SCIENTIFIC ABSTRACT GELBSHTEYN, A.I. - GELD, P. V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000514610019-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 23, 2000
• Sequence Number: 19
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

GE L I Pj11111A N? A.1 . ; SIROYEVA , C . r). ; h1; P ROVA , N.V. ; I VIE J)PI, Y11.14. ;
.. - ,LAPIDUSY VA. 11 .
Mechanism of the catalytic reactions in the partial cx1dation
and oxidative amonolyalo of propylene in the presence of
M003--D12O3. NeftekhImiJa 5 no.1:118-125 JfL-F 165. (MIhA IS: 5)
1. Nauchno-issledovatellakly fiziko-khImicheskiy institut imen!
Kurpova, Moskva.

SILING, M.I.; Q.11ZIMYN A.I.
Use of adsorption methc6:; in atucying catalysLs for wqcjr-p~wje
synthenis of vinyl acetate. Kin. I knt- 0 no.4:71'1-724 JTI-Ag 165.
('41RA 1819)
is Fjziko-khImi(:hamkII.y Institut. ',%!nnI 1,.Ya. Kn:-I-ova, ~-'('A-VR.

5 1 ul f " " ~ . ~ . ., .,I Ili" li ~-ilyll
I - . I-LLA 1-0
; 3.(! of carbon as a narrier In somo cases of catalysis. Zhur.
f!z, khim, 39 nn.8!2042..2043 Ag 06% (MIRA 18t9)
T. Vnskovs~3y fiziko-k),44eicheakly Inatitut Imen! Ka.-pova.

0t,
k1notic r!t:!iativn constanLs for tho~,
nitrl2e. F~.I:vl. Prclla. "'I
a

GFMIBSHTE)N~ A.I.i.BAKSHI, Yu.M.; STROYEVA, S.S.; KULIKOVA, N.V.; UPIDUS,
Y.L.; SADOVSKIY, A.S.
Kinetics and mechanism of oxidative ammonolysis and partial
oxidation of propylene an bismuth-molybdenum catalysts. Kin.
i kat. 6 no. 621025-1032 N-D 1165 (MIRA 1-9:1)
1. FizIko-khAmicheakiy institut iment Narpova. Sulmitted July 28,
1964.

G3~11KRMTN, I., inzhener.
,5714
"Zf~ht hoist. Strlt,-) I ro.7:21 J t 157,
M
(Hoiating mmehinery)
'mild. 1c):,4)
t

SKVORTSOT,S.G., inzh.; BYKOVSKIY, G.F., inzh.; VASIXA. I.N.,.inzh.; VOROKIN,
All)&, POLTAXOT, L.L., insh.;
GUCHUSOIKOV;-4a., Inzh., red.
(Catalog of desigu of stands$ constmotion yards$ equipment "d
devices for making prestr6osed reinforced concrete elementm]
AlIbm-katalog proektor standov I poligonov, oboradovantia I
prisposobloull dlI& Isgotoylealia. predvaritellno ua;prIash*nm7ft
Sholesobetomykh kountruktati. Moskva, ?3*ntr. biuro tekhw4 infom
No.VZh-2. 1957, 118 P. (Om 11210)
16* Akedadys stroltelistva I arkhttaktury SSMk Nauchno-Issledo-
vatel'skly Institut tekhmichemkoy ponoshchi stroitelletvu.
(Preatregised concrete)

GF-LITCHTFY11, 'el. F.
GELIMIITEYN, I. - "Pathological Anatomy and Pathology of Experimental
In
IntoxicatJon by Iniline.11 Sub 6 Jan 52, Acad Med Sci USSR.
(Disservition for the Degree of Candidate in Medical Sciences).
SO: Vechernaya Moskva January-December 1952
I

study of-' the absorption of railcactive
iodine by thyroli gland tixnors. !!ad. ri,.'. 8 no.9*34,"O 3163.
2. Tz ptologotinittomichuskorc otielenlyt,. (-.-!iv. med. nauk
Z.V. Go?, lb?rt) i kand.
nriuk Vol-A'ova) in_- t-J-,,a imen?L

BESSONOV, A.N.; GELIBLOM, L'Aj TELISTRATOV, I.F.1 SMIRNOV9 V.A.;
TAmny,--lu.S., Mitan 2 ranga, red.1 CHAPATEVA, R.I.,
tekhn. red.
(Underwater search] Podvodnyi poiek. Moskva Voenizdat,
1963 93 P. WRA 16tIO)
(Di;lng, Submrlne) (Underwater television)
(Underwater acoustics)

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,~~LIBUKH, L. A.
USM/blectricity - Bus Bars
Inductance
Aug 5()
"Calculating the 6xternal Inductance of Thin Rectangular Steel ~IUB Damp" Docent A. M.
Vinitsjkiy, Cand, Tech Sci, L. A. Gollbukh, Cand Tech Sci, Kharlkov
"Elektrichestvoll No 8, 37-39
Gives deductions from formulas for external inductive reactance of thin rectangular steel
bus bars. Formulas deduced agree well with experiments.
FA 16'jT23
Z:
I llj~ "iA~1

USsR/zlectricity - Control Circuits Feb 51
Transbents
"Analysis of the Operation of an induction Pover-
-x Directional Relay With a Cylindrical Rotor in
F-7 Transient Processes," L. A. Gelkbukh, Cand Tech
lc:_~
C_ Sci, Xhar~kov Elec Eng Inst
1-4
"Elektrichestvo" No 2, pp 2.1-25
Investigates action of single-phase induction
pover -directional relay vith cyl rotor resulting
from transient currents in its vindings during
fault. Proves nonselective operation of the re-
lay is possible under large voltage changes, This
USsR/Zlectricity - Control Circuits (Contd) Feb 51
ca.7n be prevented by connecting capacitance and effec-
tive resistance in the vbl.tage vinding. Submitted
10 Aug 49.

MM/Mectricity - lmductim Keating Sep 52
Arc Quenching
"Wtion of a High-Frequency Electric Arc in an Are-
Quenching Grating," Prof 0. B. Bron, Dr Tech Sci,
L. A. Gellbukh, Cand Tech Sci, Leningrad
"Elaktrichestvo" No 9, PP 7-3.2
Discusses electrodynamic forces acting on a hf elec:
arc in an are-quenching grating. Shows that ef-
fect arising in the quenching of a hf arc by a
gmttng are essentially different from those occur-
Lng in the quenching of a dc or pover-frequency
232T48
a"'! inposing nev requirements on the design
Of Witching equipment for hf currents. Sub-
mitted 8 Dec 52.
232T48

AUTHOR GELIBUKH L.A. Pk - 2546
TITLE da_T-c_uI-a-"-dn__0'f Induced Magnetic Moment of Ferromagnetio
Ellipsoid of Rotation under Alternating Magnetic Field.
(Raschet indutairovannogo magnitnogo momenta ferromagnitnogo
ellipsoids, vrashoheniya v peremennom magnitnom pole.-Russian)
PERIODICAL Zhurnal Tekhn. Fiz. 1957, Vol 27, Nr 3, PP 548 - 559 (U.S.S.R.)
Received: 4/1957 Reviewed: 5/1957
ABSTRACT As with magnetizing there is always a partial drazging in of
the lines of the magnetic field into the objectv Ralleyta
formulae give rise to considerable errors for farromagnatic
bodies on the occasion of the calculation of the magnetic
momenta. An approximated calculation method is suggested and
a marked occurrence of the surface effect is assumed. The
voltage of the exterior field is determined by the vector H
t
o
which can be divided into the components H in the
longitudinal and Rb in the transversal axil of the ellipsoid.
Accordingly, the induced magnetic momenta will be m and m
-
b
Neyman's method with due modifications is applied. he
strata thickness 6 with an evenly distributed magnetizing
t
Intensity is inser
9d Instead of the shell thickness. The
magnitude is determined and then the correctness of the
approximatbd method is checked by exakt compulation.
CARD 1/2
induction diikr-enZ9--- -Tne approximatua matnuu; SAW.V.-. 7
give any phase relations between these momenta* The result
obtained can also be generalized for bodies of a different shape.
Neot, the magnetic moments of the longitudinal and of the
transversal components of the magnetic field are compished. The
equations obtained define both components completely. If
0 and Cr co are inserted, the formulae by Ralley
Ao
and those fpr the magnetic moment of the ferromagnetio ellipsoid
in a static field are obtained. Thus the correctness of the
method shown here is proved. magnetic transparency).
(With five illustrations)
ASSOCIATION: not given.
PRESEN72D BY: -
SUBMITTED: 20-7. 1956.
AVk1LkBLZ: Library of Congress.
CARD 2/2

105-0-5-~U/31
(Leningrad)
AUTHORi Gel'bukh L. A. , Candidate of Technical Sciences
TITLEs Heating of a Ferromagnetic Ellipsoid in an Alternating Mag-
netio Field (11agrev forromagnitno6p ellipsoids, vrashcheniya
v peremennom magnitn 0m pole)
PERIODICAM Elektrichestvo, 1958, Nr 3, PP- 50 - 51 (USSR)
ABSTRACTs Here, the heating of stretched bodies by means of induction
is investigated, viz. of such bodies, which can be replaced
by equivalent ellipsoids. In this way the influence of the
finite dimineiona of the body upon the energy, which is ne-
oessary for its heating, can be taken into consideration. It
is assumed that the exterior magnetic field is everywhere
parallel to the great axis of the ellipsoid. It is assumed
that the surface effect appears intensely. The computation
is-carried out for the constant magnetic permeability e4and
for the specific electroconductivity it of the materialp
taking into consideration the hysteresis losses. The prob-
lem is solved by means of the method proposed by L. R. Heyman
Card 1/3 (Reference 5). The investigated body is replaced by a ferro-

105- 58-3-12/.31
Heating of a Ferromagnetic Ellipsoid in an Alternating MaL-netic Field
magnetic cover with a thickness S equivalent being equivalent
to the depth of penetration of the electromagnetic wave into
the metal. The metal is located in the static magnetic
field of equal strengthw This cover weakens the exterior
field acting as a f erromagnetic screen. In the case of an
alternating field the eddy currents within the cover must
behave in such a way that they completely compensate the re-
sidual field in the interior of the ellipsoid. After having
computed the amperage, the energy delivered in heating by
means of induction can be obtained. In Reference 5 it was
shown that for the case of a ferromagnetio sphere In the
alternating field the results of computittion according to
this approximated method agree well with the results of the
computation according to the exact method. This permits to
apply the approximated method in the case of an ellipsoid
as well. The thickness of the wall is assumed with
dequivalent a
where Q denotes the angular velocity of the electromagnetic
wave. For the purpose of simplifying the computation a cover
Card 2/3 formed by two confocal ellipsoids is investigated, instead of
!iell

105- 1 12/31
Heating of a Ferromagnetio Ellipsoid in an Alternating Magnetic Fret
the elliptic hollow space with equal wall strength. It is
shown that in the case of a greatly stretched ellipsoid in-
tensely showing the surface effect, the volumes of the cover
are equal, if the thickness of the cover in the equator plane
S - Mr/O S equivalent* For this case the strength of the
magnetic fi Id H inside the hollow space (Reference 6) can
be determin:di Ehuation (3). If H is knownp it is not diffi-
cult to compute the linear current density within the cover
(per unit meridian length), which is necessary for compen-
sating this field strength. Finally, the equation (a) for
the energy absorbed by the ellipsoid is derived. Then an
example is computed. There are 2 figures and 6 referenceal
8~u Swift",
SUBMITTEDs June 20, 1957
Card 3/3

SOV/49 -58-10-4/15
AUTHOR: G-I-.11 "ULI.-' A,
a settled Field Due to the Polarization of
Oblate and Y'rolate j,AvroJLa:3 (i.Ascliot; u..-3Laroviv:3he,,o:iya
C3
polya vyzvtnnoy polyarizatsii tel. itacyushchii-di forau
vytyanatogo i 3zhatogo 3feroidov)'
PERIODIV"AL: Izvestiya Akademii NauK SSSR ,riya aofizicheskaya,
1958, Ar 10, pp 1192-1201 (TJSO-'R)'
ABSTRACT: Ref.1 considers the fields due to C)olarization of
sl~,herical bodies. The spheroids considered in this article
are assumed to be situated in unif3ria, rAectrir, fields E
The corductivity of the spheroid is Yi and of the medium
ye . The prolate 3ilhoroid is considered first using the
coordinate syitc;-ii pr.)posed in Refs. 2 and 3, vinich is
Connected with Cartesian coordinates by the relations (1),
(2) and (3)' ea and 9b denote the iidlxced polarization
in cross-sectiDns along major and minor seLii-axes of the
si)heroid. 11(~nce the conp-onents, of i.,,du--ed pola-rization
'"' ) at any point (TI ~) can b(; written in the forM
Gx I C-t 0 "
Eqs.(~) and For Umall current densities (up to 1-2
,ia/cni- see (Ref K" d k can -oe cDasidered nro-
Card 1/5 1 -1))' a all

SOV/49
A CalcuLati ii )I, a Settled Field We to the Polarization of Ob a 'd
Prolate 0-~Jl(.;roids
portional to the nor-rial current density -it the corre,~3,,-~)nd-
inr~ VointS on tile surface. Tile potential of "he extcrnal
U u
applied field due to the comp.,nent E x can be v;ribten a3
Eq.(12), if the plane x = 0 is con6l(!_~red ti--, haviii.- zero
potential. Similarly, tile potential dm to E can be
written in -the form Eq.(13). T'ne disturbed fiRld potential
can be ex-Dressed inside the suheroid by U 301LItion of the
type Eq.(il) and outside by t6 type Eq.'10). This gives
lon-itudinal and transverse fields of t~;e forra Eis.(14 and
15'5. Tile boundary conditions aU the iiuirface (TI 2~ Tl.~ are
Eqs.(16) und (117). These traasforfa to (to deta-mine
Lho arbitrary coastants (A and B)) and can be solved in the
form Eq.(20), For very elongated spheroids (Tl,,, -,p 1) tile
functi.ons P, Q, - Pl' , Q11 , vi4,iich a~;-)ear in the forekLoing
equations, can be expressed by the a~.qpr3,xi-;'aLi,,)ns shZW41.
C,ard 2/5

SOV/49 -58-10-4/15
A Calculati~~n of a Settled Pleld due to the FIRapIzation of. Oblate and
Pro 1:3 L-e Spheroids
3ubstitutin- into En.(20) (-22) for
A Lind A' PutLiw- valw.,z of A and A: in the
firjv' of tite equations detormin,~s tac -Dotential
outsid:) tile soh~~roid. T'Ais rapre6oot~; ou.-i of tho poten-
tial due to induct,~d and U:i.-- i),it-c-itial due to the
field disLurbance caused bj the diff-re:--L conductivity of tile
body and inediu:.i. If k P is !)Lit eq'1,k1 to Zero in tllose
equatijii3, the coofficients A and A nD-.i to the
p
induced polarization field onlj. At la:,,-,-, d'L,taaces from
the body, the induced polarization can be r~"Garded as due
to tvo T,iutually perpenc~icular di-poleo directed along the x
and z axes. The electric mouent~3 of these dipoles can be
determined by the approximation that, au" di.;tant ooints the
sDheroidal coordinates can be considered ao onherical polar3.
I:; thiz; the j)otential is ropresent-~,d by the equations
(25') and (261) whicii are co.iipared to th,,~ norual equations
for such a dipole (25") and (20"') . T,.is Silre3 Eqc.(27) and
(28) for the moilents. If U-io condiactivity of the body is
cf)noldt~rably Groator than thlat of t~-i.e (Yi~~ Ye)
Card 3/5

SOV/49 -58-10-4/15
A Calculation of' a Settled Field dud to -the Polarization of Oblate and
Prolate Spheroids
then Eqs.(27) and (28) simplify to the forms (27') and (281).
Next t~e induced polarizatijn of an oblate j;;heroid io cor.-
sidered (Fig.2). The coordinate oystem. in this case. is
re la' Lons Eqs.
connected witla Cartesian coordinates 'u-)r th,
(29) and (30). As before, the induced :)alarization can be
expre3sed in t-rins of the formulae (33) Lind C~4) and, in the
same mavaier 7 8b and ga are represented by E,-Is.(35') and
(361)~ The disturbed field potential outside is determined
by expressions of the type Eq.(37) and, _1-3ide, by express-
ions of the ty,.je Eq.(38). Hance the lon,,itudinal fieid is
represented b Els.(39) and (40) and tiae transverse field by
Eqs.(41) and ~42 . Eq.(45) L,J-Iives the final value for the
cooffici,---rit A and thore is an analor,-OUZ; equation for A'.
For very flattened spheroids (q I