SCIENTIFIC ABSTRACT KOROLEV, S.I. - KOROLEV, VSEVOLOD ALEKSANDROVICH
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CIA-RDP86-00513R000824820002-5
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RIF
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S
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100
Document Creation Date:
November 2, 2016
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2
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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AUTHORi Korolev, S.I., Lupandin, V.I. SOV-113-58-9-13/19
TITLE: A New Non-Hardening Mastic for Caskets (Novaya netverdeyu-
shchaya mastika dlya prokladok)
PERIODICAL: Avtomobillnaya promyshlennost', 1958, Nr 9, PP 35-36 (USSR)
ABSTRACT: A mastic for gaskets of impregnated cardboard, paronite and
pressed cork to be used in motor car engines was developed
in 1947 by engineer L.14. Koposov. This LK mastic consisted
of 45% of autonitroenamel 624a, 40% of castor oil for tech-
nical use and 15Pf of solvent 646. The castor oil being too
oxpenaivo a substance, laboratory experiments were made to
find a suitable substitute. A product with similar proper-
ties was eventually found in the emulsifying agent from
chemical wood pulp, tallol oil. A composition of 30' of
this oil together with 70% nitroglyphtalic foundation proved
satisfactory. Laboratory tests with 225 engines were suc-
cessful. In June 1957, the Yaroslav Engine Plant switched
over to the new mastic, which resulted in over 31,000 rubles
Card 1/2 in annual )3avings.
AU!.
A New Non-Hardening Mastic for Gaskets SOV-113-58-9-13/19
ASSOCIATION: Yaroslavskiy motornyy zavod (The Yaroslav- Eng.ine Plant)
l. Gaskets 2. Adhesives--Preparation 3. Adhesives--ApplicatiorL,;
Card 2/2
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ACC NRj AP6003320 (IV) SOURCE CODE: UR/0365/66/002/001/0052/0050'
kUT,HOR: Al'tovskiyj R. M.; Fedotova, A. G.; KoroLev-# S.
ORG*. none
TITLE; Investigation of the corrosion properties of yttri 1. Effect of the pH or. 1
the corrosion d electrochemical behavior of yttrium
SDURM Zashi 7 ta metallovs v, 2. no, 1, 1966, 52-56
TOPIC TAGS; yttriums corrosion resistancep electrochemistry,
ABSTRAZT: The effect of the pH on the corrosion resistance and stationary electrode
potential of yttrium containing 0.1% 0, 0.3% Si, and 0.3% Cu was studied in solutiors
of N&X + HX and NaX + NaOH types (X was the anion of Cl- or N03-). The corrosion of
yttrim in nitrate and at a pH >3 in chloride solutions ofi-.urrbd with 4f/decrease, in
corrosion rate with time. This indicated the formation of a proteictivel-Tilm (probably
hydroxide) on the surface of the yttriume The dissolving of yttrium practically ceased
to exist after 50-75 hours of the experiments The rate of corrosion of yttrium de- j
creased with increased pH, especially in the acid region (pH 2- - 4). The corrosion r~-ta
was somewhat lower in nitrate than in chloride solution. The metal was in the passi-.,b
state at a lower pH (10-5) in the nitrate solution than in the presence of Cl- (pH 2.3).
Yttrium practically did not dissolve in bidistilled H20 with and without addition of
Card l/
L 01300-67
ACC NR,
L 01300-67
ACC NRt AP6003320
alkalies. Thereforej the presence in solution of NO - and especially of Cl- has no
effect on the resistance of yttrium to corrosion* Rermodynamically, yttrium should be
a very active metal electrochemically. The standard potential of reaction Y = Y3-1-+3o
Is - 2.37 v. But even the most negative potentialsof yttrium in the solutions studied
were 1 v more positive. This suggested the presence of a protective film on the yttr!;-I=
surface even in the active state of yttkum. The curve of,stationary potential - PH
for yttrium in chloride solution consisted of three parts, The stationary Potentials
at a potential below 3 and above 10 decreased with decrease or increase of the PH.,
respectively. The potential slightly increased with a decreased PH in the interval o'.
PH 10-3* According to Go Vo Akimov and 1. L. Rozenfeld (Isoledovaniya v oblasti eleko-
trokbimicheskogo i korrozionnogo povedeniya metalov i splavov,, Oborongizj, M&j, 1950).,
this can be explained most satisfactorily by the presence of potentials of the film-
pore type on the metal surfaces A complete passivation of yttrium in chloride solution
occurred at PH 13* Me :inflection on the curvp*t PH 3 indicated a change in surface %I
conditions. Probably,, at: PH 10-3%. The authors thank A. P. Komar and V. 1. Baranov for their
interest in these investigatio'ns. There are 4 figures, 2 tables, and
7 references: 4 Soviet-bloc and 3 non-Soviet-bloc.
SUBMITTED: February 24, 1960
Card 5/h,
f
b3b72
s/048/60/024/009/005/015
B013/BO63
0 0
AUTHORS Vorob,yev, A. A., Korolev, V. A.
ometel Under
TITLE: The operation of the Ionization Alpha Spectr
High Loads
PERIODICAL: Izvestiya Akademil nauk SSSR- Seriya fizicheskayal 1960,
Vol. 24, No. 9, PP. 1086 - 1091
TEXT: In the present papers the authors suggest a method of raising the
permissible loading of ionization chambers up to 10 4 pulses/sec. The
duration of the pulses occurring in the ionization chamber depends on the
duration of electron accumulation in'it. By adding 10 1. 15%.ofmethane to
the argon and by shortening the distance q down to "Oo5 cm it is possible
to shorten the duration of the build-up of pulses down to 0-5 - 0.4,usec.
It is apparently convenient to shape pulses by means of two short-circuited
circuits. This method is particularly advantageous because pulse tails can
be prevented and the constant component of the pulse spectrum is almost
zero. The authors thoroughly studied the effect of the rise time on the
Card 1/2
83672
The Operation Of the Ionization Alpha
Spectrometer Under High Loads S/048/60/0
PUI60 height (Fig. 13013/B063 24/009/005/015
Operation of 1) and the
0(-sPOetrum Of a Pu238 Signal-to-noise ratio (Figs- 2 and 3). The
the spectrometer under high load was checked by measuring the
Besides, the source with an Utensity
to tne input spectrum Of generator Pulses was m of 8 . 103
Of the
(Figs. 4 and 5). amplifier together with the easured, Pulses/sec.
was C' Pulses which were supplied
10 kev. When The cc-spectrum of pu238 Of 0~-particles
noisc analyzing the results ob is shown in
Fig. 6. Its half
makes the largest contribution to tained,
nOise Can be largely reduced by switching On addi the authors -width
(45 kev). This
least 40 - 50 kev. Some applications the half width line note that radio
reascn to believe that the half-width of the Ot-line can be reduced to at
finally M;ntioned. The authors thank tional tubes. There is
for hialp in the work 'of a strongly loaded spectrometer are
_j.
1 Bri-~,ish. There are 6 figure A:_Eaadd_eJ_.-'i and
8 and 3 refere F -Sobolevskav
o;Y - -
ASSOCHATIoN: nces' 2*'r -7 _a
Fiziko-tekhnicheskiy ins e, anj'
Of Physics and T h titut Akadem-ii nauk SSSR Linsti.tute
demy of S
ciences USSR)
Card 21?-
83673
h 0
AUTHORBt Voroblyevp A. A., Komar, At Peg
TITLEa Investigation of the Alpha Deca~lof
Ionization Alpha Spectrometer 11
S/048/60/024/009/006/015
B001BOO
I oroley, V,- A.
U 235 b Means of an
PERIODICALs Izvestiya Akademii nauk SSSR. Seriya fizicheskayag 1960,
Vol. 24, No- 9P PP- 1092-1098
TEXTt The present paper contains the results of an investigation of the
o(-decay of U235 , which was carried out by means of an ionizationc(-
spectrometer. The spectrometer was tuned to a r-spectrometer. The authors
studied a spectrum without coincidence with I-Lquanta (Figs. I and 2) and
a veries of C--spectra coinciding vith different groups of alpha particles
(Figs - 3 and 4) . A source enriched in U235 was used f or the measurement.
The. spectral line of U 234(98~) showed, however, the highest intensity.
It was used to stabilize the amplification factor of the amplifying part
of the ek-spectrometer. Besides, this line served as a standard for the
Card 1/2
83673
Iwrestigation of the Alpha Decay of U 235 S/046/60/024/009/006/015
by Means of an Ionization Alpha Spectrometer BW/B063,
measurement of the energies of U 235 alphas. The energiesp intensitles,
and forbiddancea of the alpha gwaps are given in Table 1. The results
of the analysis of the U 235c~-spectrum agree with the results of Ghiorso
although the latter are only of a qualitative character. The a-spectrum
of U 235 has been recently studied by S. A. Baranov and A. 0. Zelenkov
by means of a spectrometer of high luminous power. The energies of the
lines they found are fairly consistent with the data obtained by the
present authors* Table 2 gives the results of the determination of
multipole or 4--transitions. On the basis of measurements of 0(- and f-
spectra, the authors suggest a possible a(-decay scheme of U235 (Fig- 5)-
The levels were identified with the help of Nilsson's scheme. Though
this identification cannot make a claim'to finality, it does not contra-
that the experimental data available at present. The authors thank
S. A. Baranoy and A. G. Zelenkov for diBcussions and information, as
well as M. F. Sobolevskaya for her assistance in the measurements.
There are 57igures, 2 tables, and 9 references, 3 Soviet, 3 US, and
1 Danish.
Card 2/2
L r
82602
S/056/60/039/01/11/029
CIC2 1A (19 5~~ 0 -BO06/BO7O
AUTHORS% Voroblyev, A. A., Komar,,A. P., Korolev, Y, A.
------------ - -
TITLE- Measurement of the Energy of the oL-Particles of an Emitter
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol, 39* go. 1 (7), pp. 70-72
TEXT:. The authors measured the ocparticle energies with the help of an
oL--spectrometer. The ionization was determined by comparing the pulse
heights of the oL particles with those of the generated pulses whose
anplitude could be measured to an accuracy of - 0.01%. The chamber used
was filled with 97% Ar and 3% CH 4* The width of the cr line was 35 kev.
Table 1 collects a number of relevant data. Th 228 was chosen as a stand-
ard. In the first column of this table the energy1falues deduced by a
magnetic analysis are given, the second column gives ionization I, and
the third the ener calculated according to the formula (1)
(Est - 84)/(Ea - 84~ - Ist/I CK- , where Est and E0C denote thecx energies
of the standard and the emitter under investigation. There is good
Card 1/3
826o2
Measurement of the Energy of thex-Particles S/05 60/039/01/11/029
of an Emitter B006YB070
agreement between the first and the third columns, from which the con-
clusion is drawn that the method of energy determination from the
ionization in thectspectrom*ter is suitable. The following results are
obtained:
At 217: 7.064 + 0-005 Fr 221 s 6-336 + 0.005
PO 213 & 8.368 + 0.010 U235 1 4-396 � 0-003
I
U235 t 4.211 + 0-003 U238 1 4-190 + 0-005
II - -
These values are compared with the results obtained by other authors.
kgreement is good in some cases and not so good in others. Some particular
cases in this connection are discussed. Thus, for example, the values
obtained for the two intensive U 235 lines (I and II) diverge consider-
ably from those obtained by magnetic spectrometer (Ref. 6). In connection
with this, it is pointed out that the measurements lately made by S.
A. Baranov, A. G. Zelenkov et al. (Ref. 8) of the oc spectrum of U235
with a new magnetic spectrom*ter led to the following values:
Card 2/3
82602
Measurement of the Energy of the 06-Particles of S/056/60/039/01/11/029
&-n Emitter B006/BO70
BI - 4.394.t 0.002 and E, - (4.213 � 0.002) Mev, and these agree very
well with those obtained in the present work. There are 2 tables and
-9 referencess I Soviet, I South African, 2 Canadian, and 5 American,
ASSOCIATIONs Leningradskiy fiziko-tekhnicheskiy institut Akademii nauk
SSSR (Leningrad Physicotechnical Institute of the AcaLemy
of Sci 8, USSR)
SUBMITTED: March 22, 196o
Card 3/3
S/12o/61/000/002/010/042
Z032/Z114
AUTHORS: Voroblyevs A.A., and Korolov, V.A.
TITLE: A method for measuring the transparency coefficient of
a grid in a pulse ionization chamber (0
PERIODICALt Pribory i tokhnika eksperim*nta, 19161,ANo-21 PP- 78-80
TEXT: Green's reciprocity theorem can be used to determine
the potential V+ induced on the collecting electrode by positive
ions. The latter to due to the fact that the grid introduced to
screen the collector in not 100% efficient. The present authors
point out that the theoretical treatment of the problem given by
0. Buneman, T.E. Crenshaw and J.A. Harvey (Ref.l: Canad. J.Res.A,
1949, 27, 191) in very complicated and, moreover, is based on
various simplifying assumptions. They therefore suggest a method
for the exerim*ntal determination of the grid transparency
coefficient. Their argument runs an follows. The potential V+i
induced by the i-th positive ion located at a distance x from
the electrode I (Fig.1) con be shown to be given by:
V + W/Cu (2)
Card 1/ 5
S/12o/61/900/002/010/042
E032/ElA
A method for measuring the transparency coefficient of a grid in
a pulse ionization chamber
where 9(x) in the potential at the point x, which appears under
the following conditions. The high-voltage electrode and the grid
are earthed, the collecting electrode in at a potential U, and
there is no space charge. The potential distribution in this case
is shown in Fig.l. We are interested in the region between the
high-voltage electrode and the grid. At a sufficient distance
from the grid the field Ed in a constant, in which case
,#(x) Eax (3)
The potential V+ in then given by
N
V V No ii cOB 0 Ed/CU (4)
where in'the average distance of the ions from the beginnifig-of
the track and 0 in the angle between the direction of the track
and the normal to the surface of the electrodes. in order to
determine Ed the chamber is filled with pure argon and a high
Card 2/ 5
S/12o/61/000/002/010/042
A method for measuring the E032/ZI14
voltage is applied to the collecting electrode (U = 2 kV) while
the grid and the high-voltage electrode are earthed. The pressure
in the chamber is adjusted so that alpha particles emitted from a
source mounted on the high-voltag* electrode stop within the
region in which the field in still constant. The field Ed which
penetrates beyond the grid extracts a fraction of electrons
produced by ionization and pulses appear on the collecting
electrode. Next, a compensating positive voltage bU is applied
to the high-voltag* electrode and in adjusted until there are no
pulses at the collecting electrode. The pulses disappear when the
compensating field El d and Zd are equals i.e.
EId = 2d - &U/d (5)
where d in the distance between the high-voltage electrode and
the grid. Hence V+ a No AU Ik coo S/CU d (6)
Thus, in order to determine V+ it in sufficient to carry out a
simple experiment involving the determination of the compensating
voltage &U. The authors recommend pure argon an the working
Card 3/5
S/120/61/000/002/010/042
A method for measuring the tranmparency.E032/EI14
gas. Beat results are obtained by determining the compensation
point using pulses from the high-volt&ge electrode, since in this
case the sign of the pulses will change at the balance point.
In this way an accuracy of 3-5% in A U/U can be achieved. The
experimental results are found to be in agreement with those
computed by Buneman and Crenshaw and Harvey (Ref.1) (see Table),
the discrepancy between the experimental data and the theory
being negligible in the case of grids with low transparency.
Acknowledg*ments are expressed to A.P. Komar for interest in this
work and to G.Ye. Solyakin for taking part in the discussions.
There are 2 figures, I table and 2 ref*rencess 1 Soviet and
1 English. A,
ASSOCIATION: Leningradskiy fiziko-takhnicheskiy institut
(Leningrad Physico-technical Institute)
SUBMITTED: March 24 1960
grid r, mm r, mm r, mis acalc. a*xp.
1 0.05 1 5 58 mo65 o.oo61
2 0.05 3:0 58 0.0-185 0.0-143
Card 415
S/120/61/000/004/003/034
E032/E514
AUTHORS: Voroblyev, A.A. and Korolev, V.A.
TITLE: A study of the properties of an argon-methane mixture
as the working gas of an ion�zation chamber
PERIODICAL: Pribory i tekhnika eksperimenta, 1961~ No.4, pp.42-46
A
TEXT: W. N. English and G. C. Hanna (Ref.l: Canad.J.Phys.,
1953, 31, 768) have recommended argon-wiethane mixtures as a
suitable working gas for ionization chambers. The present authors
report some measurements of the properties of such chamber!!~, All
the measurements were carried out with a plane ionization chamber
containing a grid. The gas mixture was made up of commercial argon
(Ar - 99.9%, 0 2 - 0.02%, N2 - o.o8%, co2 - 0.005%) and commercial
methane. The following quantities were measured.- 1) Electron
drift velocity, 2) the recombination rate- 3) the magnitude of the
saturating field, 4) tho electron attacbment effect and.the maximum
permissible field, 5) the average energy ov the electrons in the
gas and 6) the dependence of the ionization on the energy of
a-particles traversing the chamber. It was found that with this
gas mixture it is possible to choose the electrode potentials sotai:
Card I/V
A study of the properties of ... S/12o/61/000/004/003/034
I E032/E514
1) the recombination effects (between electrons produced during
the ionization and the corresponding positive ions) are reduced
to a minimum; 2) there is no appreciable attachment of electrons to
neutral molecules and 3) the electrons can pass freely through the
intermediate grid. The electron collection time can easily be
reduced to 1-0.5 psec and a plateau of several hundred volts is
obtained, e.g. with a methane concentration of 5% the collection
time is approximately 0.7 jLsec. The ionization was found to be a
linear function of a-particle energy in the range 5.4-8.8 Mey.
An important advantage of the argon-methane mixture is that it does
not require any additional purification. Acknowledgments are
expressed to A. P. Komar for his interest in this work and to
M. F. Sobolevskaya for assistance with the measurements.
There are 5 figures, I table and 8 references! 3 Soviet (1 a
translation from English) and.5 non-Soviet, The following
Eriglish-language references are given., Ref..l (quoted in text),
Ref-5: C. E. Melton, G. S. Hurst, T. E. Bortner, Phys.Rev.,1954,
90, 643; Ref.6: G. Bertolini, M. Bettoni, A. Bisi, Phys. Rev., 1953,
92, 1586; Ref.7a D. Strominger, T.M. Hollander, G. T. Seaborg,
Rev. Mod. Phys.t 1958, 30, 2-
Card 2/4 -'~?
29594,
A study of the properties of S/120/61/000/004/003/034
9032/014
ASSOCIATION: FizLko-tvk~wicheskiy :Lnztltut AN SSSR
(PhyaLco-tecbuical. institute AS USSR)
SUBMITTED: March 24 iOo
Fig,3: Amplitude V 0i pulses at the collecting electrode on:
p.d. between high-wattage electrode and the grid and
p.d. between the 1grid mW the colloctor,(nethane concentrations
are marked on the curves.
retfta^
vg,wmfd
Card
!KPFx,PM,CM
Lvq."W"q
.2,
1, IrT
.- KOROLEV,-V.A.
Soz4a morphologic types of ore bodies In the Kara-Mazar Muntaino.
Geol.rud.mestorozh. no.4:98-100 Jl-Ag 161. (MIRA 14:10)
1. Karamazarakaya poiskovo-s"yemochnaya ekspeditsi7a.
(Kara-flawr Mountains-Ore deposits)
88402
5/020J61/136/004/008/026
B019/BO56
AUTHORSt Konart A. P.9 Academician of the AS UkrSSRO Voroblyev, A. A.0
and Korolev, V. A.
TITLEt Measurement of the Fluctuation of Ionization Produced by
a-Particles in Argon
PERIODICALt Doklady Akademii nauk SSSR, 1961, Vol. 136, No. 4,
pp. 795 - 797
TEXTt In the introduction, the authors refer to the frequently used
measurement of ionization caused by nuclear particles for the purpose of
determining the energy of nuclear particles. A relation given by V.Pano
(Ref.1) for the mean square fluctuation of the number of ion pairs with
constant energy of the ionizing particles is written, and it in found that
this formula is suited for determining the upper limit of the mean
fluctuation, but not for acre exact computations. Besides, Fano assumed
that the ratio between the probabilities of the various inelastic
processes in independent of the nature and energy of the ionizing
particles. The measurements carried out by the authors were made by means
Card 1A
88402
Measurement of the Fluctuation of Ionization 5/020/61/136/004/008/026
Produced by a-Particles in Argon B019/BO56
of a-particles emitted by Ra 224 (Ea 0 5.681 May) and of a-particles emitted
by Fr 221 (z a 0 6.336 May). The ionization chamber was filled with
chemically pur* argon + 1-5% CE49 whereby recombination could be prevented
under certain conditions. Electronic collimation was used, whereby the
resolution and, thus, the quality of the spectrum could be improved. The
electronic means for *improving the signal-to-noise ratio are briefly
described. The measurements are graphically represented in Figs.1 and 2.
The half-width of the Ra 224 a-line is 17 key and has a mean fluctuation of
7.2 key. This mean fluctuation 6 in composed of 6 n ~6 2 + 62 + 62 , where
N p 0
6N, 6p, 60 are the mean fluctuations which are due to the fluctuations of
the ionization, to radio noise, and to other causes. In the came of Ra 224
60 in negligibly smallo and because 6p 0 4-7 kav, it follows that:
61 - 5-5 key. For Fr 221 , 6N- 6.0 key was obtained. From a discussion of
the results, the authors conclude that 6 N say be described by
Card 2/4
U 'T
88402
Measurement of the Fluctuation of Ionization 8/020/61/136/004/008/026 A
Produced by a-Partiolos in Argon B019/BO56
(4)
N a) a 5-8
for different E.. Ea tiust be given in Wtv. Ifi the relation 6 PNO M
given by Fanot where N is the mean number of ion pairs,.F in found equal
0
to 0.22, and its upper limit is given &9-F 0.33. The authors thank
M. F. Sobolevskaya for her help in carrying out the measurements. Therear
2 figures and 8 non-Soviet references, 5 US, I Canadian, I German, and
I French.-
auk SSSR (ine'titut*e
ASBOOIATION, Fiziko-tekhnichoskiy Inatitut Akadenii n
of Physics and Technology, Academy of Sciences USSR)
'SUBMITTEDi November
1, 1960
Ca~d 3/4
IL
88402
B/020/6 i/1'3''6/'O--O-4-[10-'O-S-lj-~O2~
B019/B056
4MIAW
ow -
M..A
x
fime 1. a-CneK-rp Ra"'
Card 4/4
20318
S/02o/61/137/001/009/021
B104/B209
,~2 6 , 2j
AUTHORS: Voroblyevt A* A-* Komar, A. P., Academician AS UkrSSR,
and Koroley. Y. A.
TITLE: The possibilities of reducing the effect of ionization
fluctuations in gases
PERIODICAL: Doklady Akademii nauk SSSR, v. 137, no. 1, 19611 54-57
TEXT: The authors based their work on a paper by Fano (Ref. 1: U. Fano,
Phys. Rev., 12, 26 (1947)), in which an expression was obtained for.the
mean square fluctuations of the number of ion pairs at a constant
energy of the ionizing particles. Fano's calculations show that these
fluctuations are determined chiefly by the redistribution of ionized
and excited atoms. Evidently, their total amount fluctuates less.
The authors have now determined the amount of fluctuations of the total
ionization, taking Fano's method as a basis. In this manner, they obtain-
ed the mean square fluctuation S2 of the total ionization 7: 25
.j
Card 1 4
20318
S/020/61/137/001/009/oq,
The possibilities of reducing ... B104/B209
2 E )2
A k
j P ~nk N0 . No denotes the mean number of ion pairst
0 1
W W0/(1 + a(,-P.)/P) W0A, 1, M Z:Pk the total probability of
ionization in inelastic collision, W 0the mean energy of ion pair
production without additional ionization, and n k the number of ions
produced in the k-th oollision. The relations
PW, Pj, (WI - E')' P,' , (W, - Ej' )(88)
+
INon 11036 (8a)
4D (a) [(W - W,)2 + a , (W - W.), + (I W"T (86)
W2, . P P (8b)
are obtained for F. The last two terms in (8a) are due to fluctuations
.of the energy losses during ionization and excitation, and do not depend
Card 2/4
I-M
S/020/61~137/001/009/021
The possibilities of reducing ... B104/B209
on the additional'ionization. 4b (a) is determined by the redistribution
of the number of-ionized and excited atoms, as well as by the fluctuations
arising in the additional ionization. In*the limiting case where
additional ionization is missing (d - 0), E
. (8a) goes over into the
formula of Fano. Fig. 1 shows the. ratio as depending on the
~
0
obability a of additional ionization for He and Ar. It is seen that
(cf) for argon drops to nearly one-thirtieth with rising probability,
7
and for helium it drops to nearly one-hundredth. The first of the terms.
appearing in (aa) was found to be always about 0-03, and the second is
negligible. From this it follows that the accuracy of measurement of the
energy of ionizing particles is considerably improved by recording all
ionized and excited atoms. There are 1 figure and 3 non-Soviet-bloc
references.
ASSOCIATION: Fiziko-tekhnicheakiy institut Akademii nauk SSSR
(Institute of Physics and Technology of the Academy of
.Sciences USSR) 25
Card /4
Ro
The possibilities of reducing
SUBMITTED: December 9, 1960
Card 4/4
2031.8
S/020/61/137/001
B104/B209
39479
oz;,O z-, i,7 Z 2,,'--
0 2 C~ 4
S Vorob yev, A_ Komar, A. P. , Yorolev , V. A.
,~,17 2 LE Decreal-a of ionization fluctuatiGns of c I e i ar-7-on
1 T
U` D z "i, v - 43 ,
-C.," L Zhurnal
-428
no. 2(6', 1962, 426
116,1 tlfiat Lnu
-iL Llut'-ors ha(I Sho-;jn ourlier (D 3351t, !D7, 4, j
icnization fluctuations as-ociated with redistri*nutions of of
zi-d ionized izoloculea can be reduced by a .-ascous
--i n io-ization ootential io,.,icr than the enerZy of lo~~-.ost e--.c-tud
L
lwvol of the !)rincinal com:ionent. Here, the autho-ro -.-_,-ied '11-0 c*.-Iecl~
ibiiit-y b- rimen' . Th e y u s ~ a a -) u 10 0 d i wr I i z a 0 -., I c c. b (: r ra d
a~-on cont-Anin- 0.1
L; 7 /'1 Nr 2 ' 0.02 2' and an acetylene y.
i ;j ioa-iizat ion ot, e n t 3. a 1 of 11.3-45 ev is lov;ar than the lowe,,;t- ~,r,--on 1eva-
('1.5 ev), the acetylene _-;11dition increases the ionization. The i0,,, .;.a4,
f Luctuations vvoze calculated 'rom the half-width of -the a-line
1 224
.631 'Yev) of -Ra for comparison, the --eajuremenis nere re-eate"
5
Cird 1/2
KOROLE ..STRIZUE.VSKIYY V.A., prepodavatell
Operation of diesel locomotives by the Tashkent Railroad an
leigthened closed cycles. Elekt.i tepl. tiaga 5 no.XO.*18-19
0 161, (MIRA 14:10)
1. Zamestitell nachallaika alushby lokomotivnogo khozyny-jtva
Tashkentskoy do~rogi (for Korolev). 2. Samarkandskiy
zhele=odorozhnyy tekhnikum (for Strizhevskiy).
(Railroads-44anagement)
WROLEV, Vitaliy Arrkatd~'~Yevlch, insh.; KASHTANOV, F., red.;
KARPINOVICH, Ya. , telft. red.
[Automation in machine and assembly shops] Avtomatizateiia
v mekhanoeborochnfth tsekhakh; is opyta raboty Minskogo
traktornogo savoda. Minsk, Goa.izd-vo BSSR, Redaktsita pro-
izvodstvannoi lit-ry, 1963. 62 p. (MIRA 16:5)
1. Minskly traktornyy zavod (for Korolev).
(Minsk-Tractor industry) (Automation)
VOROBITEVP A.A.; KOMAR, A.P.; KORDLEV, V.A.
Decrease of"the fluctuations of ionization produced.,
,W d-particles
in argon. Zhur. eksp. I todor. fix. 43 no.2:426-448 Ag 162.
(HM 166)
1. Fiziko-tekhnicheakiy institut izani A.F.Ioffe AN SSSR.
(Ionization) (Alpha rays) (Argon)
VEDENSKIY, 0.1%; DMITRIYEV, NJ.; KO'TLEVJ,..V?'A-.; TURGUNCV, D.T.;
I - -, .. - ~ A
MELINIKOV, V.Ye., red.; MEDVEDEV, G.G., inzh., retsonzent;
MURAVIYEVAp N.D., tekhn. red.
(Maintenance and repair of TGM3 diesel locomotives in the
depot) Remont teplovozov TGM3 v depo. Moskva, "Transport,"
1964. 107 p. (MIRA 17:3)
KOROLEVY V.A., inzh. (Tashkent); NIKITIN, V.I., inzh. (Tashkent)
Current maintenance of diesel locosiDtives on lengthened haul
distance sections. Zhel.dor.transpe 45 no.10:64,66 0 163.
(MA 16:11)
1. Nachillaik lokomotivnogo otdola Tashkentskogo otdeleniya
Sredneaziitskoy dorogi (for Korolev).
-7
zt~
ACCESSION NR: "4033111 5010/64/000/003/0069/0071
AUTHOR.. Alkhazov, G. D.'.' V~rdbly'ev. A. A-';,.1Kord1eV"Y. A.;
Seliverstav, D. M.
TrME: Simple countingunit for's-slow' multichannel analyzer
Way Z, '1964, 6 '-7l
SOURCE: Pribory* i tekhnika eksperin;e no 9
r mult
TOPIC TAGS: pulse height'analyze' Ichannal, pulse height analyzer, slavi
multichannel analyzer, pulse counter, pulse counting unit
ABSTRACT: A simple counting'Wdt intended for low (up.to 100 pulse/sac)
counting rates to described. 'The unit in'recommiended for long -duration few-
pulise applications where reliability the main requirement. The 32-tube
counting unit was used In a 20-channel- time analyzer and tested for several.
monthe under actual opera#ng,condition's. The a-c line supply voltage is
stabilized by a farrorssonncs-~ stabilizei only;. variation of the plaft voltage
Card
R
ACGFMION NR: "40331111
within 200;-250 Y.does not *esult in false The powier consumption is
200 w. A simplified conniction dlapam'ix sbd*n and e4laiiied ii the'article.
Or it.-, art. has iI *f 1jure-9
ASSOCIATION: F1z*o-tekbnkhe0kiy4nst1tut AN SSM (Physico te chnicAl
Institute, AN SSSR)
SUBMITTED: 2OApr63 AT D-, PRESs j3060 ENCL: 00
SU33 CODE
/-,.No REF, soy: 000 OTHER:,000.
Card'';,1/Z.
NIKIFOROV, 11,A.; KUDFYAVTSEV, N.A.
Tiat'Lers to the editors. Uzb. geol. zhur. 8 no.-4,.8&-89 16.1,
(MIRA 18:5)
1. Sredneaziatskiy nsuchno-issledovatallskiy institut geologii i
minerallnogo -gyri-yag Tashkenti, i Tashkentskiy politekhnichaskiy
institu-IL.
KOROLEV, V.A., inzh.; KIKLEVICH, K.A., inah.
mechanization of the removal and conveying of scrap metals.
Mekh. i avton. proizv. 19 no.7:18-24 J1 065. (MIRA 18:9)
1
KOROLEV, V.B.
The KS-13 automatic checking and sorting machine. Biul.tekh.-
ekon.inform. no.9:4'(,!-49 161. (MIRA 14:9)
(Sorting devices)
SOV/136-58-5-11/22
AUTHORS: Kolpashnikov, A. 1. , Candidate of Tecl~nical Sciences, anci
CIta-Mtg-Kuahg, t_ Korolev, v.D., EinCineers
TITLE: Hew Developmeats in the Production of 11.11heets From Almdod-um
and. its Alloys (Novoyc v proizvodsLve lioLov iz alyuminiya
i ego splavov)
PERIODICAL: Tsvetnvye NIetally, 1958, Vr 5, pp 62 - '~O (USSR)
ABSTRACT: The authors give a condensed account of the results of
their work on the imDrovei:,ent of the technology of alu-
minium and aluminium alloy sheet production. This has
already been published in I'Aviatsionnj~e m-,:Zterialyll, lc'5~/,
nr 2 (Pekin, Chinese People's Republic). Their conclusions
are that their investic~ations have established the possi-
bility of hot-rollinE ingots uithout edr,-_ trimming and of
raising the reductions in cold-rollinL-;:,- to 90;'~ and ovcr
without havinG to resort to intermediate annealing and
without impairin&~ mechanical properties, surface quality
or structure. The new technolOLy 'F-as been adopted
Card 1/2
rn
qg
36- 58- 5-11122
iiew Developruents in the Production of SheetJ2 fro-E Alwiiniu'r,, and its
Alloys
at Soviet and Chinese works.
There are 6 figures and 5 tables
1. Alimin-an--Processing 2. Aluminum alloys--.Processing
Card 2/2 3. Sheets--Production
2%
TIT-LE: Investigation of the stability or a gyrocw~~ss with the methods of nonlinear
mec4anics
rekhanika tverdogo
SOURCE: Inzhenernyy zhurnal. k tela, no 21 1966, 191-192
TOIIC TAGS: gyrocompass# nonlinear equation, nonlinear vibration
AB.4.TRACT: The conditions for instability of a gyrorompass in the case of uniform shipi
circulation (t) = -'PW SiA (oil - NJ
aro determined using the asymptotic method of Krylov-Bogolyubov a-ad a variant of the
snut1l paxameter method. The system of d:Lfferential equations describing the small
osoillations of the_sensing element of the gyrocompass is written in the forms
;W + Vs IP2 + v** - (ps - vl).cw 201E, (ps - v$) ain 20P4
112 IjA + v2+ (p0 0) cos 20% 'is (pl - vI)sju 20j, Oil
whare
Fa
ZI coo 0 - 7481n 0,
Cai-d 1/2
C
KOROLEV, V.D. (Moskva)
Stability of a two-rotor gyrocompass. Izv. AN SSSR. Mekh. no.5;141-143
S-0 165. (MIRA 18:10)
SOV/136-59-4-12/24
AUTHORSt Kolpashnikov, A.I., Candidate of Technical Sciences and
Korolev, V.D., Engineer
TITLEt Homogenisation of Duralumin Ingots in Modern Air-
Circulating Electric Furnaces (Gomogenizatsiya slitkov
duralyusina v sovrem*nnykh elektropechakh s
vozdushnoy tairkulyatmiyey)
PERIODICAL: Toyetnyye metaliyj 1959, Nr 4, pp 64-69 (USSR)
ABSTRACTs In the production of strip, homogenisation is important
as it achieves the following: 1) an improvement in the
mechanical properties and in the structure; 2) a decrease
in anisotropy of mechanical properties occurring during
rolling; 3) removal of internal stresses and 4) an
improvement in anticorrosion properties. The present
work investigated the rate of heating, the time of
heating and the rate of cooling. The homogeniaing
temperature must be lower than the eutectic temperature.
The temperatures most likely to be useful were found by
heating and examining metallographically. The influence
of the homogenising treatment at various temperatures on
Card 1/3 the structure and mechanical properties was investigated.
SOV/136-59-4-12/24
Homogenization of Duralumin Ingots in flodern Air-Circulating
Electric Furnaces
The alloys used were D16 (4-5 Cu, 1.5 Mg, o.6 mn,
0.3 Fe, 0.25 Si) and DI (4 Cu, 0.7 Mg, 0.6 Mn, 0.3 Fe,
0.3 Si) and the homogenizing temperatures varied from
400 to 5006C (tables 2 and 3). The influen~ze of soaking
time at 490*C is given in Fig 1. increase in time results
in increased plasticity (e.g. DI increases from 2.7 to 8%
after 36 hours). Fig 2 shows the effect of different
treatments. 2 Hours at 400 and 6 hours at 44o-46o*C have
little effect on the mechanical properties. The
metallographic structures show no solution of the second
phase. Even with 36 hours at 4ko-46oe there is no
significant difference in the plasticity or the structure.
An analysis of the mechanical properties and the
structures showed that the most efficient homogenising
treatment was 6-12 hours at 5000C. This gave the optimum
plasticity and allowed successful hot or cold rolling.
It enabled hot rolling without scrap on the edges and
Card 2/3 cold rolling without any intermediate temper. Thus output
SOV/136-59-4-12/24
Houtogenisation of Duralumin Ingots in Modern Air-Circulating
Electric Furnaces
could be increased bY 7-8%. The influence of
homogenizing treatment on the mechanical properties
of hot-rolled specimens is shown in Fig 3, 4 and 5
and cold-rolled specimens in Fig 6 (the broken line is
after homogenizing). It can be seen that good properties
are obtained after hot or cold rolling. Hot rolling with
a finishing_t;mVerature of 38o-40oc followed by a slow
cool to 240 2 0 gave good plasticity. The change in
properties of 1 mm strip with homogenising treatment is
shown in Fig 7. An air-circulating furnace (type
Gidroaviaprom) gave good results. There are 7 figures,
3 tables and 3 Soviet references.
Card 3/3
L 2~616-66 pdr(l)&cc Gy
ACC N.R: AP6009539 (A, 9) SOURCE CODE: UR/0413/66/000[ibb-570-01"ST60-1-!~-
AUTHOR: Samaylenko, V. F.; Kqm1evV..D.
ORG: none
TITLE: A magnatosensitive system for a qj&WjMttar, Class 42, No. 179484 [announced
by the Special Design Bureau of the State Geol2gical Committee SSSR (Osoboye kon-
struktorskoye byuro Gosudarstvennogo geologicheskogo k0mitetaISSR)
SOURCE: Izobretenlya, prvmyshlennyye obraztay, tovarnyy4e znaki, no. 5, 19669 75
TOPIC TAGS- magnetometer, magnetic field intensity
ABSTRACT: This Author's Certificate-introduces a magnetosensitive system for a mai-
netometer. The unit contains a permanent indicator magnet mounted on tension wires.
The fzequency range of measurable variations is expanded by making the indicator mag-
net from a highly coercive barium ferrite in the form of a parallelepiped with the
long exis parallel to the filament. The length of the edge parallel to the filament
-is at least twice as long as the axis of magnetization.
SUB CODE: 91V1 SUBH DATE: 02Jan64/ ORIG REF: 000/ OTH REr., ooo
UDC: 550.380.8
Card
ILOLPASHNTKOV. A.I., kand.tekhn.71auk; KOROLSY. V.D.. inzh.
Industrial processes in the production of alumi= alloy
shoats. Trudy KATI no.44%39-4 16o. (KIRA 13:6)
(Aluminum alloys) (Holling(Ketalwork))
tDSETROV) P.P.; SOKOLOV,, N.V.A KORULLV, V.D.; DEMINTIYEV,, V.F.; KUZNLTSOVA, R.M.
I
High durability drilling ropes. Metallurg 7 no.12:28 D 162o
(MIRA 15:12)
1. Beloretskiy staloprovolochno-kanatnyy zavod.
(Wire rope)
L 5~126-66 EWT(d) BC
ACC NR: AP5W6933 SOURCE CODM UR/0373/65/000/005/0141/0143
AUTFDF.- Ko scow)
ORG: none 2-7
TITIEt Stability of a two-rotor gyrocompass %'k'A
SOURCE: MI SSSR. Izventiya, 14ekhanika, no. 5, P65, 141-143
TOPIC TAGS: stability criterion, gyrocompass., Integral Pqiintion, approximation
metLod
ABSIRACT: A now technique is outlined for integrating the free oscillation equa-
tioll of sensitive elements in a gyrocompass, Starting with the set of differential
eqwitions for a two-rotor gyrocompass, the following integral equation is obtained
Card 1/2
29560
B/122/61/000/005/011/$13
D221/D304
AUTHORS: Kogan, M.G.* Candidate of Technicalk Sciences,
Korolev V.F Kleymenov, A.I., ana Baranovo LeNer
gineers
TITL3: Bathe for ultrasonic cleaning of components
PERIODICAL: Vestnik maehinostroyeniya~ Ino. 5, 1961, 68 - 69
TEXT'.- The Scientific Research Technological Institute developed
a series of baths, M-15-UB-18 (UZV-15-UZV-18) for ultrasonic
cleaning of components. They are made of stainless steelg and Dour
cea of ultrasonic vibrations of 20 Kc. in the form of magnetostric:
tive transformerev type nMC-6M (PMS-6M) are fixed into their bot-
tom, The radiation diaphragm of each transformer is a square with
a 300 mm side, The baths are enclosed into soundproof casingsp
which form a decorative facing at the same time. 6eals are provi-
ded in the covers of sound insulating casings. An outlet is fixed
under the coverg and the former is connected to the ventilation
system of the shop. The coiled pipe in the bath is used for-feeding
Card 1/3
29560
S/122/61/000/005/011/013
Bathe for ultrasonic cleaning ... D221/D304
cold or hot water to control the temperature of the cleaning fluid.
The 'vibrators are cooled with normal feed water which is consumed
at the rate of 3 1/min per vibratoro Gnerators Y5r -lo (UZG-10) and
UZG-2.5 supply the oscillatory power (10 and 2.5 kw respectively).
Cleaning the components is achieved by organic dissolvents or in
water solutions of alkalis and synthetic surface active subatances.
The use of acids is limited by cavitation and corrosion reqiatance
of baths and of the radiation surface of vibrators. Gasolene q0_
r
A.
WA ('Galosha) as per rOCT- (GOST)443-56, is the most widely used
organic dissolvent for removing grease and mechanical ingress of
dirt, Cleaning components of resins and nitroenamels takes place
in acetone mixed with alcoholp at a temperature of 3000. Use of
chloride organic dissolvents is restricted by their toxicity. Nor-
mally, cleaning in organic dissolvents is accomplished in two or
three consecutive baths9 the last one for final cleaning. The du-
ration of operation depends on the degree of dirt and the form of
conponentsp and varies from 2 to 5 minutes. Cleaning in water Bolu-
tions of alkalis and synthetic surface active substances takes pla-
ce in one bath. A description is given of materials employed and
Card 2/3
TTJ-RGU1.'OV, Dadakhan Tufgwicvi-ch; DNITRIYEV, Niko-lay i-varovich;
BELM."KH, Alek2andr Davidovich; A~,QLEV, V.sevulod
Aleksandrovich; CHMMYSHEV, V.I., red.
[Specifiliv,ation of diesel locorotive depots; from the
experience of the Central Asian Rail T-oad I Spetsializa-
tsiia teplo,.uznykh depo; iz opyta Sredneaziatskul. dorogi.
Izd-vo "Transport," lc)6.4. lie, p- (1vUR A.17:8)
MosIcva
XCF..C LEV, V. F.
209'i2 Korolev, V. F. "Iekhanicheskoye doyen-ye korv. II.,ornik dokladov Pervoy
Vsesoyuz. Konf-tsii po iroloch delu. 1949, s. 236-42
SO: U,,TCI-'13 ZHURNAL -'3ATEY - Vol. 28) 1,oskva, 1949
1.