SCIENTIFIC ABSTRACT SOLNTSEV, N.A. - SOLNTSEV, V.P.

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• Collection: Scientific Abstracts
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• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 25, 2000
• Sequence Number: 14
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

N.A., red.
klomprehonsive FeDgraphicall stu-,'-ie.-; in the Za,-a.,,lk reglon
Mooccrw "rovince) Kor.1,1ek-snyo issletiovanf-*fa
v 2amji:jkor ralone 1-:onkov2koi oblustl. ".'oskvn. f-"osk. k;os.
unIv. ".V.:.raonosovi&, 11961. 32 p. ("'A;fA 1'7:F.)

3OLNTSEV, N.A.
Organizing landform expeditions and caleulating field work
norms. Vest. Moak. un. Ser-5: Geog. noo2:69-71 Mr-Ap 161.
(MIRA 14:4)
(landforms)(Physical geography-Research)
IL@ *
.1.

m
VIDIVA, A.A.; SOUITSEV, N.A.; TSESELICHIM, Yu.N.
The Kasimov "opolle.ft Vast. Mosk. un. Ser. 5:71-74 My-je 161.
(MMA 14: 5)
(Kasimov District-Physical geography)

A . A SoIntsev, N. A.)
Some additional and more preciBe elucidationa in the problem of
landacape morpholog7. Analele geol geogr 15 no./.:82-87 O-D 161.
(Phyaical geograpby)

SOLNTSEV, N.A.
Some supplements and more precise definitions in the field of
landform. morphology, Vest. Mosk. un. Ser. 5: Geog. 16 no-3:53-
57 MY-Je 161. (MMA 14:5)
1. Laboratoriya landshaftovedeniya Moskovskogo gosudaretvennogo
universiteta.
(Landforms)

SOLNTSEV, N.A.
-------------------
fttura.1-geographical regions of Moscow Province. Vopegeog. no*31s
5-19 1619 (mA l4s6)
(MoscoiO -Province-"ical geography)

,DAUHKIN, Yi.,.; 60ATOOV, N.; SOLCV'Yr;V, A.
6oviet gacgraphers-hydrologists are asked a question. Izv. Voes.
geog. ob-va @3 no.4:375-376 Jl - Ag 161. (MIRA 14:7)
(Hydrology)

'11L;JNA, A.A.; ScLNTSEV, N.A., red.
(Met@odological instructions for large-scale field studies
of land characteristics for agricultural purposes in the
central part of the East European Plain]Metodicheskie uka-
zaniia po polev@,-.m krupnomasshtabnym landshaftnym issledova-
niiam; dlia tselei sellskokhoziaistvennogo proizvodstva v
srednei polose Russkoi ravriny. Pod red. N.A.SoIntseva.
(MIRA 16:2)
Yosk. gos.unlv., 1962. 119 p.
(East European Plain--Agriculture-Maps)

SOLNTSEV, N.A.
11 ------
Hain problems of Soviet landform studies. Izv. Vaes. geog,
ob-va 94 no.1:3-14 Ja-F 162. (KIRA 150)
(Landforms)

SOLNTSEVP N.A.
Amplitudes of the rhythm of natural phenomena in a lawWbrm.
Vest. Moak. un., Ser. 5z Geog. 17 no.6:63-67 H-D '620' (KUU 16:1)
1. Laboratoriya landshaftovedeniya, geograficheskiy fakulltet
Moskovskogo gosudarstvenn*d universiteta.
(Landforms)

GV,JZDETSKIY, N.A., prof.; ZHUGHKOVA, V.K., dots.; ALISOV, B.P., prof.;
VASILIYEVA, I.V., dots.; VARLAMOVA, M.N., tekhnik-kartograf;
WLGOVA, L.S., dots.; ZVORYKIN, K.V., st. nauchnyy sotr.;
ZEMTSOVA, A.I., assistant; IVANOVA, T.N.; LEBEDEV, N.P.9 at.
prepodavatell; LYUBUSHKINA, S.G.; NESMEYANOVA, G.Ya., mlad.
nauchnyy sotr.; PASHKANG, K.V., at. prepod.; POLTARAUS,B.V.,
dots.; RYCHAGOV, G.I., at. prepod.; SPIRIDONOV, A.I., clots.;
SPIRNOVA, Ye.D., mlad. nauchnyy sotr.; SOLSTSEV, N.A.0 dots.;
FEWROVA) I.S.J. mled. nauchnyy sotr.; MTSU-ICH@K-, M.N.,
mlad. nauchnyy sotr.; SHOST'INA, A.A., *lad. nauchnyy sotr.;
Prinimali uchaotiye: BELOUSOVA, N.I.; GOLOVINA, N.N.;
XALASHNIKOVA, V.I.; KOZWVA, L,V.; KARTASHOVA., T.N.;
PANIKOVA@ L.I.; URKIKHO, V.; PETROVA,./K.A., red.; LOPATINA,
L.I., red.; YERMAKOV, M.S., tekhn. red.
[Physicogeographical regionalization of the non-Chernozem
center] Fiziko-geograficheskoe raionirovanie nechernfzemnogo
tsentra. Pod red. N.A.Gvozdetakogo i V.K.Zhuchkovoi. Moskva,
Izd-vo Mosk. univ., 1963. 450 p. (MIRA 16:5)
(Physical geography)

SOLNTSBIV) N.A.
Some theoretical problems in I - dTaamico. Vest. Moak. un. Ser.
5:Geog. 18 no.2.50-55 Mr-Ap 163. - -' (MIRA 16:3)
1. Laboratoriya landshaftoveden*& Moskovskogo gosudarstve=ogo
uaiversiteta.
(Tand ozus)

SOLNTSEV, N.A.
Aleksandr Aleksandrovich Borzov's theoretical views. Vest. Mosk.
un. Ser. 5: Geog. 19 no.2:12-16 Mr-Ap 164. (MIRA 17:4)
1. Kafedra fizicheskoy geografii SSSR Moskovskogo univarsiteta.

IS,@dCIT-3FOt A.G.; !I.A,.
Vj'j.-Wr BorisarlCb SOdnV4# 3.905- ; on hie &lb birth6my.
Vczyt.YWk,un.."lor*5: Gooee 20 nno4tw., jL-Ag 165. (!"If%h JC312)

ffYABClll-K(YV A.M., prof., SHCHUKINp I.S.; SAUSHKIN, Yu.G., prof.;
GVOZDETSYIY, N.A.; MARKOV, K.K.; ANUCHIN, V.A.; SOLNTSFV,
A.A.1 doktor geogr. nauk
Senior Soviet Geographer;1875- ; 90th birthday of Aleksandr
Nikolaevich Dzhavakhlshvili. Vest. Moak. un. Ser. 51 Geog.
20 no.5:82 S-0 165. (MIRA lPil2)

614MU
Aphle
09pper-Coutainfax Jdac virodawon v
the sep4ration ol copw by mftq of W
and (Nogyanall, N., 1, 50intley. E
na anti I.,
(,Vj, A.51.157TIM5,11-11, 0,119
Ii a, .1 4ay. 95@.
325-330: R,-f. 2Aidr.. Kht"j., 1956, Abstr, 'NO. 7092.
-Re polarographic determination of Cd in samplei
of -= r-containing materials from zinc production
@ p
is d bed with yarioui methods of separation of
Cu siter decomposition by vlua regiA and HISO,,
It was found that polarographic determinatiGa of
Cd can be carried out with a sufficient degree of
accuracy by separating Cu by means of thiosulphate
and thiocyanate. R. Loko

SOV/137-57-1-1619
T@anslation from: Referativnyy zhurnal. Metallurgiya, 1957, Nr 1, p 215 (USSR)
AUTHORS: Troitskaya, M. I., Polyakova, V. V., Solntsev, N. I., Filippova,N.A
T rr L E: Orgarization of Analytical Work at the Gintsvetmet [State Institute
for Nonferrous Metals I - Results of Work During the Last Five
Years (Organizatsiya analiticheskoy raboty v Gintsvetmete. Itogi
raboty za posledneye pyatiletiye)
PERIODICAL: Sb. nauch. tr. Gos.n@i- in-t tsvet. met., 1956, Nr 12, pp 5-13
ABSTRACT: The Gintsvetmet [State Institute for Nonferrous Metals] has three
laboratories: One for chemical analysis, one for physical methods
of investigation, and one for the study of the material composition.
An account is made of the nature of the work of these laboratories
in the analysis of raw ores, the middlings, and pure metals.
N. G.
Card 1/1

LT I
ell
!':!4:1@ Alm I 7'5r;,:,s -kh Xlrt.- i' Prodkklov O-A
1-1, .. jnh.tw uvial;@,cs :, I . 4".. @,!, I
@,f @-AVtnt:,. %ut@rio ite(l),
are
tinite (11), (M), aijA hyttrwncite (IV) were
Investi T'he tke@;t 3,@Ieetivc: ull-icats (@,uud sverc 1.6N
tabn InVi
0 (JARN NLI@- V 6&,Aved only It.
. .1
llll@ 1.9 but not M md I ii dc"d. bdf,ectly

7
C
J@
-ZThe simp(Wiadiation o' -ae-p a-@Httla'n-c&
f
lchlaVt@lnd determination of 11 r- A
by a
'Gm-Re -@' 'F Ru'l I -4@ykh
etbod. N 1, Solnt,et
I g A dw't "Jutg rk"O" Sb and Ai in to a
I I,, V'@iulnctrlc flxsk, add 2 g 'anhyd- NL13@k)4 apd 15
rn 1 (1-94), and heat gradually to fumes of i0s.
'I bell,--er 011 flaik witha funnel and h"t until deenh- r tioij
of the triixt@ To the colorlens ni-
z'g
-IT20- ana-licat -10min. to removc- SO,. -Then to the wol- - -
soln. cont g. 12N HSO4, add 3 g. tartarie acid, 3 g. NaCl
1,arid 1.5 ml, 11C1 (I.N). Put the flask an a sand hat i at
F 55--60' and beat for 3 hrs. @Vtcr adding W-70 ml. JJtO.
licat to 70' and titrate with 0.5N KDr0s (indicator ruethyl
orange). The mahod is basi!d on the tvolotiun 6f As as
-IsCl. at 55-60'. Curves of the rate of evolution of AxClj
at diffurent conditions are preszntN1, N. C.

SOVI,, 137-58-8-18101
Trans lation I rom: Ref e rati vnyy zhurnal, Metallur8iya, 1958, Nr 8, p 270 (USSR)
AUTHORS: SoIntsev, N. 1. , Chudina, R. I.
T IT LE: Application of Polarography in the Phase Analysis of Ores and
Their Conc@ntrates for Lead Compounds (Primeneniye polyaro-
grafii pri fazovom analize rud i produktov ikh obogashcheniya
na soyedineniya svintsa)
PERIODICAL: Sb. natichn. tr. Gos. n. -i. in-t tsvetn. met. , 1958, Nr 14,
pp 80-92
Atis'rRACT: In the phase analysis of ores and their concentrates, 15 -
257o solutions of various salts are used as selective solvents.
Taking into account the volume of the solvent and the wash
waters, the optimum conditions for the polarographic deter-
mination of all forms of Pb are created directly in the solution
obtained. The records are adduced of the determination of the
total contents of Fb and of the determination of Pb in the form
of anglesite, cerussite, galenite, and also Pb in the case of
the presence of crocoite and wulfenite, pyromorphite, and
vanadinite; pyrornorphite, mimetisite, crocoite and wulfenite;
Card 112 plumbojarosite, bieberite, and bedanite. The results of the

SOV/137-58-8-18101
Application of Polarography in the Phase Analysis (cont. )
determinations of various forms of Pb are added up and compared to the total
Pb contents. The discrepancy should not exceed 100/0.
N. G.
1. Orco-Amlysis 2. Lead-Datfmination
3. Fol-arog-raphic anLly--Is
Card 21Z

SOV/1 37-58-8-18108
Translation f rom: Referativnyy zhUrnal, Metallurgiya, 1958, Nr 8, p 271 (USSR)
AUTHOR: SoIntsev, N. 1. , @_-hudina, 11. 1.
TFFLE: Employment of Amperometry in the Phase Analysis of Ores and
Concentrates for Zinc Compounds 'Primeneniye arnperometrii
pri fazovom analize rud i produktov obogashcheniya na soyedine-
niya tsinka)
PERIODICAL: Sb. nauchn. tr. Gos. n. -i. tsvetn. met. , 1958, Nr 14,
pp 103-111
ABSTRACT: The possibility is indicated of the determination of Zn com-
pounds in the products of phase analysis with the aid of the am-
perometric titration of Zn with a solution of ferrocyanide with
a Pt anode. The titration is carried out in an ammonium- acetate
medium in the presence of Pb, Cu, and small quantities of Fe.
Cu is combined into an ammoniacal and Pb into an acetate com-
pound. Fe oxide is quantitatively precipitated in the form of the
hydroxide (basic salt) which does not react with the ferrocyanide.
If Fe is present in large amounts, the titration is carried out in
an ammonium citrate medium wherein Fe is combined into a
Card I /Z stable citrate compound. The anodic polarization of the indicator

SOV/1 37-58-8-18108
Employment of An-iperometry in the Phase Analysis of Ores (cont. )
electrode during amperometric titration permits the determination of Zn in
the prest-nce of a vanadtte ion which does not produce any anodic reaction.
Gr likewise does not produce any electrode reaction on the anode and does not
impede the titration of Zn. The amperometric determination of Zn in ores
reduces the duration of a phase analysis considerably. Methods are adduced
for the determination of the total Zri content and for the Zn contents of adamine
and calamine, of smithsonite, descloizite, sphaterite, calamine and smithsonite
and Zn in the insoluble residue.
A. M.
1. Zinc compounds-Determinaticn 2. Zinc ores-
Vol=ctrie analysis
C a r d 2/2

SOV/1 37-58-8-18090
Trans fat ion f rom: Ref e rativnyy zhurnal, MetalItirgiya, 1958. Nr8, p268(USSR)
AUTHORS: SoIntsev, N. 1. , Leont' yeva, K. D.
TITLE-, Analysis of the Phases of Tungsten Ores and Concentrates
(Fazovyy analiz vollframovykh rud i kontsentratov)
PERIODICAL: Sb. nauchn. tr. Gos. n. -i. in-t tsvetn. met. , 1958, Nr 14,
pp 155-168
ABSTRACT: A method of phase analysis is described which permits one to
determine separately the W of tungstite, scheelite, wolframite,
and hubnerite. The weighted test sample is treated with NH 40H
(sp gr 0. 91) at 600C during 4 hours agd filtered. After the re-
moval of NH3 by boiling and using Ti+as a reducing agent the
tungstite W in the solution is determined photocolorimetrically
with rhodanide. The residue is again dissolved in I -N H?CZ04
solution at 200 during 2 hours and filtered. In the solution
scheelite W is determined gravimetrically after decomposing
HZC10, with return aqua regia or colorimetrically in oxalic-
acid slition. The residue is treated for 20 min with Z.4-N
HCI solution at 1000 and filtered. In the solution the hu"brierite
Card 1/2 or wolframite W is determined. If both minerals are present

SOV/1 37-58-8-18090
Analysis of the Ph4ses of Tungsten Ores (cont.
then the ratio of the W minerals is determined according to a graph and the
W contents of each of them is calculated. In the insoluble residue the re-
maining W is determined. It is indicated that in minerals in which both
hu"bnerite and wolframite are present the precision of the determination of
each of these minerals is decreased.
A. M.
1. Timgsten ores-Analysis 2. Tungsten-Determination
Card 212

SOLUTSEV.0 NIII
Determining oxidized copper bound vith minerals of enclosing
rooks. Sbor. nauoh. trud. Gintsvetmeta no.18t104-108 161,
(KEU 16:7)
(Copper ores--4,.nalyBis)

SOLMISFIVY N.I.; CHUDIM, R.I.; XULICHIMINA, R.D.
Determination of chryaocolla copper. Sbor, nauch. trud,
Gintavotmeta no.18:109-117 161. (MIRA 16-.7)
(Tailings (Metallurgy) -Analysis)
(Copper,knalysis)

SOLNTSEV, N.I.; CHUDINA, R.I.; SAVIVA, Ye,V.; KULICHIMIMA, R.D.
Phase constitution of molybdenum-bearing precipitates obtained
from molybdate solutions by reduction with hydrogen. Sbor.
nauch. trud. Gintsvetmeta no.l8zl55-164 161. (1-aM 16:7)
(@1olybdenum,-MetaUurgy)
(Vapor.-liquid equilibrium)

SOLNTSEVY N.I.; CHUDINA., R.I.
Chemical phase a Alysis of alkali melts for lead compounds.
Sbor. nauch. trU3. Gintavatmeta no.19:750-755 162.
(MIRA 16:7)
Alkalies-Analyois)
Iead compounds-Analyoie)
@

SOLNTSEV, NJ*; USOVA, L.V.
Separate determination of copper,, chalcocitep and bornite
in ores; oone investigations with digenite and betakhtinite.
Sbor. nauch. trud. Gintsvetmeta no.19:756-772 162,
(MIFLA 16:7)
(Copper ores-Analysis)

O.A.: KUSMAIMIA, T. 1.
TimAn-Pechora area. ?rudy VNIGRI !r7.
(Timai Ridge--GeoLorj) (Fenhira Y,"

LNTSEV, O.A.
l4otamorphic achits. Trudy VITIGRI no.133:5-18 '59-
(MIR& 13:1)
(Timan Ridge-Schists)

DFIRNSIP."@,V'i M.A,, Yp*,LG",NIY-.Ctl,.'.- liTi"EV. N,A.-, SOLNTSEV
J- O,A.
I
Prc&;@e@;tn for ttie devt@l.);,nert. c-' the gas drid cll !ndustries of
1-te A-S.S.F. NefL@ khc3. .3 nc.,IA34-19 Mr 165.
(MIRA 2,M)

MAT
174 M
.1w
afl,

1201-2-9/10
AUTHCR: Mishkevich, R.I.2 Candidate of Technical Sciences,
-__S_olntsev P.I., Eng., and Smirnov, A.V. Dr. of Technical
Sciences.
TITLE: Low Temperature Nitriding of Structural Steel. (Nizkotemperturnoye
azotirovaniye konstruktaionnoy stali).
PERIODICAL: Metallovedenle I obrabotka metallov, 1957, No. 2, PP. 49-54
Ms.S.R@)
ABSTRACT: The experimental work was carTied out by engineer R.V. Chudnovskaya
and four assistants. The authors Investigated the possibi;ity
of utilsing a nitriding p=-t@ess at a tempeisture below 400 C.
As a result to the experiments described a low temperature catalytic
process of nitriding at 380:1C (.60 to 80 hours) and 4300C (24 hours)
was developed which permits obtaining a Rockwell C hardness of 42 to
50 on structural alloy steel for a layer depth of 0.20 to 0.25 mm;
there is a steep decrease in the hardness from the surface towards
the core. By using the n1triding processes described here, the
development of Type II temper brittleness In nitrided components is
eliminated and the obtained nitrided layer is free of any brittleness
Card 113 usually encountered on suzh layers In 38Amio.A steel. The process

129-2-9/10
TITLE: Low Temperature Nitriding of Structural Steel. (N.lzkotemperturnoye
azotir-ovan:Lye konstrukt@5ionnoy s,@ali).
described here Is jSrA in a nLmber of Soviet factories and two of
the 3uthors of this paper have an tauthor's certificate" for this
process. Fig. 2 gives the change of the hardness and depth of the
nitrided layer as a fun!,tion of nitriding processes (380 430 and
4900C with catalysts ard 530 and 5800C without eatalystsi for four
different steels. Fig. 3 gives the change of the micro-hardness along
the cross section of the nitrided layer as a function of the nitriding
process for 35XM steel for equal nitriding processes. Table I con-
tains literary data on changes of c;' zrtain parameters during the
reactions. Table 2 gives the Cr content with depth of the nitrided
layer for the 35XH3M steel. Table 3 give3 hardness of the nitrided
layer in the 135N scale as a fwn,:tion of the temperature and the
holding time duzring nitriding.
The text Includes 4 sets of graphs, and 3 tables. There are 5
Card 2/3 references, all Russian.

129-2-9/10
TITLE: Low Temperature Nitriding of Structural Steel. (Nizkotemparaturnoye
azotirovaniye konstruktsionnoy stali).
ASSOCIATION: -
PRESENTED BY: --
SUBMITTED:
AVAILABLE: Library of Co%ress
Card 313

PETROV, A.K.; SPIMUSKIY, V.G.; KHIZHNICHMO, A.M.; SHILYAYNT, B.A.;
DANILOV, A.K.; BGRODULIN, G.M.; ZAMOTAYEV, S.P.; MARXARYANTS, A.A.;
SOIMSW,, P.I.; SKIRNO7, Yu.D.; VAYNBIRG, G.S.; CKCIROKOV, N.V.;
KOLOSOV, M.I.; MIKIN, G.S.; MWOVAR, B.L; IATASH, Tu.D.;
TWRO'YMOVIGH, Tu.Te.; VINOGRADOV, V.M.; SVXDFr-mv S, N.N.;
SKOROXHOD, S,D.; KATSIIVICH, L.S.; SMOMBERG, Ta.A.; MIUUYIOVO
O.A.; PATON, B.Ye.
Reports (brief annotations). Biul. TSNIIGHX no.18/19t67-68 '57.
(MIRA 11:4)
1. Zavod Ikeprospetsatall (for Speranskiy, Borodulin). 2. Chelyabiu@
skly metallurgichookiy zavod (for Xhizhuichenko). 3. Uralmashzavod
(for Zamotavev). 4. Treat "Xlektropechl" (for I'aynberg). 5. Noskov-
skiy inatitut stali (for Okorokov). 6. TSentral'MT nauchno-iasledo-
vatellskiy Inatitat ahernoy metallurgii (for Sellkin, Syede-Shyets).
7. Institut elektroavarki AN USSR (for Paton, Madovar, lata'sh).
8. TSentrallnaya laboratoriya avtomatiki (for Yafroymovich,
Vinogradov). 9. Gieogneupor (for Skorokhod). 10. Treat "ZLektropechl*
(for KELtsevich). 11. Thilisskiy na=hn@>-issledovatellekly institnt
okhrany truda Toesoyamogo teentralltago soveta profsoyuzov (for
Shtromberg).
(Steel-Metallurg7)

SOV/ 137-58-7-14457
Translation from: Referativnyy zhurnal, Metallurgiya, 1958, Nr7, p75 (USSR)
AUTHORS: Markaryants, A.A., Solntsev, P.I., Smirnov, Yu.D.
_77PA
TITLE: Degasification of Steel Under Vacuum in the Manufacture of
Forgings (Degazatsiya stali pod razrezheniyem pri proiz-
vodstve pokovok)
PERIODICAL: Trudy Nauchno-tekhnicheskogo obshchestva chernoy metal-
lurgii, 1957, Vol 18, pp 582-591
ABSTRACT: The degasification of 34KhN3MF steel was accomplished by
means of pouring the molten metal from one ladle into another
under vacuum; 6 to 7.5 minutes were required to transfer 20-22
tons of metal. The vacuum apparatus was composed of a cham-
ber with an intermediate casting device, a heat exchanger
equipped with a filter, three vacuum pumps, and three reserve
containers for the creation of preliminary vacuum as well as
for accelerated removal of gases. Ingots weighing 18.9 and
13.4 tons, made of steel the properties of which it was desired
to investigate, were converted into rotor-type forgings. The
macrostructure of the latter exhibited no peculiarities what-
Card 1/2 ever. Compared with stock prepared from regular ingots, the

SOV/ 137-58-7- 14457
Degasification of Steel Under Vacuum in the Manufacture of Forgings
overall quality of the plastic properties of metal in the internal zones of
forgings prepared from vacuum-treated ingots was significantly higher. The
influence of the vacuum is most apparent in the magnitude of relative shrink-
age. Vacuum degasification of steel reduces the harmful effects of hydrogen,
and its employment is advisable when it is desired to effect a leveling of
plastic properties of the metal without resorting to protracted periods of
tempering.
Ye.K.
1. Steel--Forging 2. Steel--Degasification 3. Vacuum systems--Applications
Card 2/2

SOLNTSEV, P.I.; GERSHKOVICH, V.I.
Durability of press mold plates during the press molding of
grog products. Ogneupory 27 no-3:120-126 '62. (MIRA 15:3)
1. Leningradakiy korablestroitel'nyy institut (for Solntsev).
2. Borovichskiy kombinat ogneuperov (for Gershkovich).
(Plates, Iron and 3teel--Testing) (Refractory materials)

SO ki
-> r PHASE I BOOK EXPLOITATION SOV/6162
Trubin, V. N., Candidate of Technical Sciences, and 1. Ya. Tarnovakiy,
Dpator of Technical Sciences, eds.
Kovka krupnykh pokovok; rezulltaty Issledovaniya tekhnologicheakikh
rezhimov (Production of Heavy Forgings; Results of a Study of
Technological Methods). Moscow, MashgIz, 1962. 223 P. 3800
copies printed.
Reviewer: 0. A. Ganago, Candidate of Technical Sciences; Tech. Ed.s
N. A. Dugina; Executive Ed. of Ural-Siberian Department ()hshgiz)3
H. L. Kolosova, Engineer.
PURPOSEs This book Is intended for engineering personnel of forging
shops and engineering and design offices at heavy-machinery plants,
as well as for those working In sclentIflo-research and planning
organizations. It may also be useful to students at higher educa-
tional establishments.
Card 1/6

Production of Heavy ForgIngs; (Cont.) sov/'6162
COVE-RA#13: The book reviews te@.hnological problems of forging large
steel ingota. The effeat of reduction and conditions of deforma-
tion on the quality of r@rgings is discussed on the basis of re-
searoh work done at heavy-machinery plants of the USSR. The book
offers practical suggestions on Improving the.quallty of large
forgings and reducing the amount of labor required to produce
them. I. Ya. Chemlkhova,.V. 1. Tarnovskly, and-V. P. Bakharev
4,-ook.part In prokpar.ing the copy for publication'. 'There,ake-193 ref-
erences, mostly Soviet.
TABLE OF CONTWM:
Foreword
3
Ch. I. Effect of Tei@hnological Parameters of Forging
on the Quality of Forging* 5
Deformations and stresses during drawing and up-
settin operations (Tarnovskly, I* Yee, and Ve No
Trubini 5
card 2/6

Pioduction of Heavy Forgings; (Cont.)
Forging of 3@-ton �ngots (.Nwxmenko, V. G., and D. I.
Fillmonov
Optimum reductlors In forging 5- to 35-ton ingots
Ch. III. Changes in Metal QLallty Occurring During the
.awing of Differently Shaped Stractural
Alloy-Steel Ingots
General. prInciples
Forging of long in ots (3-5, 6.9., and 10.8 tons) of
361[h]N-3.W. qtee'L @Brpnmbn, M. I., and(,-P-1. L SoIntsev.)
Forging of dIfferently sYsapsd 6.-g-ton 361chil3ff-steel'
Ingots (Brenman, M. I., ankP. 1. Solntsev)
For Ing of large (up to 42 toni-y-a-1167- steel:- ingots
tGuilubyat-nikov, N. K.)
Optlyttiza r&duction In forging alloy-steel ingots
Ch. IT. Kffect oil' Upsetting on the Quality of Forgings
Basle prln-Aples
sov/6162
92
102
104
104
107
124
136
143
145
145
Card 4/6

ACC NR, AT6036655
SOURCE COD E: UR/0000/66/000/000/0282/0283
WVOR: tJozzhukhin, A. S.; Kuznotsov, V. I.; Nushakova k'aya, 14. S.; Ffakhalova# 09919
.@@@@@@@Shostak, V. I.;Kudrin, 1. V.
ORG: none
TITLE: Elfcct of radioprotoctive drilgs on the functional condition of the human
organism Z@aper presented at the Conference on Problems Of Space I*dlcine hold In
Nascow irom 24-27 ray 19667
SOURCE: Konforentsiya po problemam kosmicheskoy maditsiny, 1966. Problemy
kosmichaskoy meditsiny. (Problems of space medicine); materialy konferentsil,
1;0scowl, 1966, 282-283
TO-.11C TAGS: radiation protection, space phamtcology, cosmie'radistion biolost.0
effect, human physiology, space medicine, motion sickness
ABSTRACT.
The eff*eCt of cystamine on the functional 4iondition of the human'oiganism
iwas studied On the the basis of the hypothesis of A. V. Lebedinskiy). Five
hundred heathyvolunteers were used. The maximum permissible dose of
cystamine was established as a dose of 1.2 [units not given) per single appli-
i cation, or 0.8 units every 6 hr for 24 hr, or 0.6-0.8 units once a day for a
1 month. Adminisiration of cystamine in the doses indicated did not cause
any qWnificAnt ch.ange@s in.work capacity, 'hematopoiesis,. or. in cardiovascu-
Card

ACC NRI AT6036655
Ilar, respiratory, digestive, excretory, or'nervous system function. How-
ever, administration of cystamine did lead to complaints of lethargy and
brief unpleasant sensations In the epigastrium in 1016 of the cases, After
-administration of the drug some increase in sensitivity to motion sickness
and to the effect of hig1j;I.Mperatures was noted among.
jCW. A. No. 22; AMD Report 66-116jl
SUB COM 06 SUBm IDAISS ~6
Card 2/2
v

[Rural conotructi@ln jr, the Virgin TerritO-Yl Sallskoe
,troitellstvl) Stroilzdat) 1964.
89 F - (MIRA 1,7:9)

- SomiTSEV, S.S.
We shall meet the 22d Congress of the CPSU with high production
indexes. Gidroliz. i lesokhim. prom. 14 no.6:18-19 161.
(MIRA 14: 01 )
1. Khorskiy gidraliznyy zavod,
(Khor-flydrolysis)

LOKSBIN., S.V., inzh.; SOLIMV, S.V., inzh.; TANYGIN, B.S.. inzh.
Tower cranes made of standardized unitoo 1,%kh, etroit 19
no.8:16-18 Ag 162, (KmA 16--7)
(Granes.0 Derricks., Etc*)

IVANOY, Boris Nikolayovich; TKALIN, Ivan Hikhaylovich; SOLNTSXV. Vyacheelav
Aleksandrovich; SHTRUM, Viktor Livovich; SWYDV,--R-omn-Izrayie@@
vi-CE--,--WAYAHGXIY, losif Isaakovich; BORISOVA, Volya Petrovna; ARUTYIJ-
NOV, V.O., retsenzent; BUkIMITM, L.I., red.; SOBOIRVA, Ye.K.,
takhn.red.
[Technology of the manufacture
&-iia eloktropriborostroaniia.
590 P.
of electric instrumentel Tekhnolo-
Moskva, Goe.enorg.12d-vo, 1959.
(MIRA 13:4)
(Electric apparatus and appliances)

L @L2,@p-66 an Fwp (j wK=, gm
___
4R; AP6026152 SOURCE CODE: UR/0076/66/040/007/1650/1652
AUTHOR: Shirokikh,_P. K.; Bystrov, V. M.1 Ponomarev, V. V. SoIntsev
V. A.
ORG: Moscow University im. H. V. Lomonosovs Chemistry Department 11@
ftskovskiy gosudarstvennyy universitet, Khimicheskiy fakul'tet)
TITLE: Heats of combustion and enthalvieslof formation of some
acetylenic aminesI I
SOURCE: Zhurnal fizicheskoy khimii, v. 40, no. 7, 1966, 1650-1652
TOPIC TAGSi acetylanic amine, heat of combustion, enthalpy of forms,
ABSTRACT: The authors have prepared high-purity samples of the fol-
lowing acetylenic aminess
ClImOCIVII,
C11-OC112N(G113)2
(C11-CC11z)gNC113
(C11-CCH2)3N
C112-C11CMCCH2N(C113)3
(C113)2NC11xC-CC11jN(C11s))
The heats of combustion of these amines"were determined calorimetrically
by a procedure described -in the source. The values of the heats of
COM VDC; 541.11

L 4LZo-66
ACC NRs AP6026152
P Table 1.
Card_,3L/,<
I-AU, cal7g.' j
compoun.
U JV- const; I- 293t

910,7
9105,3

Average 911n,4�3,6

QUON "16.7

9914,0

CATION 10040,5
10017,8

-AH,
10044, t
combustion (after the necessary,,
correction:) and the calculatpd
values of ntha-1pies of forma-
tion of the amines are@given
in Table 1. The calculation
procedure is.explained in the
source. Orig, art. hast
2 tables. JBOJ
kcal/mol. Wformkcal/mol
)-cowt.T-2M.16C 'T - 293.16C
502,2�0,2 49,2�0,2
=,01.0,4 .41,1�0,4
t077,4:k0,3 111,4�0,3

C604
SOV/ 14 1-1-5 -6-.18/ 28
AUTHORS: Solntsev, V.A. and Tager, A.S.
TITLE: Theory of the Interaction of Two Electron Beams Moving in
a Periodic Electrostatic Field
PERIODICAL: Izvestiya vysshikh uchebnykh zavedenly, Radiofizika,
1958, Vol 1. Nr 5-.6, pp 127 - 138 (USSR)
ABSTRACT: The problem discussed was partly investigated by the
authors in two earlier %forks (Refs I and 2). The
analysis given is carried out under the following
assumptions: 1) the electron trajectories are recti-
linear; 2) the constant component of the electron space
charge is compensated by ions; 3) the excitation of the
higher-order space charge waves in the beam is neglected
and, 4) both beams are of the single-velocity type.
The two electron beams are fully intermixed and move
along the axlj@ z with velocit ies
VW W and -v (2) W- the velocities change with a
period L . This ch.@@ge of velocities can be secured
by employing a periodic electrostatic field. The
C-ardl/5 equations of the high-frequency components of the current

U647h
sov/14l-1-5-6-18/28
Theory of the Interaction of Two Electron Beams Moving in a Periodic
Electrostatic Field
densities i(l) and 1 (2) in the two beams are described
by (see Refs I and 2):
d2 1(1,2) W di(1,2) W2
+ 2j
dz2 v(1,2) dz (V(1,2))2 (4)
1 dv (1,2) W .(1,2) dl(1,2) jwj (1,2)a
+- = J V(102)x -14- - E(z)
V(1,2) dz dz ) (v(112))3
where E(z) Is the longitudinal componer-t of the high-
frequency field, J Is the constant component of the
current density and I = e/m . The solution of Eq (4)
is in the form of Eq (6), where y denotes the propagation
constant for the zero space harmonic of the current. By
Card2/5 introducing new variables, defined by Eq (7), Eq (4) can be

06471:
SOV/l41_.l-5_6_i8/28
Theory of the Interaction of Two Electron Beams )Wving in a Periodic
Electrostatic Field
written@ as Eq (8). The integratlon of this leads to
Eq (9). The solution of this is in the form of Eq (10).
On the other hand, Eq (6) may be written as Eq (11).
Now, Eq (9) can be solved in terms of the series defined
by Zqs (12) and (13), where r' k and ra k are given by
Eqs (13a) and (13e,)* By substituting the series of Eqs (11)
and (13) into Eq (9) and carrying out the Integration. ali
infinite system of I-Lnear alge@fflc equatWs is obtained.
These relate the amplitudes cn and c n- and are given
by Eqs (15). If the systcao is to give sIgnIfIcant solutions,
its determinant should be equal to zero, as defined by
Eq (16). This represents a genexal equation of the
dispersion of two intermixed electron beams. If the space
charge is compwatively small-, the system obeys Eqs (18)
-nd (19). The dispersion equation is, thex-*Ifore, given
by Eq (20). If the avexage plasma f-requencies of the waves
in the beams are equal, Eq (20) is represented by Eq (22);
Card3/5 the solution of this is in the form of Eq (23). The solution

C6h7h
SOV/141--l-5.,6-18/28
Theory of the Interaction of Two Electron Beams Moving in a Periodic
Electrostatic Field
is plotted in Figure 2 for various values of a_, The
relative width of the interaction bands is given by
Eq (24a). On the other hand., the maximum amplification
in db per unit length of the beam is expressed by
Eq (26a). Eqs (24) and (26) show that the efficiency of
the interaction of the electron beams depends on the
coefficients a. . It is shown in the appendix to the
paper that the coefficient a. . for a system with sinusoi-
dally varying electrostatic potential, is given by Eq (28),
where yS is defined by Eq (29). On the other hand,@for
an electrostatic system with a stepwise change of the
potential (Figure 4), ak is given by Eq (30), where
YC is defined by Eq (31). The dependence of a k on tpc
is illustrated in Figure 5. Normally, the spread of the
electron velocities (which was not taken into account in
Card4/5 the above analysis) has a considerable influence on the

C-6474
S OV/ 14 1-1 6 -18/ 28
Theory of the Interaction of Two Electron Beams Moving in a Periodic
'@lectrostatic Field
characteristics of a two-beam tube. ThIs effect can be
evaluated approximately (M.I@ Rodak - Ref 6). The electron
velocity distribution function is given by Eq (32), where
N 4notes the density of the electrons, while v T is a
parameter characterising the spread of the electron
veloclties@ The dispersion equation for vT can be
written as Eq (33). On the basts of the above analysis,
it is concluded that the introduction of a periodic change
in the velocity of the electrons in a two-beam tube leads
to the appearance of the higher-order interaction regions;
these regions lie in the vicinity of the frequeucies which
are practically independent of the magnitude of the space
charge of the beam. There are 5 figures and 7 references,
of which 3 are English and 4 Soviet.
SUBMITTED: May 12, 1958
Card 5/5

AVTBM a Golutkov, P.T. and Tolarizig. ek. To.
TITUS tb*,S*con4 All-Valon OoAfore=o an Radivelectranics, of
11 Miastry of Eightr Iducation, of the UM (Vtoraym
I.:Ooyuxza,y& konferontolys XTO SM po radloslek%realks)
Seem Ites
2CUOMCALs ladlotekh-1k, I Slokltrownm, 1958, *1 3. ar
pp 440 - 4" (usa)
ADSTRACTi The canforonc* %oak ploce during September 23 ;t29. 1957.
at S&ratov@Alj gowu6aretvanczy univeraltes Los
X:G: Chorzysbovskago (Saratav Bta%o University laosL
XG. Chormyshavskiy). Apart. from, the universities, the
coal rence was attended by the representatives of some
ocio:;Lric reaearch, institutes of the Soviet ant
Ukraimian, Academies of Sclo=o, various 1-od-trial
estabilahments Lod the interested mlutatrIQ16 WA
arrangement stimulated %be discussion and ovalusSlon of
the papers presented and permitted the determination of
plans for the future research to be carried on% by %be
universities im the field of radloolectronLas-
'Comparlson-of the Iffi4ancy ;rt-ertaa
00"rAtioM of Millisetre Wave&- by A.S. Tager and
Application Of the Meher Spatial Mw*Ouics of the Rjectro-
maguelic Yield 14 SlOwing-4own Systoxa- by A@A_Toger and
1:0 the 31"Ci794;@@C; 60a@tjOjj-
lax ;,haAQX*::& appoarLAG at "A JQM%10=
--.M-.rP*,m1t 16 necessary to mention silo
:The C&ICulation, of JunctLonso by TAJL@jhU*Xar4

I @ 7 2 22
9, Slu-8116.010co 1,. 1
'?, AC)O, /AD-) I
Translation rrom. Referat.1vnyy zhurnal, Fisika, 1960, rio, il, p, 344, # 30759
AUTHORS, Solntsev V A Tager, A.S.
TITLE! Electronic Waves In a Periodic Elec!rostatlc Field and "Meir In-
teraction With the Field of' Wavegulde Systems
PERIODTCAL., Tr, Konfer,@ntsli po elektronike 3"'Ch, 191@',-,. Moscow-U@ningrad,
Gosenergolzdat, 1959, PP. 112-132
TEXTz The propagation of a weak high-frequency signal in a rectilinear
electronic flux with the velocity of electrons varying periodically along the beam
was theoretically studied, Space harmonics of the current are considered, con-
ditions of increasing their amplitudes are obtained at the motion of the beam in
free space. The interaction of current harmonics with the electromagnetic field
of the waveguide system was studied by the methods of the weak signal,.heor-1. The
analysis was-performed with allowance for the reverse effect of a HP field on the
electronic beami, It is shown that an effective int-e-raction of the electrcnic
beam with the fast waves of the wavegulde system can be brought abont. at. certain
relations between the velocity of electr3ns and the perod of its vartation. The
Card 112

87222
S/058
AOO 1 /.400 1
Ele,2tronic Waves in a Perledic Elect ros ta- i@, Fleid ani Their lnterar--@,,:)r, With the
Field of Wavegulde Systems
effectiveneSs of such a device (elect ros-,atic undula-@or) was compared, w.,thA,n the
framework of the linear theory, with the effectiveness of the initrurrient of Abb
(LBV) or JIOE5 (LOV) type; It Is shown *hat the non-relatlvis@t!c undulator does
not yield a gain in maximum frequency. Conditions are speciflAd under which an
employment of periodic electrostatic focusIng In LBV does not resul'. In deteriora-
tion of their characteristics,
A.S. Tager
Translator's note,, This 1,@ 11he full trantziation of !he vriginal Ru*sian abstract.,
Card 2/2

06340
SOV/141-2-1-12/19
AUTHORS: Solntsev. , V.A. and Tager, A.S.
TITLE: Periodic Interaction of Electron Streams
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Radiofizika,
1959, Vol 2, Nr 1, pp 101 - 110 (USSR)
ABSTRACT: It is shown that where interaction takes place, non-
evanescent processes occur not only in the fundamental
band but also in narrow, higher-frequency intervals.
The effect is independent of current density but is
limited by dispersion in electron velocity. Previous
analyses have most often been concerned with two electron
streams having differet,constant velocities. The forms
of interaction studied here are shown in Figure 1. In
the first three variants, parameters of the electron stream
chan6e periodically; in Figure la, velocity; Figure 14
stream diameter; Figure 1B, drift-tube diameter.
In the structures of Figure lt- the interaction is modi-
fied by slots in a screen and in Figure I by a
"slalom" focusing arrangement. With contfnuous inter-
action the maximum working frequency depends on plasma
frequency and velocity dispersion as discussed in Ref 1
Cardl/3 (V.M. Lopukhin). The reason for the existence of discrete

o6340
SOV/141-2-1-12/19
Periodic Interaction of Electron Streams
bands of frequency in the interaction with a periodic
structure is best seen in the case of Figure lt' .
If the streams only interact over the length of a slot
then the phase change of the faster space-charge wave
between one slot and the next must equal that of the
slower wave or differ from it by 2Mc , where k is
a whole number. The simple formula quoted in Ref 1 then
becomes Eq (3). An alternative viewpoint is that the
higher order bands arise from synchronism between, e.g.
the m-th spatial harmonic of the slower beam with the
n-th of the faster one. If the relation between current
density and stream cross-section is Eq (8) and replacing
the high-frequency component of velocity, current density
and space charge by equivalent quantities in Eq (11), the
relation between equivalent current density and longitudinal
electric field is Eq (15). The longitudinal electric fields
induced in one stream by current in another are Eq (16).
If thin streams are considered )the expression (A.6)
derived in the appendix allows for the reduction in the
Card2/3 axial component of Coulomb force in comparison with the

i. r-;ri tpract I on
lcj6o) !-,,i pp (Olorkiy State i'niv
wo'gjo;.)
LoL

9,/300 S/109/60/005/07/008/024
1140/H163
AUTHORSt Solntsev, V.A., and Tagert I.S.
.74
TITLE: U"ft@50*8'1" Waveituide Systems'11%y an Electron Stream
with Prescribed Modulation
PERIODICAL; Radiotekhnika i elektronika, Vol 5, No 7, 1960,
pp 1100-1111 (USSR)
ABSTRACT: In the majority of published work on the theory of
waveguide excitation by prescribed currents, mono-
chromatic currents with prescribed space distribution are
considered. The most general theory of monochromatic current
excitation of waveguides is given by Vaynshteyn (Refs 11 2).
On the other hand, in the theory of the Cherenkov and Doppler
effects in waveguide systems, the radiation of a point charge or
an elementary electric dipole moving rectilinearly along the
waveguide is considered, The spectral density of the current
connected with such a charge or dipole is constant over a very
wide band of frequencies. In real electron devices the current
spectrum has a complex character and does not reduce to either of
the cases considered. The basic formulae obtained by the two
methods differ from each other in principle. The present work
ri
Card 1/2

.A683
s/tltl/61/004/004/015/024
@S'*79_ (//4*1 9-@'02/E435
AUTHOR: Solntsev, V.A.
TITLE: Parametric amplification and frequency conversion in
a wide electron beam
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniyg Radiofizika,
v.4, no.4, ig6i, 712-725
TEXT: The author examines theoretically the propagation of-a
weak HF signal in a wide rectilinear electron beam conforming to
the travelling-wave law. The background foLr the analytical
treatment is developed from the first principles and the formal
analysis is used to explain the functioning and properties of
these time-dependent amplifiers and mixers. Great attention in
given to the most outstanding feature of these amplifiers, viz
the low noise level. The whole problem is reduced*to a
solution of an ordinary differential equation of the second order
d' V1 A, M
- + - P V. =0'
W6EM dt' I_U/V0
I'p M (()/Vo W TWO (EY301 0)
Card 1/4 -- -----

30683
Parametric amplification
s/141/6i/oo4/oO4/015/024
E202/E435
similar to an equation of a heterogeneous long line. This
simplification is achieved by considering the time of arrival of
the wave packets into a long line, instead of the "running time",
and by transformation into a moving coordinates system. The above
equation leads to general expressions for the HF voltage and the
current respectively viz
V (z, t) (A It-to (z, t)] a (z-ut) +
I - U/VO (2- Ut) (12).
+B It-43 (z, 01 b (z-ut));
aA It-t, (z, t)] aa (z-tit) dB It-to (z, 01
(2, 0 to X
at at
ab (z-ut) P2 (Z-Uj)
X +U [A It-to(z, t)j a (z-ut)+ (12a)
az I I -U/.Vo (Z-@,_t_jp
+ B [t-tu (z, t)] b (z-tit)l
Card 2/4

30U3
SPA1/61/004/004/019/026
Parametric amplification 9202/8435
in which A and N j are arbitrary functions 801VO& IS the Usual
manner from the boundary conditions.' The latter are famd'fron
the geometry of the problem as& Iresult In a states of two
differential equations of the first order. Ultimately these are
solved and re-subotituted' giving'all'the (physically) ad"esibler
solutions, Having osJLvod*ths-m4I*_probl*m, the author oessidors
a special case, vim that of parametric affiplif@eatloa siat frequency
conversion with a weak slauseldal.itgual. more the amoral
solution Is given by taking account of the ps iodisity, Finally,
& dotailed*analysis of noise to given and it a found' that the
minimum noise coefficient for,& psOAMetrie, a litter of this tYPO
occurs when the electron Sun *tltho amplifterja desigmedits mush
a way an to suppress the frequency .@squal to 31times the amplified'
frequency. Acknowledgments arv@ .**pressed to AiS.Tager ter
advice. There are 2 tables andt.1referencoi @5 Soviet and'
4 non-Soviet, The references to.anglish langimse publications
read as followso Skst.11 W,M.Louteell, C#ftato# Proof 2=0 v6469
707 (1958h Ref.2s W,H.Loulsell, J, of Bloatioules and Control,
Y.6, 1 (1939), Ref.6t L,N,Namlsy,,NsNaRow@t Proof Z=j V#441
Card 3/4

3003
1/004/004/015/024
Parametric amplification ... 2202/3435
904 (1956)1 Ref,71 A,W.Qouldi@ vi4i. IRZ, V.410 419 (19500
SUBMITISDi October 11, 1960,
Card

OVCHAROV, V.T.; SOUITSEV, V.A.
Simplified nonlinear equations of a traveling-wave tube.
Radiotekh. i elektron. 7 no.n:1931-1940 N 162. OGRA .15:n)
(Traveling-wave tubes)

44189.
B/109/62/001/012/005/021
D266/D306
AUTHORS: Oveharov, V. T. and Solntsev, V. A.
TITLE: Application of simplified nonlinear equations of a
travelling wave tube to 0 typq tubes
PERIODICAL: Radiotekhnika i el.ektronika, v. 7, no. 12, 19620
2013-2023
TEXT: Simplified treatment of 0 type tubes by the authors (Radio-
tekhnika i elektronika, v. 7, no. 11, 1962,*1931) leads to numeri-
cal results very similar to those obtained by earlier investiga-
tors, The transit time is expanded in a Fourier series and the cur-
rent is obtained in closed form if higher order terms of the expan-.
sion are neglected. The approximations are claimed Z Abstracter's
note: The effect of electron-overtaking is not analyzed7 to be va-
lid up to arbitrary values of a.c., but they lose valizlity for
large velocity modulation. The nonlinear partial differential equa-
tion system is reduced to an ordinary differential equation system
_Yhich can be easily solved on a computer. Comparison with more
Card 1/2 4r

ARDlication of simplified ...
S/109/62/007/012/005/021
D266/D308
rigorous TWT calculations shows that the simplified theory correctly
predicts the weak nonlinear effects, i.e. the presence of gain for
larger values of b (Pierce's parameter), absence of gain for large
input signals and large losses, etc. The equations are used with
slight modification for describing the properties of BWO and klys- @X
trons. The authors believe that the equations can be further sim-,
plified and analystical solutions - suitable for the dbsign of
tubes - can be obtained. In the present-paper approximate analyti-
cal solutions are confined to bunching in klystrons. There are 16.
figures.
SUBMITTED: January 17, 1962
Card 212

A'.'V,l!. 1112 'VIV V '-' ; I A
. .- -
Selecting operat"orial fri@@ju,@n,::y ir, 1@,, 'he ccreen rethrd.
izrl.tekh. no.9:F-10 S lf,5. (MT-RA 18:10)

SCIVrsxv II.A.; JT@7, G.G.
Simplified nonlinear eruaticns of
finite values of the amplific-ation
elektron. 11 no-1:58-67 Ta 166.
a trave7lr--lta%fc Vube aL
parame-uell-. Padiotekh. i
(Mm@ '19:3 )
1. Sub--@tted September :'6. ir"64.

I.I.A.
Solution of th-., charm!terlstlco equation of a tralx!lin@,-wavv.
tube with a iarre space charre purameter. F'adiotekh. i elcktron.
11 no.i:()F-74 Ta 16j). OIETT@,'. 19:' )
11
1. -September 26, 1@464.

SOIXTSRV, I.G., inzhener; GRITSIVETS, I.I.: KEMKOV, A.S.
Some.problems of producing excavators and cranes in the sIxth five-
yeex plan. Stroie i dorl mashinostv. 1 no.12:3-7 D 0569 1
(MLILA 10: 1)
(Ixc&yating machinery) branes. derrick@, etc)

d
Z
ogj

Vo
A
S
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Z
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S
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i

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C --.-a
U1 S.2
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-A

4461 *at A44080" uhtn@
MAOC L P" 'Stil" I 'OZSWTJ t 040 *MOO
TWo s 9*0 T vc (I',) Scat
is 8.0 T 9-t 0*1 7 Vs
(DOW
.004SUOR saw A 66*4
;0 NOTSIM OR% UT got's "M tot as A VIWTI an

FETIRMAIM, M.M., inzh.; RBIN, L.Te., doktor tekhn.nauk, LIVIN. H.S., kand.
tekhn.nauk, ZULI, N.M., kand.tekhn.nauk, PLNTSZT,,V.M., inah.,
KORSHUNOV, A.P., inzh.
?,d 1;M.in 6 end 10 kv. over ad networks.
ge@jj ?I thjfjjtr
V
n0eux me N VU 13:12)
1. UGPI nTyazhpromelektroproyekt" (for Fejermark). 2. Teeaoyusnyy
nauchno-iBaledovateltakiy inatitut alektrifikataii sel'skogo khozyay-
stva (for Ebin, Lavin, Zull)- 3. Giprosellelektro (for Solntsev,
Korshunov).
(Electric power distribution)
(Electric currents--Grounding)

KORSHUIIDV, A.P., inzh.; SOLM.UXq-X-14-., inzh.
Designing of efficient power lines with 6 to 10 kilovolt
rating for the electrification of villages. Ilek.sta.
31 no.4:71-76 Ap 160. (MIRA 13:7)
(Electric lineo--Overhead)
(Rurai electrification)

23000
s/186/61/003/002/010/018
Eill/E452
AUTHORS: Solntsev, V.M. and Tolmachev, YU.M.
TITLE: The reaction of the solution of U 08 in sulphuric acid
I. Kinetics o 'f some reactions wiN powders
PERIODICAL: Radiokhimiya, 1961, Vol-3, No-2, IPP-187-194
TEXT: The present work was devoted to the examination of-the
formal kinetics of reactiom of powders in solution. The authors
consider first reactions whose rates -.dm/dt do not depend on
diffusion 'factors but only, for.a given value of the rate constant
K, on the phase contact area S . Here m is the mass of
material at time t . Assuming that all the particles of a powder
are identical in size and shape, the authors derive
(5)
MU - M.1 -it.
where mo is the mass when t = 0 and
.10
i
3MO3
Card 1/5

23000
S/186/61/003/002/010/018
The reaction of tte solution ... Elll/E452
.t
So being'the surka ce when t = 0. A form of this relation is
used in studying @reactions of solids with gases (Ref.2: R.L.Farrar,
H.A.Smith, J.Phys.Chem., 59, 7, 763'(1955)). The authors do not
consider the recent treatment of P.Barret, R.Hartoulari and
R.Perret (Ref.l: C.R., 248, 20, 2862 (1959)) to be applicable.
The authors used Eq.(5) in studying the solution of U308 in
sulphuric acid at a temperature controlled with an accuracy of up
to 0.10C. The oxide was prepared by heating uranium peroxide at
8000C and U233 was-added to give nominally 104 alpha-particles per
min per mg of o;iale". Samples of solution were -taken periodically
from the reaction vessel, 'fh'e-solids were removed by centrifuging
and the alpha-activity of the residue-on 'drying the solution on a
platinum disc was'then'measured. Without'm*ixing, the reaction was
found to be of the seco@d order with respect to 'the acid concentra-
tion C L/for C = 4 -10 mols. Fig.1 shows the relation
(03mo-1m 3) in mg as a function of time (minutes) for'
between (m.
the 0solution of U308in 6 m H2S04 at Wc. T@e results indicate
th@t the powder form is suitable for the investigation of solution
kinetics. For pow s with mixed sizes a non-linear relation is
obtained between ml,75 and t: this can be resolved into a
Card 2/5

.23000
S/186/61/003/002/010/018
The reaction of the solution ... Eiii/E452'
series of straight lines characteristic of the various fractions.
This treatment gives for the rate'constant k -the equation
33.na 3
A 0,
where q is the total surface of all fractions and. n is the
number of the fractions. The authors have used this treatment to
anilype the published data on the solution' of various samples of
DISO in dilute sulphuric acid; these data do not conform to Eq.(5)
because the samples consisted of mixtures of size fractions.
Assuming that dye adsorption per unIt sux-face of MgO Im the
'work, was independent of the way in which the oxide 'was produced and
was the same for all samples,,the authors obtain the following
7: n 3
fk W- j_j (13)
P
tard 3/5

23000
S/1&6/61/003/002/010/018
The reaction of t4e solution ... El11/E452
in which f is a..proportipnality factor and p is the percent
absorption of dye.@ Thii can be used to determine rate constants
for the solution @f powders of mixed dispersion provided the total
powder surface is known. The authors next consider reactions
controlled by diffusion through a layer of reaction product. They
assume, for simplicity, that the.layer does not alter the particle
volume and obtain the equation of W. Iander,(Z.anorg. u. allgem.
Chem., 173, 1, 1 (1927). Next they assume that particle-volume
changes in the reaction and.obtain an equation
Q.. + mp)"- k1l. @(21)
Here
AIOdjV
a- --@ - . .
OUP (20)
Mo and do being the molecular weight and density, respectively,
Card 4/5

23000
s/l86/61/003/CO2/Oio/ol8
The reaction of the solution ... Elll/E452
of the original substance, 111p and dp those of the product
P = I - a. Eq.-(21) is a more accurate rate expression than that
of Iander and becomes identical to it if a = 1. There are
2 figures, 4 tables and 4 non-Soviet-bloc references. The
reference to the English language publication reads as follows:
R.L.Farrar, H.A.Smith, J.Phys.Chem., 59, 7, 763 (1955).
SUB'i,,IITTED:' April 21, 196o
M
Fig.l.
Card 515
ZOO 300
8pevir. Mum

29820
S/02 61/140/006/017/030
121. WOO B103YB101
AUTHORS# Blinova, N. I., Solntsev, V. M., and Tolmachev, Yu. M.
TITLEt Some particularities of the interaction between uranium mixed7
oxide and acids
PERIODICALt Akademiya nauk SSSR. Dokladyg v. 140, no. 6, 1961, 1314-1316
TEXT: The authors studied the discrepancy between the initial and final
UO 2+ 1 U4+ ion ratios on dissolution of uranium mixed oxide in acids
2
without oxidizers. This ratio is 21l on final solution, vibereas in the
initial stage, mainly U(VI) is dissolved, so that the ratio U(VI) t U(IV)
is much higher than 20. High-purity U 30. powder was dissolved in C02
atmosphere at constant temperatures (25 or 900C) in a) sulfuric,
b) perchloric, and c) acetic acids. The solutions were anal zed after
100 min (H2 so4), 10 min (HClO4), and 40 min (CH 3COOH). U(IV@ was determined
in the solution by titrating with KMn0 4' the total quantity of U by
Card 1/4

820
S7012Y61/140/006/017/030
Some particularities of the interaction ... B103 B101
precipitation as ammonium diuranate and igniting to U30.. Ratios of
76 : I in a), 60 11 in b), and 300 1 1 in c) were found for the beginning
solution of U308. After 2 hr,)the ratio U(VI) : U(IV) in the solution
became 1 tl and remained constant, until dissolving was completed. A
precipitation is deposited in the final stage of dissolving, in which the
ratio varies between 20 and 10. Once the ratio of lil is reached in the
solution as well as in the precipitation, the composition of the
precipitation does not change anymore. This is a dark, slightly violet
colored powder which becomes grey-green on drying in air, the ratio
U(VI) i U(IV) approximating 21l. A ratio of 10 is maintained for 48 hr in
the powder, when the water is saturated with CO 2- When U30. is dissolved
in HNO 3' a stable ratio of 20 is conserved in the powder during the entire
time of dissolving. It was found that the uranium atoms in U 30. do not
play the same role. It is difficult to find a different explanation for
the varying U(VI) : U(IV) ratios in the solution and in the precipitation
during the reaction of U30. with acids. It is presumed that U 205which is"
Card 2/4

S/o 20J61/1 42NO2006101 7/0 30
Some particularities of the interaction ... B103/B101
possibly a compound of U(V) forms in the final stage of U 308 solution
in acids. Probably@ U(V) disproportions to U(VI) and U(IV) in a ratio of
lill when it is dissolved in acids. It might be possible, however, that
U205 is not a compound of U(V), but for instance UO 3' UO 2' When it is
dissolved in acids, a ratio of U(VI) t U(IV) - 10 will result. In this
case, U306 should have a composition of say UO 3* UO 3. UO 2' UO 3*U2 05is
suggested, until the structure of U 308 is finally cleared up. The U 3 08
formed reacts, however, much slower with acids than the initial U 308
molecule. It is presumed that the peculiar course of the reaction
described is characteristic of many chemical compounds; oxides, sulfides,
and further compounds (basic and double salts) of metals, the atoms of
which show different valences, will react, presumably, sometimes in an
analogous way. Papers by Vikt. I. Spitsyn, G. M. Neemeyanova, Ye. A.
Kanevskiy (ZhNKh,5, 1938 (1960)) and by 0. M. Nesmeyanova, G. M. I
Alkhazashvili (Atomnaya energiya, 1, 330 (1960)) are mentioned. There are
3 tables and 6 references$ 4 Soviet and 2 non-Soviet.
Card 3/4

29820
S/02 61/140/006/017/030
Smt.particularities of the interaction... B103YB101
ASSOCIATIONt Radiyevyy institut im. V. G. Khlopina Akademii nauk SSSR
(Radium Institute imeni V. G. Khlopin AS USSR)
PRESENTEDs May 24, 1961,by A. A. Grinberg, Academician
SUBMITTEDt May 18, 1961
VK
Card 4/4

ILINOVA, N.I.; ROMANOV, G.A.; SOLNTSEV, V.M.; TOWACHEW, Tu.M.
Magnwtic properties of U205. Dokl. AN SSSR 147 no-5lUl2-ln3
V 162. (MA 1612)
1. Radiyony inotitut im. Y.G. Iblopim M WM Predstayleno
akademikom A.A. Qrinbergm,
(Uranium oxides-41agnetic properties)

1,3k27c@@j fr.,JG(J)/9,QT(m Pi@_4/@s_4 IM0-
/ES/,TG
ACCESSION NR: AP4043855 j S/0186/64/006/004/0463/0466
Solntsev, V. N.
Kurbatov, Vo
B-linova,
AUTHOR:
V.;
N. L;
TITLE: A roentgenometric study of the system U sub 3 0 sub 8 U sub 2 0 sub 5
SOURCE: Radiokhimiya, v. 6, no. 4, 1964, 463-466
TOPIC TAGS: uranium oxide, oxide crystal structure, xray diffraction pattern,
latticeconstant, rhombic lattice,.uranium pentoxide
-ABSTRAM The authors prepared U20@ either by dissolving U30 in sulfuric acid orl
-by reducing U30. with hydrogen at 3 6C, and then determined Re lattice constants-
by x-ray diffraction analysis during the reoxidation of U 0 to U 0 * They found
2 5 3
that, as U 205 is saturated with oxygen, only the U 0 crystal struegure is ob-
served in all the intermediate stages, and stable h1fraction lines characteristic
of the U 30. lattice appear only after reaching an empirical composition of UO 2 62*
The entire range of compositions from U 0 to U 0 is thus homogeneous. Visual
5
comparison of the x-ray diffraction patierns lea the authors to conclude, in op-
position to the hypothesis of Mil-ne (Am..Miner., 36, 5-6, 4171% 1951) and others,
that the IU308 lattice is a deformed U 0 lattice. On the basis of homo-logy,the-@_
2 5
C
r
a d_ 1/2_

SOUT "EV , V.N 0 * 111C 11, AC I DIV p Yu . M.
j dIssolut-Im in H2SO4- RAdiukh.1miia 7
Plermodynamics I cf "' 309 O-LIPA 16:1)
no.6:719-722 65.

L i-V-'T(-a)/E`AT'(t)/1ET1
'60@@ -.-
ACC NR- AP6022502 SOURCE CODE: UR/0054/66/000/001/0129/0132
1AUTHOR: Kozhina I I.; Os.@pqya, V4 V.; Solntsev V. M.J Tolkachevj--
--* S. (d6-d--easeU, ---. -
ORG: none
TITLE: Certain properties of uranium pentoxide
-A, 7 I'll
SOURCE: Leningrad. Universitet. Vestnik, Seriya fiziki i khirnil,
no. 1, 1@T&; 229-132
TOPIC TAGS: uranium compound, Inorg9nic oxide, x ray analysis, heat
resistance
ABSTRACT: The dimensions of the hexagonal cell of U 05 were measured
and the thermal stability of U 0 was determined. Tge hexagonal cell
size was established: a = 6.8V@� 0.001 kX and c = 4,118 + 0.001 M.
The composition of the hexagonal phase of U 0 obtained at-low
temperatures varies within the range U02,k?2-5U0 U 0 is
0 -to226Kqqe2:5
disproportionated at temperatures above C a hexagonal
and cubic. At temperatures of '145 - 1700C hexagonal U308 and cubic
U02+Y are formed; and at 8oo - lOOO0C# hexagonal U 3108 _X 8;5 cubic U4099

L 4A-M-6-6
ACC. NRI AP6022@02
= 5-43 0.01 A0 are forme do Orige art. bas: 3 tables*
SUB CODE: 07/ SUBM DATE: 02jul65/ ORIG REF: 004/ OTH REF: 007

X., j., 71
Jun 2,5 1963
IV 7
PHUR I BDOK MWITATION SOV/16261
Kernonergie und Flotte; Artikelsaw1ung (NucleaMftergy and the Na
Collection of Articlesy LBerl1n] Deutecher Mllitarv6rlag (1961T.
232 P. Errata alip Inserted.'. 2000 copies printed.
Translation from the Russian of; Atom:Wa,"rSiya, I flot.
Translatorl Erika Steuk, Lieutenant Commander. Responsibility for
Geman edition. -Clius Gruszka, Mnginosrj U-1 Klaus Krumeleg.
MPOSS: This eollootion.of.arti6les Is intended for officers of the
AMY, c6uet guard, and merchant mirine.
OOVERAGEt mts.* book, &.translation from the Russian, oontains i5 ar-
ticles dealing with the application of nuclear weapon* to naval
combat Operations. Chaptere 29 and 25'have been aupPlownted 'wIth
additional data for thIs ed1tion. The devastatIng features of nu-
clear explosions are discubs9d. Attention Is also given to the
protooticn Of personnel shipep end coastal'faallities against nu-
cleal@ wftpons,:and. tb .,t6 -prebont) and futmv 4WIloatIbno of nualear
Card 1A

Nuclear Energy and.the Navy (Cont.) sov/16261
pc@wer plants to shipping. No p reonalitles are wentioped. There
are-16 references: 10 Russian Mcluding 3 translations.from
English-language sources), 1 French, 1 Clerman,.1 English, I Ameri-
can, and 2 either English or American.
TABU OF CONTENTS:
Foreword
1. A. Badov, Engineer Lieutenant Colonel, Docent, Candidate of
Technical Sciences. The Dangers of Nuclear Weapons Tests 9
2. .3. Sergeyer, Captain (Navy). Explosions of Nuclear Weapons
In the Air and Above and Under Water 22
3. V. Byabehuk, Captain (Navy). The Shook Wave 32
4. K, Arkh1poY, RMIneer, Lieutenant Colonel, Docent, Candidate t
4
of Technical Sciences, and V. Olre:-@cos Engineer, Lieutenant.
Com6andor. Light Radiation 42
0% Ad
Card

Nuclear Energy and the Navy (Cont.) SOV/6261
19. A. Uvarov, Engineer Lieutenant Commander, Docent, Candidate
of Technical Sciences. U.S. Nuclear;-Powered Submarines 162
P. Mikhailov.. Engineer Lieutenant Colonelj Candidate of
Technical Sciences. Depth Charges 189
21,, M. Rudnitskiy.. Engineer Rear Admiral. Nuclear Power
Plants in Warships' 192
22. N Solntsev -.Engineer Captain (Navy), Docento'Candidate
Sciences. 'Utilization of Nuclear Power Plants
in Shipping 19T.
23. V.- Zvonkov, Corresponding Member, Academy of Sciences USSR
Honored Selentibt and Tec4nologist RSFSR. Nuclear Power
Plants in Transportation 204
4-
24. N. Varvarov, Guards Colonel. Nuc'.ear-PoweredIFlyIngBoat 209
Card-5/9

W.

L '514656-65 &4T(I!)/.EWP(m)/EPF(c)/EPF(n)-2/F, fR/EWG(m)/FCS(k-)/,EWA(1) Pd_j/Pr-h/
_P1,__VP_U_h/Pi-4 WW10OX
ACCESSION NR: AT5010481 UR/0000/65/000/000/0055-/oo
AUTHOR: Avduyevskiy, V. S. (Doctor of technical sciences); &Y-/
_IL=uknm..V, L, (Engineer); Soln sev.*V. P (Candidate of technical
sciences)..
TITLE: Experimental-investigation of the structure of the hnnnAjkrg@
laver and heat tranaftr on a rough surface
124
i SOURIE: Issledovaniye teploobmena v potokakh zhidkosti I gaza
Moscow$
(Investigation of heat exchange in liquid and gas flows).
Izel-vo Hashinastrayentye, 1965, 55-90
TOPIC TAGS: boundary layer, heat transfer, rough surface boundary
i layer, subsonic air flow, displacement thickness, momentum thick-
neits, surface roughnes's effect
ABSTRACTs The structures of boundary layers and the heat transfer
In subsonic air flows along smooth and rough surfaces near the for-
1 ward stagnation point are experimentally investigatode The experi-

ques used are described in detail
mental'set up, modelsi and techni
(site Fig# I of the Enclosure). Steel and copper disks 300 am In
Cord-, I

L 54656-65
ACCESSION NRs AT5010481
diameter were used as models In the study of both processes. A'method
for measuring the local heat transfer coefficient which made
was used
It possible to determine the heat transfer coefficient a from the raw
latlon a - (cG/F)n* where c is the specific beat capacity, C the weight,
of the body, F the surface, n the rate of heating, and # the coefficient
of nonunl-!ormity of the temperature field. The boundary layer thick-
nesso di-aplacement thickness, and momentum thickness were determined
for axisyrimetric flows over smooth surfaces and surfaces of various
degrees of roughness. A comparison of the results obtained here
with theoretical data obtained by Loytsyanskiy (Mekhanika zhidkosti
I gaze (Mechanics of Fluids and Gases),1957.Moscow)-showm a rather
good agreement and that the heat transfer coefficients obtained
experimentally are somewhat I rger than the theoretical values., Thai,
a
dependence of the momentum,thickness 8Nx,on the free flow velocity
is also established. The results ofaxperimental investigations of
the structure of boundary layers along a rough surface to the cases
of flow along a heat-insulated surface and in the presence of heat
travisfer are given In grapbio and discussed. The results are sum
marited and their accuracy to evaluated on the basis Of the toots
performed, A series of conclusions -is outlined. OrLS, art. bass
43 I!IAures and 6 formulas@ IASI
Card j

Z4