SCIENTIFIC ABSTRACT VERKLOV, B.A. - VERMEL, A.YE.

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December 31, 1967
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SCIENTIFIC ABSTRACT
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VERKLOV. B.A.. inzh. Rural-.33% coal cutter. Ugoll Ukr. 5 rw-4:37-38 Ap 161. N RA 1414) (Coal mining machinery) PONOM&RENKO, V.A., kand. tekhn. nauk; KRAVCHINSKIY, S.Yu.; V!R!IDI!~_..B.A., kand. tekhn. nauk; LYSYUK,, V.S., inzh. Establishing an optimumchart for underground mine hau:~age by the olectron modeling method. Ugoll Ukr. 9 no.12il9-21 D 165. (MIRA 19:1) 1. Donetskiy nauchno-issledwatel'skiy ugolInyy institut (for Ponomarenko, Kravchinskiy). 2. Kommunarskiy gornometallur- gicheakiy institut (for Verklov, Lysyul.). VERKLOV, B.A.t inzh. Determining friction losses in case of prepole transmission of internal engagement. Vest.mash. 41 rio.8:11-14 Ag '61. ~MIRA 1,4:B) (Gearing) PETRENKO, P.V-;,ELIKIN, I.L.; KAZAKOV, S.S.; VOZHIK, D.L.; DEHISOV, V.V.; PUCHKOV, V.I.; BOGUTSKIY, N.V.; SAVEL'YEV, I.P.; KOLENTSEV, M.T.; MZRKULOV, N.Ya-; 3%-RK~OV V A - _- '--RZHOVA, V.V.p OVSYANNIKOV, P.A.; SOSNOV, V.D., oty. r2, otv.red.; ZHUKOVA, A.P., red.; LEVIRA, T.I., red.;-RONINA, N.D., tekhn. red.; OVSEYENKO, V.G., tqkhn. red. (Practice of using cutterloaders]Opy-t Lspollzovaniia ochi- stnykh kombainov; sbornik statei. Moskva, 1962. 102 p. (MIRA 16:2) 1. TSentrallnyy institut tekhnicheskoy informatsii ugollnoy promyshlennosti. (Coal mining machinery) USSR/Microbiology - Microorganisms Pathogenic to F-3 Humans and Animals Abs Jour: Ref Zhur - Biol., No 18, 1958, 81571 Author Ygxkgz4-K2-.,3 Pletneval G.G., Blankman A.L., Vishnevskaya, N.V., Korneyeval G.A., unskeya, AsI., Lurle, A. Ya., Isakovich, S.P. Title Vaccination Against Tuberculosis of Children and Adolescents Having a Positive Reaction to Intra-Dermal Injection of Tuberculin. Orig Pub: Vopr. okhrany materinstva i detstval 1957, 21 Wo. 61 1+0-1+3 Abstract: No abstract. Card 1/1 42 it Is 4 W it It U It 0 0 AII U AJ 00 OL-0 A is got, IUOO 1- 1.9 4t WON&$ Osocosul &-a pfcfwq~ MNS (7anf. Lah.. 104-11. 14. 111). j39 tachnient by "WAM nf whi a Ith fm 1e ILI rh photumj,.nwmphm fwf nw.j.,kj, 4.41, be taken pn it Zoo* 400 .00 zoo te it 60 1 1 ~ 1'." 11 '106 i*svelr 00 g ~400 X*o ,so 000 It I a - S L ASITALL1106KAL 1.11911AIU119 CtiSSWICATIC" C-1 i M g_,, 6W-1 %),A#, Clot o" 'I. a i-S I u 4 to to ODIC Kit its 01112t It MIKLOR 1,K4 0 : : 0 0a 0 0 0 0 0 0 0 Vfo* 0 to 0,0 te o 00 0 0 0 0 0 to 'm to 0 0 o so GIs to to 0 q 0 o 0 a 4, et 0 0 0 0 0 *it I -. K- ~, "." I 31009. VERKOV, 1. 1. OD BAKKAL, S. A. Lechenie samoprsizvollnoy !~angreny tkanevoy teraptey po rantocly akademika V. P. filatova. Khirurgiya, 1949, No. 9, s. 65-69 VA Sixth conf,~~renca of the Bolshevik ?dirty. 1"restlianka 31, 'ro. 1~52- 9. Monthl List of Russian Accessions, Library of Ccngress, November -195X2 uncl. 1' VERKUTOVv A.N.1 ANTIPENKOP V.S.; ASEYEV, L.-I. - -------------, Homotransplantation of the skin an a method for the acceleration of wound healing Xbirurgiia 36 nog 5:106-3.13 My 160. (MIF-A 14: 1) iSidN GR&nING) (WOUNDS-TREATMENT) VERLAlql,, A.F. SoIring Volterra second-order integral equations b7 analog emputers. DDp., AV-MM no,l2sl568-1570 162. (KIRA. 16:2) 1. Imatitut kibernetiki M UkrSSR. Predstarleno akadmaikom IN UkrSSR T.K. Musb3covym LrMushkov., VJQ& CIntegral equations) (Electronic analog compatexa) ACCESSION r1R: AR40110439 S/0044/64/000/001/B107/B107 VSOURCE: Ref. zh. 14atematika, AbG. 1B514 AUTHOR: Verlan', As Fe TITLES: Method of simulating differential equations with boundary conditions oil jolectronic mathematical machines of continuous action 'CITED GOURCEt Dopovidi AN URSR, no. 4, 1963, 451-1153 TOPIC TAGS: differential equation, electronic mathematical machine, continuous action mathematicai machine, algebraic equation model, automation proce6a, differ-:' ential equation simulatior, resolution process autonwition TRANSLATION: Author proposes to find a solution of -the system of differential ~Iequations dX -/(I. X W) with boundary conditiona QX(0)+xxV1)+Pi(r)-Y .with the help of iterative formula (Lxi,., to) y-xx,, yj)-pxt (r), -Card 11/2..,. -ACCESSION TIR AR4040439 !Vectors X(ti) and X(T) are determined by means of solution of system (1) on elec- ttronic mathematical machine of continuous action at initial conditions equal to 1. For automation or resolution proceas it is necessary to have memory unit tXk(O)' iand model of algebraic equations. N. Lyashchenko. iDATr. ACQ: 03Har64 SUB CODE: MA ENCM CO VERLANIP A.F, Determining the frequwcies of natural vIbratians b7 means of electronic models. Dop. MI URSR no.6:733-735 163 (KIRA 17W 1. Institut kibernetiki All UkrSSR. Predstavleno alcademi,.Com AN UkrSSR VJI. Glushkovym [HIushkov, V.M.I. y~4RIANI,,Aratoliy,.Fedorovich,, aspirant Conaerning A.I. Petrenko's report OComposition of a problem using a model," Izv, vys. ucheb. sav.1 elektromekh. 6 no.9t 1126 163. (MMA 16s12) 1. Otdel matematicheekogo modelirovaniya instituta. kibernetiki AN UkrSSR. T Cl P I C T A CS nnnkniu,. r ~n!Pt!: i 1 1 rn in u it; )(I kinri, )n,(- k f t -I rq I r)r-. r -i rt ? ~' -P-f !I)!- :- ;- ~, . I ~ 7 i ~ , i_, ~.- . , - . -,Tfl n T~-t- . llf~4 Il-ri4wrl. firin ,T'7-, -1; -,r-' I- . I . IT' I I Card A L2- if f (X) + A K(x s ) F1 y (a) Ids a ere Studied under the assumptions that sol u t f--is -of t h e 9 ceq jations J;. r r st p a c e t n e p o s 51 1 1. 6 considered. Tha a olu tL oc c t t h e a eeqja t I ,)is 6 e G 12 C 10 L n C 5 C' U- o f a 2e" ra, a-, c-'s A It- rk d i v r Pm o f rh e nm- r P. r de a i 2ne d it o r e a k i a L i. e a .- ' L ~l I -. u ~ a L i ~". :1 CCD t L 14484-65' ACCESSION N R ac""at ion a n a y z t- C " j i I j . , - 'AUTHOR: Verlan', A. F. TITLE: Integral equ-ai ion -31ve r SOTTRCE: Avtomatflm -pr ft-or"et rover iyn, no, 3., 1964, Z4-J5 'rr)Mr, 3nff--;-zr, Int fiolvent. aq --Ertl equatif-m. selver A RA,, i F--~Tild~3al f 1, 1 r i;-i t r~ t 'ae v~ t);i i 1 7- ft, WWI V f- 8 t LA I I t k-ex 1 T z hA ui I i n a w id t! -j cf)p,! of ~A! i ng rion! i ne, 7 ACCESSION NP-- AP4C46109 wita various modes of regular kernels. I ~ASSOCIATXON.,,- InbUtwIlibewsiatild AM of variational methods witi','. zi;i a7i"-'O~q cc-mp--Iier SOURM' AH UkrSSR. Institut kibernetiki. Hibernetika i trychis- ~R!757---rn7t- -7-'tnci conp~ater engineer Lna) Kiev, Haukova durxe-a, 1964, 3-7 TOPIC TAGS- integral equation, F,.-edhoIr,-i e-4u.ation, anaLog 4pproximation tlieory, least scwar(is metliod, polynomial approxr-imation Me a thod- of arwroximating an inte- -qTON NPli AT5004746 ACCES anlution of a Fred- 74 -e. n- - S" OCIATION f - r) p P 7- I Fimcticn qmeraticr) b1ccY, inteqra-I : .1 4 . ~lj I I I No ~/ 'I k. J 4 ACCESS!' A q ti L-: r Irl e 0 ACCESSP)N NR: AT5064748 that the function geneeator degcribxid Lr, this arti -le in superior to st se, anfl, can b, cr-,rst rur-tc-d f rom fileinents widely used in wnalag cc;nputer technology OrLq. art. ras: 4 figures and 7 formulas. -~:~~-JASSWIATIONt.~ None SUB CODE: DP# MA -z SUBMITIZID: 30gep64 ENICL- (11 NR REF SOVI* 001 OTHER.- 001 17 S Ou! Lnlegral tran z,-, TOP:C Tl,.i;,-); AMINUCT. Mis Wthor Certif cate pri~3r,-- for rjoivina in,c~Zr.-,j eqlj-rL- -macted tc thf. r~ouir Cc FUMY, Georgiy Yevgenlyevicb; CREZDOVj, Gennadjv Ivanovich; VERLANI, Anatoliy Fedorovich; 14EL'NIK, T.S.V red. - (Methods for solving boundary value problems usinb anslog computers) Metody reBheniia kraevykh zadfich na elektrw nykh modeliakh. Kiev, Naukova dumka, 1965. 144 p: (MIRA 18:3) I* Ghlen-korrespondent AN Ukr.SSR (for Pukhov). L 18580-63 .EWT(1)/BDS 4FFTC/ASSD/SSD ACCESSION NRs AP3001277 S/018116310051006/159511600 ,;AUTHORSt KondilenX9, I.I.1 Verlan,, R.M,; Karotkov,, PA.l Strizhevaldy,, V. :5 ;TITLE: Indioatrix of the combination scattering of light in a crystalline nedium ~'SOURCEi Fizika. t,~ardogo tela,, Y, 5. no. 6. 1963o 1595-1600 TOPIC TAGSs combination acatteringp, indicatrix, Si# -0. optic axis,, crystalline material iABSTRACT: The authors have studied the conditions of dependence (of the lindicatrix) of combination scattering of light in crystalline material both in Itheory and in experimental work. The theoretical expressions are derived from previous works (V. L. S trizhevskiy, M. 3, 2929, 1961., and FTr, 4. 14920 1962) iThe experimental work is basically similar to previous work on liquids (I. I. 'Xondilenko di PI.A. Korotkov, and V.1 . Strithevskiy,, Opt. i. spektr., 11, 169, 1961), The authors obtained general formilas determining Vie indicatrix in any arbitrary stal. Vibrations of 466 cm-1 in quartz were firat used in experimental investi- ,cr7 :gation of the indicatrix in a crystal in the angular interval of 40-1400. The experimental data agree with theory. The authors show that a study of the indic- atrix of combination scattering may serve as a mthod of investigating oriented Card 1/2. L 18580-63 !_Ac6nii6i ,systems. To illustrate the method (with a few simplifying assumptions) they determined the Angle formed by the Si-O bond with the q%tio axis, This value iproved to be 55u, which corresponds satisfactorily with the actual value of 540441. There are disadvantages to the system., however, limiting V.3 usefulness, Xhief of these is the presence of parameters in the formilas that are unkncrwm-- :components of the tansor of combination scattering* Furthermore,, the spectrum of ,combination scattering is -not always capable of experimental observation. Orig. ;art. has: 1 figure, 1 table.. and 13 formulas. 1ASSOCIATIONt Xiyevskly gosudarstvenr" universitet in. T.G., Shevchenko (Kiav State University) lijan63 UTE ACQj - OIJu163 rIGL: 00 SUB14ITTED: 4 MB CODE: PH NO REF S(jVt 009 OTHERt 001 Card 2/2 VERLANS, A.F. 1;- 1 1 ~. lyre of storwe devices in solving problems by means of analcg computers. Kat. mod. i elek. tsepi no.1:41-44 163. (MIU 16:11) L 11038-63 UT (d) /EWT (M)/FCC (v)/BDS/ESC_2 AFFTC/ASD/)iFnC/IZSD-3/APGC Pe-7,7Pk--_ F(/P-i_jj/Pq_jf kd~=ff MI: ArM2147 9/2923/62/000?~W/bO54/0D56 AUMM %.JAnF1 A. F.- 71 TTT.12: Sol-ring the TredhQlm lzitE~zrsl equatior o0, thi! -secand kind v,-Itb electronic ana.Log computers SOURM: VY-*-_h1slitel'nkTa matenatika i tekhnaa; trudy* aspirantov Tmstituta kibernetiki AN UWR. lzd-vo AN UWR, 54-56 analog ccWuter AWTRAM: ThIs wail-known equation can b6 solved either by the method of sucaes- or by tbe-- EL-Mel le--Iterativa~ -method. rh both- emes special, devices -are required In addition to, a standard ar^IQZ computer. As In many cases eZatlon can be replaced b7 a degenerate kemtl, the author suggests, for such cases, a method of solution that requires a rtandard analog conputer only. Any computer containing accumulators, integrators, nil-tiplying unitsl and nonlinear-function units is suitable. Orig. aft. has: I figure, 10 fo=Llas, and I table. Institat kiber=tnd Alt USSR- (rhatitute of Cybernetica, Academy of _71. -- - - - - - - --- .ACCES31UT 110: AP4002276 S/0139/63/000/005/0113/0117 AUTHORS: Verlcm, E. M.; Strizhevskiv, V. L. TITLE: Triple Fermi resonance in a carbon tetrachloride molecule ~MURCE: IVUZ. Pizika, no. 5, 1963, 113-117 TOPIC TAGS: carbon tetrachloride, Fermi resonance, oscillatory ener&r level 'nteraction, resonance interaction, fundamental Fermi resonance dcublet, degenerate resonance level, CCl4 absorption band, oscillatory absorption band. laSMACT: A theoretical study has been made of the Fermi triple levels in carbon tetrachloride represented by 2 V Ll + J/ + j/ and 2( j/ + ii ). Of these,v is fully . 3; 1 3 4 1 4 1 syr-netric, whereasz/ and a are triply degenerate. The wave function of the 3 4 perturbation system is written as T-= Cl?%+ C276+ C3 The potential ener8y term is represented by a cubical function of the normal coordinates, and the system of linear homogeneous equations is given by 1/2 ACCESSION NO: ILP4002276 3 C., 0; 1 1, 2. 3 V , A. E. F,. Th6 solution of the characteristic equation then yields respectively 1590, 1566, and 1534 for the three ener&r levels considered. These results show reasonably good a,-reement with the experimental values reported by M. P. Lisitsa, V. N. ?.'!alinl-.o (Cot. i spektr., 4, 455, 1958). "The authors are grateful to M. P. Lisitsa for evaluating the analysis." Orig. art. has: 11 equations and 1 table. ASSOCIATION: Kiyevskiy gosuniversitet imeni T. G. Shevchenko, (Kiyev State University) SUBMITTED: 28Feb62 IRTE ACQ: 02Dec63 ENCL: 00 STB CODE: PH 3 NO IREF SOV: 008 (YTHER: 001 KONDILENKO# 1,I.1 3q~~O I,M.; KOROTROV, F.A.1 STRIZHE7SKIT, V.L. Indicatrix of the Raman spectrum in a cryatalUne seditxn, Fiz. tver. tela 5 no.6:1595-1600 Jo 163. (MIRA 16:7) ~t 26049~0 AM) 1&0 GG AITMOR: Verlazi, E. H. OEG: none TrM: Investigation of the shape of a tensor and temperature dependence of the Rman effect of' gas polyatomic molecules S(MRCE: Optike, I apektroskopiya,, v. 20, no. 4. 1966, 605-615 TOPIC TAGS: tensor analysis, Raman effect, temperature dependence, polyatomic - molecule AIGMCT: With the aid of the electronic wave functlon of the adlEtbatfra approxima- tion, forms of the tensor of the Raman effect-have been found for various oacillationi of the XY2 mOle!cule vith C2. aymmetijr_.V"aa shown Oat at a distance from the ab- sorption zone, the tensor of the Rnman effect is prajAically sy=etrical. Dissy-m- vietry of the tensor increanes in proportion to approximation of the incident light frequency to frequencies of the cathode-ray oscillat,iry absorption of the molecule. A close connection between the excited electron-oscillatory properties and the in- U!nsity linee In the apectrum of the Raman effect wa-a d4at-ormined. in an earlier study (H. V. Vollkennhteyn, M. A. Yellynahevich, B. T. Stepanov, Kolebanlya molokul, t. 2, M.-L., 1S)49), it waB ohow-n that the oscillatioa-frequency change of the Moleculf In the excited electron state leeds to deflection of the temperature-dependence line. ..D01 1 L 26%9-66 Uw ACC NR, AP6013021 The definitions presented indicate that In gases these abnormalities are small erxd cannot elucidate any significant deflection in liquid-9. 'The author thaalte; -X.Svander for his valuable advice and interest tr. th-4s work. Origart. has: --37 fo -~~on author's Wvs rmu1aa.--T:RWs tractl- -S-UB CODE, 20/ Sm DATE: 16rov64/ Mir, REF-. '010/ Ccr.2/2 L 36434-66 EuT ( 1 ACC NRt AP6015421 AUTHOR: Verlanj E. M. ORGS none SOURCE CODEt UR/0051/ 0808 TITIZ: Effect of the characteristics of the transition state on Raman-s-ooctra of gases -? SOURCE: Optika I spektroskopiyap v. 200 no. 5, 19661 w4oa TOPIC TAGS1 Raman spectrum, excited electron statev ground statep vibration frequency I 10STRUICT., The effect of the dynamic and geometrical characteristics of a molecule (vibration frequencies of nuclol, vibration form, anharmonicity, equilibrium position of nuclei, syrmetry of molecule) in a transition state on Raman spectra are treated by asswning that the frequency of incident light Q is far from the froquoncies cor- responding to purely electronic transitions of the molecule. It is also assumed that the adiabatic approximation applies. Tuo cases are consideredt (a) the symmetry of the molecule in the excited electronic state coincides with its symmetry in the ground State; (b) the symmetvf of the excited and ground states is different. 4% shift In the equilibrium position of the nuclei, a change in the form of vibrations and fre- quoncies, and the anharmonicity of tho electronic state cause the appearance of over-i, tones and combinatioii tones and affect the line intensities and the temperature depen-',_ UDCt 535-375 L 3643L iCC NR. AP6015421 dance of the lines. A change in the symmetry of the molecule reinforces the intensity of the incompletely w1metrical vibrations. The author is sincerely grateful to L' i N. Ovander for his steady interest and helpful suggestions. Orig. art. has: 15 for- mulas. SUB CODEz 0 VSUEM DATE& 26Dec64/ ORIG REF: 0061 OTH RM 001 ACC NRt AP60IY40 AUTHORS Verlang E. M, ORGS none SWRCS CODES M4oo51/66/o2o/005/0q16/0q17 TITIES Selection rules in Raman spectra 94 SMACES Optika, i spektroskopiyaq v. 209 no- 5s 19669 916-917 TOPIC TAM I Raman spectrum., selection rules, excited electron statep ground state ABSTRACTS Theoretical and experimental studies indicate that the symetry of a mole- cule may change when it passes to an excited electronic state. In this articlep, the selection rules have been extended to this case. The symmetry &20? a of a MolecUs, Ir the ground state and excited electronic state are designated C respectively. For simplicityp the discussion is Limited to cases where groups C an4 CJ have irre- ducible unidimensional repreiefitations. It is also assumed that CJ is a subgroup of group CO, It is shown that (CO) To (0)) X T.0 (CO) X r,,, (0) X Ti (C*)- and that for lima of the fundamental tone and the special case where T000) in a single rGPr*0GntAt10nj. (CO) = To (C") X F/Ij M) y T, (0). 112 UD01 535,375-001J L 3441.5-66 ACC NNs Ap60151ft It is concluded that the *a1lowed" vibratiom in Haman spectra wJU be only those which are contained in an WApansion of the product r.,(C*)Xr,,,(C'*) in irreducible representationg of grrL, CJ. This selection rule becomes the usual one in the case where groups C and C coincide. It can also ba readily verified that all the vibra- tions of a molecule with D2h symmetry In the ground electronic state (even Au) are Nallo-ded" in Raman speotra.-Yt this molecule decreases its symmetry to C2. in excited electronic states. Author Is deeply grateful to L&-j*-Orander for a discussion of the results. Orig. art. has$ 5 forwilAs. . SUB COD31 20/ SM DAT91 29SqA5/ OPM MWt 002/ OM RZF8 001 AP6018442 AUTHOR: Verlan. E. M. SOURCE CODE: UP/0051/66/020/006/1003/1009 ORG: none TITLE: Combination scattering of light by gases in the absorption band SOURCE: Optika-i spektroskopiya, v. 20, no. 6, 1966, 1003-1009 TOPIC TAGS: combination scattering, light scattering, absorption band, diatomic mole- cule, complex molecule, quantum mechanics ABSTRACT: The case where the frequency of the irradiating line lies within the ab- sorption band was investigated. Since scattering is a second orderprocess, it was necessary to consider the initial, intermediate and finite state of a quantum-mechan- ics system: molecule + radiation field. The analysis involved diatomic gas molecules, I. e., the model of a one-dimensional harmonic oscillator. The empirical reaults ob- tained confirmed previous conclusions regarding the effect of the intermediate state on the line intensity in combination scattering spectra. It was demonstrated that the intensity Is proportional to the fourth power of the frequency when removed from the absorption bands. The closer the process approaches the absorption band the greater the number of deviations from this law. In the absorption band, the frequency reia- tionship is a function of the properties of the resonance electron level. It appears, UDC: 535.375 (2060'3) L 42901-66 ACC NRs AP6018442 that in polyatomic molecules this can bring about a different frequency relationship between fully symmetric oscillations and oscillations which am nat fully symmetric. The nonsymmetry of the combination scattering tensor was a';..so analyzed. It was estab- lished that the nonsymmetry increases as it approaches the absorption band. The fre- quencies at which the maximum light intensities oc~:ur are derived. The author thanks L. N. Ovander for constant interest in the work and for valuable advice. Orig. art. has: 28 formulas. SUB CODE: 20/ SUBH DATE., 26Dec64/ ORIG REF: 006 CcrI . . ....... . . ACC NR% A?3026657 SoWtCE CODZ': Mi/0181/66/003/000/2li35/2'i'%1)9 AUTHOR: Verlan, E. M.; Ovander, L. X. ,ORG: Kiev State University im. T. G. Shavchonko Wyevski gosudarstvannyl univer- 1Y !sitet) TITIZ: Rezonance Raman scattering in crystals SOURCE: Fizika tvardogo tela, v. 8, no. 8, 1966, 2435-2439 TOPIC TAGS: Rar-zr. scattering, exciton, absorption coefficient !ABSTRACT: According to a theory developed earlier by one of the authors (Ovander), the! Stokes component of the Raman scattering in a crystal should be treated as the split- iting of a 11511t cxciton into t-do parts. One ia a light exciton in the region or cr"J~_ I ital transparency; the other is almost purely a mechanical vibration, Which eventually, I :heats the crystal. A study is made of the resonance REman scattering, taking into ac- 6unt the mechanical dispersiom of vibration and dxnping. This limits the intensity of, e lie light sc-4-tering in the resonance point. It is shown that auxiliax~j waves aris ear exciton abso-.-ption and car, play inportant roles in the case of thin plate-s. it follows from the theory that the absorption coefficient (for the ordinary wave) gro-4-- faster than -Che intensity of the Raman scattering as the incident light frequency ap- proaches the z-baarption band frequency. Orig. art. har.- I figure, 17 formulas. IjSUB CODE: 201 SUBM DATE: 28,layGS/ ORIG REr: 005 1 The te-action 0! V. V. n~t.carboxt. M! C: Teihnol. Tri' C;!or-nation of active C, driLd at 12N)', with Clt rrixed ~Q_ Y;--,!defl soinc CC4 at -700-SW*; adv~i' -,f Feas was ineffective. Z30- W83 any k-LI41 formed in attempts at chloriiiation by brauzz M mixt. or C with SbC4 in a scaled tube 100 hrs. at N-0-400*. (2) Thermal decumpli. of CC4 vapor over active C decreases, at a given temp., with increasing rate of flow r. and, at const. r, linearly with the temp.. at r - 0.10, 0.60, 3.10, g,/min., the wt.-% CCI. dc,~ampd. was: at 44DO*, 12.1, 6.1, 4.9; at 5W. 21.4. 17.6. 10.6; at OW', 39.5. 25.0, 15.1; at "d(K)', 52.5. 3:3.6, 23.9. The decrease of the de- C01111111. Vield with decreasing time of contact is rapid only up to al;out r - 0.6, considerably slower vrith further in-1 crmsing r; the slopes of the lines giving the degree of de- j cornpn. as a function of temp. art. steeper the lower the r. I The catalytic effect of C on the decompn. of CC4 is I dcrnonstrated b) 2 runs without C: at r - 0.10 and 1.59, wt.-' -0 CCI. decompd. at 4(W, 6.0 and traces. at -,-00*. 36.0 and 15.0; the degree of decompn. reached at 500*14 i.,hc pmence of C is attained only at 700* in the absence of the catalyst. (3) The products of the thermal do.- com,yn of CCI. are Ch, C%Cl,, C~Clo. and C40.: at a lower temp. (400') more C,Cl. is farmed, w,%L- higher temp. (700) favors formation of C-Cla mid particularly j C.Ch. (4) Thermal dccompn. of C70, on acdve C in- creases nonlinecrly with temp.; at r - 0.20, 0_'13, 6.30, 0.33 g./min., the wt-% C,C14 decompil. was: at 500*. 12.3, 9.6. S.S. 4.3; at 600*, =_1, 17.3, 113.0, 124; atl 42.1. 39.S. 36.8, 26.0. The, products are Cl:, C-04, and CgCl,. (5) The catalytic effeet of SCh rn the formation of CC14 is due to the reactions 2SCls - S20. + C!:. 2S + C - C&~ SiCh - SCI, + S. and C-S, -4- 6CI; - CCI, + S-03. The mechanism of the thermal decompu. of CC14 6 represented by CCL - CI + CClj -CI + CCl- Cl + CCI C2Cl# C12 + C20. Ch + C 'C6 - C.C4.1 The assumed polymerization of the C~Cls into CC4 is in agreement with Ott ~Lnd Dit-us k C.A. 37,1 X. Than I Distr: 4E3c/4E3d 64 Tht first flullgariall etperiluellial fludev mdar. C. v. V e r I e Vol. 54), 1057, No. 10-- 7Q), 5 The reactor under crins,, rVict it pit it; Ill;, hills of l1licla- if 20M1 k%v. Tbs: max livit will 11.1ve u S is ~.10 161C. tile (I Mot"i", vm-4cc. 3hulerator mid reflector of tlv-- hutero- Iser sq getwVus ruactor collsint of 11,0. lyrallimil 110W eltricilml It to 10% ill UI:2 k villployed for Ind. Tile -2- YlinNricul heating clentents urv kirmllgcd 1-k 111111- Mill, C V J. dtm A hill churge of theactivezinte 6 practiculiv sufli- ' 11rs. 'I'lle s.14.11gli flud collslnl~timl (if cicut (or ~,Lvcrjjl the reactor, deta. of (lie saft-ty devick-1, olis-laticill of tile 111:111illulatori are puld-Attil lit detalh 1110slik-Ilk-lit Chuckill", alld Control (if ill. reactor llower lire effecteli with i"llizatiun civitalsers. All prembw-i frLAu which radioactive gases 1112), gaill ucccm to tile aft 31114.41 lic, Aelit ulidvr jisugutive pressure and a coukaut exchallgIci i. 'llu-, volume of air 'of :iir itust be stialtitaltied lit theto f.; f dischat It the 80 in Mack Is 95,4M h"I per lumr. throtil, _ CILUS. TUt litalth Of tile Staff WJU W proteeftd J.y spitt-111- doslusetric elleckups. According to -piatis HK atic reactor will tq put Into service at the end (if 1018 44 ~ V 0 it "Interaction of Nucleons Through a Mesonic Field,11 Byul. Polskoy Akad, nauk, otd- 3. lp No 3-4p 1953P pp 91-94 A method of an approximate solution of the equation of the mesonic field is given by expanding the resonic potential into series in inverse powers of velocity of light. It is applied to determination of interac- tion of nucleons within the frame of the classical meson -.1-heory. 'rhe po- tential of nucleonic interaction is derived from the law of conservafion of energy-nomentum. RZh Fizp No 3j 1955 VERLE, I. "'Equivalent' Potentials in ClEtssical '-EqLiations of Motion", (Theoretical Physics, Quantum Theory) Byull. Polsl-~y Akad. Nauk, Otd. III, No 7, 1953, -pp 281-285 AbB W-31146~ 1 Feb 55 VIRLA. 1. 1. New approach to the -problem of the effects of relativistic terms in the meson theory of nuclear forces. Xhur.eksp. I teor. fis. 25 no.1:19-35 Js 153. (KLR& 7:10) (Mesons) (Nuclear forces) (Yield theory) USSR audeqns. The etnerm tvr~tzr- mcceaulty aprfied In q;rA=mn mechaiiki A:Ur-!i ivy" poz(ble. tmw approach to the VvWvr, of tic dcuteran (2 bodkis)