SCIENTIFIC ABSTRACT VERT, ZH.L. - VERTEBNYY, V.P.
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December 31, 1967
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SCIENTIFIC ABSTRACT
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3/081/60/000/012(1)/001/002
A0061AOol
Translation from: Referativnyy zhurnal, Xhimiya, 1.960, No. 12 (1), p. 86$'
# 46084
AUTHORS- Tverdovskiy, I.P.., Vert, Zh.L., Karpova, H.A., Mosevich, I.A.
J~ -1 4
TITLEt On the Solubility of Hydrogen In Alloys of Palladium With Silver,
Copper and Gold ~1
PERIODICAL: Sb. tr. Goa. in-ta prikl. khimii, 19f)9, No. 42, pp. 182-198
TECT: The author puts forward a scheme of distribution of electrons and
"vacancies" in 4d- and 5s- bands in the Fd - Ag system and in 4d- and e- bands
in the Pd-Cu system. Using simulation notions and assuming a limited number of
vacancies for hydrogen dissolution in the Pd - Ag, Pd - Cu and Pd - Au systems,
isothermal equations of hydrogen dissolution in the alloys are obtained. They
serve to determine the magnitude of the chemical potential of hydrogen dis-
solved 6 1" H. and the coefficienttG , characterizing the deviation from the
idea2 state In the Langmuir equation. An equation is obtained for calculating
Card 1/2
S1108116010001012(I) /00 1/002
A006/AO01
On the Solubility of Hydrogen in Alloys of Palladium With Silver, Copper and Gold
the differential heat of hydrogen dissolution Q ((B and its applicability
is demonstrated. Authors' reEume
Translator's note: This is the full translation of the original Russian abstract.
Card 2/2
IP
114) S-10,111/2 0- ' 2--4-30 "-,r)
AUTIIOI,ts~. Tvr!:,dovsk~'y, 1. P., 7e::A, Zh.L., Foiidrushrf, Yu. D.
. ..........
TITLS~ Datermination of 'he D-Ime-no."ons -)'L an Elf-ientzovry Cc'.'
Ca-'-,h.)dP-palaz-.,,zed DisporsLon Alloys Pd-A-,.l and Pd-Ou
PLRIODICAL~ Doklady Akademii rAWc SSSR, 1959, Vol 127, Nr 4, PP 835-837
(USSR)
ABSTRACTi In the present paller, the latti2,,i -arameters ~,f an
were determined during :11-s polazization. These I.nvest4,--P-'Ions
permit checkidg of some assumItions coric~!rn-.ne the d~-:pcndelce
,)f the cvervoltaU,-~ of the hydro--en deposition on -~h~-- inter-
atomic. distans-es in the alll%r-q. Investizatf-ons ver~i c:ar-r.-*c-d -)--t
by means of the b'-na-.,, dispei-sed a-11:3~7s =--ntloned. i-n tlhe t--tle.
These alloys dissolve hIydr,---,c-n in a n~.if v;A-Lde
I~on interval . TM dissol-ved hy-3 r')gon ;.,,3,s a-, i M.Imxtiiil ly anod'i
polarization of the alloy unt~.l thq deposilion rf tho firz.,
hydrogen blibblee. For "he recordings, a spcoi.,:~71 P'exi--Ius
was ~.ised (Fig 1). The recarding mas made by mear-s Df EL UPS-'/O-l
diff-ractometer. The lattLee Periods coluld to det-7---rzired up t,., an
Accura,-Y of t 0.001 kX. '11he cxpotim,~nta 7io-.i made ~;.n IN 111~30 4-
Ca-fd 1/2 solution at room temperaturo. Tho data obtafriced fof 4.-hz%
Det:_Lz-zr.-&'na '-ion if the Dimensions of an Elcmentn:r~~ Cell 6f 'JOV'/2C-'2'7j-I-'0/60
Cathod-1-1-OrA~!,ized D-ir3persion Alloys Pd.-All and Pd-r.,.i
t4o:
"at periods '.s c:ompiled In tab-le i. The values nbtaire'-;
showed an error of or_'_y-XO.0V ',X. The 'L:~7,-: the
I.ytically depos-.'Ited all-
r co-uld not be zbtain,-d' with th,~ same
'
a.-ouracy. The lattioe for tho alloys afte-r
are shown by figure 2 for the -7aTicus aystems vith d-_'ffer':nt
Al.- and Cu-c;ontent, and also- -.n the jpv~oe.=;s f-f hydr-j:n
Therp was g.~cd agrcuement with V-P -.c-s,.Ctz;
Kl~zret-sov (Ref 10). Thp enla-rg?mort' .)f th,:. ;,aram- ', ~:-s
- nentary cell resu'.~ed ~n p-;re pailadi!~Tr. '3-, 'ho
of tlia eleL
ductior. of Cold or Cu It dp.:!reasc-6. and
~r. _,onten~ of 650f Au c,,1- 1013' G,~L, rcapoE,;f,'-veIy. A-~ 1, 47, '7 P1; M
.1c.r.tent, flio solutflIty of hydro-on In the al].2y a'.sc-
dc,wm to zerc,.AcharZe in the -:.urront intonsity fhe cmrp'...-
.1 rv -
.A.4 -i..ts had near'y no effect o.- ihe lattice paiamiAu-9. The-- are
3:f!av-re:F, *i table, and 15 7 ef vihi--h arer- S_v~_E.'.
ASSOCIATION: Gosudarstvennyy inatitut prikladnoy khirnii
(State Institute of Applic-d. Chemist-my)
PRESENTED. Alril '13, 1959f by A. 11. Frimkln, Acudeml.,jrii
SUBMITTED. April 117, 41,059
Card 2/'~'
VERT,-Zh.L-.-;-- KAMENTSEV. -M--V& Cdecea-riedl
190AAMMUMAM
Reduction of T102 bjr carbon in binar7 mixtures vith Ye, A1203, S102,
CaO and Si. Zhur.neorg.khim. 4 no.1:17-22 Ja 159. (KIRA 12--2)
1. Yeesoyuznyy nauchno-iseledovatel'sk1y institut abrazivov i
shlif ovaniya.
(Titanium,cpcides) (Reduction, Chemical) (Carbon)
5(2) SOV/78-4-1-4/48
AUTHORS: Vert, Zh. L., Kamentsev, M. V. (Deceased)
TITLE: The Reduction of TiO 2 With Carbon From the Binary Mixtures
With Fe, Al 2 031 sio 2' CaO, and Si (Vosstanovleniye TiO 2
uglerodom iz dvoynykh smesey a Fe, Al 2030 Sio 2' CaO i Si)
PERIODICAL: Zhurnal neorganicheskoy khimii, 1959, Vol 4, Nr 1, pp 17-22
(USSR)
ABSTRACT: The reduction process of titanium dioxide with carbon was
carried out with a mixture of TiO 2 and petroleum coke. Iron,
argillaceous earth, ouartzsand cleaned with acid, calcium oxide
and metallic silicon were used as additions. The tests were
conducted in a closed graphite crucible in a tamman furnace in
a CO atmosphere within the temperature range from 1250 to 18000.
For temperatures of 800-12500 a tube furnace with silite bars
was used. The reduction products in the system TiO 2- C, TiO 2- Fc-C
and TiO 2- Al 20 3- C investigated were tested by X-ray analysis.
The X-ray analysis was carried out by V. I. Kudryavtsev and
Card 1/3 M. I. Sokhor. The reduction of titanium dioxide with carbon
SOV/78-4-1-4/48
The Reduction of TiO 2 With Carbon From the Bina~y Mixtures With Fe, Al 20z;
SiO 2P CaO, and Si
at normal pressure starts at 9000 and ends at 13000C. On in-
creasing temperature up to 18000 the reduction product con-
tains titanium carbide. The TiC content r 4 ses up to 60% ir the
solid phase. The reduction procesi) is not influenced by an
increase of the carbon content in the reduction mixture. Thc-
gradual reduction of TiO 2 from the lower titanium oxides to
the formation of titanium carbide is confirmed by analyses of
the X-ray structure. The influence of various additions upon
the reduction processes of titanium dioxide with carbon was
investigated and it was found that iron influences the reduc-
tion process positively. Within the temperature range
16oo-18ooO titanium dioxide is transformed into titanium carbjd%.
The specific effect of iron during the reduction process of
titanium is explained by the fact that iron can separate
carbide. Aluminum oxide improves the reduction process of
titanium dioxide. Calcium oxide, silicon dioxide and metallic
silicon do not influence the reduction process of TiC 2 with
carbon. There are 6 figures, 2 tables, and 12 referi-ncesp
Card 2/3 9 of which are Soviet.
SOV/78-4-1-4/48
The Reduction of TiO With Carbon From the Binary Miytures With Fe, 1-1 r,.
2 2~12)
Sio 2' CaO, and Si
ASSOCIATION: Voonoyuznyy nauchno-irj.,)lodovatollokAy instJtut ll)lrll','.lv0v i
shllrovaniya (All.Unlon Scintitific Reuvarch 1w;t1tute of
Abrasives and Grinding)
SUBMITTED: May 15, 1957
Card 3/3
MT, Zh.L,; YAMEPTSEV, Y.V. (deceased]
I
Interaction between FeS and TO2 in tho preoence of carbon.
Part 5. Zhur. neorg. khim. 3 no.5:1200-1204 My '58. (MIRA 11:6)
l.Vassoyunyy nauchno-iseledovateltaki7 institut abrozivov I
shlifovaniya.
(Iron sulfide) (Titanium oxides)
Vr t.
AUTHORS: Vert, Zh. L., 1,a:,.icntscv, T' V~ (Decuased)
TITLE: V. The Interaction Between ?eS and TiO in the Pr---se-n:c-
of Carbon (V, Vzaimodeystvije FeS n Ti6 2 V :1 r i 1: Ut C, t. v i I
ugleroda)
PERIODICAL: Zhurnal NcorGanichcs%oy Khinii, 1952, Vol -J, 111r 15.
pp 12oo-1204 (USSR)
ABSTRACT: The interaction between TiO - FeS and carbon~as well as
2'
the influence on this reaction of other components such
as A.120 3P Sio2and CaO;wereinvestigated in the present
report.
Titanium sul'Aide (in solut--on in FeS) is formed
by interaction between TiO 2 and FeS in the presence
of carbon?at a temperature of 1300 0C. The formation of
titanium sulfide sets in at 13ooOC and attains ita
maximum value at 16oo to 17000C. The output t1lecreaocz,
according to a further rioe of temperature. ThQ for=
mation of titanium sulfide as a single phase aas not
Card 1/2 observed. The formation of titanium sulfide increasef
Ve The Interaction Between ;eS and TiO 2 in -the 78- 3-1~-2,',/39
Presence of Carbon
accordina to a rise of temperature. In the )rcnen,3c- of a
surplus of carbon, titanium aubsequently binds with car=
bon by forming carbide. The increase O-V
f the FeS -~:ontent
in the intial nixture favors the forilation of ~itaniu_m
sulfide. The surplus of carbon, on the other hana, inhi=
bits the reaction. The proce3s of the formation of ti=
tanium sulfide is not inhibited by the addition of
3 and a mixture of Al 20 3 + Pe 20 3' The for,aa+i3n of
Al 20
.
titanium sulfide, on the other hand, is reduced by the
action of calcium oxide, because the sulfur is bound as
CaS. SiO favors the complete linkage of tilaniun ith
2
sulfur.
There are 5 fiGurcs, 2 tables and 11 references, of
which -are Soviet.
ASSOCIATIOli: Vse,,oyuznyy na-achno-i33ledowiteltskiy instit")t abrazzivoV
i shlifovaniya (All-Union Scientific Uesearch I,,stlitute
6f Abrasives and Grinding)
SU1]'1ITT7_D: May 15, 1957
AVAILABLE': Library of ~;on:~reas
Card 2/2
1, Titanium cul-fide--olyrttiagic-,.Fffects of crirbca 2 k, r., i -,~cn
4 = U-Ma- V-1;1_.YW1'14i1
I M
U~BR/Inorganie Chemistry. Complex Compounds. C
Ab's Jour Ref Zhur - Khimiya, No. 8, 3.957, 26498.
Author Vert, Zh.L.i Kamentsev, M.V.
Inst
Title Formation of Ferrous Sulfide at Interaction
of Pyrite with Pig Iron Shavings.
Orig Pub Zh. neorgan. kh1mii, 1956, 11 No. 99
2171 - 2175.
Abstract The half of the pyrite sulphur, which easily
evaporates at pyrometallurgical processes
requiring the introduction of sulfide S, can
be utilized if bound in FeS according to the
reaction FeS,-'*Fe - 2FeS M.. In order to
investigate he conditions or' FeS formation,
bricks of pyrite concentrate (brand KSF-2)
and pig iron sbavings were prepared using
Card 112
20-5-32/48
AUTHORSt Vert, Zh. L., Kamentsev, 11. V. (Deceased), Kudryavtsev, V. 1.
and 5okhor, M. I.
TITLEt by Carbon (K voproau u vosata-
Reduction of Al
0
2
3
novlenii Al203 uglerodom)
PERIODICALt Doklady AN SSSR, 1957, Vol- 116, Nr 5, PP- 034 - 837 (USSR)
ABSTRACT: It was noticed by the authors that during the reducLion of TiO,
by carbon in presonce of Al 20 in a atmosphere 01 Co at 1650 02 a
loss in substance occurred. A;parently Al 20 entered into the re-
action. It is stated that the interaction bhween 9120 and C be-
gins under normal pressure at approximatively 2200 . IP, the va-
cuum the temperatures amounted to 1560 and 1750 - The pressure of
the gases above the reaction mixture reached 1 atmosphere at 1980 0
a fact which agrees well with the above mentioned data. The auth-
ors inve8tigated the interaction between A120 and C between 1500
L
xture A120 -C-TiC,
and 1900 , fu3thermore the interaction in the
2
d of the
in order to eliminate the influence of the lower oxides a
oxycarbide of Ti. The molar relation of the components is given in
table 1. The experimental method and the characteristic of the com-
Card 1/4 ponents is given. Theexperimental results given in figure 1 show
20-5-32/48
Reduction of Al 203 by Carbon
0
that a considerable reduction A120 begins above 1600 . Titanium
cozoundo do not influence this progess. The loss in filuminum 00
gas and the carbide formation are lcw, compared to the quantity
of the liberated oxygen. Thus the reduition process is deocribed
neither by the equation A120 + 3C x 2AI + 3C0 (2), nor by 2A1,0 34
+ 9C 0 Al 03 + 6CO (3). The c;mpariuon betwuun tho romnIning qp~~io-
tity Of tAe free C, as well as of the quantity of C necesuary tor
the formation of titanium carbide and for the re,'Luction of Al2 0
and the chemical properties of the products admit the assumptIO2
that during the reaction some lower aluminum oxides are rroduced
in free oE bound form. The x-ray analysis showed that beg-inning,
with 1650 corundum o~-Al 20 partly changes into a new spinel-like
compound. With rising telapeLture inorgases the spinel content at
the cost of the corundum which at 17,':0 vanishes completely. The
now product is macroscopically a white powder with a greyish-blu-
ish tinge. Table 2 gives the computation of the radiogram of thia
t3pino,l phase. According to utructure type and value of the con-
stant lattice the spinel pha3e raminds to a great extent of the
low temperature intermediary aluminuat modification r- Al 0 In
reality, however, it is of different structur6. Fort 1.) A12 8 is
Card 2/4 here reduced up a lower oxide. 2.) The here described spine-1 phase
20-5-32/48
Reduction of Al203 by Carbon
consists of corundum, whereas# U.f -"2'g lo a transition form
from the hydrooxide forms of al Ei to orunduma 3#) Clear lina5
in the spinal radiogram prove a high degree of the crystallization
state of the phase in question. It 'A stable, is neither in water
nor in hydrochloric or sulpPric acid decomposed, nor in cold or
by long boiling. Above 1750 a second phase ~s found which quantity
increases with the temperature rise. At 1900 black crystals are
formed in the inner which are covered by a light Cray crust. It
consists to 90 % of a hexagonal phase and is very stable, too. It
is analogous to the superoxide A120 (reference 6). The progressive
reduction of the aluminum oxides agrees with the temperature curve
of the oxygen leakage. The structure of the above mentioned black
crystals ib not yet deciphered up to now. There are 1 figure, 2
tabbs, and 6 references, 2 of which are Slavic.
Card 3/4
20-5-32A8
Reduction of A12 03 by Carbon
ASSOCIATIONS All-Unton Scientific Research Institute for Abraaiveu and Polisi-dag
(Vaesoyuznyy nauchno-issledovateliskiy inutitut abra:&ivov i shli-
fovaniya)
PRESENTEDt May 159 1,957o by I. P. Bardin, Academician
SUBMITTED: May 13, 1957
AVAILABLEt Library of Congress
Card 4/4
USSR/PhysiJ Chemistry Kinetics. Combustion. B-9
Explosives. Topochemistry. Cat,,dysis.
Abs Jour : Referat Zhur - Mimi)a, Ito 2) 1957.. 3636
Author : Vert Zh.L., Kwientsev M.V.
_Uo
Title : Forma -n of Sulfides ca Interaction of Iron SulfiJe
with Oxides of Metals. TII. Interaction of FcZ with CaO
OriGr Pub : 721. neorgan. khiFAij 1956, 1, 110 3, h89-498
Abstract : A study was rmdej at 400-18Wp of' the interaction of
FeS with CaO (pure and with adnix-tures of U 0 Sio
C and F E'20 )) at the iixitial imlar ratio FeS: MO = 3-2.
Reaction batwecn FeS wid C-10 starts at 4coO in the so'lid
phase. Maxina in CaS yield (and correspoiLding minina of
Cano yield) are obsQvied at 550, 73.5, 900 mid 11000; rL'-
nina in CaS yielcl and r=xi=_n in C,-..o -- at 630, 800 (for-
vntion of CaO.FeS) rind 10050 (foryntion of CaO.Fe2O3)'
In the presence of C in the proportions CuO:FeS:C-
1:3.2:1.2, increase of tcr-,paratur(., to 14000 results in
Card 1/2 137
--------_------------- _-- -------------------------- ------- - -------
A
...
v
11 15P
MOSIWIOH, I.A.; TTMMVSIIY. I*P.; VERT, Zh.L.
Sorption of hydrogen by disperse paUadiump-gold al!-jyv. Trudy GT
uo.42:173-181 159. (MIRA 13:10)
(Palladium-gold alloys) (wrogen)
wpm
Formntion of ferrous sulfide In the remotion of pyrite with Iron ships.
%hur.noorg.khtm. 1 no.9:2171-2175 5 1569 (MLRA 10:1)
1. Veasoyusnyy nauchno-issledOTAtOl'skly institut abrasivov I shlifova-
niya, Leningrad.
(Iron sulfides)
VERTAN, Magda, dr.; KOTAY, Eva, dr.; KIFOR, Olga, dr.; SZIGETI, I., dr.
Determination of thrombocyte adhesiveness (with a modified
Bobek and Cepelak method). Med. intem. (Bucur) 17 no.6t749-
752 Js 165.
1. Lucrare efectuate, in Clinica medicee I, Institutul medico-
farmaceutical, Tirgu-ftrea (directort prof. P. Doczy).
US-0/9-edicine Biochemistr7
Card 1/1 Pub. 22 - 34/59
Autho.re t PaUadin, A. V., Academician; and Vertkymerv N.
- ...41baAM"IL4 46.;MA;L :
a-:tru7.1n-~ In 11-e -antral narvoi-s system at v-LrIoLs I=ctional
atates
Periodicali Dok. PJI SSSR 1021'2, 319-321, Fay 11, 1955
Abstraot t 7)e f7f -q-t~,4-nine amino acid containiniz ths 915 radio isotope
a va ~ i rvo At i;7-qt,,:kd ielqrririe t',ie rejuvena~ior.
Thr nyperlir(n's ve"
Institution Acad. of So., IJkr. SSR, Inst. of Biocheimistry
Submitted Ranh 179 1955
VERTEE, A.I.
N.F. Fogreborv and the study of the hydrogeology of Estonia.
Infoxm.abor. VSEGI no.48:71-80 161. OURA 15:7)
(Estonia--Water, Underground)
Vr-_a,rE,
23-4-14/18
AUTHORSt Lerte, A. 1. and Mark, E. Yu., Cand:idates of Geologico-
Mineralogical Sciences
TITLE- On the Stratigraphic Position of thq Pyarnu (D a 1) Formation
2 1
in the Estonian SSR (0 stratigraficheskom polozhenii Pyarnus-
kogo D al) gorizonta v Estonskoy SSR)
( 2
1
PERIODICAL: Izvestiya Akademii Nauk Estonskoy SSR, Seriya Tekhnicheskikh
i Fiziko-Matematicheakikh Nauk, 1957, # 4, PP 392-393 (USSR)
ABSTRACT: The stratigraphic position of the Pyarnu formation, which
lies in the lower part of the Middle-Devonian system in the
Estonian SSR and adjacent regions, is sufficiently well
determined by K. Orviku (Ref. 1,2), W. Gross (Ref- 3 to 5),
D. V. Obruchev (Ref. 6, 7) and R. F. Gekker (Ref. 8, 9).
Nevertheless, in 1953 an article by S. N. Naumova and S. V.
Tikhomirov (Ref. 10) was published in which they came to
the conclusion that the Pyarnu sandstones were similar to
the lower part of the Tartu formation.
The authors of 'the present article contend this conclusion
and show, by the comparison of lithological and paleontolo-
Card 112 gical data, the differences between the Tartu and Pyarnu
'On the Stratigraphic Position of the Pyarnu 23-4-14118
sandstones. Therefore, they conclude that there is no basis
for re-naming the Pyarnu formation into the Sub-Narva one as
proposed by Naumova and Tikhomirov.
The article contains 2 Estonian, 4 German and 8 Russian
references.
ASSOCIATION: Academy of Sciences, of the Entonian 3SR, Institute of
Geology
SUBMITTEI)i 24 May 1957
AVAILABLE: Library of Congress
Card 212
LUTHOR i Verte, A. 1., 20-5-33/54
TITLE On tie Laminarite and Superlaminarite Stratri of the Lower Cam-
brian in the Estonian SSR (0 lyaminaritovykh i nadljaminaritovjkh
sloyakh nizhnego kembriya v Estonskoy SSR)
PERIODICALs Doklady Akad. nauk SSSR, 1957P Vol- 115, Nr 5, PP. 971-974,(USSR)
ABSTRACT- The occurence of these strata in tho rerpective area is denied by
some geologists. These statements, for the following reasons, do
not conform with the actual facts: As early as ill 1940, Asatkin
drew the conclusion that a suite of Lauinaritis loams exist in Es-
tonia, although it is not so widely spread and has not such a fi-
xed position as in the area of Leningrad. According to a verbal re-
port of Oepik, A. they were found in some cross-8ections of Cam-
briun loams in Estonia. They do not occur, however, in the bore-
holes of Tallin-Paldiski. As early as in 1939, P. Kents stated the
occurrence of a layer of violet-red and bluish greenish loam of 1
to 3 m thickness beneath blue loams with Platysolenites antiquissi-
mue, the latter kind occurs also in the aforementioned layer. Its
stratigraphical position remained open. Post-war results of borings
for water now permitted and alread.,r t;iore substantiated the assu-,,p-
tion of the occurrence of strata, as mentioned in the title, in
Estonia, including Tallin. (see fig.1 and 2 icross-sections of the
Lower Cambrium from Leningrad to the Baltic in Estonia).In this
Card 1/4 place, the rjthmical structure of the lowers Cambrian 3ediments and
20-5-33/54
On the Laminarite and -~,uperlaninarite Strata of the Lower Cambrian in
the Estonian SSR.
the advance of thvoe rythris from the teningrad area to Estonia be-
comes apparent. Up to three rythms occur. They begin with coarse-
claotic rocks and end with fine elastic rocks at the top. The rythm
be sinning with A I a + Al b (basis of the lowest rythm) are fully
described. Wori.i-ducts were found in theloaams, sand-stones are pal-
eontolgically barren. The loams concerned, because of the occurrence
of algae residues, are known as mentioned in tl,,e title. These re-
sidues are, accordin,-, to Asatkin, 'Sapropel films. The middle rythm
(A bi + Ajb2
1 1 2) isp in parts, completely lacking. The loams of the upl-
er rythm are knovin as blue loams in geoloL~ical publications, where-
as the sandstones deposited beneath them are I-,nown as superlaminari-
tes. A zone of alternating deposita of loams rith sandstones is par-
ticularly abundant in Pl~_Aysolenitas anti(jaissimus. Besides the lat-
ter kind, according to A.Oepik, Plaurotoinania, Kunda Opik, Hyoli-
tes blickwithi Oepik, Linquella, and others, as well as the afore-
mentioned La.antiquissimus and the Sapropel filras still occur. The
thickness of both the sand stone and loam layers increases from West
to I~jst. The Laminarites and the blue loams diff er in the same di-
rc-ction in the Lower Caj1jbriujj. The layers coi-,cerned begin to assume
a wedge-lika structure in the llorth-.iestern boundary zone of the slc-
pe of the Baltic crjotalline shield, so that the position of alter-
Card 2/4 nating layers of sandstones and lcams in the direction of one or
20~5-33/54
On the Laminarit,~ and -~Juperlaminarite Strata of' the Lower Cambrian
in the Estonian SSR.
the other strati.-raph-ical atratum is rendered difficult. Concern-
ing the fluctuation of the number of rjthms from 1 to 3, it may be
Said thatboth the number and the thickne3s of individual layers
may be explained by the mobility and position of the cryntalline
fundament during sedimentation in the marine area of the Baltic.
These rythas, according to a report by Paasikivi -continue to be
L)
observed in a wide area of the Ru~,sian plateau. Th~_ lower and midd-
le complex belong to the Valdaja plateau, whereas the upper rythm
belongs to Sokolov's Baltic com~jlex. Both the red coior, arid the
oblique position of layers, as -Kell as their position on the cry-
rtion that they represent
ntalline fundament give rise to the asse
Continental formations. On the other hand, the upper parts of the
sub-section of the sand-stones and loams covering them, are of
iviritime origin, according to the lithographical charactQristic
feature. The lack of algae residaes of' Laninarites antiquissimus
an-d of the sepropel fili.is in the loans covering thz: so-called
"Gdovschell sand-stories, in not a proof of the lack of Laminarites
loams as a certain stratigraphical unit. These renidueu can either
be ?resent, or lackinz or they may also be pre3ent in higher hori-
zons (according --.o Uepik). Therefore the occarrence and tho s~rati-
1-;raphical position of the Lamiriariteq-and of the superlaminarites
Card 3/,j in Estonia become by far more cc,nvincing by the method of investi-
On the Laminarite and Superlaminarite Strata of the Lower U'ambrian 20-5~-33/34
in the Estonian SSR.
gation and comparison of analogous litholooical ma-qse3.
There are 2 figures and 7 Slavic references.
ASSOCIATION: Institute for Geology of the AN Estonian SSH (Institut geologii
Akaderiii nauk EstSSR)
PRESVITED: Nalivkin, D.V., Academician , December 28, 1958
SUBMITTED: December 18, 1956
AVAIIABLE: Library of Con.-ress.
Card 4/4
VMM, A.
Goologo-lithological subdivision of the lower sand and clay strata
of the Devonian on the territory of the Antontan SM. 'Dok-1. AN
Ssm 105 no.4:782-785 D 155. (KLRL 90)
1. Prodstavleno akademikom D.V. Salivkinym.
(Ratonia.-:-Geology, Stratigraphic)
-- VZRTI A. I
.. - NrUx, -
Tectonic nature of a small done-type otructnre near Tallinn.
Vest.LM 14 no.6;155-157 '59. (MMA 12t6)
(Tallinn region-Geology,, Structural)
VAITA, -..
Prospects of obtaining mineral waters ia the Zstonian S.S.R.
Yop.kur.fitiotor. i Iech,fi2.kul't* 21 nool:60-62 Ja-Mr 116.
(MIRA 91-9)
1. Institut geologii Akademii nauk Estonskoy SSR.
(XSTONIA--MIN.SRAL WATMS)
V)WA, A.1,
On the lamInarite and superlaminarite strata of the Lower Gfu*rian
in the 31stonlan S.S.R, Dokl, AN SSSR 115 no.5t971-974 Ag 157.
(MIM 110)
1. Institut geologli Akademii nauk Istonskoy SSR. Predstavlano
n)mdanikom D.V. Nalivkinym.
(31stonia-Geology. Stratigraphic)
61 Ard
AUTHOR., Verte,.L.A., Engineer
86933
A16l/AO26
TITLE: Automation of Foundry and Metallurgical Processes by Electromagnetic
Pumps
PERIODICAL: Mekhanizatsiya I avtomatizatziya proizvodstva, 1960, No. 9, PP. 15-17
TEXT: Transportation of molten iron by the existing means requires more
labor than before when the output of the blast furnases grows due to automation,
and in foundries the transportation from furn&oes to conveyers is still taking
high labor numbers. The described electromagnetic metal pumps, developed by the
author, are based on the same principle as the latest electromagnetic pumps used
in atomic reactors for pumping liquid heat carrier - sodilin and potassiun alloy.
The motive forces in metal inside the pump are pr*duced by Interaction of magnetic
fields and electric current passed through metal. The article gives a brief des-
cription of two pumps. The flat three-phase induction pump (Fig. 1) Is designed
for refractory me'tals. Cooled-pipe windings place-d in the slots of maEMetic cir-
cuit produce a running magnetic field that penetrates the walls and the duct in
a refractory tube, the ends of which are the inlet, and the outlet of the pump.
The output end may be connected with a pressure line or remain open. /in electro-
Card 116
86933
S/118/6r)/C,X/009/004/099/
A16l/AO26
Automation of Foundr-j and Metallurgical Processes by Electromagnetic Pumps
magnetic field controls the metal flow out of Lhe open end. A running magnetic
field produces induction currents in metal along the duct axis and In the same
direction with the magnetic field. Metal flow out of the pump can be stopped by
reversing the field motion. The inductor has to be supplied with three-phase
current of 300 - 500 cycles frequency, but In most cases the usual frequency is
sufficient for controlling metal flow under moderate pressure (of few a.tm). The
work capacity of the pump, or of pressure produced by It can be controlled
simply by controlling the voltage of the feed current; the remote controlled ATHV
(ATMK) autotransformers are suitable for this purpose. The other pump (Fig. 2)
is & cylindrical three-phase induction pump, of better design from the engineerkg
point of view. Its duct has annular cross section, and the magnetio circuit is
divided into several sections in the shape of a star. This pump develops a pres-
sure 2 -3 times higher than the flat one, but the cooling of the inner core is
difficult. It is therefore better suited for nonferrous metals with lower melt-
ing point than ferrous. The practical application of the pumps has not yet left
the experimental stage; they have been tested with mercury and stannilun, and
zinc overheated to 7000C, PKBNIIST- have dez!,gned an automatic device for feeding
molten brans Into pressure die casting machines. It is a flat pump built Into a
CaM 2/6
86933
s/n8/6o/ooo/0o,O/CC'04/C09
A16l/'AO26
Automation of Foundry and Metallurgical Processes-by Electromagnetic ?=,ps
teeming furnace; liquid metal rises In an Inclined refractory tube into the
machine pressure chamber, and after filling the chamber (the metal level is
measured by a radioactive indicator, or a time relay is used) the running magnet-
ic field is reversed. Similar feed devices for Dluminum alloys are under de-
velopment at the Institut fiziki A11 Latviyskoy S,3R (Institute of Phyzics of AS
Latvian SSR). At Avto*zavod im, Likhacheva (Autoinobile Plant imeni Likhachev),
it is Intended to test a closed chute heated by gas and fitted with an Inductor
over Its entire length to pull metal on horizontal and ascending chute sections.
This experimental installation will be 6 m.,long and serve for moving liquid cast
iron from cupolas to mold boxes moving on 'e-onveyer. Metal itill be poured into
molds by a flat induction pump inside a drum ladle. This unit will simulate the
future doser consisting of a reciprocating ladle with a pump. Automatic control-
ling of continuous teeming of steel or nonferrous metal may be arranged as shown
(Fig. 3). GIPRO.MEZ is working on el.ectromagqetic pump systems for the transporta-
tion of large metal masses from blast furnaces. The electric part of induction
pumps may be considered finally developed, and the work principle finally tested
with nonferrous metals. For ferrous metal, more durable refractories for the dLict
still have to be found, and this must be done by the appropriate institutes and
Card -3/6"
86933'
S/118/60/000,/009/004/009
A161/AO26
Automation of Foundry and Metallurgical Processes by Electromagnetic Pumps
plants. There are 3 figures.
Figure 1:
Flat pump: 1 - housing; 2- filler
(concrete); 3 - magnetic circuit; 4
- refractory'tube; 5 - heat insulation;
6 - pipe winding; 7 - panel for termInals;
8 - minding lead-out; 9 nipple for
.cooling-water hose; 10 duct for liquid
metal.
card 4/6
Pifc. i. mocxso TDexdm3HUrf JIII;tyX1',HJII If W rt
113COC:
86-933.
S/118/60/000/oog/004/009
A161AO26
Automation of Foundry and Metallurgical Processets by ElectromaVietic Pumps
FIgure 2:
Cylindrical pump: 1 - housing; 2 - magnetic
circuit; 3 - core; 4 core lining; 5
- refractory tube; 6 winding; 7 - duct /0
for liquid metal.
Card. 5/6
Pnc. 2. Llif-umavHvecKHR TpexdM3110
HH;jVKUIfOIfHUA IIACO.:
86933
S/118/60/000/009/004/009
A161/AO26
Automation of Foundry and Metallurgical Processes by ElccLromagnatio Pumps
Figure 3:
Automatic system for controlling the
metal flow. in continuous teeming: I
- furnace; 2 - induction Pump; 3
- crystallizer; 4 - ingot; 5 -
- pulling mechanism; 6 ATMK voltage
regulator; 7 - electric motor; 8
- electronic regulattor; 9 level
transmitter.
P)fc. 3. Cxema aBTOmaTuqecxoro PerY.13PI008HAS CTPY;l
Card 616 %teiama Tipit HenpeDuelloA P33.'IHBKe:
rtma 2201 7
------ -- -
~,__!IRTA, L., inzh., izobretatell
Ylov of fire in magnetic boundaries. Izobr. I rate. no.11;22-25
N 160. (MIIU 13: 10)
(Foundries-Zquipment and supplies)
(ftnetoolectric machines)
S/136/61/000/006/002/003
E073/E535
AUTHORi _KeiLte -J,.,.-A-
TITLE: The Effect of the Apparent Change of the Specific
Weight of Liquid Metal Produced by Electromagnetic
Forces
PERIODICAL: Tsvetnyye metally, 1961, No.6, pp.61-64
TEXT: If passing an electric current through the liquid
bath of a metal, which is located in a miagnetic field, the
direction of the current and the field can be so chosen that the
electromagnetic forces act downwards and add to the gravity
forces. This manifests itself to the outside as an increase of
the specific weight. The apparent increase in the specific
weight of a metal due to the uniformly distributed electro-
magnetic forces acting downwards can be expressed by the
following equation
10.2Bj 3
Y1 = Y (I + Y . 10 g/cm
where y - specific weight of the liquid metal, g/cm
Card 1/6
The Effect of the Apparent ... S/136./61/000/oo6/002/003
E073/E535
B - Induction of the magnetic field, gauss; j - current density,
A/cm . In analogy with magnetohydrodyna.mic processes which take
place in alectromagnetic pumps for liquid metals, these phenomena
can be referred to as magnetohydrostatic phenomena. If the
liquid metal contains non-conducting inclusions (slag, oxides
etc.), the current by-passes these inclusions and does not produce
electromagnetic forces in them and thus there is no increase in
their apparent specific weight. If desired.the same effect can be
applied to Itreduce" the specific weight of a liquid metal with the
electromagnetic forces directed upwards. This effect was
verified using an external magnetic field and a conduction method
of feeding the current to the liquid metal. Prior to the experi-
ments, a theoretical investigation was made of the possibility of
passing a current of sufficient density through a liquid metal
placed into a strong external magnetic field. It was found that
the influence of the magnetic field and also the close proximity
of the iron masses of the core of the electromagnet do not
produce an increased instability of the surface of the liquid
metal or an intensification of the un.desirable pinch effect
Card 2/6
The Effect of the Apparent ... S/136/61/000/006/002/003
E073/E535
compared to what occurs as a result of the magnetic field
generated by the current flowing through the liquid metal. The
experiments were carried out by means of a modified electromagnetic
mercury pump, a photo of which is shown in Fig.2. The magnetic
field was produced by the coil I consisting of ten turns of a
copper strip wound around the core 2. A flat container made of
bonded perspex 3 was placed into a 15 mm gap inside the core.
This container with mercury simulated a liquid metal bath with the
dimensions 4 x 50 x 40 mm- The current was fed in through the
electrodes 4 and 5. In the final experiments the electrode 5
was connected to the current source by means of a copper bar 6
which was inside the gap of the magnet aTLd in it the direction of
the current flow was opposite to that of the current flow in the
bath. The system was so designed that a stable current of 300 A
could be fed to the mercury. First, the intensity of the pinch
effect in absence of an external magnetic: field was determined. it
was found that the applied method of suppressing the pinch effect
produced by the magnetic field generated by the current in the
metal bath was effective; during preliminary experiments, without
Card 3/6
The Effect of the Apparent ... 5/136,/61/000/006/002/003
E073/E535
the busbar 6, the movement of the mercury during current flow
was very intensive, whilst in the final tests there was no move-
ment. Following that, the external field was applied and as a
result of this the level of the mercury dropped and a part of the
mercury was pushed upwards into the gaps between the electrodes
and the walls of the bath where there was no passage of current
and, consequently, no electromagnetic forces occurred. In
subsequent experiments, this was prevented by filling out these
spaces with atearine. In the subsequent. tests, tungsten wire
(specific gravity 19) of 2.5 mm diameter was provided with a
coating of vaseline or glue (to act as a non-conducting substance)
and was dropped into the mercury (specific gravity 13.6). Without
current flow the tungsten wire dropped to the bottom but, on
passing current through the mercury, the wire floated to the
surface and remained there until the current flow was stopped.
During the experiments the surface of this mercury was not
completely horizontal and there were "mounds" 3 to 5 trim high at
the edges; in the central part the surfa,:e of the mercury was
horizontal. Professor A. I. Volldek expLains these "mounds" of
Card 4/6
The Effect of the Apparent ...
S/136/61/ooo/oo6/oo2/003
I-.073/E535
the mercury around the electrodes by the nonuniformity of the
magnetic field in the ga-p of the electromagnet. This phenomenon
has no connection with the pinch effect and can be suppressed by
equalizing the electromagnetic forces in the liquid metal. The
following conclusions are arrived at:
1. The described experiments cozifirin the effect of the apparent
change in the specific weight of a conducting liquid inside a
magnetic field during the passage through. it of an electric current.
2. This effect can be applied for devising new methods of puri-
fying metals. ,plications requires check
The possibility of such -IT
experiments with metals containing o-cide!i~, slags, fluxes etc.
There are 3 figures.
Card 5/6
The Effect of the Apparent ... S/13(5/6:L/Ooo/oo6/oo2/003
1:1-07 VE5 3 5
Fig.2
4
Card 6/6
6/1-18/61/000/008/002/005
D267/D304
AUTHOR: Verte,_L.A.~ Engineer
TITLE: An electromagnetic trough for transporting molten
iron
PERIODICAL: Mekhanizatsiya i avtomatizatsiya proizvodstva,
no. 8, 19611' 39 - 43
TEXT: The Moskovskiy avtozavod imeni Likhacheva (Moscow Auto-
mobile Plant imeni Likhachev) has developed a new type of elec-
tromagnetic trough for conveying molten metal. The assembly
consists of an open, lined iron c'hute surmounting an inductor
that runs its whole length and generates a traveling magnetic
field that acts on the molten metal. The stream of iron is
heated from above by panel gas burners litted in the insulated
lid that covers the chute. The inducto:r* consists of a mag-
netic waveguide of electrotechnical steel with a water-cooled
wave winding of copper tube. The method of calculating the
inductor is described, a method based on the concept of the
Card 1/3
s/1-18/61/ooo/oo8/002/005
An electromagnetic trough... D267/D304
equivalent slope angle,ii;e., the angle at which the natural
flow chute must be ihc n d so that the longitudinal component
of the force of gravity is equal to the electromagnetic-forces
acting on the molten metal. An experimental check of the cal-
culating method showed that it was quite accurate when metal
with a high specific resistance was used and when the inductor
is powered at low frequency. The chamotte for lining the trough
and its production technology were developed by Candidate of
Technical Sciences V.P. Zegzhda of the Vsesoyuznyy institut
ogneuporov (All-Union InstLtute of Refractory Materials). The
assembly was tested by passing white iron at 1500 - 15500C
through from one end to the other. Tests showed that the se-
lected slope angle of 100 was excessive. For a metal flow of
40- 60'tons/hr it proved possible to pump the metal up a rising
incline. This has the advantage of clearing slag from the
metal since the slag is not affected by the electromagnetic
field and does not climb the incline, Reversal of the travel-
ling magnetic field effectively cut the -stream of metal; the
Card 2/3
S/118/61/000/008/002/005
An electromagnetic trough*** D26'7/D304
method could therefore 6e used for controlling the flow of mol-
ten metal through the trough. The active power of the inductor
is about 10 kwt per meter of trough. Tests showed that the
copper section of the pipe winding could be increased 2 - 5
times by decreasing the lumen for the cooling water. The ac-
tive power for a trough of the same section could, thereby, be
reduced to 4.5 kwt/meter. This could be further reduced by
1.5 - 2 times by using tubes of special section. In this way
power consumption for conveying molten iron up a 1.5 - 20
rising incline could be reduced from 0.2 kwt-hr per ton-meter
on the pilot installation to 0.05 kwt-hr per ton-meter. The
use of a horizontal trough would cut power consumption server-
alfold. There are 6 figures and 1 table.
Card 3/3
28053
S/136/61/000/009/001/007
E073/E335
AUTHOR: Verte, L.A.
TITLE: Electromagnetic pumps and prospects of their
application in non-ferrous metallurgy
PERIODICAL: Tavetnyye metally, no. 9, 1961, pp. 56 - 61
TEXT: In conduction plunps current is fed directly to the
liquid metal and, simultaneously, a strong magnetic field is
applied in the perpendicular direction. Such pumps can be
used primarily for circulating alkali metals, which have a
high conductivity and low corrosivity in closed circuits, so
that the metals are protected from contamination. An
experimental conduction pump for liquid lead was built and
tested successfully at Gintsvetmet but it has not been developed
sufficiently for industrial use. Conduction pumps can be
operated both on DC and AC; in the case of DC, the efficiency
reaches 40-50% but in the case of AC the efficiency is
appreciably lower, In induction pumps tho current in the
liquid metal is induced by the electromagnetic field without
direct contact. An experimental induction pump was built and
Card 1/3
28053 S/136/61/000/009/001/007
Electromagnetic pumps .... E073/E335
tested as early as 1956 at the "Elektrotsink" plant. This
pump was capable of lifting about 400 :kg Zn per minute to a
height of 640 mm; the power consumption was 4-5 W.
Experimental specimens of induction puinps are being tested for
liquid aluminium and iron. These are fitted with water-cooled
windings made of copper tubing. Selecting the correct material
for the pipes through which the liquid metal flows is a difficult
problem. The Vsesoyuznyy institut ogneuporov (All-Union
Refractory Institute) has developed a technology for producing
fireclay-graphite tubes for such pumps, which withstand
satisfactorily the effect of molten pi,& iron, aluminium and
zinc alloys. The drawback of these tu'oes is that they have
a minimum wall thickness of 5-10 mm. rhe work aimed at
obtaining protective coatings on the surface of thin-walled
metallic nichrome and 4ustenitic steel tubes is of great
importance. The most promising for the majority of molten
non-ferrous metals are coatings of molybdenum disilicide,
a lum iniu m o x i'd e a, borides and other similar compounds.
If the problem of producing thin metallic tubes with satisfactory
Card 2/3
28053
S/136/61/000/009/001/007
Electromagnetic riumps E073/F,335
protective coatings is solved, it will be possible to reduce
considerably the size of the air gap and to improve the
efficiency of induction pumps. The problem of starting-up and
stopping the pumps is briefly considered. Induction pumps
could also be used to regulate the flow of metal for the
purpose of automation in semicontinuouis casting. Vie induction
regulator is so designed that the level of the metal in the
crystalliser is automatically maintained and when the flow of
metal to the crystalliser is stopped, -this flow is diverted
into a rotating mixer. The rotating mixer permits freeing the
pump channels from the liquid metal whan the pump is to be
stopped. There are 4 figures and 3 Soviet-bloc references.
Card 3/3
S113016110001012100-2/0")6
A006/A101
AMIORt
Ite, L,-A.
TITU3- Controlling the tapping of liquid cast iron with the aid of a
running electromagnetic field
PMIODICAL: Metallurg, no. 12, 1961, 6-8
TEXT: An electromagnetic runner for removing liquid cast Iron with th,~,
aid of an electromagnetic field, was designed and tested at the Moscow Automobile
Plant imeni Likhachev. The runner bed is lined with pressed refractory blo2ks
and is located over an Inductor which consists of a three-phase water-cooled
tubular winding and a dented magnetic conduct (Fig;. 1). The runner is coverid
with heat insulated lids with built-in panel gas torches, which are Intended to
maintain the temperature of the liquid cast-iron. During the testing of a six
meter long section of such a runner the cast iron moved behind the magnetic fle.U,
both along a horizontal and at an inclined position of the runner. The cast
iron was refined from the slag which moved downwa:-ds along the sloped surface of
the jet. The use of the new runner will make it possible to direct the liqlaid
metal as desired, to accelerate, or to stop Its mDtion by switching over the
Card 1Z4_1'
~5
5113016110001012100 1/01~6
Controlling the tapping of liquid cast ... AO06/A'LO 1
inductors, It wIll then be necessary to mount, besides straight rurLner sectionz-,
"switc-hes" for the transfer of the metal from one runner into anot"ller. Szra
formation In the electromagnetic runner will lbe allmInated by a nt-w prz~4helti-,],K
systein which Is now being developed a'. the Plart. Tile n,3xt stag-~ of tnt.rodue-
Ing the electromagnetic technique will be the transport of liquil cast. iron w1tr,
the aid of Induction pumps. Simultaneously the system of closing -the casL :rc-,
tap hole will be changed. The refractory material otill be re-pla-d by -:L-.'-
electromagnetic field which will make it possible to clost or open the way
the metal, to control Its flow, and to stop It, It necessary. The con3t.-~_i~tlor
of a "magnetic tap hole" is much more complicated than th,~ desigr oP tine afore-
mentioned runner. The ferrostatic pressure of the inetal rol-unir in ~he 'blas"~
furnace is very high. The induotion pump preventir~; the outflow of bast
iron -through the channel of the refractory pipe Must counterbalan:,e ~Ihe
pressure of 5 atm. The cross section of the chamne"I rrrus-P, be largs e~nojgn 1~r,
assure the rapid teeming of a considerable amount ot metal. _Pr1~fti1tL11_g Of '-n-
inductlon tap hole channel Is arother problem which must. be iqolLro~d, as tne
metal should not cool off in the channel. -This requir-s power ~?upply f,r(;,n
special generators. Some experts consider a varriard. without preheat'.rg tile 1~dp
hole channel, where the cast iron jet Is not completely 1nt,~rr-,iD*.t-d,
Card 2.1.4-.,
S11 3o/6 i/bw/b i2lco 110C6
Controlling the tapping of liquid cast ... A0061AI01
This method would) howeve r, vequire a substantial change in the existing blast
furnace technology. Therefore, it will be easier to introduce the variant where
the basic mass of cast iron will be tapped periodically. To prevent obstruction
of the tap hole chamel by cooled-off metal, a small amount of cast iron will
pass through It to the teeming machine. At the Plant Imeni Likhachev a test
model of an induction tap hole was designed which will Fig. 1:
be used for automated cast-iron pouring into molds mov-
Ing on a conveyer line. There are 4 figures.
ASSOCIATION: Moskovskiy avtozavod imeni Likhacheva
(Moscow Automobile Plant Imeni Likhachov)
Fig. I
Legend: I - refractory lining; 2 - winding; 3 -
magnetic conduct; 4 - lid; 5 - panel torch.
Card 3~Y
VERTE, L,A*
Electromagnetic pumps wW prospects for their application in
nonferrous metallurgy. TSvet.met. 34 no.9:56-61 S 161.
(I'Mul 14: 10)
(Honferrous metals-Metallurgy) (Electromagnets)
VERTZ,, L.k., inzh.
Electromagnetic trough for transporting molten metals.
Elektrichestvo no-5:74-77 My 162. (MIRA 15:551)
1,. Moskovskiy avtozavod imeni Likhac:heva.
(Liquid melals)
VERTE, Leonard Arturovich, izobretatell
Metal flown in pipes. Imobr.i rats. rA).11:6-8 N 162. (MIRA 15:12)
1. Glavnyy spetsialist Gosudarstvernogo noyuzwgo instituta po
proyaktirovaniyu m9t&UurgicheakWi salrodov.
(metallurgy) (Magnetoelect.-ic machine3)
01001 UM/W a/UO2
,--7-AlrlHOL---- Verte, -L*--A. Enggzinecr
"CMILs in foand;7 r
PORIODICAU: Melldi-anizataiiya i avt-omatizat5ira proizi-odstuva, no. 1, 1963, 40-42
TECT: TI-in-galled metall ---)WYl-) ducts nablc co-msion-res-is-twit coaztngs (al=4,-
nxmi omtde in the exoerinentall m=-) d~~VE:.Lopcd in tne
4,.-:~Caj Tn:,~ i t1 (ilicz--, 7-ade of norrie uailic materials. have
stivall; (Taili-nn poj--te,~,-.
been devein.-~cd to tron--~~r~.
'E
tut oi.-neu-orov (Ail-UnLon f -jr- n-z ny
_r-,_JO~Lo t'0 ZL-IC, a' 1_1:-4 :Tr-. nr'T'j-10,1S "0 :~C)Itp-n cast
1~ - - -Y -17-
iron. ",'Irj fIrSt me:tais wiei,e
Elek-l-otsin-k Plant. An i-,Lfted ar 3ut 4c/j- kcr of zi-nc Dc-.- -,unute TO
a hei.yht of 64.0 m and re-qp.:4-red albout d 5 fc~:r DaveioF-nen-6ai wore is-
~~l r C I arla 0'- 11 Hr d--L
u-n der 7-1 y D Lrminc-~ a:,7 -4 -- 3yS . ---C-
-- ~ -- - t
tenL -"I ve experi once 41. nr-t tc Sn at ~ul ~ 1- -,ur- -,,, 0 11 Sno u-i Li P'a V G- a S -.r
5!-~Ort as an,-; "~~Idu6s of' mpui -Pust te remo7vd from The pi-.mp w*Irlen -Lha
flow is stoppGd. Am eiecti-Dm.-agne-Lac siphon for L.quid zInc Na., de-veloped
Card I*of-2
S/1U.'/63/OW/001/002/m
so that elloot.-cm-agnetio mfMt" dtd nnt ha o to ho an-nnoo"e 441.refttly ith metal
ballut. E.Lectromagnetic pumps c_nn aino hcwaz~ laquld notal, t,,LI5 effect being a. func-
tion of the frequency, the comiuctivity of the met,-1, and the cro-,s section of the
,,~frequency cu=ent (_1 :f) c-f~) fr,~m 7 thn~,~-7hare ;~enerat'ors is
duct. Hi g
e.-c, e, 1,i e r. tr m % a
atorn developed in tn"
Tnst:_tute) i-y Profpq,3,~,r J ")L, -11 1, J'n (M C~').St 'Lne
I - , ,
stand-a-rdized pa:-ts r Was,
developed for tr-_nsT)ort4_ri_7 unv Dress,_xe head. This de,,Ice in
whe avtozalmd Lri. t,4F~ J1 4
a
cast iron at a terapera'~-_re a, a f Z'
at the maximm incline and severai ti-m-3 Viat amount when the chute mas horizontal.
Power required was about bu knv. Three, flgoures -aere given.
VERTE, L.A., kand. tekhn. nauk
Experimental induction pump for liquid pig iron. -nektrichestvo
no.12:64-66 D 163. 1 (MIRA 17r1)
1. Goaudarstvennyy soyuznyy inatitut po proyektirovaniyu
metallurgicheskikh zavodov.
U-RLE_,. Leonard Arturovich; ,VOLIETEK, A.I., doktor tekhr-,. muk., prof.
ka:~d. tek~n. nauk, do+e.,,
retsenzent; -Y'a.D.9 red.
(Electroiragnetic conveying of liquid metal] Elektrom-agnit-
nyi transport zhidkogo notal'Ia. -!o.-,kva, Metallurgiia,
1965. 235 P. (I'll'A 18:3)
I'ACC NAj 00 0
18
:AUTHOR., Verte. L. A. (Candidate of technical sciences); Filimonov, S. S.
(Candidatc'*o-f-fi-efO~dAriii~ences)
ORG: none
TITLE: Induction pum for liquid aluminum
P
Mekhanizatsiya i avtomatizatsiya proizvodstva, no. 5, 1966, 16-18
TOPIC TAGS: liquid metal pump, electromagnetic pump
IABSTRACT: In 1961, a new induction pump was developed for the purpose of circu-..
elating liquid aluminum through an experimental heat-exchange circuit at the Power-
Engineering Institute im.Krzhizhanovskiy. The pump's essential parts (see figure)
,are: I --housing, 2 - magnets, 3 -three-phase windings made from cooling-wat4ir-
carrying copper tubing, 4 - aluminum-carrying graphite channel, 5 - starting heaters,
6 -graphite connection nipples. The pump has a capacity of 0. 195 x 10-3 M3/sec and
develops a pressure of I kg/cm"; phase voltage, about 4S v. The pump has had over
30 operations; overa,11 worldng time, 150 hre. Orig. art. has: Z figures and I table.
112.
*. 621.65/68:656.546.621
-ACC, NR, AP6026505
IT I _3 =m
NIN\
LW
SUB CODE: 13, 09 SUBM DATE: none
Cctd -2/2
VMHj L.A.; KISELIGOF, Yu.S.; SUGHKOV, V.N.
Exp!Drimental induction pmp-feeder for lead aLloye. Kbi-m. prom.
40 no.llt858-859 N t64 (MIRA 18t2)
VERVE, L*A*
Magnotohydrostatic purification of li(JUld Mer, i1. fr-)n n: ~.-
metallic inclusiono. Fiz. mot. i metsill3ved. 17
772-773 1,~,r 164. 1.,7,9)
VERTEPOVA, V.M., kand. med. nauk; IVANOV, A.V.
~-7~ -~. , - , ~,
Radiography of the vens, cava In urological diseases. Urologila,
no.6sl3-16- 11-D 163. (MIRA 1719)
1. lz urologicheskoy kliniki (zav.- prof. I.M. Fpchte)n) I
floskovskogo meditsinskogo instituta. imeni Sechenova.
7OLUVfU,7*rsuc,dr.;.TKRTX5, Bodog,dr.; HASSU.Jossef,dr.
Problem of morbidistic steroid therapy of pemphigus. (h-v.
hatil. 101 n0.22-'770-771 29 W7 160.
1. Budapeeti Orrostudomanyi 11g7stem, Bor-on Ksmikortant Klinika.
(PMPHIM ther.)
(CORTICOTROPIN ther.)
(CORTISONE ther,)
VERTIBMATA. I.P.; IZ"YUROVA., A.I.; KOLTUNOVA, A.S.; LITVIKOV, A.S.;
a ~ 0 AUJFYWL I , M OA.
Sanitary state of bodies of water in the lenin Volga-Don
Navigation Canal system during the first year of its filling.
Gig.i san. no.3:9-17 Mr 154. (MLRA 7:2)
1. Iz Institute, obahchey i komminallnoy gigiyany Akademii medi-
tsinskikh nank SSSR.
(Volga-Don Canal--Sanitary affairs)
VERTEDNAYA, P.
Wnrk.q rf the All~lfn;rn Ppqt TnqtjjajtA,
_, (Min. of kri. R-MIR),
Number 3, 1933, 189 pages. Section on the Study of Peat Beds;
"Certain Data on the Biology and Chemistry of Water in Expezmintal
Pits of the 1,Vtishchi Peat Industry." by Vertebnaya, P.
SO. Botanicheskiy Zhurnal, Vol XXXV, No 1, DO 100-110,
Jan-Feb 1950, Rvssian bimo per, Mosco~A;ningrad (U-5511,
12 Feb 1954)
VERTEBNAYA, ?.
Works of the All-Union Peat Institute, (Min of Agri, RSFSR)
A Compmidium of Instructions
Number 5, 1933, 108 oages,/&Mk1mnon the Study of Peat and Peat Beds:
Part 2. Field Geobotanical Studies:
IlBrief Instructions on the Hydrological and Hydro-chemical Study
of Boggy Bodies of Water."
SO: Botanicheskiy Zhuranl, Vol XXXV, No 1, 100-110,
Jan-Feb 1950, Russian bimo per, Mcscow/Leningrad (U-5511,
12 Feb 1954)
VERTE, A.M.; IMYNSALU, iu.I. [Heinsalu, J.I.]
Studies of karst carried out by the Institute of Geology of the
Academy of Sciences of the Estoniarj S.S.R. Nov.kar.i spel. no.3.-
83-85 163. (MIRA 16:10)
YATXBULYA, P. 1.
Hicroflora of waters of the Lenin Volga-Don Navigation Canal.
Biul. HOIP. Otd. biol. 61 no.1;51-60 Ja-I 136 (KM 9:6)
(TOWA-DON CANAL--A=H-WA!rxR ncBA)
UB=Nku, P.I.
Biological investiptiou of the Don RVver and TSimlyansk Reser-
voir In 1952-1953 from the point of view of sanitation. TnAy
probl. I tem. Gov, no,7:175-180 '57. (MM 10:4)
(Don River--Algae) (TO W yansk Reservoir--Algae)
I
MOMAYEV, Ye.A. I
I-nMMP 1- - ~-- ~ --,
Experimental basis for the permissible concentration of the
sodium salt of dichlorophenoxyacatic acid (2,4-D) in bodies of
water. San.okhr.vod.ot zagr.prom.stoch.vod no.5:158-166 162.
(MIRA 17.-6)
1. Tr9titut, obshchey i kommunallnoy gigiyeny imeni. A.N.Sysina ANN
SWI-IM. I
A*,Zj&gWstarohiy nauchnyy sotrudnik; IZIYUROVA. A.1., star
shly
nauchw sotrudnik; 110IMOVA, A.B., starshiy nauchuyy sotrudnik;
RUMLI, M.A., starshiy nauchnyy sotrudnik; TIKHVIUSKAYA. N.M.,
starshiy nauchnyy sotrudnik
Role of sauttary preparation of the TSimlyansk reservoir bed on the
quality of water. Gig. i san. 22 no-1:72-76 is 157. (HOA 10:2)
1. Iz Institute obahchey i kommunall noy gigiyeny AMU SM.
(WATER SUPPLY.
byg. aspects of watershed (Rua))
TMTZBNAYA s P. I.
Observations on the intensity of photosynthesis and respiration
of plankton in nVaz'ma Reservoir on the Moscov Canal.
Trudy Gidrobiol. ob-va 10:8-24 160. (MIRA;.13'.9)
(nyazlm Res eriotr-Phytoplankton)
DRACHEVI S.M., prof.; YMEBWAYA, P.I.; IZ"YUROVA.. A.1.1 KABANOV, N.M.~j
KOLTUNGVA, A*So; iqLDAIAA, A.A.' IZMEMV., N.Y., red.; BELICUKOVA,
Yu.S.0 tekhn. red.
(Sanitation problems of the supply and utilization of water in arid
districtsIGigienichaskie voproey khoz:taistvenno-pittevogo vodosnab-
zheniia 3. vodopoltzovaniia v zasushli-vykh raionakh. Moskvat Medgiz,
1961, 206 p, (Water supply) NIFLA 14ill)
VgRTEBNYT, P. 1.
Subtlitutes for scarce techulcal mnterlals. P. I
boxi. Lesnayu rom. 1943, Nu. lo/l 1,
"CgIVC11 lor tile prepn.#jwYvlvl rowhionju, rep)j.-,- f
Calq-_-Nj tile CVTIVI'(Tcr*ll 'Fler 'til"Ittille ttl-~
api'Me of lutb,r, ilid (I"lli (Ild
111i iiic
subf.-itutes iot surce tecboi~al inaterials P~
tT "'
I)Iiyf I.eynaya Pions. 1943, I'lu. if)/l I,
ureal-vt-It forthe PrvPll.(J%olmvj CUI.Ilki-J~l -0
I --nk r Ait,,~;wic
jutg~all~ for Stearn -mm7c cvT%TLL tl!"; P
nA ii,,itmal
IrAtlull dl!~L,- ltl"M atal ru-T-FTF-cco
~f Li
00000000000000
00 4
00 :,of
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Subadbdog f0f mar" tOdLAIU] MAltiiti
-00
0: liftyl. briolaw; Pr~w, 1943, '40, 10111, lo-Wripft
lul-moild fm tmm~nciflr cylilidefo; fibri mlw-fulc ffir 00
00
Il
i
M
ly-r
.
l
00
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goo
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Ilp OF to to Ar a 't it
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- 0-0; * 0 * 9 0 * 08 st 4 at 0 0 *10 0 * 0 4 a -0 a 000 0 0 * 0 a a sj
LEFIN, G.F.; VISHNEVSKIY, A.V.; LI SI-CIUN [Li Hsi-chlangl; BUDIMKIY, A.M.;
BORCDULIM,, R.I. i ~BIIYY 0 P.
,~a.; REVELISKIY, I.A.
Exchange of experience. Zav.jab. 28 no.6:753-755 162. (KM 15:5)
I. Kramatorskiy nauchno-iseledovatollokiy i proyektno-tekhnologi-
choskiy institut mshinostroyeniya (for Lepimp Vishmvakiy).
2. Institut metallurgii imeni A.A. Baykova (for Li Si-chan,
Budnevskiy).
(Metallurgical analysis)
SOV/76-32-9-37/46
AUTHORS: Kalinin, I. A., Ver-t-ebnyy, P. Ya. (Zagorsk)
TME: Calculation of the Physical Dosage of t-Irradiation (Raschet
fizicheskoy dozy Vizlucheniya) II. The Dosage Intensity From
a Flat and a Three-Dimrnsional Source (II. Moshchnost~ do7y
ot ploskogo i ob"yemnogo istochnikov)
PERIODICAL: Zhurnal fizicheskoy khimii, 1958, Vol 32, Nr 9, pp 2192-2198
(USSR)
ABSTRACTt In the previous article (Ref 1) the strength of radiation from
a point source of radiation was calculated. In the present
paper the radiation strength from a level source is calculated
This calculation is made for the general case and is then ap-
plied to three specific examples. Nomograms are shown for the
following cases; 1) the strength of the gamma radiation at a
point 1 m above the center of a circular source of radiation
(Fig 3); 2) the strength of the gamma radiation at a point I m
above the edge of a circular, level radiation source (Fig 4).
For three-dimensional radiation sources tha formula is again
given for the general case and then demonstrated with two
Card 112 examples. For these example cases nomograms are also givent
SOV/76-32-9-37/46
Calculation of the Physical Dosage of T-Irradiation. 11. The Dosage lntensi~y
From a Flat and a Three-DimenBional Source
1) the radiation strength of a circular cylindrical radiation
source (Fig 6); 2) the radiation strength at a point on the
surface of a cylinder or a ball when the linear over-all
dimensions are greater than or equal to the mean free path of'
the gamma quanta (Fig 7). There are 7 figures, 1 table, and
5 references, 5 of which are Soviet.
SnMITTED: February 14, 1958
Card 2/2
USSR/Nuclear Physics Instruments and Installations. Methods of
Measurement and investigation C-2
Abst Jourml t Reforat Zhur - Fizlka, No 12, 1956, 33879
Author 1 Kalinin, I. A. and Vertabnyy, P. Ta.
lustitutiOlk I None
TItle i Calculation of Physical Dose of Ga",a Radiation. 1. Dose from
Point Source. Determination of Thickness of Shielding
OrIgInal
PerlodIcal I Zh. fiz. khiaii, 1956, 30, No 2, 457-463
Abstraot I A simplified method is given for calculating the thickness of
shielding layers for the case cot point sources, based on the
assumption that the scattered rays can be calculated from a
relationship of the form 1 + " (I., thickness; /,L, attenua-
tion coefficient,; o4, coefficient depending on the.kind of
.medium),
QLrd 1/1
allatlon In planning electric power supply for industrial
uterprises. Prom.energ. 12-no.6:17-20 Je 057. NUA 10:7)
Gosudarstvannyy politakhnicheskly In2titut 1*114romelektroproyekt.
(Blectric power)
FEDOROY. Anatoliy AnRtollyevich; VERTERM, V.I., redWdor; 1ARIONOV, G.Te.,
tekhnicheskiy redalctor.
[Supplying industrinl establishments with electricity] Elaktrosaab-
zhanie promyshlennykh predpritatli. Izd.2-os, perer. I dop. Koakva,
Gos.energ. izd-vo. 1956. 463 p. (NIM 9:5)
(Electric power)
SOV/81-59-24-84749
Translation from: Referativnyy zhurnal. Xhimiya, 1959, Nr 24, p 9 (USSR)
AUTHORS: Barohuk, I.F., Vertebnyy. V.P., _K_o_n_s_tA=,noy, B_ tleme-t-5, O-F,
Paseehnik, M.P.-----
TITLE: The Spectra of.Fast Neutrons Scattered From Atomic Nuclei
q
PERIODICAL: Tr. Sessii AS UkrSSR po mirn. ispol'zovaniyu atomn. energii. Kiyev,
AS UkrSSR, 1958, pp 94 - 101
ABSTRACT: The spectra of neutrons inelastically scattered from the nuclel of Mg,
Al, Fe, Ni, Zn, Cu, Sn, Cd, Hg, Ph and Bi were studied by means of
ionization chambers filled with hydrogen or methane, and a sc ntillation
counter with an anthracene crystal. The reaction D (d, n) Hei served as
source of neutrons with an energy of 2.8 Mev. The experimental data
obtained by means of ionization chambers were corrected for the "wall"
and "induction" effects; the curves have singularities in the points
which pertain to the excited states of the nuclei. The results of the
Card 1/2 measurements are presented in the form of graphs and tables.of the 0
.The Spectra of Fast Neutrons Scattered From Atomic Nuclei sov/81-59-24-84749
energy levels. The authors point out that in heavy nuclei in the case of inelastic
scattering of the neutrons only individual levels are excited. It Is therefore in-
correct to consider the process statistically in the case of energies of several Mev.
1. Sadikov 0
Card 2/2
L 1- it- ljju-V-~l .--, ~~/,
iz.
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i9
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ar F.
29
or
91
&Age P
VIRTIBNYY, V*P. (Vartobnvi, V.Pj; VIASOV, M.Y.; PASICHNIK, M.V. [Pasichnyk,
TOTSKIY, I.A. [Totelkyi, I.A.]
Spherical electron-pulse ionizatlon chambers for the study of fast
neutons [in Ukrainian with summary in English]. Ukr. fiz.zhur. 3
noo2:196-203 J4r-AP 158. (MIRA 11:6)
(Neutrons) (Ionization chambers)
~1- (a C) 0 0
AUTHORS:
TITLE:
28434
S/165/61/006/002/UO6/020
D210/D304
Vlasov, M.P., Fedorov, MoB*# anql~
14thane diffusion cloud chamber for neutron
spectrometry
PERIODICAL: Ukrayinslkyy fizychnyy zhurnal, v. 6, no. 2, 1961,
186 - 190
TEXT: In this article the authors describe the constructions and
operation of a methane diffusion cloud chamber for spectrometry of
neutrons of energy 1 to 3 MeV. The construction of the chamber is
shown. The chamber was operated at one atmosphere of methane using
methanol for diffUBionp giving a sensitive volume of 3 cm high by
20 cm diameter. The electrodes are made of two screens connected
together and kept at a potential of lkV relative to the base plate
and the methanol groove* The flow of the cooling liquid nitrogen
and the methanol temperature were controlled automatically to give
base plate and methanol temperatures -70 and 100C respectively, to
Card 1/2
Methane diffusion cloud
2!,434
S/18 61/006/002/006/020
D21OY3)304
within � 0.50C. The chamber was operated by means of an electronic
arrangementq given in the original paper, which starts the neutron
generatorp switches on the electric field and the pulse lamps, and 1A
winds the photographic film in the required sequence. The chamber
was tested by analyzing the neutron spectrum from the D(d9 n) reac-
tion in the direction of the denterium. beams of 150 keV energy,
and the dispersion of the apparatus was found to be 8 % half-in-
tensity. There are 5 figures.
ASSOCIATION: Instytut fizyky AN URSR, m. Kyyiv (Institute of Phy-
sics, AS UkrSSR, Kiyev)
SUBMITTED: August 229 1960
Card 2/2
AUTHORS:
TITIZ:
PERIODMZ:
16
c;/i35 02YO07/009/003/Oo6
V234 308
Vertebnyy, V.P. and Kolotyy,' V.V.
Design of a neutron monochronator consisting,'of
several discs with a longitudinal axis of- rotation
Ulwayiiialkpl fizychnyy zhurnal, v. 7, no. 9, 1962,
975-979
TEXT: The authors deduce an approximate equation for the
.bath of a neutron and apply it to the calculation of the maximum
possible nunbcr of slots in rotors consisting of two, three and four,
discs. This number is found to be 2jtR/(2s + 2a), w1here R in the
d-stance of the neutron fron the axis of rotation, 2a the distance
between slots and 2s the slot vidth. They also quote cxpresnions
for the -resolving power and an,approximate formula for the iiit~nsity
of noutrona at the output. It is concluded that the weight of the
.rotor can be made several tinics smaller than in designs i-rithout
slots. There are 4 Eigures.
Card 1/2
--/1S5/62/007/ooq/oo3/c66
Desi&m of a neutron ... D234/D308
ZOSCCLVION: Inctytut fizy1cy XN URSR Kyyv (Institute of Phycics,
'L
~
S UkrS311, lUev)
SUBHUTTED: January 30, 1962
Card 2/2
h 16h 3
3/135JG2/007/009/004/oori
D234/D300
AUTHORS: Vertebnyy, V.P. and Kolotyy, V.V.
The shape of ncutron pulse and the transmission
function of a two-rotor neutron chopper. 1. Choppers
with planc slots
PZRIODICAL: Ulla-ayinslhyy fi--iychnyy zhurnal, v. 7, no. 9, 19621
980-991
TEXT: The calculations arc firot made for the case of a
siagle rotor, a problem ifnich was already ponsidered by V.I. Nosto-
voy and others. The calculations are then extended to the case of
two rotors. The transmission function is found to be
f(Z'OL) 2 fl(Z' .00 -I Z4_ 4 jOC(z2 + 8 v--1 + Z2 X1 z4 (1~3a)
3 (12 4 + 12~
X
if 0 ~