SCIENTIFIC ABSTRACT KORSUNSKIY, M.I. - KORSUNTSEV, A.V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000825010011-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 14, 2000
• Sequence Number: 11
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

S/057/62/032/007/00,1/013
Electrostatic analyzer with B104/B102
regulate the ion-optical properties of each sector separately. A circuits
diagram for the supply of electrodes wherein the voltagee arrive at the
deflecting electrodes_by way of volta6e,dividers is discussed. There
are 6 figures.
ASSOCIATION: Kharlkovskiy politekhnicheskiy institut (Khar'-kov
Polytechnic Institute)
SUB'IMITTED: August 16, 1961

155 -16
S/02 62/142/006/008,1019
(/0 113'1-0:3~rl /0 5s-, B104YB10.8
AUTHORS: and Genkin, Ya. Ye.
TITLE: Thp interpretation of the L02 emission band of niobium
PERIODICAL: Akademiya nauk SSSR. Doklady, v. 142, no. 6, 1962,
1276-1277
TEXT: In a previous work the authors had corrected the L P2 emission band
of niobium (Is;v. AN SSSR, ser. fiz., L (1961)). The cleaf cutoff in the
corrected band corresponds to the Fermi energy limit (Fig. 1). If all five
electrons of the outer shell were collectivized in solid niobium, the
width of the emission band would 'be 15.6 ev. The width of the corrected
band, however, is only 12.1 ev and it iB assumed that only some of the
five electrons are collectivized. It has been shown by T. G. Berlincourt
(see below) that niobium has a positive Hall coefficient, p-type conduc-
tivity prevails. This is in agreement with the opinion stated above. The
short-wave part of the emission band is attributed to the collectivized
electrons, while the long-wave part is attributed to the non-generalized
electrons. In solid niobium, 1-1 to 1.3 electrons are collectivized in
Card 1'/2

7 7 S,/b58/62/OOo/0o7/o45/O68
_1~10 Ao6l/Alol
t
l
AUTHORS: Korsunskiy, M. I., Pastushuk, N. S., Litvinova, L. B., Mokhov, 0. D.,
TITLE: Negative photoconductivity in mercury-doped selenium layers
PERIODICAL: Referativnyy zhurnal, Fizika, no. 7, 1962, 32, abstract 7E245
(In collection: "Fotoolektr. I optiob. yavleniya v poluprovodnlkakh".
Kiyev, AN US SR, 1959, 220 - 226) ' 1/_~
TOM The photoconductivity of amorphous Se layers doped with mercury vapors
was investigated. The -layers were produced by evaporation of Se In vacuum and
condensation on a glass backing. A comparatively low-inertilal positive photo-
conductivity and an inertial negative one were observed when illuminating the.
layers with white light. On an increase in the concentrition of mercury atoms
in the layers the value of positive photoconductivity dropped, while that of nega-
tive photoconductivity rose to a certain limit, and thereupon-dropped. Both
negative and positive photoconductivity were examined as functions of the layer
temperature, of the intensity and the spectral composition of light. In additiou,.
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S1849162,10001000~0061016
A006/A101
AUTFIORS Borovikova, 0. P., Kors
TITLE: On the effect of micro-admixtures upon the X-ray emission spectrum,
of germanium L-series
SOURCE: Vysokotemperaturnyye metallokeramicheskiyje materialy. Inst. metallo-
ker. i spets. s -pl. AN Ukr.SSR. Kiev, Izd-vo AN Ukr.SSR, 1962, 4o
45
TEXT: The authors studied the effect of admixtures in amounts as low as
lo-3 to 10-2 at.% upon the X-ray spectrum of Ge L-series using specimens with
proportioned admixture content. Experiments were made with one pure Ge speci-
men (admixture amount below 1013 cm-3) and four Ge*specimens with different
amounts of antimony. e concentration of the antimony admixtures varied within
5.6 - 1017 - 4.8 - 101Pcm-3. The authors studied the correlation between the
oisplacoments of spectral lines Lp6 and 14 95 in respect to lines LLj1,2 and Lp,
respectiv ely, (as established in a previous investigation) and the concentration
of antimony admixtures in germanium. The experiments were-carried out on a
Card I/P

On the effect of micro-admixtures upon...
S/849/62/000/000/006/016
A006/A101
high-vacuum high-intensity X-ray spectrograph with a curved mica cr-jstal, using
a mixed method of exciting the X-ray spectra. The addition of jo-3 to 10-2 at.%.
antimony to single-crystal germanium was found to cause the displacement of
spectral lines Lp in respect to L,, of
,6 112 and of lines LIY5 in respect to Lp1
germanium toward the short wavelength side by-.1 - 2 ev, The magnitude of dis-
placement !IE- is proportional to the cube root of the concentration of
`6 - `1 S
2
admixture atoms. It was observed that the wavelength of lines L ~`2 and LA Of
germanium with antimony decreased as a result of the displacement of MIV,V levels
in respect to LIII and,LII levels. This displacement is approximately five'd
less than that of level N, in respect to M1V,V levels. The authors thank V. Ye.
La5hkarev and Ye. G. Miselyuk for the specimens made available. Mere are 2
tables and 2 figures.
Card P_/2

s/84q/6P_/coo/oo0/0O5/016
A006/A101
AUTHORS. Korsunskiy, M. I., Genkin, Ya. Ye.
TITLE.: L-scries of niobium in different compounds
SOURCE. Vysokotemperaturnyye metallokeramicheski~e materialy. Inst. metallo-
ker. i spets. spl. AN UkrSSR. Kiev, Izd-vo AN Ukr.SSR, 1,062, 36
39
TFZ(T: Information is presented on preliminary results obtained by the in-
vestigation of L-spectra of'niobium in compounds of Nb with nitrogen (6.32; 6.8;
8,1; 10.2; 11.9; 12.6% N), silicon, and hydrogen. These investigations con-
t1nuc fitudlo-a proriontod by ri. Pnuling at a nominar In 1960, dealing with L-spec-
tra of niobium in its nitride, carbide and diboride. The present studien are
being conducted by the department of general and experimental physics in coopera-
tion with the Institute of Sinters and Special Alloys of AS UkrSSR. The Lp2 line
was selected as a comparison line. The exposure was selected in such a manner
that the Nb LP lines in the investigated compound and In pure Nb had the same
intensity. L R2 and L72 emission bands undergo strong changes in shape during
Card 1/2

s/84q/6P_/ooG/ooo/oo5/o16
L-series of niobium in different compounds A006/A101
the transition to Nb compounds with nitrogen and to various concentrates. These
changes indicate a considerable difference in the nature of bond of the sub-
stances investigated. The spectra obtained can be divided into two groups.
Group one includes spectra of Nb in combinati,n with nitrogen at 6.32, 6.8 and
12.6% N concentration; spectra of Nb In combination with Nb 5P13 and spectra of
previously investigated compounds NbN, NbB2 and NbC. In these spectra the La 2
band is not displaced and its shape changes in that the outline of the compound
band remains within the contour of the LR, band of pure Nb. The atomic charge
does not change substantially. The second group includes emission spectra of
substances whose L32 bands are displaced and do not remain within the contour of
L,111 bands of pure Nb, i.e. the band occupied by valent electrons is displaced to-
12
ward the side of lesser energies, and expands. Such spectra are shown by Nb-
nitrides with weight concentrations of 8.1; 10.2; 11.9% N and a Nb-hydride
specimen. In these compounds a partial transition of electrons takes place from
hydrogen to Nb (in Nb hydrides) and from nitrogen to Nb (in compounds with ni-
trogen). There are 2 figures and 1 table.
Card ?_/2

S/18 62/004/010/060/063
BI 02XB1 04
AUTHORS: Korsunskiyj M. 1.9 Genking Ya. Yeof,and Lukashenkog L. I.
TITt's ill M L II iSsjF i6i eEjes o ni
PERIODICAL: Fizika tverdogo tela, Y. 4f no. 10, 1962, 2986 2967
TEXTs The wavelengths of the L and L edges of the emission spectrum
of me.tallic. 1 N >116 --(5223.5�0.2)X and X ('5022.91 0-3)X,
L
should agree with the corresponding absorption edges. Since no data are
available for the Lii absorption edge, and since for L III the only
published value'is 52i2.1 X which disagrees with the corresponding
value from the emission spectra, the,zkboorption edge wavelengths were
measured-again.'---The authors used an X-ray spectrograph with a quartz
analyzer (do, = 3336.00 X, R 700 mm).- The results w,eres
(5223.6to-4) X and XL (5022.8�0.6) X.
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3/l8lj62/004/010/060/063
The L III and Lli absorption... B102/B1.04
ASSOCIATIONs Kharlkovskiy politekhnicheskiy.imtitut im. V. I. Lenina
(Kharl.kov Polytechnic Institute imeni V. I. Lenin)
SUBIAITTEDs June 18, 1962
Card 2/2 Y

- ZASHIVARA, V.V.; KMSUNBKIYP ML
Electrootatic analywr vith a linearly diatribated potential
on deflecting electrodes. Zhuretekhefiz, 32 no,7t840-847
JI 162. (MM 15:8)
1. KharIkovakiy politekhniebookiy institut.
(Electric apparatus and appliances)

KCRSUNSKIY, M.I.; GENKIN, Ya.Ye.; VERKHOGLYADOVA, T.S.
Corrected LB2 niobium emission band and bonding forces in the
system niobium - notrogen. Porosh.met. 2 no-4:35-38 Jl-Ag 162.
04IRA 15:8)
1. Kharlkovskiy politekhaicheskiy institut imni V.I.Lenina. i
Itlititut metallokeramild i spetsialin;ykh splavov AN UkrSSR.
(1-ray spectroscopy) (Crystal lattices)

Yj-
S/139/62/000/006/023/032
E039/E435 1/7
AUTHORS: KorsunskiY,_kf__I., Reznik, M.B., Trutent, R.M.
TITLE: Possible method of measuring.the concentration of-ions
formed by hydroionization
PERIODICAL: Izvestiya vysshikh u~chebnykh zav'edeniy. Fizika, no.6,
1962, 152-156
TEXT: A stream of ions is itLj.ected with a.velocity u inside a
'.metallic cylinder to which they transfer their charge and chanige
the potential v of the cylinder. The rate of change of v is
determined by means of an electrometq)r.- A simple method is
developed for determining the mass spectrum of heavy negative ions
and the total quantity of light ions in the flow from a hydro-
ionizer of the Mikulin ty 0. It is shown that there are negative
ions with masses from IOM to 10-14 g on unit charge and that the
mass spectrum is linear overthis range. A method is also
-'developed for-determining the ratio of the numbers of positive and
-negative charges Z = N+IN- from the limitihg value of the
potential curve and the mass spectrum, and verified by measurements
on the rate of discharge of'a metal sphere (10 cm dia) when placed
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S/139/62/000/oo6/023/032
Possible method of measuring E039/E435
in the stream of ions. A, comparison of the.rates of discharge of
the sphere when charged positively and negatively gives a value of
the ratio Z which agrees-to within 109'a' of the value obtained from
the mass spectrum. There are 5 figures.
ASSOCIATION:- Kharlkovskiy pQlitelchnicheskiy i'nstitut imeni
V.I.Lenina (Kba,rlkov Polytechnic Institute imeni
V.I.Lenin)
SUBMITTED: June 7, 1961
IX
Card 2/2

KORSUNSKIY,, 14.1.; GRECHKO, Ye.A.; L" A.I.
M"
Dependence of the relaxation tide of the
anomalous
photoconductivity of selenium on the wavelength, and the
eleatron-bonding energy in long-lived traps. Izv. AN
Kazakh. SSR. Ser. fiz.-mat. nauk no. 2tl4-18 163.
(MRA 17:6)

KORSUNSKIYI M.I.
Nature of the anomalous photoconductivity of amorphous
selenium. Izv. AN Kazakh. S.I.W. Ser. fiz.-mat. nauk no. 2:01-39
163. (MIRA 17:6)

KORSTJNSKIY, M.I.; GENKIN, Ya.Ye.
Change in the character of the bonding forces in the system
niobium - nitrogen. Izv. AN Kazakh. SSR. Ser. fiz.-mat.
nauk no. 2:70-75 163. (WRA l7t6)

45346
$/1s 63/005/002/028/051
B104Y3102
AUTHORS: and Postushuk*.N. 9.
TITLE:
Adhesion. levels in amorphous selenium doped with mercury,
PERIODICAL: Fizika tvordogo tel.ao v- 59 no. 1963* 559-563
TEXT: The kinetics of the phot 6conductivity of amorphous selenium with
Hg impurities was studied, in the- ranges 360 - 460 mo and 600 - 720 ap at
different light intensities and temperatures. The photoconductivity-
relaxation curves were found'.to be S-shaped (FTTt 3, es 1961:1 2,~30 1960), :
like the relaxation curves of: the monopolar'photoopnduotivity in CdS
single crystals observed by Ryvkin and Paritskiy. This proves -the
existence of adhesion levels with 0,37 ev in amorphous' selenium. Some
parameters of the semiconductor were estimated from the B-curve
by a
method suggested by Paritskiy and.Ryvkin. The adhesion level concen.;
tration is 2,1013 am -3. 'The 4u&ntum yield between 360'anA 460'mp is
-2
2,10 and th carrier lifetime it, MOM seaq and between 600 and
5
720 mV it is or
:.5-10- and >0.31 sea, respectively., The effective carri
card J /2
Card 212

R~~kU,,,Xjq LAGUNOVj, A.S.; BAYVE-LIj L.P.
Using induction transducers in measuring displacements at high
tenperatures. Izm. tekh. no.8sl6-19 Ag 163. (MIRA 16:10)

/048/63/0,'!7/003/0'11'/025
B117/B234
'ORSs
UTh Korsunskiyj X I.,#. and Genking Ya. Ya
A
TITLE; X-ray spectra of niobiumAn the M-phaae range of the
niobium-o gen system,-
Xy
SSSR--- I ------ --tV --Seriya-_fiziche9kaywj---
PERIODICAL Ives Y&O
V. 27 no .3t.4963 v'- 362:-_30
TEM Fluorescence spectra.were taken of.niobium In compounds havihg
ifferent concentratio en~(0.27#- 0-45, 0-51~ by weight) and the
d na of nitrog
in the, 0(-phass range were examined. It was s own
emission liands of LP h
the Fermi bound
that the ohort.,wave- part.-of-the. band.direc.tly, adjoining ary
remains praotically. unchingedl. pointing to. the. conclusion. that the- number I
f colleotive electrons - remains ..constant or scarcely alters. The.spectral. i
0
intensity of,the.long-iveve-m&ximum,increases.. Its width slightly'decreasespi
-the bound valency electrons# but. the increased
Indicating-a. longer.life of.
spectral intensity.can.beiaseribed.only 0 a change in the symmetry of the
function of the boundvalanoy electrons; i.e.' the symmetry of their wave
Ca d 1/2

-- ---- S/00J63/027/003/019/025
BI 06/U38
'AUTHORS: Korsunakiy, Lukashenko, L. 1.
TITLE: Optimum excitation conditions for X-ray spectra in the.
0
5 - 10 A.range
PERIODICAL; Akademiya nauk SSSR., Izvestiya. Seriya fizicheakaya, v. 27#-
no..3, 19631 409-4114:
TEXT: The.optimum excitation conditions for soft X-rays with wavelengths
of 10 2. were calculated.. The electrons in the anode housing were
assumed to propagate in straight lines. The probability of continuous
radiation at a frequency I/ when the electrons are slowed down was,
calculated with Kramer's formulap and-the energy losses of the electrons
determined with Widdington.'s- formul a. Results. 1) The condition
E /EVV , where Eo is the energy of the absorption edge and E,, the-,
0
energy corresponding to~the frequency vo is fulfilled when fluorescent
radiation is excited by a continuous spectrum or when absorption spectra
are studied employing non-photographio recording of the X-rays. In this
case, an element furnishing.the greatest possible radiation intensity in
Gard, .1/4

~MA
S10481631027100310191025
Optimum excitation conditions:for X-ray ... Blo6/B238
---- -- -be of-high Z -and - must'_
the 5 --10j range is recommended. The element must
lie at the *.Dase of a rising partof the curve pM/f'Z - f(Z),.where pis the'
linear absorption coeftiaient of the anode material for a radiation with
frequenoy 1) # M the atomio weight of the anode material, and (/ the denaily -
of the anode material. The.voltage on the tube corresponding to thin
element is,read off from Fig._1. 2) The element for the anode must be
chosen ir~ s-ach a way that the wavelength of the line of maximum intensity
in the exciting series is a little shorter than that of the absorption.
edge of the series con,taining,the line to be excited. Here again, the
voltage is read off from Fig. 1. 3) When the investigation of the
absorption spectrum features photographic recording of the X-rays# in which
case B Ik 0 in the visible spectrum. It is also shown that in the short wave region,
Card 1/2

L 06137-61'
ACC NR: AP6031174
'
do.. should become zero and change sign. The hypothesis that the long-lived trapping
ter is a colloidal particle dispersed in amorphous selenium is advanced. Orig. art.
19 formulas, 4 figures.
CODE: 20/ SUBM DATE: G7May65/ ORIG REF: 006,

.4T_
ACC;Nft: AP6003808 SOURCE CODE: UR/0181/66/068/001
AUTHOR. Korsunski F-ridman, V. H,
ORG: institute of"..Nuclear Ph sics, AN KazSSR, Alma-Ata (Institut yadernoy fizikl
AN Kaiif�~)-.
TITLE: on some properties of a high-voltage photoelectric effect in thin CdTe layers
SOURCE: Fizika tverdogo tela, v. 8, no. 1, 1966, 263-264
TOPIC TAGS: photoelectric effect, photoelectromative force, photoelectric cell,
cadmium telluride
ABSTRAC7~ An investigation was made of the high-voltage photoelectric effect in
cadmium'telluridd'Ithin layers.,4 Two methods were used to measure the capacity C of
the layers: 1) The.quantity of electricity Q in a specimen was determined by charg-
ing- id
h'
ballistic galvanometer calibrated withp the aid of a normal solenoid. The ratio
Q/V Ph represented the capacity C. 2) A known capacity C 0(electrostatic voltmeter)
was connected to a layer charged to a potential Vph. The potential difference V was
then measured. C was calculated from the relationship V(C + CO) = V C. Thi6 values
obtained by both methods coincided. The C of the specimens appeared0o be of the
order of 10 cm, thus considerably exceeding the capacity expected on the basis of '
geometrical conditions. The-large capacity of CdTe layers indicates that these
Card 1/2
Card 2/2

M 9 1 W M ft IM-MR, I _100 i a
.L 06303-67 Wr (riVOWP (t)/=! WP(c) JD
ACC NR. Akd5_4~f SOURCE CODE:
I ~Pj A
AUTHOR: Volchek, A. D.; Garger, K. Korsunakiy. No I.
ORG: Institute of Nuclear Physics, AN KazSSR, Alma-Ata (Institut yadernoy fiziki
KazSSR) A
jTITLE: The lux-ampere characteristic of amorphous selenium at constant irradiation
: Fizika tverdogo tela, v. 9, no. 5, 1966, 1625-1627
TAGS: photoconductivity, selenium, spectral memory, dark conductivity, lux am-
characteristic
,STRACT: The behavior pattern of amorphous So specimens with anomalous phatocanducti-
.ty-under simultaneous irradiation by two monochromatic light sources was Investigated.
Se specimen was irradiated at a wavelength of %650 my, and with a constant irradia-
on at a wavelength of 450 my. The equations of the kinetics of dark and light condue-
,vities agree with the experimental data; the value of the dark conductivity Is a func-
,on of the light Intensity. Orig. art. Me: 2 figures, 5 formulas.
CODE: 20/ SUBN DATE: 02Dec65/ ORIG REF: 002
1 qz)~- - . --- __ __-

L 21711-66 EWT(1)
ACC NR, AP6004888 SOURCE CODE:
UR/0057/66/036/001/0132/0138
IAUMIOR: Zashkvara,V.V.; Korsunskly,K.I.; Kosmachev, O.S.
OW: none e-
TITIZ: Focusing characteristics of an electrostatic mirror with a cylindrical f told
SOURCE: Zhurnal tekhnicheskoy f Iziki, v. 36, no. 1, 1966, 132-138
TOPIC TAM electron optics, mass spectrometry, electrostatic field , elective
potential, charged larticle, ion energy
ABSTRACT: The authors discuss focusing of charged particles by the electrostatic fielc
between two coaxial cylindrical electrodes. The ions are assumed to originate In a
point source on the common axis of the electrodes and to enter and leave the Inter-
electrode region through circular slots in the inner electrode. Charged partl *clog wit]
a certain energy. dcipending on their charge and mass, the potential difference between
the electrodes, the radii of the electrodes, the distance between the slots In the
inner electrode, an& the position of the source, will be brought to a focus an the axii
It is proposed to employ such a system of electrodes to record the energy spectrum of
charged particles by keeping fixed the positions of the source and detector and vary1M
the potential an the electrodes. The focusing conditions are derived. It Is shown
that not only first order, but also second order focusing occurs If the angle between
the initial trajectory and the axis is 420 200. The authors also calculated the as
1/2
UDCt 537.533.3

- L 21711-66
-~Rf - -AP6004,888
.order aberrations and the effect of finite source size, but in the present paper they
only discuss the results and do not present the calculations. The energy resolution
can be improved by employing multiple focusing with suitable irises In the Intermedlat
image planes to eliminate oblique trajectories. The linear dispersion in energy of
the cylindrical capacitor is approximately equal to that of a 1800 spherical analyzer
of equal size. The quality of'focusing is adequate for analysis of Lon beams with an
angular divergence of 360o In the radial plane and several degrees In the axial plans.
Orig. art. has: 17 formulas, 2 figures. and I table.
SUB MR.- 20/ SUM DATE: Q3Uay65/ ORIG REF: 002 OM RV: 000
Card Z/ZFDL-

L 28083-66 - EWT1'm)/FTC(_f)A
V?G(M)/EWP(t)/ETI XJP(c) RDIN/M
ACC NRI AP6015609 SOURCE CODE: UR/0020/66/1681002/0318/0319
X)
AUTHOR; 'Korsunskiv. M. 1. (Academician AN KazSSR); Fridman, V. M.
ORG: Institute of Nuclear Physics, Academy of Sciences Ka9SSR (Institut yadernoy
fizi~i Akademii nauk KazSSR)
TITLE; Pectral distribution of the high voltage photoelectric effect i n CdTe thin
films 77
SOURCE: AN SSSR. Doklady, v. 168, no, 2, 19660 318-319
TOPIC TAGS: photoelectric effect, photo-emfheat effect, cadmium telluride
ABSTRACT: An investigation was made of the effect of the substrate temperature
during the deposition of a CdTe thin film on the spectral distribution of the short-
circuit current. It was found that with substrate temperatures higher than 310C, no
sign inversion occurs when the incident light wavelength is varied in the range of
450-900 mp. At substrate temperatures of 250-300C, the sign reverses when the
wavelength is shortened; with decreasing temperatures, the inversion can be obtained
at increasing wavelengths. The above results are compared with those of
Adirovich (E. I. Adirovich, V. M. Rubinov, and Yu. M. Yuabov. Izv. All UzSSR, ser.
fiz-matem., no. 6, 63, 1964), who obtained sign inversion by changing the angle of
the deposition of the molecular beam. In order to establish whether it iz the sub-
strate temperature or the oblique deposition that is primarily responsible for the
I Card 1/2 UDC: 539.293

~ I- -
3-,;~tra cof
eq ~-nterftOmlc ly-r, Df
10 i 1701-a709 E
Wt. yar.18.rnok- fZAL AN Klis*S~Rv
July 5j, 1965,,

T~ 0034 5-66 61-1T(11 ~b)
~-T W-7J-G . ..... ... --
ACCESSION 1111: P5019224 UR100 /65/049/001 /0124/9126
5
-Jk !,~, > -44T 1
AUTHOR: Ki*koin, L Ks; Senchenkove A.-F.1 Gel'man* -r. V,.,; Korsunskiy, M. M.;
Naurzakov; 51 Fe
TITLE: Electric conduElkilt
X and density of metallic vaps-r
SOURCE; Zhurnal eksperimentallnoy I teoreticheskoy fiziki, Y. 49, no. 1, 19656
TOPIC TAGS: mercury, electric conductivityt pressure effect, temperature dependence
high temperature research
ABSTRACT: The article describes an investigation of th e electric conduct~tv
~IL of
~Imercurv in the transcritical range of temperatures and pr-essurea. The experiments
Ve-recarried out in a chamber in -which pressures up to hOOO stm could be establish-~
ed by means of gaseouo argon compressed with a thermal compressor. The mercury Vas
contained In a capillary whose mid-section could be heated electrically to 2000C" 1~1
The transcritical conditions were established only in 'the middle part of the capil-
lary, The mercury was activated In a reactor before the experimentag and its den-
'aity was determined by measuring the y radiation from the Hg203. The measured
.quantities were automatically recorded with multichannel automatic plotters The
Cord 1/2

00345-&
ArCESSION HH: AP5019224
faniily of curves platted at different pressures made it possible to deterndne the
Ivelectrical equation of state" r = f(p, T) and the thermodynamic equation. for the
density p = ~(P, T) Jr - resistivity, P = density, T = temperature, P = pressure).
The critical temperature of mercury was found to be 1450 t 50C. The.meas .urement
accuracy was insufficient to determine the temperature coefficient of resistivity,
but it was found to be negative at densities below 7-8 g/cm3 and close to zero at
higher density. A more detailed description of the results and of the experiments
will be published elsewhere,..Orig. art* hast 2 figures;-
ASSOCIATION: None
SUBMITTED: igFeb65 ENCLI, 00 SUB CODEz 3M# TD
NO REF SOV: 001 OTHERt 003
Card

PQ z, Lk- /,j - e,
Y)
FUN I BOOK ZXPLOrrATION s(YV/4054
Akademiya, nwyk SSSR. Institut nauchnoy Informatsil
Rhimicheskaya promyshlennost' SSSR (The Chemical Industry of the USSR)
Moscow,, Gookhimizdat, 1959. 457 P. Errata slip inserted. 4,100 copies
printed.
Sponsoring Agency: USSR. Gosudarstvennyy nauchno-tekhnicheskiy komitet.
Ed.: R. S. Romm; Tech. Ed.: P. V. Pbgudkin; Editorial Boardt A. P. Vinogradov,
S. I. Vollfkovich, N. M. Zhavoronkov, M. 1. Ivaaov, V. S. Kiselev, I. A.
Lunach&rskaya (Scientific Secretary), S. S. Nedvedev, B. D. Mellnik" A. N.
PI-ovskiy, A. Ya. Fombenko (Chief Ed.), and A. V. Topchiyev.
PURPOSE: This book is intended for the personnel of the chemical industry. It
will be of interest to the Seneral reader interested in the development and
structure of the Soviet chemical industry.
card 1/6

The Chemical Industry of the USSR SOV/4054
COVERAGE: This book contains 18 articles on various aspects of the Soviet
chemical industry. Among the developments in the production of raw materials
for the manufteture of chemical products discussed are: 1) the use of rev
materials synthesized from natural gas and petroletm'to roplace food products
in the production of synthetic rubber, alcohol.. detergents, etc.; 2) the
production of acetylene from natural and petroleum gases for the synthesis
of vinyl chlorides scrilonitrile, chloroprene, trichloroprenes 1, 4-butiedienes
and other organic substances., based on methods developed by M. G. Kucl2erov,
A.Ye. Favorskiy aad others; 3) the production of acetylene from saturated
hydrocarbons by cracking methane (and its homologs) at 1450* in an electric
are between two special electrodes in a gas reactor, by pyrolysis (thermal
oxidation) of methane in an improved-'f~xrnace designed by B. S. Grinenko, by
high-temperature pyrolysis of propane and butane in tubular furnscess or by
other methods of producing acetylene for the production of synthetic rubber,
ethyl alcohol, and other organic substances; 4) the synthesis of halogen deriv-
atives of aliphatic hydrocarbons for the production of solvents, refrig-
erants, pharmaceutical products, etc., and 5) the production of rubber ac-
celers.tors from nitrogen-containing aliphatic hydrocarbons. The history of
plastics production in the Soviet Union is reviewed, and n a, locations,
and products of plants as well as the names of outstanding personalities in
the field axe given. The technical level and prospects of further develop-
ment of different branches of the plastics industries are also discussed
Card 2/6

The Chemical Industr7 of the USM SOV/4054
along with methods of manufteturing plastic articles. A special ap-
paratus designed by Ye. M. Mogilevskly and designated "VA" which permits
preparation of viscose solution in one operation is discussed. It is being
used to replace the complex, conventional equipment with great savings in
space. General trends in the technology, of synthetic fiber production am
also discussed. A historical review of synthetic rubber production and
the achievements of outstanding Soviet scientists in this field am given as
well as names, locations and products of synthetic rubber plants. Rubber
production and the manufacture of rubber goods am similarly reviewed.
Statistical data and outstanding personalities in the development of the
aniline dyes, paints and lacquers,: mineral fertilizers, insecticides and
fungicides, sulfuric acid, sods, mineral oLlts,, radioactive and stable
isotopes, and chemical reagents industries am given. Catalytic processes
and automation and automatic devices used in the chemical industry, axe
also discussed. Thirty-eight photographs included in the book show outside
and interior views of some Soviet chemical industry plants, as weU as
their manufacturing, material-handling and laboratory equipment. N=arous
personalities ead facilities axe identified in the body of the text.
References accompany individual articles.
Mut 3/6

The Chemical Industry of the USSR SOV/4054
TAMX OF COMMS:
Introduction 3
Prsun#4&y. O._V._, N.A. Dalln. A.N. Flianovskly., and R. I. Chernyy. The Basic
-Org-wic Synthesis Industry 11
Garber, M. 1. 2he Mastics and Synthetle Resins Industry 75
Birger, G.Ye.,, and A.A. NDnkin. The Chemical Fibers Industry 132
Zakharchenkop P.I. The Synthetic ftbber Industry 13T
Suslyakov, A.V. The Resin Industry 166
Korolev,, A.I. 7he Aniline D~e Industry 197
Belovitakly, A.A. 7he Pftduction of Lacquers and Faints 219
Kel'Aikov, N.N. Chemical Means of Protecting Plants and Eliminating
Weeds 234
Card 4/6

The Chemical Industry of the USSR Sav/4054
Boreskov, G.K., and V.S. Chesal v&. Catalytic Processes in the Chemical
Industry 4W
Yelahqn, N.N., an& NAL. AM. Aitt6mti6n 6P +Jm Oh&ade&1 TA&wtAea 439
AVkUAMZ: Library of Congress
Card 6/6
JA/dwm/f&l
9-16-6o

Koltsumay, 0. V.
Publication of new books on the technology of basic organic
synthesis. KhImprom. no.8.718-720 D 159.. (M14 13 -.6)
(Ghemistry,.Orsanio-Syntheels)

KOMNSKir
Indumtz7 of basic organic synthesis In lwland. Xhim.
prom. no.42-343-348 Jo 160, --7kIRA 13:6)
(Great Britain-Chomistr7,' Organio-Synthesis)

KORSUNSKIYP O.Ve
Some problem involved in the developwnt of the fundazental organic
entbesio industry In capitalist countriese Xhimeproa* no*643~443
is 61. (IMA 14:6)
(Chadstry, *rpaie-synthssis)

PAVLOVY Boris Alekseyevich; TERMIYEV, Aleksandr Petrovich.,
. j9 Y., RUYHADT--',
prof. Prinimal uchastiye-XOB=
Ye.G.; ZITSER, A.I., red.
[Course in organic chemistry] Kura orgar4-heskoi khimii.
Izd.5., perer. Moskvap Khimiia, 1965. 686 p.
(MIRA 18:5)
1. Chlen-korrespondent All SSSR (for Terentlyev).

I - rwgaiq~-
4~~; r 6 ~- -1 /4/ 01- 1 - j 5-, - (9 -
ICBSUNSKIT, B.G. - yj
-.0-- nub
Acoustical study of the vibrato in artistic voices. Probl.fiziol.
akust. 1:i5g-165 149. (KIRA 10: 11)
1. Akusticheakaya laboratoriya Moskovskoy konservatorii.
(VIBRATO) (SINGING) (NUSIC--ACOUSTICS AND PHYSICS)

9DRSUNBUT, B.G.
atieml study of the loudness of n singer's voice. Probl.fiziol.
akust. 2:153-160 150 (KIRA 10:11)
1. Xomisaiya po fitiologichookoy akuatike pri Otdelenti biologicheskikh
nauk AN SSSR, Moskva.
(SINGING) ;(,!MUSIC--AC(XJSTICS AND PHYSICS)

IMEMKIY, S G."',
Iffect of the spectrum of the perceived sound on its pitch.
Probl.fiziol.skust. 2:161-165 '50 ~KIRA 10:11)
1. Komiesiya po fisiologicheakoy akustike pri Otdelenil blologicheskikh
nauk AN SSSR. Moskva.
(HWniG) (MUSICAL PITCH)

- tnisig 1%,3 GrjApnvljU&ph; SIXOTOV, Igor' Dmitriyovich; GIN9BURG, Z.B.0
redaktor; fultumll, X.P., tokhnichookly rodaktor.
[Illectric musical instruments] Slektromusykallny* Instrumenty.
Kooky&, Goo.onerg.1si-ve. 1957. 63 P. (Massovais radiobibliotob%,
no.271) (NIRA 10:11)
(11;~Rjcal Instruments, Blectric)

P a
I i
ii q.11
.4U Ck
A 4j3f
2U
9 Is
3 a g -0 ,
ills

KUKHTIYO F.1 VINOKUROV, A.9 mkbmd Ag~UNSKIY, v.
Renovation of the M-14W-trench digger. Prom.stroi.i inzh.
soor. 4 no.5s54 Sa-O 162. (MIRk 16:1)
1. Nachallnik preisvodetymmo-tekhnicheskogo otdeleniya
Nikopollskogo gidromtroys (for Kukhtiy). 2. Starshly
proisvoditell rabot proizvodstvenno-tekhniches~ogo otdeleniya
Nikopollskogo gidrostroya (for Korsunskly),
(Excavating mchinery)

93-5-12/19
AVTHORS-, _JJgXj3MskiZj__V, B., Upachev, V. V., Mazur, A. A.)
Chief 2r*1-ne_e_-r-s7ff the Refineries Under Construction
TITIE: Over-all Designing of Refineries (Za komplekanoye
proyektirovardye neftepererabat5wayushchikh zavodov)
Organization of Refinery Designing (Ob organizatsii.
proyektirovaniya neftepererabatyvayushchikh zavodov)
PERIODICAL: Neftyanoye Khozyaystvo, 1957, Nr 5, pp. 47-51 (USSR)
ABSTRACT: The planned expansion and construction of large refineries
in the Soviet Union calls for a great deal of work on
the part of designing engineers. This work is useless
unless it Is properly and efficiently organized.
The Minister of the Petroleum Industry of the USSR,
M. A. Yevseyenko, raised this question at the 20-th
Congress of the Communist Party of the USSR, but so far
no measures have been taken to improve designing.
Three shortoomingt in designing refineries and petro-
chemical plants are discussed, namely: 1) the separation
of individual designing organizations from the projects
Card 1/6' designed by them; 2) the distribution and separation of

Over-all Designing of Refineries (Cont.)
93-5-12/19
designing organizations from each other; 3) a large number of
designing organizations designing the same plants. The follow-
ing organizationq are now engaged in designing new refineries:
Gipronef tezavod (State Institute for the Design and Planning of
Oil Refinerle~), Giproazneft' (State Institute for the Design
and Planning of the Azerbaydzhan Petroleum Industry), Lengl-
progaz (Leningrad State Institute for the Design and Planning
of Synthetic Liquid Fuel and Gas Plants),-Giprogrozneft' (State
Institute for the Design and Planning of the Groznyy Petroleum
Industry), and branch offices of the Giproneftezavod and
lengiprogaz. From time to time, the plants are located at a
distance of several thousand kilometers from the designing organ-
ization. For example, the Molotovskiy Refinery is designed in
Leningrad, the Yaroslavl' Refinery by the Rostov-on-Don branch
office of the Giproneftezavod, and the designing of the Fergana,
Irkutsk and certain other refineries is done in Baku. Designing
of individual refinery installations and units is often done on
a subcontract basis by special designing organizations belonging
to other ministries. The designing work could be done by the
main designing organization, which would avail itself of the
Card 2/5

Ove~r-all Designing of Refineries (Cont.)
93-5-.12/19
aervices of specialists on a consultative ba3lz. An a result there
are sometimes ten or even more organizations designing the same
plant. Such an arrangement reoultB in voliuaes of unnecessary
correspondence, dealing with the changes in the designing schedule.
It takes weeks and sometimes even months to solve problems which
ordinarily should be solved within an hour. Chief engineers in
charge of refinery designing visit the construction site once or
twice a year, while directors and heads of other sections of the
designing institute visit those plants even less frequently.
As a rule, the engineers never see the units designed by them.
Blueprints are frequently prepared too late or prematurely. There
is a lack of coordination among various spec W ized construction
crews. Isolation and separation of general designing organizations
frequently upset the over-all designing schedule, cause duplication
of work and lead to ignorance on the part of one institute of what
other institutes are doing. In designing the Stalingrad Refinery
it was discovered that a cinder dump had been superimposed over
industrial-waste treating plants and the industrial-waste treat-
ing plant over a trtu* pipeline. This situation had to be
Card 3/ 5
Over-all Designing of Refineries (Cont.)
93-5-12/19
remedied without the participation of the general designer, i.e.
Giproazneft', while the cinder dump was designed by ROTER, the
treating plant by RO Vodokanalproyekt and the pipeline by
Giprotransneft,. A somewhat similar situation occurred in
connection with the laying 01' a pipeline (Lengiprotransneft,)
over a dike, designed by the Kharlkov Promtransproyekt Institute
across the Tatlyanka Arm. Mie dike was constructed before the
plans for the pipeline arrived and consequently it had to be out
~-,o a depth of one meter and ilLfter the pipeline had been laid it
had to be backfilled. These examples show the harmful effects
of the multiplicity of desig:aing organizations, their isolation from
each other and from the construction projects on the course
and speed of the construction of refineries. This situation
can be remedied, first Of all, by having all the designing done
in one institute of designing, for example, in Giproneftezavod.
This institute should have specialists representing the allied
fields.and all the bibliographic material and archives dealing
with the construction of refineries should be transferred there.
The institute should be made responsible for the selection of
refinery sites, development of general plants, designing problems
Card 4/5

BUROVOY, I.A.; KOi~-;UNAiyp V.I.
I*thod for the removal of large settling particles from aPFaratus
witli a fluidized bed. Khim.prom. 41 no.6-453-455 JO '65- (MIRA 18:8)

I
kRICHEVSKIY, G.Ya.; KORSUNSKIY, V.1,; DENISOVA, I.A.
Waste heat utilization in the roasting of granulated copper-
zinc charge mixtures in a fluidized bad. TSvet. met. 36 no.10:
1 35-40 0 163. (MM 16:12)

~ORSUNSKIY. V.I.; KRICHEVSKlYt G.Ya.
Nomogram for calculating heat conditions of furnaces for the
roasting in a fluidized bed of copper-zinc concentrates and
charge mixtures. TSvet. met. 38 no.8:38-42 Ag 165.
(MM 18:9)

KRIG!fEV.`kIY., G.Ya.;,KOk--,1'JgSKFY, if.].
Experimental determining of the cc-eflf'--' ciun!, (-T ilea', Iransfer in
rurnaces with a fluidized bod for Oia cX sulf'-J"I-
matorials. Rhin.prom. 41 no.6,.4j.J--I/-) Je 11'5.
J- -4-+- 1
( tc. Rt. 18 -. 8 )

C2 IX
AUTHORS:
TITLE:
PERIODICAL:
82553
8/181 60/002/007/035/042
B yBo6o
Korsunskijr. V. M., Lisitsa, M. P.
I
--In-f-r-ar-e-d--A-bo-o-rpt~ionknd Hole Band Structure of Tellurium
Fizika tvardogo'tela, 1960, Vol. 2, No. 7, PP. 1619-1623
TEXT: L.' I. Korovin and Yu. A. Firsov suggested the use of data on infra-
red absorption for clarifying some partioulars concerning the valency son@
structure of tellurium. Their group-theoretical investigations revealed
that two variants are relevant for the form of the energy spectrum of the
hole band: one ellipsoid in the center of the Brillouln zone or two 0l
lipsoids in the C-direotion. k decision can be made when the form of t;8
band, which is established by the type of isoenergetic planes is known.
To determine such a form was the main task confronting the investigations.
In the course of them, the authors examined the edge of characteristic
absorption for two directions of the light vector and background absorp-
tion. The test pieces used for the purpose were made of tellurium single
crystals, that had been produced at the Leningradskiy inatitut poluprovod-
nikov (Leningrad Institute of Semiconductors).-Foile were cut in parallel
Card 1/4

82553
Infrared Absorption and Role Band Structure of S/181/60/002/007/035/042
Tellurium B0061BO60
to the C-axis, then ground and polished. As a consequence of such treat-
ment, differently oriented miorocrystals fozmed on the surface of the test
pieces, so that the reflection coefficients of the latter were practically
the same for both polarizations (Ell 0, E_LC) in the wholo spectral range.
The experimental' error in the determination of the reflection coefficient
did not exceed 5~- On taking account of all other factors, the total error
was found to be Ak/k - 15%- In Fig- 1, the tranamissivity and reflectivi-
ty curves are shown for natural and polarized light for two specimens
(Specimen 1: 0-83 mm thick, impurity concentration = jol4cm-3, Specimen 2:
0.37 mm thick, impurity concentration c4-1016 - 1017CM-3). Only the curves V(
D and DU (penetrability in the ordinary or in the ENC-polarized light,
respectively, for Specimen 1) exhibit a minimum at X - 11 p. By making use
of these data and results from Ref. 7, the authors calculated the absorp-
tion curves for polarized light; they are shown in Fig. 2. The position
of the absorption edge was then determined from the point of inflection
(let line of the table) and by means of the extrapolation of the linear
part of the curve to the point of intersection with the abscissa (2nd line).
Card 2/4

82553
Infrared Absorption and Role land Struc ture of S/181/60/002/007/035/042
Tellurium B006/BO60
The results are:
"it 0m h9l, ev VL cm hV,. ev
2600 0.39 26oo 0,32
2530 0-315 2470 0.308
The thermal width of the forbidden band was found to be 0.33 + 0.01 ev.
Some problems concerning the structureless background borderi7ng with
the characteristic absorption edge and extending far into the longwave
region, are discussed next. It appears certain that it is closely
related to the free carriers* That the absorption coefficient in the
background is dependent on polarization, is explained by the dependence
of the effective carrier mass on the direction, The'main issue is then
first disousetidg namely, the hole absorption band shape in the region
A - 11 Pi It is shown in F19, 3. The three possible functions (4), (5),
and (6) or k(Y), based-on the one- or the two-ellipsoid modelp are
written down. A number of experimental results admits only (5) and
(6) for selection, and the fact that the absorption band is symmetrical
Card 3/4

BDq Pr-4 R f W.
L 191 165-63 .--_'_E _(c
ACCESSIGI HR: AT3002M5 S12%V63100,10WIM
iAUTHORS,. Korstmakly. V. 9 Faydy*shp A. N.
Lumineeicence and excitation energy.
TITLE transter 16 anthracene crystals
SOURCE: Optilat i spek-troakoo-ye; sbornik state~r. v. It. Lyuminestsentariya. Moselm!
~-vo
R.. 1963p 119-127
TOPIC TAGS: absorption, luidneacence, piciton, orgenic,crystal,
ABSTRACT: A thorough, analysievas made of th~ absorption and I neseence spebtra;~
of. pure anthracene, crystals 40 antbrac r
one mixed with 7.9 x.20- 1 3.9 x .20-5 and
=341zol naphthacene in a t
7 8 x'10 emperature range 300-90K. From the data
gathered calculations Were mnde to deterattne the probability of excitation Wargy
trensfer and the diffusion length of exciton displacement using a phenomenological
..argument-and the microscopic theory.of M.'Trillfaj (Chekh. Fiz. Zh.t 81, 510,, 1958)f
These calculations indicate that the dip -dipole resonance theory of excitation
ple
cnergy transfer could be used in studying energy transfer pr6cesses.in organic
c~-Ystals. In the region.investigated.. the excitation energy transfer was shovn to
vary only slightly with temperc~tixre. Orig. art. has: 5 figures, 3 formulas, and
2 tables.
Lc~rd

ZIMA, V.L.; XORSU!qKl~~, V.M.; FAYDYSH, A.N.
Spectra and the -conditions for the transfer of electron excitation
enOrgy in pure and doped anthracene crystals. Izv.AN SSSR.Ser.
fi:,.', 27.mo.4,019-523 AP 163. (MIU 1624)
. (Anthracene crystals-Zpectra)

XORSUNSKIY, V.M. (Korsunslkyi, V.M.]j FAYDYSH, A.N. (Faidysh, O.M.]
Energy transfer in anthracene crystals with ad=13~~es of phenazine
and acridine. Mr. fia. zhur. 8 no.6:677-683 'Je 163.
f(KIRA 16:7)
1. Kiyevskiy gosudarstvormyy universitet in. Shevchenkol,
(Anthracene cry*Ws-Spectra) (Quantum theory)

L 10588-63 ASD Fc-h/pr-h Tyr.7
ACCESSION HR.-AP3001396
S/0020/63/150/004/0771/0774~
AUTHOR- Xorsunskiy, V. M.; Faydy*sh, A. N.
TITLEs Migration of energy of the triplet level in benz2ghenonstrystals
'~,,~OURGEt AN SSSR. Doklady, v. 160, no. 4, 1983, 771-774
TOPIC TAGS: triplet exciton, transfer tif energy, benzophanones naphthalene,
!naphthacene, phosphorsecenoe, energy, triplet level
49-STRACTs To demonstrate 'It,
_riplet exciton", the transfer of energy of the
1:triplet level frmt donor to acceptor molecule or.transfer between simil ar mole-
oules, the transfor of energy from benzophenons crystals to admixtures of naph.,
'thalene or naphthitoone was studied. Phophoreacence spectra of benzophenone with
different ooncentrations of n ane;br nj2hjhacene~are given. The triplet
l6vel of bezizophenone -was lowered -while-that -of -the dih solved naphthalene
increased. Since naphthalene does.not emit at Lambda 385 millimicrons, the
emission must be explained by.onargy trensfer from the benzophenone. In nkoh-
thacene the energy is transferred to the: first excited singlet as demonstrated
by the presence of afterglow: in the excited material (Lambda -- 436 millimicrots)
!and by the decreaiie in the duration of phosphoreseenoe in benzophenono caused by
Card 1/2

ACCESSION N.R:. AP4020313
S/0302/64/000/001/6028/0031
AUTHOR: Derkach, V. P. (Candidate of technical sciences); Zhivkova, T. P.;
Korsunskiy, V._,M.; Oreshkevich, A. 1.
TITLE: Luminescent matrix for photorecording images produced by electronic
computers
SOURCE: Avtomatika i priborostroyeniye, no. 1. 1964, 28-31
TOPIC TAGS: luminescent matrix, computer, computer output, computer output:
photorecording, EL-510 phosphor, EL-460 phosphor
ABSTRACT: Experiments with recording the output information of computers on !1
luminescent 256 x 256 -element plates ("matrices") and photographing it are
described. Each element is 0. 5 x 0. 5 mm., and the distance between elements in
0. 5 mm. A line -by-line exposure is used to ensure higher speed and contrast of
the plates coated with EL-510 (green) and EL-460 (blue) phosphors.
C.,d lj$~-

GOLUB, A.I.; KCRSUNSKIT, 're.l.; LYAM, A.Ye., spotsred.; DAMASEINA, GO.,
'T . rod,
red,,; tekhn
[Advanced operating "thods for wrapping machineal Pbriedovys
metody rdboty na* xamorty-miushchikh mashinakh. Moskva, Plshche-
promizdat,' 1956. 29 ps' (XIM 110)
(Wrapping machines)

SAIAMOV, K.P.; BERNAR, D.N.; Ye.V.
Building underground units for a continuous steel casting
plant by the open caisson method. Osn., fund. i mekh. grun.
7 no.3:18-21 165. (MIRA 18:6)

Korsuntsev., A, V.
The following isamong dissertations of the Leningrad Polytechnic
Institute imeni Kalinin,
"Current-Limiting Cutoutsp for Protecting High-Voltage Condenser
Batteries against Puncture." 22 June 1953. A procedure was developed
and verified. experimentally for calculating the protective~action (amplitude
of the pa ssing current) for a current-limiting cutout of any type which func-
tions in a Eystem of condenser batteries. The procedure of tyrdcal tests
was firmly established.
SO: M-10461, 28 Mar 56

GERTSIK, A.K., inzhener; KALININ, Te.V., kandidat tekhnicheakikh nauk-,
KORSUHTSg,. A.V., kandidat takhnichookikh mauk; HXRKHALU, S.D.
An2nener. MWAM
Reinforced insulator strings for oberhead lines. Blaktrichestvo
no-3:69-72 mr 156. (MM 9:6)
I.Nauchno-issledovatel'skly Inetitut postoyamogo toks.
(Electric insulators and Insulatioz)

It -,'I V~~.
MARCaUO. TsAo, kandotakhn.nauk; ROZOVSKIT. Yu9A., lmnd.tekhn.nsUk;
SHM, B.S.9 kmnd,tekhn.nauk; KMSUW6Wi---A.V., imnd.tekhn.rLauk,
red.; DWOT, Ye.D., red.; MWVVW. L.Ya., takhn.red.
[Series capacitors] ProdolInsim eakostusis kompenestsits linit
elektroperedschl. Moskva. Goo. energ. ird-vo, 1957. 47 p. p.
(MIRA 11:4)
1. OHO trust, Moscow.
(Condensers (Blectrteity))

KORSMITSEV., A.Y.
.. __.--__.___..._ ------ -,
Using the theory of similitude for calculating the pulse characteris-
tics of concentrated ground connections. Nauch. dokl. vys. shkoly;
enarg. no.1:217-222 '58. (MIM 11:10)
1,31auchno-iseledovatellekly institut postoyannogo toka.
(Ilectric currents-Grounding) (Dimensional analysis)

AUTHOR: Korsunt5ev~ AV 105-58-5-8/28
.L, Cand4date of Technical
iences
TITLE: The Application of the Similarity Theory for the Calculation of
the Pulse Characteristics of Punctiformly Distributed Grounds
(Primeneniye teorii podobiya k raschetu impul'sz~ft
kharakteristik sosredotochennykh z&zemllteley)
PERIODICAL: Elektriohestvo, 1958, Nr 5, PP- 31-35 (USSR)
.ABSTRACT: The impossibility of experimentally determining the natuml amount
of grounds in the case of high pulse currents caused the laws of
similarity of these processes to be studied. The development of a
method based upon the theory of similarity (Refs 8, 10, 11) formed
the subject of the problem to be solved by the Institute for Paral-
lel Current. Derivation of similarity criteria was based upon the
conce]~tion of the spark zone. The boundaries of this zone, which
is affected by the discharge in the ground, are determined by the
critical gradient of the po+.ential Ebreakdown' whereas the internal
resistance is assumed to be equal to zero. The investigations car-
riea out at the Institute %4th respect to the characteristics of
Card 1/4 ground discharges confirm the existence of ramifications of the

The Application of the Similarity Theory for the 105-58-5-8/28
.Calculation of the Pulse C haracte ris ties of RlnctifomV
Distributed Grounds
channel, of a low voltage drop in -tile channel, and of the possibil-
ity of utilizing the cono;.Ttion of a "spark zone" for purposes of
carrying out calculation;3 in practice. It vas Ibhown that the in-
fluence exercised by configuration and the position of individual
elements of the ground steadily lose its importance with increaz-
ing ourrent, and that total dimensions acquire basic importance.
The measurements of such a more or. le3s synnetric construction of
grounding are best dharacterized by the distance s between the
geometric center of the ground lead on the surface of the earth and
its most remote point. This distance is described as the oharac-
teristio dimension of grounding, and is here assumed to be a = 15 m.
The data available make it possible to disregard the inductivity
and the capacity of the electrodes (Ref 5) in the owe of such a
distance. The so.-cal.led rj-'i;heoram of the similarity theory (Ref 8)
is applied. The number of ram-ables is here restricted to 'Iwo di-
mensionless IT, and n2. The experimental curve F11 = f(FJ2) ful4
represents all complicated pro3esses actuall taking place in the
of the criterion
ground. The similarit oriteria (17) and (18
equation 09) FT1 = q~2) are deri-ed. In or-der to check the pos-
Card 2,/4 sibility of constructing the criterion cn-%rve (i9), the aataL

The Application of the Similarity Theory for the 105-58-5-8/28
Calculation of the Pulse Characteristics of Funotiformly
Distributed Grounds
available in publications (Refs 3,4,6,7) were used. In spite of
the fact that experiments were oarriea out by different authors
and under different conditions and amperages, an average curve was
obtained with sufficient accuracy, with deviations of individual
values of about 8%. This proves that the curves obtained can be
used for calculations carried out in practice. The curves consist
of two sections; a horizontal one with low values of rT2, and one
declining in the range of high rT2 values, each ground lead having
its own horizontal section. The declining sections coincide for all
ground leads. The physical significance of this development is the
following: The horizontal section of the curve for each ground lead
corresponds to the constant value of the resistance P,
u ("pulse re-
sistance" of the ground lead ) in that domain of rT values which
corresponds to low amperages. Within this domain t9ere is no spark
zone round the electrode or, if there ia, it is negligible. - With
an increase of current, and thus also with an increase of 72-
Card 3/4 values the spark zone begins to develop (salient point of the