SCIENTIFIC ABSTRACT L.F. CHUDAREV - L.I. CHUDINA

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December 31, 1967
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SCIENTIFIC ABSTRACT
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- OR/0000/66/0001000 a6o:~4446 CODE: /0124/0127 ~M-0.70&i Prokoshkin, D., A@; Vasiltyova, Ye. V.; Chudarev, L. F. ORG;' none TI-LISt Investigation of creep in niobi\m a3loys by the torsion method ."".`~OURdk~j AN SS.SR. Institut metanurgii. Proystva i primeneniye zharoprochnykh splavoV (Pi-operties and application of heat resistant alloys), Moscow, Izd-vo Nauka,- iO66r 124-127 T07 %C! TAGS: niabium base alloy, creep, titanium containing &Uoy, boron containing a116SK, molybdenum containing alloy, torsion stress -ABSULACT: The- investigation.was made on samples ofnibbium with 5, 8, and 10-weight per.d'ent molybdenum, alloyedwith titanium (up to i0d&), boron (up to 2%), and zirconium (up to 10%). A figure shows the dependence of the deformation on time for different ;V.'~,-teraperatures, obtained by conventional and temperature cycle methods for a.niobium alloy w#4.5%,molybdenum-and 00 ~~% boroni The closeness of the values of the oreep _b rate at the same tomperatur . y the two methods, indicates that the temperature cycle method difi'be used even in the case of complex alloys. To obtain comparative values A. t"-creep rate, the temperature interval of the experiments was varied somewhat as a-fun6tion of the composition of the anoy-. In particular, alloys containing 10% AT03446 titanium and 10% zirconium were tested at lower temperatures. A second figure shows a semilogaritlamic plot of the dependence of the deformation on temperature for a large number of different alloys.. Ahe values of the effective activation energy for creep can be determined from the slope of the straight on the plote On the basis of the experimental results the conclusio n is drawn that It is not possible to establish a correlation between the activation energy for the creep and the activation energy for- nutnAiffuninn- OriM_ nrf. hAjM IIN "rA.R LOOM 2/2 k;WPte),tEWTtm-)/FjWP(wJr/T/EWPtt-j/#ET-1- -IJPtz)- - jD/WW/JG ACC NR; AP6019643 SOURCE CODE: uR/o14q/66/ooo/O03/Ol18/Oj22 ~AUTHOR: Prokoshkin, D. A.;,Vasillyeva, Ye..V.; Chudarev, L. F. ORG: Higher Technical School im. N. E. Bauman (Wsaheye tekimicheskoye uchilishche) VITLE: Investigation of some properties of nibbium, alloys SOURCE: IVUZ. TsvetnaWametallurgiya, no. 3, 1966, il&122, and insert facing- P.-122 MPIC TAGS: niobium, niobium alloy, molybdenum containing alloy, titanium containing alloy, boron containing alloy, zirconium containing alloy, alloy property ABSTRACT: The microstructure, room- and high-temperature hardness, oxidation and.',', creep resistance, ape i;lc weight and electric res* tance have bee%-nvestigated in c Y Nb + 5% Mo alloys ad )% 77 dit4pnally alloyed with M Ti 2% AInd 2% Zr. IThe alloys were-.. melted from 99.78%-Pure1b, 99.95%-pure Mo,. 99%-pure B _iu-id 99.9%--pure Ti and Zr~ -in a. nonconsumable electrode arc vacuum furna ce d homogenized in a vacuum of 10-4 nm Hg for 25 hr: alloys with Ti at i4ooc and ot~e alloys at 1600C. Cast and, annealed Nb-Mo. and Nb-Mo-Ti alloys had a single-phase;Kscrostructure without noticeable dendritA-- liquation. Alloying with boron brought about a clearly defined dendrite structure which'*remained after the addition of zirconium. Annealed alloys with boron contained segregations of a boride phase with a eutectic. Alloys with zirconium contained dis- persed phases with a very complex composition. As the composition of the allaya Card 1/3 669-0-91,018 T. AVAC';17-44 -- ---- ACC NRa AP0196h The rate of creep' calculated from the data on hot hardness showed that boron-containinj ai.lloys,had a-la-wrate of creep, although their hot hardness increased significantly with increasing temperatur;e., This is explained by the strengthening of the solid solution with molybdenum and by,the,form-ation offine dispersed boride precipitates which block the shear planes., - The -oxidation resistance of niobium is- most effectively 'increased by alloying with M and.Ti, which forms (Nb, Mo, )205 solid solution and a 5Nb compound with.monoclinic structures in the cale. Because diffusion ce th 205 2T102 M;e r ce of oxygen, through the lattice of - these phases is much al er than through the I i sl of B-Nb2O5'scale on unalloyed niobium the oxidation r of the alloys with d a of Ti is significantly lowered. Alloying with B and Zr in the amounts investigated (2% each) had no substantial effect on the oxidation resistance of the alloys, Orig. art. has: 1 figure and 2 tables. INS] SUB COIZ: l1/. StJBM DATE: laTan65/ 'ORIG REF: 0071 OTH HEF-. 001/ ATD PRESS: Ca 3/3 m iii d 6' 6 '-corn-es to,an-end."Th A -a~~spec e n rgy 'd lies:td-t investigation of co plex A-4pectrat mu_ltiple~~colhcx ence-lapp m an'aq ace ,ne~crystal_~late~ -photoelectric multiplier-of the is CIW~ analyz=g.c,hannel for. the, registraiioiv~of- P:rray6 alone_-.~.If in, the other channels- iricidenc'es'oi,---y-'quiin'-taL with,-P-partficles occu r*: the anal zing channel can yield the., y -the P-spectra Py j 8,Vy, and ftyly.. With, this' method . -relative intensities of the com--. ponents: of: the, complex.0-spectrum. vrill:ba altered and1he,weak P-COMPOnents become susceptible to4rivestigation.. Also,, such an experiment permits a quasi partition" ofa c6mplex P-spectrum into its. components which in certain cases (for examplet for the'maximum energy of the P-components) yields a more accurate result than isobtained from'the sununary F-spectrum. To investigate the back- -coincid ndes -- d ground of random! e an toxhake measurements on delayed coincidences. (0. 1 to 5 ~L Be 413lay lines arfm placed in.the channels., When the coincidence of th channels is electronically, riot iittairied the e'quiprrient will determine the rando m coincidence, the riumber. of *hich: A a e value of the activity to the. r0 *rtio' ' to tl%c' If quadruple rando I mth,power whert m, is the multiol M: t gf th - otric c coincidences are :regi III,.. their number decrea= extre itere' Y mely rapidly with the Card 2 /3 The method..of inultiple time.. co,.ihc'i(le,nce A scintillation -betawspectrorrxeter'*':.. 8/798/61190.610001-011/012 C8137* and Hiz sotovesl~r a~ 4iierl):crv'staland f6r the twin GsIIIITI%~:er~ftt.l cry stal -is--, 12.1 -wit a.'t,%,~in.CkVrI0 ."zIfiord~_than ZOI7*. In the latter case the Cohipton- on: i e 6 __T' distr. -ray spectrum-F ibuti q.jnt n-, e he -separation of. the- noise and, cosmic rom the, spectrum F7 of the electromagnetic. radiation, of-the 'given P-pr6paration.- by means of the P-4a7y4a"orbing third_ plate-,is- -de.scribed# and-the number of -ab-, sorbed rays is-~naiytically estimated. , Exper1luentally obtained F, and F curves are also -sho .vm. ,The, ~P-;spectrw df p3Z.i - C45 nd. , .-are plotted, in terms of t?e number of pulse re -istered in 3.0 sac# Nvversus~. the energy E, and also as a Fermi-graph.- 4% 9 -correlated, with'the t heoretical curve. The e The Ca spectrum Is d 'viatibas at-thfi -high-energy end are attributed to,-the. inadequate resolution of.the.spectroftieter:iind-.,.~., .-to the randorn summation, of the ~uls.eamplltudes; those at the.low-energy.end are -J"; at%buteAto absorption In the - foil. - The experimental spectrum of a combined Ca + 13'". preparatioa-is depicted -in both-the -N-versue-E and the-Fermiw-graph,~- form. - The random. summation of the amplitudes- of the pulses in a 0- spectrometer.. and their effect on the shape of the:,P--a-pectrum.is analyzed, and it is shown correction for twofold and even threefold random summations should bc.calculate .d in certain cases a - There are - I I figures, 2 tabulated calculation schemes P. and 4 references (Z Rue sian- language.,Soviet papers and Z.Russian- language translations of English- language books-., Beta and gamma- spectroscopy (Author I a name not given). Fizmatgize. Mos_cowvl9�9; Elinore#E.#. Sands#M. Electronics in nuclear Card 2/2 physics.- For. Lit.Publ. House, Moscow# 1953),- sum in 1467 CHUDARS, Ya. E. CHLIDAR.S Ya. E. and TAUM, 1. Ya. im &* AUTHORi TSCHUDARS,Ja. FL - 2760 TITLEt Computation of the Attenuation of a Monoenerget ic Electron Bundle in a Substance Layer..(Russian') YERIODICALt Latvijas PSR Zinatnu Akad. Westiso 1957# Vol 1, Nr 3 (116) . pp Ill - 121 (U43.86R.) Receiveds 5 / 1957 Roviewedt 61 1957 :OSTRACTs The results of the disouseed approximation method for the.cou- cupation of the atten"tion,of a-monoonargetic electron bundle agree with the rem ults found experimentally by G.G.SEELIGER (see table and curve 1, fig. I II)o Electrons range mg/sj -with .energy Seoliger's Formula by Formula by (116v) Value Kea and Pon- Kea and Pon- fold fold Constant: 1,265 Constants 1.24 0996 395 39013 391 09336 95 929T 9595 0,,256 63 5993 6197 0,159 3097 2993 3012 Card 1/3 Computation of the Attenuation of a Monoenergetic PA 2780 Electron Bundle in a-Substanoo Layero The best agreement with experimontalresults is obtained by a modification of the constant of 1,265 to 1924 in the formula found by, Kazand Penfold (see table). This approximation method Was developed with a view of ,correcting the computed ourvest' in the first part bytaking account of the theory of a single scatteringp in the~second part by taking account of the repeated reversecl diffusion of the electron after deviation of the'electron from the bundle. The probability of the penetration of the electron in P(I '0 P(E 09,x PI(E ) + P"(E ), where P(E O,X corr . oqx oPX oPX dej -ppro i'bability of the-penetration of the electron without correction (curve 2# fig.11 - ii)* P (E ) - the oqx correction .factor.for the single deviation afid P*(E 09:) r~- versed deviationa Conclusions$ The probability of the penetration.of the monoenergetic electron Into the interspacie-of up to 3 NOV through the subItance layer is computed bythe fornmla (1) 'Card 2/3 P(E 0 9 St PR Computation of the Attenuation of a Monoenergetic Electron PA 2780 Bundle in a Substance Layer. This formula aneutirs the questiones 1) In what way is:the.zonoenergetic parallel electron bundle attenuated in dependence on the thickness of the matter? 2) In what way does the intensity of the bundle at a certain layer of matter change on the-occasion~of a modification of the energy of the electrons? The computed values agree with experimentally values found by SEELIGER for aluminum, silver and lead. In the case.of the correction of P"(E the formula.00) results for the correction of the coeftfoient for the re- flection of monoenergetic rays of the substance layer. (11 diagrams and 6 citations from publications) ASSOCIATIONs Institute for Physics of the Academy of Science of the U.S.S.R. PRESENTED BYs .SUBMITTED: AVAILLBLEt Library of Congress. Card 3/3 TIZI,,Lnnmd Cougmes.of Nuclear, Spectroscopy (TIZI yeabsessodmoys savembehanly. po yedomay .pektrookopii). I MIMI=: Uspokht fisichaskikh cook, 1958, Val. 63. Sr 4. pp. 721 - 72Z (USSR) ANSTRACT: The ath Congress of XQcl*", Spectroscopy took Ylace In Leningrad from January 27 to Februury 3. 195S. It was attended by 300 scientists from the USSR. further by scientists from ChInap France, Poland, Csoeboolovalls., Hungar7, Zastra, Germany. rugoolawla, and the Honest Democratic Republic. 4 win lectures and about 90 reports more heard. The main lectures dealt with problems concerning nuclear models the a. and P-docars V.r&diatlon. Internal conversion* and unclear Isomerism. 31.34sholepavo Corresponding Homber# Academy of Sciences, USS19 ipestod the conference. Lectures we" hold bys T.Tu. Coacher. Y&. T. Inopin, S.P.Taytko (PTI,AS ukrSSR) on light mantel Poker (W Un-Library AS USSR); Yu.N.Shirokov (11CU-Noscom State University). L.A.SI1v (LYTE-L" _14chnical 7 Institute) at &1t on levels In o and. Al 51 D.C. Alkbasovp A.P.Orluborgp G.K.Cusinsklyo K.I.Y*rokbInsa and 1.1114saberg (LYTI) an having found no rotational levels at I(I NoT in Crs Imp and 31n nuclei. The same research work&ro *Is* j1ported *A jg* discovery of vibrational 7-lavols in W1 , W164. W1 - nuclei by moms of the method of the Cmloab (Kalon) excitation at lsxc~ i NoW. L.K.Pokr 3358) 'Save a survey report: "Concerning Some Particulars In Vibration" levels of Defamed Nuclei". Lectures we" hold also by: D.P.Zaretekly (AN 5532 - A*SSR) on red I&%Ion transition,$ IA Wormed nuclei with the spin - 1/2g V.S. Shpinelt 2 1171 WU (2nd Scientific jog_rnh Institute of Pbyelcow Moscow State University) an the level displacement end the probOllit f dl ' 0 - and J- transitions in odd a uclail V.Fyz:rXrr1YO3fOANn SnSSR - AS USSR) on the laflence of the spin-orbital coupling upon the magnetic moments at the nuc2elp A.X.Baxi (IN 5333 -AS USSR) an the azistono* of light nuclei with high neutron or proton a T.A.Krartsaw (VI-Leningrad PolytochnIc Institute) an the"a" formation of nucleon pairs In oucloil L.L. Col-din. A.A). P111ye# G.K.11ovikovav X.A.Tor-N art Irovy" (TTL A 3 3 SSR) an alpha dsc&Y 60 rotational levels of odd aucloil T.V. X*Ncv (AX S= - IS USSR) an alpha decay of nonspherical Nual-i (Ourvoy)s A.I.Alikhanov, G.P.Yelis.jr.v, Y.A.Lychiszor. T.T.Irablor (M AN 335A) on p.I&sj&.%jon T.mou-sents at electrons emitted In the p-d.qay of To$ a, Lu177, AC 92,53, 1.1a6 (at. 0,1,-~ -1) 48 well me in %hat of 3r 9o and T94 -1)jT.P.1ud*kc. (As $331 - AS a Sralgo. measure- sent of the (0-Y) angular correlations in Bal -decayl I.A.3urgov and Tu.T.Tomkhov (TTL AN USSR) an Investigations of the eleatran-soutran correlations and she resonance scattering of y-radiAtion in v and I.N.Vadshafav (11109-11oloow State University A ';hoobremastrablung of longitudinally polarla*4 electraral A.I.Mukhtarov and Tu.S. Peraw (MOU) on the effective cross section of the scattering of Polarized electrons and positron. at p ar1xvi I*ctranal *I Ta.,I.Chud"s and 1.7a.Tsurs (Riga) an the 4.t.mination or '-wax-rWrOmy of tba component. of the complex P-op*ctma according to the 70rol-disgrams, Z.11.3and. L.E.Eyryanola. end vu.F.Auala., I= (Leningrad State University) on the cos- Putatlom of the probability of the permitted and of the rowlil"as septum of electrons 11a1 a uncives. as 40506 S/263/62/000/013/013/015 AUTHOR: Saulite, U. A.,.~tudam Ya. E. 1007/1207 TITLE: Scintillation P-spectrometer PERIODICAL: Referativnyy zhurnal, otdel'nyy vypusk. 32. Izmeritel'*~*tekhnika, no. 13,1962,70, abs- tract 32.13.508. (Radioakt.iziuc.heniyai metodyikhissled. Riga, AS LatSSR, 1961,123-134) TEXT: A scintillation P-spectrometer is described. It contains a double CsZ(n) crystal in the shape of a 19 x 9 x 2 mm lamella, a