SCIENTIFIC ABSTRACT SOLOVYEV, YE. - SOLOVYEV, YE.S.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001652320016-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 25, 2000
• Sequence Number: 16
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SOIDVITZV, Ye., Inzh.
Using monolithic slag concrete In constructing buildings. Bell.
stroi. 9 no.5:15-17 Ag 154. (Mlii 13:2)
(Farm buildings) (Concrete construction)

SOI,OVIYKV,Ye., inzhaner
Walls of clay and rushes for farm buildings. Sell.strot.10
no.6:11-14 Je'55. MuA 8:10)
(Walls) (Building materials)

SOIAWYXV, To., inzhener.
Concrete work under winter conditions* Self.stroi.11 ne.):19-20
Mr 156. (MLRL 9t7)
(concrete construction-CsIA weather conditions)

SOIDVIYXV, Ye., inzhener.
Yaster drylug of lumber. Sell.stroi. 11 no.6sl2-15 Js 156.
(Lumber-Drring) (MMA 9:9)

SOLOVIYV, To., inzhanar.
-- ~-- -;`- -
Erecting farm buildings using monolitbic slag concrete.
SmIl.strot. 11 no.9:25-27 S 156. (NLRA 9tll)
(Slag concrete) (Farm buildings)

; , . I- ~.
11 P /I- // I
SOLOVIYNV. Yo., inzh.
taylke, slag concrete walls between brick columns. Sell. stroi. 12
no.10:23-25 0 057. (HLRA 1001)
(Walls)

SMYIYBV# TO., inzh.
Wing awphalt floors. Sell. strol. 12 00-31-23-25 Mr t58,
(Yloors. Concrete) (NM 11-13)

GXRASIMOVg N.A.0 kttnd.tekhu.nauk; UWVSKIT, S.Lp inih.j MALEVMNYY,, B.N.,,
inzh.; KUPCHINq D.V.p inzb.j SOIDVIYEVo Yo.A.t insh.
TestIng the refrigerating plant of *Smotopoll't the refrigerator-
ship. Khol.tekh. 38 uo.2z4l-" Mr-Ap 161. (KM 140)
1. 14ningradskiy tekhnologicheskly Institut kholodillvoy promyshlen-
nosti (for Gerasimovq Tam~iskijq Malevannyy). 2.'Baltiyokil
sudontroitelinyy zavod (for Kupchix~ SoloV?yey).
(Refrigeratl6n of-ships )

SHARAN't I.G.; PARTASHNIKOVA, M.Z.; MAFJROVA, t~*.I.; SCILVIYEV, Ye.A.;
7FLICHENOX, S.L.
Analytical application of calcion (prepared by the Institute
of Chemical Reagents) for complexometric and photocolorimetric
determination of calcium. Trudy IRF-k no.25s203-214 1,3.
IMIRA 18:6)

S/020/63/148/002/025/037
B189/B101
AUTAORSs Bozhevollnov, Ye. A., Solov'yev, Ye. A.
TITLEi Sensitivity increase of the luminescence reactions to cations
with organic reagents by freezing the solutions-
PERIODICAL: Akademiya nauk SSSR. Doklady, v. 148, no. 2, 1963, 335-53T
TEXTs A description is given of the determination of gallium and niobiu*
with 2,21,4--trihydroxy-5-chloro-(l-azo-1l)-benzene-3-oulfonic acid (I)
and of magnesium with 2-hydroxy-3-sulfo-5-bhlorobenzene-(i-azo-i,)-20-
hydroxynaphthalene (11) at nitrogen temperature. The fluorescence excited
Vy UV light was measured with a spectrofluorometer. At a 0.0004% concentra-
tion of I and with a gallium content of tho solution of 4,mg/ml,.pH w 2*29
the luminescence of the I-Ga complex at nitrogen temperature was ten times
more intense than at room temperature. The adsorption maximum was shifted
from 580 m,,tat room temperature to 546 m/,Lat nitrogen temperature. At
the same concentration of I as mentioned above and with an indium content
in the solution of 2 /,g/ml, pH - 5-8, the luminescence of the I-In complex
at nitrogen temperature was 100 times more intense than at room temperatum
Card 112

ACCESSION 11R: AP1033608 S/0032/64/030/004/0412/0413,
AUT'10.:S: Bozhevollnov, Ye. A.; Soloviyev., Ye. A.
TrL'L~-: Rapid method f or lead determination
SOUACE: Zavodukaya laboratoriya) ve 30,, no, 4. 1964p 4124a3
:A".i: lon.t Aiialypia, quantitative load determinationp fluorescent lead
1cid chloiide luminosconce, freezing lead chloride load chloride
co,Vlox, quartz mercury lwv PM 4o UFS 2 filter
ARMACT: It was found that by freezing solutions containing lead chlorides
their fluorescence was greatly enhanced., making it possible to determide (in
6~
liquid nitrogen) quantities within the 10-4 - 10-1o' range* A mixture of 1 ml.
of the analyzed solution and 0.1 m.1 IM (sp, er.1019) was cooled with ice-41& G1 to!
-200 or with alcohol-dry ice to -710. The luminescence of the frozen samples was
then compared with standards under a quartz-mercur,.t lamp PRK-4j, with a M-2
filter. The samples were placed as close -to the lamp as was possible. This
method permitted the determination of 1 microgram of lead in 1 ml of the solutione'
Card 1/2

ACCFZ31ON N14s APLODW
lo interference was introduced by the presence of Has X0 Be# Has Ca. 3r, Baj Zns
A.1) Gaj Tij Sn., Tap Cr., Hn. Co,, His Bi., wd Sb ions# $=33 concentrations of Fe
and Cuhowever, extinLpaished the fluorescence,
ASSOCZV1011t Vsosoyuzny*y nauchno-issledovateliskiy Institut khindches'kikh
reaktivov i osobo chisty,*kh khWchaddkh veshchostv (All-Union SaieAtifia Research
Institute of Chemical Reagents and Specially Pure Chemicals)
SOMTED S 00 DATE ACQs 26Apr64 EMLs 00
SUB CODE: CH NO REP SM 002 02HSRs 000

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n.4,-)bc chlstykt- khlmichpskt~-i vesY-~hnstv,
August 8, 1961.,

30LOVIYIY# Te.Y., &Astor
Controlling tuyere performance by the drop In blast pressure.
Hatallurg 5 no*7110-U' A 160* (MIRA 13:7)
1. TSeAkontrollno-ismeritelInykh priborov I avtomtiki rhel-
7abiaskogo metallurgichookogo savoda,
(Blast furnaces--Iquipment and supplies)

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SO'1/124-59-9-10799
Translation from: Referativnyy zhurnal, Mekhanika, 1959, Nr 9, p 162 (USSRI
AU'MOP, S010vtyev, Ye.G.
awm-- 11~0
TITLE: On the Calculation of Thin-Walled Sk6w Spar Designs
PMOD1TAL; Tr. Kuybyshevsk. aviats. In-ta, 1954, Vol 2, pp 90 - 96
ABSTRAr.'T., The article has not been reviewed,
Card 1/1 v

CMUIC4 IWAJ.--F (L S61riv my, (R&Ja.A4m,A..
SlAy1juni'164, V-Or's; ~IO 3 pp 76-1$)
Thor two "JoAl liela 4onkal
404du(t;w ImsWe a cl-lin4mall rmulvttor. an4f (61 coaxial
cyitWrital 1,00%dixto" 'With con*al k3m,"al sarface of
external tooductoc The wave inspeclancV. defined as
the ratio of th4 p.d. between the con4acton to Me
current AvwwS in am of them, it c%kuUtcd. TbA teat
P&A of tm dirwIlmoft 09"6 In tb* first &PPIWimawn
tho charatt"th~ irspedAnce of 4 So
live having the
.qy
"me tUmeaskim at the conwal lun~64 )a'it the given
t fteadson the Xvuvwtry, j
the medium %nd the w& Itngth, iticteasjq with
inCteA60i wavalength.

LT1_17F/-1V_-1C5 - n-j - 2 0"
Card 1/1 Pub- 153-20/30
Author Solov'yev, Ye. G.
Title Circular and Rectangular Waveguides with Longitudinal Diaphragms
Periodical Zhur Tekh.Fiz) 25, 707-710, 1955
Abstract Propagation of electromagnetic waves is analyzed in a circular and
rectangular waveguides with longitudinal diaphragms set periodi-
cally. The problem is solved by "stitching'! of the fields along
the boundaries. The electric field between the diaphragms is ap-
proximated according the rule of the traveling wave. An
obtained dispersion equation of the propagation constant is ana-
lyzed in the case where the vaveleneth in the waveguide Is longer
then the diaphragm period. Two references,
Institution
Submitted July 20, 1955

AID P - 4551
Subject USSR/Electronics
Card 1/2 Pub. 90 - 5/11
Authors Solov'yev, Ye. 0. and L. V. Belous
Title Theory of the spiral line enclosed in a cylindrical
semiconducting envelope.
Periodical : Radiotekhnika, 4, 31-35, Ap 1956
Abstract : The authors investigate methods of suppressing oscil-
lations and stabilizing a traveling-wave tube by
applying attenuation. To achieve attenuation of waves
reflected at the output and causing oscillations, the
authors used semiconducting attenuators uniformly
applied along the length of the tube. Best results
were obtainedAwith a thin layer of Aquadag applied on
the inside oMhe quartzitt envelope in order to be
close to the spiral. An analysis of dispersion equations
permits finding that there is a point of maximum
attenuation. The authors find the dependence of

AID P - 4241
Subject USSR/Radio Engineering
Card 1/1 Pub. 90 - 7/8
Author Ye. 0. Solov'yev
Title Propagation of electromagnetic waves between two
circular cylindrical surfaces In the presence of
longitudinal diaphragms periodically located.
Periodical Radiotekhnika, v. 11, no. 1, 57-6o, Ja 1956
Abstract Between two conducting coaxial cylindrical surfaces,
infinitely thin conducting diaphragms evenly spaced and
of equal length are located. They form a periodic
structure in the direction of wave propagation. The
author approximates the longitudinal field between two
diaphragms In terms of traveling waves. He obtains the
dispersion equation for the propagation constant. This
equation closely coincides with the dispersion equation
for a rectangular waveguide with longitudinal diaphragms.
One drawing, 2 Soviet references (1953, 1955).

CJ . . . . . .
yf,
report prownted at the First T*dmlwd Conflormee on the or jkw
Techniques Into the Xlectrima towAlator Ldwtzy, 12-15 Mhr 1958v State Set.
Wch. Ccmdttee of counan or YlInletere of ~.

88&3
8/147/60/000/004/015/016
10-9110 E081/E235
AUTHOR: Solovlyev, Ye. G.
TITLE: The Question of the Method of Approximate
Calculation of Secondary Stresses in the Complex
Resistance of a Thin-Walled Bar
PZKODICAL: Izvestiya vysshikh uchebnykh zavedeniy,
Aviatsionnaya tekhnika, 1960, No. 49 pp. 142-154
TEXT: The problem of the strength of a complex assembly
consisting of a covering with stringers or ribs is formulated
mathematically, and a deficiency in the approximate method
proposed by Ye.P. Grossman (Ref. 1: "Calculation of the Strength
of Longeron Wings", Trudy TsAGI No. 628, Oborongiz, 1947) is
pointed out. An improved method is suggested and applied to
the calculation of the longitudinal forces R in the ribs of a
thin-walled construction, having five identihl longitudinal ribs,
fastened in the lane x a 0 and loaded by a twisting moment M in
the plane x =-t Mg. 3) E and G are respectively moduli of the
first kind of the stringer material and of the second kind of the
wing covering material (Abstracter's note: This is a literal
translation of the definition of E and G on p. 142; E and G are
Card 1/4

W23
S/147/60/000/004/015/016
E081/E235
The Question of the Method of Approximate Calculation of
Secondary Stresses in the Complex Resistance of a Thin-Walled Bar
usually symbols for Young's modulus and shear modulus and it
appears from the context that t"ey aro used in this sense in the
paper) F i is the cross-sectional area of the i-th longitudinal
rib. The results are shown in the following table:
Accurate
solution Ye-P-Gro4sman's solution Author's solution
R kg
i RU) kg
i R(2) kg
i R(l) kg
i R(2) kg
i
1 4.8801 6-7883 - 5-0634 4-8721
3 -5-9733 -0.81975 -2.4542 -6.1125 -5-9701
in which Ri is the first ap?roximation
i I
imation to the longitudinal force in the
R 2 is the second approx-
I-th rib. A comparison
Card 2/4

88623
S/147/60/000/004/015/016
E081/S235
'The Question of the Method of Approximate Calculation of
Secondary Stresses in che Complex Resistance of a Thin-Walled Bar
of the exact and approximate solutions is also made for the case
in which the third rib has a different cross-section from the
othern and for a pyramidal thin-walled construction. The
conclusions are as follows: (1) Grossman's approximate method
can be successfully applied if the covering can be represented
as the conjunction of r weakly twisted panels having weak stringer
assembley and framed sturdy longitudinal elements. The problem
then leads to the compatible solution of r - 3 heterogeneous
second order differential equations with variable coefficients.
(2) The proposed approximate method allows: (a) calculations to VY
be made of a conical caisson by the method of sections; (b)
reducing the problem to evaluating axial forces in the elements
of lonGitudinal assembly to the separate integration of the
second-degree equations with variable coefficients, regardless of
the dependence on the relative thickness of the elements of the
longitudinal assembly and of the form of the contour of the cross-
section of the construction. (3) The proposed approximate method
gives an acceptable degree of error, but it only deals with
Card 3/4

88623
S/147/60/000/004/015/016
FMl/E235
The Question of the Method of Approximate Calculation of
Secondary Stresses in the Complex Resistance of a Thin-Walled Bar
secondary stresses, that is with corrections to the principal
stresses as found by elementary mothods. There are 5 figures and
4 Soviet references.
ASSOCIATION: Kazanskiy inzhenerno-stroitel'nyy institut,
Kafedra stroitellnoy mekhaniki
(Kazan' Institute of Construction Engineering,
Department of Structural Mechanics)
SUB1.1ITTED: March 30, 1960
Card 4/4

"?,/3 00
0.~ o
AUTHORS: Solov'yj~yj,__Te.A.,
TITLEs Stub Dolay System
Amplifier in the
21655
s/io9/61/oo6/oo3/oio/ol8
3140/Z135
and Karlova, Ye.K.
for Paramagnetic Travelling Wave
:entimeter Band
PERIODICALs Radlotekhnika i elektronika, 1961, Vol.6, No-3,
pp. ko6-4og
TEXT: The article describes work based on that of Do Grasse V~
et al (Ref.I: Bell System Techn.J., 1959, 38, 2, March, 305)-
The main difference from the earlier system consists in the wide-
band matching circuit (Fig-3) and'the introduction of the pumping
signal. The matching circuit provides smooth transformation of
the high-frequency field of the delay system to the H10-wave in the
rectangular waveguide. The pumping signal-is fed through a
rectangular waveguide entering the side wall at the centre of the
delay system on the side of the rose ruby so that the E-pumping
vector would be perpendicular to the side plane of the stub system.
To decouple the working and pumping channels, the planes of
polarization of the two channels were taken mutually perpendicular.
Making the narrow wall of the fundamental waveguide small enough
Card l/ 5

21655
s/io9/6l/oo6/oO3/0l0/0l8
E140/E135
Stub Delay System for Paramagnetic Travelling Wave Amplifier in
the Centimeter Band
so that at pumping frequency this channel will be a cut-off wave-
guide, the two channels are sufficiently'decoupled. The
fundamental signal cannot enter the pumping channel since for it
the pumping channel waveguide Is also cut off. The entire system
was designed for immersion in a pewar flask. Experimentally
obtained disRersion characteristics for a stub system of height
0.222 are given in Fig.4, and thd sertion loan of the system
in Fig.6. P,
There are 6 figures and 2 referencost I Soviet and 1 English.
SUBMITTED: January 29, 1960
Card 2/5

21655
5/10q/G1/006/Ou3/uIv/olG
E140/E135
stub Delay Sy5tem for Paramagnetic Travelling Wave Amplifier in
t:Ic Centij;.otcr Dand
Fir~-3
.11 1 . I .
Card,3/5
0

log/6l/Ou6/uo.-'/o 1(;/olU
~/L135
Stub Delay System for Paramagnetic Travelling ',dAve Amplifier in -
the Centimeter Band Fi -. 1j: Curven 1-5
relate to n system with a
cross-section ns _qhown in
0 Ftg. 4a; Curve 6 to a
LN system with a cross-section
-is stiown In Fig. 4b.
Curve 1- cx = 0.065. m=23;
Curve 2- a = `-045, m=21;
Curve 3- OL = 0.030, n1=20;
Curve 4- a 2, o. o65 with
4 rubies, Me45;
Curve 5- M = U-030 with
rubiesi M*38;
Curve 6- (X a. OXIO with
rubiesi m 28.
Card 4/5

21655
s/ioq/61/oo6/oOI1p/Olo/0l8
E140/E135
Stub Delay System for Paramagnetic Travelling Wave AmplIfier
in the Centimeter Band

PAIC. 6. I(PUBWO 2UTYX&IIHR UJIKM'
I- da - 0.0m; I - a -
Fig. 6
Cnrd 3/5

S1108162101710031002/0)09
Waveguide with parallelogram D299/D301
field into separate regionst in which the solutions are known,
then, either the fields or the impedances are compared at the com-
mon boundaries between -the so.-arate regions. Prom the figure it to
evident that there are 3 Duch regions. The problem is simplified
by linking tile fields not along the entire boundaries, b'ut at dt-
vidual points. From the equations for HmO_ and 1110 fields, and by
1:omparing the impedances at 2 points, one obtains the sought-for
dispersion equations a)
Otg xm - jI(x Ln a) (4)
0 m
wher-L, x. = kxm a/2 is the dimensionless phase constant, and a
the generalized waveguide-parameter. By setting, a
a.1
one obtains the well-known dispersion e uation for rectang-j'Lar wa-
veguides. With small values of x m (4) reduces to
Card 2/3

S/108/62/017/004/005/010
D288/D301
AUT110' A: 'Solovlyev, Ye.G.
TITLE: Contribution to the theory of a "comb with oblique
teeth"
PERIODICAL: Hadioteklinika, v. 17, no. 4, 1962, 34 - 37
T_-XT: 'Wher, dealing with electromagnetic wave propagation in wave-
Cuides of arbitrary cross-section, it is desirable to choose a re-
fei-ence syutem of which the coordinates line up with waveguide
Such a non-orthogonal system ie adequately described by fo.L-
loviing coefficients2 gXX ~ 1; g yy = 1; gzz = 1; gxy = 9Yx = sin 0,
all other coefficients = 0. The Hertzian magnetic vector is written
downp and the obtained formula is used to derive expressions for E
und If. A difficulty arises in determining the phase conatant for the
boundary conditions; a first order of approximation io obtained by
assuming identical phase constants in the upper open part of the
waveguide and in the lower pockets# divided by teeth, It becomes
Card 112

S/108/62/017/004/005/010
Contribution to the theory of a D288/D301
Dossible to establish the dispersion equation in terms of physical
dimensions of the teeth and their pitch. Two dispersion curves are
reproduced, showing retardation v.9, wavelength for 0 = 00 and 0
450, good experimental verification for the latter case being
shovin. It is confirmed that a comb with an oblique row of teeth
(8 ~ 0) causes less retardation than the conventional waveguide
1".1ith a straight combp (9 = 0). There are 2 figures*
SUBLUTTED: April 26, 1961
July 27, 1961 (after revision)
Card 2/2

AID Nr- 974-4 22 1May
GRAPHIC -ANALYTIC SOLUTION METHOD FOR A SYSTEM OF NONHOMO-
GENEOUS SECOND ORDER DIFFERENTIAL EQUATIONS MSSR)
Solovlyev, Ye. G. Izvestiya vysshikh uchebnykh zavedeniy. Aviatsionnaya
tekhni'ka , 7no~,963, 167-175. S/147/63/000/001/020/020
A method of calculating the strength of a thin-walled. slightly tapered stiffener.
based on the calculation of the strength of a bearn of variable cross section
subjected to axial pull and flexural loading, is presented. The problem is re-
duced to the solution of a system of n-3 nonhomogeneous second order differen-
tial equations, which are integrated by the successive approximations method
and the graphic method of B. Cough. The algorithm for graphic construction
of the bending moment diagram and for the elastic curve w(x) by Gough's method
is presented for boundary conditions of the first kind. The error of an approxi-
mate solution w(x) Is estimated. The proposed method makes it comparatively
simple to calculate the first approximations of axial stresses In longitudinal
strips of thin-walled, slightly tapered stiffeners. Second, third, and higher ap-
proximations of axial stresses are similarly obtained. ILK) -
Card 1/1

Alfir. 990 -9 14 J=e SO L 6V 'V6 (/j A. 6,
r4jdASER FOR AMPLIFICATION IN THE 3-cm BAND (USSR)
Ka;1ova, Ye. K., N. V. Karlov, A. M. Prokhorov, and Ye. G. Solov'yev.
Pr ory i tekhnika eksperimenta no. 2, Mar-Apr 1963, 107-1167---
S/120/,63/000/0021025/041
Performance and construction details are described for a 3-cm traveling-wave
materwhich used a waveguide section containing two ruby rods attached along
th ase of a comb delay array on opposite sides of the teeth. The ruby had a
Cr I* concentration of about 0.07% and was 2 mm in diameter by 100 mm long;
the ~ed (isolating) ruby rod had a Cr 3 * concentration of 1 to 2016. The external
hf niagnetic field was elliptically polarized in the plane of the comb,with its
major axis normal to the traveling-wave line of propagation, in such a manner
thatat an eccentricity of 1.5 the energy density of the forward wave on'one side
of the comb array exceeded backward-wave density by 25 times. MeasUrement
of energy density in the delay section was achieved by comparison of the EPR
absorption line intensity in a DPPH sample, when the latter was located alter-
nately in the feed-in and delay sections of the waveguide. The amplifier was
Card 2/2

11 rir. 99U=9 14 J-"--
TW 14ASO FOR AMMICATION [Cont-dl S/=/63/000/002/025/041
operated in a nitrogen-free He cryostat, type RP-09 , which included magnetic
shim disks to achieve a uniformity of external field of 11 gauss over the 100-mm,
working length. Amplifier performance. with a pumping wavelength of 1.2 crn
and external field of 4300 gauss showed 10 db of clean gain at 4.29K He tempera-
ture, and 21 db at 1.8*K. Mhe bandMdfh exceeded 20 Mc. Critical dimensions and
alignments of the maser elements are discussed. Photographs of the delay
element as well as the overall enclosed system are included. ISH)
Card 2/9

L 222-63 EWT(d)/EWT(1)/BD5 AF?TrC/ASD
ACCESSION NR: AP3004087 S/0108/631018100710020/0024
AUTHOR: Solovtyev, Ye. 0.
TITLE: Theory of a nonuniform helical line
SOURCE., Radlotekhnika, v. 18, no. 7. 1963, 20-24
TOPIC TAGS: helical line, nonuniform line
ABSTRACT: Propagation of electromagnetic waves in a helix with a continuously
varying pitch, as used in TWtubea, Is theoretically considered In the article.I
A method for calculating amplitudes and phase velocities of electromagnetic
waves along such a helix, based on the principle of variations, is offered. The
method permits determining field components of the nonuniform helix at any
cross section. Orig. art-haB: I figure and 23 formulas.
ASSOCIATION: none
SUBMITTED- 17Feb62 DATE ACQt O5Aug63 ENCL; 00
SUB CODE: 00 NO REF SOV: 001 OTIHM. 000
Card I/ a

t 32444-65 r6WT(d)/Emlf(m)/W(W)IW(T)/T-;j*M(k)/WA(b) Pf-4/Peb
IJP(C) IM
ACCESSION NR: AP4048616 8/0147/64/000/004/0117/0120
AUTHOR: Solovlyev, Ye. G.
TITLE: Designing Udo-walled hulled rods by the method of successive approximations
SOURCE: IVUZ. Aviataicnnaya tekhn~. 4, 1964, 117-120
TOPIC TAGS: thin walled construction, successive approximation, aircraft desim,
Hardy Cross method, secondary stress, beam analog, hulled rod
ABSTRACT: An attempt to made to overcome the difficulties encountered In the Integr*-
tion of the system of equations developed earlier by Yu. G. Odinokov which apply to the
problem of designing weakly-conic, thin-walled hulled rods with an open or closed crods-
sectional outline. A beam analog is used and applied to a sample problem for which
computational result8 are tabulated. This method, even in first approximation, permits
secondary stresses In the elements of a longitudinal assembly to be obtained with an
accuracy acceptable for practice. Two to three approximations are completely sufficient
for practical purposes. Higher orders of approximation are associated with carrying
out elementary operations on cumbersome expressions. In the method of successive
approximations the A coefficients and their ratio are comparable to the distribution
ik
Card

L 32444-65
ACCEMON NR: AP4048516
coefficients of the well-known Hardy Cross method. In this connection the method
successive approximations may be considered as a similitude of the Hardy Cross method
applicable to discretely continuous systems. 1"he graph-analyUc method makes It
possible, with a relatively small expenditure of labor, to find In first approximation
the secondary axial stresses in elements of the longitudinal assembly of a weakly-conic,
thin-waUed rod with grooves. Orig. art. has- I table, 3 figures and 7 formulas.

-C 14P
A
[ A11'i)001578
SOURCE CODE: UR/0 120/65/000/006/0124/0125
1AUTHOR: Abazadze, Yu. V.; Solov,12va.-Ye. G.
1ORG: none
ITITLE: Meaaurin, the group velocity In delay systems
.Jamoliftera
SOURCE: Pribory I tekhnika ekspertmenta, no. 6. 1965, 124-125
TOPIC TAGS: paramagnetic amplifier, quantum amplifier , electric meqf1urIng
instrument, delay circuit I
ABSTRACT: An outfit Its briefly described which is intended for measuring the
group-velocity delay in the middle of the passband (about 50% of the band). The
measurements are carried out at a fixed modulating frequency and, therefore, no
error due to frequency variation (usual in earlier methods) is introduced. The outfit,
consisting of standard instruments including an oscilloscope showing brightness
markR on Its screen, has an error of 2ye or less. "The authors wish to thank
Kh. Saberov and Yu. V. Pavlov for their participation In the experiments. 11 Orig.
art. has: I figure and 3 formulas.
SUB CODE: 09 / SUBM DATE: 16Dec64 / ORIG REF: 003
Card I/ I
Q 621.37
A

L 8igi-66 EKC(k) -2/i~WP WET I LIP(c)
ACC NRs AP6023067 SOURCE CODEt UR/0109/66ioii/007/1196/1199
WGIJDIJG
AUTHOR: Solov'Yev, Ye. G.; Abazadze, Yu. V.; Isayev, S. K.; Stepenovas
Yeo G6; Krynatskly, I. Be
ORG: none
TITLE: Traveling wave maser using chromium-doped rutile and a magnet
with superconducting windings
SOURCE: Hadiotekhnika i elektronikas Y, 11, no. 7, 1966, 1196-ligg
TOPIC TAGS: solid state maser, traveling wave amplifier
ABSTRACT: A traveling-wave maser using a rutile crystal doped with
Cr3+ is described. The maser uses a magnet with superconducting
Windings and is designed to work at the lower end of the decimeter
band at a temperature of 4.2K. The device is placed --ither in a
kryostat or in a heliumAicrocooler. The z2aser uses a dielectrically f
loaded delay comb structure (see Fig. 1), and was found to have the
following characteristics: tuning range, 100 Mc; amplification, 15 to
20 db; bandwidth (at a 3-db levelX 10-12 Mc; pumping power, 100 mv.
iC rd 1/2 UDC, 621.378.5-029.63

L 38191-66
ACC NRi AP6023867
Several vays or increasing the gain
of the device are given. Origo art.~,
has: 4 figures. [IV)
Fig. 1. Basic maser components
1 - Coaxial cable; 2 - teflon
screv; 3 - excitation pin; .
teflon filling; 5 ferrite
disks; 6 - teflon holder;
T - active crystal; 8 - pumping
waveguides
SUB CODE: 091 SUBMDATE-., IIYAY651 ORIGM: 003/ OTHMW: 002
ATD PF&W 5045
2/2

- ~ - -I ~c
AYONSKIY, S.I., professor, zaslushennyy dayatell nauki Tat. ASSR.- Aski-DYMIL.
Te.L. redaktor; GUBIR, A., takhaichookly redaktor.
(Physical and colloidal chemistry] Yisichaskaia i kolloidnaia khtmila.
Moskva, Goo. izd-vo OSovetskaia nauka.0 1954. 266 p. (MM 8:2)
(Chemistry, Physical and theoretical) (Colloids)

SOLOVIYNV, Te,,Io
Reccr.struction of the crcv= of the IXJ-3 electric furnace.
troltell no.11:13 1 160. (MIRA 13:10)
(Ilectric furnaces)

Y E
11,A I

Su,N)vIYz-,v, YU01. (Novosibirek)
Soluticn of the axIsy-=etric problem In the theory of elasticity
for bi--ply c3mected bodies of rev:~lution, Irzho zhuro .4 ro.3s
469-476 16P. (MTRA 18s7)

KOSTYUK, H.S.; BtMUX, A.A.; _SOIDVITIV, Te,M.
Yractional composition of milled peat in the course of the tech-
nological operationot of drying and harvesting. Trudy inst. torfe
AN BSSR 8:106-113 159. (MM 13:22)
(Peat-Drying) (Peat-Harvesting)

SOIA)VIM, Taygenly Mlkbaylovioh; POGODIN, L*L,# nmuc" redal
SKIRNOV, Tu.I., red.; ?SAL, R*Ke, tekhn.red,
[Manual for engineers of commercial fishing boats) Poooble
motorletu ryboproeWelovogo sudna. Leningrad. Gos.solusnoo
izd-vo sudontroit.pronqshl.. 1960. 354 p. (MIRA 13:11)
(Marine engineering) (Fishing boats)

". , - 1. .. -41 11 - 0. ..
Disnertation: "Irivastigation
'and 'Itbc~i 3ci, "oz;z:u,;
- . L~,
i*.o:;cc,,.,, 11o 13, Jul h.
uf Lne -~lcw of jL-q Solutionz -'etween Nio .';curxl
~ctroleur-i *.,z;ot, 1~53- .,,cfcrativjr,-.,-
Su: JUk, 1,67o. 356, 25 Jan 1955

AID P - 1094
Subject USSR/Engineering
Card 1/1 Pub. 78 - 5/21
Author : Solov1yev, Ye. M.
..........~
Title : The problem of reasonable wear of bits
Periodical : Neft. khoz., v. 32, #10, 18-19, 0 1954
Abstract Discussion is presented of B. S. Fedorov's analytical
determination of the wear of the bit as related to re-
duction of its productive drilling speed. The author's
discussion of Fedorov's basic equations indicates the
erroneous nature of the latter's interpretation and
conclusion. Five Russian references (1949-1951).
Institution : None
Submitted : No date

SOU)VIYEV, re'N.
........... ~ -
Xore on the criteria of effectiveneois of the operation of bilos Nef'JJO*
khos, 33 no.2s26-28 1 1550' (K= 8:4)
(BoriAg machinery)

SOWVITZV. Ta.M.
Calculating hydraulic losses In an annular "ca. Reft.khos.
35 no.1:40-44 J& 157. ()UA 10:2)
(Oil well drilling fluids) (Hydraulics)

SOWVIVEV. Ye.M.
I
Method of calculating well cementing. Izv. vys. ucheb. rav.: DOW
i gaz no. 5:4?-48 1.511. WRA 110)
1. Moskovskiy neft" noy institut im. sicad. I.M.Gubkina.
(Oil well cementing)

DMININ, Aloksey Pnvlovich, dotnont (deceased); SOLOVIXE, Ylevgeniy
Kntvoyevich.,,--dotsent. Prinimal uchnstiye: BORISMIKO, L-.T-..
k ~, n T.- t-aM...nou'k. TIMOYgTZV, H.S., lnzh.0 retsenzent; PWROTA,
Te.A., vodnshchly red.; F3DOTOYA, I.G.. tekhn.red.
[Drilling oil and gas wells] Burenis neftianykh gazovykh
skvnzhin. Hoskvn, Gos.nnuchno-tekhn.izd-vo neft. i gorno-
toplivnoi lit-ry, 1959. 495 p. (MIRA 12:11)
(Oil well drilling) -

LEONIDOVA, A.I.; SOLOV'YEV, YOA
A method for maki4g artificial sandstone. Izve vys. uchab.
zav.; neft' i gaz 5 no.3:37-41 162. (MIRA 16:8)
1. Moskovskiy institut neftekhimicheekoy i gazovoy prcayah-
lennosti imeni akademika I.M. Gubkina.

LEUD.WUW,p A.I.; ijjLUVIIhV, le.hq_
Relationship between the durability and permeability of cement stones.
Trudy MINKHiGP no.40:114-121+ 163- (KhtA 1614)
(Cement--,Permeability)

A.I.; !;OLOV',Tz',Vl Ye.14.
Effect of presmae and temperature on the filtration of eezont
olurries. Izv. vyah. ucheb. zav.; neft' i gaz 6 no.3;19-22 163.
(KIRA 16,~7)
1. Moskavskiy Institut neftekhimicheakoy i gazovoy promyshlennost.i.
imeni akadenika Gubkdna,
(Oil weU cementing)

tt !.(~j ~, ~ I!.,' . , .1.
A
ii,!- -,f All-Unirm Sta:xiards I.-ir plug~-.Ing roment; a t*pIc for
'- I OvapA m:7)
di" `j!,V!On. N(~~ft. khr,7. ~O no.12:17.12 D 162.
(Oil well cementing)

LENH1,07A, A.I.; ;-;(,,1k)V1WV, Ye.M.
Effect of filter cake on the water yield or cement slurries.
1zv.vys*ucheb.7av.; neft' i gaz 6 no. 12:29-32 163.
(MIRA 17:5)
1. Hoskovokly inntitut, neftekhimicheskoy I gazovoy promyshlennosti
im. akademika I.M.Gubkina.

SOLOV-IEV) Ye.M.
Some theoretical problems of oil well cc.-zeLt-ingo Irudy 41[114:Jhi~~i r,:).40:
133-138 163. 0L U 16:4)
(Oil well cementing)

ng
Yy
14
r.V I I i z o xn r,

.V1,
gazcriiy
Clul,k Ina I Uf --a-sk I y nt:f tyan:~y nauzhn.-,-
ly fl f7 t

L~ t
v 7
to r.-n, i ~t

- ~ -1 . . . I.- . ..
I i .,
,,.I I I! ~ , -~, , ~-.j " ~', " -~r i .: - -I n -, -,- -. - ~ , 4 t." . ",f*
1. 41
. 'T I
,: . P: - .,~, '~3.
I I I- .. - 0 ( ! -I . R ". 1 -1 - ~ --, ~

SOLOVIfIENJ Ye.M.i LEONIDOVA, A.i.
Investigating t~o3 filtrat.l.on prDperties of oil well comonts.
Trudy MINKUG? 46184-9) 164. (MIM 17: 6)

A.I.; 6CLOVI-LIV,
Efcuct of cc,.-aont-:l:urr)r flll.-:r losa on th-3 ntructuro and properties
of hardened cemont. Izv. uchell. zav.; rieftt i gaz 7 no.2:60 164.
1. lloskovuUy instItut noftekh.1--aichoskoy i gazovoy promysYdennosti im.
ak%doialka 1.11. GuLkina.

A -'a I J :'Ji 'al I'l i

Q"!

S.", 'ILL!Y,
IN,,torm!nIng the vollume of annular orace ir, the well cement!n
DAF-val, I
. Tieft. khoz. 42 no.11:45-48 R 164 (HIM V42

ill- -, ~ :.iv - ~ L. ,
J;- -
of w, !J,~ :n,-A,i3ilv of cc:-o:rlf. Olurr-J. Burenle
no,7:23-27 164. (MIRA 180)
1. 11fimAly neftyan(ri Inatitut i Mogkov-
91A-ly ordnna Tr-ulovcgo Kru3nogo Zmimeni Institut neftekhirsicheakoy
I ,az,,)vcy lremysi;'llonnustl im. alkad. GuUkina.
0

I I I 1 11'. V.
SOIPVIY~'V, Yp.,11.; A.!.; SHORT',IN! 0 N.!;.; J~,",MHUIX)7A#
Nitrolignin as a reducer of the viscosity and water loss of
cement slurry. izv. vys. ucheb. zav.; neft' i gaz P no.3:25-29
165. ( ,,ERA is: 5)
1. Moskovskiy Institut neftekhimicheskoy i gazovoy promyshlennosti
im. akad. GubkJna I Institut organicheskoy khimii AN SSSR.

ARDAYNV,B.V.; SOLUVIYXV,Te.P.
Machine for trAnaverse rib-veneer gluaing. Der.prom.4 no.6:25-26
Je '55. (Mmu 8: 10)
1. Tavdinskiy fnnernyy kombinat
(Veneers and veneering)(Woodworking amchinery)

SOL-OVIYEV, YE. P.
USSR/Metallurgy - Foun&ry, Xquipment SeP 52
"Mechanism for Closing the Bottom of a Cupola," Ye-P.
Solov1yev, Engr
"Litey Proizvod" No 9, p 16
Stating that existing constructions for opening and
closing bottom of a cupola are unsatisfactory, brieJOY
describes new improved mechanism for 5-ton, cupola.
Mechanism is simple to make, dependable, wA safe to
operate. Includes drawing.
Pit 03M
233T76

soLOVIYEV, Yuriy Pavlovich; WAKISHEV, Irinarkh Sergeyevichp
red. [deceased)
[Selection and hookup diagrams of auxiliary thermo-
mechanical equipment of industrial electric power plants
and boiler systems] Vybor i skhemy vkliucheniia vsporogatell-
nogo teplomakhanicheskogo oborudovaniia promyshleMkh
elektrostantsii i kotellnykh. Moskva,, Energiia, 1965 199 P.
(MIRA 18:7;

i & H v 1 or, (). I ) F
$ '""1 1 '" SIPLOITIT111 &W/130
Conre To PO spektras"Pil t.
aDoct-0.3-ps" (P.p.,
rvAeo 04 spect"-sac;y. 8 of th. lot,
L. vol. "Oloswar S stro
pe
""ta, 195T- 499 v. 4 ooo
"Into - (34rlogs It., ftsehmy
Addltlmoj Spa
MoOrS ;I A60nall Akadenlya nauk 33". looloalfs So
sPektrookopli. Uzor' S.L.1 Toaft. Zd.# T
Zdltorl&l am. Z'L"b'jstord,,Q;S I
Mmnt- a-S. fteter or 1%lAts"alslam (nom
ft IlrAju, I'L D'o am
f.A: 'bO;j,'*p for ~'101411 -4 MathomAtioal sole"Os'
Kandtalr1g, V 4' C r a rAY6 0&1 AM hatho~ootjooI Sdlgmo,o
cawidate or " '11414 Of TalWO4 Sol.".
"411441 am mathanotloal 0 "Yokly, S.M.,
at* Of thIG-441 11A M&V.*mtj@ solonods, k%xs"mkaj, L 9
C&JW'44t* Of PhlmiaoZ &1 34104006, MlILww;u' ;.;:.
A. To.. C&Mld&to of '" Mot'10"t,484 Solonoes am alambe"..'
CaNd 1/30 "421olu QW Mothomatleal Jot..",
NOvako I-Z-, andLU
Iftrion ww the xetat1ftu
Rrroot
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=

of T6
zoo.
"tl,, ,,,
rawro
t-- of SOft Parr
Oa tw Ufftred
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T&jv* "A- S4IIwv A S
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*- remotion In ig* '04AW,
but"lone
Wabbe
ft
OtQft of ;Ulum
r In &be p,,*Os
N.A., old S A LIght addGuen

84opy good " - - b0godkim.
Skurur St%4 me latergotlut--od Spootre.
an of nub 423
bor mw
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Nolf.409 r zetthylOhO Vtlt2am-) 8*1 V&Katlms
%war tb. 1
alac PA"as
0 426
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Me"s or xafft",
N.V.. To p
Odubft"
Of Ubs Yll
5 430
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00stromospla
ftre at some Alsols polpme
coo'd S7/
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s
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J. 2, No I
R.,
62-74(IQS7).--Tt;ft1YM q-tctra cA dicctyl (1), LeradcMitic
(U). Irtradcraric (III). dw-ane [IV), Xmi cct;me M Kcre
Studipd rt4 a fum,~U.,_m of temp. nr-.Ar tht 7-r. wtve~kngfb ti~-
ticm. The %tx~.-rptkjn spectrum of I at 20* plssccv~d r.1y
eme Wad. IMVmn -1, but at 75' there wcm pentnt 137161,
13740-, W~' Kud talk)-tra. "I h*fRj.;. On hir-.11int I fri-m ".
to In Iftf 1.37(0- %Ud 1379- CETI 1,91ndl U..

ds kit I' a. 1 70.. cm. t e u at
352.6, IS70.0, and 1379 cm. -1 The chaugti In the intem-
-
40- sked
hirs of the 1312, 130-, and the U
1370-cm.-I ban& wc-.r in up?o*-Ite dIrmd,-n vi each tither

nt 26"' t~_' _' - *. 'ngf-.
WbAM the teMp. of It WaS r&bWJ.1ri.~ =0
tMtrgY Of PXAtkmal Ltmncra vm,% 111(1379. 1370) - (M.
-AM1379, IM2A) - I(m, AH(Mij. 1543) - 1W. all
N~OZ 1352-13) - M0, 1110370. 130) - QV. and 411
(137,4 , 1312) - 7,% LcAl./izijle. Th,! %mctmm of U1 at
~0. C=tallled 1379- 1:Z*&. L343- wnd 1311-c=_-I
and aLso & vreak I bgnd; In t!tc c*,t. state ovIv the
'
r
t,-, 200
thr
-1 bzuA. fhi ticattnj IU (rom 20
'rue ii I V.- mid 1343--C~- tmcda d ~_
mc:g-.m
arld that at IJI.- and

of 63metiglt" a in -w-cie A11(1379, 1355) alt
IWO, 1"3) - WO, AM( ,311, 1343) - M, 411(1311,
3.15) - 2W kcul./muk. The spectium (J IV at fixca
temp. cmtairml 1277., 1.3W- 1354-. and 1379-cm. -1.
and at - 75' 12N7-, aud 1.3 # 0-,cm. -6.1rand 4. The W;~
prmaticc if 1343-cm," and IWrl,-cm. -I' Ixtivii, with 1he
Change III the State (10111 ~"Iifl to liquid, wa, (I'daned r() the
riftatifmal isomers of IV. With an increast ill the ttillp. from
"Off to VA), the true trarksmi&-inn vf the 137ILk-cm.-I b4nd in-
creik:5,cd frum to IS.5,,e that of 1351- arid 1343-m.-$
batid, dccrcaficd frolil '141,7c, to 191"C AU41 fruln rol to 48%,
rc,fp. From the teTjIp..iot(-jj,jty r4i~ithin.,&B(13719. 11343) -
7,A) kcLI-ImclIc und 105J kcA.1mole.
III the I ruw of liquid V wcg r t I"'. I I-, IJ 13 _' 1371.1-
cm.-I, will A -75' INuill.;.
~%t te-np, from 21)" t,~ VW t1tv :tlj,. trim if the 13'6-
-1 b-111.1 il"l rv "C3 Ir"nj W 14- r" .%fill that A 1:311-
cm. d I Iff~wc'vr. lo.cuu-'e Ole
" in, rk ,f."
-cill !)";Id t'.11 ."Alitki ilk (lie ;p'N'truirs -1 "JIM V Owar
I.jI.t if tlie nitati, if ti mltr.
file Itti W&gram
eq,opit-at.

57-28-3.2,/AA
AUTHORS: Flaks, 1. P. , Solov'yev. Ye. S.
TITLE: The Determination of Capture Cross Sections of One ai;6' TWO
Electrons in Sin,-Je Collisionj of Double-Charged Ions With
,as Atons (Opredeleniye sechcniy zakhvata odno,-~o i dviAh
k
'
elektronov pri odnokjWykh 3tolkroveniyakil dvukhzariadnykh
ionov o atonami ~;,iza)
1.1iurnal .2ckhnich~~slel:oy Fiziki, 195S,
PERIODICAL: ~4. Vol, 28, lir 3, pnp.612-0522
(I.SSR)
A36TRACTs 'A'he captxire crosi sections of og and Wo eleWona in Wair.
collizions of double-charged fro + , Ad+- ,Kr +- and Xe +-ions
with the atoms of an inert "foreign" Can within the ranCe
of the ion-enerjy T from 6 to 60 keV are here determined in
an experimental way, For the determination of the capture
cross sections C51 and 0'20 the mass-spectrometry nethod
of the recording o fast ions and fast neutral atoms (de-
scribed in Reference 1) was employed. In the investijated
Card 1 enerCy ranCe the authors observed an increase in the

~he Do to rm i ri :it i on of cit 1) t u re c ro aof (.,nt, ~Iwro I
Sin:,le CO.'liSiO-- 04' DZI-11ble-C~i,0'.-ed Ionj ',,~'Lth
r,_ cron3 sections -xi th increaoini
21- ; ion-oneri-,j.
T 60 keV the (71 033 nection is largest I; ~~Ie xc,-
-IJ-pair ( 0- 2 .) 1_7~ 2) .." ! 6- <
4~ 1 C)' 1 a21 21' .1b c1l d smallest in Xe '--Ho % 21
CM /. The existence of the czipturo procesi, aC two elec-
trons in the case of Ne2-r_ions in fie. Ar, Kr, Xe. in the case
of Ar2,_ions in lie, Kr, Xe, in the cage of Kr24- J.n Ar, XP
and in th? case of Xe2, in the Ar. Kr was deteni1ned in an
experinental way. In the case of the enuneratei lcn-atom-
-pairs the 6'. -cross section in~~reases xith incroasin,-;
ion-energy and2h; highly depnndent on tile nature of the
ion and of the aton. In all invest.,gated pairs at the same
ion-velocity Cr > U'_ , but in some pairs the cross see-
21 20-
tions T 21 ~nl ar n +cloae to the alba-)Iute value.
E;..,. at T - 00 keV R)r thevAr - Kr:vgir tile c~.-ost section
(Y - 6.10-16 c02 and 6' - 5.10 cm2~ As a rule dr
21 21
and '5"20 are greater in coliolsions or light ions with heavy
atoms. in two endothermic cases the cross sections of the
capture of one electron and in 5 enJothernic cases those of
the capture of two electrons were measured. In endothermic
cases tile cross sections G, a r, d 0,"'- as a rule decrease
21 2Q
Card 2 with increasing absolute value of the resonance-defect" A E.

57-23-3-2,q 33
1"he Determination of Capture Croso Sections of One ar;d _'w0 11;
SinCle Collisions of Double-CharCed Ions 'With Gas Ato-~is
In exothermic oases no definite dependence of the crosa sec-
tions and AY or, the quantity A E was f ound to exist
'T21 2?a
By comparing the da for "symmetrical" capture processes of
two electrons differing by the sign of the quuntity E it
was found that in case that 1AE 1> 10 eV,
In Uic exo-
thermic case is considerably higher. In c atj AEI/-6eV
the magnitude of the Cr -cross section Is little dependent
20
on the sign of 6E. The assumption is expressed that in the
exothermic cnse,46E having a considerable value,an excitation
of the colliding particles takes place. Data for the total
capture cross section 6. W cr + e- are j-iven. 'hese
1: ii
characterize the general weaken ng of Ue dou~lc char-ed
ion-beams in the different gases.
The authors were advised by N. V. Fedorenko, boctor of Phy.
sical-Mathematical Sciences and V. 11. Dukellakiy, Professor.,
There are 10 figures, 1 table, and 14 references, 4 of which
are Soviet.
Card

57-28-3-24/33
AUTHORS Fl&ks, 1. k., Solovlyev, Te. ~;.
TITLE: Measurement of Capture Cross Sections of Electrons for Singly
Charged and Doubly Charged Ions of Natural Gases (Izmereniye
secheniy zakhvata elektronov odnozaryadnymi i dvukhzaryadnymi
ionami v "sobstvennykh" gazakh)
PL~RIODICAI,t Zhurnal Tokhnicheskoy Fiziki, 1958, Vol. 28, 11r 3, pp. 599-
-611 (USSR)
ABSTRACTs Here the cross section for the capture of one and two electrons
bj means of doubly charged ions was measured and the dependence
of these cross sections on the ion energy was determined. More-
ovor he c-roes sectlons fur the resonance capture of the elec-
V.ons by meanz of singly charged ions were deterrained. All
measurements referred to the cases of interaction of the ions
u1 inert gases and of the atoms of natural gasvs. The cross
sections in the case of the singly charged ions were measured
i the ion energy-range of 3 30 keV and in the case of
doLluly oharEed icns in that of 6 -:-- 60 keV. The here applied
L;Cthod "or the det,~rmination of the cross sections is based on
Card 1/), the recording of fast atoms or ions which had formed from the

MeASUrOMCI'lt of Capture Cross 'io-ctivns of E'lectrons for Singly 57-28-3-24/33
Charged P-nd Doubly Charg-2d Ions of Natur4il Gajes
iuns of the primary beam due to collisions vith the ga3
atoms htppening b-.,t once, which were accompanied by the
cnIlture of the electrons. The cro4is sectionsO' of tha re-
-jollal'100 capture of tha electrons waa measured ~O men-15 of the
+ 4 . Y
Ne Ar Kr+- a%d W-ions.. The obtained da. ree wi'.h
-a ar
theory by Firsov (reference 1). Vie -r6so sec~ionsO',' of the
-.~tnture of one electron by means of Ile +-, Kr Ar *- and
xe -iuns wt-.~e measilred, 1r. the enerey range investigated the
sectil-1.3 cuntinuougly ircreaae wit), the iu:i engre-
_y.
The c6istenc,,~ of lth,~: ca7n~ture ~,rocess of two elec%rons .al means
2;
of Ne-+"I Ar2+-, Kr and Xe _io:-3 was e-c;,,3r!rierta11Z observ-
e6. T-e cross sectiun 620 of the capture of two el,~ctrons de--
it. ali cao.?u investirated with the increas- of lor.
envrF.,r. For Lhis re%~,or. it was concluded that the c'uptar-2 of
two electrons is a reionance process. Doctor of Physical and
Mlathenatical -;cienGes N. V. Fedorenko advised the aut h or ti.
Head of the LaLoratory,Profes3or V. M. Dukellskiy shuwed per--
manent intereot- it, this work. There are 17 figures and 22
references, 11 of which are Soviet.
ASSOCIATION: Leningrads%iy Fi--i'-o-tek,,aaicheskiy inBtitut,,AN JSjR
Card 2/~

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report presented at the 4th Intl Conference on Ionization Phenomena in Cases, Uppsala,,
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S/057/60/03o/o6/17/023 81596
J9 0 0 3012/B064
AUTHORS: Afrosimov, V. V , Win, R. Not Solov'-Vey, Ye. S.
TITLE: - Rare Gases
Ca2ture of Electrons by Proton In
PERIODICAL: Zhurnal tekhnicheskoy fiziki, 1960, Vol. 30, No. 6.
pp. 705-710
TEXT: This paper gives the results of the measurement of the full capture
cross section in the capture of one electron by protons with an energy
of 10 - 180 kev in He, Ne, Krj and Xe and of the capture arose section in
the capture of two electrons in Ar. Furthermore, the elastic and inelastic
proton scattering was investigated, ihich is connected with the
transitions H+---&~H0and H+ ~ H-, A short description of the measuring
method is given. For measuring the full capture arose section the condenser
method was applied that had been described in the previous paper (Ref. 6)
by the authore.The diagrams of Tables 1 - 4 show the curves obtained
for the relationship between the energy T and the full capture cross WK
Card I~1

Capture of Electrons by Protons in S/057J60/030/06/17/023 81596
Rare Gases B012/BO64
In previous papers (Refs. 8, 9) issued by the authors' laboratory it
Was stated that the relative probabIlity of the inelastic processes in-
creases while the distance between the nuclei of the colliding particles
decreases. The results of the present paper show that this conclusion
can also be applied to the processes in the capture of the electrons and
that this seems to be a general law in Inelastic atom collisions.
The paper (Hof, 5) by Ya. M. Fogel', R. V. Mitin, V. F. Kozlov, N. D.
Romashko, and the paper (Hof. 11) by N. V. Fedorenko and V. A. Belyayev
are mentioned. Professor N. V. Fedorenko and Professor V. M. Dukellakly
showed an active interest in the present paper. There are 6 figures
and 16 referencea: 11 Soviet and 5 English.
ASSCCIATION: Fiziko-tokhnicheakly institut AN SSSR, Leningrad
(Institute of Physics and Technology of the AS USSR,
Leningrad)
Card 3~4

23723
S/057/61/031/006/007/019
B116/B203
AUTHORS: Illin, R. if. and Solov'Yev, Ye. S.
TITLE: Ionization of argon by oxygen and nitrogen ions
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 31, no. 6. 1961, 680-687
TEXT: The authors measure7d the total ionization cross sections (a-), the
total electron capture cross sections (a 0), and the argon secondary ion
production cross sections (a ) for the ions N% 0% N" 0" NO*. and NO*
on 2 2 2
with energies of ';-160 kev In argon. They found that a- and the produc-
tion cross sections of doubly, triply, and quadruply charged argon ions
(d oV a03 . and oo4 ) increased with an increasing number of atoms in the
primary ion. They established a relationship between the capture of two
electrons leading to the transition 04----*0- and the formation of multiply
charged ions. Argon was chosen as gas target because ionization and
electron capture by hydrogen ions have been thoroughly studied for this
gas by V. V. Afro3imov, R. N. Illin, and N. V. Fedorenko (Ref. 2: ZhETF,
Card 1/6

23723
5/057/61/031/006/007/019
Ionization of argon by oxygen and ... B116/B203
charge, the number of nuclei with given Z is inseparably connected with
the total quantity of electrons and the particle dimension, it cannot be
stated which of these factors has a determining effect. Without con-
sidering the Z of the nuclei, the nuclear quantity itself does evidently
not play the main part. The cross section 6 01 is composed of the cross-
section ac of the single-electron charge exchange and the cross section
1 01
(1 01 of the single-electron ionization. The corresponding processes may
be written down in the following manner: I+ -& A-*I * A+ (1)
I+ + A )I+ + A+ + e (2), where I+ is a primary ion, A a gas atom. The
course of the o 01 (v) curve is mainly determined by (1). This is confirmed
by the following characteristics of the curve: (1) The ool(v)- and
a0(v) curves show a certain similarity. (2) At v