SCIENTIFIC ABSTRACT ILIN, OLEG PAVLOVICH - ILIN, R.N.

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SCIENTIFIC ABSTRACT
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ANKIMIYUK, Vyacheslay Leont1yev1ch;-LL1j-Nj-P~e1,9. Favlovichl TETERINA, L.Nap reds !i- -1. .", I ~ ~ ,, [Automatic control of electric drives] Avtomaticheakoe upravlenis elektroprivodami. Minak, Vyashaia shkolap 1965. 469 p. (MIRA 19M k .. . souRcC coaSt UR/0143/66/000/005/0040/0045 AUTHOR: AnIdilmyukq Ve Le (Docent; Candidate of Technical Sciences).*-Iltint Oo Pe (Docent; date of Tbchnical Sciences); Sheyna, G. P. (Engineer) ORGt Belorussian Polytechnic institute (Belorusskiy politekhnichoskiy Institut) TITLE: Selection of motors,for electric drives with frequency control at constant power SOURCE: IVUZ. Energetilca, no. 5, 1966, 40-45 TOPIC TAGS: electric motorg frequency control ABSTRACT:-A-method in sxial~zid tor" seleoting i'motor'for- a.systoin cif froti" dontrolled drive in the POwconst, operating regime. The method is based on 'the condition of produotion-of &'minimal size motor, in consideration of the "problem of determining the frequencies at whioh the fixed range of control ,and power can be provided with series produced asynchronous motors, The authors call for development of technical conditions or state standards with rqspoot to permissible values of voltage, ourront and.rotation rate Of Aeries produced aBynohronous motors used in frequenoy controllod_olootrical drive---., jrjst*;w.--An..oxsj-vjo., Of Orig. art. has% 19 formulas. ,rJNS: 37,0611 SUB CODE: 09 / SUBM DATEs 1711ay65 / ORIG REP: 006 Mxh3 140 0 WIN, P., 1212h0 We indroduce advanced methods of construction. Sill. brud. 12 I I no .3.2,15-16 D 161. 1 (MIRA ~5:2) (Ukraine--Construction industry)(Precast concrete construction) MAGIDO B., insh.; IL'Ifi, P.p insh. - Transportation of long elements. Na stroi. Roo. 4 no.5118 * . 163. (KM& 16s0) (Precast conorste-Transportation) (Truck trailers) J Sons characteristics and problems of the development of patrols= refining. Beft. khoz, 40 no.12:13-18 D 162. (MMA 16:7) tpetrolewa-~ fining) J'L'ill, F.A. y, hiAl r);, For the putrolour, I t, faii.c. i tokho tcjij--,. A rasr,~,l ',? nc,.7;1--- i* 'i 'i OILRA 17: 12) I f I , - T - I - - ---- - - --- - _-- ----- - -- -- - -- ---- -- --- -- - - -- - -- ----- ZAPOLISKIT, N.Y. IIPK-2 and PK-2 wb electric caterpillar crane.* P.I.Illin, 5.1h.Mwi- fete. Reviewed by K.T.Napollskii. forf.prous 31 no* 0 (XLU 7sll) (Crane@, derricks, sta.) (Illin, P.I.) (Kheifets, 3.1h.) Type of folds In the coal deposits of the Southern Ural Basin. 8w. geol. A0.33330-133 * 160* (XIRA 1):11) (Southern Ural Basin-Folds (GeoloCr)) xuLESHOV,, Alokoey Vasillyevich; nlut Pavel, Ivanovich; PEMV,, V.P.9 red.; ZKMIKOVAO O.S. 0 t (Safety measures. in the peat Industry) Tokbnlka basopasnosti v tor- fisnoi promoblemosti. Xookvag Ooso onarge isd-vol 1960# 166 Po (MIM 14t6) (Peat industry-Safety measures) T KMM' N.G.-- DIKASH10 --A-OD -- - --- W !N -P L-- I ON N For'sissible,pitch of cable sinding ,a the drun of a hoistlng mohin*. Ugoll 29:no.Ils27-31,154. (KM 7:11) 1. Otdol Glaynogo konstruktora Nova,-Xramtorskogo washinostroltellno- go SAToda In, stalina. (mine hoistim) w w NISIMY, Nikolay likoloyevich; XUZHILI, Kakelm Goorglyevich; DIKASHKO, AlsksahAr Dominikowlah; ILOIN, Petr Uftch; rARPTSM,N958, re- daktor; ZAPHIMA,K.A., kNORMFO, 2IIuXxjL,Ts.I,, tekhnicheakiy redaktor [Kine hoisting machinery (mechanical part); constraction atlas] ShW&tnys pod"emaye usshiny (mekhanicheskaia. chast); atlas kom- struktaii. Kookwa. Ugletakhtsdat, 1955. 114 p. (MW 9:1) (Mine hoisting) KUZHE:Ll, M.G.; ILlIk, P.L. Mine hoisting machinerys SboreNovo-KrAm,naahinostroi. zav. no.1:17- 51 159o (MIM 16 12) SNEGOVSKIY, F.P.j, kand.takhnonauk; POLIDOROV, A.V.0, lnzh,,A_ILIIN P.L.p insh.; VILBSKIN7 D.N*j insh. .,T, Industrial testing of an ore-orushing ball mill with hydrostatic b6aringeo Vost.mashinostr* 45 no.1041-42 0 165. (MIRA l8ell) ILIINt P.P.; SELIVANOV9 S.A. Improve the quality of reinforced concrete ties. Putt i put.khos. 7 no.7t2l-22 163. (min 16,1o) 1. Nachallnik putoobeledovatellskoy stantaii, Kiyev (for Illin). 2. Starshiy inzh. putepbsledovatellskoy stantaii, Kiyev (for Selivanov). A V It w A -A V 114 40 Osr-01111.1t FOO(I 0 0 19A 7=b 1 n4 00 sot . ter a fwki of ull". Wa, by 4m Wa l electramomic wow" twtwwa ctxmkug plate., of's 00 a ll 600 00 00 *90 of a 000 Goo goo see as !we* too 0- 4. , u 1649--lo lit mA * p W Of d N . , , J 0 0 so 0000 90GDANOVICH, N.M.; MOCH&LIN# V.S.; IL111, P.A.: MOT,X.S., rsdaktor; MEMONO' M.M.j takhAichesk 1 &IT Blements of the theory of navigational gyroscopic Instruments] I lementy toorii navigatsionnykh giroskopicheskikh priborov. Uningrad, lid-vo *Norskoi transport,' 1956. 270 p. (MM 9:8) (Gyroscope) 41rivo WIN, P. A. (Candidate of Technical Sciences) (Litmo) wThe creation of now small-size designs of gyroscopic registers of ship rolling-, paper presented at the Second SoienWiC and TOCIMiC41 Intervus Conference on Problems of Contemporary Qyroscoprj* Te. F, Otyagint Secretary of the Organization Committeej Leningrad,, Izvestiya UchebpVkh Zavedenity., Priborostroyeniye., No. 5t Sep/Oct 19581 pp 161-163 The Second Intems Conference an Problems of Contemporary 0yroscopy Techn*ue, convoked by decision of the Ministry of Education USSR, took place In the Leningrad Institute of Precision Mechanics and Optics from 24 to 27 November 1958. 13, AUTHORS: TITLE: PERIODICIL: 83465 S/146/60/003/004/005/010 B004 B056 M. K., 111in, P. A. A Gyrocompass9for La"tituds Determination With Indirect Correotion Isvestiya, vysehikh uchobnykh zavedeniy. Priborostroyeniyog 1960t Vol- 3, No- 49 pp. 43-47 TEXT: By controlling a gyroscope with moments applied to its suspension pin it is possible to produce an apparatus which simultaneously indicates the true meridlian-direction and latitude. On an astatic gyroscope in Cardanic.ouspension (Fig. 1) a gyromotor acts as sensitive element, upon whose.vertical axis correcting moments sot by means of a moment trans ducer. These moments are proportional to the angular velocity & of th; deviation of the main axis of the gyrosoope from the meridian planei V~ - k&. This correcting moment is calculated by means of a computer ob- taining all data necessary for determining the value M5 . By means of the geographically orientated coordinate system 05 If , which to connected with Card 1/2 83465 A Gyrocompass for Latitude Determination With S/146J60/003/004/005/010 Indirect Correction B004/BO56 the earth, and the coordinate system Oxyz (fig. 2) the authors derive the equations of notion of the main axis of the gyroscopes This paper was 'recommended by thstafedra girookopichookikh i niavigatsionnykh priborov (Chair of Gyroscopic and Navigation inettuments). There are 2 figures. ASSOCIATION: Leningradskiy institut toohnoy mekhaniki i optiki (Leningrad Institute of Precision Mechanics and Optics) SUBMITTED: February 27, 1960 Card 2/2 1. 06 V 811?3115 1/000/10 1OM/t22- a 25-Al WOU A004/A101 AWVAt Vin; ?.A. . . .... . .. ........ New.arooompass for the mariti" transportation fleet P=DICALt Referatiw4y zhurnal, Hashinostroyeniye, no. 16, 1961, 21-22, ab- straot,16DI52 (V sb, "I- .V& N*zhvux,,naucbno-tekhn. konfersh Iya VO probl. novr*m. girpokopii". Loningr4d, 1960,'3 - 9) IMI In accordance Vith the planned inslamotions of the XX Congress of the XM on the extension of moritUm transpo~-tation and the *quipping of the transportation and commercial fleet with up-to.Aat* navigation instruments, the Ianingradakiy institut toobnoy makhaniki I optiki (Leningrad Institute of Preci- Sion Mechanics and Optkon) to Other With the- Toontrallrqynauoh~o:ioslodovaiol'- skly Institut mors)cogo flota TeentrAl Scientific Research Institute of 'the Mari- time Pleat) has developed a new gyrooompass design. The peculiar feature of the sensitive element of the gymoompass consists in the fact thit the internal sus- pensioh axis in located vertically, while the external axis is placed horizontal- lyo,so, that, consequently, during rolling'the,vortical ring does not imediately affeat!the gyrosoope as regards its vertical axis and so-called compensation Card 1/2 27022 S11 ~rA I 1/00O/b16ttO9/b22 Now gyrqoompass so$ AOO 01 'weights.0an be dispensed with which are bala-np'ing the moments of inertia of the vertical ring relative to both axes.- Owing to the mentioned arrangement on the sisponalcm axon it in possible to effeota damping of the free gyroscopo oncilla- tions by "Ights independent of the main pendulum, to do away with tne "fooe bearings of the mercury vessels and to adjust the damping factor in operation without stopping the gyroscope. The mercury vessels n**d.-not be suspended on se- parate supports. They are fixed immediately to the vertical ring. The sensitive element. has a torsional suspension of the vertical axis whiah is centered by high- sinsitivity ball bearings, the horizontal axis resting on balls. The pilot assem- bly conplets of the following unitst 1) ~he gyrocompass proporl 2) food unit of the AMr-i 'oG (Amo-ioB) ty0 (serial output)j , .3, AM-10 (R(M-10) revolUtion, controller (serial output); 4) corrector of'speed and constructional errors of the gyroscope; 5) 15H distribution box (serial output); 6) 2314 course recorder (serial output); 7) column-type bearing repeater (serial); 8) bracket-type re- poster (serial). Two pilot models of the gyrocompass were tested on ships. 0. Flidlider [Abstractor's notot Complete tranelition] Card 42' %. ILIINJ P.A.- Small gyroscopic device for recording the rolling of(a ship.- . . Izv.vya.ucheb.zav.; prib. 3 no,3166-73 160, MIRA w *0 , 1. Leningradskiy institut toohnoy mekhaniki i optiki. Rakomendovana Orgkomitatom vtoroy nauchno-tekbnioheskoy meshvuzovskoy konferentaii po problemam sovremennoy giroakopii. (Gyroscope) (Stability of ships) PL40 I BOOK EXPWIrATION SM15615 Bogdanovichp Ifthail Mitrofanovich.. and Petr Alekseyevich 111in Giroskopicbeskiya pribory i ustroystva; osnovy teorii (Gyroscopic Inoty =-anto and Devicesj Pundandhtelar of the Theory) Leningradp Sudprowoz,, 1961, 359 P. Errata slip inserted, 6..goo copies printed. Revievers: A, N, DokachsyevF Candidate of Technical Sciences., A. Yu. Ish"in kly., Acadexicianjo D, R..Xerk:Lnp Doctor of Technical Sciences,, Ia. G. Ostronakhov., Engineer,, Scientific Ed,#., N. V. Butenin; Ed.: Ye. L Shaurak; Tech* Zd,t R, X,~ Taal, PMPOSEt This book is intended for students of instrwant building in schools of higher education and in naritim schools. It my also be useful to technical peraDwel eng4od in desliml and manufacturing gyroseopic instruments and devices. COVERACM: The look presents problem of the theory and principles of operation of various gyroscopic instruments an& devices, Stress is laid on instrunents vh1ch are videly used in practice, Rovever., some nev circuits Aich as yet Card 1/10 .Gyroscopic Instr nt (Cont.) 807/5615 ha no widespread application., such as gyroscopic latitude indicators and Zlzry gyroso are discussed. The authors Unank N. V. Butner., Professorp : Doctor of Physics and Mathematics,, A. Yu. IshUnskiy., Professorj, Academdeianp D,, R. Herkin,, Doctor of Physics and Natheniatics, A. N. Dokuchayevj, Docentj, Candidate of Technical Sciences.. Ya. 0. Ostromukhov.. Engineeri and V. A. Pavlov., P. 1. Siydov and S. S. Rivkin., Professors., Doctors of Technical Sciences, for their advice. There are 49 references: 45 Soviet., 2 English,, and 2 German. TA331Z OF CONEWSs Foreword .PART 1, ME" PROMM OF M THEM OF THE GYROSCOPE Ch. I. The Gyroscope and Its Dynamic Characteristics 1, Definition of the concept of "gyroscope" and its dynamic characteriftics, 5 2. Tbeorem, of mwWnts 7 3. Euler's dynamic equatione.as applied to the gyroscope 9 Ch. Ir. Basic Properties of a Gyroscope, 1. Stability of the main axis of a free gyroscope 13 Card 2/10 t3 / AjT pEo ILI IV 01 Sal a O~ OV& eaOul vooT O~ Al 0 '0061 a a Tee eaet . 1096 &e bu 01 voo ~ -00,13e .10,t 5;~ a a ,XLe tUe Tell ;rli.'bT TyLe 600? 066 ' '01a' 0 e& ,.a 10 'Go Tjp 0,913. aesAls tea 'bl It CIA , t-ce~ 9$~-S- e0t -real? 0-me-n-t tTOle ell" J~l TetVo J043T~ ele'a to Veo tyLe 006 .,Ae % U~Jll 10~A6 to el t IL ST tue 060t e Tpe%06- 06 Sea, 6TOS',X161~011e`aay" a t iA Te VA a 1~.OJLIS I J?eTV 8j:a V 0,11 Ts*~, t~.Olo 11 1% ele tTee 0, tae tt~e V, -4VOT, Leo~ ,-~010 t 0 it 0 0061 00.0v0 ~Jjj3. im t ~A ~06 tue Se 3,eLcl O-ri's 000 JeO't je'aet' OOT& i ~TA . tUe V~ot a., a so O-V 0 tua 60 0~.60 . I t act ,,Te 0 so 0~ to - a Ot tA a. ".01N I of ,,Oe O'DO4 29644 B/146/61/004/004/008/015 The effect of base vibration D201/D306 self-oscillations in the absenoe'of vibrations. The approximate so- lution of the differential equationf, Then becomes VC, sin at+.!"-"J!x O-Al +V Ca dos #t+ ae 2P r IV + J MIPVCOS(Pt-GL_ W), + 4pI hS _.7 fr be'seen om this thdt'~ dam ifig of the sensing*element is, p n ded i the. gyroj the-o6dillations given by the terms in-brack n eta will be damped.' After'-'the.decay,of self oscillations' the-z-axis ....,.oscillates only -wiih-'forced,oscillationsi The amplitude of moment; -..m~occuring-.-during the,vibrationo,.of the-base and on angle-0, and on the -ratio of frequencies p and,po.To evaluate the magnitude of for- ced ~Osbillatioins which -introduce the -error into -the indication of the gyro anumerical exAmple~,is solved for such a gyro with air ~.cizshions. The.-numerioal.results'ahow that the'base vibration provi-. Gird~k/3 29644 S/146/61/004/064/008./015 The effect of base vibrations D201/D306 ded its frequency and amplitude are constantt above a few C/sq does not affect the indications of a gyro with two degrees of freedomf since its period T is seldom less than 30 sece It is stated that if the vibrations of the base have varying frequency and amplitude# experiments show that the gyroscope cannot be used any more to de- termine the meridian plane* This article was recommended by the Ka- fedra giroskopicheskikh i navigatsionnykh priborov (Department of Gyroscopic and Navigational Instruments). There are 3 figures and 1 Soviet-bloe reference. ASSOCIATIONt Leningradekiy institut tochnoy mekhaniki I optiki (Le- ningrad Institute of Precision Mechanics and Optics) SUBMITTEDs December '/,, 1961 Card 3/3 A LATITUDE GYrIOCOMPASS dl- nd A I'lin !z v DY 1 OF C 'forr.1 NVI.I. Q.- 0 ta 11-1 e dc, el,-4-jert. The, Z~ la o 1 L U_ _, _ c;c,*,,,:),,?:ny 4 _- L' To obtain a tc) ob.-Lain a verticzAL ~O 0 nrr ;ty of th" C'a anr_ L'n the Vt?- M~yl r P -ision. r%lechanics and Optics. 1 6' .e LC-rl r- f7:Z', PROKOPCHUK, B.I.; IZRAILEV, L.M.; num. P.A. IZONOV, B.N.; SUSOV, X.V.;,' KOS7RYUKOVp-M.S. Diamond potential of1he Lena Valley; new diamond-bearing area in the northeastern part of the Siberian Platform. Trudy IAFAN AN SSSR Ser, geol. no.90.15-122, 163. (MM l6tl2)., WIN, P.V, novator-aytoovarshchik - I - - ~.. - Autg4wtic-weldln _C.-c! iitor and Inwvator. Hashinostrottell no.ls - , Ps ' , - I (NIA 22tl) I 1. - (Ille~trlc woldlvg) JULIA- P.T., Inshener. Cape for chemi-cal water purification filters. Inergetik 5 so.8:20 Ag '57. (mm 104L0) (Water-Purif lost Ion) AUTHORt Illin, P.V., Zngineer 91-58-8--4/34 TITLE: The 7iuallit'lly"I'101of Chemical Water Purifying Filter Caps (0 kachestve kolpachkov fil'trov kbimvodoochistok) PMODICALi Energetik# 1958t Nr 8, pp 11 (USSR) ABSTRACT: The author discusses the various types of filter caps pro- duced, criticizes their shoddy quality and defectiveness, attacks the indiscriminate use of unsuitable types in the wrong equipmentf quotes an example of the unnatural wear of three filters in a TZT90 and calls for the quality to be improved. There is 1 photo. 1. Water--Purification 2. Filters--Applications Card 1/1 Illino R. ___ . .- - .. . 712mlog with polmisind lUht filters, Sov, f0to 17 no.3:53-55,Nr 157. (Pbotograyby-Ligbt filters) NOW 1096) .1 ILI INP R. Bias lightening and darkening in full exposure. Sov, foto 123 no.508-39 W 163. (MMA 16 t 10) R., kand. iskusebm eniyat kinooperator; DUBSOW, Ta.0 tekhn, [Speoial lighting in television] Spetsiallnoe oeveshchenis v te2evi- denii. Moskva., Goo. kom-t po radiovesbabaniiu i tolovideniiu., 1961. 85 'PiTelevinion) (Lighting) (MIM 14:10) BLTUSICIN, To. M., inzh.; IL'IN# R.A. lush.; PAMUTOV, T.P., lnzh. Operation of oq#piwnt subjected to boiler inspection without accidents. Bezop. truda v prom. 3 no.6t2g-30 Je 159. leDDIgepruduenekly savod kraelteley. (Industrial wafety) SOV/124-58-7-7415 D Translation from: Referativnyy zhurnal, Mekhanika, 1958, Nr 7, p 12 (USSR) AUTHOR: Win, R.F. TITLE- On the Dynamics of the Ascending and Descending Sections of a ,Hoisting Cable (K dinamike opuskayushcheysya i podyma- yushcheysya vetvey pod'Iyemnogo kanata~ ABSTRACT: Bibliographic entry on the author's dissertation for the de- gree of Candidate of Physical and Mathematical Sciences, pre- sented to the In-t matem. AN UkrSSR (Institute of Mathematics, Academy of Sciences, Ukrainian SSR), Kiyev, 1957 ASSOCIATION: In-t matem. AN UkrSSR (Institute of Mathematics. Academy of Sciences, Ukrainian SSR), Kiyev 1. Hoists--Mathematical analysis 2. Cables--Porformance Card 1/1 A UTHOR t TITLEs PERIODICALt kBSTRkCTi C ard 1/2 ua#_R.41r~ SOV/21-58-2-8/209 On the Mutual Influence of Mine Ro a Branches (0 vz&Laov- liyanii vetvey pod"yUmnogo kanata3 Dopovidi Akadexii nauk Ukrainetkoi RSR# 1958f Nr 21 PP 147-152 (USSR) Making use of the Lagrange method the author presents a sy- stem of differential equations for hoisting equipment with a friction pulley treating the mine rope as a visco-slantic threado Under the assumption that kinetics of the motion proceeds according to a trapezoidal tachogram, the author gives an approximate solution of this system by the asymp- totio method* The solution makes it possible to investigate dynamic stresses in the mine ropes for the shallow depths of hoisting ( up to 300 m ) taking into account their in- On the Mutual InfIluenoo of Mine Rope Branches SOY/21-58-2-8/28 perfect elasticity, A criterion for dying out of dynamic stresses in the mine ropes has been found. There axot 1 schematic diagram, 4 graphs and 7 Soviet references. ASSOCIATION Dusprop*trovskiy goeudaretyennyy univernitat (Dnepropetrovsk State hiversity) PRESENTEDs By Member of the AS UkrSSR, G.K. Savin SUBMITTEDt April 229 1957 NOTEs Russian title and Russian names of individuals and insti- tutions appearing in this article have been used in the transliteration ,c-- ILOIN. ILY. (Illin, R.Pj (Aispropetrovsk) Vj~lcs of mine bolate with a driving rope pd24Wo P97kle mkb. 6 no.2tl86-291 160. (UM 23SO) le Vaspropetroveldy CosudantysaW mlTerallots (Mine belstinc) ILIIN, R.F. [Ilfin, R.11.1 Onepropetrovsk), Slightly nonlinear three-dImensional mrmmant of elastic rods, PrYk1. mekh. 10 no.4t450-453 164. (MIRA 17t10) 1. Dnepropetrovskiy sellskokhozyaystvennyy institut. n, 3N1 11. 1 AFROSIMVp V. N. I and FEDORM01 n. V. ------------ "Ionization of Molecular Hydrogen by Protons," paper presented by Fedorenko at Conf. on Physics of Electronic & Atomic Collisift, flew York University, 27-28 Jan 1958. B - 3,102,929 4-4(7) 1UTHORSt Afrosimov, V.V.t Illint R.N., SOV/57-25-10-2V40 Fedorenko, II.Vi TITLE: Ionization of Argon by Hydrogen Ions (Ionizatsiya argona ionami vodoroda) PERIODICALs Zhurnal tekhnicheskoy fiziki,V61 2q..Nr 10, pp 2266-2274.(USSR) ABSTRACT: This work was intended to furnish information on the charge composition of the secondary ions and on the total cross sectioZ4 which can be ascribed to the production of free electrons and of secondary ions in the collision of hydrogen ions with the argon atoms. Argon was used as a gas target for the reason that it yields the most detailed data on the ionization by electrons and ions. The experimental method has already been described accurate- ly in the papers cited by references 1 and 2. The experimental set-up as a whole has been described in the paper cited by refer- ence 9. In this paper only a short description of the experimental conditions is included. The charge composition of the secondary + inns of afgon which are produced by a single collision of the R H2' and R3 ions with the argon atoms was the object of study in Card 1/3 this work. The energy interval of the primary ions extended from Ionization of Argon by Hydrogen Ions SOV/57-28-10-27/40 5 - 180 keV. The following quantities were determinedt The total cross section of electron capture by hydrogen ions (6'0) and the total cross section of free electron production (a) and of Ar+, Ar 21+ , Ar3+0 and Ar4+ secondary ion production, which are denoted by a'11 and ' , respeotively. It was found that 6, 0 61020 e03f 604 0 in all cases decreases, continuously with an increase in the velo- city of the primary ions,.whereas the curveslgv)exhibit a maximum. This maximum is located near velocities which are about the value e2/h (according'to Bohr (Bor) the velocity of the electron in the hydrogen atom equals 2,2.108cm/sec). The curves 602(v)' 6'03(v) and 6'04 (v) exhibit a maximum in the same velocity region. The maximum-values of the corresponding cross sections for an elec- tron impact are, according to data provided by W. Bleakney(Blik - ni) (Ref 3) by many times smaller. The cross sections of the pro- Card 2/3 duction of secondary argon ions by ions 11% H+ , and H+ are 2 3 "Ionization of Argon by Hydrogen Ions SOT/57-0-10-27/40 oompared-to those of the production by He + and No+ ions travelling with,the some velocity, the pertaining data.,being provided by reference 2. It appears that the cross sections of the produc- tion of Ar 2+ , Ar 3+ and Ar4+ ions increase with the nuclear charge of the ionizing particles. If the ionizing particles are multi- atomic molooalse the corresponding oross sections increase with the4norease in the-number of the nuclei contained in the primary ion. Professor V.M. Dakellskiy and O.B.,Pirsov discussed the work mith-the,author.'There are 6 figurest' 1-tabl:e, and 14 references, 8 of which are Soviet. SUBMITTED% January 17, 1958 'Card 3/3 AUTHORS: Afrosimov, V. V., Win, R. N.p SOV/56-34-6-5/51 Fedorenko# N. V. TITLE: The Ionization of-Molecular Hydrogen by the Ions H 2 and Ht. (Ionizataiya molekulyarnogo vodoroda ionami H+9 Ht ana Rt 2 3 PERIODICAL: Zhurnal skeparimentalinoy i teoreticheskoy fizikip 1958# Vol 34, Nr 69 PP 1398 - 1405 (USSR) ABSTRACT: This paper investigatis the ionization of hydrogen by the-ions H+, A+ and K and the distribution of the secondary 2 3 ions with respeot to e/m in the energy interval from 5.- 18o keV,, The experimental device and the method of the investigation were described in a previous paper of the authors (Refs 1405). The beam of the primary ions (which is homogeneous with respect to the energy and composition) entered a colliWon chamber. The low pressure (from 1,10-,~ to 105-jo-4 torr) implied the homogeneousness of the collisions of the primary ions with the gas mole- oules. For'the analysis of the secondary ions with respect Card 1/4 to 6/m a magnetic mass spectrometer (with sectors) was The Ionization of Molecular Hydrogen by the Ions SOV/56-34-6-5/51 H4-, H+ and Ht 2 3 Card 2/4 connected with the collision chambe The ion urrents in the analyeat or amounted -to 2.10-T; - 2.10- IT Three diagrams show the total gross sections of the capture of the ions'15+9 H+ and Hr; these cross sections are 2 3 plotted against the velocity of the primary ions. The first diagram gives also the theoretical dependence for thercharge-exchange of protons in atomar hydrogen. The pair e- - K' is not a resonance pair. It seems that-the 2 2 elecriron is captured to an excited level of the molecule H The capture of an electron by the ion H+, Is a o9meplex process as the stable state of the Llecule 3 3 is not,known. This capture probably causes the dissociation of Ht into a'moldcule H and a hydrogen atom. The cross section cr' of the prodhtion of the secondary ions 14 H+_ is the sum of the cross sections of the ordinary charge siohange and of the ionization with the removal of one electron. In the region of the velocities of the primary The Ionization of Molecular Hydrogen by the Ions SOV/56-34-6-5/51 H+ H+ and H+ 2 Y. ions ve, 2Athe cross section of t he ordinary charge ex- change f:rmd the main portion of the arose section Or,+.-But in the region v >62/~the principal part of 0 2 is formed by the cross section of the ionization. In the region V>02/~ the cross aection a H+ is the greater the 2 more nuclei make up the primary ion.'In the same region a + Hi decreases continuously when the velocity of the*primary ions increases, and'it is greater than the corresponding cross section of the electronic impact. The following part of this paper deals with the production of secondary protons. The arose section of this production is smaller than the cross section of the production of the molecular ions E+. The secondary protons are produced mainly by the dissociation of H+ ions. The last part of this paper deals with the pr9ductions of free electrons. The authors thank V.M.Dukeliskiy,'Profeasorg and O.B.Firsov for the Card 3/4 discussion of this paper and for useful critical remarks. 2~=' ~j MUN __- Raw- The Ionizati n of Molecular Hydrogen-by the Ions SOV156-34-6-5151 H+ and 2 2 3 There are 7 figurseq I tableg and 16 referencess 4 of which are-Soviet. ASSOCIATION: Leningradskiy fiziko-tekhniohaskiy institut, Akadefidiumik SSSKLmin- ~m&2Vmk*1-Teohnioal Institute As USSR) .SUBMITTED: January 8j 1958 "Ionization of Inert Gases by Protons." report presented at the 4th Intl Conference on Ionization Phenomena in Gasesp Uppsala., 17-21 August 1959. IL11N,, it. N., Candidate of Phys-Math Sol (dies) -- "Ionization., electron cap- ture, and dissociation in collisions between hydrogen Ions with kilo-olectron-volt energies and atoms and molecules of gases". Leningrad, 1959. 11 pp (Laningmd order of Lenin State U im A. A. Zhdanov., Phys-Teah inst of the Acad Sol M%), 150 coPieO (KL., No 20., 3.959,o 109) 24(5) AUTHORS t J11in, R. N., Afrosimov, V. V., SOY/56-36-1-7/62 Fedorenk_o-t-1f-.V. TITLE: Ionization of Air by H + and H+ -Ions (Ionizatsiya vozdukha 2 ionami H+ i H+) 2 PERIODICAL: Zhurnal ekeperimentallnoy i teoreticheskoy fiziki, 19590 Vol 36, Nr 1, Pp 41-48 (USSR) ABSTRACTs Hitherto, the ionization of air by ions has been investigated mainly in connection with investigations of the energy dependence of the proton range (Ref 1), and ionization cross section was only inaccurately determined (Ref 2). Direct measurements of the ionization cross section in air by protons are not known to the authors. In the present paper collisions between positive hydrogen ions and air molecules are in- vestigated, and the formation of secondary ions by the knocking out of electrons and electron exchange is observed. The total ionization cross section is measured by means of electron re- cording during the passage of an ion beam through air. The simultaneous electron capture of H-ions was already investi- gated by reference 4. The investigation of the componition of Card 1/4 the secondary ions was carried out by means of a mass Ionization of Air by H + and H + -Ions 2 Card 2/4 SOV/56-36-1-7/62 spectrometer. Also the production cross sections for these ions was determined. The measuring method was already des- cribed in references 3 and 5 and is discussed in short. The monochromatic ion beam penetrates into a collision chamber in which air pressure amounts to 1.5 10- 4 torr. It contains a measuring condensers.which, by means of an ion current, permits determination of 6+ and &'_ cross sections. The total capture cross section is 6'10 - 6+ - 6*_, and for the production cross section of secondary ions it holds that 6,A:n* w I G'+ C4A"4 (WA,# - relative Intensity of An+-ions). The total measuring error amounted to about +12 %, in which case +6 % related to pressure- and +6 % to current measure- ments. Spectrum lines were recorded of the following ionst N+ 0+ N+ .0+, N++, 0++, Ar+, and in the residugl gas 2# 2' 9 (after evacuation of the chamber, pressure 5-10- torr) H+' H+, and H20+. A spectrogram of these secondary ions is 2 shown by figure 1. Resultat Total capture cross sectioa of electrons by primary ionst Results are'given by figure 2 (energy dependence of 6110, comparison between measured data with the results of references 4, 7, 6). Ionization of Air by 11 + and H + - Ions SOV/56-36-1-7/62 2 Total ionization cross section 6_: Energy dependence G'_(E is shown by figure 4, the velocity d;pendence by figure 5-*'*' Fo r H+ at 60 keV 9 6' 6. 3. 10-10 cm and f or H~ at 140 ke'V: -01.2.1o-15 OM2 is given. The maximum in an energy O:a 19ge 2 of 50 - 120 keV is given as amounting to (8.6 - 12-5)-l cm From measurement of velocity dependonce It follows thatair- ionization by- rotons and H~-ions taxes place in the velocity range of v< e /~ , where there is no ionization by an electron collision. Production cross section of secondary ionst Figure 6 shows the energy dependence of 6' A-44 in the case of ionization by proto 'ns, figure 7 shows the same-in the case of ionization by 4-ions. The formation of simply charged molecile Ions in nitrogen and oxygen was also investigated, the dependence of 6' o4 on the velocity of primary ions is shown for nitrogen A by figure 8 and for oxygen by figure,9.-.~Further, results of production cross section measurements of single - and double- aharge-atom ions in nitrogen and oxygen are given. The production cross sections V 0++ and 6* have a maximum at V ft 0 - 1.5) e2/%1 6,0++ p-, 1.10-17 CMNI+and 6'NA-+-S 3.10-18009 Card 3/4 and in the case of ionization by H + 6'0++ 219. 10-1 cm2 2 Ionization of Air by H + and H+ -Ions SOV/56-36-1-7/62 2 and & N++ 0-11 2#4.10-17 am? The authors finally thank Profes- sor V. M. Dukel'skiy and also 0. B. Firsov for their advice and discussions. There are 9 figures, 1 table, and 12 referen- ces, 4 of which are Soviet. ASSOCIATIONC' Leningradskiy fizl~ko-tekhnicheskiy institut Akademii nauk SSSR .(Leningrad Physico-Toohnioal Institute of the Academy of Sciences USSR) SUBMITTED: July 29, 1958 Card 4/4 5 (4)''24(0) AUTHORS: TITLE: PERIODICALt ABSTRACT% ,Card 1/3 Fedordnkol N, V,-' Afrosimov, V. Veq sov/56-36-2-6/63 Illing R, X.1,Kaminker, D, M* The,Disoociation of the Molecular H+-Ion in Collisiona ina Gas- 2 (Disaotsiatsiya molekulyarmogo ions, H + pri stolknoveniyakh vgaz 0) 2 Zhurnal eksperimentai#'6y i1eoreticheskoy fizikit 19599 Vol 36,,'Ifr 2p PP 385-392 (USSR) In the..introduction., the following possible dissociation prodesees in inelastic collisions are discusseds + 0 + + H H H H_ + H 2 2 2 + 0 0 + + H H + '11, H H + H, 2 .2 H+ + Ho. H+ H++ 2 2 + 2 al. The publications dealing with this subjectq Fogel' al, Sa"lpoter(Ref 2)p Effat(Ref 3)# Fedorenko(Ref 4)v Damodaran(Ref 5~ and others are discussed.- The Dissociation of the Molecular H+-Ion sov/56-36-2-6/63 in Collisions in a G" 2 The present paper gives a report on-the results obtained by measurements of proton formation cross sections in a energy interval that'is between the intervals investigated by references.4 and 5. Invostigations were carried out in the atomio gases helium and argon as well as in the molecular gases hydrogen and air-*I Measurements were carried out in a mass- spebtromotrical device such as is described'by references 8 and 9. The collision chamber and the analyzer used Is shown In form of A sohematical drawing (Fig 1) and is descAbed. For the invebtigation otecattering a similar method was used as in refeiences 11 and 12. Measurements were carried out for R+ ion energies (T) between 5 and 180 kev. The formation cross 2r sections for protons and R--ions were investigated; results are shown by diagrams (Pigs 2-5)o For hydrogen and helium the course 6 +(T) shows two maxima# a broad one in the range of 100 - 160 kev, and a smaller one at about 15 kev (Pigs 2. 4). For argon and air the curve at first takes a curved, and from about 40 kv onwardeq a nearly linearly rising course (Pigs 3, 5). Card 2/7 The cross section of the formation of negative ions was measured The,Dissociation of the Molecular H + Ion soy/56-36-2-6/63 in dpllisions In a G" 2- 0. 1.6 -18 2 nly in Argon for 12 kev .10 cm ; With an energy incre4sqlof up to 180kevv, showed a monotonously steep increase. The' authors furthe.r.ifavestitated the angular diatribution of H+ ions with a primary energy of.24 kev scattered 2- .. in. argon without a change of e/mq as well as the diitrittktion'ofthe H+ an& H- ions formed as a result of dissociations, Figure 6 shows-.the course-followed by thd angular distribution f (e) in collisio .nchambers with 5.10 -6 torr and 1-5.10-4torr(Ar)o The authors arrive at the conclusion that'vith a decrease of the distance of closest approach of the nuclei of the colliding atomic partiolesp the relative piobability of scattering with dissociation increases. The authors finally thank O.B. Firsov and V.-M.. Dukellskiy for di cussions. TL-ere are 6 figures and 20 refVrences, 13 of which :re Soviet. ASSOCIATIONs Leningradskiy fisiko-tekhnloheskiy inatitut Akademii nauk SSSR (Leningrad Physico-Teohnioal Institute of the Academy of Soienoesy 'USSR) SUMITTEDs 'July 290 1958 Card 3/3 I *IN Roman Nikolm L Vovlehj~-71071S p Ye.,A* 9 kand,takhn.vauk p re4 1 BOGATOVA I V.S.p red.; GWIMAp,V.Aet tekbnrede (Pbotograpbr -vith mtural 3.igbt) Yotografirovanis pri oateotvom= omohWwmii, Pod A lvgloaq, Moskyap Gooolzd-vo *Iakuastvogu .r"' " lot 0' 1960a 71 p. iUus (Bib2 eks fotqUub:iteliag no.19) (KMk 3,4:6) S/057/60/030/06/17/023 81596 (a 0 0 B012/tO64 AVTHORS: Afrosinov, V. V'j 11118P R. N-11 Solov'Yov, Ye. S, TITLE: Cuture of Electrons by Protoni in Rare Gases PERIODICAL: Zhurnal tekhnichookoy fizikip 1960, Vol- 30, No. 6, pp. 705-710 TEXT: This paper gives the results of the measurement of the full capture cross section in the capture of one electron by protons with an energy of 10 - 180 kov in go, Net Xro and Xe and of the capture cross section in the capture of two electrons In Ar. Parthermore, the elastic and inelastic proton scattering was investigated, which is oormooted with the transitions H + o H0 and H+ 1 short description of the measuring method is given. For measuring the full capture cross section the condenser method was applied that had been described in the previous paper (Rot. 6) by the authoxv.The diagrams of Tables I - 4 show the curves obtained for the relationship between the energy T and the full capture cross te Card 1/4 Capture of Electrons by Protons in Rare Gases 3/057J60/030/06/17/023 81596 section in the capture of one electron by one proton in Rep No, Xr, or Xse Table 5 shows the relationship between the velocity and the fall cap- ture cross section in the capture of two electrons by one proton in argon, The analysis of these data shows that the full cross section In the cap- ture of two electrons decreases at T > 100 kov with the increase in volooi- ty-of about v-9. i.e.9 it decreases much mor0 rapidly than the full cross section in the capture of one electron (about v-2 in this range). Table 6 shows the angular distributions of the protons of the primary beam at the residual and working pressure in the chamberg as well as the angular distributions of tho neutral atoms HO and the negative ions H- which were formed during the capture of one or two electrons by the proton The slight extension of the angular distribution of the protons when the chamber is filled with gas (curve 2) proves that the charge is not affected by the scattering of the protons. On the basis of the data obtained it is shown that the capture of two electrons induces a relatively closer approach of the colliding particles than does the capture of one electron. Card 2/4 ~4 t CapIture of Electrons by Protons in 8/057J60/030/06/17/023 81596 Rare Oases B012/BO64 In previous papers (Refs. 80 9) issued by the authors' laboratory it was stated that the relative prob"ity of the inelastic processes in- creases while the distance between the nuclei of the colliding particles deoreases. The results of thepresent paper show that this conclusion can also be applied to the processes in the capture of the electrons and that this seems to be a general law in inelastic atom collisions. The paper (Refs 5)-by Ya. Us Fogel', R. V. Mitin, V. F. Kozlov, N. D. Romashko, and the paper (Refs 11) by N. V. Pe4orenko and T. A. Belyayev are mentioned. Professor ff. V. Fedorenko and Professor V. Us Duksl#ikiy showed an active interest iv the present paper. There are 6 figures and 16 references: 11 Soviet and 5 English, ASSOCIATION: Fiziko-tekhnicheskiy Inatitut AN SSSR, Leningrad (Institute-of-Physice and Technology of the AS USSR9 Leningrad) Card 3/4 Capture Of Elootrons by Protons In ,Rare Gases I SUBMITTED: JanuarY 309 1960 3/057 60/030/06/17/023 81596 B012YBo64 w .Ctcx %nTft .4--wet-C 14 P-Wr4s A'T IZ -Za pta As tcl%-oj -~xrtn 4nv jos A -n-v=z -5644 zprm*lvf. vw~- -5el L it --Co-lg it *I 4uru- St 1 -11 A a&ti--a am ft;Acrrox #-wn airw tom. io Awtaqw I a *2 W-0 %-r-mr4. 2 8 L A Ails,--s a r4 IM-a-M.'a 0 A -j rrou auv%--rd wta cy -wrA -rirtns-a vv 7 0 'IUUIOrPQ 0 0 r'17;-4 A 7 r it Z-5--07M D s -0 T%O=VC P=V OXY =4:V.7 pta to. I C x-M-V. -A J A, -P e-,,4 =nL!Tr%t*Acm mam a tv. a r .0 .02-q"= 0 It *q M-t= SWO ACTTV;F 0 WT Dl4Q'4*fT4 a9" I ZO MTi-'nP*AM. A I?"* &VON J A '"-Vtrr.-Y H 11 'MT,---OUAlt IV /23723 8/057 61/031/oo6/007/019 B116/B203 c2i, a2s..7 Al AUTHORS: Illin, R. N. and Solovlyev,. Ye. S. TITLE: Ionization of argon by oxygen and nitrogen ions PERIODICAL: Zhurnal tekhnioheskoy fiziki, v. 31, no. 6, 1961, 680-687 TEXT: The authors measuri;d the total ionization cross sections (ii-), the total electr6n capture cross sections (cr ), and the argon secondary ion 0 production cross sections (a.- for the ions N*, ot, N" 0 , NO and N on 2 2 02 with energies of 15-160 kev in argon. They found that a- and the produc- tion cross sections of doubly, triply, and quadruply charged arg9n ions (CTo21 6039 and ao4 ) increased with an increasing number of atoms in the primary ion. They established a relationship between the capture of two electrons leading to the transition 04~~O- and the formation of multiply charged ions. Argon was chosen as gas target because ionization and electron capture by hydrogen ions have been thoroughly studied for this, gas by V. V. Afrosimov, R. N. Illin, and N. V. Fedorenko (Ref. 2: ZhETF, Card 1/6 23723 8/057/61/031/006/007/019 Ionization of argon by oxygen and B116/B203 34t 1398, 1958). Test plant and measuring method had been thoroughly described in previous papers of the authors' laboratory (Ref. 1: N. V. Fedorenko, V. V. Afrosimov. ZhTFp XXVI, 1941, 1956; Ref. 3: N. V. Fedorenkop V. V. Afrosimov, D. M. Kaminker. ZhTF, XXVI, 1929, 1956; Ref- 4: N. V. Fedorenko, R. N. Win, V. V. Afrosimov, D. M. Kaminker. ZhETF,.L6, 385, '1959). Fig. I shows the function a0(v), where v is the velocity of the primary ions, as well as data obtained by H. B. Gilbody Z and J. B. Hasted 'Ref. 7: Proo. Roy. Soo, A, jAO, 382, 1957)- It is shown that the first maximum on the o (v curve for the pair N+ - Ar 0 2 corresponds to the capture of an electron in the ground state, and the second, blurred maximum to the capture in various excited electron states. The 6 (v) curves form three groups corresponding to one-, two-, and three:atomic-primary ions. These groups lie in such a position that the ionization cross section becomes larger with the increase of atoms in the primary iong these cross sections being nearly in the ratio of 1:2:3 with equal velocities. Thus, the total ionization cross section for nitrogen- and oxygen molecular ions evidently depends on the inner structure of the primary ions. Since, in the case of molecular particles of the same Card 2/6 Ionization of argon by oxygen and ... 23723 8/057J61/03i/oo6/007/019 B116/B203 oharget the number of quolei with given Z is inseparably connected with the total quantity of electrons and the particle dimension, it cannot be stated which of these factors has a determining effect. Without con- sidering the 2 of the nuclei, the nuclear quantity itself does evidently not play the main part. The cross section col is composed of the cross- section aC of the single-eleotron charge exchange and the cross section 1 01 dol of the single-eleotron ionization. The corresponding processes may be written down in the following-manner: I+ + A-44 + A+ (1) I+ + A--.'*I+ + A+ + e (2)t where I+ is a primary ion, A a gas atom. The course of the dol(v) curve is mainly determined by (1). This is confirmed by the following characteristics of the curve: (1) The a 01(v)- and do (v) curves show a certain similarity. (2) At v H-), andl on the other hand, the electron excitation of the negative ion (due to collision) sh6uld not be large. The authors thank N. V~ 'Fedorenko and V. M. Dukellskiy for a discussion. There are 7 figures and 12 references: 11 Soviet-bloc and 1 non-Soviet4loc. ASSOCIATION: Fiziko-tekhnicheskiy institut im. A. P. Ioffe AN SSSR Leningrad (Physicotechnical Institute imeni A. F. Ioffe of AS USSR.Leningrad) SUBMITTED: july 16, ig6o Zl Card 5/6 28922 8/056j61/041/004/005/019 B108/B102 AUTHORSs Afrosinov# V. Vog 111ing R. 1.9 Oparing V. A.,Soloviyevo U.S., Fedorenkog So TITLEt Ionization of argon by atone and by singly and doubly charged Long of aeon and argon PERIODIOALs Zhurnal.1koperimentallsoy i tooretichookoy fisikiq V- 411 not 40 9 iq6it 1048-1055 TEXTe In order to study the effect of the charge of primary particles upon the total ionisation cross section# the authors examined ionization by collision with particles of 20 to 360 kovo Argon bombarded with Art Ar+v Ai"t Not No*, and No++ was chosen for the experimentse The experimental arrangement is shown in 71 1 It is basically the ease as that described in earlier publications fi. i. Yedorenko, ZhTF# Z6j 1929t 1959 and 1941t 1956), Fast neutral atone were obtained by resonance charge exchange of a monochromatic ion beam in chamber B, Ions that were left in the beam emerging from B9 were eliminated by capacitor X. The total Card I/~ 28922 8/056/61/041/004/005/019 Ionization of argon by &tons and by B108/B102 ionization cross section the slow-Lou production cross section Ilt ands sooti;n r. for slow ions of charge n were measured. the production cross On The random error was �12% for worv with fast ions, and �15% for fast atoms. 6-was found to increase monotonically with increasing particle velocity. The contribution of stripping to 6_ also increases with increasing particle velocity. Moreover, this contribution is the greater, the lover the charge of fast particles. Thereforop 6~ vill.be smaller for monoenorgetio particles with a high charge than for sonoonergetio particles with a small charge. As a general rule, it has been found that CT is greater for those fast particles which have more -electrons in their sheath. These results are in accordance with those of other authors (I. P. Flake. ZhTF, 31-9 367, 1961). Iffon was found to rise with increasing charge of the bombarding ions. It is lowest for atox-atom collisions. This is caused by charge exchange and by ionisation with oapturep which predominate in atom-ion collisions. Professor V. M. Dukellskiy is thanked for his interest, and I. T. Sheftell for having supplied the resistance, thermometers used in the Card 2/5 28922 8/056/61/041/004/005/019 -Ionization of argon by atoms and by B108/B102. collector. There-are 10 figuros,and-14 reforencesi 12 Soviet and 2 non- Soviet. The reference to the to-gliah-language publication roads as followas H. B. Gilbody, J. D. Hasted. Proc. Roy. SoojS Lk2409 382j 1957- Mention is made of D. M. Kaminker (ZhTPq gjg 18439 1955) Wd-0. B. Fireov (ZhETF, 15179 1959). ASSOCIATIONt Leningradakiy_fisiko-tekhnichookiy institut Akadomii.nauk SSSR kLeningrad Physicotechnical Institute of the Academy of Sciences USSRY....-. PUBMITTEDI May 139.1961 Legend to Fig. Is. ~oolils,i on -chamber,' measuring capaoitort M A - mass analymer,for.,elow ionti.F oollootor for fast particles H 20 and H are pumps eva.6uating the-l'oollision,ohamber to about 1 2*10- 3 mm Eg. Card ILIINq Roman likolayevich (lUrii Ekellohikl the #kill of a notion-picture cameraman) IUrii EkellchikI masterstvo kinooperatora. Moskva, Isku4- stwo - 1962. 1" p. (MM 16:2)'*. ;(Eke'llchik, Nrii-Israll'ovich, 1907-) M. M-111-M-0 R VACON-1 17- 3/056j62/042/003/004/049 q, ~j B117/B112 kUTHORS1 Solov'yevj Ye. S., Illin, R. N., Oparin, V. A.$ Fedorenkop N. V. TITLEt Ionization of gases by fast hydrogen atoms and protons PERIODICALt Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 42, no. 5, 1962, 659 - 668 TSXTs The ionization of H He, Ne, Arp and Kr by fast hydrogen atom 20 N21 and protons of 10 - 180 kev was studied, and the ionization cross section# the strippi ng cross section for fast hydro t and the production en it omal cross secti on for slow ions with vari m ratios were systematically ous e~ measured to obtain information on the ionization of inert gases and nitrogen. The measurements were made by the-well-known condenser method which was s upplemented by the mass analysis of the composition of slow ions. The experiments were carried out with a previously described devico (Ref. 19t N. V. Fedorenko, V. V. Afrosimov# D. M. Kaminkerl ZhTF, L & . " 1929, 1956, Ref. 20s N. V. Pedoranko, V. V. Afrosimov, ZhTPj At 194 19 _ 1956; Ref. 211 V. V. Afrosimovy R. N. Illin, V. A. Oparin, To. S. Bolo'TV" Card 1/4 ;8/056/62/042/003/004/049 Ionization of gases by fast... B117/B112 N. V. Fedorenkoj ZhETFP 41, 1048v 1961). Accidental errors did not exceed t 15~, except the cross sections d and 6 (t 30$). Theoretical and + experimental data more comparable only to a limited extent. The stripping cross sections calculated in the Born approximation showed satisfactory agreement for energies above 60 kov. When the energies were lowersdo the divergence between the relevant experimental and theoretical curves in- creased. Analysis of the experimentally obtained ionization cross sections proved the applicability of the Born approximation for the range of high 9 For the range of low velocities v v 0 . could not be applied any more, since the cross sections for ionization by fast atoms were always~a little greater than those for ionization by protons. In addition,'~ths cross sections for ionization processes of the same kind increased with increasing target atom Z. The stripping curves, of the fast atom (cross section 6,) and the curves of the production of singly charged ions of inert gases (cross section a have abown that in 01) y reach kaxima at velocities vIbLv The peaks observe moot cases the d at 0 Card 2/4 Q Ionization of gases by fast.** S105Y621042100310041049 B117 B112 lower velocities are qualitatively interpreted by a quasimolecular modelt in which, owing to the drop of ionization potential, the peaks of the ionization arose sections are shifted toward lower velocities v Is From.the point of view of the quasimolecular modA the proton-atom system of the inert gas seems more stable with regard to ionization than the H-atom-atom system of the inert gas. The probability that a partial ill be ionized after the decay of the quasimolecule depends on the elect;own binding in the atom in question and on the ratio of statistical weights of': possible states of charge. These two factors may effect a "competition" between the ionization processes, which must influence the position of the peaks of the ionization cress section. The curves for the production of singly charged ions of inert gases and for the stripping of the hydrogen atom confirmed the assumption that the position of the peaks depends not only on the ionization potential of the relevant atom but also on other. factors. The maxima for velocities vrj(1 - 1.5)v were determined for 0 cross sections ai(H) and a,(H of ionization by atoms and protons,... 2 Si respectively, The experimentally obtained position of the peaks an the Card 3/4 S/056/62/042/003/004/0,49 Ionization of gaues by fasts** B117/B112 curves of cross sections for production of slow argon and krypton atoms in also given. It is noted that, as in the case of krypton, the peaks on the curves for two-electron and three-electron ionization (d d W) 02(v)t 03 argon correspond to about the same velocity v -v. As in the case of max interatomic collision# the position of the peaks is presumably determined by the ratio of the internal electron velocity of the second partiole to 'Vi - the velocity of the relative motion. V. Us Dukel'skiy and 0. B. Firsoy are thanked for valuable hints. There are 7 figures and 23 referenoess 10 Soviet and 13 non-Soviet. The four most recent references to English- language publications read as followat R. Curran# T. M. Donahueq Physs Rev., 118, 1233, 1960;. is W. Hooperg E. M. McDanielq D. 1. Harting D. S. Harmer, Phyo. Rev., 1219 1123, 1961; J. W. Hooper, E. Us McDaniel, D. W. Harting D. S. Harmer, Abstr. of the II Intern. Conf. Electronic and Atomic Collisions, Bouldert USAq 1961s p. 0 - 8o, H. B. Gilbody# J. B. Hastede Proo, Hoy. Soo., A240s 382, 1957- kSBOCIATIONs Leningradskiy fiziko-tekhnicheskiy institut Akadenii nauk Suit (Leningrad Physicotechnioal Institute of the Ac&d~W oV Sciences USSR) SUBMI79Dj July 21, 1961 Card 4 j"j SMV'73V, 'Y3.$.#' -IWNo R.N., OPARM. V.A., nWFZM, N.V. Olorilsation of cases helium Ions and fast belius atoms** Report nWAtted to the thirdt lati,,Confe on MWAve of Electrodes and Atomic Collislonsp loadons InglaW 22-26'July'103 SOWVITSVO To. 3.1 WIN, R. W*j OPAMNq V. A.1 FMRENW,, N. V. ronization of Oases by Fast Helium Atom and Singly-Cbmrged Helium raw report presented at the'2hth M"Ung of the rna. conwittei for suctrochenical, Thermodmaics and Kinetics (CITIM) Nosaowo 29-25 Avg 19630 Ioffe Pbpico-Tooh Insto AGO& Baia =Rt Ismingred USSR SOLOVIIEVP Yeoso; T11INp R.!-L OPARINO Y.A.1 nDMNXOt N.V. Ionization of gases by fast atom and singly charged helium ions* Zhur, ekspe I tear, fist 45 no,3t49&502 6 t63, %.~' (KMA 16:10) 1. Fisiko-tekhnicheskiy institut imeni A.F, Ioffe AN SSSR. (Ionization of gases) (Helium), ILIINP RGNOI.*". Iskusetvovedobeskikb vauk, dots.1 LEBMEVA, L.j, M, [Work'ofa tolevislon cameraman) Rabota operatora na tolovidenil. Moskyap Vagoo goes in-t kinematografilo 1964. 67 pe (KIRA 28j6) ACCESSION NR, AP4031139 S/0056/64/046/004/1208/1211 AUTHORSs ;~!ino R. Nq Xikiani, B. 1.1 Oparino V. A.; Solov'yev, Ye.-S.i Fedoren o, No V. TITLE: Dissociation of positive hydrogen ions in collisions With atoms and gas molecules SOURCE: Zh. eksper. i teor. -fiza, v. 46,,no,..4, 1964, 1208-1211 TOPIC TAGSs proton cross section, hydrogen, nitrogen, helium, a gon, particle collision, ionization phenomenw ABSTRACT: The purpose of the work was to repeat the measurements of the cross section for the production of protons following dissocia- tion of molecular ions H*" with energy 10-180 keV in hydrogen, nitro- gen, helium,. and argon* sing the same setup ~as previously, (ZhETF v.. 36, 385, 1959), but with a more thorough elimination of the* main sources of the systematic errors. Copparison. of the data obtained Card 1/3 ~ACCESSXON NR: AP4031139 on these cross sections'with the work published by others shows that overla wide energy',range the majovity of the curves obtained in re- cent-work lies bet%Jeen the data of Sweetman (Proc. Roy. Soc. v. A256, 416, 1960 and privAte communication) and the early work by the authors, with the 4skceptio~ of the early data -by C. F. Barnett (Second UN Ifitern. Conf. 6n.'Peaceful Uses* of Atomic' Eftergy, Geneva, 1958, Report 1789) whicW aie considdrably below. Taken together,,. the various data cover almost the whole range of kiloelectron volt ener- gies. For hydrogein, the maxima discovered and reported in the early work are confirmed, the first being due to the predominant contribu- tion of the dissoa4tion of Ht ions into atoms' and protons, and the 2 second being related to the dissociation into two protons. A separate measurement of these two crossisections by J. Guidino (C. R.'-. Paris, v. 253j, 829j, 1961) confirm -these results. Orig. art. hass 4 fi4ures and 1 fO`%'=ila. 1/3 ACCESSION MRs AP4031139 ASSOCIATIONs Fiziko-tokhnichookiy institut ii. A. P. loffe AN SSSR (Physicotechnical Institute AN SBSR) SUBMTTEDs 180ct63 DATE ACQs 07K&y64 EMCL& 00 'SUB CODE% NP, GV UR REP SOVs- 005 OTHERs 006 3/3 -- ---6l a - - I - I -- .- - . ,, ,- F -.TirF -11, iw~Li~~e -e-w~KKin . 1 1, fW ___j A. i A - I - --- - - - - - - - -- . - - - , -. -, - - I- I 1 11 Z , * - - - . - - a--j &no Z salmew- I I -- .- : ',, i ',-.r- : I- -, . Ir ~ v i , ACC "at APNVIM SOURCE CODE: UP1038616VOwlOOT103201031k, A10 AUTHOR: n 11 Inp Rs N a; Oparinp , M. A Solov levo Ye, 0 FedoregLwj N. V 41;~~ ORG: Ptweicotechnical Inati&Rte in. A. F. Toffe Acadew of/Sciencen SSSR Flziko- tekhnicbeskiy institut- Akadenii nauk SfflR) of VrAo 6 1 - TITIZ: Charge exchange pfigalMline metal th formation of highly excited-hydrogen atoms, SOURCE: Zhurnal eksperimentallnoy. I teorsticheskoy fiziki. -Pis'na Y -redansiyuo (Pr1lozhen1ye)o Y. 2p no- 7., 1965, 310-314 TOPIC TAG$s protonp charge exchangep alkali metzi twdrogen, excited allte ABSTRACT: The charga exchange of 10-180 kev protons in vapor of Li, X&J, X, CsP and MS was iwmatigated vith an &In at using thin process to obtain highly excited bydro- gen atoms* An atomic beano obtained by charge exchange of the protons in the vapor of these metals and purified to eliminate the charged particleso vas fed into a re- gion vith strong electric fieldp of intensity E < 160 ky/cm. The ratio of the curren of the secorklary protons, produced upon Ionization of the highly excited stoma in the field Ej to the total current of the atoms I(E) was measured. This ratio character- ftes the relative charge-exchange yield of the highly excited atoms. The total cross section for proton charge exchange and the ratio of the total mud)er of atoms pro- duced by charge exchange to the number of protons in the primary bean were also me&- sured in individual experiments. These made it possible In turn to determine the cross section for the charge exelmuigeacconpanted bj production of highly excited Card 1/2 L 98A2tM ACC N1b AII~M990 ate". Plats of the cross sections against proton energy are presented both for metallic targets and (for caqwlson) for He., 'Nej Arj aW_H2.___ The plots- -show Ahat_ _f6 - -_ -i- -the-cross. sections- -for -alkaline. Metals and r Magnes um above 15 key decrease with Increasing energys A characteristic kink-was observed for both cross sections in the region 30-70 keyp beyond,which the decrease of the cross sections slows down* The presence of the kink on the curves can be attributed to the fact that at low energies the outer weekly-bound electron of the metal atom takes put in the charge exchange, while at high energies .& greater role is played by, charge exchange with participation of the electrons from the filled shellp analogous to the outer shell of an Inert gas. The latter In confizued by the similarity of the plots for the alkalini metals and magnesium and the simila plots for Inert gases at high energies. 7he main conclusion ofthe investigation in that vapors oi? Alkalin and alkall-earth metals are more suitable targets for the production of highly excited atoms of hydro- gen at energies btlow W key, and that molecular hydrogen and inert gases are pre- ferable at higher energies. , Orige art, has 3 3 figures. am CODZ: go/ sm DATxj 26ja65/ ORIG MWI 002/ OTH PZF: 002 LS h o2w:67 ACC NRj APS025252 S=C19 CODE: UR/0037/66/036/007/124IA250 AIMHOR: IlIng R,.N,i opsrln#V*Ao; So Yedorenko.N.V, Leningrad (FIXIko-tek- orta: PhyAlcotachnical Institute IN* AsFoloff,V? AN SSSR# i hnicheakly institut) TITLE: Electron attechmen 11t0 protons in JhAJLj1qW vsR2 with the formation of highly e-ke-ft-ed hydrolle toms ~4'1 SOURCE.- Zhurnal tekhnicheskoy fizikI, v. 3.6l no. 70 1241-1250 TOPIC TAGSl proton, charge exchange, gas target, atom, excited state, alicall metal, inert gas, hydrogeng carbon dioxide# plasma injoctiont ARSTRACTs The iuthors have measured the croob .'tections of U, Na, X, Cs, He, No, Ar. and H for the ulectron attachment reaction of 10 to 180 keV protons with particular attenhon to the eross mectlons f(,r pro,at-tion of highly excited hydrogen atoms. The measurements were undertaken because of taoir Interest in connection with Injection of plasma into magnetic traps* The been, ln,tially of protons, successively traversed the 12 cm long heated target chamber, a *qjak traiaverse olectilc field which removed the charged particle#, a strong (up to 160 kV/,.-m) electric field which ionized the highly excited Atoms, and a magnetic fivId which acparated the ions from the remaining, neutral stoma, The neutral atoms were recorded with a secondary emission detector Card 1/2 -AM-539.186- L 02273-67 t-'ACC NRI' '"'60'25253 which was calibrated against a calorimeter, The alkali metals were introduced directli into the target chambers and thd pressure of the vapor target was determined from the temperature of the chamber, Thin target data were obtained for all the target mater- islas and thick target (up to 0*4 ca torr) data were obtained for Na and Ne and, at some values of the Incident.graton energy# for X. Cos and COgg The results are pre- sented graphically and in t ular fom,- they are discussed at some length and are compared with theoretical calculations and with data of other investigators. It in 1concluded that at incident proton energies up to 30 keV the alkali metal vapors are efficient targets for producing both highly excited and modorately or unexcited -by- drogen &tons but that at higher proton energies the inert gas and H targets are more 1 offoctive for producing highly excited &tons, The authors thank YuggeDemkov for dis- cussing the resultse Origs art,, hast 7 formulasp 7 figures# and 3 tables, SUB COD11 20 BOU VATM 0SAug8b OHIO, Rat 008 OTH UPS 013 2/2 Ymb i Card I&SID, R. S.= "Investivation of s7stems of c,)mblniw! a precisinn eche- 11 iut'a with aupolemstitary dispersion adaptatinn." "In Fighar Mu- I cation UL611t. 1-b:;c,-,w Order of lenin and -^.Tder )f Lator Re.1 Banror , Koscow, 1956, (Dissert-ati s I "Alcher Teclinica.1 3&,),,)l irmni DamAn. -1 )n for the Dagrao of OnndillAtO in Technical .60: KrIlalma-ra leti An I N-) - 22, 1956