SCIENTIFIC ABSTRACT BOBKOV, Y. - BABLOYAN , A. A.

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1. BABYOV'*- 2. USSR (600) 4. Pi-e 7. Continous casting of Dil*s. Eng. Tekh. molod. 21 No. 2, 1953. 9. Monthly List of Russian Accessions, Library of Congress, May -1953. Unclassified. BRASLAVSKIY, M.; SHCHEWKOV., A.; BIATNOV, M.; STROGANOVA, V.; BABKOV, -Ye.- - . . -- . T. Information. Avt. transp. 42 no. 5:55-58 My 164. (MIRA 17:5) 1. Glavnyy inzli. TSentrallnogo konstruktorskogo byuro Ministerstva avtomobillnogo transporta i shosseynykh dorog RSFSR (fo-- Babkov). BABKOV, Yevgeniy. inzhoner. Tt~~ .14.-~,-,-,.>.' Snow plow. Tekh.mol. 22 no.2:18 F '54. "MIaA 7.,2) (Snow plows) BABXOV-FSTFRY%INJ, V.%, inzh. EmDirical calculation of the fastening of slot and wedge boit locks. Sbakht. strai. 8 no.Qi19-20 " '64. (MIRA 17%12) 1. Leningradakiy gornyy institut, - D USSR/MedicineA u l t l 46 e ro erma o ogy ogy FD-29 Card 1/1 Pub. 17-10/23 Author : Babkova, A. A. Title :Electric reaction of the cerebral cortex in skin diseases Periodical ;Byul. eksp. biol. i med. 7, 37-40, July 1955 Abstract :Author reports on her studies of the effect of peripheric irri- tation on the electric potential of the human cerebral cortex under normal and pathological conditions. She used an encepha- lograph to study healthy persons, patients with light-induced dermatoses, and those with "tactil" and painful skin irritations. Author determined that even in fairly insignificant and just adequate irritations of the skin changes in the electric activity of the cerebral cortex are noticeable. 'hanges in the reactivity of the higher divisions of the central liervous system during skin irritations do not depend on changes in disease conditions. Cer- tain electric reactions of the cortex to irritations may result in impulses to healthy as well as diseased parts of the skin. 17 references. 10 USSR, 7 since 1940, no graphs. Institution :Clinic of Skin Diseases, First Leningrad Medical Institute imeni I. P. Pavlov (Dir. - Active Member Academy Medical Sciences USSR 0. N. Podvysotskaya) Submitted :3 Sep 1953 ROKOVA, A.A. Problems of Inhibition in skin diseases.,.Vest.ven. I dorm. 30 no.6: B-14 N-D '56. (MIRA 10:2) 1. Iz laborstorii fistologii I patologii koshi Almdemii meditsiliskikh nauk SSSR prof . O.R.Podvysotskaya), Ieningrad. (RIFIRI, in various die. impaired inhib. in skin dis.) (SKIN DISBASIS, physiol. inpaired inhib. zf reflexes) PODLUBNAYAq Ye,T,j BABKOVAq A.N.1 EPELIMAN# A.A. Ultraviolet absorption spectra of some essential oils and aromatic alcohols. Trudy TSNIISP no. 8:117-122 159. (MIRA 14:1) (Essences and essential oils-Spectra) (Alcohols--Spectra) PODLUBNAYA2 Ye.T.; BABKOVA$ A.N.j-__EPEL'1IANjA.D.; EPELIMANq A.A. Interferometrie method for determining the concentration of essential oils from Zin in solutions. Trudy TSNIISP no. 8;151- 157 159. (MIRA 14:1) (Essences and essential oils) (Alcohols) we 7-P -*V-0 4 0 v 11 it is Is 16 1; a 19 a In 'n a I, a a v A "Im It u III J. . 36 v 38 0 v j A) Pe A I I L T T A M-11111 M 10-194-it-1 1 -0 1 4p 41 Ai m -00 -09 .00 00 jr Ole 00 09 00 "AdArPUT11 PMPCUW Of hOMW &M IMOU" 711111611111941111 LAY&M -M ) -00 and 1. MAvh%A (Comid. md. (tW.) Arad. Nei. VJ(.$-';.. 1941 -11116 80, 11). 32-341).--41n K~rja.j Stable promotc%t Mills ~xl;utr. The almirption rumem for Rrgtm pit , Ill.% it' asul 10 V. 'racticalky illentical tin INVASOW WW unlivotnoted tupwAll.m. 'I'lle AdIvAt"I -00 .imi-iqltion of h%An4mn wW ethylem at ovilinary tetul*raturva it it%. lsoilt-tet. do 0 ~ry ratwh grra ter mi Ow MnIoled tungpten thjuj on the unpinkmoli.l. LIT 4: 6*0 t:69 I1 4,3. In 4 --- 'L --- a0 0%. all &i--cFV . -iw 14 A t 6 WT &LL L V rI,W-KAL~ III 64TURt -CLAttOK.AT00 - . . - .1 _- - r - r 11610413 .19 0.1 Gm jjjjj-C Is It go n- 1 U e 0 0 9 a 0 0 000 0 oleo 0 0 * 00 0 0* *so 0 6 * 0 0 0 0 0 0 4 0 0 0 0 9 6 0 0 0 & a 0 0: 's 0 a * 0 0 q 0 0 0 * 0 0 0 asigiii 0 t jABAKOVAr-Lyubav-LMaksixovn . kand. ekon. nauk [deceased]; KANTER, A~L, tL _'. red.; RAKITINy I.T., tekbn. red. (Production management and organization in an industrial enterprise] Upravlenie i organizatsiia proizvodstva na pronyshlennom predpriiatii. Moskva, Izd-vo "Znanie.." 1961. 39 P. (Narodnyi universitet kuI'tury. Fakul'tet tekbni o-ekonomicheskii, no-5 (MIU 24:10) (Industrial organizations -1 .1' '3"OVA, ". I -I I t , I . "Cperation of -~Lxial Compressor Stages on Nonrated Capacities." Cand Tech Sci, Central Sci Res Broiler and TurDine Tnst, Le,%,ingrad, 1954. (RZMelm, Feb 55) SO: Sum. No. 631, 26 Aug 55 - Survey of Scientific and Techrd~-:al DissertatL,ns Defended at USSR Higher Educational int9titutions (14) AUTHOR: Babkova, M.M., Candidate of Technical Sciencee. 114-6-4/11 TITLE: The dependence of the steepness of the characteristics of an axial compressor stage and its range of stable operation on its design parameters. (Zavisimost' krutizny kharakteris'u-- i1mi diapazona, ustoychivoy raboty stupeni osevogo kompressora ot ee raschetnykh parametrov.) PERIODICAL: 'rEnergomasbinostroeniell (.Power Generation Machinery Construction) 1957, Vol-3, No.6, pp. 13 - 15 (U-S-S .R.) ABSTRACT: Axial compressors used in gas turbines and elsewhere are often :ceqtUred to operate stably and efficiently over a wide range of conditions. But the characteristic curves of axial compressors are steep and have a narrow range of change of output for constant speed. Therefore, in designing axial compressors it is often necessary to investigate the possi- bility of extending the range of stable operation of the compressor by changing the position of the boundary of pump- ing and changing the steepness of the characteristic. Little work has been published on this question. There are two main reasons why the characteristic curves are steep and the output range at constant speed is narrow. The first reason is the great sensitivity of the characteristic of the blade profiles to change in the angles of attack. The second reason is associated with compressibility of the working Card 1/4 medium which, when the working conditions are changed,.alters The dependence of the steepness of the cna.,- an axial compressor stage and its range of stable on its designv ",eters. (Cont.) il4-6-4/11 the best ratio between the sectional areas of the different stages* This article considers several possibilities for improving,the compressor characteristics by appropriate selection of design parameters of the initial stages. T1B problem is examined in its simplest form leaving aside the question of efficiency and using an approximate method of investigation. A diagram is given of the dimensionless triangle of velocities of a stage, and corresponding mathematical expressions are derived for the coefficients of flow, of theoretical,-heads and. of the.degree of reaction., It i's shown that ~~~eristlc's'of ~ih~oretical Sead-Iiinus coefficient of flow are S.traigbt lines which pass through the origin and through certain other points so that the steepness of the theoretical charaeteristios will be greater for small initial values of the coefficient of flow and of theoretical bead, wha%~Dvvr the degree of reaction. It Card 2/4 follows that in order to reduce the steepness of the The dependence of the steepness of the characteristics of an axial compressor stage and its range of stable operation on its design parameters. (Cont.) i14-6-4/n Card 3/4 characteristicsof multi-stage compressors it is advisable to increase the head in the initial stages,. Tests results on various compressor stages show that the regibn of stable operation of a stage is usually characterised by a single value of range of change of angle of attack. -Test results are given for stage characteristics with various degrees of reaction and it i& found that the range of stable oper- ation diminishes with reduction in the degre!q of reaction. The experimerts confirm the theoretical conclusion that a stap a greater degree of reaction will have a greater ran.-SeO*tput and head than a stage with a small degree of reaction.. It is also of interest to compare character- istics which can be obtained by arranging stages with different values of initial reaction. using the--same blading on the runner. The corresponding characteristics are plotted. A graph is also given of the change of--de-gree of reaction with change in the conditions of operation and a graplf of the chAhge- in'the theoretical hea& cmffinient-and degree of reaction with change in the working.conditions. It is concluded that the compressor characteristics can be improved by proper attention to design and in particular I I D ie dopendence of the steepnesi3 of the characteristics of an axial compressor stage and itus range of stable operation on its design parameters. (CO11t.) 114-6-4/11 that -the steepness of the head cbgracteristic of the stage is greater the less the initial values of the coefficient of flow and of the coefficient of head of the stage. When these initial conditions are constant, and the difference between the angles of attack are approximately the same, the range of stable operation of the stage is increased by incre-asing the degree of reaction. There are 5 figuies, and 2 literature references (1 Slav-,c). AVAILABLE: Card 4/4 RABKOVA, M.M., kand.tekhn.nauk, Effect of the distribution of flow coefficients through stages on the rated characteristics of axial compressors. Energomashino- stroenie 3 no,12:27-29 D 157. (KIRA 11:1) (Gas turbines) 44. BABKOVA, M. S. Origin of quartz sands in the western part of the Baikal region. 12'r. v7se uchavo save; geol.1 razr. no-3:57-68 Mr '58. (min 11: 10) l.Iftutskiy gosudarefteaW ualversitst in. A.A. Zhdanova. (Baikal Mountain regie*-15~Lmd) DAVIDKOVIGH, A.S.; GONCHAROV, Yu.G.; GEYZENBLAZEN, B.Ye.; BJABKOVA, T.B.; FRYADKO, V.D.; BELETSKIY, Ye.P.; KOLESNIK# A.S.; Analy,als of the efficiency of work output of the automated ore dressing section in the Krivoy Rog Central Mining and Ore Dressing Combine. Met. i gornorud. prom. no.4:64 JI-Ag 165. (MIRA 18;10) BABKOVA, V.I.; MYASNIKOV, A.L., professor. Demonstration of a patient with non-hemolytic congenital -trap. arkh. 25 no.2:81 Mr-AD 153. (MLEA 6:r) (Jaundice) R"KCIVA, Ye.l. (st.Ternopol", Lt-vovskoy dorogi~ At the Ternopol' Division. Pat; i Put-khOz- 6 no.5.45 :U- (INMI 15,,4) (Ternopoll -"egion--Ra:Llroads-.Ihi-ntenance and repair) z A11THORS: Yesellson, D. N., Shvets, A. D., Bablidze, R. A- 56-1-38/56 'TITLE: On the Film Flow Rate in Solutions of Helium-Isotopes (0 skorosti perenosa po plenke u rastvorov izotopov geliya) PERIODICAL: Zhurnal Eksperimentallnoy i Teoreticheskoy Fiziki, 1958, Vol- 34, Vr 1, pp. 233-234 (USSR) ABSTRACT: The influence of He3 dissolved in He II upon the film flow is, as is well-known, reduced to the decrease in the flow rate. It was of a certain interest to investigate this fact more thoroughly and therefore the authors made tests with a solution of helium-isotopes with a helium content of 1,5; 497; 7,0 and 9,6 %. The apparatus used for these tests consists of two elbows of a thin-walled capillary tube (diameter i,oS mm) of equal leni;ths communicating over a helium-film, The film flow rate R = v6 was measured by the measurement of the rate of change of the liquid level in one of these elbows. In this connection v signifies the rate of the motion of the film and 6- the thickness of the film. The temperature interval immediately following thek- -point was investigated. The results obtained here are Card 1/3 illustrated in two diagrams. One of these diaarams On the Film Flow Rate in Solutions of Helium-Isotopes 56-1-38/56 illustrates the dependence of the fili.,i flow rate on the tenperature and the other diagram -3the dependence of the film flow rate on the content of He . AccordinE to the results found here the film fl?w rate increases with increasing concentration of He . When havint~ data on the dependence of the density on the temperature for the solutions of the helium-isotope8, the following conclusions can be drawn: The filr,,i flow rate in the temperature range investigated here is directly proportional to the density of the su erliquid component: R = A~s/~ , where A - - 3,2.10_~ cm3/CM8ec. moreover the temperature of the phase transition He I - He II for the solutions gi-ven here might be determined from the beginninC; of overflovinG over the film. The values obtained in this conziection are in satis- factory agreement with the analogous results obtained by other methods. There are 2 figurcs, 2 tables, and references, 4 of which are Slavic. ASSOCIATION: Physical-Technical Institute Alf Ukrainian SSR (Fiziko-teklinicheskiy institut Akademii nauk Ukrainskoy SSR) Card 2/3 On the Film Flow Rate in Solutions of Helium-Isotopes 56-1-38/56 *SUBMITTED: October 5, 1957 AVAILABLE: Library of Congress Ca-.1 3/03 8/056J~L2/043/004/060/061 B104/B186 AUTHCHS: Andronikashvili, E. L., Tsakadze, Dzh. Se, Bablidze, R. A._ TITLE: Study of rotated He Il near its A-point using the method of secondury sound PERICDICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki., v. 43, no, 400), 1962, 1562-1563 TEXT: H. ---. Hall ane:;%-;. P. Vinen (Proc. Roy. Soc., A 238, 204; 215, 1;956) showed that the&:establishment of a steady motion in He II on t'ransition from rotate:d He I into rotated He II -(i.e., slower formation L of Onsager-Feyninan vortices) can be studied by referdnce to the scatterine of secondary sound waves from the vortices. The following experiment was made on liquid He ,contained in the cavity between two' coaxial cylinders (ring-resonator). This resonator can be rotated about its axis of symmetry. The emitter and the detector for secondary sound were installed on the inner cylinder. A special device enabled the resonator to be rotated uniformly. The emitter was fed by a highly stabilized audio frequency generator. The signals received at the Card 1/3 S/056J62/043/004/o6o/o6i Study of rotated He II near B104/BI86 detector were amplifie,d and conducted into an 3TM -09 (EPP-09) recorder. A:t temperatures around the A-point (2.09 and 2-150K) the resonance . frequency was fixed in motionless He. The temperature of the He was then raised to 2.250K bY stopping evacuation. The resonator was set in motion (00 . 0.96 sec and after 3-4 minutes Ile was again pumped out at a rate of 2 mm Ug per minute. The amplitude of secondary sound war measured at the moment of passing the previously fixed temperature. The same measurements were also made with motionless He. The measurements at a fixed temperature of 2.150K showed that the maximum amplitude of secondary sound ddes not change, i.e., the formation of vortices slows down. The amplitude becomes lowe!r when the temperature is raised somewhat above the ;~-point and is then again reduced to 2.150Y. without the resonator being stopped. The measurements at fixed tempgrature of 2.090K give another picture: at the first reduction of temperature the amplitude of secondary sound becomeslower by 2V;'o. The same reduction is reached after 1-5 to 2 minutes rotation at the same angular velocity when the tie is kept at a temperature of approximately 2.090K. The time that elapsed before this slowed down the formation of Onsaller-Peynman vortices is estimated to have been 4 minutes(at 2-15010- Card 2/3 S/056/62/043/004/060/061 Study of rotated lie II near B104/B186 ASSOCIATIGN: lns~itut fiziki Akademii nauk Gruzinskoy, SSR (Institute of PlNysics of the Academy of Sciences Gruzinskaya SSR) S U B 141 T T'--'D Augu~t 31, 1962 'Card 3/3 .44229 W056/62/043/006/021/067 N Q.0 .1 B102/B104 AUTHORs Bablidze, R.-A.' TITLE: Transcritical oscillation conditions for He II PERIODICAM Zhurnal eksperimentallnoy i'teoreticheskoy fiziki, v. 43, no. 6(12),-19629 2066 - 2093 TEXT: .The transcritibal oscillation conditions~'Wiiere studied by the method-' of second-sound attenuation. Axial torsional oscillations were excited by,' &mechanism that allowed of varying the oscillation ri d d amplitude pe o an oi the resonator (Q - 1500 in He II at rest at 1.60K) between'2.8 and 12S see.and 0.06 and 2 radish*.,,, edspectively. Thus the maximum linear velool-, ties on the resonator periphery could be varied from 0-5 to 90 mm/sece Second-sound source and detector were applied at top and bottom of the resonatorg respectively. The measurements were made at 60 to 3000 cPs. The heat flux density dispersion did not exceed 5-10-4w/cM2 . The sound signals were amplified (amplification factor of,resonance amplifier -,407)' and then fed to an illn-09 (EPP-09) recorder, The appearance and stability of quantized Onsager-Feyrmn vortices was determined from the additional Card 1/3 S/056/62/043/006/021/067 TrAnscritical oscillation B162/B104 attenuation of second sound waves on them. The total dampinig coeff.i- cient is giveh by + where refers to the resonator at rest'and ('-J, lo-a"?,esonator oacillatingoat the frequencyti and the amplitude 1) where qiie the quality factor of 0 2qo the-oscillating resonator and 110 and u2 are the resonance 0frequency and the second-sound velocity. All measurements were made at 1.6 K+and-Ou I'Mio. 2 was measured between the first and the last pulse-height maximum of C econd-sound signal as (ti) with const and with t-J-const. The B results show that Wt f) - C(Vo A) where A 1.28~+0.29 mm/sect r 3/2.m _5~2 Verit - B 1.510-+0.011, C - (5-00+0.2l)-10-78ec m The time dependence of* was obtained as rI(t) -~7Mexp(-o.693t/t,) + Kexp(-0.693t/,t-2) with tj - 14.20~+0.86 see and T 2 - 2.10_+0.28 see; M + K - 4-1(0)1 Ml()A+K) - P, where P varies between 0.2 and 0.5. The t.imesl& 1,2 are the halfliyes of two different types of quantized vortices. P(t) describes the decay of Card 2/3 S/956/62/043/006/021/067 Transcritical oscillation ... B102/B104 quantum turbulence; the rate of this process is given by - 1/0 t, - - V. Z 621 t 0.693 K exp (_ t)] 4j M exp + The results agree qualitatively with the.Onsager-Foymm vortex concentration. There are 6 figures. ASSOCIATIONa Institut fiziki Akademii nauk Gruzinskoy SSR (Institute of Physics of the Academy of Sciences Gruzinskaya SSR) SUBMITTEDs July 20, 1962 Card 3/3 ANDRO,-IKASHVILI, E.L.; BOLI.D A.o; GUDZHABIDZE, G.V.; H -- _Z&,,,R TSAILkDZES D.S. (Tbilisi) "Experimental study of generation and disappearance of vortices at a phase transition from a quantum liquid into a classical one and vice versa". report presented at the 2nd All-Union Congress on Theoretical and Applied Mechanics., Moscow, 29 January - 5 February 196h Arm ACCESSION HR: AP4025917 S/OOS6/64/046/003/0843/0844 AUIHOR: BAb.l-idzev. Ro- A*; Teekadzet Dzho So; Chanishvili, Go Ve TMZ: Concerning the shift of the Lmrbda point in r-otatimig liquid heliun ,SOURCE: Zhurruil eksperimentallnoy i tecmticheskoy fiziki!p v. 46,, no. 3, 1964, 843-844 TOPIC TAGS - liquid heliun, Onsager repunan vortex, Lanbda point, - Lambda point shift, liquid heliun relaxation mechmism, helium I, heliun II ABSTRAM To ascertain whether the retention.of the onsager-FeyrimaIn vwtices in- liquid heliun whose temperature is raised above the X point is due to a shift of the A point or due to the relaxation mechanism pmdicted by E. L. Andricnikashvili et al (=F v. 46, 157j 1964), an experiment was set up to determine th#:~ .-k-a... shift by observing the discontinuity in the heating (or cooling) cm-ve of rotatuig and stationary helim on passing tbrvugh the A point. 7he experiments were made at rotaticn speeds (0.057 - 0.56 sec _') hi&ar th9n used by ArWrmikashvili %W to 5 X 10 4 K. It is =%cluded thet mitt this (0.055 see) and were WMW Card jACCESSICN NR: AP4025917 accuracy them is no shift of the A point towards either higber or lower tempera- tures over the entire range of employed angular velocitiei. "The authors take this opportunity to thank E. I" AndrmikAshvM for his sti=jlating interest in the present work."- - Ori . act. has: 1 fi .9 guze ASSOCIATICN: Institut fWJd M GnwSSR (PtWeics ITiedtutel, M Gv=SSR)q SURII=: 30ep63 WE ACQ: 16Apr64 ENCL: 01 SUB CODE: Ri NR W SOV: 001 OMER: 000 Card 2/3 ACCESSION NR 8 AA025917 Block diagram of set-up: I - resistance thermometerv 2 - organio-glass beaket -. 3 - =ercury contact slip rings 4 - Iron core 5 - rotating electromagnet 9=LOSM8: 01 1 Card 313 BABLIDZEY R. A.; TSAKADZE, Dzh. S.; CRANISHVILI, G. V. Shifting of the I -point in rotating liquid helium. Zhureksp, i teor. fiz. 46 no. 3:81+3-844 Mr 164. (MIRA -17:5) 1. Institut fiziki AN Gruzinskoy SSSR. BABLIDZE) R.A. 1. ~!-- ... .. Studying the supercriticO oscillatory mode in helium II by the method of second sound damping. Trudy Inst. fiz. AN Gruz. SSR 9: 171-183 163. (MIRA 17:7) 0 , L 1223-16-66 MIT(d)/EWT(l )19,4T(m) I EFF (n)-2/9-7r(t) IJP(a) JDA%VGG. ACC NR: AMW4916 SOURCE CODE: UR/0056/66/050/001/0046/0050 AUTHORS! Andronikasbvili, E. L.; ~blldze, R., Tsakadze, Dzb.S.' ORG: Institute of Physics, Academy of SciencesgGeorgian SSR ~5 3 (Ins ti t-'u`F'f I YfRY -Ak-a-d-em-Y1-ii-au-Tc--TiV~-ffi oy TITLE: Damping of second sound In rotating helium on going tbrough the phase transition tem2erature- SOURCE: Zhurnal eksperimentallnoy I teoreticbeskoy fiziki, v. 50, no. 1, 1966, 46-50 TOPIC TAGS: liquid helium, quantum liquid, vortex, rotation, resonator, sound propagation, relaxation process ABSTRACT: The purpose' of the study was to investigate the formationil guanti&i ices in rotating helium, which has of OnsaEer-FeZnman vort I no t 'bge-e Tsui 'iciently studied to date, particularly in those cases when the vortices are formed in rotating helium going through the pbase-transition temperature. For the purpose of investigating the kinetics of the vortex formation, the authors constructed a resonator Card 1/2 L 22n6-66 ACC NR: AP6004916 in which second sound could propagate in a radial direction. A second axial resonator was constructed, in which the second sound could propagate along the axis of rotation. The experiments have shown that in the immediate vicinity of the phase transition point the rotating helium II becomes foglike, as a result of uniform dis- i tribution of' vortex nuclei. It is deduced from the experiments that! initially there is formed an isotropic mass of vortex nuclei, which gradually be-come aligned into a system of vortices oriented along the axis of rotation. The relaxatlon times were measured for dif- ferent rotating speeds and for different degrees of supercooling, and it Is concluded that the relaxation time of the classical type of motion in a rapidly rotating quantum liquid is of the same order as the time of formation of the quantized Onsager-Feynman vortices at large angular velocities. The authors thank Yu. G. Mamaladze for a discussion of the results and N. S. Gavrilidi for help with the experiMEtnts. Orig. art. has: 4-figures aind I formula. SUB CODE: 20/ SUBM DATE: 06Aug65/ ORIG REF: 003/ OTH REF: 001 Card ACC NR, AP6o37o62 SOURCE CODE: ug/6656 clef;- 7 6676~llc AUTHOR: Bablidze) R. A.; Gavrilidi, N. S. ORG: Institute of Pbysicsp Academy of Sciences, Georgian SSR (Institut fiziki Aka- demii nauk Gruzinskoy SSR) I TITLE: Concerning thecondensation of rotating helium II SOURCE': Zhurnal eksperimentallnoy I teoreticheskoy fiziki) v. 51, no. 5, 1966, 1341- 1343 TOPIC TAGS: liquid helium, quantum liquid, low temperature research, acoustic speed ABSTRACT: To check on the cause of the increase in the density of helium II when 'the latter is rotated, first observed by E. L. Andronikashvili and G. S. Tsakadze (ZhETF Pis'ma v. 2, 278, 1965), the authors have measured the velocity of first sound in..rotating helium II at temperatures 1.40 - 2.10K and angular velocities 0 - 70 ..se.c71, Since the results of Andronikashvi3-i and Tsakadze disagreed with those ex- f:pec ed under the assumption that the condensation is due to centrifugal forces, the advanced the hypothesis.'that the condensation is due to the presence of .:,quantized vortices themselves. 'The measurements were made by a procedure whereby ~,.S~sbort sound pulses were transmitted to the investigated medium and the travel time ..,6f these pulses along.a certain segment of definite length was measured. The results show that within the range of angular velocities and temperatures measured, the speeds of sound remains constant (vithin 1%) at all speeds of rotation. This refutes the 1/2 ACC NR: AP6037062 assumption that rotatb* helium II has some *anomalous compressibility, and cu.-;queriv, 1y a different mechanism is necessary to explain the condensation effect. Orig. art.1 I has: 3 formulas. I SUB CODE: 2o/ sum DATz: iojun66/ ORIG REF: OOV OTH MF: 001 SbNA, thl SMIADO a rating, H. bid'Uh. 'o 0111VA all",- - -- - ,1 7 V., - UT "UTIAM o.jUt"A Io mfmmw to ft3wirimentA by tbo outl.* 00.'m Jr, iniptiruIny. It iv liolv) sbzl mm *mk,.w wts~slm kl~ urfim WWI himll" stuit-1; by -Iliv mitt iiimvitiwl of 40~' 147. i. U., -)ry' of] ilm Awl Zing ft), lvmliv~bjj jo blio ii U, lw &fit, tu kt.,prml- Sim o"M BABLIK, L. -L- Acuity of hearing following paracentesis. Mechr. Ohrenh 84 no.7-8-9:165-IM Jul-Sep 1950. (CIM1 20:1) 1, Of the Pirst Clinic for Bar-Nose-Throat Diseases of Vienna University (Head-Prof. Imil Schlander. N. D.). JANCMUSKI, Zygmunt; BABLOK, LesFek, CZ-APLICE!, Maciej Clinical and histopatboloEical evaluation of "filse" KlinefelLerls syndrome. Endokr. Pol. 15 no.2:253-263 I-Ir-Ap 164', 1. 1 Klinika Poloznictwa i Chorob Kohiecych w 'Varszawie (Kierownik: prof. dr. T. Bulski), Cddzial Indokr,,,ToJoj!iczny (Kierownik: doc. dr. J. Teter). 1 1.) MEYLAIMS, M., master, J ro'l-ovdsinc-n PC; -,. komandir samoleta, pilr,',; 2 k2assa, FABLINDJR~,, -;., ~.rm:.-ndjr is a second pJlot for an An-2 airplane needed? rrazhd. av. 21. no.lli25 N 164. (MIRA 1-8-3) BABWYAN, A.A. Torsion of prismatic rods of a box-type cross section with a alit. lav. AN Arm. SSR. fiz.-mat. nauk 11 no.2:89-97 158. OGRA 11:6) 1,Institut matematiki i mekhaniki AN ArmSSR. (Elastic rods and wires) AUTHORS.~ Abramyan, B.L. and Babloyan,A.A. SOV/22-11-4-9/11 TITLEg On the Bending of Thick Round Plates Under Axial Symmetric Load (K izgibu tolstykh kruglykh plit osesimmetrichnoy nagruzkoy) PERIODICAL? Izvestiya Akademii nauk Armyanskoy SSR, Seriya fiziko-mate- maticheskikh ns~k, 1,058., Vol '11, Nr 4, PP 95 - 1o6 (ussR) ABSTRAM. The authors consider a thick round plate which is fastened so that the whole lateral face is free of radial displace- ments and that a point of the plate axis does not suffer an axial displacement (see Lu'llye [Ref 1]), The authors in- vestigate the b6nding of the plate under arbitrary axial symmetria load acting on the base surfaces. The problem is solved by the solution of the tasie equations of elasticity theory with the aid of the Fourier method. The boundary conditions are assumed to.be-piecewise continuous and to be of bounded variation. 'Without giving the inter- mediate calculations whioh are probably very extensive, the authors present explicit final expressions for the in- Card 1/2 I On the Banding of Thick Round Plates Under Axia-IL SOV22-11-4-9/11 Symmetric Load tegration constants and the coefficients of the stress function. In two tables and in several diagrams numerical approximative values (probably very inexact) for an example are g1ven. There are 3 figare8v 2 tables, and 111 references, 7 of which are! Sovietv 3 English. and 1 German. ASSOCIATIOIT: Institut matematiki i mekhaniki AN Armyanskoy SSR (Institute for Mathemaii-.9 ana Mechani-Is)AS Armenian SSR) SUBMITTED: April -10p 1958 Card 2/2 ABRAMYAX, B.L.; UBLOTAN, A.A. ...... I- - --, Torsion in anisotropic cylinders. Dokl.AN Arn.SSR 27 no-5- 269-275 '58. (KIRA 12:5) 1. Institut matenattki I riekbaniki AN ArmSSR I Terevanakiy gosudarstvennyy univerRitet. Predstavleno akademikom N.Kh. Arutyunyanom. (Torsion) Ollastic plates and sballs) 16(l),24(6) AUTHOR: Babi SOV/22-12-3-8/9 TITLE: Torsion of a Shaft With a Thin Strengthening Layer by Single Moments PERIODICAL: Izvestiya Akademii nauk Armyanskoy SSR. Seriya fiziko - matematicheskikh nauk, 1959, Vol 12, Nr 3, PP 89-94 (USSR) ABSTRACT: The author considers a shaft of length 2 1 with a circular cross section strengthened by a thin additional outer layer of the thickness 6. At the ends of the shaft there act the same moments of torsion 11, in the middle of the shaft there acts the inversely directed moment 2 M. The roblem consists in the determination of the tension function ~(r,z) of the equation 2 2~- 0 M "br2 r eb r z2 and the boundary conditions (2) Glt + G '& r Sr2 (s)P(s)ds 26(2-1) 0 where r(s) is the radius at the considered place and Card 1/2 Torsion of a Shaft With a Thin Strengthening SOV/22-12-3-8/9 Layer by Single Moments ON dz r dr P(s) . r-r y -ds - z ? -a -. The solution is found as a series in terms of Bessel functions containing the well-known formula of A.Timpe f-Ref 2,7 as a special case (S-0). The author gives numerical values for the 2 . 10, S-0.1, R-1, 1-21L He mentions K.S.C case - hobanyan. G I There are 2 tables, 4 figures, and 3 references, I of which is Soviet, 1 German, and 1 English. ASSOCIATION:Institut matematiki i mekhaniki All Armyanskoy SSR (Institute of Mathematics and MechanicsAS Armenian SSR) SUBMITTED: April 16, 1959 Card 2/2 S/022/60/013/005/002/008 C111/C222 AUTHOR: Babloyan, A.A. TITM tending of Circular Bars Having Longitudinal Notches at the Side PERIODICALs Izvestiya Akademii nauk Armyanskoy SSR. Seriya fiziko- . matematicheakikh naukt 1960, Vol. 13P No- 5, PP- 17-25 TEXT: -The author considers the bending of a circular prismatic bar with a central-cavity and a lateral notch (fig. 1) (Fig. 1) Card 1/ 6 Bending of Circular Bars Having Longitudinal S/02 60/013/005/002/008 Notches at the Side C111YC222 The external force Q acts on the free end in the bending center and is parallel for the y-axis. In the cross section the tension function F(X,Y) satisfies the equation Q6-(x - MO) (1-1) 11 + (Y)i -2J f where x0 is the coordinate of the center of gravity of the cross section, J is the moment of inertia of the cross section with respect to the y-axis' f(x) is an arbitrary function, V is the Poisson's coefficient. On the boundary of the cross section, F(X,Y) satisfies the condition (1.2) a - ly 2 _f(x) dx S 2J I dS Because of the symmetry, the authors only consider the region ABCDEGF where the normal derivative of F(XPY) must vanish on AF and ED. Putting 2 2 (1-3) f (.0 and t t (1-4) x = be coo y - be sin Card 2/ 6 Bending of Circular Bare Having Longitudinal 9/022/60/013/005/002/008 Notches at the Side C11I/C222 then one obtains from (1.1) and(1.2) v 2 2 (1 + 22)Qb3 3t (rx 0Qb 2t (1 -5) V F(t, tp) M (I + IY)J e coo y - T-1 -+-,-,Tj e and ~F _413 .2t) d(e t coo T (1.6) 7-S 2J dS The tensions IC and Z rj are expressed by F(t,y) t ~jy 2 r (t, LF )- - --L t + _qh: (62t Coo Lf Z if be t 2J (1-7) c (t, 2F + Qb2 (e 2t _ 1) sin ry be t 9;p 2J From (1.6) there follow the boundary condition ir(06%f), F(t,Lfl), F( , where t, Tn(falues of ln-~ t2' F(-tl' Y) T ' t2 Corresponding to (Ref- 3) the function F(t,tf) is sought with the arrangement Card 3/6 Bending of Circular Bars Having Longitudinal S/02 60/013/005/002/008 Notches at the Side C1,11YC222 Fl(t,y ) in the region I (1.10) F(t,kf) F2(t' q) in the region II 73(t,Y) in the region III and corresponding boundary conditions. For the determination of the Fi(t0f) , (1-5) is solved by a separation of variables under consider- ation of these boundary conditions. For the integration constants one ob- tains two infinite systems of equations being completely regular and having free termis bounded from above and tending tQ zer6. An explicit expression for the coordinate of the bending center is given. In the numerical example s 2.9359, 2%pl - 'K , three cases are 5 distinguished I. t, 89 0-3947 t2- 0.6823 II. t, . 0.677 t; 2 - 0-400 III.t 1 - 0.8968 t2= 0.1801 Card 4/6 Bending of Circular Bars Having Longitudinal S/022J60/013/005/002/008 Notches at the Side CIII.IC222 The table 1 gives the estimations of the coordinate of the bending center from above +) and from below (Y and its mean value -x. + table I t A - 2s, a a a ring sector - - 3-3102 case I - 1.5153 1.4820 - 1-4987 case II - 0.5080 0-4837 - 0-4959 case III - 0.2058 0.1911 - 0-1965 02 z (t,y) Table 2 contains value of - some points on y 0 table 2 t points (010) (-t,,O) (-tj "W) (0, 7,~) t 2 ringsector -- -- 2.0202 -- M592 case I - 1.5276 -2-1324 1.2283 0.8334 0-5846 case II - 1-0038 -1.2889 1-0537 0.6413 0-5239 case III - 0.6592 -1-0783 0.9697 0-5459 0-5008 F.in - 0-5007 -0-9395 0-9395 -- 0-5007 rf 5/6 Bending of Circular Bare Having Longitudinal S/022/60/013/005/002/008 Notches at the Side C111/C222 There are 2 tables, I figure and 6 Soviet references. libstracter's note i The regions IJIJII are not defined. (Ref. 3) is a paper of B.L. lbramyan and A.A. Babloyan in Prikl&dnaya matem&tika i mekhanika, 1960, Vol. 24, No. 2, PP- 341 - 3491 ASSOCIATIONs Institut matematiki i mekhaniki AN Armyanskaya SSR (Institute of Mathematics and Mechanics of the Academy of Sciences Armyanskaya SSR) SUBMITTEDs May 25, 1960 Card 6/6 ABRAMYAN, B.L. (Yerevan); BABLOYAN, A.A. (Yerevan) Torsion of circular bars having longitudinal grooves or teeth and a central cavity. Prikl. mat. i mekh. 24 no. 2:341-349 Mr-A~ 160. - (MIRA 14:5) 1. Institut, matematUd i mekhaniki AN Armyansko,.r SSR. (Torsion) AHRAMN. B.L., RLBLOYAN, A.A. Torsion of round rods with longitudinal grooves or teeth and a cavity through the center. Dokl.AN kru.SSR 29 no.5: 293-209 '59. (MIRL 13:6) 1. Institut mateuatlki i mekbaniki Almdemii muk Armygmakoy SSR. Prodstayleno akad' AN krmyansk~y SSR W.Kh. Aratyanyamm. (Blastic rods and wires) (Torsion) RABIDYAN, A.A. (Yerevan) Bending of circular rods having longitudinal side grooves. Izv.AN SSSR. Otd.tekh.nauk.M9khA mashinostr. no-5.-66-73 160. (MIRA 13-9) 1. Institut matematiki i mekhaniki AN ArmSSR. (31astic rods and wires) 80253 S/040/60/024/02/19/032 AUTHORS: Abramyan, B. L., Babloyan, A. A. (Yerevan) TITEL: The Torsion-0of Rou~nd" and Teeth in Longitudinal Direction a7d With a Centrally Situated Hallow Space PERIODICAL: Prikladnaya matematika i mekhanika, 1960, Vol, 24, No. pp. 341-349 ' TEXT: The authors consider the torsion of a round prismatic bar which possesses a centrally situated hollow space and on the outside or in- side wall of which there occur symmetrically distributed longitudinal grooves..The side walls of the notchings are planes going through the axis of thebar. With the aid of the method of (Ref.1,2) the authors obta'LL a rigorous solution. The integration constants must; be deter- mined from linear infinite systems of equations which are perfectly regular In the sense of Kantorovich and which possess free terms bounded from above and tending to zero. In two special cases (a.) six notches b.) one notch) a numerical calculation is carried out. The same torsional probelm for notched bars, however without hollow space, Card 1/2 80 S/040/60 024/02/19/032 The Torsion of Round Bars With Grooves and Teeth in Longitudinal Direction and With a Centrally Situated Hollow Space was investigated in (Ref.3,4). There are 7 figures, 4 tables, and 5 references: 3 Soviet and 2 Roumanian. ASSOCIATION: Institut matematiki i mekhaniki AN Armyanskoy SSR ics and Mechanics AS of the Armonian SSR SUBMITTED: April 19, 1959 Card 21/2 BABLOYAN, M-.A. Flexure of prismatic rods with cross sections in the form of a ring sector with a: groove along the curvilinear portion. Dokl. AN Arm. SSR 31 no. 4:193-200 160. (MIRA 13:12) 1. Institut matematiki i makhaniki Adademii nauk Armyanskoy SSR. Predstavleao akadem-ikom AN Armyanakoy SSR N.Xh. Arutyunyanom. (Flexure) (:~Iaatic rods and wires) BABIDYAN, A.A. Flexure of round rods with longitudinal lateral grooves. Izv. AN Arm. SSR. Ser. fiz.-mat. nauk 13 no-5:17-25 160. (MIRA 14:1) 1. Inatitut matematiki i mekhaniki AN Armyanskoy SSR. (Flexure) (Elastic rods and wires) S/022/61/014/002/002/006 B112/B203 AUTHOR: TITLE; PERIODICAL: ~abko An_ ~A- A~- y Bending of a round cylinder with longitudinal teeth or a notch Izvestiya Akademii nauk Armyanskoy SSR. Seriya fiziko- matematicheskikh nauk, v. 14, no. 2, 1961, 31-44 TEXT: The author studies the bending of prismatip rods, the cross sections of which have the shape of a ring sector with sy'mmetrically arranged teeth and of a ring with a sectorial notch. L. S.-Meybenzon,. A. C. Stevenson, M. Seegar, Ya. Y. Burak,and others were concerned with similar problems. The author applies the external bending force P to the free end of the rod along the symmetry axis of the cross section, i.e. , he presupposes free from torsion bending. The stress function F(x) Y) satisfies a differential equation: V'F(x, y) y ff(y)i with the boundary condition: Card 1/3 S/02 61/014/002/002/006 Bending of ... B112YB203 .aFaP 2_ x x - 1 f(~' where x is the center-of-mass as 1 [21 0 2 ds 0 coordinate of the cross section, J the axial moment of inertia of the cross section with respect to the axis.1tf'(f(y) an arbitrary function, and a is Poisson's ratio. The author set Y) - b2 - Y2, and introduces new coordinates t,T : x - betcos y, y - betsin Y j thus, the equation for the stress function takes the form: V2p(t, T) = jb3 1 + 2a e3t sin with the boundary condition: j 1 + 6 T aF Pb3 [2t d(et sinTI e - 1 - 2 t These equations are E -2 e cos.] b d9 solved separately for each part of the properly subdivided cross section, essentially by the method of separation of variables. The solutions contain coefficients Xk and Yk which satisfy two infinite linear systems of equations: Card 2/ 3 Bending of ... S/022/61 /014/002/002/008 B112/B203 CO.'. 00 Xp . :~7 akpYk + P p, Yp :~: bkpXk + Qp. The author shows that these kal k-1 systems are completely regular. Then, he considerB a number Of special cases illustrating them by numerical examples. For the simplest case(solid cylinder without a notch), the stress function has the form: C sin y [.3t -3tj sht - sh(ti + t) Pb3e-2ti F(t, T ) . e shtl Bht'i + _j sht-sin There are 9 figures, 2 tables, and 10 references: 6 Soviet-bloc and 4 non- Soviet-bloc. ASSOCIATION: Institut matematiki i mekhaniki AN Armyanskoy SSR (Institute of Mathematics and Mechanics of the AS Armyanskaya SSR) SUBMITTED: November 24, 1960 Card 3/3 30388 ILI 1%2,7 hil 1193 S/022/61/014/004/002/010 D299/D302 AUTHOR: Babloyan, A.A. TITLE: On axisymmetrio deformation of a finite circular cy- linder of transversely isotropic material PERIODICAL: Akademiya nauk Armyanskoy SSR, Izvestiya. Seriya fi- ziko-matematicheskikh nauk, v.14, no.4, 1961, 61-70 TEXT: An exact s6lution is obtained for the problem of axisymme- trio deformation of a circular cylinder of radius R and height 2h, the external load being symmetrically distributed with respect to the middle plane z=0. The Elliott-Chakravorty formulas are used. It is noted that Elliott's formulas can be derived from S. G. Lekh- nitskiy's formulas. In the case of axisymmetric deformation, the stresses and di lacements, expressed in terms of 2 "harmonic" functions ?l and ?2 (r,z (r,z) are given by formulas which involve the coefficients k, c and-J, where V1 and-j2 are the roots of the equation Card 1/9 30388 S/022/61/014/004/002/010 On axisymmetric deformation D299/D302 4 2 clic 44~ + ~13(C13+ 2c 44 C11C3311) + '33c44 (3) k1 and k 2are found from c44 + k (c13 + c4.4)= k1 03~ - = 2 c11 (c 13 ' '44 ) + kic44 0i (4) the functions f, and f2 satisfy the equations 17 2f1 +,1)2 ~2 fl =0, 1 1 -;Z-r 1~72 2 ~2 f2 = 1?2 +'02 - 00 ~Z2 Card 2/ 9 On axisymmetric deformation ... 2 ~2 i + =~r -i Tr- (5) The roots of Eq. (3) are either real numbers or conjugated complex numbers. Both cases are met in practice, For an isotropic body, when cil = C33 2P, one obtains c12 '13 044 30388 S/02 61/014/004/002/010 D299YD302 In general, these roots are not equal, Solving Eq. (5) by the me- 0 thod of separation of variables, one obtains the following funda- Card 3/ 9 30388 S/02 61/014/004/002/010 On axisymmetric deformation,.... D299YI)302 mental system AIO(-OiAr) + BKO(ViAr 9 EC sinAz + Dcos/jz [A sh &-z- + B ch -"' Lcjjo~ur)+ Djo~ur) 1 r0i 1 AT, (7) where A and are arbitrary positive parameters, I,K, J and Y are Bessel functions. The function T, is sought in the form i(L2 _ ~2 00 Ti(r,z) = a z + b - _+ A(')I r)cosikz + i 2 2 Z k 0 ('Oik i k=1 Card 4/ 9 30388 S/022/61/014/004/002/010 On axisymmetric deformat.ion D299/D302 + 0(')chd!kz- j .~Axk r)6 (1-1.2) (8) k,m I k k IV i Wwro ic Whp andpk are the roots of the equation J , (.,UkR) = 0 Thepe valuou, of q9i are substituted in the formulas for the streBees and dinplaoements. Furtherg tbe stressed state of a circular cylin- der io conoidered, described by OD z) A (z) = 1. y, k .1 Cr (R, z.) ==f2 p', = yovcoq ).kz. 4~ k-1 (0 Card 5/9 3 3/02Y6VO'l 4/00'4/002/0 10 On axisymmetric deformation ... D299 ,02 h) f3 (r) to,< r R) ,X v: (r, h) ~ f4 (r) k-1 (14) By virtue of the symmetrical load-distribution, Icrz (0,z) = u(0,z) = 0 (15) Trz (r-,O) = w(r,o) = 0 (16) Expressions are obtained for the unknown coefficients Aq b and 01 these expressions yield an infinite system of linear equatbns Card 6/9 30388 S-022/61/014/004/002/010 On axisymmetric deformation ... 99/D302 00 Xp a kp Yk k=1 -19 21-0 00 Yp 2 bkpXh Bp (21) k=1 (a,b,4o(o, B, are given by formulas). It it- ~ihown that system (21) is regular and that the coefficients X and i --an be calculated by ap- proximate methods. Substituting the obtu values of the coeffi- cients in Eq. (7). one obtains expressioi~,-. for 71 and T2, whence the formulas for the stresses and displo--~..:.ients can be readily de- rived. The same method can be used for .!;Iving the problem with Card 7/ 9 30388 ~j/022/61/014/004/002/010 On axisymmetric deformation ... D299/D302 non-symmetrical load-distribution, and *,~~,- problem of a sloping cy- linder. These problems reduce to solviii~- a regular infinite system ~7 ,' of linear equations, whose free terms ii, an upper bound. By alter- ing the boundary conditions, it is pos.,-10ie to solve problems, whose exact solution is obtained without. having recourse to infi- nite systems. There are 1 figure and 15 i~,~i'erences: 10 Soviet-bloc and 5 non-Soviet-bloc (including 2 trar~~J:itlions). The references to the English-language publications read !'ollows: H. A. Elliott, Three-dimensional stress distributions in iiexagonal Aelotropic crystals. "Proc. Camb. Phil. Soc.'' 44, 522-533; J. G. Chak- ravorty, On the distribution of stress in !-in infinite circular cy- linder of transversely isotropic materit:, caused by a band of uni- form pressure on the boundary. "Bull. C.,)-I. Math. Soc.", V. 48, no. 41 1956; Love, A Treatise on the Mathelfl.~L'~!,--al Theory of Elasticity. 4th ed., New York, 1944. ASSOCIATION: Institut matematiki i mek.,;:oAki AN Armyanskoy SSR (Institute of Mathematics :11.d Mechanics AS Armenian SSR) Card B/ 9 On axisymmetric deformation ii.i SUBMITTED: February llt 1961 30388 8/022/61/014/004/002/010 D299/D302 y Oard 9/9 BABLOXAN,.A.A.; TONOYAN, V.S. Some problems of the torsion of shafts of varying cross section with mLxed boundary conditions. Izv. AN Arm. SSR. Ser.fiz.-mat. nauk 1,1+ no.6:49-63 161. (NIRA 15:1) 1. Institut matematild i mekhanild AN Aruyanskoy SSR. - (Boundary value problems) (Elastic rods and wires) BABUMAN, A. A. Cowiento on one problem of the axisymmetric deformation of an infinite circular cylinder made from transversely-isotropic material. Dokl. AN Am. SSR 32 no.4:189-195 1.61. (MIRA 14:8) 1. Institut Matematiki i mekhaniki AV Armyanskoy SSR. Pred- stavleno eblenom-korrespondentom 1,14 Armyanskoy SSR S.A. Ambart- sumyanom. (Boundary value problem) (Deformations (Mechanics)) BABLOYAN, A.A. Solution of the plane problem of the theory of elasticity for an angular sector in an area of stress. Izv.AN Arm.SSR.Ser. fiz.-mat.nauk 15 no.1:87-101 162. (MIRA 15:2) 1, Institut matematiki i mekhaniki AN Armyanskoy S* 11 (Elasticity) 36022 S/022/b2/015/002/003/009 D218/D302 AUTHORS: Abramyan, B.1.p and Babloyan, A.A. TIM,': On one case of axially symmetric deformation of a hollow cylinder of finite length PE'HIODICAL; Akademiya nauk Armyanskoy SSRf Izvestiya. Seriya fizi- Ko-inatematicheskikh nauk, v. 15, no. 2, 19b2t 87 - 99 TEXT: The -authors report an exact solution of the axially symmet- ric Droblem of-the theory of elasticity for a hollow cylinder of fi- nite length. An arbitrary load is assumed to be applied to the side surface of the cylinder, while normal displacements and tangential stresses are given at the ends. The solution is given in the form of Pourier and Fourier-Dini series. A numerical example of the so- lution is given. It is pointed out that the previously published so- lutions ivere approximate. There are 4 figures, 1 table and 12 refe- rences: 10 Soviet-bloc and 2 non-Soviet-bloc. The references to the Miglish-language publications read as follows: MI.A. Binnie, Philoso- phical Magazine, London 212, 1941, 336-347; D. 'De Allen, L. Fox and Card 1/2 S/022/62/015/002/003/009 On one case- of axially syrL-retric D218/D)-02 - R.V. Southwell, Phil. Trans. Roy. Soc. London, Ser. A., v. 239, 1946P 501-537. ASSOCIATION: Institut matematiki i mekhaniki AN Armyanskoy SSR (Institute of Mathematics and Mechanics, AS Armenian SUMITTED: October 7, 1961 Card 2/2 38086 S/040/62/026/003/009/020 D407/D301 AUTHORS: Abramyan, B.L., and Babloyan, A.A. (Yerev~n) TITLE,: On a contact problera involving the twisting of a hollow half-s,oherd PERLIODICAL: Prikladnaya matematika i mekhanika, v. 26, no. 3, 1962, 471 - 480- T3.XT: The twisting of a hollow half-sphere by an arbitrary axisym- metric load is considered. The solution of the problem is obtained by means of conic functions. The equation for the displacement func- tion 'Tr(r, z) is 2~1 + a2y 0. + 2 r Or 2 5r Passing to a new coordinate-system, Eq. (1.1) is written: + 2 -'~ + 3 L" - 4 j0 (1-4) Card 1/3 S/040/62/026/003/009/020 On a contact problem involving D407/D301 Solving Eq. (1--4) by the method of separation of variables, one ob- Uains the following particular solutions d 2 2 W71 IAP-%+iLki (t) + BQ-'I-+Ikt RVI Tk(t) where d ( CP. (E) + DQ. (1 -7)' T; Th (t) L-31121C Sin Pki + Doospki Pn and Qn are Legendre functions, P_ 1/2 and Q_ 1/2 are conic func- tions, A, B, 0 and D are arbitrary constants, n is a positive nat.u7 ~-al--number. Torsion of a hollow heLf-sn-here with radii b and c (b