SCIENTIFIC ABSTRACT KHIZHNYAK, N.A. - KHIZHNYAK, N.D.

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000722020017-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 17, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

AUTHOR; "izhnyaki_N..A. 3()v/5j-2d_,t_32/35
TITLE.- TheAernelsof Max-miell-2quations for i1et.ero&onou--! Modia
-a
(runktsiya 'Grina uravneniy blakiavella d 1Y n(.-odnorodP_ykJi ire,
PE;U'IDDICAL: Zhurnal tekhnioheskoy fiziki, 195U, Vol 28, Vr, 7, PP.
1592 1609JUSSR)
ABSTIRACT: :Acoording@,.to the method of the Kernel :the macroscopic
Maxwell equations for.limited bodies are deduced in
integral form and several problems to 'be Solved with
these equations arelinvestigated (homogenous fi,,u-r2SP.
diffraetion of, electromagnetic waves at small.bodies a, o.).1
The integral equations describing the electro_magnetio@
field at all space points are deduced-(in the preuence
S -ten _o
of finite or infinite dielectric* with random s rs of thLi
,
dielectric and magnetic permeability).'The physical-
importance,of the integral summands for the. poihts --uri thin
and outside the electric.field is investigated.@Anulozoua
equations for the two-dimensional case are deduced..It'is
shown that the.anisotropic dielectric'ellipsoid and the
anisotropic elliptic cylinder are the only convex:bodie3
Card 1/2 the field of which is homogenous in the external

9.13QOf9.2520$9.2~572.,9..k230-1 77955
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AUTHOR:. Khlzhnyaj@, N. A

TITLE: Z:
led
Theory -of 'W vekuldos Fil With Diel.ectric Disks

-PERIODICALt
@413---',
-ronlka 61 5j Nr
Radioteklihika. I (slekt ig6o, v' 3), pp
.
11,61 (USSR)
ABSTRACT:. wwith_the incraasing@importance' of walreguideb filled with--` .
dielectrlc.@disksr as delay systems.in-.traveling wave
.@acceierators -.powerful amplifiers and oscilla ors.-o. SHF
there is aneed for a n exact,theory pf such waveguides,
taking the thickneso of disks and apiirtures in disks
into-,conBlderatlon. Th13 paper [e-mail] results
of work done by the author in this fleld during the
period 1953-1957;. reference is made also to-,his
thesis (Library of the Physic a-Tec hnical Institute. AS
UkrSSR, 1951)*, ;(1) Wavegulde Propertles WhenTilled
With-Dielectric.Disks of Finite Thickness Without
Central Orifice. Such a waveguide is equivalent to-one
Card 1/15 filled with an aniaotronic dielectri.2. The equivalency,

69901
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?i /300
E140/E435

AUTHOR zhnva
T TLE:'
not, &@-:,rhakgedl! Disc Moving Un
if oivily in

PERIODICAL: ot ro-nik& :1960
Radii ekhnika:@: elekt I Vol 51 Ar

654-661 (USSR) -
pp
AIDSTRACT I The losues of due- to polarization 6C the
and Cherefikov.-radiation@%f a charged disc 'in unifoiw@:
motion In a -delay - system, waveguide @ (uniforip'ly loaded'b
y
a homogeneous and Isotropic dielectric) are calculated.
.It in shown that the@ fi'eld-entablished by @the disc
consists- of a.-field.,"carrie,d'along".by.the'~dis,c and a
field which ,"separate a of f The power f 16v and energy
stored in,,these@'fields is calculated. In @,r'onsider
thick discs: or. systems.@.of discs the ."coherency'$ conditions.,.,-...
:are found.: By.a coherent system :the author means one n
which the energy lost-by a system of N particles
exceeds that Iof a single particle by the factor N2.
The author indicates how to avoid a formal, infinite..
radiation power in the treatment of real s@ystems' where
Card 1/2 the number of particles -is, very large (may be assumed,

25375
8/089/61/01'1/001/004/010
B102/B214
-VTHORS I Khi z hny ak, 14. 1. Tolok, V.-T., Chechkin, Yo.Y.I.Nazariovo Ntl$
TITLEt The po4sibility of acceleration of large pulsed currents in
electron lineAr-accelerators
PERIODICALt Atomnaya' energiyal V. 11, no. 1, 1961, 34 40
TEXTt This paperpresents an.evaluati6n of the suitability of different
electron linear acceleratora for accelerating intensive yulsed currents
since their region of application is only incompletely known as yet. , The
theoretical studies published here are based essentially.,on the work
carried out over many years at- the Fiziko-tekhnicheskiy institut JX USSR
(Institute of Physics and.Te.chnology AS UkrSSR), Kharkov. First, the@
acceleration.of pulsed currents in electron traveling-wave linear- accelera-..
tors is discussed. The effect of the pulsed beam on a traveling - wave
Accelerator Ace 10 cm).and a waveguide type accelerator is studied
.(Ir/2 wave,
The moat important effects are threes 1) Achange of eloctrodynamic
acceleration conditions. For v 0= cthe electron beam affects the electro-
dyne. mic properties very little, for v 0< c much more. With a load of a
Card 1/4

25375
The posd bility of ... B102/b214
current ofl-,@-la the amount of change in the phase.velocity@of the wave is
0- 2.6% (P-0-5)t1-3% (P .0 7), Q25% ( fS - 0. 9); ( P - v to). 2) Effect
of thd energy 1-dtios in ac;elerating system*' There 1113 adisplacement
of the synchronous phase toward the wave peak, i.e. toward the limit of the
region of phase stability. It ispossible to improve the energy ratios by
increasing the injection energy of the electrons of enlar3ing the section
with an alternating phase velocity of the wave. In sections with constant
phase velocity (=c)tthe loading of the accelerator by-the electron beam
leads to a decrease of the electron energy at the output of the accelerator.
For example, 12 Mw are required to obtain a pulsed curren@b with la and
5 Mev having a width of the energy spectrum of 10%. 3) Effect of the
dynamic conditions in traveling - wave accelerators. The:?e is an upper
limit of .the current; for example, at an accelerating field of
E = 100 kv/cm this limit lies at 10 a. In the following the acceleration.
z
of pulsed currents in linear acceleratore.with standing waves is discussed"-
in an analogous manner. An acceleration system is considiared which con-
sists of one or more connected endovibrators in standing wave operation.
Tr waves, h t-_ 2m) In the decelerating phaset the beam is screened off from.
Card 2/4

S/089/61/011/001/004/010-'
The possibility of_*06 B102/B214
-the field by drift tubes. @Por the acceleration of higher' currents this
system has a,number.of advantages over the traveling-wave' s ys t em, - as there,
are: 1) Change of the 'eleotro*dynamic conditions. When the condition
6
14-4-10 (X/R)4 J@o/q + JW/Q -.-D -As satisfied, the change, of the ele.etrd-
0 0 0'',
dynamic properties caused,by the elbctron:beam d6es not limit the accelera-
rissonator). JW the
ted current. NO is the quality factor of the unloaded
h.f. power, loss to the acceleration of the current of J amperes, D the
0
h.f. power losses to the walls of the system, and R the-radius of the
endovibrator.) 2) Change of the electrical conditions of acceleration.
There is a lowering of the pulse duration, and there7is aA optimal energy.
-5
,given by W 1.44-10 q D . The maximum charge that cam be accelerated
opt 0 @o
to W is Jt- 2-10-44E/E coulomba This type of accelerat6r can acce lerate
opt
much higher currents than the one mentioned before. FinaLly, the problem
of particle dynamics in a standing wave accelerator is diiqCUBSed. The
longitudinal (phase) and transverse (radial) motions are separately dis-
.cussed. The authors thank K. D. Sinellnikov, and Ya. B. Faynberg for
Card 3/4

5/08 1 /001/005/010
B 10 2 @B 241
4,
AUTHORSs Tolok, V. To Bolotin, L. I., Chechkin, V. V4@ 9 Nazarov No I.
Xhizhn,yak, K. A,
TITLEs 'A high-current electron accelerator
PERIODICALs -Atomnaya energiya:, Y.- 11P no. 1, 1961, 41 -215
TEXTs This paper presents A description of the 5-Mev electron linear-
accelerator ti,-sivned, built, and sItudied in 1955 at the P'.ziko-tekhnighesk@V
instutiAAN.USSR (Institute of Physics and Technology AS U1:rSSR). The
acceleration system consists of two coupled endoVibrators;excited to
standingic waves with f - 137-4-10-6 cps. The accelerator is fed by 12-
autogenerators,each of which delivers to the endovibratoris up to 100 kw
with a pulse duration of 400 Pseo- Each resonator is a 16-faced prism,
'1100 mm long, the diameter of the inscribed circle of the.prisms being.
1500 mm.
The prisms are made of.1 mm thick copper strips secured to a,
solid body. The drift tubes (100 mm. diameter) form accelorating gaps,ea6h
600 mm long. . The h.f. generators work in two cycles withL self excitation.
The 12 modulators deliver at the anodes of the generator-l;ubea voltage
Card 1/4

25376
8/089J61/0il/001/005/01W
A high-current electron ... B102/B214
pulses of up to 25 kv.- The resonators are kept in a vacuum chamber
-6
maintained at a pressure of (1-2)*10 mm Hg by two diffusion-pumps. The
electron gun (with tungsten cathode in the form of a flat spiral) is
placed inside the drift tube. A special modulator supplies ths gun gathode
with negative voltage Pulses Of UP to 70 ky and durations of 0,2*10'.11 and
2.10-6 sece in normal op Ioration the injection current is 6 al on pulsed
over-heating of the spiral i t amounts to 40 a. The construction of the
injector provides for the possibi lity of using an L - cathode. The phase
difference of the it vibrations in the resonators is checke.1 by an electron-
beam phase meter, and the pulse height by a two-beam oscilloscope. The
radial focusing of the beam at the output of the injector Ls accomplished
'"by the radial component of the h.f. field. The oletron velocity at the
output of the first acceleration gap is almost equal 'to th@a velocity of
light and is not further affected by the.radial component z)f the field. In
the first gap there appears also a bunching effect which narrows the phase
width of the beam from 2.2 to 1.6 radians, which value remains practically
constant in the following gaps. At the exit of the accele:"ator the beam
arose section is -10 mm with an aureole of about 60 mm. It is focused on
Card 2/4

25376
77
/089J61/011/001/005/010
1 @igh-current electron 3'102/2214
the target by means of two magnetic-lensesi its ditmeter,then become ;MM.,
To study the possibility of obtaining the maximum current, the parti cle
energy spectra were recorded at the output-of the 9,66elerator fot.different
currents. The-following results were obtained% A current of S. 5 a with
0 4,
a pulse duration of 0.2,psec is. obtained for hn electron ene,Mv f 4,-5 Mev F
e
A curr nt' of 15 a with a pulse duration of 0.2 @ksec and -an e ledtron energy
of 3..8 Mev is yielded from@the mitximinaftbe charge that can be acceleratedt.@
6
(3-10- @coulomb). At 'this pulse.duration,a current' of up to 25 a may be,'.'.
obtained, but.the maximum el;c'tron energy is onl Mov.and llohet, energy
spectrum" d t
i s@..broa er. To_rOduce I ,h ii the;-(Ionsequen
bra' of the@ @speptiitiiii@, :r d
do nin@
e
_t@-is :ne-does, ncreaLve he OnWay-, a
zes6uators. -A iii; r @Aecrease -of lhi 61ec ron energy for obtaining.
t
creased 6urrent is not converient because for radial Tocusing the.elec
tr
-time
must have --elativistic velocity,ln the first gap.., The.value.of the
average of the:current
for-this accelerator.,i@.up to 50,ua f or .15 pi
Which must be increased t;'160-150 Pulses/sec'for increasing'.the' average
current. The authors thank K. D. Sinellni%ovi P.- M-@ Zeydlita;," and Ya.- B*]-
Faynberg for discussions. V. I. Veksler and V. V. VladimirsR,iy. are. mentibn6&`
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AUTHORSs Selivatiovo No P q Pay nb erg, Ye. Bq Stepanov,'X. 1.9
KhizhnjjLk, N. 1.
T iant of a linear proton mcoel6iitoior'@'
IT LE i Choosin$ thi besf@'var
S OU@ CE4 Teoriya i raa,ohet'linqynykh uskoritelpy,- abor:iiik '80ateyo.4i I
V& Xoeoowf
tekhn. i4st. ANI"Ussf * @Bd. -by @Tj Kukoli
G6satojtiAdat, 19020,186, 202@
-that of wAveguides with die'l
TAM -.Two theories arl' studi6di eatbic Oull
-fi',tted inside, 'used to @taco el orate* proton*- to high energies, and '.Of
J-,
:ra4i&l focusing using alternate focusing'andlkdef cusiug I@ases.. r WhId :,th
e
0.,
dielectric constant tgo conductivity d,.-,d(X,Y$Z) a.reitim'M-
independent, +-.k?Z divZ-- d(@n ok xlc'.)S holds, wh e
gra or
2
2
k itd(iA, 440 "denoting he t eikue@nq:and. J.Ahe tuiirent-den
t
the, base f 'a d rox)
"o In axisymmetri and zero@turrek the'pro uct- A,(r@x)
R(i)Z(Z). is formulated 'go &a-'to:obta.in th6'o.omponento ol' eleotric.@, and
magnetic field strengthev.
ard.
L

8/66i
/62/000/000/oij/
Choosing the-beist'variant of;.. B125/BI02
-':t - er (,w+tb)/(a'+b) (a+b -Aj6@tb) 'The mean. phao a vel6oity in
:z
it, is
guide containing dis'ps is smaller than that in,an empty waveguide,
greater than that. in one containing'a-dielectric'.."The attenuattQn'of-- the
fields due to the infinite conductivity is proportional to 9 M;4 where.
4.,( a+b
03)
Y COO
(as+i)(a+br) I/Ta 4- b) eol.
71-
als +b
:and m The power losses
--pe unit- lengW from a waveguide
co
-1()S=t,YS. When the structural
ing dielectric discs amount to@D (1-0
period remains,oonstant, the. phase@ velocity -.of a wave in *.a )raveguide itt'041
with dielectric diso@ is varied bj changing the.,Pelative thickness, a/by"-.
of, the diaos. Linear accelerators withalternately arranged magnetic lens .ea.-
poesess_regions of stable motion in the y and z directions uorresponding to@
certain values of magnetic field gradient and lens length. The etabilit
conditionlof the motion in auch:traveling-wave acoeleratora-.reads
a-
Jfr. CO$ IF$
-a
H CE M TS 0!5),
Card 3/4
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3 022@
S18151V6210001000101
Choosing the best variant of...@ B125/BI021
'where 1 is the length of the,-lerts:* Proceeding from the oquation of! mot iofi.
of a standing wave accelerator with drive tubes when there fire six 6agnet,ic:
lenses per period, 'the condition obtained for the region of,stable, particle,
motion is given by

E
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7 6/661/62/000/600/ .C114/622
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. 4125/BiO2

AUTHORs, Khizhnyakt N.-, A.

TITLE I '@ta -ing'-4i-qle@trio'
on a tr,@.V! eli'g
A waveguid4 cc in discs workin@;
.
n/2 Yraire
J.-
SOURM., Teoriya i iasohet.',lin4Ynykh uaariteley, aborfilk'statey.t41t'!
^
tekhii. ins t . AN USSR.-Ed. by T.".V. Kukoleva.
M,)soows
Gosatomizdat,
19629 203 210

The
TEXT .
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The wavele ngth X in the waveguidOr is taken tb be of, the a me:,Ordei in the

perioid'of 'I @@the dispersion equation
the structure (a+b)

'
@
Pie +P21)
k
L
-
.
Cos placos p,b sin pa sin P,b,
,,
2ppic
holds for waveguides for accelerator's
(F-) liritho'ut
with dielectric discs
apertures ,
,
in thest then the r-f,power flux is obtained as
S sin k3L o
((FO
7T
- I

I ard I
C
14 OW)
X

6

2
i)0/0
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000/
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k waveguide oontaini go." B125YB1
0
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Besee
ro-or
t of the it
r,
the first roo I
R t -t
e *aveg,dide cr
he radius of h
.
0
,function J d a is the distance and b the thickness 61 the dis'Cof
0 0
2x/X p2 k 2 d P2 2
a+b, k 2RA, k '/R)':o and k.
L 2
9 .0
:,S on- th'
9, axii@
The equation defining the eiffective'-@el_eotrio field etrength
,
0
of the waveguide is, 'obtained fro 8)0 :together, vith

sin kL _L Ll
ru
S
Us

For thin; discs
@'(P) holds, and L/ @8(a+b)/(a+p_b) !I/S
.
2. r:
h
is,,,the-',longit idihal compohent of-.t 9 dielo tric@cd t t
ae+b
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1 ted,.
a+b aP-+b When,_(1)_,1s:.is@,1a
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ik" R2
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special.case
v alues and b
@with the effeoti e 'u. (L)/L In the
,
r
Card 2)4

SSION NR: AT4036075
A
CCE
efficient (M ion mass) m _@-@electron mass), so that the gradient@-
of temperature becomes equalized much more rapidly than the density
gradient and the former need be taken into account only on the plas-
ma boundary.- The diffusion of a plasma pinch detached from the walls
in a longitudinal magnetic field, or the diffusion of a plasmoid in
a reference frame connected with the plasmoid,.are considered neglect-
ing longitudinal spreading.. It is assumed that the plasma is stable
against various types of disturbances. It is shown that the self-
similar soiution describes well the qualitative pattern of diffusion,
of.the plasma pinch transversely to*the magnetic field for arbitrary
initi al smooth particle-density distribution. Self-similar solutions
can also be obtained-for the temperature distribution.. Magnetoby-
drodynamic instabilities can cause plasma-to leave the pinch at a
rate close o.the.thermal velocity.of the ions' On.Lhe other handi
t
instability can produce turbulences in the plasma and also conse-
quently incriase the dififtelont "Zn conclusion we &Lee grateful)to
K. D. Sinellnikoi and A* X* -Akh;Lyezer for-continuous'interest.in the
Card

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ACC 'NR,: AT5022287

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114N,
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AUTHOR'@ N.- So Kh zhnYa*,_.N@L
71.
c etchnical .
ORG: Academy'of- So ences 06ii ot nstittgg-Wademiya. niadk tJkrSSK
riziko-tekhnichoskiy.institut)
---TITLE: - multiveldcity- plasmoids-
R ivistitut Doklady, no4 074/P-028, -1964..,
SOURCE: :@AN _UkrSS :Fi_ziko-tekhnidheskiy:
,Prodo nyye kolebaniya v Mao kolmthom plazmannom puchke, 1-8,
9
TOPIC TAGS,: plismoi4i:, I be klVetr(m
il@ftvi J
ABSTRACT: Thermal--- dis on 1i 'to determine themodulatin
persi Jhj4ystrons is st died
a
ation of axwAie
properties of: beam bunching _T - ei:appropriake equ motion and-.H s: equ
tion!@ are wiitten, for'. the -4on and, electroTuv for the @ collisionless -case. By.-select-
ing particles within-a smail velocity.interva l..,moving through modulating: grift.,
Euler's equation can:ba written'dit4'a non-linear system results. Approxim4tion me-.
-.--tho.d3--are.-use.d..tol--rhow--th,at-,inLtL&I therma~,L.-diapersion,-Int-roduc,es--i-tiultit)~lfing-fac-
tor which. -lowers the @,value @ of the@_ cm-rent density of the bean.: The m ultipl.@ing-lac'-*a,
tor is determined for the case ofla step fimction distribution. The assumption.of a
-Maxwell distribution isalso discussed. multiplying factor is shown to have.a-
09 pace and it is det is,
meaning of coherence in vel dity a ermined that Lta struct

L 31285-65
ACGE-,&%ON NR: AP5005348
AUTHOR: R22alov# N. S.;
,SOURCE: Radiotekhnika f eI'e&tJeoziik_a, v. 100 no. 2, 1965, 334-340
TOPL-C TAGS: electron beam, _t@ @st=-"/
A single-variable problern of the irterartinn cif 4 field-, ompersa-..,!d
ai.'I @,;@,@n a J'arnmat-ad dielectrlc %, ho.;@- n".) r@o4 4. r-"'-i
A litipersion tI--(4ia--i'
ri I
.)n ii c.n a c V
n s
'%mPlItuder'. Formulas for the d r. 1 t viidl i- -r e_,; c, nan r p
the exr@t7i,

L 31281)-65
ACf-=SION NR: AP5005348
:@!'tude of the modulating voltage be,:ornc-6 The p(ji;s;bIIty of
ibrvi, mLchanisrn for compersati.- v the e- narve. effactii m a
A -iri Al :r-,:
M]-I T ED: 0ZJan64 ENCL: 0) SUB 7,ODE: EC
S 0 V: 005
OTHER: 003
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tI.LIILt:ZiX. 'tL4&, 4fjww VA04(dal @,L , In-UM.UnIly UPX-UIV_.YfIYUMVgCF LermoyaUCL-ROWSW Z -
sinteza (Physics of plasma-and problems 'of-controllable themonuclear synthesis)-t-
doklady -konferentaii.- - no.-- 4.-@- Kl,ev@,-,@Yaukova -dumka IL965 389 40
TOPIC*TAGS: magnetic trap, relativistic particle, plasma charged particle parti-
cle trajectory, Particle motioa,. magnetic field
ABSTRACT:@ The, pmpertj.48_ of c6reed particle motion irt magnetic traps of the "pick
et fenr
.e" and .%agnetic. wall" (with negative' field curvature) typeSJire con-suered
and their trajectories:deterwined.by numerical integrations-The traps are. charac-
terized by axial -symmetry and Wall angles between field lines. L The analytical
form of the,fields is-dis"Ibed by-the expansion of the scalar magnetic
Card: 1/2

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@kCCVESSIOH HR: APS012047 i@@ /64 /0827/
@_Ml 1 @"R: nizhnyak, N.A.
I ")ne It -ad in;_1 I
-.1comeit of
magnetic f leld
S@M=: Zhurnal tewinicheshcoy fiziki, v. 35, no. 5, 1965, 827-032
1UP 11-: 1A.GS Wharged particle motion chargred parti:@le beam, 1,)Tyitwinal maf@netia
-1' r1r
The author calculated the magn-@tic mornent (ratio of the trutriswerse:
jnergy to the magnetic field styerqth) acq%iired by a ch-Irge Particle
the tmiform region ot an axially symetrllo mrqgTieti,- ficlcl. I f t.'Ie
pa rt- i c le moves on t1le axia the magnetic moment rera.ris zerr)! otherwiac- thf_@
inoment depends on the distance of the particle In tt.c field-fred region
symmetry axis, the velocity of the rrlrtic)@, the wt.netic field '7,trength
region, and the manner In -which thc lo@igtud@io.I mvignetic fleld
NIP
large dlstance!@ tr) it- 1;-.'i
,4'@b from zero at
Liii@ are performed by solving the eq ua t I on.; 'I"" I Mrzi -Ii
Card 1/2

ACCE3SION 1M.- APS012047 2-
-f the =K-netie field and tho !qf1Djt1')n-Q PO (7-lb-tained to
i@ wt
.1 i 0, t, yvr@ f f f 1 1
v@i i n t r. i n
1 It, f-, 1 " 1i I i
in the dstarcf--
Ign -"U5 i
@ etic :told. In conr` L;if-
M
Aclidenician K. V.Si neJ. nik cf ', I
,n t he
t 0 y U. S . A zFDAky- I or ntwte ro ug d I s c u@ s i u ns urig. rt. has: 34
u --I-g .

us @:A hd- @ 1: - d6hse plaiftf@'
-h4 jliiitl
f tald Is diac wed. f or -t -
Calculations are hased '611 th6 flotj6j; J&t& ft 100pi, rlo@el, the equations: r
Obtained from the MtgnetchydrodynarJ:@ equations by :-ategratingg in
,o lonq
qA ad -nd tL
ii *,ed 611- if'* acreage rr a Z@
tile Variation of t-hd---
t. A
to its f inal unif value rn th :case of a raref ic-1 plasma the relative ch
Orm
of the magnetic field due to the plasma eurrunt is neg'igible and each plasma
mioves in the unpertuvbed field. In tne caso cf ft dense plasma- tho
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CC; rd 2/2

2 0 1 Wr (0-M&PA(w)-@1
I)f /Fab-10 IJP(c) AT/
1jR,,'O()57"6 5/035/005/U847/0857
NR: AP5012049
AUTHOR: Kh1zhMk, N.A. Y
T17T : I
E Motion of a finite planma in the magnetic fiv1d of a toroidal soleno
SOTIRCS- t~kh-nic-h-e-,q--ko-y*-,-Ii'ziki-,---V- -35 no.' 5, 1965, 847-857
TOPIC TAf-ar 0iis6a:--:-,mag Plasma pola riza tion, pla 8 Ma f low , plasma drift
RACT! Me idthor-dise-uss tot- - 4
A T_jT d f V t he: motto a- plasssa of finl.te extent in:a
f i dwlt@-. curved lines of force, such as 17 prod,,@ccf- by a toroidal sole-
:!iscusnion was undertaken because it has fo-vl (B R, @S I f rr inov et
c ond i t i on -)e pl,i , mia w i1 f,) Iow the
6 1962) that under suitable
Onci ir@qf- hPivy lmn@irltv .ojms @E
F -3 3 1 , . I fia s s how n t ii,, t t_ s_- t , nIr.
I q-90)
predict that it will not. The auth:>r fir-it solves the equations
for a 9 Ingle charged particle In an ax i1a s yru@t7 i. i- -c i1eld havllig only
an azi-muthal component and dizicusses the motion of a rarefied plasma an the basis
It is fou&4 that the rarefield alasma tends to follow the lines
th@it --inder suitable cu;ulitions of vellnc t,;. f1el ! strength, 'rind ftelld
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7
L 52016-65
ACCESSION NR.- AP5012049
curvature, the plasma will lose heavy impurity ions to the waLls of the container.
T- (",icuss the motion of a dense plasma the iuthor use: tile P-jultions of the drift
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