SCIENTIFIC ABSTRACT BRYUKHANOV, O. N. - BRYUKHANOVA, L. S.

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LEVIN, A.M.; BRYUKHANOV, O.N. Testinginfrared gas burners. G&z.prom. 6 no.7:18-19 161. (MIRA 17:2) LEVINP I.M.; BRYUKWOV.-- I Flame stabilitj in relation to bickfire -in gas burners. Gaz. prom, 7 no.9:21-24 162, (MIRL 1718) LEVRI, A.M.; BRV-Uh-WXOV. O.R. Investigating infrared-radiRtion gas burners operating on coke-oven gas. Gaz. prom. 8 no.12:20-22- 163 (MI-RA 18:2) naw~hnyy sotrudnik; LEVIN, A.M,, kand. tekhn. naukL.Mj2Eql2Qk, WTUHANOVA, T.A_ ml.;-ldshiy nau!-hnyy sot.-Ldn-ik~ OYSYU7-A,, G4M,~ mlladnhiy- nauchn),7 sotrudnk; KHAYUNA, M.A., znladsh-ly nauchnyj sotrudnlk regimes and ffpectral characteristics of infrared gae brar-,ers. Ispoll. gaza v nar. khoz. no.~03-740 163. (MIRA 18,9) Laboratoriya bytovykh gazovykh priborov Saratovskogo goaudaratvennogo hauchno-Issladovatellskogo i proyektnogo insi;4-tuta po ~spollzovanlyu gaza v narodnom khozyaystve. ~~6 EV,T(1)/SqP(e)/EWT(m)/T WW/jjw' ACC NRt AR6010522 SOURCE CODE: UR/0196/65/000/010/TO05/TO05 AUTHOR: Levin, A. Bryukhanov 0. N. 4~~'l , _4 . e5o TITLE: Problems of combustion stabilityl~ SOURCE: Ref. zh. Elektrotekhnika I energetika, Abs. 1OT36 REF SOURCE: Sb. Iopollz. gaza v nar. kh-vo. Vyp. 3. Saratov, 1965, 116-169 TOPIC TAGS: combustion chamber wall temperature, flame propagation, gas flow, fluid flow, flow velocity, combustion mixture ABSTRACT: Experiments have been performed to determine the value of the critical velocity gradient of the flow of a gas-water mixture and to study the Influence of the wall temperatare of the flame channel on the conditions of the origin of a~,~Iame jump (F ) into brass tubes 6, 8, and 12 min In vestigations were performed oil the limItB of FJ through apertures of ceramic plaL!te rYvvlt~J: th~e aim of establishing the mechanisms of the origin of FJ In flame chan- nels of small diameter. Determinations were made of the most efficient dimensions of aper- tures in M radiation burners. A method Is presented for determining the possibility of the appearance of FJ during the heating-up of the flame channel walls. The Influence of the con- figuration of the flame channels on the FJ was investigated. (Translation of abstract 156 illus-_ Cardl 0_1~ UDC: 662.6 L 42829-66 ARGO10622 tr~jlons and bibliography of 27 titles. V. Sp SU~ CODE: 21 Card 2/2 L 0231"7 EtIT(I)/T I (c) 'C N" AR016569 souna CODE: uR/olq6/65/oDo/Ol2jTO19/TO1q AUTHOit Levins A. M.; Bryukhanov, 0. N. TITLE: Effect of radiative reflux from a heated component on the operating sta- bility of infrared gas burners SOURCE; Ref. zh. Elektrotekhnika i energetika, Abs. 12TT5 REF SOURCE: Sb. Ispol1z. gaza v nar. kh-ve. VYP. 3. Saratov, 1965, 170-174 TOPIC TAGS: IR radiation, IR source, radiation effect, radiative heating ABSTRACT: The authors study theL effect which radiative reflux from the article being heated has on the warm-up of ceramic plates and the operating stability of infrared heaters. Natural gas was used in the tests. The specimen used for heat- ing was a 1 mm plate made from grade 3 steel. Ceramic plates perforated with holes: 1.55 mm in diameter were tested. The results of the study show that an increase in the heat radiatee by the specimen and an increase in the temperature to which the. plate is.heated results in the possibility of flame breakthrough and reduces the reliability of inCrared burner operation.L Radiative reflux during drying and other' types of low-temperature treatment has no effect on the stability of burner opera- tion. 3 illustrations, bibliography of h titles. [Laboratory of Gas Devices]. L. Tragova. [Trzuslation of abstract] SUB CODE; ~ ~,21 LCard 1/1 UDC; 662-951.2 26688 S/056/61/041~005/43/038 ;4Lo 7W (los-r B104/B108 AUTHORS: Delyagin, N. N., Shpinelf, V. S.,.Bsryukhanov, V.A. TITLE: Resonance absorption of 23.8 kev y-quanta by Sn 9 nuclei in 10 crystals PERIODICAL: Zhurnal eksperimentallnoy i teoreticheekoy fiziki, v. 41, no. 501), 1961, 1347-1358 119 TEXT: The resonance absorption of 23.8-kev y-quanta by Sn nuclei in SnO SnO,. P-Sn,and SnNb crystals was studied. Sn119m in SnO was 2' 3 2 ubed.'as gamma source., The. I authorsderived-thej o,rmula 00 - C/0 + 10 a (u) Xf I exp dx I + (X+ W (5) X= E-E. Y E*Vle C =a 'n. r/2 r2l - Of which enables them 't6 calculate t~. of th~ :b..~jtion spectrum 25 measured by experiment. r is the total width of an absorption level, v the relative velocity between source and absorber, f' is the absorption~ ,Card 1/6 26688 S/056/61/041/005/003/038 Resonance absorption of B104/B108 probability of a I-quantum without recoil, r, is the number of atoms on 1 CM2 of the absorber, x is a parameter determining the contribution of 4o the investigated y-quanta to the overall counting rate. The line width in the resonance absorption spectrum as a function of the thickness of the absorber is derived from formula (5). This formula is discussed for cases where 1) the source contains nuclei of an isotope, 2) the emission lines are split up, the absorption lines are not split, and 3) the absorption lines are split, too. Because of quadruple interaction, the Sn 119 ground state is not split*(spin 1/2). Consequently the'absorption spectrum consists of two lines of equal inten'sity. The distance between these two lines is 1 2 1/2 - e Qq (1 + .1 2 p.where Q is the nuclear 2 zz 3 1 quadrupole moment, andrq is a parameter of asymmetry. For a given velocity v0 the unsplit emission line coincides with one of the two components of the split absorption line. Resonance absorption is then + exp + "0 1 + (x Pe (V0) = %f +x% Card 2/6 ---- 26688 S/056/61/041/005/003/038 Resonance absorption of B104/B108 The resonance absorption of the compounds mentioned above as a function of the velocity of the absorber relatively to the source was determined at nitrogen and room temperatures with an experimental device shown in Fig. 1. The SnO2 source was prepared from tin enriched in the SnI18 isotope up to 920/6 and irradiated by thermal neutrons in a reactor. The absorption probability without recoil was determined from the dependence of F_(v) on the absorber thickness. Results are given in the table. The calculation of f? is possible if the phonon spectrum of a real crystal is known. Calculation of P in Debye approximation is discussed. F. L. Shapiro (un, 32, 685, 196o), V. A. Lyubimov, A. I. Alikhanov (Izv. AN SSSR, seriya fiz., 2 6 1960), K. P. Mitrofanov, V. S. Shpinell (ZhETF, _~Ay 107 P A-0, 983, 1961), and Yu. M. Kagan are mentioned. The authors thank N. Ye. Alekseyevskiy for valuable discussions. There are 7 figures, 1 table, and 20 references: 7 Soviet and 13 non-Soviet. The 3 most recent references to English-language publications read as follows: W. Visscher, Ann. of Physics,.2, 194, 1960; H. J. Lipkin, Ann. of Physics,.2, 332, 1960; S. De Benedetti, G. Lang, R. Ingalls, Phys. Rev. Lett., 6, 601p 1961. Card 3/6 Resonance absorption of ... ASSOCIATION: Institut yadernoy fiziki universiteta (Institute University) SUBMITTED: April 27, 1961 26688 3/0 56,/61 /041 /0 0 5/003/03 8 B104/B108 Moskovskogo gosudarstvennogo of Nuclear Physics of Moscow State Fig. 1. Experimental device. Legend: 1) Pulley; 2) cam; 3) contact disk of the amplitude modulation device; 4) holder for absorber; 5) source; 6) palladium filter; 7) lead collimator; 8) low temperature vessel; 9) absorber; 10) lead collimator; 11) NaI(Tl) crystal; 12) photomultiplier. Card 4/6 S/128/61/000/003/004/008 A054/A127 AUTHORS: Levin, A. M., and Bryukhanov, 0. N. TITLE: Drying cores by means of infra-red gas burners PERIODICAL: Liteynoye proizvodstvo, no. 3, 1961, 10 TEXT: In drying small-size cores, tests were made to replace the electric infra-red lamps by infra-red gas burners, pm-3 /GII-3/ type, 400 1/h capacity, 3,320 kcal/h temperature load, 57 - 60~o of the total ra- diation heat produced by the burners is reflected from ceramic plating heat- ed to 800-9000C),. Infra-red gas burners are more reliable than electric lamps and have also a higher radiation capacity (9 kcal/sq cm), while the drying costs are reduced 6 - 10 times. However, when placing the test spec- imen (made of sand-clay mix, with a 8.5%,humidity content, and D = 66 mm, H - 22 mm) at a distance of 200 mm from-the burners, under a gas pressure of 156 - 172 mm water column,_With a surface temperature of 2200C, for a period of 20 minutes, the core center was not dried. Upon raising drying time, the core-edges got burnt. Better results were not obtained even when Card 1/2 B/128/61/000/003/004/008 Drying cores by means of infra-red gas burners A054/A127 increasing the burner distance to 300 mm. The specimens could be dried com- - pletely when a break in radiation was made every 5 - 7 minutes. The drying process took 50 minutes, including interruptions, with a net drying period of 40 minutes. There are 2 figures. ASSOCIATION: Saratovskiy nauchno-issledovateltskiy institut "Giproniigaz" (Saratov Scientific Research Institute "Giproniigaz") Card 2/2 BRYUKRAN,OY - -- --- Constructive cooperation. Sov.profsoiuzy 5 no.7:23-27 i1 157. WaA 10. 8) I.Predsedatell savkoms profsoyuza Sumskogo ordene, Lenina r, shino- 'a stroitellnogo zavoda imenj Frunze. (Sumr-Machinery industry) BRVnMANOV, V.; KULTURIN, A. ~-'Cdfiitk~tion on "Novyi Ural* State Farm. Sall.strol.11 Li.e.12J no.1:15 Ja 157. (MLRA 10:3) 1. Direktor sovkhoza "Novy7 ural" Chelyabinskoy oblasti (for 'Bryukha- nov) 2. Sakretarl partiynoy organizataii(for Khalturin ). (Chelyabinsk Province-Gonstruction industry) BRYUMNOV, V.A., Inzhener; KAIWINSMY, V-1-, inzhener, MOTIN, Yu.G., M inzhener. The high degree of general mechnization in the One-Chuna Forest Industry Establishment. Mekh trud.rab. 10 no.1:20-24 Ja 156. OQU 9:5) (Krasnoyarsk Tarritory--Liimbering--Vachinery) P14BE I BOOK EUWITATION SOV/3682 Bryukhanov, Valent evich Mirovozzmaiye K. E. Tsiolkovskogo i yegO BaUCIMO-tekhmicheskoye tvorchestvo (K. E. Tsiolkovskiy's'Philosophy and ~Us Scientific add Technological Work) Moscow.. Sotsekgiz, 2959. 170 p; 20,000 copies printed. Ed.: A. Arsenlyev; Tech. Rd.: L4. Ulanova. MPOSE: This book is intended for the general reader. COVERAW: T12e book is based an Wolkovskly's published writings and unpublished doements. It was origi-11 planned, as the dissertation of the 2ate author. The book gives a brief accomt 6f Tisiolkovskiyls scientific and technical activities and an apprasial of his work. There are-no references. TkW OF OONTEXTS: Introduction 3 Card 1/2 P. IC. E. Tsiolkovskiy-8 Philosophy (Cont-) SOV/3682 Ch. f. Philosophical VielM Of K- E- Tsiolkovoldy 9 Ch. go methodological Problems of Seience~and Technology in the Creative Vork of K. E. Tsiolkovs1dy. His Contribution to 64 Technical Progress Ch.III. The Philosophical Siviticance of K. E. TeiolkovskiY's works on Space Rockets 3.13 Ch. It. K. E. Tsiolkovskiy's Criticism of Some Varieties of "Physical" I Idealism 137 Brief Conclusion 267. AVAILABLE: Library of Congress . I AC/RN/ec Ca;rd 2/2 7-12-W I ~ 82612 S/056/60/039/001/028/029 J9 4~ CS~2 0 B006/BO63 AUTHORS: Delyagin, N. N., Shpinell, V. S.9 Bryukhanov, V. A., Zvenglinskiy, B. TITLE: The Hyperfine Structure of I Rays'l P oduced by Quadrupole Interactign in the Crystal-Lattice PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960, vol. 39, No. 1(7), pp. 220-222 TEXT: In the introduction to this article the authors describe several publications dealing with the above-mentioned subject. A. I. Alikhanov and V. A. Lyubimov (Ref. 5) studied the resonance absorption of 23.8-kev gamma quanta of Sn119 nuclei. The authors themselves studied the hyperfine structure of the 23.8-kev level of this nucleus. The hyperfine structure is due to the interaction between the quadrupole moment of the nucleus in the excited state and the internal electric field of the tin crystal. Metallic Sn119m served as source, which moved relative to the absorber. Contrary to similar experiments, the source used here q1 Card 1/3 82612 The Hyperfine Structure of I-Rays, Produced S/056/60/039/001/026/029 by Quadrupole Interaction in the Crystal B006/BO63 Lattice underwent linear acceleration within ceftdin limits. Measurements were carried out at the temperatures of liquid nitrogen. The X-radiation of tin (26 kev) was almost completely absorbed by a palladium film 0.06 mm thick. The y-quanta passing through this filter were recorded by means of an NaI(Tl) crystal. The pulses coming from the single- channel pulse-height analyzer were linearly phase-modulated in a radio device, viz. simultaneously with the changes in the source velocity, The modulated pulses were fed into a 100-channel pulse-height analyzer of the type AM -100 (AI-100). Bach channel corresponded to a certain velocity of the source. The measurements were made with two absorbers containing Sn119, namely, metallic tin and SnNb alloy. The dependence of resonance 3 2 absorption on the velocity of the source for a tin specimen 20 mg/cm thick is shown in the upper part of the Fig. on p. 221. The curve has three peaks at 0 and �1-46 mm/sec (velocity of the source). This corresponds to a hyperfine structure of the 23.8-kev level, and is explained by the interaction between the quadrupole moment of the nucleus in the excited state (spin 3/2) and the electric field of the crystal. Card 2/3 82612 The Hyperfine Structure of y-Rays, Produced S/056/60/039/001/028/029 by Quadrupole Interaction in the Crystal B006/BO63 Lattice This interpretation is confirmed by measurements with the SnNb3 absorber (30 mg/cm2), which are illustrated in the lower part of the Fig. The spacing A of the components of the hyperfine structure was ,8 = (eQ/2)g2V/-3z2 . (1-15tO.25)-lo-7ev. There are 1 figure and 6 references: 2 Soviet, 2 German, and 2 US. ASSOCIATION: Institut yadernoy fiziki Moskovskogo gosudarstvennogo universiteta (Institute of Nuclear Physics of Moscow State University) SUBMITTED: May 25, 1960 Card 3/3 8h972 S/056/60/03 9/003/058/058/XX Boo6/BO70 AUTHORS: Delyagin, N. N., Shpinelt, V. S., Bryukhanov, V. A~, Zvenglinskiy, B. TITLE: Nuclear Zeeman EffectYin Sn 119 PERIODICAL: Zhurnal eksperimentallnoy i teore 'ticheskoy fiziki, 1960, Vol. 39., No. 3(9), pp. 894 - 895 TEXT: The present "Letter to the Editor" is the continuation of a pre- vious paper (Ref-4) in which the authors reported on measurements of the dependence of resonance absorption of 23.8-kev gamma quanta emitted in 119M ' the Sn decay on the velocity of the source relative to the absorber. The authors have again carried out analogous measurements, but thie time the absorber was placed in an external constaut magnetic field. In this case, a Zeeman splitting of the absorption line took place, and a hyper- fine splitting was observed in the spectrum, from which the magnetic 119 moment of the excited 23.8 kev level of Sn could be determined. The Card 1/4 84972 Nuclear Zeeman Effect in Sn 119 S/056./60/039/003/058/058/XX B0061BO70 gamma source was a foil of white metallic tin (94% of Sn 118 ) exposed to thermal neutron irradiation in a reactor. The absorber was SnNb 3 in which no quadrupole splitting of the 23.8 kev level -,lakes place accord- ing to Ref. 4. Thus, the observed hyperfine splitting of the absorption line is only a consequence of the Zeeman effect. Fox the measurementap the source and the absorber were cooled to nitrogen temperature. The absorber (20 mg/om 2 SnNb3) was placed between the pols pieces of a mag- net producing a constant magnetic field of 129150 oe in the absorber, and the measurements were made with and without a magnetic field. The ground level is split in two and the excited one (3/2) in four sub- levels under the action of the field. 6 Mi transitions are possible be- tween these. By changing the velocity of the source (positive and nega- tive velocity) 12 lines must be observable. The shape of the absorption speotrum. is dependent on the magnetic moments 1~'J and pil of the ground 119 and excited states of the Sn nucleusl on the rela'-ive signs of these moments; and on the quadrupole splitting Jof thA- excited state. The re- sults of the measurements are repressnted in a diagram 8497- Nuclear Zeemarx Eff eot in Sn 119. 8/056j6O/O39/003/058/058/XX iBoo6/BO70 (ordinate counting rate; abscissa velocity of the source and the corresp nding energy shift). The distance between the hyperfine struc- ture colponente-was determined from the spectral measurement tobe 1 1+0.2).10-7 ev. This is in good agreement with the,value obtained in Ref:17. From the positions of the three maximat A wa a found to be 0 (1.1+0 ) muclear magnetone and the moment of the 23.8 kev level to be 3 11 -.9�0-4) nuclear-magnetons. This value is considerably higher th:n+th(at given by the aingle-particle model. A. I. Alikhanov and Ve A. Ljubimov are mentioned. There are I.figure and 5 references: Soviet U-57man, and 1 French. ASSOCIATION:. Moskovskiy gosudarstvennyy universitet (Moscow state University) SUMITTED: July 4P 1960 Card 3A Card 4/, S/076/61/035/001/012/022 B0041B060 AUTHORS: Cherneva, Ye. P., Barabanov, S. R., Bryukhanov V. A.. Pashkovt A. B., and Tunitskiy, N. N. (A'o-Ecow TITLEs Change in the selectivity of monofunctional sulfonated cation exchangers as a function of the concentration of initial electrolyte solutions and the charges of exchanging ions PERIODICAL: Zhurnal fizicheBkoy khimii, v. 35, no. 1, 1961, 189-191 TEXTt The authors wanted to study the selectivity of the sulfonated cat- ion exchanger of the type KY-2 (KU-2). The exchanger was obtained by. copolymerization of styrene with divinyl benzene and the subsequent sulfonation by means of chloro sulfonic acid. In H form, this resin is a polyacid, while in salt form it is a polyelectrolyte, whose anions are strongly bound to the resin, and whose cations are mobile. The following aspects were investigated through a study of the equilibrium of ion ex- change: a) the dependence of selectivity on the exchanger capacity; b) the dependence of selectivity on the cross linking; c) on the initial Card 1/3 S10761611035100110121022 t/ Change in the selectivity of B004/Bo6o concentration of the electrolytes, d) on the valence of exchanging ions. The weighed-in portion of dried resin was shaken for 35-40 hours at room temperature with an exactly known volume of an electrolyte solution of a known concentration, and the concentration of the components in the solution was then determined. A resin with equal cross linking (7~-), but different capacity (0.16 mg-equiv/1 and 4.63 mg-equiv/1) was taken for the RH + - Ca 2+ system. The coefficient of selectivity was calculated by B. P. Nikollskiyts equation: K (F 1/2 /n 1/2)(n./K ). N, n are the equivalent portions of cations in Ca Ca H resin and in solution, respectively. The following results were obtained for resin with the capacity 0.18 mg-equiv/l: for 0.895 N CaCl 2 K = 0.35�0-1; for 1.90 N CaCl 2 K - 0.12+0.03. For resin with a capacity 4.63 mg-equiv/1, K amountedto 8.99�0.82 for the first mentioned concentra- tion of CaCl 2, and 4-75�0.07 for the second concentration. Resin, cross- linked with 7% and resin with 24% divinyl benzene displayed no change of selectivity in the RH+ - Na+ system. Resin with 7% cross linking displayed Card 2/3 S/076/61/035/001/012/022 Change in the selectivity of B004/BO6O on a rising concentration of the external solution a reduced selectivity in the RE + -Na+ and RE + -La3+ systems. With constant specific loading, capacity, and cross linking, selectivity increased with the valence of the ion charge. There are 1 figure, 2 tablesp and 11 referencest 3 Soviet-bloc and 7 non-Soviet-bloc. ASSOCIATION: Fiziko-khimicheski~ institut im. L. Ya. Karpova (Physico- chemical Institute imeni L. Ya. Karpov) SUBMITTEDt May 13, 1959 Card 3/3 1 '~-7 BRYUKRANOV,. V.A.; EELYAGTN, N.N.; ZVENGLINSKIY, B.; SHFINELI, V.S. Energy shift of gamma-ray transition observed in the resonance abdorbtion of r-quaiata in crystals. Zhur. eksp. i teor. fiz. 40 no.2:713-714 F 161. (IAIRA 14:7) 1. Institut yadernoy fiziki Moskovskogo gosudarstvemogo vniversiteta. (Gamme rays) DELYAGIN, N.N.; SHPINELI, V,S~; BRYUKHANOV,_V~.A Resonance absorption of 23.8 Kev. -C-qunnts. by Sn-119 nuclei in crystals. Zhur. eksp. 4. teor. fiz. 41 no.5:1347-1358 N i61. (MIRA 14:12) 1. Institut yadernoy fiziki Moskovskogo gosudarstvemiogo universiteta. Quantut lattices) SPPINELI, V.S.; BRYUKPANOV, V.A.; DELYAGIN, N.N. Isomeric energy shifts in the 23.8 Lev, gamma-transition in the Snug nucleus, Zhur, eksp. i teor. fiz, III no.6:1767-1770 1) 161. (FlIRA 15.1) 1. Institut yadernoy fiziki Moskovskogo gosudarstvennogo universiteta. (Gamma-ray spectrometry) (Tin) (Isomerism) S/120/62/000/001/003/o6i E032/E5i4 AUTHORS: Bryukhanov, V.A._, Delyagin, N.N., Zvenglinskiy, B., -S-orgeyev, S.K-.and Shpinell, V.S. TITLE: Measurement of the resonance absorption spebtra of gamma-rays in crystals PERIODICAL: Pribory i t-~khnika eksperimenta, no.1, 1962, 23-'28 TEXT: In a pi-evious paper (Ref.5: Zh.eksperim. i teor.fiz., 196o, 39, 220; Ibid 40, 713) the authors described an apparatus which was used to investigate the Mdssbauer effect (23.8 kV gamma-rays on SnI19 nuclei in crystals). In this apparatus the reIntive velocity of the source and the absorber is varied linearly with time with the aid of a mechanical device and the intensity of the gamma-rays corresponding to different valu4s of this velocity is recorded with a multi-channel kicksorter and an amplitude modulator working in synchronism with the device producing the above velocity variation. In the present note the authors, give a more detailed description of the apparatus, including both the mechanical and the electronic parts of it. A typical absorption spectrum for a SnO 2 crystal (9,mg/cm2 target Card 1/2 Measurement of the resonance S/120/62/000/001/003/o6i E032/E5i4 and 6 mg/cm2 source, both at room temperature) is shown in Fig.6 Lig It is reported that t9,,, width of the 23.8 keV excited state of Sn is (2.6 + 0.25) x 10- eV. There are 6 figures. ASSOCIATION: Institut yadernoy fiziki MGU (Institute of Nuclear Physics MGU) SUBMITTED: June 15, 1961 Fig.6 Card 2/2 BRYUKHAVDV. V. ; GDLIDANSKIY, V.I.; DELYAGIN, N.N.; MAKAROV, Ye~F.,* L-Y-L SHPINELI,V.S. Observation of the M*dssbauer effect in a tin-containing polymer. Zhur. eksp. i teor'. fiz. 42 no.'2s637-639 F 162. (MIRA 15s2) 1. Institut khimicheskoy fiziki AN SSM i Institut yadernoy fiziki Moskovskogo gosudarstvennogo tmiversiteta. (Polymers) (Gamma-3:ay spectroigetry) C) 0,4, 0 .A CS 10 cr 0 10 ea 4.,l C~:* ~,,Io coz:, c C-fl -,o OT~ GO s -e 7~q'CL rj . 0 C 01.1 r, P-n. a"; - ~yl .,.Ces'3 . I , C- ,.-1 0 1 ,0 Te S'f, 0 01, 0 sl s ox t he n4c i N4 0 015-f qf~%o ~.Vj ~-,c . .,j . .tie"," 0 010 -5,e .., 0- 0 Be 0 Ve e '15 O.U Ge .e ~e- "0 !T'. 0 -oe 0 e V. ryukhalov V A GollciansklY Sn v', 3 1 ev I ll~ a " 10 V- ~1'1~ I - -o v Y e u lCorytko, Ira Of .-..bssba,aer Slecu Z3 0 of .Pecu, ., UI rest che,,nical 1 e f e n e a and the Tc) elfect V. L5, retiches"-OY Inoy teo L vnurnal e- 448-A52 r T b Iudies on -eir si, n cortinuatiOll - 637, "~62), the au t- V ,--allo-tin COM'DGunds 427 on of 93 .,3-ke anal -V the resonance abs=?~-L eflect in - ) on the one a :,:6ss"O-,uer avples, e-9- Sn(c 6,i5 It - - 119 Iany ex t,_,e::, show . -,oimi , nuclei- on the o that in 00.1,1 -,,-,e us-,'a! I ine S t n c ,,bssb~ucr -i-ituted th 0 titutcd Uroups (-4s,~X4 identical su)z" jibs u s~nolet; ,,illereas vit'll d if 'L ef ent iffe, in -Aidth and ini~ensi'Y, ,,,o lines d dou'olet occu.-s. The Card 1/2 Peculiarities of sneotr&... ~ii 0113 10 on t' e 3:e'io of TJ to X. Tn amorphous media, e.g. Jn r, t- a n1;0 the I,:'bssb.,uez- observed -for the first time. The _,-Iac_- co-_-;-I,oL-iti,)--.. maE the SnO Sio B 2 2 2 and i's sol-'d lline S-i(CH The spectra of crysta 2 0 5 Polymethylmethacrylate and of cr~jtalline Sn(C 21T5)jl, an] 01, it's 210 solution in dichloroethane are identical. Sai.,ic of the ~cta J~ indicate that the ~,ecisive facljoz deteziiini-Irl, the chape of t-he Spectra (isomer shift and OUad-ld-)Oie 3701itutuinf--) are _;Ihe molleculLa: bln~_Z; closest to the tin nucleus. There are 5 ffigurez-j and 1 tablv. ASSOCL'kTION; Tnst-itu' k. niches' him -oy ~izil-i Akademii nail! e of Chemical Physics o-f 'Che Aca-ce-my of Sciienc-3c U~;S.-,'. SUBMIIITTED April 12, 1962 Card 2/2 svt5o MIDAife .0. I p cm-k7 23 1 02/B 10,1 Bryukhanov, V. A., DelyaCin, N. N., C~palenkoj Shpinel.l, V. S. T I TE Some characteristics of spectra ol~' 23.6-%ov Lwm-,.~a ranys laj S-,,119 nucle.-L -21CD-!O,'~- U I'llurnal ekjDcrimentallnoy i teoretic"cz'-.0~1 :~:Lzlcl, Y. no. 2(8), IQ"', A32-477 Th i s paper Give~; some ne-w esults on '.-e ef-f--,ct o.- ~-,n n'ec~e-. cont a-i-ed i- cr-!st-alline com-.:)ounds and a-:,.so tions of t, ~l e resonance absorution saectra. SnI1,41.-I . u introduced into 2 rerved as an The 27.8-'~ev //cm source (thic;~-;iess "5=L- . Ell at, orption . probability wit' Dut xecD41 en~r-y loozes was at - ~ 1.j ull - Ll -- - 77 an-~7 300O X. 5:)ma of the comoounds sho-.i very de-.)endence of this orobcbility. The most M') o a n t r e a r I -. I E~ -)-:?rt-ain-in.~ to the ma,-1,11-tud-a of tl)e chezical iz~,-mer :hi"fts an6 of u can 'oe ~uulitatively ci... e c'- e iz i c a 1bond in the co;,-,~,)ounl-l--. These reL-ul~.rities aze: Card 1/2 Some cha-n--c+~--riS c'nilft in teta-avalent tin c-3-m-)ounu*s --nc- I'::G-- S n C-0 S n I ale ~3tc n Cl LC:..L e , mc-lt S, 1). (2 ) r2:1 " l*co.Mcr 31-lift of the bivale'l-6 c o:.! r oun d -.1! 0'.1 u vrient nes. (3) A .uad::~unole 'no J 'han th-at of the tetra -- - - ;, on oos-,-rve~, v.~ith the b--valent tin co:..- interaction decreasez r.-itl, dec-ea3in: of f0 1107., in -'r C OZL,.) Ou n ae V c~ SI connectc~a 1;.4th the tll. , SrSnO , Bv-%,JnO,l Sr.O,,, Sns k,aSr() 21 , , 0, SIIC! 2H 0 S-,I--. SnBr and S-,(, 21 L.,- ~u z 2 2 2 I O-C)lf I (:Zr\oo,,,-\ - - P a S C G z; ab,sornt4-on ~.~robab il i ty -atios f'~77 \ . 2.,", 5-7, S - 5 , secluence) -1, 1.25, 2.8 , Th-e -intprnretation D--" the i-ezuIts-confirzo t"e S-.-il"9 nuclear excitation raises tl) e e f f - c t I %I -M 0-- OL,:~123S 1,7-,61 There zi:7e 2 f.-Lu:.-a-, ribut ion 17 67 - , 2 3 0 0 IA T 1 O'N7 lnOtitut- ya-',e-:no,.- fiz-i-Ic.J. ITr-l-tule of N7,clic-Lr -"Physic-- of un-i'versiteta k-,.. L State University) I SU31:1,2`21,~D arch 1 1 )62 Card 2/2 S/056/62/042/005/007/050 B125/B108 kUT"HORS; Bryukhanov,.V. A., Delyagin, N. N., Shpinell, V. S. TITLE: Magnetic moment of the 23.8-kev excited state of the Sn 119 nucleus PERIODICAL: Zhurnal eksperimentaltnoy i teoreticheskoy fiziki, v. 42, no. 5, 1962, 1183 - 1165 TEXT: The nuclear Zeeman effect on Sn 119 was investigated by the method oi Moessbauer absorption, using SnO as a gamma source, and tin-iron as 2 well as tin-manganese (MIn2SO alloys as absorbers. Resonance absorption spectra with well-resolved components of magnetic splitting were obtained for 1Yn2 Sn and also for tin-iron alloys with a tin content of up to 10~-'. The magnetic moment was measured cn'tin-;iron alloys containing 1.7% tin (enriched up to 75% with Sn119), while cooling the absorber with liquid nisro-en. All six spectral components were well resolved; their intensi- 0 ties agreed with those expected for an unpolarized absorber. It follows from the data collected in the tables A 0H - 2.80 t 0.06 mm/sec and Card 1/2 S/05 62/042/005/007/050 t'lagnetic moment of the.. . B125YBIOB ,pH - 2.02 � 0.07 mm/sec (~-- - -1.041 of the nuclear magneton, and)t 0 PO denote the magnetic moments of-the ground state and of the excited state 119 nucleus, respectively, H is the mean field strength). The of the Sn isomeric shift of the absorption line in the alloy is +1.36 t Oxi mm/sec. The magnetic field acting upon the tin nuclei in the alloy is 68 - 2 koe. This internal magnetic field depends on the composition of the alloy. There are 1 figure and 1 table. The most important English-language reference is: 0. C. Kistmer, A. W. Sunyar, T. B. Swan. Phys. RGv.t 1239 179, 1961. ASSO.CIATION: Institut yadernoy fiziki Moskovskogo gosudarstvennogo univer- siteta (Institute of Nuclear Physics of Moscow State Universi- ty) SUBMITTEDs December 15, 1961 Card 2/2 BRYUKWOV, V.A.; DELYAGIN, N.N.; SHPINELI, V.S. Magnetic moment of the excited state of the Snl-19 nucleus at an energy of 23.8 Kev. Zhur. eksp. i teor. fiz. 42 no.5: 1183-1185 My 162. (NMA 15-.9) 1. InAtitut jv4dernoy fiziki Hoskovskogo gosudarstvennogo universiteta. - (Tin-Magnetic properties) (Quantum theory) BRYUKHANOV V A.- DELYAGIN, N.N.; OPALENKO, A.A.; SHPINELI, V.S. --------- :~ ~r_ ~~Z - Some characteristics of,141 spectra of resonance absorption of 23.8 Kev. r-rays by Sn nuclei. Zhur. eksp. i teor. fiz. 43 no.2:432-437 Ag 162. (MIRA 16:6) 1. Institut yadeftoy fiziki Moskovskogo gosudarstvennogo universiteta. (Gamma rays-Spectra) (Tin) ERrUKHANOV., V,..A,.; GOLIDANSKIY, V.I.; DELYAGIN, N.N.; KORYW.0, L.A.; I- I ~-, 1.1 MAKAAOVY Ye.F.; SUZDALEV, I.P.; SHPINELI, V.S. Gharacteristics of M~ssbauer sp4tra of tin orgTAc compounds and the role of the nearest chemical", bonds in the Mossbauer effect. Zhur. eksp. i teor. fiz. 43 no.2:448-452 Ag 162. (MIRA 16:6) 1. Institut khimicheskoy fiziki AN SSSR. (M~ssbauer effect) (Tin compounds) BRYUKHANOV, V. A., DELYAGIN, N. N., KAGAN, YU. M., "The Mossbauer Effect of Sn119 in Vanadium, Gold, Platinum and Thallium," report presented at the 3rd Intl. Conf. On the Mossbauer Effect, Cornell, Univ., New York, 4-7 Sep 63. ACCESSION NR: AP4012533 S/0056/64/046/001/0137/0141 AUTHORS: M!Lkha_n9.v,*~,,V4 A.; Delyagin, N. N.1 Kuz'min, R. N. TITLE: Resonance absorption of ijamma quanta in magnesium stannide. 23.8-koV absorption line with natural line width .SOURCE: Zhurnal eksper. i tearet. fiz*,*v. 46, no. 1. 1964, 137-141 TOPIC TAGS: Mossbauer effect, photon absorption. resonance photon absorption, magnesium stannide, recoilless gamma quantum absorption, magnesium stannide chemical bond, recoilless resonance absorption probability, tin 119, absorption line, absorption line width, natural line width ABSTRACT: Continuing earlier Mossbauer-effect studies of tin oxides (ZhETF v. 40, 713, 1961 and v. 43, 432, 1962), the authorylinvesti- gated resonance absorption of 23.8-keV gwnma quanta by Sn 9 nuclei .-over a temperature range from 77 to 290K in Mg2Sn, which has a struc- Card A/ - - X ACCESSION NR: AP4012533 .ture of high symmetry, so that the electric field gradient at the tin-nucleus should be zero. The experiments were also aimed at finding a source of 23.8-keV gamma rays with natural line width. The probability of recoilless absorption of the gamma quanta was found to be 0.77 and 0.28 at 77K and at room temperature, respective- ly. The width obtained for the absorption line in Mg 2Sn was 0.32 + 0.02 mm/sec, -which.agrees'vell with the value obtained from The lifetime of the 23.8 keV'excited state. In view of the pre- dominant role played in Mg2Sn by the interaction between the tin and magnesium atoms, the contribution of the optical vibration is con- siderably reduced for the heavy tin nucleus. In this connection, interest is attached to the study of*compounds with structure iso- morphic to fluorite (P tSn2or 1rSb2 with metallic bonds, where an increased effect of the optical vibrations for the tin atoms is ex- pected. "The authors thank Y,U,. Kagan for interesting discussions of COM -2/1 ---- - -~ ACCESSION NR: AP4012533 the results." Orig. art. hasi 4 figures and,2 formulas. ASSOCIATION: Institut yadernoy fiziki Moskovskogo, gosudarstvennoago universiteta (Nuclear Physic6 Institute* Moscow State University) SUBMITTEDt l8Jul63 DATE ACQ:. 26Peb64 ENCL: 00 SUB CODEt PH REF SOV: 007 OTHER: 003 Card 3/3 BRYUKHA DELYAGIN, N.N.; KAGAN, Yu. 1.9MUMadzi Mossbauer effect on Snug nuclei in a vanadium matrix. Zhur. eksp. i teor. fiz. 45 no.5:1372-1377 N 163* (MRA-17:1) 1. Institut yadernoy fiziki Moskovskogo gosudarstvennogo universiteta. .ACCESSION NR: AP4042372 S/0056/64/047/001/0080/0083 AUTHORS: Bryukhanov, V. A.; Delyagin, N. N.;- Shpinel', V. S. TITLE: Connection between the isomer shifts of the 23.8-keV gamma- transition of the Sn-119 nucleus in metallic solid solutions and the dynamic properties of the matrix SOURCE: Zh. eksper. i teor. fiz., V. 47, no. 1, 1964,- 80-83 TOPIC TAGS: tin, solid solution, isomeric transition, Mossbauer effect, gamma scattering ABSTRACT: This is a consequence of earlier measurements by the authors (ZhETF v. 45, 1372, 1963 and v. 46, 825, 1964) of the iprobability of recoilless absorption of 23.8-kev gamma quanta by Sn119 nuclei in various metallic matrices, which yielded good agree- ment with the theory of the Mosisbauer effects and showed that the results can 1~6 interpreted on the assumptionthat the force con- 1/5 ;ACCESSION NR: AP4042372 1stants are unchanged. In this investigation, the isomer shifts of the 23.8-keV gamma transition of Snl-19.introduced as an impurity in Ivarious metallic matrices were*measu-red. The measurements were made for solid solutions with low tin concentratioili(l--3 at. %) iThe data obtained were compared with a parameter proportional to the effective force constant. A simple. and unique,connection was established between the electron density at the nucleus of the im- purity 7,"-om and the dynamic characteristics of the host metal (Encl. 02). It is indicated that an explanation of the observed relation entails difficulties in view of the great variety in the properties of the-host metals, but several alternate possible ex- planations are proposed. "The authors are grateful to Yu. Kagan for valuable discussions and also to P.,L. Gruzin in whose labora- tory some of the alloys were prepared." Orig. art. has: 1 figure, 2 formulas, and 2 tables. ASSOCIATION: Institut yadernoy fiziki Moskovskogo gosudarstvennogo 2/5. ACCESSION NR: AP4042372 universiteta (Nu*clear Physics Institute, Moscow State University) SUBMITTED: 13Feb64 ENCLs 02 !SUB CODEt NP NR REP SOVs 003- OTHERs 001 3/5 ........... . ACCESSION NRs AP4042372 ENCLOSURES01 2 Values of pararneter ();M,, proporticnal to force emstants 6. JLUjCtX mm/se 0, K A g - +0,20:~0,02 M 4,76 C -0,13 �0,()3 325 6.71 Au +0,15:1:0,02 170 5,69 In +0 96:1: 0,05 12.0 1,91 TI +1,01�0,03 96 1 88 Pb , 20 � 0.05 �i go 1: 63 v o 27�0,04 390 7 74 Pt -0 42�0 04 220 9:44 Fe -0:42�0:06 420 M5 " Pd -0,37�0,03 275 04 8 Sa +0,69�0,03 170 3:43 Card 4/5 ACOMSICN 11R: AP4042372 2 isoffler shifts*vr.. parameter e ~Gurd ENCLOSURZ: 02 mm/ sec Pb Pb TL T, In ,~n Sn 45- A9 -A9 Olu 0 u 40- u Cu C v Pd 0Pt Pd 0 atm. -ACCESSION MRS AP4023912 5/0036/64/046/oo 3/0823/0828 AUTHOR: Bryukhanov, V. A.; Delyagin, N. N.; Kagan.Yu. TITLE: 7ho Mossbauer effect on Sn-119 nuclei in gold, platinum, and thallium matrices SOURCE: Zhurnal eksporimontallnoy i teoreticheskoy fiziki. v-46. no. 3, 1964. S-23-S2S MFIC TAGS. Mossbauer effect, tin 119, gold matrix, platinum matriz.11 thallium matrix, light Mossbauer atom, vibration-speotrum, discrete frequency, recoilless resonant absorption, absorption probability, force constant, alloy concentration affect ABSTRACT: Followini9an earlier similar investigation of the Koss- bauer effect on Snl in a vanadium matrix, (ZhETF v. 43, 1372, 1963). the present study was undertaken for the purpose of an abso'!----,L,- lute comparison of theory and experiment in the case of a light Xossbauer atom, 'when there are no discrete frequencies in the vibration spectrum. To this end. the probability for recoilless resonant absorption of 23.8-koV gamma rays by SnJ-19 was measured in matrices of gold, platinum,.and thallium over a Ado range of tame peraturos. The measurements wore made in solid iolutions of tin in i gold (1-7 and :3.2 at% tin)p platinum (1.3 at% tin) and thallium i Card ACCESSION NRs AP4023912 (3.6 and 9.2 ae& tin). '1he experimental data were compared with the theoretical results of Yu. Kagan and Ya. A. Iosilevskiy (2hRTF v. 42, 259, 1962), "Which.were obtained under the assumption 'that a force i constant remain unchanged. 7he agreement obtained for the probabil- ity of the effect between the experimental-and the theoretical values! extends over a whole range of temperatures and is the same, within experimental error. for alloys with different concentrations. Orig. art. has: 1 figure and I formula. ASSOCIA71ON: Institut yaidernoy fiziki Moskovskogo gosudarstvennogo universiteta (Nuclear Physics Institute, Moscow State University) SUMMED: l8jul63 DATE ACQ: 3.6Apr64 IMCLs 03. OTURs'000 SUB CODRs PH NO RU SM 004 1 ord 2/3 C ILMESSION NR: AP4042558 S/0056/64/046/006/1996/2002 AUTHORS: -Bryukhanov, V. A.; Delyagin, N. N.; Kuz'min, R. N., Shpi- S ------- nel', V.' TITLE: Mossbauer effect in binary compounds of tin .-SOURCE.- Zh. eksper. i teor. fiz., v. 46, no. 6, 1964, 1996-2002 TOPIC TAGS: Mossbauer effect, tin, tin compound, resonance absorp- tion, phonon, lattice parameter, lattice conatant ABSTRACT: To provide.a simple interpretation of-the decreAse.of the- effective Debye temperature e, which is used to characterize the probability of the Mossbauer effect, with decreasing temperature, in analogy with the explanation of the increase in e with decreasing :temperature presented by the authors earlier (ZhETF v. 40, 713, 1961), 119 the authors investig'ated resonanceabsorption of y radiation by Sn. nuclei in the binary compounds SnAs, SnSb, SnTe, and SnPt over a Card ACCESSION.NR: AP4042558 wide range of temperatures A simple model of the phonon spectrum, constructed by superposing-the Debye.and the Einstein spectra, was used in the analysis. The probability of recoil-free absorption and its tengerature dependence for All four compounds cannot be de- s6ribed by a--siIWqle parameter in the Debye approximation. This re- sult is attributed to the influence of the 9ptical branches*.of the phonon spectrum. The measurements of the absorption line widths, quadrupole interactions, and chemical#isomeric shifts are used.to analyze the properties of the chemical bpnds and the structures of the investigated compounds. The structure and parameters of the lattices were detbrmined by x-ray analysis. Although the experi- mental results agreed qualitatively with the model, there was no. quantitative agreement and the observed temperature dependence of 8 exceeded the predictions based on the considered phonon-spectrum model. "The authors thank A. I.' Firov for his assistance." Orig. art. has: 3 figures, 3 formulas'and 1 table. 'Card-, 2/5 ACCESSION NR: AP4042558 ASSOCIATI*ON; Institut yadernoy fi.ziXi Noskovskogo universiteta (Nuclear Physics Institute, SUBMITTED: 17jan64 DATE'ACQ: SUB CODE: SS, NP NR REF SOV: gosudarstvennogo Moscow State University ENCL: 02 007 OTHER: 001 Card 3/5 ? -------------- ,ACCESSION NR: AP4042558 ENCLOSUREs 01 Principal bharact6risties of the Mossbauer effect 71 SnAs �0,02 o,3A:L0,0 0,67�0.03 D,U�0.02 '.?'40.05 1. 2' i45�15 Js0�10 SnSb 0 42 ).a, 0,80�0 0.1 0,70tO I(M )'31� (I" :h 0, M5 0 v I jn�G 144�3 SnTo . 0,16 ~0.01 1 51�0:02 1,4A.3�0,030.17�()0j0 070�0,006 3 1 120t.) 139-3 SnPt 6.3(1�0,04 -0:22�0,02 -0,30�(1,02 0.50� ' 145�15 210:hlo I Compound, 2 mm/se.c * 4/5 Card-- NR. AP4042556 4sr ENCLOSURE: 02 SnPt SnAs Sn5b We Ix I 100 M, ?Af Temperature dependence o 'f-recoilless absorption probability (left) and of the effective.,Debye temperature for the compounds SnAs, SnSb, SnTe, and SnPt BRYUKRANOV.,V.A.: DELYAGIN, N.N.; SHPINELI, V.S. Interrelation between the isomer shifts of the 23.8 Kev. ransition in the Sn119 nucleus in metallic solid oiutions and the dynamic properties of the matrix. Zhur. r eksp. i teor. fiz. /+7 no.1:80-83 J1 164. (1.gRA l?, A .9) 1. Institut yadernoy fiziki Moskovskogo gosudarstvennogo universiteta. BATURF., V.V., glav. red.; red.; TSIIXELI , LJ' red.VOSKRESEN~;KIY, Ye.N., red.; ILID'A, red.; LEMOV, B.N., red.,- LUNCOISGAUZU1, G.F., red.; 1,11MAYA, V.14... red.; MORALEN, V.'V-.., red.; RALKOVETS, O.A., red. (Yethods for the interp7atation of the materialu of aerial photograpIV in geological studies; raterials] Metody de- shifrirovaniia aerofotoraterialov pri geologicheskikh is- sledovaniiakh; materialy. Glav. red. V.V.Baturin, V.N. Briukharov, L.N.TSikkell. Moskva, I?d-vo "Nedra," 1964. 150 P. MIRA 17:7) 1. Vsesoyuzn3ry seminar po geologicheskomu deshifrirovani),u pri geologiclieskikh issledovaniyakh, Moscow, 1961. 2RTUKRANOV, V.N.; SMIRKOV, L.H. ,%.- ONOW Secondary 156. transitional disharmonic (Folds (~ITKUNOV,- V.19.,- KUZ 'MIN, Yu.Ya. Gas prospects in upper Pliocene sediments of the northern Caspian Sea region. Geol. nefti i gaza 4 no.5:20-26 My 160. (MIRA 13--9) 1. Vsesoyuznyy aerogeologicheskiy trest. (Caspian Sea ~fegion-Gas, Natural-GeologT) -PPv.LrMr%o-YI-v.--n.-I tm~ml, V. A. and LTMGMGA=N, G. F. "Aerial Photography in Geological Explorations in the USSR report submitted for the United Ltions Seminar on Aeri4 Survey Methods and Equipment, Bangkok, Thailand, 4 January - 5 Feb 1960 BRYUKHANOV, V.N. Ways of using color aerial photographic materials for geological purposes. Risved. i okh. nedr 28 no.2:9-14 F '62. (MIRA 15:3) 1. Kompleksnaya tematicheskaya, aerogeologicheskaya ekspeditsiya. (Aeronautics in geology) (Photography, Aerial) BRYUKHANOV, V.N., inzh. Problems concerning the normalization of the unit consumption of electric power for railroad traction purposes and analysis of factors affecting this consumption* Izv,vyo*uobebezav.; energ. 4 no.4;45-50 Ap 161. (MM 14:5) 1, Irkutskiy finansoyo-skonomicheskiy institut. Predstavlena kafedrami vysshey matematiki i fizikil, statistiki i obshchetekhr44-- cheskikh distsiplin. (Electric railroads--Current supply) %__ BRYUMMOV, Vlafflmi Mkolayevich starslAy prepodavatell Setting norms for the consumption of electric power for freight train traction purposes. Izv, vys. ucbeb. zav ; elektronekh. 4 no.3:3.59-167 161. iMIRA 11,:7) 1. Kafedra obshchetekhnicheskikh distsiplin Irkutskogo finanso,voekonomicheskogo instituta (Plectric power distribution) (Electric railroads-Current supply) BRYUKRA D-P-inzh. Norm setting for eleotric power consumption for train traction. Trudy LIIZHT no.176sll5-121 161. (MIU 15-.5) (Electric rai3xoade-Current supply) BRYUKHANOV, V.N.; KOZITSKAYAP M.T.; NEVYAZ[iSKIY, I.I. soje problems in the theory of geological interpretation. Trudy VAGT no.8:109-12j' 162. (Aerial photogrammetry) NIRA 15:11) - M BRY(MIANOV, V. N. ""Use of aerophotography for the exploration and appraisal of natural resources" (To be presented orally) report, to be submitted for the United Nations 0 Mference = the Application of Science and Tecbnology for the Benefit of the Less DevPloped Areas - Geneva., Switzerland, 4-2o Feb 63. BHMLJ~IOV, V.~11.,- KOZLOVJ Va. Methods for speeding-up medium scaled geological mapping. Sov. geol. 7 no.6t128-134 Je 164 (MRA 18:1) 1. Vbesoyuznyy aerologiches?.cly trest. BRYUMANOV, V.N.; KOZLOV, V.V.; X LIDI-KONDRATIYEV, Ye.D. Earth under a stereoscope; aerial photography helpB geOlOciSts to determine mineral resources. Priroda 55 no.1:23-32 Ja 16C. (MIRA 19:1) 1. Vsesoyuznyy aerogeologicheskiy trests Yloskva. BRYUKHANOV, V.; REPIN, Yu., doveremyy vrach; PEMOV, K., doverennyy =ach Life dictates. Okhr. truda i sots. strakh. 6 no.11:18QO N 163. (~nRA 16: 11) 1. Fredsedatell Chelyabinskogo sellskogo oblastnogo soveta professionalInykh soyuzov (for Bryukhanov).- UWOT. P.; KOLDUMV. Y.I. [translator]; Impitan I ranga, redaktor; BILIKOV, A.F., redaktor; SKIRNOVA. R.I., tekhnicheskiy redaktor [The navy in the atomic age. Translated from the French] Plot v atomnyi vek. Perevol a frantsuzakogo V.I.Kolimeeva. Pod red. M.N. Briukhanova, Moskva, 1zd-vo inootrannoy lit-ry. 1956. 271 p. (Naval art and science) (HIRA 10:1) (Atomic warfare) BRYBOAMOV) YuvAv, )~.-#:olkcvrfk ~-- -. '-oc~nerat'cn of the AIr Fn:m- w4~li wabnarines, Mor. abor. 48 - -- - 11 !~L%.W.1-46 AD 1t';. (11:RA 18s6) 6~i~Ekxo, F.D.,, polkovnik; BRYUMMOV, Yu.A., podpolkovnik ,- - ~~ a ww, - ~- ~ -~ UBe of aviation in marine landing operations. Mr. sbor. 46 no.7: 42-48 J1 163. (MIRA 16:11) BLIROV, G.F.; BRYUKHANOV, Yu.N. Efficiency of seismic prospecting In the Perm Province portion of the Kama Valley. Geol. nefti J gaza 9 no.1:49-52 Ja 165. (MIRA 18:3) 1. Per!nneft'. D013YSBEVA, S. j.BH11JKR=VA, L. Use of bulls from the Gorki Leninskiye Livestock Farm and their offspring for increasing the butterfat percentage of oows. Agrobiologiia no-4t496-500 JI-Ag 165. (MIRA 18--11) 1. Zaveduyushchaya otdolom -.bivotrovodstva Chelyabinskoy osudarstvennoy sel'skokhozy&ystvannoy opytnoy stanstii for Dobyaheva), 2. Gjavnyy zooWkbnik opornogo punkta po t povyBheniyu zhirnosti moloks. Reepublikanskoy laboratorii pri Chelyabinskoy goeudarstvennoy opytnoy stantsii (for Bryukhanova). "Inv2,Ai-ation -)' th,3 .1 elastic st,!Je." ~ilvx h i ~ I!, -I the I ne list imeni V. 1956. Ur of Cancd6ate in -Phyzicoralheujntic~l Sci.,3"ces)- SO: lh'niz~bnavg i,--to:-,is' No. 22, 1056 -AMIMUNOVA, L.S.; SHCHUMN, Ye.D. Effect of m.arcury coating on the stability of zinc monocrystals at low temperatures [with summary in English]. Inzh.-fiz.zhur. 1 no.8:116-118 Ag 158. (MIRA 11:8) l.Institut fizicheskoy khimii All SSSR, Moskva. . T2inc--Metallography) 7j /\j C AUMORS: Bartenev, C. H. , Bryukhinova, L. S. 57-2-17/32 TITLE, The Influence Exerted b,,7, t,ii-- Irtcrnolccular Interaction, the Cross-Linhin- and the 2e..~I-err7ture Upon the Destruction and the Time Dependence of the Stu~enZ;tli o.' Qlloutc,iouc-Lilze Polymers (Vliyttniye mc-:We11-.u1Z7,tvno~;c vzainodeystviy-a, poperechnoGo U --iiiye i vremennuyu zavisi- sshivani,ya i temperatur na ran.,ushe -, .1 most' prochnosti kauchukopodobny-kh polinerov) PERIODICAL: Zhurnal TeMinicheskoy Fizziki, 195,", Vol. 20, Nr 2, pp. 287 - 295 IUSSR) ABSTRACT; The following nonerjstallizing rabbers were investi-ated here: polybuta-diene-rubbero, b-zatad iene- styrene -rubbers w4 butadiene- -ritrile-rubbers. Cross-linka~;es wore introduced into the rubber by moans of sulfizr-wilcanization in an electric presj at 143 OC. The time from 41-h,-- moi-,iant of the be,7innin,- of strain until the division of the sanplc into two parts (rupture period or life) was measured; It is shovn that the time d-_-,.)endence of the strenCth in rubber-like polymers is differont fron -6hat of solid bodies Card 1/3 and f0110173 the e;!Ijd~ical formula J_ = 11 0"b. With the increase 57-2-17/32 The Influence Exerted by the Intermol-rular Interaction, the Cross-Lizlin,- and the Temperature Upon the DestrucLian and the Time Dependence of the Strenl;!!-th of Cuoutchouc-Like Polymers in the intermoiccular interaction (polarity, cross-lin!:iiZ_ , fil- ling), hoviever, it approaches the dependence characteristic of solid substances. Onc4of the rcasons for the behav:br of the group of caoutchouc-like pol'ymers is their capability of tAolecular orientation on defoi~.iufion. It is fi-zrther sboar, that the tem- ~erature depondcnec c),P the Ltren,-Vi of rubber-like polymers fol- lows the exponential llaw. '..'his temperature-dependence differs from the tc:.iperaturc deponJI-ence of the stren.gth of solid poly- mers by the fact that under variou:j strains no pole occurs at the tomperature-curves, whereas in the case of solid polymers siich a pole exists. This is explained IV the non-exponential dependence of the life of rubber-like polymers on strain. The temperature over tine dependenca of the 3tren~thU~f rubber- -like polymers fol"ovis the formula 9- . C 0' e RT, ahere b and C are constants dependent on the type of rub.)Pr and the structure of thj vulcai.i.zation T)roduct. U is the activation ener- 67. All rubber-lil:o arc in the case of lastin,- cracks eharacteri:Lad W a destruction taking; placo in two sta,--.az. In ',.I first stu~e t'-e rwu~;h surfact- of the place of crack develops, Card 2/3 in the second _ta~-e tlue snocth cne. In Vie case of an elast-ic ~7-2-17/32 on r 3 P '-r: -xerted by the Inte=oleGular Interan' tl;c C -aid The influence 13 the Temperature Upon the Destr,.iction and tho Ti;i~.~ Dependc;rjCe 0-7 thi, st--enath of Caoutclhouc-L-JI-E! NlyMer3 crach the fact is specific th.,t, in noriparison to the solid bo- --ones at 'lie crach-j-,,r-race c~ r-,- -er-l-"he I - bl. J. di4e s , the order or polyr,lers is an inverse one, wb3re the first of breack .4-3 characterized by a fibrous mechanio.-,i of destruction. It is shown that a decrease in strain, of the rumb--r of cross-llinkai;es (the equilibriuin :aodulus), of the inturrolecular irteraction (the polarity) leads to a d-isplacement of the nirror zone by the roti-h one. A cliange cf tenparature influences the rel-ition of the mirror- and the rough zone, in dependence of the 'Kind of rubber, in different ways. There are 10 fi-ures, 2 tables, and 9 references, all off which are Slavic. t, , imeri Pote2kin. Chair oF Theoreti- ASSOCIATION: Peda-ociml Ins-'itute,-Moscow C-11 Physics. Scientific Research Inotitutc of the Rubber Ineu- stry,Mloscow. (Moskovoki.7 peda,,.-ojichcskiy institut ii.-i. Po-tawkina. Kafedra teGreticheskoy fiziki. Naucbno-issledovatellski-y insti- tut rezincvo-y promyshlennosti.Moskva) SUBMITTED: January 24, 11057 AVAILABLE;: Library of Con-ress Card' 3/3 1. Rubber-Test resulAus 2. Rubber-Test methods Likhtman, V. f., Kochanova, L. A., _;-:rvuk.~-,anr, __17; T T I-T'L.'-,' Th--~ TrittTe Destruction of Single Zinc Cr,,sta2s (C) khrupirkom razrushenii monokri:,tallov tsinks) T-1: RI ODIC AL: DoUndy kkadernii naiii, SSS)R, Vol. lln'o, Nir 4, PP-757-760 (ussH ) ABSTRACT: The single-crystal samples were produced frori pure zinc (01q,,Q9 %) bv the method of vone-crystallization which had been develo-oed -in the a.,uthors' laboratory. The rules govern- inU the brittle del-truction of single zinc crystals with different initial or�entatiojis of the basic n1ane w1th respect to the axis of the vire (13 0 00) -,-.ere inves- tigated by means of uniaxial rotation idth constant velocity of the extension (r%.,12 lilo min-' ) of the sam-oles in inactive und surface-active media. A diagram shows the results of the experinents carried out with einf-le z~n ..,c crystals at the temperature of liquid nitrogen. The plastic di-s-lacement pre- cedin.- the destruction is all the e_-e!LTe.r the s,;.aller Card 1 Besides, the normal tenzioriv necesoary for the break in 9he SOV/2o-120-4-10/6',j The Brittle Destruction of Single Zinc Crystals basal plane decrease considerably with ;ncreasing X 0. Thu. brittlP breaking off on the basal plane is facilitated b-,r a previoua displacement in this plane. At relatively hi6h normal tensions in the basal plane a slight displacement Yill al- ready be sufficient to cause elastic. breaking off'. The ex- perimental data ohtuined gave the following results: The so-called Zonke Law of the constancy of vertical noi-mal tensions does not apply to single zi.nc crystals in a brittle state. r1a.-3tic disDIacement causes defects in cryst--l struc- ture which prove to be the original cause of destruction. I-Io "consolidation -when breaking off" was observed in the case of single zinc crystals. The rules governing the brittle de- struction in single zinc crystals at low temperatures apply als*o if transition to the brittle state occurs under the influ'qnce of a strong surface-active medium-(e.g. mercury). A bri.ttle state of a single zinc cry5tal that is caused by mercury satisfies the same general regular rules as the vis- cosity due to low temperatures. There are 4 figures, 1 table, Card 2/3 and 15 references) 8 6of which are Soviet. qlh,~ Brittle Destruction of Single Zinc Crystals SOV/2o-120-4-19/67 AS!i OC T AT ION: Institut, fizicheskov khimii Ak--demii nauk 3iSil I (Institute of Physical Chemistry AS USSR) PRESMMD:: JanuarY 31,1958, by P.A. Rebinder, Academician SLTR4M'bM: January 22, 1958 1. Single crystals-Mechanical properties 2. Single crystals-Te8t~ methods -3. Zinc--Crystallizatibn 4. Zinc--Fracture 001"I 3/j 67397 J -5 0 0 /,p, P-2 00 "fT~ SOV/181-1-9-21/31 AUTHORSt Bryukhanova, L. S., Kochanova, L. A., Likhtman, V. I. TITLE: The Rules Governing the Brittle Dest.ructior~ f Single Zinc Crystals ~I, PERIODICAL.' Fi.zika tverdogo tela, 1959, Vol 1,.Nr 9, PP 1448 - 1456 (USSR) ABSTRACT: The.pre8ent paper offers a contribution to the problems related to modern technical requirements concerning the investigation of the relationship existing between the mechanical properties of-metals and the chemicophysical influence exerted by the medium surrounding them during deformations Firstj a number of pertinent papers is partly dealt with in detail, among others, publications by Lcademioian P. A. Rebinder et al., Kishkin, Iiikolenko,.Ratner, Potaka, Shcheglakova, Rozhanskiy, Pertsov, and Shchukin. The authors of the present paper investigated the rules governing the brittle destruction of a single zinc crystal wire at different orientations of the base plane to the wire gxis (130,, 800) at liquid nitrogen temperature (-196 C) at 0 41A elongation at a constant rate (-12-IL/min). The single crystals 67397 The Rules Governing the Brittle Destruction of Single SOV/181-1-9-21/31 Zinc Crystals were pure to a degree of 99.99%, and were prepared in the authors' laboratory by zonal crystallization. The critical shearing stress in the base plane attained - 130 9/mm at these temperatures and was independent of the orientation of this plane to the crystal axis, as shown by special experi- ments. Mercury was used as surface-active material. Figure I shows the measuring values and the calculated dependence of the limit of the plastic dislocation (a ) of the single zinc m crystals on the orientation angle of the base plane (;Y, ) The (o V+I)sin(4~-~/Y steep decline of a m is described by formula am sin 2 ;(0 where F is the limit of elongation before,tearing, is the final orientation of the base plane before tearing. Figure 2 shows the dependence 'of the normal tension N, acting upon the base plane, on the displacement a -during deformation at different values. The following holds; N - P sin ' sin Card 2/4 TO 67397 The Rules Governing the Brittle Destruction of Single SOV/181-1-9-21/31 Zinc Crystals P is the indication of the dynamometer, proportional to the degree of elongation.-Table 1 contains the values of a mg 'N ms; and Sm (shearing stress) for 6 ;To values in the moment of brittle tearing. Figure 3 shows the dependence of the yield limit P8fand the critical normal tension N 0 at the yield limit anjo at constant S 0 and figure 4 the dependence of * , N S on Y. . F shows a symmetrical course, first M. M. M 0 0 0 * drop with growing to, a minimum at - 45 and another rise; 5 Q ) rises exponen Z, ially with growing, ; a q.) drops 0 0 X0 m exponentiallyt N m(4) rises and Sm(~.) shows a linear drop with growing k0- Figure 5 shows the drop of N m with rising pre-def ormation ('CP're ) at 200C. (The samples were first elongated at room te 'mperature, only thereafter cooled, and further elongated to the tearing point). All these experiments were also carried out under other conditionst the transition into-the brittle state was not attained by cooling, 6t by Card 3/4 the action of a strongly surface-active Poo"+ tu-I ' 67397 The Rules Governing the Brittle Destruction of Single SOY/181-1-9-21/31 Zinc Crystals shows the measured am-, Nm_# and 8m values for this case, and figure 6 the function P(F_) for nonamalgamated (full circles) and amalgamated (emgty(ciroles) single zinc crystals at Y. - 48' and T - 20 a the values coincide within the measuring accuracy). Figure 7 shows a ("") for amalgamated MxAo and nonamalgamated samples at 200C; in the first case a M decreases with in the latter case it rises strongly. Figure 8 shows a m(Xo), %(X,), and Sm(T,) for amalga- mated single crystals0only, figure 9 P(&) for both types at X0 = 480 and T - -196 C, figure 10 Nm. (&. pSe ) for amalgamated samples at 200 and nonamalgamated at 185 C. Shchukin (Ref 15) is mentioned in the text. There are 10 figuresq 2 tables, and 17 references, 9 of which are Soviet. ASSOCIATI01V: Institut fizicheskoy khimii AN SSSR Moskva (Institute of Physical-Chemistry of the AS USSR Moscow) SUBMITTED: February 20, 1958 Card 4/4 S/138/61/000/012/003/008 A051/A126 AUTHORS: Bartenev, G.M., Bryukhanova, L.S. TITLE: Static deformation of rubber-like polymers PERIODICAL: Kauchuk i rezina, no. 12, 1961, 12 - 15 TEXT: Static deformations are defined as being those which remain con- stant. A study was conducted on the deformation of rubber-like polymers under conditions of the relation between tensions and deformations, related to a given time of observation. A single-axle expansion was investigated under static loads of various magnitude for non-filled rubbers, based on non-crystallizing rubbers: CHE (SKB), CKC-10 (SKS-10), CKC-30 (SKS-30), CHH-18 (sKN-2), cKH-26 (sKN-26), CKH -4o (sKN-4o); with high-elastic equilibrium moduli 2.6 � 1 kg/cm2 and 8.8 � I kg/cm2, measured according to the HHMPII(NIIRP) metliod. The following symbols were used: F - weight of the l6ad in kg, So - initial area of the transverse section in cm2, f = F/So - conditional tension or specific load (on the initial cross section) (kg/cm2), 6 - true.tension calculated according to the formula:(5 =?L f, where 7~, - is the multipl'icity of the expansion, ~k- - 1 = 6 - expansion deformation (relati4e elongation). The static moduli E Card 1/2 S/138/61/000/012/003/008 Static deformation of rubber-like polymers A051/A126 were calculated from the slope of the lines obtained (relation between deforma- tions and corresponding true tensions, relative to the same time of observation), by using the Boltsman equation. The following conclusions are drawn; The law of proportionality, previously established for equilibrium deformation of rubber- like lattice polymers is noted also for non-equilibrium static deformations at constant deformations (tension relaxations and at constant loads (fatigue). Thus, in calculating the static deformations within certain limits, the law of proportionality may be applied, if the resilience-modulus is taken into-account as being dependent on the duration of the loaded state. These conclusions were found to coincide with the mathematical theory of Boltsman. There are I figure and 10 references: 8 Soviet-bloc and 2 non-Soviet-bloc. The reference to the most recent English-lano-tage publication reads as follows, F.P. Baldwin, J.E. Ivory, R.L. Anthony, J. Appl. Phys., 26, 750 (1955). ASSOCIATION: Moskovskiy pedagogicheskiy institut im. V.I. Lenina i Nauchno- issledovatellskiy institut rezinovoy promyshlennosti (Moscow Teachers Institute im. V.I. Lenina and the Scientific-Researoh Institute of the Rubber Industry) Card 2/2 28094 s/181/61/003/009/028/039 B104/B102 AUTHORS: Bryukhanova, L. S., Andreyeva, I. A., and Likhtman, V. I. TITLE: Rupture strength of metals and the effect of surface-active metal melts on it PERIODICAL: Pizika tverdogo tela, v. 3, no. 9, 1961, 2774-2778 TEXT: The temperature and time dependences of the strength of amalgamated zinc and gallium-coated cadmium has been investigated. The wire samples were zinc crystals, polycrystalline zinc, and cadmium, Their diameter was 1 mm and their length 10 mm. A contact method was employed to coat the zinc samples with a thin Hg film (5 4) in a mercury-nitrate solution. The cadmium samples were electrolytically coated with a gallium film. A rela- tion between the lifetime and the angle between the basal plane and the sample axis was clearly established for differently oriented zinc single crystals. The values for logT (T denotes the lifetime in see) for every and different loads are located on straight lines. According to S. N. Zhurkov, the activation energy U of the destruction is given by U U0 - TP, where y denotes a structure factor and P the load. Test results fulrash Card 1/3 S/1 871I.M1005100910261039 Rupture strength of metals and B104 3102 13 UO = 35 kcal/mole. This value agrees with those of other authors. Tests of zinc single crystals withX--500 at 20 and 500C show that for different loads the time elapsing till the sample ruptures is considerably diminished by the Hg film (from several days to seconds). The same result-s have been obtained for amalgamated polycrystalline zinc and gallium-coated polycrystalline cadmium samples. It was found that the empirical relation 'r = T0exp (UO kT YP) cannot be used to estimate U0 and y for Zn and Cd samples coated with Hg or Ga films, The effect of the films is not connected with a thermal activation but is the result of adsorption of surface-active atoms. The presence of surface-active substances will not affect the length of the destruction process as long as the normal componet of stress is small. However, if this component reaches a value zorresponding to the tensile strength of the metal, the surface cracks will grow rapidly and cause the sample to rupture. The rate of growth of these cracks is related to the rate of surface migration of the surface-active substance, It is not connected with any thermal activation of the destruction process. There are 6 figures and 10 references: 9 Soviet and ~ non-Soviet. The reference to English-language publications reads a's fl-A 9/1 26094 4--~" S/181/61/003/009/028/039 %\ Rupture strength of metals and ... B104/B102 follows: K. H. Mann et al., J. Phys. Chemistry, 64, 251, 1960. ASSOCIATHON; Institut fizicheskoy khimii All SSSR Moskva (Institute of Physical Chemistry, AS USSR, Moscow) SUBMITTED: May 3, 1961 Card 3/3