SCIENTIFIC ABSTRACT BELENKOV, V.P. - BELENOVSKIY, P.N.

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000204310007-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Sequence Number: 7
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

BFIMOV, V P
The BZ-49 automatic machine for grinding reamers.
Biul.tekh.-okon.
inform. no.6:21-22 160. (MIRA 13:1)
(Grinding machines)

YEVSTAFIYEVp A.G.,, kand.tekhn.nauk,- LEVIKOV, P.M.; KOTENKO,
L.A.;
BELENOV, Ye.A.
Characteristic process parameters of continuous washing of the
fraction
boiling in the 140-1450 range* Koks i khim. no. 5.39-41 161.
(MIRA 14:4)
lo Moskovskiy institut khimicheakogo mashinostroyeniya (for
Tevst&flyev,,
Belenov), 2. MKGZ (for Levikov)- 3. TSentrallnyy
nauchno-issledovatell-
skiy ihstittit kompleksnoy avtomatizataii (for Kotenko).
(Coke industry-By-products) (Benzene)

.BELENOV, Ye.A.; BOYARCHUK, P.C.; ZYKOV, D.D.
Method of calculating mass transfer coefficients.
Kh1m. prom.
40 no.10:754-756 0 164. (MIRA 18:3)

--BELENO YO.A.; A3TAKHOV, V.I.
Certain features of the mass transfer equations. Khim.
prom.
40 no.10:762-763 0 164. (MITRA 180)

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28.(W. Mar. 3 1. i9a, ZrOGilstreated with& The t
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PMl9Pct Is thcu treated In the UOUSI manner 10 PPt- Fe and the filtrate is
treated with 0
a Zu dust or metallic U.
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so 0 a 0 0 e 4 * 0 * 0 0

SUKHAREV, N.; BULYCHEVA, 0.; BWNKOV E.
Rapid method for determining the moisture content
of meate
Was. ind. SSSR 12 no.1:1.1-13 161. (MIR& 14:7)
--~14eat'IN-ying)

vttrt Ft!!~ to sla A*Cftntytk tea in amk a

BELENKOVA, L. Yu.:
BELENKOVA, L. Yu.:
"Investigation of the conditions for formation of the
cut-off layer in selenix= elements." Yin qigher Educatien
USSR. Leningrad Polytechnic Inst imeni M.I. 'Kalinin.
Leningrad, 1956
(Dissertation for the Degree of Candidate in Technical
Sciences)
So: Knizhnaya Letopisl., No. 18, 1956

BRIMOTA, M.A.
Influence of lipoeain on the course of acute and
chronic dysentery
in children. Yop.okh.ust.i det. 2 no.3:27-30 MY-Je 157.
(MIRA 10M
1. Iz Sverdlovskoy 4-y detskoy infektsionnoy bol4nitay
(glavu"
vrach M.N.Romanenko. nauchnjv~ rukovoditell - doktar
maditainakikh
nauk V.S '.Dabrova)
(DYSJWT]IRY) (PANOR19AS)

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it

M. lK BClCUk-Mi.'_FWka UeUU01; i McCuUmedftie. v. 2, no.

Detamfol the
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SOV/126.6,4-9/,14
AUTHOR: Arkh-grov, V I 1303ankoyn- M-M.,
Rikheyevq M:N:, U0_iseyeV~_A,,I0 'and Polikarpovat I.P.
TITIE: The Effect of Small Additions of Antimony and
Beryllium
on Ageing of the Copper-Silver Alloys (Part 1V. On the
Problem of Causes of the Effects of Small Alloying
Additions on the Kinaties of Ageing of Alloys)
(0 vliyanii malykh primesey surlmy i beril3i.,-- na
stareniya splavov mod' - serebro (k voprosu o
prichinakh vl2'.yaniya malykh primesey na kinetiku.
stareniya splavov. 1V))
FERICDICAL:Fizika matallov i metallovedenije, 1958, Vol 6,
Nr 4, pp 633-642 (USSR)
ABSTRACT: In his previous work (Ref-1-3) the result.of which
indicated that small additions of horophilic elements
(elements showing preference for the grain boundaries)
present in a supersaturated solid solution could affect
the kinetics of its decompositon by the mechanism of
adsorption enrichment of the-structurally distorted
zones linking the nuclei of decomposition with the solid
Card 1/11 solution matrix, Arkharov studied the effects of
single

SOV/126-6-?4-,.9/34
The Effect of Small Additions of Antimony and Beryllium on
Ageing
of the Oopper-Silver Alloys (Part lV. On the Problem of
Causes of
the Effects of Small Alloying Additions on the Kinetics of
Ageing
of Alloys)
additions. The object of the present investigation
was to study the simultaneous effect of two horophili,.*
additior-s. The experimental alloys whose detailed
chemical analysis is given in a tabile on p 633,
contained 6% Ag with 0.2 - 0.5% Sb and. 0.02 - 0.3% Be
added either separately or jointly. The alloys*were
melted in a H.F. induction furnace,'in a graphite
crucible with borax used as the co-wering flux. The.
cast ingots were heated under charcoal to 8000C, held
at the temperature for 2 hrs and cooled in the furnace.
They were then rolled to strip 5 mm thick which, after
a homogenising tx-eatment consisting of 50 hours at
8000C was used for the preparation of the experimental
test pieces. The pxo-less of ageing was studied by
measliming the -variation of hardness, magnetic
susceptibility and electrical resistance. The
Card 2/11 measurements cf Rcokwell ha:rdness were taken at

1.-0 ..
-1 V.2 4
SOV/126-6- -j
The Effect of Small Additions of Antimony and Beryllium on Ageing
of the Copper-Silver Alloys (Part IN. On the Problem of
Causes of the Effects of Small Alloying Additions on the
Kinetics of Ageing of Alloys)
15-30 minute intervals on specimens solution treated
at 780 - 7900C and aged at 37000. Mavaetic
susceptibility was measured with the aid of a magnetic
balance at room temperature and at 370, 400 and 4200C.
The measurements were taken at 10-15 minute interv la
and in every case the value of relative magnetic
susceptibility was determined, i.e. the force actin
on the in:vestigated specimen was comparecl with the force
acting on a standard nickel sulphate specimen placed in
an identical magnetic field. Electrical resistance was
measured by the comparison of potential drop method,
using a poteatiometer and a sensitive galvanometer.
.In this case, both the solution treatment and ageing
(at 3700C) were carried out in vacuum and the
measurements wezv taken at 15 minute intery ls. From
the experimental data the average rate of ageing
Card 3/11 (vcM = the ratio of the maximim increment of the studied

SOV/126-.614T9/34
The Effect of Small Additions of Antimony and Beryllium on
Ageing
of the Copper-Silyer Alloys (Part 1V. On the Problem of
Causes of the Effects of Small Alloying AdditionE on
the Kinetics of Ageing of Alloys)
property to the length of time required to affect this
variation) was calculated for various investigated
alloys and the results were reproduced graphically.
Figl shows how vem (assessed on the basis of hardness
measurements) of alloys with a constant Sb content aged
at 37000 varied. with increasing Be content. The
g-exiation, of V (calculate& from the data on magnetic
suscaptibilityrof alloys containing 0.2% Sb and aged
at 370, 400 and. 4200 with increasing Be content is
shown in Fig.2, while Fig.3 shows the effect of Be
OIL V (determined on the basis of electrical
resisfta~ce measurements) of the 0.216 Sb alloy aged at
3700C. The effect of the Sb and Be additions on tho
course of the ageinf; p-rooeaa in its variouis stages was
determined on the. basis of the measurements of magnetic
Card 4/11 susceptibility, since this property could be
meastured

SOV/126-6--Ar-9/34 '
The- Effect of Small
of the Copp*r-Silver
the EffOCU of Small
of Alloys)
Card 5/11
Additions of Antimony and. Beryllium on ping
Alloys (part JV. On the Problen of Causes of
Alloying Additions on the Kine-ties of Aping
with higher &OCUMOY and without the necessity of-
interrapting tha-heat treatment. To this onal gmpha
showing the time-dependence of 4 Xwere constructed,
,6 X being the difference between the values of the
relative maipetic susceptibility of two alloys aged for
a given period at 37000: one with and the other withou-b-
the addition(s), the effect of which was being examined.
In this way the effect of Sb and Be (added separately)
on the &going-process of the Gu-Ag a Oy a shown on
Fig.4. It un be seen that while i aceelerates
assing at every stage of this prooess-(this offset
being most pronounced at t = 30 mia) the effect of
beryllium is quite different: In the first stages of
US sping treatment this addition accelerates a.gaing,
but beginning from a eertaiA momant, it slows the proesss
down. (The higher the Be content the aarlier is the
moment at which its delaying effeat comes into op*ration

SOV/126-65,4-9/34 .
The Effect of,,qTnall Additions of Antimony
of the Copper-Silvor Alloys. (Part IV- On
the Ef foots of small Alloying Additions on
of Alloys)
Card 6/11
and B&3?ylliux On Ageing
the Problem of Cauws of
tkLe Kinetics of Ageing
and the greater is the magnitII&C-of the effect.)
The effect of 0.2% Sb on againg.of Cu-Ag alloys
containing 0.02 and 0.1% Be (Fig-5) is sind-lar to its
effect on the binary Cu-Ag alloy. The saw applies to
the effect of sium1taneous additions of Sb and -Be,,
except that in this case tho inaximux value of LN X.
decreases with increasiag Be content (Fig.6). The
effect of Be on kin ties of ageing of the, Cu-Ag alloy
containing 0.2% Bb is much more complex. At amall
concentrations (0.02%) beryllium accelerates aping of
the Cu-Ag-5b alloy (graph 1) in all stages of 'the
process, A. reaching its mwdzm after 1 hr. 0.1% Be
slows the process down in its initial stage and
accoloratika it slightly in the fiml ta When
present in larger quantities (0.2 - ON
SWit slows
down the ageing process of ths Ca-Ag-Sb alloy at every
I

SOV/126-6-4-9/34
The Effect of Small Additions of Antimony and Beryllium on
Ageing
of the Copper-Silver Alloys. (Part 1V. Oii the Problem of
Causes of
the Effects of Small Alloying Additions on the Kinotics of
Ageing
of Alloys)
stage, its effect being most pronounced at t = 30 min.
The following interpretation of the obtained results
is offered by the present authors: The average rute,
Ye of the isothermal decomposition of a super-
saKrated solid solution of silver in copper is
markedly affected by small s3"IMIltauisously present
additions of Sb and Be. even when these elements are
present in concentrations considerably lower than their
respective solid solubility limits. When added
separately, antimony accelerates and beryllium slows
down the process of decomposition. Howevwrs these
effects are not additive when Sb and Be are present
aiiaLitaneously: At a given Sb concentration vem
increases at first with the increasing Be content,
reaches a maximum and then slowly decreases (Fig-1-3),
The higher the content of antimony the higher are the
Card 7/11 values of v., for any given beryllium
concontrations

SOV112ra-6 - 4--'9/34
The Effect of Small AddLitions of Antimony and Beryllium or.
Ageing
of the Copper-Silver Alloys. (Part 1V. 0a the Problem of
Causes of
the Effects of Small Alloying Additions on the Kinetics of
Ageing
of Alloys)
including those corresponding to the maximum values
of vcm* These effects can be explained on the basis of
a hybothesis of internal adsorption of the Sb and Be
atoms in stru&..urally distorted zones limking the
nuclei of decomposition with the solid solution matrix,
it being postulated that, the alloying elements can be
adsorbed not oaly as separate atoms but also in the form
of complexes containing atoms of bcth additious. As a
result of the adsorption of complexes the free anerg;7
of the distorted. zones ii? dec=,eased in regions whero -
owing to the specific charaoter of the distortion - it
would not be decreased b,-;r adsorption of single atoms.
The extent to v&ich adsorption of complexes affects
the kinetics of decomposition of the solid solution
varies with time since, as a result of adsorption, ihe
total concentration of both alloying alements-in ths
Card 8/11 adsorption zone is altered to a degree depending on
the

The- Effect of Small
of the Copper-Silver
the Effects of Small
of Alloys)
Card 9/11
Additions of Antimony and Beryllium on Ageing
Alloys. (Part M On the Problem of Osus*e of
Alloying Additions on the Kinetics of Ageing
overall concentration of the additions present
simultaneously in the alloy: At a given Sb
Concentration, beryllium - when present in small
quantitios - is absorbed mainly in the form of co=laxes
with the result that the concentration of Sb in tho
adsorption zone is increased and its accelerating effect
on the decomposition ofO the solid solution is rrultiplied.
On the other hand, when the Be content is high, it is
adsorbed in, tho form of single atoms which increases
its concexr~ration in the adsorption zoner, with -the
rosuIt that the rate of dooompositicn is slowed down.
The effects of Be and Sb on.the couree of the &gaing
Drocoss are also non-additive. in the in-tial stages
;f the process when formation of nucloi of decomposition
is the predominant factor affecting the kinetics of
decomposition, the effects of the alloying additions ox
nucleation due to local lattice distortions in the

S91/126-6-41_9/3)~
The Effect of Small Additions of Antimony and Beryllium or.
Ageing
of the Coppor-Silver Alloys. (Part 1V. On the Problem of
Causes of
the Effects of Small Alloying Additions ou the Kbaetics off'
Againg
of Alloys)
vicinity of the solute atoms are non-additivt borause
- owing to the fact that Be atoms are smaller and Sb
atoms larger than the solvent atoms - tha lattiole
distortions caused by the atome of either alemant
present separately are mor& severe t:a= those caused
by the complexes formed when. the twc. alloying additlons
are present simultaneously* Ir. th* laVor stages of the
ageing process when growth of the decomposition cantvas
affected by the adsorption of the alloying elements in
the surrounding zones is the predominating factorg thle
non-additive character of the effects of Sb and. 3a is
evidently due to the fact that at first beryllium is
preferentially adsorbed, while adsorption of aiLtimony
takes place mainly in the latar stages~ This time-lag
in the adsorption activities of the two elements is
probably associated with the, fact that with the growth
Card 10/11 of the decomposition nuclai the 6haracter and
magnitude

SOV/126-46-4-9/34
The Effect of S=Lll Additions of Antimony and Beryllium on
Ageing
of the Copper-Silver Alloys- (Part 1V. 0a the Problem of
Causes of
the Effects of Small Alloying Additions on the Kinetics of
Ageing
of Alloys)
of the lattice distortions in the zones connecting the
nuclei. with the solid solution matrix are
correspondingly altered. There are 9 graphs, 1 table
and 21 references of which 20 are Soviet and 1 Englixh.
ASSOCIATION: Institut Fiziki Metallov Urallskogo Filiala.LN
SSSR
(Institute of Metal Physics, Ural Branch of the ks USSR)
SUBMITTED: 18th December 1956.
Card 11/11

18(T) PRASE I BOOK R"L401TATION SOV/3355

Akad**176 nauk 35M. Institut 24tallurall.
ftuchnyy~Aovot pa

problem^ zb&roprocbnYicb
aplavov

Zs&2*dovanlya PQ %h&rDPVDchnY3W
SPIAVLA, t. ry (Studies on 84&t-r,-
Pi

aLstant
Alloys. vol. 4). Moscow, lzd-vo AX 335R,
19,59. 400 P.

d

Cn ?

.
Xrrata lip Inserted. 2,200 copies prInte
a

YA. or Publishing Nousal V. A. 111movi Tech.
96.1 A. P. GuA*vaj

ZdLtarial -ft&rd3 1. P.
Bardin, Academician; 0. V. Xurd7umov,

Academician; X. V. Agey", Corresponding
Member. USSR Academy of

3elonc tal 1. A. Oding.
1. M. Pavlov, arms 1. P. Zud1n, Candidate

.'
T*c::Ical Scj&nceo.

PURYCW3 This book Is
intended for metallurgists concerned with
--1

the at ructural metallurgy of alloys.

COVXRL=s
This is & collection of specialized studies of
various

s In the structural rstallurS7 of
host-reaLstant alloys.
m
some with des.
lee
rinci
=1:
l
ti

ca
,
p
concerned with theore
p
r
o
v,
arlptions of now equipment and methods, others
th properties

occurring under
ad'"Ons Arm Studied and re
orted on
F
d

.
or
p
etails,
-,-es's UbIs Of Contents, The articles are
accospirw by a num-
w4fdrinces.. bo h Soviet and non-3*vl*t

t
Studies (Cont.)
30V'W55
Investigation or the DIfrUSIca or Cobalt and
Iron Along
~tb~ Grata Boundaries
152
teyn. S. -2 T X Oudlccya. A. Zbukbovltskiy. and
I all
K shkl
T
L

-
- J
rr*ct or stress Sad strain on the D1
f
fusion Prateas

Diffusion Characteristics and
Ueat

to ]tight Component Mickel Alloys
*
165
Arthsraj--V-X~~. -q-XlatLzaAn. and A~]!-
-Tima*7041 --be

Irrect or small Admixtures an
the Coefficient of DIr-

fusion In
FoIYcr78t4II%D* Materials
ITO

ykarpove'.
Concernlaf Changwe
In the Effect or. Tari;us Admixturfs at
Different stages

of Aging of Alloys -
1T6
3 -
Internal PrIction or Pure Metals and Alloys

Card 6/12

S/520/59/000/022/011/021
E073/E535
AUTHOR:
--tio tFor inv_
m
TITLE. On the Influe ce or on the Maxnetic-
Propertie of Austenitic Steel
PERIODICALz Akademiya nauk SSSR. Urallskiy filial, Sverdlovsk
Institut fiziki metallov. Trudy, no.22, 1959, PP-73-75:
TEXT; To improve the strength of austenitic steels, hot and
semi-hot ifork hardening is currently applied. Change in the
4
- mechanical properties as a.result of work harpening is due in the
aused b
first instance to structural transformations 1$ y deformation
and also by the subsequent long-run holding at elevated tempera-
tures. The basic, difficulty in studying phase transformations in f
austenitic steels is the fact that the uantity and dimensions of
the rejected phase are very small and annot be detected by X-ray i.
c
metallographic and other methods (Refs. 1 and 2). In view of the
pronounced differences in the.magnetic properties of the para-
magnetic base, the carbides and the ferromagnetic a-phase,
preference should undoubtedly be given to magnetic metallography
and thormomagnetic analysis, i.e. to the study of the magnetic
susceptibility, its dependence on the magnetic field potential and
1/,7

S/520/59/000/022/011/021
E073/E535
On the Influence of Hot Forming on the Magnetic Properties of
Austenitic Steel
the temperature. The author has investigated the susceptibility of
two grades of austenitic. manganese steel...-Dotermination of the
magnetic susceptibility reduces to measur"ng the mechanical force
acting on a specimen which is placed into a non-uniform magnetic
field. The apparatus for measuring the magnetic susceptibility
consists essentially of magnetic scales as described by
V. I. Drozhzhina and R. I. Yanus (ZhETF, 1936, 6, -N'o-3,i25O). A
..specially selected shape of the pole-shoes of the electr'omagnet
enable obtaining a highly nonuniform magnetic field in 'the x-
direction. The current in the electromagnet was vari6d between
0 and 8 A corresponding to a field potential between d and 4200 Oe.
The force acting on the specimen when placed between the poles of
the electromagnet was balanced by a pulling or pushing"-force from
the compensating coil of the permanent magnet. The balancing forc*e:
was proportional to the current flowing through the compensation
coil at the instant of compensation. In this case the follo*ing
relation is valid
Card 2/7.

S/520/59/000/022/011/021
E073/E535
On the Influence of Hot Forming on the Magnetic Properties of
Austenitic Steel
i PC P
x x c
C where
Xx C const.
i c
x c x c
and this constant is determined by preliminary calibration of the
scales with a reference standard. In these equations and
Xx ? -1- 7
are, respectively, the susceptibilities of the specimen under tea
and the standard. P and P are, respectively, the weights of
x
the tested specimen and the standard i and i are not defined.
x
As a standard Mohr's *salt was used, ;he suaceptigility of which is
6
9500-10 /(T + 1) abs.units
X c
For measuring the magnetic-susceptibility at various temperatures
a bifilar wound electric heater was placed between the poles of the,
electromagnet. The specimens were parallelepipeds 3 x 4 mm cross-
section 10 mm high.
Steel 6;X3P3H9R (60Kh~GMV). Heat treatment, hot forming of the
specimens ana 3 estigation of their mechanical properties were
Card 3/7

S/520/59/000/022/011/021
E073/E535
On the Influence of Hot Forming on the Magnetic Properties of
Austenitic Steel
carried out in the Laboratory of Physical
Metallurgy of the
Institut fiziki metallov AN SSSR '(Institute of Physics of Metals,
- - ~;f -dw atr
AS, USSR ; after forming, the specimens were dropped into c
The magnetic susceptibility of quenched undeformed specimens was
28 to 30 x lo-5 abs.units. After deformation at room temperature,
the susceptibility changed only slightly (within the range of
measuring errors). Equally, deformation at the temperatures 500,
.1000 and 1100% did not produce any appreciable change ~n the
~susceptibility. The temperature dependence of the maghetic
susceptibility of this steel (after 22% reduction) is plotted in
Fig.! (magnetic susceptibility vs. deformation temperature, *C).
.The slight change in the susceptibility after deformation permits
the conclusion that,for the given degree of deformationf, the
austenite remains stable, i.e. it does not decompose under the
effect of cold (200C) or hot working. The stability of the austen-
is attributed to tha chemical composition of this steel (0.58 to.
'0
.71% C, 8% NI).
Card

S/520/59/000/022/011/021
E073/E535
i On the Influence of Hot Forming on the Magnetic Properties of
Austenitic Stee
Steel 1(4OKh3GI8) Specimens of this steel were worked at
temperatures b9'tween 20 and 1100*C at steps of 1000C. The depen-
dence of the susceptibility on the deformation temperature 00 is
plotted in Fig.2 (for specimens with 22% reduction). The suscepti
-5 abs.
bi-lity of quenched undeformed specimens was 30 to 32 x 10
units; deformation at room temperature led to a sharp increase in
the magnetic susceptibility, Ito 300 x 10-5. An increase in the
1 deformation temperature led to a reduction in the susceptibility;
at the deformation temperature of 1000C the susceptibility was
5, at 2000C it was-33 X 10-5 and further increase in he
97 X 10
t
ti-
deformation temperature did not lead to any change in the suscep
bility except for the temperature range 550 to 600*C, where a
10-5 was
relatively small increase in the susceptibility of 47 X
observed. The considerable increase in susceptibility during cold
working indicates austenite decomposition with rejection of a
ferromagnetic a-phase. Austenite decomposes also at the deforma-
tion temperature of 1000C; the presence of a ferromagnetic phase in
17-Card.5/7-

S/520/59/000/022/011/021
E073/E535
On the Influence of Hot forming on the Magnetic Properties of
Austenitic Steel
specimens deformed at 100% is proved by the dependence of the
susceptibility on the magnetic field potential. At deformation
temperatures above 2000C austenite does not decompose.-The slight
increase in the magnetic susceptibility in the temperature range
550 to 600*C can be attributed to processes of ageing, which are
accompanied by rejection of carbides and also of the a-phase. The
sharp change in the mechanical characteristics (a ,, a.),observed
in some cases for slight changes in the deformatio telperature
(200 to 2200C) are apparently due to the appearance of.a*ferro-
magnetic a-phase owing to the influence of the deformation at these'.
temperatures. The investigations described in this pa'ee form part
p
of work carried out jointly by the Institute of Physica~ of Metals
AS USSR and the Urallskiy zavod tyazhelogo mashinostrolYeniya
(Ural Heavy Engineering Works), Acknowledgments are expressed to
work and to K. A. Malyshev for his
M. N. Mikheye for direFtins
constant assistance. There are 2 figures and Soviet references.:
Pard 6/7

S/520/59/000/022/011/021
E073/E535
On the Influence of Hot Forming on the Magnetic Properties of
Austenitic Steel
Fig.1
Ao
Q 100 600 -Zoo
Fig.2

0

1

so

0
VC. 011~0 o0a $to 1000 '40
Card 7/7

81908
S/126/6o/oio/ol/013/019
EIII/E335
AUTHORS: Belenkova, M.M., Kodlubik, I.I., Malyshev, K.A.,
Aikheyev, M.N., Sadovskiy, V.D. and Ustyugov, P.A.
TITLE-. InFluence of Deformation of Martensite on the Cold
Shortness of Austenitic Steels and Their Hardening
in Plastic Deformitiont-
PERIODICAL- Fizika metallov i metallovedeniye, i.96o,
vol.io,
No. 1, pp. 122 - 130
TEXT: Investigation of a series of austenitic steelJ has
shown
that some have a tendency to brittle fracture.11The authors
point
out that martensite formation during co]A-shortness testing
is
the-probable cause and that liability of austenitic steels
to
fcm martensite in plastic deformation depends on the
position of
the deformation temperature relative to the martens�te point
(Rerf 2) and the temperature at which austeni-te and
martensite
free energies are equal. Their present work dealt with the
following steels (analysis in Table 1):\i~LQqjj, 4OG18Kh4,
40G18Khg, 40r.18Kh4N4, 4ornfth4M, 4oGlfth4NV.~I~oGA,
50r.18Kh4,
50G18Kh4N8V, 50G13Kh4N4, covering the composition ranges W:
o.4o - 0.55 C. 0-0-71 Si 17-30-18.6o Mn.. o-8.o Cr, 0-8-32
Ni,
Card 1/4 1~

81908
S/126/60/010/01/013/019
Elll/B335
Influence of Deformation of Martensite on the Cold Shortness
of
Austenitic Steels and Their Hardening in Plastic Deformation
0-0-71 W, 0-0-010 S, 0-0.067 P. 60 mm, long pieces were cut
from
12 x 12.mm forged bars. The pieces were heated to 1150 0C and
cooled in water. Magnetometric -tests showed no martensite
trans-
formation on cooling to -196 OC. Standard notched test-pieces
(2 nim deep notch, I mm radius of curvature) were used for
impact
t;ests from room to liquid-nitrogen temperature. Alpha-phase
(deformation martensite) was found with great sensitivity by
measuring magnetic susceptibility (Ref 3) of austenite on
3 x 4 x 9 mm pieces cut from the fracture region of impact
speci-
mens, Mohr's salt being used as the standard. In a second
series
of experiments the austenitic steels after quenching from
1150 oc
were rolled at 20-600 OC to give 30% deformation. Figs. 1-3
show the toughness of the various steels as functions of test
temperature, the effect of the various alloying elements
being
brought out; magnetic susceptibility as functions of test
temperature being similarly shown in Figs. 4 and 5. Figs. 6
and
7 show deformation of martenaite structures and Fig. 8 the
fractures obtained at various temperatures. The dependence of
Card 2/4 Lr

81908
S/126/6o/oio/oi/ol3/olq
El1l/E333
Influence of Deformation of Martensite on the Cold Shortness
of
Austenitic Steels and Their Hardening in Plastic Deformation
tensile strength, yield point, toughness and magnetic
susceptibility
on deformation temperature is shown in Figs. 9, 10, 11 and
12.
4OG18 and 50G18 steels showed pronounced cold shortness,
which
could be considerably reduced or completely eliminated by
additional alloying with chromium or nickel. The reason for
the
cold shortness is deformation-martensite formation during
low-
temperature impact testing. The good effect of alloying the
manganese steels with chromium and nickel is explained by the
increased austenite stability with respect to
plastic-deformation
induced martensite transformation. Formation of such
martensites
is the reason for the greater hardening of manganese
austenitic
steels in cold compared with 200-300 OC plastic deformation.
In
stable austenitic steels, additionally alloyed with chromium
and
nickel, hardening in cold and semi-hot work-harden3Lng is
pract-
ically the same. There are 1.2 figures, 3 tables and 5 Soviet
references.
Card 3/4

81908
S/126/6o/olo/ol/013/019
EIII/E335
Influence of Deformation of Martensite on the Cold Shortness
of
Austenitic Steels and Their Hardening in Plastic Deformation
ASSOCIATION: Institut fiziki metallov AN SSSR (Institute of
Physicsof Metals of the Aq.Sc.. 5LR
Ural'skly zavod tyazhelogo mashinostroyeniya 1m.
S. Ordzhonikidze Aural Heavy Engineering Works
imeni S. Ordzhonik1-a-z-e-T-
SUBMITTED: February 23, 1960
Card 4/4

S/129/60/000/oll/004/016
E073/E535
AUTHORS: Belenkova, M.Mj_, Kostenko-, A.V., Mikheyev. M.N.,
Stoinakaya, E.E., Pogrebetakaya, T.M. and - Y $A.A.,
oprgenson
TITLE: Engineers. ing, V
Influence of Heat Treatment and Nitrid n th3
Mechanical Properties of Austenitic Steels,
PERIODICAL: Ketallovedeniye i termicheskaya obrabotka metallov,
1960, No.11, pp.16-20
TEXT: A nitrided layer of austenitic steel can be ferro-
magnetic, although the core of the component can remain
paramagnetic.
By changing the preliminary heat treatment it is possible to
obtain
an austenite with various degrees of alloying and various
compositions of the secondary phases. Changes in the phase
composition during preliminary heat treatment of austenitic
steel
may bring about changes in its magnetic properties due to
formation
of 6-ferrite resulting from quenching at elevated temperatures.
For
this reason, the authors considered it of interest to study the
influence of preliminary heat treatment and nitriding on the
mechanical properties of austenitic steel. Two steels of the
following compositions were investigated: (in %)
Card 1/5

S/129/60/ooo/oll/oo4/oi6
E073/E535
Influence of Heat Treatment and Nitriding on the Mechanical
Properties of Austenitic Steels
Steel . C Si Mn Cr Ni W Ti S p
D0122)(EI123)i~ 0."18 2.27 o.65 14.54 13-80 1.79 o.84 0.007 o.o16
IXIJH~T 0, 0 0.58 0-53 17-78 8-70 - o.64 0.013 OaO20
(lKhl8N9T)- - Ol
The magnetic properties were studied after preliminary heat
treat-
ment followed by nitriding. The steel lKhl8N9T was additionally
subjected to "wrong" nitriding: tinned specimens were charged
into
a furnace simultaneously with the nitrided specimens of the same
steel. The magnetic properties of the steel E1123 were determined
after normalization annealing or after normalization annealing
and
ageing. The normalization temperature was 1150 and 1070*C. The
preliminary heat treatment of the steel IKhl8N9T consisted in
quenching from 1150*C in water and subsequent ageing. Both steels
Card 2/5

S/129/60/000/011/oo4/ol6
E073/E535
Influence of Heat Treatment and Nitriding on the Mechanical
Properties of Austenitic Steels
were aged for 8 hours at 8000C. The specimens were in the form of
12 mm diameter, 5 mm long cylinders. The magnetic susceptibility
of the steels E1123 and lKhl8N9T in the paramagnetic state was
measured by means of magnetic scales at various field strengths
as to determine the 'X(H). For investigating the magnetic
propi:rstoies
of the nitr�ded steels, specimens in the form of tubes with an*
external diameter of 8 mm, a length of 60 mm and a wall
thickness of
0.5 mm were used. The external surfacesof the specimens were
ground
whilst the internal surfaces were machined by means of a reamer.
Prior to nitriding, the specimens were etched in a hydrochloric
acid
solution at 700C for 5 min and then nitrided in a laboratory
furnace
at 600*C, with a holding time of 65 hours for the steel EI123 and
75 to 55 hours for the steel lKhl8N9T. The 75 hour holding time
corresponded to the maximum depth of the nitrided layer for
specimens
with a wall thickness of 0-5 mm. The magnetic properties of
nitrided
specimens were measured ballistically in an open magnetic
circuit.
On the basis of the obtained results, which are given, the
following
conclusions are arrived at:
Card 3/5

S/129/60/000/011/004/Oi6
B073/E535
Influence of Heat Treatment and Nitriding on the Mechanical
Properties of Austenitic Steels
1) Changing of the normalization annealing temperature of the
steel EI123 from 1070 to 1150*C and additional ageing for 8
hours at
800*C does not bring about a change in the susceptibility of
thisztM2.
2) Nitriding changes to a considerable extent the magnetic
permeability
of the investigated steels; the nitrided layers of both the
investigated steels were f erromagnetic and this is due to the
formation
of nitrides, impoverishment in alloying elements of the austenite
and austenite decomposition.
3) As a result of nitriding, the magnetic permeability of the
steel Y
EII23 increases consid6rably (by a factor of 3) as compared to
the
steel lKh18NqT.
4) Increase in the depth of nitriding brings about an increase of
the maximum magnetic permeability; with increasing relative
depth of
the nitrided layer of the steel EI123 from 23 to 48.5% the
maximum
permeability increases by more than double. With increasing
relative depth of the nitrided layer of the steel lKhl8N9T from
50
to 93.65%, its maximum permeability increases from 3.7 to 19.8
gauss/0e.
Card 4/5

S/129/60/000/011/004/016
E073/9535
Influence of Heat Treatment and Nitriding on the Mechanical
Properties of Austenitic Steels
5). The results of the described investigations lead to the
conclusion that it is possible to monitor the depth of the
nitrided layer for a number of austenitic steels by means of an
electromagnetic method. There are 1 figure, 5 tables and
5 references: all Soviet.
Ca rd 5/5

S/126/62/013/004/019/022
/ep. ')S-o L-) E073/E135
AUTHORS: Be I ta nkQXa
M.M., Mikheyev, N.
Pogrebetskaya, T.M., and Yurgenson, AeA,
TITLE: Magnetic properties of the steel 1)(3..8H 9 (lKhl8N9)
after heat-treatment and nitriding
PERIODICAL: Fizika metallov i metallovedeniye, v-13, no.4, 1962,
622-625
TEXT: The authors and their team found earlier that the
greater the content of elements forming stable nitrides, the more
will the austenite become impoverished of alloying elements
during nitriding and the more intensive will be its decomposition
and the rejection of the cx-phase. The influence of nitriding on
the magnetic properties of steel similar to the previously tested
1 X 18 H 9T (lKhl8N9T) steel but not containing titanium was
studied to verify this conclusion. The compositions of the two
steels studied were:
IKhl8N9: 0.14,/~o' C; 0,66% Si; 0.85% Pln; 17.68Yo Cr; 9.02% Ni,
0.07% Ti; o.ol6% s; m16% P.
Card 1/4

.P
Magnetic properties of the steel... s/126/62/013/004/019/022
E073/E-135
IKhl8N9T: 0.1% C; 0.58% S�; 0.53% Mn; 17-78% Cr; 8.700% Ni;
o.64% TI; 0.013Yj S; 0.02% P.
The magnetic properties were determined after heat-treatment
(quenching from 1150 *C in water, followed by ageing for 8 hours
at 800 *C). Both steels were paramagnetic in the quenched state
and their susceptibility values were nearly the same. After
a7eing the susceptibility increased somewhat, the permeability of
b,t,"i steels after quenching and ageing approached unity and did
not depend on the field strength. In the nitrided state the
max2.mum permeability of the steel without T:L was considerably
lower than in the steel with Ti. For a relative depth of the
nitrided layer of 57.4% the steel lKhl8N9 had a maximum
permeability of 1.8 gauss/0e, whilst for the steel IlChl8N9T the
maximum permeability was 3.7 gauss/Oe for a relative depth of
the nitrided layer of 50Yo. The structures of the n1trided
layers of both steels were identical, consisting of austen:Lte
and carbide grains in the heat-treated state; the structure of
the nitrided layer was reminiscent of sorbito, due to the
partial decomposition of the'a-phase and the carbides during
Card 2/4

Magnetic properties of the steel.. S/126/62/013/004/019/022
E073/El35
nitride-formation. The following conclusions are arrived :-,t:
Nitriding c1langes considerably the magnetic propertles of
steels
IKhl8-\'9 and JKh18N9T; the ferromagnetic nature of the nitrided
layer is due to the formation of the a-phase during nitriding.
The steel lKhl8N9T has a higher permeability in the nitrided
state than the steel IKhl8N9, and the difference is attributed
to the presence of TI in the former, which forms stable nitrides
and impoverishes considerably the y-phase of Ti, reducing its
stability and bringing about rejection of OL-phase. The-
stability
of the austenitic structure after nitriding was determined by
the
concentration of admixtures required for forming uniform
austenite and by the ability of the components entering into the
austenIte to form stable nitrides, The nitrided skin of
austenitic steel components should have low permeability values.
There are 4 tables.
Card 3/4

S/126/62/013/004/019/022
Magnetic properties of the steel.. E073/P-'135
ASSOCIATION: Institut fiziki metallov AN SSSR
(Institute of Physics of Metals, AS USSR)
Urallskiy turbomotornyy zavod
(Ural Turboengines Works)
SUBMITTED: August 26, ig6i
Card 4/4

ARKHAROV~ V.I.; BELENKOVA,,,M.M.; MIMYLIVA, M.N.;
MOISEYEV, A.I.;
POLIKARPOVA, I.P.
Change of magnetic.Busceptibility and the behavior of
small impurities
in the decomposition of an Ag - Cu solid solution. Izv.
AN SSSR.
Ser. fiz. 28 no.ltl4g.151 JA 164. (MIRA 17tl)
1. Institut fiziki meta3-lov AN SSSR.

ACC NR: AR6027503 SOURCE CODE: UR/0137/66/000/004/IO19/1019
AUTHOR: Belenkova,,M. M.; Mikheyev, M. K.; Malyshev, K. A.;
Sadovt;kiy, V. D.;
Ustyugov, F. A.
iTITLE. Phase transformations during the deformation and tempering
of austenitic steel
SOURCE: Ref. zh. Metallurgiya, Abs. 41127
REr SOURCE: [Tr.] In-ta fiz. metallov. AN SSSR, vyp. 24,
196S,.54-58
TOPIC TAGS: metal deformation, austenite steel, martensitic
transformation, grain
size, magnetic susceptibility
TRANSLATION: A study was made of the magnetic, electrical and
mechanical properties
t6f 601WIGN8V austenitic band steel subjected to deformations of
10, 25, 31, and 431%.
after quenching from 10500C. For the same deformation conditions,
a fuller decomposi-
,~ion of austenite occurred in large-grained samples as a result
of the variation of
ni-~
,the position of the martensitic point for a change of grain size
(the point of the i *
Itial martensitic transformation of large-grained -;;xnples was
located higher than fine-
grained). Under the effect of deformation in the steel, a much
greater amount of a-
phase formed than during tempering. A definite correlation was
found between the na-r
;ture of the magnetic and electrical property changes on the one
hand and the mechanical!,
properties on the other, as a function of tempering temperature.
Thus, a drop in a,,
UDC: 669.15126174124.781.017.3:621.785.78
Card 1/2

_AC'_C__N_R: -AR602-7-5-03
id a aof samples deformed at 200C was found beginning at
400-450OC; a-, these same tem-
~ratures the lowering of electrical resistivity was initiated.
Magnetic susceptibi-
,ty increased after 5000C, while * and a k decreased. It was
concluded that the chang-
in mechanical properties were caused by processen associated
with the formation. o-f
-phas e during cold deformation. During tempering of the
defomed samples, the a-phase
: the original deformation is dissolved and some quantities of
the ferromagnetic phase;
spear in separate portions owing to carbide formation. 1.
Tulupova.
JB CODE: 11,13
2

BELUIKOVA, M.Ta., zeditsinakaya sestra
C~:~ ---------------------
ReInforcIDS bandage for the lower abdome. Ned.sestra 19
no.8:34
Ag 160, (MM 13:7)
(Baum AD UnAGM)

BEIINKOV., N.Yu.; CHIRKOV., V.D.
L-lechanism of the synchronization of neuron activity.
Zhur. vys.
nerv. deiat. 15 no.1;128-139 Ja-F 165.
(MIRA 18'.
1. Kafedc-a norri-,allnoy fiziologii, Gorlkovskogo
meditsinskogo
instituta.

BELENKOV, N.Yu.; KALININA, T.Ye.
Distribution of primary responses to acoustic stimuii
in the
cerebral cortex. Zhur. vys, nerve de'Lat, 15
no.2:285-294 Mr-
Ap, 165. (MIRA 16;5)
1. Kafedra normallnoy fiziologii GorIkovskogo
meditsinskogo
Instituta, Gorlkly.

8/08 V62/000/017/075/102
B156/B186
AUTHORSt Sa,ttar-zade, I. S., Belenkova, R. M., Bayramova, R.
M.
TITLEs Catalytic transformation of petrolatum over gumbrin
PERIODICALs Referativnyy zhurnal. Khimiya, no; 17, 1962,
474,.abstract
17M171 (Azerb. neft. kh-vo, no. 12i 1961, 41 - 43)
TEM The thermocatalytic decomposition of petrolatum
(temperature of
solidification 56.90C, n 20 D 1.4565, d20 0.8551, mol.wt. 643,
acid number
0.0) in the presence of unactivated or activated'gumbrin has
been in-
vestigated, using a ratio of the petrolatum to this catalyst
of 20 at a
temperature of 3500C and at atmospheric presgure. The
experiments were
performed in a three-necked flask connect6d to a condenser
coil, with
,continuou's agitationg and lasted-6 - 12 h. It was proved
that the
petrolatum is transforme,~L almost identically whether an
unactivated or an
activated catalyst is used, the products being 51. 53~Z of
liquid and
26 -' 3.11,46 of solid hydrocarbons respectively.
Investigation of the group
chemical composition of the fractions obtained showed that
they are of
Card 1/2

. S/081/62/000/017/075/10'2
Catalytic transformation of... B156/B186
methane-naphthene-aromatic type. The gases formed during the
transforma--
tion of the petrolatum consist mainly of saturated
hydrocarbons. LAb-
stra'oter's note: Complete trans lation-I
Card 2/2
0

NIKONETS, I.F.; BEISNKOVA, T.A. (Llvov)
Effect of aimidoD ine on immunoganesis and the prothrombin
forming
I yr
function of the llvPr, Vrach. dclo noJ120-21 Mr 164.
(MIRA 17%4)
1. Kafedra gigiyeny p1taniya (zav. - prof. A.I.StoLnnakova)
Llvovskogo wditsinskogo in5tituta.

BFLENIKOVA, T. G.
Belenkova, T. G. - "The functional condition of -ongested
klineyl qnd its
physiotherany," (In the ge9ding: T. D. Belenkova), Sborn1k
trudov (Tomskiy
obl. mauch.-issled. in-t fiz. metodov lecher-I.ya i
kurortologil), Vol. V!, 1949, n.
358-82
SO: u5241, 17 December 1953, (Letonis 1zhurnal Inykh Statey,
No. 26, 1949).

GROKOVA, I.A.; BEI-EM , Ye.Q., starshaya evinarka;
ZAYTSN, V.S., red.;
TIKHONdYA__,__I-.K.. -tekhn.red.
[You gave' your word; keep it!] Dal slovo - adershi!
Leningrad,
Lemisdat, 1959. 84 p. (MIU 13:4)
1. Sekretarl partlynoy organizataii kolkhoza wPervoye
maya" Get-
ohinakogo rayona, delegam XXI 911yesda IM (for
Gromova). 2. Agi-
tator kolkhosa imeni MCI parts"yesda Voevolozhokogo
rayona (for
Beleakova).
(Agriculture)

BASOV, N.G., BELE IOV E.M.; LETOKIIOV, V.S.
Synchronization of oscillations in a semiconductor laser with
several p - n-rjunctiona. Fiz. tvcr, tela 7 no.1:337-339 Tq 165.
(MIRA 18:3)
1. Fizicheskiy institut imeni Lebedeva All SSSR, Moskoia.

I 2.53o-66- ZWA(k)/11BD/EWT(1-)/ZFd(k)-; T/EWP(k)/ZWA'(m)-2/EWA(h) S M./IJP(c)
WO
'ACCESSION NRf AP5022875 UR/0051/65/019/003/0465/0467.
621.375.9-.5j5
;AUTHORv Belenov, E. M.; Letokhov,_V._S1t,
ITLE: Generation high rectional coherent radiation
T of 1y di
-v. 19,.no. 3,.-1965, 465-467
SOURCE: Optikai I spektroskopiya,
','TOPIC TAGS:' ~,Aaserj cSherent radiatiop,stitnulated emission, laser array
-'ABSTRACT .Generation-of highly dire tionallcoherent radiation by an
arraiy-dVeouple d
c
;lasers is di-p-cussed., The two methods-described are based on the
interference in thel',.
'far zone of 1) doherentbeams from several synchronized lasers (an
arrangement-for-j-.
two lasers is shown in Fig. 1 of the Enclosure), and 2) coherent beams from
reflecting,
:surfaces (Fig, 2) of a single laser. Jn,the first case the follow-Ing three
operating
tregimes are possible: a) synchronized-generation by two lasers, b) iudependent
opera-
tion of two1asers, and c) gin eration by one.laser with a cavity inthe shape of
The results of-an earlier paper (4kademiya nauk,SSSR. Doklady, v. 161, no. 3,
1-7-
1965, p. 556) are used to obtain the criterion for the ekistence
of.the.synchronized-
regime which can be achieved.by using gas lasers. A similar analysis can also
be'
conducted for more than two lasers. The coherent laser,emission which
interferes lu-
!
Chard 1/4

C.LgG JLA ayllr-[llccpujmftlL;.LQll ox LWO aullerm
Card

BASOV, N.G.; EFIXNOV,,_~A; LFTOKHOVt V.S.
Diffraction synchronization of lasers. Zhur. tekh. fiz. 35
no.6tlO98-
1105 je 165. (MIRA 18: 7)
1. Fizicheskiy institut imeni P.N.Lebedeva AN SSSR, Moskva.

BM,ENOVV E. M.; CRAYFfSKIY, A. N.
A maser with two series cavity resonators.
Radiotekh. i
elektron. 8 no.1.158-161 Ja 163. (MIRA 16:1)
(masers)

~7 7 7 -.77, 7.7-
~CM-th''-fir6t,~re rt'
h po ~_by_: thb: autli6raL-.(RadioteXhnika I--eliakt-go
t
kail S."158i 19 atio for~the,maser os6ill_tliona Are-
~63). The equ ns a
-apilied,to.masersw
P~ ith.. two, separated resonators with opposing,mole..7
beams .arid to.a maser-withclosed-circulation of,themolecule
cule,
he:-froquoncy shift-due:tot e~ a .0 -is eval-~.
beam*,T h tr' veling wave ' f fecl~
--- ----------
Ai 9 ___. -
a s- showa':,thif zr4s AtW-.twd-.t4ddonato-ta--~iti~,tan im
ed. e an -d
_dt
-1 cat
V

BELENOV, E.M.j aRASTSKIY, AON&
Molecu.3ar osoinator with two resonators arranged in
succession. Izv.
vys. ucheb. zav.; radiofiz. 7 no.3:479-490 164. (WRA
l7slI3
1. Fizioheskiy institut Im. P.N. Lebedeva AN SSSR.

L M)'3,)4_6f' rVIA (k F1-D/0W;'
r
-ACCESSION, INR: AJP5P~26 Ukjdo5WW0i6 ~/085810 5
14
XMOR; aejenov~-~'E4- Mv; Or-,ewkiy*-'A_tLN4-
lvl~~X~Myl
171- _'d fi ecif 07
_~~ma e- or-a~_,sp brad
P 2.3 fo ways, f.
they:-can- be appliea to er6.tion.at~other:vavelengths'.:-, ropos s . r, o
ut* t* of a~neon-helium lazer,are as tollows: 1Y allitioli
increasingthe ou pu..power
dec4 of. motastables 2
of- a buffer gas, which enhances,thle- increase in the,
...working gas temperature, f -elect rofis;- pulsed exm
-wach - increases the enermr .0
citation, which Xe~ulU_ in dnadvantateous- population of the upper working
level-,.-
n -luminescence re ch results,
g'the period; 4) inc ase 'in the resonator length,'whi,
-irk more modes in the Dopplek _1131e'-vidth; 51 increase in.'the lezigth of
the dischai6
th r; and 6) reduc-
tubet Which leads to aproportional.risein e.output.powe tion ib.-
the characteristic-size-A of the diseharge.t1ibe-while maintaining increasing
d

L 54772--65

off,
ACCMI NR#
-AM5=

.

-ASSOCIAZO

ou CODSI

~c t7

'xk7.

l W`
~7 i
N

'
i

~
jam2sj

WG/WH:
r,kcUsloil XR.-, .4$dibu~ vii!020/65 /161'/004fQT99/6Soi-,
-JAVMOR., Dasov, N. G. (Carresponding,member'.0, SS~R); Pel~=T, E.
H.; lit-othoVIV.

--The angular modulation characteristics were measured as a function
the output p6wer6'.Reductidn of. the beam divergence . by :f ilt6ring
laser apparatus cans rue-
out certain modes, is discussed. Rotating, t
ted for -the' (a modift
measurement. of the : laser. emission spectrum ca
tiorl of the Sagnae experiment) is-described. The results show tbat
-o 'the. laser 'can' be increased by. adding a buffer
the output power f,
-gas :to. In'tensify, the.decay.,of: the, metastable neon., by.
increasing
the temperature bf--tbe working~gas,.by using pulsed eicitation
to--. -
populatethe upper..working level,by increasing the resonator-lengtht
of the d1sebarge tu6e., and bX decreasing tbe~tr,ans-.
the length,
verse dimensions of:'the" dchargetube. The'autbors.t
.di
hank Yu. P.
Trokhin -V.. N. Lukanin B. 11. ProkoPoV B. I. Belov F. S. Tifov.
J_ I
A.-F. Sucbkov,for*a,:. discussion of the results and 7-help.
witb-.tbe:'
calculations. Orig.,:art._.bas:,l6 figures~&nd 13 formulas.
OOD)t 2 OIJTG.~ REF** 22/ 'OTH REP:: 020 sui* DATE.
SUB P/
jwne
Card .2

OL.61 FBD!WT ~C(k)_Z/TJEWP.(k)JWA(h) WG
2 (1)/EL
&
WUAG% WDE: UR/0020/65/161/004/099 01
ACC NRz AP6011996
!as
AU 3R); Belenov, E. H.; Letokhov,
THOR: N. G.: Corresponding:member AWSS.,
-ov, 14 i
0 P~Yeic .4
RG 3Institut it, P%'_ N 1,6bedev, AN I SSSH (Fizicheskiy institut AN SSSR)
TITLE: Limiting cross-s Iection of a laser ~Izw
SOURCE
AN' SSSR.~ Doklady, v. 161p no- 4,1965s 799-801
~TOPICJAGS: ',laser be. ',~ laser theory~
am
am-cross- actions lasers having
ABSTRACT: :, In principle,-bq 3 0& continuously-6peratine
&r resonators can be liffiited,owina to tho-del ad interaction of remotte
parts of
AY
'the laser or mismatching of the natural freque-ncies of the' various parts
of the
-rezon&~o-. in (Z~Modul e lasers the beam cross-secti
-I U I I aied pul z . on is linited because
-the PLas.~.c;~.-.cration time is of the o"rder of time required for the
resonator
oscillations to become established. Beams ol' both typea of laser are
considered.
In the first case the problem is treated !~y splitting the laser into hio
coupled
'th interaction.. in the-second case, gen
psublaser5ll and then analyzinq 9 oration can
occUr la O.-la of 1-wo modest a) development of individual incoherent
11streams", and
A.
-b) confluence of adjacent. "stream" with coherence becoming established
due to dif-
field exchange. Under the given conditions the maximum cross-oeetion ot
~'goneration in case 1:13 about-5 cm; in case 2..it is 6 and 4.am
resPectivelY for
-the two modest- The authors thank V# I* Morgov for.a series of useful
disciid6ionso
Origs art-* hasIA'formulas. [.JFRST 7-
OTH JW-.- 001-
-,SUB CODE., 20 SUBM DATE: 24Nov641 OR16 WW: 004
Cwd -
M
MIN=
7~ - ------ 10~16_11_120

ACC NRx AP5028331 SOURCE,_ODIX: ibW0057165 Oil/21-26=0
/035/
AUTHOR; Belendv, E. M.~, Letokhov, V., S.
ORG% Physics Institute im. P. N. Le-bedevq- AN SSSR (Fizicheskiy i
-Moscow astitut)
kj7
TITLEt. Onthe theo of' coupled Iad~rs 674#
ry
SOURCE: Zhurnal.tekhnicheskoy fiziki, v.~35, no.,11, 1965, 2126-21128
-TOPIC'TAGS:
laser,jaser synchronization, diffraction synchronization, laser
couplinq
ABSTRACT* Specific eased of-the.spchronizatioa of several lasers and
p-n Junctions
were described earlier by the authors withN. 0. Basov (ZhTF, 25. 6,
1965; 25, 5,
1965, 809;,FTT,'7,.337, 1965). In this-let6er to the editor of
Zhurnal tekhnicheskoy
-jizikii.the authors r"aport on the results of a theoretical
investigation of a two-
laser synchronization under more general conditions: different field
amplitudes,
delayed interaction, interaction through the active medium (apart
from the resonator
coupling), and permittivity.dispei6ion. Orig. art. has: 10 formulas.
[YK
SUB CODE: EC/ SUBM, DAM. l3Mar65/ ORIG.,:REF.* .003/ ATD PRESS:
COM

-77-7-- -7
FBD/ZWT(I)/H~C(~)-2/TA?VIP(k)/IWA(h) IJP(c) WD
ACC NR,. AP6006804, SOURCE CODE:' UR/0386/66/003/001/0054/0658
Reldnov,-E.~M.* Markth. Ye.' P.; Morozovi V. N.. Orayevskiy,,.A. N.
'ORG: 'Pb= ics Ins:Litilte im. P, W, LObedev..Aca emy-.of -Sciences
-.6155R (Fizicbeskiy
nstitut Akademii nauk SSSR)
..,,;TITLE: Interacti6n between traveling waves in a ring laser
SOURCE: Zfiurnal~eksperimentallnoy i-teoreticheskoy fiziki. Pis1ma v
redaktsiyu.
Trilotheniye, v.'3, no. 1; 1966, 54-58
TOPIC TAGS:
fa Is, laser, ring laser, helium ." neon lahe'r, laser R and D,
traveling
iwave: interact on
._ZABSTRACT.- An investigation of beat frequencies,in.traveling waves
generated in a
1ring laser. on. a rotating platfQrm, may. be used for highly.
accurate analysis of the
statistical, and 6ther,:charcieteristics of laser emission. However,
fre
~quency splitting.h.of the-traveling:waves takes.place only at rates
of rotation-V
I greater than some'criticalvelocity V O=Mcr/w,
cr (or the corresponding quantity A,,
'where V is the linear velocity of a resonator mirror' k is the wave
vect;r Cou
!pling between traveling waves causes mutual synchronization at
frequencies below. the
1cri:tical value which resultrAn single-frequency conditions. The
authors studied
Card 1/2

q
L 17985-66
ACC NR: AP6006804
'tbe_q,uantity A as a function of the`
cr parameters ofa,ring las,er'...A helium-neon-
.laser was used in t~-is experiment (Ai3.39 1j). .A spectral analyzer
was used fo~
asuri
me ng the.beat frequency A. The captureband Acr was studied as a
function'of-
;
e coefficient of transmission for-the output mirror. A reduction in
transmission
causes- a sharp change, in the band. .' Experiments were conducted on
attenua-
tion of.the beam reflected from the.external.mirror by using a
filter. Attenuation
-es the,capture bands. Various opticalsystems were used for
,of this signal redw
passing the direct,and reverse beams to the photoelectric mixer with
a simultaneous
reduction in. the,enorjW reflected into the resonator from the
external mirrors.'
Figures are given sh .owing two . modi fications of systems for
reducing the capture band
to $Wcps.' Theig of the resonator-wias reduced for a-further
reduction of the,band*
r
i This was doneby replacing one of the opaque mi rors in the
resonator wiC-.,_a:se'mi-
transparent mirror. The result was a,reduction in the capture band
from X-0 to 50
cps at the same output power. The magnitude of the capture band is
determined by_~.~
the reverse reflection of enerU from'various elements -in -the
resonator' scattering'
by, nonhomogeneous media, and , the 'nonlinear depl3ndence. of
polarization on the field.
-."The aiathors are grateful to-A. G.-Bas-ov for
valuable consultation and.interest n~_
Ithe work~and to V.-V. Gromov for assistance in carrying out the
experiment!, ~.Grig.
-2 figures 2 formulas
art. has:~
AUD CODE: 20/ SUBM DATE: .23Nov65/ ORIG,REF: 002/ OTH' REF: 003/ ATD
PRESS:

Bf-1BN0V,-.F-.M.j ORATEVSKU, A,H.
Kinetic proCOBS88 In a gas laser, Opt. i "ktur. 18
no.5e858-865
W 165. (MIRA 18,20)

ACC Nib.
AP6011405- SOURCk CODE:' 1I4/=T/66/W6/=/W.II7/05Go
''AUTUORt, _Ii_ it- OraZ
A-N__
6"i*j ORO:. T NIlAbede*,- Moscow, institut)
_-qizichexki
;`-TITLI.*~- Cha' resonator.-no ocular bean,oscillator--
wQ
t7i
urn :Aeil"ic~Oikoy-lj~ iki, '4. ~'38_ -noe 19a -560
557
J,
--bean'
'4,11 :~TOPICI Wail: vioiiiculir r: olectr6iil so resonant as, ityg,
line,wldth:~
c V
"pis 4i A,
_tKII-USMCT.~.' In, two ea r1lor,papers
tt;k .~ , . .. A I - ~ -- (Radlotekhnika: I elektIV41ka,,pt 1381
19613~1 lave,
79
lk- Vuz6V ,~ Ra Itif laika j, -10641thi authors hivo'~djscupsed
nolecuhiUi
no" a
Zz
~ogclllstor'i in *b1th"two
cgvity'keoonaiorm-are-traverood',oucce'ssively by,both,of two
time T* which
-oopon,itely'directed.molocular beavis,.and have defined
a:cbaracteriatic
determines the frequency distribution -~(Iine-width)-of the
oscillations, Haire they
present results of a calculation of f*. Thd calculations were perfo
d~b techniques
rue y
described in the references,ciUd.aboveand are'not described in detail
here; they
involve-solution of SchAdinfer's equation for the-bean
moleculesAnteractin'C with the
resonator fields and Maxwell s.4quitions forthe resonator fields
excited by the beam.--7
Expressions are given for T*'and for
the difference between the geAerated frequency W
th-6-frequency of the molecular transitIon4w,.terms of the frequency
of the nDlecular,,
-,.transition, the. resonant'-f requencied and Q factors of the
resonators, the f Leld,
strengthelin the resonators., the the
matrix elewnt of the molecular polarization for
1 1/2

I -I -T " " Cl "~ 1.
:-I. -, - .- - I..
I
u - .!- .0 i :
. ion ")" t- , ~Ic , ,
Kinntics o' ~,!Al ~1, -r-.-- t, .-
Z'.ur. lo~~- . ?- z. 77, no. 1-1 1,952

~- I % "
TONKEL, I., inzh.; RELICNOV, I. ~ h.; SICROK0. V.,
inzh.
How to protect the wood of birch from rot. Mast.lesa
no-5:11
14T '37. .(MIRA 10:10)
l.TSentral'ny7 nailchno-isaledovatellskir institut
lasosplava.
(Birch) (Wood--Prbservation)

--,
.I . - - --- -1-1 1 "-
Construction on the Oldsia Lenina,* Collective Farm. Sell.
stroi.11
no.5:7 MY 156. (Km 9:9)
l.Prodeedatell kolkhoza "Ideya Lanina", Orlovskogo rayona,
Orlovskoy
oblasti.
(Farm buildings)

BELENOVp M.
Mass forms of economic education. Vop,okon, no,5;n6-ng w f6l,
(MIRL 140)
1. Zaveduyushchiy otdelom, propagandy i agitateii TSentrallnogo
komiteta, Komim-Isticheskoy partii Kazakhataaa, Alma-Ata.
(Kazakhstan-Economics-Study and teaching)
(Conr~nist Party of the Soviet Union-Party Work)

SAPARGALIM, G.S., kand. yurid. wruk; PALI GOV, N.H. , akad.;
BOGATYREV, A.S.;
AFANASIYEV, A.V., prof.; B7XOV, B.A.; SHAKEMATOV, V.F., kand.
istor.
nauk; POKROVSKIrp S.N.t akad.; SAVOSIKO, V.K., kand. istor. nauk;
NUSUPBEKOVt A.N.p kand. istor. nauk; BAISHEY, S.B.9-akad.;
G0RPKH-
VODATSKrY, I.S.g kand. istor. nauk; AKHKETOVl A.9 knd. istor,
nauk;
RAKH314OV9 A., kand. istor. nAuk; PIVENI, N.F.; CHULANOV, G.Ch.,
dcktor
ekonom. nauk; BOROVSKIYp Y.A.v kand. ekonam. nauk; SYDYKOVI
A.S., kand.
pedagog. nauk; ZHANGELIDIN, T., kand. filos. nauk; KARASAYXV,
L.K.;
KANAPINq A.K., kand. istor. nauk; HUMOV9 M.D.v kand. ekon=. nauk;
KARMAYEV9 So% 9 kand, med, nauk; SMIRNOVAp N.S.v
doktor filolog.nauk; SILIGHENKOp H.S.9 doktor filolog. nauk;
YERZA-
KOVICH9 B.G.y kand. lakusetvavedcheakikh nauk,- RYBAKOVA, N.;
MUKETA-
ROV, A.I.; 'BOGATENKOVAj L.I.; MJWDAKBAYXVj B.; SIRANOV, K.S.;
SRVYD-
K09 Z.A.9 red.; HAHTSOVAt L.B.0 red.; ZLOBINt H.V.0 tekhn. red.
[The Soviet Kazakh Socialist Republic] Kazakhskaia Sovetskaia So-
tsialistichebkaia Respublika. Alma-Ata, Kazakhskoe gos. izd-vo
1960. 477 P. (MIRA. 3.4:6j
1, Akademiya nauk Kaz.SSR (for PaVgovg Pokrovskiy, Baishev)
2. Chlon-korrespondent Akademii nauk KazSSR (for Bykovj Smirnovap
S:Lllchenko)
(Kazakhstan)

VINNIGHENNDjA.V.,jinzh.; LEBEpLVA,, T.P.j
kand.tekhn.i~m&;-BELENOV, VA., inzh.;
KLIGKANI V.V., 19snd.tekhn.nauk
Tmproving the technology of classification yards.
Zheldor.transp.
44 no.306,41 Mr 162o (KTRA 110)
(Railroad"ump yards)

LEBEEEVA, T.F., kand.tokhn.nauk,;. BELENOVp V.X,t
lnzh.; SUKHANOVO A.N., inzh.
Yeohardze the car h ki RperationB in stations. Vast.
TSNII
MPS 20 n0-5245-47 062' WRA 1538)
.(Railroetda-Making up ~riins), (Railroads-Eleatronic
equipment)

UMOV, ?.P.; UMEEVA, T.P. - KORSH V.B. I "&V. V K PETRUNENKOV,
AJA.;
M 0 .
T;SUOV, L.B.; ASHIIM(aN, Al. inzn,~ reteenzu=,- Iwa, V'YUOP
jy~zh., red.; VOROTNIKOVA, L.F., telftorede
(Technological eqnipment of railroad stations] Tekhnichesk'oe
canashchinie stantaii, Moskva, Transibeidorisdat, 1963.
153 p$ (K= 16t6)
(Railroads--Stations)
(Railroads-Equipment and supplies)

LEbEDEVA, T.P.; STRAKOVSKIYt I.I.; TISHKOV, L.B.;
LOMAKINA, N.N.;
ZABELLO M.L.; SLDIKOV,'P.P.; PETRUNENKOV, A.Ye.; B
ARUTYUNOV, V.A., inzh.,, retsenzent; PETROVA, V.L.'
inzh.,, red.~;
BOBROVA, Ye.N., tekhn.;red.
(Basic requirements rel.ated to the technical
equipment of
classification yards]--.Osnovnye trebovaniia k
tekhnicheskoidu
osnashcheniiu sortirovpchnykh%stantsii. Moskva,
Transzheldorizdat
1963. 218 P. (Its TRUDY,.ho.270). - (MIRA 17:3~

4MM(
for- WW. 4.4-
21.
war bld m
CW-U&Pl B,
cWj AW.~ Nr
Cal .-V k tk hr rzactkms C4
dih bk aM (11) with
11 z4onaNT 1A e 11t0, UrAer N
Obly.krgnmso by addn..tj
maltit of me withurlabL-v i 4 1
tto ~ AM with mlie"t &&VItratku Wtzg
vot . at, -1 1 or "35Y sm anch tca!M. imentially n,,
-le"- 'PACC Wi ut ftch zddtnds, TN P=tble
I
rMamadt"s oaf ctloati In (lie system are dkcumd. It
ws3.#.hi2qm thut aqwhay1ttfits can be used to tnitixte the
p4ymarU;&tkte of butadkitti the %yum "ith U btliW the
moct c&*Ive a the two. , jStTo,-Jvt j)*Lymtd2AtkA acwvs
at- -164 -with Om% Wf~T %&1t; of
butadkze with PhM.Clilin etaukiom is Atia Indlucc4 well
A it PH a-It"Mth tran. tutc it VH T. lisW 1 In the Oldeln,
with cu,m%a as catub-su bOng WrAt tffectivi In bWlC
medlilml. U. : rmtlail= _. of ., polyw4dutim In 4queous
mauffts trAdu ftfimce d ral"dws S)ltcaus at tmms-
tuaris U04w wo &fx4 * "y Of mkmtmbus of polyme.
Chiba. 1W. 1257, 0 bowlifae
an hdilated by syitkrrt~ of- the' "W.Oan-tvducom type
with dihidmimMek meld, llhCv*!rsWlI ((xdU
b
mild, hr sr.4 064n MA c6r-.
OM=t was OA%'Pf- th,- mtbsimcr, hy,$vo~vqv
pezolldt chat d. ahbough

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with

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links). With
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criswilm iven In tho Un-
untdict! LaZ. G. -M. icosol4poff

_

KMBMCXFA# GA*j M=qMVJAO-L.M*
4
sopmum at OMMAGdonla (Mulga) hydmto frm rooto
Of Prenscs -- --------- ota at sebmi) Lug. &W. zbw.
prW, kldm- 38 m.5*114&aW NY 165. (HMA 28M)

MUMMA, G.A.; BEjEEO_yagAU-,-L.&.,,--
Chemical study of Prangos ornata Kuzm. roots. M-Im.
prirod. soed.
no.6:430 165. NIRA 19:1)
1. Botanicheakiy Ingtitut imeni Komarova AN SSSR.
Submitted July 5,
196i.
1 11 -

KUZNF,TSOVA, G.A.; BELENOVSKA2,r LSM. &---we
Furocoumarine obtained from the above the ground part of the
Prangoo f~dtschenkol (Rgl. et Schmal.) Eng. Kor. Zhur. prikl.
khim. 38 no. 10:2368-2369 0 165, (MIRA 18:12)
1. Botanicheskiy institut Imenj V.A.Komarova AN SSSR. Submitted
July 25, 1964.

ZAPOL'84~, N. V., kRndIdRt takhnicheskikh nank;
BXMOVSKff, P,N.,
Whener.
Results of laboratory investigation on the wear
resistance of
cast iron ship machinery parts, Trudy TSNIIRF
no.28:73-92 154.
(KLRk 9:1)
(Cast iron-Testing) (Kechanical wear)