SCIENTIFIC ABSTRACT PARIKOZHKA, I. A. - PARIN, B. V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001239220016-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 97
• Document Creation Date: November 2, 2016
• Document Release Date: June 15, 2000
• Sequence Number: 16
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

PAIIIKOZHKA -GA.,t-PUGACHq A.B.; EERMAN, N.A.1 FROIDVp P.A.
System for checking the inmdation of coymunication cables vith
plastic sheathing. Ilektrosviazi 17 no.5s49-57 Yf 163.
(MMA 16:4)
(Electric cables-TeBting) (Coaxial cables-Testing)

PAHKOZHKA. 1.A.
Deternining the distance to the location of the insulation fault
bY bilateral measurements vIth a bridge of vnriable-rptlo arms.
Vest.svinzi 18 no.4:9-10 Ap 158. (MIRA 11:4)
1. Starshly inshener Kiyevskogo otdelenlya ?Sentrallnogo nauchno-
iseledovatellskogo institute avyazi.
(Telephone cables-Kensuremente)

FUGACH, A.B,,, lush,; PARMOVUA -I-.I.
SPI-2 instrument signaling lowering of insulation resiatance In
cables. Vest.eviazi 18 no.10:11-12 0 '58. (MM 11:11)
1. fachallnik laborstorii Kiyevskogo otdeleniya Nauchno-iseledo-
vatel'skogo institute svyazi (for Fugach). 2. Starahiy inzhener
Kiyevskogo otdeleniya Bouchno-issledovatellskogo inatitnta avyazi
(for Parikozhka).
(Electric cables)

Q, PARIKOZ ho I.A.
Error of the bridge method for locating damages in the insulation of
cominication cables. Elektrosviazi 16 m.1:62-70 Ja 162.
(MRA 15:2)
(Electric lines-Fleasarements)
(Electric measuremerts)

PILRIKOZHKA, I.A.
Imating insulation damage in the strands of a cable containing
circuits with long-distance feed. Elektrosirias' 16 no.5:54-62
(MIRA 15:5)
my 62.
(Telephone lines-Maintenance and repair)

BOV/111-58-4-11/34
AUTHOR: Parikozhka, I.A., Senior Engineer ICONIIS
TITLE: Determination of the Distance to tho Location of an Insul-
ation Defect by Two-Side Bridge Measurements with Variable
Ratio of Arms (Opredeleniye rasstoyaniya do mesta povrezh-
deniya izolyataii s pomoshchlyu metoda dvustoronnikh izme-
reniy mostom a peremennym otnoshemiyem plech)
PERIODICAL: Vestnik svyazi, 1958, Nr 4, PP 9 - 10 (USSR)
ABSTRACT: A method is described by means of which the distance to the
location of an insulation defeat may be determined. The
method may be used not only when 'there are undamaged con-
ductors in the cable but also when all wires are damaged.
The methods available sofar (Murray, Varley, Fisher) have
certain disadvantages and cannot be used in all cases. The
method described by the author is partially based on the
Murray method and may be used ihen the insulation resist.-
ance of damaged wires is within the limits from 10 kilo-
ohms to 50 - 60 megobms or higher. Figure 1 shows the
arrangement of the measuring circuits. On communication
Card 1/2 cable lines this method may be performed with the instru-

SOV/111-58-4-11/34
Determination of the Distance to the Location of an Insulation Defect by
Two-Side Bridge Measurements with Variable Ratio of Arms
ment "KP-50", do bridge "UMV" or other devices. The method
may also be used on open air communication lines having a
contact resistance of 6 - 10 kilo-ohms or higher. There
are 3 circuit diagramis and 1 Soviet reference.
ASSOCIATION: KONIIS
1. Transmission lines--Maintenance 2. Electrical equipment
-Performance 3. Electric U~ridges--Applications
Card 2/2

SOV-111-58-10-10/29
AUTHORS: Plugach, A.B., Chief of Laboratory, Farikozhka, 3enicr
Engineer
TITLE: Device "SPI-2" Signalizing the Decrease In Insulation Re-
sistance in Cables (Pribor SPI-2, signaliziruyushchiy o
ponizhenii soprotivleniya izolyatsii v kabelyakh)
VERIODICALt Vestnik avyazi, 1958, Ur 10, pp 11-12 (USSR)
ABSTRACTt Devices used in main cable lines for signalizing decrease
in insulation resistance have several drawbacks: they need
considerable quantities of electric energy and several feed-
ing points; the life of tubes, etc. in these devices is very
short; they are insufficiently protected against disturbances,
The device "SPI-21' has been developed which has no such draw-
backs. It contains two relaxation relays with one thyratron
each, and an automatic block for switching the opticai and
acoustic signalization on and off, if the resistance Df the
line insulation is reduced to the critical value, The de-
vice is of simple construction and is smaller in size than
Card l/ 12 type "SPI-l". It is fed by only one source of 160 - 220 v.

SO'l-111-55-10-10/29
Device "SPI-211 3ignalizing.- the Decrease in Insulation Resistance in abi-es
The current needed i3 only 5 - 8 ma.
There is 1 diagram.
ASSOCIATION: baboratoriya XONIISa (Laboratory ICONIIS)
1. Electric cables--insulation 2. Insulation (ElIectr~c)----TeqtI,,-.g
equipment--Effecti-veness
Card 212

PARIMM, Michal, ings
The Ruzin vaterwork. Vodni hoop 13 no.2:52 163.
14

EIHE, E. ; PARIKS H - Spil CEY D. ; hUFAIS, A.; SFAIVULisj- Z.
I , , -, ""Li
_trarislato.*i -M.,LE A. [translator); GULBIS, V., red.
jy -
(Promising sj,'--- -")T" I Tar persr,ktiviem Skabbaribas
augiem. Riga,Latvijas Valsts izd.ba, 1963 P. 64 P. [1n
Latv-ian'j (MIU 17:7)

PAUL2~
4~v- Ided velding in foundries. Zvaranie 12 no.5:133-136
0
1, Zdarske strojirny a alevarnys nop,

PARIL, JjrI
Development of velding in the national enterprise Zdar Machine
and Metallurgical Works during the last ten vearm. Zvaranie 11
no.1:12-15 Ja 162.
1. Zdarske strojimy a slevarny.

21-7000 77258
S Ov/~
AUTHCRS: Ki-,,'
A.
Parilies
E.
,
,
,
TITLE: Tashkent Conference or~ Peacef-~-,, Use
Scien,'-ific and
PERIODICAL: Atomnaya energiya, 191SO, Vol -~
Nr 2
pp
,
,
ABSTRACT- Tf-.f~-,
19 5

o'- h e rria 1; U., i ~e piC. -4 A! h
,ector ~AP ne In s t e o r M a r P
A D
r,epcrL---j -_,:i prc,:,r,ess s,1-Je!Aii"c

-he
T~,. S. id V I
report.,2d oi. peacef'~-;i
.9. V. Starodubtsev, V'.ce Prr.?:,iderit ,Df'
c i e ri c eU L b e 1, 11 S R, p ~D 1%, --- o i i i n 'I., es 'L- i 1,
1-he -laboratory o" ji(-adei-,;y of Sr-`~ences,
.,ja,., Ji.-Ided
and radic Ff ft~y report-s wert,-
Card jlLi cm ri-;clear physics, ri'liclear reactions, and rw

T a Shi, ent Con fere-rir-, e a -_-e
so.,
Atomic Energy. S c J. en f--' ar; J Ef. C- C~ 1.";I,
News
Ca rd 2'/4
s c a
j j
vi,? r
_~ncler a,
or i a p p uri a r :-agne' j re,_; 1,~I
c a t c-, ~ i a J ~ c~ a C ID t' ~3 1-i
p 1 c S -1 A 1-
R;,, d
and nuclear radiati,-n iri technolcgy and 4,11
Twenty-nine reports and 10 Drief communi cat.
ven, In the report:,) were: descrill-)ed auttl-_)ma!~
a a-d 3~_,
un r.i i,
Re p r, r made al2c, r,
defec'.r"-~,-raphy ~_,f
Repcrt was made -~~n cf Ci~'~~_:
COG Ra. , !~:adr- a~, he lr.:3,
Ph~ Bic-3, E-ademy !,f' M" SSR.
Nlell' 1' rc;ck:~ aiA -n
ad ~a
D e

Tash~.ent Conference or, Peacef_~_' U_~e_ 7 7 2:::
Atomic Energy. Sc fil c ar:i En::--' ne-er' .g SOV"ll-
News
and nii,,luar radiatJon In
comin.unicat ions were gi-,. en. Several proble!-,.~s _i[-. !'ai4,,-
chemistry, radiation chemistr"j, application of radic-
active isotopes in chemistry, chemical analysils of
radioactive isotopes, preparation of p',,ire cz~mnpc~-_--is,
Lnvestiga~.-ion of kinetics of chemical reactions
isotopes, and gamma-spectroscopy were examined.
In the section of radloactive isotopes and -uclear
radiat4c.!. in medicine, ISO reports and ~onr~m
e re J, -odine app'icat~,~~-
gi Radicac_-~e L
treatmen' c." s;'oltur '.~.,as di3r-_issed, and Ccr:A1
e e ff e c in -nedical of ~r
la'ignan_
cf' appl_',~a!Lior; rad-ii1a,,.,"'
and reac, I ma s ~j
C) a!
_)9 repGr-.~; and 0 weve Prl. CrlE.- ri
(J;
ad 4~at ict, t? r egi,ieri. h I r
~'.as L.-Y, tc-t_- radioa.--i p - -
Card -~/4 method. PI-iysiologic-al, ILJ.olchemi,_,al ",a . d
S

Tashkent Conference c)r- 5
Atomic Enerf;y. Scien"'il'iic ar,.d O'ov
News
by irradiaticn ol' 1-1
alld u:1 upp 1 1 (-~J!
' I on
a v i c u I
as d 1 -1 c~s d .1j t~ a % i 0., ~D 1, i.: 41
n~isbandr a!IJ r,
-1 n, a rIv p ra J I
n :.a , me(-, t
P.-epa ra t. i Ll, if Rad 1. ao 1.1,,,~,.r-),-~s i~, 'USSR" (E.E
Ku I i s hG M Fra dk Ji Co, id d-' 1, ~L;j -,3 a nd A sp--,
za ~ i ori c) f Ra d i oa c: t ie I z3 o I- ~_;pefPa ' hi~ I o.
'I'- 'k c! v~:,is
.L,)ra e S 1 2, e a t-
M;-- c Js TI.
I . B Aic!L'
L-ashke-i!-
Pfz-~ace
Card 4/4

31065
311661611000100610061010
BI 02/b1 38
q
~AUTHORs Arifov, U. A.$ AcademicianAS Uzbekskaya SSRv
Khadzhimukhamedov# Kh. Kh.* _
!~arilisv ~_ I-, Kishinevskiyt L. M.
TITLE: Scattering of ions on metal surfaces
PBRIODICAL: Akademiya nauk Uzbekskoy SSR. Izvestiya. Seriya fiziko-
matematicheakikh nauk, no. 6, 1961p 50 - 56
TEXTs Experimental results of scattering of alkaline ions from hot and
cold metal targets are discussed and compared with theoretical consider-
ations. The aim of the investigations was to explain the sudden increase
in the ion scattering coefficiention reduction of the ion energy E. from
1-15 kev to some hundred ev. The scattering coefficient K. is defined as
'the ratio between scattered ayid primary ion current. The K (E ) curves
0 a 0
were plotted in the Eo-range 75-1600 ev at T a 300 K for Na and K scatter-
ing from No, Na from W, Mo and Ni and Cs from 11o. In all cases Ks
Card 1/3

3106
S~1661611000100610061010
Scattering of ions on metal surfaces B102/B138
increased rapidly with diminishing E and increasing mass of the target
0
atoms. At E,>800 ev K. increased with ion mass. At high temperatures
(T:.1500'DK) Mo targets were bombarded with Na, K, Rb and Ce ions. K8 fell
with increasing E0 and ion mass. For CB ions no fast scattering was
observed. The lack of Cs ion scattering at high temperatures means that
Cs ion scattering on a cold Mo target must be due to the film of adsorbed
heavy atoms which evaporate at high temperatures. The coefficient of ion
scattering from metal surfaces can be estimated from the relation
Ks=aofft,ell 60being the elastic forward scattering cross section, N the
number of target atoms per cm3 P Ae the effective depth of back-scattering.
2
a a UP . The collision parameter p is found from
0 0 0
Me Cos Mo.)
podr Ms
UW (P 2 (5)
Card 2/3 V

31065
S/16 61/000/006/006/010
Scattering of ions on metal surfaces B102YB136
r0 lenotes the least distance between colliding nuclei, p 0(E0) was
calculated for a Firsov potential U(r) 1 2 Y(z Z )r/a
r 1 2
(0. B. Firsov, ZhETF, 1958, 34, 447). ~,is the screening function. Eq. (5)
was solved numerically and the results were compared
The deviations (at low energies the theoretical curves
high, below, the experimental ones) are explained by
dependence of ~e on E0 was neglected. It is assumed
scattered from Mo atoms, but from heavier ones, e.6,.
and 10 references. 9 Soviet and 1 non-Soviet.
with experimental ones.
lie above, and at
the fact that the
that Cs4 is not
HE. There are 5 figures
ASSOCIATION: Akademiya nauk UzSSR (Academy of Sciences Uzbekskaya SSR)
SUBMITTED: July 26, 1961
Card 3/3

31068
S/166/61/000/006/009/010
Ot/p 3,~/1003~ B102/B138
AUTFOR: Parilis E. S.
TITLEs Theory of ion field induced electron emission
PERIODICAL: Akademiya nauk Uzbekskoy SSR. Izvest'ya, Seriya fiziko-
matematicheskikh nauk, no, 6, 1961, 78-80
TEXT: The possible existence of a necessary and sufficient condition for
field-induced electron emission from a dielectric is examined. The
mechanism considered is the neutralization of a slow positive ior. -,.hen
hits a solid surface. This neutralization is assuired to be an Auger
process with the probability W (E), ,(E' being the density of
'h'IH 12
tha final states of the excited electron and H 12 -.he matrix element of the
two-electron transition due to Coulomb electron interaction. It is a
function of the wave functions of the initial (V and final('
+ :I ~2 T3 T4
states. 11,1hen an ion, A,collides with an atom, B of a dielectric, the
2
CE.rd 113

31068
5/166/61/000/006/()09/010
Theory of ion field induced electron B102/B138
H12 expression can be integrated only in strong-coupling approximation.
This case is discussed for two possibilities. 1) 1/ and vf belong to the
+ ++ 1 2
same atom D: A + B4 A + B + e. This is impossible, 2) T, end T2
belong to neighboring atoms of the dielectric: A+ + B + B -)A + B+ +B+ +e.
1 2 1 2
This is possible but very unlikely. For field-induced electron
emission not only must V DIf (Vi-ionization potential), T-work function)
but also free electrons must be present on the surface. This condition
is not fulfilled for dielectrics. Even if a metal surface (e. g. Mo) is
covered with oil which forms a dielectric film, field-induced electron
emission will stop although VO 2~ is not violated. Finally it is shown
that field-induced electron emission can be observed only if the kinetic
enorgy of the ihoidert ion satisfies the inequality E0 Ea("o)
Fox ion energies of-1 kev and above field-induced electron emission is
ob3erved also from dielectrics. This emission in,3reases rapidly with
inareasing ion energy and is continuously changing into kinetic emission.
Card 2/3

'11205()
0(1,063, Ila 0) S~18-i/61/003/004/022/030
B1021-B209
AUTHORS:. and Kishinevskiy, L. MI.
TITLE: Theory of ion-induced electron emission
PERIODICAL: Fizika tverdogo tela, v. 3, no. 4, 1961, 1219-1228
TEXT: The field-induced electron emission has already found satisfactory
theoretical explanation and description, whereas for electron emission due
to ion bombardment (often called "kinetic emission") a proper theory is not
yet available. The existing theories are either too specialized or disagr ee
with.experimental results. The theory of Ya. 1. Frenkell, for instance, is
not in agreement with the adiabatic character of the deformation of the
ionic electron sheath at energies