SCIENTIFIC ABSTRACT SHEVCHENKO, V.I. - SHEVCHENKO, V.V.
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CIA-RDP86-00513R001549210015-3
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RIF
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S
Document Page Count:
100
Document Creation Date:
November 2, 2016
Document Release Date:
August 23, 2000
Sequence Number:
15
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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SHEME I~jvQ_,-V, 1,~~ ALPATOV. Ye.N.
--- -I
New devices for the electrolytic preparation of metallographic
sections. Zav..Iab. 28 no.7: 883-885 162. (MIRA 15:6)
1. Ukrainskiy nalLichno--issledovatel7skiy trubnyy institut.
(Ifetallography)
SHEVCHENKO, V.I.; ALPATOV, Ye.N.
1. -- - --- .......
Method of studying the three-dimensional microstructure of alloys.
Zav. lab. 29 no.9:1095-1098 163. (MIRA 17:1)
1. Ukrains.kiy nauchn6-issledovateltskiy trubnyy institut.
ACC NR; AN,03L'OV, SOURCE CODE: UR/0079/66/036/009/1642/1644
AUTHOR: Shevchenko, V. I.; Kornuta, P. P.
ORG: Institute of Organic Chemistry, Academy of SciencesiUkrSSR (Institut organi-'
cheskoy khimii Akademii nauk UkrSSR)
TITLE: Phosphorylation of cyanoacetic acid
SOURCE: Zhurnal obshchey khimii, v. 36, no. 9. 1966, 1642-1644
TOPIC TAGS: cyanoacetic acid, phosphorylation, phosphorus pen'tachloride ellnvoGr-o-)
C01)WOUA-40
ABSTRACT: The reaction of cyanoacetic acid with PCIS (molar ratio 1:2) in
benzene at 20-25*C yielded 1, bp.102-1050C,.n2O 1.5896:
D
NCC11,C0011+2PC15 o 211C1+POC13+C1.'P=NCC1=CHCOC1
At eemperatures-above 80-~-850C,'t r*eacts with PCI~ to form
II, bp 92-930C, nb2o l..5711:.
C.rd 1/3 UDC: 547.239.2
'_ AC-CNR, _AP603f384__.:___
PCI,
C13P=NCC'=C,,1COC1 ------- P. C13P-INCC12CIIC'COC' C'31)="4CC'=CClCOCL
Compound III (bp 88-91*6, n20 1.5611) may be obtai"ned I;y th~
D
reaction of I or II with elemental C1 or with FC1- -or by boiling
for 14--~-15 hr a mixture consisting of 0.1 mole cyanoacetic.
acetic and 0.45 mole PC15. Thus the course of phosphorylation
of.cyAnoacetic acid.depends on the conditions:
Pci. PG1. PCI,
NCCII,COOH NCC112COCI C13P=NCC1=C11COCJ
_11C1 PCI,
C'3P=NCC12CHC1COC1. C13P=NCCI=CCICOCI
C1.,P=NCC12CC12COC1
Card 2/3
ACC NRt AP6031384
III in benzene solution reacts wicTi glac.Lal acetic acid to torm j
IV, bp 78-80*C, n20 1.5339, d20 1.7555: 'WA-5Q; CBE Noq?121
D
C13P-NCC1'CC12C0C1 + C113G0011 --I' 11G1 + C113COCI + C120PN=CCICC12COCI
SUB CODE: 07/ SUBM DATE: 02jul65/ ORIG REF: 005/
~Lq.,d 3 / 3
J_J-L04
S/185/62/007/001/01L/01~1
D29C-/D302
Shapiro, V.D., and Shevchenko~ V.I.
ITTLE: --~ec' of elec-,,rostatic i*_,~Stabil~ties on the d4strib-
.::,~ -v L _- u _L 1.
Tion fu-nc-uion, of an electron beam whic'11 interacts wit*.-~
a plasma ir a magnetic field
U~
U-r--.raY.-ns I kyy f i zychnyy zhurnal, v . 7, no. 1 , 196 2,
!ODIC ~J,:
63 - 86
T -T- 2ori.,*Ul.~s are (derived for -he tem-oerature variatiOns and rec-
tified velocity of an "almost mono-energetic" electron beam, inter-
actinE with a plasma in a magnetic field. I-Phese formulas are obtai-
ned by solving the equatioxi for the distribution function f0. This
ecuatlioii is obtained Z-ror, the kinetic equation, by omittir-6 the ir,
ueural of pair collisions:
df, e Of.e &A e 6f,
jvH*1 ---~_ E, - > - -
61 Mc 3~ n, av inc dv
This integral is ovAtted, as fairly "fast" processes are considered.
The case is considered of !ongitudinal axiaily-symmeturic Plasma os-
(;arci 1/3
V185/62/007/001/014/014
of elec6rostatic izstab-llities--- D.299/!)302
U L -
cillations,
az-;su-,i;ed tha"U
slowly with
for,mations,
in a p-Lane per-p-endicuiar
the Diasma oscillations
co.,,-.,-oared to the pjlasi,-,a
one obtains from 2q. 0)
-P -
~. 0, 0
0 11 0v i ik
to the mraf:netic -,,ield. It -'s
are linear --nd. that fo cii-miges
oscil-latiOns. After trans-
t-he expression:
af
.- 0),
0v k
w,r) ihe ier-sor o-"' the di-F-Pusion coe-,-*f4cients ir- veloC4'y
ere aik is . L t, -- - - - t,
s7pace, in the presence of Ghe ma-netic field. A --Formula is -iven
C~
ror zhe case of instabilities due to th
-ior the tensor a ik e Vavi-
lov-Chcrenkov eff"ect, and to the --nomalous Dop~).Ler ef -fecz. ~by sol-
ving Eq. (4), one obtains formulas for -,,he lon.-itudinal- and trans-
verse temperatures and for the rectified velocity of the be,---a.. The-
se formulas Yield, in the case o17' a sufficiently rarefied plasma:
(A, 7). y'-T
- T~ . 12.- N~u3 (7)
M, (A 7)
T. V. T.
Card 2/3 It T.
S/185/62/007/001/014/014.
~;_~'Z'ect ol~' electrost_~-tlc ins-I.-r-bilities ... D29OI/D302
.Lor instabilities due to the anonalous Dop-pler e_ffect, and
Ic-
0 T) :j. 10-3 e (A TI U2, I JV' 1 (A 7~ (,IT)
(71)
T. T.
To To H
'(A, 7): (.17).
MIAU -iT
2.. iv,
_L or i-stabil4'es due to the Vavilov-Chererikov effect; il% formulas
(7) and (71), denotes -olasii,.a density, N beelia density, r
and and ~c z-re given by expressions involvi-1,El- N , w and
~D
2
e
',here are 6 Soviet-bloc references.
ASSOCL~TION: Fizyko-'ekhnichnyy i.
-qstytut JAIT URSH (Physicotechnical
institute of the As UkrRSR), Kharkiv
S U D I .'! T T" E DSeptember 2, 1961
Card 3/3
38860
S/05 62/042/006/017/047*
B1 04YB1 02
AUTHORS: Shapiro, V. D., Shevchenko, V. I.
TITLE: The nonlinear theory of the interaction of beams of charged
particlas with a plasma in a magnetic field
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v- 42,
no. (3, 1962, 1515-1528
TEXT: The:changes of temperature and the directed velocity of a beam of
charged particles on interaction with an electron plasma in an external
magnetic field is investigated in the "quasilinear" approximaiion. The
investigation is limited to the initial stage of the*process, where th ze
oscillation amplitudes are small and the time variation of the beam
parameter causes no significant change of the dispersion coefficients.:
During this time the amplitude increases linearly as in the linear theory.
A,n equation is derived which describes the change of the initial
nonequilibrium distri.bution function of the beam and of the plasma as being
due to interaction with the plasma oscillations. The.changes in the mean
values of the velocity and the temperature caused by the Cherenkov effect,
Card 1/2
/0 A
S/05 62/042/006/017 47
The nonlinear theory of the ... B104YB102
and by the normal and anomalous Doppler effects are determined.
ASSOCIATION: Fiziko-tekhnicheskiy institut Akademii nauk Ukrainskoy SSR
(Physicotechnical Institute of the-Academy of Sciences
Uki~iinskaya SSR)
SUBMITTED: September 20 1961 (initially)
March 14, 1992 (after revision)
Card 2/2
SHAPIRO, V.D.;
Quasi-linear theor7 of the instability of a plasma with
anisotropic ion velocity distribution. -Zhur. eksp. i teor. fiz.
45 no.5:1612-1624 N 163. (MIRA 17:1)
.... SHEVCHENKO, V.I.
- ---- - -- ---- 1-- "
Integral representation of a vector holomorphic in a sphere.
Dokl. AN SSSR 153 no.6:1276-1279 D 163. (MIRA 17:1)
1. Novosibirskiy gosudarstvennyy universitet. Predstavleno
akademikom I.N. Vekua.
11-''i I~ 11 %"I V. 1.
.,jo-stage bra'-ng u-' elec--rons ;n 0..t,Te traveling-wave tubes
-nd tackward Iio-Lek-l. 7
a -wavt tubes. jz*,,. vys. ucheb. zav.; rau
no.4:517-523 Jl-Ag 164.
17; 11)
~. SHEVCHENK05% V.I.
Boundary value problem for a vector holomorphic in a half-
space. Dokl. AN SSSR 154 no.2:276-278 Ja'64. (MIRA 17:2)
1. NovosibirAly gosudaratvennyy universitet. Predstavleno
akademikom I.N. Vekua.
SIEVCHENKO, V.I.
Construction of local and global homemorphisms for a certain
class of equations. Dokl. AN SSSR 153 Ao.2:300-302 N 163,
(MIRA 1602)
1. Novosibirskiy gosudarstvennyy universitet. Predstavleno
akademikom I.N.Vekua.
KARPOV, P.A.; SHEVCHENKO, V.I.j TEBYAKIII., V.V.; NECHAXEVA, M.A.;
NAZAE19996--'i.K. -' - *--4'-
Unconformity in the Upper Frasnian substage in the western
part of Volgograd Province. Geol. nefti i gaza 7 no.12,./+1-41+
D 163. (MIRA 17:8)
I- -
r3HLVG,HFNYf',9 V.I.
Golrer contiru1tv of solutions to singular integral nquations of
the normal tyTe. Dokl. AN SSSR 163 no.233,06-3,08 J1 165. (Ma-RA 18-.7')
1. N3vosibirski- gosudarstvennyy universitet, Submitted January 8,
1965.
S SR 163
21035:-1 8 7
L ~8492_66 EPF(nj_~/FWf(1)/FTQ(f)/FWG(m) IJP-U,) Al
ACC NRs . AP6013117 SOURCE CODE: UR/0057/(;6/036/004/0627/0639
AUTH03: -Shevche
kikko
_t3
ORG; :none
TITLE, -On the nonlinear theory of the instabilities,of a plasma in-a strong -electric,
field
SOURCE: Zhurnal tekhnicheskoy fiziki, v 36, boo A 19665, ~627-63 -
9
TOPIC TAGS: plasma stability, plasma oscillation, relativistic plasma, plasma
magnetic field, plasma-electric field, betatron, nonlinear effect,
ABSTRACT: The author discusses those unstable electrostatic and electromagnetic-
oscillations of an approximately uniform plasma ins strong electrie.field-that cannot
be stabilized by application of a strong magnetic field. The calculations were under-
taken because of the importance of these instabilities for theoperation of a plasma
betatron. The paper is divided into two sections of approximately equal length, In-'
the first section the linear theory of the oscillations is given. Thermal motions ar
neglected and the electrons are assumed to.move with respect to the ions with the
velocity u PC in th direction of an external magnetic field, which is of sufficient.
strength that 2 2),
9