SCIENTIFIC ABSTRACT MARGOLIN, S.F. - MARGOLIN, K.M.

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SCIENTIFIC ABSTRACT
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MkqGCLIIT, Sh. F. "Investigation of, the Mobility r)f Trenchiru! Plm-,,s in Marshes." Cend Tech Sci, Department of PhysiccmLthematfcal band Tc-c,-,-ri-*c:..l Sci, Acad Sci 3elo-russian SSR, 18 Oct .54. (8B, 7 Oct 54) Survey of Scientific and Technical Dissertations Defended at USSR Higher Educational Instit-ations (10) SO: Sum. No. 481, 5 May 55 MOKHOVP P.D.; KAPIENKOV, I.F.; MARGOLIN, S.F. Combined hydraulic press system. Kuz.-shtan. rjroiz-,. 3 co.3:35-36 Mr 161. (MM 14:6) (Hydraulic presses) 80880 s/i26/6o/ooq/o6/00/f/025 Magnetic Studies of Cr--Ge Xlloys E073/E335 that alloys with Go concontration, abovp 50 have i Curie temperature between 100 and.110 6K and are ferromagnetic between 77 and .110 K~ In these alloys only one phase is ferromagnetiz and is very probably close to the c1lemical compound CrGe 2' There are 6 figures and 3 references, 1 of which is Soviet, I German and I English. ASSOCIATIONg Institut fiziki metallov AN SSSR (Institute of Metal Physics of the Ac.Sc.USSR) SUBMITTED; July 11, 1959, initially. December 9, 1959, after revision. Card 4/4 80860 S/126/6o/ooq/o6/00~_./025 Magnetic Studies of Cr-Ge Alloys E073/E335 the dependence of the magnetic susceptibility on the germanium concentration at room temperature and in a magnetic field of 13 900 Oe. As can be seen, the maximum susceptibility occurs in the region of 66.6 at.0/1') Ge. Figure 5 shows the temperature dependence of the reciprocal of the susceptibility for an alloy consisting of 33.3 at.% of Cr and 66.6 at.0'o of Go in a magnetic field of 10 8bO Oe. As can be seen,above 225 OK the Curie--Weiss law., C X, '.: _- T - (DP is satisfied, where G p = 142 OK point). Using these experimental that the number of Bohr magnetons an alloy containing 66.6 at.O,O' of photographs for alloys containing of Ge are shown in Figure 6, The (paramagnetic Curie data, it was calculated per chromium atom in le is 2.3. Micro- 65, 66.6, 75 and 80 at_% general conclusion is 80880 S/126/60/009/06/00WO25 Magnetic Studies of Cr-Ge Alloys E073/E335 the magnetisation of the alloys was determined by a ballistic method in fields up to 3 000 Oe, by pulling thein out from1he measuring coil, The magnetic susceptibility was measured with the aid of a pendulum magnetometer (Domenical, Ref 3) in fields up to 16 000 Oe. Figure 1 shows the temperature dependence of magnetisation 1 (gauss/cm3) for alloys with different concentrations (as indicated) in a magnetic field of 3 000 Oe. As can be seen. the Cr-Ge alloys have a ferromagnetic transformation 0 temperature between 100 and 110 K. The maximum values of magnetisation are found for alloys containing 66.6 and 70 at.910 of germanium. Figure 2 shows the temperature dependence of the magnetisation of the alloy containing 66.6 at.9b' of germanium for different fields (as indicated). As can be seen, the ferromagnetic transformation temperature lies between 100 and 110 0K. Figure 3 shows the magnetisation curves for alloysoof different germanium concentration (as indicated) at 77 K. As can be seen, the alloy with 66.6 at.% of germanium has the most rapid )/1, increase in the magnetisation with field. Figure 4 shows 7 00 80880 /025 S/126/6o/oog/o6/004 AUTHORS: Margolin, S.D. and Fakidov, E97a/9335 -------------- ~i V-% . I TITLE; Magnetic Studies of Cr-Ge Alloys PERIODICAL: Fizika metallov i metallovedeniye, 1960, Vol 9. Nr 6, pp 823 - 827 (USSR) ABSTRACT: The present work is concerned with the-r-HADL21-ic properties of Cr-Ge alloys with Ge concentration between 50 and 950' 0 'D in the temperature region 77 - 320 K and magnetic field.~ up to 16 000 Oe. The alloys were prepared from 99.9970,,o pure germanium and high-purity electrolytic chromium degassed in a vacuum at 1 000 0C. uartz containers charged with the samples of the allay were heated to 1 100 0C and kept at that temperature for 2 hours. They were then cooled in the furnace down to room temperature, Next. tha alloys were gradually heated to 900, 800~ 700 and 600 C and were maintained at these temperatures for 5 hours and subsequently cooled to room temperature in the furnaces Altogether 13 alloys were prepared with Ge concentrations between 50 and 95 at.al). Alloys having a concentration of 70 and 750,'('3 were prepared twice in -A 1'/ 4 order to compare results. The temperature dependence of 4--l"' 3260? 3/137/6i/ooo/oi 1/060/123 Magnetic investigation ....... Ao6O/AlOl 0.5 deg/min. It was established that the investigated alloys have two points of ferromagnetic reversal. The true Curie point of these alloys is 2831K. The low temperature point of ferroiiiagnetic reversal (1300K at a field of 2400 oersteds) is a phase transition of the first kind. The ferromagnetic state of the alloys is caused only by the Mn3Ge2 compound. The coercive force HC of this alloy attains a maximum value of 520 oersteds at 2310K, and vanishes at 146 and 2800K. The anomalous course of the temperature dependence of the magnetization of the alloys under investigation is explained by the fact that they may be in one of two anti-ferromagnetic states depending on the tem 9era- ture. At T < 1130K the magnetic moments are oriented at an angle of 180 with respect to one another. At temperatures~> 1130K the magnetic moments turn by jump through a small angle, leading to the rise of an uncompensated magnetic moment. It is noted that HC and the remanent magnetization, beginning at a field intensity of 1500 oersteds are independent of the field, Whereas the magnetization of the same specimen continues to increase linearly. A. Rusakov [Abstracter's note: Complete translation) Card 2/2 '226-r 7 S/137/61/000/011/L)60/123 Ao6o/AlOl AUTHORS: Margolin, S.D., Fakidov, I.Q. TITLE: Magnetic investigation of alloys of the manganese-germanium system PERIODICAL: Referativnyy zhurnal,,Metallurgiya, no. 11, 1961, 9, abstract IlZh56. (V sb. "Magnitn. struktura ferromagnetikov". Novosibirsk, Sib. Otd. AN SSSR, 1960, 211 - 2106) TEXT: Alloys of Mn-Ge were prepared from electrolytic Mn (99.8%) puri- fied of gases, oxides and impurities, and Ge (99.997%). A large number of alloys with >40% Ge content were prepared. On the basis of the data from microsections it was established that only in alloys with -_~1.50% Ge does one find exclusively a chemical combination of Mn3Ge2 and Ge. fn the remaining alloys besides Mn 3Ge2 one also finds Mn5Ge3. Magnetic measurements were carried out in fields UP to 2700 oersteds at 77 - 3500K using the ballistic method. The measurements were carried out at a temperature variation at a rate of 0.2 - Card 1/2 NaEmetI2 Structuzei SOV/5526 of a Hy3terasia Loop 195 Klrc~.nskiy, L. V., A. I. Droltin, and D. A. L~iptAy (InArltute of Physics, Sibrriar, ziranclh AS U~3,SR, Kra-mny,-,riicl. Elr~,ct of Ela3tlc and PL~-.tic D,~forwtatlOn5 on th" of 'r,~~rmo- miZngtic HystcrccI3 201 o-r-olin, S. D. and I. G. Fakidov [Instltutr- of Phy3lcs of i-~tal.-, Ab uozri, Svcrdlovsk~. T-L3)gnz,,~lc Studip.3 of ALloya of the lll-'Anganese - Cermanlum 3yatem 211 Kir---nslcly, L. V., and B. P. Khromov [Irr..titut,~ of P~,y-jic,-~, flilb,.rian Branch AS USSR, Irrasnoyart3k]. Study of thz Apprz,;,ch- to-Saturation. La-w on 1"ionocry,,italo of Iron Silicidf- 2 Y( DtyaVov, G. P. (Physics D~partment of f-he University). Current State of the Prob1cm Conecraing tM Study of Parity Effect3 in the Approach-to-Saturation Region 221" Card 10/11 (Cont-) S 011/5 2 6 Ma6netllc Structu 0 COVERAGE: The collection contains 38 scientific articles presented at the All-Union Conference on the ".'.aFnetic Structure of 7erro- magnetic Sub:~tances, held in Krasnoyarsk in June 1958. The ma-- terial contains data on the maZnetic structure of ferromagnetIc materials and on the dynamics of the structure in relation to magnetic field changes, elastic stresses, and temperature. Ac cording to the Pore-aord the study of ferromagnetic materials had a successful beginning In the Soviet Union in the 1930's, was subsequently discontinued for many years, and was resumed in the 1950's. No personalities are mentioned. References accompany individual articles. TABLE OF COINTE-TrS: Foreword 3 Shur, Ya. S. [Inst1tut fIzIk1 metallov AN SSSR - institute of Physics of Metals, AS USSR, Sverdlovsk]. On the Magnetic Structure of Fcrrora.,netIc Substancez Card 2/11 Cr PHASE I BOOK E7-FLOITATIGN SOV15526 Vscsoyuznoye soveshchanlye po ragnitnoy Btrukturo ferromnagnetikov, Krasnoyarsk, 1958. Magnitnaya struktura ferromagnetikov; materialy VacaoyuznoEo sovu3hchanlya, 10 - 16 Iyunya 1958 g., Kracnoyarzlk Structure of FerromaZnetic Substances; gaterials of thia All-Union Conference on the 'e1agnotic Structure of Ferromagnetic Substances, Hold in Xrarnoyarz-11c 10 - 16 Juno, 1958) Novosibimk, Izd-vo 'Ibirskogo otd. All SS.SR, 1960. 249 p. Errata slip Inserted. 0 1,500 copies printed. Sponsoring Agency: Akademiya nauk SSSR. Institut fiziki Sibirzkogo otdelenlya. Komisslya po magnetizmu pri Institute f1zIk1i metallov Or-NIT. Resp. Ed.: L. V. Kiron3kiy, Doctor of Physical and 1,athernatical Sciences; Ed.: R. L. Dudnik; Tech. Ed.: A. F. Yazurova. PURPOSE: This collection of articles is intended for researchers In forromagnotism and for motal scientists. Card 1/11 SOV/126-7-1-27/28 Magnetic Studies of the Manganese-Germanitm Alloys alloys could be explained using Dzyaloshinskiyls theory (Ref.5). Acknowledgments are made to K.B. Vlasov for his advice. There are 2 figures and 9 references, of which 5 are Soviet, 1 German, 2 En,-lish and 1 French. ASSOCIATION: Institut fiziki metallov AN SSSR (Physics of Metals Institute, Ac.Se. USSR) SUBMITTED: February 25, 1958 Card 4/4 SUVI 126 -7 Magnetic Studies of the Manganese-Germanlum Alloys have two ferromagnetic transition points. The true ferromagnetic Curie point in these alloys is 2830K, and it is confirmed by the alloys obeying the Curie- Weiss law above 2800K. (2) The low-temperature ferromagnetic transition point is a phase transition of the first type. This is con- firmed by thermograms obtained using Kurlakov's pyro- meter which indicated a transition at 1130K with a latent heat of transition. It is also supported by the temperature dependences of magnetization which are not single-valued and depend on whether the sample is heated or cooled (Fig.2). On cooling of a 30-70 Mn-Ge sample in a magnetic field of 2432 Oe the transition temperature is 1180K, while on heating the same transition occurs at 1300K. (3) It is possible that the anomalous behaviour of Card 3/4 temperature dependence of the magnetization of the Un-Ge SOV/ 12b -7 -1 -27/28 Magnetic Studies of the Manganese-Germanium Alloys magnetic transition points the authors continued their investigations of the 30-70 Mn-Ge alloy as well as extending their studies to sampies with higher amounts of germanium. It was found that all these alloys consisted of only two phases: a compound Mn3Ge2 and pure germanium. Some of the results are given in Figs. 1-and 2. Fig.1 shows the dependence of the coercive force H., magnetization I and remanent magnetization Ir on the applied magnetic field Hi for the 30-70 Mn-Ge alloy. Fig.2 gives the temperature dependence of the magnetization and coercive force of the 30-70 Mn-Ge alloy on heating (eireles) and cooling (crosses). From Figs. 1, 2 and other results the authors draw the following conclusions. Card 2/4 (1) The Hn-Ge alloys with 40 at.% of Ge or more AUTHORS: Margolin, S.D. and Fakidov, I.G. SUV/126-7-1-27/28 TITLE: Ma ~eti`cStudo ~of the Manganese-Gormanium Alloys (Magnitn ye issledovaniya splavov sistemy marganots- germaniyT RERIODICAL: J?izika Metallov i Metallovedeniye, 1959, Vol 7, Nr 1, pp 157-159 (USSR) ABSTRACT: The authors reported earlier (Ref.1) that an alloy with 30 at.% of Mn and 70 at.% of Go has two ferro- magnetic transition points between 77 and 398011 in fields from 20 to 2400 Oe. One of these transitions occurs at 2830K and the other at 1480K in fields of 38 Oe and at 1300K in fields of 2432 Oe. The maximum of magnetization occurs at 1730K at all field intensities. The authors' work showed that the ferro- magnetic state of the Mn-Ge alloys is due to Mn3G82 Card 1/4 only. To elucidate the nature of these two-ferro- 126-2-25/35 Temperature de-Dendence of 16he magnetization of the alloy containing 30 at.% Un, 70 at.% Ge. There are 2 figures and four references, one of 'which is Slavic. (Note: This is a complete translation). SUBMITTED: March 11, 1957. ASSOCIATIO14: Institute of Physics of Metal, Ural Branch of the Ac.Sc., U.S.S.R. (Institut Fiziki A-letallov Ural'skogo Filiala AN SSSR). AVAIIABLE: Library of Congress. Card 4/4 126-2-25/35 Temperature dependence of the magnetization of the alloy containi,l,- 30 at.% IAn, 70 at.% Ge. equals 10 0C and is independent of the field stren'-th, whil8t the second is in the tem-Derature ra-n.j-e -125 'o -143 C and does depend on the raagnetic Leld stren-'a. The maximum maCnetization occurs at 100 C for all the field strengths comprised in the tests. FJL'-.2 ~'-Ie magnetization curves of the 30 at.% Mn, 70 at.% Ge alloy at variuus temperatures, which indicates that for field strengths up to 2400 Oe. the magnetization has P. linear dependence on the magnetic field strenu?-th at the temperature of liquid nitrogen. For elucidatin- the CD 0 physical nature of these two temperatures of ferromai~--Ietic transformation of the alloy containin.- 30 at.% L'In a-nd 70 at.% Ge and other alloys of this system, the authors propose to continue their investigations using more intensive ma-netic fields and lower temperature!:,. Fit U _.l shows the temperature dependence of the magnetization of an alloy containing 30 at.% Mn and 70 at.% Ge au various magnetic fielg stren~;ths (magnetization, Gauss vs. Uem-perature, K). Fig.2 shows the magnetization curves of an alloy with 30 at.% LIn and 70 at.% G(j at various Card 3/4 temperatures (177, 2221 146 and 77'K). 126-2-25/35 Temperature dependence of the ma,~netization of the alloy containini- U 30 a.t.% Mn, 70 at.% Ge. 30 at.% PAn and 70 at.% Ge,investi6ated by the authors: of this paper,was produced from electrolytic :-qangaxjese of 99.896 purity, purified by distillation in a hit_:h frequency furnaceland germanium of 99.997% purity with a specific resistance of 1.4 Ohm/cm. The alloy was produced from a mixture of Mn and Ge placed into a quartz ampule wliich was evacuated to 10-5 mm Hg. The quartz ampule and its contents were heated in a furnace to a temperature exceeding about 2000C the melting temperature of the allo~7 (according to the diagram of state), held for two hours C) at that tenperature and, f8 llo%,ring that, the i.,ielt ;Iras cooled to a temperature 50 C below the melting point at which it was held for two hours Eind then slowly cooled in the furnace to room temperature. From the thus produced alloy a specimen 0.402 x 0.302 x 2.0 cm was made; the ma6netic measurements were effected by ;,eans of a ballistic method. It can be seen from the curves of the teimperaturc, dopundence of tho mavnotizatiozi ~11ioan in Fig.1 that the alloy containing 30 at.% Piln and ?0 ;3~.% Ge has two temperatures of ferromagnetic transformation Card 2/4 in the case of a field strength of 2400 Oe. One of these AUTHORS: Margolin, S.D.,and Fakidov, I. G. 126-2-25/355 TITIdil: --iemperature denendence of the magnetization of -6he alloy containing 30 at.yo Mn, 70 at.% Ge. (-.eemperat-arna.-ja zavisimost' nariagnichennosti splava Min 30 at.%, Ge 70 nt.%). PERIODICAL: Fizika Uetallov i Metallovedeniye, 195?, Vol.5, No.2, pp. 368-369 (USSR) ABSTRACT: The results are described of preliminary investi.-ations of the temperature dependence of the magnetiz~.tion of the alloy containin- 30 at.% Mn and 70 at.% Ge ii the temperature range liquid nitrogen up to 120 C, in ma,-)netic fields between 20 and 2400 Oe. Zwicker, I.,et alii (Ref.1) studied the diagram of state of Un-Ge alloys and showed that the compounds Mn. 5Ge2 and Mn5Ge3 are strongly ferro- magnetic at low temperatures. Gastelliz (Ref.2) described results of maEnetic investigations of Mn 5 Ge 3' Guigg, K. J., et alii (Ref.3) give data on the residual magnetization and the coercive force of Mn 5Ge and Mn 5Ge 3' Fakidov I. G. (one of the authors" et alii (ief.4) detected existence of two temperatures of ferromagnetic transformation when studying the electric conductivity of Card 1/4 the alloys of the Mn-Ge system. The alloy containing ~k ~ 1'~ , S'v - USSR/Electricity - Scriconduct-rs Abs Jour Ref Zhur Fizikr-, Nn '), 1~,57, 11 - 70"0 Authnr 1~ I' D Fakidov, I.G. .0_'~LEO i I n- J - ? Inst Ins tit-u-t-c-o-FTF-'-hysic 9 ( fIs, '~r P I ~rrnch, .,C r 4ovy - f Sciences, USER, ~vcHlc-vsk. Title i Use of Fhot,~resistrmcos of C;,-,I: iu, f~ulfi,2r- in Ccnjurlctirn with Phos, hors as P Dvtoct,r for Go Rrys fr(-,-. C, 'C. Orig Fub Fiz. '~CtP.11CV i IC~551 It No 2, 379-7j83 Abstract i'i -hotor-sistanco ~f "dS is quite sonsitivu, tr' the visiblv end to X-r!,yo. etto :Its -dc tc uso C~',-, crystcls to roe-rd the herl --- rrys hcmc shcwn thrt the CC~6C' (1.17 !,r,:' 1." 1"' sensitivity rf CdS tr rradi-tkn frc: ~~ " '~ V j is s-.ell. It is shovn t~f~t in conjuncti,-,n with Thr, snhre scent ;,~P.I (TI) or Csi (T1), ~-hich o it. un'-or the influence cf g~--rr, rays n visi~lo lip-ht of - frcqi:cncy close tQ, the fr,~quoncy of the r-.rxi: u:-i sonsitivity cf C,'~', the photoresistnnce er...'I be used as c dtectcr f-r !7r,- 2 -~,ys fr"-.r. Co6c. The !idvan- tage of such r- detect,,lr over scin'till-tion counters is the si,,rlicity of the electricrl circL)it and the absence of the need for Fhoto:-.ultiplicrs r-mid hiF.h-viltage stabilized surrly. H '11 MUUMLIN, L. D. S. D. Marp-olin. 4xperimental investigation of magnetic surface effect in a ferroma.-Metic ring. P. 686 1,ib. of electrical Fh,~nxnerA Institute of Physics of Metals Ural Branch of AcadenV of 3ciences, U53R April le,, 1950 SO: Journal of Technical Physics, Vol. XXI, No. 6, June 1951 21 ')Ifsy 50 "Diatributlozi'6f M6gn6t-ic IjAuction, Accotrding tO,, Depths I of 'a Forrom5guetic Ring Placed In .an Altex* ;640~tivg S16ctr'=q&~)tic Fields" S. D. Margolin limt fh~ln of Met ~.Ii )Ural Affiliate,. Acad Sci WSW., D"Ok:Ak N66uk SSSR" Vol LXXIIs4o 3p pp .493-495~ Dienctives, App for meae'Uring mw~petic induction And r6ma+Am4 readings,, which are then used to chack tho~reticai formulae developed earlier ("Zbur: Takh :Fiz"': Vol XVII 'No 10, 1306' 1940), for diatrib~ijmn or Ind=tIonI Bs ~by depth a, in f erro=qgmUc USORAbysica magnetic Induction 21 MAY 50 (Contd) - plate, placed in,alternating sinu~oldal electr=og- netic field, Submitted 20 Mar 50 bY Acad I.. F. 175T86 Apr Perramagnetism. Fields, Electromagnetic "Xddy4urrent Losses During the MAgnetic Skiii- :Effect in Sheet Steel.,":_S. 3). Margolin, Inat Tb~s of Metals, Ural Affilliate Acad Sci USSRJ "DO'k Ak Hauk SSSR" Vol Lw' Tio Author explains how hie =tho%l can be-used to determine eddy-current losses in ferromagmetle sheets located in a variable electromagnetic field, allowing for dependence of magnetic permeability =u on magnetic field intensity. 39/49T108 UBW/Physice (Contd) Apr 4� Submitted by Acad 1. P. Bardin, 17 Fab 49. 39/149TIOB MAPMUN, S. D. PA 20/4M2 USSR/Physics Oct 48 Steel Plate Magnetic Fields "Computing the Magnetic Skin Effect In Steel Plates and Relationship of Magnetic Permeability to the Charge of the Magnetic Field," S. D. Margolin, Inst Phys of Metals, Ural Affiliate, Acad Sol USSR, 10 pp "Zhur Takh Piz" Vol XVIII, No 10 Presents nev method developed by Margolin for com- puting electromagnetic properties of ferromagaetic laminas In an AC field vith accounting of relation- ship of magnetic penetrability and voltage of the magnetto field. Subaitted 30 Doc 47- 20/49T92 KARGOLIR, S. Transfer of a blast furiaco from Florida to Texas (From: "Iron Age" 1945) Stall ? ne.2:177 147. (KIRA 9:1) (United States-Blast furnaces) KARGOLIM. S. Production of lightweight. blast-furRace slag (From: 41ron and Steal Engineer.* R9.7, 1945). Stal' 7 se.2:175-176 147. (United States-Slag) WaA 9:1) MARGOLIN, S. - Rebuilding Raglaxii's ferrous metallurgical bLdustry. (Free: q%e Zxglzeerg ses.4713-4714.i946). Stall 7 no.2:171-174 147. (Great Britain--Metallurgy) (KLRA 9:1) KARGOLIH, S., referent. Flow of gases and coke coasumption in blast furamces.(Frem: "Blast furnace steel plant." me-7, 1945). Stni, 7 ao.1:86-87 147. (Blast furnaces) (KLRA 9:1) Vto- 0 0 000' 0* fte (row tau Uft 60 el A so 4 00 so es .3 00 sago." WIP Iv.1 c" f& -.~-V-T- u 1% &V 10 Ll 11 1 p 0 q 0 a (fall, lode 64M It a K cc te (c Ic 0 0 0 00000600*00#04 a 0 4L 4- ast in I a fm a 4 a I w (a 0 As 4 34 KIN 4M a 41b 000000006*606000 T-14 a Vo Vo So a goo 10 '7 Jun HARGOLIN, P S N15 722-105 -M3 1952 Operativnyy uchet zagotovok selts?okhozyayst;vennykh produktov (Operational accounting of stocks of agricultural products) Izd. 2-e, perer. Pod. red. G. G. Petrova. Moskva, Cros Id-vo Tekhnicheskoy i Eknonomicheskoy Literatury po Voprosam Zagotovok, 1952. 251 p. tables. OKULOV, Igor$ Borisovich, inzh.; SHUBIN, Boris Minich, inzh.; Prinimala uchastiye GVOZDEVA, Z.P., inzh.; 1%RgQLLN,_P.A.,_inzh., retsenzent; BELOBORODOVA, O.S., inzh., retsenzent; DUGINA, N.A., tekhn. red. rElectrnDla~+-ingIGallvanicheskie pokry-tiia. Moskva, Mashgiz, 1962. 176 p. (MIRA 16:2) (Electroplating) 1*4R,601,1AI /a MARGOLITN,_ Business accounting by crews in grain centers of Moscow Province. Kuk.-elov.prom. 21 no.2:6-9 F '55. (ten 8. 3 ) 1. Hoskovakaya. oblastnaya kontora Zaptzerno. (Moscow Province--Grain handling) MAROLP', 0. YA. 22322 Margolin, 0. Ya. Znacheniye M. termodinamiki. (Doklad na nauch. kruzhke Dek. 1948 G.) sbornik rabot studentov - (Leningr. Koradlestroit. in-t), Vyp. 1, Bibliogr: 10 nazv. V. Lomonosova kak osnavopolozhnika pri kaffedre termodinamiki 16 chlenov nauch. Kruzlikov 1949, S. 7-14-- SO: LETOPIS' No. 30, 1949 KI-Jil`~ OLIN, 0. YA. 2?322-k~,r--cliu, 0. W. ZnL~chontya M.T. Lomonosovl Aak Oanovopf)lozhniku Tormodinpniki. (Doklfjd lia Natich. Kruzi-.ke Pri 4fedre Tormodinamiki 16 Dek. 19V,, G. ) 'Ijborn J~';t'; ~) 0 t Studontov-Chlenov lianch. Kruzhkov (14xilziCr, Kor.,.(ilestr6lt. In-T), Vyp. 1. ) cAgo Cl. ?-14. Bibliogr: 10 K~V. SO: latoPial !in. 30 1949 BACHURIN, A.V.1 UMLIN, N.S - KONDRASHV, D.D.-, GORICIOV, N.V.; ROGOVSKIf-, YAMPOLISKIY, M.A.; TYUKOV, V.S.; RWSHTFSYN, L.A.; GERASHCHENKO, V.S.; KOTOV, V.F.; BAZAROVA, G.V., red.; PORTYANNIKOV, N.S., red.; GERASIMVA, U.S.,, tekhn. red. [Commodity and monetary relations during the period of transition to communism] Tovarno-denezhnye otnosheeniia v period perekhoda k kommunizmu. Moskva, Ekonomizdat, 1963. 386 p. (MIRA 16:5) (Economics) MARGOLIN, Nison Solomonovich; KHOLIN, I.A., red.; PONOPWOVA, A.A., t~~. r-ed-. (Financial planning; finance and currency circulation in the national economic plan of the U.S.S.R.] Planirovanie finansov; finansy i denezhnoe obrashchenie v narodnakhoslaistvannom plane USSR. Moskva, Gosplanizdat, 1960. 158 P. (MIRA 14:2) (Finance) (Russia--Economic policy) MARMLIN, N. S. Currency ',uestion Important lever of currency circulation r-lannin~-, (Balance of money Lnco,.-.-~ -3x,--n:"-'turas of the population. Reviewed by A. Aa-,rny-j). Cen. i kr~!. No. 1, 1952 Library of Congress, BArch 1952. Unclassified. m.vk~OLI 14, ',1 S Balans Denezlinyk~ri Doknodov 1 .,,as?hoaov ~Naseleriiya (Acco-In7, C;- and ixpenses of the Populatioa) kuskva, -,osplanizciar,, i))i. 13) P. Cataloged from Abstract. Problems of* Theory and Practicu in the Co:apilatiu., ol' Accounts. of C, 1-1 1-7, 1- r1 The problems of bal-ai.cing Ur.e nat.-J.-mls --ii-l ex., t, I Gf~ ~~ i, 1 - - -,; - ~ I ~ - - 7 - t- 1, . ( '. - - -) -4 0- ~ J$ I- . . I- I - - I,- , Hr7' ~,- ' - "27 MARGOLIN, N. S. "The Use of Starting Boxes for the Heating of Trolley Buses," SO: Prom. Energet., No. 5, 1948. Mbr., Moscow Electric Transportation, -c1945-. ANTIMONOV 9.S., prof.; VEDENIN, N.N., kand. yurid. nauk; GENKIN, D.M., prof.; GRAVE,. K.A., prof.,- YEPANESF[NIKOV, N.V., dotit~; ZHUKOVA, L.F., dots.; KT,44, Ya.A., dots.; LIVOVICH, Yu.Ya.; )!AMQLIN,-M-Z.; 140ROVSKAYA, T.A., dots.; POLENINA, S.V., kand. yurid. nauk; SADIKOV, I.N.; FIALKOV, M.A., kand. yurid. nauk; YAZEV, V.A., kand. yurid. nauk; YAKHNINA, N.A.I. kand. yurid. nauk; KIRAKOZOVA, N.Sh., red.; ELIKINA, E.M., tekhn. red. [Government trade regulation] Regulirovanie gosudarstvennoi torgovIi. Mosk-va, Gostorgizdat, 1963. 339 p. (MIRA 16:7) (Commercial law) SUKHININ, S.D.; MARGOLIN, M.Ya.; YERPULEV, N.A. Improvement of the preparation of acetic acid salts. Prom. khim. reak. i osobo chist. veshch. no.1:26-27 163. (MIRA 17:2) MARGOLIN, M. Ya.[Marholin, M. IAJ; SMWAIIK, 0. K.; KUSHNIR, M. M. Continuous method of production of a potassium-butyl flotation agent. Khim. prom.(Ukr.] no.1:30-31 Ja-Mr 162. (MRA 15: 10) 1. Donetskiy zavod khimicheskikh reaktivov. (Flotation-Equipment and supplies) HAWOLIV.-,$tkhail, .71adimirovich, konstraktor; USPEUSKIY, N.M., red.; AIOR AMOY, B.I., te' .)red. [Target pistol and its repair] Sportivnyi pistolet i ego remont] Moskva, Izd-vo DOSW, 1958. 94 p. (HIRA 12:5) (Pistols--Kaintenance and repair) Calculation of a Vacuum-Tube Osciliato.- Wit- a COMIDIel Sovll', o8-1 3- io-6/13 Load Operating as a SurE7e Gezierator A,9=IATION: Vsesoyuznoye nauchnin-t,'kh"Ich skoye obshahestvo rad:Loteakhniki i e1ektL-owfyazi im. A.S. Popove (AU-Union Scientift-1- and Technicall Socie-~-y of RadIo and COMMMice-Jor-8 Eaginewing iw-- A. S. Popov ) Card 4/4 Calculation of a Vacuum-Tube Oscillator With, a Com--lex SCIV/1,58-1 3- 1 c-6/13 Load Operating as a Surge Generator to be composed of two unequal pulses with a vertical trailing edbre. It is shown that the error of the calculation according to these simplified equations does not exceed 55, which is quite sufficient. The sarle method also permits to compute pulses at In the last section the load characteristics and its application in the case of a complex load and of a surEe-generator mode of operation are investigated. Two examples, taking into account the second and third harmonic which cause the unsymmetry of tuning, are presented. There are 9 figures and 8 references, 8 of which are Soviet. SUBMITTED: May 11, 1956 (initially), and November 15, 1957 (after revision) Card 3/4 Calculation of a Vacuum-Tube Oscillator With a Comr-lex Load Operating as a curare Generatur coefficients of the series expansion of the current pulses into a Fourier (Furlye) series versus the relative load resistance R X Ra (1), where Ra crit denotes the load resistance a o'tit of the cutoff mode of operation, which is specified by formula (2). If-the plate load is complex, the plate alternating voltage is not in phase with the first harmonic of the plate current. Hence the plate current pulse in a surge-generator mode of operation becomes unsymmetrical and exhibits a phase shift with respect to the grid y,oltage. The dependence of the shape of the plate current pulse up9n the mode of operation is investigated, a symmetrical and an unsymmetrical pulse being considered. The components of the unsymmetrical pulse are investigated and for the case of S> 1 simple formulae are derived for the calculation of the expansion coefficients. in order to Card 2/4 simplify the mathematical labor the current pulse is considered AUTHOR: Ma Member of the s cv/-i o e - 11 o - 6/1 Society TITLE: Calculation of a Vacuum-Tube Oscillator With a Complex Load Operating as a Surge Generator (Rasche"t lampovogo generatora s kompleksnoy nagruzkoy v perenapryazh5nnom rezhime) PERIODICAL: Radiotekhnika, 1958, Vol 13, Nr 10, pp 29 - 38 (USSR) ABSTRACT: This is the first presentation of a method for the computation of the operating schedule and of the load characteristics of a vacuum-tube oscillator in the case ~ >1, which is of paramount practical importance. denotes the coefficient of plate voltage efficiency. The method of analysis is based upon the utilization of generalized load characteristics. It is distinguished by a particular feature. This is the possibility of using the load characteristics not only if the load is varied, but also if the mode of operation of the oscillator is modified (Ref 8). The load characteristics are shown Card 1/4 as a function of the coefficient.,~,~ and of the normalized Interrelation of Vacuum-tube Parameters and of SOV/108-13-2-12/15 Those of a Triode Transistor There are 8 figures and 3 references, 2 of which are Soviet SUMIITM: November 12, 1956 Card 3/3 Interrelation of Vdcuun-tibe Paramaters and0f J. SOVA08-13-2-12/15- Those of a Triode Transistor Card 2/3 emitter, of a_ vVzMm-tube with earthed cathode, of a.. ~,trjode transistor with earthed collector, and of an vacu=_tUbe ~ with earthed anode viere investigated. Comprisingly is said: 1) For the analysis of _VaCWML- tube-- and ~.triode transistor , diagrams the same system of equivalent parameter S0 (slope of the current characteristic), Rio (internal resistance, caused by the internal feed-back), and'D0 (a factor analogous to the amplification factor in the valve) can be used as well as the equivalent diagram which is based upon the consideration of the YaMM-tube and the tricue transistor - as current generator. 2) The equivalent parameters coincide with the valve parameters (S' RiD) in the case of the valve. In the tridde transist6r the equivalent parameters can be rather simply brought in connection with the h-parameters. A difference between the valve- and the semiconductor parameters is due to the existence of the factor of the positive feed-back (D* ) in the triode transistor AUTHOR: Margo Li 5--ht-c- SOV/ TITLE: Interrelation of Vacw=-tike Parameters Lnd of ',',,ose of a Triode Transistor. -. (Vzaimosvyazt mezhdu parametrami elektronnoy lampy i poluprovodnikovogo trioda) PERIODICAL: Radiotekhnika, 1958, Vol. 13, Nr 2, pp. 79-85 (USSR) Received: April 25, 1958 ABSTRACT: Between the , triode transistor .; and the vacuun-tube there is a great difference with respect to the internal physical processes. In spite of this the same computation method and the same equivalent diagram can be used in the analysis of processes connected with the external current circuit. The reason for thisisthe fact that the Vacuum- ' tsibe -- as well as the triode transistor can be considered as current generators. The fundamental equations for the equivalent current circuit (8), (9), and (10) are derived~ These are then used for the analysis of the separate diagrams. In the case of high frequence the equivalent parameters become complex. The schemes of: a triode.trp-a- didtdr- with earthed basis, of a., vacuum-tibe wi th Card 1/3 earthed grid, of a triode transistor : with earthed The Electron-tube (cont.) 409 Z. I. Model', I. Kh. Hevyazhakiy, an& N. S. Beschastnov, for their contribution in developing this method. There are 15 references, all Soviet. TOLE OF CON"LEM: Foreward 5 PART I. ANALYSIS OF AN ELECTRON-TUBE POWER AKPLVIER Ch. 1 Underv I age Conditions 1-1: Effect of grid aux-vent on plate current 1-2. Load charazteristic equation 12 1-3. Calculation of pulse flattening 16 Ch. 2. Over7oltage Conditions 19 2-1. Cwputation of ccmplex pulse components 19 2-2. L