SCIENTIFIC ABSTRACT KOBELEV, L.YA. - KOBELEVA, V.A.

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000723410006-8
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 19, 2001
• Sequence Number: 6
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

-27/341
AUTHORs Kobelev, L.Ya.
TITLEt Oa the Problem of Description of an Electron-Ion
(K TOPrOBU OpiSaniya elektronn-jonnoy p'L%zmy)
FMODICALMsika 149talloy i Mstallovodenj3o, 1958, 7o1 6,
Nr 49 Yp 754-756 (USSR)
ABSTROTs
card 1/2
Pl:~S
Classical and quantum-meehanical kinetic equations of
an 6100trou-ion plasaa (Ref.1 2) do not allow for tbo
virtual processes of interactions of electrons and ious
with the self-consistent field of the plasma. When
these virtual processes are taken into account & system
of interacting particles is described in the self-
consistent field approximation by means of Schwingers
equations for the non-relativistic Greents function
(Bef.3). :Me author derives the Green's function for
a system consisting of two types of interacting
particles, eg, electrons and ions. He also deduces a
weneralisati n of the dispetsion. relation for an
electron-ion plasma which allows for the virtual
interactions of electrons and ions with the
SOV/126- t, -4

SOV/126-6-4-27/34
On the Problem of Description of an Electron-Ion Plasm
self-consistent field of the lazaa. The paper is
entivel;j tbooretical-AWMawlsdpe~ts aro made to
Co=eupouding Member of the Ac.Sc. USSR S.Y.Vonsovsk-Ly
for his advide. There are 6 references of which
5 are, So-list and 1 English.
ABBOGIATION:Uraltakiy Gosudarstv"nxqy universitst looni
A.M.Gorikogo (Ural State University imeni A.M.Gorlkiy)
SUBMITUDs 15th April 1957-

AUTHORz SOV/126-6-5-35/43
TITIE: on Correlational Corrections to the Hartree-Fock
Equation (0 korrelyatsionrqkh popravkakh k uravueniyu
Khartri-loka)
PERIODIOALs lizika Metalloy i Metallovedeniye, 1958, Vol 6, Nr 5,
pp 943-945 (USSR)
ABSTRAM Behaviour of a system of interacting particles,
described in terms of the self-o=istant field approxi-
mation, is determined by the Hartree-Fock equation for
a wave-function or a density matrix of a particle in
the self-convistent field. of all the other particles.
Processes of virtual interaction (absorption and emission
of virtual quanta), as well as changes in exchange forces
due to polarisation of the self-*miotent field, are
neglected, The present paper introduces correlational
corrections into ,the Hartres-Fock equations which allow
for the effects of polarisation and virtual procisses,
These corrections are calculated on the assumption that
the polarisation and virtual processes are snail
perturbations, The perturbation theory method is used
Cardl/2 in these calculations. kn equatior, for the density

BOV/126-6-5-35/43
On Correlational Corrootiong.to the Hartree-Fock Equation
matrix is derived (3q 12) in which the correlational
corrections are given by the last term. The energy of
an 0100trOn in the SOlf-waSistent fields with small .
correlational corrections (for larisation and virtual
processes), is also calculated fRoq 13). Acknowledgments
are made to Professor a. V. Vonsovskiy for his advice.
There are 5 references, 3 of which are Soviet and 2
English,
ASSOCIATION: Ural'skiy gosudarstvennyy universitet imeni
A* M, Gorlkogo (Ural State University imeni A.M.Gorlkiy)
SUEMITTED: May 61 1957
Card 2/2

AUTHOR: Kobe SOV/126-6-5-38/43
TITLE., on the Effect of Correlation on the Prequency of Plasma
Oscillations (0 vli7anii korrelyatsii na chastotu
plazaennykh kolebaniy)
PBRIODICAL-. Fizika'Ketallov I Notallovedeniye, 1958, Vol 6. Nr 51
pp 948-951 (USSR)
ABSTRAM The effect of the exchange correlation on the frequency
of plasma oscillations in a s stem-of interacting
particles was discussed by Sifin (Hot 1). Teloonskiy and
Zyryanov (Rat 2). Correlation due to interaction of
particles with the Ovacuux* of the system is dealt with
in the present paper. It is assumed that the correlation
energy is small compared with the energy of fundamental
excitations. The correlation correction to the dispersion
relation of the system Is calculated by means of the
Green's functions using the technique first described by
Bonch-Bruyevich (ief 3). The author starts with the
dispersion relation for fundamental excitations of a
system of interacting particles given, in the momentum rep-
cardi/3 res4atation. and with the magnetic interaction neglected, in

SOV/126-6-5-38/43
On the Xffsot of Correlation on the Irequency of Plasma
Oscillations
the form
p2 - is2 GO(pl)ro-(p; p1p, - p) 00(p, - p)dpl 0
(2ft)4 + 0 +
where 00 is the approximate expression for the Green's
functioeof a particle correspondin to, for example,
a particle distribution with un4 ora density;
is the vertex part expressed in terms of Go
~o a 1, When the correleion-energy is small, the
tex part can be written approximately as:
r 0 a I - 182 G1001, P2)00(Pl - P2 - p)DO (p2)dP2 -
0 ow)" S + + Q+ (2)
where D is the-solutim of the equation
0+
0
1
3 DO+ 1 + OPODO+
C&rd2/3 Using the form. of r given by Eq (2)t the author
0

SOY/126-P-5-68/43
On the Effect of Correlation on the Prequency of Plasma,
Oboillations
calculates the dispersion relation (Eq 6) which includes
a correction for the correlation due to interactions of
the particles with the "vacuum". Nq (6) is used to
derive the dispersion relations for a system of bosons
(BIJ) and a degenerate Fermi gas In the second
ha of the paper the vertax part (rEgv o0Nq Mis used
0
in its general form and a now dispersion relation (Eq 12),
is obtained for the same conditions as Xq (6). Nq (12)
is then used to derive the dispersion relations for a
system of bosons (Eq 13) and a system of fermions (Eq 14).
There are 5 Soviet references.
ASSOCIATION., Ural0skiy gosudarstvennyy universitet imeni
A. M. Gorlkoso (Ural State University imeni A. H, Gorlkiy)
SUBMITTEDs October 28, 1957
Card 3/3

24.6060 657n
BOV/139-39-24W30
AUTHOR s lobelevt L,Ya,
TITLE s On the Calculation of the Vortex Part of a System' of
Interacting Particles
PERIODICALs Izvestlya vyashikh uchobnykh sayodeniyt Fisikas 1959,
Wr.91 pp 60-68 (USSR)
ABSTRACTs A highly theoretical paper concerned with the derivation
of expressions for the vertex part In the theory of
systems of nonrelativistit interacting particles, Single
particle,areen functions are used (cr Edwardal Her 1).
Approximat*"#xpr*AAions Ar& derived for the vertex part
using the methods put forward by Vard (Ref 2) and
lAndau at &I-(Rof 3)s It is shown that the vertex ports
for systems of bosona and.fornions, calculated under
various approximations taking into account an Infinite
number of Feynman diagrams, strongly depend on the moment&
and energies of the particles. It follows that for systems
of strongly interacting particles with T la Og the
approximation T aLl is very rough, The s*lf-consistont
Hartree-Fook field approximation in the case of systems
with large density., strong interaction and T w-0 may not
Card 1/2 describe some important 1,roperties of the systems For

10.4ooq 66596
AUTHON i Kobelev, LAS. $0V/139-59-3-4/29
TITLEt BF the Speo of Sxoitaticns of an Interacting Boson
system
PERIODICALt Izvestlya vysshikh uohebnykh zavedeniyg Fizikay
1959$ Nr 3, pp 23-30 (USSR.)
ABSTRACTs Behaviour of a system of bosons was studied by many
workers (Refs 1-5). Qualitative explanations have been
advanced for the most Important properties of the SPOOM
of fundamental excitations of the superfluid state such as
the presence of two branches of the spectrum (Ophonono and
"'roton" branches) and non-monotonio dependence of the
phonon energy on momentum. Dependence of the honon energy
on the wave vector, obtained by Brueckner and Cwad&
(Ref 4) does not, however, agree with the experimental form
of this dependence (got 2 . Moreover, Brueckner.and
Sawada's theory fails to pr4dict two velocities of sound
in liquid helium ind the asin results of Brueckner-Sawada
and Lee-Huang.-tang's theories (Refs 495) can be deduced
from Bogolyuboy's work (Ref.2) using hard-sphere inter-
Card 1/3 action. It seems unlikely that the strong interaction of
Particles with the vacirm of the system, which is imports, t

-SOV/139-59-3-4/29
On the Spectrum of Szoiiations of-an Interacting Boson System
Card
2/3
at low temperatures -leads only to small corrections to the
solf- consi-stentINk mothod results. The author therefore
sets out to study &~systw of bosons using mathematical
motho.ds which would allow scire fully for the interaction of
partioloswith the vaouum of ' the system and would load to a
relationship between the two velocities of -sound in liquid
helium. The author disaussais the phonon branch of the
speatrum of fundamental.axol.tations of a boson system at
low temperatures' using''tho Orson's functions method. The
system is described fully by, means of the Green's functions
of the particles and of the electromagnetic field. The
Groan's funo'tions-aro doduosd from equations with
variational derivatives$ similar to the well-known
equations of Schwingor's quantum field theory (Ref 7).
The dispersion relationst between the energy of fundamental
excitations and momentung are given by the poles of the
Orson's funations of the partiolos and of the interaction
fieldo For the hard-sphoro interaotiong the author shows
that two branches of aaousti* vibrations are possible, each
with a different sound velocity. The paper is entirely
theoretical. Acknowledgement is made to Corresponding
V
.. , I

'14(3) 24(4) SOV/126-7-2-21/39
OF
EKUS: Xobelev
,JL,ja. and Sokolov, A. V4
TITIZ: Ta--m-agnoto-Optical Phenomena in Ferromagnetic Binary
Alloys in the Par Infrared Frequency Region
(0 magnetoopticheskikh yavleniyakh v ferromagnitnykh
binarnykh splavakh v oblasti. dalekikh infrakrasafth
ahastot)
PERIODICAL: Fizika Metallov i Metallovedeniye, 1959, Vol 7t Nr 2,
pp, 289-291 (USSIR)
ABSTRACT: The dependence of the Kerr and Yaraday constants on the
alloy composition and the degree of long range order
in the above frequency range is calculated. The
calculation was based on the theory of binary alloys
given in Rot 2, The tw nstants are given by:
F
(12 V2) VFA (1-0 (q-c) 2,q2+BY2
*21. 0 7---w
.72 (8)
0%.0 2 2 Y2
0(3.-C) (q-0) A + S
Card 1/2 1 -VO T--w

BOV/126-7-2-21/39
Oh Magneto-Optical Phenomena in 7orromagnetic Binary Alloys in
the Par Znfrared Frequency Region.
where V 0 is the offs0tive frequency corresponding to
the spin-orbit interaction V is the frequency of the
incidont radiation, 4 is the degree of long range order,
c describes tho'composition of the alloy, A is a
constant independent of c and the degree of long range
1/2 and q-2c for
order and qwl for c > c < 1/2; B is a
~constantj 7 is the spontaneous magnetisation of
d-electrons which is a function of c and 19 and w is
the matrix element of the operator representing the
magnetic spin-orbit electron interaction energy,
Professor-.9, U, Nookov and A, N, Levkov are thanked
for the discussion of the results. There are 3
references, two of which are Soviet, 1 Englishe
ASSOCIATIONS: Institut fiziki metallov AN SSSR (Institute of Metal
'Physics Ao,Sc., USSR) aind Urallskiy gosudarstvennyy
universitet imeni A.M. Gorl.kogo (Ural State University
imeni A.-M, Gorikiy)
SUBMITTED.- July 2, 1957
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boom

5/139/60/000/004/042/044/XX
9031/9413
AUTHORt -Kobelov, L.Ya.
TITLEs On the Application of Repeated Integrals Along the
Trajoator.%Jn the Theory of Gre*nfs function for a
System of Non-Rolativislic Particles NN
PEMOrCALt tavestiya vysshikh uchabnykh zavedeniy, flzika, 19601,
No.4, pp,206-216
T9XTs Green's function for a system of non-rolativistic inter-
acting particles Is written-with the aid of repeated integrals
along the trajectory in a functional space and calculated using
the mathematical apparatus of integration in functional spaces.
In order to us* the expression (1.1) for Green's function at.,
tomperaturo. T = 01 It Is necessary to solve the equation
I H(V A (x) G1(Xy/A) 6(X (1.3)
at
It will be assumed that the Qr,s*nls: D,,,j In (1.1) Is
known. Yokto method is used to solve Eq.(1,3). The solution is
,expressed by equation (2,7). For a system of particles it is
more convenient to use retarding and advancing Groan's functions,
Card 1/3

8/139/00/000/004/049/044/XK
2031/2413
On the Application of Repeated Integrals Along the Trajectory in
the Theory of Greents function for a System of Non-Relativistic
Particle*
Gr and Ga which are obtained by integrating Sq,(2,7) with
respect to p0 and in solving Zq*(2,6) choosing a.zontour of
Integration with rospeot tg-.p* corresponding to conditions on
VI ret and VJL adr similar to -those on Gret and , Gadve 'To find ao
a solution of Sq.(2.6) suitable for determining the functions
Gr and 6^ fora system of interacting particles, the boundary
condition VILM /9"00 .6(; - F)_ in not.sufficient, mine* the solution
of Sq.(2.6) must sotisfy additional boundary conditions Imposed by
the choice of the contour of integration. The solution of Zq.(2.6)
in the form or repeated integrals depends on the choice of the
correct measure in thefunctional space. When this solution to
obtained an expression can be given for Or, tq.M-6), which Is
a particular solution of the Cauchy problem (1,3). Substituting
this Gre*nl.s function In (lol) and carrying out the functional
integration withrespect to the external fields various Green's
functions are obtained for it - 0,1,2,3. These are quoted
(Zqs. 00) to (43) By way of a first example the perturbation
Card 2/3

S/126/60/010/002/025/028/XX
2032/2414
AUTHOR: Kobeloyl LoYa.
TITLEt On the Caltulat-M of the Response functions for a
System of Interconnecting Particles
PERIODICAL; Fizika metallov I metalloved*n1ye, 1960, Vol.10, No,2,
PP-306-308
TEXT.- The aim of the present note Is to derive corrections to tho
expressions obtained by Xubo for the response functions, the
corrections being due to the interactions between the particles.Iq
The discussion is concerned with a system f interacting Fermi
Particles and it in shown that the correct response function Is
g1ven by
r y) Y) (Ir yl)H (YJL) �r(y, - y)dyl
my YO
r x (x YI)v0(y, yo) fp(yl - y)dyldy,
GUY yl) MYO 0
f
r
Mo
+ G (x Y) rh (Y) X y1ho
Card 1/2

8/126/6o/olO/002/025/028/=
2032/19414
On the Calculation of the Response Punctions for a System of
Inter~--onnocting Particles
where the first term in Identical with the Kubo function, the.
setond term in proportional to the Pauli (paramagnetic) field of
the system due to the interaction bttween the particle*, the third
and fourth terms are due to interference effects between the
particle density function and the natural magnetic field or
magnetic moment of the system. In this expression the diamagnetic
terms are neglected although it Is said that they can easily be
lntrodu4*d, There are 2 reforencess 1 Japanese and I Rnslish,
ASSOCIATION: Urallskiy Sosudarstvonnyy universitot im, A,M,GorlkoSo
(Ural State 'University imeni A.M.-Gortkiy)
SUBMITTEDt March 25, 1960
Card 2/2

VONSOVSKry, S.Y.1 KOHSLKV L, U.
quantm theory of the ferrompetism of collective electrons.
hi, ut.i metaliared, ii no.W264U A t61. (KMA Us 6)
1. Institut fisiki ustanov mi sm I Ural Iskir gosudarstvanm
univermitet Imeni A.M. Gorlkono.
(Electrons)

A/ t 26/61/012/(K)6/o0'%/o;rS
AtifilMi Yonsovokly. S.V. and Ktobelev, L.Ya~
TITLF. On the energy or magn;f ir -*--"T-PFr-AFrTVn-betwP"n ~two
iqystem-q% of Antorncting elpetrona
PERIODICAL! Flattka motallov I metal lovedenive. VA2, no it. 1961,
TEXT.- In the m-d-mndel of tranoition metals put forward by
the first of the prosent authors (Rof.1, Z64TV. lq46. 16, 981)
It is m"qumed that the magnetic properties or a cryotal containing
stoms of tranpition -element* are almont. entirely deterl"ined by
the sub-system of "internal" electronm (d- and U-electro"s).
which are looked upon an a Aet of localired spin particle*. The
outer particles (x- nnd p-electrons) contribute mainly to the
electrical conductivity and rtor them it in the Fermi energy
which Is the significant quantity, In the progent paper the
Authors discuss the interaction of two "etm of electrons with the
hope that this might throw some light on tho theoretical
foundations of the The paper starts witis the formu-
lation or the general #,quntiono, for a qymtem or fermt quast-
Card 1/3

(in tile viiergy Or magnetic
2032/9514
rt1clex In a crystal con%j*tjnx or two *uh-nvotems.
r
7nXte-par t Tho
a icle OXCItntioniq of thoote ftub-"
by means of tho nporator'Spinor f0inctionx qyptrM'% Art', 4019cribeel
and
which represent the treation and RfInthfiRtiOn Of' elementary
vXcItAti-Onx (P.Y, condoictioti electron%. holon etc.), use-ts
'" ^do or the Pingl-pnritcle Grorit functionst AA originally
described by. 1. Schwinger (11vC.3 Proc ,Na t Arad Sri 10M
37, 4j2), Tile derived set of eaunijons for the mingle-partirlp
tpmperattire GrPPn Tionction is then it-ard to determinp the sivertrism
of elementary Pxvitntions noid the mair"ettintion Of* the mystem.
The andilvol a t.~q tile" stakil 11'red to tho rA%P of forromaXnet *c
"Yetellin And term% resPonmIltle For tile mastnetlv aninotrnov of the
Cnr,rJ 2/11

on the pisprty of, Max"01
1c
.
systom ntid tile contillblation due to the men" electrostatic energy
are neglected. The vnergy spectrism fis then examined In detal.1 an d
it io 01hown hnw tile Magnetization-depetelent termit vnry when one
or both oC tile nub-tsymirmp may be tooked ispon no coliective or
locall7eff. There are 12 reference-4: 6 Sovipt-hinc atid 6 non-
sovlet-bjoc~ The Engti"h-janXuage referencen read att frillow4st
Ror.,s- vchwingrr' 1. PhII.Mmit., 19-53~ 44, 1171,- jjej,.q. Steiner Es
Proc.Rov.Soc., 1918, A165, 172, Ref.10: Kniquia T. Progr.1'hoor.
Phys., 19ib, to, 41;1 t1of.12- Marschall V. Phyoi. 14060, 118,
19.
ASSOCIArIONS: Institilt fiziki metAllov AN S6.,R (its4titiste or
Phybicx or Metalm AS USSIO and
Ura,llxkiy jecistiniveriiitot Im. A, M. tsorlkogo
(Ural Stat",11isivorptly Imeni A, .4. tiorlicly)
SUHMITTEII: July 20, )961
Card

IOBSM ~ thy&*
Graphic representation for the dmalty function of the mawtim
isation of a partiole rystwo lavovyssuabobesavel fis. nq*3s2S5-
163 161, (KMA ]AsQ
1, 'grallskiy gosudaretwenM uuivvoltot in, A.M.Gorlkogo.
(Quantum statistics) NPOtic fieum)
v ism= m 11-70"RM

S/139/62/000/001/027/032
J4
4t, a!100 E032/9114
Kobelev, L.Yat., Filippovj B.N*q and Khodenkov, 4o SW
AUTHORS:
TIT On the effect of the spin-orbit interaction o
LE:
electrons on the energy of a spin wave
PERIODICAL: Izvestiya vysshikh uchobnykh tavedeniyl
Fizika. no.i, 1962, i56-161
TEXTs The spin-spin and spin-orbit interactions of the
electrons in a ferromagnetic are known to lead to a change in
the spin-wave energy# This change is of interest in connection
_'4
with the theory or the constants of anisotropy of ferromagnetice,s-, ,
In order to.doscribe the increase in the energy due to the spl:1-''I
orbit effect$ the authors use the Schwinger uethod involving
single-particle Green functions, The dynamical Schwinger
principle is used to set up the equations for the single-
particle temperature Ctreon functions including spin-orbit terms k...
General expressions are then derived for the energy of
elementary excitations and for the change in the apin-wave
energy due to the spin effeats,for, TV 10 OK and T 10
Card-1/2

Meat of the spiu-crbi~tia interaction of electrons an the
erargy of the spb wma Isv*vV*vWwb,z&v.;fIz. no.lol%-161
162o (KMA 15s6)
1. Urallskiy gosudarst"Mry udymitst imed I.M. 4lorlkogo.
(Ilectrons)
W.

a,
~_, i'_ --L, /
A~('MW-10'5 M44 AP3003560
,-'AVTHDI%s ObeJAYA-LeZU-1
T=Ixs gmaut sbaory of tams j*"t4s"m%mr* pollmorlsatton
Soum AN a=s Dou"A To JAI# a4, to 12630 03-316
I TOPIO TADS: qU4At= tboory$ 1mviAft1W4A*x* POlVartgatiOut elmOtMe P901020
exoitod
ADMUM OvA at the veriante-of quqmtum-tbm*r7 of test law-tevpralturs
merizatton conditioned by coUeetlve latereetiou of qmtel-Vartioles (eleatranso
protons, szoltor.A, *%a*) responalblo for the polymerization is omutinsd* Tbe,
moat important part of %be tbeor7 to %be explanation of the inactive Oaftoterl*-
tic of the proOess W the possibility of predloting several physt4al pbsomma
(polywrizing waves# resonance pb"omua# vw=ll*o in kinstlas 0011001109 $to*)#
wh1oh allow the verification of %be tbeorre The papervao presented hy heademician_
V. A. Kargrin on 8 AprU 1963, Ortq. art hass no igraphio materima. -
ASSOCIATIONs Urallskiy gomWarstysnWy universitot In, A. W, Gor1kocio (Vral Stato'l...-
Unim-pi -.y)
itam 1/9 1

4-92224A
AFkOOOl19 800CZ COD91
SOURCIt Refe she FiSUMP Abe. SMS
AUM t Kabollyj L. Y&
OW: -none
TIT t Wfect of strow g!jWjg fjolds on the proc*goes of formation of swpu--
molecuUm structures in synthetic and biological po, S
C172 D SOUWls Obo. Fla. magnitno ywl*nW. Byerdlovski ;040 3-22
TOPIC TRGSs polymer ftsical chadstry,, vave Motion, polymer structurep offignstic
field
7PAMIATION: A theory in constructed for the formation of supermalecular a
such as %undlos." "multispire.U." eto.,, frost Simla structures. The
the structures to described in this ew " a phoss transition in 4, system Of PAM-
oleo responsible for their fonstlon,, &M the bowpolar fftesso vMch are the 00100
sequences of the overlap of -the veve functions of these particloss, %ibith are U
Identical states, ploy the principal role. One of the consequences of the theory Is
the presence in the supormlecular strwtwes of collective =wW excitations of
the structurra vw"sp %b1ch am pro~te through the supermalocular structuree. A
ualitativv investigation Is made of the possible influence of stroog msgvatlo fields
oe) cc the processes of formation of supormolocular structures.
Ma COM 2D, 07

. I - , I -I " I .I . Z-~D .
-- Aptrl&7rl.
. A -, -4
~~ 1 4 - I

Ito

iofl Im. W-14matm

loan, U.N.
Diagustia significance of bloM In cancer. Klia.med., Moskva
29 noslsO Jan 31. (MAL 203)
I* Of the Propodoutio Thw*Vmtlo Ollnlo (Dirootor -4rof.Lle
levelkay)o Saratov Medical Institute# Samtore

xq!M
Some probless occoaming tho mortality rat* in rhwunatie rev4r,
Vope rwmo 2 noU75-78 Ap-jet62 (MIR& 17 0)
L Is Pskovkoy -oblastnoy bollnitsy No,2 r relikikh hAa1&
(glaynyy vrwih L.T.Surtpar).

SOV/21-59-I.-21/26
AUTHORS: K6_ObSlOv, M.V. and Sakhatskiy, I.I.
TITLE: JOn ~e Fsathe~ring~rust of the Dabovskiye and Anatolian
Granites (of the North-East Azov Seashore) (0 kore
vyvetrivaniya Dubovskikh i knatoliyekikh granitov
(Severo-vostochnoye Priazovtye)).
PERIODICAL: Dopovidi Akademli nauk Ukrainslkoi RBR, 1959, Nr 1
pp 81-84 (USSR)
ABSTRACT: The chiefly detrital weathering crust of Tertiaryage
in the region (t to A&Mdye and Anatolian granites at
,the North-East Azov Seashore is described. The crust
deepened in upper tertiary time, was destroyed, and
the heavy minerals (ilmenite zircon and monazite)
were extruded and accumulatea at a distance from the
~granite mdea. The area, in addition to the South and
North-West Azov shores,can be prospected for ilmenite.
Recently$ geological prospecting has discovered deposits
Card 1/2

SOV/21-59-1-21/26
On the Weathering Crust of the
of ilm enite embedded in the tertiary sandstone and
hardened kadlint in an area North of the Dubovskoy masif
There are 1 map and 7 Soviet references.
ASSOCIATION: Eirovskaya geologicheakaya okeped.-itsiya (The Kirov
Geological Expedition)
PRESMITED: August 12, 1958t by V.G. Bondarchuk, Member of AS UkrSSR
.Card 212

)LTJ
Two t on tbs sovAhm vidge of the Donets Usine DOP*An UM U0491
2277-1280 160; (KIPA 13 110)
1, Pr9datavlow aladodkow AN UM T.G.%uWohukn.
(%Data ustn-Imt)

BUTURLINOV, N.V.j PANOV, B.S.1 XOIWLrv, M.V,; rlRMV G.F.
Now data on Devonian igneous activity In tho sou%westeru
margin of the Donets Basin* Dokl. AN wsR 156 no. iir-17-
820 Je 964. (MIRA 17:6)
1. NnetskJy politakhnichaskiy Institut, Predstavleno akadosikm
D.S.Korshinskim,

vuDaRADOvo V.A. C"bradovs V,A#jj lowas K-V,, EKOWleys X.V.j
Now data an underground waters in the oostern pm*t of the
Xonsko.ygyfigkq& trougb. Oeolerhur. 22 no.2s94-97 162.
(MIRA 13j4)
1, Kirovsksys skspeditaip.
(Donets Basin.-Water, Underground)

MWr, B,.F. (Mbakwah aW=f X*Ts, (Hoskn)i KOMVj N-T I $T=Wt tol-
p Av indogsa
(riam9nda)l UKABOYS X.v. ?Nookft); MM-T
Newft *T"t ftsUo Arl~ zo,1209-109 D 162.
(KMA 25t22)
1, UmsUk* Novo-TroiUkoye., VwsUkaya
944
abl, (for Ze evT. 02. 0'ret Vb4molyakogo obsbekostn
bel 1 2 TSwtmI'm7y a
(for
Piro", mmtuv
a we
sual

loam It V,
zmt pbn*,ma in the souOus cuUkil4m of 00 &MOU WA
and Pair ~p. 1w, 12 SBM Urseoc* so,1173-47 Ja-Y #63o
Nwourstwo g6olo i dauvay nodr AM

MODSWO so I Ovauff, P,
VoUraw labor conditions, 11"teugle 8 moj)120
JaRk 1314
'to Predes"140 Permtoge obleou proteopsa r&Wchlkb
woweblouno,sti (for Zebelew)e 26 SavehWashchly otdolou trudai
sarabotMay pUty FeMkW ONCOM WofsorDS& raboebM vpllwy
IProWMbUWW$t, L(for Tevelkov)e
mu")

I TV8=T I P,
Applyins proaresel" practless, Aut. ud. no.losIS 0 139
NM 1333)
1, Predeadatell Peru&-^%u oblastsogo koslteta profsoywm rabodW&
ugollnoy proWshlemostl Mobelay)o 2* Zavsdaubobiy otdolon
trada I uro'botuoy platy Mom (for Taysikov).
I(Coal abse and sizing-lator proftativity)

KDZLSV.-&s-#Pitan
Determin4ng the distame between ships, Roob, trwwo 22 no.5t
53 -W 163* f-XIU 16t8)
(sup h&Wlbw)

KOBELEV. Hol. KUMLIHMO V.S.; ROZEmnL I D,, S. To.
Present atate, of the mantiftature of electric motor rotors wA
To 164.
stators. Lit. proisve no,60943
(Him 181

KOBFLEVp P. Ps
XX lot OsoaviakhIm, C20 vaArs or the society for Prmotion or Defense of
Aerochemical Construe tiw- -(Z& oboronu, 1947, no* 1-2, P. 4-5).
DICt TLrQ4,Z3
Neotlozhnye zadachi Osoaviakbins, ghe U=ent ta'30(3 of the Society for Promotion
of Defense and Aerochemical Constructiqv. (Za dboronu, 1946, no. 21, p, 1o-130
DW: TL504.Z3

S/123/160/000/008/010/017
AOO4/AOOl
Translation froms Referativnyy zhurnal, Mashinostroyenlie, 1960, Not 8. pp.
108- i09, 38i00
AWHORt
C:
Tr=: The Machining of' Components With the Aid of Milling Cutters14
-Designed by the Turner V.Ya. Karasev
PERIODICALs Stalingr. prom-at' ~Sovnarkhoz StiLlIngr. ekon. adm. r-na), 1959,
No. 12, pp. 25-27
TE(Ts The author presents Investigation results of the and cutters,
designed by V.Ya, Karasey, tested at the Kirov Plant. Considerable advantages
'VT7 -07 8)&T ad
of these *utters showed durInS the machin *? eMl&j9T (lXhl ) gr 9
stainless steel, which raised the efficiency more than twice. Owing to an enlarged
812e of the chip grooves, the efficiency of machining n*n-ferrous metals Is con-
siderably -increased. Thus the feeds during the tooling of copper reach a mWl.
tude In the range of 500-900 mm/nin, while aluminum alloys ara. machined with
foods of 1,000 mm/min. Milling -of heit-trestod compmentA of high-sUrength alloyed
Card 1/2
S/123/60/WO/00SPIP/tI7
AOO4/AOO1
The Machining of Components With the Aid of Milling Cutters Dea1gn*d by the Turner
V.YA. Karasev
steel grades showed that the efficiency increases by 30-0% without lowering thS
durability of the cutter. The now cutters.are particularly recommended for the"
machining of grooves, surface finish comes up to the 6th class. Tables of the
recommended cutting conditions are presented, There is I figure.
Translatorts notes This Is the full translation of the original Russian abstract.
B. 1. M.
Card 2/2

TRETOYAKOV,, A.V.1 ORACHKVp A.V.;
A.V.
PAvIew of the book bUr leMoMmorovich and A.S.Fllatov *Yore@ FA&surs-
unt during rollingow Stall 24 no.7t638 Jl 064s (MIRA 1812)

TRETITAKOVO A.V.0 kand. tokhn, nauk; TERMIIEVp V.S., kand, tokhn. nauk;
KOBELEVO V,Aq lush.; POZINA, R.A#, lush.
Investigating strip tension of finishing machino collers.
Sbor. ot, XIITIAZHWPA Ura2msbsavoda no.6:260-274 165.
(MIRA 181 U)

26gi
0 1~ I
S/ e ~1/000/012/021/028
0
5'. IS 0 0 B103 202
ATITHORS: Tologinj V, Go, KaboloYt Vo A## Mushonkof Do V.
TITLE: Alkylation of butylones by moans of isobutano In the
presence of hydrogen fluoride
PERIODICAL: Referatlynny shurnal. Xhimiya, no. 12, 1961p 524, abstract
IM62 (Tr. Vass. no-i. in-t neftekhim. protsessovp 19600
VYP. 3# 193-194)
TEXT: A mixture consisting of 44A of isobutylone and 56~ of n-butylones
was alkylated by means of commercial 90% isobutano in the presence of a
catalyst (98-0 HF + 1.2% 80 2)' at a temperature of 300C, a pressure of
10 at overpressurep and a volume ratio KF : -hydrocarbons of I : 1. The
experiments showed that the alkylato yield Increases from 177 to 193(A
with an increase of the molar ratlo isobutane : butyleno from 4 : i to
10.8 , i. In this ease lighter alkylates are obtained with a low final
boiling point. This method warrants - as compared to the oulfurie-acid
alkylation of the same starting material ;L higher yield (by about 10%)
Card 1/2

26195
3/081 61/000/012/021/028
Alkylation of butylenos by means of B103YO202
of aviation alkylate with an octane number higher by 1.5-2 points.
(Abstracter's note: Compl^ts translation.)
Card 2/2

MOLUNSWO O.N.; DMIANp 9,9.1 BARKAX, B.A.1 KODSM~ T.~*; TMMINP Too$
CaWytio toomerization of *-pentans. Ixv.M.uohob.say.;
'rh4m i khia.takh.3 no.20"-363 160. (KM 24s6)
I# Toosoyusuyy rAughno-ionlodovatellakly institut neftekbalabookiM
protosisaw,

" .1 - - WtOtwVT" .
jittit J~-V - a. Ir ZA CH, A~
Wave Guide*
Wave omAuctarse Phdio Doe 2j 1"2o p, 19-n
Discusses med for maw guides. Ix ration nodes, and velocity and attenuatiod
of waves in we" guides. Rectangular wave guides 2.3 x I an are used for tramadttift
a frequency of 10,000 m (3-ca). Theory of vm guides vas developed by
L. I. )bndellshtam, B. -A. Vvedenmkiy# A. 0. Arenberg, S. M Pqtov, P. To. Krawmshkin#
H. N. Malow, A. V. Tatarimv, wA others.

"Magnetic Operative Hwory Devict with Di"o-oder Employing a Ocund-Ribbon Magnetic Core'
a paper presented at the Conference on Methods or Developuient or soviet Mathematical
Machine -Building and Instrument -Building p 12-17 March 1956.
Translation no. 50, 8 oct 56

KOBE= VIV
*Prowmmd Acoess Resnetio Memory" 190
bubl by Inst. Fagot Mechenlas *jA CooWuting ToobnIques, Aced. 8o1. U398
"PIP,
fw, RR i
RIONS Vn=

Kdbelev,o Y.V.,, AM Yu. Is viamn
M"Mit"We I&PORtnayushcheye ustraystwO a PI qpmvlaniym Usametic
Mm=7 Deylae With PrqP control) KoscZ.71W. 17 p. 5M eagles printed.
Sponsoring Agencyt AkM#ai" nauk SM. Institut tochncy moMani]d I
vyChIsliteltuar tekhalki
No contributors mentlawde
MOM: TUN tooklot' Is inten410 for taftlea ad s6iontifte porsomal dealbw
irith computers
CoMtA=: The woAors Alsews the onlication of:mpstia shift MiStOrs tO A
gpecialpurpose digital, casgater sawr at MjLU espaeAty and 9oqwmtl&1 addre s-
lue it W" detondued tUt sWA an a"llostion would result in a conside"ble
sixplificatian of circiults -and In a r*ducticu Of camponents 0 Read out P.-A vrito
in for such a sawry am be perfors" vith a tr*A4lstwlZ*d 1086"tIc shift
Card 19

Xapatle Xwm7 Doyle* With Propm Control
register* ftess, principles vore verified an an experlawatal device of 16 bits
50 amory locations, TOchalaians L.B. Yefinow,, T.Af* Chvyrev and R.N.
triTchenkove panicipated in the construction and adjustment of the sawntle
starap. ftere am to references.
2A= W C I Till 19:
Introduction
I.- Principles of Construction of a Magutto Starap With Program"
Control
2. 1xperimental Results
AVAILAZZ: Libr=T of Congress ("72JAX6)
JP/wrc
Card 2/2

66263
44(6) BOVIISI-1-7-19121
AUTRDRSt lobolov# V. V.9 Washkoilobt 1. 1.
TITLXI on the Arbitrary Ismagnotisation of the Xn-Ig and NL-Zn Forrites
PERIODICALs FisIk& tyerdogo tolas 191% pp~ 1140-1146" (USSR)
ADSTRACTs The ronagastization (hysteresis RPVt I Os) of several toroidal
Xn-Mg &Ad Si-Zn forrites of the types YT-19 1-20# VT-2p
3-415-Pt 0-1000P 0-2000 axe oisained by experiments. The
chemical composition and the magnetic properties of the fer-
rite* are displayed in table 1, The change of induction Is sessur-
ed by meani of a ballistic galmomster with an accuracy of~ 1%.
The switching La'and off of the current by moohanic contacts#"
*ausing breakdowns* was substituted by an electronic equipment
(circuit diagraa# Fig 1) produciing the necessary Ragnottaing -
currents for ridgeloss current control. The rid4eloss control of
the current Is attained bj connection of an Integrating cell
with time oonst"t of OeOl sea. Jefort measurement the ferrite*
*or* magnetically prepared# looo they were 3 - 6 tines re-
magnetized by Hmax -a 4 - 5 No. The results obtained are dIs-
Card 1/2 played by tables as well as 'by diagrams and admit the following

"263
On the Arbitrary Reasgastisation,of the Mn-Mg and $I-Zn Perritoo
conolusionst 1) Ths magnetic state# prevailing in the examined
ferrite* after the 4n& of the first current impulse Is not slW%-
ad by anew aoting impulses of current with equal polarity.
2) The periodic Influence of current impulses, with saternating'
polarity causes the formation of a partial cycle of the
hysteresis which Is shifted In the direction of the initial
state, The center of this cycle does not tend to soy* In the
direction of the origin of the coordinates in the B-1 plans.
3) The assumption of a remspetination of ferrite& in layers
offers the possibility of determining the
trajectories of the .,A08mribed ,~Vofttli in the interior of the
01"imun hysteresis loop. There are 6 figures, 3 tableso and
6 references# 2 of which are Soviet*
ASSOCIATION# Institut toohnoy mokhanIki I vyohialltollnoy tokhniki,, AN SSSR
Yknb'sl (InsItitute.0t PmIsIft Heahaulas and Computer Technology.
AS USSR Moscow)
SUBMITTED$ April 18j 1958
Card 2/2

Irr"OL-110 TOVO
DselUomphle device for "cording the bystersels loop of
flat farroWmatia f um] ustanoom due ostainocraftroymna
pstoll claterest" ploakft ferromagaltafth planok* Moskva*
In-t toohnoi mkbsnM I wychislitellnol takhalki Aksd,mnk 8=9
opaph)

zomm I.T
[06011logrobla device for "carding the Iwatereals loop of smell
ferrite aores.3 Ostaillogrofichaskmis ustonawks Me sulatils
YOU gisteresles mllft forrilowIM sordochnIkov, Kooky*# In-$
toohnol mkhoniki I vyoUslitellnol takMiki Abd,zwuk SMO 1904,
20 pq (XMA 14s2)
(cargo (Ilectrialty)) (11ognotic measurements)
(Osoill"h)

PHASE I BWK EXPLOITATION SOV/5550
Akadenlya Natk SSSR. Laboratorlya, magnitnykh elementov.
Magnitnyye elementy; abornik statey (Xagnetia Elements; Collection
of Articles) Moscow, 1960. 313 P. 700 copies printed.
Sponsoring Ageneyt Institut toohnoy mekhaniki I vychisutellnoy
tekhniki Akademii nauk SSSR.
No contributors mentioned.
PURPOSE: This collection of articles is Intended for specialists
concerned with digital computer technique.
COVERAGEt This collection of articles contains a part of,the
papers,lesued In 1956-1959 by the Laboratoriya, magnitnykhtle-
ment,7-v Institute tochnoy mekhaniki I vychislitellnoy takhniki
AN SSSR (1,aboratory of Magnetic Elements of the Institute of
Precision Mechanics and Computing Technique, AS USSR). They
cover the following topics% polarity reversal of ferrite acres;
static and pulse characteristics of ferrtto cores with a rea-
Card..11/-*

Magnetic Blements (Cont. SOV/5550
tangular hystereels loop and the equipment used for determining
them; the operation of push-pull shift registers using ferrite
diode elewent8j several types of storage devIcesi now magnetio
oomponents; tr&z&-.&axorsj and magnetic Input drives. No per-
sonalitles are nentioned, Roforenoes accompany each article.
TAXZ (W OONTEM i
Foreword
Is Kobelev V.6,,V and 1. 1. Hadashkovieh. Concerning the Prob-
re-zi-Of Ili; *S;lf-Reversal" of Magnetic Polarity at Xn-Xg and
Ni-Zn Ferriten (1958)
2. Bardizh, V. V. Problems of Pulse Magnetic Polarity Reversal
of Ferrite cores (1958)
3. Bard1zh, V. V., and V. V. Kobelov. Calculation of Magnetic
Polarity Reversal Cidi -08 of YeFrits Cores (1958)
Car4-2/A
3
6
16
33

Xagnetic Elements (Cant.)
A. Bardl Sho V. V. Characteristics of Cores With Rectangular
Hystareft LOOP-4957)., 57
S. Vi XUO YU , 1. Squirmont for the Investigation of Magnetic.
Core Properties (1957)
75
6 obel
x
V- 05011209vaPMO IUStallation for-Taking the
k
s
Hys
op of ftall Ferrite Corso (1959) 96
70 NobelayLi.-SA. Operational Stability of Magnetic PqM-pull
WMr f-lUe-gle tore (1956) 115
80 BorezhnOY: -Y& -F-- OP*r&tidg Register On a PAPOtOStriation
(1-57i
D
l
rA
o 9
0
1
n
"
e 3
9. Kobeley VO V00 and JU I V Magnetic Storage Dovj~ce
with -Pf!tC, getbftM Oont;;1 bAr
16
3
Cand-*+-

gill
ISO 6
t A
P;1
.1 1 Jill
.........

-11- -W
I.A.1 PrInWIS uabas"s ~~I!!.LIAZAROVv A.D.1 MY.
CMWVAo R.N.
fi2mi.#p-
Iftudy of the rompsUmt1as tits of farrompatia
rransil-C.
slawatel Iseladov0de va ni perampichimaa fe
AL
vWM pUnooboyM elmestov. MaiWas lib-t toobnal adunw
v"hitUtollsoi t*Uwd)d Akad. mk SM9 1961, 23 Ps
(MU 24,16)

,PBK~~Vvf KMMM= 0 -A.A. I - Pilvimu sobastiye 0 R.N.

11721161/0001000/004006--
AUTHOR: Kobeley, V. V.
TITLE-. The hysteresis loops of monoaxial ferromagnetic films.
SOURCE: Akadem'iya nauk SSSR. Institut tochnoy mekhaniki i vychislitcl'n
tekhniki. Magnitinyye alementy ustroyotva vychislitellnoy tekhnim.
sbornik statey. Moscow, 1961, 56-84.
TEXT: The paper reports the results ofan experimental investigation of
thicknesswise single-domain layers termed "films" in the sense of C. Kittells, (ind-
ing (Phys. Rev.. v. 70, 1946, 965) that with ferromagnetic layers of a thickness.,*,
smaller than a ce'rtain "critical" value an optimal state exists in which the mqnet-
ization vectors are parallel to the surface ol the layer. It is not implied that ~he
magnetization vector must be parallel over the entire area of the film. that ij, that
the film must be single -domained over its entire area. For example, a filra is in a
multi-domain state after demagnetization by AC. Two processes occur during
change of magnetic state (magnetic polarity reversal - MPR): A reversa) process
and a process of the formation and growth o.,domains. The speeds of these Z pro-
cesses are different: Polarity reversals occur over a time of nanoseconds, whereas
the displacement of boundaries requires a time 2-4 orders higher. Inasmuch as the
most effective film would be one in which tho processes of domain formation would
Card 1/3

The hysteresis loops of monoaxial .... S/721/61/000/000/003/006
be inhibited as much as possible and MPR would occur only by means of % reversal
of the magnetization, the paper examines the problem of the behavior cf an ideal one-
domain film in external fields. It is concluded that all the variously- shaped hystere-
tis loops of monoaxial film elements can be described in terms of the rota.ion (re-
Ve r9al) model. Equations are adduced for the various different classes of hysteresis
-ODS. The "ilm elements tested were obtained by precipitation on an arnor phous base
xhich exhibited monoaxial anisotropy. The best concurrence between experiment and
-~-ieory is found in specimens having similar values of the coercive force for boundary
displacement and for rotation. The experimental investigation of processes of bound-
ary displaccrnent can be shown most clearly and most conveniently by means of the
-n
.. agnet~zation hodograph. In all instance@ of MPR of monoaxial film elements, do-
main formation was observed. The incidence of boundary- di r. placement processes is
m,nimal in an external field close to the "heavy" direction of magnetization, that is,
d~rect~ori of maximurn energy in the element. In the MPR of a film element exactly
along the ''light" (that is. the direction of minimum energy in the element) and exactly
aiong the "heavy" direction of magnetization, no processes of rotation of the magnet-
,,c moment of the specimens were observed. The coercive force can be readilA meas-
u red by the rotation method. namely. by directing upon a monoaxial filrn eleme it a
,onstant and a variable field directed at an aagle of 450 to the "light" axis and y alter-
irig the constant field until the characteristic "rectification" of one of the bran1hes of
Card Z/3

/721/61/000/000/00 1006
AUTHORS: Kobtlev, V.V,, Korsunskiy, A. A.
ain structut
TITLE. The dom a of inonoa3dal ferromagnet c films.
SOURCE: Akaden~iya nauk SWIL. Listitut cochnoy mekhaniki i vychislitelln4
takhniki. Magnitnyye elementy untroystv vychislitellnoy tekhniki;~
sbornik statay. Moscow, 1961, 85-96,
TEXT: -The paper reports this reault of an experLnental investigation. in w1kich
the observation of the tnagneUc_4tru4;ture of ferromagnatic films was perform -ad by
the use of the magneto-optical Kerr effect. that is. the rotation of the polari ' on
plane of light that- is polarized in the plant of impingement or perpendicular rat*
during its impingement in the direction of the magnetic moment (the meridio II
Kerr effect). The direction of the rotation is determined by the di rection of tic
magnetic moment, whereas the magnitude of the angle of rotation is substantially
dependent on the magnetic moment Wielf. Thus it is possible to use a polarizing
element to extinguish almost completely light reflected from one region of a ferro-
magnetic film (for a given direction of the magnetic moment); because of the small-
ness of the effect there remains a fairly small but noticeable portion of the light re-
flected from another region (with a d-fierent magnetic moment). Thus the refkction
Card I/Z

7777; -7
The domain a truz-
potentially into res; y -contrast *ith
a to ervatilor, of' r
-the domain s ruc. a of & large
t dCAU 4 to p-rovide any means for enlarging the Imago. The
-optical "Ixi ant used I Milar to thit described by J?owler. C. A.. and E.M.
Fryer, Phys. Rev., v. 94, 1954, SZ, Th.% light source used was a krypton-xpon
high-prosioute 'light rCAA IZO (GSVD I W). The method of the making of 4 ,he ferra-
magnetic film element by vacuum spra)ing the forromagnfitic materW onto a heated
clean glaso "to placed in a magnetic A#14 parallel to the plane of the basr, is de-
scribed. "'he spraying vacuum was 3-1W-I'mm Hg. the base T 300oC, the tuagnatic
Jleld 50 4. The alloys sprayedw'ere Permalloys with CNQ from 80 to 83%Q_' The
domain structure of a mon"xial film sIxicimen during magnetic polarity reversal
(NIPR) along the low-energy (",light") axLi and along the high-energy ("heavy") a3de
are describod and illustrated by photographs. This is supplemented by a description
and photogra.pha of th6 bright- and dark-iLrea patterns revealing the domain structure-
during MPR by a field directed at an angla to the "light" axis and by a fierld-Ahai- -it
close to, but not coincidint with, the "heavy" axis. There Are 12 figures avA
references (Z German and 6 Englirsh-languagi).
Card Z/Z

7:1
VTHOR. Katie V~ V.
JJTLE: tqu*nant 6ri- the oscillographic recording of hymerevis loops of plilia r, J-1
ferromagnetic films. Ilk
S
-4~URCE: AkAdemiya- nauk SsS*'-.. -.1as titut- toe hnoy m vkhalika i vychislite 0YU-7---1--
tokhniki. mag-nitnyy*-elementy-ustroystv vychislitellnoy tekhMki;-
sbotnik statey. Moscow, 1961, 131-146.
TZ:XT: The paper comprises a review o.1 theproblerni encountered in t..e re_f ord-
ij~ of the hysteresis loop (HL) -of film-type lierromagnotic'elements, specifies t~e re-
"irements to be imposed on an oscillographic equipment designed for that purp*'Se,
-MW describes a specialired equipment, its- o:~eration, and its performance. Theklm-
h der. the solenoid (130-mm long. 45 coils, 40-mm diam), the setup employed,11or
t~lrl_ - e
recording oi the HL of one of th Alm elexuants of a collective matrix, the,
niethod employed in identifying the -proce-soc i of rotation (reversal) and displacerbent,
t8c general Orcuitry of the equipment, tho d,isign and problems encountered with,-In-
t4 grating amplifiers. the circuitry and methcd employed in the imposition of consitant
rOagnetic fields, and the measurement of the coercive force and the residual induction
the film elements are described. The messurement of the residual induction 14
qard I/Z

1- 7
Equipment for the oscillographic recording S/721161/000/000/006/006
preferably parformed by-ths-mothod.of the aoro standardi in which the core stand.ard
is placed at tho input of the integrating amplifier in lieu of the solenoid and the film -
holder assemply. whereupon the sensitivity of the integrating amplifier in maxwells
per mm y-wise displacement of the beam ai the oscill*graph screen is determined.
Thereupon a measurement of the rnagnitude of the HL of the film element, upon re.
placement of the solenoid and the film-holdor block, is determined, whence -knowing
the number of coils - the residual magnetic flux of the film is readily determined. To
avoid the many complications involved in the measurement of the coercive force,
1his measurement Is performed by means of the establishment of a constant field
directed along the-axis- of -the-solea*id.-Thiv inUntily of the field Is measured with
great accuracy by a ballistic galvanometer; the field displaces the hysteresis loop'.
Ind the magnitude of the displacement permits one to calibrate the amplIfter aloag
fhe horizontal axis of the oscillographin 0 /mm. The applicatic'n of the necessary
j1phasell correction of the amplifier for the x axis is described. General character-
Istics of the equipment: Operating frequency 1 kcps; max. amplitude 61 the variable
field 70 6; max. sensitivity with 1-cm-diam specimen in thickness 50 A, In flux
0.005 maxwell: number of windings of the coil 100; magnitude of the magnetic flux
permitting the photographing of the loop Mai maxwell. There are 14 figure's and 6
references (I Rua slan- language Soviet, 5 English- language).
Lrd Z/Z

03
S/04e/6i/o2c/oo5/o17/O24
B117/11201
THORS: Kobelev, V~ V*$ and Korsunskly, A. A.
TITLE-. DQm%in struf3ture of unlarial ferrot&gnetic films
PERIODICAL: Akademiy% nauk SSSR. lavestlys. Serlys, fizich#skaya,
vo 25,,no, 5, Wt, 626-635
TEXT: The present 1tvastigation was the subject of a lecture 4ollver*d at
a symposium on thin forromagnatio films (Kraencyotrolt. Julv 4 to 1, 1960).
The magnotla atruiture of forromagnotto flIms was iat~iiiod vith the aid of
the magnetcoptionl Xtrr effect, The lptics of thq dPvioq used in the
investigation van almilar to that desArlbed in Ref Z (Fooler C A-,
Pryor E. M., Phys- Rev 52 (1954)) (Flg- 11 Thq light source vat a
krypton-xenon IAMP Of the typo rcu_uo (OSVD-120)-- Th4 polaritoro were
gyropntite polarizing folly. The hom,)g9neous aAgnotic field was brought
about by meRns of %vo pairs of r4etanjular coils (r44&rtqd in perr#n4ioular
to each other. The field H? lying in the plane -,)f bea% tnaidence was
produced by ono pair. and tht porpondIcular field Hr ty the other. The
spoolmens wore rroduood by sputtering ferromagnetic material. In vacuum
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2580)
S/048/61/025/015/017/024
Domain structure of unlazisl,... B11,0201
(3.10-5 mm Hg) onto*& polished glass backing with a temperature of 3000C1
the magnetic field was 50 oersteds. Perstalloy-type alloys withai niakel
content between 80 and 85 % *or^ usod line speolmere I cm in diameter
each were sputtered simultaneously. "Ahe ba-Aingq ver4 18-18 so large and
0.2 = thick cover glasses. The specimens produced in this may displayed
a distinct unlaxial anifiotropy. A domain structure of a fairly uniform
type generally sptpArs in sulh specimcna durirg mapr~otir r*y*rA&I. The
magnetic reversal of specimen no. 11S (85 % Ni, 17 016 F#) 1400-X thick was
examined as an eximple.. Due to an *x1guous amount of Incident light, the
domain structure in practically not detectable under Yisual observation.
A highly sonsitivo film (180-250 rGV (GOST) units) -wag therefore used for
taking the pictures with an exposure time of 1-3 minutes. In the positive
field of 0.1 o# the first domains first *ppear in the form of bright wedges
at the lover and upper edge of the file element. With growing field they
first become slowly larger, then quickly diffuse into one Another, and the
now phaso covers almost the whole surf%c#. Once th@ specimen Is almost
fully saturated, nuclei of the former phase are still left over at the
edges. Nuclei of the new phase appear in all cases. without exception, at
the film edge. where the demagnetizing field has Its maximum value. The
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Domain structure of unlaxial..* BIWB201
hys'ujr*ois loop relative to a number of pictures Is presented In.Fig. 3.
The second par%, whiohoharaoterts*s the magnetic reversal of the specimen
on the passage from the negatlyt to the positive fields, was construatod
considering symmetry# and drawn with the aid of a thin lint. During
magnetic reversal with a field oriented along the axis of easiest
magnotizing,and when at the same time applying a field along the axis of
heavy nagnotislig, domains Appear, those structure differs little 'from the
previous one. Still, there are tons particular aspects here: the
stronger the field 9, oriented in the direction of heavy magnetising, the
smaller will be the parts -of the field H in which the domains aria# and
*xpand. The field Hs *hiah aorresponds to the end of magnetic reversal
drops more slowly. The first todges are Inclined toward the direction of
the outer field. This Inclination Is reduced with a growth of the domains,
and near the specimen center the boundaries run about parallel to the axis,
of *&stoat magnetizing. The larger RX, the narrover and longer the first
*edge@ will be. Their number riots and at -the same tire it can be
observed that the boundaries deviate from the axis of eftsiopt magnetizing
not in the direction of the field but in the reverse direction. A fine
domain structure then appears, %be walls of which are inclinei In
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t.-TW-- 1.
25803 5/048/61/025/005/017/024
Domain structure of uniarial.... 3117/B20!
different directions. The case of a magnetically uniaxial 'film -which Iv
divided in domain# and which to placed In an arbitrary outer field to
examined more closely. A scheme illustrating the Inalinaticn of the
boundaries in a magnetically uniaxial film is presented by Fig. 8~ It Is
easily found that the domain structure can exist only In tho presence of
such fields as correspond to the points within the astrcil. Thor* are
two stable states in magnetization. The boundary is assumed to shift In
the fields h. and hy* This corresponds to point P within the astrold.
and ?. Is characterized by the acute
The direction of magnetization# T, 2
angles aI and a24 The angle.&a between the boundary and the rAxIs of
e
&#lost magnetizing to found to be equal to y -900. AM. (a I -a2)/2.
Sven without having analytically precise formulas for a 1and a2 It to still
clear that &a can assume no high values. The extreme values of,&a can be
easily found within the rang*
h2/3 . h2/3,41, b ;kOi h ~1~0 (11)
2 X X 2
by the method of undefined Lagrange factors. A system of equations Is
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25803
8/OOJ6-1/025/005/q1 7/024
- #--
Domain struRjurs of r17/1201
found by-thit nothadj**h1oh baessingle trivial solutiono:
a wa2shxwhs~O- obrrssporAs to U's salient point. There is
As 'a consequence, thl'
maximum nor minimum wit~ln the re "on (11'
maximum of An to at the boundarv of this reglor. 441s maximum can be
3 h~j Gz3W
susily found -If h and h are expressed by a2 b Vocog a 2~
x 8 8 21
The f inal f Ormulli roadst
f
(14).
at 2the left- and
The argument h side Is 2boo. Its maximum oan'be to
- 4
differentiating formula.04) with respect to '42 As a result
and &%az 150. 0 5) The. observed Inclination of the domain wall.' Ift
tfit Idea that Jn first approximation the magnetic r6tatione within the
domains are ind*pondefitof thO,exisUnce.and of the shift of the
boundaries' between the domains, the" are S figu"i and 8 aon-diwlet-Voc,
refer*nossi The four references to Inglish-language publications r~jkd1r&a 'L"-~.
follows: --Williams loot-Obervood Rot J; Appl, J1hYs;9 LOo 548 (19,57)1.
Prution U.0 Philos. Vagsg Ditto J. Appl. Pbys. 111o# -
1063 (19 9) and
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25803.1, -
8/048 61/025/005/017/024.
Domain.structuro of untaxial". 3117 3201
335 (1960)) Proobeter 1. 1,# Vathressel S.f linberg 0. 0. MOCO (NS
ICIP K 2.
ASSOCIATIONs Institut toohnoy'sekbaniki, I vyabislAtellsoy tokhnikl
Akademii vauk SSSR.,(Inotituto of P;eoi*Aon Vochanics -and
Computing ToobnIque of the Academy of Sciences VSn).
Legend t0 71 8, It OP ties. of
a device for observing the
domain struciure of :ftrro-
magnetic films. I# ligbt
sourcol 2, condenser Unsl
3, diaphrapi, 4, -collimator
I*nsl 5,-intsiference light
filterl 6# p6larizerl 7f,
specimonl,S# analyserl
99 objectivol 10# projection
#croon*
Card

AOI~W. v V.1 KORSUNSKII, A*A*
Domain structwe of uWayJal ferrouWsUo fl2m* Xxv&U L%LS*ro
fLs, 25 no,5t628-633 Ry 161, (=i 246)
I's botitut toobnoy asibs"41" 1 V70hialltellAO7 teklm4m AkedsoU
auk SURO
Obtall'a film--4bpotio properti") (ML900toopu")

5
3/126/62/OJL3/003/021/023
1039/2135
AUTHORi Kobolev, V.V.
!0 TITLAs A now method for measuring anisotropy in
forromagnotic f ilms
PERIODICALI Fizika motallov I notallov*doniyos vel3s n0-3. 19621
467-470
T2XTJ "an the azisotropia constant X In loss than.
103 *rSmlcm3 its measurement becopes difficult by the usual
methods based on forromagnatic resonance, in the case of thin
film of ferromagnetic materials pondonsed under vacuum In-&
magnetic field the anisotropy is small and is usually determined
'~i) by measuring hysteresis loops in a direction at riShtangles to
the magnetic axis, In the ideal uniaxial film the two branch*&
of the hysteresis loop morSo into one line* then Hk WI'
whore I Is the saturated maSnotisatione
For weakly anisotropic films this method gives very inaccurate
';25 results* In this.paper Is described a method which enables
anisotropio constants of 10 orSs1cm3 to be weasuredg and at
x a 10 *rSl*a3 it is possible to obtain an accuracy of about
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s/jLao/62/ooo/oo9/o26/o36
2192/2382
AUTHORSt Kobolov$ V#V* and Korsunskiyq AeA#
TITM 4 simple null indicator for the magnetic field of
a forromagnotic~film
.'-PERIODICALs Pribory i. tekhnika *ksporime~ta, no. 5, 1962,
TEM A forromagnotic film having-& singl*.-&xis anisotropy
remains in an unstable state when it is magnetized along the
"difficult" axis* When a weak external field jparallol to the
Iloasy" axis is appliodg the forrogmagnatic film assumes one of
two possible stable states* The instrument descriied is b&
on this principle. This-is illustrat9d in FiSe 2. A 2 500T
thick film is.mads of 82% Mi. and 18% F* 2nd deposited onto a
slassbase 2 (a glass plate-18 x -18 mm )* The magnitude of
the residual magnetic flux of the file is 0.2 maxw*11. An..
alternating ma notic field of a frequency which can be varied
from 1..- 10 kc~s is applied along the axis of difficult
magnetization by means of a flat coil W, # consisting of 25 turns
of 1 mm wir** The signal coil W (so* Fig. 2) consists of
2
t ard 1142

XOBEIZVO V.Y.-
(4steresix loops of ula3dal ferrompstio fIlwjPetli
gistoresism, adnoomqkh ferromapitrOb plemoko Moskva# ITK
i VT AN SM 0 1961. 63 p* (MnA 15s9)
(hrrat4s) Mrsteresif loop
(nootronto calculating wchimes~

I
NOBELEVO YOVS
C-
Equipant for the obserntion of hysteresis loops in mgnotic elt=nU
with an extremely low residual flwce Trudy Insto Nomptand,mer i
im prib no,60289-299 062, ()ORA 16s5)
(magtotio materlmls)(M4petlo mamurennte-Equijmnt and suplaioe)

~qrfd - - 24
I I .-, ~ .- - . -- -- - -- , -~- * , - , , - -
=-- .. =:A

Corn aa a crop pmeading wintAr orcra. 7enladella Z7
f65, I-AWO
V*rebk.)vsbiyn opytusya stattmiya VseaVanxgo
davatallakogO indtitUta bAtIrT42ys

MM/F-mi
.'.ba Jourt IWO rauir-Diol.) rtV 201 1958t 92543.
~Iitlu WAC211al In8tIIIICt Ir. `.'Or84L'8 -
Orir, rub: Kotievodst--ro) 1957, Vo U, 21-23.
Astract: 1wruatiGmUcaw voru corducted at the stud frrz
in 2-ioscovp Torsk mul &-bardinsks Wh= livlrc; in
hoita, 77ep of tt-.o sm-ma a fcv hotwo or days be-&'Cro
LpIving birth approach uthor pruvmt i=s, a;vl in
W~ of tho casoc they Clvo birth at Uw a= t".
The foalnC (in 70~ of casou) takes place at i-doat.
;Xtor foaline the m a display an active -4cfersive
reaction, espaciolly whan the colt is azleep, ard
Carl t 1/2
32

tjssrt/p,-.m "Idmis. 'norsou.
,'.ba Jour: 14f Zhur-riol,,, Ifu 20p 19580 92543.
also a Weitivo ramati(m t*w,-aa tho colt In the
forn of llckUg it vith tLolr lipe wA naIGMaZ
floftly. -Me roxo tcuchas the lipa of tile foal with
1wr ovn Ups and tl-.Ia activatca the suckina reflux
in the colt.
2)2

Relation between the grmth of an entire function of two
comolax variablas and the distribution of slAgulariUss
Of the funotion assaoiated with its lsv. vysuabob.
$"of mt* z**3s59-" 162# (=A 1529)
I# Ural IsklY gosuWst"w*T univervitet, Imni A.M. 0 ortkoco.
(ftmtlons of vomplax Variables)

I r VMIK, A*D& XMWWA s Me
'Inhibit in dreenterr boolill dvxlng the GOOLMA
sollylty of satigotlese lbarjalkrobloleapido I Imu* 29 so*71"
A 1$8 (am lite)
Is In Duepropstrovskop lastituta spidniologil I m1krotiolocile'
(gRIULU y1 vain vin Uj# effect of drags on,
satitiotles# resitso In ooebin*d offs of varlow d2up
on Sbipll& dymonterime, resist, In oomblued sidsln* (too))

Nodo of action of certain trace olovents on the development of resistance
to streptoWelu, Antiblotild 4 n0,519"" 159, WU 12S3)
lustitut spidesiolocill s1krobiologli I gigiretwo
sumlam Is *aruaol.)
ima WJKWS

17(2,12)
AV=RSj Chornomardik# A.B.o Koboloya, P.S., Ponamareva, V,O., and Kovalonko, A.1.
Tr=s The Combined Action of Antibiotics. Author's Summ=7.
30
PMWICALt Zhurnal o1krobiologil, opidoulologil I Immanobiologil, 1%9,ARr 6,
pp 118-Ug.(USM)
AUTHOfts Tests wore m to study the oambinodaetion of antibiotics and also of
-antibioties in various salts,an microbes,, particularly on,the development
of their resistance to antiblatlas. In the first test It was found that
magnesium sulfide and magnesium chloride accelerated the appearance of
Plorobal variants resistant to streptonvoln. by as such " 2-3 time,
whereas small amounts of cobalt sulflAo or cobalt chloride had the reverse
affect. It,was further found that this action is Inherent In the mWoolum
and cobalt Ions ad not In the 304 or C1 groups. Moreover, these substances
had no effect on the rate of appearance of strains resistant to synthemyolft.
The s*oonA series of tests investigated the effects of combinations of any
two antibiotics m Psoudomonas aeruginosa, pathogenic Bacherichia coll
strains, ShIgolla f1waserl -and Proteus. 7he anUblotloo used wares
streptonWoln, polysixin, ooliMain, torruWain, synthowyoln, eamoline and
Card 1/2 penicillin. The tests showed that a trace of polymixiss In a subbaoterlo-

The Combined Action of Antibiotics. Author's Summary. 3W/26-"-&23/46
static concentration of 10 decreased the antimicrobic action ;or aoiuwain
by about twice. The reverse sequence of this did not take place. ftntho-
mycin, had the sun antqanistla effect an streptomyoln. Nelthsr at"Pto-
mWoln nor colowain had -an antagonistic affect on synthopyaln activity.
mono or the other combinations of antibiotics had either an antagonistic
or a synorgio effect cc Peoudomon" aoruginosa - simply a summiation one.
No combinations of blomyoln, terramyoln, colimyoln, polynixin, strepto-
nyoin,, sanazin, synthomyoin or furaoillin had either an antagonistic or
a nynergic effect on the Esohorlahla coll or ShIgolls, flwmert strains.
ASSOCIATION: Unspropetrovskly Institut, opidemiologil I m1kroblologil (Dnepropetrovsk
Institute of Epidemiology and Microbiology)
SUBMITM: February 8, 1958
Card 2/2

CHtRX00H0lKo__A*BG UWA14909- -A.D. PONCHMA9 VjO..j KOBUMA9 P.S.
Antibiotle-mistant aoU ba*toria in the proventlon of Utestiml
dysbaoterioois. Zhure nikroblo2. spU. i lo=. 31 no.7s73-76
11 1600 (KIPA 1389)
1, In DasjV4)P*tftln*og* Imtituts opidadalwdl I mikrobt
(ISOMICHIA COLI) - S_f_mi_:ia_cmw I
(ANTIBIOTICS)

CEMOMMIKo A*BeJ KOVALMMO# A*Dj PMCMUWAy V.0.1 -KOSELZVA# P.Ye.
Compamti" study of the offeat of oerULa antbdcrobW pnpLmtionm
an pathopnic bacteria. AntiblotIM 5 no609&M JIJM~160.
4 130)
1. Daepropetrovskly Institut, epidevilologLi I mikrobiologilo
(ANTIBIOTICS) (MM)
(BACTZRIA9 3"M OF MW ON)
le,
Y
D.
RON

WV/ 93-58-20-7/19
11(0)
AMM Soloyev, T.M. "love, V.A. &M Obelobayeva, N.A.
S M3s Flats MA as of Output of the Oil Deposits
(Tvmpy I V62Aota Vmbotki salsiber nerti)
.I (' -
M=t fieftyana2v kbosysystws lg'A;rXr 10, PP 31-35 (UM)
ABMTACTt 2he Tuymasy Oilfteld vas discovered in 1944 wA the initial estimate
of petroleum reserves In the Ur &M Dforwtions was me& in 1949. A
second estimate was mads by W VNIZ E6itute in 1954 and a tblrd by the
Uveazaaeft, M in 19W. fte capacitr of t1w D, &nd Dn formations an given
in Figs. 1-2 wA the production rates In relation to the initial &M cumat
estimates of reserves an given In Tablas 1-3. The data abow that the actual
production coefficient for Us two formations Is 0.43 Instead of 0.58 as
determined by the Initial estimate -of the reserves. 2be low production In
relation to the reserves presents a serious problem for the fartber develop-
meat of the large Devonian oilfieldso but the scientific and research orgaals-
ations do not botber to analne the industrial data an the Dr and D3M form-
ations. Ibex* an 2 figures and 3 tables.
Card 1/1