SCIENTIFIC ABSTRACT ZHMUROVA, I.N. - ZHODZISHKIY, I.L.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R002064830012-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 92
• Document Creation Date: November 2, 2016
• Document Release Date: July 20, 2001
• Sequence Number: 12
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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5/070/62/007/003/015/026
E132/E46o
AUTHORS: Khaimov-M ll.kov, N.Ya -Zhmurova. Z.I
Bagdasaro
v -Kh S Akulenok, Yolq-.
TITLE: On the questio'n:of thesectorial growth of crystals
PERIODICAL. Kristallo$rafiy no.3, 1962, 437-441
A, V-7
TFXT:. Certain regularitie in the.production of ittacro-
nonuniformities in crystals.during their growth from solution are'
discussed. The connection.between the forms of the growth
pyramids andthe cond.itions.of crystallization are examined.
Using the example of alums it is shown that the develcpment of a
sectorial structureis connected with the trapping by the growing
crystal of.mechanical.impurities and. with the inclusion of
structural'impurities. The Lfollowing signs can be used to
diagnose the.,.kinds of,'defects in crystals. The relative rate of
growth of a face which in being spoilt is, in the case of
structural impurities, significantly-decreased (blocking) butin,
the-case of mechanical impurities it is significantly increased.
in-the first case, if the-s .ymmetry of the crystal allows it,
.,:the defective face.forms the basic shape of,the crystal and in
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1.1ERSHA.UXAMA, OkOgEt Issakovua ~ZHKYXHOV, Ivan Vikolayevich; JPILIPPOV.
A N. red&; SHHSTOVA~`LJt,_,. :red,`
I'Vorkeral.and national.4iberation movement,dmdng theyears
he
f
.7irut World War] Raboohec' I natsionallno-oovoboditallmoo
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gody pervoi mirovoi voiny. Moskva, Isd
A051pri TeX OBS..19590 -63 a. (KVui 12.06)

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mober and comPOOttion of the IsOlf-
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",Y. A~f
.0i Is of the Easterw'Regions (Goirt o SOV16443
Vol'ga~regiow to Sakhalin...:"The,following characteristics are given:
properties, elementary composition, fractional
-.content from iabop. to 5000C properties of.commercial petroleum
.,products or -of ,their, components,,ash composition, and the.hydro-
carbon,composition..of.dissolved:gasoi Fractionation curves
characteristics,of individualfractionso and evaporation data.are
also given for most of.the crudes& There are 16 references: 15
Soviet-and I non-Soviet.
IPA n? V .1t, rAw?1r17WVPO f A%-J .4--AI
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FAVMAO Serafimm Nikolayevna;.MIATSKAYAj, Zoya Vanillyevna; YMCH17,04,

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-Oils of Eastern Regions of the USSR (Cont.) SOV/1441
and faculty
members at petroleum vuzes,
COVERAGE': ;This book consists of.:two:partsi, The first part constitutes
a. card index'listing the-oharaoteristios of crude oil-found i*n
eastern regions of the USSRv aswell as of Its !pnd products,
The second*part-4s a eontinuation of the.handbook published in
1947.under the title Soviet Crudes. It oontains more data,
however,, and treats a much larger number of crudes. The card
indix shows the properties of crudes as well as the products
obtained from;.them by straight-run distillation. Card format as
well.as the method of showing the characteristics of crudes and
their productswas adopted by.the All-Union Scientific Research
InstItute of Petroleum Industry, and approved by.the All-UnIon
Council for the Study of.Petroleum,, Its Products, and Methods.
Used,To Analyze Them. Earlier work done by Professor A.S..
Velikovskiy, Candidates of-Sciances S.N. Pavlova, P.S. GoFman, and
Ye. F. Rudakova had been used in this book. P.N. Yenikeyev was
consulted in matters dealingwith petroleum geology. There are,
no. references given.'
Card 2/ 22
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L 2428-7-66 9-4ti 1)/EWT(m)`/EWP%'j) Rii
ACC NR, tj6oo7U02
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AUTHOR:,. Zh*T A. I Kol V0. P. Volkavj s. V.
'3's
TITLE: Vipleta-triplet sorption-Upetra76f solid sGluti, of certain organic
_cnmpounds
SOURCZ::'_ Opt
no,2 1966
p Y 003-30T
`TOPIC -TAGS if '.absqrptfon:s]~ectr'=j. solid so1Utio.*$-organ1c~so1ventj, nonmetallic. or-
ganic derivativep:organic amideo fluorescence quenchingp halogenated organic courpound
ABSTRACT- To obtain more data on- the mechani sm and kinetics of formation of zeta-
stabli siated of organic molecules.* the authors determined at low temperature the
spectra of the triplet-triplet absorption of alcohol solutions of several amino-
ic aciM and anthracene derivatives, and investigated by means of triplet-trip
absorption 6 action of specific fluorescence quetchero on the population of the
metastable state. The measurements were based on a comparicon, at fixed wavelength
of the trananisaion of samples under additional intense excitation capable of ere- lel
ating a sufficiently large population of the metastable stateti, with the transmission
--in the absence -of' excitation. The apparatus is described in detail. The tr
iplet-
triplet absorption method was also uaed to study the action of h gens on the
anthracenco, 2-
of the:metastable--states, In the case of
crease- in the7trlplet.~trlVlet 6 -so-' ion density in- the presence f bibml6a'v-4 a
0 a

:T7
2/2
all

`Acd'- NJ Ri-AIJ6030720- SOURCE COD4 UIVO368/66j'00!Vd*UZM/O2j5
AUMOHs zhWOvafi Ie A.; XolobkovF V. P.; i~W o T. 1. Hakhlina$ 0. A.
OWS none,
TITIZ s: Study of the luminescence of glawactivated by holmium'
SOURUEs. Zhurnal prikladnoy spektrookopiip v. :5; no. 5# 1966,t 228-235
TOiIU TAM, luminescence,, holmium, rare earth metal,.glass, ~:bsorption bandp energy
band.structurep radiation-intensityp quantum generator
ABSrRACTs This study was made in order to obtain additional data on tho mechanism of,,
interaction of,rare earth activators with glass,inaamuch as such information might
make it.possible to utilize:glaaa in thedesign of.optio quantum generators. The ab-
sorption and luminescence characteristics of glass of various coniposition activated by
holmium were studied in the-4300-30000 cm -1 range at room temperature as well ae,low
temperature. A diagrak of theenergy,levels and the transitions between them was
drawn,for the trivalent holmium ion,in the.glass on the basis of fhe position of-the.;
absorption and luminescence bands. The luminescence of holmium in the glass was oon-,
centrated predominantly in the 5000 cW*l band (transition V7 -1, VS). Ther.eforep the
effect of,gla" composition# aotivator ooncentration, and temperature on tim rormp
position# intensity, and duration d the M oArl was studiedlin detail. A 1081
WGs 666.11.0105
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MVZC~ MMIIV~*`~ir.'--;!~ 4~R!;v OfT
B/051/60/009/003/013/019/XX
201/E191
Investigation of the Duration of Phosphorescence in Solutions
of, Organic Compounds at OC
extent a change of 5 due to an external medium is reflected in
.,the probability r. Tables-.1~and 2 list the values of 7
Phos,
OC4,0C) and 6, at -196 OC 'for 17 compounds in 21 solventA.
~,-The compounds dealt with inTable 1 are:
"(I) 3-acetylamino-N-methylphthalimideg
4-acetylamin-o-N~-methylphthalimide~
(III) 316-dia.cetylamino-N-methylphthalimideg
(IV) 3-methylacetylamino-6-methylphthalimidee
The compounds,.listed in Table.. 2. ares
M. 3-metti~lacetylamino~-N-methylphthalimideI
M) 4--methylacetylamino"N-methylphtha~limidel-
(VII) 3-hydroxy-N-4ethylphthalimidej
(VIII) 4-hydroxy-N-methylphthalimide,
UX) 3.1amino-6-nitro-N-methylphthalimidel.
W 3-dimethylamino-6-mothylacetylamino-N-mothylphtha*limideg
(XI) 3-dimethylamino-6-acet,,rlamirio-N-methylphtha:kimideI
Card 2/3

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ild,

:Z2Ol/El9l
'On. the Problem of the.Effect of Solvents.on the Electronic Spectra
Of Orga ni c:'Mol e cules:. .
2n2
p
2a +,2 2n2 +
e :is
where,' -the 'Aielectric constant and n is the
Experimental data 'a
refraotive.indox of the.solvent. lso:
disagree with a theoretically predicted inverse
proportionality between the :effect of solvents on the
spectra and ~ -the moleoular,radii of the solvents (Fig 2).'
The authors follow-eArlier workers (Ref,s 9-13) and suggest
that.it-is wrong in principle to attempt description.of
the'effect of solventslon the spectra using macro-
properties of these.solvents, since such effeot is
primarily due to~short-ra.nge intermolecular interactions
governed,by,micro-properties of,the solvents. k semblance
of..the-relationship between the shift in the electronic.
frequencies and the.dielectrialconstant is due.to thelaot
Card that.the dielectric,constant is governed by the micro-
.2/2.
properties of the solvents. There are 2 figuresand
13 references,-of which 6 Are Soviet, 1 English, 2aapanese
:and., ~,.German,
SUBMITTED: -Augus t 12 19 59
I ~117I I;

Borgmant V.,A~q Zhmyrevat 10 A*# 3/020/60/131/04/018/073
7V __ K-016b
Zelinskiy
~ov B013/BO07
TITLEi The Influence'Exerted by Heavy Halogens on the Probability of
Transition.to the Metastable State and the Probability of
beactivation of.This State
PERIODICALt, Doklady._.Akadenii nauk,SSSR9 196ov vol,i3i,.Nr 4P 781-784 (USSR)
TEXT i The.present paper is.intended'.to show more clearly than was hithirid.~'
.-..'done thaVtheaotion of:extinguishers of the halide type on the fluorescenoeof
organic compounds results in a higher probability (r) Qf tronsition of -the
excited molecule to the metastable state and to show the influenoo.exerted by
and 9 respectively of transitions
..~,these extinguishers on the probabilities q2
from thelmetastable state to -the ground state,with and without emission..
Besides..thersalts.,of hydriodio acidi the authors used bromides as extinguishers.,
q2.4s'less increased by weak bromide.extinguishers. In order to obtain a higher.
A An some casom and clearerextinction in others, higher concentrations
phosph
of iodides vote used. Table I contains the absolute yields q and q-
f.luor phosph V
of fluoreacence,and phosphorescence, as well as the rater of damping v* of
fluoresce Iace at oertain~concentrations of the salts of bromides and iodides in
Card 113
1 1: 1 Alffif if D;f 1, lt~ 1::;~::
f P F,

The Inf luence -Exert ed bk.Rsavy.-Z&lo no on,the 5/020J60/131/04/018/073
~ge
Probability of , Transition to the Metastable State~ B013/BOOT
-and~.the.Probability-..of'Deaoti*ation of This ~-State
organic substa hoes in.1methyl alcohol. The damping of pbosphoresoeme.
was carried'out b a
y me no-of a deiiceAeveloped by B. ra. Sveshnikor and P. I*
:Kudryashovj,and short-time recordings were carried-out by means of the r-meter
-designed by,X~.A. Tolstay and P., P., Yeof ilov.: Dif f erent malts of, one- 'and, the,
same,-halogen hydracid have the sameeffecto kt the same molar concentration
theylhave,the same effect:on the yield,6f fluorescence and the duration of.,
phospho"escenoe.. Nextp theauthors describe anattempt made to prove that theicd
:are no: 'lurther- complicating circumstances and errors in measurement. The use
of bromides and higher concentrations of iodides made it possible to
illustrate clearer cases of increase in q der the action of extinguishem.
phosph un
Details are described..In all cues the duration of phosphorescence decreases
considerably.wM increasingq A qualitative comparison of the yield of
p osph
luminescence and.the.,duration:of phosphorescence shows in some cases that also
the pres -ence of:iodine in the solution.ino:,-eases x considerably. Halogens have
a particularly strong effect-on x~if bromine and iodine are contained in the
phosphorescent moleoule..The deactivation of only 30 per cent of alladsokbing
molecules falls to the portion of- radiationless processes. Introduction of
Card ~2/3

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8/051/60/008/03/027/038
H2Ol/Hj9l
-the Problem of the EM t~of Solvents.on the Ble tronic Spectra
o
n ea a
of Organic~Molecules.,
~2ja2
A-
2e- +: 2 P 2nff + 2
wh e.-~F,~ i-s-the'die'lectria constant and
er n is the
refractive,,index'of the solvent. Experimental data also
disagree :with a, theoretically predicted inverse
pr.oportionality:betwe-en the effect of solvents on'the,
spectra and the molecular,radii of the solvents (Fig 2).
The authors follow earlier workers (Refs 9-13) and.suggest
that it is,wr6ng in principle,to attempt description of~
the eff eat of solvents M thespectra using macro-
properties,'of.these solvents, since'such effect is
primarily due to short-range intermolecular interactions
governed.by micro-properties,of the solvents. k semblance
of , the relationship between the shift in the electronic'
frequencies and the dielectric constant is due to the fact
~Card that the.dielectric..constant is governed by the micro-
2/ proper ties of the solvents. There are 2 figures and
13.references, of which 6.are Soviet$ 1 English, 2 Japanese
and )+..German,,,
SUBMITTED: August, 12 1959,
AM 4 1 '00 :9 lp
L

00 67925
SOV20-129-5-3~/64
AUTHOIRSO, J~Zhm;yioya, J. -A. IUZolinskiyj V. V. 9 Kolobkovf V. P.f
krasnitskaya, Be IYO
TITLEt k. Univerial- Scale of the-Effoot of Solvents on the Electron:
-Sr4otra~bf Oreianiacomp~ounds

'PERIODICALt -Doklady~Akademii naukosasRo 1959, :Vol ~129, Nr 5, py 1089-1092::
S
-T6,.t*authoro giva'a.:ohort surveyon the publications dealing with
thie -oubJeot.andtzention the papre by A. 1. Xipriyanov Rot
V. V, Zolinakiyj V. Pt Ko lobkov and L. G. Pikulik (Ref
V. V*, Zolinskiy, V, P. Kolobkov and I. I. Re-..nikova (Ref
They 'ouggest'4-sinino-N-mathyl-phthalimi4Le7 so standard substance.
means of, whion-they,oonotruct Me' oca e mentioned in. the
title'.. If-tlia..fluorooo#Ade.qpeotra,-frequenoies are plotted.on
'the ordinate and them various solvents on.the abscissa (at
distances which correspond to the differences between the
standard substance) the frequencies of the maxims of the
f 1' op fral
uorescenoe so
of most of the organic oubstanoes,for a
,
cortain.solvent are on a straight line Figure I showo:ouoh
Card 113 diagrams for'so'mo~phthslimido derivatives. In the absorption

67925
SOV/20-12 -5-35/64
9
A Universal Scale, of the Effect, of.Solvents on'the Electron Spectra of
Organic Compounds
speotra.the.points ire on a curve. The reason for the Aif-~
f erent, effeot,of ih*e: solvent 'on the fluorescence- and absorption
spectrum 4ill be dealt with 'by the authors at another place.
Figure Vshows the position of the.maxima of the fluorescence
spectra in different solvents for o-methoxybehzoic acid, amino-.
and its derivativeso malimide.derivatives,
acridine and 2-aminoacridine. The authors set up a snale for
79 solvents in which zero is-the position of the spectrum of
4-amino-g-.methyl!!Phtlialimide-vaporj 100 - the pooition.of.the
speotrum,of this oubstance.in water (Table 1). Certain rules
governing the order of.th.e solvents on this zoale are founds
.'Aa3C
the, maxima,,' of- the fluorescence spectra are in all solvents
fl
containing -,#,idroxyL groups between .16000 and 19000 om- wheis
-19600 cm- 1 For
.:the.'aloohols,form_a'.subgr up between 17600 and
max
the esters, is,between 18800 and 21600 cm for other
~between 211700 and 22050 om for aromatic hydrocarbonsibetween
Card 2/3

lfl-

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uc;~ Pr
-ACC-.NRt---Ar-66-29-OQ4:--:~~~-- -CODE.- UR/4O___j_j__j__/M2T/M3O
,AUTHOR:,, Asatiani-, T L.;GazMan, K. A~; -ZULYXq'V1f. X. - Ivanov, V. A.; Matevosyan,
M,;
Nazaryan, A. A., Filozor, A. F..i Sharkhatunyan 0.
ORG; Institute of nLaico GKAE (Institut fiziki GM)
TITLE:, On the possibility for measuringlonization of charged particles in a streamer
chamber
Fizika, V. 1, no. 2, 19 -130
SOURCE: AN ArmS'SR. Izvestip 66, 127
TOPIC.-TAGS ionization chamber part icle tr ack, charged particle, neon, proton beam
ABSTRACT:,- Data aria given'from experiments conducted to determine the possibility of
measuring the specific ionization of charged particles in a streamer chamber. The
LYaP synchrocyclotron at OIYaI was usedfor passing protons with energies of 660, 200,
100 and 50 Mev through a .streamer chamber measuring 5Ox35xl5 cm filled with pureneon
to a pressure of I atm. The results shov 1.8�0.4 luminescent centers per cm of the
proton track with a,root-mean-square deviation of 0.29 mm from the approximating
straight line * Microphotometric analysis of the films shows that the proposed method
may.be used for measuring the ionization of charged particles. In conclusion.the
authors thank.Corresponding,m,ember,AN.BSSR A. I. Alikbanyan and Doctor of physical and
mathematical sciences.A. A. Tyapkin forrCooperation and interest in the work. The
authors are especially grateful to Candidate of physical and mathematical sciences
Card 1/2

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SOV/1Z4-58-ll-ljO58
Translation from: Referativnyy zhurnal,' Mekhanika, 1958, Nr 11, p 171 (USSR)
AUTHOR: `~~~Odl ~Zlshsk~ly. C. - ~A_
TITLE: The, Effect of Nonuniform. Heating on the Frequency of Natural
cAllations of Sa - Dis ks of -Constant Thickness (Vi.
W, tyaniye
neravnomernogo nagreva na chastoty sobstvennykh kolebaniy
pill nykh diskov, posto~annoy tolshchiny)
PERIODICAL: Tr. Lenin ich. akad. 1957, Nr 82, part 21,1pp 149-164
gr. lesotek,hn
ABSTRACT. The fr quenc of naturatt ansverse oscillations i s w disk of
e y r na a
constant'thic,'kness,'is'inyestigated by the Bubnov--Galerkin method.
The disk. With a..r.igidly attached arbor-hole contour and a otrc5,5-
free outer. peripheiy, is subjected to nonuniform axisymmetric
heating. , Th.e diffe.rential equation of the problem consists of an
equation of the,fr6dAransverse oscillations in a circular, plate of
constant thickness subjected to, the action tensile stresses (produced
by nonuniform heating) symmetrically distributed over its middle
surface. The' approximate flexure expression is taken in the form
2 -B, BZ 2,
Card 1/3 w a0 (r~a) r+ r I. sin (k0+ 00 sin (wt+a 0
b

SOV/lZ4-58-11-13058
The Effectof Nonuniform He ating on the Frequency of NaturaI Osci
Nations (cont.
uter
where: r and 0 are the polar-coordinates; a and b, the arbor-hole and 'o
radii of the disk; k, the number of node diameters; w , the angular frequency of
oscillation;~_ a' and 00-, . Constants determined from the initial conditions; BI
0
and B2, constants -determined from the boundary conditions on the external circum-
ference of them disk (the boundary conditions on the internal arbor-hole circumfer-
ence:., are isatisfied automatically),~. a is an arbitrary constant, The distribution
0
of terriperature -along a'radius'-is aisumed.to follow a power law. All integrals
entering.in the formula.for computation of natural frequencies are given. The
instance when k=O,. in, the case.of a uniformly heated disk is compared with the
known exact.'solution (expressed in Bessel functions) of theproblem. of the
natural oscillations of a circular plate of constant thickness. In the Computational
example given, the, frequency of the natural oscillations of a saw disk is deter-
mined for k .values of 0, ~ 1, 60 as well as for the temperature differences,
between the outer and inner circumferences equivalent to 0, 15, 30, 45, and 900ce
Also determined are the llcriticalll.tempemtures corresponding to zero frequen-
cies in different forms'..of oscillations and coinciding with the failure of plane
disks. It is pointed out that, since at k=0 and k= I the frequencies of a uniformly
heated disk increase the disk cannot fail (the critical temperature is negative);
at k>l, the frequencies of the'disk diminish and "critical" temperatures exist,
Card 2/3
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