SCIENTIFIC ABSTRACT ZAROCHENTSEV, G.V. - ZAROCHATSKIY, V.

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CIA-RDP86-00513R001963830003-8
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S
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100
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November 2, 2016
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September 19, 2001
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December 31, 1967
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SCIENTIFIC ABSTRACT
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669-66 EWP )/EWP(k)/EWf (d)/EWr(m)/T/EWP(I)/EWP(V)/EWP(t)/ETI .. IJP(C) JD ACC NR, AP6028856 SOURCE CODE: UR/0381/66/000/001/0013/0021 AUTHOR: Zarochentsev, G. V. 0R0: TaNTI MPS B TITLE: Attenuhtion of U~irasonic oscillations as a w an5 for studying and inspecting, metal structure SOURCE: Defektoskopiya, no. 1,, 1966, 13-21 TOPIC TAGS: metal heat treatment, ultrasonic inspection, metal property, ultrasonic vibration, plastic deformation, nonmetallic inclusions, phase composition, carbon steel, work hardening, cyclic strength propagation of ultrasonic oscillations in steel. It is sho"M that the *1 f ultrasonic oscillations in steels is a function of phase compositign,1 arbon content, structural form and the degree of coniMm-ation by nonmetallic 4 inclusions. Data are given which illustrate the relationship betueen. the attonuation of ultrasonic o3cillations and structural transformations which .take place in wo3A zones, hoat-affoctcd zones, and areas subjected to vork hardening and considerable cyclic strosocs caused by fatigue processes. ~Cases ara.pointed out in which_tho.stresscd atato of the metal has an ofroct on its acoustic conductivity. Orig. art. has: 4 figures. (JPHS: 35,8043 SUB CODE: 20,, 11 / SUBM DATE: 26Apr65 / ORIG REF: 015 / CTH REF: 015 Card 1/1 --,,/ ITC! ABSTRACT: The author studies the nature of attenuation of ultrasonic.oscilla'- tions in metals and the effect %-diich heat treatment and plastic deformation s I ,have on acoustic losses. Particular attention is given to the condition f 50V/112-5$-22-46876 Translation from: Referativnyy zhurnal, Elektrotekhnika, 1959, Nr 22, p 217 (USSR) AUTHOR: Zarochentsev, G.V. T=: Ultrasonic Metal Teatinglq PERIODICAL: Vestn. Vses, n.-I. in-ta zh.-d. transp , 1958, Nr 3, pp 14 - 20 ABSTRACT: Given are some characteristics of metals (modulus of elasticity, Poisson factor), which can be found from the speed of ultrasonic wave propagation in tests pieces with certain dimensions. From the degree of absorption of US-oscillations at different frequencies, the mechanical. properties of a material can be judged,, The absorption of ultrasonic waves varies de- pending on the size of gra-in, impurities, heat treatment of' metal, etc. M,G.S. Card 1/1 ZAROCTIEVTSEV, G.V., Icand. tekhn. nauk. Cold breaking of railroad raila. Trudy TSNI1 MPS no.154:121-144 158. (MIRA 12:1) (Railroade-Ralls-TeetIng) SOV/137- 57- 1-1380 Translation from: Referativnyy zhurnal. Metallurgiya, 1957, Nr 1, p 183 (USSR) AUTHOR: Zarochentsev, G - V. TITLE: On the Evaluation of the Brittle Strength and Cold Brittleness of Railroad Rails (Ob otsenke khrupkoy prochnosti i khladnolomkosti zheleznodorozhnykh rellsov) PERIODICAL-. Tekhnika zhel. dorog, 1956, Nr 3, pp 21-24 ABSTRACT, Whole railroad rails of the R-50 and R-43 types, made of open- hearth, Bessemer, and experimental converter steel were tested for cold brittleness (B) and dynamic strength at +20, -20, -40; -60, and -800C temperatures. The ak was also determined on standard specimens. The results are presented in the form of charts and diagrams. A chart of the typical fractures of rails under a drop hammer at temperatures from 1-20 to -800 is adduced. The effect of various elements on toughness and B is adduced. Carbon de- creases the ultimate resilience (rupture work) and raises the tem- perature of the transition of the rail material into the brittle state Tb' P and N decrease the cold resistance; As increases the Card I /Z ultimate resilience and raises the Tb' The dependence of B on Si, SOV/137-57-1- 1380 On the Evaluation of the Brittle Strength and Cold Brittleness of Railroad Rails S, and Mn contents was not established. Comparative tests of untreated and of normalized rails revealed significant increase in the ultimate resilience of normalized rails of both the open-hearth and the Bessemer steel; this advantage increases with the decrease in the testing temperature: The work for the break- down of normalized Bessemer rails increased by 1776 at -400 and by 185% at -800. It was established that there is no correlation between tests at ~20 and at _800; hence, industrial acceptance tests performed at ambient ternperature do not represent the true degree of B; the necessity of supplementing these by low- temperature tests is noted. To decrease the B of rails the following measures are recommended: Flaw -detection, improvement of roll-pass design, perfecting of the converter process, and normalization at 8000 with soaking for three hours and cooling in air Z, B. Card 2/2 ZAROCMTSEV, G.V., kand. tokhn. nank; XOZHEVNIKOV, G.I., inzh. Ultrasonic and magnetic testing methods for determining the quality parameters of rail hard-facing. Trudy M911 MPS no,243t 104-130 162. (MMA 16:6) Railroado-Railo--,~Te sting) Ultrasonic tooting) ~ (Magnetic testing) Mm ILL VVIV FRE IR MISOV) V.I., kand. tekhn. nauk; g4qC11,ENTSEV-,-,G.V- Tenting of the atructure of t,,he raetal of spring suspension ro115 for electric locomotives. Vest. TS111I NP-11 113 no-5:34-36 164. 0-11RA 1,7:11) FA~awm NR, Ap4o39638 S1018116W9061006MVASM ALM10Fat ZaroC12611tOGY, Te. V.; Popov, Ve A# TMEs Ground states of biaxin' antifenoomagnitic material SOMEt Flaika tvardogo Wsp v, * 6, no. 60 1964, 3.579-iOS TOPIC TAGS: antiferromagnatic material, antiferromagnstism., aniq0tropio medimm. magnetizabicnq magnetic propert7 ABSTRACTs The ground states of a biaxial antifexTomagnetio dielootr1a are found and compared with the ground states in the'uniaxial caseo The phenomenological* Hamiltonian is written for a biaxial antiferromagnoticp a,,system of siapetic atoms which ie'divided into two magnetic sublattices. Pros this the ground state enogy density In gi7T by IL W JIM) M.'Mj when %.is the MWwtisatlon of the i-th oubUttice in the Vound otate.. is- C'Wd :L/3 Is' ACCIMUM IM3 AP4039638 the constant of the exchange Interaction betwaan sublattices., P-1-P, -P U. - -- ;r am constants of the magnetic anisatropyO and H is the constant uniform external magnetic field. Minimizing So as a function of the oiLentation of MLO leads to-, the determination of the antiferromagnstic growA states an a funotlonW the magnetio field H and of the properties of the crystal magnetic anisotropy* for .0 Iheie: wo'thhe typea of antiferromapaticaj and A;r f4w wWh p and respoctivaly, In the ground state H,, "'A H20 are antipardUal anti directed along the Oz) Ox. and Oy wcos (edges ~c, a,, and bof the rhombio magnetic caU) respea ~"~--'Itively For H j 0 each of the'three types can be subdividod Into 10 cases whic; r Cj~rd 2 HERE! Acassiou NR, AM39630 are discussed in deta4l, The authors thank A. Is Akhiyezer and Ve Go Barlyakht-ar for discussion of the results and valuable advice. Origo art. hut 50 equationsp 33 diagrams,, and 3 tablese ASSOCIATXONt Fiziko-teldudcheskiy institut nizkM te=peratur., Kharkhov Gosuniverr-itet)Rostov-na..,Donu (Pbpicotechnical, institute of Low-TwVerature,, Khnr ov State University) SOHMED x 080ct63 DATE ACO l9Jun64 ML: 00 SUB GMEs SSj, EN NO REF SM 003 MHERs 001 4b Card 3/3. r T ACCESSION NRs AP4043376 6/0181/64/006/008/2489/2494:- AUTHO!~Ss Zarochentsevo Y** V.'; Popov& V. A. TITLEs Energy., spectra and resonant-frequencies of biaxial anti- ferramagnet SOURCE: Fizika tverdogo tela,-,v..6, no. 8, 1964, 2489--2494 TOPIC TAGS: antiferromagn6tigm, spin wave theory, ma4netic aniso tropy, energy distribution,.' resonbLnt state, copper ccnyipound authors have shown earlier (M, v. 6, 1579, 1964) ABSTRACT: The that antiferromagnets with biaxial magnetic anisotropy exist and include CuPl2 .2A20 and Cuga4, In the present article they calculate the energy spectrum of the elementary spin excitationa.(spin waves) of such an antiferroatagnet using the phenomenological theory 9f.sp in, 1 waves, which-in applicable bosj~in-syskem statea close.tothe ground Cord 1/2 'ACCESSION NRt AP4043376 ~-state. The properties of the antiferrowagnetic resonance frequen- c es are also Investigated. The results are compared.with the uni-' axial case. -The expressions obtained for the resonance frequencies in CuCl .2A 0are in satisfactory agreement with those of H.-J. 2 Gerritsen (3 "., ica, v. 21, 693,1 1955) .. "The authors thank A. I. ar for a disicussion of the wo Akbiyezer and V. G. Bar yakht ri and for vice." .Orij. 'axto t~has: 22 formulas. -valuable ad ASSOCIATIONs L$iziko-tekhnLcheskiy institut nizkikh temperatur AN UkrSSR, Kharlkov (Physii~oiiiiftnical Institute of Lovi Temperaturese AN UkrSSR) SUBMITTEDs'. 22Feb64 ENCL,. 00 SUB CODEs .88 NR REP SOVs 22Feb64 OTHER: 002 Card 2/2 ZAROCRENTSEVI Ya.V. (Zarochantawv, IE.V,]l POPOV, V.A. (Popov, V.0.1 -1 - 1 -1 -1- . - ~ ~ , Energy spectra and resonance frequencies of biaxial antiferro- magnets. Ukr. fiz. zhur. 10 no.4:368-381 Ap 165. (HIM 18:5) 1. Fiziko-tekhnicheakiy institut nizkikh tempereCtur AN UkrSSR, Kharlkav. ZARODOV, iWiEL VA6Ii,yi-,VICll EPP. .R92419 ZARODOV, PAVEL VASILIYEVICH, OPYT EKONOMII BENZINA NA AVTOBtJSAKH (EXPERIENCE IN THE ECONOINLY OF GASOLINE IN BUSSES) MOSKVA, AVTOTRANSIZDATt 1955. 26 P. DIAGHS.t TABLES. ZARMOV, Pavel Vasillyevich; SHELYABSKAIY,V,A., radaktor; GAUKTIONOVA, te" M-I Meekly redaktor [Economizing gas on motorbuses] Opyt okonooll benzina na ayto- busakh. Mosk7a, Nauchno-tekhn. izd-vo avtotransportnoi lit-ry, 1955. 26 p. (MMA 9:2) 1. Shofer 29-y avtokolonny Leningradskogo gruzovogo avtotreeta (for Zarodov) (Gasoline) (Motorbuses) ZABODUM, A. G.; PFTHENOV~ T. A..; 'Concerning the Elimination of Protein Opalescence in I/ailein," TTudy 11'auchno- kontrollnogo Instituta Veterinarnykh Pr2paratove Moscow, Vol 3, 19'5?, PP T9 -9 -T. 9 3 F,3 3 , A ft t AUTHOR'S: nak-iv. -i.L. and -Nikitrin, G,S., Zqrosh!;.hi rolling-of alloyr.- ith IA strangt. clevatcd,t n hir h at M- fN-I URC YE allov" (I~VIC-Iliycm; INT ov y y oprotsei3sy obrabotid mot no novyin prota obrab. rict. 'doldndy Sove5lich davleni i v r- Ed. by -.yw V-. D. Golov-1-ev. ---Ioscow-, 'I? s SSR, 'T. -clevatcd temnera-'Ures )r o normally fol n cnc r, OrIt 11 cd on ca,.uip. tT, s e a c IC I-11c t i ult , th-:~ equlpm-nt i2 oftell DVC!--- unal 5 t 0 0 1. z -ind d. tions Cannot be dama- ed. The roDing conal L r, 4L I 10 (1. wit-hout "unwidn- tho st.-Q.,if-th of the i-actal at thc rollin- I'C-'.ICC tile :1resent in-vowti-a-tion 0011ducted On tile !',1-8 67 I - 8 12 6 CC 21 o 6 6 -2 11 .52) and L 6 R '~v i ta 11C ti to !.~Ca~!Urcnlcnts of the roll force P ~Vrerc a onduct ed on' i n. o t s T fr M 90. 0 1(4- v-i t a cros5-4;~c t on r, n"inG f:rom 1.30 to 190 23C) M41-.4 'S' I - x o z; ewrer(- "olled hot (1"130 - 1 30 OC) oil tho roduction fro1z. -tile initia-1, dimert-,ioun, to 7 - 39 Ti x qrcssure i-.ras 'he-macasureMents be-ing 73 1, c 1) Cia t at 1 Cach alloy. The C:Zperir.-I'autal "ralues ol"~- US 6d' to a -1i. esa of the alloy;~z ;~;tudi4d to -vwtioxl~ bY the aVeragge roll prossure - 1- !6 i-- P C's ~t function of ~the_ OP rat 10 w1h er e :Ls the length of doforma~tion_region In a S3.ven pas.s .(calculated or, in some cases-, determip*cd ezzperimentally) and h is the .a~"itfLmetical +Ila th c esz of t1ae specimni' baHro enterim- and aft -Ir kc pa- nre re !Cavilvr The -ranhs produced in Figs. and Tile rc5iilts ritiolm. ill Fi,3.. ralate to alloys -indica,ted-by each Cur Iv.0. - The curves in Fig. relate to the f0lloltiag, alloys: I roll in,, t ermT .1 1 0 5 .3 a r a t ur e t = 1150 1100 Oc) 2.- _42