SCIENTIFIC ABSTRACT VANYUKOV, L.G. - VANYUKOV, M.P.

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• Collection: Scientific Abstracts
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• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 9, 2001
• Sequence Number: 1
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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[Keeping bees in two-story hives] Bodershanis pchel v dvukhkorpusnykh
ulliakh. Moskva. Ministeietvo aellbkogo khoziaistva SSSR, 1956.
folder. (MLRA 10:!,)
(Bees)

BIZBORODOVA. A.; DATSIV. V.; TAII=OV, K.
Practices of apartment-house offices in taking care of children.
Zhil.-kom. khoz. 8 no.12:20-21 158. (KIRA '13:1)
1.Sekretarl Chelyabluskogo gorkoma komsomols (for Bezbor,odova).
2.Sekretarl Ufimskogo gorkoma komsomola (for, Datsiv). 3.Prodoedatell
roditellskogo komiteta. pri zhilishchnoy kontore 1!o.3 Petrogradskogo
rayona Leningrad&. (Children-Kanagement)

TANMOV, X.
Plenums of trade-union committees. Sov.profsoluzy 4 no.12:61*46
D 1566' (KLRA 10:1)
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i rechnogo flota.
(Trade unions)

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VAIIIYUKOVt. M. P. and Alcksandrov, B.A.
"Or)tic "easurenents of Uie Phenomenon of a Directpd Dlast.," a i-c,.-,Qrt at
onp, of thu. scs3ionu of tiie Gc,-~cral AzZeMblies of OF11-211 in l,',Id4.
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USSR/P~hys~cs - Spectra, Flash 21 Sep 53
~"Photoelectric Method of Recorrlim~ Variation in
Tim of Spectra of Light Flashes, ~U.P. Vanyulkov
and.11.D. Khazov
rAll SSS.RY Vol 92, No 3. pp 523-524
Describes an improved apparatus for photoelectric
recording of spectra wb1ch shows immediately curve
of spectral distribution of endpsion at any epeci-
fied moment. The resolution in time depends only
on the rapiclity of recording of phenomena on oscil-
lograph, which for the time being is 10-8 see.
268M
Indebted to S.E. Prish, Corr Mem, Acad Sci. WSR
and to Acad A.A. Lebe(lev, who also presented ar-
ticle, 20 Jul 53.
268T92

'%W'W
USSR/PhYsIcs Electron-optic photography FD-897
Card 1/1- Pub 153-6126
Author : Vanyukov, M. P. and Nilov, Ye. V.
T'4tle : Application of the,electron-optic image-converter in pbotography
of rapidly occurring processes
Periodical : Zhar. tekh. f iz. 24,, :L209-1218.. Jul 1954
Abstract : Possibilitj of employing electron-optic coavjrters is istudied
with AEG-type electrostatic focusing as fast-acting shutters
by switching them in by means of short voltgge-pulses. At in-
stantaneous illumination of the order of 10 lux at the photo-
cathode, a redistribution of brightness and distortion of the
image occur. These phenoaena are due to space charge in the
tube and the potential relief on the cathcde. Various stages
of the spark discharge in argon were photographed at exposures
of 0.4 to 2 microseconds. Indebted to A. A. Lebedev. Eleven
references including 5 foreign.
Institution
Submitted March 9, 1954

U41AWics., lile';C~,C6'~~ J., bischarge phenomena FD-3203
Card 1/1 Pub 153-12/28
Author : Vanyukov, M. P., Isayenko V. I., and Khazov, L. D.
.............................
Title : Investigation of light phenomena associated with the growth of the
channel of a spark discharge
Periodical : Zhur. Tekh. Fiz. 25, No 7;' 1248-1256, 1955
Abstract Experimental investigation using an electron-optical converter, of
the space-time expansion of the visible and infrared luminescence
of a spark discharge channel, and of the propigatim of the shock
wave generated by the discharge revealed: (a) the shock .ave sepa-
rated from the plasma of the discharge; (b) a layer of heated, non-
ionized gas emitting infrared radiation in the farm of arc lines
was formed between the shock wave and the plasm; (c) the tempera-
ture of the discharge in inert gases increases with the atomic
weight of the gas; (d) the average channel temperature was deter-
mined from measurements of the spectral density of energy bright-
ness to be'57,OOOOK. Authors thanked Acad. A. A. Lebedev for
assistance. Diagram, graphs, photos. Ten references: seven USSR.
Institution
-Submitted November 24, 1954

ITTBJECT USSR PHYSICS CARD 1 / 2 PA - 1700
AuTh%~R VANJUKOVIII.P.
TITLE The Application of an Electron-Optic Transformer for the Study
of Past Effects.
PERIODICAL Usp.fis.nauk, 60, faso.2, 295-326 (1956)
Issued: 12 / T97~6
This is a survey of works published in the course of the last 5-6. years on
the application of an electron-optic transformer as a rapidly working shutter
as well as on the electron-optic development thereby obtained. By way of
illustration, the results of investigations carried out by using these new and
most effective methods of rapid photography are mentioned.
1. The electron-optic shutter and its application: At first the 11i,ethods of pro-
dneing Buoh a shutter are discussed. The first attempts in this direction were
made with a standard type electron-optic transformer with electrostatic fo-
oussing. In the Soviet Union such work was begun by dynamic operution in 1949
at the suggestion of the academician A.A.LEBEDEV, and already in 1950 the first
positive results in form of three-electrode transformers with electrostatic
focussing (type AEG) were obtainedl in 1951 the impulse circuit of a standard
type five-electrode transformer was constructed. Furthermorej a transformer
with combined electrostatic and magnetic focussing is nentioned, and a trans-
former developed specially for short exposure photography is distmosed on the
basis of a simple draiving. Constructional elements and the oiroult of this
device are discussed. On the occasion of the investigation of easily repro-

Uap.fis.nauk, ~0, fasc.2, 295-326 (1956) CARD 2 / 2 A - 1700
ducilule phenomena it is advisable to use the simple photographic nethod. By
re-taking the photograph at different stages, it is possible to obtain a
aeries of pictures by which the development in time of' the phenomenon is shown
with sufficient clearness. With the help of the oleoti,on-optic transformer it
is possible to build a high frequency stroboscope by means of whiob it is
possible to watch and to investigate periodically recurring phenomena with a
much higher frequency than would be possible with an ordinary stroboscope.
With the help of the impulse circuit of the electromagnetic transformer it is
possible to construct a purely electromagnetic scheme for television in colors.
The defects occur.ring in the pictures produced by means of this Impulse
circuit and a possibility for the increase of the resolving power of impulse-
like connected electronic lenses Is discussed. By the method desoribed it is
possible to obtain pictures of better quality than with the same optics but
with parallel current feed.
2. The electron-optic development and its ap2lications. The electron-optic
transformer can be used also for the high-frequenoy development in space and
time of light phenomena. The various methods to be employed are disouesed.
INSTITUTION:

51-6-26/26
AUTHOR% None given.
TITLE: XI Lecture imeni Academician D.S. Rozhdestvenskiy.
(Odinnadtsatyye chteniya imeni akademika D. S.
Rozhdestvenskogo.)
PERIODICAL: Optika. i Spektroskopiya, 1957, Vol.II, Nr.6,
p. 828. (USSR)
ABSTRACT; Complete Translation.
The XI Rozhdestvanakiy Lecture, named after one of the
founders of the State Optical Institute Jxieni S.I.
Vavilov, took place at that Institute on '16th May 1957.
Two papers were presented at this lecture.
In his paper "On Colour Vision"o Prof. G.N. Rautian
described the retina as a triple receiver of radiant
energy which, as a first. step, limits, orders and analyses
the information received by the eye and then compresses
Gard 1/4 this information for coded transmission to the brain.

XI Leoture imeni Academic .Jan D.S. Rozhdestvenskiy. 51-6-26/26
The three-dimensional character of colour as a retinal
stimulus forms the basis of MaSurement o1' colour and ite
representation in an affine vector space. Of great
importance is the problem of the basic physiological
system of colour determination since the coordinates of
colour in that system characterise the spectral sensi-
tivity of the three types of receivers on the retina.
Rautian discussed the method of finding directions of
the physiologically important coordinate axes by tests
using dichromats reported in the Yustova-Nyuberg work.
He also discussed other methods used in USSR and based
on dichromatism. which is either temporal (N.T. and
V.W. Fedorov) or spatial (M. Bongard and M. Smirnov).
Establishment of spectral sensitivity curves of the
retinal receivers would lead to the most direct methods
of study of colour vision* This was shown on the
example of a new anomaloseope rO 0 and the results
Card 2/4 obtained with it which widen our knowledge of the

XI Lecture imeni Academician D*S. Rozhdestvonskiy. 51-6-26/26
multiplicity of forms of colour vision and oermit us
to construct a more elastic and precise classification
of-these forms. Another example quoted was the
proposal for rationalisation of street traffic signals
to make them correctly understood by all dichromats.
At the end of the paper the author discussed some
new attempts at interpretation of the ph,&nomena which
form the basis of selective sensitivity of the retinal
receivers.
Candidate of physico-mathematical sciences M.P.
,Vanyukov presented a paper on "Emission by a RTX,7-
V65-p-erature Pulse Discharge".
This paper presented the results of the study of
certain optical characteristics of spark discharges in
heavy inert gases (argon, krypton and xenon) at
Card 3/4 pressures of 4-10 atm. Using a now photoelectric

XI Lecture imeni Academician D.S. Rozhdostvenskiy. 51-6-26/26
technique temporal variations"of the discharge were
recorded in the spectral regica from 2500 to 10000
and dynamics of the variation of the form of are lines
in the process of disehar 9 wals deterniined with
rerlution in time of 10-f see and in W6Lvelength of
1 . The brightness of the sl)ark-disft,hCLrge channel
has a ltmiting value which in xenon at 5 atm is about
11 x 106 stilbs. In capillary-tube d1scharges
brightness increased continuously with increase of the
discharge energy and no saturation in ':)rl.ghtness was
observed. In the capillary discharges brightnesses
up to 50 x 106 stilbs and temperatures up to 940000K
were obtained.
AVA,TLABLE: Library of Congress.
Card 4/4

SOV/120-58-6-17/32
AUTHORS-~V~ ~~and Isayenko, V. I.
TITLB: A Pulsing Tube Circuit for Obtaining a High Discharge
Repetition Rate (Skhema vklyucheniya im Ulf kh lamp s
bol'shoy chastotoy povtoreiLiya vspyshek~ snyjcn
PERIODICAL: Pribory i tekhnika eksperimenta, 1958, Nr 6, pp 85-88
(USSR)
ABSTRACT: Stroboscopic tubes are normally connected in a circuit
consisting of two inductances, two capacitors and an ajx-
iliary inductance for triggering the tube; the circuit Lr--
shown in Fig.l. One of the difficulties in employing -ca~.
circuit is that comparatively low repetition frequenr,----,;-s
are possible, A more elaborate circuit, based on the same
principle, was therefore developed. This consists of
supply unit (see Fig.2) and a triggering unit (see Fi~2
The circuit is suitable for operating a stroboscopic triode
(marked S in Fig.2). The storage: capacitors Cl and C2
in the circuit are charged from a constant voltage source
through a choke L I by means of two groups of high-voltage
diodes, B, and B2 . The triggering unit consists of a
frequency generator (a multivibrator) and a delay circuit;
Card 1/2

SoV/120-58-6-17/32
A Pulsing Tube Circuit for Obtaining a High Discharge Repetition
Rate
by means of two blocking oscillators it produces two pulses
0
of..3 lis duration, which are_qpaced at 15 lis apart. The first
pulse of the triggering unit is employed to close the
oscillatory circuit consisting of Cl and LO in the supply
unitl while the second pulse triggers a thyratron which supp-
lies a pulse to the triggering electrode of the stroboscopic
tube. The diodes B and B in the a-apply circuit of Fig.2
provide clamps for tAe storaga capacitors, so that these can-
lidt be charged negatively. By emp-loying the circuit it is
possible to drive the tube at repatition rates up to 4000 pps,
but the discharge energy is reduced with increasing repetition
rates. Thus, for example,, at 500 Pps the energy per discharge
is 3.5 joules while at 4000 pps it is only 0.23 joules. The
paper contains 3 figures, 1 table and 12 references, of which
4 are English, 5 are German and 3 are Soviet.
ASSOCIATION: Gosudarstvennyy opticheskiy instJ.tut(State Optics. Insti-
tute)
SUBNaTTED: December 9, 1957.
Card 2/2

Vfi p),
51-4 -1-13/26
AUTECRS: Vapj3jkov, M. P,Mak, A. A. and Ures, Id. Ya.
TITIa: Instantaneous Brio-itness of a Spark-DischarLe Channel
in a Capillary. (Mgnovennaya yarkost' kanala iskro-,ro,-,o
razryada v kapillyare.)
M;RIODICAL-. Optika i Spektroskopiya, 1958, Vol.IV, Nr.1,
pp. 90-92. (USSR)
AlOTFACT: The paper reports results of measurements of the spectral
density of briL;htness of a spark :Lischarge ch,,--nnel in
capillaries ffilled wit-h. air at atuospherie pressure, or
with xenon at 4 atm. The technilue of measurement and
apparatus are deocribed in Ref.2. Capillaries filled
with air were Glass tubes with internal diameter of
0.252 0.4 and 1.35 mm and an inter-electrode distance
of 10 mm. Capillaries filled with xenon wore quartz
tubes with an internal diameter of 2.5 I=. BriChtness
Card 1/4 was measured in the direction at riL;ht-angles to the

51-4 -1-13/26
Instantaneous Bric~htness off a Spark-Discharoa ChaLnel in a
Capillary.
capillary. For the sake of comparison, neasurements
of briL;htness of the spark discharge ,.,ere -1'-O..e also in
an unbounded a-*;.r jLap. Fib-.1 shows curves, for air,
of bhe spectral density of briL;htness as function of
the wavelength under var.-ous discharge conditions at the
moment when bhe spectral density of brif~--htness at,
4111-94 R reaches its maximum. At constant dischar~,e
energy narraviinc- of the discharge channel by the
capillary produces am increase of lij-he channel briChtness,
particularl7 in the short-wavelenU,-ih part of the spectram.
Decrease of the capillary diameter cannot be carried on
indefinitely since in very narrow capillaries bx-i,,,~htness
decreases (e.6. irt M5 mm capillary brif-
,litness is
Card 2/4 less than in the 0.4 rm capillal-,r). Increase of the

51-4 --1-13/26
Instantaneous j3rir- 1-ness of a " arl-DischarSe Channel in a
L.~h u tip
Capillary.
energy of discharGe thrcup;h a capillai7 increases
bri,ghtness. The hiFI-~ast brightness of 50 x 106 stilb3
was obtained in a channel 0.4 ini wide, filled with air
at atmospheric prossiare, on discharf,inG a 0.011 ~LF
condenser charged to 29 kV. The briGhtness temperatu-Ire
for this case was 94 0000 K. Increase of the inter-
clectrodo, distance from 10 to 20 rini does not
appreciably chanLe the spectral density of brightness.
FiS.2 showo the rezults for xenon in a 2.5 mn capilla--y
filled with xenon at 4 atm (curve 1*' and for a
spherical pulse -r-I i scharp-e lartip also filled with xe.'Ion
(curve 2). ThQ rcs)~tltr, of Fig.2 show that briChtness
Card 3/4 in a capillary filled with xenon x 106 stilbs) is

51- 4 -1-13/26
Instantaneous Brightn,ar.2 of u spark-Discharge Channel in a
Capillary.
loos than 0'ic- corr.-jspondinE5 britSlitnoos In the :-;plicrical
D-MI) (11 x, 1.06stilbs). This is dae to -U'.,ie fact Lha'G
the discaarl-;e-channol wid-11-h in a 2.5 mu c_-pJ_llary' is
limited by that capillrli~j at a comparatively late starze
of t'Alo di-charL~o. and 2 show tbat radiation
from a capillary discharf--e ddffers considerably from
bla(.-._'.~z-body radiation (dashed. curves), except atu hi0h
onqr6-y densitics in 'Uhe discharge channel (FiG.1,
~aurves 1 ancl 3). The- results obtained are suruaa-rized in
a table on p.92. There are 2 firures, 1 table and 5
Card 4/4 refeiAances, of whiCh L~ are Russian and I American.
ASS0CJIA!2IG1T: State Institute of Optics irzoni S. 1. Vavilov. (Gos
opticheshi~ iLi. 3. 1. 11avilova.)
0UMIITT~`Jj): March 18, 10,,'-7.
AVAIIABU, : Library of Congress. 2. Cepillaries-Spectral
1. Capillaries-Spark discharge-Brightness density

Wkiand.fiz,-mat.nauk; DOMTSOV, A.F., in2h.; ISAYEVKO. V
insh.; MAK, A.A., inzh.
Sectional high-ressoure spark discharge lamp. Svetotakhnika 4
no.4:9-11 Ap 158. (MIRA 11:4)
l.Gosudarstyannyy opticheski7 institut.
(Blectric lamps)

'VANTUNOV, M,P.; GORDKHDVSKIY, TUIN,
Conference on hi;h-speed photography and cinematography.
Usp. fis. nauk 64 no.4-.790-795 AP 1589 (MIRA 11:7)
(Photography$ High-speed) (Ginematography-Scientific applications)

AUTHORS: V.-inyukov' 11 - 'v-,17"fak, A. A. SO V/5 3 -66' - 2 -6~ /9
TITLE: Pulsed Light Sources of Great Brielitness (Impullonyve
istochniki eveta vysokoy yarko-'ti)
PERIODICAL: Uspekhi fizicheskikh nauk, 1958, Vol 66, Tir 2, PP 301-329
(USSR)
ABSTRACT: The present paper is an abstract compiled from 100 Soviet
and non-Soviet publications. It gives a concentrated survey
of the present stage of spark-discharge devices, their char-
acteristics, and their theories. Chapter I.: Spark discharges
in gases. Emission of radiation caused by the sloving-down
of electrons in the field of positive ions (free-free tran~-i-
tion), by the recombination of electrons anl ions (transi-
tion from a free to a bo~lnd state), and by transitions from
bound to bonnd states - enission of considerably broadened
lines.
1. 1) 1-othods of producing spark discharges of high intensity:
Connection between U0s C9 L, Qt, molecular weight of the
gas,
pressure; discussion of a pulne tube oith condenser ac-
cordinr-
_ to PrUngel (Fryungell) (Ref 11, J"ig 1), scheme of
Card I/ diccharge circuit with condensers connected in parallel

Pulsed Light Sources of Great Brightness S-IIT/53-66-2-6
(Fig 2, Ref 12); pulse tube with ceramic condensers (Fig 3)
as constructed by Vanyukcv, Dobretsov, Isayenkof Mak - 28 U,
0*022 pF, OoO6 pH, to 4 kW; coaxial condenser according to
Fisher (Ref 15), high-voltage toroid condenser (Ref 16);
discharge circuit for large PU13eB and small L - investigated
by KomelIkov and Aretov (Ref 20)$ construction of 48 different
condensers -134 PF, operating voltage 650 kV and L = OqO25 P11;
maximum current in the circuit 2.1.10 A.
1 2) Methods of measuring brightness and temperatures (Refs 152
2~ - 27). Measurement of temperature in spark dischar,-es
(Refs 25, 28); photographic method (Refs 24, 27); lec-
tric method 'Refs 4, 11, 15, 22, 23, 26, 29, 30-3251;Iojt)hOcto-
chronograph ~Fig 6); photoelectric device for the measurement
of brightness developed by Vanyukov, Mak, Parazinskaya, (Ref 22,
Fig 7). Furthevaore, a number of theoretical investigations
was discuased as e.g. the invectigation of the distribution
of atoms and ionization in the channel of a spark discharge
(Refs 22, 23, 29P 31) 32); investigation of the spectral dis-
tribution of radiation (according to Planck's lav); KomelIkov
and Parfenov (Ref 44) calculated the plagma temperat-ure in
spark discharges a 2cording to the theory of -the pinch effect
Card 2/ fiq (Ref 45): 21,TkT - I , where I denotes the discharge current

Pulsed Light Sources of Great Rrii7 -66-2-6 /9
~,ht -es s SOV/33
an-l IT, - the number of particles per cir. of Vhe length of t',ie
discharge channel.
1. 3) The maximum degree of brightness attainable by means
of spark discharll,es in Casea. SYstomatic inveo ti Ja t ions carried
out by Vullfson, Libin, Charnaya (Ref 46), investit:ations of
the saturation effect (Refs 22, 25); pliotoolectrio. methorls;
investigation of the spectral intensity depenlenco3 on time
in the individual parts of the di3charge channel (.Vigs ~1, 9),
:h dependence on L (Fig 10) (Refs 22, 47); investi,-!ation of
the intensity of spark dischar4,es in air (Ref 4G), in noble
gases, nitrogen, oxygen, and helium (Ref 26), etc. Table 1
shovs L collection of valuesfor the temperature and brij-htness
of various gases arvanged according to authors %nd refer-
ences.
1- 4) Physical processes limiting the brightnesq of spark
discharu"es (Refs 4, 15, 22, 2~, 26), X-el'dovich ('2effl 51, 53),
Rayzer (lief 52); dependence of the abnorpt-ion coefficient of
radiation on '1', formula by Kramers;(Rofs '17, '6; Fi,3 14):
dependence of the spectral density of briF~.htness on A. Dolgov,
1.1andel'alitam (Ref 55) inv,'.aLigated the density distribution
Card 31#q in gas in a spark discharge.

Pulsed Light Sources of Great Brii;htness
II. Spark discharges in capillaries (Refs 13, 101, 25, 59 etc.).
Wiring scheme for partallel. nondenaers, C. - 100 uF L 1,5 01.
Investigation of the optical propertieo ~f the plasr's n
spark discharges (Refs 25, 29, 31, 32, 40, 50, 60, 61). Para-
meters are shown in table 2. Investigation of the connection
between temperature and voltage (Fit, 17, Ref 32); the influence
exercised by the material of tube walls (Refs 52, 60, 62-64)-
III. Sliding spark discharges (discharges between electrodes
located on the- surface of dielectrics). Duration of flashes:
10- 6 _ 10-7 sec (Refs 65-74, 13) "Defatron" (10'_ 6oec, 200 J,
22 kV) wiring scheme for defatron sj~ark (IischirEe (.-ng 1a).
IV. Electric wire explosions (the wire material over
into metal va in th~ manner of an explosion, high terji~eva-
Por6
ture plasma, 10- - lo-7 sec) (Refs 76, 77-87), determination
of temDeratures: refererice3 28, 29 (20 000 - 30 000 0K); photo-
metrical investigations (Ref 91); reference 91: T = 150$000 0K,
V. Shock waves, Propa,~,ation of 9hock waves: Zelldovich, Ra,,rzer
(Ref 53), further, references 92 - 97, del' ermination of the
temperature of a wave front in inert gases etc.
VI. Possibilities of further increase of te:.,.i)erat1ures, Short
survey. Theoretically, it could be possible to attain tem.-
Card 4/04 peratures of the order of 1090K (Ref 100). There are 20 fiGuresf

24(3)
'WTHORS: Vanyukov, Y. F., Yak, A. A. so -'.~/2 0-12 ~-6- 18/550
---------------

TITLEt ------
On the Temperature of the Channel of a Spark Discharge
(0 temperature kanala iskrovogo razryada)
PERIODICAM Doklady Akademii nauk SSSR, 1958, Vol. 123, ur 6, pp 1022-1024
(USSR)
ABSEUCT: This paper discusses the results obtiAned by measuring the
temperature of the channel of spark discharges in argon, xenon
and hydrogen by determining the spectral density of channel
brightness for wave lengths which correspond to the center of
gravity of the lines. These measurements are carried out foT
various rates of entering of the energy into the discbare~-
channel. Measuring methods were discu3sed in a previou3 papez,.
The measuring apparatus is discussed in short. The rLdiati-or.
was investigated in argon for the linas 4806; 4348, ana 35E~3
in xenon for 2900 and 2600 A. The results of the measurements
are shown by 2 figures. In the investiGated interval of variaticn
of contour inductivity, the discrete radiation (lines) of argor-
and xenon reached practically the extreme value. Continuous
radiation, however, at < 4000 1 by far does not reach
Card 1/2

'On the Temperature of the Channel of a Spark Discharge SOV/20-123-6-18/-
~0
saturation value. The continuous and the discrete radi~Ltiz)n o~'
the discharge In nitrogen (p 2 atm) van inventi&ated in tho
spectral region 400o-6ooo I Under these conditicrs, briChtness
was saturated at wave lengths above 5500 X for continuous
irradiation and also for all the investigated lines
( A 4097; 5001; and 5045 R ). According to Planck (Plank)'~~
formula for the irradiation of an absolutely black bu"Ay, tklh~
authors calculated the temperaturea which correspond to tl,.-;
spectral densities of the brightness for those wave lines of
the discrete and of the continuous spectra for which a
saturation of the brightness was observed. The straggling ~f the.
temperature values for various wave lengths 13 very
especially for xenon and nitrogen. According to thes2 icquIti,
the temperature of the channel of the spark discharEe only
a small extent depends on the rate of entering of the enerf-
into this channel. The distribution of the temperature over the
cross section of the channel appears to be uniforra. The authors
thank V. R. Muratov who assis-*,ed in carrying out some of the
measurements. There are 4 figu:.-esand 9 references, 8 offtich are Sov.,,U4
PIU-SENTED: July 7, 1958, by A. A. Lebedov, Adademician
SIMMITTED: June 27, 1957
Card 2/2

.21(7)' SOV/54-59-3-5/21
A UTHORS: U ny-uk*%-1_U.,F
_j, Yermakov, B.A., Mak, A.A., Muratov, V. R.
TETLE: Recording of the Variation With Time of the Contours of
Spectral Lines in the Radiation of a Spark Discharge
F3RIODICAL: Vestnik Leningradskogo universiteta. Seriya fiziki i khimii,
1959, Nr 3, pp 25-32 (USSR)
ABSTRACT; In the present paper a three-channel photoelectric apparatus
for the recording- of the variations with time pul3es of the
discharge spectra is developed for a wide intensity interval.
The scheme of the apparatus -J'Is represented in figure 1. The
spectral decomposition of the periodic discharges was made by
means of a monochromator according to Eberth and Fast with a
plane diffraction grating fo:~ interferences of fiist order. The
grating was constructed by F.M. Gerasimov in the GOI Laboratory.
During the recording the gra"'ing slowly rotated. It was
connected with an electron selfrecording potentiometer of the
type EPP-0.9 over a synchronous transmitter. Tho angular
velocity of the grating could be adjusted gradually from 60 -to
129 2-5, 0-5, and 0.1 X/min. The radio apparatus concisted of-
three uniform channels permitting a simultaneous recording of
Card '1/3 the spectrum at three different instants, i.e. the amplitude of

Recording of tho Variation With Time of the Contours of SOV154-59-3-5121
Spectral Lines in the Radiation of a Spark D13charge
the pulse obtained at the outlet of the electron trigger is
proportional to the value average with respect to time At of
the signal to be investigated for a given period of delay t 3
The pulses obtained are thus modulated according to the
speetral radiation distribution of the pulse source for time
These pulses arrive at a collecting scheme, subsequently at a'3*
direct-current amplifier, and finally at the selfrecording
potentiometer. The three channels recori in the time intervals
0.05- 0-45,asec, 0.4- 20/zisec, and 0.5- 50,psec. For the
determination of the best working conditious the time of
adjustment of the collecting element wa~3 varied. By means of
this device line contours and also the 13hift of the mF-xima to-
ward 0.1 R may be observed. The limit 61' the time resolving
power with time is 5.10-8 sec. In the figures 2-7 the contours
of the spectral lines of nitrogen and heilium in spark disch"rge
tubes are represented. Herefrom it may lie seen that the lines
widen mainly in the first stage of discharge (Fig 7) which
indicates a Stark line widening. The maximum. concentration of
Card 2/3 the charged particles is observed at the beginning of discharge.

Reco.eding' of the Variation With Time of the Contours of ~ S07/54-59-3-5/21
Spectral Lines in the Radiation of a Spark Discharge
It was found from the helium line 11 41386 1 that it is
r~1018 CM3 . Also the arc discharge spectra of helium could be
recorded. The observed asymmetry of the lines could be
ex
plained by 'he direction of the line shift. There are
7 figures and 7 references, 3 of which are Soviet.
SUBMITTED: April 14, 1959'
Card 3/3

-- yANEMYX.P.; MAK, A.A,
Brightness of some pales, light sources. Usp.rmvuchfot. 6:31-34 '59.
(KM 13:6)
(Slectric disaharge lighting)

KOT, M.P.; DDBRITSOV, A.F.; ISAYZM, V-1.; MAK, A.A.
Powerful pulse light source. Usp.nanch,fot, 6;33-37 '59.
(Alectrio discharge lighting) NIRA 13:6 )
(Photography, Flashlight)

SOV/109-4-8-10/35
AUTHORSt Vanyukov 01 Mak, A.A. and Muratov, V.R.
TITLE: Time Spectra of the Radiation of Spark Discharges in
Inert Gases
PZRIODICALt Radiotakhnika i elektronika, 1959, Vol 4, Nr 8,
pp 1284 - 1285 (USSR)
ABSTRACT: Some data relating to the time spectra of the light pul s
in the spectrum bandwidth, ranging from 2 500 - 12 000 le
were recorded by means of the equipment devised by the
authors tRef 1). A detailed description of the equipmert
was given in Ref 2. The time resolution of the device
was 5 x 10-8 see. The spark di~icharges investigated w3re
produced between spherical electrodes in tubes filled
with argon, krypton or xenon; the pressure of the gas
was 3.5 atm. and the inter-electrode distancewas 10 mm.
The voltages applied to the tube were from 5 - 12 W,
the storage capacitance was 0.01 to 0.05 pF and the
circuit inductance was 0*1 to 12 IiH. It was found that
the radiation of the discharge consists of a continuous
background and a number of broadened lines, many of -hich
Cardl/2 can be identified with the lines of single- and
v"

Soy/109--4-8-10 35
Time Spectra of the Radiation of Spark Discharges in Xnert Gases
double-ionised gas atoms. If the storage condenzor is
decreased, the line in the vicinity of X =-3 000 X
is intensified. The lines of the double-ionised atoms
appear during the initial stage of the discharge and are
rapidly - attenuated with time; the Bingle-ionised
atoms appear somewhat later and their attenuation is
slower. There are 3 Soviet references,
SUBMITTED; March 5, 1959
Card 2/2

"702
2"020
AUrMORSt Gran~,.kiy. V.L., Lk~yanor. . u., spim, . G.V. and
Sirat.oke I G
TXTLSi Report 0. the Second AII-0-i- C-nf.r..4o am, C-9
Zlectronic.
elchnike I Iktr.nikO, 1959
PRUODXCALs Redio t Vol 4. Xr 5.
pp 1339 - 1358 USSR)
coaf.r.acap was orX.=I-.d by it.. A-3-U31R. the
ABST&Wrt Th
MI. mtry of Righr 3d.c.tion an4 Moscow state UcAversity.
:,

- 11*th
T. o4o of Reducing the Ca&rgy %mat in the
V
or 11, Rr.&kdown-.

OA
GO *
X
d
radLachargea and
k*
K.
nvcl
b-1
-
,~ ~
:~.
L
.
;
t!!.:
j
Zlectrad" In UISh
Vacuum'.
T-A. SUmmor and Q.,F "tuboy - mlnv.stlg&tL*n or tao
*F*4iasx"__~C Initiation aaa-Wevelopment of a 51gh-voltags
Discharg. In Tacuuo,w.
-8-X. R-YkhruAjd and -V- Ulm' tsl-.y- - -Th. Ch-moter-
lztI4. of IS.Itla. I. ELLSU-oe"- In X.S..tjc 1PI.ld&,-.
kjj-TArA_3.ji.& at al. dealt wIth the tra-for of the *~%ctrodo
material during the fro-breakdown stag. In wax,mumm. 7:>
*.a. Raeoxxv at aL. _rho Motion of of
Xlectric Breakdown In Taco= .
The third section dealt with the problems or electric
spsZkx. serous and thoirpractical applications. It was
Presided over by I.S. 3tokoLln1kow. The raLlowInig poper.
war. road&
T.X-LmxLL*v at al. ~ *PrOb* IUV4JBtjgAt1QU Of the A.C.
C-me" FLel
C.S. Alak A-A',a - w3lanentary Processes in the
Zang of Co"aa-typ* Camduators at Atmospheric Prossuras*.
"Appearance of a Corona Discharge In
Hydrogen and ml rg*n"
P.N. C14.tyA*., at al. Sea. Pr.p.rti.s or the Cora"
-
etem'
lld~ic.l S
C
1
d
J
EA
.
.
o"
lyEA41
rag.mI
-gain ffy
,
y
y
~
fol-d pp a of Discharge
-1
M-N
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111:5
:A
o
osmur*. of
at
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a PIa
n
.
I
10-3 - 1.0 me us-
;x. - 'Method. c uipis, zonimati.m or
KLr By Mommai at Acro-I..i. ." (..a V 1333 of the Journal).

~Z~jfanjn&aX al. - mTj:v Spectra of the Radiation of
X at
&Spark DischarSo in Inert C~Aoxs (see P 1284 of the
Journal).
L
I

-
:produeti n of IU&h
~.Ak
or p 0L.c
:r
~
Field aC
p X&Ljjn afluenco of the Kra.tl-

. an the Dividing Saf.c. of rwo Media
Lria Jim;h:1
r

S
Stakollmlkow, . elfew Data Froo the Study of L,onx
ProportLes of the Breakdown of Cosiprossed
tr~ paratively UaLrarm Field I. the pr..~. or
Locallood Non-umlformitL..'.
teal-an .- ad 0'4-tll*gr.phlo
~ M;..u:po 1"t the Dl-c~arx. L,ags,
I- rKalockri... to.. p 1-157 oi tn. jo.-44?.
A paper by P.M. Zj~lutykh dealt with V.- probXes, of the
basic theory or the electric I L omLom (seA p 1330 or the
Th. fouxtb, .-tio. was V~..Id.d ever by 3.Tla. Lmlk-ym,nav
am4 was aamermad, with the ~A-statioas" end low-
fr.q.ammy d1scharg.., Th. r.11--L._ p:p.r. -or. r*.4s
d A A L.b.d- - 'Th X.tur:ojof th..t
-.,~-_Iphll Z~1.,gMctr zxpz oft
an No I.
,Metal Wires.
V.A. 31mamov - sPropacation of Plas=a Treat LooAl Pulse
-Ob..
-,J 7/1S G.G. T7.;f.,., z .1. - of .. Slootr.
fT-nAa_LCc_s1I`y~C%xmpr*sx*d Are by M-ns of an ILI actrom-opt teal
Convertors.
and or
U.-Ilif.oZ 21 se tria Viejo E. ^7~ I..
end
glsst~.. model of th
A.M. AndrLanov at &I. Lbt-b-ition of KagnotLc and alsetri,
A -P.Wi*rr. 1. Pu J:D Lee
-9 (9-91.4d) "Sp..tr .... ,I. D.t-ftI_tLm
lf tn; Plas". tt- Let.-
I.. 1.326 .fI's j ur. ).
Th- P-m by 11.rdi.g r,...d I-L of Laterest mad
Ac d-ic _kd d the that
"I . e1 tr
be of
f

i'uv/bl -6-1-3/30
AUTHORS: Vanyalco,7, M.P., Yak, A.A., and Iduratuv, V.11.
TITLE: Time Svc-,tra of ZmJ13rioA by Sparic 01schargan in Inart Gases
(Vreiasnv-,.7a spektr,7 izlucheniya iskxovogo rarryada v inertnykth ga2akh)
ftRiODICAL: Optlk:& i Spaktrockopiya. 1951), Vol o, lir 1, pp 17-23 (U SR)
ABSTRACT; The presont paper desoribes time spectra of ttie intensity of emission
by spherical puls e.-dis charge latpa filled -with argon, xenon and
krypton, at 3.5 atm. The author sbidied tAe emission in the 2500-5500
region obtainable -,;ring various ccmbinatioas of capacitance and
indtz-,tanee In thq -.~;Lsnkv-eging cir,%n~.4_ 1%a time spsctra were obtained
with photoelectric apparatui., whose reaol-rlng power was about
5 x 20-Bsec, developed earlier and do&cribad in Ref 2. An Ebert-
Faqti monoanraLat-ir, with a mirror objective of 320 mm diameter and
a diffraction grating wilk 600 liner./M, was used. The relative
spectral 5R-aviv1-.,lty of the apparatus was measured using a standard
incande3s,enb lamp ~Raf 3). The absolute energy) scale for the
intennity of oziesion was obtained -j by using an incandescent
at 4140 ,
lamp moas noottral anisrgy density was kmown for that uivalength. Tna
aps,~tral slit-widtha tuivl -were fram 2 to 20 1. The instantaneous
Card 1/3 values of the emission intensity of Iyalso-lis charge lamps war* measurel

S OV/ 51 - 6 -1 -3/30
Time Spectra of Emlasior. b,..r Sparle Disenarges in Inert Gases
at varioun t:onei t, counted from the beginninK of the discharge. The
first r9cord was always obtained Lwith the exception of curve 1 in
Fig 5) at the moment, of tho max1m,;,m intensity of emission. Th* results
of measurements are given in Figa 1-9 in the form of two or three energy
spectra c,btainwl at various times. The results for argon are given
in Fige I ana '.;, fcr 'krypton - in Figs 3-5. and for xenon - In Figs 6-9.
The re-sults of these !igurei snow that increase of inductance in the
d1scharge circuit redunes the intersity of continuous radiation and
consequently the line, emission bacemes clearer. It vias found that
in thn prat-op-~ of a spark discharge a continuous spectrum and
linti of Youbly iccired atoma appear first. Later the intensity
oz zuc auubly ionized lines iecrea8os and instead the lines due to
ringly Ionizel stams appear in the sp&-Arun. The latter lines decay
moro slowly. ttian tne contInuous background. 'rho spectral distribution
Card 2/3

BOV151-t;-1-6130
Time 3 pectra of Emiazion by Spark Discharp8 in Inert Gfitaus
(;:C tha ctntimao,:--i t;acicground diffar3 groatly from that exnacted of
a bla.,.Ic Nmy and was rou-n4 to be oil- g1j&tly dqMojant on the
wavelength. This affoct may be doe to aow-.auifOj-,,dty of' the
tempera-wre (11.-ztrlbttiop. in rvirca of tne clischarge channel
and aLA'..;c :11~e ro) -Ln the abRorpuion coefficient
of this ais~~narj,.,,q plaime. In varivw. i~-,~,tral. ra.4.Lons. There are
pros and Soviet roforow~cm.
9 fip
SUERITTEDs Mar,h -~,. 1?r~.,
Card 3/3

VAIUMOV, 14.P.- TE%,i=V, B.A.; MAK, A.A.; WRATOV, V.R.
ft --I- ~ -M-Wwii-w
Record of the time variations of Opectral UnP contmirs in the
emission froj a apark discharge. Yest.LGU 14 no.16:25-32
1 '59. (Spectrum analysis) (MIRA 12:10)

24 0), 24 (8)
AUTiORS: 8-23-6 .612"
Mak, A. A. 3 011/4 '1
TITLE: Maintenance of High Temperaturesby Means of a Spark Dischargc
PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheskaya, 1959.,
Vol 23, Nr 0, pp 962 - 964 (USSR)
ABSTRACT: In connection with the development of light sources of high
brightness, it is of E.;reat interest to find out how a maximum
temperature within the spark channel may be maintained, and
to obtain a picture of the temperature distribution in the
mentioned channel. In the present paper the results of an in.-
vestigation of the temperature within the spark channel., ob-
tained by measuring the spectral intensity of the brightness,
are described. The methods of measurements were pre-iously dc-,
scribed in another paper by the authors (Ref 1). The invest-J-
gated lines of argon, xenon, and nitrogen are &given. The ds;~-
pendence of the maximum spectral intensity of argon an the in-,
ductivity of the discharge circuit for 8 different wave leng-h5
is given in the diagram of figure 1 and similar diagrams fcr
the other gases investigated were elaborated (Ref 2). Frcv.
these data the temperature was computed by means of Plan,~kle
Card 1/2 formula and the results are summarized in the diagram X

Maintenance of High Temperatures by bleans of a Spark SOV/40- 23- 8 --6/2c
Discharg-e
figure 2. It may be seen from the results that the tempeiatiare
within the channel is constant in a considerablE wide ran.we of
energy source and that the limits of -14-his method of vcrk may
be determined. The absence of a temperature gr-adii-nt wjth~r
the spark channel, previously detectod by P. G.. ',nr!
S. L. Mandellelitam (Ref 5), is mentioned in the further dig
cussion of the results. There are 2 fig-area and 6 so-iet ref.,
erences.
Card 2/2

-'r - -- - - - -
- - V~ nmov 2 1-1. P. - HAKj- A. A. -
Investigation of Spark Discharge Channel BrightresE in Variolis Cases.
re-)ort submitted for: The 5th International High Speed Photography Congress,
'Washington, D. C. 16-22 Oct., 196o.

VAMKOV, M.P., kand.fiz.-Mtem.nauk; 1WENKO, V.I., inzh.
Load limits of s;ark discharge tutes. Svetotekbn1ka 6 no-3:
7-11 Ytr '60. (MIU 13:6)
1. Gosudarstvennyy opticheskiy inatitut.
(Zlectric discharge lighting)

496%1f
X2"
FMODICALs
ABSTRACT:
Card 1/2
69271
8/051/60/008/04/002/032
1201/1691
'-kov, M.P., ~ ~kAA, and Iduratov V.R.
An Invostigation of gark.Dischar in Hqiumi4
Optilm i spektroskop,&ya, 1960, Vol of Ir 4, pp 439-"5 (USSR)
The authors studied the time dependence of the are and spark line
contours emitted by a spark discharge in hellvm. The discharge v&4
produced by 2.5-10 kV pulses from a 0.05 p? capacitor (the inductance, L,
of the discharge circuit was 0.16 or 3.6 or 25 VE). The sparks passed
through a discharge tube filled -with helium of industrial purity at
a pressure of 2.6-12 atm. Emission was recorded in the wavolength
region 2500-5600 A aoisler discharge tube war. used to produce
a calibration spectrum. It was found th&t in the jnWal stages of
the discharges a strong continuous baftround was emitted, superimposed
on which there were two intense spark (He II) Unes at 4686 and Z203
(Figs 1 knd 2). Are lines of helium (He I at 3188, 3889, 4470, 11471
and W16 1. of, Fire 3-6) appear later, about 0.3-0.6 psoc from the
beginning of the discharge. Both the spark and the are lines witted
by these discharges were strongly broadened and displaced due to the
Stark effect. The asymmetry of the are lines was due to their
---s 7-
04. O-r

85051
S/0,51/60/009/006/'Ol 5/018
50 40 E201/B191
AUTHORS: Ba a shQX.,~F. Va 11ya4g-Z M,, PMura tov. V, R
and Hilo-v, Ye.V.
TITLE: Image-Converter Recording of Spark-Dischar Spectla
Resolved in Time and Along the Channe ross-Section
PERIODICAL: Opt.1ka 1. spektroskopiya, 1960, Vol.9, No,6~ PP 790-791
TEXT; The authors describe a method of recording rapidly
changing spark-discharge spectra using small portions of the
discharge r;hannel. The apparatus Is shown schematically in Fig.,l.
Light proceeds via a. monochromator M and is projected by a lens
04, on the photocathode of an image converter -)on (EOP) fitted
with an electronic shutter, The shutter Is connected to a
generator of square Pulses 3. The generator Is synch.-onized
with the discharge by meanj of a photomultiplier 1 and a
sy.nohronization circuit 2. In this way one obtains a spectrum
on the image-converter screen at a time governed by the delay
between opening of the electrcnic,. shutter and the beginning of
the disoharge, Exposures can be ,,raried from 0.1 to 10 psec Pnd
Card.- 1/2

85051
S/051/60/009/006/015/018
R20VE191
Image-Converter Recording of Spark.-DI s charge SpectTa Resolved i--l
Time. and Along the Channel Cross-Section
spectra. can be recorded 0.07 t-:~ 25 1
~seo from the b9ginnIng of
dAscharge. The imaga-converter screen is photographed wlth a
~~:amera, denoted by t in Fig,1. The method was appl.led to a.
10 kV 6ischarge across a. 14. mm gap in alr8 N I~ N II, and 11m
lines were recorded 1, 5 *, 10 and 21 pse:~ from the beginning
of the discharge (Fig.2'1).
There are 2 figures and I references: 3 Soviet and 2 Engligh.,
SUBMITTED: June 22, 1960
Card. 21L

8603& 1
a(0. Al?/3
S/020/60/135/003/013/039
B019/13077
AUTHORS: Vangkov, M- P., Mak, A. A., and Sadyko a, A. I.
AVN
TITLE: The Maximum Brightness of a Spark DischnLielChannel
PERIODICAL: Doklady Akademii nauk SSSR, ig6o, vol. 135, No, 3, PP, 557-559
TEXT: The authors ' investigated the maximum brightnet!9 of a spark dis-
charge channel int-a on,11nitrogen, airandVelium at extreme high current
-E& -
surges (U/L~~ 101 2a/sec). The high-pressure chamber used for these tests
was developed by V. R. Muratov. The light was obtained through a special
window. The discharge circuit consisted of the following parameters:
C a 0.1 - i,0 microfarad, L - 4 - 6 henry, and U = 2 - 10 kv. The dis-
charge gap was 1.5 mm. In the range from 4000 - 9000 A the continuous
background was studied,also the lines He II with 4686 A, Ar II with
4348 A, N III with 4097 A, and N II with 15045 A. The results show that
the maximum brightness depends on producing an opacity of the discharge
channel. With an increasing current surge the opacity will first appear
in the red part of the spectrum and shift over to the blue part as the
Card 1/2

W34
The Maximum Brightness of a Spark Discha..-ge
Channel
S/02~60/135/003/013/039
B019 B077
surge increases. With the above-mentioned parameters of the current
circuit opacity is easily obtained in heavy gases. The authors mention the
relation between atomic weight and pressure of lChe gas which will produce
a maximum brightness. The theoretical results agree very well with those
found experimentally. There are 2 figures, 1 table, and 9 references:
6 Soviet, 1 German, and 1 US.
PRESENTED: May 25, 1960, by A. A. Lebedev, Academician
SUBMITTED: May 20, 1960
Card 2/2

-ANDREYEV, S.I.; VANYUKOV, _M.F.
I , 16-7_ :L07888 cord
LquiFment for producing light flashes of a
duration. Prib. i tekh.eksp. 6 no-4:76-79 Jj--A9 161.(RIRA 14:9)
1, Gosudarstvennyy opt.,cheskiy institut.
%Electric discharges-)-,

20728
S/05i/6i/oio/oo4/oo6/OO7
(44r0 113rr,11L11) E032/E314
AUTHORS: Balashov., I.F., V Ifuratov, V.R.
and Nilov, Ye.V.
TITLE: The Recording of Time-resolved Spectral Line
Profiles by Means of an Image Converter
PERIODICALt Optika i spektroskopiya. 1961, Vol. 10, No. 4,
PP. 540 - 541
TEXTs The present authors point out inRef. .1 that the
image-converter method can be used to record time-resolved
spectra of various parts of a spark discharge. The present
note reports results obtained with this method in the
recording of time-resolved spectral line profiles. The
method has the advantage that a single flash is sufficient
to record the profile. The apparatus employed is said to
have been described in*Ref. 1. It incorporated the
(ISP-51) spectrograph with an 800 mm foca! length
camera. The image-converter was switched on by I 4s pulses
at different times after the onset of the discharge. The
image of the spectral line was photographed from the image-
Card I
/,#Z 4 Optika i vptkf r0s)Copiya , 116o, Vc 1, No, 61 pp 71o-'791

20729
S/051/6i/olo/oo4/1oo6/O07
The Recording of E032/E314
converter screen with a 1;1 magnification, using a photo-
graphic objective with a focal ratio of 1:1.5, Fig. 2 shows
the distribution of the intensity at the centre of the H OL
line across the channel of a spark discharge in hydrogen.
Fig. 3 shows the H a profile emitted by the central zone of
the channel. Preliminary calculations show that by using the
highest-sensitivity image-converters (Butslov et al - Ref. 6)
and with an intensity corresponding to the saturation region
(Vanyukov and Mak - Ref. 7) the profile of the spectral line
can be recorded with a spectral resolution of 0.1 A with an
exposure of 1 nsec.
There are 3 figures and 7 references; 6 Soviet and
1 non-Soviet.
SUBMITTED: October 14, 1960
Card 2/3

-VAITMOV, M.P,; MURATOV, V.R4; MUKHITDIIIOVA, I.A.
zl~
Tim radiation spectra of spark dischar es in inert. gases
in the region between 5,000 and Xpo(Y~ 1. Opt. i spektr.
U no.3:312-318 3 161. (MIRA 14:9)
(Electric discharges through gases)
(Radiation)

ANDREM. 3.I.; VANYUKOVI M.P.
Using a spark discharge for producing intensive scintillations of
a duration of 1o-7 to 10-8 see. Part 1. Invostigation of electric
processes in a spark diqdharge of nanosecond duration. Zhur.tekh.
fiz. 31 no.8:961-974 'Ag 161. (MIRA 14:8)
(Electric discharges) (Scintillation (Pbysics))
(Oseillography)

') 156
S/l20/62/&b/GO3/020/048
3,7- a 0 e". 2 3 of, 7- 96 1~ E039/EJL35
AUTI-IORS: Andreyev, S.I., ~anyukov, M-P and Serebryakov, V.A.
-L-- I
TITLE: The use of ferrites for the generation of powerful
high voltage pulses of nanosecoxlq duration
Ve"
PEi~IUDICAL: Pribory i telichnika eksperimenta, n1-3, 1962, 89-92
,m%I.T: Tho characteristic sharp change in the value of the
mtagnetic peri-iiazibility ~i of f(;rrites with increasing magnetic
field causes the ~;oa--,ri,,tion of a high. voltage pulse Up when a
ferrite,element is included in a spark discharge circuit
U ',(t) di
p 0 dt
where: LO is the inductance* of the ferrite element at ji = 1;
di/dt is the rate of change of currant in the circuit. The
ferrites (:-.~i,Zn) 1>-6co (F-6oo), :t-looo 0,~-iooo), 4)-2000 (F-2000),
(NI-Zn) M T -2GOO OiT-2000) and f erritas with rectangular loops, are
investigated. There appears to be little difference between the
voltage pulses obtained using Ni,Zn group and the ferrites with
rectangular loops. Amplitude and duration characteristics of the
Card 1/2

The use of ferrites for the generation.. S/120/62/000/003/020/048
E039/E135
pulses produced by the ferrites F-2000 and W-2000 are investigated
in more detail. It is shown that voltage pulses of - 10 kV and
lastin- a few nanoseconds can be produced acroiss a 100 -n-
resistance using F-2000 (i.e. 1 Megawatt pulse) with a discharge
capacity of 3300 )if and inductance 0.1 lihenry. Pulse lengths of
-30 nanoseconds are obtained usinS the ferriti3 MT-2000 but at a
much lower voltage. The effect of circuit parameters on
amplitude, duration andfrequency of pulses is described in detail.
There are 5 figures.
ASSOCIATION: Gosudarstvennyy optichaskiy institut
(State Optical Institute)
SUBMITTED: September 21, 1961
Card 2/2

ANDREMI S. I.; VAHMOV, M. P,; DANIEL', Ye. V.
Method for reeording the radiation spectra of a prulve dimebarge
vitb a time revolution of 10-8000. Opt*', i spaktr. 13 no.6:
863-865 D 162. (MM 16:1)
(Osoiliography) (Electric discharges)

03 L9 6/032/001 /ooa/ol a
S/ 5177
BI 46 BI 12
AUTHORS: Andreyev, S. I., Vanyukov., vI. ,El Komolov, A. B., (Deceased)
TITLE: Development of the spark discharge channel with very steep
current increase in the discharge circuit
PERIODICAL: Zhurnal tekhnicheskoy fiziki, V. 32, no. 1, 1962, 57-62
TEXT: The authors experimentally study the validity of the hydrodynamic
theories on the development of a spark discharge channel by S. 1.
Drabkina (Ref. 1: ZhETF, 21, 473, 1951) and S. I. Braginskiy (Ref. 2:
ZhETF, ~4, 1548, 1958) fo~r_a very steep current inc.:ease in discharges up
to I joule in air. Data on the widening of the spa:rk channel were
recorded by an electron-optical converter type IMM-3 (PIIA-3) with oxygen-
cesium and antimony-cesium photocathodes. The authors operated with
500-7500 pF capacitors, a voltage of 3-23 kv, and an inductivity of the
discharge gap of 10-80 nHy. It was shown that the hydrodynamic theory by
Drabkina agreed with the experiment in the first quarter of the oscilla-
tion period only. For later periods, the theoretical values o-f both the
channel width and the widening velocity are too high. The values of the
Card 1/2

~!948
S/057/62/032/00',/008i/018
Developnent of -tile spark discharge ... B146/B112'
channel width according to Braginskiy, however, agree with the experiment,
even after more than one period. The radiative energy losses are not
expressed in the formulas by Braginskiy; therefore, the good agreement of
his theory with the experiment gives proof of the low effect of radiation toe
on the channel development. The widening velocity of' the channel in the
initial stage of discharge agrees in theory and experiment, attaining
10-12 km/sec; at the end of this stage, which corresponds to the period
of growing electrical conductivity and lasts about 5-10- 9 sec, the
amperage attains the value of 300-600 a for discharge in air under
atmospheric pressure and an electric breakdown voltage of 30-40 kv/cm,
while the channel radius is 0.05 mm. There aire 4 figures and 11
references: 10 Sdviet and 1 non-Soviet. The reference to the English-
language publication reads as follows: H. Fischer J. Opt. Soc. Amer.,~L79
981, 1957.
SUBMITTED: March 22, 1961
Card 2/2

34209
S/057/62/032/6o2/m/022
21. ~Y311 B124/Bl()2
AUTHORS: Va. F., and Isayenko, V. 1.
TITLE; Study of light emission from the electric explosion of thin
wires
PERIODICAL: Zhurnal tekhnicheskoy fiziki, V. 32, no. 2, 1962, 197 - 201
TEXT: The development of thecloud of explosion priducts and of light
emission in electric explosions of different wiros was studied by using
electron-optical devices. Current pulses were cbtained.by discharging a
20,,*f capacitor bank which had been charged up to 10 kv.. The inductance of
the disoharge circuit was O.5q/Ah, and the steepness of current rise was
2-10 10 a/sec. It has been shown that the propagation rate of the front of
explosion products increases with increasing diameter of the exploded
wire and with a decrease of its length, Light emission originat,.as in the
narrow channel between the shock wave and the dense cloud of explosion
products. The channel propagates to cover the whole surface of the ex-
roducts. Gas and vapor temperatures behind the shock wave front

3342G9
5/057/62/032/002/010/022
Study of light emission B120102
3 o
reach 4-10 K and more, which leads to considerable ionization of the
metal vapor giving rise to discharge. The time between the moment when
the current passes through and that when the cloud begins to expand is
proportional to the diameter of the wire and independent of its length,
The time lAg between the moment when the cloud beginE to form and that
when light emission starts increases with the wire length. Its dependence
oil the diameter is complex. At an explosion velocity of 2.5 to 3 km/se..-;,
light emission sets in almost simultaneously with the explosion. Explosion
of a wire takes place at a current density of about 5-10 7 a/cm2 irrespec.
tive of its diameter, This value is in good agreement with previous re-
sults., Wires 0.1 to 0.2 mm in diameter exhibit a marked change in propa-
gation velocity of the cylindrical shock wave at the moment when the glow
covers the whole surface of the cloud of explojion products, As to the
differences between the shapes of glow channels in spark discharge in air
and in an explosion of a wire caused by current fluowations in the dis-
charge circuit, it has been concluded that, with the rapid increase of
current from the second halfperiod onward, a shock wave is generated. which
propagates either through the heated gas, or through the heated metal va-
Card 2/3

34209
S/057/62/032/002/010/022
Study of light emission B120102
por. Since the least ionization potential of air gases is above 13 ev,
while that of copper vapor is 7.7 ev, it is quite natural that secondary
shook waves give rise to more intense glow than that effected by the shook
wave due to spark discharge in air, When the current in the circuit of
the exploding wire is periodically changed, the glowing metal vapor forms
hollow cylinders propagating at the rate of 20 to 30 km/sec. N. N. Dmitri-
yev and V. I. Druyan are mentioned. There are 5 figures and 10 references:
6 Soviet-bloc and 4 non-Soviet-bloc. The reference to the English-language
publication reads as followas Exploding Wires, Edited by W~ G. Chace and
H. K. Moore, Plenum Press, Inc., New York, 1959-
SUBMITTED: April 26, 1961
Card 3/3

s/05Y62/032/003/017/019
B142 B 102
AUTHORSt Vanyukovp 11. P., Isayenkop V. I.j and Travleyev, 0. N.
TITLEi Discontinuities in the spark channel which develope at high
repetition frequency of discharges
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 32, no. 3, 1962v 37.2-374
A -0
TEXT: Irregularities occurring in high-frequency spark discharges in
the'spark channel were studied. The sparks were photographically examined
in an ~'.L-500 (ISSh-500) lamp filled with xenon of 4 atm. The discharges
were 'Ailmed (running speed of film, 40 m/sec). The inage scale was 10.
The frequencies used were the limits at which the studied phenomena
appeared. At f - 400 cps, the position of the spark channel between the
electrodes is stable. The appearance of the channel is determined by
shape and arrangement of the electrodes. At f u 2000 cps, the channel
bends considerably and takes a different position with every discharge.
With bozh frequencies, the mean power was approximately the same (130
watts at 400 Cps, 160 watts at 2000 cps). Points of discontinuity appeared
in the channel at .3- ~-'4-kcps. The channel seemed to be interrupted,
Card 1/2

S/05 62/032/003/017/019
Discontinuities in the spark channel ... B142YB102
individual points of intensive glow became visible. Several discharges
may occur in one channel. The paint of diacharge may shift along the
channel with every discharge (velocity of shift - 1-2 m/400). 301nutimen,
the discharge zone broadens near the electrodes. An fntense afterglow
occurs in the discharge zone for 50-200,ttseo. This afterglow is assumed
to te caused by metal vapor (evaporation' of electrodes) which has a much
lower ionization potential then the other gas. The winding path of the
spark is explained by clouds of heated gas which form in the channel and
along the boundaries of which the spark runs. These local hedtings
cannot be eliminated between the individual discharges since high pres-
sure gradients are missing, and convection is only sufficient to shift
them. The discontinuities in the spark channel are explained by the fact
that in gases of poor deionization capacity the current does not flow
through the narrow channel but throuCh a w-ALder gas zone. Thus, the
current density is lower in these sections.and, with it, also the
luminous intensity. In air,,these phenomena were not observed, even with
frequencies of up to 20 kc/sec. There are 3 figures and I Soviet
reference.
SUBIMITIEDt June 14, 1961
Card 2~2

S/057/62/032/006/Cl5/022
B108/B102
AUTHORS: Andreyev, S. I., and Vanyukov, 114. P.
TITLE: The use of a spark discharge to produce intense light flashes
lasting 10-7 - 10- a sec. 11. Optimum relationship between
spark energy in air and duration of the light flash
PERIODICALs Zhurnal tekhnicheskoy fiziki, V. 32, no. 6, 1962, 738 - 745
TEXT: The effect of the discharge parameters on the speed and duration
of energy delivery in a spark channel was studied in order to arrive at
the optimum relation between discharge energy and length and intensity
of the re.�ulting light flash. On the basis of earlier work (7,hTF, 31,
9061, 1961) it was established that under stiff discharge conditions 85
95% of the total energy stored in a capacitor is delivered in the first
semiperiod of the current oscillation. This fraction is determined only
by the degree of the discharge y - U 0/L(di/dt) max* An inorease in dis-
charge energy through raising the operating voltage entails a decrease in
the ovarall duration of the electrical process. However, the duration of
Card 112

3/057/62/032/W/ol5Xe~2
The use of a spark discharge ... BIOB/BI02
the light flash always increases with the discharge energy. When the
discharge energy is given, the discharge time will decrease as the capacity,
is reduced and the voltage U is increased. An increase in discharge
energy when its duration is ~o remain unchanged can be achieved only if
the discharge gap is prolonged. Aperiodic spark discharges in air with a
length of the electrical impulse of 20-10-9see were got at discharge ener-
es of 0-13 joules. Such a discharge produces light flashes of
(40 - 45)-10-9 see. '47hen the length of the spark channel is given, a
definite relation exists between the duration of the flash and the-maximum
ene:~,-y which can be set Afree in the discharge circuit. Experimental data
are ziven. There are 4 figures and I table,
3Ub;,IIT7'ZDs June 13, 1961
Card 212

S/057/62/032/oo6/ol6/022
B108/B102
AUTHORSt Vanyukov, M. P., Isayenko, V. I., and Travloyevp G. N.
TITLE: lRecovery of t"he electrical strength of a spark gap in repeated
discharges
PERIODICAL: Zhurnal tekhriieheskoy fiziki, v. 32,-no. 6, 1962, 746 - 75~
TEXT: The range in which the voltage of a spark discharge can be controlled
and the limiting load of a spark gap were determined. The recovery of a
gap as depending on the frequency at which the discharges follow was
examined. It was found that in the first 10 - 15,~,seq after the discharge
has stopped the disruptive strength of the gap remaina virtually unchanged
(200 - 40%j v). The disruptive voltage is only slightly dependent on the
Cap length. The subsequent stage of the process is the collapse of the
channel sheath and becomes obvious in a rapid rise of the disruptive
strength owing to the cooling of the gas. Strength in this stage increases
at a rate of 50 - 120 V//,Isec. The stage with low disruptive voltage is
longer in xenon than i-i air. This is due to the greater mass of the xeron
atoms,-mj~ich sustain the channel after the end of the discharge for a
Card(-1/29

3/057/62ltO32/006/0161;022
Recovery of the electrical strength Bloa/Bio;!
longer time'than in air. Extreme recovery rates (up :o 125 v/r
se-) at
very high frequencies are due to a decrease in energy of each individual
discharge and to inhomogeneities in the gap. At too high frequencies, the
strength is either lost completely (continuous discharge) or causes an
un3table oDeration. If the gas is blown through the gap the power per
unit length of the channel can be increased considerably (up to 400 wattM-
At high frequencies, however, blowing has no essential. effect an recovery.:
This is obviousl~r due to the fact that the E:as at the moment of discharge
is in a state of intenSG movement. There are 6'figuros.
SUBMITTED: July 24, 1961
sk
Card 2/2

ANDREYEV, 6114 uv-~~Ov STAROVOYTOV, A.T.
Effect of an external magnetic field on the litait chwaracteri s tics of
a pulsed discharge in helium. Zhur. eksp. i te.)r. fiz. 43 no.3:804,807'
062a (MIRA 15-10)
la Gosudaratvennyy opticheskiy institut.
(Magnetic fields) (Electric discharges through gares) (Helium)

ANDREYEV., 8.1 - VANYUKOV M P.; STAROVOYTOV, A.T.
F.ffect of an extermal magn tic field on the development of
a pulsed discharge in argon, Zhur. eksp, i teor. fiz. 43
no-5:1616-1,618 N 162a (MIU 15:22)
1. G~udarstvennyy optiaheskiy institut imeni S.I. Vaviloira.
(Electric dischargpe through gases)

S/120/62/000/002/029/047
E192/E382
AUTHORS: Andreyev, S.I., Vanyukov, M.P. and Daniel', Ye*V.
TITLE: Increase in the-intensity and reduction of~the
duration of a light burst radiated by a spark discharge
PERIODICAL: Pribory i tekhnika oksperimenta, no. 2, 1962,
127 - 129
TEXT: The discharge system which was Inlrostigated
e;:p criment ally is shoini in Fig. a. The tube contains 5 metal
plates 1 , which are in the form of steel discs, 0.2 mm
thick and 12 mm in diameter. The centres of the discs are
provided with brass inserts 2 , whose heads are hemispherical
and have a curvature of 0.2 mm. The plates are furnished with
sector-shaped apertures As outlets for the light. The discs
are kept in position by means of the dielectric cylinder 3
which is also provided with an aperture. The spacing between
the discs is determined by the thickness of the dielectric
wasl
hers 4 , the dielectric being perspex. The system is
mounted between two massive brass electrodes 5 . The overall
Card 1/ 3

S/12o/62/000/002/029/o47
Increase in the intensity e-ev E192/E382
length of the air gaps is 4-3 mm. The discharge is initiated
under the following conditions (Ref- 3 - the authors - Z11.
teklin. fiz., 1961, 31, 961): capacitance of the condenser
C = 0.015 -ILF, voltage U = 15 IcV and inductance of the circuit
L = 11 n1-1. Tho'constructional details of the circuit were
described in Ref. 4 (paper read by the authors at the Second
Conference on High-speed Photography and Cinematography). The
experiments vrere carried out with single discharges in air-and
the electrical and light characteristi-cs of the discharge were
compared vrith those of the similar characterics of a normal
air gap, 4.9 nri long. It was found that the discharge was
oscillatory and that the presence of a number of metal plates
in the gap resulted in an increase in the gap resistance. The
measurements also showed that the additional metal plates led to
a 300,'0' reduction.-in the duration of the light bursts and a
1.8-fold increase in the intensity of the light emitted per unit
length of the gap (when compared with the performance or a normal
gap). This increase in intensity and reduction in duration of
the discharge was observed over the whole investigated spectrum
Card 2/3

S/12o/62/000/002/029/047
Increase in the intensity E192/9382
from 4 000 - 6 400 A.' The spectral-density distribution was
unchanged by the presence of the metal plates.
There are 7 figures.
ASSOCIATION: Gosudarstvannyy opticheskiy institut
(State Optical Institute)
SUBMIWED: July 29, 1961
Fig. a:
Card 3/3
5
All"

VANYUKOV.- 11. P. -
Sixth International Congress on High-Speed Photography. Zhur.nauch.
prikl. fot. i kin. 8 no.2:157-158 Mr-Ap 163o (MRA 16:3)
(Photography, High-speed-Congrebses)

34023
8/056/62/042/001/048/048
3 /,5,0 ~lo t/ ~, Iq 9 2-,3 B142/B112
AUTHORS: Andreyev, S. I.,
TITLE: "Channel propagation of strong miniature sparks" Remarks to
the article by B. A. Demidov, Yu. F. Skachkov, and S. D.
Fanchenko
PERIODICAL: Zhurnal eksperimentallnoy i il-oreticheskoy fiziki, v. 42,
no. 1, 1962, 309
TEXT: The conclusion drawn by Demidov, Skachkov, and Fanchenko as the
result of their studies on spark discharges of capacitors of low capacity~
that the spark channel expansion at a rate of 60-80 km/sec is doubted. It
is supposed that the substantiating picture does not represent the very
spark channel, but the stage of streamer discharge preceding the channel
propagation proper (analogous to the picture taken by Saxe and Chippenda14
Final studies on the propagation rate of the channel are still necessary.
The lines of investigation persued by Saxe and Chippendale should be
followed. Also the rate at which the amperage is supposed to increase at
the beginning of the discharge is considered too high for the investiga-
Card 1/2

"Channel propagation of ...
34023
3/056/62/042/001/046/048
B142/B112
tions made by the authors with the use of 500-5500 pF capacitors with
hard sparks of 0.01-1.0 joule show, that the maximum of the amperage,
which depends on the resistivity in the spark channelo is reached only
a few nano seconds after the beginning of discharge. Since here only
capacitors of low capacity are concerned, the current is expected to
increase even more slowly than was found by the authoxa. There are
4 references: 4 Soviet and 1 non-Soviet. The reference to the EAglish-
language publication reads as follows: R. F. Saxe, R. A. Chippendale.
Brit. J. Appl. Phys., 6, 336, 1955-
ASSOCIATION: Opticheekiy Inatitut im. S. I. Vavilova (Optical Irastitute
immi S. I.. Vavilov)
SUBMITTED: April 25, 1961
Card 2/2

VANYUKQY* M, .. kand. fiz,ma%lem.nauk- ISAYENKO, V.I.,, lnzh.; TRAVLEYEV,
.9, 1
G.N., inah.
Regulation range and load Iiialts of high-pressure stroboscopic
pulse lamps. Svetatakhnika 9 no.8t20-23 Ag 163. (MIRA 16:8)
1. Gosudarstveanyy opticheskly institut.
(Electric lamps)

7--63
Jix)0
L
LA F 0 C LA NTL/ 5 S D - - F 1 - 4 A o4, -G G /J H BH ttlq
-ASD iADC
j
Bat JWJ0000%14
AUTHOR: VaArikov, m. P.; Isayenko, V. I.; LY11bimov, Y,--L
TITIE: Tim vwriation of the SPectrMl cOMPOzitioA-)f the emission of the
ruby, laser
ika i apektroakopiya, v. 14) no, s, 1963, 7'34-736
WMCE: opt
TOPIC TAGS: ruby laser emissionp ruby laser spectrum
'h ru
TEX11; Time-sequence Photographs of the emission lLae qpe,.,t.-im of t. e by
laser bave been obtained. The spectral lines ware sepe:mted by a Fabry-
Perot.interfercmeter and detected bj an electron-opticaL Jinage converter.
Various ruby sapples were used in the laser, ezd the irx-.erferometer base
was varted from4 to 25 nn. The pumping energy of the laser was also
varied. Pho";raphs show that the energy of the laser pulse can consist
of one, two, ar three lines and that emission vavelensth can vary from
1/2
Card

L 10078-63
ACCESSION NR: AP3000594
t
pulne to pulce 1ritbin an InUrval of 0.2 Angl3trom, viti, 1-10 apparent
regularity. Tht results coincide with those obtained by- 1D.,ghes and by
McMurtry and Siegroan. Orig. art. has: 3 f igitres.

L 18854-63 EPF(C)/EWT(I)/EWP(q)/EWT(m~/BDS/EED(b)-3 AFFTC/ASD/
AFMTC/RADO/APGC/IJP-(;)/ASD.-.-,Pr-4 ja
A=SSION HR. AP3003958 S/0057/63/033/007/0859/0863
AUTHOR: Andreyev, S.X.; Vanyukov, M.P.
TITLE: Investigation of the influence of afterglow on the duration of ultrashort
light flashoyroditeed by spark dis&Arges
SOURCE: Zhurnal tekhnicheskoy fiziki, v.33, no.7, 1963, 859-863
TOPIC TAGS: light flashp spark discharge, high-speed photography, nanosec light
source , He, Ar,, N, helium, argont nitrogen
ABSTRACT: In recent years a number of investigators have reported obtaining nano-
second light flaf;hcs from spark discharges in air, hydrogen and nitrogen. Spark
discharges in inurt gases, which have a high light yield, tire not used for obtain-
ing brief flashes owing to the persistent afterglow of such gases, But actually
the reports of different experimenters on the total duraV,an of light flashes in
inert gases are conflicting. Hence It was deemed of Into'_,zist to undertako a sys-
tomatic investigation of *the role of afterglow as regards the duration of light
flashes appearing as a result of high-power nanosecond dischargeu in di.'foront In-
ort gases. The Cases tested were Ap He and K2. The discharges were realized in a
Card 11,0.2,,,

L 18854-63
ACCESSION NR: AP3003958
circuit with a C -a 900 pr capacitor ut voltages V f rom 4 to 25 W. The entire cir-
cuit was mounted in a sealed chamber which was f illed with the investigated gits at
different pressures to 25 atm. The discharge current was recorded with a time re-
solution of 10-9 sec; the discharge radiation with a resolution of 3 x 10-9 see.
..The afterglow time tag wan determined as the difference between the flash time tf,
measured at 1/3 the peak intensity, and the total duration t. ol the discharge cur-
rent. Oscillograus show that Ue electr* processes in the gap depend on the na-
ture of the gas: discharges i;rA_pnd H ~ In. N2 are oscilictory.
eAre aperiodic; those
to for A and He is shorter than for N2--);/Curves for tag versus the rate of energy
release in the gap are presented. *AT low discharge energies (under 0.01 joule)
none of the testel gases exhibit afterglow. Increase of tag with discharge pc7ter
(and rate of oner-,Py liberation) is greatest ir, A, aad very wealc in ';2. With Jn-
creasing pressure tag increases in A, but not in He and K2.. WLth iricrease of the
[:ap width tag dec.,eases in A, but remains virtually constant in He am' -'42. T12 us,
.Por discharges in argon one can reduc,~ the aftorglov time and -;otal emission lima
.X.
by reducing C and increasing V and the gap wieth. 31onsoquantly, flashes of t1o
same short duratian as in N2 can be realized In He wA A, but only tt great arcri-
-.fice in intensity. Orig. Art. hast 4 figures and l.table.
C,Ord 21p.2,

ALI
.j:
T= VA92=0 07 =LCM-614100=5=10ri or Ift-DOM OYA03 IAW VJT?Wdl, i:U9S;Q
Vaayukov, V. I.. Isayeako, and V. V. Lyubimov. Zbuxnal eksperimontallnoy
i tooraticheszoy fiziki, v. ", no. 4, Apr .1,963, 1151:4152
S/056/63/044/004/OC,6/044
h. e
,xiation of the spectral composition of the output of a neody=ium.-
~.dopee. glass laser with tIme is iavestigat~ed. A glass cylinder 60 = long
and 3 *T=, in diameter containing ~4 Nd2O3 was used. A spectral dispersion
-ot-14 adc mplished by a_dIfrra__
-sad-the-tim"
-reso_
ou wash
-ers-of
see .:-Mie-results,-with-superthresbold
Iti" 1 5 pumibing pow
_bj mic are showa in the illuntratica. The simul-
taneous production-of several lines with superthresholA Punping ywer is
-__.exp2ained as due to the establishment of populatioa inveraLon for several
pairs of sublevels at the same time.

6 June
Tl:-2- VARIATION 02 SPEC-4= COMPOSITION (Cont'd] S/u56/153/044/004/OC6/044
Pz
-0 513,
7
Oc
Card 2/2

L 10524-63 FdA (k )/F-5D/T-- /3W',1,!BD5/F-E-Cf b
VA : ~
MDIM3/t~ "DID
6/0056/63/04/003/1493/1496
D
1
7
AUMCM: Vamyv1wr,,MP.; Isayenko, V. I*; Serebryakov, Vo tko
TrM t ImestieAticu of directivity of emission of an optical quantua generator
SOURCE-t Murnal ekspero I teoret, flzlki,, vo 44,, noe 5, 1963, 1493-U96
TOPIC TAGSt IaAer, - qpissfon directioni - rod cross cection, neodymim-dom-ed
ABSTRACT: Neodymium-doped glass ro&-.w1tb cross secticw of various shapes
have Ueen studied !,g deteralne the effect of the shape on the direeticnal
properties of laser
emission. The polished eads olf the somples received e.
dielectric coating. The semples were p=IA,--d by ~vo _?a1ped lan- -tni t.-*rl--
The distribution-
c0011Ution zones - In the rod was Photographed. - The results chow the stimulated
emission frcm rods of aquare,, rectangular, and octagonal cross seaticn, can be
'01.!opagmted La several di5crete directiona. The preisence of these directions is
Mm

I

(1)/EWT(m)/EWP(t)/EWP(b) rJP(c) J
vrr I
E
ACC-R4 AT6001393 SOURCE MDEs UR/3160/64/009/000/01IS/011S
AUTHOR.-=Vanyukovi--H~=P#=(Canadate -of physico-milthMatical-sclonces) 9
r n4we
TITLZt Study of pulsed light sources of limiting brightness
SOURCE: AN SSSR. fl UspekhL, asuchnay
lotogran =,V. 9, 1964. Vysokeekorostnaya f6tograftya I kivenatograflya (High-speed
photography and cinematography), US
TOPIC TAGS: light source, gas discharge spectroscopy, helium, nitrogen, arrgonq
_-7- --optic-:brightness -------- - --- ----
ABSTRACT: In order to determine itse limiting brightnesses of pulsed light sources?7.1
the -brightness of the spark discharge channel- was studied- 11n am-atmosphere of helium
-argon, nitrogen, and-air at high rates of current buildup An the discharge. To this
end, a discharge circuit based on a low-irduction cylindri;:&! capacitor was develop-
ed. Measurements of the n-pectral density of the dischargo channel brightness were
based an the continuous and line emission In the 4000-9000 A range. In all gases . -
studied, the limiting brightners was successfully obtainedi It was found that undor-
limiting conditions the di3charge channel is opaque and radiates like an absolute
black body with a t perature equal to that of the channel, Orig. art. hast 1 table
~.SUB CODE: SUBH DATE: OU/ ORIG REF: 002/ OTH REF: 000
Ll~ardln

L-11,Q68-6k ENT(l)/DIA(m)-2 IJP(c) AT
ACC NR, AT6001394 SOURCE CODE: UR/3180/64/009/000/OU6,10120
AUTHOR: Vany3tov, M, P. (Candidate of physico-mathematical sclerces); Isayenko, V.
ditd: none
TITLE: Spatial instability of the luminous element of high-pressure pulse lamps
operating under repeated flash conditions
SOURCE: AN SSSR. KomissiyA_po r~yuchnpy foto afii I kinematograffi. Uspekhi nauchwr
L _gr
fotografii, v. 9, 1964, Vysakoskorostnaya fotografiya I kinematograftya (High-speed
photography and cinematography), 116-120-1-
-TOPIC-TAGS.* flash lamp, spark gap, electric discharge
ABSTRACT: A photoelectric method was developed for measuring the probability distri-
bution of the positlon of.sp dischaWe channels in space when the gap Is cut in
under repeated discharge conditions. The spatial distribution of the channels de-
pends on the shape of the electrodes. The width of the distribution is 0.35 mm for
conical electrodes and increases to 1-2 mm for electrodes in the shape of a hemis-
phere or frustum of a cone. The widths of channel dis tribution in ISSh-_ type - high--- -
press ure pulse lamps range from 0. 5 to. l._5 mm. Methods- are --deicribed- for Aipro_ ving
the., -spatial - stability - of ---th6 - cifannel- _~tvo auxiliary electr*des into the
P tord 1/2

IM
.ACC NRt AT6001394
--spark gap when the gap is flushed with a stream of gas having a low breakdown capaci-
ty and when a surface discharge on a ceramic surface is used. Orig. art. has: 6
figures, I table.
SUB CODE: SUBM DATE: 00/ ORIG EMF: 000/ OTH REF: 002
Card'-&--

L X1067-66 EWT(l) IJP(c) V, W/G G - - -
ACC NRs AT6001395 SOURCE CODE: UR/31P.C,/64/009/000/0121/0125
_~-ALMOR: Vmukov, M. P. (Candidate of physico-n4thematical sciences); Ivayenko, V.
_LL. ; MV, 7
ORG: none
TITLE: Limiting loads of pulse lamps operating wider repeated flash conditions
SOURCE, AN SSSR. Komissiya po natichno fotografil i kinematografil. UsIxil(hi nauchngy
fotografff- v. 9, l964.7Tys-oko-ikoros-tnaii-Toto-grWffy-a-T-RTn-eiiii-tog-r;irlya (High-speed
-photography and cinematography), 121-125
TOPIC TAGS: light pulse, spark-gap-,-flash lamp, electric discharge
ABSTRACT: The article deals with the recovery of the breakdown resistance of a spark
gap operating: lUnder-c6n-dttio-ii-"f-i4ap~eated-flashes-wi-th-a-IJ.miting-load-3t--a-discharg,
repextition rate of up to 20 kc. In operation-with a given flash repetition rate, the
limiting power of a pulse lamp can be raised by increasing the capacitance of the
working capacitor. When the discharge repetition rate is increased, t~e power expend
ed in the lamp Is determined by two opposite factors: a &