SCIENTIFIC ABSTRACT PAVLOV, V. P. - PAVLOV, V. S.

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• Collection: Scientific Abstracts
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• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

AUTHOR: Pavlov, V.P. (Mo,.cow). 24-4-5/34
TITLE: On the mechanism of formation of spheroidal graphite in
magnesium inoculated cast iron. (0 mekhanizme obrazovaniya
sharovidnogo grafita v magrLiyevom chugune).
PERIODICAL: Ak'
Tekh.
Nauk" (Bulletin of the Ac
"Izv
3c
Otd
Nauk
.
.
.
.,
.
.
,
-7,--M7, No.49 PP-33-39(USSR).
Technical belences Section
ABSTRACT: According to Gorshkov, A.A. (Liteynoye Proizvodstvo, 1955,
'No*3) addition of pure magnesium or of magnesium alloys
brings about a rapid evaporation of magnesium which is
accompanied by tile formation of a very large number of
biibbles which rise upwards gradually decreasing in dimen-
$ions due to the consumption of magnesium vapours on the
reactions expressed by eqs. (1) and (2), P-34; a complete
elimination of these bubbles cann t take place due to the
fact that they form spaces where the partial pressures of
other gases approach zero and to which,hydrogen will
diffuse which is neutral relative to the magnesium at tile
liquid iron temperetures. These almost immobile bubbles
in the still liquid iron will contain carbon, formed as a
result of the reactions, in the form of graphite crysta.,1-
isation mclei. Since oxided irons yield more CO and C09,
Gorshkov concludes that such irons should be used for
obtaining magnesium inoculated cast iron. To verify the
Card 1/ 3 theory of Gorshkov the author of this paper investigated
the treatment with magnesium of iron which was prelimin-

On the mechanism of formation of spheroidal graphite in
Tagnesium inoculated cast iron (Cont.) 24-4-5/34
arily degassed. In a 70 kg ladle 350 g (0'.5%) soda was
placed first and, after filling the ladle with -iron,
treatment was effected with 1.5 kg of an*alloy containing
7.92% magneBium, the rest consisting of 75% ferrosilicon.
A.specimen of standard dimensions (30 mm dia) witiistooe,
a bending stress of 125 k&/mm2 with a sag amounting to
14 mm; the micro-structure was that of a typical magnes-
ium iron, Fig.1, P.35. A second ladle of equal capacity
was preliminarily treated with air-dried timber; after
treatment with an alloy of the same composition as in the
previous cage, the obtained iron had a bending strength of'
113.2 kg/mi~ with a deflection of 14 mm. Irons treated
with the same alloy but withuut preliminary d assing had
a lower mechanical strength, namely, a 111 VMID2 bendin,6
$trength with a deflection of 6 mm. The results do not
confirm the views of Gorshkov. It appears that the mag-
nesium refines the iron without actually reacting with
the iron or getting dissolved in it but fo=iiqg varbides.
Soot particles which form in the iron as a result of the
reactions caused by the magnesium are the fundamental
nuclei for graphite crystallisation which determine its
Card 2/3 shaping; the soot particles become rolled in the moving
liquid and assume spherical shape. The dimension of the

On the mechanism of formation of spheroidal graphite in
magnesium inoculated cast iron (Cont.) 24-4-5/34
soot particles of various types varies between 3.6 and
400 up.
Card 3/ 3 There are 6 figures including picro-photographs. There
are 11 references,-all Russian.
SUBMITTED: September 11, 1956'.
AVAIIABLE:

FAVLAW, V. P. -.-- -
Technology of preparing magnesium cast iron. Lit. proizv. no. 2.37-
38 F 161, (MIRA 14:4)
(Cast iron-Metal-lurgy)

PAVLOV, Vladimir flavloldch; MELINIKOVA, U.M., red.
.....
[!oVmoro and rwtalo) Polimory i motall. Monkva, Znu-
nie, 1965. 45 P. (Novoe v zhizni, nauke, tekhnike.
XI Seritat Khimiia, no.10) (MIR.A. 18:10)

: - I I " V. w
I, I "P , . ~ , 1 1.
. !, . I ~ '. - ,,1 . . ... .

: ;. . ~J I - . '. . , -11~
: -c' - . i
. 8j - - lu...

PAVLOV) V.P.
Circulation of liquid in a bubble apparatus with peric.lical
action, Khim, prom. 42 no.9t698-700 S 165. (MI-RA 1819)

PAITMV, V.P.
fact of residual manf,5ilm, on the form rX im
inst iron. 1,.,v. vyv. ucheb. zav.; nl.;)m. met. '1 r,..'/z187-194
164 Olf U 18)
L. Mus~ovskly aviatteimi.y
.7 insll!-,ii.

KUSHNAM, D.M., kand.tekhn.naukj_PAVLOV, V.P., inzh.; ZELITSER, Yu.1.,
GHEFWANOV, G.S.
Industrial testing of a maabine, for charging a hole with "igdaOit.0
Gor. zhur. no.9:46-47 S 162. (KRA 15'9)
1. Gosudaretvennyy inatitut gornokhimicheakogo syr1ya (for
Krahnarev, Pavlov). 2. Gosudarstvennyy proyektno-konstruktorskiy
institut avtomatizataii rabot v ugollnoy pronyshlennosti (for
Zelltser). 3. Institut gornogo dela iv~ Skoohinskogo (for
Cherepanov).
(Isplosives) (Blasting-Equipment and supplies)

PAVIOV. V.P.. Inshener.
Joining wood lingitudinally with tootbad tenons. Der. i lesokhim.
prom. 3 no.10:5-8 0 154. (MLRA 7:11)
1. TSentrallnyy nauchno-looledovatellskiy Institut mokhanicheakoy
obrabotki drevesiny.
(Woodwork)
li ~Sj , I- ~ ~, -,,.) " ~ ~ ~I

PAVWV, V.P., in2hener.
--
Testing skis mode of one piece of Manchurian ash. Der.prom. 5
no.2:1? F '56. (KWA 9:5)
1. T;Sentral'nrj nauchno-issledovatel'skiy institut mekhanicheskoy
obrabotki drevesiny.
(Skis and skiing)

PAVLOV V P 4~oo jand Tech S^,i -7- (diss) "Study of -b4~
r Pt
16 pp -Nith 22 cm. (,'.tin of di,,-
MO 3 11 19 57 - _,her Au-
cation USSR. Moscow Inst of ForestIlEngineering), 110 copies.
(KL, 21-57, 103)
-64-

PAVLOV, V.P., inzhener
Resistance of veneer tenon joints to compression and impact
banding. Dar. prom. 6 no-3:16-17 Mr '57. (MLRA 10:5)
1. TSentraltnyy nauchno-issledovatellskiy institut makhanicheakoy
obrabotki drevesiny.
(Woodwork--Testing)

PAVLOV, V.P., sadovod-lyubitell (Bagullma, Tatarskaya ASSR)
Black rot can be cured. Zashch. rast. ot vred. I *r/,I. 8
no.6:55-56 Je 163. (MIRA 16:8)
(Bt4;ul'ma-Apple--DIe"sos and pefits)
(Dugullma-Canker (Plant diseme))

lou 1 V i
E, Ei
-u or t, a n
n ~l
c .1! ur. f7 c, :t p
Ex T, C -!ii--
i., r. c, w a r a c r
c r o u b 1 o r c, v a t c; Ti :3
I A d f com n a rk
vi ce ('2 s1(- 1'.

ill

S/1'/ 9/ 0 0 0/ 0 6/ 014/ 0 21)
Invc-stigation of an Anonalous"y V.-Iicous Bu-14y In a
f~SS ~;cndition
I i-ru i na t e dThe twistin;, moment was measured as a
_iin~:!tion of rotation velocity, and at the same time an
~_'~ial flow, varying between 1.48 x 10-3 and 1,62 --m3/sec
maintained through the viscometer. Control
(,Wperiments on the circumferential flow were carTied out
the rotation plasto-viscometer PVR-1 (Ref 1). The
is aralysed mathematicalIty and expressions obtained
for the mean axial deformational velocity, DIO, the
,,ircumferential deformational velocity, D2, and the
_1,~.'Lorm,ational velocity at the wall, Dl (Eqs 1 and the two
;)receding equations). Graphs are given of log Dlo, log DI
zind log D2 agalnst log rl and log r2 a-c temperatures of
35 and 500 (Figs 2, 4); r2 and ri are respectively
z~-e mean and the axial tangential stresses, &.am ina I.- i on
..f the curves for the grease for the high resin extract
-ind for the grease geconditLoned at a deformation
"'elocity of 5.1 x 10 sec.-l in a rotary homogeniser
that the axial and circumferential flow have
-he two flows
ssentially the same characteristics. If 'U
_~-re of the same order of magnitude, there is a strong
0

S/1 79/ 59/000A '16/014/029
L
Investigation of an Anomalously Viscois Body Ln a
t 4
:3 sCondi L on
influence of circumferential on axial flow. At low
:~:Lrcumferential flows, there is practically no influence
on axial flow. At high circumferential velocities, the
Lixial flow of the anomalously viscous body bacome3
c, w tc
)nian. Some increase in circumferential viscosity is
bserved at high axial. velocities. This effect
'i-minishes if the temperature is raised, and also if the
is preconditioned by subje,,:ting it to high
,--formational velocities. Figure legends are as followq,
1 - Schematic arrangement of tLe apparatus for
.,;,--estigating flow of an anornalously viscous body under
~Iic- action of two simple shears,
A Fig characteristic
,,continuous) and neutrallsed (dotted) flow curves for
,!:-,tract- Fig 3 - characteristic (continuous, dashed)
neutralised (dotted) flow curves for fatty greasq.
(,haracteristic (continious) and nentralLsed (dotted)
~1.cw curves for fatty grease, the structure cf which was
'r,--fker. down iF. a homogeniser at a deformation veiccity
~s ,1 X 104 see-1. (In Figs 2-11 tho Hrttr-d I ines
-oresent the curves DjO('Z'j.1' obtained for oxtract and

017-,1 Ox 3 S IJ t
a t i ~- ;~-- x !.s- I -" -I c ~ -, i-n 17~,' trie, twin rc,'Latif.,n
V C, t e 1- s T- t 1 n .- ep r e D r,t s-
D 4,3 r e,- a- c! e
7 1 S s
p PV F - 3 Le a I a j, yr e s /,-,Lr-
air
a n v e -,;,um ed Tc i
C) ~n t 11 c-- nu es a -1 ir, tile u-) r~!C, at t~ic, tc~p u1
p a e 1,2 w~l I ax :1 sz c i ill , r b, at I ~
ayial vll,,,~:(!-i,.~
f d .3 1- c-, -11,1 a ty f,-)r ex r a T
C. I UM f e i ~!ri t, - a E, i el,:)cj ty f(-,,.r fatt7 i.,
ef 160 ~,,:) 5alic, 1-1-00 F 1 g 7 .. cuf .765
ch"inge of' :,i v E~ .-I ,-oni ferent 1,111 v] ~!C~-i.ty on
arl (I c, J'- rIT13 T L ~i ~7, s I t 5 ', C
e I L.
W~.
SU BE I I'l ED 1 A

ASTAKROV, A.V.; PAVLOV, V.P.,PAVLOTSKIT. I.P.
Spectral representation of the n-partial summit function
in tho one-dimnsional case. Nauch.dol.-I.vys.shkoly. fiz,
mat.nauki no.2:124-127 159. (MIRA 13:3)
1. Moskovskly gosudarstvannry universitet.
(Potential. Thenry of)

SAYFULLIND M.S.; PAVLOV, V.P.
Evaluating the current o-fl yield of the flooded section of bed
VI in the Ashit sector of the Arlan oil field. Geol. nefti. i
gaza 8 no.lOt27-31 0 164. (MM 17:12)
1. Neftepromyslovoye upravleniye Arlanneft'.

FAVLOV, V.P., kand. med. nauk
Indications and methodology for the Intra-articular introductlon of
hydrocortisone in infect"ous nonspecific polyarthritis. Sov. med.
27 no.11%111-116 N 164. (MMA 180)
1. Otdolenlye infektsionnyk), rollartritov (zav. - prof. M.G.Astapanko)
Nauchno-1 sol.- d ovate I I skogo instituta revmatlzma (dir. .. deystvitelInyy
chlen AIC SSSR prof. A.I.Nesterov) AMN SSSR, Moskva.

PAVWV, Ifsp. (Mosk7a, 1-ya Pryadillnaya ul. d. 2/9, kv.38)
Chmges in renal hemodynamlcm foLlowing m1tral commiseurot?v
in patieits.with m1tral stenosime Grud.kbir. 1 noo2s 184$
Mr-Ap 159o (MIRA 16:7)
1. 1z kafedry fakulltetskay khirurgii (zav.-prof. A.A.Busalov)
pediatricheskogo fakul'teta II Moskovskogo meditsinskogo institu-
ta imeni N.I.Pirogova.
(MITRAL VALVE-SURGERY) (KIDNEYS-ELOOD SUFTLY)

LOSKUTOVA, L.T.; MAKOTINSKIY, M.P., kand. arkh.; RUDINA, M.A., arkh.;
SHPANOV, I.A., arich. Prinimal uchastiye LIVSHITS, A.M., inzh.;
GROMOV, V.L., kand. tekhn. nauk, retsenzeng; KRASNOVSKIY,
N.V.,- kand. tekhn. nauk, retsenzent; P~YWVJ.P., kand. tekhn.
nauk, retsen2ent; PODZOROVA, N.G., inzh., retsenzent; FOLOMIN,
A.I., doktor takhn. nauk, retsenzent; GURVICH, E.A., red.
(Catalog of finishing materials and elemental Ketalog otdeloch-
nykh materialov i izdelii. MOE,-,.a. Gosstroiizdat. Pt.$,'[Wood
and paper] Derevo i bumaga. 1962. 36 p. (MIRA 16--8)
1. Vses*Uznyy nauchho-issledovatellski_v institut novykh stroi-
tellnykh materialov.
(Finishes and finishing)

KUSHNAREV, D.M.; PAVIip_p_V.P.
Study of the danger of stray currents in using electric deton-qtcrs
with nichrome filament bridges. Vzryv. delo no.48/502-98 162.
NIRA 15:9)
1. Cosudaretvennyy nauchno-issledovatel'skiy institut gornokhimi-
cheskogo syrIya (GIGMS).
(Blasting)

BUNIN, O.A.; MOSKVICHEV, N.T.; PLPMIN, S.A.j Prini-14 uchastiye:
. GORSHKOV, P.V.,- SMIRNOV, V.M.; F~AVWV,12,; ISAYEV, A.P.;
IAVROV, G.V.
Operation conditions of the dye aging and reducing
apparatus. Tekst.prom. 22 no.lo:64-67 0 '62. (MIRA 15:2a)
1. Ivanovskiy riaurlmo-issledovateliskiy tekstillnyy
imstitut.
(Dyes and dyeing-Apparatus)

KUSHNARKV, D.M., kand.tekhn.nauk; PAVLOV, V.P., insh.
Explosives with the simplest ccepocition. Shakht.stroi. 6 ro.ll:
24-25 N 162. (MA 15:12)
1. Inctitut gornokhimicheekogo isyrlya.
(Explosives)

J. -11-J"
A- .1 -nmu.-. 9
0"" _TJ J.
P.
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p A- Ran
wrms-tmd ng~t~w ~q -n
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M J. Tnws~ at .
09~ 4-4 f L42
r'l'ddy P-- J- -T~Z -T-n-TTV 4 ~Tr- ~d

Ww, V.P.,- ingh.
Work required by various methods of reinforcing prestressed
concret6 products in conveyor-line plants. Trudy NIIZHB
no.27:133-149 162. (MIRA 15:9)
(Prestressed concrete)

FROZOROVSK.rr. G.N., kand.tekhn.nauk; PAVLOV, V.P., In2h.
Special nroblems in the Industrialization of construction In
villages. lav. Uit no. 1:58-614 '60. (MIRA 11 :9)
(Farm buildings) tPrecast concrete construction)

P AV LC I; , V . 1'. , Cand i c-Fi 1 -'C-i -- (I i-,~3) "~,Atiun of tr~u - li~
tne po-stoper a ',.I; v,~ ,:er. o~i . " , 11-Itz,, . 1 1, p~ ; (".3ccon ~ :-~U: -, " - I I., ~..-
1.
.,.e.,-I-Ical I,n--. ', - i L. * . 1 . -'- -' r o - ~ v ; r' ~,- - c G :~ -: , -- ; ~- T - 4 c -. r. r, ,~, - ': .- , *1
22-601 1144) .11 1.. -- I

TINGGRADOV, G-V. (Moskva); PAVLOY,,V.P. (Hook-va)
Ilastic and strength properties of soft bodies. lzy.AN SSSR.
Otd.tekh.uauk.Nekh. I mashinostr. no.2:134-141 Hr-Ap '59.
WRA 12:5)
(Deformations Nechanics))

/ -, ~-) V ~ (~ /. I , "
i j
LARCHEITKO. Ye,G.. kandidat tekhnicheskikh nauk; PAVLOV. V.P.
AnBwers to rapdorst quastions. Geod. I kart. ne.8:66-70 0 '56.
(MIRA 10: 1)
(Surveying)

ilAVL-C)\,/ v.p
bXRMVSXIY, V.Ye.; VASIIMNKO, M.I.; VELIER, R.L.; VMWVSKIY, A.M.;
VERNER, B.F.; VOYDAIA)VSKAYA, Ye.N.; VOL'SKIY, A.N.; GLAZEDVSKIY, A.A.,
GRANOVSKIT, B.L.; GREYVER, N.S.; GUDIRA, N.V.; DOLGOPOLOVA, V.I.:
KOCHXVSKIT, V.A.; KOVACIISVA, Ye.B.: EURTAVTSEV, P.S.; LEBEMY, A.Z.:
LlSOVSKlY, D.I.; LIKHNITSKAYA, Z.P.; MATV8Yh'V. N.I.: MELINITSKIY, A.N,;
MIRONOV, A.A.; MIKIWEVA, A.A.; MURACH, N.N.; OKO', A.B.; OL'KHOV,11.P..
OSIPOVA,
,J*,6j ROTINYAN, A.L.; SAZHIN, N.P.; SMYUKOV,N.N.;
SIDOROV, P.M.; SOBOLI, S.I.-. KHETFETS, V.L.. TSXYNTR , V.M.-,
SHAMINAZAROV, A.K.; SHEYN, Yn.P.: SHERDW'TIV, S.D.; SHERMAN, B.P.;
SHISHKIN, N.N.; SHLOPOV, ~.P.
Goorgii Ivanovich 1311nov. TSvet.met. 28 no.6:62 N-D 155.
(MIlLA 10 - 11)
(Blinov, Georgii Ivanovich, 1911-1955)

sli 28/61/C00/002//W7/009
A054/A 133
AUTHOR: Pavlov, V.P.
TITLE: Technological problems in magnesium iron production
PERIODICAL: LIteynoye proizvodatvo, no. 2, 1961, 37 - 38
TM: The modification of iron with magnesium can easily be carried out In
workshops where Iron is poured into the molds with 70-kg ladles filled from the
cupola by a mixer. After filling the mixer with iron the slag is removed and the
magnesium foundry alloy is added with the aid of an iron rod held over the metal
surface. The opening of the mixer is then covered and the magnesium foundry al-
loy to lowered to the bottom. During the modification the iron temperature drops
by about 20 - 250C. Gases are removed from the mixer through pipes connected to
the fan system of the workshop. The method ensures magnesium modification to any
required extent. It is safe, does not require special space in the workshop and
can be integrated into the continuous conveyor casting system. There are 2 fig-
ures and I Soviet-bloc reference.
Card 1/1

VASILIM, I.G., inzh. (Leningrad)j PAVLOV, V~P.;, imb. (Leningrad)
Two-channel electronic switch for the cathode oscillograph.
Elek.i tepl.tiaga 6 no.404-35 Ap 162. (KERA 15:5)
(Oscillographs)
(Electric ovitchgear)

S/155/59/000/02/023/036
AUTHORSs Astakhoy, A.Y., Pavlov, V.P., Pavlotskiy, I.P. %
TITLE: Spectral Representation--oT-5~n-n-particle Green Function
dimensional Case
PERIODICALs Nauchnyye doklady vysshey shkoly. Fiziko-matematicheskiye nauki,
1959, No. 2, pp. 124-127
TEXTs Spectral representations of arbitrary multi-particle Green functions
are obtained in the case where the field functions only depend on the time
(unidimenstonal model). The results confirm that it is principally possible
to obtain the representations from the causality conditions and from the
mass spectrum alone ; a direct application of the results is possible, e.g.
in thermodynamics.
The authors thank N.N. Bogolyubov for the subject and the guidance, and
A.A. Logunov, B.V. Medvedev, M.K. Polivanov for advices.
There are 7 references: 3 Soviet, 2 American, 1 Swiss and 1 Italian.
ASSOCIATIONs Mookovakiy gosudaretvennyy universitet imeni M.V. Lomonosova
(Moscow State University imeni M.V. Lomonosov)
SUBMITTEDs March 21, 1959 CO
in the Uni-
Card 1/1

d7TT-HORS: Zavlyalov, 0.
TITLE: Matrix element
PERIODICAL- Akademiya nauk
25478 S/02 61/139/00 1 //0 1
B1 04YB231
1. and Pavlov, V. P.
of the reaction 7 + N4 7 + 'V + N at low energies
SSSR. Doklady, v. 139, no. 1, 1961, 79 - 62
TE)-LT: The authors had two aims in mind when investigating the rehcti-ns
mentioned in the title: to find expressions for the matrix elements, on the
one hand, and, on the other hand, good results serve as argument for the
primary conditions on the analytic behavior of the amplitudes in these
processes. As is shown by the present work, well verified formulas are
obtained by considering the closest singularities of the S-matrix. in
addition, prospects are outlined for improving these formulas. The three
reactions
r + P--)t T - + n; (1)
+ p --)T 0 + le + n ; (2)
+ p )1T- + To + P. (3)
Card 1/7

25~78
S/ ,20,
Matrix element of the reaction ... Bl-4/'B2,71
are examined and for simplifying the kinematic computations the nucleons
Rre assumed to be scalar particles. p,, p 2' P3$ p4t and P5 are the mcmenta
of the Ir"--meson, of the If-meson (at the end of the reaction), of the
neutron, of the ?,-meson (at the initial stage of the reaction), and of the
proton. The reaction (1) is described symbolically by
A 112
S = 1 t iA1 6 (Ep 211 (ti 1(j 2115W4(j 5) The amplitude A1 only depends on 2
invariant combinations of the p 1" invariants u ik ~ Uki ' (pi + Pk)
can be composed. The diagonal elements of the matrix u are related to the
2
masses of the particles participating in the reaction by u ii , 4 mi. The
conservation of momentum imposes 5 relations on the remaining 10 invariant3i
1 2 M2 (k = 1,2,~,4,5). Thus 5 among 10 variables u turn o-it
T~'k ik - 'k ' ~_ 1 ik
to be independent. For an independent variable the authors choose the
energy s 1 . U23 in the center-of-mass system neutron -2--meson, the energy
9 3 ' U 12 in the center-of-mass system of the ~_ and 17-meson, the energy
Card 2/7

;5478
S/020/61/139/001/010/018
Matrix element of the reaction ... B104/B231
a a U in the center-oll-mass system neutron and"q;'+-meson; u is chosen
3 13 35
for the'momentum transfer between the nucleons, and u for that between the. ;y,
14
mesons. As of late, the energy in the main channel of the reaction has been.

designated as u In case of the threshold energy W the
(M.+ ~)2
15
0 0
following applies: 9 a o', +/~,)2, so 4 2
M and /A denote the massed
1 2 3
of nucleons and mesons. If W exceeds the threshold energy the following.,
2 2 2 2
-W + M + 2/" i8
-,:~4/, and a, + 92+ 'S
applies: s1
A') 9
2>(M +
,
3
,
3
positioned within the region marked in Pig. 1 by broken lines. it is
moreover the authors' aim to obtain linear terms of a matrix element
expansion according to relative momenta of such part1cles as are parti*cip-
ating in the reaction. It is assumed that expression

t
+
A I (misIs3) A (44s~3 +
(s, (I S! it) (4)

CO OD
0
oji Is') ds'
+
Card 3/7 Sj) (S' S, it) (s, sop (s, S, =,a)
CN-LO,

Matrix element of the reaction ...
254T8
3/02 61/1-29/001/010/016
B104
X231
represents a good approximation of A
near the -threshold. 6~ (Y2, and 6-,
are determined from the unitarity condition. In (4) the closest
singularities are taken into accounti not however the pole terme of the
2 2
form ( a Sows Y )(S M ) nor the depend7enoe of A on the
1 .1
momentum transfer uik' which is, however, admissible in the approximation
wanted in this case. it is shown that the assumption of A being analytic
1
with respect to the variables u in the range of their values is justified.
ik
Finally the authors obtain
A, (sists,) A, (s,?4
+ ju, (sj + 10, (s,) + ju,
3
+ dr
A 310) S, (5)
Card 4/7

25478
B/02 61/139/001/010/018
111atrix el-ement of the reaction... B104YB231
and
ka
A,tt wn - -t-n); (6a)
yo~~w + + M,
kii
(A itt (n*n - :t*n) + A ~n*~ ep)) (66)
Ykf, + + Y;
as kit (6iB)
2
2.
A;(sososo) is-the amplitude of the reaction(l) with W (M + -In
1 2 3
addition /(xl-x-iE) - 13-1/(Xl-x) + i3r~(xl-x), whereTis the symbolof the
0 2
principal value. Due to the fact that the relation s a a - k applies to
the expression figuring under the integral of (5), the integral terms can be
neglected and
A, (-%SZS3)- A, (sls:sZ + i 1(y, (s,) + cr, (h) + cr, (Q). (7)
Card 5/7

-.2
1508-
,
S/020/61/139/001/010/01.8
Matrix element of the reaction... B104/B231
is obtained. Similar expressions can also be obtained for the reactions
(2) and (3). (7) not only determines the amount of matrix elements but
also'their phase. The expression (4) leads automatically to correct
expressions for the matrix elements wi th an accuracy up to the terms of
second order of the ralative moments. The au-thors thank A! A. Logunov a*d
L. D. Solov'yev for di-scussi6ns. There are 1 figure and 2 non-Soviet-bloo
references.

ASSOCIATIONt Matematicheskiy institut im. V. A. Steklova Akademii nauk
SSSR (Institute of Mathematics imeni V. A. Steklov Academy
of Sciences USSR)

PRESENTED: February 28, 1961, by N. N. Bogolyubov, Academician
SUBMITTED: Pebruary 23, 1961

Card 6/7

ACC NR, AP6025651 (_A SOURCE CODE: UR/01413/66/OOO/Oi3/0101/0102
::7VLNT3R; Zhukov, Yu. A.; Maminov, Ye. K.; Yanu6his, Yu. ?.; Pa,4crr, V. P.
3,-13 :None
T:T'-E: A device for testing footwear under dynamic conditions. CIU13B 142, 11o. 183467
lannounced by the Military Academy of Rear Lines and Transportation (Voyennaya aka-
demiya tyla i tran6porta))
SOURCE: Izobretaniya, promyshlennyye obraztsy, tovexnyye znaki, no. 13, i966,
101-102
'10KC TAGS: footgear, test stand, wear resistance
This Author's Certificate introduces: 1. A device for testing footwear
under dynamde conditions. The unit consists of a movable 'Last for the specimens of
footgear to be 'Vested, an attachment for controlling the pressure on the last, a
drive with crankshaft, connecting rods and cam mechanism, removable abrasive s-urfaces
and registration equipment. The machine components are mounted on a stand. -Irx in-
sta-Ilation is designed for comprehensive testing of a number of properties of foot-
gear, e. g. water resistance, sole durability and thermal insulation properties. T.-,e
device is equipped with a platform which is driven with a reciprocating motion syn-
chronized with that of the last. The abrasive surface or medium which interacts wita
Card 112 _ _ ___ uDc: 620.A.-685-31---

ACC NR, AP6025651
the fow~wear is located on this platforta. 2. A modification of this de,,ixe des~.,~ned
for t-asting performance characteristics both separately and in combination. Relay
units are used for recAprocal connection of the starting and registration devices.
I-last; 2-drive;
3--abrasive surface;
4--platform,
SLB CODE: 13, 15/ SUBIM DATE: IOMar65
Card 2/2

KOVTUNO G.P. [Kovtun, H.P.]; KRUGLY101, A.A. (Kruhlyk-h, A.A.];
FAVIDV, V,S.
Dstermining the vapor pressure in metalm from the vaporization
rate* Ukr. fiz. zhur. 6 no.3:386-389 My-Je 161.
(MIRA 14:6)
1. Fiziko-tc!7hnicheskiy institut All USSR, go Khar'vkov*
(Vapor pressure)

~)/) V L 0 V, V, 3,
~Z=
IVkWV, V.YE., MGLYKV. A.A., PAVWV, V.S., KOVTUN, G.P. &4D ATID!;EN.KO,V.M.
OXesaurment of t~w) vapor pressure of uranium containing compounds.*
Ropvr,t presented at the IAEA Symposium on thA Thermodynamics of !,Tjcloar
Materials.
Vienna, Austria 21-26 Pay 196-9

-1 17855~63 ~_..EWTOOADS M7T21PASD
ACCESSIDIUM.AP3003692: Z,695/0899
Ai=oa. Paylov V,S`. Danilyan, G.V.*,,Xoro11koj,
V~--TITLZ - RU inement of the decay~scbem-e Inl-16 /Report of the Thir eentb AnWa
scopy he-137TIi-xi
onference-on Nuclear Ppectro
ev, from 25.January to 2 Februarp
SOW=- AN SSSR, Iz-v, S criya lizicbeskayn, v.27, no.7, 1963, 895-BDD
topic TAGS~ Isoto'e activation,,
P nuclear spectrometry, decay schemes'ln
AMILACT: 'The primary-, purpose: ot tile worlt V, a's to - OValliate the SezsIbility ol u
Ing! a - closed'loop activation syptem for _.5tul:ting tho,decay of shortm-lived nuclides.
by.means of a magnetic gamma-spectrometer, in.view of-the f not that magnetic recoil:
s3~ectrometers are characterized by high nccuracy Sor obtaining energy nnd intensity
V.11,Uos but have tho*dr-awback of low efficienc , 'so that in tbo, case of short-lived..,
y
isotopes several activations are necessary to study the S ru a
ull spect M., The ctiva
on consisted of two stainless steel'tubes
-,one used, as the source, the oth-
r1ocated in the neutron :flvx near tho core of a heavy-WAtor reactor -.0 contrifu-
l
a
circulating pump an expansion chamber'nnd appropriate stainless steel connect-.
_Uilg.,tubing. The loop geometry vas such that 'tho Arradiation time was nbout 20 sec;.
b transit time 1rom irratiation tube'to source tube abou 8 sec. the full cycle

117855-63
,,,.._;,ACCESSION NR; AT.W03692
time 50 sec. The total volume of,the system, was about 5 liters. InI25
ed. -for, the test ekporiments, neutron capture.by this isotop results in f ormation
In116 in the ground state (T 13 sec) and in isomeric state (T = S4 min). The-
-'~I,material vas-eirculated in the,nctivation loop in the form of a, water,solution of
_In(NO3)3 (1 510 g per-5*:litors vater soiution).-- The neutron and gamma background was
dtte,nuated.by-:one B~C and 10 stool blocks with a total length of-1500.3nm. The Ban-
ma-ray spectrum of InI16 was measured 'in tho'rnngo. I.Tom.0.7 to 1.8 11W in 13 hev
steps 10.nin counting at each field, value). The 13-see activity 1vss distinguished'
by-damping the ranctor for.Z nin intvrvals.~ 'The onorgiez,and Intensities of
-"'~~-','~'the':Zletected~gamma-rays ;are tabulated together with the energy vnluos reported by
other authors. A relined decay schemo- is presented (see En losuro). "In 'conclusion:
c
*o,take this opportunity to thnnk N.A.Burgov for useful discussions. and
nce im th5'worjt.- Orig.art.has; I formula 4 :figures and
and G.V.Rottor for assista
.1 table.
ASSOCIATION- Inistitut teoretichesUoy I oRsperimental noy I Ixiki Goshumitota po nir-
nomu: is ol Zovaniyu atomnoy enorgil SSSR (Inst. al Theoretical h
p Bxporimental.
~-s gs . Stato~Committee on Peaceful Uses of Atomic 13norgy, SSSR)
-i SUUIMD- 00.:., ~ACQ: 02.ku-63 EXCM.01
SUB CODE: M SD NO REP SOV: 00-0 OMR: 007
C,
ari?,Ak,

KOVTUN, G.P.; OUGLYKH, A.A.; PAVLOV, V.S.
Electron gun for determining the evaporation rate of non-
volatile materials. Prib. i tekh. eksp. 9 no.2:130-132
Mr-Ap'64. (MIRA 17:5)
1. Fiziko-tekhnicheskiy institut AN UkrSSR.

"I- - PAVLOV9 V.S.
Heat exchange in zonal glass furnaces. Stek. i ker. 18
161. (,,ui~A 14:3)
(Glass furnaces) (Ifeat-Transaiosion)

PAVLOV, V.S.
Treatment of corn seeds with new growth promoting substances before
planting. Zemledelie 24 no,1:69-71 ja '62. (MIRA II-2j
1. Leningradskiy sel'5.kokhozyaystvennyy institut.
(corn (maize)) (Growth promoting substances)

dk
S"' uo, 5/ ()1 "OOu//OO3/Oo5/010
U208/D31)
AUTHORS KruUykh- A A Pavlov V.S ancl Tv.diins'):yy, 6 P
T ITLE Grain growth in c~irotriii_,.Ln
PERIODICAL Ukrayins kyy fizyciinyy zhurnal v ~,, no. 3. 19b!.
-)94-397
TEXT; The study of grain growth in chromium is of practical inter-
est in connection with the use of chromium as a heat-resistant mat-
erial In literature there are data on the recrystallization of
chromium of various degrees of Durity. but there are none concerning
C)
grain growth. V i Axkharov, V i 3hangarev (Ref, 1: R-al, 6. no. 1.
82, 1958); S T-M Johnstone (Ref, 2- Nature. 181, 806. 1957) In
the present study, grain growth was investivated under isothermal
annealing for the purpose of (IeLerminin~% the rate of growth and the
activation energy. Ghromium was use(I aith an admixture ar, ';pecilied
in the table. The specimer,'. were ma:le of.glates which were obtain-
ed by condensation in a hign vacuum (I ,10 mm lig), on a tanta'um
surface at 5000C, The plates were rolled at room temperature so as
C ard 1/4

23292
S/185/61/006/003/005/010
Grain growth in chromium D208/D302
to thin them by 30~i'a'. Then they were annealed for 10 hours in a
vacuum, at 9000C Thus a near-equilibrium structure was obtained
The author stresse.,., the fact that after the treatment the widLh of
the d .2ndrites was reduced from 50 to 30 f, (microns), After anneal-
ing at 9000C,. the plates were again rolled at room temperature, and
the growth was investigated (by ~-etallographic methods) after anneal-
ing at temperatures of 900. 950. 10M L050 and 11000G. ,Phe results
show that the thermal fluctuations are greater at high temperatures
than at low, and they lead to centers of recrystallization which are
more numerous at 11000C than at 10600C This explains the fact t:iat
the average size of the gr2ins is smaller at 11000C than at 10500i~.
Ilie linear dependence of D on time shows th-at graiii growth in
chromium follows the statistical law D
2 _ D2 . Kt (1)
where K ~ Koe - ~T (2). Do - diameter of grain at t z 0,
K - rate of growth, activation energy which is numerically c(l,,ial
or nearly equal to the activation energy of self-diffusion at the
boundaries of the grains, Ko equals 1 cm~/sec in the investigated
temperature range D9
0 was obtained by extrapolation The rate of
Card 2/4

S/18
Grain growth in chromium YI) 61/006/003/005/010
D208 302
growth at Vnrious temperatures was calculated by Eq The temp-
erature dependence of K in coordinates IgK - I was linear. The
T-
obtained value of the energy of activation was 53 � 5 kcal/g.atom,
which is in agreement with B.S. Bokshtein, S.T. Kjsh]-~in (Ref. 5:
Zav. Lab., 23, no. 3, 316, 1957) and Gondolf 2akston (Ref. 6:
Arch. Eisenhifttenwesen, 30, no. 1, 55, 1959). The equations were
taken from D. Burke, U. Tarnball (Ref. 3: UP1,1, 1, 368, 1956) and
P. Feltham, (Ref. 4: Acta.Met., 6,.no. 8, 539, 1958). There are 4
figures, I table and 7 references: 3 Soviet-bloc and 4 non-Soviet-
bloc. The references to the English-language publications react as
follows: S.T.M. Johnstone, Nature, 180, 806, 1957; P. Feltham, Acta
Met., 6, No. 8, 539, 1958.
ASSOMATION: Fizyko-tekhnichnyy instytut AN USSR (Physicotechnical
Institute, AS UkrSSR) 1(har'kov
SUMITTED: July 1, 1960
Card 3/4

) VZ 6,V,
P
umlsl~id Stat~/Hijd'cs - Hech-nical Properties of Crystals E-9
and Poly-Crystalline Coupounas
Abs Jour : Ref Zhur - Fizika, No 11 190, 1083
Author : G~Wdukov, M.G., Pavlov, U.A.
Inst : Institute of Physics of Metals, Ural' Branch kcademW of
Sciences, USSR.
Title : Relaxation of Stresses in Alloys of Aluminum with
M&Epesium.
Orig Pub : Fiz. metallov i metallovedeniye, 1957, 4, No 1, 123-130
Abstract : An investiption vas nade of the relaxation of stresses in
alloys of aluminim with nagnesium at a tenperature range
fron 100 to 300 C vith initial stresses of 30D g1nmA.
It vas established that there is an increases in the rela-
xation stability of Al-Mg alloys, compared with pure alu-
minurn. 7he increase in the relaxation stability is
Card 1/3

SNMUD, Fred, I,; MWILL, Anthony; SWWGV,Tu.V. [translator]; DITAK06-
NOV,A.I.,Etranslatorl; LTUBIHOV.S.A. (translator]; VOLUDIN,N.V.,
[translator]; RUSAVOT.P.L. redaktor;PJM
RASIMOV,Te.S., telffinicheekly redaktor redaktor; ON-
[Protection for people, buildings and equipment from the atomic
bomb. Translated from the Raglish.) Protivostomnala zashchita
lludei, sdanti I oborudovaniia. Perevod a anglilokogo IU.V.Seme-
nova i dr. Moskva. izd-vo inostrannot lit-ry, 1955. 292 p.
(KLRA 9:3)
(Building. Bombproof) (Atomic bomb--Safety measures)

~ 'PVL,11/ ,/"0 '-
ALIPOV, N.Y. [translator); LUSHNOV,
IOVLIWA, N.A., tekhn.red.
N.P., red.; PAVIOT, V.S., red.;
[Nuclear weapons. Translated from the English] Atomnoe oruzhie.
Pod reds B.P.Lushnovs. Moskva, Izd-vo Inostr. lit-ry 1957. 71 P.
NIRA 11:4)
1. Scotland. Home Department.
(Atomic weapons)

*I
LAWSON,D.I.; ILIPOV.N.V. [translator]; PAVLOV V.S., redaktor; BIMA,
M.A., tekhnicheEkiy redaktor fe`~'-:- I
[Fire and the atomic bomb. Translated from the Nnglishl Atounais
bomba i po2hary. Perevod a angliiskogo N.V.Allpova. Moskva, Izd-
vo inostrannoi lit-ry, 1955. 44 po (HLRA 9:3)
(Atomic bomb)

STEPANEENKO, M.G., doktor tekhn.nauk, prof.; PAVLOV, V.S.
Method of calculating tank glass furnaces with developed working
end arrangements. Stek. i ker. 19 no.):1-6 Mr '62. (MIRA 15:))
(Glass furnaces)

KOVTUN., G.P. [Kovtun, H.P.]; kMUGLYKH, A.A. [Kruhlykh, A.A.]; PAVLOVI, V.S.
Vapor pressure and the evaporation coefficient of nickel. Ukr.
fiz.zhur. 7 no.4x436-438 AP 162. (MIRA 15:8)
1. Fiz-Lko-tekhnicheskiy institut AN UkrS.SR, g. Kharikov.
(Nickel) (Vapor pressure)

PAVLOVP V.S.; DANILYAN, G.V.; KOROLIKOV, I.Ya.
More precise definition of the InI16 decay scheme. Izv. AIN SS&R.
Ser. fiz. 27 no.7:895-" 163. (ICRA 16:8)
1. institut teoreticheskoy i eksperimentallnoy fiziki Gosudarstvennogo
komiteta po mirnomu ispollsovaniyu atomnoy energii SSSR.
(Indium isotopes--Decay) (Gamma-ray spectrometry)

PAVLOV, Ye&S9
Deep faults and the distribution of enodgenic mineralization in
the Maritime Territory. Sov.geol. 7 no.2:18-29 F 164. NIRA 17:3)
1. Vsesoyuznyy nauchno-issledovatellskiy institut minerallnogo
syrIya.

ACC N% AF6036452 SOURCE CODE: UR/0370/66/000/oc)6/0169/0172
AUTHORS: Kruglykh, A. A. (Kharlkov); Favlov, V. S. (Kharikov); Smirnov) Yu. N.
(Kharikov)
ORO: none
TITLE: Oxidation of zone-refined cerium
SOURCE: AN SSSR. Izvestiya. Metally, no. 6. 1966, 169-172
TOPIC TAGS: cerium, cerium oxide, oxidation kinetics, oxidation
ABSTRACT: The oxidation kinetics of cerium was studied as a function of the purity
of the metal. The experiments were carried out in the temperature region of 150
300C. The mass increase of specimens was determined after the method of V. Ye. Ivanov,
A. A. Kruglykh, V. S. Pavlov, et al (Opredeleniye uprugostey parov
uranosoderzhashchikh soyedineniy. Sb. Termodinami-ka yadernykh materialov, Vena, 1962,
735). In addition, the microstructure and x-ray structure of the surface of tae
oxidized specimens were determined-. The experimental results are preeented ir, grapi-,s
and tables (see Fig. 1). It was found that the oxidation of 99.3' Ore cerium
follows a linear oxidation law, that of zone-refined cerium (zone-refined up to 200C)
follows a parabolic law. The oxidation of high temperature zone-refined cerium (zone- :
refined above 200C) follows a linear law. The complete combustion of compact 99.3,-ta'
Cc occurs at 300C. It is concluded that the removal of low-valence type metals from
UDG-
.69!

ACC NR. AP6036452
AP /06, (g/cj2
Fig. 1. Kinetic oxiaation
curves for the oxidation
before
of 99.3% Ce. (a)
and (b) - after zone-
refining; L P - mass
increase of specimen
zoo 4017 no 0 zoo Ox T, 12:1~
cerium increases the stability of the metal towards corrosion. The authors tnanic G,
N. Kartmazov for his help in the evaluation of the experimental results. Orig. art.
has: 3 tables wA 2 graphs.
SUB CODEs //
Card 9 19 p 07 SUBMDATFs 16kpr65/ ORIG W: 0031 OTH REF: 002
a
ZWT
Woe

7-
b
3on isale
/
too C
-C

far

15(2)
AUTHORS: Steparienko Z, G kavlov V S, SOV/72-~)9 4 2121
TITLE; On the Effect of a Blocking Device on the Thermal Balax;p of
the Cooline Part of a Tank Furnace (Vliyaniye zagraditel-nogo
ustroystva na teplovoy balano studochnoy chasti vannoy pechi)
PERTODICAL. Steklo 1 keramika 19c,9 Nr 4. pp 6 11 (USSR)
ABSTRACT: For the purpose of increasing the opecific output of aWal
the melting temperature of the furnace must be increased Since
the working temperature of the glass mass must , however, remain
unchanged in this case, the processing part of the furnace had
to be screened off However,, it was found in this connection
that the temperature of the flow of the glass mass to be
processed was considerably lower. Since nothinE else had been
changed in the design of the furnace this could only be ex-
plained by the introduction of' the lower colder glass mass
into the flow to be processed which was confirmed by temper
ature measurements performed by the teplotekhnicheskaya labora-
toriya Inatituta stekla (Heat Engineering Laboratory of the
Glass Institute) and foreign inveatigations (Ref 1) This
might, however, cause deterioration of the quality of the
Card 1/3 glass mass For this reason, investigations had to be carried

On the Effect of a Blockine Device on the Thermal SOV/72 2,Z'
Balance of the Cooling Part of a Tank Furnace
out in order to find a dezAgn of screening which would ;-uaran-
tee an increased output of glass mass without a deteriarat'Lor,
of the quality, In fiGures 1,2.3. and 4 the different types of
furnaces with and without shuttle are shown and discussed
The velocity of the upper layer of the glass mass was deter-
mined by using floats and the amount of the convection cur-
rents by using the A. A. Sokolov formula (Ref 2). In table 1
the technical and operational characteristics of the furnaces
investi.gated are given and table 2 gives the ther-mal jalances
of the cooling parts of the tank furnaces In table i tho
balance of the glass mass in the range of the blocking devices
of the furnacesis given Ulaximum specific temperature dro-,s may
be observed in tanks with deeply immersed shuttles and low
screens This explains the opinions expresned by I ! Tukh
and M R Fpel'baum (Ref 3) In table 4 the thermal b;ilan~ns
of the flow to be processed in the range of the screening de-Tlrh
of the furnaces investigated are given Figure 5 show-5 the
dependence of the output of first--quality glass on the coef
ficient of the introduction of the metal. The investigations
Card 2/3 carried out of the furnace output as well as the operationaa

On the Effect of a Blocking Device on the Thermal SOV/72-~Q 11-2 2,
Balance of the Cooling Part of a Tank Furnace
and technical tralues are considered to be a beginning of the
investigations of a screening device which makes it possible
to find an optimuz design and optimum operational conditions
for increasing the fusibility of the tank furnaces without
risks The influence exercised by the blockin(r, device in the
quality of the production muot also be thoroughly investigated
There are 5 figures 4 tables and 4 references 3 of' which
are Soviet
Card 3/3

VIIRIS, K.K.; POLLTAK, V.V.g PAVWV, V.S. _
Spbeific amount of glass output as an indicator of the productl~vity
of tank furnaces. Stek.i ker. 17 no.3:9-14 Pr 160.
(Mr" 13:6)
(Glass furnaces) (Glass manufacture)

STEPARZKO, M.G.; FAVL(YV, V.S.
Ways of inproving the productivity of pot furnaces for plate glass.
Stek.i ker. IS no.8:12-15 Ag 161. MU 14: 8)
(Glass furnaces)

L 11436-67 Elffr 1 FCC GY/GD
ACC NRI AT6021020 SOURCE CODE: UR/0000/65/000/000/0096/0100
AUTHOR: Pudovkin I. M.; Pavlov, S.; ealLetoy B. P.; az ntacy,
Tanichev, A. A.
iORq: none
TI~LE: Some results of observations of secular variations in the geomagnetic
el iments of Kamchatka
f
SOURCE: AN SSSR. Inatitut fiziki Zemli. Naetoyashcheye i proahloye magnitnogo polya
ZeTali (The present afi~pas_t OC-the dearth's magnetic field). Moscow, Izd-vo Nauka,
1965, 96-100
TOPIC TAGS: geomagnetic field, geomagnetic drift, secular variation
ABSTRACT: Wcal and regional characteristics of secular variations in the geomagnetic
field on Kamchatka were studied experimentally in 1961 and 1962. Regional differences
in the average annual values of D, H, and Z are shown in Fig. 1. From these differ-
ences isopores are constructed. The variations ranged for 6D from -5.5 to + 2.4; for
SH from 3 to 41y; and for 6Z from -19 to + 22y. The quantity D was measured with an
accuracy of � 1'. 1, H with � 5y, and Z with * 13y. All three elements (6D, 6H, 6Z)
clearly show the zonal structure of secular variations which agrees with the general.
orientation of the basic tectonic structure of Kamchatka. Local anomalies are illus-
trated in Fig. 2. According to these results, a complex morphological
4

Fig. j.. Keglon" aliuwa- -A ---
Periods denote observation points; numbers near the perioda show differences (1962-
1 1961) for 6D (in min), 6H and 6Z (Y )

L 11436-67
-ACC NRi A .TW-foio
i~'Si~flfl
f
3.0 if
it
C'q 11 R-'\ NI
lilt JI j
/ If
CR 0
Fig. 2.' Local anomalies in secular variations on Kamchatka in the region of Vauzhetka.'
Periods denote observation points and differences (1962-1961) for 6D (in min), 611 and
6Z (inY

L 11436-67
. I ACC NR. AT6021020
. 16tructure of secular variations exists on Kamchatka. Both local and regional anoma-
lies are present. Further studies into the anomalous character of secular variations
by magnetodynamic methods are recommended. Orig. art. has: 2 figures.
SUB CODE: 08/ SUBM DATE: 2lSep65
4

-, L 1,12(c) JDAXAM
ACC NRv AT6010591
SOURCE CODE: UR/0000/65/000/000/0163/0168
AUTHOR- Amonenko, V. M.; Kmg!ykh, A. A.;,.-Pavlov, V. S.; _Dlyakov, L G.
Balenko, E. P.
ORG: _ Physicotechnical Institute, AN SSSR, (Fiziko-tekhnicheakly institut AN SSSR)
TITLE: On the possibility of purifying cerium by zone recrystallization
SOURCE: AN VkrSSR. Fazovyye prevrashchenlya v metallakh i splavakh (Phase
transformations in metals and alloys). Kiev, Naukova dumka, 1965, 163-168
TOPIC TAGS: metal zone refining, cerium, recrystallization, 3 0.NL.
ABSTRACT: The object of the study was to determine the distribution of fmpuiritfesl~
(lanthanides, silicon, magnesium, iron, and copper) in cerium during zone melting of the
latter. The process was carried out at 3 x 10-10 mm Hg on cerium wfilih-WOWR-Fbeen re-
melted for one hour at 1423K at the same pressure. no molten zope was produced by
electron bombardment, and its travel rate was varied from 5 to 0. 15 MM/min. The refining
process turned out to be most efficient at a rate of 0. 5 mm/min. However, zone melting is
not effective in removing other rare earth metals from cerium. Iron, copper, and silicon
impurities are driven to the end of the ingot and have !! distribution coofficlent K < 2. After
ten passes, the iron content decreases by a factor of 5, and the silicon and copper contents
decrease by a factor of 10. Magnesium 1B removed chiefly by vaprization as the zone Moves
Card 1/2
1
, Card

L 32066-M EWT(m)/9WT(t)/Er1 IJP(c) JD/JG
ACC NR: AP6013334 SOURCE CODE: UR/0363/66/002/004/0578/0681.
AUTHOR: Amone-ko, V. M.; A. A.; Pavlov, V. S.; Mosova, L. N. '2
ORG: Ph~sicotcchnical Institute, Academy of Sciences UkrSSR (Fiziko-tekhniche6k'
institut Akadernii nauk UkrSSR)
V1 IF
TITLE: Purification of cerium by electric transfer combined with zone melting
SOURCE: AN SSSR. 17.vestiya. Neorganicheskiye materialy, v. 2. no. 4, 1966, 578-581
TOPIC TAGS: cerium, metal zone refining, metal zone melting
ABSTRACT: To determine whether cerium can be purified by combining electric transfer
with zone melting, molten cerium samples were refined by passing a current of 5.3 A/mM2
in a vacuui-. ."or 50 - 150 hr. Iron, silicon, copper, and oxygen impurities were f.-lund
to move to the cathode. The experiments were then repeated in helium; after 200 hr, the
amount of impurities remaining in the cathodic and middle portions of the sample dropped
below the sensitivity limit of spectral analysis. The samples were then subjected to zone
melting, whose effectiveness was found to increase when an electric current (6 A/mm2)
was passed through the metal. The amount of impurities thus dropped from 0. 245% in the
Card 1/2 UDC: 546.655

PAVLOVY VOSO
ipplication of growth promoting substances to corr.. Bot.1 inal. Bel.
otd. VBO no.6#43,48 164. (MIRA 180)
*.

S/I l7/6O/G00/D06/00-'/0 .1c
A004/A--,--2
AUTHOR: Pavlov V.S.
TITLE, Spiral Borin Tools
PERIODICAL: Mashinostroitel', 1960, No. 6, p. 21
TEXT; The author reports on new high-speed and carbide-tipped spiral
boring tools which, in contrast to those manufactured abroad and by Soviet plants
(e.g. "Frezer~'), distinguish themselves by a more simple manufacturing technclogy.
The new high-speed steel boring tools do not undergo mechanical tooling but are
cast by the dispensable pattern method with insignificant tolerances for the
grinding of the main back and auxiliary angles. For operations at higher rates
and for the machining of materials with a higher degree of hardness, another
tool design has been developed. This cutting tool has a monolithic carbide bit
and is designated for the boring of 15-20 mm apertures and for threading operations.
The tip is fastened with the aid of copper solder. Another design of spiral
boring tool was developed for the machining of apertures in the range of 20-25 m-m
and more and for the cutting of internal threads. The tools are fitted with
carbide bits of the T15-16 grade (for steel) and BK-8 (VK-8) grade (for cast iron).
Card 112

S/117/60/000/006/003/~10
Spiral Boring Tools A004/AO02
Since only the front edge of these bits Is ground - the back angles of the tool -
are permanent as they form an Archimedean spiral and screw line - the life of
these tools exceeds that of ordinary boring tools by 5 - 6 times and results in
savings of carbide. The author describes a simple device for the grinding of
spiral boring tools. There are 4 figures.
Card 2/2

-L'U443_62 EPA(s)-2/EWT(m)/EPY(n)-2/E~P(t)/Zi&(b)~ _Pt__7/Fu_4 !JP(c;-)
JP/WW/JW/Ja
ACCU010 IM s: A?50UO69 MV0183/65/010/004/04*010.
EnLl ~kh A. 'A..- (Xz1Ug1ykb pAA IKuvtuni He-P.
AMORS (Kovtunj, G. P.)j Tzrlavy
M=f Wurited- vapor, tension of erbium
eaziarium,,. and yttefbivxi 3
PX 22
SOURM Ukrevino 14y fizychnyy zhiurma vo - lo no. 4~ 1965,, 432-439
orbi=, samariump ytterbi=j rare. earth element etrt-
TOPIC MW 0 vapor tenrdon$
.,Rion method$ sublimation heat.. sublimation entroW e
_ABSnWTs -,Cozrtinu~ an earlier investigation ofthe vapor tension of gaftlia-i
and disprosium (Ukre fix"bn th y9_ 91 not 10) 1964) the authors detemine Van-,
satura
ted vapcri tension of erbivmp sv=r1uwj. and ytterbium in the twperxture
ramen 915e.-1180, 84--721p and 3901-494C reapective3,y by the Knudsen efffualt~A
*dj, -in vhicb the - difference between the veights of the efftsion cell befora t~md
after the experiment Is determined. The eMsion chamber and the oven UnfA to haat
it are WIMM in 5u. I of the ftalame, 2h* esperlmental reml-to fit vell the
foL Ing 13
UvUS wPatimst log PM 6-9 - (13230/T i log PM 7.4 - (870V..T
c6m ~1/3

:ACCESSION NRS AP4040990 S/0279/64/000/003/0158/01W
!AUTHORS Ammankop V.M. (Kharkov); Krug3^h, A.A. (1harkov); Pavlovp V*3*
. . .......
(Kharkov); Tlkhinakiyp GoF* (Kharkov)
;TITLES Evaporation rate of components in thermal dissociation-of
,Yttrlu= and lanthanun ber7llides
SOURCE: AN SSSR. Isveatiya. Motallurgiya I gornoye delo, no. 3, 196jo
i158-160
ITOPIC TACSt yttrium, yttriun beryllide, lanthanuu, lanthanum berylli&,
beryllide dissociation, beryllium vapor pressure, thermal diosocier
Ition
ABSTRACTS The evaporation rates of components of yttrium and lantha-
nu-m beryllides during thermal dissociation of yttrium beryllide at
1040-1290C and lanthanum beryllidt at 1060-1270C have been deter-
,mined. YBe,3 and L Be, beryllides vere prepared by sintering 99.95%-
pure beryllium powd:r vith povders of 99.82-pure yttrium or 99.4%-pure
lanthanum. From the auslysis of x-ray diffraction patterne,chemical
analysis of the condeneste,and calculated values of the vapor pressure
i
of yttriump berylliump and lenthanum, It is concluded that both beryllides
!Cord

KRUGLYKE, A.A. [Kr-uh-'yYh, A.A.jj FAVLOV, '1.S.; TrKHRISKIY., G.F.
17'ykhir,s'kyi, F.P.]
Vapor pressure cf solid yttrium. Ukr. FJz. 2~-,,Ur. 9 no.2:
( %,I I F,', ' ~ . -7 )
214-215 P64 J.. I
1. Fiziko tekhni,-,haskiT incstltut AN Uk-r&'QR, K~arlkov.

AUTHORS: Krug ly A. A.
T IT LE. R -r Y s a I z i i n f
PERI,jDI,-'AL. FlzarLl.
pp
A BS TR A,"

0 -
x 3
.
0.
"hi
va cuu,-.,
a t a ;Lli:!!-,,:)C---,, ll*-~!-(A -~f If 5~~
struct;~ire, 491,-. plates lw~--trc s,, b j e c
G Y i (1 1 z I c- c i t
in air the refl,)ctir)n ln -trr~a ii, r ~il i r i wa
by allnoa II 1"c '~Qo
-7~6'3T' t C~ ~U -"I', C T ~ 5
5 hou r s a
1
Card 1
Specimens w~,rr- again J e f r m e (l by aj,7n~- '~iq i
re 11 A i-,i,, und--~r th (3 same d L 7~ c n:1 a

2",/0 0

Recry-, tal i iza
right-ang-es
Tj e c irl c- n -i
F,
f t 2 -f
sc

c'll t--'e
o nd i nate
e a bc

eo z, in e

Card rvr t
2
/ 2 tom
- ere L, t~l
Soviet E
ASSOC IA f I GN r v V

SR
SUBEITTED:

S/032/60/026/05/47/063
/Rr)~00 BO10/BO06
AUTHORS% Amonenko, V. M., Kruglykh, A. A., Pav
Tikh1ngW17y, G. F.' Wv
TITLEt Manufacture of a Berzllium Foilv~
PERIODICAL: Zavodskaya laboratoriya, 1960, Vol. 26, Wo. 5, pp. 625-626
TEXTt Beryllium foils of a thickness of 20-300 u are used for the
manufacture of X-ray counter tube windows. 'With the existing methods
for the manufacture of such foils there is the difficulty of obtaining
foils which are sufficiently plastic at room temperature. A method
according to which beryllium is deposited by vaporization on a polished
molybdenum lamella in vacuum (approx. 10-6 mm Hg) is described. The
beryllium is deposited by vaporization on the preheated molybdenum
lamella from a BeO-crucible at 1300-15500C in vacuum and then treated
thermally (in vacuum). The dependence of the plasticity of the finished
beryllium foil on its thickness (Fig. 1), on the temperature of
condensation (Fig. 2) and the length of the thermal aftertreatment
(Fig. 3) was investigated. Vacuum tight and plastic foils are obtained
Card 1/2

KRIJGI.W . A.A. [Kruhlykh, A.A.]; PAVLOV, V.S.; TIKHIHSKIY, G.F.
(Tykhinalkyi, H.P.)
Grain growth in chormium. Ukr. fiz. zhur. 6 no-3:394-397
My-je 161. (MIRA 14:8)
1. Fiziko-tekhnicheskiy institut AN USSR, g. Kharlkov.
(Chromium--Metallography)

S/18 62/007/003/014/015
D299YI)301
Kovtun, H.P., Kruhlykh, A.A. and Favlov, V.S.
On determ,-ning the vapor pressure of metals by the
T' E.
rate of evaporation from a cylindrical cm cibe
FEIRIODICAL: Ukrayinslkyy fizychny-y zhurnal, v. 7, no. 5, 1~1,~21
336 - 5~7
'2---'XT: The depenuence of the rate of evaporation on thp ra*.,.
o-, the leneth - to the diameter d of the crucible, was investigated for
~~,Iver 0.15) and chromium (-- 0-5); -~,is the ooefficient of eva-
'poration. Molybdenum crucibles were used, with different i/d. From a
lormula, obtained by the authors in an earlier investigation, it follows
that if the ratio ,d is sufficiently large, the vapor pressure can be
determined by the formula
G 2 7- R T
P 'PRT
5 - K M
Card 113

5/185/62/007/003/014/015
On determining the vapor pressure ... D299iD301
where G is the rate of evaporation, S -- the evaporation surface and
K -- Clausing's coefficient. A figure shows the dependence of the rate
of evaporation on *. /d. It was f ound that, from a certain value of /-i
on, the rate of evaporation changes only insignificantly at constlint
/d, f--r
.emperature. There exists, for various metals, a certain ratio
wr.~ch the vapor pressure is ex,;~ressed by forraula (2). For chromiur-.,
value is /d ~~ 8.5. In order to verify this assumption, the vapor rrc--,s-
u--e of chromium was measured at temperatures of120O - 13500C. The eva-
poration took place simulataneously from 2 cylindrical crucibles, w-*'.,.
/d = 6.5 and"/d = 4.5, respectively. The rate of evaporation was f(--ina
to be practically equal in both the long- and the short crucibie. A flim-
ure shows the temperature dependence of the vapor pressure, caiculate(;
by the rate of evaporation from the crucibles with L./d = 8.5. By prc)ce---
ing the results by the method of least squares, the following equation
for tne vapor preagure of' chromium in the tomperature rayVe of 1200-15'-~Olv
is obtained: IgP - 10.590 - 20830/T, which is in good agreemnent witY. t--
results of other investigators. There are 2 figures, 1 table and ~ ref-r-
Card 2/3

S/185/62/007/003/014/015
On determining the vapor pressure ... D229/D301
encess It Soviet-bloc and 1 non-Soviet-bloo. The reference to the Englisr.
!anjuage publication reads as followot M.G. houaman, .1. Jarwood, J.Aj,pl.
Phys., 5, 7, 1954.
kSSOCIATIOI;i
SUBMITTEDs
Fizyko-tekhnichnyy instytut AN URSR (Physicotechrical
Institute of the AS UkrRSR), Kharkiv
December 1, 1961
Card 3/3

3/1'85/62/007/004/014/018
Yro D407/D301
AUTHORS: Kovtun, H. P., Kruhlykh, A. A., and
V. S.
TITLE: Vapor pressure and evaporation coefficient oil
nickel
P2RIODICAL: Ukrayins'kyy fizychnyy zhurnal, v. 7, no. 4,
1962, 436-437
T-XT: The vapor pressure and the coefficient of evaz=ation
01 nickel were dezer~,ined by the method of evaporation from a
cylindrical crucible and by Knudsen's effusion method. The
first method was described in an earlier work by the authoro.
Thereby, the vapor pressure was calculated by the formula
G r I RT~
.P
S K CAI M
Card 1/3

Vapor !ressure and ...
S / 18 5 /6 2110 () 7 /0 0 4/0 14/3
D4U(/J_~Ui
o~-served. The resu-I I's obtained by -.he first. and sec~,ncd
were -n zood agree::~en-,. led -~c the conclusion that ~'-e
Coef.-cfent of evar=ation of nickel does not d,-ffer
--n-' ty. T -,~re and 9 ref,~roncos: '~)v-
:-,ere are 1~, ') -
and 5 non-Soviet-b-oc. 4 most rucent re_",?rL',`,Ces
zn,:- -!-~n.-uage
- 'ish c a f , n s:- t:aJ a s f o 11 c),. s
4-;
Soc., 62, u
382~ Vj
J. Che:7~. '_`oc . , ' ~5 Hi_rt'., a-nd
26, 1,216, I~t:17- ',':,rth and G. M,. lound, hy i~
Ciiem., 64, 619, 1960.
S- 0 C, _- AT 3 _N F '_zykc,-tejk',.n_-'chnyy instuytut AN "iHSH (PhYsico-
tec',-.nical :nstitute of the AS UkrRSR), Khar'-4-v
S'~: IL, -. 2 T Sep~ember 23, 1961
Card 3/3

AMONENKO, V.M.; KOVTUNJ, G.P.; KRUGLYKH, A.A.; PAVLOV, V.S.
Absorption of air by aluninum oxide. Ukr. khim. zhur. 29
no.10:1109-1110 163. (MIRA 1'7..l)
1. Kharlkovskiy fiziko-tekhnicheskiy institut AN UkrSSR.

ACCESSION NR: AP4033131
s/0!20/64/000/002/0130/0132
AUTHOR: Kovtun, G. P.; Krugly*kh, A. A. a Pavlov, Y. S.
TITLE: Electron-beam gun for detern-dning rate of evaporation of low-volatility
materials
SOURCE: Pribory* i tekhnika eksperimenta, no. 2. 1964, 130-132
TOPIC TAGS: electron beam gun, low volatility, low volatility material,
vaporization rate, evaporation rate
ABSTRACT: Unlike J. Pierce's ideal system (J. Appl. Phys., 1940, 11, 548).,
the gun described in the present article has both cathode and anode in the form of
two semiplanes at an angle of 1350. Three guns. (see Enclosure 1) have a
common anode 1 and separate cathodes 2 with moly lead-ins 3. Slits 4
(55 x 5 mm) serve to pass the electron beams, while alit 5 (40 x 6 mm) is intended
for viewing. Channels 6 pass cooling water. Max electron current, 1-1. 5 amp
1/13

ACCESSION NR: AP4033131
at8-10kv. Specimens of up to 8x30 mm. are acceptable. Tungsten and graphite
specimens were heated up to 3. OOOC. The gun is recommended for studying the-
evaporation rate, vapor pressure, recrystallization, cyclic thermal treatment,
and other high-temperature problems. Orig. art. has: 2 figures and I table.
ASSOCIATION: Fiziko-tekhnicheskiy institut AN UkrSSR (Physico-Technical
Institute, AN Ukr&%Q
SIMMITTED: 3OMay63 DATE ACQ: I lMay64 ENCL: 0 1
SUB CODE: PH
NO REF SOV: 000 OTHER: 003
2X
-77777

ACCESSION NR: AP4029844 8/0279/64/000/002/0177/0179
AUTHOR: Kovtun, G. P. (Khar'kAyv); Krugly*kh, A. A. (Shartkov); Pavloy, V. S.
(Khar1kov)
TIUSt Vapor Paramours of solid beryllium
SOURCE: AN SSSR Xxv. Metallurgiya i gornoye delo, no. 2, 1964, 177-179
TOPIC TAGS: vapor preasure, beryllium, evaporation, Langwuir method, Knudsen
sublimation
ABSTRACT., Since the purity and technollogy of beryllium have been improved, it has
;become necessary to know the temperattiuc dependence of vapor pressure for the purest
~types. The authors have determined the vapor pressure of beryllium the over-all
purity of which considered non-metallic impurities at not less than 99.95%. 71.2
Fe, Si, Al, Cr, and Ni impurities did not exceed 0.001% for each component. The
calculation for the.vapor preasure was conducted by the following formula (using
Knudsen's method)
P
iv M
Card 1/2

;ACCESSION PIR: AP4029844
I P f -2,tRT (2)
'in Langmuir's method av M
wbere P is the vapor pressure,, G is the vaporization rate; R is Clauzing's coefficient
cc is the vaporization coefficient. Orig. art. has: 3 figures and I table.
ASSOCIATIONt none
SUBMTTED; 13Jul63
SUB COMs IML
CDrd 2/2--
DATE ACQ: 30Apr64
WD REF SOV s 000
ENCL: 00
OnMR: 003
.. . ...