SCIENTIFIC ABSTRACT ZAVOYSKIY, V.K. - ZAVOZIN, L.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001964010017-2
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 15, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

22882
S/089/61/010/005/010/015
Steady boiling of n.volume heated liquid B102/B214
oonntant. This relation is now used to determine tho liatribution of the
vapor bubblej acoording to size. Tho liquid Is aasumed to be strongly
bolling and therefore in rapid motion no thnt a mean 14fotime of' tbe 1)ubble
.(independent .' of the ape of the bubble) can be Introdutled. r to 1.iA--%j-iendent
aluo of the aize of the bubble. Parther, the probability P(t) iE introduced
which gives ~ the probability tLat t).,e bubble does no `t leave th~ liquid
volume during the time -t: _P(t.)dt (-I/,r)e-t/Td t; P(Odt I. if f (R) it,
0
the distribution function showing how the bubbles are distributed according
to their radii then on account of f(R)dR P(J)dt.-
3/2 12 It
f (1.1)dR aR1/2 exp(-aR , )dR, %here a (ry")-L . Sinae a in
T kau cyl OT 3 /x
constant one obtains for the most probable bullble radius: R prob
If the new variable x -R/R in introduced there resultua:
. _Lxl/2 xP(_ 1 X3/2 prob gn
f (x)dr a2 e T )dx with f (x)dx - 1 . That is, if ths~ man t
probable raditia of the bubble ity known tro di.t3trjbutj.nn function of the
Card 2/3

Blong 61/010/005/010/015
steady boiling of a volume heatel liquid B102YB214
bubbles in size is also known. The ratio of t average to the most
probabl e radius is given by: 'ff/R prob - 3F = 3 ~Yi + 2 3),il 1.87. The
ratio of the total surface of the b"I)I)Ies to their total volume it) given by
4itf ~n.~
S/V - 4n n. where n is the number of the bubbles. Approximately,
3
n
3
S/Vtfo.86/Rprob' The validity of this formula was checked by an instrument
1~ .*
desoribed in the previous paper mentioned above. There are 3 figures and
1 Soviet-bloc reference.
SUBMITTED: September 1, 1960
Card 313

ZAVOYSKIY?---V,K,
Kinetics of a boiling homogeneous reactor. Atom. energ. 14 no.6t
579-580 Jo '63- (MIRA 160)
(Nuolear reactors) -

---- --- ------ ZAVOYSUY
Changes in the density of a volume heated boiling liquid(6e to
pulBewine variations in power supply. Atom, energo 15 '~o.21
164-165 Ag 163. (min 1618)
(Ebullition)

ZAVOYSKIY., VA [Zavoislkyl~ V.M.1; KRUTIK-H-OVSKAYA, Z.A. [Krut7khovolka# Z.Ael
Effect of the anisotropism of magnetic susceptibility on
the accuracy of residual-magentism measurements. Dop. M
URSR no.6:736-739 f61. (MIRA 1L.6)
1. Inatitut geologicheekikh niauk AN USSR. Predstavieno
akademikom AN USSR V. G. Bondarchukom (Bondarchuk, V.H.I.
(Magnatiom-41easurement)

Z"OYSKIY- V.N.; KRUTIKHOVSKAYA, Z.A.
Remanont magnetism of ferruginous quartzites in.the southern
termination of the Krivoy Rog eyficlinorium. Izv. AN S&;P.. Ser.
geofiz. no.8:1150-3-157 Ag 161. (14IRA 14:7)
1. Akademiya nauk USSR, Inotitut geofiziki.
(Krivoy Rog-region-Quartzite-Magnatic properties)
Mix== 411:..~AZZW~V~

KRUTIKIOVSKAYAp Z.A,; ZAVOYSKIYO V,N.
Experience in studying the magnetization of ferruginous quartzites
in the Kremenchug Magnetic Anomaly. Geofiz.abor. no.ls85-98 162.
(KMA 1613)
1. Inatitut geofisiki AN UkrSSR.
(Dnieper Valleym-Quartzite-Hagnetio properties)

KRUTIHOVSFAYA, Zoya Aleks.1ndroimart-I ZAV~-~GKIY,-,UadJmir
?4ikPlajeVICh; FODQLYANKO~ S-e-ularm Mlldwiylovr--~;
AVEITKO, Boris Yakovlevich; SUBBUTIN, S.I.: alademA.,
otv. red.; SMDYTJK, O.P.j, red.
(Magnetization of the rocks of iron ore formatlom of
tho Greater Krivoy Rog awl Ilagnotic Anomly] Na-
rMplichonnoLit' porod Lholezorudnykh fomatoil Bollshogo
Krivogo Roga i IM. (By] Z.A.Krutikhovokaia J. dr. Kiev,
Naukova DurLka, 1964, 178.p. (1411RA 18-2)
1. Akadairiya nauk IRSR, Kiev. In3tytut geofizzyky.

ZAVODO'KIYI V.YU.
Shitting potentials for an elastic stratified ira:=~:0-netris
Akust. zhur. 10 no.3:289-292 t64. (KrWi 17:11)
1. Akustichaokiy intstitut AN SSSR.. Moskva.

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t4i3azuremer,ts3 of the rulative value of parszw~gnetic
absorpt!!Dr~ ,j, perpandliul&lr =1ioletic f!e1!!q 9t a
~1- x 1-~' icc axe Performed for the
F- C rC 1,
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AA-
A)so i,, 10) i70-3014C.)

ii
EM
Measulewcal of the susceptibility Of A.
("POUG sublIt4aCts to wafts. of,
Aw. Rklpd. Te-O"ON, J. 114134
IY56-61(1047); J. Ilk 0.11~1;8119111.
11, No. 2
947V wo self-triductInn cloic. tied with, and im.
"d
tho substaftice Ovu-nid" are dliposeil at 4n dogle
Nse in'
k a , V/2' slid a COMA4. magnetk &IJ 11. forms sin
an%k (00 "Ith Me fligh-frequellcy tnagrittle AtIll
ff d al 1. Ilia e,m,f, of muwal Indoct,ince i fit the
meituring coll 2 Is a function of (fit coTponents of the
maglittle suWPIP'.111ty, X1 Xj, X1 And.xi (the real and
the Itrui&ary parts perpenlikutar to and parallel to 11.)
and of the auSles a and 0. Wasuremento on anhyd.
WS04 at 290'9 -, X - 16 ctn , give, (or xi , a shirp Mill. at
about it. - NO and a fuit max. at about OW oefitcds,
for X' These find.
L a sliarp taix. at about 700 oersteds.
Ing% are discuswd from the point of view of Renkel's
theory (J. Expil. T/Morel. 11hp. 15, 402(1946)).
AcoW WSA'

I.Ivoi-ky 1164f. Totr,f. I'triti. Ifill. 17, M" %414. 0, Ad"
44,-31161. Ilit lt."twij. Tho wumms,-i rinym at,, 1,61iM, (f.-PS
oleaO.In'"Irtif s of I Ito a 1-ttrito It n IQItt 1111gil4io Ito I111411wit of It-It" IwiV
w( the .Met 4 1110 cq~.J, in tho ptv~etpv 1,( 4 to #M. lim4i" 110
in ew.wdinatevt V/111 micz
'thild H, l1w. ctifir" Auto, a mattimn"I,
rolit1wrtl by IL fall to negative V-Sluew, and a minimum. For vlortntloir
111fitel. tho ratio VII/ At the, 11SAXIInum 10 a i- &VI ~ Pi", and the Valf-width
& Le. the IfistAniv rn)m tim maitimuln to All IniIIIIIIIIIII, AM Oe. IfightV
tholterm uirkrl jwywder, alstairk-d by rrdoctitill it( a salt with hydrinit-11. Aim-a
loci 4111irrixtooti ")mnt* curves. one Willi it - A-44 - lip', anti Ili- 0-ther
with to - 2.73 V Ito, too MOIXIMA, at It - WA) and 1,001 flo., still very
The diffe"m Is wrJW In Art 4A)rl foatiffit4MAIV
'Indmtooti VAR of tho Surfarr.. which 14 tnuth gaw Immilismst In the #III,,
der. Traipfnmer lron gives st - 2-d -,~e Ito, A - 7" 1) f le.. i.e. murh
iag"her than In nickel. Hardening or annealing Ime no oigulfictint ritecl,
r
"lip m4pietnoltin erwNtarim behimvitmir it( (~rmutxjttwfie mittlat4mv-d 14 thud
Analtig,tatt tn that 44 pammopwfir stilwant", l1w maWnetir (wid It r"tilto
In A a )bt of the otwilly Irvel Into 24 ; I Itub-Irvetm. anti If Is rvl4ted W v hy
H - r9pti, Where to - 1. 2. 3 . . . V, it two thertf,,re Iw- imi4el"I lhai,
fi,r nhArl. It - 139XI Op, (wrPsismuN 6) a , , 1. avol /I , (0011 1%,, W x -- 41,
HIM file IATPIA f4diff V - 1 -116, ch"O f.1 11W VOIIWR f1( Vin-frin do VIPA4 SIO
of Itarlwit. rplop Ihe Iwomi'lov, ofilm, two 1114%jola. the -1411 -forrilichrl mwwt
Ito * -- I but mmt lip at lo"I # - 1, and Ito- inalowile tat"mria it , .1 Ih,hr
nimpteivem. The ahmence of the main ukaximum lit pon, nickt-I ow, meju
Vilher ve". 1,rw pr(dombilify twiftern ovigh1XI"ring AlIblevela, 4,r that the lev,-l
1114 for ork-pt4twu oftheattin 1,-. 9 to 14mm"It-W.
JICA ZA M Sf&fc-

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Ow. IS, 4(M1946)) thtWY Of ruf.
metooon ram"", kadfas to the rtktka X*/Xd - 2ft%W /
U-s' - r4)' + 4v%,"1 bctwvu the tooff. 3t' of Parawavvetic
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the positias of aw max. ;I X111f). As Owd(Okma 0
(t - 1AWU &CtW. AS - UO1W MRSAOMS, W M 411
dw less.), dw oamatawy d tbe W-width of 3t#. and dw
"sere Abomptift" (1.0' a an"# X, Ott H ~ 0) et r < 100,
This aftakt an W tomb-"4 by Lewes late aw"t the
effect of the IntaudW beta t
lemons"" coxv., As s rmik of mxb fatau4m, The
InturAl 9" wiG broaden the trainauce an a r"Unwrl.
c&Uy no both Wa. so thmi the poslika of the Ms. win ft-
-nula usaffacted, wbervasibewWth willbedeld. by dwla-
tMW km ff.. - sesolusactowo* Oka. kAds to t M rx-
M"a 3COAs - F)I/ft* + #-00+4
bet"" FM
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11
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4W9 NO r)y (Where .1 ruard
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4
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Selo 1947
I
Paramagrietism
WEpetic Sunceptibil-ity
w9urament of Pararnagoetic SUQI~oeptlbility Vit-11
11mater Waves,w Ye. X. Zavoyali , Kazan pr, ACaA
USM, 7 pp
Mr. Emper. i Tecrat Piz!,, Vol ~XVII, No 2
xUrement of active part of magnotic susceptl'M-
I If paramagnetics in frequen~lea not greater th&n
JD kc is acoatuplinhed b7 vali-developed wthod,of
Jmtlon- For higher frequencies, a sufficiently
wise and practical useful ms~hod of measurnmaut
i not been suggested. Necessity of such method ja
57T%
1,R/Phya (Contd) Feb 194.7
rious es'peciallv to stud'y PA"MoSpeti reazatima.
UV of, the latter, and speciflioally +
be pb
magnetospin resonan e, led authors to considera.
of method they describe. iole alooap-Meara
Mmglish In !Jaarnal of Phynicat Vol XI, No 2,:
~7

Tons
VODsteivaning the Magastic and Kwhanical msni
the Atema of Solid Bodies)" Ye. Zamcqsk-ly, Ita-zan!'
StAte Tj; Kazan 3r, Acad Sai UM, 2 pp
I*Zak4kad Nank SSSR, Nova-ftrm Vca wh, No 9,
j Nagnatic spin reacnance in solid and liquid bodlels~
M.~;
~Pemjtg exact determlinatim of Iand's factor fc .
i vagn tic ions, but dose not perzdt si=.iltansoui ~ 40
t4rainatim of magnetic and mechanlea xommts#~;
Proves resonance metho& can be utilized v.111~th hI&
doame of accuracy to determine spin an ve.11 sa:
USSR/Pbysics (ConfA)
nagastic moment of an lcm. Submitted by Acad a
D. Landau,, Apr 1947.
ZOr
nj
5

vq

SUBJECT USSR PHYSICS CARD 1 2 PA 1510
'AUTHOR .ZAVOJSKIJ,E.K., BUTLOV,M.1T.j__PLACffOVA.G.,,_ STOLIMIGG.E.
-TITLE On-1he - Lu~n-e_Bcence Chamber.
PERIODICAL Atomnaja Energija
1 .1, fasc. 4, 34-37 (1956)
Issued: 19.10.1956
The present work contains an accurate description of the main elements of this
chamber. Such amain element is the electron-optic transformer which is con-
s'ructea in accordance .withthe principle of the,cascaaelike eleetron-optic
amplification of light. This transformer coneiats of an input- and some ampli-
fication-casoades which are connectqo,-by--a#n-optieal-contitcf---/.L--thinlilm),.-On.-
-of - - --the----- h----__-photocathode~- ---
f ot ez~_~%
--is fitted. The focussing of.the electro .nic image is discuckeed. In the.domain
between aperture and ser en- tw --pairs-.of deflecting -lenses-a'r'e fitted for----- - -
-----high--f requenoy -dove lopment.--The- - inert ia is is--,-c har -ac- ter. of this-device is of
great advintagel it permits a development in cadres and a continuous high fro-
quency development with a resolving time of 10 a and 3.10-12 sea respectively.
In,the-case of static operation all cauqados are fed by a sectioned high fre-
quency source. Forthe recording of the traces of the cosmic raya a pulne-like
methcd of feeding the output casoade -wafilhowever,nelecto4-In frequent-
cases- the-cascade e
_Aa_~~ -as iik"ig
hu--t- --are -photomul-tiplier,
icytrcuitg. "Impalse-e teraf, - --synchronized- by--means of ~ a
poworwithrespeot___
ime Cwith4-.resolving
to time of 4-10-8 sea). The mode of operation of the luminescence chamber do-

0"5~f/oy -7e 'IV,
USSR/Nuclear Physics C-2
A s Jour Refere. Zhur Fizika,.No 5, 1957, 3-1017
Author Zavoyskiy, Ye.K., Smolkin, G,Ye.,
Inst
Title Investigation of'the Time'Resolution.of Plane-Parallel
Spark Counters*,
Orig Pub Atom energiIya.,. 19501,No.41 46-50
Abstract t It is~showa that the resolution time of plane-parallel.
spark count.ers can be reduced to 10-10 seconds by redu-
cing the interelectrode gape and increasing theworking
voltage... An investigation of thereeolving.tIme was made
from the gomma ga=e coincidence by det4raining the rela-
tive delay of the discharge in two cgunters, which regis-
tered cascade gamma quanta from a Co 0 compound (lifetime
of excited level 1.33 Hev of Nj60 is approximately
Card 1/2
,Card 2/2

ZAVOYSIIY Ye I - ALITSHUIJM, S.A.; KOXYREV. B-M-
Paramagnetic resonance. Izv.AN SSSR.Ser.fiz. 20 no.11:1199-1206
N '5 6. (MM 10-5)
Ofaclear magnetic resonance)
(Magnetic materials)

TY 11 Y~ I
Ij/
ir
U-3
Category ; USM/Electronics Electronic Optics
Abs Jour : Ref Zhur - Fizika, go 2., 1957., No 4281
Author Za ki
_, ~vo y., Ye,*K;l) Fanchendo,, S.D.
ic ~~
Title c e.s of Electron-Optical Chronography.
Prig Pub Dokl- AN SSSR, 1956, 108, No 2, 218-221
Abstract Description of a method for using the electron-optical conv rter for
the 4*udy of prooiesses of very short duration (10-9 -_ 10-14, secon4W)-
using the method of scanning the electron image.' The factors limiting
the time resolution of the method are avinlyzed: the electronic chromatic
aberfatio'n; t~e finite thickness of the'pb)6tocathodA, the finite
Admension.s of the sourcb of light)-and chromatic and spherical *Verra-
tions of the input optical synt6m. The authors reached 4the conclubion
that the limiting time resolUtIon of this method is 10- seconds.
Bibliography,, 5 titles.
Card.

PHASE IBOOK EXPLOITATION SOV/1365
L'vov. Unil-raybet
Materialy X Vseaoyuznogo oovaBhchaniya po spektroskopii, to 1:
Molakulyarnayjx-spok,tron~-.,)piya (Papers of the 10th All-Union
Conference on Spectroscopy. Vol. 1: Molecular Spectroscopy)
[L'vov] Izd-vo Llvovskogo univ-ta, 1957 499 p. 4 000 copies
printed. (Serlea: Its: Fizychnyy zbi;%Yk,, vyp. 5N)
Additional Sponsoring Agency: Akademiya nauk SSSR. Komissiya po
spektroakopii. Ed.! GazerP S.L.; Tech. Ed.; Saranyukj. TvV*;
Editorial Board: Landstergs GwSoj Academician (Reaps Ed#, Deceased),
Neporent, B.S., Doctor of Physical and Mathematical Sciencess
Fabelinskiy, I.L., Doctor of Physical and Mathematical Sciences.,
YabrikAzt, V.A., Doctor of Physical and Mathematical Sciences,,
Kornitskd.V, V.G., Cwndidate of Technical Sciences, Rayskiy, S.M.,
Candidate of Physice-2, and Mathematical Sciences., Klimovskiy, L.K.,
Candidate of Physical and Mathematical Sciences,, Miliyanchuk., V.S.,
Candidate of Plyjaieal aad Mat.1,11ematical Sciences,, and Glauberman.,
A. Ye., Candidate of Pbysical and Mathematical Sciences*-
Card-1/30-

Papers- of -the-10th All--Wi4-b---(C- -t- S-
on ov~13-65
EURPOSE: This colloot4
working I the fiel 01' articlea 13 intended for scientists
n d of spectroscopy pnd for engineers and
laboratory analysts who Ilse
work. spectroscopic methods in their
COVERAGE. This collecticqn Of articles is concerned with theoretical,
experimentalo andft-eahnical problems in molecular spectroscopy.
The application o n0lev-ular spectroscopy to various fields of
theoretical research is described in articles covering chemical
structure$ If-Inetiesp catalYsiso theory of the chemical bondirg,
properties of crysta2s, offect of radiation on substance, etc.
Good coverage is alflO given to the use of spectroscopy in
organic and inorganic teolazology including the study of petro-
chemicals.# polymers, glasl3j, phosphate, boron compoundsj eta.
Each article is followed by references* The text includes tables
and figures.
CalFd--*~~

Papers of the 10th A311--U-nion. (Cont. S OV/1 3 65
TABLE OF CONTENTS:
Academician 0 S. Landsberg- Obituary
&
Academician G.S. Landsberg. Introductory Speech
at the 10th All.-Union Conference on Speitroscopy
Zavoyskiy, Yes K,, 8, A, Alltshuler, B.M. Kozyrev*
'-Na-r-a-m-agR-e-t=a Ile-sonanoo
Broude, V.L., V.S. Medvedev, and A.F. Prikhot1ko.
. Spectrography of Benzene Crystals at 20.4*K
Brodin, M* Ss., and A,F, Frikhot1ko. Absorption and
'Dispersion of Light In Certain Moleoular Crystals
Prikhot1ko., A.F.., and M.T. Shpak. Polarization of
Absorption Bands of Impurities in Crystals
;rm-
5
7
13
14
16
21

SUBJECT USSR PHYSICS CARD 1 2 PA 1795
AUTHOR ZAVOJSKIJIE.X.p SUOLKIN,G-E-
TITLE On.the intermolecular Transfer of Excitation Energy in Crystals.
PERIODICAL Dokl.Akad.11auk# 111,fasci 2, 326-330 (1956)
Issued: 1 1957
The present work endeavors to carry out immediate photogkIaphio registration of
the dimensions of the domain in which energy transfer takes place in a large
stilbon crystal on the occasion of its irradiation with the a-particles of
210
Po .The authors found that the transfer of excitation energy takes place
at distances of some millimeters.
The dimensions of the domain of-intermolecular energy transfer in crystals can
be estimated with comparative ease by means of a luminescence chamber. For this
purpose it is sufficient to photoeraph the traces of the ionizing particles in
these crystals. The authors carried out such experiments with crystals of
anthracene and CsJ(Tl), on which occasion they caused a-particles of Po 210 (with
5,3 MeV) to impinge upon the surface of the crystal under a small angle. The
images of the traces were projected by means of-a microscope (200-300-fold en-
largement) upon the photocathode of an electrpn-optic transformer. The a-par-
tioles in the crystals of the anthracene and cesium iodide had ranges of 34 and
27P, The amplification coefficient of the eleetron-optio transformer was
sufficiently high and made the photographic registration of an electron flying
out from the Input photocathode possible. Some photographs of the traces of
IN

D.ok1.Akad.Hauk,111,faso.2, 328-330 (1956) CARD 2 / 2 PA - 17.05
a-particles are attached. The imaiges of the traces In some cases consist of
single points. Each point corresponds to an electronemitted from the Input
photocathode. The number of points per unit of length of the trace is deter-
,mined by the light-yield of the crystal, by the quantum yield of the photo-
cathode of the eleotron-optio transformerp by the properties of the optics
used and finally by agreement of the speotroseneitivity of the photocathode
with the emiesion-opectrum of the aVy9tal. The traces in the anthraceno and
in the cesium iodide were photographed at the same conditions and the emission
spectra of these.orystals agreed fully with the curve of the spectral sensi-
tivity of the antimony-cesium cathode. There follows a rough calculation of the
number H of the points for the total range of a-particles. 11 ,,10 is found for
anthracene and N -.150 for CsJ(Tl). These values agree satisfactorily with the
experimental data obtained by the authors. In the case of anthracene and also
of CSJ(Tl) luminescenoe-light in thus radiated from such molecules as are
located at no groator dintanoo from thq pla.~fcke of the paaaAgo of the a-pnrtiole
than tho minimum diatonoe 1e) *till roool-vsblo by tho oxperimantal davice.
INSTITUTION:

SUBJECT USSR / PHYSICS CARD 1 2 r" - 1011
AUTHOR ZAVOJSKIJ, E.K., BUTSLOV,M.M.t SMOLKINVG.E.
TITLE The Utmost Amplification Coefficient and the Inherent (Own) Noises
of Eleotron-Optie Light Amplifiers.
-PERIODICAL Dokl.Akad.Nauk, 1119 faso.5t 996-999 (1956)
Issued: I / 1957
There exists a certain limiting value 1111m of this amplification coefficient
which corresponds to the smallest possible signal, an electron emitted from the
input photocathode of the light amplifier. ng, is here roughly estimated
according to the formula I I m - nal where A onates the number of sleotrone in-
oidiAg on the surface unit 0 the screen which is nece ary for a normal record-
ing with an optio density of 012 to OP4- With n-109 (:6t1v2.1o4 ev) and
cr- 1o-4 cm2 one obtains ~ 105. The authors were able to realize one #Ingle
electron with the typo 95 11mht amplifier. ror this purpose at first the eleo-
trons of the dark emission of the input photooathodo were used. According to
various ezperiments the majority of light flashes doom not carroapond to single
electrons at operating voltages of from 8#000 to 20,000 V, but to whole groups
of electrons (electron packets), which fly away from the Input cathode. There
are thus two different components of the dark emission of the SbCs of the yhoto-
cathode: the "single-eleetronia" and the "multioleotronioll component. From the
minimum optic density of the negative it is not possible to register the single
elootrons, because then separation of the one-electron component is too difficult.

Dokl.Akad.Rauk, 11-1, fasa-5, 996-999 (1956) CIRD 2 2 PA 1911
'For the raiia'41o separation and registration of an electron# and for the pur-
poss, of determining the character of the emission of the multi-olootron 002-
,ponent of inherent (own) noises the defoojesing of the electronic Imago in the
input cascade of the light amplifier was used here. On thic occasion quantita-
tive measurements of both components of the dark current were successfully
carried out. The fact that the two components are created in different manners
iop above all, indicated by the dependence an temperature. When the photoca-
thode was cooled in liquid nitrogen, the single electron current vanished com-
pletelyp which indicates its thermoolootronio origin. At the same time the
multi-eleotron component of the dark current remained practically unchanged.
The data available at present m not sufficient for the determination of the
origin of the multi-electronio dark current. Possible causes are the auto-
electronic emission from the unevennessom (aphoroliths) of the photocathode
or the bombarding of the cathode with heavy ions.
The aforementioued experimental data prove that the utmost coefficient of
slootron-optio amplification is attained and that a further increase of sensi-
tivity must be attempted by increasing the quantum yield of the photocathode,
Besides# the registration of an electron permits the study of such phenomena
at which only ono photooleotron (or a secondary electron) flies away from the
input photocathode,
INSTITUTION:

-LYAn
ZAVQV9KIY,-Ye.K., ADIASEVICIII B.P.~ Bb IVp S.T,~ POLMIIIT~ Yu.P.
"Sources of Polra-Ized Particles."
paper submitted at the All-Union Conf. on Nuclear Reactions in Mcdium and LOW
Energy Physics, Moscow, 19-27 110'vember 1957-

SUBJECTs USSR/magnetic Radio-Spectroscopy 25-5-5/35-
JUTHORt Zavoyskiy To K Corresponding member of the USSR Aoadomy of

TITLEs Parazagnotic Resonance (Parampitnyy rexonans)
PERIODICALt Nauka i Zhisn' - May 1957, No 5, pp 10-12 (USSR)
ABSTRACT# The article contains a description of the paramagnetic ro-
sonanca phenomena, which are explained an the aboorbtion of
radio waves of Larmore frequency by paramagnetic materials.
A description is given of the arrangement for demonstrating
the resonance. It consists of a radio frequency generator,
which gdaerates the high frequency magnetic field. The par&-
magnetic materials under investigation are placed between the
polso of a powerful electromagnet. The current in the electro-
magnet can be changed by a variable resistance. A galvano-
motor or onaillograph is connected into the circuit of the
raaio frequenoy generator, whose indications are very sens-
itive to the amount of energy absorbed by the paramagnetic
material.
Card 1/2

TITLEs Paramagnetic Resonance (Paramgnitnyy resonans)
The paramagnetic resonance was discovered by the Soviet
scientist E.K. Zavoyakly in 1944. With its help the magnetic
qualities of atomic nuclei can be studied as well an the
structure of numerous liquids and solids.
The article contains four figures and one photo.
ASSOCIATIONt
PRESENTED BYs
SUBMITTEDs
Card 2/2

4%UTEOR ZAVOYSKIY E K FA 2716
:TITLE for the Polarization of -a -Proton Bundle.
(0-voBmozhnom matode polarisateli puchka'protonov - Ru3sian)
.,-_
--_PMIOD1CAL Zhurnal Eksperimo i Teoreto-Miki, 3,957;,-Vol 32, Kr 2,
, PP hoa-1108, (U.S.S.U.)
Received 5/1957 Reviemed 6/1957
AMTRACT bundle of protons (as well as deute~onsi tritiumo He 3# etc#) P433-
ing through a thin,9 ferromagnatic film magnetized up-to saturation
must "polarize'? because the p6lailzed ferromagnetic electrons are
captured by protons. Actually., the obtained hydrogen atoms will bt
polarized after the capture of such electrons with respect to the
electron spin. If they are magnatized outside themagnetio field once
more by causing them to pass through a thin foil (or through a gas
jet), the protons prove to be partly po2arized, The percentage of
the protons issuing from the second foil vill be equal to half of
the percentage.of1he polarization of the neutral atoms with respect to
electronic spin. The polarization-degree of hydrogen atoms is defined
by the.probybility 9f the capture of "ferromagnatic" electrons by
protons divided by the probability of the capture of non-polarized
electrons. The power of polarization -will 4pparently delpend on the
velocity of the protomi and on the type of the ferromagnetic. If 3d-
and a- electrons are captured with equal probability, the degree of
polarization of the protona in the ci*e of the applL.,ation of an
Card 1/2 ir6n foil must-attain -157.. The interwity of the current of pola-

AUTHOR ZAVC Y jK I Y, 56 W502'
4T.'ITLE A Source ox Polarized Nuclei for Accelerators,
(Istochnik polyarizovaunykh fader- dlay uskorlteley-Rusaian)
iBRIODICAL Zhurnal Eksperim.i. Teoret.Fiziki,1957,Vol 32,11r 4,PP 731-735(USSR)
ANTRACT The paper under review discuoues the possibility of constructing
sources of polarized protons(and of some other nuclei)by utilizing
the Lamb shift of the levels 2S, 2 and 2P1/2and the metastability
..of.tho first-lovel.In a-La'mb exp1ment with an atomic hydro",Pen
bundle it is possible to obtain polarized proton buildlentif the
hydrogen atoms(which are polarized with respect to the electron
spin) are brought out adiabatically in their metastable state from
the magnetic field,and If they are ionized by light or electron
collision.In the paper under review,its author considers the rioBt
efficient method for the polarization of protons.Through a cavity
that is-filled with.atomic-hydrogen and that is situated in a ho-
mogeneous magnetic field of H=540 oersted there passes,an electron
current.Then conditio
naare created in the cavity at which,(1),the
'
density of occupation of the levels 291/2 is considerably higher
than the density of occupation of the P-stateaj,(2),the ionization
-of.the-atoms takes place mai 'nly by the 2S, /j,Itates.Here it is poa
niblejwith the aid of the reconance field, 0 leave in the gas
prac-
I
tically pure 2S4/20tates, which leads to a polarization of loo~.2 of
the protons.With the aid of the usual methoda,the polarized protons
Card 1/2 then can be brought out of the cavity and introduced into the ac-

A So urce of Polarized Nuclei for Accelerators. 564,_114/52
celerator. All atoms remaining in the metastable state are pola-
rized ivith respect to the electron spin.Under influence of the
field with resonance frequency,one of the remaining mixed metastab-
le states is transferred into the corresponding sublevel 2Piani
,from therelduring the life duration of the P-state(T ),into't e ba-
sic state 'S /2 Thus a polarization of the atomic nuBlei in the
2S1/2 state 1b achieved.With the aid of the methods subsequently
discussed in the paper under review it Is posiible to oelect the
optimal conditions for the intensity and for the polarization of
the proton source.The intensity of the source is limited mainly
by the diffusion of the resonance radiation in the hydrogen. It is
posuible to utilize the atron.- diffusion of the resonance radiation
in the hydrogen.It is ponnible to utilize the strong diffusion of
the Lyman's radiation also for the purpose of realizing the pola-
rization of protons.
(No reproductions)
ASSOCIATION Not Given.
PRESENTED BY
SVD14'ITTLD___ 1-4-.-12.-1956- ---- --
AVAILABLE Library of Congress.
Card 2/2

ZAVOYSM Ye. K. (Correspondent-mu=er: AS USSR)
"Phenomena of Electron Paramagnetic Resonance"
Lecture to be delivered by Soviet Scientists at the Brussels Exhibition,
August 1958. The delivered lectures will be ava:Dable in English, French,
Flemish and German as individual brochures.
(Priroda, 1958- No. 8, p. 116)
I -al imgz

3(i

;AUTHORS,
Butalov, S07/2o-121-1~-l
3/50
_
,Y-o1 sciences, Uss", Kalinyak,
CorrespondiYig tlembor, tkcadWM
A. A., Nikonov, V. B,, Prohof'7eva, V. V., 5;molkln, 0. Ye.
TITLE: The U5e of M~iltistage Electron-Optical Light Amplifiers
in Astrophysics ( 0 primenenli mnDjjokaskndnykh olektronno-
opticheskilch u3ilitelay svets. v astrofizike)
PERIODICAL: Doklady Akadamii nauk SSSR, Vol 121, Nr 5, IV~57F'
pp 615 - 818 (USSR)
ABSTRACT: This paper investigates some problems connected with the
application of electron-optical light amplifiers in
astrophysics. The authors estimate the increasu in
efficiency of the utilization of the photon flux with
respect to the usual photographic method. Under the
investigated conditions, and in the case of equal dimensions
of the pictures, the efficiency of the electron-optical
.,method is by &0 4.10 times higher than in ordinary photo-
graphy. An increase in scale on the photocathode of the
light amplifier reducos the increase in sensitivity of the
ol,)ctron-optical method compared with a usual photographic
card 1/3 plnLo by 160 timen. An ovtlma.tion of tho nannitivity

-The.Use of !,Tultistaze Electron-Optical Light. A=plilfiers S07/2r,-121-5-125/50
in Astrophysics
of the light amplifiers given a value of the order of 1000.
The use of an electron-optical amplifier usually cannot
increase the penetration range of tile telescope. But the
reduction of tile times of exposure by hundreds of times of
its amount due to the high eennitivity of the light amplifier
essentially changoa the posuibilition.of the astrophysical
Investigation, The short times of exposure permit the
investigation of rapidly varying processes of very faintly
visible objects and a considerable increase of the utili-
zation coefficient ofthe astrophysical instruments. The
reduction of the times of exposure is very important for
astrospeotroscopy. The above-discussed considerations
are confirmed by the results obtaified by experiments carried
out by the authors in the Kr;rmskaya actrofizicheskaya
observatoriyd AN SSSR (CrimeenAstrophysical Observatory
AS USSR). The proper noises of the light amplifier may be
neglected in comparison with the b:;ckground of the sky.
According to the experimental values, the use of the light
amplifier permitted a reduction of the timeo of exposure
Card 2/3 approximately to a thousandth part of their former amount

The Use of Multistage Electron-Optical Light Amplifiers SOY/2o-121-5-13/50
in Astrophysics
w1lioli attififnatorily agroon with tho above-givon orritli-,iato.
figUVO ohowa tho photographo of 2 oxtragalactic nebulae
which *viere taken by means of a light amplifier. There are
4-figures$ 1 table, and 6 referencea, 3 of which are Soviet.
ASSOCIATION: Krymskays astrofizicheskaya observatoriya Akademii nauk SSSR
(CrimeanAstrophysical. Observatory AS USSR) Glavnaya astro-
nomicheskaya observatoriya Akademii nauk.SSSR (Astronomical
Main Observatory)AS USSR)
SUBMITTED: April 14, 1958
.Card 3/3

BUTSIDY, 90M.; ZAVOSKIT, U.K.; PIMOV, A.G.; SHOLKIII, G. To.; FANCUM,
S*D*
Electron optical method of the photograPtw of ultrabigh-speed
processes. Usp.nauch.fo't. 6:84-89 159. (gIRA 13:6)
Slootron 9ptics)
otograp~q, Inatantaneous-Scientific applications)
W

BOLOTIN.. V.F.; ZAVOYSKU.J. Ye,K.; OGANOVO M.N.; ISMOLK.Ult G.Ye.;
STRIGMIOV, A.Rik
(Uso of electron-optical light amplifiers for spectroscopic
studies of a weakly radiating plasma] 0 primenenii elektrorno-
optichaskikh usilitelei oveta dlia spektrookopicheakM is-
sledovanii slabosvetiashcheisia plazvq. Moskva, In-t atomnoi
---anergii,-1960,- -3-1 p. (MIRA 17:2)
0"f t9m,

Iammmmummum
A
t, 11
'IEHATOV A. P. ; BLINOV P. 1. BOLOTIN ~ V. F. ; BORODII, , A. V.
GAVRIN, P.P.; ZAVOYSKIYY YO.K.; MOVAN, I.A.,- OGANOV, M.N.;
FATRUSIXV, ; RUSANOV, V.D.; SJOLKINP
G.yo.;, STRIGANOV, A.R.; fRANK-WfaETSKIY# D.A.; CM021YKIT,
P.A.; CHIKIN, R.V.
(magnetoacountic reBonance In a plaumn) Magnito-zvukovoi
rezonans v plazme. Moskvas In-t atomnoi energii., 1960. 23 P.
(MIRA 17:2)

lau
k-r-
It
UA'
114 110~ ~11
0 A I u 212
V? t
it
A, A 31
~~l 1 ~__(v ~tlz

0

1 6TOI
5'/ 3f/605/001/020
V
31041/3205

Z v ski's V Kovan, I., A. 2-1runhev, B. 7.
AUTHOI S: 0

TI~LE: Magn6tosonio method of plnoma ioni,,.,*. tion
PERIODICAL., Zhurnal tekhnicheskoy fiziki, v. 31., no. 5, 1961, 513-15117
TEXT: The conventional methoda of Droducing concentrated plasma are
discu3o6d in the introduction. It is noted that the an-olication o.:" th!5sc
can or.!,, bc
methods to a ma~-netic field is li~iited.' Th'o 'he-1-mal metho
10 n i t 11,J 4 -,,:.1
I for atomo of low ionization poli"entials. loniZation by

current 'cauncs Ins'ab il i ties, and ionizati by an o3cillatin~; elect.-;'~r
on j
beam reeta ,-.ith expGrimental and't-echnical difficul-Ils-1-. The concent_: -
tion of plaoma attainable by h-f d;-:;charge is limit-_,j 'by th-_ nlz_sma
Proo-aency, and the production of ccrxantratcd Pla~:r:,:i by a lon!zitudin--I-
alternatin~~ field requirec 'U;lc usc of :ni-lIli:-,,:?'.er a---- sub-m-41-11-moter
The autbors tested 3everal method-z of obt-cining concentrated plasma, -zhich
arQ. not limited by the plasma frequency. Thin i3-achieved by an Liter-
nating electric field, the electric vector of,which is perpendicular to a
Card 1/5

j
4.

7~,
J,
5/057, 61 '03, 020
I f -) v - x
Magnotooonic meth d B I 04/IB205
tron and
static magnqtiq f1ald. This method mal.wa it poo3ible to use elec
ion-4qyolotron or magnatosonic renonancen. Tho latte.- mothod 1'7 not
limihed i-- to the attainable plaama concentration. It z:iakes u.9c of
mc.-metosonic oucillatlions of a lim3.ted plnsma yolume,, and from the theOry
of tbaoe oscillations it follows that' the vclo(~ity amplitufle of the
azlinuthal electron drift iri given by v 01/wj ( 1 where V denotoo the
-o'ron
volodty um litude of the rudial pla not ion, For the kinetic el-
e n er, -ey one has E MV! (3)
2. 2 wiwe 4-rn,
where !T _i ni too the strength-, of the static mo_~-netuic field, H the
% .0 u
amplitude of the alternating narnetic field, and ~e its frequency; (o. and p
e i
are the-elec~ron Lnd ion cyclotron frequencies, respectively, and n e
'trat4onu. jo4ization by radinl -aZnetiQ zound
8enoten the electron, ccncen
is possible if its enerGy io 'UL-,,ic-r than the ionization eneray. It is
obvious that the required rtmp 1i -1-1 e of the alu'er'lati-ng field is the higher,
the higher are the concentro~tion slyrengt*- of atlatic. field. -,,--th a
Card 2/5

22770
3/057/61/031/005/001/020
Magnetooonlo method... B100205
,glv-en amplitude of the h-f field ~ and a given.plaema concentration, there
exists a threshold H* of the static field strength above which ionization
will not be posalble any longer. By increasing the amplitude of the h-f
field, the strength of the static field and the attainable plailma
concentration can be extended Infinitely. In a strong static field,
however, a very strong alternating field is required for obtaining Ugh
conoon-trations Ly radial magnetio jouril. Ionization by magnetle sound
has been obsoryed experimentally lit a quaoi-atatic field in several
Ina Liu llat iona, Effective lonization. ooourrad both below itnd Above the
15
hybrid froquoroy, rtioulting in oonaentrationo of more than 10 om
Tho Ionization brid the nature of rooonanoe 4nd won alwayu nooompanled
by the penetration of an altornAtiklq field into the plaama. Fig. I ahown
resonance ionization by a h-f magnetic field vith an increaae of the
quaal-statlo magnetic fluld In time. By blanking it 3-am probe aignal it
wau pooelble -to Indicate a concentra Ition higher than 10 12 om-3. The
penetration of an external h-f field was observed by means of a magnetic
probe introduced Into the diacharge apace. In fields larger than H*,
cohoentration dropped considerably. It could be ahown that in experiments
Card 3/5
!!;MMR
'N'S '111,71V 111

B/057/61/031/0051/001/020
Magnetosonlo method.., B104/B205
with it quasl-s tat lo'magnetio field, 114~ is a linear funation of rl. Thi a
can be explained by formula (3). The calculated valuen of If* are somewhat
lower than the experimental ones, i.e., ionization can be achieved more
easily thanjwolild have been expected frcm the drif t. This car. be ajeribed
to longitudinal, ourrents which are due to the fact t1v,t the o0aillations
are, riot completely radlal. Based or, these reaulto the authors desJgned
the model of a plaoma source with magnatosonic ionization. The plar3ma
comes from the source which Is placed In a magnetic field and flows along
the field Into a m-epi3urlyg volumo. In pravlous experimenta a plaona
column having a diameter of 6 om and a concentration of 101~ am-3 wan
obtained in the measliring volume at a rated power of the Ionization
generator of 4 kw. The experiments were made~above the hybrJd frequency,
in weak magnetic fields where the drift motion Imparts energy to the
electrons, which is sufficiently high for ionization. There are 4 figures
and 8 referencen: 7 Soviet-bloo and 1 non-Boviet-bloc. The reforenoe to
thG Eriglish-language publication rea4a as followst P. C. Thonemarin et al.,
Nature, 181, 217 1958
SUBMITTED: July 21, 1960
Card 4/5

20452
3/056/61/040/002/005/047
B113/B214
7, //,S-ff 11CO)
AUTEIOR$t Zavoyakiy, Te. K.,,Skoryupint V, A.,
TITLEt Magnetic analyzers of emission spectra
PERIODICALs Zhurnal eks~perimentallnoy i teoreticheskoy fiziki,.v. 40,
no. 2, 1961, 426-432
7.1
TEXT: An investigation,is made of the extent to which the 'phenomena of
paramagnetic atd other forms of magnetic resonance can be used for the
study of emission spectra. Some methods are described in this paper.
Theory and descr!ption of some cagnetic spectral analyzers (USA) are
given. The principle of such an analyzer may be seen from Fig.l. I is
the input broad-band,appliance which guarantees the connection of line 2.
with the radiating system. 3 is the load resistance of the line, 4 is a
broad-band detector; 5 is a recording instrument, for exampleg an
oscilloscope; and H is a quasistatic magnetic field. For a spiral wire
without.ohmic loss, the decrement of damping is given by
aro 1/4 -J

2 2
-------- 3/056 61/040/002/005/047
Magnetic analyzers of.. B113/B214
4VIg' 2N6f(v)rn
23 S(S + 1) M(M 1)
a Mo 23 + 1' .(4), where ris the
frequency, g - spectroscopic splitting faotor,.P - Bohr magneton. N
number of paramagnetic particlesp & - density of the paramagnetic, k
Boltzmann's constant, T - the temperature, f(9) - a function having the
form of t~e paramagnetic resonance curve, 3 - spin, M quantum number,
r- - dielectric constantp/4 - magnetic permeability# nj number of
windings per cm of the line, and r - radius of the spiral,
ASV%jtA2N8f (V
)
S(S+I)-M(m
kTAC 2s+ I
holds for &: coaxial line. The total damping factor of -the line
:length is-'given bys at + ao + cc, j where (90 Is the part- due to -lose in
the oonduotor# and a, that due to lose without resonance. If the
spectrum'oonsista of one or several monochromatic lines# thent at a rate
7 1
of change of the maghetio field of 7-10 oe4seo- a transmission band of
tard 2/4

20452
S/056 61/046/002/005/047
-.Magnetic analysers of... B113)B214
3.5 107 cps is necessary for the-recording instrument in order to record
the;e lineal for continuous emission spectra# the frequency need not be
so high. If thnre are = grams of a paramagnetic in the line, the highest
energy that can be absorbed by it in a time smaller than the relaxation
time T is equal tot U (NIA)(gp2H2/kT)m (9). If the pulse duration
0
r (TO, the pulse output in W w UA which causes the saturation of para-
Mgnetic resonance. To avoid this, W must be less than U/T. A ferrite
can also be used, but it has the disadvantage that there is a non-
resonance change in the lose due to the change of the constant magnetic
field, Perrites xor which this is not the case and which have a narrow
resonance line can replace paramagnetics in the region 1>3 cm. Four
MSA circuits were investigated. The first works on the principle of
compensation at low and high frequencies. Two similar lines containing
a paramagnetic are used. The second work* as a discrete 'Oresonance"
The third is a spectral anjilyzer which uses the in-
duced radiation for tive-1-amplif icat ion of weak signals. Finally, the
fourth is an induction USA. Measurements were made of the damping
L Card 3/4
-W M, R
T_V'R~PTZ' M-F~F z IM"?

20452
8/056J61/040/002/005/047
Magnetic analyzers of*.. B113/B214
factor bf the line, of the non-resonant loss in the paramagnetic, of the
sensitivity of MSA, and of the dielectric constant of the paramagnetic.
The compensation principle of the MSA was also tested. Also the para.
magnetic resonance curve of MnSO4 , shown in Fig. 30 was recorded for a
rate of growth of the magnetics field dH/dt - 2-5-10 9 oe, For a trans-
mission band'of-the amplifier of 2 Me/see, the measurement of the
sensitivity of USA gave the result 10-9w. Experiments with ferrites
showed that they can be used in 11SA. It ist thereforet possible to use
the phenomenon of magnetic resonance for static and dynamic analysis
of the radiation of a wide range of waves, where MSA can be used best
in the millimeter and sub-millimeter ranges. Academician A.Ye.Arbuzov
and Professor F. G. Valitova are thanked for the preparation of the
diphenyl-picrylhydrazyl preparations, and Profescor S. A. AlItshuler for
discussions. There are 5 figures, 1 table, and 2 refereAcest I Soviet-
bloo and I non-Soviet-bloo,
OUBUITTEDt July is, 1160
i; 0 41 V 15 y 0 1: 41
Card 4/4
Lq
3F; M r4Q~

S/05 611041100210241028
B125YZ138
AUTHORS: Bartov, A..V., Zavoyakly, Ye. K., Frank-Kamenetakiy, D. A.
TITLE: Magnetoao0ustio resonance in strong magnetio fields
PERIODICAL: Zhurnal eksperimentalfnoy I teoreticheskoy fiziki, v. 41,
no. 2(8), 19619 588-591
TEXT: The authors put aside the previous limiting condition W 2 in
-0
-1- th f
order-to study the-possibi i y o --- e--ocourrenoeo resonance p enomena,
----of the-magnetoaooustic type in a-plasina with-a-concentration variable-in-
time.- They study the case where the plasma frequency is of the same
order as, or less than, the eleotronnyclotron -frequency. Here,o) e
denotes the electron cyclotron frequency. This case occurs either In a
rarefied plasma (low plasma frequency) or in very strong magnetic fields
(high cyclotron frequency). A plasma with a cyclotron frequency higher
than collision frequency is said to be magnetized (with regard to
collisions). If the cyclotron frequency is higher than the plasma
frequency, the electrostatic oscillations will be magnetized. Such a
Card 1/5
i

27202
S10561611041100210241028
magnetoacouatic resonance in strong.*. B125/B138
2/W2 XnMC2/u2
plasma shows oscillatory magnetization. Then, the ratio Wo e- 4
is about the same as the ratio of electron rest energy to magnetic energy.
Thus, a plasma with magnetic energy higher than the.electron rest energy
will undergo oscillatory magnetization. In a rarefied plasma, the
resonance frequency.of magnetic sound will, with a purely radial
propagation, approach the loWbr hybrid frequency, The following general
expreesion for the lower hybrid frequency is derived:
j + 4),U)
lu 21. OW 0 0 0).
h 1 2
0 0
The approximate formula derived by D. A. Frank-Kamenetakly (ZhETF9 21o 6699
2 2
1960) holds for Wo,"Wi0e. When tj" the lower hybrid frequency tends
0* loot 2 2
towards the ion cyclotron frequency, and when or~~W 9 towards the
0 a
geometric mean of ion-electron the cyclotron. There is a wide interval
2 2 j in which the approximate formula for the lower hybrid
we Woo ), 4), We
Card 2/5

27202 :S/056/61/041/002/024/028
Magnetoacoustic resonance.in strong... B125/B138
frequency re ado tj2v W2 ~j/(.) (2)4 Herep the lower hybrid frequency is
proportional to the plasma frequency. Ata given magnetic field strength
(w0 0, const) the resonance frequency of magnotic sound decreases with
increasing a0incentration in a donee plasma and increases in a rarefied one.
In botmedn, it should paon through a maximum. If the maximum is flat
enoughq resonance may occur.ovora wide.range of concentrations. Tho
dispersion relation
big' + b3Q3 b2Q* big b0 --'0-:, (7)
b4- 3A + B + 2R (I + ctg2 0).
A2 + 3AB + Bs - 12A + B + R (I + cjg2 0) 11,
b2 = (A + B) R + R (I + Ctgl 0) 12 - AB (A + R),
bi - AR 1A +-R. + BR dg- 0 (1 + Ctg 0)
bo = ARI ctgl 0 (1 + c1g2 0).
defi nes the-d imeneionless frequen 2 i~). Neglecting all
cy, W A) 0
coefficie nto except b2 and b,, the following approximate formula is
Card 3/5
A I
-7 -1 -1

S/056/61/041/002/024/028
Magnotoacouotic resonance In atrongooo B125/B138
.2 BR 2
obtained where cot ge.1 +I-+ + 'I + i) (8). The
'a cot I R A
formula corresponds to the "long cylinder approximation". In these
formulas,-A utjo/~io' (4) indicates the equare..of the Alfvln,index of
refraction; B to) /W is the ratio of the cyclotron frequencieel
R 22/(Zi t) M 21.
8 r r -k
ki0 ki i Is ; tang I/k Here, &J,is resonance frequency; Wc is
3' 1
asm-a-freV"mayT-w-aix4-"r4-th"leotron-&pd~Liori-cyaI tron-ayal-ic
0
s
frequencies;- k and k are the -radial -and the longitudinal wave numbers;
3
r Iand 'r the-eyolotron' radii at.the velocity of - lightj and O(Q~Cn/`2.
e
Under the usual experimental conditions, the I'lon cylinder approximation"
is satisfied with sufficient accuracy. When 9 wn721 the maximum in this
approximation lies at A - ~BR, and the maximum value of the dimensionless
frequency is VB-R/(2B +Jik) (9). The position of the maximum is only
slightly shifted, whereas its hsight~increases considerably. The authors,
investigations are of great importance in the interpretation of
Card~ 4/5
771

.2 710
S/056J61/041/002/024/028
Magnetoaooustic resonance in strong... B125/B138
experiments on magnetoacoustio resonance under non-linear conditions,
There are I figure and 7 references: 4 Soviet and 3 non-Soviet. The
reference-to the En-glish-language publication reads as follows: P. Auer,
H. Hurwitz, R. Miller. Phy3. Fluids, 1, 5019 1958-
L
SUBMITTED: March 16, 1961
Card 5/5
M . . . . . . . . . . . . . . . . .
Asia.
R
.0 581

BABYKIN, M.V.1 GAVRIN, P,P,; ZAVOYSXIYO YeA.1 HUDAXOVL-1-----MQr1YUP11t---v A,-
Turbulent heating of a pla3ma. Zhur.-eksp. i toor. fig. 43 no.2.-
43-1-421 Ag 162. (KM 16:6)
(Plasma (Ionized gases)) (Electromagnetic waves)

UBYKIHP Ma.; ZAVOYSKIYI U.K.; RUDAKOV, L.I.1 SKORYUPINt V.A.
Observation of a double-flow ion ivAabilit7 in turL-ilent
heating of a plasm* Zhur. eksp. i toor. fiz. 43 no.5:1976-1978
N 62. NIRA 15:12)
(Plaama (Ionizod gasea))

5/089J63/014/001/007/013
B102/B186
AUTHOR., aVOYBkiY, Ye. _K-
TITLE: Collective interaction and the problem of producing high
temperature plasma
PERIODICAL: Atomnaya energiya,.v. 14,.no. I ,1963, 57-65
TEXT: The author gives a review of the present position of theoretical
and experimental investigations into the mechanism of the turbulent
heating of plauma. The mechanism depends on the'fact that a large part
of the energy from strong electromagneticoscillations is absorbed by the
plasma through a kind of resonance absorption. As a consequence df the
collective interaction there an energy d1ocipation occurs and the plasma
electrons become strongly heated. According to a two-current mechanism
e 1b-ed-b"-i-B-.Kadomtzev_the ene -r-gy- o f-the e7.ectrons can be transferred
to the ions. The following problems. ~re treated in detam. Th-e-zbm--
ditiona for the build-up of eleatron oscillations in the plasma, the-.
build-up of ion oscillations, the pinch effect in a turbulent heated
plasma, experiments relating to collective interaction. The results
Card
-it !XMkkM

-S/089/63/014/001/007/013
Collective interaction and the !D102/B186
given here were already publiahod.by: ?L-V. Tlabykin et al (IAEA Plasma
Confdranoe at Salzburg, 1961,1 Paper 209; Zh ' ek erim. i iqor. f iz. v 43,
no'.2(8),411 1962; 5:1~62 A.-Ved~enov, Ye-. P.
01962;'43,4,1547, '43 5,1 ~71
Velikhov,-%,qe,.Sagdeyev (Yadernyy sint~z (Nuclear.o~ntheais),I,82,1961)),,
B.B.~ Kadi omt ev (Sbornik "Fizika plamy",("Pla'sma Physics"), v. 4 t M. Izd-vd
AN SSSR,*1958,P-364); D.A. Frank-Kamenetakiy, (Zh.eku~er. i teor.fiz-39,,
669,196o), [Abstracter's note: cf also Vedenov)'Velikhov, Atomnaya.
energiya-13, -pp- 5-24, 1962 and i)AIT 146, -1, 65, 1962-11
SUBMITTED: October 15, 1962,
Car(] 2/2
R LK 7 1 -

-KAPMLqOV- F.-V.;
MAKSIM07j, Go P.; CHMOWKH, P. A.;'
SILUMN) V, V.
The experimental plasm apparatus C-1 with screw magnetic
fields. Atom. energ. .14 no.22143-150 F 163.
(MIRA 16:2)
(Plasma(Ionized gaves)) (Magnetic fields)

'I,
. , ; i4
- *~~ -
n"no, N"Ell-MMIM 4-n-IN, ww~mz au 7A .

n
;W zwlj~ I I
AC Mi AT6001404 SOURCE COM tflt/3180/64/009/000/0175/0183
_~~AUTHOR:---Bolotln,-V. F-,-Demidov.- D. A.;- Zavo nk Ye_. -K..- $knchlcova Yuj F,,,
SmolLf~, G, Ye. - Fftnehenko, S. D.
ORG: none
vj "Ol,
TITLE: Flurther development of the clectrooptical chronop
~aphic rje h2, and Its application
to physical plasma investigations .,, u,~i,
SOURCE: AN SSSIL Komisslya po nauchn f6t9gr atografil, Uspekht nauchnay
_f.__tF _64~7 a
Vy-kk6a wos nay,
fotolTaffl, 'D fotogrftflya 0it a (Ifigh-speed photog-
-raphy and cinematography), 175-183 and Imiert facing page 169
TOPIC TAGS: time measurement, electric disclLarge, electrooptic image Intensifier, plasma
diagnostics
ABSTRACT: It was established earlier thatt the multistage electrooptic converter invented by
Prof. Al. M. Butslov has a limiting brightness.aniplification coefficient which allows it to
register single photons Micorctical disctuisions t;howed that similar setups can have a re-
solving time down to I all see and some spark radiation ticanning experiments achieved a
resolution of 3. 10-l". This led to Vic use of similar devices in clectrooptical chronography.
This article surveys tJio principlus of operation of electrooptical devices and the reau JLq of
plasma Investigations using clectrooptical chronograph The authors cover J) the method-
ology. of clectrooptleal chronography, including power lAding and synchronization of multi-
stage clectrooptical converters and time scanning of converted images; and 2) physical

f,_37-662-66
ACC N1,
AT6001404
studies of the plasma Including processes In spark discharge plasnian (circuit and block
dfagrmns of setups for time scanning, spark channel widening velocity data), use of (Acctroop-
tical chronography for the study of 11F-fleld interaction with plasma (block diagram of a de-
vice for the study of plasma luminosity during magnetoacoustic resonance), and a brief dis-
cuselon of special features of clectrooptical Investigation of p1w9mas. A resonator for the
scanning systems was proposed by R. V. Childn of the Butalov laboratory. OrIg. art. ban:
11 figures and I table.
SUB CODE: 14, 20 SUBM DATE: none ORIG 1W, F: 015
2/2
J~Card

IACC 8/0056/64/046 /002/(1511/0530
-ESSION NRi AP401921
-:AUTHORS: Baby*kin,, M. V.; Gavr1n,,P. P.; ZavoyakirtzYe. K.1 Ruda-
V, ---- ---
-.-kov, L. I.; Skoryupins V. A.; Sholin, 'G.
TiTLE: New results o*n the turbulent heatIng of plasma
eksper. I toor.-Siz., v 46 no 2 - - 2964 - 511-530
_-TOPICL-TAGS: -plasma,, plasma heating., turbulent plasma, heatings plasma
eleptron heating, plasm-alon heating collislonless plasma heating,
plabma confinement, plasma confinement timev electron confinement
___---t1me,,-Ion confinement time
ABSTRACT: This is a continuation of earlier work by the same authors-
on turbulent plasma heating In a rapidly alternating magnetic field
(Yaderny*y sintezp Appendix 111,,,1962; ZhETF v 439 pp. 411,, 15.470
and 1976, 1962). The present paper reports theereaults Of ex Im ts
08 Ibl feT en
with a net netup, the paramettrs of which have made p a e I
rapid collinionless heating of the plasma electrons to 1.5 keV by a
strong nydrodynamic wave propagating in the plasma transversely
Card

.-',ACCESSION NRS AP019216
the magnetic field; (2) investigations of the confinement of
a plasma in a magnetic trap; '(3) observations of the c6llisionless
heating of ions) which accompanies the turbulent heating of the
electrons under certain conditions. The electron temperature was de-,
termined from the absorption of the electron bremostrahlung in thin
carbon films, from the ratioiof the rates of decay of various spectral
lines, and from readings of a probe. The plasma concentration was
determined by optical means. The noise producedAn the plasma was
due to ion cyclotron oacillatigps and to mAgnetic sound resonance. A
plasma electron pressure of 101~1 eV/cmJ (approximately 20% of the
alternating mg! �netic field pressure) was obtained In the concentration
range from 101 to IOIJ/cm3, Confinement times were-130,gaec for
100-eV Ions and^j60 Asec for 590-eV electrons. No strong Instabil-
ities were observed during the time of plasma confinement In the trap.
Ion cyclotron waves and natural oscillations of the plasma column were
Card 2 1 , .
Al

I;R-M4*19216-
iACC
bbserved. A theordtical MeChOnism is proposed for this electron
heating and is found to agree qualitatively with experimental results.
Q'~ig. art. hae: 17 figuraa and-10 formulasi
4SOCIATXON3 None
A.
13Aug63.'
S7MITTEDt DATE ACQ: 27Mar64 ENCL: 01.
SUB COM PH NO REP SOVO 008 OTHERs 002
!Card 3/4

ACC NR' AT7008874 SOURCE CODE: Ui~ 65/66q/6o6/ooTj/6ooa
AUTHM: Zwiyoki7, Yo. K. (Ac~adordlcian)
ORG: none
TITLE,: Progress in plastra studies
SOURCE: Pi-oble-my temoyadernykh issledovaniy,.1965, 3-8
4 PIC IAGS: plasma heating, plasma Jet, plasma oscillation
SUB CODE: 20
AT--5Ti="T: The advances in understanding of thet"o basic unre-
solved problema of plasma physics - the heating of plasma and the
are d1scuaced
containment of such plasmas within a given volume'
on an alementary level, Tile first npparont stumbling block has
beer. the need for extremely high magnetic fields (about 100,000
oerateds) to keep the I billion-degree plasma from leaving the
magnetic trap. In addition,, the proceso of heating the plasma
seemed to deform the trapping maSnetlo fields$ leadlru& to an cc-
Cape of plasmas, The first hope of plasma stabilization appeared
when it was discovered in the Soviet and US laboratories that
small admixtures of cold plasma stabilized'the so-oalled channel
Instability# The next*otep was In the direotion of plasma heat-.,
Ing-by means of clectron jote.whioh, upon entering tho planma#
o;;,;~117atlona and oauao the turbulont heatInS of
Card 1/~_-

ACC NR,
-AT7008874
This heating seems to proceedduring oueh short inter-
plasma.
!-vals that the plasma does not have time, In spite of its high
,temperatureq to escape the magnetic trapping field. It Is clear,
however, that all these advanoev z4ofer to experimental apparatuses
!which are ntill very small as compared 'With those needed for car-,.
~:rylng out tents which would be of praotical interest. Further
'progress may come only after other large-soale preliminary Invos-,
1tigationa'conducted basioally at the aolentiflo-ronearoh level
'rather than in the domain of engineering applicaiions. Orig. art. has: 1 formula.

-- - _r
-7
ACC NR' AT602-1838 (h) ---i OUR-CE- CODE-t- U'R/606-6/65/000/000/0100/0108
AUTHOR*, lavonkib V. K.
ORG: All-Union-Polyteobnic Institutes Moscow (Voesoyuznyy
politekbnicbeBki,y institut, Moskva)
TITLE:~ Heat transfer in a iquid
3OURCE#.- Teplo--i massoperenos, t, III: Teplo- i messoperenos pri
fazovykb prevraebobaniyakb (Heat and mass transfer* V, 3t Heat and mass
transfer in phase transformations). Minsk, Nauka. i tek6nika# 1965,
100-108
TQPIC TAGS: beat transfert boiling
ABPTRACTi In the most Eeneral form of the problem, the heat flux can be
deioribed in tbe foll.owing manner:
q(Q= N(Q dv rj(j (R, Q dR. (1)
wbere is the density of the vapor; f is the distribution function
of the bubbles, It is evident from the above that to determine the heat
C.rd 1/2

-7-7 L 40883-66
ACC NRI- AT6021638--- - -
flux it 18 necessary to know the rate of growth of a vapor bubbla, the
distribution of the bubj)les, and their total number, The article next
considers the growth of an ensenble of vapor bubbleoo and derives the
corresponding equations, Finally, the author proceeds to the
determination of the beat transfer coefficient, making use of the
following basic formulation -of the problem:
k. q (6)
SIAT
wbere'3" is the.total pbase separationsurface, and k is the heat
transfer coefficient from the liquid'pbase to the vapor phase, Origs
art, base., 9 formulas and.3 figures,
SUB CODE: 20/ SUBM-DATE: 09Dec65/ OHIO REFr 007/ OTH REF1 003
I Card 2/2 fi9Z oP
------- dd

?..AV(,IYSKIf, Ye.K., akedomik
-c -)
I I F,!-~ t r~r- a*' :j: -, ~ ' ~ -a - --:~ - p '- * - ' :? -"7 ~ f '-,- - ~ ~ ' 1 ~ x., f : e .
- . . - 'R I I

ZAVOZIN L., izoh.
"For tbo operator of mirA electric locwotLves*:b7 Z.A.Vasillev.
Roviowed by L. Zavozin. Sov.shakht. 10 no-4142-.43 Ap 061.
(MIRA 14:9)
(Electric locomotives)

KARATYGIN, A.M., kand. teldin. nauk; KORSHUNOV, B.S., kand.
tekhn. nauk; MASLOV, Ye.N.p prof.., doktor tekhn.
naukt retsenzentj ZAVOZIN`,.L,F.,.inzh , red.;
IVANOVA, N.A., red.izdva; ELIKIND, V.L., tekhn. rod.
(Grinding and lapping metal-cutting tools] Zatochka i
dovodka rezhushchego instrumenta. Izd.2., peror. i
dop. Moskva, Mashgiz, 196.1. 270 p. (MIRA 16:12)
(Metal-cutting tools)
(Grinding and polishing)

A,STRAK.HANTSEV, Vaniamin Ivanovich; ZONOV, B.V,, otvared.; ZAVOZIN, L.F.,
red.; LAUT,, V.G., tekhn.red.
[Anga0ra and its basin: t1ins I gy-I.Angara- I- so-,
-of-'he-by#o _o
_~:Wsisoior,4idrologichoskii -ochiirk- ___R6skv&- .1%dr-vo- Akad uk
SSSR, - 1962 - -90 p (Akad6miix- ;;Wk M.M.'Sibirsko na
0 otdolenis.
Vostochno-Sibirskii geologichaskii institut. Trudy, no.12).
k - (IURA
(An&ra Valley-Hydrology)

F "AU CH
J HA
-711,~~~-,~~,~,~Fe-.-~r~--~-f~-y!~~F.,~7~~-.Fll~,i~L:~,~4i~I ~-~W_94 iflE'
im

ROZENBUT, Grigoriy BorlsovIch.- PODPRIJZMIIKOV, Vesilly lvanovi!~h;
KICHKIII, VIA-tor Vasillyevlch; LORASOV, Mikhail Petrovich;
KAIMI 111H, Aleksanir Nikolayevi-b-, ZAVOZnl, L.F., ved. red.
[The UB--2in K~a~--!)pef:d L)Jnw~ ~~istrokhodrmifl struglovaia ustFl-

BOLISHAKOV, A.G. , inshener; ZAVOXIV- rodaktor;- IJOW(RIVAi- XiAo p 4A
~- ---: - - - -,- 0 -- -
- -U~ -~4~ N!
fekhnichaskly redaktoic.:WK, .1,"w -- W:4
Illectrician in.coal preparation and briquette factories] Xlektro-
slasarl ugloobogatitel'afth I briketnykh fabrik. Koskya, Ugletekh-
Wat. 1952. 239 p. (Microfilm] (KLU 7: 11
(Ilectric apparatus and applianose-Raintenance and repair)
A
(Coal preparation)
Z

BCDITWO, at redaktcr; ASTAKROV, A.Vs. redalctor;
ILOINSKATAi-7F.-N..-takhnichookir redaktor
[Reference booklet for operators of mine pumping Installations]
Pumiatka dlia*machinista shakhtnoi vodootltvnoi ustanovki. Monkva.
UglotakhWatl, 1954s 53 Pe (MLRA 8:10
(mine Pumps)
:~g-- x. g ~gg~p

em
ZAVOZMI L.F.j, DIYAKOVAq G#B*q otv-rades SlIELYAR, 8- Tas, teldin.rede
[min-0 hoists] Shkhtnyi Dod*em* Monkvn, UCleteYhlzdat* .1958. 74 p.
(Mining machinex7) (MIRA-11:9)
p~
Pik II fS, IN, 91 aw

IVOTSOV. Yevganfy 1111ch-
L.r.. otyatstvamwir rodaktorl ASUMV,
-4-'AUDOTA, YesX., takhnIcheekly -
A.Y., redaktor it v&,
-rodaktor
[The bilge pum'p operator] Mashinist shakhtnogo vodootliva. Hoikva,
Ugletakhtsdato l956. 155 P- S7)
(MU4 pumps) (Nicrofilml

ZATOZIN, Loonid,Filippovich; DITAKOTA, G.B., red.izd-va; BEKKZR, 0,G*#
takhn.red,
(xina-hoisting machinery] Shakhtnys poedwemnye ustanovkI.
Moskva, Goo.nauchno-takhn.izd-vo lit-ry po gornoun delu, 1960.
357 P. (HIRA 13:7)
(Fdne hPisting) (Hoisting machinery)

ZAVO Ani inxho
Schield timbering ("Powered shield supports are the baste of
efficient coal n1ntne by r.R.Xratenko. Revlew&i by L.9avoclo).
Kast.ugl. 9 no.12-.20 D 060. (HIRA 13312)
(Mine timbering)
(Kratenko, 1.14.)
1