SCIENTIFIC ABSTRACT MOKROUSOVA, A. N. - MOKRUSHIN, S. G.

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CIA-RDP86-00513R001135010001-9
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RIF
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S
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100
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November 2, 2016
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1
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Publication Date: 
December 31, 1967
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SCIENTIFIC ABSTRACT
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R L 5*000 E Ew @];ro6 Kook, 400 M, 0 1 F, VA 4@ tam . ro: q* Alo , , , N@o McnotZOVAS A.11. Experiment in the assembly of autmobile tires. K=ch.i razo 21 no. 5.-54 my- 162. 09M.- 15:5) 1. KirovskLy shinW zarod. . (Tires, Rubbor) FROKOPENKO, A.I.,, kand.seliskokhoz.nauk; HOKROUSOVA,, L.A. Naturalization of a new parasite, Zashall. rast, oft-attd, i bol, 8 no-11149-50 N '63. .I -(MRA 17:1") 1. Abkhazskay'a karantinnaya laboratorlya (for Prokopenko). 2. Star- shiy agronom kbkhazskoy karantinnoy laboratorii (for Mokrausova,). XOTSHOT, G.K., inSh.; KOIMOUSOTA. N.I..Lrjh.; =TAROT, re.P.. kazid. takhn.nmtxk -,*-.--.----- -- Computing plannad car movements an an electronic cal- culatiV machine. Test.TSKII WS 19 no.5,.23-25 160, (KM 13t8) 1. Inmtitat komplakenrkh transpo-.tzWkh problem Akademli. Mak SSSR. (Railroads-Traffie) (Alectronlic: calculating-, machines) PETROVI A.P.j doktor tekbn. naukr pror.; DUVAMAIII S.V.p kand, t6khne nauk; A.BADUROVA., Ye,V,,,, inzho; ZINIHAVIEV, H.M., inzh.; KILWKLM... Yu.S.., inzh.; SX4A?,INA,K.A.S, irte-..; ZLVIYAWV, B.A., kand. tel-kn.nauk; HKOIAM K.A. doktor takhn. nalkj, prof.; VASILIYEV, G.S... kand. takhn', nauk; 13IOWNTAY, 14-A... inzh.; FROLDVI I.A., inzh.; SIDELINIKOV, V.M., in2h.; nzh.; POZAI-WITIRp- E.Lp kand, tekhn. nauL; Z-16-HGO E.A.,q retsenzent; MAKSI-MOVIGII,, D.M.p kand. tekhn. nauk.. roteenzent; EWE.. V.Yu.# inzh,, red. [use of electronic digital computers in compiling train sheets]Sostavlenie grafilca. dvizheniia poozdov na elektron- rqIch tsifrovj-kh.vychislitel'nykh mashinakh. Moskvap Trans- zheldorizdat, 1962. 199'p. (KRA 15:9) 1. Chlenw-korrespondent, Akademii nauk SSSR (for Petrov). (Hailroads-Train dispatching) (Railroads--Electric equipment) AVAITOV, B.S.; MOKROT., A.T.; MEGIMIKOV, YU.T. PSK-1 sliding welding bracket* Kadi. i nafto obor* no*IC41-43t6/+ (HM 17 ej) 1, &Lvad imeni Patrova,, g. Volgogradw AUMV@ W4, t UWAM rca-.VuF-CWM awLtIM of 4all . Kuufakbo 4MIAmtnok". - twi&24-25 At #654 OUR& 2*321 30454 JW 54 S/126/61/DI2/003/009/021 AUTHORS: Xrishtal, M.A., and _@@@V TrJrLP..- Work hardening of surface layers'formed by diffusion of iaolybdenum into iron and its alloys PERIODICAL: Fizika welvallov i metallovedeniye, vol.12, no.3, 1961, 389-394 TEXT: one of the shortcomings of the diffusion method of surface-hardening of metal components is that they produce diffusion layers whose hardness and strength decrease'vith the distance from the surface. Means of attaining uniform mechanical properties across such diffusion layers are required, and a possible method for achieving uniformity in the mechanical properties is described in the present paper, The method proposed in based on the fact that (a) the variation of hardness is associated with the gradient of the alloying element concentration across the thickness of the diffusion layer; and (b) the rate of work-hardening of ferrite dnereases with increasing content of alloying add:,tions. Consequently, a diffusion layer subjected to plastic deformation should work-harden most in its softest part Card I 1@1 el 30454 Work hardening of surface layers S/126/611012/003/009/021 E193/E135 and leastin the hardest region with the maximum concentration of the alloying additions. To verify this proposition a series of diffusion experiments were carried out. Diffusion couples were formed by a molybdenum fail (0-04-0-05 mm, thick) sandwiched between strips of iron or one of the five types of iron-base alloys, containing up to 5 at-% Co, Si, Cr, W, and V. Good cont4et at tite diffusion interface was ensured by spot-welding the components in hydrogen, after which they were subjected to a vacuum diffusion treatment for 10 hours at 1250 OC. Each diffusion couple was sectioned, and microhardness, HJL# measurements were taken across the thickness of the diffusion layer at regular 2.ntervals. @Each type of the specimen was then compressed to 10, 20, 30 and 40% reduction in thickness, after which the micro- hardness measurements were again carried out, the degree of localised deformat�on c, %. in the diffusion layer being deter- mined from the decrease in the distance between the original micrahardness tester@indentations. Frank these data the so-called specific microhardness &HIL/c (where AH,@L in the increase in HIL due to deformation c) was determined which gave the measure Card Z/ XY, 3CJ454 Work hardening of surface layers ... S/126/61/012/003/009/021 E193/EI35 of work-hardenabLlity of a particular region of the diffusion layer. The results are reproduced graphically, those obtained for the 5 at.Y& Co-Fe allay being shown in Fig.3 where FIT, ,L (kg/mm2, lef t- hand scale), &Hp/c, and c extreme right-hand scale) are plotted against the distance (mm).Crow the surface of the diffusion layer formed by diffusion of molybdenum. Circles ind squares denote HIL before and after 40% total deformation, respectively; the variation of localised deformation c in a specimen deformed to 10% reduction in thickness is denoted by white triangles, black triangles relating to specific microhardness (AHILle) of specimens deformed to 40% reduction in thickness. Analysis of these and other results showed that hardness of the diffusion layers studied varied across t,---eir thickness in accordance with the variation of the molybdenum content. The effect of plastic deformation (compression) an the variation of Hpt el and across the thickness of a diffusion layer was also dependent on the molybdenum contents the regions of low Mo content being preferentially work.hardened. This proved the possibility of using plastic deformation to attain greater uniformity of mechanical Card 3@@ 30454 S/126/611012/003/009/021 Work hardening.of surface layers E193/E135 properties across surface diffusion layers. The beneficial effect of plastic deformation was most pronounced in the diffusion layers formed by molybdenum in the Fe-Sis and least noticeable in the Fe-V alloys. There Are 7 figures and 12 references: 4 Soviet-bloc, 4 Russian translations of foreign language articles, and 4 non-Soviet-bloc. The English language references read as follows: Ref.2: C. Austin. Trans. ASK, 1943, Vol.31, 321. Ref.4: C. Austin, L. Luite, R. Lindsay. Trans. ASK, 1945, Vol.35, 446. Ref.5: C. Lacey, M. Gensamer. Trans. ASM, 1941f. Vol.32, Sa. ASSOCIATION: Tul'skLy mekhanicheakiy institut (Tula Mechanical Institute) SUBMITTED: December 19% 196o Card S/126/62/014/002/0o6/oI8 Elll/E192 AUTHORS: Krishtal, M.A., and___W@krov, A.P. TITLE;: Data procn-saing in reaction diffusion PERIODICAL: Fizika metallov i metallovedeniye, v.14, no.2, 1962, 200-204 TEXT; A general method of determining diffusion coefficietits is described and app'lied'to molybdenutn and tungsten solutions in a- and y-iron. The method is especially interesting for elements forming substitutional solid so -lutions in a- and y-ironi and relates to the situation where an a-phase layer grows through diffusion on the y-phase specimen. The-diffusion specimens were prepared from electrolytic@ iron and alloys of Fe + 3% w1w W, and Fe + 1.901i w/w Mo, respectively. The method of melting and annealing was -described in MI. v. 12, no. 3, - 961, 389. For tungsten the diffusion coefficient in a-iron was 9.6 x io- 1-1. cm/sec at 1090 OC and 3.2 x 10-9 at 1280 'C; .Z,n y-iron 5.6 x 10- 11 at 1090 OC and 1.4 x 10- 9at 1250 *C; for Card 1/2 Data processing in reaction ... S/126/62/014/002/006/016 Elll/E192 molybdenum the values were 7.0 x 10- 12 at 800 and 3.3 x 10- 9 at 1250 OC in alpha, the values in gamma being substantially tho same as for a-iron. The activation energy f9r diffusion of tungil-en in a- and y-iron was 71.0 and 81.0 kcal/f atom, respecLivc!), om the entropy change 17 and 23 cal/S atom. C, respectively, For Mo the diffusion activation energy is 57.0 kcal/& atom in both a- and y-iron, the entropy-change values -.@eing 9 cal/g atom. "C, There are 2 figures and 2 tables. ASSOCIATION: Tul'skiy mekhanicheskiy institut (Tula @Jechanical Institute) SUBMITTED: October 20, 1961, initially, and March 201 1962, after revision. Card 2/2 Nacbmism of diffusion in body-centered iron. FIS.wt.i metmuoved. 15 no.14%458 Mr 1.63. .(KML 164) 1. Thl skly '"khanicheekly institut. (Crystal lattices) (Diffusion) . . . . . . . . . ................. ACCESS= uR: APW17364 S/M26/64/(XL7/002/0285/M6? MOR:' Kokrovs A. Pe TITLE: &,a of formation and vacancy concezmr4ioa measurements in irod-molyb- ra asnim alloys OOURC Fizika metallov i-metallovedeniyes v. 2.Tj, no. 20 E 19as 265-287 V,?1C'TAGS: lattice vaca=y, electric riesiAtance iron molybdenum alloy, activa- @ioh energy ABSTRACT: Large- vacangy creation in lattices at high temperatures Introdaces an I idditional electric resistance which is an exponential functiom temperatump thus Ar Y&SM Q3 - inergy of vacancy formation, It - gas constant, T - absolute taqwaturee: I In #vestigation was zv-4e of this resistance as -a function of Usperature in lrmk-. -alloys with variable compos num @01A& @ . It Is shoun that tho vacancy conc n- irAtIon Increas" exW, nenti&14 with Uqwrature, and for a fl=d twperstan the Vt. -card PURCE-60bg: -uitloi~~'(/66/000/009/1076/ioT6I V