SCIENTIFIC ABSTRACT BOYKO, A. N. - BOYKO, B. T.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000206630009-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 9, 2000
• Sequence Number: 9
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

GUSSAK, Venianin Borisovichi NASrROV,,
YaWyaAirsaidowicb;
SK#bRTSOV,Yuriy Aleksandrovieb;BMO, A.N.., red.;
SOHOKIIIA,
Z.I., tekhn. rea. ---------
[Soil formation on loess accumulations of various
ages and
the fertility of Sierozems] Pochvoobrazovanie na
lessovvkh
akkumuliatsiiakb raznogo,vozrasta i plodorodie
serozemove
Tasbkont, In-t pochvovedeniiat 1961. 159 P. (MIRA
15-.7)
02bekistan-Sierozem, soils)
(Uzbekistan-Loess)

L
511A- 65 Uff P4-;k/P_j'-4/M~o~ IJP(c BB/GG,
A?%=SST0_T_KP: APS015523 UR/0286/65/000/008/0064/00614
681.14
AUTHOR: Boyko, A. N. ; Sitnikov, L. S. 1, Utyakov, L. L.
JITLE: An adder. Class 42, No. 170202
Byalleten' hob"towly tovarnyRh maRov, no. Bo 1965, 611
tTOP1C-._TA0S:'-1ogic,,_6 d 5D 7,~
uter
A
This Author's Certificate introduces an adder which contains a chrono-
t-.~n, pulse shift logic circuits, flip-flops, "AND" or "OR" logical
elements. The
device is designed for improving the reliability of adders with
pulse-tiTre number
r~_ -res entat ion. The first logical shift circuit is connected to
the 1hrcn3tron
w'ier-_ the first addend is stored and to the first input of the
second logical shift
circuit, The first input of the first logical shift circuit is
connected to a
sour-ce which supplies a sequence of short trigger pulses. The second
input of the
first logical shift circuit is connected to the carry output F-)r the
preceding
digit. Tqe aec-and input of the second log-1cal shift circuit i~;
connected to the
cbrrnotron where the first addend ir. stored, while the output of this
circuit i5
Card -1A

.L 5114,14-465-
I-ACaSS101-1 ITR: AP5015523
connected Ito the -first input of the third logical shift circuit.
The second input
Df -he third logicai shift circullt is conne cted to the
chronotr,:~~n where the second
addend is ~~,tore,,I, the output of the third circuit is connected to
the unit input of
the first flip-i-Elop for. storage of the sun,~, and the neutral
input of this circuit
is connected to the ,ource o f short trigger pulses. The chronotrons
for storage
nF the fir.., a::-! sriccnj addends are connected to the first an-!
second inputs of
the "OR" gate nespectively. The output of thp "OR" gate is connected
to the 1~irst
iTiput of Ul~~- F~Arst "ANID" tg,~-t,. Tha second input of thp "MD"
gate is connected to
a sovirce of short pulses which are shifted with ref3pect to the
pedesall pul!ie
qu,,~nce by an inter,.,al whi-.1i corresponds to some number greater
thari the base cif
,numh,er system minus I and less -than the base of tbe number sys*em.
'7he
'the first "AND" gate is connectecl to the unit input of the first
f~',ip-f_ Lcj~,
i neutral input of this flip-flop is connected to a source of pulses
which a~~-
e,] by half a period. The flip-flop output is connected to the first
input oF *hP
vt M" oate which forms the carry. The second input of this gatp
conuiecr-~
Ai
source of un:t durai-lon pulsf~5. The pbase of thpse pulses
cnin.:id'~- wJtl~ ep'. 3 e
of the pedestal puLge sequence.
ASSOCIATION: Institut matcmatili SO Ali SSSR (Institute of
Mathematics,90 A14 SSSJR)
Card 2/4

L 5144-65
I -
i!ACCESSION NR: APS015523
i
!SUBMITTED: MecU ENCL: 01
I
In pxr sov: oDo OTHER:' 000
I
1. 1
SUB CODE: DP

7
5
ACCESSION NR: AP5015523 ENCLOSURE: 01
Pig. 1. 1--logical shift circuit; 2--short trigger
pulse sequence; 3--carry for previous digital place;
the f�rst addend is stored- _15--
7 4--chr-onotron,-,vhe.re_
input'for thefirst addend; 6--logical shift circuit; F,
7--chronotron where the second addend is stored;
8--input for the second addend; 9--logical shift cir-.
cuit; 10--sum flip-flop; 11--logical "OR" gate; 12--
logical "AND" gate; 13--sequence of pulses which are
shifted with respect to the pedestal pulses by an in-
terval greater than R-1 and less than R, where R is
the base of 'the nuriber system; 14--flip-flop;
pullse8 for meturn to -the initial state which are.--
sh.ifted-by half a period with respect to the peclestai
pulses; 16--"AND" gate; 17--pulse of' unit duratiOn
Uird
_777

LEV, Vasiliy Tarasovich; PAK., Susan; _BOYKOj A.Np red.;
SOROKINA, Z.I.,
tekhn* red.
[Practices in-obtaining high bast-fiber crops on the
Sverdlov CoUective Farm in the Verkbne-Chirchik District
of Tashkent Province] Opyt polucheniia vysokogo urozhaia
lubiarqkb kulltur v kolhoze im. Sverdlova Verkhne-
chirebikskogo ralona TashkentBkoi oblasti. Tashkents M-vo
sellskogo khoziaistva TJzSSR, 1962. 34 P. (MIRA 17:2)

KOLYAROVA; Lidiya Fedotovnap kand. sellkhoz. nauk; KANA6H, S.S.)
akademik, otv. red.j BQYKO,,..A.P., red.; SOROKINA,
Z.I.p tekhn. red*
[Cottonsee d pro6ction in the Uzbek S.S.R.) Semenovod-
stvo kblopchatmika v Uzbekskoi SSR. Tashkent, M-vo sell-
skogo khoz.UzSSR, 1962. 59 p. (MIH 17: 1)

ACCESSION NR: AP5010948 uR/o286/65/000/007/0131/013-0
AUTHOR: Boyko, A. 11. ; Sigorskiy, V. P. Sitni~ov, L. S. ; Utyakov,
L. L.
TITLE- Be rs-ible-counter. " Class 42, No. 169879
V
SOURCE: Byulleten' izobreteniy i tovaimykh znakov, no. 7, 1965,
131-132
TOPIC TAGS: re-versible counter, counter, pulse counter
ABSTRACT, The proposed rever'sibli counter utilizes a high-stability
pulse-phase
element. To improve stabilituy'- the counter is constructed as shown
in Fig. I of
Enclosure. Orig. art. has: I figure. U.,
ASSOCIAITIOU: Institut matematiki 50 Ali SSSR (Institute of
MathtmaticsA SO-
AN SSSR)
SUBINUTTED: o4jun64 ENCL: 01 SUB CODE' :EC
WO REP SOV: 000 OTHER: 000 ATID PRESS; 3239
1/2
77-

ACMSI ON INR AF50 1 ENCLOSURE: 01
4 5_
3 S 7
neirerslible,co-anter
I Direct-count Dulse source; 2reverse-
count pulse source; 3 - trigger; - AND
gate; -5 - shapers 6 - generator of high-
repetition pulses; 7 - wnticoincidence cir-
cuit; high-stability pulGe-phase element.
14rcrd V2

1"'UTFOis: 7~0:eko, A. N.; Porodeteldy, V4 Y.; 4~gq Sitnikovl_ L. S.;
MITLE: Sumator.,/Glass 42t No- 169687
SOURM.- Byul leten.11 izobre en V4,itov* W-kh =Akov,, no iT 1965 134
WFIG TAGS. au=ator
6ES517fUCT: This Author Certificate presents a sun~ator containing
chronotrons, logial,
IM" and "Oil" circuits, and a transfer shaper circuit. To sum numbero
the digital i
lol-rders of which are r6presented in the tine-pulse form with an
arbitrary numerical 1,
ibase, the chrenotron storing the digital order of the firot term is
connected to the,
ichronotron storing the second term and also to the 110IR11 circuit
su=inf- the lenC7th
'of the first term with the unit transfer length (see'Fig. I on the
Enclosure). T'he
loutput, of the "OR- circuit is connected to the "OR" circuit sunming
the lerk;tyl of
;,,he terms and transfer and to the "M" circuit separating the
difference of the sud,
iand the numerical base. The latter two circuits are also connected to
the Output of I
;the chronotron storing the second term. The output of the circuit
summing the
lieng-th of the terms and transfer is cormected to the logic trannfer
shaper circuit
land to the decoupling "OR" circuit whose second input is connected to
the "OD"
LCard_1A_.

----------
ACMSION M3 AP5610956 n
!circuit. The ohtput of the "OR" ciTcuit is comected to the
chronotron storing the
;sum. Orig. aTt. has; I diagram.
3 none
sum-na. i4.T=63 INOM ' 01 STJB CODE
REP SOVe-IODD OTHMs ODD

1301K0, A-. P. Eng.
IJSM (600)
Imbering - Carpathian Mountains.
7. Log-pulling by cable in the forests of the Carpathian Mountains.
Mekh. trud.
rab. 7, No. 2, 1953.
9. Monthly List of Russian Accessions Library of
May
Unclasslfied.,~

PLANSIN. oty.rod.; SLM, T.T.. rod.; SARAMI. ?.T.,
takhred.
[Pundamentals of the efficient organization of
lumbering]
09novy raistonallnogo postrognita prolsv9detv'Innogo
protsessa
lesorazrabotok. Isd-wo L'yovskogo univ., 1958. 124 p.
()aRA 12:1)
(Iminbering)

KORDYUM, Ya.L. [KordiumpIE.L.); BOYKQ A.P.
Embryology of Gerbera anandria Schultz. Dop. AN UIR-'R
no.8:1109-
IM 162. (MIRA 1822)
lo Institut botaniki AN UkrWRs

XK
Hydrodynamic forepasting~of,pr6niois _--ftOdb on-4--mein atwo~~-
spherip lev&2 for the,wbole globs,~ tild-
awount. Dok2, AN SSSR 153 no.6WO3-1)66'4~'43
i'4,"P, Vsl~..'- Ru 1l'1"'
Vychislitellnyk meteorologichqs~"e Predglta42iio
akademikm A.A. Dorodnitsynym.

BOY KO, A. P.
Forecast of the mean monthly values of the altitudes of the
500 mb. surface for the earth's northern hemisphere. Trudy
MMTS no.5:35-40 165. (1,(jRA 18:12)

~GW
FW7.(1)/FrX
ACCESS1 -N~- -AT4048452 B/3118/64/000/002/0033/0044
AUTHOR: Bovkb. A.P.
TITLE: Hydrodynamic long-range forecasting of -pressure fields for
the entire earth
with orography of the northern and southern hemispheres taken into
account
SOURCE: Mirovoy meteorologicheskiy tsentr. Trudy*, no. 2, 1964.
Voprosy* gidrodin-
amicheskogo dolgosrochnogo prognoza pogody* (Problems of hydrodynamic
long-range
weather forecasting), 33-44
TOPIC TAGS: long-range weather forecasting, weather forecastin
ydrodynamic
weather forecasting, atmospheric pressure field
ABSTRACT: This article describer, a new method for long-range
hydrodynamic forecasting
of the pressure field at the mean level of the atmosphere and gives
examples of the use
of this method in worldwide forecasts; the paper was presented at the
Vsesoyuzny*y
nauchnoy konferentsi! po dolgosrochn3f*m prognozam pogody* (All-Union
Scientific
Conference on Long-Range Weather Forecasting), 20 March 1963. rhe
point of depart-are
in a forecast for the entire earth is a nonlinear vorticity transport
equation for the rinean
level and a linearized balance equation. Ile problem is broken down
into three parts:
Card 1/9

L16612-65
ACCESSION NR: AT4048452
a. determination of the stream function field fo.- an initial time on
the basis of the
known initial distribution of heights 11 of the 500-mb surface; b.
forecastingof the
stream function for some moment of time; and determination of H from
the predicted
values of the stream function. 'Ae solution of each part of this
problem is presented.
The author presents an example of such a world forecast of the
pressure field. Initial
data were AT500 charts for 0300 Moscow time on 20 July 1962 (Fig. I
of Lhe Enclosure),
predicted chaxts are shown in Fig. 2 of the' Enclosure; actual
pressure fields are shown iv
Fig. 3 of the Enclosure. On these charts B ~ highs and 11 z lows
Comparison of these
predicted charls with charts computed using Influence functions
reveals that when
trigonometric polynomials are used the forecast is better than when
influence functions
are used and computation of trigonometric polynomials on an
electronic computer is
faster. "In conclusion, the author expresses appreciation to Ye-_N.
Blinova,
Corresponding Member of the SSSR Academy of Sciences. for formulating
the problem and
valuable advice." Orig. art. has: 49 fcrmWas and 3 figures
ASSOCIATION- Mirovoy moteorologicheskiy tsentr
CoM 2/9

L 16612-65
ACCESSION NR-. AT4048452
SUBMITTED: 00 ENCL. o6
4.40 REIF SM. 002 OTHER: 002
Card,
SUB COT)f.:: Es

BOYKOj A.P.., inzh,; ERTJK, M.T., inzh,
Adjustment .of a gas combustion process in a boiler with turbulent
burners. Elek. sta. 34 no.5.,16-19 My 163. (MMA 16--7)
(Boilers)

YANKO, F.I., inzh.,- STEPANOV, L.A.. inzh.;_BO);%
Inzh.
. - ,
. Washing of regenerative air heaters of boilers
operating on sulfur
containing mazut. Energetik 12 no.3i12-13 Mr
164.~(MIRA 17:4)

USSR/Cti-lt-ivated Plants. Decorative Plant-s. Idd
Abs Joua? : Rof Zhir,7-Biol., No 157 19507 68424
kut.hor : :Kdstryukova, K.
Inst :Iciev University.
Title :Obser",tions on tha Filowerins of the
Striped Hippeastrwa (Hippecistrun
vitta-ttva Hcrb.
Orig Pub :Nauk.. zap. IUyvslk. un-t, 1957, 16, iTo 1,
13-21
Ii.bstract:In a totc-a number of 35 seedlings, t1ic cha-
ractoristics of Darent-nl form ware found
in only two Hippeastrum vittatLuii seedlings-,
the remaininc, seedlings differed greatly
from tho -na-rental form. Subs equentlN7 , fiVe
.Loprois -i~,,ere isolated which differ fropa the
Card 1/2
209

USSR/Cultivated Plants. Docorativo Plants.
Abs Jou:, z Ref" Zhu-.-?-Bjolj7 No 15, 1956i 68424
parental form of Hippoastrum vittatum
in both Dattern and the coloring of the
0
blossoms. These forms can roproducQ both
vegetatively anO from seed.
Card 2/2

ACC NRi -,NP6036826 CODE 1~ UR/0021/66/000/011/1416/1417
AUTHOR: Kostets'kyy, B. I., Ivzhe nko, I. F.; Boyko, A. S.
ORG: Institute of Civil Aviation Engineers. (Inatftut inzhencriv
Ts~vil'noyt'aviatslji)
ITITLE: Diffusion phenomena in plastic deformation of friction
surfaces
SOURCE: AN UkrSSR- Dopovidi, no. 11, 1966, 1416-1417
TOPIC TAGS: metal diffusioni metal plastic deformation, metal
friction, friction
surface, friction surface deformation
ABSTRACT: The chemical composition of the surface layer of an L62
brass specimens
subjected to friction tests in couple with heat-treated SbKhl5 steel
specimens has
een studied. It was found that plastic deformation of brass induced
by friction
b
was accompanied by a diffusion of the greater mobility component, in
this case zinc,
to the friction surface. The depth of the diffusion-affected zone
and the degree
of heterogeneity depended on the specific stress and the rate of
relative motion.
The maximum concentration of zinc was found to be at the surface of
the specimen
(see Fig. 1). Orig. art. has: 1 figure.
1 Card' 1/2

kii6036826
Fig. 1.- Variation of zinc content along the
depth of diffusion zone
1 - Relative displacement velocity 0.003 m/sec,
A4
surface layer temperature 20C, specific loads
2
0.40 n/m ; 2 - same but a specific load of
0.20 n/02; 3 - relative displacement velocity
5 m/sec, surface layer temperature 150C,
specific load 0.001 n/m2; 4 initial speci-
men
20
SUB CODE: 11,2-(>1 SUBM DATE: O3D*c65/ ~ORIG REF 007/ OTH REF: 003/
Card 2/2

t6Mq,A, T,
Automobile,Industr,,, and Trade - Yoscow
Practices in economizing electric energy at the 1. V. Stalin
Automobile Plant.
Prom. energ. 9,, No. 1952.
-2
June 1953; Uncl.

BOYED, A.T
Art If to Ial Insemination In controlling trichomonlasis In cattle.
Veterinarlia 35 no.3:62-64 Mr 158. (MMA 11:3)
1. Glavw velvisch Kirovogradekogo Sakhavoklotresta Ukrainskoy
SSR.
(Trichosonisais) (Artificial Insemination)

.................

POYK(), A. V.
BMO, A. V. -- "The Effect of Cutting Drains on the Water
Economy and
Physicochemical Properties of Soil and the Growth of Plants in
Cranberry-Mossy and Pteridium-Fern Pine Forests." Acad Sci
Belorus-
sian SSR. Inst of Socialist Agriculture. Yinsk, 1QI~5.
(Dissertation
for the Degree of Candidate in Agricultural Sciences
SO: Knizhnaya Letopist, No 1, 19,56

XOSTSTURVICH. N.I. [Kastsiukevich, N.I.], kand.sel'skokhousystvennvkh
nauk; BOYM, Aj. [Boika, A.V.], kqnd.se1'skokhozyayvtveAnykh nauk
Effect of improve'sent cuttings on the gross productivity of.pine
plantations. Vests, AN BSSR. Ser. blial. nav. no.4:37-44 '57.
(MIRA 11:6)
(FOREST MANAG109f) (PIIm)

124 -57-2-254 3
Translation from: Referativnyy zhurnal, Mekhanika, 1957, Nr 2, p 145
(USSR)
AUTHORS: Boyko, B~ B u k in, S. 1.
TITLE: Establishment of the Value of a Band in Optically Sensitive
materials During Plastic Deformation (Opredeleniye tseny
polosy opticheski chuvstvitell nykh materialov pri ikh plastiche-
skoy deformatsii)
PERIODICAL: Sb. nauch. tr. Fiz. -tekhn. in-ta AN BSSR, 1955, Nr 2,
pp 54-65
ABSTRACT: Examination of the construction of a "band-width versus
maxi-
mal tangential stress" relationship for optically sensitive mate-
rials during plastic deformation. The authors apply plane con-
centric torsion to accomplish this. Two concentric rings are
provided, of which the outer one is fixed,* while the inner one
is capable of rotation at a given angular velocity. The annu-
lar gap between the -two rings is filled with a material to ~be
investigated; after pouring the material is allowed to cool
until it adheres firmly to the lateral surfaces of the rings.
Card 1/2 Rotation of the inner ring then sets up a pure shear strain
in

124-57-2-2543
Establishment of the Value of a Band (cont.
the specimen. The quantitative results were evaluated in terms of the
bands
and the wave length of the light (the light source was an Hg lamp
with a wave
length ;~ = 5770/90A). It is noted that the extent to which the
specimen mate-
rial becomes doub *le-refracting, in the material investigated, was
proportion-
al to the values of th~ maximal tangential stresses for the stress
interval
from 0 to 26 kg/cm (at still higher stresses the specimens
disintegrated).
From the linear relationship obtained it follows that the value of a
band in the
material is constant for the maximum tangential- stress range
investigated.
Inasmuch as this conclusion is founded on concentric torsion, which
is charac-
terized by an absence of hydrostatic pressure throughout the
specimen, the
author further investigated the effect of hydrostatic pressure on the
value of
a band (this problem is experimentally solved by extruding the
specimen
through~& -square opening in a draw plate) and show that the value of
a band
in the material does not depend on the hydrostatic pressure.
177 Optical materials--Plasticity 2. Optical materials V. P. Netrebko
--Stresses 3. Mercury lamps--Performance 4. Light--Refractive
properties
Card 2/2

AXIMOVA, K.I.; BAZRXNOV, M.F.; BAKHVALOV, G.T.; BEZKUJB3NKO,
N.P.; BERMAN,S.I.;
,. _VJNOGRADOV, S.V.;
BOGDANOV, Te.S.; BODTAKO, M.N., BOTKO B B
GAGU-TORY, X.V.; GLEX, '%p - G";*RADUSOV, P.I.; GUSHCHINA,T.N.;
YMLITANbV, A.K.; TZSIZDT M.P.- ZDZTARSKIT, A.V.; ZAKHAHOV, N.V.--
ZAKHAROTA, M.I.: IARCHEVSift, V.I.; KOKAROV, A.M.; IX)RZMMKO.
0.T.:,
LAMM , V.I.; KALITSIT, M.V.; MILLER, L.Te.; MILOVANOV, A.I.;
MIRONOV, B.S.; NIKONOROVA , N.A.; OLIKHOV, N.P.: OSIPOVA, T.V.-,
OBOXIN, N.Te.; PERLIN, I.L.; PLANSIN, I.N.: I!ROKCtP'YL7, A.D.;
RMANTM, H.V.; SIVERMED, V.P.; SIMIN, P,'I.; SMIRTAGIN. A.P.;
SPABSKIY, A.G.; TITOV, P.S.; TURKOVSKATA, A.V.; SHAKHNAZAROV,
A.K.;
SHPICHrmsiry, U.S.; TURISHTOVICH, N.A.; YUSHKOV, A.V.;
YANUSMff ICH, L.V.
Sergei Ivanovich Gubk1n. TSvet.met. 28 no.6:6o-61 N-D 155. (MIRA
loal)
(Gubkin, Sergei Ivanovich, 1898-1955)

,Call Kr: TA 406.G83
AUTHORS: Gubk~n, S.I. (deceased)$ Dobrovollakly, S.I.,
Boyko, B. B.
TITLE: Photopla8ticity (rotoplastichnost')
pUB. DATA: Izdatel'stvo Akedemii nauk Belorusekoy SSR,Minsk, 195T,
164 pp. 4,000 copies
ORIG. AGENCY: Akademiya nauk USSR. Fiziko-Tekhnicheakiy InstItut
EDITOR: Gorev, K.V. Academician, Academy ofSoiences, BSSRj
Ed. of Publ..House: Kholyavskiy, S.; Tech-Rd.:
Aleksandrovich, Mi.
PURPOSE: This monograph is intended for enWeers and scientific
workers familiar with the methods of photoolesticity.
COVERAGE: The monograph,describes the fundepentals of a new ex-
perimental method for Investigation of plastic deforma-
tion processes-and states of stress. This consists of
passing polarized light through optically sensitive
materials which are subjected to residual deformation.
This method Is called photoplasticity by its authors.
Card 1/ 6

Photoplasticity (fotoplastichnost') (cont) Call Nr: TA
406.G83
The results of this work may be applied to modeling (I.e.,
model testing,,,etc.) various plastic deformation processes.
The origin of the present volume Is described in the
foreword
as follows: "One of the co-authors of this monograph, S.I.
Gubkin, organized a laboratory in 1949 at the
Physico-Technical
Institute of the Belorussian Academy of Sciences to develop
the
photoplasticity method. Initial investigations in this labo-
ratory were conducted by S.I. Gubkin and S.I. Dobrovollskiy.
Some results1of these inveqtigations were published in
Doklady
AN SSR in 1959 and 1953. B.B. Boyko joined the laboratory in
1952. By the end of 1954'the investigations carried out by
the laboratory provided a preliminary solution to one of the
basic problems of photoplasticity namely, determination of
the
stress condition using the methoaof pho'toplasticity under
conditions of a viscous flow. With the solution of this
problem which revealed the basic characteristics of the
method,
we can now consider photoplasticity acceptable as an inde-
pendent method of research. In order to accelerate the re-
finement and introduce this useful method, the Scientific
Council of the Physico-Technical Institute of the Belo-
russian Academy of Sciences recommended that the laboratory
publish a pertinent~monograph. This volume generalizes
Card 2/6

Photoplasticity (cont)
Call Nr: TA 4o6.G83
the results of these investigations as carried out at the
Physico-Technical Institute of the Belorussian Academy of
.Science under the supervision and with the participation of
Academician 3.1. Gubkin. The task of preparing the monograph for
publication was apportioned as follows: S.I. Gubkin drew up the
plan and prepared the first and sixth chapters for printing and
also did the general editing; B.B. Boyko prepared the fourth
chapter for printing and also the second paragraph of the fifth
chapter; S.I. Dobravollakly prepared the second and third
chapters
and the first and third paragraphs of the fifth chapter." All
problems of modeling plastic deformation processes whezethe
photo-
plasticity method is used can be subdivided into two groups:
1) Analysis of stress distribution in plastically deformed
bodies, and
2) Study of physical phenomena during plastic flow (such as
the mechanics of flow and destruction, the nature of
residual stresses, the nature of material fatigue,
relaxation, creep, elastic after-effects, contact friction,
etc.)
Card 3A

Call Nr: TA 06.03

Photopla
sticity (cont)

TABLE OF CONTENTS

Page
Foreword

5
Ch. I
Nethod of PhotoplasticIty
7
1.
Photoelasticity
7
2.
Necessity of creating an experimental method for

studying
state of stress during plastic deformation
11
3--
~Classification of rheologic behavior of solid bodies
14
4.
Principal tasks of photoplasticity
23
5.
Fundamental features
of the photoplasticity method
27
Ch. II.
Naterials Used in the
Photoplasticity Nethod
30
1.
Requirements Imposed on materials
by the

.
photoelastici.ty method
30
2.
Requirements Imposed on
materials-by the

photoplasticity method
31
3.
Classification of
materials
33
11
Effect of the'na'ture of the deformed material

on stress distribution characteristics
45
Card 4/6

Call Nr: TA 406.G83

Photoplasticity (cont)

Ch. III.
Special
Techniques of the Experiment
49
1.
Optical installation and-devices
49
2.
Preparation and processing of models
52
3.
Techniques for the
experluent
59
4.
Photographing the Isochromatic and isoclinal lines
61
Ch. IV.
The Viscous Problem in Photoplasticity
63
1.
Viscous flow
63
2.
Optical anisotropy under viscous flow conditions
70
3.
Some
specia 1 'features in modeling a plane problem

under viscous flow
conditions
85
4.
simplest plane problems of viscous flow
91
5.
Peculiarities of the state of stress on the contour

of a model
and some ways of processing experimental

data
log
Ch. V.
Modeling
Pressure-forming Processes
113
1.
Stamping
113
2.
Extrusion
133
3.
Punch
Impression (Piercing)
142
Card 5/6

Call Nr: TA 406.G83
Photoplasticity (cont)
Ch; VI. Practical Significance and Prospects for the
Photopl6sticity Method 154
1. Practical significance of the photoplasticity method 1 4
2. Prospectd for the photoplasticity method 1~9'
BIBLIOGRAPHY 163
AVAILABLE: Library of Cot*ress
Card 6/6

BOYICO, B.B.
"Obtaining Specimens of Silver Chloride with a Finegrained Structure
by Mleans
of Cyclical Deformation"
ftornik nauclinykii trudov, vjj). IV, Minrk, IA-vo-Au BSBR, 1956,
261P.

BOTKO, B.B..
Preparing fine-grained silver chloride "cimns by cyclic
deformationse Sbornauch.trade Flso-tekk4inst. AN BSSR
no.4:229-240 158. (MIRA 11:11)
(alver, chloride--YAtallography)

BOTKO, B. B.
Forced optical anisotropy in the flow of amorphous media.
DOkl.
AN BSSR 4 no.6:332-336 Ag 160. (HIM 1398)
1. Institut fiziki All BSSR. Predstavleno akad. AN BSSR B.I.
Stepanovym.
(Anisotropy) (Deformations (Mechanics))

-t -4-70 A C- - - jZM
00
k-Y4 ft-t ~,,. 4~
A.,
AUTHOR.. Petrov, N. Z.; Roykzo, B. B.
TYME: On generation in a laser with external mirrors
SUJRCF: Drarnal ~-,,r-lldadnoy speldroskopii, v. 2, no. 1,
TOPIC D-10-3: laser, laser ndirTor system, laser action, lptl-mm
1F-LsAl,.j conr-
_~j 4',j -:~y_
ABSTRACT: in view of the possibility of lDterference effects In a
jagel. N
-~crnall ;-id-rors, c:ne to the high morochromatielty of the laser
thors cb;-alnefl a re--ui,-,r solution of Mi-rvell's enuations for
41hE lascr :r,
r ~hc t'hat diffraction effects can be negiec! ed. it s h-ri'
P- f-reaL-uf&,;y cci~;e.;pon,diii_r tc --ptizal laslfn-~,
condtio--- it
laser generation frequenries and that at this 1rt1qu-ijCY f-,
_.r, -n~ a7- closer to %aximall 4 han to va`,,,er Vh oF-
A- Lc3r of
at. an arv-,'e to the - is of the red is --n P~
ax --n
Tr u Q of t h egy Et en, i + s t hn t
ai riec. for ffe -ent W1 c S , but at f:- -,3
"In co-ic I us 1--n iE
I.o a d,~vendsnce of thi, fie-,-.:ency on the P~.ngle.
1/2

B. 1. ISA
p~ ~av and B. A.
13 fcnml~as a
ASSOCLITIOR: Nscne
e a userial c gc!u siciii of the remdtt
FINC L 00
3UP. COM Ir

L 5413-66. EWA(k)/FBD/44T(1)/
-~;Ep(k)-2/T/PIP(k)/EWA(m)-2/&A(h) S Wa
F/O P3 4 / 0'2
ACCESSION NR: .AP.5029990 UR/0368/65/003/00 J? C17
621.375.9 : 535.89
qq .7
AUTHOR: Boyko, B. B. V. Vashkevich, I. MYY
Petrov,-.N..S.; Valyavk
.~TITLE.. Plane parallel plates -as 'laser re
flectors
SOURCE: Zhurnal prikladnoy,~spektroskopii, v. 3, no. 3,J1965, 234-237-
TOPICTAGS: Iaser$ ruby laser, resonator, geometric optics, laser
pumpings
reflecti6n co'efficient -
'ABSTRACT: The~assump*tion that near-maximum reflection coefficients
occur in ex-
periments with laser reflection systems-is directly.verified. A
simple method is
used: reflectors with well-kno~m reflection coefficients are replaced
by the test
'plates and the operation.of theJaser in the first configuration is
compared with
~that in the second-. The ruby crystal used was a rod 120 mm long and
12 mm in dia-
meter and had matte-lateral surfaces., An IrP-2000 lamp,was used for
excitation.
According to the experimental methodology, one reflector was used,
consisting of a
dielectric mirror having a reflection coefficient very close to unity.
!In this case the reflection at the other end is determined purely by
the.Fresnel
ACard 1/2
69-610 636

L: 5413-66
iACCESSION NR: AP5025090-
:coefficient, which is,0.076 at a wavelength of 6943
Next,.two identical plane
'parallel reflectors-were selected-:such that the same threshold
pumping energy was
mrequired. :These quartz platesp were~10 mm thick, flat to within 0.1
k, parallel
to within 1.511 and.formed a configuration equivalent to one with a
single ideal
imirror with respect to the threshold pumping energy. In all of the
numerous experkee
Tnents, both with a single mirror and with the plates, generation
occurred at a.
threshold energy of 2070 joules and was absent at 2010 joules; losses
were there-
fore'assumed to be identical. it is shown, in approximation, that the
calculated
reflection of 27.6% is close to the maximum of 33.2%, and closer
approach to abso-
lute maximum can be achieved with thicker plates.. Tests were also
made.with glass
plates, the outer surfaces (away.from the ruby) of which,were spoiled
by a special..~~
coating. The threshold ing-energy was only 3% greater than for the
previous
pW1V
case. Here too the reflection coefficient was very close to maximum.
Uncoated
i-plane-parallel glass plates, it "Jound, can pr~ovideveflectivity of
30 to 50% in
~,lasers. Amons~other advantagess such,plates are stable and reliable
and provide.
I
laser tuning capabilities. -The'authors.acknowledge discussions with
B. A. Cotskiy,
A. M. Goncharenko and F.-I. Fedorov, Orig. art. has: I figure. (14]~q~
ASSOCIATION:. nongr
P
SUBMITTED: 25Dec64 ENCL: 00 SUB CODE: C~o
SOY: 003 OTHER: OW ATD PRE
2

.ACC NRi AP7004142 SOURCE CODE: UR/0051/67/022/001/OW/OiLZ
AUTHOR: 11 Boyko) B. B.; Fetrovj N. B.; Va1YaVXoj1 V, V,;
Y4BbkeV1Cbp I* M.
ORG: none
TITLE: Prism reflectors to reduce loser beam divergence
SOURCE: Optika i spektroskopiya, v. 22, no. 1,, 1.967.. u9-i22
TOPIC TAOS: laser beam.. beam focusing, solid state, 3jLser# laser
output, optic
prism, light reflection
The discussed prism reflectors make use'of total internal
reflection near
the limiting angle. The advantages claimed .over right-angle total
internal reflec-
tion prisms are that their efficiency does not depend on the cavity
length and that,
they produce less noise, luminescence, or various parasitic modes.
Tnsts made by
the authors have shown a rhomboidal prism with acute angle equal to
the limiting
angle to be the most effective with respect to reducing beam
divergence. These
prisms were also compared in the experiments with the.prisms
t~escribed by J. A.
Giordmaine and W. Kaiser (J. Appl..Phys. v. 35Y 3446s 1964) (both
types of prism
were made of fused quartz). The rhomboidal prism with limiting
angle 43o24,10":t 02'
proved most effective for a ruby laser (120 x 12 M with ground
lateral surface)
operating at about 3 times the threshold. The generation of
inclined rays rather
than those of the desired beam is suppressed in such prisms by the
strong dependence
UDC: 621-~75-9: 535

ACC NR, Ap7oo4142
of the*reflection coefficient on the incidence angle of the beam.
Peplacement of
Ahe ordinary cavity mirrors vith rhomboidal prisms in.mutually
crossed position
reduced the beam diameter by about one-halfp vhereas 9, right prism
produced prac-
tically no reduction in the beam diameter. Although,the use of the
rhomboidal
prisms caused some reduction in the absolute value 'of the generated
energy, the
energy density increased by approximately 3 times."It is concluded
that the use of
i
rhomboidal prisms to decrease the angular divergenc !e.can be used
in various solid-
state lasers. Orig. art. has: 4 figures* (021
SUB CME: 20/ S(W DATE-.'- 12,Aa5/ ORIGI MW." 001/ OTR UPI 003
ATD PRESS: 5115
2/2
Card

AUTHOR:
TITLE:
Boyko, 13. F.. 76-1-5/32
The Determination of the Chemical Composition of FiDeIY-
-Dispersed Solid Phases in Multicomponent Syste::-,s 'by Means
of the Indifferent Component ,.ethod (Opredeleniye
khimicheskoGo sostava tonl:odispersnykh tverdykh faz v
mnogokomponentnykh sistemakh po motodu indifferentnooo
komponenta)
PERIODICAL: Zhurnal Fizicheskoy Xhimii, 1955, Vol. 32, lir 1, PP- 35-42
(USSR)
ABSTRACT: At first the motivation as well as the characteristics of
the method of indifferent components is given. Tl:.e method
for the arrangement of the phase diagram for :-:.ulti-component
systems with 4, 5, 6 and 7 components is shown. By means of
an example of the Fe203-H2O - NaCl - CaC12 system with a
solid phase (Fe203 - H20) the author shows that in the
presence of several componciizz in a system, which can be
absorbed by the solid phase, the positive adsorption of one
of these causes a negative adsorption of the other compononts.
0
Thus calcium chloride displaces aodium chloride fro-m the
Card 113 adsorption layer in t'his system and forns its adsorption

The Dotet,.-..iination of the Chemical Composition o. I - 76-1
Pinely -5/32
-Dispersed ~Olid Phases in Multicomponent Syster.-is by Means of
thn
Indifferent Component Method
layer .,iith.boundary concentration on the surface of the
sol-*Ld phase. The intensity of practical boundary adsorption
of CaC12 is equal to 3,9%. The author shows that sodium
chloride has ne-antive adsorption and th~;t it amounts to
2,ol%. With the investigation of the ternary system P0203
H20 - NaCl with the same solid plinue sodium chloride was
adsorbed more poritively. The ariount of adsorption was 0,8851.
It is obvious that the no.-ative adsorption of sodian
chloride developed because of its displacement from the
adsorption layer b-j potassium chloride. The author points
to the incorrectness of the final conclusions in reference
3 of Danillchenko and Frid-man, as thea are based on a
diagram which in reality was not obtained when investigating
the Fe20 3 - H 0 - NaCl - CaC12 system. The composition of
the investiCafed solid phase calculated accordin& to
reference 1 -Droves the result obtained the graphical way.
Thus the investigation of the Fe203 - H20 - 1',--C1 - CaC12
system shows that the mTthol of the indifferent comDonent
Card 2/3 can be used successfully in the determination of the

The De'termination of the Chemical Composition of FUely- 76-1-5/32
-mapersed Solid Phases in Idulticomponent. Sycte.-_ by Means
of the Indifferent Component Method
fine-disperse solid phase in multi-component systems. This
especially where other methods of analjois fail. The
advantage of this method furthermore consists of the +'act
that it does not call for special equipment or expensive
reagents. There are 6 fiGures, 2 tables, and 8 references,
7 of which are Slavic.
ASSOCIATION: Kuban Institute of AGriculture, Krasnodar
(Xubanskiy sellskokhozyaystvennyy institut, Krasnodar)
SUBMITTED: July 31, 1956
AVAILABLE-. Library of Conareas
Card 3/3

SKOROKHODOV, A.N.; TARNOVSKLY, I.Ya.; BOYKO, B.M.
Investigating contact stresses during tPx rolling of complex
shapes, Izv,vys,uchebozav.; cherne met, 8 no-4:112-116 165.
(MI.,U 1834)
I.- Urallskiy politekhnicheskiy institut..

258:14
S/142/6o/oO3/oo6/oo4/oi6
E033/EI35
AUTHORS: Boykot B.P., Minakovat I.Is, and Savellyeva, Z.1.
TIT19:t Synchronisatlon of a reflex klystvon loaded by a
resonator
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy,
Radiotekhn:Lkat.1960, Vol.3, No.6, PP. 581-591
TEXT: After brief mention of previous investigations, the
author considers the theory of synchronisation, by an external
sinusoidal e.m.f., of an oscillator having two degrees of freedom,
i.e. of a reflex klystron inductively coupled to an azixiliary
loading resonator. The external e.m.f. is connected in series with"lle
the loading circuit. Letting the voltages on the oscillator
circuit capacity and on the loading circuit capacity be x and y
respectively, then In d soft regime with symmetrical valve
characteristics, the equations of the system in the dimensionless
form are:
g2 2
x + x 2c (I x x a y i
2 E sin r,
y + y )y _2cly al x + 1 0
Card 1/ 8

25814
Synchronislation of a reflex klystron... S/142/60/003/006/oo4/oi6
E033/EI35-
where: Il are the ratios of the partial frequencies of the
circuits to the frequency of the external e.m.f; c*-O 0 is the
dimensionless increment of the oscillator circuit; e1 > 0 is the
dimensionless decrement of the auxiliary circuit; a, al are'the
coupling coefficients between the circuits. The solution of Eq.(l)
for detuning slightly greater than the synchronisation band is
sought in the form x = A sin(z
y = B sin(T V)
The case when and a = al is considered and the equation
for the family of amplitude curves is:
2c CE2 *-92+-& 2 Be ea2 + a4 - 8M2
Z3 _ z 2 8 1 + z 16 1
C(ci2+ 2 C2 C2(Cl2 + 2
CL2 Eo2 0 (3)
2 2 2
Card 2/8

25814 -
Synchronisation of a reflex klystron ... S/142/6o/oo3/oo6/oo4/ol6
E033/E135
where: z=A2 and I- J2002(l -g) =2&.
Since the general expressions for the boundaries of the regions of
stability ore very unwieldy, only the particular case of a fixed
ratio cillej = 1/2 (which in often approximately true in
practice) in considered. Then the conditions for.stability are:
z
3 2 16 2 4R2) 16 &22 _ 4112 4 -;;0 0;
(2) z 2z + (I T A2 + T z+ --73 5
(3) z5 + 4 2 22 Zli + ~26 2 56 2 181, Z3 +
0 q --3 9 02 -9 1 + -9 ) -V/
+ IL024 A 2 + 256 212 + 92 R2 80 z 2+ (4)
9 2 -9 2
+ (.1280 2 512 22"2 64 12 +.16 z + 2 +
62 79- 52 &2
--9 9 9
+ a56 2R2 16 2 22
9 42 1 + 9 'PO 0;
'Card 3/ 8

25834
Synchronisation of a reflex klystron s/i42/6o/oO3/oo6/oo4/ol6
E033/EI35
(4) (12 &22 + 3) z 2 + 64 &22 + 8n 2 16 z + 64 24 +
2 2 2
+ (80 321 ) &2 + 4(1 2) > 0. (4)
where: &.2 = &2/46, 2 ?1 2 =Ot2/4E12 E0 2/4c12 p2.
Thefamily of amplitude curves z = f(& 2) for fixed external
e.m.f. and inter-circuit coupling values are plotted and the
instability regions found (as shown in the figures which are
reproduced in the paper). When q2 > I and the equality of the
partial frequencies of the circuits does not depend on the
coupling, then the first condition of stability can be written
uo
z
- 2
where u 4(.1 - 'I).
0 lei
When 112 1 then the first condition for stability is:
VO
Z
Card 4/8

25814 -
Synchron1sation of a reflex klystron ... S/l42/60/003/oo6/oo4/ol6
E033/El35
where v 2 cl,
0 791,
The significance of Eq.(4) is discussed. By substituting
Z = U0 = 4(1 - L-) in Eq.(3), the depeldence of the absolute value
let
of the synchronisation bandwidth on the external e.m.f. amplitude
and on the coupling to obtatnedl
&2 2 AP
o2
and
+ (6)
2 max 2 2
JAI Ak
A 0
02 2 02
where Ao2 4/u-.- = the amplitude of the oscillations of an
autonomous system with two degrees of freedom. The synchronisation
bandwidths of oscillators with one and two degrees of freedom are
then compared. It is shown that with coupling greater than critical
Card 5/8

25824
Synchronization of a reflex klystron ... S/142/60/003/oo6/oo4/oi6
E033/EI35
and with small external amplitudes, the synchronisation band
divides into two bands which merge into one when the coupling is
reduced or when the synchronising amplitude is increased. This
bandwidth is substantially wider than the synchronisation
bandwidth
of an oscillator with only one degree of freedom. The
synchronisa-
tion of a centimetric reflex klystron oscillator with an
auxiliary
resonator, consisting of a standard waveguide closed at one end
by
a piston and at the other by a diaphragm with a rectangular slot,
was investigated experimentally. The experimental layout is shown
in Fig-5. The following were investigateds 1) the dependence of
the power of the synchronized oscillations on the detuning, with
fixed coupling between the oscillator and the external resonator
and with different synchronizing powers; 2) the dependence of the
power of the synchronized oscillations on the detuning', with
constant synchronizing power and variable couplingi 3) the
dependence of the synchronization bandwidth on the ratio of the
synchronizing power and the power of the synchronised klystron,
both with and without the auxiliary resonator. The theoretical
and experimental results agreed qualitatively and the data show
that.-by using the auxiliary resonator, a considerable increase
Card 6/ 8

A

CHEREPANOV, A.A.
Synchronization by a *O-eide signal from a 600 Not klystron
and an
800 kc,, L-C-oiciUatore'V~it.Hook.uneSer.3i
Fiz.,astroii.l8so.lt5j-5j
(MIRA-26SO
1. Rafedra teorii kelebanly Moskovskogo universitsta,
(Oacillatorat Electric) (Mystrous)

-,- _i

L 17342_6-_~ FEC`b)_2/~- A t, _4ZP
ACMSSICN NP : AR5009712
SOURCE: Ref. zh. Fizika~ Abs. 2Zh187
AUMOR: -Bcrvko, - B. P.
TnU: S~mcbrvaizaticn of 3-cm-reflex klystrm with nenlinear
reactanm at the
thix-d undertcne
P17M - SOURCE: Sb.- Itog-. naud1m Oxentsiy~L_ Yazandk. un-ta
za.19652
Yeian M-t v963,s 69-71
TOP14C-TA-GS: reflex klysL-ani- synchronizations ncnlinear
reactance, non-
linear capacitance, frequency looldng- paremtric diode
TRANSLATIM: Results are presented of an experimntal
investigation of tl-e syn-
chrxmizaticn of a 3-cm klystcn oscillator, the r-escnatcr
system of which iro-,ludes
a ncnlinear capacitance, by wans of a signal in the 10-m band.
It is indicated
that the s3mchrcnizaticn of the klys tra is due to the presence
of tk~e rmlinear
capacktanoes on which a hanmmic of the! locked-in signal is
produced. It is nated
that the influenc-n of the exter-aal reactance of pararetric
diodes used for syn-
lchrcnizaticn purposes is smEL11 and be mm-4fest cnly at large
anplitudes and for

~-, I Card 2/2 a q ... . . - . I
. 11 ~11 -' -

BOYKO B P~
Synchronization of a reflecting clystron loaded
with a
resonator having a nonlinear p-n junction
capacitance at
the third harmonic. Vest. Mosk. un. Ser. 3: Fiz.,
astron.
20 no.5:64-73 S-0 165. (MIRA 18:11)
1. Kafedra. teorii kolebaniy Moskovokogo
universiteta.
Submitted May 23, 1964.

BOYKO, B.T., Cand Tech lei -- (diss) "Study of the
processes or "If a supersaturated
CcAa solution in fine films of Al-Ou alloys-"
Khartkov, 1958, 15 pp (Min of Higher Lducation UkSSR.
Kharikovrpolytechnic Inst im V.I. Lenin) 150 coTAes
(KL, 50-58, 123)

PAIATNIK. L.S.; B
Aging of AI-Cu alloys of variable composition [11 In thin
film.
Isv. vyr. ucheb. say-; fts- no-3:112-116 158. (MIRA, 11:9)
1. Kbar1kovskly gnsuniversitst Iment A.M. Gor1kogo I Khart-
kovRkty politekhnichaskly Inatitut Imni V.I. Lenim. -
(Aluminum-copper alloys-Notallograpby)

SOV/126-7-3-39/44
AUTHORS: Palatnikq Lo S.,, Lyubarskiy, I. Mo and ~B. T~.
TITLE: A Contribution to the Nature of the "White Zone"
(K voprosu o prirode "beloy zony")
(k reply to the article "X-Ray Investigation of the Structure
of Surface Friction" by ..Kostetskiy et alJi (Ref.4) )
PERIODICAL: Fizika metallov i metallovedeniye, Vol 7, Nr 3, pp 03-474
(USSR)1qjj
ABSTRACT: B. 19 Kostetskj* and co-workers (Refs.1 and 2) have
expressed the assunption that the "white zone" which forms
at the friction surface at certain rates of slip of the
rubbing surfaces, consists either of a layer of oxides
(11oxidizing wear" according to Kostetskiyls classification),
or a secondary quenched structure (thermal wear). Falatnik
(Ref;3w) did not find iron ox4dea in the portion of "white-
zone hich he investigated by X-rays. The authors of this
paper have come to the conclusion that Kostetskiyls hypothesis
in erroneous. The basic objeotions of Kostetskiy and his
co-workers (Ref.4) in connection with the present authors'
Card 1/2 artiele (Ref.3) are the following:

G
A Contribution to the Nature of the "White Zonelt
(a) In the paper by the present aixthors (Ref.3) the already
well-Imown fact that tAie layer formed during thermal wear is
a hardening structure has only been confirmed again.
M A white layer which forms In thermal and not in oxidizing
wear appears to have been investigated in the paper (Ref.3).
'It has boen shown by the authors of the present paper that the
great hardness of the "white zone" (in spite of the great
quantity of auatenite). is duep nQt to the absorption of
oxygen or nitrogen from without (Ref.-5) eta., but tot he
formation of a definite highly dispersed haterogensaus
structure as the product of a solution of ear-bides and the
subsequent very rapid quenching in which dispersed carbides
are precipitated. .
There are 5 Soviet references.

AUTHORS:
TITLE-
PERIODICAL
ABSTRACT:
Card 1/2
Palatnik, L.S. 9 Boyko, B.T., Ko3-j7irh, V.M. 32-24-4--17/67
On the Preparation Methoaics and the Calculation of Samples With
Different Compositions (K metodike praparirovaniya i rascheta
obraztsov peremennogo sostava)
Zavodsk.-xva Laboratoriya., -1958, Vol. 24, Nr 4, pp. 422-424 (USSR)
On the basis of the method worked out by S.A.VekshinskV(Ref I),
the following method was worked out for electronographio investi-
gation. In principle it oonsists in the fact that on a horizontal
plate (the collector), which is divided into three surface~~.sectiona
by means of two vertical plates, the metal vapors emerging from'
the test crucibles ara collected. Outside of the two separating
plates the pure metal condensates, whereas between them the alloy
is separated. For the purpasa of calculating the concentration of,
the alloy two methods can be applied: Firstly, the method of sym-
metric lines, and, secondly$ the method based upon the radius. For
the control of the arrangement of the separating plates the photo-
metrization of the plates of the Iyure components may be used.

Ga the Preparation Methoaics and the Calculation of 32-24-4-17/67
Samples With Different Compositions
Photometric ourves of copper and b.'smuth plates are given from
which the symmetry of distribution may be seen. Two var.seties of
the method are mentioned; in one of them a horizontal plate col-
lectuor of g'lass with three slots is used, the arrangement of which
can be displaced in the vacuum, so that several experiments can be
carried atit continuoimly. The composition of the alloy can be mod-
ifieJ by modifying the heating of the crucible. In the case of the
second variaty a glass plate with on2y one slot is usea, so that
the pun metals ana the alloy are deposited on one and the same
strip. Investigationa were carried cfat With simult-aneous eand suc-
cessive ei-aporation of copper and aluminum. The method described
can be applied only if certain conditiorLs are satisfied, which is,
however, not aiffimait at certain e~mporation- and condensation
conditions. The method can also be applied for three.-component
systems. There are 4 figarea, and 4 references, 3 Of which are
Soviet.
ASSOCIATION: Kharlkovsldy politekhnioheak4-y institut im. V.I. Lenina
(Rharlkov Polytechnic Institute imeni V.I. Lenin)
1. Alloys--Analysis 2. Metallic vapors--Condensation
Card 2,/2 3. Photometry--Applications 4. Metals--Vaporization

AUTHORS:
TITLE:
PERIODICAL:
ABSTRACT
Card 1/3
Palatnik, L. S., Bo~vkot B. T. SOY/2o-120-5-231/67
The Investigation of the Processes Involved in a Retieated
.coripo!;.ition of a Solid -Al-Cu .133oltition (Issledovanlye
Drotsessov rovtornogo raspada tverdogo rastvora M,'I-Cu)
Doklld,,r Alcademli naixk 'SSISR, 12o, Ni- 5, pp. 10
1958, Vol- -1017
This is a study by the viethods of electron diffraction and
electron microicopy of the processes of the repeated decompo-
%;ition of th-~ 4-n~ase and of their separation from a solid
in film-3 of the alloy Al.-Cu with a thickness of
Tl-it3 allc-y was prepared according to the method. of
Vek~-,hlrtskiy (11of 5). Both. components were
evaporatecl
simmltaneoiisl,~ and were condensed upon a cold collector. Am
allcv in a chilled atate tialwa the structure of a
chilled oversaturated (monphase) solid a-solution. By heat
iiig this alloY to 50 - 300 the homogeneous solid a-solution
separiting s Pinely di!~riers?p a-rhase The
.Pf_rt_-'-c)v-s of the --phriso htrrc- a aize of abotit 10 A. At
0
4 'D ~-' uha particles of the Q-)hwie co-ilitsce to aconsiderable-
degree. Tf, the alloy is heated to 480 the coatesced particles

3,~71/2-1, 20--f -?.;%/157
The Investigation of the Proceases involved in a Rspeated
Decomrosition
of a Solid 41-feu Solution.
Irt~ ~OMIA-vt('2Y divnolved in tho solid u-solution. 'Wnen the
,iamplo i~i cooled down to 440 0, the P-Phase is again separated
,-solution. This nrocezq of the dissolution
ot tke 0-phase.and tile subsequent decomposition of' the solid
~to 480 0
is reproduced as ihe Iteliting hild the sub-
f,teouent Cooling in repeated. The oluctroti-micro.9corical
nicturef, aml the diffract-ion patterns a-re also repeated. The
- -j- ) Ii7h e n
e
x.re-t .-nerital. evidence can loo oxplained as follows: 1
the thin film of Al-Cu solution is condensed, a finely
dis,jea-se, homogeneous solid c~-solution, which is considerably-
oversaturated, is formed, exhibiting a 6trong tendency to-
wardo decomnoeition, The pronounced orientation of the
Q-Dhave after th8 dissolution of their coarsely grained
Pueticles at 480 and after a further reoeated decoinDosition
of the ovez-3aturated solid ty-solution at cooling doNvnj the
"memory phenomena" and their disappearence at a conriderable
overheating is oonneoted with the diftuslon mechsn_!!~m of the
(fssolution process. The overheating of the solld a-solution
favors an aisimilation of the inhomogeneities of the con-
Card 2/3 centration and increases the probability of the formation

Tht~ 1rivoctAiraLion of the InyC).V(!d In a _~,Levoated Decom
v0sition
'u :c)lu'ion
0.6 a Salirl A].-(,
and of the gtolath of tho nuclei of' the '--Ov.~2e `%ri tho allote,
Vaun the conoentr.,tion of copper in the local doriuin_~ in
the eurface layer of atoms decreases. There arc- 2 figuren
and 6 refereraeo, 5 of which tare Soviet.
MS 5, 0 0 1 W I ON Khailkovijk-iy gO3UdRr:3t-,ren.,yj- universitet
im. A.M.~".orliogo
(XJ),&_rIkoV State University im6ni A. iI.I. Gorlkiy)
Fh_-rI',--ov.skJ.-T nolitc-khnichooki,, institut itn. ~.cnina
(Kharlhov Tblj!tachaiical Institute imeni V. I. Lenlln)
FRESIENUED I&Arch 25, 1958t by 13. A.. "Vekshin-skiy, Member,
kcademy of
R
Scierces, U55,
SUBMITTED: 'Warch 23, 1958
1. Aluminum-copper alloy filus--Decomposition 2. Aluminum-copper.
alloy films-Electron diffraction analysis 3. Aluminum-copper alloy
films--Phase studies 4. Electron microscopy--Applications
Card 3/3

SOV/1,26-8-2-26/26
AUTHORS: Palatnik, L.S. and Boyko, B.T.
TITLE: Electronographic Ga~lysl`sby TSuperposition Method
PERIODICAL: Fizika metallov i metalloveden-iye, 1959, Vol 8, Nr 2,
Pp 318 - 320 (USSR)
ABSTRACT: The proposed method is a further development of the
superposition method in X.-radiography. In the present
method, however, the position of the samples (thin films)
is unchanged and the electron beam is displaced to
penetrate them alternately. Thus, the oscillating beam
produces two displaced electronograms on one photograph.
Deflection of the beam is brought about by feedIng
impulses to two divergent plates placed between the
diaphragm and.,the object (Figure 1). The displacement
canbe varied by varying the amplitude. Examples of
photographs.are shown in Figure 2. The method can be
used in two ways. The,first is to use standard
electronograms of a two.-phase system, e.g. Figure 2a for
Al -- Bi. From a comparison of lines on the standard with
those of an unknown heterogeneous alloy, the volume-
Cardl/2 concentration of a phase in the alloy can be determined,
The superposition of two thin filmg ean be used in other

sov/126-8-2-26/26
Electronographic Analysis by a Superposition Method
ways, e.g. for a determination of thic-kness. In the
Second use of the dsacribed method, the quantity of an
element is determined by weakening the intensity of its
line until it is on the limit of visibility, somewhat
analogous to X-ray spettrographic analysis. This is very
effective in the study of oxidati,-_n and chemico-thermal.
treatmentat where thin films exe Rormc~d.
There are 2 fig-arer~ and 2 Sovj.et r,;~ferenut~a.
ASSOCIATIOM Khaxlkovskiy gosudarstv,enny-y mniver.Aitct im.
A.M. Gorlkogo (Khar2kov State Unj.lrerAity im. A.M. Gorlkiy)
Kharlkovsk�y politelchnichoirkly im-stitut im.
V.I. Len-Ina (Kharskov Institute Imeni
V.I. Lenin)
SUBMITTED: Jarvaary 25, 1959
Card 2/2
usoommix.6i, 763

9(6) SOV/32-25-6-16/53
AUTHORS: Palatnik, L. S., Boyko B. T.
TITLEa Electron Diffraction Somiquantitative Phase Analysis
(Elektrono-
graficheskiy polukoliehestvennyy fazovyy analiz)
PERIODICAL: Zavodskaya Laboratoriya, 1959, Vol 25, Nr 6, pp 690 -
696 (USSR)
ABSTRACT: The present paper gives a description of a method of
electron
diffraction phase analysis; it has been developed from the
method of superposition in radiography (Ref 3). Unlike the
radiographic'method, the position of the samples is not changed,
but the electron beam is shifted, so that two dislocated electron
diffraction patterns form on the same photographic plate (Pig 1).
The dislocation of the primary electron beam is effected by a
voltage pulse (of rectangular shape) from a pulse generator of
the type 26 1. In taking the electron diffraction picture the
intensity of.the line of the given free component is expressed
by an equation (1.) (Ref 3). To take two different free structure
components of a two-component alloy, equation (1) is
correspondingly transformed and equation (6) is obtained. A
Card 1/3 delaying multivibrator (Pig 2, Scheme) may be used to widen

Electron Diffraction Semiquantitative Phase Analysis
SOV/32-25-6-1,6/53
the frequency range of the 26 1 generator. Examples of electron
diffraction analyses (with superposed electron diffraction
Pictures, figures are shown, and it is stated that.the
sensitivity of analysis dQpends on the sensitivity threshold
A B/B for the determination of the diffraction line.
(B. blackening,of the background,A B - difference of blackening
of the line and of the background); A B/B with given B may be
determined according to the Neff curves (Ref 5). The sensitivity
of the method was investigated on metal foils of Al, Ag and Bi
(Table). The semiquantitative phase analysis described in based
on the fact that in the elecetron diffraction investigation
of a mixture of.two components which differ relevantly as to
the ordinal number (e.g. Al and Bi) in films of a thickness
of 100-300 R the weaking of in-tensity of the diffraction lines
of a component may be avoided at-,'the expense of the absorption
in the other component. This is proven also by experiments
carried out to develop the experimental technique on Ag-Bi
and Al-Bi mixtures. The analysis of the mixture Ig-Bi was
based on the sensitivity threshold of the diffraction line
Oard 2/3 (111) Ag (Fig 6, electron diffraction picture), and it is
stated

Electron Diffraction Semiquantitative Phase Analysis SOV/32-25-6-16/53
that the pre-determination of the sensitivity threshold of
the diffraction line satisfies only one component. There are
7 figures, I table, and 7 Soviet references.
ASSOCIATIONi KharIkovskiy gosudarstvennyy universitet im. A. M.
GorIkogo
(KharIkov State University imeni A. M. Gor'kiy)
Card 3/3

_7
S/126/61/011/001/012/0'19
E021/E06
i,~AUTHORS:... :Palatnik, L.S. an
OY
U49
!-~TITLE
y_.Alloys in Th'i
The Phase Diag_ran I.& n Films,
_y of
-,-PERIODICAL, Fizika metall a ye. l96l,,Vol.ll-'-:9oA,
ov i1 met Noveldeli
pp.123-127
-TEXT: electronographic study.of7the phase diagram of Ala-'CuA12
;i-a loys in thin films has-been carried:out. Films tontakning-fro
m
i~O to 30 wt.'% Cu with thickness of~about 150, 250-and 0 A waa:-~-
..30
ma de by simultaneous evaporation and.condensation~of weighed
'The onor
portions-of Cu andAl f ilms were heated in the.electr,
hi apparatus with 'continuous measurement
of temperature. The
grap ic
_p lase transformation temperature was
found by a change in.
diffraction pattern. In films 250 A thick, unstable suoersaturate~
i'solutions,were formed with a copper content of more than 25%. Thel
(110) and (200) lines of the 0-phase were observed after quenching
well a's -the a solid solution lines.. Heating at 1000C led to
~4,
further decomposition. of-the soli:d solution. In alloys containing.
25%-co per, when heated to 500*C only the diffraction lines of the
p
0 phase.,were observed. Thus a~solid solution of i Al", in' CuA12 MUS
t
-have-- been formed.. Alloys with 1 as
than.25% copper in-the

------ -- ------
89945

:S/126/61/011/001/012/019

,
.,E021/E4o6

The Phase Diagram of Al-'Cu Alloys in Thin.-,Films

1'.
4uenched state consisted of homogeneous metastable a solid-

precipitation occurred on'
;,solution. With less than 18% c4per,

'.,'.T":-,.Vhea tin
g up.to 1000C. At higher temperatures, the 0 phase

~-:~~-`!.'dissolved in the a phase and at 520*C was completely
dissolved.

t of 18 to 25%~complete solution did not occur
With a copper conten

-and a m6tastable eutectic transformation
occurred at 5200C. With

increase in thickness of-the film the
limiting solubility of -copper

-'-:decreased and th6 temperature for
the reversible transformation,

.-a -0 ZZY a increased. Thus the
equilibrium diagram for thin films

from that in the massive-state..,
Fi the-
Jls~:different
g.4 shows

.
---equilibrium- diagram for a film 250 A-thick. There are,4
igures,

1: table. and 6 references: 5 Soviet and.1 non-Soviet.

ASSOCIATIONS: Khar1kov3kiy gosudarstve
nnyy universitet

im. A.M.Gorlkogo .(Kharlkov. State University...

imehi A.M.Gor'ki

Khar'kovskiy po
itekhnicheskiy institut

:;imeni V.I.Lenina)(Kharlkov Polytecbnical Instit
ute

-imeni~V.I.Lenin)'--

iCard 2/1

2)J175
S/126/617611/006/001/011
4t 70iv E021/E3o6
B.i.
and
AUTHORS; Palatnik, L.S., Fuks, M.Ya., Boyko,
Pariyskiyj V*B9
TITLE: Electronographic.Study of Substructure of Thin
Condensates of Aluminlum by.the "Microbeam" Method
PERIODICALt Fizika metallov i metallovedeniye, 1961, Vol. ll,-
No. 6, pp. 864 - 869 + 1 plate
TEXT: The electron, microbeam.is suitable for studying
indi Idual reflecti-ons from crystallites of dimensions 100 -
300 1 and for evaluating the relative misorientation between
crystal-lites. Thus, the el ec trono graphic microbeam is a
direct method of observin the substructure of crystals.
Aluminium films 60 - 200 1 thick, condensed in vacuo on a
cold surface, were studied by this technique. The fili2s were
transferred to aluminium foil with holes of 20 to 70 ji . The
thickness of the film was estimated by a photometric method
with an accuracy of 1096. Photographs were taken in a high-
temperature electronograph with electrostatic focusing. The
films were heated at a rate of 30 0C/minand electron-diffraction
Card 1/6

Electronographic Study ....
24475
S/126/6i/oll/oWooi/oll
E021/E306
patterns were taken at room temperature, 200., 300, 400 and
450 OC. The mean linear dimension of a coherenti,,reflecting
region for films heated to 400 OC was 14o - 335 A. This is
similar to the mean dimensions of mosaic blocks determined
by X-ray investigation of deformed polycrystals.
The Debye ring at 20 and 200 OC appears continuous and diffuse.
Heating to 300 0 C results in the appearance of intensi Xe spots
but the general background is still 0retained. At 400 C this
background is very weak and at 450 C it disappears. The
number of spots remains practically unchanged on increasing
the temperature from 300 to 450 OC. Photographs are ine ded
for the (111) ang (200) lines taken from a fiIii, 125 rthick
on an area of 20 ji , heated to 3001 450, 400 and 450 C"C (X15).
At a magnification of 60, spots of increased blackness can be
seen on the electron-diffraction patterns taken at 20 and 200 OC.
The complete results are tabulated. The mean linear dimension
of the crystallites was calculated from two formulae:
Card 2/6

Electronographic Study ....
3
cp as 0
24475
S/126/61/011/006/001/011
E021/E3o6
(2)
and
L := 4V 0/1, (3).
mhere v is the mean volume of the region giving coherent
0 refloctions and
h is the film thickness.
The size of the crystallites increases with increase in
temperature. The degree of misorientation of crystals in
condensed films is somewhat greater than the values for
ordinary crystals. This may explain the high resistance to
plastic deformation and high rate of diffusion of such films.
There are 2 figures, I t,ablo and 13. references: 7 Soviet
and 4 ron :;oviet. Tho two Mr.glish-language references
quoted &re: Ref. 10. Quar~'el, A.G., Roebuck, J.S. Proc. Roy.
Card 3/6

24475
S/126/61/011/006/001/011
Electrono-raphic Study E021/E3o6
0
Soc., 1934, A.145, 676: Weaver, C., Hill, R.M.. Advances in
Physics, 1959, Vol. 8, 375.
ASSOCIATION: Kharflzovskiy gosudarstvennyy unIversitet im.
A.M. Gortkogo (Kharlhov State University im.
A.M. Gorlkly)
1Qiar1kovshiy politekhnicheskiy institut
in. V.I. Lenina (Kharlhov Polytechnical
Inst1tut im. V.I. Len-in)
SUBMITTED: January 21, 1961
Card 4/6

47
S/126/62/013/ool/oo5/o18
7 R02l/U.58o
AUTHORS: 1 Palatnik, L.S.,Boyko, B.T., Fuks, M.Ya. and
Pariyskiy, V.D.
ri'VIX: Electron diffraction study of the substructure of
thin films of aluminium, silver and gold, condensed in
Vactio
PERIODICAL: Fizika metallov i metallovedeniye, v-13, no.1, lt)62,
71-76
XT: ic influence of f ilm thickness and substrate tempera-'~_;.:':
E TI
T
ture on
the mean size of mosaic blocks i%ras investigated in thin
condensed films of aluminium,, silver and gold. Aluminium of
99.999io' purity and silver and gold of 99.9% purity was used.
Evaporation was arried-ott fr a cone-shaped tungsten spiral at
V 0m
rates of /I- x 10-9,.5 _-4 10-, , and 10:11 S/sec. for Alt Ag and Au,
respectively..-Condensation occurred on a heated glass plate. The
filins w-cre separated-.by immersion in distilled water and caught on
n films
metallic holders.of foil'contliini g 0 2-0 4 mm holes. The
were examined by electron diffraction using the (220) ring. -The
effect of heating the films was studied. The true diffraction.
bronde2ing-was-found by harmonic analysis (Ref.6: B.Ya.Pines..
Card.1 3

El cc tron diffraction study 5/126/62/013/001/005/o18
E-021/ri-58o
rentgenovskiye trubki i prikladnoy rentgeno-
strukturnyy analiz (Fine focussing X-ray tubes and applied X-ray
structural analysis), GITTL, 1955). The main
contribution to the
broadening arises from the small size of the mosaic blocIcs. Ifli e n
there is a marked difference in the coefficients of expansion of
the holder anti the 'film, the Intter is subjected to plastic
deform -Ation in the process of heating which is accompanied 1) y a
refining of the blocks. With rapid heating, recyrstallisation
does not remove this effect. Therefore, thermal coefficients of
the film and holding material should be approximately equal. With
increasing film thickness of aluminium and silver, the broadening
of the lines decreases both in the initial anti annenled states.
Continuous heating of aluminium films UP to 150% in 2-3 min leads
to refining of the mosaic blocks, whereas Neating to higher than
1500C results,in coarsening. Heating silver and gold in the region
20-4000C also results in coarsening. The mean linear dimension 6f-~
the blocks in aluminium. film. is about half that in silver and gold
films, and coarsening during henting takes place less intensively
n1
in 1, u.minium. , The probable reason for th.is difference is the
formation 'of highly dispersed aluminium oxide. Th e mosaic
Card'-2/3

A 7,701
i/013/0b.4/009/022
60
AUTHORS: PiklAthik, L.S., Rodlk*na, N.I.
TITLE: Electron-diffraction investigationiof the structure
of superheats "azixd~--ou'percooled'..liqOid'metals
PERIODICAL: Fizika metall*ov i.Me'tallov0dsiiiye,.'v.l3, no.4, 1962,
555-560
TEXT: The ten,dency,for super,cooling to--occur-increa,ses with
decreasing'thickness of a liq ui d-metal layer and can be-very small
with very thin films. Thi., structures:. of ,f-liquid tin (99.99% pure)
during supercooling and'superheating, a,nd-6f liquid indium
(99.999% pure) on superheaiti"j'w'er1e'st%kdi*d bk electron
diffraction. Films of tfio".~tent,metals'-.w4ire.heated directly in'
the electron-diffrac.tion a'ppar I4tus by' pass,ing.d.c. through their
holder (a tantalum by 100C the. intensity
curves show four very prowiiinped'maximmi.' This is- less~ pronounced
on superheating by 30 0C a"''' i- I I- g by 700C
.A.*appears on.supeiheatin
On the radial-dlstribution-"curi-es-for the supercooled tin there
pear on superhe
are six maxima; the third_'4nd,-_fifthdisiap ating by
30% and there in a radial'-- phange' the 'c~urwe having only three-
Card 1/2

S/126/62/013/004i 009-0--
Electron-diffraction investigation ... 9111/9435
maxima. Comparison with.,data"for closo6t.packing and for white,*
tin showed that on supercoolink-1he short range order of the
distribution of the atoms-is. nilar *,to,,that of crystalline white
air
toi7c -tho atoms-,& 0 Al
tin; on superheatin by- Id most in closest
packing. Crystalline indium has almost 6losent packing.
On superheating indium by 3596and 809C and comparing the obtained
i -curvea, it can be seen that the: 1,X
ntensity and radial distribution
number of atoms.in the:firit coordination.sphere decreases to
7.2 and 6 at the lower and'higher temperat'urs,'respectively.
Indi= behaves on fusion differently from-other closest packed
metals in that the number of atoms in its first coordination sphere'
decreases but behaves similarly on increasing the superheating
Apparently a coordination number of 8 for li- id indium is the
. V
highest. There are 4 figures and 4 table,&-.
ASSOCIATION: Kharlkovskiy politekhnicheskiy institut im. V.I.Lenina
(Khar1kov Polyiochnical Inatituto-imeni V.I.Lenin)
SUBMITTED: July 31, 1961
Card'2/2

34321
S/032/62/028/003/007/017
a 0 B101/B138
,LUTHORS: Fuks, M. Ya., and Boyko, B. T.
TITLEs Electron diffraction investigation of the substructure of
condensed metal films
PERIODICAL: Zavodskaya laboratoriya, v. 28, no. 3, 1962, 300 - 305
TEXT% Pure aluminum was vacuum evaporated an to various bases (film
thickness 65 - 240 f), and the substructure was studied by electron
diffraction analysis. It was found that harmonic analysis of inter-
ference lines can only be used to eliminate instrumental effect and
not
to determine lattice micro stresses. A series of tests with aluminum
films on tantalum bases shoved strong deformations due to
differences in
the c6efficients of thermal expansion of the two metals. Therefore
when
stidying the substructure of thin films bases should be used whose
ex-
pansion coefficients do not greatly differ from those of the film to
be
investigated. To determini block sizes, a microbeam was used which
irradiated only a 10 - 20~ sector of the film. Aluminum foils about
1*
thick were perforated by a~needle or an electric spark, and the film
was
Card 1/3

S/03 62/028/003/007/017
Electron diffraction investigation... B101YJ3138
deposited on the sector contained by this opening. "Microdot"
electron
diffraction patterns of lines (111) and (200) were obtained for
film of
125 f thickness at 300 - 4000C, and measured photometrically At
4000C,
the linear dimension of the reflecting blocks was 200 - 300 i;
this is
the same size as that obtained for mosaic blocks by X-ray
diffraction
analysis of deformed polycrystals. The angle of disorientation of
ad-
jacent blocks was found to be more than 30. Photographs of the
aluminum
foil backing did not reveal any substructure. The background
between the
point reflexes indicates that there are some smaller blocks
besides those
due to annealing. Thus, the sizes obtained by the microoeam
method are
not averages, butiho96 of the larger blocks. The average size can
be
found from the diffraction broadening of the lines; it was 90 2
at 3000C.
This method may permit an investigation of the substructure of
films of
refractory metals, if the irradiated area is reduced to 1 - 2
)!,2 and the
light intensity Of the electron diffraction photography is
increased.
The following authors are mentionedi B. Ya. Pines (0strofokuBnyye
rentgenovskiye trubki i prikladnoy rentgenostrukturnyy analiz
(Focusing
x-ray tubes and applied x-ray diffraction analysis), GITTL
(1955), and
B. Ya. Pines and A. F. Sirenko (Kristallografiya, 7s 1 (1962)),
There are
Card 2/3

5/032/62/028/003/007/017
Electron diffraction investigation... B101/B138
3 figures, 2 tables, and 13 referencest 10 Soviet and 3 non-Soviet, The
two references to English-language publications read as followst
J. W. Menter, D. W. Pashley. Structure and Properties of Thin Films,
New York - London, Ill (1959); C. Weaver, R. M. Hill. Adv. in Phys., 8,
329 375 (1959)-
ASSOCIATION: Kharlkovskiy politekhnicheskiy institut im. V. I. Lenina
(Khar1kov Polytechnic Institute imeni V. L, Lenin)