SCIENTIFIC ABSTRACT ALEKSEYEVSKIY, N. - ALEKSEYEVSKIY, E.

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SCIENTIFIC ABSTRACT
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W91 The Fermi Surface of Tin 5/056/60/039/005/005/051 B029/BO7T along the binary axes [100] and L0101. Detailed statements are supple- mented by Illustrating the transformation in stere^qr&phic projections a' -ong the direction of the magnotic field. The seconA part of this Vapor deals with determining the directions of plane sections of an open Formik surface. Thera are several types of current diagrams with Qg .. const(a), where a denotes the angle formed by the current and the open cross v*otion or a certain crystallographic axis (119). Using these polar diagraas of the current intensity it is possible to de- termine *hother the cause of the quadratic increase of resistance for a given direction of the magnetic field is the compensation of volumes (V1 . V or the presence of open trajectories, and it in possible to 2) determine the direction of these trajectories. Two special cases are them Invoatigated. The experimental results are given and discussed in the third part of this paytr. Tin was produced by zone melting at the tekhmologicheekly otdel IFP AN SSSR (Institute of Physical Problems of the AS USSR, Department of Technology). The resistance diagrams of a pecluene whose axes enclose a small axis [ 11 tin * angle with the 001] (00 L Zhurnal eksperimental Inoy i teoretichoskoy fiziki, v. 43, no. 2(0), 1962t 731-733 "he cl-.F-n,&(t Ir. rosistivity of transition metal single crystals Re, !Za) with the change in field strength of a strong magnetic field .,U,) to Mae 15-3 IWO) was studied at 4.20K. The results show '.he. Pd and Re have opon Fermi nurfaces. The Fermi surface of id is similar to that of et. 7hu square-law increase of resistivity of 11o with increasing na,;netic fi*ld strength is indicative of a closed Fermi surface. There ar. 2 fidwas anti 1 table. Inttitut fizicheakikh problem Akadezii nauk 850R (Inatitute of Physical Problems of the Academy of Sciences USSR) S/056/62/043/003/009/063 B125/B102 AUT11023 Alekneyevakiy I H. Ye., Fam Zuy Kiyen, Shapiro,, V. C., TI-A1,1:: Anisotropy of the 140'ssbauer effect in a *",-Sn single crystal Zburnal experimentallnoy i teoreticheakoy fiziki, v- 43, no. 3(5), 19629 790 - 794 TF-C" : The resonance absorption probability flof 25.8 kev I-quanta in vhite tin rav ,tttidied at 770K and 2950K. The lamellar absorbers, about 57 5 =f/t:L2 talck, were out out from 'i-Sn single crystals in the (001). (1;IN 1 ; jind ( 00) planor.. The trial measurements viere made %ith a poly- crystalltne Vin foil. The I-quantum nources, concistinr of Sn 119M nuclei in SnO. (68,4 sn 118 ; q 5 mg/C thick), ivere irradiated in a reactor. In all experinents tho source *as kept.at room temperature. The figure shows three spectra. laken at 770K under identical geometrical conditions. Probably becawto of quadrupole interaction, the half-vidths of the lines observed are greater than the theoretical half-widths if allovance is Card 11~ r . S/056/62/043/003/009/065 Anisotropy of' the Olsebauer..# B125 B102 made for the effective thicknessev of absorber and source. The L-radient of *he electric field in ~-Sn crystals is axisymmetrical in first approxima- %ion, Ule axis of symmetry being perpendicular to the (001) plane. The componentp of WIC absorption spectrum for the (001), (101) and (100) planes have the relalive intensities a a - 9/7 and a - 5/5, a - w /2/' 1'2; it -col; i5/2 Q)' '+1/2 ((5/3)-cos Q). I +j2 is the resonance absorption probability of the .*~-quanta to the correspondinj7 sublevel.*0 i;3 the anr,c bet-seer, the :salmmetr~ axis of the crystal and the direction of the incident t-quarntum. nie greater the quadrupole splittinr cnd the smaller the effeativ-e absorber thickness, the greater the shift of the absorption maxizi= towar4a the more intense-component and the asymmetry of the line. The rusonDnce absorption probabilities at 770K are f -.1:0.67:0.89, ut 2930K, f :17 There 100:11,01 601,.fp"ly , 1:0.95;0.75:0-80- are I figure and 3 tables. ASSOCIATION: Inotitut yadernoy fiziki Moakovakogo gosudarstvennogo Ainiversiteta (Institute of Nuclear Physics of the Moscou Card 2114, Mate University) 3/056/62/043/003/009/063 Anisotropy of tho 110"aebauer... B125/BI02 SUBMITTED: April 49 1962 Fig. absorption upectra taken at 7TOK for plates vith different orientations a (001), ~-, - (100), polycrystal. The thin vertical lines show the positions of %hu absorption maxima. Card 3.15 3/056/62/043/006/022/067 B102/B104 AUTHOPS: Alekseyovskly, N. Ye., Caydukov. Yu. P. TITLE:. The open cross stations of the Fermi surfaces of cadmium, zinc and thallium PERIODICAL: Zharnal eksperimentallnoy i teoreticheskoy fizi'l, V. 43, no. 6(12), 1962, 2094-2104 TEXT: Investigat ions of the Fermi surfaces of Cd, Zn and Tl single crystals based on meavurenents of the anisotropy of the electric resis- tivity of these crystals in strong magnetic fields are reported. Q300/14.2 was equal to about 10,000 for Cd anA TI and 15,000 for Zn. All menaurements were made at 4.20K and in fields of up to 33 koe. In most cases the sample axes were perpendicular to 1, in a few the deviation from orthogonality van 140. The angular dependence of resistance, at H-const was 4etermined from automatic records of the amf with an W) -09 (EPP-09) recorder, aj~/at van 6-701min. Of Od the axI a vere oriented along (10TO]. [7010) , and [0001] , of Zn along 1161-0 - (7110) Card 1/3 S/0~6/62/043/006/022/067 The open croee sections of the B1W/B104 and [00011 and of T1 only ea lea wi*4"n its axes in the fOO01) plane were curves of the samples with the axes along inveq~if;ate4 . F!?r Cd the Q(1; L1010) and 1,201(ki were almo t equal double-leafs in polar coordinates with deep -minima In the dir:ctlonB 1r2TO] and [61-10) . The sample with the axle parallel to (00011 showed almist no asymmetry; Q gres according to a square law for tkny direction of . Zn samples with their axes parallel r :hosed, injontradistinction to Cd, a second deep and to LIOTO~ or ~71101 narroT minimum o Q t it 11 LOOO, . The sample with its axis parallel to Lo 001.; showed no anisotropy of C, 0 grew quadratically for any A I/ direction. For TI Q(~,) was measured at Eaconst with about 30 saPples whose axes lay inihe 0001~planel Off -A 1) [0001 1 .Q grew linearly for 1: ~10001,:, for other direction, 0 Ythe gros4h followed a square law. The results showod that Cd, Zn and Tl possess open Fermi surfaces, For Cd the open trajectories of the conduction electrons in a magnetic field are parallel to LOO011, in Zn they are pi~rallel to ['00013 or lie in the LO001J plant, in TI they lie only in the LOOOIJ plane. The stereographic projection of the distinguished directions of the magnetic field for the Fermi surfaces provides explanations of the Card 2/3 S/056/62/043/006/022/067 The open cross noctions of the B102/B104 anisotropl of 0 in all the cases investigated. The topology of the Fermi surfaces is discussed in detail. There are 13 figures. ASSOCIATION: 1xistitut fizicheskikh problem Akademii nauk SSSR (Institute of Physical Problems of the Academy of Sciences UsSR) SUBMITTED: July 24, 1962 Card 5/5 1 0 1 MIERATIOT, X.N. Supavooductivity of some bimry mW ternat7 allopi Zhur.skep. i tw.ria. 43 no.6t2UO-=3 D t62. KMA 16:1) 1. M*otitut fisichaskikh problem AN SSSR. caupeivonduativity) (Alloys) ALEKSWVSKIY, N.Te.; SAVITSKIY, Ye.M.; BARON, V.V.; WIMOV, Yu.V. 3fract of alloyed elements on the superconducting properties of the compound V3.3i. Dokl.AN SSSR 145 no.ls82-84 JI 162. (KRA 15s"r) 1. Institut fisichookikh problem AN SM i Institut meta-Uurgii imeal A.A.Baykova. 2. Chlen-karrespondent AN SSSR (for Alskmayevskly). (Superconductivity) (Vanadium silicide) (Molybdenum silicide) to X!! Afti, W'I 101 1', I fl Rr ~i j, if t, .. . . ....... JUL, 41 41 11 11 41 lick Y~i 111' 1 1 1pill film 11; ~1,11 p I 14 1i P P In ILI, Ii I It t-- fir, t6 iTER Oil 1111 YEZOROV, V-S- AMESLIEVSK Manuring the resistance of single crystals in a pulsed magnetic Mild. Mar. eksp. i tear. fis. 45 no.3t448-454 S 163. (KVA 16 r 10) 1. Ins-titut fiticheakikh problem kN SSSR. (Cx7st&ls--G&lvanomgnetic propertiets) (Yagnetic fields) ACCESSION NR3o AP4031138 S/OOS6/64/046/004/121)5/1207 AuTHou j Aiaxseyevskly, W. Yo.: Yegorov, V. S. TITLEs Concerning magnetic breakdown in beryllium SOURM Zh. ekspqr. i teor. fiz., v. 46, no. 4, 1964, 1205-1.207 TOPIC TAGS: beryllium, galvanomagnetic~efbect, magnetic field, re- sistivity, miAgnetic breakdown ABSTRAM 'Mis is a continuation of work reported earlier (ZhETF v. 45, 388, 1963) and aimed at checking the change in the variation of resistance with the magnetic field above 50 kOe. The measure- ments were suide on a single crystal of beryllium in dif."ILA---ent effec- tive fields at temperatures 4.2 and 78K. Pulsed magnutic fields were used in a measuremnt procedure which was also described earlier (ZbETF 45, 448, i963). The results are in good agreement with those obtained earlier. in that the change in thelaw of resistance rise Card 1/4 ACCESSION NR: AP4031138 occurs at the same value of the magnetic field (45 kOe at 4.21C and 40-50 kOe at 78K). This behavior of resistance is attributed again to magnetic breakdown. It is emphasized, however, that this inter- pretation of the results is only qualitative and cannot be usfkd as yet for quantitativo estimates. Orig. art. has: 2 figures. ASSOCIATION: Institut fizicheakikh problem AN SSSR (Xnatituto of Physicn Problems AN SSSR) SUBMITTED; 050ct63 DATE ACQ: 07May64 ENCL: 02 SUB CODE: Mt, SS NR REP SOVs 003 OTHER. 002 Qwd 2/4 AccessioN mt; AP4031138 4MA I / a,, Apr . M-1 J, ol ZNCLOSURE; 01 Angular diagrams showing the va- riation of the resistance of be- ryllium In a transverse ragnetic, field. The hexagonal axis 15 per- pendicular to the current. H Is perpendicular to the hexagonal axis in the direction of' tte arrow Curve 1 (obtained in stationary field T - 4.2K, H - 5 kOe; 2 - 7L-and 44 kOe; 3 - 4.2K 6id 34 kOe;-4 - 78K and 150 kOe Card 3/4 ACUSSICIN n: AP4031l38 ZNCLOSIME t 02 w Af r AW411U AW Depenidence of change In resistance on the magnetic field when the field in perpendicular to the (0001) axis. Curves 1 - T 4 1!K 2 78K Car4-4/4 (a - linear scale, b - logarithmiO5 ' I ACC M APMIYA SOVX:x CODN: 'AUTHW% Alauems)d3r~ x. Ye. Mostituto of Acadow of Sciences SSSR (Ingtitut f1tipleakilch Vroblft Akadadi 33&1* SSSH) TITTZi Use of ruby to obtain lufMUw taqexatures by adiabatic demMaetixation SCURCZ: Zbwn&l eloperimentallmy I tooraticheakcW fiziki. Pialma v redaktaiyu. Pri'losbaniye, v. 4, no. U, 10, 46"70 'TOPIC TAGS: ruby* "imbatic praicess, paramagnetic cooling, Curie point, low tempera- ture research ABSTRACT: In vlaw of nuwroux d=culties (aW decomposition, lov thermal conductlv-4 Ityp brittlemoss) of the oubstswes pvseft3,y used for sdiabatic~demsgwtization cool- Ing the authars wMwimented with a cylindrical ruby crystal vbose geometical axis v" inclinad -,6o* to the principal crystal axis. The chramium content wat Ai' eadectrompeat (-e,3 koe) was used In most wasurements, but a superconducting- solenoid magnet (-55 kOe) was used in acme of them. The initial ten;=-stur* van 1.4X. An in- &xect pr*osdure hM to be us" to massure the w4patic tauqmmture vben the mupar- cm&wtivg sojenoidl was used. fte tMrAition tempentures of Cd filme evapozsted at )inllrm tampemturs on ous of the polished fuss of the r-ubV was measvied by a vathod described XW the avUiow earlier (unth utern. Conf. an Iim-Temipamture Physics, Mo$- cKw, 3966).' It Is oaae2nded from the results thAt In spite of having a magoetic aus- Ceptibility lower Vban the - poxemagnatic "Its, ruby is perfectly suitable for use in AdI8bWtI0-dCW4PGtftA%IcQ apparstut for the production or infralow temeratw!es. :[f a field of --90 We is used, the final temperature can reach -0.05K. Since the curie point of ruby may The quite 14%4 It can be used in mazw cases as the second stAW* in twt-stage adiabatdv-demegnetimtion apparatus. Ruby can also be used in cyclic ix~- stallatlon, we than the use of superconductift switches may be more convenient than, in instal.1stiosta vith paramagnetic "Its. Ruby is especial3y convenient for the In- v*aUvLtion or thIA statal and semiconductor film at in-fralow temperatures, since its surtIsce am be poUsibed to a high degreep and the crystal itself has a hi&Ahsrual. =ftatlidtW. COS. art* bast 2. haUrS. am CWB-. 2DI MM WMS XWep~S/ OM MWj 0021 M W: 003/ An PRMI 4108, L ^CC MRs 80 E CODE -LfR/0363/66/002/012/.? 56 APT002141) k LJRC i /2ift AUTHOR: N. Ye.; Ageyev. N. V., Shamray, V. F. ORG- Institute of Witallurgy im. A. A. Baykcyv Ac&desw of Sciences SSSH (Ins-titut ;netallurg~l AkadEMli Sauk SSSR) TITLX: The critical temperature or the transition to the superconducting state of ,the 8-phaue in the Nb-Sn-Al-Ge sy*tem SOWCE: AN SSSR. Izvestiye. Neorgsnichaskiye materialy, Y. 2, no. 12, 1966, 2156-2161 :TOPIC TAGS: niobium tin allow* aluminum containing alloy, germanium contair.ing alloy. euperd-ondueti &,'cr, anal"on- temperature -alloy transi- t I am teaporature IAB&MCT: act&-&Uoys of the Nb-Sn-Al-Ge syste 'a with various contents of the alloyIng i elements were levitation malted from 99.82-pure niobium and 99.999%-Vure aluminuing tin and*germanium. homogenized at 600C for 250 hr and water quenched. Kb3sft, NbjAl nd Nb3G* compounds were found to have a teaqperature of tranoftion to the su~rconducting state (Ter) Of 18-1, 17.4 and 7.1K. reopocti,vely. With Inc asiag Sn content, in alloys of the psoudobinary n ISM463~d **ction, Ter gradually decreased. reached a minimum at the Sn:kl ratio of 131. and gradi-tialy increased again with a further increase In the SOL tant. I* alloys oil the Xb3Sn-Nb3Ge section, Ter dropped &harply with ,.-Card 113 9; 1 Fig. 1. Critical temperatures OV) of alloys of the - 3tb3SU-Nb3A1-*b3G* sectiou xpr 41 Cd, 2/3 AM N& APT0024031 an increase of Nb3G& content to about 702. and then remained almost constant. WLth small Inemwas in the On content of alloys along the Nb3A'-ffb3Ge section, T alithtly increased to a maximum in an alloy vith a 4:1 Al,.Oa ratlo, anic" decreased continuously vitb Increasing Ga content. The AOC NRI APT002403 CompDaition dependence of T., 3 in the Nb Sn-Kb3Al-Nb3Ge section is shmen in FIg. 1. Ihe critical temperature T was also found to increase wil:h the incrassing dogree of ordering of the iltvastisated alloys. In the Nb-&t-%U-Oa eyetemb the value of Tc appears to be determined mainly by the. density of states at the Fermi surface. Orig. art. hai:' I figures. am cous: u, 2o/ auzx DATz: ogxar66/ o.Rio REr: OOT/ OTH REP: 008/ ATD I Card 313 ACC N;tt AP7001546 ---SOURCE. CODE:- WC020/66/171/003/0566/0569 AIMIGR: AIC-k8cy4IVakI;j,,U_,,T,%s, (Corresponding -member AN 5SSR); Dubrovin, A. V.; V. I.; Fedotov, L. N. ORG-. Central Scientific Research Institute of Ferrous Metallurgy im. 1. P. Bardin (TuentraL'tiyy n4uchno-iusledovatel'skiy inutitut chernoy metallurgii) TITLE: Basic properties of 65BT-type superconducting alloy wire in sper-Imcna and solenoid4; 5OURCE: .0 55SR. DoIclady, -j. 171, no. 3, 1966, 566-569 70?':C 7A,33. suporconducting alloy Iniobium titanium alloy, zirconium conti.ining alloy, r~iobium; titanium alloy wire, alloy wire superconducting property AMRAC7; A r4thad of protecting superconductors from dam3ge during the transitlon from suparconducring to normal state has been developed. The 65BT superconducting niot-iurrit art lum alloy wire (65% niobium and some zirconium) was developed by tze 'Institute of Precision Alloys at the Central Scientific Research Institute: 1 of Ferrous Mtallurgy. At 293, 77 and 20K the wire has a tensile stri-n th of $1. 140 amd 192 kgjmm2' a notch touthness of 18.5, 5.8 and 4.4 kg/Zi. =d -a resistivity of 70, 59 and 56-10- ohm-cm, respe -ctively. The cr:,tical temperature of the wire is 9.71C and the critical magnetic field at 4.2K is 9:# kiLo-oarateds. It was found that a .thin copper coating effectively tMG9 .537,312 6f. ACC MR. AP7001546 prevents wire dwmge durIng the transition from:the superconducting to the nornaa stato. Wire 0.2$ = in diavater wasi coated with a layer of copper, Iq-20 p thgck, and used for solenoids with field intensities of 19 and 54 ki-lo-ocrateds. The solenoids withstood long periods of operation and proved to bo stable and reliable. They were used ir. studying galvanomagnetic properties of pure metals In semiconductors, in investigating. the critical paramters of materials, etc, DrIg. art. has: 4 figures'and 2 Eibli4'.7 SUB ODDE: 11. 09, 20/ CM-1 D&W 30jul66/ OIRIG REF: 001/ OTH REF: 003 ATD PIXSS: 51LI 212 ACC Nts AP' "2Q3 SOURCE CODES UR/0363/67/003/oolj*0061/0066 A.UrHORt Jaakneyevoklys if. 'ro.1 SamsorAw, G. V.; Shulishova, 0. 1. =2 Lwtitute of Pht6rials Science Probl=sp AcadxcV of Sciences, UkrSSR, Kiev i (Institut probl= matorialovsdardys Akademli rAuk tkrSSR) i TITLES Superconductrtivity of solid solutions of transition metal carbides ani nitrides, SOMEs AY $3SI'L Xwestiya. Hoorganichaskiye, nateri&3,v, v. 3, no. 1, 1967, 61-66 TOPIC WS: srupordamduotivity, carbide, nitridew transition metal co=oound ABSTRAM 71h* twriperaturoa of transition to the superconducting state were atudied in systems of solid ablutions TIC-NbC, ZrC-NbC. HfC-NbC. ZrC-TaC, HfC-T&C, HI*C-xoC, TaC-MoC, hbC-NbN &W T&C-NbC, constituting a class of compounds with a face-conterod cubic Nacl-"* latUce. The transition toweratures were determined from tlo change in the mutuAl Induation of the masuring colis on an alternating current bridge. All th,* VaIU*3 of the tritical temperature were extrapolated to a zero magnetic field. For all syutemn excapt T&C-NbC, a nonlinear chAng* of the critical temperature with the composition was established. The observed regularities in the change of the critical temperature in these solid solution systems are an&3,vzed, and it is -po3tu- lated that change of T with the composition results from a changae 4,-& Us density of i the eleetrcm %tA#&* &-ig. A. 1w% 11 figure, 7 tables and I for=O,. SbB COM 0?,20/ OUBM DATM 154i&1 = XVS 004/ OTH REFS 013 Cwd umi 537.312 62 ACC NR,AP-~ODMI (A) SouRcE CODE-.- UR/0126/67/023/001 AU1.110R: AlekseyevakiY, N. Ye.; Ivanov, 0. S.; Rayevskiy, 1. 1.; Step- a noir A OaGt inatitute of Metallurgy Im. A. A. Baykov, Academy of Sciences SSSR (Inutitut metallurgii) TITLE: Phase diagram or the n1obium titanium-zirconium system and superconducting propertibs of its alloys ,SOURCEt Finike metallov I metallovedenlye, v. 23, no. 1, 1967, 28-36 !TOPIC TAGS: nlobi~T5 titanium zirconium .system, alloy phase ~Iagram,, 40 alloy r - &-Y Z"16, ABSTRACTU study 'has been made of several alloys of the niobium-titanium-zirconium sYsten at~five sections with a constant niobius~content of 6. 12. 30, 50 and TO%. Alloys were melted from 99.7%-pure'Lodide zirconium, 99.8%-pure iodide -titanim and 99.7%-pure cemet niobium. Phase diagram of the sylteml at 500, 550, 600 and 800*C vere plotted on the basis of obtained data.it v- f-ivd fr~= the phase diagram that the area of splitting Into two 801id 6*1Ut1on* ONb + 0Zj gradually narrms vith the introduction of titaniun mc: 669-1017:537.312.62 Acc7mhAF7005751 into the alloys. At temperatures below 5250C. ternary alloys of the area adjacent to the niobium comer of the system are in a tvo-phaAe state The one-phase area of Pgb-solid solution at 550-500*C Slqb + aTi-Zr- juts otit into the ternary system along the line bisecting the niobium s,gle of the diagrom. An even decrease of the critical temperature of transition to the superconducting state was observed In alloys which were in the state of B-solid D*lution and vere subjected to a high degree of cold deformation (96% reduction). At a, wap1ste replacement of zirconium with titanium, this decrease was 1-20K (see Fig, 1). In sections at 30 mA 50% (Ti + Zr) of J. Card 2/3 ACC Nth APTOO 5T51 A..., -.. .-_ _*T Mia 40i - oil sit An Fig. 1. Composition dependence of the temperature of transition to the super- conducting state for alloys of the Y niobium-titanium-zirconium system a - 161 Cast specimens; e - (5) cold deformation (90 reduction); sectionsi 3; a o 11 A?.J jo section 17 St SO of xi alloys cold-deformed and amealed at S!jO-C. only a sma-11 iecrease of critical current density in a field of 200000.oerateds vas noticed vhen about half'the zirconium vas replaced vith titanium. Orig. ~Lrt. hav : 10 figures and 2 tables# (TD) SM CODEg JI/ SUBM DATE: none/ ATD PRESS; 511T ACC NRI AP7006124 SOURCE CODEt UR/0056/67/052/001/0040/0041 AMORt Alekno vskAy. H. Yo.; Mikheyeva, M. M. ORG: none ,TITLE: The supercon4uctino properties of aluminum film SOURCE: Zhurnal eksperimentaltuoy I tooretichaskoy fiziki, v. 52, no. 1, 1967, 40-41 ITOPIC TAGS: aluminun, bluadnum film, superconductivity, 044 A ME49- "C)Alrl, C.-C C.q X_ ~000 Al 7" AIWSTRACT; Tits supereoaducting properties of thin aluminum films, obtained by vaporization mad condensation in a 10-6-10-7 set H& vacuum at liquid nitrogen tem- perature and **nealed to room temperature, have been investigated. It was fow.-Id that the critical temperature increases with decreased film thickness. For instance, the critical temperacure of a film, 8.9*10"6 cm thick. was 16280K. while that of a film, 7.9-10 q cm thick. was 1904*K. It is concluded that, since the experimeat was conducted in vaciant, the high critical temperatures of thin aluminum films were not the result of the foxuation of oxide layers on their surfaces. LTD). SUD ODDZtRP20 / $USX DAM none wauv, x4A~ I SM. U.S.; XGMUA, N.Y. 1 SHAPOWNIXOT. Ta.P.; 04hOM A.Lt AMUM. K.A.; MffzOROT, P.L.,- TARAJIO. ?.I.; IIKSVTZVNgJLI .741 AWNW, I.N.1 GRABOTSKIT, V.T.; KNOGGLIMO OUItIvisUou, practlooo for Increasing crop yieldt in Oroxnyy ftovincol 'AirotelibriahavIde wropriiatiia Po povysbanitu Obdulliasti, ilia Oratmenakat oblatti.10 Gro", Gromenskov alaid-vo. P%.1. EOttittratIon of field cropej Poleyodatvo. 1945. 1.78 P. (MIRA 13;8) 1. Or=M. Oblastucy semlInyy otdol. 2. Glavuyy agronom Gro:snauskogo 01satuago vamll"go, otdols (for Milov). 3. Groznenskiy Oblastnoy 1winslou" otdal (tor SkIba, Rogothins. Shatoohnikay, Stepanyuk, Aptokarev). 4. DIrettor Q;Wtuoy stantaii Grawnenskay oblesti (fox Ovalbovskly). S. In*paktor Iuvjwktur7 po.tortoispytonlya sernovvkh L'iftallohnfth kdlltur I trav kiniaterstys sellskogo khozymystya Slum (for Ywomblot). (Orosn.*y Provinas-Iriold crops) ALIMM Y, V.P- (7470T) I I" problem co=ernlng the Jet theory. - Plrikl.mat. i mekh. 22 no.6 - 813~83S X-D '58. (MIR& n: 12) (iota) 10(2),10(4),16(1) AUTHOR- A3.ekseyevskiy.V,P. ZOV/4'-11-2-9/11 TITL---~ ri -1he Velocity Field Caused Ity tlie Acticn ef Inqtantaneous For:es An aot Infinite Layer of an Ideel Incompressible Fluid PSRIO!:1CLLs Ulkrainslkiy natematichaskly zburnal, 1.959, T:~'l 11, Nr 2, PP t99-203 (USSR) ABSTRACTs Tbe academician U.A.Lavrerttlyev eDnjectured that the determinaticn of finite defornations of different media (metals etc.) in the fAighborhood of points of attack of atrong impulsive chargea (wxploaions) can be carried ott apprcximately by the velocity field appearing in an idea'A lncompress~ble fluid by lmyalaiTe ch.arge. With regard to the importance cf the deformation prvblem the author determines the veltoity field in the plane and s4tr4aetric oase. T-,o obtaln-M tiolds show a good qualitative a.11reement vith experimentally obtained deformations of eurfuces of steel platee in the neij~,hborhood of openirgs enlarged by aa explosion. There are 4 figures, and 2 Soviet references. SUBVI"TID.. July 15, 1957 Card 1/1 i~,&CKIJFLYEVE KIY, V-V- *A1WLME7SFM, V.V. CAM TECH SCI Dispertatlow Olavestigation and Calculation or a New Bimetallic Mechanism." 5 xa7 49 ScientUic Council of Sci Res Insts Min of Electrical Industry. .80 Vecheryaya MOSkv4 Sum 71 WINAlactricity - mou", mmuma NOT 49 Xlectric 8yotems, Protection view Series of Thermal Relays," V. V. Alekseyevskiy, Cand Tech Sci, Sci Res Instj Min of Klec Ind, 2 pp "Vest Blektro-Prom" No 11 scribes Type TPA and TIM thermal relays, designed Sci Res Inst, Xin of Elec Ind, intended for pro- Z ~AcUng AC and DC Installation& from overloads. In- Oluaes two photogmphs, tvo graphs, and block dia- 157T35 I kandMat tekbalchemItM nauk; 10SWUN, A.G.. AMR, "TM ~G* 4tvannyy redaktor; LMBMW, N.M.. otystetyenayy redaktor; ARVIWYAN, G.A.. redaktor; SASUUN. ?.A.. takhniCheakly redaktor. [Use of blostals in the construotion of OloCtrie apparatuses] Primiwni* bluetalloy v elektroapparatostroonli. Irevan, lid-To Akadesii nmk Araismakol SSR. 1953. 253 P. (MLHA 8:2) (Zlectric apparatus and applIances) 8(3) SOV/1 12-58-3-3826 Translation from: Referativnyy zhurnal. Elektrotekhnika, 1958, Nr 3. p 45 (USSR) AUTHOR. Alekseyevskiy. V. V. TITLEi -Substation Assemblies (Komplektayye trans for mato rnyy* podstantaii tipa KTP sel'skogo khozyaystva) PERIODICAL: V ob.: Raboty M-va elektrotekhn. prom-sti SSSR po mekhaniz. i awtornatis. nar. kh-va. Vol 1, M. , 1956, pp 118-1Z2 ABSTRACT: An Armenian electric manufacturing plant (Armelektrozavod. Yerevan) produces type KTP step-down transformer -substation assemblies for outdoor installations. 10/0. 4-0. 23 kv with one transformer 20-100 kva, intended for electrification of agriculture. The KTP comprises: an enclosed frameless cubicle (with switch gear) made from sheet steel, and an outdoor oil-type soli-cooled flange-type transformer. The KTP operation in guaranteed with ambient-air temperatures between -350C and +350C. The switch gear and the transformer are mounted on two metal slide rails anti are Card 112 8(3) SOV/112-58-3-_3826 Type KTP Rurad Transformer -Substation Assemblies rigidly fastened to each other by metal strips. The switchgear has two sections, low-voltage and high-voltage. The following 10-kv equipment is mounted in the latter: a 3-pole disconnecting switch, high-voltage fuses and valve-type lightning arresters. Side doors in the switchgear cubicle are provided which open only after the disconnecting switch has been opened by the handle mounted in the low-voltage section. High and low bushings of the transformer are mounted on one of its broad sides and are enclosed in a metal housing. The KTPs are shipped assembled from the factory; only the hich- voltage bushings are dismantled from the switchgear top. The KTP Met&l UtTUCture weighs only 0.4 tons. The overall KTP cost including the maw-iting work is 20-25% lower than that of a standard pole-type outdoor substation. The electric -connection diagram and technical data of KTP equipment are presented. I.S.Shch, Card ZIZ AIJ=EYEVSKIY, V. , inzh.; CIIXTINYAN, Up, insh., 1-1-ATEVOSYAN, M. , inzh. flirpixI~t,d lnsuluta~~ Input for Idgh-voltage units. From.Arm. 6 no.10: 6 3-66 0 163* ~,A, (Min 1,111) - ArripiruikLy ':Ilial Vswoyuznoio nauchnL-isaledovatellskogo irist-Uuta alokt.romoki.aniki. I ' " - ' - ACIC Hka' Aj).60297fi2---* -19OLM CODE r-UPYO,~i%76CI006100tloogglcil06-1 . . e I Aleksayer~iy, V. P. (Kiev) AVMORI ORG: none ,TITLE: Penetration, of a barrier by a high velocity rod SOURCE: Mika gw*n1ya L vuyva, no. 2, 1966, 99-106 TOPIC TAGS: metal property, solid mechanical property. metal stress, deformable pro- ,'ectilo, impact t"t I ABSTRAM An analytical treatment of the problem is given considering three parwnetez of the barrier matarla! as variables: the dynamic hardness, sweific stress of iation and the specific work of displacement. An expression characterizing penetr3tLon lis derived in tores of the rialo of penetratica depth to the length of the portion of ;the rod used up. An experiment conducted an a copper barrier penetrated by an iron m ivith a velocity of 1470 m/soc shoised satisfactory agreement with the expression deriv- ad. The linitatiom of the wTresslon am discussed. Orig. art. has: 2 figures, 17 ,SUB CODE: 11,201 SUM U%TE% I"uXG51 OR113 REF- 00S1 OTH 11EF- 001, UDCi S32.$01.32 cam 1/1 77. AIEKSDYEVSKXYI V,V.; KAUP-ETYAJi, Ye.B., lnzh. -11 .. . ...... Now sarlen of d1stvibution fram5formors with 160 - 630 kv.-a power rating. Vest. alaktroprom. 31, ni).4s25-26 Ap 163. OM 16:10) 1. Chle-n-karrespondart AN krmysnrk-,-y SSR (for AlaV-.s(jyevskiy). 71, T~r~ ACC 0() COMs UR/0292/65/000/009i to/opt-l -N Z*AbW A ArALM); CILUMA CiuWaA v v IV,-- Xlebaftbran. L V M w J; OIA CjW TTTLE9 40atrld WWMW~ 'Up 16 ~100 kW ith p.. -late w4 magnetic wedges SCURM rcit T%~*~~10~'~4# 1 IM rcit 0-13 TOPIC U~Si syriii irl ABST=T'i IiAr ~d, synchronouA~pneratorwup to 100 kw capacity have had f1softn coils e&ddmd ~ Oeiziolos~d ~slfti~ which, hats required much labor for building O,bllity bdo~ MA astA ad to build these machines with genera Po ' 1I prefal-!O-taiad t3W ossttintl-.; rols placed in open *lots and covered "vith :ftuz~fw: WOW OC. 0;r . ti tad, a 90,4-iron 1096-bakalite- rd sition in r an the b:at material for the magnetic wedgmt. 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