SCIENTIFIC ABSTRACT MOSKALEV, V. A. - MOSKAALEV, V. V.

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CIA-RDP86-00513R001135330002-3
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November 2, 2016
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December 31, 1967
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SCIENTIFIC ABSTRACT
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VOROBIYEV. A.A.; KOSUMV. V.A. Investigation and development of cyclic electron accelerators at the Tomsk Pelytechnical Institute. Atom. energ. 4 no.3:229-237 Kr '58. (KIRA 12:3) (Tomsk--Particle accelerators) AUTHORS: Vorob'yev, A, Professor ' Directcr, and Moszalev, V, A. C:@: f Tech.nical Sciences Docent, IITI.a,,-. Formation of a Beam of Rays from a betatron (Formirovaniye puchka luchey betatrona) PERIODICAL: Izvestiya Vysshikh Uchebn7kh Zavedeniy @.'le K t i ome ?@I a nik, a, 1958, kir 9, PP 5-5 (USSR) ABSTRACT: Usin6 the available daLa on the distribution of y-radiatioD from a 10 MeV betatron the authers constructed a collimator which had to satisfy certain requirements. Distribution of radiation in the y-ray beam from the 10 MeV betatron is shown in Fig 1, v;@,ere 1 is the theoreticb1 curve and 2 is the curve obtained experimentally, The authors calculated the thicknesr: of a lead collimator wha(@h was nec.essary to limit ii, radiation intenE.Jt,@ outside the beam to 0.0@% uf the intensity on the beam ax.-s, This calculated thicI4@ness was found to be 15,5 cm and the actual collima,,or made by the authors i,.ad a thickness of 1? cm. fhe construction of the collLuatur- is sho@-rc in Fi@, 2. The collima@,or Cnrd 1/3 was placed between the roils, of the accelerator electro- Formation of a beam of Ra-@s froL, a Beta@rcr_ ma@net. The collimator could be adjustea to mE,_ @h@, beajn and the collimauoi axes coincide, The of the collimate(i beam coula be altered by usii-r- i. chELngeable colllar.,3 show-n i-n Ri filter of coni,:all fori;i aus used tu ;iuike the Int-,n. -7 3 f y - j, ad i a t ij n ; i, i f () v:i- a c r @) j,-: % ra! : o 11 i,@vi t (,, dF I shows the ca@cuiated (curve 1) az-vi adjusted (c,_@rves _', @) prot'_,Ies of th.@ _op@_,er@ used, Fi@, 4 sll@)vjz_-, t-he .f thf.@ colli:aated :,dtiiout wi@h the copper filter (curve @Z). A saall di@j) la (5-4 mm) of the -ollimal.GT@ a_XiS Witt! respect tu tLe L"-"r- a-xis causes a consideranle chin@-e in tht tistritut,;or- (-f raiiation acrcss the beam curv@ 3, Fib 4), The used the collimated team to measure the isodoses in water. They u5e@j a special dosi,:,eter @.ith a thimble-type ionisaliori chamber Whose -.-vork.in, voli-En- was 1 cm3 and which had a thin @,,raphite viall, Tne r(@sults of the dosimeter mea-nurements are @@towri in Fit, Card 2/3 TI.e maximwa dose was obtained at 21U ram belovi @@;, 141.1 - Formation of a Be-nL, of, @ja@'ys fl-or :@,.,@-t-ror Surface. Fig 6 ejves a SCtle:Latlc OL -,rje betatron and tne collimator assemblies. The -e are 6 fiE-,ures t;rui ? ref,,-r---n( es , one of .-.n-icr-. i jov@Let, one EnGlisti. j,66uCiATIuN: Tomskiy politeshni,nesKiy 1r1jr-4tut (Toinsk Polytechnic@@L lnstituL,@) 6U3IiiITTED- SeDtember 25- 1958 Card 3/3 SOV/1L,4- Moskalev, V.A.t Cand.Tech.ScL, Docent The Second Inter -vuz ',onforenre -,n Electron Accelerators FER:_,'1--'AL; Izvestiya vysshikh uchebnykh zavedeniy@ Elektromekhanika, 1958, Nr 12, pp 142-143 (USSR) A@3,-RA'T: The second inter- vuz --onferen(-e @-n electron accelerators was helddt 'U-he Tomsk Pulytechnical In,'-'_ In the early part of 1958. There were 146 reports, presented to four sections. The -onfurence was atteri;-: by more than 700 representatives of @i organisatirns including scientific organisation--, vuzes, and industrial undertakings from various parts of the Srv,.,@! Union. Fifty-six reports were presented to the IL,--.w- energy electron accelerator' section, 1f1c,3t of theM bt7 rIE! devoted to the development of Indust T' I tyl)O.; (,) f L)O!,.:k * fhe reports of sevoral in3t1tutes Lha*, have severa. -/",I: experience of the use of betatron-; w@-_-re of particu.'a., Interest. A number of reports were I-_,ncerned with improving the electronic circuits and stabilising t,,e power and intensity of radiation of betatrons. Other dev,@!- pm@_-nl reports dealt with linear accelerat,@,r,_- and the V-11, SOV/144_58-i2-17/19 5@: (@rirl Inter- vuz Conference on Electron Accelerators of new types of betatrons for use in industry. The se-@:_n on 'the application of electronic accelerators in tne national economy' heard with great interest reports ci' Tomsk Medical Institute on the treatment of cancer anA radiation diseases. A number of reports were pre_ientei the procedufe for locating defects in steel products. Reports were read on the use of accelerators to solve problems of geophysics. A new metftod of accelerating electrons to very high energies is based on the use (:* travelling waves in a closed wave-guide. Staff of tne Moscow State University and of the Physical Institute th.e Ac.Sc. USSR read a number of reports about the influence of quantum fluctuations of radiation on the motion of electrons In very high energy accelerators. T,,.e fourth section considered the development of electr,@,-, accelerators of very high energy. The reports were (r.- c-orned with the theory and practical design of several types of accelerator. The closin@- session indicated t`i- development programme for new ty-pes of electron accelerator and their practical application in the national economy. 1 SO V/144- 5c,-1 @-17/1@) 1 .- S.- Inter -I vuz 4onference on Electron Accelerators AS30 Tomskiy politekhnicheskiy institut (Tomsk Polytechnical Institute) Ll/ MOSKALEV, V.A. Detector of betatron Irradiations. 'Ie9t. rent. i rad. 33 no.6:63- 64 11-0 '58. O(W 12: 1 ) (IMMOTHIRAPY, apTmr. e. inatruments betatron detector Ohio)) (NUUMAR PHMIGG, Gnme) 21M S0V/lD-5q-1-17/-,- AUTHORS: Vorob7yev A.A., Moskalev V.A. TITLE: Some Characteristics of Betatron Target Radia-,,,.n at 10-25 MeV (Nekotoryye kharakteristiki luchey betatronov na 10-25 Mev) PERIIDICAL: Izvestiya Vysshikh Uchernykh Zavedeniy, Fizika, 1959, NY 1, pp 102-106 (USSR) ABSTRACT: Results of experiments on the spatial distribution rf betatron target radiation are reported. It is shown t,-@at the experimenkal data are in pod agreement with the theory given by Lowson (Ref 2). The measurements were carried out u3in@.- a special detector (Ref 3). The detector includes a thimble ionisation chamber with j working of I @.m and a graphite wall whose th@-z- ness may be varied from 3 mm to the equilibTiLLn @al,-)@@ The detector could be continuously moved over a 1 m radius (.ircle, the rotation axis of the dete@t,):- pas5lrig through the tarrer- Fig I shows the spatial distributLon in the plane of the orbit of the radiation in the main beam at 10 MeV. Curve 2 is theoretical (Lowson) and Curve 1 was obtained from experiments. The discrepancy Card 112 between the theoretical graph and the experimental one (on the right hand side) is due to target ed@e effects SOV/1 1711)- 10 - -- Some Characterist'-s -if Radia'-,-F- -at desc.ribed -,r) Ref TY,e fjl-@ width at 'Ial @!L- intens i ty (-.u -ip h(- d i s t r i b-,1 t i cjrl 11, rnp dirertion (Fl@, F e To r p ,- Imme t. r i c a i a n6 wj-dth at half ht-!g1-,t 170@ Fig @ gives t@',e FP-I*, L a distributl(@,r. -,f bo-,-al -,-)ri at 10 of the r. , Thr- jrve r.a a max imum, Tr) P i a I I i -,; t 7 1 b,i t n a E-V z i. good agr ee,-rie rit w * t I, the rneory, ri-I e 'I-?, Wa S t @:- Y n', p t- I- -Y by , *P"- - L '@ it j " rl in (@cpper an.-j !,?Li 1, 4 Mev r, @,a3p of iO Fle'l beptatrc)r- .,ard 2/@@ The-,e ar,- and LO referenr,@-s, , I Englisi. aiv-i @-, S,@,ri,-- .7 ins t '@ t A I ASSOCIArION: Tomski- Pr,-, fezrrli, @iesz .Ly (Tomsk Instit.l.ite- imeni S.1-:- Ki-,,,) SUBMITTED: July 14- 3/13 9/59/000/0 5/00 5/026 9032/9111+ AUTHORS: Moskalev, V.A., and Akimov, YU.M. TITLE: A bo-uke Chamber 10 MeV Stereobetatron PERIODICALs Izvestiya vysshikh uchebnykh zavedeniv, Fizika, 1959, Nr 5, pp 26-30 (USSR) ABSTRACT: A brief description is given of a betatron which Was brought into operation towards the end of 1957. Details are given of the electromagnet, the electromagnet supplies, the control circuitry, the vacuum system and some preliminary results obtained with the machine. & photograph of the stereobetatron is shown in Fig 1. The magnetic characteristics have been described in an earlier paper (Ref 2). The radius of the Gquilibrium, orbit in both of the accelerating systems is 13 cm and the maximum induction on the orbit Is 2700 gauss. The accelerator control circuitry is shown in Fig 3. The vacuum system consists of two independent chambers made of molybdenum glass. The pressure is (2 to 5) x 10-6 mm Hg. The Gard angular distribution of the intensity in the horizontal 1/2 plane is shown in Fig 4. The dose rate at the distanr/:@ of 1 m is 3-3.5 r/mIn for each of the accelerating 8/139/59/000/05/005/026 E03 2/&114 A Doublo Chamber 10 MeV Steroobetatron systems. At the point of intersection of the two y ray beams the dose rate can be up to 7 r/min. The angular half width of each beam is 250 which is in good agreement with the theory. The stereobetatron is Card designed mainly for use in medicine and metallurgy. 2/2 It Is also intended to extract the electrons and to obtain crossed electron beams. There are 4 figures and 2 Soviet'. references. ASSOCIATION: NII Tomsko ,go politekhnicheskogo instituta imeni S.M. Kirova (Scientific Research Institute of the Tomsk Polytechnical Institute im eni S.M. Kirov) 'T1-J): December 27, 1958 S/1 39/ 59/000/05/007/026 F-u32/&114 AUTHORS: Moskalev, A. @F-Uippov, M.P., Skorikov, A.G.$ and Skyortsov, Yu-,?f,_ TITh;",. A High Pulsed Current Stereobetatron PERIODICAI: Izvestlya vysshikh uchebnykh zavedeniy, Fizika, 1959, Nr 5, PP 35-44 (USSR) ABSTRACT: The Tomsk Polytechnical Institute has designed a 25 MeV stereooetaLron sucn tnat the beam current at the target is of the order of a few amps during a fraction of a microsecond. The shape of the magnetic field was based on the theoretical studies reported in Refs 3-7. The present paper gives a general description of the various features of the betatron including the construction of the electromagnet, the supplies, the injection scheme, the extraction scheme, and the design of the two independent vacuum systems. The machine Is now being built. It will be used to study electron interactions in the two crossed beam3. There are 10 figures and 14 references, of which 12 are -/j Soviet and 2 English. ASSOCIATION: Tomskiy politekhnicheskiy institut im. S.M. Kirova SUBMITTED: December 27, 195@3" __,,,,/59/ooo/o6/oo2/034 9032/3114 AUTHORs Moskalev, V,A. TITLE: C@@s, t.ru.c.ti-on' and'flagnetic Characteristics of a 10 MeV Double Chamber Stereobetatron PERIODICAL: Izvestiya, vysshikh uchebnykh zavedeniy, Fizika, 1959, Nr 6, pp 5-9 (ussH) ABSTRACT: Fig 1 shows a drawing of the electromagnet of the st,ereobetatron but no description of this magnet is given. It is stated that the distances between the sources ol radiation is considerably greater than in an flordinary" two beam betatron but the cost of the machine Is only 15-20% higher than the cost of an ordinary betatron. The steroobetatron was brought into operation in December 1957 and can be used for both medical and industrial purposes. It can also be used to study electron-electron Interactions. The static magnetic field of the betatron is Illustrated in Fig 2, In which a refers to the left pair of poles and b to the right pair. The field is set up by a special magnet Card construction which was described by Rodimov in Ref 5. 112 Fig 3 shows the azimuthal phase rionuniformity of the 69146 S/139/59/000/06/002/034 9032/F.111+ Construction and Magnetic Characteristics of a 10 MeV Double Chamber 3tereobetatron magnetic field. Curves 1 represent the "natural" phase nonuniformity for the two pairs of poles, and.curves 2 show the "natural" phase nonuniformity in the case of poles of the special design described in Ref 5. Fig 4 shows the position of correcting coils for the two pairs of poles and the resulting corrected azimuthal nonun1formity of the field. This nonuniformity does not change by more than 0.7 oersted. It is suggested that by placing two targets in each of the chambers and using the two half periods of the magnetic flux it is possible to obtain four beams so that it may be possible Card to irradiate two objects simultaneously by the stereo 2/2 beam. This paper was presented at the Inter-Collegiate Conferenep on Aeselerators (Tomsk, February 1958). There are 4 figures and 10 references, of which a are Rnglish and 7 are Soviet. ASSOCIATION- Tomskiy politakhnicheskly institut Imeni S.M. Kirova (Tomsk Polytechnical Institute imeni S,M. Kirov) SUBMITTED: December 27, 1958 S/139/6o/ooo/006/026/032 E032/E414 AUTHORS Sokolov A A Professor of Moscow State University Stalin Prizewinner Doctor of Physico-Mathematical Sciences, Vorob'Vev, G A.. Docent and V A , Docent TTTLF On the 50th Anniversary of the Birthday Of Aleksandr Akimovich Vorob ve-, PFRroDrrAi. Irvestlya vysahtkh uchebnykh zavedenLy, Flzika, t96o, No 6, pp 161--164 TEV7 A A Vorob'yev was born in 1909 He attended the Tomsk State University between 1927 and 1931 In 1931, he graduated from the Division of Physics and Mechanics In 1935 he produced a "brilliant dissertation" and became a senior scientific worker and Docent of the Tomsk State University in the Department of Experimental Physics In 1936, A A.Vorob yev organized the High-Voltage Laboratory at the 61.berian Phy-4).totechnacal Institute and becarde its head In 1939 he --Uccessfully completed a dissertation submitted for the degree Card 1/ 5 S/13q/6o/ooo/oo6/O26/o32 9032/9414 On the 50th Anniversary of the Birthday of Alek.,%andr Akimovich Vorob yev of Doctor of Physico Mathematical Sciences This di.4aertation waN based on experiments carried out at the High-Voltage Laboratory and was concerned with the electron theory of the breakdown of dielectrics On completing his doctoral di"s-ertation. A A Vorob yev began work at the Tomsk Polytpchni,@al Institute as the Head of the Deparzment of High Voltage Technology In that post he showed great scientific and admiriLstrative ability and soon after was mppointed the Dean of the Power Engineering Division and later Deputy bcieniifi@ Director since !944, A A Vorob'yev has been Dare:,.or of the Tom%k Polvtechnical Institute In the forties 3 A Vorub'vtv devoted his attention to the development of part.-cle accelerators and the phyatics of dielectri@i In 1947, a small group of sci#ntists working at the Tomsk llolyt@,chntc&l Institute, and headed by Professor Voreb yev began wGrk on the design and manufacture of betatrons The first betatron p-oduted in the Soviet Union wa5 designed and Card 2/5 t@/11'1/60/000/006/026/0@' E0@2/E@ 114 on t h., i0t h %nn i v@r qe-- y of the f3i r thday of Allok-4endr Akimuvl@h Vorob yev mttdt toi, th&-.s group in 1948 A 4ertc-i of 19 Me-V oetatrons. was producF.d ioon afloT and the acceir-rators designed at the rom-,k Polytechni,-al In-ititute began to appear in the scientif:, F%tabli.uhments of the Soviet Union Over 50 electron a@ci-14-rators have been produced up to the present time and P-) and V-) Mt-V bptafroix,5 from the Tomsk Polytechut-cal Institute are working at Moscow, Leningrad, KLVeV Dnept0FIt-tro" Ka?an t-tt Two 15 MiPV betatrons have been set up at Peking Univergity and the C-hLn-Khua Polytechnical In&tttute On P@ofp%qrr Vorob'yev s init3istive, the T,,.amsk Pokytechni.ai ln,,ttitute h-&s now a large team of spef;ialkste in at@celerator teLhnology In 1958, an In-%titute of Nuclear Physic.-i Eli-:tron.,-% and Automation wa4 opened at the Tomsk Polytechnical In%titute tind it,4 activitleg are @.oncerned with the development @if iow, medium and high energy eltctron accelerators At the present time A A Vorob'yev dire--'@,% the Laboratory of ElectzonLc% and Automation which t-.% conterned with the fard 3/5 s/i3q/6o/ooo/oo6/026/n,@2 E012/E414 On th@, 50th Anniversary of the Birthdgy of Alck.4andr Akimovich Votob yew (I#-vt 1upmeani (if new 4@.cejerator in;.?,@_jlatkons including a new W3VeRUide d(,-ifratcr t!uggested bv VorGb yet, which w1il be ,apab;e of producing -ery high en*-.rgy elettron@%. although the o-.-ctall dimen..4ions of the installation and the high-frequ--n,N Power con-tumption will be small Renults obtained in this ,13rv@*ion wo-re reported by Vorob,y.@.v at the twernational C_t_nlvrence ois High Fnergy Accelerat-)rs which was held in Geneva in 11)59 In the fifties, Prefessor Vorob YeV &!so directed @hk.,/ rtsea,@h in he physILA Of solid dielectrics Among Profp.4,, Vosob yev s publications are "Charged parti@.le acceleratco 'El"kirital st:-ength of soliLd dielectrici" 'High-voltage ie,hnology", Ultra high voltages' and othet monographa, Piofessor @orob yev is the &uthor of some 200 scientifi- paper-4 and 7 monographi and textbooks He is a member of the Communiit Party of the Soviet Union (since 1940) and has frequently bepn elected am a member of the local committees of the KPSU in 1959, the -&titans of Tomsk unanimously eiec@ed him as thekr ford 4/5 swq/6o/ooo/on6/026/0'@2 9032/E414 On the 50th Anniversary of the Birthday of A I eksandr Ak I movi ch Vorob 'yev Deputy to the -:.upr-eme Soviet of the Rus,@tan Federal Republic Professor Vorob"yev is the holder of many Soviet awards including the Order of Lenin In 1960, he wa% awarded the honorary title of Honoured Scientist and Technologist of the Russian Federal Ropubltc Card 5/5 MOSKALEVY V,A,?, SKVOIaSOV, Yu.M. Two-cha-mber bota'ron for medi?ina.1 use, Med, rad. 6 no,1:62-.64 :61. U'G@%A 14! 3) (BETATRON) MOSKALFV V.A.; KHFSIN, G.L.; NAGIBINA, I.M. :_I Interferometer for studying stress fields in transparent models. Izv.vys.ucheb.zav.; prib. 5 no.4:80-84 162. (KIRA 15:9) 1. Loningradakiy institut tochnoy aekhaniki i optiki. Rekomendo- vans, ka-fedroy spektralInykh I optiko-fizicheskikh priborov. (Strains and stresses) (Interferometer) 41319 3/05 621032100910021014 B125YBi66 AUTHORS: Moskalev, V. A., and Okulov, B. V. TITLE: Intensity of betatron radiation as a function of injection voltage PERIODTCAL: Zhurnal tekhnicheakoy fiziki, v. 32, no. ), 1)62, 1040 - 1041 TEXT: The relative dependence of betatron radiation inteneit y on the I injection voltage is derived from the equation % - (E,/2eRO) I(E,/E 0 )2_1@8 by B. N. Rodimov, P. A. Cherdantsev, and T. A. Vedvedeva (Izv. vuzov, Fizika, no. 5, 6 - 15, 1959). E 0 - m c2 is the elect-ron rest energy, 2 0 Ei . U i + M0 c is the electron injection dnergy, U i the injection voltage, e the electron charge, R 0 the radius of the equilibrium orbit, 9 the croes- sectional area of the region of the focusing forces. The dependence of the charge QM entrapped into the acceleration cycle - and, therefore, also of the intensity of radiation - on the injection voltage is linear up to ,-100 kv, but becomes nonlinear above 100 kv owing to relativistic effects. Card 1/3 J/057/62 /03 2/00 )/00213 14 Intensity of betatron ... R125,/B186 This dependence is approximately quadratic at -1000 kv ani becomes cutic at still higher voltages. The @Jependence of the raliation yield on the injection voltage was experimentally checked at a 25-Mev stereobetatron (injection voltage 350 kv) of the Nauchno-issledovatel'skiy inatitut yadernoy fiziki, elektroniki i avtomatiki (Scientific Research Institute of Nuclear Physics, Electronics and Automation). The injection voltage was measured using a 5000-ohm divider between 50 and 250 kv at intervals of 20 - 30 kv. The dose rate was measured using an ionization chamber and a "Kaktuall-type standard dosimeter. Up to 250 kv the increase of the betatron radiation intensity with increasing injection voltage corresponds to the theory (Fig. 2). The desired considerable increase of radiation intensity requires injection voltages of 1000 kv and more. There are 2 figures. SUBMITTED: September 23, 1961 Card 215 ri t,: D-- @n@loncu je ,,/,57/62/",32/,-,0 1-)@21'011, b 12 5/ h 1 A ris i ty on t nj t.-c t ion vc taFv. Card MOSKAL&V I V.A., kand. tnkhn.nauk Local stresses in the Diaphragms of compressors. Vest.nash. 42 no.3:29-33 Mr 162. (MIRA 15:3) (Diapbragns(Minhanical devicewl) -1 MOSKALEV, V.A.; Oi'?,Uh .LNII:ILKOV, "j.A. Generation of' ihort radiation pulses in a betatron with a w.le gap. Prib. i tekh. e:@rp. 8 no.5;26-29 S-0 163., (MIRA 16.12) 1. NaUchno-i-,.ij@dc)vnt,.,JIskiy inst-Aut yadern(:y "ziki, i av-tomatiki '11,-):nLikogo polite,@Iinlches,,cgo instituta. MOSKALEV, V.A.; OKULOV, B.V.; OTRUBENNIKOV, Yu.A.; MORTON, Yu.m.; SKORIKOV, A.G.; SHESTAKOV, V.G. Results of the operation of a 25 Mev. pulsed two-chamber atereobetatron. Izv. TPI 122:50-53 162. (MIRA 17:9) ACCESSION NR: AP4041009 S/OIZO/64/000/003/0032/0033 AUTHOR: Moskalev, V. A.; Shestakov, V. G., Okulov. B. V.; Skvortsov, Yu. M. TITLE: Method for measuring accelerated charge in a betatron SOURCE: Pribory* i tekhnika eksperimenta,@no. 3, 1964, 3Z-33 TOPIC TAGS: betatron, betatron measurements, betatron accelerated charge ABSTRACT: A combined - direct and indirect -- method for measuring a charge developed by the authors (registration no. 34 311. priority of 0 1 Feb6 3) is briefly described. The target current pulse is recorded simultaneously with a signal induced in a special "indicating electrode. 11 Ja an energy under I Mev, the electrode signal is calibrated directly and then the calibration is used for measuring the charge with any energy. Two o,3cillograms taken at 0.5 and Z5 Mev illustrate the method. Orig. art. luas: 2 figures,. ASSOCIATION: none SUBMITTED: 07Jun63 ENCL: 00 SUB CODE: NP NO REF SOV: 015 OTHER: 002 Card 1 /1 T ROBIPV, Aleksandr Akimovich, doktor fiziko-matematicheskikh nauk; ,11.)SKALEV, Vladilen Aleksandrovich, prof. kand. tekhn. nauk, (totsent Development and use of betatrons in socialist countries. izv. 7ys, ucheb. zav.; elektromekh. F no.4:480-481 165. Nl""I., Ir-': r 1. TomBkiy politekhnicheskiy inttLitut. M091YENTS, A.A.; !TUf.s-1r,`V, V.A. Sourco of 7-ray radiation for Ugh-apacd photo,,Taphy of CIT-1 'A=GCCA--'3. 'J3;;.naUC..%.,'Ot. 9:ra-1?2 '164e O-M@A w8u) TOPIC-TAGS: particle accelerator, betatron- torotroup indicator electron accelers, r to ABSTRior t -iii indbicti6zi -electron accelaratbr is Bedy the construction of vhich-in shown In Fig. I of the Entilosure. A rising current in the vinding 1 prodaces a tor- ;oidal magnetic fleld vithin bhe toroidal enclosure 2 containing a toroidal feir P, netic eiore 3# Electrons injected around the periphery at 4 are accelerated by betatfta action and execute toroidal orbits in region 5. Drift of the electrons in the to- ; roidal magnetic field lo iuppressed by applying an appropriate potential dLfferencid between the core 3 aDd the wall 2 of the chamber. At the end of the acceleration period the electrons strike the ring-shaped target 6, producing bremss which is :1 ocuse d-on a point on the axle, where materials to be investigated or patients to be treated may be placed. The theory of the accelerator and the feasi bility of its constructioa are discussed briefly. It in concloded that much great;L L 49257-65 ACCESSION NX: AP50108W currents can be obtained with a torotron than with a betatron# that the torotron is much simpler than a linear accelerator, and that the torotron is much smaller and lighter than the high current induction accelerator of N.C.Christofiloo et al. Cdigh current linear iuduction accelerator for electrons. Voklad. na Mozhdunarod- noy konforeutaii po unkoritelyam zaryuzhennykh ebaotits ffoport to the Interna- tional Conference on Charged Particin Accelorators7 Dubna, Aug.1963). Orig.art. has: 11 formulas and 2 figures. 102] j ASSOCIATION: none SUBMITMD: Mar64, ENCLI 01 BUD CODE: Np NH BEV SOVt 002 OMER: 001 .ATD PRESS: 324 gord 2/3 L 4925*7@_65 APS010800 ACGESSION.INRt ENCLOSURE: 01 0 --soot ion (t-9 ................. jr to otvorI_-._.' Pigs 1, Schematic diagram-0 r 1 - magnet winding; 2 - toroidal chamber; 3 - ferromagnatic core; 4 - electron injectorsl 5 - electron accelaration regionj 6 ring.targets Card 7 ACC NR: AT7003998 SOURCE CODE: UR/0000/661000/000/0123/0131 AUTHOR: Goncharov, V. Ya.; -4ookalev, V. A.; Okulov, B. V.; Ponomarev, V. P.; Skvortsov, Yu. M.; Slupskiy, A. M.; Shashov, V. V.; Shestakov, V. G. ORG: none TITLE: Stercobetatron for 15 Mev SOURCE: Mezhv-uzovskaya konferentsiya po clektronnym uskoritelyam. 5th, Tomsk, 1964. Elektronnyye uskoriteli (Electron accelerators); trudy koll-ferentaii. Moscow, Atornizdat, 1966, 123-131 TOPIC TAGS: stercobetatron, betatron', Vne-V ABSTRACT: A two-chamber 15-Mev atercobetatron was built in the Tomsk Polytechnic Institute; it is designed for two cross brernastrahlung beams with a dose rate of 1000 r/min. m in each beam. The electromagnet and pulsed-oupply system of the accelerator are briefly described. Designed along conventional Card 1/2 ACCNR: cLectrornagnet ri@_ interpole space, a maximum flux density of 16000 g in the yoke, and a flux dei,-*'-- ... ---) Q in the pole Shoes. Resonance- circuit current, 300 amp; capacitor bank, Lu. -_ -farads. At 15 Mev. the excitation voltage is 345 v, magnetizing voltage, buu, - Electrons are injected at a voltage up to 200 kv. The electron gun has st.-tinless-stee-A I-rtrodes and is kept under a "floating" potential. A two -tantalum -pla U-Q inflector receiv@:s 3-rrLicrosec 30-kv pulses. A beam-extraction winding carc,.,q 15-microsec current pulses up to 2000 amp. The accelerator chambers are er,@:-,aupted (down to 8x 10-'g torr) by titanium pumps. Orig. art. has: 8 figures and 2 tatpips. SUB 41 CODE: 09. 20 SUBM DATE: 06Mar66 ORIG REF: 006 Card 2/2 A;,-70021 29 V. :40skaley V 1 Dina, Vo, non- T :T DotCrzuninj the sum of principai stresoej -.,;@*uh the aid )f in+.(,."_, _1s(,ooyu7.naya koriferentsiya po met-, ryazheniy. 5th, Lenin@@-ad, 1964. Polyarizatsionno-opti(;.,..-.:~,,-iy mc-toa n--i,ryazheniy (Polarizing-optica'l m,,-thod of investif.-atin6i t:-.1dy Leningrad, Izd-vo '@cn-.njr. univ., 19606, 5211-52i TJ*-:C TA,',Z: stress analysis, optics, optic mea3ure.,ent, optic Method, interference, interferometer, multibeam interferometer A3S-@L', 7he ccnstruction and performance of a d(.v,.:-,e uJed fu:- tuu(2 principall str-esscs in materials are dc3cribed. The work waj don@,, _'-t '.rj" :nstitute of Precise Mechanics (Leningradskiy institut tochnoy .','oscow Structural Engineering Institute (Moskovskiy inzhenerno-atroitf_,@'r@fy The device is the triple-plate interferometer IT (see Fig. 1). The consists of three light-separating covers A, B, and C set on glas.-3 plates. ',he paths are shown in Fig. 1: rays 1 and 2 form the interference pttturn of intensity, and all calculations are referenced tu thoua two. '2110 VAI-11_1t@Ull 1.01C th(j Card 1/3 ACC NR: AT7002129 L jar T I .4 b ATO el@ C Pr D, 1-1/7 F" L 4 g. Triple-plate interferometer: a principal dJaGra_L of thc aevi::e; b - optical diagram of the interferometer; A DRSh-250 lamp;.,J7. J':3- 706 lamp; 31 rotating mirror for source shift; K - condenser; Aj input diaphra-Sin; CO light filter; 0, - collimator objective; 02 - camera objective; A,B,C interferometer plates, 3 2 - rotating "ocular-photo" mirror; D and D output diaphra&La3; TT - rotating ocular prismi 3,, 2 3 OTT - photo attachment distance between the light-separating covers may be equated with the leng-th of t@qe optical. paths of the first and second beams. The path difference between paths 1 and 2 is given by Card 213 ACC NR, AT70021,29 -here N is the order of interference; tec- variatio,-i c:." thickness of the modei; r, r'!"@-actl3r, 11-idex of t,,.;, model. Also, from Hooke's Law all -F -,)I and for o-_ - 0, it follows that + GY). L whero '.; Ln,l LL are th(., modulus of ela-,jtioty and Poisron'3 coeffi@;ient., Principal stresses are then related to the order of interference by the eq'!;It@(J"I Ek Thi- autho:-s 11ustrate by example how the device may be used to dC!te:-=inL- t,-.o of principal stresseq and each principal stre3s individually. The device @tje-." _j noted as beina simple in con3truction and in use, compact, and 91,abl@@ :'e.@ '-., Q r- t vibration Lind temperature variation. Orig. art. has; 5 fig-reo and 5 S-UB CODE: 20, 13/ SUBII DATE: 14Jun66/ ORIG IREF: 004/ OTH REP: 007 Card L -i3o4o-66 ACC NRI AT65001403 SOURCE CODE: UR/3180/64/009/000/0171/0172 AUTHOR: Vord'vey. A A Makalev, V. A. ORG- None TITLE: An x-ray source for high-speed photography of various processes SOURCE: AN SSSR. Komigsiya po' nauchnoy fotografti I kinematdgralli. Uspekhi nauAnoy f6tografti, v. 9, 19004. Vysokoskorostnaya fotografiya I kinematograftya (High-speed photography and cinematography), 171-172 TOPIC TAGS- x ray photography, high speed photography, stereoscopic photography ABSTRACT- The authors, describe a 25-Mev high-current stercobetatron for studying high- speed processes. The device produces two bremsstrahlung beams which intersect at a given point. The beams may be emitted simultaneously or with a time spacing of up to 50 psec. Pulse duration S 0. 2 r6ec. 'Me betatron accelerates an electron charge of 10-7 coulomb, which Is (5-6) * lot electrofis per cycle. A 0. 2 psee pulse penetrates 140 mm of lead. The size of the focal spot is 1 x 3 mm. Preliminary studies show possibilities for an Increase In the accelerated charge and a reduction In the dimensions of the focal spot. The unit may be used for stereo x-ray photography of processes lasting less than to- second. Non-simultaneous beam generation may be used for photographing a process from two points of view with various time lapses between frames. There are possibilities for developing :rd 1/2 1- 13014o-.66 ACC NR, AT6001403 0 a stereobetatrou for operation at 1000 cycles per second. Orfg. art. his: I figure. 1081 SUB Wqg@ 141- .SUBM DATE s- nonel ORIG REF; , 001/ . ATV PRESS: , W f / I . - -@, k.- . .- ruo Ili @', V ,i , LEBEDEVA, Yu.A.; @IASVALQI@. J.D.* CHUKOV, S.V.; CHUMAKOV, V.I.; KAPLANAS, 0.[translatorl; MEDCNIS, A., red. (Protection against mass destruction weapons] Kaip saugotis nuo mnsinio naikinimo ginklo. Vilnius, Valstybine politinea ir mokslines literaturos leidykla, 1962, 31 P. (MIRA 16:5) (Civil defense) 14/5 163.3 . V9 MOSKALEV, V D Vaesoyuznoye Dbrovollnoye Obschchestvo Sodeystviya Armii. Aviatsi.i. I Flotu. Uchebrioye Posobiye Po MPVO (Manual for Fegional Anti -Ad rcraft Defense) Pod Red. V. D. Moskaleva (1 Dr.) Moskva, Izd-Vo DOSAAF, 1956- v. Illus., Diagrs., Tables. Lib. has: 1956, 1957. G40-RBUNOV. Ivan Petrovich; XOTLUKOV. Konstantin Grigor'6.V7ich;-UQj4jjgaV Vladimir Demlynnovich; KMWVSXAYA. M.D.. red.; AILDRIAN - B--q-7M"" -W [Civil defense groups and their trAining] Deiatviis grupp samo- zoahchity i ikh podgotovks. Hovkva, Izd-vo DOSAAF. 1957. 92 p. (Civil defenBe) kHM.,, 11-2) GORBUNOV, I.P.; GLUKHOV, J.P.; KOTLUKOV. K.G.; KOSKALL7, V.D..-- SIPATLOY. Tu.A.; SMNTAH, M.N.; SMROV. M.I.; BTKOV. S.G., red.; KAMMATA, M.D.. red.; BLAZIUMOVA, G.I., tekhn.red. (Training method@ for members of civil air defense groups) Keto- dike podgotovki lichnogo nostava gruprp namozashchity. Moskva. Izd-vo DOSAAF. 1959. 165 P. (MIRA 1):)) 1. Vzonoyuznoyo dobrovollnoyo obahchostvo nodoyetviya armli, aviateii i flotu. (Air defenses) 1-110341:4 EWA(b)/EPF(n)-?/Wr(M)/DD@/ES(b) AFFTCAPGOAMASa ru-41 *-'=--Li-- K2 PHASE I BOOK EXPLOITATION SOT/6423 Mebedev., Yu4 V. D. K00k&187,r T. Chukor,, and V, 1. Chumako7 70 .Kak zashchishohatlaya, ot oruzhiya, massovogo; poriucheni-y'a (How to Protect Yawaelf From Weapons or Kane Contamination) Kascow, Izd-vo D6340,1962. 30 p. No* or copies pr'inted not given;- .ftonsaring.Age=Xg Shtab grazhdanskoy oborony. Ed's A.-A, Vaviltyev; Toah. Mi 0. X. Blazhonkova. 2M?OSZ&. ThIs booklet Is Intended to acquaint th* general reader with. basic alvil. defense procedures, and, is recomimended for Itthorough COMAGE: This booklet briefly, deiaribes the effect of mass 4estrue- tion weapons, i.e., nuclearB gd bacterioloxica w and chemical," a 8 lists measures for piotecting the population--3gainst, their effects. Card 1/2 JL --A6 AOWN@O@&teat -Yourself J@rom Weapon& (Cont.) SOV/6423 TABLE OF CONTINTSt 6h! I.' Kodorn Na'as Deatrud'tion'Veapons 3.' Ch.-11. What Must be Done at Throat of Attaoic Ch. III. Responses to'C1v1l.Vefe'ftxe.S1gnals' 15. Ch. IV. .-First-Aid,: 21 ve Everyone Must-Know Now to Administer'First Aid 'Ch. VI*' How.to Prevent the Humful-Effeat of Poifonaus, Radioactive, and Bacteriological Weapons 28 AVAILABLE: Library of Congress (tmq@6.R% 1962a) 1SUBJECTz Civil Defame ChI16@ AQ/dk/tem Card 2/2 0-1-63 KOTLUKOV, Konotantin Griggorlyevich; MOSKALEV, Vladimir Dem0yanovich; GODINER, F.Ye., red.; SORKIN, V.Z., tekhn. red. [Aesi,onsibilities of the population concerning civil defense and rules of conduct undar conditions of enemy attack] Obia- zannosti naseleniia po grazhqanskoi oborone i pravila pove- deniia v uslo-iiiakb napadeniia protivnika. Moskva, Izd-vo DOSAAF1 1964. 45 P. (MIRA 17:2) 85893 (.,990313.2,03) 7,f 0 10 elY, / / 6 2. ) B0067BO60 A @i-JR 3: Moskalev, V. i. and Ordanlyun, S. S. Study of the Effect of Small Chromium- and Bismuth Oxide Additions Upon the Dielectri C and Piezoelectr-ic Properties of Polycrystalline B-arium Titanate PERi)DI@AL: Izvestiya Akademii naak SSSR, Seriya fi::ic@iLs./,ay@a. 1)60. Vol. 24, No. 11, PP 1412-lzjl'@ TEXT: This is the reproduction of a lecture delivered at the Third Conference on Ferroeiectricity which took place in Moscor from January 25 to 30@ 1960. With a view to finding novel piezoelectric materials with parameters stable also at hiiiher temperatures, the authors studied the effect of smaller chromium- and bismuth oxide additions to BaTiO 3' Commercially pure substances were iised for preparing the specimens; bismilth- and chromium oxide were che-.1ically and analytic@illy pure, respectively. The inixtures werp preheated at 1220 - 154007- (' ho@ir!!) lind Card 1/4 85893 Study oC the Effect of Smail Chr-@@mium- and SIOA,8 '(3/02,1, Bismuth Oxide Additions Upon the Dielectric B006/B06Q and Piezoelectric Properties of Polycry9talline Barium Titanate the final heating temperature rani, 'e was 1280-1340 0C ',12-5 ho@irq) A',* specimens had practically zero porosity at the beginnin@;; they ;vere "hot" DOlarized in the air, at temperatures near the Curie point Thc: electric fields applied ranged, depending on the composition of the specialen between 8 and 15 kv/cm (15-60 --in). 6 and tan S were meas@red on a Tesla bridge at 1 kc/sec and E_ = 40 v/cm, the piezoelectric 7.oduli '-einE determined by the resonance - antiresonance method, All @'easure:,.ents were made under air cooling. Some of tf- 'e measurement results -ire tah-lated; tne data obtained are in agreement with thos applied by other aut:.ors. A st-dy of the solid solutions of the BaTiO - Bi2 03* 3TiO2systemj (desiL;nuted as A - B in the following) and BaTiO 3 Bi20 3' 3TiO 2 -Cr203' 3TiO2(A-B-C) nhowed that the ntroduction of' biomuth ton.,3 or bitimuth j,:)nj 4 r: I I r - () I rl I i I [[I iona in BaTiO 3 concile-fibly reduces the teiqperLtL1f'0 f1t,'1h1l1ty Of 11,11C BaTiO3 parameters. In the compounds I: 95,-,@ A - 5% B; 11- 96.1,'@ A - 0 6/'0 C f - 3;0 B, and III: 94A%A - 0.6@@- C - 574, B (all values in ", by weiC@:t) Card 2/4 -.85893 Study of the Effect of Small Chromium- ond S/048/60/?24/011/029/036 Bismuth Oxide AdditiO.13 Upon the Dielectric 3006/BO60 and Piez6electric Properties 'of Poly- crystalline Barium Titanate the second phase transition was not to be ?ound in theo:.(t) curve as far @o--n an -80OC; varied only inconsiderably in the'range-80 - +50 oc (-1- 900); tanA- f(t) in weak fiejLds remains practically constant in the range -80 - +1000(f (tan @-3%13)- In Figs. 1,2 the temperature dependence of Diezoelectric_parameters is illustrated for compounds I, II, III, BaTiO 3 and 94,"'BaTiO - (;%CaTiO . The additLons were all Xound to have a flattening effect@"upon 1he curves,3the least to do so being the calcium titanate sIddition. The other additions not only have a flattening effect but also cause the curves to run nearly parallel to the temperature axis..Fig. shows tan4.f(E); here as well, the additions have a flattening effect, the most favorable-being found to be I (the losses increase slowly and lineal--ly with E). The best effects were found to be gi ven by additions on fres j"; and (d 31-E Y'oung)2. The latter parameter (which characterizes the specific acoustic power)is for Il and III tro to three times as large as Card 3/4 85893 Study'of the Effect of Small Chromium- and S/048/60/024/011/029/036 Bismuth Oxicle Additions Upon the Dielectric B006/BO60 and Piezoelectric Properties of Poly- crystalline B rium Titanate for ceramicsPrith 6@XaTiO,l despite a reduction of the piezoelectric modul@r- Th 3 figures, 1 table, and 2 references: 1* Soviet and 1 US.' .2re are I I TK. T TK 2TOPOM CO&SO. d,,.10- tips cocras, see. % af-ro nepe. 20 -c.e;t. CUSM 101111. C B.TiO, 120 1550 is 1,9 99,4%BaT1O,-O,"JCrtOa-3TiO2 120 8t. I IOU to 1.3 '98,3410 13&TiOs-1,7q6CrjOs -MO, 125 CYOOO 800 0 0,9 -06,50~Ba'riOt-3,50;CrlOg.3TiOl@ 125_ 2M 450 -30 Legen@ to the Table: 1 Co.1position, ','/, by weight 4@ at 200C 2@ Curie temperature 0C 5 Temperature of the second phase 0 3) cat the transition, C Curie point 6) d .1CP at 200C, CGSE 31 Card 4/4 140SKAW-1 _yj@jgjr-j-asifovUjb; GERIWIOV, Alekeandr Aleksandrovich; SHA- TSILLO, 0.1., red.; FOtIrCIfh'V, A.G., red. izd-va; BELOGUROVA, I.A., tekhn. red. [Description of systems using three-phase magnetic amplifiers for controlling the power supply of electric furnaces) Oplaanie usta- novok a ispollzovEniem trekhfazrqkh magnitnykh usilitelei (TI-1,U) dlia regullruemogo pitaniia elektricheskikh pechei. Lenirgrad, 1961. 20 p. (1,eningradskil Dom nauchno-tekhnicheakoi propagandy. Obren pe- redovym opytom. Seriia: Prorrichlermaia energetika i gazifikatsiia prompredpriiatii, no.3) (14IRA 14:10) (Electric furnaces) (Magnetic amplifiers) (Electric power supply to apparatus) E V TOTA *8 Pa_V WUIVA=jN WX Sm WY Alovema M"OIIMTOIV3 mad. WA*4W7=04, Way, m$1255). in RMIM., Tho tutsl cnil-netion W@rsat*s monotonically frm M Usy, The for tim reaction p + p + p + a Increases monatomicaUy from (2.0; 2.0) x 10' 4e at 450 MW to 1.3) x W4"en0'at 060 MeV, Uw threshold energy for this reaction ties between 410 IdsV a" MV, which m-.comtm for 4ft the Lugo uncertalMits ta,Uw kma-awma glass- settions. SUBJECT Uq,),R / 1,11mic"; C,@ 111)1 PA - 1(j)") AUTHOR DZELEPOV,V.P., i'-',OSKALBV?V.1. TITLE The Total Cross Section of pd-Interaction in t@ie Energ@- Interval 390-650 1!4-11- PERIODICAL Dokl.Akad.11auk, 110, fasc-4, @39-541 (19@@6' Issued: 12 / 197-67 The present work discusses the determination of this cross section on the synchrocyclotron of the Institute for Nuclear Problems of the Academy of Science in the USSR by measurinE the reduction of the intensity of the collimat@_d Droton bundle by samples of ordinary and heavy water at "good" geometrical conditions. Arrangement and method of the experiment were similar as with V.P.DZELEPOV et al, Doki.Akad.1,auk, 1049 360 @19';5). A scin- tillation counter registered all protons deflected from the original direc- tion of the bundle uD to 30. Triple and quadruple coincidences as well as retarded quadruple coincidences were meaaured, and results were shown to- gether in a table. The scattering cross sections a n(n-d) = cT (D 20) -0 (H20) remain constant within the energy interval of from 390 to 650 MeV and within the limits of measuring errors. At an energy of 390 MeV, Cp(d-p ) agrees practically with the value of a p(p-d)- (31,6.2).10- 27cm2 obtained at a proton energy of 406 MeV. t0thl cross sections of pd-interaction were computed on the basis I The Dok 1 . Akad. Vauk, 1 10, f a s c. 4, ') 39 -') 41 ( 19 @ 6) C ARD ? / 2PA - 163@ of the total cross sections of pp-interactio:i found by the authors and by S.V.MEDVEDI. U pd increases by about 25/4o if proton energy increases from 390 to 650 MeV, which is apparently due to the increase of the cross sections of meson production on the occasion of elementary nucleon-nucleon collisions. A comparison of the3e results with the total crosit sections of nd-interaction provides an argument in favor of the charFe symmetry of nuclear forces at high energies. Also the difference between the sum of total cross sections for free pp- and np-collisions and the total cross section of pd-interaction is given. At a proton energy of from 580 to 650 MeV this difference is somewhat greater than measuring errora and amounts to about 8@6' of the deuteron cross section. For the observed reduction of the deuteron crostj section the following reasons are given: screening of one nucleon of the deutoiron by the other, interference effects, forbidding of some final 9tates of nucleons by the PAULI principle, and the simultaneous interaction of all thr?e particles participating in the collisions. By the methods of the diffraction theory, 2 C1d 1 + C2 -(a 1 C2/4n)(1/r )d is obtained for the total cross section of th_@- deuteron. Here c 1 and cl2denote t@.e cross 3ections for the free nucleons, and rd-1,7.10-13 cm is the radius of the deuteron in the triplet state. The satis- factory agreement between computed and expEarimental data seems to confirm R.J.GLAUBERIS explanation of the deviation from additivity of the nucleon cross sections of the deuteron. INSTITUTION: Institute for Nuclear Problem!i of the Academy of Science in the USSR DZHM-EPOV, V.P.; MOSKAW.V, V.I. TotAl cross section of pd-interactions in the 390-650 14ev energy rnr4ple. Dokl. AN SSSr 110 no.4:539-541 0 156. (MMA 10: 1) 1. Instutut yfLdernykh pro@)lrim lkFtdemii nauk SSS't. Predmtnvleno tkadmal- kom L.A. Artaimovirhem. (Nuelmnr reactions) 352 8 ]'(.)'I'A 1. CRC6S M III ::t IAEV PH(117ON" WITH NUCLEI Y, 1. M"W@v L@ V GayrilovaW &k2j. of ue!"r 9 2t1-=--7 I @' lady @ - @ L 110, 9,2-4MF@6) Out. 21@ tin A.2,E-,an, Total cross aectiomi for the interactions of 650-briev th Be. C, 0. Al, Cu. Sn, Ph, and V nuciel vore Tneasur-1C.11i a eynchrwyciotron using the iiii-thtidn previ- ously Ued by V. P. Daholeliov at %I, Mokindy Akad. Nallk 8.21,8,11. '104, 38011955,@ for total cross sectionti of fp,p) anJ (P.d) The We Its gijon showing he valuus of the toW cruse sections. j% and cross stwdom of Inelastio InleranDon o,,. Worpolistions of tht, v3lues obtained for a, frova tho availablo valuum for protons with tf5 to 408 Mev phowud that the r!rat;d ut-eti,mm for light wiviel increaao about 10 tn 2a% with pruton erurgien up to 653 Mov. I'ho cross sc-otionn of InAaittu Interar-Aionj muaiiured for 134- Wit protwis colitc1th, Mth)n limit, 4 arr4c with or,@A aectlotiB at 00 Mvv, Tbe , t,,t- i,-t 1u, 0- Ititeractin-1 tit 86t, Ntev jirigon, kvith ti-,, U, rd Al, 1- imijivl&, with I@ii tf)[alm-d datit, wbilt, fur the h,,4vv iawiui of HAd Mvv t6o er,jt- iii-7tion ti `,toiluaLed about IA, I'lle r4dif fnr qtuikk It worv (Jeforvinv-0 .... I ho ba,d@ of It, VAIUDS, It VOW" fit @tll ww", I fiwl! Lt.- to U Itij .." t I%i' titralght line it r,,A, 'Ahl@rtt I " (I.vt , o.fia) , I-J " Froul the ridation (j, /N W, it IM -itivit Owl the 11cav I art) ;tjj;jn,-,1 noij fijr firmull.-I tit lhu alojvv t-wr - YI(w, While tho III-,bt -'ilviol !J11mv it volvd.1,91'abio iralay.tr avvy (jt.V.J,l A 21(a) SGV/56- -5-6- 3e, 44 AUTHORS: Budagov, Yu. A., Viktor, 3., Dzhelepov, V. P., Yer=Glov, P. ?., Moskaley,,_1., 1. TITLE: The Electron-Positron Pairs Which Are Formed in the Decay Te - e- + e+ + Y (Elektronno-pozitronn@ye pary, obrazovannyye pri raspadetro - e- + e+ + y) PERIODICAL: Zhurnal eksperimental'noy i teoreticheskoy fiziki, 1958, Vol 35, Nr 6, pp 1575-1577 (USSR) ABSTRACT: In a diffusion chamber, which was filled with hydrogen (up to 25 atm) and was irradiated with a 150 MeV negative pion beam of the synchrocyclotron of the Ob"yedinennyy inatitut yadernykh iseledovaniy (United Institute for Nuclear Research), 14 cases of a charge exchange scattering of negative pions by hydrogen + 0 with following 11-0 --we- + e + y decay of the'tT -meson were recorded according to the Dalitz (Dalits) scheme. This chamber had a sensitive range of 380 mm diameter and operated in a 9000 Oe constant magnetic field. These 14 cases were found Card 1/3 when looking over 45000 stereoscopic photographs. Two of these SUVI 56- 35-6- 38/44 The Electron-Positron Pairs dhich Are Formed in the Decay -iro - e- + e+ + Y photos are attached. The results obtained by the evaluation of plates with electron-positron pairs skre given by a table. The electron energies E_ and the positron energies E + could be de- termined from the curvature radii of the traces with an inac- curacy of not more than 10-15%. The total energias E - E_ + E+ of all pairs are within the interval of 17-270 &IeV, which cor- responds to the energj spectrum of the y-quanta formed by the decay of neutral plonj (produced by re-charging). The table also contains the correlation angles a (in the laboratory syutem) between the electrons and positrons of the pairs and the angles 0 between the direction of motion of the center of mass of' the pair and the incidine, negative pion. For the general form of angular distribution it holdu that P (a)-, con8t da/a (R. If. Dalitz) (Ref 2). Because of' the good correlation between the electrons and positrons produced by the decay Tr 0 ___O_ e- + e ++ Y the angular distribution of pairs must be in very good 0agreement with that of the y-.Iuanta originating from the decay ir ---0- 2y. Card 2/3 The kinematics of none of the 7 pairs with exactly determined SOV/56-35-6-38/44 The Eloctron-Positron Pairs Which Are Formed in the DecaylY 0 -- e - + e+ + Y total energy corresponds to the decay'ir0 --o-e- + e+. Besides, not a single decay gations are still Krasnoolobodtaeva graphs. There are which are Soviet. 1 --o-e- * e + + e- + e + was found. Investi- being continued. The author thanks L. I. for her help in looking through the photo- 2 figures, 1 table, and 11 references, 2 of ASSOCIATIONt Ob"yedinennyy institut yadernykh issledovaniy (United Institute for Nuclear Research) SUBMITTED: August 26, 1956 Card 3/3 KSKALEV V. . 1. , FLYAGIN, V. B.,, 3 HATET, T. , RTIDAGOV, YU. A. , DZIMLO'07 , V. F. v DZHAKOV, H. I., IVANOV, N. I., LEPIWV, V. I., wMe One-Meter Propane Bubble Chamber in Magnetic Field" paper preeented at the Intl Conference on High Energy Physics, Rochester, H. Y. and/or Berkly California, 25 Aug - 16 Sep 1960. (--w Qz, -j) I -j -"I ot 3-1 .41 A Iq F- 11-3 4 1 :-I --w .-r7. Is o U : v 4o"Ic (n.w -1 c 7 T -Y 4 4. 7, `4@0 'C ...... I:. T'.. p- 1- -1 a. ........ ... . '*d p- "d ...j q%j. ...S. (V V" I- ... -d .'It I -T.4 q% J. Vqj .4:j,:qjEqII IT.. -zp. , I I 1.1; qs lq p-j-Iq. jz -TV. .%I ..IT .... ... $1-T jq, qsl. P-Tlu Q,t- '-*q _U ;.p ...... . @'Ji, .42 11 Ilu -1 1- '611 'IV. I '. t:' - I tz-g.r, Vq3 ZT- Itot -4d or -I Z--4-13 .... I I -TTZICCZMA J. f-C R, .1 t@ I.j It -.Uz -d (lug BUDAGOV, yu.A.; )MJOLOV, P.F.; KUSHNIREIIKO, Ya.A.; MOSKAIEV, V-I- Z-@ Excitation of the He4 nucleus by 150 16M. Zhur. ekep. i teor. fiz. 40 no.6:1615-1617 Je 161. (MIRA 14:8) 1. ObOyadiaennyy institut yaderny'kh iseledovaniy. (mesons) (Helium) v i@@.z BUDAGOVO Yu.A.; YMAOLOV, P.F.; KUSH1111LENRO, Ye.A.; ?!BSKALEV, V.I.; SARANTSEVAp V.R.1, takhn. red. [Interaction of 153 negative JT-mesons and beliur-1 Vzaimodeistvie otritcatallnykh 5T-mozonov n geliam pri energii 153 Mev. Dubna, OblledinentWi in-t iaderrWkh isal., 1962. 32 p. (NMA 15:3) (Nuclear reactions) (Mesons) (Helium) I-IA 0 1 5/05YO2/042/005/009/050 B104 B 102 T 32, S Buda6ov, Yu. A., Yermolov, P. F., kuahnironKo , Ye - A. , 1:oakalev, lnteract.@o.-i between IL -,MLflor,8 iii-id heliUM els@,erimental ' noy I teoreticKoOkOY flziki , v - 42, 11)1-1206 4 In, interacti&n bvtween I 53-114ev P, -nesona a,-,d He at 17.6 atm E @rejsure Una a MaE@netic fie:d of 1 CC, @; oersted3 wa.9 s-u:--ed i r. a dif@usion ciamcer. T'-Ie maximum drop of the magnetic field s*.re:@,- -n the central ran,@e of the c-perating volume was the Oaximum i ' form@ ty of tne za,@;netic eld wa@i t4d. The mean meson energy was n e e,@ the c,;rvature of the meson tracks. The half-width of the ez3r, @nerL;y di-stribution in "he cnamber was 9 Yev. The and electron ad.,:.'.x-ure aas @".6 + 2)'. 'he total r.- ir-,teraction crose section, the elus*ic scatterini., cross section, and the cross sections for a number of @ne:ast`c processes were determined Ly measur-ing the total length of n--:-,esGr, trac?s in the chamber. The angular distribution of elastic n- He Ourd 1/2 @:6 162 'C42 /3,@5 CG@lorr .a.nteraction bet;,ieen I 1,3-1@ev . . . 3104 3102 ir,teructi c,,-, i@i of di f'i ructional r,a*.ure eii Lh a di sti nct first ,inimurn (at Ln a a e c C, nd max izum a t 1 U_ 00 @,'alculations of elaitic scattering n t h e'3aa @a o f an oit i cal mode. .-j @4 th square ccm-ll ex potential IV V - V + iV,, showed that beat aCreenent with experimental data was c,b-.a,_r,ei with VR. _16 + 7 Mev, V T- -63 + 6 14ev, ro . 1 -5-10 cm. Those valut@s arree with those found by it. @,. Frank et al. (Phys. Rev., 101 1 ) 56 ',"ho distrioution of r,_-mesons quasi-elastically @,cu-.tered from intranuclear nucleons is compared with theoretical results iat son e t al . (N-uovo C Iz., 10 , 45 3 , 1956' .The probability of L.,;' tipl. @.Jon scattering from iuclei and the chari;U exchange scattering c2,s6 sectlon are outimattid. The cross section of inelastic scattering - a Js -0 ".1 char. exchange . about 10,4 of the cross section of inelastic :n*vzaction. 'I"here are 6 figures and 4 tables. @-`3@,C:ATION; Ob"yedinennyy institut yadernykh iesledovaniy (Joint Institute of Nuclear Research) S -; 3:., 1,@T -_ DDecember 29, 19061 Card 2/2 Ju ot D7111"WTV, V.P.; YFRIMUIM, T'.F.; '-1()SKA1J-,V, V.I.; FILICHENFCV, V.V.; IM. Elastic scattering of d P- mesic atoms by protons, de-,@terona, -nd compound nuclei. d"bur. eksp. i teor. fiz. 47 no.4:1241-1@-16 0 164. (Mli-A IF: 1) 1. Ob"yedinennTf institut yadernykh issledovaniy. L 36462-66 Wr(m) ACC NRo Ap6o18802 SOURCE CODE: UR/0056/66/050/005/1235/1251 .AUTHOR: Dzhelepovi V. P.; Yermol-ov,- P. F.; Moskalev, V. I.; Fillchenkov, V, V, ORG: Joint Institute of Nuclear Research (Ob"ycd1nr--nnyy institut yaderfi-ykh isaled6-vaKiy-) P, TITLE: Negative muon catalysis of-,,nuclear reactions of c4. -f- p+ and dlt+d-C+P+IA- and the formation of Pdi&andddp Molecules in gaseous hydrogen SOURCE: Zh eksper i teor fiz, v. 50, no. 5, 1966, 1235-1251 TOPIC TAGS: muon, hydrogen, deuterium, nuclear reaction, catalysis ABSTRACT: The yield of nuclear reaction of dtL+p@pdjA--1JeJ+jA- and dp+d-ddIA-P+I+V have been measured in a diffusion cloud chamber filled wfth hydrogen and deuterium at pressures ranging from 7 to 23 atmi Card 1/3 L 36462-66 ACC NR: Ap6ol8802 The muon transition rate from the deuteron muon atom to carbon and oxygen has been found from experimental deuteron muon ranges and Auger electron yields. The formation rates of proton deuteron muon and deuteron deuteron muon molecules (reduced to the density of liquid hydrogen and deuterium) have been found to be A,vdp - (IJ:t0.5)-104 geo-4, Addo - (0.75:L0.1 1) -104 MC-' -Estimate of the relative yield of the reaction dt&+d--9-ddA--*tA+p shows that the relation of the yield Of dp+d--*.ddIA--*Ctt+p to the yield of dt&+d-ddj&-p+9+p- is less than 0.14 with a 90% probability. Analysis of experimental data on the reactions dp+p-pdp-He'+,.- and dp+p,pdp,j,,,,+Y leads to the conclusion that the resonance mechanism of the formation of deuteron deuteron muon molecules is likely to be the reason for the large yield of the two deuteron fusion reactions under conditions of experiments conducted by the authors. The authors thank Yu. V. Katyshev, M. Friml, L 36462-66 ACC NR, Ap6o18802 and Ye. D, Shcherbakov for their particip-tion In the In1t1al 7tage of this work, and S. S. GershtqjEjor h1o valuable dis,@usslons. art. has: 9 figures, 19 formulas, and li tables. [!3ased on au-.noral abstract] (NT1 SUB CODE: 20/ SUB14 DATE: 23Dec65/ ORIG REF: 012/ OTH REF: 010/ 3/3 ACCESSION NR: AP4042565 S/0056/64/046/006/2042/2045 AUTHORS: Dzhelepov, V. P.; Yermolov, P. F.; Katy*shev, Yu. V.; Moskalev, V. I.; Fil'chenkov, V. V.; Friml, M. TITLE: Catalysis of the nuclear d + d - He 3 + n fusion reaction by negative muons SOURCE: Zh. eksper. i teor. fiz., v. 46, no. 6. 1964, 2042-2045 TOPIC TAGS: nuclear fusion, muon, mu meson catalysis, negative mu meson, hydrogen, deuterium A13STRACT: This is a continuation of processes in gaseous hydrogen (V. P. Intern. Conf. on High Energy Physics V. P. Dzhelepov, At. energiya v. 14, al., ZhETF v. 42, 439, 1962), and is previously unobserved reaction d@j + earlier research on mesic-atom Dzhelepov et al., Proc. 1962 at CERN, Geneva, 1962, p. 484. 27, 1963. V. P. Dzhelepov et aimcd at observation of the 3 - dd@L . He3 + n + This Card 1/3 AC(;ESSION NR: AP4042565 reaction is one of the fusion reactions P IC + + dIL + d - d4ji PIL -@- ( I 10,11 --,- 11, + P which were investigated earlier. The experimental conditions made it aloo pouniblo to rogigtor ranction (1) and obtain Boma ontimates of the yields of reactions (3) and (4). The tests were made with a diffusion chamber filled with deuterium to a pressure of 7.2 atm. ,,ihere 20 events of the hitherto unobserved reaction (2) were detected. The ratio of the yields of reactions (2) and (1) is 1.20 + 0.37. Fstimates of the relative yields of reactions (3) and (4) give, with a probability of 90','., w(3)/w(l) < 0.13 and w(4)/w(2) < 0.13. The yield of the reaction (1) agrees with the data obtained by the au- thors earlier, but the yields of reactions (1) and (2) measured in Ccrd 2/3 ACCESSION NR: AP4042565 the experiments exceed by one order of maqnitude those that can be expected on the basis of the data on reaction (1) obtained in Iiquid deuterium by several authors. Estimates of the yield of reaction (5) call for additional data r'eduction and will be published later. Orig. art. has: 2 fiqures and 5 formulas. ASSOCIATION: Ob"yedinenny*y institut yaderny*kh issledovaniy (Joint Institute of Nuclear Research) SUBMITTED: l0Feb64 DATE ACQ: ENCL: 00 SUB CODE: NP NR REF SOV: 003 OTHER: 005 I I Cord 3/3 L 13487-65 EVIT(m) D1J&AP/AFWL/S$D/ESD(t) ACCESSION NR: AP4047891 S/0056/64/047/004/1243/1256 AUTHORS: Dzhel2eov, V. P.1 Yermolov, P. F.j Aoskalev#-V. I.1 Fil'n-, chenkov, V. V.; - E@ZKAMIJ-A' TITLE: Blaatic scattering of dMu mesic atoms-by protons, deuter- ons, and complex nuclei SOURCE: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 47, no. 4, 1964, 1243-1256 TOPIC TAGS: elastic scattering, mu mesic atom, proton scattering, deuteron scattering, complex nucleus scattering,-scattering cross section, ABSTRACTt This is a continuation of earlier experiments by the authors (ZhETF v. 42, 439, 19621 Proc. of 1962 Intern. Conf. on Hig h-Energy Physics at CERN, p. 484t Atom. energ. v. 14, 27, 1963) and describes further experiments on the kinetics of d4 atomic pro- Card 1/4 L 1.3487-65 ACCESSION NR: AP4047891 cesses. The range distribution of du atoms in hydrogen containing :various concentrations of deuterium and of Z-impurities (C, 0) and @the hitherto unknown cross sections for elastic scattering of d@L -atoms were measured,. using a diffusion chamber in a magnetic field. -1 _diam@t_e_r__386___ - - __ therftagnetic --field was The diffusion chamber has a mm. :7000 Oe, and the negative mesons were obtained from the OIYaI synchrocyclotron, slowed by a filter, and stopped in the gas of the .chamber. A detailed description of the experimental setup and con- .ditions was given in the cited earlier papers. The data reduction procedure and program are described. The cross sections were de- termined by a X2 comparison of the experimental distribution with those calculated by the Monte Carlo method.- The values obtained for the elastic scattering cross sections agree well with the theory. The lifetime of the dp atom in hydrogen gas containing Z-impurity concentrations of 1/4000 and 1/800 is 1.25 1 0.16 and 0.42 1: 0.05 psec, respectively. The crons sections for the elastic scattering of dp atoms in the various processes, obtained experimentally and the- -Card - 2/ 4 L 13487-65 ACCESSION NR.- AP4047891 oretically, are: Prricr-,%s F-xneriTmnt 3 4p + d-@-dp + d (4,15�0.29) -10-10 5-,11 1 1 10@1,1 i do+p-dp+p (0,1 i - dp + Z-d;& + Z @(1,2�0,3)-10-1# 1 10-18 An analysis analogous to that described in the a rticle is in progress, for the scattering of p@L atoms by protons and the results of the pre- .sent work are being applied to an interpretation of the yields of the nuclear reactions p + d@t -+ He3 + 4- and dp + d -+ t + P + wbich will be reported later. "The -authors are grateful to GerghtMjj, KP.IZ;Lr I._N,. Silin, R. M._.gujyayev, and V. Mo imy Tsunko- for useful discussions and valuable remarks, and to L. I. Krasnolobodtseva Yu,..jjL_�AyjLiVac and T. --9. Ob"Vezdnova for help with the measurements." Orig. art. has: 10 figures, 9 formulas, and 4 tables. 13487-65 !@-ACCESSXON NR: AP4047891 ASSOCXATIONt Ob"yedinenny*y institut yaderny*kh issledovaniy (Joint Inutitute of Nuclear Resear SUB14XTTBD: 13May64 ENCL: 00 .SUB CODE: UP NR REF SOV: 006 OTHER: 007 Card , KOSXALE.V.,. V.M.; KHLSKIN, L.S., redaktor; KORNZYXVA, V.I., takhnicheskiy reddkfo-r' . [Textile materials used in the chemical Industry] Tekstillnys materialy, primeniaemye v khimichaskot promyshleanosti. Moskva. Goo, nauchno-tekhn. Izd-vo khim. lit-ry, 1954. 116 p. (KLRA 8:1) (Cheml@ftl induatries) (Textile fibers) PAIATNIK, L.S.; KOSEVICH, VJI.; MOSKALEV, V.M. Growing single crystal layers on Lig=th by the vaLcuum co:, densation method. Fiz. met. i metalloved. 16 no.3:403-408 5 163. (1,111A 16.11) 1. Kharlkovakiy politekhnicheL;kiy institut tmeni V.I.Lenina. L m Z-71,1711 ( t'rl' JD ACIE74R, A90267i4 SOURCE CoD@t UR/0181/66/G08/008/2484/2486 LU AUTHOPLI Kosevichp V. M.; Palatnikp L. 3 Moskalev -to r, @a OR3: Klarkov Polytechnic Institute im. V. 1. Lanin (Kharlkovskiy politakhnicheakiy institutT- IV-7 .;,I TITL31 Distribution of growth microstops on faces of NaCl crystals SOURCEZ iizika tverdogo tela, v. 8, no. R, 1966, 24,94-2486 TOPIC TX-j3: sodiwri chloride, single cz-jstal rrow1h A@T-'iACTI 7110 d ribution of -Acrost,@r,-- on, (Col) racus of cr-.-s.aLq was st,iiled on sin,,71e---Fista1Aayors gro-in 1@y vacaur CO.,)' on ';aCL strwln Crystals. @e:;Poratur3 T. of th,-, las yariq'@' betwe'@:-' I and mi,-ro5tons or uni:-.olocul.,tr @v)rn ar. oLor-tron uE`n- icxcor-atlon with trol@: -)artic1,!-,. f :I-LcrosteDs) 3M ;as usod for a Z tie o!* -Acrostt dripondence of Sri -in T, "@r a con,!,insution rate w = 10 A/@oc was dotf@r- '%"nod' ar,@" 5n 1,ras evaluated theoraticall't. 7@fj a=,erl,zental r3ata sho-,i that tne i:-rowtn of 'iaCl cryutals in tho IcO-4100C ranj@c is controllqd nrimarily by procosses of sur- faco migration of molecules. The remaining quantitative c@'aractnristic3 of the dis- tribution of microsteps are directly related to SS thus, the mean distance botwoon the microstops 0-3 Vr--@-M, and the area of the growth microf igure 15 Sm. 7n 9 Card--I/L L Cb437-67 ACC NR: AP6026714 1; .1 critical condition determining the size of a growth microfigure is that the free area between the microsteps be close to 3m. Orig. art. has: ? figures and 2 formulas. SUB CODES 20/ SUBIM DATES 1IFeb66/ OIZIG R&F: 002/ OTH REFS 002 2/2 44,@@ !%SKALF,V, VIII. Using the track of the AO-4 lint blcKter for the travel of the AO-6 lint blower. Tekst.prom. 23 no.1:46-47 Ja 163 (14IRA 16:2) 1. Rachallaik remontno-mekhanicheskogo otdola batviyokoy kam7ollnoy fabriki. (Spinning machinery--Maintenance and repair) S/113/60/000/002/0091/009 D207/D306 AUTHORS- Reznikov, A. S. and Moskalev, V N. TITLE: Powder electromagnetic automobile clutch couplings PERIODICAL: Avtomobil'naya promyshlennost;, no. 2, 1960, 42-45 TEXT: The article describes the principle of the powder electro- magnetic clutch, discusses some western clutches of this type and proceeds to describe the Soviet HAMVi(NAMI) cylindrical powder electromagnetic clutch (Fig. 5). The magnetic system is situated directly in the flywheel and the whole clutch weighs 22 kg, The excitation winding is fed from the armature of the engine generator but draws its current from the battery until sufficient revolutions have been developed for the generator to proceed to self-excitation. The control system is so regulated that at 1,600-1,800 rpm the generator develops maximum voltage, corresponding to the maximum transmissible moment. The clutch is set to begin engaging at 500- 600 rpm, i.e, at minimum steady engine revolutions The moment transmitted by the clutch thus increases proportionally to the C ard 1/3 S/11 60/000/002/009/009 Powder electromagnetic... D207YD306 engine revolutions. To prevent the engine f@rom stalling due to a too sudden start or during acceleration on uphill grades the system provides for some shift in the characteristics so that the power supply gives a decrease in the clutch moment in relation to the moment of the engine, The baffle plate pedal is connected to a switch which breaks the excitation winding circuit, The c'-,ttch can, therefore, be disengaged independently of the erq,,ine revolutions. Stand and road tests of the NAMI clutch have shown that the mechan- ical and electrical parts function reliably. After 10,000-15,000 km, however, the ferromagnetic mixture gradually loses its properties and must be replaced. The clutch engages smoothly and gently, makes driving easier and reduces driver fatigue, Comparative tests of the NAMI clutch and a normal friction clutch installed in a "Pobeda" car were made, With the friction clutch it was found that torsional moments exceeding the maximum engine torque developed in the power trausmission (40% in excess during a smooth and 85% during a rapid utart). With the powder clutch dynamic loading of the transmission was low and smooth. During a rapid start the torsional moment ex- ceeded the maximum engine torque by only 20% and built up to its Card 21@ Powder electromagnetic... S/113/60/000/002/009/009 D207/D306 maximum over a period of 1 second compared to 0.18 second in the case of the friction clutch. There are 7 figures, I table and 6 references: 4 Soviet-bloc and 2 non-Sov- iet-bloc. The references to the English- language publications read as follows: "Autocar", No. 3076, 12/Xl 1954, pp 778- 780; No 3245 28/11, 1958, p 303; "Auto- cartf , No 322@, 111X, 1957, p 535. Fig. 5. The NMI clutch: I - magnetic con- ductors; 2 - operating gaps; 3 - excita- tion winding;,.4 - labyrinthal ring packing; 5 - driven element; 6 - current-carrying assembly (rings, brushes); 7 - primary gear-box shaft. PHc. 5 Cuenizeime HAMM WArMHTOffDO6OAw: 2 - qsO04"e aajoPw; 3 o6m t, TK3 an3eymat"wo; 4 - i1a,511pKicy"Oe Kq:,*U(I?9Ue YnAuZe"r. 5 - SCIXOMMA *.newmm. 4 IOK.n.a@:Jjj LjreyCY"Re-fW (KO11MIA. UICT- 7 6 DaA M.SX, .. n@PeAa4 Card 3/3 SM&NOVICA, Tu.G.,L-and.tekhn.a&uk; HOSKALIV, V.-U., -UJIMV, 1.8.,kand.tekhn. naak. Determining torsional vibrations in the transmission of the GAZ-51 motortruck. Ayt.prom. no.l):10-12 0 160. (141RA 13-11) 1. Gosu(taretvannyy soyuznyy ordena Tru4ovogo Kraenogo Znament nauohno-Issledovatel'skiy aytomobillny- I avtomotornyv institut. Notortrucks-Transmission davices-Vibration) HDSKALRV, V.N. Designing a torsional vibration damper. Ot.pron. 28 nc.!.:lr,20 Ap 162. (KRA 15t4) 1. Gosudaratvennyy scyuznyy ordena Trudovogo Krasnogo Zn9meni nauchno-lasladovatellskiy aytomobillniy i avtomotornyy Institut. (Damping (Mischanics)) ,%')SKALI,,'V, MR)GE114, I.V.; VASILITFV, B.D. iroot action tinder foundation during the conntr-,icti@r of Is- ir4,,s. Oen.. funLi meldi.0-run. no. 6:20-22 1151). (MIL, P: @, ) (Youndationa) (Yrozen ground) AOSKAIXV, V.S., inzh.: FNI1001M, I.Y., inzh. Provont soll froozing, in foundation bode of Imildingp. Rech. transp. 18 nn.6:41-45 Je 159. (AIRA 12-9) (Soil froozing) (youndations) --- - -- - , .4. ''. , -, -1, 1 -1, r .Z". , a@j,)P-A LI- @ I i . , . I -t-, --" ,r'. " .'Lj3U, Leninorad 't The Development of Equipment for Tnvestigating Miole(-.a-lar wiA Crystal Structures by Nuclear Resonance" . report presented at the Ail-Union Conference on Statistical R@ io Physics, Gor'kiy, 13-18 October L958. (Izv. vyssh uchev zaved-hadiotek-h., vol. 2, No. 1, pp 121-1.?7) "UMPLETE card under SIFOROV, V. I. ) AUTHOB 3; Aleksandrov, N.M., Mouia.7ev, V,V SOv/ @ 4 8 - TITLE: Radivfrequen:,,X Sper;tz--@Frapn for the 4janti.tat)ve Investigation ')f the Limes of Nu,::1,3-ar Msenet;-, ResonanGa in Crystals (Hadiachastct- nyy spektrograf (11-ya koli-heatvonnngo Issledovaritya konturov linly yaderilogo magnitnogn rozonanit, v kriataliakh. PERIODICAL: Vestni.k Le,-iingr.91s.(-)g,) ,iYiJve:r9i',ets, Seriyu fiziki i khimil 19 Nr 3, pj, 14 -- 20 (USSR ABSTRACTs The exparimental ..nvnstigati.-.n of the nuclear magnetic resonanae limett in ^.rystals 4-:* Lmpeded by the fazit that these 11nea exhibit a conw-derable wl.dth and a low intensity. The spectrograph do- soribed,@nmthespresqr.t,pa@er 'its block scheme is represented in figure ake possib 0 he @nvestigation of the line contours, The electromagnet yoke , ,I Fig 2) is made of soft magnet steel ST-7. After the reguistion tho relativ,w nomogene.1ty of the magnet@@,: fip-,@l 076/cm.A was I ', By th a ffi,,t the 4eviaq together with corre 13 pond ing, electronic equiprifint b,3:-r--mes unJversal. It can be used In the in- veatigatlo-) @f @hcrni(.tilly itu,j-1 Ji.oplanemento in liquldm and cry.,,- tal iamples of largs voiumfa., Tho receiver of a euporlieterodyne Card 1/3 type (Fig 3) gua-z-Fintes-zi thwi ol,sarvation of the frequency shift as Radiofrequency 3pectrograph fur the i@aantitjtlve In- 30'7/54-;8 vestigation of the Lines cj-" N,-,--Iaa: Vagn-@ri-. Resanan-,a Jn Crystais well aa of tha T-A-1; 1 the am;@Iitude when t1ir. wagnetic I ak nD resonance inp, pnsaae th-rougn. lzt the former caes, t ing - aount of the geparatuT oonditi@,ns, a good qualitative represent- ation of the refiiC Is J 3 guarenveed. In the case of a carrier -1 frequency of !.I - 10' th,@ circuit can fix the frequency shift of M1 cycles@ T,a genera-or i_q built according to a diagram due to Pauild (Ref 7) with some modif;.cstions (Fig 4). The diagram of the frequency rietector rFig 5.@ ie analogous to the diagram from re- ference 8- By meana of the descrJbed device a deduction of the dispersion sigpal in a gypsum mono-crystal (CaSO 4' 2H 201) was ob- tained .Fig 6), The :urvo Axhibitb a double fine structure wh;ch is not. at variance w' *Ji *,he data presented in tine well-known F'aper by Fake (Peyk, (Rof @ Besideq Preliminary data on line oomtour3 of SOMC, ttlh+ jriti, now have not been examined were ob- tained. The auth.e:rs qxprnea their gratitude 1,0 FJ,Skripov,Docent, Head of the Laboratoriya magn! Lnoy radiospektrookopii (Laboratory of Magn-itin Radi.._-apti,!t-oscopy,@ frir valuable sugget3tions. rhere ire Card 2/3 6 figures and 9 raferen-,os, 2 of which are Soviet,