SCIENTIFIC ABSTRACT FR:BEREZINA, G.P. TO:BEREZIN, Y.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000204800010-6
• Release Decision: RIP
• Original Classification: U
• Document Page Count: 7
• Document Creation Date: November 2, 2016
• Sequence Number: 10
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTR

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_.__... _
ACCESSION NR: AT~+036o~y~ Er;c~.osu~ : 02
Legend to Enclosure Ol:
~. -electron gun cP~amber, 2 -cathode heat~.ng, 3 -cathode past,
~ -cathode, 5 - sellenoid for focusing 1on~itudinal magnet].c field,
6 -tube for produe;ing pressure drop, 7 - .plasma chamber, 8 -
bellows, 9 - mechan],cal leak valve, l0 - i retarding field ~ analyzer,
11 -second analyzer grid, 12 -third analyzer grid, 13 -Faraday
cup, 1~ -entrance flange for measurement of the beam current,
l5 -vacuum window for pumping our- tr,e plasma chamber, 16 -
nine cells, ~17 - lj.ne supply, 18 ~ to oscilloscope, 19 -water,
20 -pump, 21 -filament transformer, uiF{~ - microfarad, KOM -
kilohm, OM -ohm,
4
o~r~ 5~5 '
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ACCESSION NR: AT~�o3so~9 ~tlct,osUx~ ~ 01
+ Ge~iera~. diagram of set-up ~ ~ ~ ~~ � �~0p3 V ~ � ~ �
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ACCESSION NR: c,AT4036049
phase velocities which ,are smaller than tho velocity of light in
' vacuum, and have intens;Lties which reach 50--60 kv/m at the end of
the interaction, region. A small group of the electrons (1--4/ of _
.the total current) expe::iences an increase in energy up to 50~.
If the electron beam is initially modulated, it:~ frequency experienc--
~es a Doppl�r shift at tl~e end of the interaction. Orig. art. has:
7 figures and 5 formulasc .
ASSOCIATION: None
SUBMITTED: 00
DATE ACQ: 21May64
ENC~,: 02
SU$ CODE: ME
Card 3/S
NR REF SOV: 016
OTHER: 005
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ACCESSxON NR: AT~036049
'under which oscillation~~ are excited, the frequency spectrum, the
amplification coefficients, the character of instability, and corn-
, parison of the experime~~tal data with the theory. The electron beam
~; had an approximate ener~~y 15 keV and a current 5--8.5 A. It was
,injected in a quartz an~~ glass plasma chamber, ionizing the air in
it, producing a plasma, and interacting with the latter. After
passing through the pla:~ma the beam was electrostatically analyzed. '
.The procedures used to measure the various parameters are described, ,
The experiments have shown that the beam loses an appreciable part
of its initial ener ~� ~ ,
. gY ~ 18~)� This energy is consumed in excitation
of oscillations and heating the plasma. Some 50--609 of the ener
gY
;loss goes to excitation o~ longitudinal space-charge density waves
,and transverse electromagnetic oscillations; this agrees qualitative-I
ly with the theory, rt follows from the measurements that the am-
' plification coefficients and the maximum resonant frequency are also .
in satisfactory agreement with the calculated data, The longitudinal
space charge density waves excited in the plasma and in the beam have
Card 2~5

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ACCSSSxON NR. AT44364~9
s/27.s1/~3/000/443/ol2s/ol3a
AUTHORS: Berez~.n, A. K . J Berexins, G. P.1 Bo~.oti.n, L. ]:.; Lya,pkalo,
Yu. M.; Faynberg, Ya. B.
TxTLE: Interaction of pulsed high-current electron beams with a
plasma in a magnetic field

t
SOURCE: Konferentsiya ~o fizike plazmy* i problemam upravlyayemogo
termoyadernogo sinteza. 3d, Kharkov, 1962. Fizika plazmy* i prob-
lemy* upravlyayemogo termoyadernogo sinteza (Plasma physics and
problems of controlled thermonuclear synthesis); doklady* konfer-
entsii, no. 3. Kiev, I:zd-vo AN UkrSSR, 1963, 125-138
TOPIC TAGS: plasma rep-laarch, plasma magnetic field interaction,
plasma wave absorption, plasma wave reflection, electron beam, mi-
crowave plasma, plasma electromagnetic property
ABSTRACT: The investig~~tion reported was aimed at d�termina.ng the
energy losses of abeam passing through a plasma, the conditions
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r
~, A.~.; .1+I~1,_..~ ~QLOx'I~1, L# ~.; 8g~1~Rti, Ye,.~.
In~ract~c~ betwee ~ pza~s ed heav~rrea~t beams a~.d s playa ~n
!~ lt~ggetiQ fiRlldr +~.~11~lI`gr ~ 2~a.~t24g�~2.~jb I~r '63.
~MIRA Y~~2~
~~evtarcm beane~s ~ Q~Iasma ~~anized gases a a
~et3n f~,elds~
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yt
i..
~. ~ ..
3~05~62~032~005~014~022 ~
The passage of~intense... $104 8102 ~
'4
longitudinal "sagging" of tho potential ooours. At tho Dame time the j ,
seoondar~y elea,~rans return to tho axis of tha tube. On account of the ! ,
"sagging'" of the potez,tial thane electrons are accelerated in the direction' ~
of the analyzar and a]so in the direation of the wiode. The energyr of th�~
slarl eleotrons is dat~~rmined by the amount of Iangitudinnl aa~;ging. The
energy is praportlonaJ, to the aurr~nt atrangth and rho valooity of the
eleotron boom. The 1t~ngitudinal nagging is perhaps largest at the instan4 ~ 1,
when the current density attains its maximum value, and probably at this
same instant the aace~,erated electrons have their maximum energlr, With ;
inaraasing oontractio-I of secondary electrons at tho axis there occurs a ~.
nevr density distribut'.,on. mhe beam of the secondary electrons begins to
broaden, and the sagg;,ng deoraases. The density and the sagging ohang� e-ora ,,,~
rapidly with inoreasi--g pressure. K. D. Sins1'nikov and Ya. 8. Faynberg
arA thanked Sor disouneior_s and advioe. There sre 9 figurers. ~
:-SSOCI;~TIOIt~ Fiziko-~;ekhnicheskiy inetitut �I+i II89R Kharkov (Phyeioa~ � J
teohnior-l Institut0 A8 UkrBSR, Kharkov) ~ ;.��;
Si38~tITTED i
Card 2~2

Juno 17, 1g61
't:�~
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.-._ _ __.
~,
i~*i .
9.3!30 3`"~;'" _ _.~....
~.~ ~?Ib ~ ~ o4~/Gz~/032/oa5/ova/ozz M{
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AUTHORS; Berezin, A. K., Stupak, Y. G., Bolotin, L. I., and ~
Berezina, G. P.
TITLES The I,assssge of intonso pulsed eleotron banma through
dieaaotr;,o tubas. ~~
P~RIODIC,~Ls Zhtirnal ~,ekhnioheskoy fiziki, v. 32, no. ~, 1962, 600-605
2'~nT: The ener~,y spew;rum of 35 kev elaotronra fn quartz and glass tubes i ~!
of diameter 9 mm and l~rngth 60 snrq waa osoillographed with tho hole of an ~
electrostatic analyser (angle of aperture 20). A group of slow and another
� of fast electrons (35 lcevj were observed. .1 study was made of the ~
behavior of these grou;~a in their dependenoo on the beam enorgy, the current
strongth, the pressure of the rosidual gas,. and other faotore. Tho
following aonolusion�i,a drawn from these abaervationss ti~hen the pressure
� in the tube ie above a critioal pressure, ions and slow secondary eleatrons,
are generated by the elootron beam in the tube. Tho ions are trapped near `
the axis] and the electrons travel to the wall. 6t a certain instant '
reneutralization starts. The eleatros~ beam oontraate and a radial and
Caxd 1~2 ' �_
r
~r

..~
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.It ~
The passage of intense pulsed... a/~57/~2/o}~/ao~/o~3/a~,~ --:
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AssoczATZON, r .,
izika tekhniaheskiy in$t~.tut AID USSR Kharkov
(Phyeicotec7nieal Institute AS UkrSSR, Kharkov}
StTB,iTTTED: June 17, 19~i1 '

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The passage of intense puled... ~/~57/G2/032/OG5/n"1,x/022
B104/8102
electrons travel towards the wall s.nd the zany collect about the ~~xis of the
tube, t"+ith progressive formation of ions the electron beam i;a foc~xsed and
after time t ~ ~ the current attains a maximum va.l.ue at the exit of the tuba.
ds the electron beam eantraets towards the axis of the tube so does the
rep:-~on of xon formation. ti~hen the intensity of the brim bacomsl~
suaziciently largo, the number of electronq produced exceeds that Lost by
~ diffusion towards the wall, recombination, etc. Then reneutralization
starts, and the radial elec~wric field changes si~,ms. The electrons travel
to:~ards the axis of the tube and the space charge inside it becomes
differently distributed. Apt excesr> of negative space charge is formed at the
cantor and the current throltgh the tube begins to decrease, ~t a pressure
af�3.6.10'~ mm Hg the current strength of a pulse decreases by about 20 �o
during the duration of the ~~ulee; at a preasure of 8 10 ~
is t3O ~o. The current pulse passing through a dieleetric'~tubc;H~sthe decrease
larger than that through a copper. one. Nith the help of the facusingtimes
pranerties of a dielectric tube deaeribed mere electron beams may be
"canalized" over large distances. There are 7 figures.
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~ ..
AUTHQRS: Berezin, A. ~., Stupak, V. G., Bolotin, L. I., and
Berezina, G. ?.
~,.,..,.,..,,...,,..w.w......,.�..~.._E_.... ..T.. _
TITL~s The passage ~f intense pulsed eleat;ron beF~r~g thz�or~,~h
dielectric plpss. T '
P%RTGDICALs Zhurnal tekh�icheskoy fiziki, v. j2, r~o. 5, 162, 5`~~->~~
TvXT: Tha cathode of the r~lectron gun was a tungsten spiral 16 mm in
diameter. The pressure in the vacuum ahttmbe~r was 3.10--6 mm Hg, St was
possiblQ to produce 50 kev electron pulses with et current dens~.ty of up to .%'
1 a~cm2, duration of the ptiil,ses reaching ~.6 j~ec. The dielectric tubs
(quartz, glass) had an innE~r diameter of 8-10 mm and the pressure inside it
could be varied between 2.10-4 and 5.10_2 mm Hg. The electron density of
a pulse tivas measured by an shf rnethad while the size and the shape of the
electron pulses veers ascil~ographed. An intense electron pulse broadens an
account of the space chargE. At the same time the electran pulse i.ona.zes
the residual,gas creating positive ions and secondary electrons. The
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s/12o/62/000/002/031/04?
E14o/E163
AUTHORS: Berezin, A.K. , fitM.palc, V.G. ,,,,~,;re,zine�.~�~Fr;.}~,-..,,.
Bolotin, L,X., Lyapkalo, Yu.ri., Solopikhix:, D. P.,
and Bondar~anko, V.P.
TT'fLE : High power electron gun for operat,i.on under
difficult ~racuum conditions
PER3oDICAL: Priborry i ~.ekhnika eksperimenta, no. Z, 19~;3, 13d-138.
TEXT: An electrons gun is described giving 20 A at 25 kV
in a vacuum of 5 x 10"~~ nun Hg. Ths~ cathode is a cylindrical
tablet of lanthanum he~;aboride, vacuum-sintered, and located in
the homogeneous region of the focussing magnetic fie~.dp
A grid-form anode is u~~ed, resulting in a smaller deforusing
field than the more usual pierced disc {Fig.l). The tz~amaparency
of such an anode is al.~o satisfactory. The anode mesh is of
tungsten wire 60 ~, diameter with a pitch of 1.5 mm. In plasma
interaction experatment~~ the gun was used for several mantkzs under
continuous evacuation t~rithout replacement of any of its parts,
There are ~ figures.
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Passage of intense pulsed~U~
~-3 ~ ;~
Si'Q5716 ~ ~ 0 3?; a~6,''~ ~ 7i'O~t ~
spectrum until the iaai.s,l. f1F~jd has ch~.nged its :;:~gn$ ;,,r,y n~,t ,,,nti.l the
electrons star+, m,~va.n~; from the tube wall tr,Trrard the b~aaru axis, The results
presented in Figs, 1a, Abp 1r, have been obt~.~ined, under th.~ fnll, .�.
d.itions s val tare of ttie bean , ~ ., ~ t n~ con.
35 kv, beam ~~u.rtenty ~~~~~ tt, ~res~tzr~~ ~za the
cha,mber~ 3~6~~Oo'4 mm fiq~., It i.s final.l ~ai.ntQd cut t;r,-~t ~,
experl.ments described here alas the ener.~ r, t11F~ r!;u.rse o.f
function of pre9sure. by sp@ctrura a.f' s1.o~r ~~lec~rons as a
intensi t~ ~ and velocity a.f the p~rzu~a.r.;~f r~l ec trop beam has been
has been determined exprrri~nc~ntally ~no deta~.ls~ ho~~ever4 ar~~ L~v.,n).
CAbstractex o s notes Eseenta.a]. Ly complete transl.ati.on�-~
and 3 referencesA l So~;-:iet..~b,~o~~ rind ~ non-St~v:ist.,.l,lrac~Thera ~:r�e 4~ i'z~~~r.e4
ASSOCTATTON~ Fj.ziko~-tekhn:iclieskiy instl tut AN USSR Khar ~kov (Ins+ztute of
Physics and Technology� ~,$ ~JkrSSRy Khar~k~,~_~l
SUBMI~`r>~n ~ Docembex~ 3t~, i I~Q -
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X3733
Passage o;f intense pulseda~o ~~o57,hf~03?~006~017~0?g
B116I8201
current Tp was mounted on thfl quartz tube The signal reaching the ring was
differentiated by an RC c.irci;,it and fed to the Gseilloscope, One t
osei.ll~grams is shown iti Fagg 1ba Tl~e negati.v~e half-wave fin, the ~~scillo-~
gram corresponds tG the motion of secondary fans tawar.d the wr:..1 J, art.d to the
capture of ions near the elec tron~~beam axiso If "a'vernputra.l..zat iax~" takes
place in the beams the e:l,ectric field w~.ll change i ter sign and the ices due
to diffusion and other factoz~s~ will start moving tniv~~rd the wal 7 , wi7i.] e? +,he
secondary electrGns migrate to the beam axi:~~ The pc,;;.iti~re h,a.1s'-v;avn can the
oscil.logram corresponds to this condi,tiono
passing through the quartz tu'~ey measured w~.t~h~theeelgectrostat~r~oi~n~l.ec�,rons
permits distinguishing two se Karate elpct.t*on groups, i ~ e ~ s ..Y2e,ry
electrons and a group of s.l.ow plect.ronso groin, ot` fast
electron beam i4 allowed tG p~~ss through alinetaldtubPh�~thame cUndr.t~iun~,y the
usual consist of fast e~,ectrc~ns Gn.lyU lixper~1ment~s hI to e
the electron gun unward~ The moment a't whl,ah glow cl.ec�rc,zls appe~~~~.~t the
analyzer output as a f.'uncti.an. of the~..r enexgy is p.z-Nscn!ed ~n Fi.g. i G.~ As
may be seen fxom Figso 1 b and 10 o s:l.c~w e.Iec trorrs do n;ut appes,r in. the energ
Car. d i~~ ~ y

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' ~~~~
5~057~61~031~(}O~~017~O1g
Passage of intense pulsed,no P116~B2O1
tude of the time required fir complete neutralization of the be~~m), they
will return to the electron-beam axis Both the radial and the iongi.tudinal
component of the electric field are modified by this process Thlsy however,
hag an effect upon conditions on the passage of the beFaui t}trough the tube,
particularly upon tha Energy of secondary electrons An experimental study
has now been made of the passage of a pulsed electron beam through a dielec-
tric tub s The experiment has been conducted in the following r.nanner: A
square voltage pulse having an amplitude up to 50 kv, a duration of 4o4~CSec
(Figo 1a), and a frequency of 50 pulses second was applied to the electron
gun placed in a vacuum chamber at a pressure of 2'10-6 mm Hgo ~.~he gun per-
mitted obtaining an electron beam with an amperage of up to 1 a in the
pulsed The electron beam wss injected into a quf~rtz tube with Fin internal
diameter of 9 mm and a length of '120 mm~ On the other side of the tube, the
vacuum chamber was connecte3 ~yith a d~vice, by whicY~ the pressun�e in the
chamber was varied from 2~1~- to 10' mm Hgo Part of the beam reached the
electrostatic analyzer, by Nhich the energy spectrum of the electrons in the
beam was determinedo A 30-nm wide metal ring, used for measuring the radial
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~ _..
2" 73
s/o57~61 ~0 31 /00/017/01 g
9, 3, ~~ B116/8201
AUTHORSa Berezin, Ap ;{~, Stupak, V. G., Bo].otin, L. I., Berezina, G.P.,
Lyapkalo, Yu, M~, Seveyukov, Yu. N. --_. _._._._-~______._.
TITLE: Passage of iltense pulsed electron beams through dielectrie
tubes
PERIODICAL: Zhurnal tekhaicheskoy fiziki, v. 31, no. 6, 1g61, 751 - 753
TEXTS The passage of an electron beam through metal tubes had been studied
in theoretical and experimeltal papers by Eo Go Linder and K. J. Berngvist
(Refo 1: Journ. of Appl< Pk~ys,~, 21, 1088, 1950), by H. F. Ivey (Ref. 2s
Advances in Electronics and Election Physics, 6, 137, 1954 , anal by M. D.
Gabovich (Refo 3: UFN, 56, 215q 1955), On the passage of a beam through
a tube, the residual gas is ionized, and positive ions as well as slow
(secondary electrons appeal in tree tubed In the case of a metal tube,
these secondary electrons reach the wall, and do not participate in the
further processes related t~ the passage of the electron beam through the
tube� If the dielectric tube is "overneutralized", the secondary el~etrons
will first reach the wall, end, after a certain time (of the order of magni-
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7
.,~.

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Interaction of strong.,.
S/0 961/011/006/001/014
B 102/8 138
40"/, This is in good agreement with experi~r~ents .
and 13 references: 10 Soviet and 3 non~Saviet,
Lnglish~language publications read as follows D
Revd, ~, 18,31, 1864 (1949); D, Bohm, E. Grass, P
(1950); Vo I, Veksler, Pros. Symp. C~;RN, 1, 8G (1
S. grown, Phys. Hev,, 35, 1700 (1949)�
S UBMSTTEDs June 17, 1961
Care 3/3
There are 6 figures
The four references to
, Bohm, E. Grass, Phyla
hys. Rev,, ~.y q92
95~); M.. Biondi.,

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2~~t~
S~089~61~O11~O06~O01~014
Interaction of strong�., B102~B138
interactions The plasma density was measured by a cylindrical cavity
excited with a TM030 wave from a klystran^ Thy: upper limit of measurement
was ~.�1010cm~3� Its valor, during the passage of current vas determined
from the plasma decay law; n noexp(~-t~~), where ~ .ia the mean tiwc~ f'ar
plasma decay and no the density at tm0� The straight line n(t) was dra~vn
from thxee measurements at~d extrapolated toward t~0� Maximum electron
density was 7�1010cm,~3, wr,ile the value ~�1010cm-3 resulted from shf-
interferomstric measurements� The electron energy s];ectrum was recorded
by means of a beam catchex connected to an oscillograph� These spectra
were investigated at the input azid output of the plasma tube, and for
pressures of 4 ^ 103 and 3' 10`~ mm Eig, for which losses reached 1 1~o and 1 f
of the initial energy, respectively Conclusionss Lnergy losses increase
with plasma density and with current, and are proportional to the electron
mean free path in the plasma� Calculation of losses due to elastic
collisions between electrons and gas molecules yields ~ Oa04 ev, and ~3 ev
for those due to inelastic collisnna~ Coherent interaction, however,
causes losses of 3.2 kev if self-modulation of the beam is assumed to rich }~
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c -- ~
5~0 9 61~011~006~001~014
8102 8135
~�~~~~ Ya B�, Berezina, G� F._,
Berezin, A� K�, F$ynberg, �
AUTHORS: Bolotin, L� I�, 5tupak, ti'� G�
electron beams with plasma
TITLES Interaction of strong _ 49~
Atomnaya en''-rgiya 9 v � 11 , no � 6, 19b1 , Q93
PERIODICAL: through
nonmodulated electron beam pas~;ing
losses of a e was 2b kev, amperage 5 ~'.,
TEXT: The energy a tube
an air plasma were determ~nOCm^3'Baa ~ pressure in the discharg
electron density (7-9)�10 b cm in length, was arranged
-3 The quartz plasma tube, 4 magnetic
3.10-4-4�10 ~ Rg� lasma was outisde the focusing
rester part of the p disk 10 ~ in diameter, was
so that the g un, a LaBb
field (2000 oe)� The e~,ectron g e ulses of up to
netie field and was w1thuencyaof 50 cycles � This
perpendicular to the ma~~ and repetition fray, ut ~,
width ~~f 3.5 ~~ec, a at the plasma chamber inp
30 kev, a ulses of 9 ion amperage
gun was able to produce current A In the field-free reg~
re the focusing field wag 1200 ath down to 2 - 3 a due to Coulomb
whe flight P
decreased with increasing
�~.axd 1 / 3
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~_
MIK}'~AXLOV, VqV.; I~AR~SZ~'J, A,T. ~dec4ased~; RASKIt1, ~'a~L. f S'�l~1tULiP;, ,~i~.~, 3
OVAL V.it.; Pr~.nimala uchaatiye,~ _~Rrxx~iA,~_ G~P._ .,_ .
Granu].~.ted gr~eni.a pigments .far the paint industry. Faakokras.
mate i i.kh priao ~~ no ~3: 32-35 ' b2a (M:tRA 15:7}
(Figment)
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SHAr~lIS,D.L.9 tiBERE~INA.~ G, ~.$ SAUBENOVA, M. G.
Gand~.t~.a~~ ~'qr t~ia fc~:i;:iar~ c~~ ax~~n~.a ~c:~.~i~ ~r,~' ~>rrrl~r~~~
u~I1~x~~a~ ~a,atax~,a cultu~~d ari tt~e p~rah~dxaaly~a~ta a.~ raid.
~u.dq Insp. milcrab~.al. 3 v~.rus. AM Kazakh, SSR 7s1,1{.-1+'7 '~3.
(MIRA 1.as1~?
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BEREZINA, G,Q,
a --..-
~raduct~ian n.t" or~~A~i~ a~,ida ~t~am the prsh draiysst~ az`
Trudy Tnst, mi'.xrc~bial., .i, vir~xs, AN Yazal~hb SS~i 5;"17-SU
(lied (Botany)) (Aci~~s, ~rgsnic)
read8
'E~1,
~ t~IxA z5 : ~. }
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BSREZ;CNA, G.O,
Prnduation of l~a~~,o said from reed weehixige, Trudq Inot,~ mikrah~.o~.
3 vSru:~. AN Kazakh. 3SR 4;99w102 ill. (M):RA, ~~4)
(LACfiIC ACID
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OQ~v~~v~
ACC NR: ATb~$?
n ro ammed medical iinvestigations involving the use of computers; ' ~~~~
i I P ~'
i'c is possible to have direct inforxnatir~n inputs from a Out ut friom the ~.
also to use memory for tenlpor~Y ~ ~ rto the telemetric channel, or to
on-board computer can be dent dire y '
memory storage units, or io the doctor. programmed medical investigattone;
'th the use of an oin-board computer can turn out three types of output:
,wi
~ in the forrr~ of values for individual signs (up to 200 digits for a sing e
investigation), in the form of processed results for each of the program ,~,,,.....~
eriods (up to 20 digits for a single investigation), and in coded form
.P
indicating the general condition of the subject, any deviations present,
and the measures necessary. ~~~ course tof a programmed investigation ~ ~~
I Xt has been found that i,n ',
~ it is possible to obtain a large number of different signs and, based on
these signs, to formulate diagnostic criteria which will permit a clear ~
differentiation between normal and pathological conditions. Investiga- ;
~,tion of the diagnostic ,effectiveness of various programs under clinicil for '
conditions has found methodological justification and is useful not on y '
space but also for earths~icle medicine. Yt should be assumed that the method
of.programmed investigation with automatic processing of information ,
by means of an on-board computer will salve the problems of medical
investigation and diagnosis; under conditions of prolonged spaceflights. _ _
`[W.A. No. 2?� ATD Re ort E6-116j
SUB CODE: 0~~ ~ SUM DATE: OOMa.Y66
Card 4~~ y ' _~.. _ ~~.._: r--=---- . ~ ~ -~.~ 8117102
i
anoe and twine refleoted aignale~ an averagin,c~ of 2A2(t)~A1(~) will be
useful. The observation time T varies with the parameters of the
inhomogeneities in the ].a~~er. Therefore it sh+auld be ohosen oonsidering
the following demands: 1. T must be as short as possible to avoid
distortion of the funotior, R(t) due to averaging� 2. T must be as long
as possible to minimize tY;e effect of tkie random function f"(t) on the
measurements. Ia spite a~' the discrepancy of these demands; a compromise
value of T can be found as. the function R(t) changes more slowly than fo.
The demands can be expressed as follows:
1. 1/T to + ~/~ ~r(t)~dt~~'R(t )
~ J ~,/2 0
0
2~ ~a~ooo) `` R(to~, where a is the probability factor
determining the "oonfiden~d~al" range; is the standard of the mean value.
With numerical estimation;i these dema~~s can be written as
1) T2~24~B.SL2 (9) and 2) T1 /2 ~(2~0o)~/2azo~fn ~10)~ where
a
Card 2/4
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277D6
s/1 ea 61/ooa/aa5/oo2/aa6
p i 17 B102
9~ q/~ ~
AUTHOR: Gusev, V~ D., Berezin, Yuo V.
TITLE: Radio-wage t~bsorption measurements in the presence of large
inhomogenei';iea in the i.onosphaxe
PERIODICAL: Mosltovsk~yUnlversitet. Vestniko Seriya III: Fizika,
,~.stronomiya, no. 5 ~ 1961 s 39-�47
TEXT: The effect of large ionospheric inhomogeneitieured reflectionude and
phase of reflected radio waves and} thus, on the mess
factor R was investigated. A method to redunQntalsdataeobtainedtby~ed.
The investigations wexe xased on some experi
investigating the F2 layer. It was shown th:at the amplitudes of reflected
signals may be focused. The focusing effects are to be taken into account
to avoid errors in measu~~irg the reflection factor A study of the
t of the reflected signal showed that and
behaviox of the phase ~ I,x ~~y ~ )
fo(u,v,t) v~ere xandom fw-ctionso Th~hef reflectionsfactoraareynecessary.
averaging of the measured values of
When R is detexmi.ned from results obtained by measuring the amplitudes of
Card 1 / 4 __._
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

~9~w,~~
s/13g/EE~v/ooo/o~/o3z~o4~
The Correlation Methods ~f Invest igat~n~~~I~nospher~.c) Fluctuat~.ons
in the Presence of a S.Lo~r~ly~changing Component
fluctuationse In the typical case it is found that
~, ~ 60 min ~ Consequently the nece.,sary conda.tion
is fulfilled s~�nce ~Qo~ = 3 min and T~ >a 1.2 to
24 hourso
There are 8 figures 2 3 tables and b .ref erenc ee ., ~ of
which are Soviet and 1 Engl:ishu
AS5oCIATION~ Mosl~ovski.y gc~.su~:i.~rer~~et imen~i M~V~ ~,~,manosova
(Moscow State University i.meni MAY, Lomonosc,v~)
SUF)MITTED; March 17; 1959
Card ~r7
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

~~'~ ~:
/~~.~y~l~~/ouc~/a~~'u3:~.l0~~
~~. �~E38
Ths Correlation Methods of 2n~est:igating ~`~c~nospPier~c) FluGCUatian~
in the Pr~esexxoe of a ~law:l~y~rhr~ng~.zag Co~npanent
parameter ~ ~~x~u,l~l alie~r' t.t~e ~~~l.tc-w~.ii~; e,~~ax'e.ys7c~xY~.
~`rom the ~.n~crF,st.igat,ion i.t is concluded t.hdt t-y employing t~~e
method of thEl 1'g1.ax+.c~.ng a~rerae;ei" ~,~ is passible to
sl~.m~.nate t:hE- slow changes why-n in~~esti.i.gat.inc; the
statistical j-rapsrties of the fluctuat:ion.s~ The method
can be usafuJ: ixx the in~restxgation of the flu~:tuatians of
uJ~tx'ahi.gh.~fx'~~quency signals axxd ,n the study of the drift
of smal.l~sea:.e inhoma~;exxez.ti,.es~ The s1c~w changea caxY be
eli.minat ed p~�oua~ti.ed
Q a ~ ~~' ~ ~~~ T
where ~Oaa i.s the r�c+~~.~�~~1a.t:i.or~ rti~d~i.us of t~.e
f1.uc~tua'ti,ans and T -~.s i;i~e ~~'-e~`ac;e perx.erd of the s1.c~�
Carcl6~~
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

i
/~. 3 ~>/60/oa0/o~./0~:3./0~~ ~.
~~. ~ ~3 ,
Tie Corre~.at3,o:t~. Methrsds of In~~est.:i,~~at~~..~~~ ~oi~~o:~}~t~ox.i.c::} }~luotur~t:i,o~;~
3.n the Presence of a S'l~-w1y~-~changin~ Component
determined w.i1.h axi. e~�ror ~~fi ~Eq '.'Ma) v Howeuer~
direct~.y a.t i=; ~n~.y possible to determine the Garre~.atx.on
function �xpx~,~ssed by.,

~- X11 H~P+^~�"~ ~'t-":~^""'1'A`cp
.._.a._.._..~...._.a... ,..~.~.-~._
where sp~(t} ~ `~;},~. ~^~~.~ ~ ^~~ ~ s~'2,~ and so on
(x, - :1., Is -~: 2) ~ b~P r~est~r. is t~i.r.~~, the vala.dity of ~q (~}
it c;an be wr~,uten a5 ~q ~4) ., ~v'hex'e the symbols are defined
Card3/~ on p 180 Tt ~.s nati~T t.d
r "t l ha~r.i.zl~ a ~3era.s~~1. Sri" App.raxa.r~~at e;~~
x�and,om aha.n~e ~l :~.~. xd seen that
x5~:~~0 ni~n are supex~xmpased +~n ~$' (t) o
the spx�ead of {t) is m~c.h ~~`F=at er khan that caf ~.~~t? a
It is x�equirecY to determine the CunGt.~onn
_.d..~,~..,a....,....v...._._...~.,._.-...-.-... ....,...~..~~.......~,~.._.
_ _ ___ ~,~
~ ~.
where the h,a~�iz,onta..l. tc~i,~ .i.ines denat e statsi..iaa1 a~rera~:Y.n~
for 9 k ~ :L ~ ~, ~ ~ Nclrma.l.l.y ~, the ayerag~.ng c.an be
done aver a ;.~ a.:i.t ~ tame ~,iiterval and the fu~ict:~an aaxz be
Gard2~'7 1
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~, ~~3~~3
,~
S/~-,fig! (a0/t~0d/0.1./Q3.1,/~t?`~.I._
~~ ~ SOD F ~ g~~F~$avskiy A A~~ P~ and
.
o t an S ~ F ~ ~ y
h~i~rl;
D
'V
AUTHORS a ..
~
p o
~
Gus ev

`'~
Derex~u~~~
TITLES The Gorrelataon l~iethads of Tnvesti~atx.n~ (.Ian.osPhe~am) onent
~chan.g:i.n~ P
owl
5
1
f
Y
.
~
a
Fluetuat ions in the pr es e~1G e'� o

PERIODICAL ssh~.kh uchebnykh 7aved~niY, Fi,~,ika~
zx~~~`~~-y~ ~'x
~ ~ ~ z~,o ~~~sR)
1g6D, Nr l s ~ p 7
ABSTRAGTn The phase of a a:i~nal reflec:~ted fram the ,tanosphere can
b e r epr es +~n't acd as

where (t:~ is th4 daz-ly variation of the phase due #:a
ax~osp~ier�~c 1ayc~r-
t
he ~
.
:
the changes ~~~" the :1.o7~isat~~on in
#; d ~ ~ 1 .~ s a raridam s t ~~t iax~a.ry
t
~
i
d
'
.
~
n
a;;~
durx,n,g day
function due to the p.resenre of irregulari.ti~es in the
~ ~ t )

The func t;ian ~
ionosphere a.~id dine 'to its mot.ia~l.~
gation of the
nvest:i
i
.
.
:.s of da.rect interest .n the
annat be ~neasur
t c
d d
i
Y
es
~
,
.
ionosphereo Hai+er~e.r~,
~y
ome
It is therefore riece~ssary to separate ~~ ~ rocadure~
h a
P
me~thad~ Apt ,sttempt. ~.s made to dev~..se suc
rding of tha phase function
Cardl/~ ' 1
Fi~ur'e 1 shawl a t�y'Pical reco
S 1/
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

On the "Resolving Powar~o of Systems for the Measurement 6}Op5
of Dimensions of Tanospheric Tnhamogeneities s/o55/59/~aOO%~/011/O26
eo~4/BOOS
` with the altitud ~ Sa a 2~ 8S ~ .~ ~ 4~So ~, In a Simi I.ar ways the
foil�wing limits hold for the distanoe S of
2o8S~~, ~. 23Sp Tlie.re axe 7 figurea~q ~ tables tandalO$referenaesints;
of which are Sov~.etn a 7
ASSOCIATION; Rafedra rasP~'aeta~aneniva radiova~.n (Chair of P.ro
Waves) pa~'ation of Radio
S~BMTTTED; March X84 ~y5y
Caxd 2/z
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~900~
/00 a F6 s/o55 59/aooJo4/o1 ~ /026
9 ~ii.ckota~. S 9 BQ14
AUTHOKS a .~-...1--�.._ _~.
Berexin9 YuQY~ 9 Yi~aAOVSki _,_.~..
:~ ~,~ ~,:
,._~.:,,.:~.,~ .._._:. , ~~ stems for the MBasurer~snt of
TITLEt On the "ResoleinS POhericolnhomoBeAeities
pi-manaioas of ] on.os~ m$y~hani,ki ~
~ti Seriya matematiki,
pERIpDICAL: Yeatnik D~oskav~-iag� universite ao
~~ ki khimii9 1959s Nr 49 pp 105115 (USSR}
ae$ronomiie fi ~ �bse~in8
eneities and motion may be atudi.ed by ivea
,~pSTRACT: Ionosphsrio in~'aomog ale by the ionosphgre~ At a 8
the reflection of eathxeei~sexvatian paints an th~a st~hshow ~sce~
distribution of th this sy
the amounts of inhamogeneihies determined Y re
e resent paper deals with the definent
upper and a lower limx.tQ T p hose
f these limits and the estimate aatusrby vrhichstheap
tion a
resultso The E~uthors deacrinQ~tperepmsasured~ Figure 1 shows a
shifts of the refleoted sig a aratuse Figure 2 shows themethod
black diagram of this measuring pP
tl~e measuring triangle Details of they measuring
position of formulas fox determining
are givens Further, the authors develop
tension of ionospheric inhomogen~3Thasinve tigae
the horizontal ex the erraro
and fox estimating
measureu-ent valuehs fo~.lo~ing ~,imits hold far the st3onst ian,glef
Lion shop's that t t a ivea right observe
Card 1J2 measurable inhomogeneitiee a 6
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

89?72
~/~6~/~=~!~~aa~aoa~~ra39
AOOSf Af~Q~.
Results of the Investigation of t~r~e ~a ~rtc ue"s of ~~~4 ge~5ea? a 1~~omogene W:ies of
the Ionosphere by the Phase itteth4d
''broadc~-_I~�~{", and peramet,~ar-'4'o~~rd a~.lowirtg whe ~~syima~::cr~ o~" the p~t.t~t of e uhaatlc
variations. the results are prese~~ted o`' rovesu~.gatl.c~ns ire the per.lod frays
~'anuary 1g57, to Nlay 195$. I.t is shown that ir6homogenei�~.~.es ~.~~ the hor~.~ontal
direction are anisotropie, the dj reetion of the ? t~~ ge" dimeneiti. ~'bhe ma,~or axis
of the s~haraoter~stiaal el.llpse) apps+�oximatel,y coS tides w:. un the m+~ridlan; the
average ratio of tY~e ma,~ar and minor d.menaiosw; ~tri;! scc$r~~ric~!ty o~E' the e~llipse~
is about 2; this value and the direct~.on of tie ma,~o:M axis are nearly ir~dependant
of the time during 2~ hour$p the average va:i.sae of %.h~ m~a,~{~r axis i,s about ~ km
by night and about 200 km by ds.~yy, ~':~ze values of dr:.f t speed o� inhomogeneitl.es
mostly found are 8 - lfl kasi/n:lny the dir�ct.:.an of do i~' i ~ irc the evening a�rsd
by night northward, by day and in the mor~,~air~ soucrward, 1'`ne '`broadening`4 of
inhomogeneities proceeds move rapid by day thy.; -y nigh~r,4 he speed of o?aaotic
var~iatians ~c exceeds the dA~ift speed ar. ~"~ aver~a~~ by i , 5 times, A comparison
is carried out of the resul9;s obtained with tre va" ues a:'or~merly known. Iti is
shown that the characster~istj,cs of tl"ie la~�ge-s~'aie ~.nd sma11-scale ir~.~?amogeneities
as~isotropy~, drifts chaotic Variations) ag~'i?e w3 yr: wa:~4, nyhery which p~ rots out
card 2/3
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

� X39?72
J/dC3~,/~ yJ`~O~J~~c~G/E.~&~r~~l~
T.~~'t~~.~t~~n ~'rc~m;~ Re#'~~~~:~~rny,Y ~h~x�~z~:1~ ~~iea~'1:~1,ka, ~~~i, PJa~ ?~ p. ~?, ~~a~
AM~i~V~-tWi ~4lNV~j �t ~d~ ~~.1.~11.~U~j 4~}~ ~e~ ~r~~h LA ~~j ~r ~~C .C7e~~~i{i1j ~~~~ ~��j
K~yaY1C'VSkiy'~ M o ~ ~ .~"~"""w�--..~'.._.r�---..
~'2TLEo Reeult5 0~ �~he Tnve~tigr~~~~.~n ~:~ th~+ ~,.~~~u~i~i;,vr~ of ~ar~~~M:~~a~.+~ Tnh~mO�
geneities of the Ionosphere 1~y ~~he Ph~.se M~~..h.od
P~RTODTCAL. V sb,: ~'Drey~y i n,~odnax~adncst'i v is GE!'`~?'^t'�"', 1`Yo~ 1y Moscawj AN 9~~Ry
~9~~, p~, 7-2~ ~Engish s'~amma:y}
~~e. '~ha rr,ethod o~ messxtring end pr~oceMslr:.g i;Yar~ me~;etii~.i.s of at~gervaW:~c. s
of the ].arge~s~cal.e inhemoge:~~it,ie~ is t~:e ,~'2~+~ex~ G= -sae ~.ai>~'spere is desUri~~G~
in detail, .'T'he t~.me va~'~iaf,iars a~ '~,he p".use o:: t~Y~:e pu:~s~ ssgr_sl : s~'s::tad ~~y ~>ha
F2~la~ter of tl~e TanpspheMje wtere rev~~r~.ed b~~- trre~~ ~pw~~a st.a`io:os~ ='he ='�e~4rds
are being prooesse~z by the cvrrel.atiar. m=t ~^ ~+:.y`'. P'.~~i:r-v:~ co:~p~.~~~:~~"s� ~~~"�
~. ~'~ p ed ~~ s
following ir~Gma~;eneit~ pay�ametxrs were deug~;j~;.e.%, aF.ca~:�~nt d~^ ~ s ~'~~ d ~
~' i the speed off` ;Yia ~,,, ,~ iv~-! et'~~.~,:,s x. _.~~ ~ a~ u3~
char~aeteristiu speed ejr ~~' A ~:' yy,,
-~ y'r� L~~ tl:e irQ~�wG�.i.1Gd �::fi�y'. L~.+ =Y.:.~ :�:.. y:R..~" '..''.l.l.i~'~~ ~lii r1
speed vdj the parame .e .: �~ -� �~ y
determine the aniso grapy d~:gree off' iz:+homogs'ne'~~.~~y ~~t-,.-:1"' dimes.si~~rss aid tAme c'
C,e.rd :~3
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

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APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

.r K[Mii~aY~.,r~ r.rr1~~ MYUlilrr

0 nprearYYR tneYryRMiM t11/l~
R uRtYtY ptecnRRt a Rp ~YOCre~Yeapt~q[n w� U . RI/rMtR/M1lA [nIK~dRnRn. eatteY, nuppNr
M�R rogewnltetYw[ 1-"'~Ir' .e��MM"t YaRweR+�
p11 npR WtNkRY ~.+rnl.

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APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

SOV~2o--12 j-a~-i~~~a
,The Structure and tha ~oti.ons of I,ar~,e-~Sca~e x~lhomo~;etlc~iti Ens ~.n 1;110
xcngeph4re ~uyex ~+'~
the presenc~.~ o:f inhomo~,eneitiss in tl~e iono3~7here, the norr~al
to the fron~c of the reflected wale deviate3 fror~ the vertical
direction. 'yor $ and ~c the averr~lasma. The indicated ph�nornena are also of value for under-
standing processes occux~aing ix,, the interplanetary medium, for example the interaction of the
solar wind with the geomagnetic field. Unfortunatoly, tho str~:cture of a shock wave and its
width has still not been investigated in space experiments, but apparently this will be done in
the near future owing to the inc~ceasing volume of work being performed on satellites and
rockets. Orig. art. has: 14 fi lures and 11 formulas.
SUB CODE: 20/ SUBM DATE: 16Dec65/ ORrG REF: 021/ 0TH REF: 017
/ '~
Card
2/2
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

ACC NR: Ap6020549 .~......~~~w.y,_.._...,.a_w..---SGURCE C4vE: UR/4ri14 jGG/'004/001/OOA3/4fl2b
AUTHOR: Berezin Yu. A, (Novosibirsk); Kurtmullayev, R. Kh. (Novosibirsk;
Nesterikhin, Yu. Ye. (Novosibirsk) ~..~
i
ORG: none
~ `'/
TITLE; Collzsionless shock wives in a rarefied plasma
SOURCE: Fizika goreniya i v2 ryva, no. 1, 1966, 3-28
TOPIC TAGS: plasma shock v~~ave, shock wave front, shock wave analysis, rarefied plasma.,
shack~vave structure
ABSTRACT: The author discusses the theory of the structure of shock waves, dispersion ~
effects, shock waves with an oscillatory structu~.�e, collisionless dissipation, shock waves j
with an aperiodic profile, conditions for exciting waves, devices used to excite strong shock
waves, the basic method of plf~sma diagnosis, dynamics of cylindrical waves, and the structure
of a shock wave and physical phenomena at the front, The problem of shock waves includes a ~"
wide wcope of physical phenomena such as dispersion of plasma oscillations, microscopic in-
stabilities collisionless damping, and others. The interest shown in collisionless shock waves'
is to a considerable extent duE to the fact that instabilities developing at the wave front and the
Card 1/Z UDC: 532.593+833.9.0?
APPROVED FOR RELEASE. 06/23/11 CIA-RDP86-005138000204800010-6

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