mines and u1ning) (wages) SUBJECT I USSR/Luninescence, 48-cf-36/56 AUT110R$s Konavokly V.S. and Loshniftove. O.M. TITLE# Thernoluminosednat of Winorals tUrmolyusimosteentelys, almoralow) PERIODICAL# Invontlya Akadoell Nauk 335R0 Serija Fixichooksys, 1957, Vol 21, #59 pp 111-714 OSSH) ABSTRACT# Various sanples of calcites were Investigated with respect to thermoluninescenc9. They were subjectvd to a preliminary Irradiation by X-rays by means of an X-ray tub* BST-W yielding approximately 100 r/ooc. A photoolectrania aultiplier of the FIM-19 type was applied to study the thetwo-lumlaoscence of thee* minerals and to record the curves of Its Int4notty. The Inspection of the curves represented by Fig I and 2 to the Vapor shows that the magultm4o of luminesconco peaks 4spea4s on the time of preliminary Irradiation, laoreasing with time. The comparlaon of thormolusinescence curves of the yellow calcite, ]Fig 1, and the red-vtolot calcite, Fig 2, shows that Card 1/2 the peak of the first curve to considerably higher than that 48-5-36/56 TITLEs Thernolusinescence of Minorals (Torsoly-uninesteentelya mineralov) of the rtd-violot c4lc1t*q which Indicates that the yellow calcite Is considerabIr older than tho red-violet one. This conclusion was confirmed by geological data. Thus, the method of thermoluminescence can be applied for stu- dyieg thellge of the rocks and minerale as was suggested by Daniel* ( . In add1t1cm to this, the authors propose to use this aetho4 for the control of concentration processes to the cases when a mineral complex to be concentrated contains a mineral possessing an ability fer luminescence, The artlole contains 4 graphs. rour non.-Slavic references are cited Oon* of th4a translated into Russian). INSTITUTIONs State Institute of Rare Metals, (Glr*dttot) PRISIXT9D BYt SUBMITUDo No date indicated ATAILABLEs At the Library of Congress. Card 2/2 Viktor Sormavich 104P8 wd thO 0- of some) lr*r.ArMUd4 I OPIAU trU&. mook"t clopplitlamr. 1960, 31 P. (Olt& -IM.&Ntow wwwtw*. . skoomlebaskII& #Wwl i kmaMov w pzow,#hUtmykk, prodprilaUlakht n6-5) (Y-DA 240) (Wftox) Viktor Serreyevicht TIMAD, Hikbail Alaka"e-vichl ST.,WVA,, V.A.,F, 1 4 P07MM-0- Ll Lv F t*Wm. red, v Nandbook for wivers workinc on the imrfaso of eoal md shale aims) Pludatka. d1la rabochikhp sanittykh a& poverkhnosti. ugollrqkh L alaw- toMkk sbakht. Kcakwap Gone ususbao-tekha. l9d-vo lit-ry pa go"nomm dome 1%1. U.2 p* (=A 340) (Coal alms and mining) RIKOLISM V 5 MIMI, Y.A,j SUROVA, Y.A.j red, izd-va; FiliSM'L, L.l., I--.--.,-- ve i B L ~;rve d -0, (ffandbook of regulations for vorkers in coal and shale pits] P*,- Plats- dlIa rabochikh ugollvqM, i alavt#Mkh ratresov, Koskra, Go9.n&uehno-t*khnJzd--vo lit-rjr po gornow delup 1961. 147 p. (Coal mims arA mining-8tandards) (Vaps) (KIRA, 14fu) TYURIN, Mlkhail Alak"yevicht. V.A., red. isd-ya; KIKSMjp A.I.j, t4kbn. Me (Wide for vorkers of coal prepax-ation " briquatinc pImmtel Pa- vdatka dlia rabochikh, obogatitellrqkh i briketrqkh fabrik. Kookvap Goff.nauchno-tekbnAzd-vo, lit-rT po, gorn=u delu, 1961. 16'3 P. (MIRA 14112) (Coal prepaLration p2ante) (Briquets (Fuel)) (Wages) HILOWSM , Vik.tor Sar kba ALI Y. , pyovichl TTURIX, r'l il okee-yovichl STUMOVA, - ---- killtv Lela, UILI=, r". F fffamibo* for udwgromd wwkere in gml "d p"U aims) Pudatka d1la rabo*hMt smigLtykh a& podmurkh rabotakh r uplllWkh I olaatmmykh ah-Irktakh, KofkTar Go** " bno-t*4. ild-mo lit-ry PO gornow dolup 1961e 170 pe (MA 24SO (coal aims am minuc) SUZAKIN, Vitaliv Goorgiyevich, kand. tckhn. nauk; SHOEaJOVICH, Abrm Kikbiql-wieh, inih. PrinIzal wbisstire VkR.S1tAVSL1r, A.M.,, kand. tdkbn. nauk; 3M.C. L.A., retsenzent; NIKOLISKIY,, V.Sop otye r*d.; PGMVSKAYA, I.K.v rsd.1sd--v-; 'tFv~~~Icbn. red.; P?OZO.--IOVSUYA, VA., tekbne rod. hieducing labor cons=ing operationelz in open pit w1mal Sui- zbmdo tridocakosti rabot na k&rlerakh. Yo::kyap Ird-vo ONedrag" 1964, 213 p, (MIRA 17:3) VIktor Serfe.,evIch jdcCja4s&j; CIWINP911i, 111khall [Organization of labor &r4 wages in ;7.1res; a refferenco aid] Organizatsita trWa i zarnbotnoi pllity na s~akhtAkh; upravochme posoble. 2. peror. i dop. 17,d. F oskva, 'Vedra, 1965. 288 p. (KIIHA 18:3) NIKOL(SKIYO V.S. Work practices to a votorinary laboratcry. VeVirlrAr'lm 4-1 4-6 D 164o O'C' F; i er~ i I* Direktor Vinnitskoy voterinarnoy labormtoril. Immurr, T.Y. - - --. - , -- -- -I I allmleal @ad awgUal souldwatleas @a the trameas of Irlwalml armroldia IW rovestles of trigoutml serve ro0e Tqwe aotr*blr. 16 so., 41" As~ 1"2.9 (CUM 23:3) 1, Professor, 2,, Of tbe CHOW for Servem Dlemmos ead lowesergery (ZaA - Prot, V, A, XU*Ildcir)o Iloster SoMal lastiflato. D%UIIOVSr,gk, Kim VAksimovm. Priniml uahastipk NIKOLISKrf V',V'.. kand. tokhn.nauk, dote.; LTAPKDU, T.G.r ft*K*q takba, red, (Radio ewlmserW reader In OmmolKhrestatatils, po redlo- tekbul e n& nemstskow iaqkel pasobie d1la otudentov,, Isu- chniuahchikh imstrarx7l las7k. Maskyag VysaW& shkola 1961. 74 P. (Radio) (KMA 15: 21S JIM() Aizomphorlo PonAlon [a se 4-16 A a f 6 t 0 0 0 0 0 f 4 0 0 0 0 i L 1. - LA L- 00 Of go c 988" si *ago"" V Kul -m-guami. w9bow "Invy mwel? *bm 0 is bb"A ' ( "on almmil 4R am* cw.*. ra M. I got so too 666 041d(t%*4K&4 t-Ifft,4 4f 0 9 too It 6 11 4* V. 1. bl., 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 a 0 0 0 0 OW -0 0 a i @I a. *. i *,, 4. 0 0 * 0 0 0 * 0 0 0 a 4 0 0 0 0 : : : 0 A 9 0 0 9 - - - -&- fees 0 4 111, W 0000 W 9 0 0 . a a a a 7- 4111, L-L-A-i-AL; 1; 7 i 14-00 111 so U-6 re 1 lee r e all amppm do do ambeW 0 epiow. AL.~ i Ak m l~ M c N K T 7 a GF- mm w. o , I (we d 29" ago a t inw; aw - -I dw stbe f boo a LIZ n bmwe"Mm. rft game 60staw tow. , 4 W l 14 41 t o ) fee e 1 we"O o~ftmo aw 1 l w . 00 v0 '00 0e 00 !fee see 4 8% S t , U 1 UP t to l * sh 0 0 0 0 0 00 fe a 0 0 0 0 0 0 0 0 * , 00 000000 00000614 see 000, .- - . . , N L T . 'LL L. Z, r. L 1 8;. Nikollskly, V. V. 'The affect of bexcanal anesthesia on the oxy--en ccntent In the Efood", Sbornik nauch. trudov kurorta Saki, Vol. IV, 1948, P. 1115-117. Sot U-3261, 10 April 1953 (LeUpis tZhurnal Inykh Statty, Ho. 12, 1941). I; Ircilf"falOy, V. V. 111WOORkIr- Y*V-, ZalesskAyt;, Ma., and Chukrayeva, IN.J. 011's dytm-nice t_r IiJ4 changes and the albt=en content n oisch~rger of gonorrhea ratients under the influence or renicillin and sulfadin thprapy", Sbornik much. tr,-~rv (Rost. obl. nauch.-Issled. akushersk--g nekol. In-t), Is.,we 80 1948, p. 88,94. SO: U-3261, 10 April (Lato,~is 'Viurnal Inykh St-A y, flo. 12, 1',49). 1953 -v, I A --; Z-,lP;3F H, ': , -~ . 5idcrov, P. P. and Ulkn' Is',Ix- V- Z- *The attki,7 cf -.ritamda as a TAln-rpA=lnj,, nnd accelerriting factor in nomAl lv,~r", 5bernik nauch. tnv (Post. obl. nauch#-issled. akushersko-ginekol. in-t), Issue 8, 1g/.8, P. lIP-26 Krasnyanskiyj L. M.v Mikol'sk1y. V. it aM Skuhonltnrv, V. F. *Cn t~ie .Y of dst.,!rmining abortive p,rtians of t+,e uterus*, Sbcrnik nauch. trulov (Po:;t. obl. nauch.-Issled. aku3hirs,c-g4.nekol. in-t)., Issue 8, 1948, p. 1(P,72. SC: tr-3261, 10 April 1953 (Letopis 'Zhurn-il Inykh Statey, Nc. 1;~, 191.9). 40' .4 %M %,"bob OZ -Tlqv mK %nq %*V ZTW %0U IGOV WWO 6tt 9PO/"S 1,41W - "Otou/sm gnq% J:o nw~U&*Uob V%jA M064 S% SWJ UOTIUVOS 8,41 .1r4ji 4%w 1 SOM" %*muss nu *IMM9 Q,4ul *MftWv:s--O* du %T%do Ipw 9%=woj **T% --$.a jo uW's w4vi 9 ag " All NTVP';g. %9w1 vM &MON fSAID6110AM ex off luwq*o%g 14"ITOM *A #A., 61j 4V/60 "NIZOLISXITO T*T.*,PQTKuayl, t.k. lart"t's r"atlaso ll*klaila, Okokwa 17 ",39317-30,11W-Amm 1952,, (am 25 1 W 2a Dvpart~% of Bloa&mUU7* Awlew mollad lastitato, in the Lipids uf the Brain Under the Actim of the 7oxia of B. Pcrfrira,:C-nz,,, k. It. FaverenW,, S. Te. 011slitcyn, V. V. Ilikollskiy, Z;hair of Bioche:i and Chair of Marobiol, R3stov Statc Ned Inst Ura-In Bloldhin Zhur, Vol 25P 11cp 2, pi) 127-131 The hemolytic fraction of the toxiij of :3. i-,orfrin -cn3 (1) 4-3 MrOr~:.Cd -,OrI0 Pa313.1 17t bmin Mmjf3 t1han by arv ollwr Unlor t!io action of tt,.e tox!n of I# Vic q,=ntity Of aU lipids exrept diwAnoplaosphatideri incrvavai .1a the '~mj_ 7,110 i, content of other,*iojuble lipido increasc3, Iio::Ably !uc to their h1j% co:-,tent Of PhOIPI)Dr7lch~)Mne forried 2t 'he :dte 0~ 110 aff-ct!orl or lul action Of the lealthibane ,)n lt-cithin. A3 a reitilt -)I z~ ~iccjric reaction of nerva ti7muc to the toxin of 1, '.he canto.,it c,.' c,_,rcbroaIdc3 incm-33(.3. CCA ILrIr .rj) NIKOVSKITs V. V. MIKOLISKIYg V. V.: "On the origin and role of the h1&~-molecidar aliphatic &aids (624) in the animal orgafilam. 0 Rostar State Medical Inst. Rostov n& Donu, 1956p, (Dissertation for the Degree of Doctor in Y-edic#l Sciences) I M letopts' No. 28 1956 Moscow Sourcet KnI!tw TT!~!SjTj- Iffe: MMTALWAt N*A,g ORMEOVA, L,K, Meet Of leStalaC rOU&SIM 0u the llptd comp"Itlem of Us ble" a" Ilver 16 rate- 7drobloktim,ghwe 31 8*,61&776M 199, (Kim 13t5) Is lapa"actO of Blechendatry ~M bputmat of meet"Solea "A ftdieloff of the lbetew-u-Sm MAlml rustitate" (Lum? (UDIATIM-PETSIOWGIM 000) RiXGLISKIY, V.V.; 11KOULOYL, N.A.) WUHA-KOU, L.H. Dyrpsics of unsaturated fatt)r aoidar, of the blood in, patients subjected to mdiotherapy, Ked. rad. 5 no.12sl~-17 160, (MIRA 140) (FATTY ACIDS) (RLDIATIOU-PHYSIOLOGICAL ErF=) IK Ir-T OTALWA, S.A.;. RIKULta-r-Ti..; CMnwMTAS T'.K. W4104100 Of MJIkY w1de to the 'blood of normal wabjocto, Toy, md,kbl& 6 noW340,10-f 160, (KIA 1315) 1, Mair at Aleahomistry of the Rostov Ibdical rutitutc, (YOTT ACOS blood) KILDLISKIlr T.Y.j P-lBTSOVA, G.V. --l 19fr"t of 1-irradiation on the formation %C pancreatic enzymos. Vop.sedAhim. 6 no.40654M JI-4 c6O. (KIFA U93) 1. Cbalr of Siochadstry and Cbair of Radiology~ Rostow Kedical InstitoUe (PWRIM-45CISTIONS) (Z QAT3-FMIOI=ICJkL Eff=) 111OLISK17r V,V, SUVIlfied wrtbad for th* #Mtheele of oC -kat*Clut&rfa sold. Lab~dele 9,no.3t29-30 Mr 163. (lapA 16(4) 1. Kafedrs b1oftiall ftost6vskogo mWitainakfto, Instituta. (GLUrAltIC A%qD) GIVSKTS, K.S.; NIKOWSKIT, V.V.9 SUMOV, V.G. swir-"Joint operator motbad in the theory of wavegmi"s. lkdlotekb. 1.*Ioktron. 8 no.lDrI796 0 163* (NIRA 16tlO) state ct tj.~, 1:"jdy 'rLE7 1 7 7- LV - F.. Dtibligning i; 1-ngituditil-Ill -mAitrillitted WiviekIbn "4C) tj I)ta elektri 4~ 05'. 1$- 415 il~~IjinjCular way mu_ 4- a-t anti nu a In-n-ul A-pi-evinuo gi.11mil'-w-ork. (Rad. i V4- 9,: no.- 8, 1345); thiv articb-, prvir,-n. a~ a physical Intorpre- -to xl-~, ct-4114f -#A tr PrOPAS Do flPfls T pxxil-16-4 ~-medem~ t o- tiot conouta for -th6ixe and athr, t ipropaga ua pp rer rlti~ 9i se and paramct,-~r a ar,t! 1 .4 not c: orlqtar~t 'lver tho roq a - at tion villikritv of physical prr)~Cp;,f3pM in th~p rm~, tl:zg i~4 r-w.;iv,,gu0Je ferrite '"eir and the rotator ~r. n s t ru c 0 o n c f t lie f e r rt-,i66A w v - se r I p c r ac it v r, L a - av(; C)-fac to r %re d Tmf- C'~q IV I-rom Amd I tables. A F'TCQN: wune 00 C: cc v9Mixr64 L: i C, S UZI i- sov. clo 1 0 y .~5 . EAT(d)/E,4T(l)/T/,E4A(h) Lelf, (c h_Z8Q=6 Arx NR: AP50Z76zz SOURCE CODE: 11 RIO 10916510101011/199 z/ 1999 AUT1,10R. Nikol1skiy,,_Y._-_.Y.; Sukhov, V. G.; Korniyenko, D. L; Orloy, V. P. 4~4 % 7- none lril'LE,; Calculation oi a rectangular wavezuide filled with ferrite or ferrite and' diclectric and magnetized longitudinally 5 X: Radiotakhmika i elektronika, Y. 10, no. 11. 1965, 1992-1999 TOPIC TAGS: rectangular waveguide, ferrite layer wavegulde, dielectric layer vravegulde ABSTRACT: The method of_!iEe1!-funct1cn9 used by the authors for designing rectangular waveguldep containini-lerrite rods (Rad. i clektronika, 1964, 9, 8, 13,15, and 1965, 10, 4, 618) is extended over these configurations- two ferrite s trips adjoining the -wider walls of the wavegulde; same, ax1joining. the narrower c(Ird J/Z UDC: 621.372.853.2.001.24 L 7813-66 ACC. NR: AP502762Z Mialls; ferrite rod in a waveguide filled with a dielectric of 1, hollow ferrite rod, dielectric utrip between two ferrite strips; ferrite strip between two dielectric strips. Curves of the prop-agation constant, losses, etc. , for quasi- TE, and quasi-TE,,, modes calculated on a digital computer are presented. The Mathematical lnterp:retation of the. elGctric and magnetic fields In a ferrite- containing waveguidt. in cHocussed. Orig. art. has'. 8 figures, 3 formulas, and 4 tables. SUB CODE: 09 SUBM DATE: 2,0Ju164 ORIG REF: 003 Card Z/Z Rikollakly, "!!ewlSy .__ _ _Y;0lmIrovIch Antennas (Antaww) moscow, ra-vo, w"zow, 1%6. 0 P. mum., bibuo., tabus. Errata slip Ineerted. 15,000 eopits printed. Textbook for vW44mte studying at electrotechalcal institutes. or comwinLeations. TOPIC TAGS: antamep tatems, theorys *at"= reillation pattern, anUmm couff antenna Sagimerims MWM AND COMM: This book has been approved by the USSR Xlnlatry of Compunics- tione for use as a textbook In radio "entering institutes. The book contalms standard satertal om the course *Antennse and feeders". The principles of de- signing mltt-pwrpose mA multi-wevebmad matennes are stressed. The usual tbao- retleal problaw sw& as principles of electrodymmics, elementary radiators# e(pdysleut circuits, wevagaidWo, md otbers have been ellainatcl to We volume, S. A. Shlpkov road the ammacript, V. 1. P*Ildsher prepared a mmber of graphs# 0. Z, Ayzemberg pmavt" commiants and advices and A. K. Model edited Uw booke TAM Or Forword - 5 Introduction - 7 Mitt A?1502678Q Ch. 1, Clactrodynadc Primetples of Antomm Tbeory - 9 1. Treasmittlag MA tIMITIM emutam" - 9 2. 3100"Am redlatorm to mateass theory - 13 3. Avero4p pme. balaws " esteem "givaleat cIrtuit - 19 U. . so" elfttz m $sand a thaftmas applied to antemm theory - 24, 5. B"ia Charentieftsties of t"nswIttIft matemmiss . 26 6. B"Ic charecterlettes, oC recelving antemmais - 34 7. On the qWftlmto mad strIct antemms theory - 42 11, IffectIve DIrect1vity of 1"Istor Systomme ad Auto=& Struaters 1. Autema as a comblustion of -alamenterf reilators 2. 01screte reftator slatomis - 50 3, UONVING of 411mam systomms - 55 4. couttwom distribrAttow - 68 5. Ant4um &bow a reflactIng surface - TT 6. Weamm parmAmm - 85 7. A periodic awArce d1stribition - 9T a. Effective directivity control - Im 9. Classification of sstm~ WCOALms to atzmatum - 2a Cb* M. TrOOMMISMICS Lima - W 2, Verlous types said oomme pg rtim of the trammed"fos Uses - IV 2" Descriptlan OC trammad"Iss eam"Ums - 133 34 circular "agram - VA It. Ustemag Ila" - 132 - ACC~ Hit; - AW-~0216780 5. Important transmission lines and their elements l66 Ch., IV., Linear Antennas - 1W 1, Antennas similar to the elementary awe 180 2, Linear electric vibrators - 190 ), Linear magnotle vIbratore - 207 4. rateractlan of linear vibrators - 220 5. Systems of linear vibratm - 225 Ch. V. Surface Antename - 240 1. General remarks - 240 2. Korn antennse - A2 3. Lens antennae - 254 4. Kirror antennas - 269 Ch. Vt. Traveling Wave Antennas - 289 1. Gederal conceptions - 289 2. Uninterrupted Unew distributions 303 3. wIttelt"Wat antenam - 313 4. Surface and cavity antevow - 328 Cho VII, Puwtlowa Pocullwities of Antmmae 335 L Fledia communication and broadcasting antens" 335 2* .10dw Muteness - 341 30 *o1mr tip" at am~ - 549 Appndlx I., MUstion flold of a age -to Smuft1lud alawat - 355 APPODUZ it* ftble or tmpw#mo" - so 0=2 0q/ AM Olr*b66/ am art oa/ 14 U,SSRI Yarz. A%niMalt. 7auttIL-, C7-L Abe Tour: Ref Zhur-Biol., Ho 12, 19589 54748. Author :_Nikolfskly V. V., 3yuzyumova, L. U. Inst Itot gl-ven. Title t On the Effect of Yeast Obtained by Hydrolysis upon the Immunological Reactivity of Calves. Orig Pub: Tr* In-ta biole Urallskiy file AN SSSR, 19579 vyp. 4, 135-139. Abstract: The administration of hydrolyzed yeast in doses of 50 to 240 g. daily, between one month and six months of age, exerted a favorable effect on the growth and development of calves* The average daily weight gain of the experimental animals ex- ceeded by 100 to 120 g, that of the calves in the control group. The calves of the experimental group reacted to the reiterated injection of the paratyphoid formol-vaceine by a higher titer of agglutinins. Card 1/1 22 NMLIBKlr, Y.T., professor, doktor retoriuarmykh nsuk; STUITUNDTA. ro-K.. ....... wwm~q NNIFIMT-notrudalk; IDSTMA, L.L., aspirant. Watummal Inimulty of calve@ to dleeae*e. Taterimarlia 34 me.1c 29-34 ja 157. NWA lot 0 1. ImUtut b1ologti Vrel'skago, filiola AkMeutl mmk SSSR. Nalve~) (Tuffinity) Klg&'ULT~ V*~To- TRIYO*ffk. At #prof ~,otv*tatv*W redo: IZNOMOVA# cjktwml diamwe mistame ta C&IT" &A "we of Imrawtse it] a pr1rods ost*iitvom*l restatoatm4tt arpalms telfAt k MASISINdIft I Pu4taft as POT"Waltas Sverdlovsk. 19580 Ulp. (Alwd~ll& amok ~. Mrallakil filials *erdlevoko lmtltut 11142061. RQ.10) (*=A its 12) (calvis) (Imunity) NaTOL'Sayl, ;: vf- mLafektayia ta Imm=-Iogichns Reaktivnost' Tvari=oga Orgaai=u" Mey, lzdatel-tatvo, Ukrainiskoi Akade=li Sel'ckokho%faiatvenrqkh Nauk, 14-4- pages-, 1,100 copies." Veterltarlyn., I Vol. 38,, No. 1p p. 91, i96L. I f Uraam-ri-v~V., r7-XVa-KG, 1. F KAMM E. L. and GAIWAU, T. -1. (Correapgnding Hmber- of UASKW 2~~niaa'AcadamT of Acriculturma ScimmojL/, Prafessoro GarAldatax of Vbterinaxy Scianceac acd C4md-fdate Qr siougicma scianceaf uAsm)o Wacticus Vastraeateritis of swine Yeterlaarlyet Vol. 38t No. So August 1961o pp. 30 NIKOLtSKlY ,Vladimir lvlat:t I ; -.C`Z~ Ir.-','!-.',Fiy , V-N, v T, "4* (Infecltiou5 (vl.rus) gastroent.,eritir, of svine] Irifsk*siore. nyi (vinisq-11) gastrcen,~erlt zv"Lei. Ftavp IzAI-Y,3 Ic)64. (d p. (1,1 T 7 A 17: *9) _LTjKqk9!~.IT T V . proro EMMKO, loPop kand* voterin. nauk; ROMM, 'A 101, . - I.-- K.Asp Mnde ireterine nauk; GAYUWiKA, T.V., kand, biolog. nauk InfectIms gestroont4ritis in isw!no. Votorinarits 36 no.St 30-33 It 161 (KIP-4 1811) I* Ukrcinskays akadamlya 4allskokhozymptyannfth nauk, 2. Ch-lem korrmopmdent Ukrainskoy akadamli sollskokhozyaystrennykh nauk (for Kikollskly)e OSADcHAykr rtr.., aspirantl MIKOLIMUr, V.V,, prof,,, rA=hqy rukeyoditell raboty 9mreUon or cytopatkiogento Wsts b ewp during Uw seat@ fem of hmm-rbWo sspUcemlso fot*rlnwtia 41 W.9129 8 164. (MA IftO 1, Tmainsksys ordona Trudovogo Kressecot 'I I sellskokhosM- stvenmya skadadyn,, 1-TrIT'Inly, 7. V. gl~oll6iy, V. V. -- 'Yessu?emnt of tho To-ror of vametic her-l'W"llty and Dielpetric P~-meabllltv of F,~rrltes." "In *i!rher Fducaticn Voscow Crler of banin Avlatlon Inst ironi retro Ctc!zhcni- Vicize. "'Osccw, 1956. (TIAss-ertation for t~~. D,!tmee of Cwdldate, in T-chni-al 7plence) So; KnizWtavq .1,Atopis', No 1":,, 1711:6 USiP. / Stdiophysics. Radio Itesaurements. -#;a Jour i Hof Zhur - Fizika. go 5. 1957, No 12684 Author Nikollsidy, V.V. Inst I 'lot gLven TI tle 9Meagurements of the Parameters of Ferrites at ilicro Irequencies. Parts I and 11. Orig Pub #Radiotokhniix I elektronUoL, 1956. 1, No 4, 447-468 Abstract t7he author considers the problem of the measurcmat of all components of the mapttio permeability tensorA, aad of the dieloctrlo-oonstant tensor - of a ferrite from the incrorant in the natural frequency and bandwidth of the cavity resor4L- tor (its complex natural frequency). For this purpos*# it to necessary in principle to obtain four Independent complex inoremants. Me variation of' the conditions is reached by Card 1/5 USSR / Radiophysiog. Radio Measurezents. 1-7 '&be Jour I Ref Zhur - Fitika, No 5, 1957, go 12584 Placing the ferrite speoLmen in various portions or the resonant and maguring the dirgatimn of the magnetizing field 9-1. It is desirable that each reaction of the re- sonator depend on the minimum number of quantities to be dOtOndned. For this purpose, U10 specimen should be small r*)AtLv* to one or GOTOM1 dimensions (for example, a thin plate, a thin cylinder# a small sphere). These types of BP*OiMWS are amlyzed frai the p6int of view of aimplici- V Ud intensity Of the resonator reaction that U*y produ- ce, Ihs principle of perturbation of the resonator is Co- noralized to include gMtropic media', With thigs, a rj_ 90rous formula is obtedned connooting the Increment in its natural complex frequency with the PArknotors of' the pertur- bation region and with the vectors of the initial and per- turbod fields. The formula is applied to the measurement problem. Card s 2/5 U58R / Radiophysics. FAdio Measuromanta 1-7 ". . _ '- 1;- 1957. Uo 12584 USSR / Hadiophystax. Radio Itoasurwonts, 1.7 Abs Jour Ref Zhur - Fizilm, go 5, 1957, go 12684 Cotl4ulatLons are Given. along with for=Alss, Ibr these case@ The problem of the permissible disawater of the cylindrical speolmett is invoetigated. Oaf& are given on the construation of resonators that can be adapted for the measuramt of all the parameters of cylindrioal ferrite speoi a Tfw r*gul - tant experimental curves show that the disorepawy between the measurwent results of the components ofA- and c , wtwn usitLG the resonators. do not oxased 10 p*rcent. Card 5/5 Al / ea I. " _;A-' IV. 109-7-3/17 Card AUTEM Nikoltskirf f.T. TIMM -T&-TC-Uja-fj-o-n-_ofthe Phase Shifts of "trOPLO DIscontl=Lties in ftys Guides by means of' the Perturbation Method'a (Usabet faxovykh edvigov girotropqkh neodnorodnoster r volnovods, astodoa vow=hcheniya). PMODNALt RadiAekhnfta, J Xektronikaj, 1957s Vol'.11t Nr 7t pp.833-842 (USSR) ABSTRACTs The principle of the method 1= been considered awd Ort.- eralised to include gyTotropie.media in a number ofautgorat works (Refs.2v 3, 41 5 and 6). In.the present work the method is applied to the problems of gyrotropic discontimai- ties in waveguldes. An an4ysis is ce-rriel out under, the assumption of the so-called quasi-stationary approximation vh1oh limits the dimensions of the gyrotro ic regionB to values thA42 the wavelength of the system. Ke waveguide con- sidered (shown in Fig.1) has a gyTotropic discontinuity- Vl. ,which disturbs its regularity. It s assum d that initially- -the, fields in the waveguides &re io and, t and that its ,Dermittivity and permeability-.Are and. In the per- iurbed state the fields, are -9 ands-olt and-UtRe"permittivity and omsbility are expressed. tensorialIK (as given by- lqa. The trOJUNISOLOML coefficient of t system can then (rig-Z60 log-T-3/17 Calculation of the Phase Shifts of Qyrotropic Discontinuities in Waveguldes by means of the Perturbation Nethod. 3) A fertitei, horizantal vertically magnetised rod, Fig.2B. ( If given by, Zq. (25 ) ~ - 4) A ferrite sohere magnetised along wW of the 3 axes ~p given by Eqs.(26) and (28). 5) A ferrite diaphragm either vertical or horizontal (Flgs'.3& and 34 )q f given by Zqs.(31) and (32). Similar expressions were derived for,a cylindrical waveguide with a diso (Fig,4at given by ZQ- (33) ) and a ferrite sphere UPig. 4 go 1P given by Zq. (35 The phase shift of a ooexial line with a ferrite ring (rig.5) Is expressed by Zq.(38). The above formulae were employed to determine the phase shifts for some of the systems and the resulting values are shown in the carves of F1,g.6. The paper contains 6 figures and 6 references, 5 of which are due to the author. SUMMED: October 9, 1956. AVAILABLE: Library of Congress. Card 3/3 109-8- 13A7 AVMRt likellskIn 74'70 TITLLPt Determination of the ligen Values and Puzetiona of Gyrotropic Media, by the Met 0d of Buccessive Approximations. -rf,,..%;akhozhdeniye, sobetvennykh. znachaniy 1, futktsiy g rotropnykh sistem setodoin pool edevatel, ( nykh. priblisheniy) MIODXCLLt Radiotakhu*& L Blektronikar 1957t Vol'.11, Nr 8t pp.1074-1077 (TMSR) ,Tt This yaper proposes a method of finding the natural ABSMO frequencies of cavity- resonators and the agation, con.- stants of waveguides, which are partly fi M with a gyro- tropic or isotropic medium. The method is based on the accurate formula for the perturbation of a. cavity reson&tor or wavoguide which was give b the author in his previous works (11 2 and 3)'., The fo~aua is in the formt n f, An 01 n. f (a, Ll IL itare INtr, Is the perturbed elgen value for a. waveguide or a resona AU. the perturbed eigon f=ationav A, and a CW& 1A I AUTHOR. Ifikolskiy, V.V. 109-3-5-11/1? TITLE: Determination of the Internal Field in the Perturbation-Method Analysis by Solving the Diffraction Problem (Nakhozhdcniye vnutrenaego polya v metode vozaushcheniya pri pomoshchi reaheniya difraktsioanoy zadachl) PZRIODICAL: Radiotekhnika I Zlektronika, 1958 Vol III 'Nr 5, pp 9JO - 697 4USSR) ABSTRACT. A homogeneous plane wave is assumed to Impinge on an Isotropic cylinder of radius r, . which is oriented alonZ the axis y . The problem consists of finding the field inside the cylinder (the refracted field). If the electric vector of the incident wave is parallel to the axis of tho cylinder, as expressed by Xq.(l) the scattered field and the refracted field are gilrgn by Zqs,(35 and (4). respectively; in these equations, k - wleg and e and p are the pwameters of the cylinder. The fields have to satisfy the boundary conditions expressed by lqs.(5), from which it follows that the coefficient bn can be expresseA bv Eq.(6). On the basis of the Maxwell equations and 9q.(4)tit is show that the magnetic field :Inside the cylindcr Uqrdl/3 can be expressed by Zq.(7). If it is aosu=ed that the maenctic vector of the incident wave is parallel to the axis of the 109-3-5-11/17 Detorimination of the Internal Field In the P*rturbatioa-method Analysis by 5olving the Diffraction Problem cylinder, the internal magnetic and electric fields are expressed by 3 s.(S) and (9). respectively, and the unknown Coefficient b?- Is given by Sq.(10). If the cylinder is subjected to tRe action of two waves whose directions of agation are perpendicular to its axis but differ by an * Z* and the phase shift between the wavog is cx the = internal field can be written in the form of 1q.(12). ihe above equations are used to aralyse the behaviour of a vertical isotropic cylinder plaoed in a rectangular waveguide. The position of the axis of the cylinder In the waveguide is described by co-ordinates z - z I am X W x., (see FiS.2). It is shown that for this case the field inside the cyl W er can be expressed by Sq.(14). it is also shown that the transwissica coefficient of the system is expressed by Zq.(18) or approsiuately by Sq.(16). The above analysis did not take into account the finite conductivity of the walls of the waveguide. This effect can be taken into account if the coefficients a 0 and b. are replaced by corrected Card2/3 coefficients A. and Bo I which are expressed by Zqs.(21) Determination of the Internal Field in the Perturbation-sethod Analysis by Solving the Diffraction Problem and (22). respectively. The above analytical results were employed to evaluate the transmission coefficient V for the following system: X/s, - 1.4 11 6/60 a 9 9 d/a a 0 to 0.2 (where d is the diameter of the cylinder). The values of BO as a f anc tion of MA for the above cons are shown in Fig.3. IFig. 4 represents the values of the transmission coefficient 't an a function of - ndA 9 while Fig- 5 represents the values of the coefficients which are proportional to the amplitudes of the field on the surface of a cylinder situated either in free space or in the centre of an Rio waveguide. The paper contains an appendixt 5 figures and 8 Soviet references. SIMAIVT : December 7, 1956, AVAIUBIX: Library of Congress Card 3/3 1. III C_ & &UTHOR: I. NikolsTrJZ' Ir --7,-,. TITLE: The 3implest Case of Diffraction of a Plane Wave from a Gyrotropic Cylinder (Prosteyshiy sluchay difraktati pl,)r;koy volny na girotropnom tailindre) PERIODICAL: Radiotekhnika i Elektronika, 1958, Vol 3, Ur 6, .pp 756-759 (USSR) ABISMACT: The problem is formulated as follows. The axis of an infinite cylinder having a diameter d - 2r, , coincides with axis y I. The permittivity and permeability of the cylinder are described by the tensors expressed by Eqs.(l); the parameters of the surrounding medium are c 0 and ti 0 A plane wave propagating along the axis z impinges on the cylinder. It is necessary to find the field inside the cylinder and the scattered field. If the electric vector of the incident wave is parallel to the axis of the cylinder, the incident wave can be expressed by Fq.(3), where the angle q is read in the anti-clockwise direction. The internal electric field is given by Eq.(4), while the external field is expressed by Sq-(5). The magnetic vectors of the inner and the scattered fields are then nxpressed by Eqs.(6) and Card 1/3 (7) respectively. The coefficients b a and a a or Eqs.(4) The Gimplest Case of Diffraction of a Plane Wave fron a Gyrotropic Cylinder and (5) can be found from the boundary conditioas expressed by Eqs.(B) and are in the form or &qs.(lo =4 (11) respect- ively. If the incident wave is such that its magractic vector is ara1lel to the axis or the cylinder, as expressed by SquJ1231 the Internal and the scattered fields are er- pressed by Eqs.(13), (14), (15) and (16); the unknovm co- effi-_ients b~ and a~ in these equqtioas ari- erpresscl by Eqs.(17) and (18) respeztivell If the diameter n' the cylinde-r is very small, Eq.(65*can be written as Lrq'.,(19) and Eq.(10) is in the forna of Sq.(20); from these it follows that the magnetic field inside the cylinder is in the form of Kq.(6a) which is in agreement with the formula obtainel by Subl and Walker (Ref.1). For the case of thp incident Card 2/3 I -, ', -" '-1 OWN The Simplest Case of Diffraction of a Plane Wave from a Gyrotropic Cylinder wave having the magnetic vector parallel to the axis of the cylinder, the internal electric field in a thin cylinder to in the form of Eq.(15a). There are no fi6ures and 2 refer- ances, one of -uhich in On,*,lish and one Soviet. SUILLITTED: January 2 9 1~)57 1. Electrozaanetic waves - Deffraction 2. Electransgustic waves - Analpis 3, Cylinders - Applications Card 3/3 SOT-109-3-6-15/2'r AUTHOR: ITikollskiy. Y__T__ TITLE-, A Transverse Ferrite Rod in a. Rectangular Waveguide (Poperechnyy ferritovyy aterzhen' v pryamougol'nom.volnovode) PERIODICAL: Radiotekhnika i Elektronika, 1958, Vol 3, Ur 6, pp 826-828 (USSR) AB3TR&CT: The problem of a magnetised ferrite cylinder, parallel to the electrical vector of the H 10-wave in a rectangular wave- guide was dealt with approximately in a number of works (Refs. I and 2). Here the problem is considered more accura'-17 (thq second approximation) and the solution is suitable for engineering applications. The electrIcal field of an H 10-wave impinging on a cylinder (see Fig.1) can be expressed by (Ref.3) Xq.(l), where : x0 - wNoo'r.070 ; X -,ff/a ; ,~ - are cos(%/2a) and sin 4~ - 1r1/x, For practical applications only the first terms of the above expansion are necessary so that the field is given by Eq.(2). The fields inside the cylinder and the scattered field (without taking into account the effect of Card 112 the waveguide walls) can be expressed by (Ref.4) Eqs,(3). SOV/1-vi-3-9-12/420 AUTHOR: Ilikollakiy. Y .76 TITIZ: The Variational Principle as Applied to the Son- Absorp- tive Gyrotropic Discontinuity in a Naveguide (Tariatsionnyy printsip d1ya nepoGioshchayuahchey Sirotropnoy neodnorod- nosti v volnovode) FARIODICAI: RadiotokJinika i elektronika, 1958, Vol 3. Nr 9. pp 1207-1209 (USSR) ABS"TRACT: The system considered is represented in the -_"!figram on p 1207. On the basis of the PoInting theorem, for the space limited by the two cross-sections 31 and 5" (see the figure), it is possible to vrite two integrals in the form or Zqu.(l) and (2), in which S is the surface en- closinG tho considered volume V q While IL and c are the tensors of the medium. Since the principal waves of the type E i and H . fulfil thq conditions expreosed by Zqs:W;ttthe two cross-sections it is Donsible to -.,rite Eqs I and (5) in the form of rAIC't;.(4) -and (5), -ahore P and z repreaenU the reflection coefficient and the transmiuaion coefficlont of the i3j;Aent V~apecttvei .~. if the looses in the re-ion V are nigli ble, gqs.(I) and rez i'qn.(81 and (9), w and 0 are given (2) stilt in L here Card 112 .;07/109-3-9-12/20 The Variational Principle as Applied to the Abzarptive Gyrotropia Discontinuity in a 11aveGuide by Eqs.(10) and (11). ftpreusi)na (7), (8) and (9) permit the determination of r and v aince the functioi-,als t and t~ assume extrese values I if the losses in '%-ohe region V are negligiblo. The paper contains 1 figure and I Ezaglish reff-rence. SU'B=TTEJJ: July 59 1957. Card 212 AUTHOR s -, Nikol I - SOV/109-3-12-11/13 TITLIK.- The Problem of 1(oa-hoxog*n*oux Gyrotrapic N*d1a (K voproau o neodnorodnyi:h g4vtropnyich aredakh) FNIODICAL: Radiotekhnika i Zleictronika, 1958, Vol 5, Kr 12, pp, 1518 - 1520 (USSR) ABSTRAM The paper deals with an ultra-high freque=y model of a sodium which Is in the form of porous ferrite or dielectric containing ferrite particles. The wdtl is in the form of a system of Spheres which are uniformly distr- ibuted in a filler (see the figire on p 1519). The spheres are exall. in comparison with the wavelength and. therefore the problem can be solved by using the perturb- ation method in the quasi-stationary approximation. It is assumed that the material is situated between two parallel planes and- forms a resonator. The problem can-- siats or determining the change in. the natural rr*quoncy or the resonator whea spherica2 "impurities" are iatro- duced in between the planes. Lf the magnetic perturbation alone is considered., the frequency change can be expressed by Nq (1) (Ref 1); No in Zq (1) denotes the initial Uardl/2 magnetic field, V is the volume of the resonator and SIDV/10~.-5-12-11/15 The Probles of sion-hosogoneous Uyrotropic X-tais, 14 and k are the components of the permeability tensor of the ferrite. rron Zq (1) it in found that the ch3zge in frequency can also be expr*nsed as Nq (4). where g, is the permeability of the dielectric In the resonator. Since the frejueney chaugg. can also be expressed in terms of the components of the tensor of the equivalent permeability (see Nq (6) ) it is shown that these components are given by lqa (75 and (8). Similarly, the third component of the equivalent tensor is vWressed by Nq (9). The problem of a porouis ferrite can be solved ia the same way and it is shown that the equivalent tensor meters are expressed by Xqs (11), (12), (13) and (143"where e. , IL, are the permittivity 9 and permeability of vacuum. There are 1 figure and 2 Soviet references. MMMITTZ : July 2 * 1957 card 2/2 AUTHOR: Nikol'skir V-T- sov/to9-4-4-zi/z4 TITLIZ: On the Theory of a UHF Ferrite Amplifier (K toorit SVCh-usilitelya na ferrite) PERIODICAL: Radiotekhnika i elaktronik&, 1959, Vol 4, Nr pp 726 - 728 (USSR) ABSTRACT: The paper considers one of the possible ptaciplas of constructing an UHF amplifier employing a ferrite material. It is assumed that the homogeneous motion of the magnetin- ation in a ferrite, when subjected to the action or the field, is expressed by: -0 H 29' + Zh' cos (at + + A cos (2ut (1) = 0 1 2 + 92) The nagnetisation in expressed by Eq (2) and the equation of motion is in the form of Eq (3). If the expression for the magnetleation it substituted into the equation of motion six equations are obtained. These are represented by Cqz (5a) and (6). The equations can be employed to investigate the conditions inside a cavity resonator. Titus Card.I/JV when a piece of ferrite in placed in the cavity, the complex On the Theory of an UHF Ferrite Amplifier SOV/109-4-4-21/24 frequency of the resonator undergoes a change which to expressed by Eq (7). This equation in employed to investigate a rectangular resonator with a transverse ferrite plate; this is shown in Figure 2. The frequency change for this systent in expressed by Eq M. The quaLLty 'factor of this system can, therefore, be expressed by Zq (10), where: ILJ- - - ($L 2 _k2 From Zq (10), it fonows that for 0 or the system Is non-r*gsaerativeo The condition or regeneration or self-excitatLan in obtained when the denominator of Zq (10) to made equal to sero. The system can, therefore. be used an an amplifier; for this purpose, it should be modified in accordance with the diagram of Figure Card2/0 RED Ll V, ly , V- 72 -i re-I (Electr fjoj~ tier-ryl 64 Vo 7 -,,, 9 To] I z~i 3. e 4 A.C. kandotAkIm.nank. mtsonitatc Kt&X. A.*Xo # zvd* Erhmory of ttw olectrawgietic f Iola; mauel, for atudesto of redlo eMlaosring] Tworils olektrompiltzoga, polls; itsbobnae potable d1lo studestow redlotakholobaskage fokul'tatoo Mookwoo Goo.onercolgd-wo. 1960. 430 P. (MIRA L4:1) Madle-Smad'books. mommle. *to.) (Blectramovistis theory) HOR TITI E, 011 C , A r. 1', Lj ABS'MACT: and t,y k V I ~J CvAal, 101`1: for "he jo R - o r Card 1/13 S)0.01 W~j f c c,:, nz I ra c. r n;, Vi on slo,,~j Wave-- in a Eq. may J,t-, r-sl,wrltto~ri in the for7r,: TI iv oo I utu ion o #L7 E (1. (5) 1 s 1~ = A~+e-Jl's + B~-ejrj For real F , Eq. (6) i3l,o-,;,3 a sup(!rpocl~,lon a*, whIch, on the basIs of Eq. (2), ray 1),~ callA sta t ic . (1) Sloa clectromap 'nictic !ww,es M a j,----,irotrop-'c medium. The solution of' equations, *whi,~11. -Mrac'er*ze ~hf~ Card 33/13 On S~lo,,.i Wa'ies In a Gyrotropic -:4/2 3p-eadlng in a f,,jrotroD!c (more r a o c: o n sa nt in the d'.-rection oe in the x ca-d 4/11, and yo 41 Ecls. (1e)) and 17) ar'e a 11-11 1,Ir tO E()-'3- at"(1 From it resullun that thf,~ mai-mA.1c fl,~-ld (j," th~, -wave under lnv-4--ut 1~,at tot-, may b,-- a static wa,.,(-.-. It., 1;ropajr,at-lon constant F 1:; the form: J.- (2) Gyrot-ropic cylinder with an id,~al2y ,ase the scalar functl shell. In this c on IP Card 7/13 given in the form: -,-,I (-j I On Slow Waves In a Gyrotrol.),lo Mf~dllur- f I ~ Is to The s~!alar flinctiloy', following, bmindary 11,rilts condition: G,I 1) r whf~rre R is a radius of' l.he cylllnd~-~il. components ar- obtatrv~d A"rcm Eq 16) (2, Card ~1/1-1 j 1 In a 0 where GyrotroPlc cylinder plaCf-,'d cOaXt,".11Y 1-11 "'It" '('C.' "y Lj,,! trarMCcidental con(jj,(., tinp pipe. Foil 0113, ca3f~, f Om t hoc equa t lon. In J" Xx.J, N,l (1.111) n thrrju:~,h (5) Xagnefos. ta tic ()Ile 1 11 t, t lorij . A t 1 () I I m.,; poIntj p f r) 11 jjy any c" 1-110 !3Yst,(-' ~rj F, ld,-~jj (),- ri uI ri larv--s pla" -Iiy p 0 t r"i I 13V 0'-' 1' Card .11/ dl ittinc 0 n o -a ,via v i! s 1% a Gy, r or o pc Ives a re.,~ona.;or, c cc on Siow '.iavcs in a Gyro,'L,-ropic me(ni.z.-i SU-1:11MITTED: "( 7191 SOV/109-5-1-4/2c) attentLation, the quality factor of magnetkostatic resonators, etc. Systems in the shape of layer or of bar, as well as cases of transverse magnetization, may also be studied. There are 6 references, 1 Soviet 5 U.S. The U.S. references are: L. R. Walker, Ma~,neto- static Modes In Ferromagnetle Resonance, Phys. Rev., 1957, 105, 2, 390; P. S. Epstein, Theorj oil Wave Pro agatlon In a Gyromagnetic Medium, Rev. Mod. Phys., 1959, 20, 1, 3; M. L. Kales, Modes In Waveguldes Con- taining Ferrites, J. Appl. Pivs., 195?3, 24, 5, 60'j'; P. K: Tien, 11. Suhl, Theory of Travelling-Wave Para- metric Ferromagnetic Amplifier, Proc. I.R.H., 1958, 46, 4, 700; 11, Suhl, R. L. Walker, Faraday Rotation rf Guided Waves, Phys. Rev., 1952, 86, 1"--'2. D-ccember 22, 1958 Card 13/13 _9 :-3 0 AlY1111OR: _ILLkollokly, V. V. TITLE: Theoi-j of Forromagnetic Amplit'lero Bl:,142d on th,-, bl,:,- turbance Principle PERIODICAL: Radioteklinika I clektronlka, 1960, Vol Nr 1, pp 11~1- 1119 (UtSR) ABI`j~TRACT,. In this study the. analy,.313 of' tra-jL-llrj,,-, -e;av~~ aill Vi-rrr)- inagnetic amplifiers li explaIiied an th,., La.,J~~ o1' ti,~ dtaturbance pr 4nc 11)1(!. Vic- 111F ~iupply changreo the magnetic suscc-ptibillty of considered to be dl.-,turbance of tlv.~ Ilminai-j Constdcratlori.,3. vi., expr-~;Aon:~ rov 6,e- supplementary magnetization t.-oriponcnt.,~ aie j,tvt,Tj !'(J~, two caseo: first, when ferrIlle 13 urider thl, of two f leldo -IT and it 4) an(l :,e,-,f,rjrJ, r, , it 1,,i affected by one field 11 (a n 1. yIt L-, that the real part of the map-tictle perneal.,111A.- i),` tlv~ Card 1/6 medium has not been ch,11117,q.-d practically 1,:/ Al'A111,141ni" Theorj of Ferromagnetic Amplifiero B-A.,.;tA I 9"j) on the Disturbance Principle Sov/109-!) --I - field; It remainti conatant rit the prinary fic- I i1 d I s t r button. ThIs permits one to Identify the prim:iri rl~-Id with the disturbing field with ail accuracy lip to a spatially conatant factor. This 13 valid Alor the reocinitom as well a3 for waveguldes, the lat-tf~r 1-~avir,;: a transver3ally di3tributed field. From th,-- WmrifAl vqxiation3 two fundamental ---quations follrjv~. For th- reaonator: 41144, 6.4" where 6 and thf,~ di:~turbnnce and pr1mary frequencies, respr-etively; If0Ij t.he prlm,,iry I'liAd: IN 113 the disturbing magnetization; V0 Is thr-- Card 2/6 of the resonator; V is the domain dlsttjrbari,:~e; ;.,11(1 4) of Fi~~rrom: , I I ,,j I I" r Ik: k-.,~, Af !. on the DL-,t-.m,I)anc(-- Prln~il-!,- ti Is th,~,- ten,.:or of' magnette For 'Uc.~ wa v v 1! 111 d A111. t I e I awl aril. d I "AIII'Lanuu 'ifill -x wave C()k.i,l,l o tvi,-] SO 1A t ],;,, ,I I CI'003 Of t)W ar"d n th- r ,j i veroal cro-,13 otl-ctlon of th,2 domain 2 Re onritor, With "Ori(-~ Wif.~iral Frerp,,, IL'ItUP,11 freqiv,,nc1e3 wIth ,A rlrl~il V1 :-,rv,.v and I* equal to hall' of the freqij,2icy rA' th,~~ r I (-, 1 dIntrodi.Ani, the t2xprossloni of' hf~ i ij,j, I rj bi Part I trito Efj v i '-I I n migniAl al Ion gIvel tramfformations, thf~- i'cAlo-eilm-, e(I-Xition 1-- c E! rd 3/6 N-1ncip-1t, 'tin F sin Wh('1-(! (A) Is the pr1mary fx-equ,,-r,,(:y; a in the resonator attenuation; 0 lo the initial qualltl-,, fl Is ampliturie of -.,3,! - Aon; ~~;-:d of tile system; M n,* t 1;-, at H Is field constant of the Lannor reounance. F and p are taken from the(equation F - Fell(Pr , wh,~re P Is tge fill-in fa,-)r. Al-rztracterls Th,:- terr. "fill- In factor" 'is ~i tran3lation of the Russirin te.-n: Faktor zapolnentya); Y Is the phace of the amplifi-d signal and (D_ correspond3 to M11 Ejoation (1-1 shows that thfi? f~~.angr-, in th~? attklenuat~lon of th,-, resonator as the re~;pons,,-, on the di.;tljrbl.n;:- f 1-1d nriy be pooltive or negative. It depend.-; un tht- Car-d 4/6 relation between the slgnal and dlsti..ri~InF lirleld. Th- Thco_--y of' FeVVOM,,'11',W~t tc At.+ I i !-&, v.- on the- Dl!jturbance Pr1n._,ipJe conditlon (if ampl H' 11w, 1., 11-d by th,: 1 ri,.,l ;;3-1 11':/ ahown In Hqoitlon J(~- sin W, - 2? " ?F) > (1s) -The threshold value of the magnetIzation arld the amplifying coefficlent are given. (3) With "Two Hatural Frequon~-Ies." In this ca!se ,.In analy.71.,3 similar to that in Part 2 Is ezplain,~-11 fox, the :3,yntr~-. di3cusped by H. 3ul,l in References I and 2 of' 1;h,7~ Abstract. The resultant equation chows that thr_~ 'j, t,,:~ r uation I/Q. of the 3y3tem can only decrease. Th,~~ 1- tude of the signal always, ln~~rcaser.. It i a s 11 in 11, i r the thre3hold value of th~.- amplitu&! of and the amplIflinr voefficlent aro ~xplnln,!d. Wavegulde With "One Wave." (5) With Waves," In the f Irz;t case, the amplifierl field o1V frequency/ G) reprooents one of the wavea of tho Card 5/6 system. The oupplying field of the double 1"r-Iii-noy