SCIENTIFIC ABSTRACT KAZANSKIY, V.YE. - KAZANSKIY, YU.N.

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000721320010-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 13, 2000
• Sequence Number: 10
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

FAZAJISKIY,, V.YO,, inzh. (Moskva)
Measurement of electrical resistance with three
devices.
Elektrichestvo no,1:81-82 Ja t62* (MIRA 14-12)
Electric measuremonta)
ectric resistance-1.1casurement)
M
rN

KAZANSKIY,- VladimJLr Yovgenlyevich,'
SAVOSTIYANOVj, A.I., nauchWy
".. -.--7ed.,- BARANOVA, N.N., tekhn. red.
[Automation and remote control in electric power
6ySteM.91
Avtomatizatsiia i telemokhanizataiia
energeticheskikh
sistem. Moskva, Proftekhizdat, 1962. 182 p.
(MIRA 15:10)
(Automatic control) (Remote control)
(Electric power distribution)

LUANSKIY,, V.Ye.p dotsent
SPedial features of measuring nonwymetry current in
the
differential protection system of electric power
transformers.
Blek. eta. 34 no.3;94 Mr 163. (MIM 16:3)
(Electric protection) (Electric transformers)

_KAZAHSKIY,V_IAdimI~YAvgWi!# ~Viqh~SAVOSTIYANOV,
A.I., nauchn.
red.; CHISLOV, M.M., red.; BARANOVA, N.N.p tekhn.
red.
(Automatic and remote control in power systems]
Avtomati-
zatsiia i telemekhanizatsAa energatichaskikh
slatem. Mo-
skva, Proftakhizdat, 1962. 182 p. (MIRA 16:7)
(Automatio control) (Remote control)
(Electria power distribution)

KRZANSKIY, V. Ye.
"Some Problems in Automation and Remote Control of
Power Systems."
Dissertation for the degree of Doctor of Technical
Sciences
defended at the Moscow Power Engineering Institute,
January 1.963.
Moscow, Elektrichestvo, No. 9, SePt) pp 94-95-

-(i)/,E.OVP(c)/F',VP(V)/T/E P(t)/ 4 (0, v&
EWT(d)/ENT(m)/Ed~ N E I- /E ~h~)
I
ACCESSIrN NR: AP5026358 JU UlVO105/64/ooo 00 /bog 5
A7MOR?41Tsvetkov, V. A. 1 Birzniyek, L. V,; Vysochanskiyt V. S.;
ShakhnaZa"Iyang Y~
Kazanakiy, V. Ye.j Kapuntsov, Yu. D.1 Salekh, M. A. Kh.; Frumkinj
A. L.;
Bakkhov fq: B. A.
TIMs. Dissertations in dompetition for the academic degree of
doctor of technical;
aciencea
,ISOU*RCE: Elektrichestyo, no. 91 1964, 94-95
MPIC TAGS: electric engineering, electric power engineering,
electric equipment,
electric distribution equipment, electric rotating equipment,
automatic control,
iautomatic control system
!'AbBtidctf' -The folloviing defended dissertations at the Mospow
Po-er
"Ing Institutes V. A. TSVETHOV, 14 December 1962, on th
a then* "Autopara-
Lragnetio Phenomena and Surges In Tbree-Phase 01rcults which
Contain )Ferro-
:Magnotio Eouipment,Of his offloial opponents -- Dootor
of-Toohnioal Soionoer,,
'Professor V, A, TAFT and Candidate of Technical Saienoeo, Looturer
L. F.
DROXHOVSKAYA; Le Ve BIRZ111YEK. 4 January 1963, on the them
"Blootro-
1
r`aM1OtIO PrOOi_B_5i_i_ii Daltistage.VoltaV Regulation 01rouits in
Elootrio
i~_, L j.,
Card 3,A

L 3108-66
:iACCM31ON NR: Ap5o26358
~,Rolllng Btook with Semiconductor Rectifiers," his offlolal
oppononte
,!Dootor of Technical Sciences B. N. TIKRIENEV and Candidate of
Technical
i
~Solenoer, Looturer L. 1.. TRAYH71WI V .19 VYSOCW�KI.Y, 10
January 1963
on the theme "Methods for Controllingliho Strip Tension at the
Reol of a
old RolllN_~Ills," his official opponents -- Doctors of Technical
.Sciences Wo P, KW4ITBKIY and No No DRUZHIVIV& Yus go
SHAIggWARYAN, 18
ir6i~- - --sIZ7- 1
January 1963, on the theme ~'AiiProxlmate 14otho" Xiialy of
iFon-Station-
ary Asynchronous Conditions in Electrical Systems," his official
opponents
Doctor of Technical Sciences, Professor Lo Go WIRONYANTS mid
Candidate
of Technical Sciences, Lecturer No 1. SOX
~~tOV; V. Yo. RAZANSOY, 10 January,
4on the theme "Some Problems in Automation d Remote Controllof
Power Sys-
~~tems,ll his official opponents -- Doctor of Tochnioal
Scioncej, Professor
I. A. SYROWATHIKOV and Candidate of Technical Sciences V. K.
SPIRID01NOT;
Yu. D. KAPUNTSOV, 18 January 1963, on the theme "An Asynchronous
Electric
1Drive w4th Ron-Symetrio. Connection of the Saturation Chokes in
the Stator
.1!Cirouit,11 his official opponents -- Doctor of Technical
Sciences V. Ye.
!BOGOLYUBOV and Candidate of Technical Sciences, Lecturer Do No
LIPATOV;
'Mo Ao Kh. SJUMM, 22 February 1963, on the theme "Theoretical
Study of
the Operatlon of kinature Two-PhaGe Asynchronous Machines when
the Supply
'Voltage Is not Binusoidal," his official opponents -- Doctor of
Teennioal';
i
!'Sciences, Professor A& L BERTIN07 and Candidate of
Tsohn1oa1.SoI6Mes,.
Card 2/4
R,
'0

L 3108-66
ACCESSION NRt AP5026358
Lecturer P. Yu. KAASIXI A. L.-FRUMMIT, 0 Itarob 1901, on the
thomo ,A
Thooratioal and Experizental Study of the Formoabillty of
Anisotropla
Thin Magnetic Films," his official opponents -- Doctor of
Mysioal and
11.atbamatical Sciences, Professor 11. V. TELESNIV and
Candidato of Toolinical
Voienoes, Lecturer P., Pe LWYATSEV; L. A. BAMr0VT 19 April
1963, on
the theme "Synthesis of S teqL9 Automatio-Con ;I . and
r . I _yt_ jg_ --.I---- ~f Startinr
Stopping of Elootrio Drives," his official opponontr, -- Doctor
of Toobnioal
75olonoes, Professor A. Be SAITPLE1 and Candidate of Technical
Solepoes,
ILeoturer Tue Ye. V1711SOVe At the 1,1osoqv!_114_gher
Teohiiloal Aoa('1'omy IMM
Bauman -- G. A. IRRONOV. 10 Deoernber 1962, on the theme "A
Metbod for
_120_r_T,~_;ntaf-piograming of Lleotronlo Digital ComImtora,"
his official
;opponents -- Doctor of Pbyoloal and Hathomatical SolonceB,
Proforsor La At
FUSTEMIX and Candidate of Technical Sciences, V. Ys, PETROV. At
the
All-Union Bleotroteabnical Institute Im. Lenin -- V. Ae
VOLIKITAU, 11 1)008mo-'~
bor -1962, on the theme "Conductivity of Carborundutn," hl~
official opponents
~- Doctor of Technical Sciences, Professor V. V. BURGSDORF and
Candidate
f Teohmloal Sciences, D. V. SHISM.'"o At the AoadcuW-of
muniolpal
'Zoono ime Pamfilov -- V. A. KOZLOV, 14 januar-y'-Y9_63, on the
therm "Pro-
blems In the Use of Closed Systems for Maniolpal Blootrical
VetworkBt"
bis official opponents - Professor Ps. G, URUDINSKIY and
Candidate-0. Tooh#A
Mosl Goisnesso Leeturer F4, F* YOR01move
Ur4 3A,

L 3108-66
JACCESSION NRI AP5026358
At the All-yanion
jolentif to Tiosearcii Inc-tituto of Elootromocbeniqc L, Ya,
STAMBLAVSKIT't
theme "On Work in the Field'i at, Tutu-
.:U Tomai6i 1~6t# on 6t 111 gh Pow
'generatore and H~,,drogcnoratora,,� his,officidl opponents --
Dootor of Toob--
nloal bolenoeof Profoosor 1# It., POSTITIHOV, Dootor of Toobn1oul
Solerooo
I* Do URUBOV and Oandiclate of Teohnical Saienaso-Yus -Us "1;VX, I
YD.
_Vec~~ch Institutb of Railroad Transportationt__V'.'D.' 'TULUFOVt
Z1 Decewber,)
!1962, on the theme "Development and InYeatigatl6fi -of-A'Systom
for Auto-
Imatio Control of Rheostat, Braking of Rootifier Elootrio
Looomotiyoo," hie
;orflciai opponents -- Dootor of Toohnioal'Solonoes Do No TIMUMTEY
and
CcmdldQte of TeohniotA Soienoee B.- 0. WIENETSKIY1 V. D. MCHTSET, 21
Pooombor 19620. on..tbo tbemo_11?r6tootion of,Treotion Hotora from
5hort 01r-'.
oult Currents D4rlrq DralcIng,-It hIla offlol .-al opponIonto --
Dootor
of Technical Solcitoes, Profesuor Vo Yo. ROMWELOD and Cand1date of
Tooh
nical Sciences L. 11, TRAVJITW,. As Ve xganv, 11 January 19,63, on
tho
lthom,o "Study of.Volt", Control Systema for Power Transformora in
AG Blootrio
;Looomotivos vith Hootifi4rat" his ioffjoinl-oppolionto -- Dootor
of Tooliploal
Faiences, L. P. ISAYLT, and Engineer Do Yao BYSTRITSKIYo~
ASSOCIATION&
none
SUB
SUBMITTEDS, 60 txcLl 00 00DEC EE,
NO' REF SOV 1 .000 OW

USSR/Nuclear Physics Penetration of Charged and Neutral Particles Through
Matter.?
C-6
Abst Journal: Referat Zhur - Fizika, No 12, 1956, 34lo8
Author: Tsyp!x, S. G., Kukhtevich, V. I., Kazanakiy, Yu. A.
Institution: None
Title: Penetration of Gamms. Rays Through Water, Iron, Lead, and a
Combination of
Iron and Lead
Original Periodical: Atom. Ebergiya, 1956, No 2, 71-74
Abstract: The attenuation of the dosage of gamma rays in Fe, water, and
Pb is meaB-
ured for an "infinitett geometry. In the "barrier" geometry, the dosage
attenuation
of gamma rays was measured for mixtures of iron and lead. The
experimental data ob-
tained are compared with the results of calculations based on the Fano
theory.
I or/

~~i z -6?.

12C -2-7/3~
AUTHOR: Burmistrov, V. R. and Kazanskiy, Yu. A.
'TITL,: Compton 0'pectrometer Using Superposition of i-ulses.
(Komptonovskiy Spektrometr So Slozheniyei:i Impullsov.)
MaODICAL: Pribory i Tekhnika '-Eksperimenta, 197)?, llo.21,
pp. 26 - 29 (USSR).
ABS,TRACT: After a short discussion of the viork-in- of the Compton
spectrometer usinF5 I.-wo scincillatinr, crystals, the authors
proceed to give the description of a method which permits
a subotantial increase of the efficiency of tlicl 51)ectro-
meter without deterioration in its resolvinle chaiacteristie's.
'Three crystals are used: one central and two side crystals.
The increase of the efficiency is obtained by increasin6
the solid an6le of resolutiona by virtue of combining
pulses from the central end frow the side crystals. 'The
principle of the new method is as follows; when the
Compton scatterinG of the incident y-quanturfi hl occurs
at the Centre crystal, a pulse V is obtained a? the
output of the photomultiplier, tie amplitude of x,.hich is
proportional_to ~he enerGy of the emitted electron
(V 1= CL(Hi0 hi ). If the scattered y-quantunl IP,
.hitting the controlling crystal, is totally absorbed,
Card 1/3 the amplitude of pulse V2 at the photomultiplier will be
Compton Spectrometer Using ,3uper
Proporti Position of pulses. 120-2-7/37
2 'nal to t110 ene-vf~Y Of the scattered
V
V a= bh" "a" COUld be made equa.1 to
1 nd V2 One obtains V equal to V quantuLn:
3 V % " Combining
Pulse proportional 2 ah i0 i.e. a
independe - to the incident radiation ener,
that the nt Of the angle 0 (angle Of scattering),
dispersed quantum is ~-,;y a n d
controllin6
Crystal. totally absoi Provided
61on this With a monochro,,k -bed in the
radiatf Method would prod ce on ,tic incijellt
-responding to the energy 11)y u e
to the incomplete abso, sin0le peak cor
the controlline crystal ptiOR Plus Some energy spread due
Of the scattered quanta in
-resolution The Problem of the spectrometer
Equation 2 (full width at half heiE;ht)
peak is derived 8 is considered next.
as `ivinS the res '
n3 function of Olution Of the combined
spectrometer the depend I&VI j and n~V 2* -'For a single crYstal
tude V Of the Pulse is ence of resOlution
AV, j anrl AV2 i rom e qua 1,Aven by equation I On the ampli-
29 equation tiOn 3 and substitu 3- 1~valua`
4 is obtained., where C is tinU into u]-nU
equation
On the phot
omultiPlier
a consta.t
Card 213
and on the dependin-6
Crystal j .
0 It may be seen from e liG~lt output
quatio,B Of tLe
3 and 4 that

.-JOY/H9-5-4-10/24
;.UTHOR.'~:
Xazunakly, Yu. A., Belov, b. P.,
Matusevich, Ye. S.
TITLE:
Angular--a-nU-EffP-Ygy Distribution
of WI-Rays Scattered by Iron

and Lead (Uglovyye i
energeticheukiye raspredeleniya

T-izIucheniyat rasseyannogo v
zheleze i svintse)
PERIODICAL:
Atomn,-,.va ent~rgiya, 1958, Vol
5, Nr 4, pp 457-459 (USSR)
ABSTRACTi
Measurements were carried
out on the angular- and energy dis-

tribution of Co 60 and Au
198 It-radiation which had been scatter-

ed by lead with 1~0 r
- 2,2; 4,1; 06,5, 13,2 and iron with eo r - 2,

4t 6, 6.5, and
9,8 (Po denotes the absorption coefficient of

r-radiation and
r - thickness of the filter). Measurement took

place in
semi-infinite gpometry.

For measurements the scintillation
spectrom,?ter (C2j(Tj)-

crystal: dii-imeter 30 mm, height 27
mm) was used.

M-asurements were varr4-ed ovt at the following
angles G: 10.

20, 50, 40, '50, and 600.

Th.~.- engular
distributiom obtained arp plotted in graphs; The

r,,', 21
results obtained by the present paper and the paDers
of ref-
T-

SOV/89-5-4-10/24
".nwule.r- and Energy Distribution of T-Rays Scattered by
Iron and Lead7
erences 1 - 3 permit the following conclusions to be drawnt
The angular distribution of the intensity of the scattered
31-rRys depends only little upon the thickness of the layer
of
th#~ scattered nedium (up to a thickness of layer of 10 free
lengths of path). This determination holds for materials with
small as well as with medium or large Z (concrete, iron,
lead)
within the-r-energy domain of from 0,4 to 1,3 MeV.
G. Tsypin and V. I. Kukhtevioh advised the authors in
working out this paper,and 3, 1. Chubarov and V. I.Popov as-
sisted in carrying out experiments. There are 6 figurea ana.
4 references, 1 of shich is Soviet.
April 13, 1958

TITL~:
1 IQ- T~ '-.L.
Card 1/2
kI Iv,
"~ti)Jht-ovichj 1j,, Iazansiuy, fu.
*Ji kolals I iv i1i j, Sh. 3*., Tq'ypin, 'is Us
'file 1~assafe of Scattel,ed -,-.4iays Throuji 'ilater
rasseyanno-o y-4-iz1uch-aniya v
V ~4
'-neroiya, r 2~ Pp. 138-110
i Q'q 6 2)1N
~'ovxces cf Go
%*rays (Au 0 a , d in a large -,-,-at( r
are mounto
tanR on a mobile support in ruich a w-, that an irripdiate
tion of the detector is exclucled) and thato on the other
hanrij, lli4f-
ferent collimation. anFIes uioy be adjusted. The dependence cf.
weakenin(_! of, the y-quanta scattered iri tl,,e water on the
di3l.anc,~
between the sotwce and the dutectcr It-, nPasured and ah-o
comv:,~~-,J.
hc distance frori tile source to Ue cletector am-ounted to 3 - ~
a-1-1
- 12 lengthn of the imean free pith of y - quanta in rater. fti-~
collimation AnA-- Trre varied i6etween 3o ard i7f-,O. Thr~,t-m
curvte~;
the rcreentual decrease of the close. dependent o, thf--
:-Iistance
1. 1..98 ):u7o to 1ho cm a-790, 52,50, -120
2. GO CwG X=60 to 1)10 cr: c~-F,21, 59c, 470

The Faasace of scatter#--d-y-4i.a~re I'jr--roul-h
~.,.'ater.
D
3. !,a 211 xw7o to 14o cm CL-800, 62DO 46
The fic;ures also inciiide the ccmputerl c,.lrve,-,, the
funr-tic:1!;
j%a(E) ancl beini; taken from. reference 'o .1
cord can be founi 1-et-ween experimental and theoretical
r~,.irve3.
There are 5 fi~;uros, and 6 rel'urences, 2 of which are
3U')YITiU: Larch 16, 1957.
AV z i i LJI ~ 3 ITIE -Library of Concrens.
Card 2/2 1. G- rays-Enera-Measurement 2o Gamma
rays-3oattering

AUTHORS: Kazianskiy, Yu.A. , Belov, S.F. 89 -I-io/18
TITLE: The Spectrum of Scattered r -Radiation After Passage
Through a
Lead Barrier (Spektr rasseyannogo r-izlucheniya posle
prokhozhdeniya avintnovogo barlyeray.
PERIODICAL: PbVsice ands The`rmotecbnjqizes Df,, j~eectors,
(FiriX% _i teploteWmiika
reaktorov), Supplement Vr 1 to Atomnaya enieirgiya, 1958(
W~R)., ,, 3, Z
ABSTRACT: The spectral and angular distribution of the
-radiation of a
0.5 C Co-60-source is dealt with after the -radiation has
passed through a lead block of &or = 3.9 (given in free
lengths
of path). Measuring was carried out with a swivelingly
mounted
scintillation spectrometer. Spectral distribution %ms
measured at
0, 10, 20, 30, 46 and 600,* the respective curves are given.
Furthermore, the differential energy spectrum of the
scattered
- -intensity is given. Within the range of from - 0.5 to 1.2
MeV
experimentally and theoretically computed values agree well,
where-
as from 0-3 to 0.5 MeV they do not. There are 3 figures, I
table,
and 4 references, I of which is Slavic.
AVAILABLE: Library of Congress
Card 1/1 1. Gamma rays-Scattering 2. Gamma rays-Spectrum

CYPINp-S*G. [Tsypin, S,G.I; KUCHTEVIC.' V.I.
[Kukhtevich V I
KaANSKIJ, J.J. (
KAPIM, J. ttransialtorl
Penetration of gamma rays thrOUgh wator, iron,
lead and
Ccmbined layers of iron and lead* Jaderna energie
4
no.7.-191-193 j.1 e58,

KAZANSK.TY, Yu. A. Cand Phys-Math Soi -- (dias) r an u1stributions of
gamma-radiation scattered in a medimn.11 0- s 19599 16 pp 100 copies.
T/
Bibliography at end of text (18 title$) (KL, 43-59, 120)

21M SC)V/89-6-6-11/27
AUTHORSt Belov, S. P.*, Dulin, V. A., Kazanskiy, Yu. A.,
Kukhtevich,
V. I., Tsypin, S. G.
TITLEj Space and Lnergy Distribution of the Neutrons in Boron
Carbide
(Prostranstvennoye i energeticheskoye ragpreueleniye neytronov
Y karbide bora)
PERIODICAL: Atomnaya energiya, 1959, Vol 6, fir 6, pp 663 - 665
(USSH)
ABSTRACTs The authors report on investigations of space and
enerey dis
.tributions of 3 and 15 Mev neutrons in boron carbide. The 3
key neutrons were thejrodact of the reaction 112(112,n)110, the
15 Mev neutrons from (u3,n)He4. The test arrangement (infinite
geometry) is brief?v described. Boron carbide'i .1.18+(),05 g/cm31
neutron detectorst 1) proportional counter with BF 3 enriched
to 88%, with B10 ;2) fission chamber with natural uranium, U 235
(enriched to 75;;)v and Th232; 3) threshold indicators:
P31 (njp)S131, Al2'(n, P)Mg27,Fe5l (n,p)fAn56 , Sb 121 (n,2n)Sb
12o
116m
Cu 63 (n,2n )CU62' In 115(n,g) In .Figure 1 shows the space
Card 1/3 neutron distribution (3 and 15 Mev) in the pas~iage
through

Space and Energy Distribution of the Neutrons in Boron
sov/ag-6-6-11/27
Carbide
boron carbide. Detectors for the 3 Mev neutrons: 1) and 2),
for the 15 Mev neutrons, 2) and 3). It was found among others
that an increase of the threshold energy of the detector in-
creases the inclination of the attenuation curves of the neu-
trons. In measuring the 15 Mev neutron attenuation by means
of the indicator
Cu 63 (n,2n )Cu62 (E thresh' 10.9 Mev) the relaxation path for
the
distance source - detector R >16 cm doea not change and is
close to the transport path \r -18 + 2 cm. A comparison of
the data contained in the present paper with those from refer-
ence I (Geneva Paper Nr 2147, 1958) is briefly discussed. The
following relative capture figures are determined:
63 121 56 27 31 - 115
indicator: Cu Sb Fe k1 P n
measurement
by counter 6-511 8+2 1 o-73~tO-15 1-o4ZLO-15-
by spectro- WA
Card 2/3 meter - 1 0.65�0.15 6+2

Space and Energy Distribution of the Neatrons in Boron
BOY/89-6-6-11/27
Carbide
Figure 2 shows the energy distribution of the neutron flux in
boron carbide for different intervals (energy interval
1.5 - 15 Mev, results standardized in the interval 13.5-15
Mev).
Moreover, the ratio between a U 235 (E eff) and aB 10 (E eff)
of the reaction (n,a) with B 0 in boron carbide was
determined.
In the case of 3 Mev neutrons 0.97 + 0.03 was obtained at
Eeff' 120+10 key. In conclusion, the authors thank I. I. Bon-
darenko for advice and discus8ions',N. D. Proskurnina, V. F.
Bashmakov, A. N. Nikolayev, and V.' I. Popov for assistance
in
the experiments as well as A. N. Serbinov and I. A. Vorontsoy
for work at the neutron generator. There are 2 figures, I
table, and 4 references, 2 of which are Soviet.
SUBMITTED: January 6, 1959
Card 3/3

SOV/120-5'-)-4-4/50
AUTHOR: Kazanskiy, Yu. A.
L
0 ?AZ
i6thh
TITLE: Conversion o p_ ude Distributions into Energy Spectra.
PERIODICAL: Pribery i tekhnika eksperimenta, 1959, Nr 4, pp
32-36
and 1 table (USSR)
ABSTRACT: Sodium iodide and caesium iodide crystals are widely
used in the study of discrete and continuous y-ray spectra.
One of the difficulties in y-spectroscopy is that the relat-
ion between the energy of the y-radiation and the amplitudes
of pulses at the output of the photomultiplier is not unique.
Thus, the instrument spectrum,, i.e. the pulse height spectrum
obtained at the output of the photomultiplier for y-rays with
energies less than 1.5 Mev consists of a well-defined photo
peak and a Compton distribution due to the Compton scatter-
ing in the crystal. In the analysis of complicated or contin-
uous y-ray spectra, it is often necessary to convert the in-
strument pulse height spectrum to the required energy spec-
trum of the incident y-rays. In the most general case, the
problem reduces to the solution for N(E) -of the integral
equation given by Eq (1), where N(v) is the measured pulse
height distribution, N(E is the required energy spectrum
of the y-rays and K(E, V~ is the probability that a
Card 1/5 y-quantum having an energy E gives rise to a pulse
with an
jv~

-39V/120-59-4-4/50
Conversion of Amplitude Distributions into Energy Spectra
amplitude v . In a number of papers (Refs 1 and 2) Eq (1)
was replaced by a system of interdependent linear equations
from which N(E) could be found. The function K(E, V) is
given in the form of a numerical matrLc which is found ex-
perimentally (Ref 2), by approximate numerical calculations
(Ref 3), or is obtained from Monte Cai-lo calculations of the
function K(E. v) . The experimental determination of the
function K(E,, v) in the energy region below 2.5 Mev is
superior to the thecretical calculation, particularly when
the experim.ent involves good collixation. The present paper
is concerned with the experimental investigation of the form
of the instrument spectrum and the efficiency of a single
crystal (CsIf,Tl)) scintillation y-spectrometer. The form
of the instrument spectrum for a mono-energetic y-radiation
was investigated, using the apparatus shown diagrammatically
in Fig 1. The, caesitni iodide c Vystal. used had a diameter of
30 irun an,'. a length of 27 "u!'. it was placed in contact
with
an FEU-2c~ photom,ltiplier inside a lead screen. The y-radia-
tion was collimated by a ool-1.1-m-ator having a hole 10 imn in
Card 2/5

SOV/120-59-4-4/50
Conversion of Amplitude Distributions into Energy Spectra
diameter and 270 Dim long. Pulses from tile photomultiplier
were fed through a cathode follower into a linear amplifier,
followed by a 20-charmel pulse height analyzer. The y-ray
sources were held in a lead holder a'u a distance of not less
than 30-40 mm, from the face of the collimator. In order to
exclude y-rays scattered from the source holder and to re-
duce the contribution from y-radiation scattered in the source
itself, a 2-layer filter (cadmium and lead) was placed in
front of the collimator. The cadmium plate was 1.5 mm thick
and absorbed the 80 Kev fluorescence radiation from the lead
filter. Fig 3 shows the instrument Compton distributions
L(E 01 E) derived from the pulse height distributions mea-
sured for the various sources indicated, obtained by subtract-
ing the photopeak and the scattered y-radiation leaving the
source. Using Fig 3 the instrument Compton distributions for
various initial energies E have been calculated at inter-
vals of 40 Kev. Table I giVes a numerical matrix for L(E Olt;)
obtained in this way. The horizontal rows of the matrix give
the instrument Compton distribution for a given B 0 . The
matrix is normalized so that each number represents the number
Card 3/5 of pulses recorded at the energy E in an interval

SOV/120-59-4-4,/=D
Conversion of Amplitude Distributions into Energy Spectra
AE =:l Kev for 105 pulses in the photopeak. The photopeak
efficiency, i.e. the ratio of the number of pulses in the
photopeak to the number of I-quanta incident on the crystal,
has also been determined both experimentally and by calculat-
ion, using formula (2), in which ex is the efficiency,
d is the thickness of the crystal container, Ill is the
absorption coefficient of the material of the container, f10
is the geometrical solid angle of the c;ollimator 7 r-L ~M is
the effective solid angle of the collimator mid h is the
thickness of the crystal. The dotted curve in Fig 4 gives
ET as a function of ener~T. Using theEe data7 it is possible
to convert the instrument spectrum into the true energy
spectrum of the incident y-rays, Acknowledgments are made to
Card 4/5

z3OV/120-59-4-4/50
Conversion of Amplitude Distributions into Energy Spectra
1. 1. Bondarenko, S. G. Tsypin and V. I. Kukhtevich for
valuable discussion, and to S. P. Belov and Ye. S. Matu-
sevich for help in the present work. There are 6 figures
2 tables and 11 references, of which 2 are Soviet, 1 is
Swissl 1 Swedish and the rest English.
SUBMITTED: May 13, 1953.
Card 5/5

81743
s/o8g/60/008/05/02/Oo8
B006/B056
AUTHOR: Kazanakil, Yu. A.-
TITLE- Angular Energy Distributions of )r-Radiation Scattered
in Water and Iron /7
PERIODICAL: Atomnaya energiya, 1960, Vol. 8, No. 5, pp. 432
- 44o
TEXT: The present paper deals with measurements of the
angular energy
distributions N(z?,?L, E) of r-radiation, (CO 6o-source)
that was several
times scattered in water or iron in semi-infinite geometry.
The distri-
bution of r-radiation scattered in water was measured by
means of a de-
vice which is schematically shown in Fig. 1, while.that
scattered in
iron was measured by means of an apparatus described in Ref.
6. The
gamma distribution was in the first case measured at 5/0-0
r-values (0.5,
1.0, 1.8, 3.5, 4~5) at different 0 (0 - angle of rotation of
the
spectrometer, cf, Fig. 1), and in the second case for
different 0 only
at,uor = 5-9. For measuring r-radiatiOn scattered in water,
sources of
Card 113

8174g/o
Angular Energy Distributions of r-Radiation 8/089/60/00
5/02/008
Scattered in Water and Iron B006/B056
different intensities (137o, 6oo, 194 mG) were used. The
results obtained
by these measurements are shown in numerous diagrams. Fig.
3 shows the
distribution curves for the source-distancen'"Ir = 0,,5
and 4.5 for va-
rious 0. In Fig. 4 angular distributions of the
intensities of indivi-
dual lines are compared witb the theoretical rt~z.-ilt8 of
Ref. 2. In the
care of lino5 265 and 365 kev the deviationa are less than
4CF/6, and at
750 kev - 20%. Fig. 5 shows I. = 27sinG dQ J.N(r, 0,
E)EdE. The angular
distribution curve of intensity takes an exponential
course between
5 - 100 and 900 with an accuracy of 7 - 1096, Fig. 6 shows
the energy
spectrum of the intensity Io = 2'fff sinQN(r, 0, E)EdE. 1
0 was determined
by graphical integration of the distribution N(r, 9, E).
For comparison,
the diagram shows also the curve calculated in Ref. 1.
Fig. 7 shows
the angular energy distribution of X-radiation scattered
in iron. A com-
parison between the r-radiation fraction scattered in
water and iron
and data for concrete (Ref. 4) shows that within the range
of low
energies (100 400 kev) the fraction of a-radiation
scattered by
Card 213

81743
Angular Energy Distributions of ~-Radiation
sj1o89/6o/oo8/o5/o2/oo8
Scattered in Water and Iron BOo6/BO56
concrete is greater. The energy spectrum of intensity 1
0 for iron, which
was also obtained by graphical integration, is shown by
Fig. 8, the an-
gular distribution of the intensities 1 0 by Fig. 9. All
angular energy
distributions of scattered e..,adiation have a more or
iss distinct
maximum near energies that correspond to single
scattering through the
angle 9. Fig. 10 shows the energy distribution for iron
and lead at
0 = 10 and 400. The angular distribution of intensity
may be represented
analytically (within the limits of measuring accuracy)
by the function
10 = ke- 0/00, where 9 0 and 1-: are coefficients; k is
determined by
equation (5), 00 is given for lead, iron, and water in
the Table on p.
439. The authors finally thank I. I~ Bondarenko, V. I.
Kukhtevich, and
S. G. Tsypin for discussions, as %yell as A. N,,
Voloshin and V. I. Popov
for their assistance in the experiments. Th~ai~e f6
iigures, 1 table,
and 12 references! 4 Soviet, 6 American, and 2 Canadian.
SUMITTED: May 26, 1959-
Ll~
Card 313

u
84233
S/089/60/009/004/013/020
B006/BO70
AUTHORSs Dulin, V. A., Kazanskiy, Yu. A., Mashkovich, V. P.,
Panov, Ye.
TITLEt Investigation of the Attenuation Functions for Water
Exposed
to Isotropic and Highly Collimated Sources of_Ejsjj2m
Neutrons
PERIODICALt Atomnaya energiya, 1960, Vol. 9, No. 4, pp. 315 -
317
TEXTs In this "Letter to the Editor", the authors report on
an experi-
mental investigation of the sp ace distribution of fission
neutrons in
water, the source of neutrons being a RP-5 (BR-5) reactor.
The neutrons
came out of a hole in a concrete shield (diameter 250 mia)
and fell on a
tank (137-139-217 cm) filled with doubly gistilled water. The
neutron
beam had a total angular divergence of m5 . The neutrons were
detected
by proportional boron counters. Measurements could be made at
each point
of the tank, and the position of the point could be
determined with an
accuracy of I mm. Fig. 1 shows the geometry. Figs, 2 and 3
show the
measured neutron distributions for different values of r
(distance from
Card 1/3

Investigation of the Attenuation Functions for
S10890009100410131020
Water Exposed to Isotropic and Highly B006/BO70
Collimated Sources of Fission Neutrons
the source) and different values of h (distance from the
beam). Fig. 4
shows the attenuation function of neutrons of an isotropic
point source
m~l.tiplied by r2 (curve a), and the attenuation function of a
highly
collimated plane source (b). The maximum error of the curve a
occurs for
small r (r - 40 cm,,v20%), and the minimum error (-5%) occurs
for large
r. The error of the curve b is between-5% for r - 40 em
andtv20% for
r - 140 cm. The two curves diverge from each other by about
20%, but this
is within the limits of the error of measurement. Therefore,,
for thick-
nesses of water shield larger than 40 cm, the two curves may
be con-
sidered to be coincident. Fig- 5 shows, for comparison, the
experimentally
obtained (Ref. 2) attenuation functions for neutrons of an
isotropic disk
source (diameter 71.2 cm). The attenuation functions according
to which
the curves are drawn readt
G (r) . C nf2 N(r,G)singdG; G (r) - C OD
point 1 0 plane 2 j N(r,h)h dh; and
Card 2/3

84233
Investigation of the Attenuation Functions for
5/089/60/009/004/013/020
Water Exposed to Isotropic and Highly B006/BO70
Collimated Sources of Fission Neutrons
F2--21
Ir +a
Ddisk(r,a) - 21 1 Gpoint (R)R dR. a is the radius of the
disk; N(r,e)
r
and N(r,h) are the distribution functions shown in Figs, 2
and 5; and the
Ci are constants. The authors thank_Q-. I. Leyt)gnskiy and
V. V~ Orlov for
discussions and comments. There are 5 figures and. 4
references: 2 Soviet
and 2 US.
SUBMITTED: April 27, 1960
Card 3/3

ORIDV, V.V., kand. fiz.-mat. nauk, red.; TSYPIN, S.G.,,
kand. fiz.-mat.
nauko red.;- KAZANSXIY _X_u~jtranslatorl; KUKHTEVICH,
V.I. [translatorl;
Ye_.___~t_
MATUSEVICH, S. ranslatorl-; NIKOLAYSHVILI) Sh.S.
(translatorl; SI-
NITSYN, B.I. (translator], YUS, S.V. (tranalatorl;
VISKOVA, M.V., red.;
RYBKINA, V.P., tekhn.iled.
(Protection of transportation units having nuclear
engines; trans:Lated
articleal Zashchita transportnykh ustanovok a iadernym
dvigatelem;
sbornik perevodov. Moskva, Izd-vo inostr. lit-ry, 1961.
619 p.
(MIRA 34:12)
(Radiation-protection) (Nuclear reactors-Safety measures)

23394
S/12o/61/000/002/004/042
A4.2Z42.. E032/Z114
AUTHORS: Dulin, V.A., Kazanskiyj Yu.A., Kuznotsov, V.F.0
and
Smirenkin, G.
TITLE: A single-crystal, fast neutron scintillation
spectrometer with discrimination against gamma-rays
PERIODICAL3 Pribory I tekhnika eksperimenta, 1961, No.2,
PP-35-41
TEXT3 The transformation of the amplitude distribution duo
to recoil protons into the neutron energy spectrum in the
case of
a small crystal (negligible multiple neutron scattering)
for
which the light output depends linearly on the proton
energy, can
easily be carried out by differentiating the experimental
spectrum. In fact, in the case of stilbene which was used
by the
present authors the relation in not linear and small
crystals
cannot be used if an adequate counting efficiency is to be
obtained. The light output duo to recoil protons and the
form of
the amplitude distribution due to monoonargetic neutrons
was
investigated using a Vfn do Graaf generator and the
T(pjn)He3%
D(d,n)H*3 and T(d,n)Ho" reactions. Neutron energies in the
following ranges could thus be obtaineds 0.3-3.5, 4-7.5 and
Card 1/ 7

22394
S/12o/61/000/002/004/042
E032/E114
A single-crystal, fast neutron scintillation spectrometer
with
discrimination against gamma-rays
17-22 Mov respectively. The amplitude distributions due to
recoil protons for 4.3 and 16.8 Mev neutrons are shown in
Fig.l.
The recoil-proton energy distribution P(E) can be obtained
from
the amplitude distribution 4j(V) with the aid of the
following
relations
(~(V)dV - P(E)dE,
P(E) - t)[V(E)j ~LV - F(E) dV
dt R
The functions V(E) and dV(E)/dE which are necessary to
compute
the neutron spectra are shown in Fig.2. The experimental
values
of V(E) are well represented by the Birks theory (Ref.1)
according to which
E E
V(E) A3LdEI const dEl (3)
dEI 1 + kB-dE'tdx
Card 2/ 7 0

12394
S/120/61/000/002/004/042
E032/Ell4
A single-crystal, fast neutron scintillation spectrometer
with
discrimination against gamma-rays
If dE,/dx is expressed in Mev/cm of the range in air then
kB turns
out to be 20 cm/Mev. Fig-3 shows the recoil proton spectra
for
1.0, 1.8 and 3.6 Mev neutrons. These curves were obtained
with a
cylindrical stilbene crystal (30 mm diameter, 15 mm long).
The
curves have a hump at the high energy end which is due to
multiple
neutron scattering. The latter effect is small for neutron
energies greater than about 2 Mev. It can therefore be
neglected
at the higher energies. Fig.4 shows the energy dependence
of the
resolution of the single-crystal spectrometer. The
resolution in
the energy range 1-22 Mev can be described by the formula:
E n/E n = 20/ VKn
The efficiency of the spectrometer A can be described by:
1 - exp [ - 2:(En )dj
I(E E 6E
n
Card 3/ 7

SVP4
S/l2o/61/000/002/oo4/o42
E032/E114
A single-crystal, fast neutron scintillation spectrometer
with
discrimination against gamma-rays
where 6 E is the differentiation stop for the recoil
proton
distribution. The efficiency for the above stilbene
crystal was
found to be about 3% at 2 Mev and about 0.5% at 10 Mev
(the
differentiation step was taken to be equal to the energy
resolution ,C~hEn)- The discrimination against gamma rays
is
based on the differences in the effective scintillation
decay
constant for neutrons and gamma rays. The present authors
have
used the scheme suggested by Birks and described in
detail by
F.D. Brooks in Nucl. Instrum. and Methods, 1959, 4, 151
(Ref-5).
Fig.13 shows neutron spectra for a Po-Be source (curve 1 -
present results, curves 2 and 3 due to B.G. Whitmore and
W.B. Backer (Ref.7: Phys.Rev., 1950, 78, 799) and J.0.
Elliot and
W.I. McGarry and W.R. Faust (Phys.Rev., 1954, 93, 1348,
Ref.8).
It is stated that the overall efficiency for neutrons
having an
energy of 2 Mev has been increased to about 10%. The
gamma ray
efficiency is lower by a factor of 100. Acknowledgements
are
expressed to L.D. Gordayev, Yu.I. Baranov, V.I. Bol'shov
and
Card 4/ 7
R%~
ROt

o4/o42
S/120/61/000/002/0
A single-crystals fast neutron., E032/EI14
Yu.V. Pankratlyev for assistance in this work.
Thero are 14 figures and-9 references: 2 Soviet and 7 English.
SUBMITTED: June 26 1960
A.,
48- IIq-I
41-
44
4-4 4S 1 45 j 4s m

Fig.
Card 5/7

AID Nr. 977-6 27 may
ENERGY DISVIIBUTION OF SCATTERED NEUTRONS IN WATER (USSR)
Dulin, V. A., Yu. A. Kazanskiy, and 1. V. Shugar. Atomnaya energiya,
v. 14, Po. 4. Apr 1963, 404-405. S/089/63/014/004/011/019
The neutron spectra in water from an -15 Mev neutron source have been
measured at distances of 20 to 90 cm from the source, which was an
HNH~ n)He~ reaction with d et te'ron energy of 400 Kev. A
single-crystal
fast-neutron scintillation spectrometer with Y-ray discrimination was
used
as a detector. The results obtained are presented in the form of
histograms
which can be used for determining the relaxation length for a group
of neu-
trons with energy of 14 to 16 Mev. At distances of 30 to 60 and 60 to
90 cm,
the relaxation length was found to be 15. 0 f: 0. 8 and 14. 7 * 0. 9
cm, re-
spectively which is in good agreement with the results. obtained
previously
with a Cu e~ (n. 2n) CU6 2 indicator by B. I. Sinitsyn, [AS
Card 1/1
L
s/oo8g/63/014/005/0488/0490
Amsmai NR: AP3001181
AUTHOR: Dulin, V. _ A. ;Ka-zwwkiyp Yu At #1 1. V.
,Qtrons at the boumlary Of two
TME: Angular energy distribUtiMI-0f re
media
energi".' V, 14"n00 5 1963., 488-490
SOUR=: Atcarawa
TMC TAGS: neutron scattering, reuta=-energy distribution
ABSTMCT: V&asurements were mde of the spectra of scattered neutrons
emrsing at various angles at a bourftry Of Vater and a Plane graphite
layer. A fast -neutron scrurce with a mean energy Of 3 - 9 Mv vRs
Placed
at a 20_cm distance from the boundaryo An H sup 2 (H sup 2., n)He cap
3
amed as the neutron source*
reaction with a deuteron energy Of 900 MY conical
, the required angle vas effected by means Of a
emission W~
The neutron The neutroms Vere
collimator vith an angular resolution of abOUt 5%
ira.ed sciltil tion spe-c"tromet r-
t
recorded 'with a sirJ916'CrYstal Gamm-d"'%Crim by mans cf an AI-100
analyze~r*
The pulse rnplitude distXibutiOn V-%-3 T~ecorded -1 v%
For each scattering angle the eLmplitud.e die=ibatiOl 5 cow'rart=d t~
the
Card 14~_

L 10288-63
ACCESSION 11R: AP3001181
13
neutron energy spectrm by means Of a numerical mutrix and by a
differentiation method. The dMerence betveen the two results did not
exceed 20%, even in the energy rarge from 1. 3 to 2. 0 Wv. The
nzutron ener&v
spectrwa obtained at the graphite, -water boundary is shoun, in the
Fig. 1 of
Enclosure. The results obtained by integration of angular energy
distribution
in the range from 0 to 180* are also platted. The difference
between the
shape of measured and calculated spectra is due tothe difference in
geometry.
"The authors are thankful to An for his valuablp. obsemtions and to
H. D. Proslo=im and V. 0. Dvukhsherstnav for their help in the
vork."
Orig. art. has: 4 figures and I table.
ASSMIATICU . none
=K=m; 14Aug62 DATE Acia: 21jun63
SO CODE: 00 NO M7 SM, 003
ENCL: 01
arm: 001
Card
........... ......... .

AUTHORSt
S/056/634'1001/001/067
B108/Bi80
Bakov, As Tot Bolovt So P., ~qzansk~~uo~k., Popov, V. I.
TITLE3 Comparison of the gamma spectra from the radiative capture
of thermal and fast neutrons
PERIODICALs Zhurnal eksperimentallnoy i teoretioheakoy'fiziki,*V-
44P
no. 1, 1963t 3 - 9
TEXTs The gamma spectra arising from the capture of fast and
thermal
neutrons from a water-moderated uranium reactor in Ung Cot Fe, Nit
and Cu,,
were studied by means of a scintillation gamma spectrometer with an
NaI(Tl) single crystal. To eliminate the gamma background,
the-sample V as,
shielded on the reactor side by a Bi-Pb-Bi sandwich screen, and the
detector by a screen of organic glass and boron carbide. The
spectra of
all five substances were similar in shape (Fig. 4). The difference
in the
gamma intensities produced by fast and thermal neutrons is
attributed to
the effect of P-neutrons. There are 4 figures.
SUBMITTEDt May 9, 1962
Card 1/2

3/056/63/044/001/001/067-
Comparison of the gamma spectra BI08/BI8O
Fig. 48 . Gamma spectra of the radiative capture of thermal
neutrons
(solid line) and of neutrons of the entire reactor spectrum
(dotted) for
Fe. Legendt Ordinate - pulses per Mev.
A(M,7/MeY
Card 2/2

ACCESSION NR: AT4019059 S/0000/63/000/000/0251/0260
AUTHOR: Dulin, V. A.; Kazans1dy, Yu. A.; Matusevich, Ye. S.
TITLE: ExperimenLal methods for the study of shielding (radiation
detector)
SOURCE: Voprosy* fizild zashchity* re*aktorov; sbornik statey
(Problems in physIcB of
reactor shielding; collection of articles). Moscow, Gosatomlzdat,
1963, 251-260
TOPIC TAGS: nuclear reactor. reactor shielding, scintillation
counter, radiation dosimetry,
relative biological, effectiveness, Monte Carlo method, radiation
shielding, radiation detector,
neutron spectrum, Gamma ray spectrum, neutron distribution, Gamma
ray distribution,
radiometry
ABSTRACT: The authors call attention to the need for the study
not only of the total
radiation dosage behind* the shielding, in connection with the
development of nuclear polver,
but also of Its more detailed characteristics (a. g., the spatial
and energy distribution of the
neutrons and gar-nma-rays in the shielding, the angular and
energy distribution of the neutrons
and gamma-rays on the surface of the shielding, eto.). At the
present time, practically all
the niodorn mowis of radiation recording are used to Investigate
the spatial, energy and
Car-d" 1/4

ACCESSION NR: AT4019059
angular distributions of penetrating radiation in the shielding.
The various requirements
levied on sensors of ionizing radiation are reviewed: The point Is
made that in the problem
of the passage of radiation within shielding, exhaustive
information is contained in the
angular energy distribution at each point in space with different
geometries, the anisotropy
functions and the energy levels of the radiation sources. It is
noted that for the development
of computation methods, comparatively incomplete Information such
as the spatial distribution
of the dosage of gamma-rays and neutrons In the shielding, the
behavior of neutron streams
having energy levels above a certain threshold, the angular
distribution of streams of
gamma-rays and neutrons on the surface of the shielding, etc. is
of extremely great value'
In that it permits the application, when studying shielding, of
very simple but nonetheless
effective methods involving the use of dosage and fission
chambers, threshold indicators
and the like. The measurement of integral characteristics is
considered with special
attention to the problems of gamma-ray and neutron dosage
determination. The use
of miniature ionization chambers is discussed and eheir
characteristics are described.
Dosimetric instruments, including scintillation counters, are
analyzed in the light of their
expectable performance In typical applications. A fundamental
shortcoming of such devices
-2/4

ACCESSION NTI: AT4019059
is shown to be their indfflity to measure gamma-ray (loses when
neutrons are present.
I'lic method of pulse amplitude summing as a technique for
enhancing the operational pro-
pcrties of the scintillation dosimeter is described. 'I'lie
fiber-equivalent polyethylene
proportional doLector (for neutron dosage measurements) is
described and its operational
principle analyzed. I'lic concept of the "relative biological
effectiveness" of neutrons as a
function of their energy Is discussed, and the difficulties
encountered In Its precise measure-
ment are outlined. A section of the article is devoted to the
measurement of neutron
streams, in which It is pointed out that the technology of
measuring the spatial distributions
of such streams In the shielding does not differ essentially
from the measurement of flow
conditions encountered in the solution of other problems. The
differences that do exist,
in terms of sensitivity requirements and other instrumentation
paramctcrs, are noted.
The authors noto that gamma-ray spectral distribution studies
are currently being pursued
in two fundainental directions: (1) acquisition of data with
respect to the spectra of the
sources of gamma-radiation (for example, the reactor, the
volumetric sources of gamma-
rays, etc.); quid (2) measurement of the angular and spectral
distributions at the boundary
of the medium, which also describe the radiation sources and, on
the other hand, are
absolutely Indispensable for the computation of shadow shielding
and the passage of
Card 3/4
r
-H.

ACCESSION NR: AT4019059
gamma-rays in heterogeneous media; that is, in those problem areas
which not as yet lend
themselves to analytical computations. Various methods used in this
connection are
discussed; among them, certain experimental techniques involving
the determination of
the form of the amplitude distribution of the pulses, the "random
test method" (Monte
Carlo method), and the use of spectrometers with Nal (T1) crystals.
The final section of
the paper deals with the problem of neutron spectra measurements,
and the techniques
and instruments suitable for such invostigations. "The authors
express their deep
gratitude to A. 1. Abramov, V. I. Kukhtevich, V. P. Mashkovich, V.
1. Popov, B. 1.
Sinitsy*n and S. G. Tsy*pin for their valuable contributions to
this work".
ASSOCIATION: none
SUBAUTTED: 14Aug63 "DATE ACQ: 27Feb64 ENCL: 00
SUB CODE: NP NO REF SOV: 019 OTHER: 015
Card 4/4

Lj
T I P 1,1 ri-tlj

ACCESSION NRt AP4031132 S/0056/64/046/004/1163/1168
~UTHORt Bakov,A. T.; Kazanskiy, Yu. A.
TITLEs *Gamma rays from radiative capture of fast neutrons in man-
ganeae and copper
SOURCE: Zh. eksper. i teor. fiz., v. 46, no. 4, 1964, 1163-1168
TOPIC TAGS: Gamma rays, copper, manganese, radiative fast neutron
capture, Ga~tna s&ctrometry, thermal neutron capture, p neutron,.
negative resonance
ABSTRACT: 17"he measurements were made with neutrons from a Van de
Graaff electrostatic accelerator (using the T(p,n)He3 reaction) and
a single-crystal scintillation y spectrometer. The purpose of the
experiment was,to check the variation of the radiative-capture T-ray
spectr~km with the variation of the partial cross sections correspond-
ing to dif9erent orbital angular momenta. It is shown that, com-
Card
gil" rMAbz
0.0

ACCESSION NR: AP4031132
pared with thermal neutrons, the probability of emission of
-6-MeV
y quanta during the capture of fast neutrons in copper
decreases by
a factor 4--5. This decrease can be attributed either to the
influ-
ence of the change of the gamma ray spectrum with the ratio of
the
(n, y) reaction in different copper Isotopes, to the influence
of
p-neutrons whose cross section becomes appreciable at neutron
energy
-50 keV, or else to a negative resonance with -100 eV energy
causing
the change in cross section of the radiative capture of thermal
neu-
trons in CU63. The results for manganese show a spectrum that
does
not depend on the energy for fast neutrons and lies about 4-5
MeV
lower for fast neutrons than for thermal ones. "In conclusion,
the
authors thank 1. 1.* Bondarenko and A. Vo Maly*shev for
interest and
a discussion, L. A. Timokbin and Yu. V. Xulabukhova for
adjustment
of the 256-cbannel analyzer* and the electroatatic generator
crew."
Orig. art. has: 5 figures and 1 table..
ASSOCIATIONs None
card

Bi7l.0V , S' . F . ; r-11.1 V. h . ; YJLZ A I.'
SK I Y , Yu A.; TS)F I IN , S, X, .
,ilar dlotrIlintion of 3 and 15 Mov. neutrons in
boryllium.
Alir
Atom. eri6rg. 18 no.1:67-68 Ja '05.
(IMIFul IF:2)

Card
-. -~
I

Nc REF
Conj

L 14697-66 EWT(m)/ETC/F/EPF(n)-2/gWi3(m)/EWP(t)/DrP(b)/EWA(h) IjP(c)
TD/WW/,T /DM
ACC KR: AP6008249 SOURCE CODE: UR/OW9/65/019/005/0452/0453
AVrHORt Belov, So P.; pikdnj V, .; Ka!Eskih Yus A.; PoEov,_V._I.,-
Lobakov,,
A.
(RG:' none
TITIE; Secondary gamna-emissioPcoefficients for aluminum, copper, and
tungsten
-J-1
SOUME-. Atom-Aya energiya, v- 19, no- 5, 1965,, 452-453
TOPIC TAGS: aluminump tungetenp copper, gamma flux, neutron flux, gamma
quantum,
secondary emission, radiation shielding
ABSTRACT: The coefficient of-secondary gamma amission-the ratio of total
capture-gar-= flux with energies above threshold emitted from a shielding
surface
to the tatal neutron flux le4ving the same surface-was determined for
Al,, Cu.
and W, using the RIZ reactorfle the neutron eource. Measurewnts were made
for gazima quanta over '>c ~ev and for shieldiniz thicknesses of 20 cm
for Al,
9.5 to 48 cm for Cu, and 5 to 17 cm for W. tNA-T -65.,
SUB CODE: 180 20 SUM DATEt l0Mar65 ORIG REF: 004
CardiA WD % 539.122
'15
IM EK.

L 22419-66 EWT(n)/E*A(h)
:ACC NR: AP6007950 SOURCE CODE: UR/oo8g/0'6/020/002/0143/011,'3'
'AUTHORS: azaaQ x
_K lu,_Aj TryKQy_.,_.L,__ A. DL n, V. A.
.ORG: none
TITLE: Transformation of integral amplitude distr1hutions into
,neutron energy spectra 11_*0
Of lyll~ 0%1N_1
SOURCE: Atomnaya energiya, v. 20, no. 2, 1966, 143
!TOPIC TAGS: neutron spectrum, neutron detector, scintillation
,detector, pulse height analyzer, nuclear reactor shield, iron,
beryllium
ABSTRACT: This is an abstract of article No. 52/3404 submitted to
--.-the--sourc editor - but--not- published- -in -full.- - The
authors-improve- the
:accuracy witb-wbieb tbe-neutron energy spectrum'Is obtained by
dif-
,ferentiating the integral spectra of pulses from a scintillator.
This
!is done by using a least-squares method of determining the
derivative,
Card 1/2 UDC: 539:16,.08:539-125.5

L 22419-66
ACC NR: AP6007950
idecreasing the fluctuations that result from differentiation
of ex-
,perimental amplitude distributions. The algorithm for
finding,the
:derivative of the empirical curve is simple, since It is
based on
i
approximating a section of the empirical curve by a
second-order
1parabola. If the pulse-height distributions vary over the
differan-
~tlation section by not more than a fact-or 2 -- 3, the
obtained
'derivative will differ from the analytic value by not more
than 1
13%. The resu.its are illustrated with spectra of reactor
neutronsthat
:have passed through different thicknesses of Iron under
good-geometry
;conditions. The unpublished article contains detailed
cbaracteris-
~tics of the spectrometer employed, its block diagram, the
gamma-ray
idiscrimination system, and also results of measurements of
spectra
i,of standard source and spectra of reactor neutrons passing
through
idifferent thicknesses of beryllium. Orig. art. has: 1 figure.
SUB CODE: SUBM DATE: 03Aug65/ ORIG REF: 002/ OTH REF: 001
Card.,

L IW5~91;-70-i
ACC NKs AT6027932 SOURCE CODE: UR/0000/66/000/000/0164/oi-6~~,0:
~AUTHOR: Abagyan, A. A.; Belov, S. P.; Kazanskiy, Yu. A.; Popov,
V. I Fadeyev, I. A.J
jDubinin,-T A.
ORG: None
TITLE: On the function of effectiveness of shielding materials
with respect to captur
gamma-radiation -11
SOURCE: Voprosy fiziki zashchity reaktorov (Problems in physics of
reactor shielding)
sbornik statey, no. 2. Moscow, Atomizdat, 1966, 16?4-169
TOPIC TAGS6. radiation shielding, radiative capture, gamma
radiation
ABSTRACT: The authors compare experimental. and theoretical data
on the function of
effectiveness of shielding materials with respect to capture
y-radiation in nickel.
The function of effectiveness is expressed as a linear combination
of quantities of th
type hAp
Pa
PA
where pA and PB represent the concentrations of the respective
components in the
Card 1/3 -

0
ling materials. This function shows the change which takes
place in the functional
when a unit of substance B is substituted for a unit of
substance A where
14-T - - H
E) 18Aod'
4nr! (r, E) e BjdjLdEdV
describes the production and yield of capture y-raaiation. In
this formula O(rj, 11, E)
is neutron flux; (r,, E) is the macroscopic cross section of
radiation neutron cap-7.
ture; *Pj is the yield of y-quanta of given energy Ef per
captured neutron; At is
~
Ithe dose created by a unit flux of y-quanta of energy Ej,
10(r) is the total coeffi~
cient of linear absorption of y-quanta of initial energy Ej; Bi
is the dose factor for
accumulation of y-quanta of initial energy Ej. The function
f(x) was experimentally
studied by introducing a hydrogen-containing substance into a
nickel screen made up Of
I
sheets measuring 8Ox8OxO.8 cm for an overall thickness of 25
cm. This specimen was
surrounded by a neutron shield for reducing the background. A
single-crystal scintil-
Ilation gamma-spectrometer with a crystal of sodium iodide was
used for measuring the
I
,number of capture y-quanta with an energy of greater than 7
Mev produced by radiation
capture of neutrons in the nickel. Curves are given showing
neutron hazard functions
!with respect to capture y-radiation. These functions describe
the contribution of
!neutrons to the stream of y-quanta behind the screen as a
function of the neutron
-enei-gy and inlet coordinate. The results show that the
addition of bydrogen-containing
maLerial through nearly the entire thickness of the nickel
layer increases the inten-
Card 2

- -6'-67
n C I
V
ACC NRt AT6027932
.sity of capture y-radiation behind the screen. An exception to
this rule is the first
1
!6 em of nickel where the neutron hazard function for low energy
particles is lesSthan
the ftuiction for high energy neutrons so that a good moderator
placed at these points
reduces the intensity of capture y-quanta behind the screen. The
authors thank V. V.
10 1
r ov, V. Ya. Pupko and S. G. Tsypin for interest in the work.
Orig. art. has.
'figures, 17 formulas.
,SUB CODE; 18/ SUBM DATE: 12Jan66/ ORIG REF: 005
Q -1

- r, o5ohM7 wr W alan
AU_ NKi XT6027922 SOURCE CODE: uR/oooo/66/000/000/0072/0073
AUTHOR: -Dulin, V. A.; Kazanskiy., Yu. A.
ORG: None
TITLE: Angular distributions of fast neutrons in various
environments
SOURCE: Voprosy fiziki zashchity reaktorov (Problems in physics
of reactor shieldi
sbornik statey, no. 2. Moscow, Atomizdat, 1966, 72-73 " 4
TOPIC TAGS: angular distribution, anisotropic medium, neutron
energy distribution,
fast neutron
ABSTRACT: The authors consider the angular energy distributions
of fast neutrons un-
der conditions of barrier geometry as a function of the atomic
weight of the ambient
medium, the thickness of the barrier and the energy and shape
of the neutron source.
For media which do not contain hydrogen, the angular
distribution of the radiation
within the solid angle 2usinede from an isotropic point source
of neutrons with an
energy of 3.4 Mev at angles of 20-700 is isotropic and
practically independent of
atomic weight and thickness of the medium (for a thickness of
1.5-5 times the mean fr
path) with an accuracy of 20-30%. As the energy of the neutron
source is increased,
the dosage in this solid angle begins to show angular
anisotropy. Curves are given
showing the angular distribution of fast neutrons with an
energy above this threshold
value. The results show that the angular distribution of fast
neutron radiation for

L o5048-67
ACC-NO-I--AT6027922
angles greater than 300 is !-.dependent of the form of the
environment or its thickness
and is not even affected by the energy and shape of the neutron
source. The measure-
ment error is less than 10%. It is possible that this
conclusion will not be valid foi
a greater thickness and neutrons in the reactor spectrum. The
authors thank S. G.
Tsypin for useful consultation and V. G, Dvukhsherstnov for
assistance in the work.
Orig. t. has: 2 figures.
/00
SUB CODE!20,/2/ SUBM DATE: 12jan66/ ORIG REF: 003/ OTH REF: 001
Card

L 05056-67
Ak-L W__' '627931 Soma com UR/Oou/66/000/000/Ql56/0163
AUTHOR: Bakov, A. T.; Kazanskiy, Yu. A.
ORG: None
TITLE: Gamma-quanta from radiation capture of resonance and fast
neutron (a survey)
SOURCE: Voprosy fiziki zashchity reaktorov (Problems in physics
of reactor shieldin
sbornik statey, no. 2. Moscow, Atomizdat, 1966, 156-163
TOPIC TAGS: radiative capture, gamma, radiation, fast neutron,
radiation shielding
ABSTRACT: The authors review the literature published before
January 1964 on the
spectra of y-quanta from radiation capture of fast neutrons. The
causes for varia-
tions in these spectra and the available experimental data are
summarized. Require-
ments are formulated for studying radiation capture y-quanta
from the standpoint of
shielding design. All variations in y-quanta spectra are
greatest for the hard radia-
tion region. Where the intensity of the transition to the ground
state is high, fluc-
tuations alter the remaining portion of the spectrum. Contrary
to expectations the
spectra of capture y-quanta in almost all experiments are
practically independent of
neutron energy in the 30-500 kev range. The considerable
differences between the! spec.
tra, of capture y-quanta on various resonances as well as the
differences between these
spectra and those resulting from capture of thermal neutrons
make it necessary to mea-
Card I

L_o5,o56_67__
sure the averaged spectra of y-quanta on several resonances. These
measurements
should be made with incident neutron spectra of the form IIEn and
with rather thick
specimens for averaging with respect to neutron spectra which are
close to those es-
tablished in the material being studied. Much of the literature on
the spectra of
-y-quanta from capture of nonthermal neutrons has no practical
application for compari-
son of the necessary group spectra of capture y-quanta since the
measurements are
qualitative (do not indicate the number of y-quanta per capture). A
table is given
summarizing the experimental data on the absolute yield of -y-quanta
rrom. radiation
Icapture of neutrons with various energies. Orig. art. has: 1
figure, 1 table, 6
Iformulas.
ISUB CODE: 18/ SUBM DATE: 12Jan66/ ORIG REF- 012/ OTH REF: 023
Card 2/2
4~'

L 05069- n
67 IT JR/QD
6 uR/oooo/66/000/000/0170/0174
027933 SOURCE CODE:
,AUTHOR: Abagyan, A. A.; Belov, S. P.; Kazanskiy, Yu. A.;
iORG: None
~TITIS: Measurement and calculation of the coefficients of
secondary gamma-radiatig
SOURCE: Voprosy fiz-4ki zashchity reaktorov (Problems in physics
of reactor shieldi:Z11
sbornik statey, no. 2. Moscow, Atomizdat, 1966, 170-174
!TOPIC TAGS: gamma radiation, neutron, radiation shielding,
capture cross section
iABSTRACT: The authora conBider the coefficient of secon(Inry
einission 0 which expres-
ises the ratio of the total number, dose or energy of capture
y-quanta to the total num-1
i i
lber of neutrons emitted from a given shielding material. The
general expression for
ithis coefficient is
:S 1,(r.2,E-)X.,T(E-)I,(E)~('r.rj.Ej)dSZdEdVds
if
J4) (r,, 9, E) dQdEds
iwnere w(r, 9. E) is the neutron flux at the point r in the unit
energy interval at
I
lenergy E and in the unit solid angle about the direction Q.,
Y,,..v (E) is the radiation
;capture cross section for neutrons of energy E, 11i(E) is the
yield of y-quanta of I

L 05069-67
energy Ej per capture of a single neutron with energy E; ~)(r,
r,. Eo is the func-
tion which gives the attenuL*,ion of the stream of y-quanta
with energy Ej from the
point of y-quantum production r to the points r, on the
surface. A formula is derived
for the asymptotic value of 0 determined by the physical
properties of the shielding
material alone. A comparison of theoretical and experimental
asymptotic values of B
shows a systematic divergence by a factor of approximately 25,
the theoretical data
being overestimated. The reason for the divergence is assumed
to be inaccurate deter-
mination of neutron intensities at the boundary. In spite of
the discrepancy between
experimental and theoretical data, the nearly constant
divergence obtained for various
elements with large, small and moderate capture cross sections
(tungsten, lead, iron
and nickel) indicates that the proposed method may be used for
calculating the asymp-
totic values of 0 with an accuracy of 30X if a correction
factor of 2.6 is used. The
authors thank S. G. TM n and V. Ya. Lllupko for interest in
the work and useful re-
marks. Orig. art. has: 3 figures, 6 formulas.
SUB CODE: 18/ SUM DATE: 12Jan66/ ORIG REF: 003
Card
R

L 06979-67 EWT(m) JR SOURCE CODE: iiiVoOB9/66/020/005/0424/0421,
ACC NR: APS018354 (N)
.AUTHOR: Kaxanakiye-XV-9 Ar'. Kukht0vicht V, I-; P0.poyL_V. I.;
Tarasovt V. V.;
sh,omotenko, B. P~
;ORG: none
JITLE: Dependence of the bixildup factor on the location of the
detector behind
,the shield
Atomnaya onergiya, v. 20, no. 5, 1966, 424
TOPIC TAGS: roactor shielding, gan= scatterill9t ga=-&
detOctA", scintMgtAon
,detector
ABST.TtACT: This is an abstract of article No. 76/3559,
submitted to the editor and
filed, but not published in full. inasmuch as earlier
investigations of the build-
tip factors, with the aid of vhich account is taken of the
scattered Cam= radia-
tiony were made for observation points situated either inside
or on the surface of
the shield. the authors measured the accumulation factors with
a radioactive source
of gamma radiation (Cs13?) at difforant positions of the
detector and the source
behind an aluminum barrier of thickness equal to 2'.8 mean free
paths-."of di=9ter
Card V2 UDC: 539-122:539-121-72-

L 06979-67
ACC NR: AK418354
40 cm. The measurements were made with a scintillation detector
(stilbeno cry-
stal). The distance from the source to the shield surface facing
the detector
ranged from 18 to 150 cm. For each valuo of this distance, the
distance from the
surface of the shield to tho dotootor was variod from 0 to 500
cm. The rosults show
that the decrease of the accumulation factor with increasing
distance R has the
form (3A!Ln6)exp(-kT9) for a point-like isotropic source on the
surface of the
shiold, and the form oxp(-kpcp) for a plane parallel boam. The
test rwult.3 Vere
compared with values calculated in accordance with a
semiempirical procedure des-
cribed by the authors earlier (Byulletent Informatsionnogo
tsentra po yadernym
dannym CUU. of Wormation Center on Nuclear Data] no. 2p
Atoxisdat, 1965, p.
,305. Orig. art. has: 1 figure.
SUB OODS: 18~, SUBM DATE: 30D*c65/ OEM REF: 002 OTH REP: 002
Card 2/2

"JD
001665 souRcE CODE, UR/0094/66/000/008/0016/0018.
AUTHOR: Kazantseva
(Engineer; Orgpishcheprom)
ORG: none
TITLE: Ultrasqnics/to prevent boiler scale
i It
SOURCE: Promyshlennaya energetika, no. 8, 1966, 16-18
TOPIC TkGS: ultrasonics, steam boiler
IABSTRACT: The article reports on the experimental use of
ultrasonic apparatus
Ito prevent accumulation of boiler scale. Successful results
have been ob-
Itained so far with smaU-capaeity boilers (steam rate up to
2.5'tons/hour)
of the VGD, Shukhov., DKVR, Lancashire and locomobile types;
further work
is being done with larger-capa city boilors (up to 6
tons/hour). Ultrasonic
pulses are generated by a device consisting of a capacitor, a
thyratron and
a magnetostrictive transducer set. The capacitor is energized
from the power
line through a rectifier-usually a 6N83 twin triode with
soparate cathodes.
'W,o capacitor discharges throudi a thyratron, uswxlly a
hydrogen-fillod TG11-
4,CO/3,5 type Ishich operates over a wide range of fmquonciea
and powor, pro-
duci:ng 10-20 A pulses of 10-15 microsec duration. Various
methods of triZ-
garin., were tried out and the blocking-oscillator achoma was
found most
pro.-doin.- of all. The magnetos trictivo transducers in t~ie
form of nickel
platee 0.03 mm thick and 25X25 = area are wuldod to
3/4-wavulcngth conduita
!~_qard UDC: 0'21.187.12/-3+621-034-4~

ACC NR: A1,7001665
which carry tho ultrasonic pulBeo to tho boiler druia at a f(nt
naloctod
locationa; thora the conduito are welded to the dram wall.
Ultrisonia
pulses thus produced and carried into the operating. zone can be
effective in
a steam generator where the -yrater hardnea3 is up to 8 ppm.
Further de-
velopment worl, is required to perfoot this method of preventing
boiler Scala;
much benefit can be derived from the practical experience Zaimd in
tho
Krasnodar District of the RSSR. Orig. art. has: 2 figures. 1JPRS:
37,8111
SUB CODE: 20, 13 SUBM DATE: none
Card 2A-

I I V.!-,; Yu.4.
1114 WIAM i I
Polar rallftnce netar. Trudy fnnt. ckvsr. "W'.Ali '05.
0-9"H-l 1~8;12)

L 0902 7
ACL'NRI AV00233U ODE1 UR/2944/66/000/003/0105/0112
AUTHOR: Eazarinovo Yue Fe
13
0 RG ;none
TITLE: Hiximum principle for the problem of the miximization of an
integral
functional with variable lag
SOURCE: Loningrad. UnIversitat. Kafedra Vychislitellnoy matematiki
I vychislitalln
tsentre Netody vychislonly, no. 3, 1966, 105-112
TOPIC TAGSt ordinary differential equation,, differential equation
system
ABSTRACT:, Manufacturing proce6ses involved In the working of
various products
are ofteii described by a system of ordinary differential equations
containing
control-parameters, while production output is described by the
value of a
,certain Integral functional dependent on the retarded aroumentr
(t)9 'Whi ch is
given by the functional relation connecting the phase coordinates
of the system..,
at moments t and % (t), The determination of the process conditions
which'
:assure maximum output involves the problem of the maximization of
the functional
fe (X Y), A (%), U (t)) dt.
Card 1/2

L 09096-67
ACd-kk-,-AVoo233B
X(t) ~~ (**I (t), xn(t) I f
x 8 vector-fuincilon satisfying the system o
:differential equations
u _1, 21
.with the bounda ry conditions
(it) E r., ic Vj) E ri.
u(t) - (u u Is the control vector which must be chosen, while
r (t) Is determined from the condition
7 (X W. -V W) 0.
The case in which the lag 0 - t is constant was considered by L. S.
-PONTRYAGIN, V. G. DOLTYANSKIY, R. V. GAMKRELIDZE, and Ye. F.
HISHCHENKO in theiri,
jbook Matematicheskaya teorlya optimal*nykh protsessov
(Mathematical Theory of
10ptival Processes)4 The purpose of the present article to to
extend L. S.
PONTRYAGIN's maximum'principle to the case
formulated.suprap,/-'Origo art$ heat
20 formulas
SUB CODEs i2 PRsi 38,16V
SUBM DAM lOD~c62
Cwd-~/2 nst

I-';: I Y. Y,-:. N.
t I,~iAY, YU. li. -- "I-L-TA IIJING 111(o) CA!-
C,-ar~OIJCT I VIf I 1-~~ T I C': "N AHEN!
M ~CU~l ',,I AT I ou TFCH I:.) LiA?I- T--I '~L A F I
3UL: 6 !-,A[!
uj CANDMATE m Tvc,mICAL
VrClil-'MAYA JANLIAPY-DECEMER 1 2

PHASE I BOOK EXPLOITATION 680
Golldberg, Mikhail Markovich, Zakharov, Vasiliy Aleksandrovich,
KazanBkIZ,_ Yx~riy Nikolayevich, Leontlyeva, Valentina
P6fr_ovna, LoBiv-,--Iv-a-n-Fl-at-o-n-o-vlbh, TrostyanBkaya.
Yelena
Borisovna, Khazanov, Grigoriy Mikhaylovich, Chebotarevskiy,
Vladimir Vladimimirovich, and Sheydeman, Igor' Yur'yevich
Nemetallicheskiye materialy i ikh primeneniye v aviastroyenii
(Normetallio Materials and' Their Use in Aircraft Construction)
Moscow, Oborongiz, 1958. 428 p. 15,000 coPies printed.
Eds.: Losev, I.P. and Trostyanskaya, Ye. B.; Reviewere: Bondarev,
V.S., Engineer; Scientific Ed.: Panshin, B.I., Candidate of
Technical Sciences; Ed. of Publishing Housei Tubyanskaya, F.G.;
Tech. Ed.: Rozhin, V.P.; Managing Ed.t Sokolov, A.I., Engineer.
PURPOSE: This is a textbook for students at advanced aeronautical
engineering schools and may also be useful for engineers and
technicians in industry and at scientific-research institutes
who are interested in nonmetallic materials.
Card 1/23
771.7 77~77,

Nonmetallic Materials and Their Use (Cont.) 680
COVERAGE: The book describes the characteristics and properties
of nonmetallic materials and the technology used in their
production and also the shop processes by which they are
fabricated into structural members, assemblies, and aggregates.
The information given in the book covers the entire range of
nonmetallic materials used in aircraft construction, namely:
plastics. rubber, paper...wood and textiles, glue, lacquer,
paints, and coatings. The authors made use of the results of
a pedagogic experiment of many years standing, i.e., the
lecture
course "Technology of Nonmetallic Materials" given at MATI
(Moscow Aviation Technology Institute) and MAI (Moscow Aviation
Institute). The book was compiled by workers in the department
"Technology of Treatment of Nonmetallic Materials" at the MATI
and of the department "Engineering Materials" at MAI under the
general direction of the editors, I.P. Losev, Professor,
Doctor of Chemical Sciences, and Ye. B. Trostyanskaya,
Professorp
Doctor of Technical Sciences. The authors of the first and
second chapters are Ye. B. Trostyanakaya and I.P. Losev; of
Card 2/23

Nonmetallic Materials and Their Use (Cont.) 68o
the third chapter, Ye. B. Trostyanskaya and G.M. Khazanov; of
the
fourth chapter, V.P. Leont'yeva; of the fifth chapter, V.A.
Zakharov;
of the sixth and seventh chapters, Yu. N. Kazanakiy; of the
eigth
chapter, I-Yu. Sheydeman; of the n-D!th--cYa-p`Fe-r-,--Ye-.
B. Trostyanskaya,
and those of the tenth chapter, M.M. Golldberg and V.V.
Chebotarevskly.
The section of the seventh chapter "Mechanizing production
methods
used in molding objects from plastics" was written by 0.1.
Shapiro,
and the section of the ninth chapter "Mechanical
reinforcement of
articles made of nonmetallic materials" by V.P. Leontlyeva;
the
author of paragraph 5.in that section was I.Yu. Sheydeman. The
authors thank Ya. D. Avrasin, V.S. Bondarev, and M. Ya.
Sharov for
valuable advice and B.I. Panshin, Candidate of Technical
Sciences, for
his assistance in readying the manuscript for publication.
The book
contains 18o figures and 30 tables. There are 50 references,
of which
48 are Soviet and 2 English.
Card 3/23

Nonmetallic Materials and Their Use (Cont.) 68o
TABLE OF CONTENTS:
Preface 3
Ch. I. Nonmetallic Materials Pertaining to the High Molecular
Organic Compounds
1. Special features of high molecular organic compounds 7
2. Classification of high molecular compounds 11
3. High molecular compounds 13
Cellulose and products from chemical processing of
cellulose 13
Natural rubber 17
Albumen 20
Natural resins 21
4. Methods of obtaining synthetic high molecular compounds 23
Card 4/23

Nonmetallic Materials and Their Use (Cont.) 68o
Obtaining high molecular compounds by polymerization 24
Obtaining high molecular compounds by polycondensation 26
Obtaining high molecular compounds by the method of
chemical conversion 27
5. Synthetic high molecular compounds 28
Synthetic resins 28
Synthetic rubber 32
Ch. II. Plastics
I. Basic Components Entering into the Composition of
Plastics 34
1. Adhesives used for the manufacture of plastics 34
Thermosetting resins 35
Thermoplastic resins 40
2. Plasticizers used in the manufacture of plastics 44
3. Fillers used in the manufacture of plastics 46
Powdered fillers 47
Card 5/23

Nonmetallic Materials and Their Use (cont.) 68o

Fibrous fillers
49

Flake f,.'.lers
49
4.
Othe7 components entering into the
composition of plastics
50
II.
Molding powders and casting
materials
51

Thermosetting molding powders
51

Thermoplastic casting
materials
6o
III.
Fibera
67
IV.
Iaminated plastics
71
V.
Sheet plastics
not containing fillers
77
7.
Organic glass
77
8.
Vinylplastics
31
9.
Celluloid
83
VI.
Foam plastics
85
Card
6/23

Nonmetallic Materials and Their Use (Cont.) 680

Ch.
III. Rubber Materials

I.
Characteristic properties of rubber material determining

of application
go
II.
Basic components entering into the composition of rubber
91
1.
Caoutchoucs
used in the manufacture of synthetic rubber
92
2.
Fillers used in the
manufacture of rubber, rubber

materials and products
97
3.
Vulcanizing agents
100
4.
Softening agents and antiagers used in rubber production
100
5.
Reclaimed rubber and its used in rubber production
103
III.
Technology
producing rubber mixtures
103
6.
Manufacture of rubber mixtures with powdered
fillers
103
7.
Manufacture of rubber materials with fabric fillers
10
8.
Hard-rubber mixtures
108
Card
7/23

Nonmetallic Materials and Their Use (cont.) 68o
IV. Testing methods and Characteristics of rubber obtained
from various rubber mixtures 110
Ch. IV. Paper Materials
1. Manufacture of paper materials 115,
Preparation of fibrous raw material 11t)
Preparation of paper pulp 117
Conversion of paper pulp to paper and carboard 118
2. Papers and carboards used in aeronautical engineering 120
Types of papers and carboards 120
Basic properties of paper and cardboard and methods of
determining them 122
3. Fibers 125
4. Molded paper 127
Ch. V. Methods of Forming Objects from Plastics, Rubber and
Paper Materials
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Nonmetallic Materials and Their Use (Cont.) 68o

I.
Basic
characteristics of the technology of forming

processes
128
II.
Ordinary and pressure molding
131
lo
Methods of ordinary and
pressure molding
134

1"t,eparation of materials before molding
134

Measuring out and loading the materlAl into the pressure

mold
136

Preh eating the molding material before application of

pressure
137

Conditions for molding
140
2.
Special features of
processes in molding members made

of plastics and hard rubber
prepared in pressure molds
144
3o
Equipment for ordinary and
pressure molding of articles

from plastics and rubber
148

Pressure molds
148

Presses
153
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Rt

Nonmetallic Materials and Their Use (Cont.) 68o
Pumps and accumulators 158
III. Fressure molding of
Materials
4. PrF.,3ure molding of
5. Pressure molding of
6. Equipment and molds
Molding machines
Molds for pressure molding
thermoplastic and Thermosetting
16o
thermplastic materials 161
thermsetting materials 165
for pressure molding 167
167
168
IV. Forming parts from plastics and rubber by the extrusion
method 173
7. Forming various cross-sectional shapes from thermoplastic
plastics and rubber by the continuous method 174
8. Forming various cross-sectional shapes from thermoplastic
materials by the cyclic method 178
Car6 10/23
Mk*w la azq~Qiy

Nonmetallic Materials and Their Use (Cont.) 68o

9. Forming
various cross-sectional shapes from thermosetting

plastics by
the continuous method
179
V. Forming three-dimensional parts by
stamping
181
10. Basic operations in stamping parts from
thermoplastic

and thermosetting sheet plastics
182
11. Basic
operations in stamping parts from fiber
186
12. Various
stamping methods
187
Forming with a rigid punch and die
187
Forming with a rigid punch having a pressing frame
188
Forming
with a rigid punch and draw-die ring
188
Vacuum and pneumatic
die forming and "blow molding" of

hollow parts
189
Vacuum and
pneumatic draw-die ring forming
191
Pneumatic and vacuum
forming by use of a removable punch
193
VI. Forming large-size
objects from plastics with and elastic

punch
194
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Nonmetallic Materials and Their Use (Cont.) 68o
13. Basic methods of forming by means of an elastic punch
14. Process of forming large three-dimensional objects
from fibrous or laminated materials
VII. Manufacturing products from light porous materials
15- Manufacturing products with honeycomb fillers
16. Molding objects from foam plastics
Stamping
Forming in rigid molds
ForMing to Bc&le
Forming by "oelf-expansion" in the die
VIII. Manufacture of products from paper pulp
IX. Manufacture of some rubber products
17. Manufacture of rubber fuel and oil tanks
18. Manufaqture of rubber tires
19. Manufacture of rubber hoses
195
198
202
202
203
203
203
205
207
211
214
214
218
21
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Nonmetallic Materials and Their Use (Cont.) 68o
20. Manufacture of rubber conveyor belts and transmission
belts
Ch. VI. Wood Materials
I. Wood
1. Types of wood used in aircraft construction
2. Properties of wood
Physical properties
Mechanical properties
3. Defects in wood
4. Protecting wood from moisture, injury by fungi, and fire
5. Preservation and drying of wood
II. Wood Materials
6. veneer
7. Plywood
8. Other wood materials
Card 1343
219
222
222
223
223
225
231
232
233
235
235
236
238

Nonmetallic Materials and Their Use (Cont,)
Ch. VII. Cutting Nonmetallic Materials
I. Basic cutting processes
II. Cutting wood
1. Sawing wood
Saws
Powered cutoff saws
Operating rate for powered cutoff saws
2. Planing and milling wood
Planing tools
Milling tools
Planers
milling machines
Applications of wood planing and milling
3. Drilling wood
Card 14/t3
68o
241
247
247
247
250
255
255
255
256
2Z9
2 1
266
266

Nonmetallic Materials and Their Use(Cont.) 680
4. Sanding wood
5. Hand-operated mechanized tools
III. Cutting paper materials
IV. Cutting plastics
6. Laying-out plastics
Sawing laminated plastics
Sawing and cutting organic glass and vinylplastics
Sawing and cutting oam plastics
7. Planing and milling plastics
Planing and milling laminated plastics
Milling organic glass
Planing and milling foam plastics
8. Drilling and threading in plastics
DrillinL laminated plastics
Drilling organic glass
Card 15/23
267
267
268
269
269
269
271
272
270
272
274
275
27
272
276

I
Nonmetallic Materials and Their Use (Cont.) 68o
Drilling phenol-aldehyde plastics with powdered

filler and drilling
aminoplastics
276
Drilling foam plastics

Threading in plastics
277

9. Turning plastics
277

10. Stamping and puncing plastics
278

11. Grinding and polishing plastics
279
28o
12. Mechanizing production methods used in molding objects

from
plastics
281
Ch. VIII. Textile Materials

I. Textile fibers

1. Structural characteristics and classification of
288
fibers

2. Most important types of fibers, their composition and
288
use
Natural fibers
289

Synthetic fibers
289

Compound fibers
290

3. Physical and mechanical properties of textile fibers
292
O)l
2
II. Textile products
,

Card 16/23
298
Nonmetallic Materials and Their Use (cont.) 680

298
4.
Felt
298

Yarn and threads
299

Spun articles
300
7.
8
cloth titutes and lacquered fabrics
Leather subs
304
.
III.
ft construction
Textiles used in aircra
30
30
9.
Textiles used inside an aircraft

s; textiles
Heat-insulating and sound-proofing material

3o6

used in decorating and trimming
310

Materials for electrical
insulation
312

Fabric for aileron balance
313

Reinforcing strips
'
313
10.
exterior use
Aircraft textiles for
313

Linen-covering materials

s of wooden
airplanes
Glued-on fabrics used as covering

31

and propellers
31

engine covers
Fabrics for airplane or

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Nonmetallic Materials and Their Use (Cont.) 66o
11. Preservation of aircraft textile materials 316
Ch. IX. Joining Structural Parts Made of Nonmetallic
Materials

to One Another and to Metals

I.
Gluing nonmetallic materials
318
I.
Gluing articles made of wood and paper
322
2.
Gluing
articles made of plastics
324
3-
Gluing foam plastics to foam
plastiesp to wood, and to

laminated plastics
326
4.
Gluing wood,
foam plastics, and laminated plastics to

metal
326

9.
Gluing rubber
330
0
Gluing rubber to metal
331
II.
Welding
structural parts made of thermoplastics
333
7.
Contact-welding
method
333
8.
Welding in a jet of hot air
334
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77

N
.Vin h, 3 a
Vill 3 :ifd
9~
%I
V
19
I a
ILI

z/oil/61/018/001/007/014
E112/E453
AUTHORS; GolIdberg, M.M. and Kazanskiy, Yu.N.
TITLE. Determ nation of absolute viscosity of alkyd resinA(for
paintsi
PERIODICAL: Chem-le a chemicka technologie, 1961, Vol.18, No.1,
P~31,
abstra-,t CH 61-430 (Lakokras, Materialy, 1960,
No.1, pp.68---71)
TEXT. To follow the course W *' e3terification, a special
Viszometer with an elastic thread'is recommended, It offers the
advantage that its sensitivity can be changed over a wide range
by
using threads of varying diameter and length, It permits to
measure the absolute viscosity over a temperature range of 80 to
250-C. The viscosity graphs of some alkyd resins are shown.
Cross-se,~tion and photograph of apparatus, 6 diagrams,
[Abstractor's note: Complete translation.)
Card 1/1

KAZkNSKIYq Yu.N.
Viscosimeter for determining viscosity in the production of
alkyd resins. Iakokras.mat. i ikh prim. no.2:55-61 161.
1 1 (MIRA 14:4)
1. Moskovskiy aviatsionW tekhnologiphepkiy institut.
(Alkyd resins) (Viscosimetor)
Iz

GOLIDBERG, R.M.; KAWSKIY, Yxj.N.
Investigation of the absolute viscosity of lacquer alkyd bases.
Lakokrae.niat. i ikh prim. no.1:68-71 160. (mIRA 14:4)
L. Moskovskiy aviatsionnyy tekhnologicheskiy institut.
(Alkyd resins)

S/081/62/000/007/028/033
B168/B101
AUTHORS: Kagan, D. F., Kazanskiy, Yu. N., Nemlikher, M. Ya.
TITLE: Metal coating of plastics by the method of evaporating in
a high vacuum
PERIODICAL; Referativnyy zhurnal. Khimiya, no- 7f 1962, 623, abstract
4P81 (Sb. "Plastmasay v mashinostr.11. M., Dlashgiz, 1959,
136-143)
TEXT: Methods of coating plastics with metal are detailed and the
princi-
pal features of the method of evaporating metals in a vacuum are
outlined.
The adhesion of a metal coating to the surface of organic glass is
examined and a method of determining the quality and thickness of
the metal
layer is set forth; the apparatus for the metal-plating of plastics
is
described and the electrical conductivity of the layer is given.
[Abstracter's note: Complete translation.]
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31716
S/191 62/000/007/003/011
B124/~144
AUTHORS: Trostyanakaya, Ye. B., Vinogradov, V. IM.,
Kazanskiy, Yu. N.
TITLE: 71.:olding materials based on thermosetting
polyesters.
Communication I. Polyester molding materials with powdery
fillers
IILRIODICAL: Plasticheskiye masay, no- 7, 1962, 15-19
T --.XT :'be applicability of the Soviet unsaturated
polyesters TITH -1 (PII-I
1 (TtIGF-11), and TT"AC(TPAS)
(thermostable polyacrylate binder)
as binders for molding materials is investigated. The
polyesters were
cured in cylindrical molds in the presence of 1% benzoyl
peroxide at
1200C in amounts of 12 g each, and were kept at 1500C kor 5
hr. The
volume shrinkage was determined from the change in density
of the poly-
ester after curing. Quartz powder, talo, mica, and kaolin
were used as
fillers and mixed with the binder. Benzoyl peroxide was
added in a
mixture with styrene, diallyl phthalate, dibutyl phthalate,
or poly-
acrylate. Molding materials based on PN-1, TMGF-11, and
TPAS are moldable
for 4 hr, 8 hr, and 1.5 months, respectively, this period
depending also
Card 1/#;

B/191/62/000/007/003/011
Yolding materials based on ... B124/B144
on the shape and size of the block. If a surface-active
substance is.
added instead of part of the filler, the storage stability
of the molding
material increases, whilst addition of a thickener confers
thixotropic
properties. The following formula was generally applied
(parts by'weight):
10D polyester, 1 initiator, 84 mineral filler, and 66
thickener. Before
moldinC, the molding powder must be treated by rolling to
remove the air.
'6t from various polyesters with 60 ~
The fluidity of pastes 1,r -7eo filler
varies between 50 and 80 mm at a molding pressure of 90
kg/cm~ and a mold
temperature of 1200C. The rate of polymerization of the
po-lyacrylate and
the ratio polyacrylate:polymaleinate exert a decisive
effect on the
physicochemical properties of the cured materials. The
curing of poly-
maleinates with polyacrylates of moderate polymerization
rate is analogous
to the process of curing with polystyrene. The best results
were obtained
with the use of TPAS + PN-1. A pressure of 50-200 ka/cm 2,
a temperature
of'1201C, and a curing time of 1 min/mm were adopted for
powdery molding
materials. Table 6 shows the properties of the products
obtained. Cold
extrusion can be used for treating the molding material
pastes. Thanks
are expressed to P. Z. Li and Ya. D. Avrasin. There are 2
figures and
Card 24