SCIENTIFIC ABSTRACT FR:NESTERIKHIN, Y.Y. TO:NESTERENKO, V.V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001136700040-6
• Release Decision: RIP
• Original Classification: U
• Document Page Count: 4
• Document Creation Date: November 2, 2016
• Sequence Number: 40
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTR

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I sxo~r. xR: ; ~sot~ss~...~..~ t~o~~~~s~s/ooo~oo~/ooa~/oon~~
1~t" 553.9.08 ~
- ,AiQli# lsko 'ds~ki A. M. ` ulla ev R,,,l.~h., Luk vanuv. V. p.; Msg
: Some ~rrties of the behavior of ~rmai~~~ated ~Y colli~tionlesr uhoake
TITY~ PAP
- 8+0URCEs l~egn3tna~a gidxbdinamika, no. 2, x.9e5, '3543
T4~iC~'t'Sa � p~,~aas sht~k te~~re, shack rave hee'tir~g, plas~ra diagnostics, ~-icrc~ave,
. p~.aema ccn~~8itnt
` ABS'~RA~T; The get#eration of collisionless shocks in plasma with quasistatic axial
~ered by a etor e s stem Kith maximum
~4 :~; ` m~gnet~.~ field by use of theta-pinches tpon aB Y
energy a alaout 3004 J~ is discussed. g~mxd density in the exper3.ments Was about
- ~ ".-_ ~ 10.1 c#a Magt~e#io and opti+~al n~aeutremasaats ndfcate the formation of a cylindri
~~ ,
dal "est~net~c pieton~' driving the coiLis9~~n~iass ahoaks which concentrates along t
. z._ glasm~- axis. Also studied are the accompaunyiolg phenanena of X~ray and miaroMave
t8 ~~ txs3se er~iseioia. They diagnostic ic~�tr~ummntation (magnetic and scintillation
_ p~ and rage-convertex- caa~ara~ is des~;~rib~~d in detail and typical results are
sl~++n (e. g. cailiei~alslss shock is shown to r~ ahead ag the eurrrent shest~. It
- Card 1~ - � .~..,. - _ ~ ~.....,~...,.~._.L..a.: _...,._.~_ ..~.,__. .~~,.. _.~_~.._ ..
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L OC-3~,5~66 ~`~1T~1)/~PF(n)~2/E~1G~�)/"PA{w)~~ I~p(+~) AT
'~r~~~~R: ~Ap5dlS8gq UR;/038Z/65/ddO/QO2/dd31/dd34 ~,
53~3.9.d82.5 ~,~~,
`~'' i
'AI~'C~'IQ~s Krug~rakov, E. ~.; t~alinovsk~y, V. K. ~ Neaterikhin, Yu. Ye. ~,~
k"eaa~.bilit of te~pex-e'kttre es:d deaei~~~~i~t~exmination of nvnstationary,,,~_,~_____.._
~TITI~, y _ . _ ~.
pia~sma by ereans of optical interferometx-q
~~~~~~, ~ itne~ d~ idrodinamika, no. 2, l~bg, ~i-3~
;SOURCR: agri Y 6
~TOP'iC TACSs plasma diagnostics, interferometer, plasma temperature, electron den--
,~.~t;y
~i1B,;TRACT: The application of a Hichelson interfeicometer to nonstationary plasma
'.di,agnoatins is reported. Preliminary results on the degree of ionization, electron
,~de~nsity end plasma temperature are reported. The method consists of using streak
tQ11d`framiuK camera phota~raphy of the interferogrems, and fs used far events lasting
a .few microseconds. It is ueeful for stud3.as where plasma conaPntration is 2x1U14
~c~rs_3 and its length is l0 em or more. It is su~~gested that ir-cerrero>;rams of plas-
~tyt flor+e around obstacles can bs Uaad far dm#er~-inin~ its mean-free-path, tempera-
~t:~re, and Alfven'e velocity. A simple experitaent to determine plasma temperature
k ~;~,~ 1/2
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~ a~~a- ~~~~~~~
`' ~ACG Its AT6p0;C~e~T .~ gOll1~CE CODES UR/31~ 4/009/OOfl/007210075
AU?NO~i; Hc~M. M.; Kc~el'kav, V. S.; Nas~t~rikhf~r, Yu. Y+r. ~ilf
Ogt3: eons ~ .~ ~
TITLE; Electron-optical instrument far studying changrs in the half-width and in-
tity of spectral lines with time
SOU1tCE: $�~. Kom ~~i~t,,,,,~,o,~,,n~uc�~hn,�i'at~~ii, i kinematografii. Uspekhi nauchrw~T
fotografff, v. 9, 196b. I~ysokoskorostnay~ ~otogrya"~ �e~a o ~~~iya (E1igh-speed
photography ~r~d cinematagr~tphy), 72-?5 and insert facing Page 80
TOPIC TAGS: :[mega conrrerte~r, spectral line
AHSTRAC~': 'Plug article describes the design and testing of a deal conwarter, in
which the raoordiAg of the glow intensity and dimensions of the image as teased on the
oscillogranus ~of the input current of the photamultiplier. The test results confirm
the principle and design of the instrumenrt and, indicate that an instrument with bet-
ter parameters can be constructed. The tested; instrument can be used for recording
processes tasting 500-1000 p eec. To improve the resolving time, it is necessary to
incr~ea$e the a,ii~'icstion factor Qf the instrv~nt by two orders of magnitude and to
use a fast mu~ltipl.ier with a current linearity up to SO-100 ma and a time resolution
of 1-5x1.0-s sec. To increase the space resolution, the resolving power of thee i~ mass
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?L ~~s~~ ~
A~~ Pik: AP502 r2$al ~~
t+y 2 arc:. 'the 3,nitial. p~,s,sma cancQntration ass 5 x :LO1z to 3 x x0~'~ c~ ~.
Magnetic field tre,pping ar~d p].asn~ containn~nt were achieved ran the basis rlf tl~e
f~~~.loving obeervat.ion. An average !~0 ~t.sec delay in neutron generation (106 to
liD7 neutrons.}~ 1Q kev ion_energy attainment;, anal bremsiatrahlung radiation were
t attained after thE~ applie~3 1'isld Ho had deci:ged. Qualitative m�asurementa from
magnetic probes indicated that the trapped Field ~raa of tha order of ~ (cof.l field)
ui~th a duration com:aensurate ui.i~h neutron ~nar~ation. The trapped plas~a energy
~~ts about 10 kev. Tt~e authors thank G; ~~ud~.er far .his constant influenre and
interest in the nark and I~1`~~~ ~.a~de,~re4 for hi~~ help and participation in ::ralaat-
i~ng the results. Orig. art. hoe s iguree~ end 1 ~fa~rmula.
sous cam: ~j sow nay: l~o~/ oRiG �~ sat/ oTT~ ~: oo~
;ti
o~ zj~
..
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Acc NR: APSoz~~o Ww~AT ~, sOVRCE ~~~: UR/aim/bs/oa0%o~/018/ozz ~.
~~ ~. ~
AUT~~OI~S s ~ko.1.! d~c~y~..~,-..~~~ (Novasibir~~.); ~u~l~.~,.~~.e_~~.a~..,.. (No~o~ ib~x~ek) f
Neste (Novos;lbj~rsk); ~il'~~k ~ V'. I. ~No~rosibirsk); Ponomaronko, _ .~.
ORO ~ none ~`
~/ y~ /. ~~
TITI~Es Magnetic field trapping and pla.ema c:oni;airunent in experiments with a
collisionless shook, gave .._ f ~~Y -~
'SOURCE: Zhurna~. prikladnoy mekhaniki i tekhnit;heskay fixiki, no. 5, 1965, 118-120
TOPIC THOS s magnetic field, plasma, shock rravE~, rarefied pla ems ~
neutron generation, deuterium
ABSTRACT: Magnetic trapping and plas�a eontai~uaent tirere achieved in a rarefied,
~cylindrt~al~ deuterium plaemr~ by creating a co;llisionless Shock condition. A
1G~-cm glass- tube was placed ~.n the ceuter~.~i.ne t~f a quasi-stationary magnetia field
(How U.~ kilo-oersted, T = 5 �aeaj. In the iaenter of this sp�tem tree added a
30-cm shock coil generating s s~gnedio field H ~~3 to 6kilo-oersteds, far Trv 1.4
Card I/2

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ACCESSION NR: AP4019970
the infected plasma was 5x103 m/sec. S~lnee in accelerators of this
type there is no tray of prevent~~ ~j radi~il diffusion, the time of
acceleration must be of the orucr of 10� sec. This Imposes re~uire-
ments on the ;period of oscillations of the capacitor battery feeding
the accelerat~~r which are difficult to ~3atisfy. "The authors are
'st and useful discussions, to
~reateful to ~~. I. Budk~-~' for him lnber~.
'V� N. Lukya,nov for help with measuretnen'te, and to Yu. ~1�~ Serezin for
compui~ations. "' Orig� art. has: 3 fit~res�
ASSOCIATION: none a '
SUBMITTED: 17:iep63
SUB CODE: PH

Car~~3___ ..~...._...__ _
.. ~ ..

DATE ,ACS: ,23M~ar64' ~ EI~Ci~: O1
' NO REF SWs 004 OTHERt 003
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., .~. `
_ ...~.~..~ ry .... ~ , A~4oi o s/oo2o/64/154/QO6/1slo/1313
AclvESSZON NR. 99T
AUTHOR: Dubovoy, L. V.; Nesterikhin, Yu. Ye�
TITLE: Generation of superfast plasm. ea~ndensationa in accelerators
of the rail gun type ,
SOURCE: AA? SSSR. Doklady#, u � 15~+~ n o � E~ ~ 1964, 1310 -1313
TOPIC TAGS: aupert'ast plasma condensE~tian, plasma gun, plasma accel-
c7^ator, plasma, plasma generation, part~lcle; ionization, particle
a,ccel.eration
~:gSTRACT: :tt has been recognized that 11G is desiic~.es in theap~.asmahe
processes ~~f ionization and acceleration of part
The presenl; vrork describes experiments :ln whic~zti igheylattered Thesde-
~;~roduced outside the acceleratomi~a~t~o'ethat used by Yu� S� Azovskiy
sign of thc: plasma source is si
(Zri. TF, 3~~, 1050 ~ 1g61 }) . The plasma was composed of ~~ lmyadenoPed
particles evaporated from an insulator sn$art of the s
' gar anic glass. The average energy of electrons and ioo~ the front of
g otential. The vel,oc~.ty
ev measured, wlth a retarding p
_ cold 1/~ ~ _ -. _ ..._. __~.~.----- - _ . _ __._-. _ _.__.._ _.~.~._... ...... -
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ACC. NR; AP4009894
arui thus enables one to inv�etigate the struc~tur~l of the burst. The described pro-
cedure was used to rceasure the velocities of plasma bursts from a ooaical gun, us-
ing 3? Isilomegac;ycle microwav,~-a with the Antennas inclined 40� to the drift tube
axis. The two pa;ramE~ters of the system (micrrnvave frequency and anteiuta inclination)'
can be adjusted 1:o meet a wider variety of conditions, For example, i~t the inclina-
tion is made ve~;- large the fY~aquency can also be wad� larg�, with a resulting in-
crease in spac� resolution. airig.art.haas 1 i~ormula and S figures,
ASSC'CIATYONt none
SU~4ITTED; 3IAug6~3
S.UB CQDE = Pii
DA9T ACQ t I.OFe'b64
NR RAF 8QM1/t 00;1
E1~+CL: 00
07.~Rs OOZ
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Card ~~~ _ ~ w -~
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J l
ACCESSION NR; Ap4009944
S/DOS 7/64/0 34/OO2/p190%192
AUTHOR: Ku:rtmullayev,R.Kh.; N~asterikhin, Yu.Ye. } Ponomarenko,A.G.
TITLE; On measuring the inatF-ntaneoua velocity c-f a plasasa burst
SOURCE; Zhurnal tekhnicheskoy fiziki, v.34, no.l, 1864, 190-192
TO}?IC TAGS; plasma, plasma burst;, plasma burst velocity, plasma burst velocity mea-
surement -
A1iSTItACT; A procedure is dQSCri~yed for measuring the instantaneous velocity oY
plasma bursts by observing thal Doppler shift of obliquely retli~Cted miorowavas.
Microwave traansmlitting and receiving horns aria located on opposite aides of the
,drift tube, vrith their axes inclined to and intersecting on the ~-xis of the tube.
Yn the absence of a plasmas no signal from thEj transmitting horn c;an enter the re-
ceivor. ~11hen the plasma burst reaches the crii:ical position it reflects microwaves
into th� receiving horn. Those aro mixed with a portion of the trans�itted signal
and the beats are displayed on an osaillascape- aoreen. From these beats the Doppler
shift, and he:ice the veiocitq~ is obtained. ~'hi~ method her th� ~ufvant-.gs over sCgq
others that it; responds, at any mament, to a d;etinite seotiou~ot 1~he plasma buret
Cardl/2
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tiCC.NR: AP4009919
proximately th~~ Ra~ovslciy sh~tpo. For the point to planQ measurcracnts, a sphere of
0,005 cm radiu:~ was employed with mercur ar~
was observed in the distribution of the lag ~timesu~nonlyilag timesboccurred licity
ware multiplE~c~f a certain characteristic tune tl, and those which were ~lsohclose
to multiples ore a second much, longEar charactc~riatie timE~ t2 tended not *o occur.
Tha characteristic time tl rangErd from about 0.1 to 0.6 nanosac and decreased with
increasing L/p. For uniform field breakdown, the, characteristic time t2 also c~e-
cre~asE:d with increasing E/p and was of the order of lOt
said to be perceptiblealso in one o~ Fletcher's his;tagramshe Possibleca~eSi forts
the observed periodicities are discussed at same length with no very firm conclusion.
being reached. Something of the order of 10`~ ava:lanchEas are requirE~ci for breakdown.'
If ~�ewer tran these form initially, some sort of avalanche multiplication must oc-
~~ur, and this multiplication process ma
ors favor avalanche multi lication b y give ris.o to the periodicities. The auth-
avalanche chains observedpby W.Franko (Zs~f~Phcs.~ic EsffeCt at the cathoda as in tha
time tl would be the time tq required for an ;3valanche9toldev0elophtactheac~yristze
size. Zn an appendix, the avalanche development timE~ t critical
charge a?feats taken into account. The calculated dEjvelopmenta~imestare comparedQ
,w;tth characteristic times tl abservE~d in th~r present work Aad with 1 times
~ ob-
Card 2/3
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ACCI:~S ION NR; AP4009919
S~OOS7/64/034,l001/0040/0052
AUZ'IiOR: 1Jesterilchin,Yu.Ye. ; ltamel'kov,V.S, ; Rioylikhov,Ye.Z.
p,.. , ~ ..~..,.c .
TITLE: Short gap pulse breakdown in thQ nanose~~ond range
SOURCE: Zhurnal tekhnichoskoy fiziki~, v.3~,, no.:l, 1864, 40-52
TODTC TAGS: electric breakdoivh, pulse breakdown, uniform Yield breakdown, point to
plane breakdawn, electron avalanche, electron avalanch� multiplication
ABSTRACT: Lag times wore determined for uniforir- field breakdown and for point to
plane breakdown ~n air at pressures f ram 16 to 1.10 cm Hg~ gap lengths from~0.01 to-
0.122 em, and pulse voltages of up to 25 kV. Thc: work differed. from earlier work
of R. C.Fletchor (Phys.Rev.76,1501,1949) chiefly in that greater resolution and
steeper pulses wero achieved, shortor gaps were employed, and the pressure was var-
ied. Pulse rise times of the order of 0.2 nanos~;lconds wore obtained with the aid of
a pulso shQrpening gap. The liischarges were obs~alrved with an oscilloscope capabl�
of 5 x 10-11 sec time resolution, and it was th:ts that limited the precision with
which the lag (time between ,pulse arrival and g~xp breakdown) could be determined,
The uniform field breakdownstook pleas between 2 cm diamet�r electrod�,s having ap-
Card 1/3 .
_ _._.. --~-P..._ , ~_. ~_
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e t ~ rw 6 `' ~1`~~AF x~ ~~ ``
tiY r` 'iy ~2, _
t ~ a ~xts�s,~,~i3+�~wr% ~it.is is in
good agreement; with published results (:Ref �~ ~ Arbuzov M,P ~ ,
I,ys~-k LUIa ~ Nesterenlco YeeG~ D~1N ~-SSIt, vo90~ 1953.., 3) The si~,e
of the coherent scattering region i~ras found to be independent. of~
the method used to determine themo ~~}.e u.niform deformat ion
region in martensite crystals is cans:ida'ral'~~ly l,~rger than Ln
plast;.icall,~ deformed metals ~ c:onfir�ming th~~ con~~lueion jo. ntly
published by one of the aut]'~ors (Nesterenko) anti others ~l;!ef ~ 3)
that martensite crystals in a piece o:f harclene~d steel are
elas'ticall}~ deformed by forc~,es external to them, For isolated
martca.nsite the situation is entirely different., Static
distLtxbarices can produce changes 1.I1 t1rle intensity of x ray
interference without appreciable w:idt'h change, but special
experiments are needed to check wh~et:lier this effect could lie
responsible for the observed relit iansrrips ~ ;,t~.Idy of the eff ec t
of linear d:Lrnensions of spec:tmens on stAta c di~sturL~ances stiawed
that for martensite: i.t1 hardened gt~cel t.he~r dre due who.] l.y t c, rl-e,
presence of interstitial carbon atoms i-n the alpYra iron la t t icy ,
Card :3/4

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s/l~h/6ilol~>/~o6/t;l J/o�.%7
E11.1./T~435
Aiicro-stress�s and coherent- ~. ~, ~,
t1-12A steels hardened f i..l. irtc;s cf i1- 1':~, steel , }Y,~ r~Il l;~ner
]. 02 mm diameter specimens of U~� 12A Steel. u `lt~at. ~ tternli ~a sl~)}1t~i 1netltlnl
.;pecimens of U-12A steel a Before thE, X ,r y 1~
a Ooz inm thic), layer wars Etched off al.l file specimens exccl~t
4 e t: ~:, h e ;~ :~ f f) t h i s by a -; f c !.T n :l t~;
filings (from which very little wa.'.
e~-i ~ol.tcl so.L!it..ion ,n15n i:c~
~I
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�J l~t .~.i~~ ._ l~l~'~r'.. .. "j_ r- c; a - ._I 1~~ ~ '~i ,~iJ !
f~ ~, , .., .;; 1.~ ,; ,. ..lip, ~ `I ~titut ms~t~.?.lofYziki AN USSR�
(Cop~or-tin al~oy~~��Treitir.g)
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N~ST:~R~NKq~ Ye.a. [Neoterenko, I~.H.a; (iHtfI~STC-V, R.V.
Changes in the ~~r.yetalline struci;u:re of aging Cu-Ti al:l.oys3.
tJla�. Piz.zhur. 3 no.2:276-278 M'r ~9~p 'SH. (MiRA 11:6
l.rnstitut meta:l.a>Piziki AN 1JRa~t.
(Copper- vi ta;nit~ all.ye
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--~s
57-9-38/40
AUTFIOBs Neat�renko, Xe.C.
.. T._.._.~ _
TIIJ.Es On th� .~rtirlra .~y D.T. Y,~gil''y~'s'a " On the M�thod cr!" Dividing
a KoG - Do~ubl~et of X-Ray i~inc~a"'
(Po povodu et~at'i D.~. Yaei2"~~'a "K metodike razde2eniy,a
Kam, - dublet~~ rentgenovskik}i 7 inty" )
PERIODIC~~s Z'huxnel Tekhn. 1'iz., 195'l, 'iTcal. 27, Nr 9, pp. 2183 - 2183 (USSR)
A8S7,'93CTs Tha artial~Q p~ablighed in Zhu~wn. Tekhn. Fiz., Vol. 2~, Nr 11
by Yaeil'Y~+a :i+~ rritimized bE~aa,uee it cvntai~lA r~ ..number of in-
aoou~aoiee. 'flzd diffioultie s allegedly found by him when de-
terralnirsq the :inter-doublet c1iE-ta.noe on oone.iderably we,~hed-out
lines ere b;y nn means subst~.ntiated. The distance is determined
by the ne~ture t~f ~-ray radia~ic~n and can a].~-,~ye be easily com-
puted. 7'he I~anatruotion of the oorreatirn di,~gram Bo -f~ d` )
~ '.,$"
satually ah,~.n~ee the inter-dc~ut+let dietar+c � ,a.nd not the breadth
of the components. B denotes tree breadth of line measured,
Bo breadth ~~f the compone~mit of the K~, - doublet, cs -int�r-
doubl,et di�taa~oe. The fact t}i~tt~ the author oaf the article, in-
etead of usin~3~ tha value f(k, ~~ , x ), u�ee that of the function
Cord 1~2 f(k, ~' , x o) s leads to es+~sr~tialoerror$ f ~r some B- and
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