SCIENTIFIC ABSTRACT KURILINA, A. I. - KURILLOV, F. N.
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CIA-RDP86-00513R000927710019-5
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S
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100
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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XULIYEVp R.Sh.; SHAKHNOVICHp M.I.; SAMOVA, F.I.; MUSAYEVp G.T,;
CHIKAREVAp N.Ie; Prinimali uchastiye: ALIYEVAp A.; ALIYEVA# V,j
KATKCVA, 0.; BESSONOVA, Ye.; KURILINAp A.
Improving the quality of transformer oil from Buzovna crude
oil. Khim. i tekh. tople i masel 8 no.10:16-22 0 163 *
(MIRA 16111)
1. Institut neftekhinicheakikh protsessov AN AzerSSR.
I FA A i%,r -F,,FYF=YI7
VA
- -------------------------------------- - -
7or~ov a: A T
^T".013
A---giru fing
Tm- Tr M
t- rnp- PA-DIOD.
ACCESZKON, h1t.- AT3001316
inn't mftfxr 241) hre
2/2
KURIIJIIA) T.S.
Gomplications developed as the result of internal and subcutaneous
use of atropino preparations. Vrach. delo no.7tll,5-146 J1163-
41IRA 16slO)
1. Kafedra glaznykh bolezney (zav. - prof. P.S.Plitas) Kiyev-
skogo meditsinskogo institute. i glaznoye otdeleniye klinichaskoy
bollnitsy imeni CktyabrIskoy revolutaii.
(ATROPIRE) (671MCOMA)
14 (5) SOV/92-59-3-30/44
AUTHOR: Kurilkin, L.R., Laboratory Assistant
TITLE: The Organization of Oilfield Production and Work During
the Next Seven Years (Organizatsiya proizvodstva i
truda na neftyanykh promyslakh v predstoyashchim
semiletii)
PERIODICAL: Neftyanik, 1959, Nr 3, p 25 (USSR)
ABSTRACT: In addition to advanced methods facilitating the
exploitation of petroleum deposits, an important role will be
assumed by the automation and telemechanization introduced to
increase the productivity of labor and to eliminatemanual
work in various intricate operations connected with over-
hauling oil well subterranean equipment. It is expected that
by 1965, 60 percent of all wells of the Soviet petroleum
production industry will be automated and telecontrolled.
According to tentative calculation, it will be possible to
release at that time about 20,000 workmen. At present more
Card 1/2
The Organization of Oilfield Production (Cont) S(PI/92-59-3-30/114
than 300,000 oil well maintenance operations are carried out
in the Soviet oilfields every year. Maintenance and over-
hauling of wells cost almost 350 million rubles per year.
The organization of work in oilfields will be radically
changed as a result of introducing automation and remote
control. A certain category of specialists will become
superfluous. Training of oilfield personnel will have t.o be
revised and Its educational level raised. This program will
nece3sitate a change in the educational methods adopted by
vuzes and technical schools. All of these groblerps have been
discussed at the convention arranged in 195 by the All-Unlon
Petro"eum and Gas Scientific Research institute operating uri0or
the Gosplan of USSR. Materials pertaining t1o problems co.-"ne,~ted
with the reorganization of petroleum productixi called for by
the introduction of telemechanization, are being distributed
among various oilfield units. They will help to work out
recommendations necessitated by the introduction of auto-
mation and telenechanization.
-e)
ASSOCIATION: VNII(The All-Union Scientific and Resear h Institut
Card 2/2
IOSEV, M.T.; XMILKIN, L.R.
Oil field organiz!~~tion in connection with automatic and remote
control of petroleum production. Trudy VNII no.26:140-158 160.
(MIRA 13:9)
(Oil fields-Production methods)
(Automation) (Rgmote control)
FLYZHEINKOV, I.I.; LOSIEV, M.T.; KOL '-' 1,11 ~, T .,I.!. ; K U z--. I UK 1 . ", 1, . 1-', . ;
-t,, I . I-
TIKHONOVAt
Basic facers IlL thIO Frl'OW'il ("L JP"nr -viuct.1%,ity in ptrolaum
j.;r,-,Juf,tlon of' the Ti-rdy ~111T no-39:187-190 163.
(M I M 17: 10)
Effect of the production orjTar-,!,,,!Alon lind --!orH f, I ?
an labor productivity in ptrolei,;i~ 'i~iti.:2(Y)-213
lly, t f
ri,, a n,,r~ ,, u Is cif Llr. r- Z ~.l 7- fu T~! tro
sbor. po
1. V:3(3soyiiznyy vteCtet~rtzojyy
LOSEV, Mikhail Timofayevichj RYZHENKOV, Ivan Ivanovich; KURILKIY,
Leonid Roman 'o:VJrh;-KOLEMA5GVA, Irina Haksimovna;
TTKMWV~, LyudrAila Nikolayevna; IATUKHINA, Te.I., ved.
red.; POLOSINA, A.S., takhn. red.
(Labor productivity in petroleum production] Proizvoditell-
nost' truda v dobyche nefti. Moskva, Gostoptekhizdat,
1963. 152 P. (MIRA 16:10)
(retrbreum prod~ction-Labor productivity)
KMIIJIIN, V.S., master
All-purpose set of implement$ for mechanical assembling operations.
Suggested by V.S.Kurilldn. Rets.i izobr.predl.v stroi. no.13:
8&96 '59. (MIRA 13:6)
1. Kraenoturlinskore montazhnoye upravleniye.
(Hoisting machinery)
KURILYO) G P.,,-inzh.
New method of rudder filling. Sudostroonie 29 no.7167-68 J1
163. (MIRA l6s9)
(Steering gear) (Foamed matarials)
XMIKO, N.D., inzhener.
wk*;k,h*""!;,-*,-,~k~~..-,~10,,~ _"
Insulating the reinforced concrete slabs used In bridga construction.
Avt.dor. 17 no.2:27 S-0 154. (MIRA 8: 4)
(Bridges, Concrete)(Precast concrete construction)
KEJRILKO, T.
Cafeteria on Kreshchatik Street. Obohchaetv. pit. no.317 $57.
(MIM 1113)
1, Direktor kafe No.310 na Krashahatike, K17ev.
Wev-Restauranto,, lunchrooms, etc,)
W11
A%
is 3 1? 1 1
ILI
FAYNBERG, Ya.B.1 KURILKO, V.I.
[Adiabatic invariants for a plasma in a magnetic field]
Ob adiabaticheakikh variantakh dlia plazmy v magnitnom
pole. Khartkov, Fiziko-tekhn. In-t All U= 1 1960. 297-
303 P. (MIRA 17:2)
KURILKO., V.I.
[Kinetic theorl of the reflection of electronagnetic
waves from a novinC plaama) K kinoticheskoi teorii otra-
zheniia elektronagnitnykb voln ot dvizhurhcheisia plu~ny
Kharlkov, Fiziko-tekhn. in-t All USSFy 1960. 414~--423 p.
(MMA 17:1)
(Electromagnetic waves) (Planim (Ionized guses))
ACC NR. AP7001322 SOURCE CODE: UR/005T/661036/012/2210/2212'
AUTHOR: Krasovitskiy, V. B.; Kurilko, V, I.
ORG: none
TITLE% Oscillator acceleration by laser emission
SOURM Zhurnal tekhnic hakoy fiziki, v. 36, no. 12, 1966, 2210-2212
TOPIC TAGSt oscillator accele'ration particlea acceleration, laser beau
77'
ABSTRACT:' An analytical investigation was made of the possibility of
using laser emission an a means for amplifying particle energy. The
laser beam was considered a superposition of a large number of varioun
oscillations of close frequencies and random phases. The analysis
shows that the principles of particle acceleration by a resonant field
are also valid, under certain circumstances, in the case of a laser
beam despite the beamla wave phase differences and deviations from pure'
monochromatism. The required condition for acceleration is an appropri-
ate pulse duration, which should'not exceed a certain critical value.
Pulse duration above the critical leads to a reduction of the actelara-
tion rate. The acceleration effect is said to stem mainly from the
resonant harmonies of the field, which are most effectively absorbed by
AP7001322
the oscillator. The authors thank Ya. B. Faynberg for suggesting the
topic and for discussing the results, Orig..arts has: 9 formulas.
EWA-14)
SUB CODE: 20r/ SUBM DAM 22Jui66/ ORIG REP: oo6
-- ---------
81679
(0, ~'r)vo S/057/60/030/05/06/014
B012/BO56
AUTHORs Kurilko. V. I.
TITLEt The Reflection of Electromagnetic Waves From Moving
Surfaces
PERIODICALs Zhurnal tekhnioheskoy fiziki, 1960, Vol. 30, No. 5,
pp. 504 - 507
TEM The present paper was read at the Jubilee-Session of the AS USSR
(AS UkrSSR) held on the ocoasion of the 100. birthday anniversary of
A. S. Popov (April 7, 1959). In the reflection qf electromagnetic waves'b
from moving surfaces, the double Doppler offeotl'ocours ( 'Rof. 1). In the
case of nonrelativistio velocities of the reflecting surfaoea, a single
refleotion,may laad to considerable effects only in such cases in which
these velocities are nearly equal to the phase velocity of the wave in
the respective medium. This was pointed out for the first time by
Ya. B. Faynber . The corresponding investigation was carried out by the
latter and by V. S. Tkalich. The effects of the frequeni.,,y amplifications
and the amplification of the amplitude of the field may be conaiderab
Card 1/3
816751
The Reflection of Electromagnetic Waves From 8/057/60/030/05/06/014
Moving Surfaces B012/BO56
increased with a multiple reflection. This possibility was pointed out by
Ya. B. Faynberg (Ref. 4) and E. L. Ginston (Ref. 5). The prenent paper
deals with the quantitative investigation of these effects, which are
connected with a multiple refleotion. First, the simplified problem of a
non-steady process in a space bounded by two ideally conductive planes
is dealt withl the planes move towards each other with the velocities vj
at first they are at a distance of 2s, from each other; the field lying
between them is exprassed by the functions E(x) and H(x). The investiga-
tiorL is then extended to the entire range of the process and is applied
to a multiple reflection. Formulas (4) and (10) are derived, by means of
which it is possible to determine the field at any point between the
planes at any instant t, so that the problem appears to be volved. On the
basis of the investigation carried out, the following is foundt 1.) As
the distances at which the fields undergo essential changes decrease in
the course of time, the characteristic wave numbers increase according to
formula (10), and therefore also the frequencies of the compressed fields.
2.) The amplitudes of the fields between the planes increase with time.
The cause of this increase is, on the one hand, the reduction of the
volume, within which the field is enclosed, and on the other, the work
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The Reflection of Electromagnetic Waves From 3/057/60/030/05/06/014
Moving Surfaces B012/BO56
performed by the external forces, which move the walls with the given rate
against the pressure exerted by the compressed field. Both conclusions
apply only to < 1. Under real conditions, the dispersion of the
reflection coefficients leads to the amplitude increasing only so long
until the corresponding frequencies have attained their critical value
(Refs . 2, 6). Ya. B. Faynberg suggested the subject of this paper to the
author. G. Ya. Lyubarskiy discussed the paper with him. There are
6 references, 4 Soviet and 2 English.
AOSOCIATIONt Fiziko-tekhnicheakiy inatitut AN USSR Khar'kov (Institute of
Physics and Technology of the AS UkrSSR, KharIkov)
SUBMITTEDi July 2, 1959
Card 3/3
JURI~~,J.1.-JKurylko; V.I.]; MITROSIMICHEEKO, V.I. (14iroshnychenko., V.I#]
Reflection or electromagnetic waves by plasM,. Mr. fiz.
zhur. 6 no.3:415-416 MY-Je 161. (MIRA 144)
1. Fiziko-tokhnicbeskiy inatitut AN USSR, go IKharlkov,
Electromagnetic waves)
iasma(Ionized geses))
R
FAYNBERG, Ya.P.; Prininall uchastlye: KURILK,11, V.I.; HARCIIENKO, I.F.:
SPAPIR:)" "'~D.
Intpraction 'retwern team,5 of charFod particles and a plasma. Atom.
enprp. ',I no.4:313-'.3-5 0 161. (MIRA 14:9)
(Particlps (Nuclear physics)) (Plasma (Ionized gases))
2V65
41. .19.12 S/057/61/031/001/010/017
/.20 (~oq9l NkZ, IS-0 2_', fQ-2) B104/~204
AUTHOR- Kurilko I.,
TITLE- Kinetic theory of the reflection of electromagnetic waves
from a moving plasma
PERIODICAL: - Zhurnal tdkhnicheakoy fiziki, v-. 31, no. 1, 1961, 7 1-77
TEXT: The author investigates the reflection of electromagnetic 'waves
from a plasma moving in a space, in which the phase velocity, V
phJ' -1
of the waves is smaller than a. In experimental investigations, such re-
flectiono are studied In a waveguide. Here, the author assumes that a
decreasing phase velocity is attained with the'help of a suitable dielec-
tric. As a reference system, a coordinate sy3terj resting in the plagma
is chosen, in which the dielectric-,nicves. T_~er�ofore, for determining
the coupling between the vectors D, B, and E, 11, the Minkowski equations
may be uoed. By elimination of D and if, a system of equations is obtain
ed from the Maxwell equations, which describes the interaction between
electromagnetic waves and plasma in linear kinetic approximation:
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2 W
Kinetic theory of the reflection S/05 611~1031/001/01'0/017
B104YB204
dE-
a X. 91 -1- a E-
ds I ff'JO J&.YP
4?t/tA (1 - 02) jej cl dv,
4, jV..'P(-)
I , I ( V
E,
V n ifil) -"n 5a ..'. D-
a,= 2~('~L-1)1 a,= -4- a-;
PICO!
Me
is the deviation of the electron distribution in the plasma from
the equilibrium distribution f 0; n0 is the, plasma donsity; -'~ Is an
angle in the velocity apaoe; 6) is the freqUency of the incident waves
in the reference system; H 0 is a homogeneous constant magnetic field in
the z-direction; and V 0 is the velocity of the plasma. It is assumed
that the plasma fills the semi-space z > 0. The boundary conditions are
discussed, and wiLh their help, the following system of equation is obtained
Card 2/ 5
2 (D,--5
Kinetic theory of the reflection ... S/05"'V'I/031/001/010/01'i
B 1 04~B204
for the waves of this aystem instead of (1):
CD I
d' Ew dE"
-f.
a2E' ,
a. dz'E; (z) (K:L- (1z - --'I) -t- pK� (1z -i-
.d,
i. (I - A2) exp V,I V = oil (2)
VI
Mml
For solving this system, a method suggested by 1. Rapoport (Ref. 11.)
is discussed. The reflection coefficient is determined from the ratio
of the energy fluxes of the reflected and the incident waves:
R - m12 I M = H(O) (&) 3/2 (6).
+ m ET37 T-
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Kinetic theory of the reflection S/05 7/61 /0 31 /00 1/0 10/017
B104/B204
For m the author obtains the relation
+cD
1 n7It
M (a + 2n )dt (7).
_02p, i
-00
This relatiol is discussed for cases in which spatial dispersion is low
or strong, and also for the limiting case (1 .. p2) ao 0; finally, an
expression is given for m, which was obtained from(l) by the Laplace
method. From a discussion of th,e results obtained, the author draws the
following conclusions: Within the frequency range where for cold plasma
M' < 0 and the reflection coefficient (6) equals unity, the occurrence
0
of a low thermal scattering of the plasma electrons cau3es a decrease of
the re~flection coefficient as the result of oneru absorption. This ab-
sorption mechanism, which was first inveStigILted by L. D. Landau, causes
a damping of electromagnetic waves in a plasina i(ith non-zero temperature.
The linear dependence of the' reflection coef:,.'icient on thermal velocity
in the case of -a symmetric distribution function may be explained by an
Card 4/5
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Kinetic theory of the reflection S/05 61/031/001/010/017
B104YB204
ASSOCIATION: Fiziko-tekhnichoskiy institut AN USSR, Kharikov
(Institute of Physics and Technology AS UkrSSR, K)iarikov)
asymmetry caused by the boundary conditions. With p - 1, this asymmetry
vanishes, and the reflection coefficient depends on the square of thermal
velocity. Finally, the reflection coefficient for various special cases
is discussed. Mention is made of V. S. Tkalich, V. D. Shafranov. The '
author thanks Ya. B. Faynberg for raising this subject and for his help?
G. Ya, Lyubarskiy for his calculations, and A. 1. Akhiyezer for discussion
There are 12 references: 8 Soviet-bloc and 4 non-Soviet-bloo.
SUBMITTED: May 30,1960
Card 5/5
AUTHORS: Faynberg, Ya. B., Kurilko,
TITLE: The character of instabilities
charged particle beams and
23717
S/057/61/031/006/001/019
B10 9/B207
V. I,., Shap iro, V. D.
in the interaction betzeen
plasma
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 31, no. 6, 1961, 633-639
TEXT: The problem of convective and absolute instabilities 1,9 treated by
the method of 1. D. Landau and Ye, M. Lifshits (Mekhanika sploshnykh ared.
GIITL, 1954). In papers by A. I. Akhiyezer, Ya. B. Faynberg (DAIT SSSR, 64,
555, 1949; ZhETF, 21, 1262, 1951), D. Bohn, E. Gross (Phys. Rev., 75, 1651,
1949), and G. I. Biidker (Atomnaya energiya, 1, 5, 1956), the solution of
equations for small vibrations was formulated in the form
,p(r', t) - (p(y, -z)e i(kx-wt) (1)
with the criterion of inatability for the existence of complex roots of
the dispersion relation ~(k, w)- 0. The question as to the character of
the occurring instabilities remains, however, unsolved. According to
Landau and Lifshite, a distinction should be mfide between convective and
Card 116
23717
S/057/61/031/006/001/019,
The character of instabilities in the... B109/B207
absolute instabilities; in this connection, the behavior of the integral
+00
exp iw(k) t I dk (4)
-co
plays the decisive role. The study of this integral by the method of
Landau and Lifshits, which, for several reasons, is better than that of
P. A. Sturrock (Phys. Rev., 112, 1488, 1958), must be carried out for all
parts tj,(k) of the dispersion relation; for this purpose, the path of
integration of ~4) is changed according to Pig. 1. The curve C in the
i.~-plane (Fig. 2 with the integral
iot do
e (5)
C dk
corresponds to this path of integration. Points of type 0 do not lie on
the examined sheet of the to(k) plane; points of typp ca* make no contribu-
2
tion; consequently, (5) takes the form e-W (I). If t --Poo, only
d--
Card 2/6
23717
S/057/61/031/006/001/019
The character of instabilities in the ... B109/B207
the range 0 - 'K remains; hence,
03
[2
N d:-I
L
r.1 dw 2e (6)
e-I d
21
OW d 0 2n
All otherto(k) are treated in the same way. Then, a cold plasma (density
no ) interacting with a monoenergetic electron beam of density ni and
velocity V 1 is considered. After introduction of the usual frictional
v (-J>O), the dispersion relation acquires the form
foroe m,)eff'
41tel
Y
Wo no
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2.3717
9/057/61/031/006/001/019
The character of instabilities in the ... B109/B207
The points to be surrounded are -etrmined by
I +a -
Y + ix) 4
per 2
4 2'1/2
+a - V-
X i'j 4-
per ~2
a-
T
(Fig. 3). The points X+ , which, together with (6),might lead to an
per
exponential increase of perturbation with time, are meaningless (type tZ*);
2
here and also in the case )