SCIENTIFIC ABSTRACT SHPICHINETSKIY, YE.S. - SHPIGELBURD, I.YA.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001549920017-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 9, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

ROGELIBERG, I.L.; .; BARANOVA, L.M.; PUCHMV, B.I.
Technology of manufacturing and propetties of nickel-tungsten alloys
in connection with their use for the manufacture of filamentary-
cathode tubes. Trudy GiprotsvetmetGbrabotka no.18:233-242 160.
(MIRA 13:10)
tNickel-tungsten alloys) (Electron tubes)

ROGEWBEaG, I.L.; SHPICHIIIETSKIY, Ye.S.; AGAFONOV, A.Ki; PUCEZOV, B.P.
Some properties of oxygen and sulfur-bearing nickel for anodes.
Trudy Giprotsvetmetobrabotka no.18:243-253 160. (MIRA 13:10)
kNickel--Metallography) kElectrodes, Nickel)

DNESTROVSKIY, Nikolay Zellmanovich; POIERAiTSEV, Sergey Pikolayevich
(deceased]; ZVEREEV, V.V. [deceased]; SHPICHIMSKIY9 Ye.Swg kand,
E-N. ~q
tekhn. nauk, retsenzent; POSTNIKOVp N inz ~.j re ~senze~-,-RZHE7,
NIKOV, V.S., red.; KOSOLAPGVA9 E.F., red. izd-va; BERLOV, A.P., tekhn.
red.
[Brief manual on the treatment of nonferrous metals 'and alloys] Krat-
kii spravochnik po obrabotke tsvetnykh metallov i splavov. Moskva,
Gos. nauchno-tekhn. izd-vo lit-ry po chernoi i tsvetnoi metallurgii,
1961. 410 p. (MIRA 14:8)
(Nonferrous metals) (Metalwork)

S/0-80/61/000/020/007/013
D258//D302
AUTHORS~ Rogellberg; I. L.j 3 Puchkov, B.I.
and Titova, A. S.
TITLEi Nickel alloys of high electrical resistivity for caihode
filament bases in radio tubes
SOURCE: Moscow. Gosudarstvennyy nauchno-4Lasledovatellskiy i pro-
sektnyy institut obrabotki tsvetnykh metallov. Sbornik
nauchny_lv_,h trudov. no. 20, 1961, Metallovedeniye JLI obra-
botka tsvetnykh metallov i splavov, 1IT-124
TEXT: The present work was aimed at developing Ni alloys suitable
for the manufacture of fi.lament bases in the so-called 'economical.'
radio -lubes. Suitable alloys were required to possess electrical
resistivities, of 42 microohms-cm at room temperature and of 114
microohm-cm (at least) at 8500C. 84 different alloys were prepared
by quickly melting the charges in a high-frequency furnace. The
products were subsequently reduced with C and Mg, poured in gra-
ph-ite forms, water-quenched from 11000C, then rolled, annealed at
Card 1 3

S/680/61/000/020/008/013
D258/D302
P
AUTHORSg ~Ih-u, ee--tMa-k--~,-~ togellberg~ I. L., Luzer-berg;
A~ -A~o' ~,o omo zina, Yu. A. and Agafonov, A.
TITLE. Investigating the darkening of nickea strip due ~.'o an--.
nealing
SOURCE. Moscow, Gosudarstvennyy nauchnc-issledcvatellskiy 1 Pr'D-,
yektnyy institut obrabotki tsve-,nykh metallov, Sbornd'v
nauchnykh trudov.. no. 20j 1.961. Metallovedeniye -L'. obra-,
botka tsve-u-nykh metallov i splavov, 125-135
TEXT-~ The authors investigated the effect of composition and of
various technological factors on the occasional darkening of ni3kel
strip (grades Hnz(NP2) and MKOZ (NK02)), occurring after heazing
for 4 hours up to 780 - 800oC, annealing for 3 hours and cooling
to room temperature cver 8 - 10 hours. Darkening was due to the
-5 _ - - 6
-formati.on of a strongly adhering 10 '0 cm thick film which
was found to consist of carbon, The effect of composition cn dar-
Card 4

s/680/6'/000/020/003/013
Investigating the darkening ... 1~258/I)302
kening was investigated on thinly rolled samples of darkened strip;
the specimens were electropolished and reheated in. vacuo. They
were then slowly cooled or quenched from 780oC. Films were formed
on 92.2 slowly cooled specimens with more than 0.04% C and 0.04% S-19
but not on quenched specimens. Microscopic study showed that gra-
phitization usually started from the crystal boundarie2. The in-
dividual effec-t of C and Si on darkening was studied with samples
annealed 41n vacuo and containing 0.02 - 0.2% of C; Sj, P1g and oth-
er reducing agents~ With samples containing C alone, the darkening
occ,urred. at 0.0"!% C and more; the presence of Si raised the con-
centration -limit by 0.01%. The effect of lubrication on darkening
was studied by coating samples with transformer oil prior to an-
nealing. The presence of oil enhanced darkening in samples con-
taJLning more than 0.04% C, while it had no adverse effec* on sam-
PleS wi-th lesser ccncentrations. The chemical analysi-- of 253
plant led. rolls showed that no darkening ol-curred in rol-Is
''le 0,06% C --:auspd intense darkening,
_cnTaining 0.02 -- O~03% C, whi-
the to al concentration of reducing agent's was, qualitatively cn-
a r d 2,14

S/680/61/000/0201/008/013
Investigating the darkenin.- D258/D302
CD
ly ', related to the extent of darkening, Application~of various oils
n plant cond-itJons always resulted in dark
1 4 -L ening; yet the removal
of these oils, prior to annealing, had little effelct or. preventing
it. No dependence could be established between the COMP031tion of
furnare gases and the extent of darkening. No change was observed,
on substituting hydrogen or water vapor to air in the furna-e
space, cr on annealing in vacuo at 1o-3 mmHg, The latter treatment
even enhanced darkening. The 'laboratory treatment of quenching
CD
showed equally good results when applied in plant practice. Thus,
rolls of nickel strip were cleaned, thinned, packed in Ni and Cu
foilo-, heated for 3 hours at 7800C, and quenched in water. Only two
out of ten quenched rolls showed traces of darkening in their mia-d-
le portions, Finally., N--I strip was annealed by continuously passing
it thrcugh an elect-r-ical furnace, under hydrogen, at 8500C, at a
rate of 3 - 5 m/min~ This treatment completely prevented the oc-
curren~7e of darkening,
, provided tile strip was quenched immediately
on leavirg the furnace. The film is assumed to be formed as a re-
sult of the decomposition of a supersaturated Ni-C solid solution,
The authors assume that in the course of annealing-. carbonized oil
Card 3/4

S/680/61/000/020/008/0 13
Investiptinl-,_, t.he darkening ... D~2581/1)302
diffuses _1_ntr~ the metal and is taken up to the liml4t of C-Ionten-L.
,
n the so'-d solutiori at 8000C (0.13 C'. There are 4 tables, 5 fi-
r -1 0
gureo and 5 references.- 3 Soviet-bloc and 2 non,-Soviet-bloc. The
references to the English-.language publications read as follows,
Metals Handbook, N.Iokel-Carbon, p. !183., (1-948')~ J. J. Lander, H.
E. Kern and A. L. Beach., J. Appl- Phys- 23, !2, (1952).
Card 4/1

5HPICHINETSKIY, Ye.S.; ROGELIBERG, I.L.; LUZENBERG, A.A.; GOLOMOLZINA, Yu.A.
Prinimali uchastiye. MIZONOV, V.M.; GALAKTIONOVA,
GU.; GAVRILOVA, N.G.; SAK30NOV, I.P.; KOFEYKA, E.I.; GLEBOV, V.P.
Investigating th darkening of nickel strips during anneallfg.
Trudy Giprotsvetmetobrabotka no .20:125--135 161. WIRP 15:2)
(Nickel--Heat treatment) (Annealing of metals)

'ACCESSION NR: ARW18342
ISOURCE: HZh- Metallurgiya, Abe. l1662
s/6137/64/ooo/ool/ilol/nol
;AUT11OR: Shpichinetskiyt Ye. S.; Yemellyanova, Yu. A.
1,TITLE: Processing indium and indium-~tin alloys and their connection properties
.CITED SOURCE: Tr. Gos. n.-i. proyekt. in-ta splavov i obrabotki tsvetn. met.,
jvy*p. 21, 1963, 91-97
!TOPIC TAGS: nonmetallic radio component , nonmetallic component joining, quartz
;~ono6rystal, indium, tin, eutectic alloy,.ra~Iio Acousticsy,salt monocrystal
TRANSIATION: Research was conducted on the possibility of having a stable connec-
ition of nonmetallic elements of special radio devices produced of quartz and salt
!monocrystals, with the use of Al, Pb, Sn, Cd, and In and their alloys. Only
eutectic alloys of In with Cd, and especially with Sn provide sufficiently stable
,connection and possess fully satisfactory acountic qualities - An advantage of the
i In-Gn alloys also is their low temperature of eutectics (1170) and their adaptabil-'
lity to vacuum-solid soldering to glass. -The possibility was demonstrated of obtain-,
jing high-quality foil up to 2-3 microns in thickness out of In And its alloys with
Card 1/2

iACCESSION NR: AR4018342
Gn, without intermediate annealing at low speeds of ro" ing (1-2-2 meters/min).
To provide a strong good connection between nonmetallic elements of an instrument
l
and to provide the needed acoustical characteristics, an eutetic alloy of In with
148 plus-or-minuB 2% Sn is recommended. A strong connection is achieved under con-
idition of heabing the joined elements at a pressure of 20-25 kg/cm2 at a tempera-
Iture of 1.12 plus-or-minu.s 20 for 3-5 hours.
So cots: EC ENOL: .00
Card 2/2

DJ?kb) Pr-.4/Ps-4/Fad IJP(c) JDjMii/hW/,iH 1; qq,
ACCESSION N`R: AP5009744 UR/0136/65/0001004/0070/0072
MTHOR: Shpichinetsk~X, Ye. S.
TITLE: Study of the 'toj! ding of metals due to their joint cold rolling~
SOURCE: Tsvetnyye~metallyj no. 4,- 1965, 70-72
TOPIC TAGS: cold welding, cc .Id rollin-&,-metal
.a: bonding, zicrorelief ,
orientation, adhesion, diffusion, microcracks~. blmetal`strip nickel stiip~ copper.
strip, stripp;Lng, i~etallographic investigatiorii7~_pectjal. inve'sti tion
&a
Id rollin-
ABSTRACT: -A three-layer nicke -cc er-nickel stri wash cold-welded by c'd
iniorder to investigate the concomitant a&aslon, diffusion, and friction effects
After the cold-welding the nickel layers were mechanically stripped of the copper
and the increase in the content of copper in nickel, and of nickel in .- -copper, Wag
spectrally investigated ab a function of the roughing stress. This,was.follcwed
bv metallographic investigations of the contacting surfaces between thetwo uLetals.
immediately after their separation by stripping. Contrary to expectations the
-aetallographically observed deformation of the surface layer vas too extensiye to
,d
,7
INC-*
- ~41

SHPICHRETSKIY, Ye.S.; MACHULISKAYA, G.A.
Investigating changes in the composition and plasticity
of the copper-aluminum-magnesium alloy during hot pressure
working and during annealing. Trudy Giprotsvetmetobrabotka
no.24:311,-323 165. (MIRA 18: 11 )

24430-66 EWT P (1YJ1,AT.4E-6P (t ),/PIP (k IJP (c)
SOURCE CODE: JD/ 4/0323j
ACC INR: AT6oo6484 UR72'18'6pl65100010241031
chullska.va, G. A.
AUTHORS:-Shpichinetskiy, Ye*. S.; Ma
ORG: State Scientific Research and Deqjgn Ia�titute of
.1,Tetalit-o'-r*k-i--'--"---Ii.-I-o--B~~~v--T-G'~~-uaarstvenny-j iiauchno-issledovatellskiy i proyektnyy
insti-but splavov I obrabotki tavetnykh metallov)
,TITLE: Investigation of changes in compooition and plasticity of coppe -alumblum- i
.magnesium alloy as a result of high--femperature compression and annealing
)~7SOURCE: Moscow. Gosudarstrennyy nauchno-issledovatellskiy 1 proyektriyy institut
splavov i obrabotki tsvetnykh metallov. Trudy, no. 24, 1965- Metallovedeniye 1
obrabotka tsvetnykh metallov i splavov (Metal science and the treatment of non-
~ferrous metals and alloys), 314-323
al-c-i um alloy, copt "'I~lloy, m'ag~Lesium alloy/
TOPIC TAGS: Br.AMg6-1, 110 copper,
AVOOO aluminum, Ifig.1 magnesium
S-
'ABSTRACT: The object of the investigation was to determine the cause of the
Unsatisfactory performance.of secondary electron emitters manilfactured from the
alloy Br.AMg6-1 with 5.2-6.0%. Al, 0,9--l-3 Mg, and the rest Gu. It-wao.ouspected
Card
1/3

_L 24430-66
A.CC NR: AT6006484 4j
that the failure in performance was due to burning off of magnesium during r0 91k
iand annealing of the_Rgj-Ajli_q_ filament. J~j The alloy was prepared from oopper-MMJ
aluminum AVOOOJVand magnesium VgI.'j/The effect of annealing of the alloy specimens
after hot and cold rolling at diM.~ent temperatures and in different ambient media'
(air, ammonia, and vacuum) on the magnesium content and plasticity of the alloy was,
investigated. The experimental results are presented in graphs and tables (see
Fig. 1).
VII
Fig. 1. Change of the magnesium 43
content of a Br.AMg6-1 alloy ribbon
A- -,11,,
as a function of --',he annealing time
during annealing in air at 650C.
1 1.3e. Mg; 2 1.23~. Mg.
3
Annealing time,_ 'hours
Card 2/3.

ACC NRI AT6oo6404
it was found thatduring preheating for purpobee of hot rolling and during anneal-
ing in air, the magnesium in the alloy BrJMg6-1 undergoes selective oxidation.
D-ixing subsequent- etching of the ribbon, the magnesium oxide is dissolved, leading
;.o a depletion of the magnesium content of the alloy. Neither the degree of
compression nor the specimen thiclaiess had any noticeable effect on the oxidation
process. To obtain a soft ribbon of a given magnesium content, aimealing must be
carried out at 650C for a period of one hour in vacuum or in inert atmosphere, or,
if air contact during ~innealing is unavoidable, ia limited contact with air. In
the latter case, the alloy should have a 1.3--l-elo initial magnesium content.
Orig. art. has: 9 tables and 5 graphs.
SUB CODE: 1 j -3/SUBM DATE: none/ ORIG REF: 004

ACC Nil; APu,j_)~)47~~
jij ~1. ULiu k
1NVF!;TOR: Gurovit,;;, S-plchincts~,'y, Ye.
ORG: I, c n e
TITLE: L'Ilethod for aco,,~stic conductor
of an ultrasonic delay i-ine. C 1 -1 S Z; ;,u- 1059~J,; Eannounc;~Q t'ne State Sc*
ientific
Research and Design InsLitute cf Ailoys N;~nfLri-t-i3 Tlrocr~ssing (Gosudar-
proyel, L , j"_4
~Ut splavev -,* obrabotki
y
tsvetnykh inetLllov)j'
SOURCE: Izobret prom o)*i)r,-1.-.,, tov Fla. 1,8, li)(66,
TOPIC TAGS: piczoelt2,ctric transducer, ii1trasonic wave, circuit d~-_-iay line
ABSTRJtCT: This kutiioi-'~, CertiC'I'cite ~Lii',ro(iuces L method for connecting a piezoelec-
',ric transdl.icei, t-o. 'Llie ~icou:;.ic cen(iucf,or of all ul,Lrasonic delay line DY Using a
i metallic matc1lin-1-- ITLYt2r. Ti; ba---'~Widtil and therm;al stability of the delay line are
U
iincreased, an nik~criin ca' an' c-ouztic contact between the piezoelectric transducer
Iazna acoustic ii~c using, aii indiwm alloy 'or the Joint containing 0 5-
2
25i'~ thallium, rc. .2 c~ 20-21 k-/cm, at a temperature of !45-1500C and hold-
ing under thesc condiLioris for _3 - 6 h- c, ;j 13
SUB CODE: L;'-,-"
Co,d bmc: 621.374.5

6-2-
ACC'NR: AP6032 3 SOURCE CODE: UR/0126/66/022/003/0432/0437
AU176OR: Khayutin, S. G.; Shpichinetskiy, Ye. S.
ORG: Giprotsvetmetobrabotka
TITLE: Specific features of plastic deformation of indium and its alloys
!SOURCE: Fizika metallov i metallovedeniye, v. 22, no. 3, 1966, 432-437
'!TOPIC TAGS: indium thallium alloy, alloy bend test, alloy structure; pla'stic defor-
mation, indiwi, indiwn base ajloy, thallium containing alloy
ABSTRACT: The plastic deformation of 99.998%-pure indium and indium-base alloys
:containing up to 40% of 99.9995%-pure thallium has been investigated. Cast alloy
:specimens were electrolytically polished and bent manually to 1-2% elongation at
iroom temperature. It was found that pure indium deforms by slip, without any
sgnif-:cant amount of twinning. Indium alloy with 1% thallium deforms by slip-and
I twinning, the amount of the latter increasing with increasing thallium content. De-
l
,formation of an alloy with 35% thallium procedes by twinning only. However, indium
!alloy with 40% thallium which has a face centered cubic lattice deforms by slip
I
'without twinning. Twinning forms in indium deformed in liquid nitrogen at -196CWL-h sup
,'lines observed at the same time. The tetragonal face-centered lattice in pure indium
!changed into a face-center'ed cubic lattice in solid solutions containing over 35%
ithallium. Orig. art. has: 6 figure6. 002/ OTH REF: 002
1SUB CODE: 1l/ SUBM DATE: l3jul65/ ORIG REF:
1/1 UDG: 546.682:539.374

11 (2, 4) PHASE I BOOK EXPLOITATION SOV/2213
Groznyy. Neftyanoy nauchno-issledovatellskiy institut
Khimiya i tekhnologiya pererabotki nefti i gaza (Chemistry and Tech-
nology of Petroleum and Gas Refining Processes) Moscow, Gostop-
tekhizdat, 1959. 278 p. (Series: Its: Trudy, vyp. 4) 2,500
copies printed.
Executive Ed.: T.D. Yefremova; Tech. Ed.: A.S. Polosina; Editorial
Board*- A.Z. Dorogochinskiy (Chairman), B.K. Amerik, G.I. Kazlmin,
N.M. Kamakin, V.I. Lavrentlyev, Ye.S. Levchenko, and M.G. Mitro-
fanov (Deputy Chairman).
PURPOSE: This book is intended for petroleum engineers and technicians
in scientific research institutes, planning organizations, and
refineries.
COVERAGE: This collection of technical papers on oil and gas refining
were originally discussed at the petroleum refining section of the
Third GrozNII Scientific-Technical Congress in 1957. The articles
have been published to help further the development of the petroleum
Card 1/9

Chemistry and Technology (Cont.)
SOV/2213
refining industry and petrochemical industry in the Chechen-Ingush
ASSR. The history and significance of the petroleum refining in-
dustry in the Groznyy region is outlined by A.Z. Dorogochinskiy
with emphasis on the interdependence of the refineries and the
aircraft, automobile and rocket manufacturing industries. Change
in modern engines demand a change in fuel and lubricating oil
properties. The increased use of jet aircraft makes the produc-
tion of high octane aviation gasoline less important than the
production of the new type of fuel, aviation kerosene, the yield
of which requires a quite different refinery run. Since crudes
recovered at the Karabulak-Achaluki fields represent a valuable
raw material for manufacturing lubricating oil and paraffin wax,
their properties have been thoroughly investigated and results of
analyses reviewed. The re-equipment of the fuel producing line
of refineries at Groznyy has been carried out on the basis of
findings obtained from tests and pilot plant operations, and a
number of reforming and platforming units have been built to up-
grade the low octane gasoline produced at Groznyy. Tests were
also conducted to ascertain the advisability of applying the
destructive distillation of residues, which yields solar fractions
badly needed for catal tic.cracking unit as feed stock. Catalytic
cracking units of the 43-102 type were first put on stream in the
Card 2/9

U"hemistry and Technology (cont.)
SOV/2213
Groznyy refineries in 1952, and since that time continuous efforts
have been made to boost their processing capacity, and improve the
regeneration of catalysts. The authors make a number of sugges-
tions as to how the throughput of the above units might be in-
creased. The production of different types of pelleted and bead
catalysts, the contamination of catalysts and their reactivation
are discussed. The operation of a contact coking reactor, its
design, and products yielded by contact coking units are described.
The authors also deal with the manufacture of lubricating oils,
paraffin and ceresine wax and indicate way of improving their
properties. Electrical dehydration and desalting of crude oil and
of light products are discussed. The authors state that in recent
years extensive studies were made on the chemical conversion of
petroleum products, and particularly of gases. As a result, a
number of gas fractionators and compressors were built and installed
to produce phenol and acetone from propylene and benzene, to syn-
thesize ethyl alcohol and oxidize paraffinic hydrocarbons. An
article is devoted to Droblems of automating various processes and
developing the related control and gage instruments. The book
Card 3/9

Chemistry and Technology (Cont.)
SOV/2213
contains numerous tables with the characteristics of different
petroleum products obtained from refinery processing units, pilot
plants arid petrochemical refinery sections. Each article is
accompanied by references.
TABLE OF CONTENTS:
Foreword
3
Dorogochinskiy, A.Z. Contribution of the Groznyy Oilmen to
the Development of the Petroleum Industry 5
I. STUDY OF CRUDES AND THEIR PRETREATMENT
Bortsova, M.P., P.B. Gamayunova, A.B. Poplavskaya, and
N.P. Shpichko. Choice of Demulsifiers for Crudes Processed
at the Groznyy Refineries 17
Levchenko, Ye.S., Ye.N. Bobkova, O.A. Artemlyeva, and
Ye.V. Karaybog. Study of Crudes from the Karabulak-Achaluki
Deposits in the Chechen-ingush ASSR 27
Card 4/9

BORTSOVA, M.P.; GAW-.YU]TOVA, P.B.; POPLAVSKAYA, A.V.;_~~~. ~.,
PAVIDV, G.D.; PODILTIA)VA, A.T.; IA)VA, N.I.; ALEKSAIMMVA, R.F.;
ATARTNOV, A.G.; VOROBIYEVA, Ye.I.; GANITAIITS, E.M.; GELLETI, D.Ta.;
PARSIHINA, M.A.; FILINA, R.A.; CHMLYAYEVA, Ye.S.
Solecting demulsifiers for crude oils processed in Groznyi refineries.
Trudy GrozTTII no.4:17-26 159. (MIRA 12:9)
l.Groznenskiy neftyano7 nauchno-iseledovateliski7 institilt (GrozNII)
(for Pavlov, Podunova, Lova).
(Groznyi--Petroleum--Refining)

,6- t1? 00 69665
.,.!jT 110`~,*, Luzychtn1co. L. A., Ehpiparl, 11. P., S/153/60/003/01/005/07)8
'Kdmneva 1. 3011/3-005
ATTO
TIT. .1pproximative ',I,--"-hod of Calculating the form Of Alkanesland
Their Radicals
1~i,2110DICAL: Izvestiya vysshilh uchebnykh zavedeniy. Khimiya i khimicheskaya
IT
tekhnologiya, 1960, Vol 3, lir 1, pp 24-28 (Us-sr)
T"EXT: I. t i sthe purpose of this paper to develop a calculating scheme 'or the
standard heats of for-mation of alkanes arid their radicals. The determination o,'
this heat is coi-anlicated for the-saturated aliphatic hydrocarbons, but somctines
i.,~.iDassibi(~ fcr the radicals. The usual calculating schr~mes (Elefs 1-4) have manv
shortcomings. Therefore, the 1.Uthors sLigoested an04-her dependence for the elec'-_-.--_
neEzativity o~ carbon: E c = E0 + aIn ( 1 ) where F0 is the electric n,gativity of tl-~
c-irbon atom in ruc-Ahnne (=1.190), -a and n are empiricai constants, and !is a
certain characteristic value calculated by.the formula
ca + 0.318ZE C + 0.16 ZEC ( 2 ril' C " are the values of electric negativity
A r XIAlir
of carbon atoms in the DositionLi a-, A-, Lind r 'Go the respective C-atom. The
_iuthorL; proceed from the assumption made- by G. V. 3ykov that the fraction of the
electron cloud sent into the bond by the corre-sponding atom is proportional to the
bard 1/3
I

69665
,!c t h ~D a o ~_. Ca ! o. ul a t i ric, ~ 11.- -,/155/
V., , 6o,; cr -; `c; 1 /005/058
orrn, 7D 1) 1 1/3C05
and- 121-.eir __:ad Ic-a1z; I
~I(ictroneE:ativity of another atom which also participates ir this bond. The
~.Lrct_--on charge of thE bond is computed as the su-m o frac ic s of the electron
f - t n L
clz-ud :--.r--rit into the bond by the two atoms. Bykov also assumed that the energj of
thc bond is DrOportional to its electron charge. On the basis of these two as-
su,,,iptions t7nd with the use of equations (1) and (2), the authors computed the
e:;-lDir-ic.1 co,~fficients a and n in equation (1), further the new values of the
PrODortionality coefficients connecting the energies of the CF.- and CC-bonds with
their electron charges (A "and A hC)j and finally the values of the atomization
C -1 1 C
heat LC of the carbon. All these 5 values were determined by solving the system of
equations for determining the formation heats of methane, ethane, 2,2-dimethyl-
t~
propane, 2,2,3,3-tetramethylbutane, and the homologous difference. By simplification,
the authors obtained the formula AHO form = 49-81 - Z T. Xcal/mol (3) where T i
are the corrections computed for each C-atom from table 1. The value q which forms
part of T_j if3 computed by formula (4): q = 5.53 ZN i' 6E Kcal/mol (4) where Ni is
the indt~~x r~-f the C-atom neighboring the respective atom (to be determined from
table 2); AE is the difference between the electric negativity of the correspond-
ing C-atom and that of a C-atom in methane. Except for very high q-values, the
Card 2/3

6~?�65
Aonroximative I.-lethod of Calculating the A 11, of S/15)/60/003/01/005/053
.1kanes -and "heir Radicals form BC11/3005
same computation may be carried out with the nomograph (Fig 1) and equation (5).
I is computed by a simplified formula (6). The authors computed the A Ho form of
Y11 liz,,drocarbons on the basis of this scheme (Table 3). The method suggested is com-
r,arrd in table 5 with that described by V. M. Tatevskiy (Ref 3). It may also be
used for computations of 6HOform of other classes of compounds by Bykov's method.
V. V. Voyevodskiy is mentioned in the paper. There are 1 figure, 5 tables, and
6' references, 3 of which are Soviet.
AE C I. I C N :I'Moskovskiy khimiko-tekhnologicheskiy institut im. D. I. Mendeleyeva;
Kafedra tekhnologii pirogennykh protse3SOV (Moscow Institute of
Chemical Technology imeni D. I. Mendeleyev; Chair of Technology of
Z'yrogenic Processes)
S UB M I T T' --- DJanuary 22, 1959
Card 5/3

BORTSOVA, M.P.; PAVLOV, G.D. [deceased]; FILINA, R.A.; M.ARTIROSOV, R.A.;
SHPICHKO, N.P.; REVEZA, M.I.
Plant experiments in the demulsification of Ozek-Suat oil and
the preparation of demulsifiers. Trudy GrozNII no. 15:34-41 163.
(MIRA 17:5)

51ii !G--L-1, A.1,1.-and "ak""OVSKH
Povyshenie isrol I zovanil -La oborudovaniia v n. ekhanicliesIcilkh tsekhakh. (Vestn. Mash.,
1550, no.10, p.62-68)
imporvement in the use of m achine-shop equipment
DLC: TN4. v4
SO: Nanufacturing and Mechanical Engineering in the Soviet Union, Library of
Congress, 1553.

TSURICHIZED, M.Te.; GUSW, I.N.; RUMTAMSEVA., Z.P., inzhener, reteenzent;
SHPIGELI, A.M., inzhener, redaktor; MATVEYEVA, Te.N., tekhnicbeakiy
fe-MMO-F.-
[Routing system in production calculation and work and time planning;
from the practice of a machine-tool construction plant] Harshrutnais
sistema ucheta, proizvodstva i operativno-kalendarnos planiroyanie; iz
opyta zavodov stankostroeniia. Moskva, Gos.nauchno-tekhn. izd-VO
mashinostroitellnoi lit-ry, 1954. 111 p. (MIRA 8:5)
(Machine-tool industry)

SHPIGIKL9, A.M., Inzhener.
Practical aspects of the transition of a crane-building plant from
piece to serial production methods. Vent.mash-35 no.11:66-71 1
'55- (Cranes, derricks, ate.) (H1RA 9:2)

SHPIGELI, A.
"Reference book for inventors and efficiency promoters." Izobr.i rats.
no.2:43-44 F 159. (MIRA 12:3)
1. 11~challnik knostruktorskogo byuro ~bskovskogo zavoda "Pod"-
yemnik."
(Inventions) (Efficiency, Industrial)

SILPIGELI, A.
Now plant manufacturing oquipmont for automatic production
lineB. NTO no.7:13 JY '59. (14IRh 123: 11)
1. Nachallnik konstruktorskogo byuro, Pervogo Gosudarstvennogo
podshipnikovogo zavoda imeni L.M.Kaganovicha uchenyy selrretar'
pervichnoy organizatsii nauchno-tekhnicheskogo obshcbestva.
(Automat ion)

SHPIGELI. A., inzh.
No oil ignition in tempering bathes. Posh.delo 6 no.10:10 0 160o
(MIRA 13:10)
(Metal industries--Fire and fire prevention) I
(Tempering)

S/118/60/000/011/m/oI4
A161/A133
AUTHOR: Shpigell, A.M., Engineer
TITLEz Mechanization of management work and application of computers
for production planning
PERIODICALs Mekhanizatsiya i avtomatizatsiya proizvodstvaj no. 11, 19609
46-51
TEXT- The Moskovskiy instrumental' nyy zavo& "Kalibr" (Moscow "Kalib~
Instrumentation Plant) has started calendar planning of production by the
use of calculating m 'achines. The new organization is being introduced at
the plant by the Nauchno-issledovatellskaya laboratoriya ekonomiki i organi-
zatsii proizvodstva Moskovskogo inzhenerno-ekonomicheskogo instituta im.
S.Oidzhonikidze (MIEI) (Scientific Research Laboratorv for Production Rnnnn-
mica anA Onvqnization of the Moscow institute of Engineering 15conomics im.
6.Ordzhonikidze). The plant's computing station has four sets of 80-column
punchers, two card sorters, multiplying punchers and other completing ma-
chinery. Punchers can process numerical data only, and this means that all
in-documents have to be coded and all outgoing decoded. Great waste of time
Card 1/3

S/1 IY601000101 1/oi 2/o14
Mechanization of management work ... A16l A133
is caused by the absence of a standard code system in the country and long
designations - the "normal" standards of industry branch institutes have
designations reaching 12-15 signs including Arabic and Roman digits and
letters. The "Kalibr" is one of the major producers of tools and instru-
ments for the mechanical engineering industry in the country, and the amount
of planning work is fairly extensive. For instance, on 15 March 1960 there
were over 3,000 orders for a total of over 100,000 items of different types
and sizes of gages. Plans are being prepared for a year, for separate quar-
ters, and also for shorter periods and for separate production sections. At
uneven work load over the montbq the Planovo-dispetcherskiy otdel (PDO)
(Planning-DisDatoher Denartment) introduces changes. Calculations include
aiso labor requirements and wages. After experiments, the Research Labora-
tory has started to set up a plan of distribution of parts and operations
to work places and coordination of time tables throughout the entire produc-
tion cycle. The work requires many times sorting and tabulation. Such a
plan has been tried in a series-production section at the instrument shop
No.l. It took 8-9 work shifts to set up a plan for 250-300 items (parts'),
corresponding to 1500-2000 operations which is too long. Measures are con-
Card 2/3

S/118/60/000/011/012/014
Mechanization of management work A161/A133
sidered to cut the time and improve the planning techniques. The conclu-
sion is made that an electronic digital computer is necessary. It is men-
tioned that calculations of the production program for the 1st quarter of
1960 for six mechanical assembly shops of the "Kalibr',' revealed incomplete
utilization of equipment and a possible 10-25% output increase from same
production areas with release of a part of equipment at the same time. The
remaining equipment would then be loaded not to 40-75% but to 50-95%. The
article includes samples of calculation tables. There are 7 tables.
Card 3/3

VENGLINSKIY, V.V.; DENISaIKO, K.V.; SOTSKOV) A.A.; SHPI(ELI, A,,,M,,-
GORDON, Kh.I., inzh., retsenzent; SHAUNAZAROV, M. 7R
retsenzent; DAY011, A.Ye., inzh., red.; PETUKEOVA, G.N., red.
izd-va; TIKWTOV, A.Ya.., tekhn. red.
(Establishing technical norms in the instrument industry]
Tekhnicheskoe normirovanie truda v priborostroenii; spra-
vochroe posobie. Moskva, Mashgiz, 1962. 51-1 p.
(MIRA 15:9)
(Instrument industry-Production standards)

SHPIGELI. A.N.
Glinical aspects of calculi of a diverticulum of the male urethra.
Urologiia 21 no.4:59-60 O-D 156. (MTRA 10:2)
1. Iz khirurgicheskogo otdalentya Opochetzkoy rayonnoy bolluitay
(glavnyy vrach - zasluzhennyy vrach RSFSR S. Ya. Gen).
(URETHRA-SURGERY) (CAWULI, URINARY)

S11PIGEL' A.N.
Indications for and complications and tecbnique in kidney
biopsy. Sov. med. 28 no.10:96-101 0 165. (KIRA 18:11)
1. Propedevticheskaya terapevticheskaya klinika I Leningradskogo
meditsinskogo instituta imeni Pavlova, laboratoriya klinicheskoy
i eksperimentallnoy gematologii Instituta fiziologii. imeni Pavlova
AN SSSR (zav. klinikoy i laboratoriyey- prof. A.Ya. Yaroshevskiy)
i nefrologicheskoye otdeleniye (zav.- kand. med. nauk Ye.A. Arlyeva)
Bollnitsy imeni Uritskogo (glavnyy vrach I.G. Savellyev), Leningrad.

AUTHOR: Shpigell, A.Yu., Engineer 118-58-6-12/21
TITLE: A High-Speed Grab Carriage (Bystrokhodnaye zreyfernaya telezhka)
PERIODICAL: !.-Tekhgnizgtsiya trudoyftkikh i tvazhtilykh rabot, 1958, Nr 6,
pp 2c?-~C (USSR)
ABSTRACT: In 1957, the Yoskovskiy zavod "Pod"ygmnik" (Yoscow "Pod"yftnik"
Plant) turned out two types of high-speed grab carriages (hoist-
ing capacity - 10 tons) of 2,500 mm and ",300 mm gauges. The
main parts of the carriage are: 1) the welded frame with the
conveying mechanism; 2) the grab winch; -)) the electric control
apparatus; 4) the operator's cabin; 5) the grab (volume - 5 cu m);
6) the brush. The weight of the carriage is 22.3 tons (2,500 MM
gauge) and 23.9 (3,300. mm gauge). The electric motor of the
grab winch is of the type MT-62-10 (36 kw), end for the convey-
ing mechanism of the type MT-51-8 (17.5 kw) and MIT-52-8. The
lifting speed is 40 m/min, the moving speed - 166-m/min, and
the lifting height - 20 m. The use of these high-speed grab
carriages saves the labor of 300 workers. There is 1 diagram.
1. Overhead cranes--Characteristics
Card 1/1

SHPIGELI., A.Yu.
"Mechanization and automation in the machinery industry." Hashinostroitell
no. 4:45 Ap 161. (m uA 11+: 4)
(Automation) (Machinery industry-Technological innovations)

SHPIGEL t - I,. Yu.
.7
Special clutch coupling for cranes. Ifashinostroitell no.12.20
Le
D 16-1 (!URA 24:12)
(Clutches(Machinery))

109-2--l-14/17
AUTHOR:. Shpigel',.,~,4v-j; Rayzer, -M. D., P..r,-d Myae, E. A.
TITLE: An instrument for Relative Measu-,.-emer.'s of Alternating Magnetic Fields
(Pribor dlya otnositel'nykh izmereni-y perernennykh magnitnykb poley)
PERIODICAL: Radiotekhnika i Elektronika, 1957, Vol 2, Nr 1, pp 111-119 (USSR)
ABSTRACT: A description of an instrument for relative measurements of time-
alternating slightly non-uniform magnetic fields, based on the phenomenon of
nuclear magnetic-resonance absorption, is -presented. The instrument
measures full field distribut4on, including the residual magnetic field. The
maximum measurable difference of fields ;-n two pointsLHmax = 316HO. Error
-~ 31o Hmax. Measurements are made at H,,, ct 160 oersteds.
T~article accelerators and other engineering devices often require relative
measurements of time -alternating magnetic fields. The methods used so far
(ballistic, electron integrator, etc. Iave one common shortcoming, viz. , only
the alter rating .-field difference is measured and the residual field or a super-
~mposed magnetization field is not incl-uded. The new instrument described in
the article is free from this shortcoming. The instrument has been developed
for measu.-ing the injection field distribution of a 10-bev proton -synchrotron
Card 114

109-Z-1-14117
An Tnstrument for Relative Measurements oi Alternating Magnetic Fields
magnet, AS USSR. As a block diagram, figure 2,shows the instrument con-
sist5of a high-frequency oscillator, two identical amplification and signal-
I -
forming channels, an integrating circuit, a power supply, and auxiliary units
As the field reaches a certain value, depending or- the pre-set oscillator fre-
q7u,ency, a signal of nuclear magnetic-reson-ance absorption appears. The f-ig-
nal is selected by a pulse-height detector, amplified and shaped. The passband
of the pre-amplifter is 1. 5 - 6 kc. Signal-to-noise ratio at the pre-amplifier
output is about 40. For accurate indication of the time moment when the field
reaches a predetermined value, the signal is differentiated and amplified by a
wideband amplifier. The upper limit of the passband is 100 kc. An additional
time -selection circuit helps to suppress the effects of interference frorn other
electronic equipment in the room. The voltage front induced in a velocity pick-
up during the field change in the magnetic gap starts a phantastron delay circuit
which, in 20-60 m/sec, triggers a univibrator which generates the gate pulse.
The pulses from both trigger circuits (each about I (vsec) are mixed and fed to
a fl'-p-flop circuit. A negative square pulse appears at the output of the latter
circuit, its duration being equal to the time between the two field pulses. The
Card 2/4

109-2-1.-14/17
An instrument for Relative Measurements of Alternating Magnetic Fields
I
square pulse opens a tube integrator whose output is indicated by an indicating
instrument. One field pickup and the velocity pickup are stationary; the second
field pickup can be moved in the magnet gap. The field value sensed by the
second pickup may be higher or lower than that at the point of the first pickup.
The field non-uniformity sign is indicated by a special circuit. Some parts da+a
a-ad parameters of the high-frequency oscillator, field and velocity pickups,
sign circuit, and integration circuit, are presented. Calibration of the instru-
ment is explained. The overall error of the instrument is evaluated analytically
and found to be equal to + 376 Hmax. The error of absolute field measurements
is about 0. 176. The instrument was tested with the AS USSR proton- synchrotron,
and the results of the measurements were found to precisely agree with those
given by the ballistic -galvanometer method when an allowance for the residual
field was made for the latter. Advice is offered for quick measurement of
monotonic space-changing magnetic fields by means of a number of field pickups
and an electron oscillograph. The authors are grateful to Professor V. A.
Petukhov for his remarks in discussing the work and to A. N. Zinevich for his
Card 3/4

109-2-1-14/17
Ap. instrument for Relative Measurements of Alternating Magnetic Fields
part in building the instrument.
There are 7 figures and 4 references, one of which is Soviet, in the article.
ASSOCIATION: Fizicheskiy institut imeni P. N. Lebedeva AN SSR (the Institute
of Physics imeni P. N. Lebedev, AS USSR)
SUBMITTED: June 1, 1956
AVAILABLE: Library of Congress
1. Magnetic fields--Measurement 2. Laboratcry equipment--Performance
Card 4/4

iUTHORt SHPIGEL.I.S., RAYZER,1A.D., ~.IYAE,E.A. PA - 2132
TITLE: On the Dependence of the Amplitude of the First Harmonic Vibration
of a Signal of the Magnetic Resonance Absorption Capacity of the
Nucleus of Magnitude of Detuning. (Zavisimost' amplitudy pervoy
garmoniki signals, yadernogo magnitnogo resonanznogo pogloshche-
niya ot velichiny rasstroyki. Russian).
PERIODICAL: Zhurnal Tekhn. Fiz., 1957, Vol 27, Nr 2f Pp 351 - 354 (U.S.S.R.)
Received: 3 / 1957 Reviewed: 4 / 1957
ABSTRACT: In the present work the relation between the order of the ampli-
tude of the first Harmonic Vibration and the detuning (the difference
of frequency of the generator and Lamorta precession) was de-
termined. The investigation was carried out for the system: substance
to be investigated - high frequency generator - i.e. on the con-
dition, that the absorption signal be not saturated, that the
amplitudes of the modulating field and the breadth of the ab-
sorption line be commensurable. The obtained approximated formula
makes it possible to draw the following conclusionst The steepness
of the dependence of the amplitude (of the first harmonic vibration
of the envelope of the oscillation voltage of the generator) on
the amount of detuning is inversely proportional to the voltage
amplitude a0, is dependent upon the parameters of the generator
and the appearence of the characteristics of the generator lamp,
as well as inversely proportional to the square of the signal line
Card 1/2 width. Dependence on the volume of the substance and on the

AUTHOR: SHPIGEL,I.S2_,_RAYZER,tI.D., IAYAE,E.A~ PA - 2139
TITLE: The Sensitivity of the Generator with Self-Excitation.
(Chustvitellnost' generatora v rezhime samovozbuzhdeniya,
RUBsian).
PERIODICAL: Zhurnal Tekhn. Fiz. 1957, Vol 27, Nr 2, pp 387-390 (U.S.S.R.)
Received: 3 / 1957 Reviewed: 4 / 1957
ABSTRACT: The sensitivity of a generator with self-excitation and back-
coupling, caused by its parameters and the conditions for the
reception of the signal were investigated. The equation for
such a generator ia written down, the first approximation of
the solution is derived, and the equation for the occurring
oscillations as well as for its amplitude a
are written down.
0
The transition process of the generator from one oscillation
process to a new one is investigated. The latter is caused by the
modification of the quantity 16
1 at the expense of a sudden
0
introduction of an ad&tional decrease 4 6 at the moment t-0.
Finally, the expression for the square of he oscillation ampli-
tude of the generator during the transition process is obtained.
Herefrom the absolute quantity of the modification of the volt-
age of the generator in dependence on its parameters and on
time is obtained. The equations obtained in this manner make it
=const.
possible to draw the following conclusions: 1.) At A 6
0
the absolute and relative modification of oscillation voltage
Card 1/2

AUTHORS: Rayzer, M.D., Shpigell, I. S. 53-64-4-3/11
TITLE: Plasma Investigation by Means of Micro Radiowaves
0
(Issledovaniye plazmy pri pomoshchi mikroradiovoln)
PERIODICAL: Uspekhi Fizicheskikh Nauk, 1958, Vol. 64, Nr 4, PP-
641 - 667 (USSR)
ABSTRACT: In introduction the authors give a short survey on the
development of the investigation of gas discharges be-
ginning with the investigations in 1930/32 when Darrow,
Appleton, Chapman and Chields published their first works
on the measurement of plasma conductivity in the high-
-frequency field (refs. 1-4), up to the recently found
application of plasma in high-f requency conditions like
attenuators and antenna commutators (Bradley, AraM3,
ref. 7,8). This work is divided into 6 chapters; in
each chapter a survey on the pmaent state of the respective
investigations is given. Chapter 1: The conductivity and
the dielectric constant of an ionized gas. Starting from
the investigations by Allpert, Ginzburg, Faynberg and
Card 1/3 Morgenau (General Theory of the Interaction of Electrons

Plasma Investigation by Means of Micro Radiowaves 53-64-4-3/11
in Plasma in the Presence of a High-Frequency Field)
the electron distribution function is discussed,
the interrelations betweenc 2 or a3/2resp.arxia-1/6,-, of x,
2, X
(xf-t~ly , Morgenau, ref. 10) as well as the dependence of
W nd A on the electron density. Chapter 2:
crit a crit
The resonator method, The method is explicitly dealt with
in theory and practice. Various plants for the determination
of the plasma parameters are given in block -diagram
representation. In chapter 3 the wave guide method is
discussed in theory and practice; a block-diagram of an apparatus
which by means of a microwave bridge makes possible the
measurement of plasma parameters is discussed in detail. In
chapter 4 the cross modulation method is dealt with explicitly
in theory and practice, and also in this case a block-diagram
of such a plant is described. Chapter 5 deals with the
determination of the coefficients of ambipolar diffusion,
recombination and electron collision frequencies. Finally
chapter 6 gives the experimental result partly compared with
the results obtained in theory. A series of diagrams show
Card 2/3 the connections of the single coefficients of pressure,

Plasma Investigation by Means of Micro Radiowaves 53-6,~-4-3/11
density, energy and field quantities. The most important
experimental data concerning recombination are given in
table 2. There are 26 figures, 2 tables, and 55 references,
of which 3 are Sdviit and 52 English.
Card 3/3

SOV/120-59-1-46/50
AUTHOR: ShDigel', I. S.
C)
TITLE: A Fast Electrodynamic Vacuum Valve (Bystrodeystvuyushchiy
elektrodinamicheskiy valcuumny-j klapan)
PERIODICAL: Pribory i tekhnika eksperimenta, 1959, Nr 1, --, 151 (USSR)
ABSTRACT: In many cases it is necessary to introduce into a vacuum,
chamber a certain amount of gas (ion sources, plasma studies,
etc). The distribution of pressure across the front of the
Eas wave should in such cases be very steep. The latter con-
dition may be satisfied if the seal which separates the press-
ure and vacuum re '-ions is opened suddenly and the aperture
thus introduced is sufficiently large. A valve which will do
this is shown in Fig 1. The vacuum chamber A is separated
from the high pressure chamber B by a light metallic disc 1,
0 I'D
The seal is achieved by good contact between the disc and the
0
rubber ring 2 At the pressure of about 1 atm in B the
cm)
force actin- on the disc is about 12 k- when the valve has the
dimensions indicated in the fi-ure. A plane coil 3 is
C-3
Dlaced under the three ed:-,es of the aisc. The coil has five
rD
turns of copper sturip 3.217- x 0.75 mm9. At a lrl,iven moment two
6jtF capacitors charged to a volta~-e of 4.5 L-4- are dischar-ed
throu-h the coil. The currents induced in the metallic disc
0
Card 1/2 interact with the current in the coil and the disc quickly

SOV/120-59-1-46/50
A Fast Electrody-na-mic. Vacuum Valve
flies away from the rubber ring. The disc is stopped by the
rubber rinr'- 5 The disc moves through a -evi millimetres
0 3-
and ti--,e amourit of -as let tiirou!-rh is 1-2 elft at atiaos-oheric
pressure, Preliminary neasurements have shown that a circu-
lar slit 2 nin-, ~Iic-Ii is fo:rmed in 200 Itsec, the maxiniuni velocity
of the disc bein- 3 x 104 cm/sec. Tb-ere is 1 fi-ure.
CI LD
ASSOCIATIO14: Fizicliieskiy institut AN S3SR (Physics Institut-e of the
Academy of Sciences of the USSR)
SUBIAITTED: January 6, 1958.
Card 2/2

1OM124(3)
AUTEOTI-. Shpigell, I. S. SOV156-36--e-10163
fyl!TLE-. Plasma Acceleratior-.(Uskoreniye plazmy)
PE'I~IGDICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki~ 1959,
Vol 36, Nr 2: PP 411-415 (USSR)
LBSTRACT: Pollo-aingr 2. number of investigations carried out by other
authors (I'Lefs 1-5) dealing -~j 4 th the single acceleration of
plasma by electromal.-netic forces, the present paper describes
experiments --arriod out for the purpose of acceleratinE plasr-a
in the vacuum by ri*an~; of cnn axially symmetric nc~n-uniform
pulsed maonetic field. The oxp%arimental arrangement is
represented schemo-tically bv fiGure 1. it ~-onsists essentially
of a vacuum chambcr, pulse device, pre-ionization device,
acceleration coil, and control circuit. The vacuum chamber
consisted of two coaxial cylinders; the one (interchangeable)
was made of orCanic glass or pyrex (payreks) with a diameter of
150 mm and a length of 500 mm, the other of copper, with the
same diameter and a length of 700 mm. Pressure a-mounted tD-
(2 - 4)-10- Ng . One end of the copper cylinder -,.,as closed by
means of a brass flange, the other was connected with a glass
Card 1/3 cylinder the other end of which was closed by means of a flange

rlasma Acceleration
SOV/56-36-2-10/63
of organic glass. rigure 2 shows the latter. It has an
electrodynamic valve developed by the author (Ref 6). The
oscillatory circuit (condenser TM 2, 7-50) had a frequency of
-w 120 kilocycles at voltages of from 10 to 24 kv. The generator
(500 W) operated at 15 megacycles. The following was measured:
a) The rate of acceleration of the plasma in the direction of
the z-axis (= direction of acceleration) and in the direction
of the radius. These measurements were carried out photo-
graphically by means of photorecorder SFR-2m . The corresponding
photographic reproductions are shown. Figure 3 shows the motion
of a plasma in air in the case of an exposure of V = 280 micro-
seconds; figure 4 shows the motion of a plasma in helium at
T = 220, 280 and 400 microseconds. Figure 5 finally shows a
radial picture,1c = 280
,#sec of a plasma motion in air.
Ion energies for nitrogen and oxygen were between 80 and 190 ev,
for hydrogen 40-120 ev and for helium 120 - 280 ev
b) The rate of frontal motion -and the duration of pulses in a
plasma of given density was measured by means of an r-f pulse
generator (datchik)(densities of loll-1013cm-3) and a wave
0 cm-11 Fig
guide, which records plasma densities of 1 12 7% -ures 6-9
Card 2/3 show the oscillograM3 recorded at various voltaEes and T-values

Plasma Acceleration
ASSOCIATIOH:
SUBMITTED:
sov/56-36-2-lo/63
(air and helium). The measured dependence of the duration of
impulse of a plasma having a density of 1012 cm of z is shown
by figure 11, and figure 10 shows the corresponding oscillogram
at n ~~10 12. The maximum in figure 11 is z = 35 cm and
T = 150JAsec. The author finally thanks V. I. Veksler,
M. S. Rabinovich, and L. M. Kovrizhnykh for discussions,
E. D. Andryukhina for assisting in carryino out measurements,
and Ye. A. Smirnov for assembling the device. There are
11 figures and 6 references, 3 of which are Soviet.
Fizicheskiy insti4-ut im. P. N. Lebedeva Akademii nauk SSSR
(Physics Institute imeni P~ N. Lebedev of the Academy of
Sciences, USSR)
August 23, 195S
Card 3/3

81681
5/057/60/030/05/10/014
B012/BO56
/0. -900orA)
AvrHORS,
TITLE, Some Charaoteristic Fa&tur4. of Goa Discharges
PERIODICAL, Zhu~val t.khnLch "I" jv ft.ikl, 1960. vol. 30, on- 5,
Pp. 538
IM. The r.. road, I the kth International Confdrence on
I.at. .,ItoIUP,,1, 1, 1953. 1h.,:"tl,r" ,rri.4
porLaonts for the purpose of explaining the i.rinON ... r. d by
hLos of the plamst , which are described. The
., I4'::r!b:adY"-
cried out in axially #Y=etric hamageneous and C n-
!
r.".:'b -drtlar
at' toIIhe - frawIC1,11
du tIr
the p2.. . The fo ing of the ph~%o-ocw mentioned -are . of
the O:P%ur0* of th.~~ti. lLt!ld) y the ,,inventle.t.4
..,I ;h MhOCk waveal t1g.
I :h,,;lth%O:~QI We- -'.the ~om;leto current
nd g. OtIO- pt.%ur. of to
I. . 41..ba,rda, in hydrog.., !l
So chsrmot.ri-ti. Fastu.. Q"f I.du.ti,. Goa 81681
3Z. berg... 5/05 60/030/05/10/014
30 1 ZY-05 6
dI,:h -w-.dt'h:t.d.rI"&Cubr1..,
fir I he, _r,
.&If id orIrib to f I.r
r11,1 to 'b%-1--,:hsah.r radius take. place. 1. "'. 3a, "he d
for .Id.Ibe A Chords 1. No VIC*
A '..%I ti
..11.d --gostio Airrar- 1. shown . Ch.., -y-stri. field, the
'be ourr:ot Y_ ?16. )b shows the
dor'b. ot1l. r t*d. by special win 41 C, radius R and
dl":'::C: I,
let --- I
11 d-In, h: 9 62 1 F- 4 1 Nay be :-upoth. the ..M.,.t
the . CtA ". first he 11-p.rl.d of the field h.mg. f.-aji-44ly-
To rIfthe PlAwma- Th. curra, Clarity r ... real
'Can *1 the ONa"t PI
a ...PtuaIn "t"t. d':tr'b
ad g C,
,1 6. 1 i..tI
f
f part 0; -':t" .....I-no-11 -b1 -Mr. uxrutt"V .
InoI'v,stid%.
tio- of tthe =gnN I- fl by h.*p1.tms. T
the her. the -no.
Iof _goato . Ib that 1.
.:,.an
:h-b-r.,. Cylindrical shock wave is fou.dtnd
IIn the breakdown In the -S.
5;~I- 't I%* h~'U partly joniga.
It. h pro of the',
,he our th.on uIIyIor ...... .nd
9441rat.d within this rands ssy,
Went, I* too owes Of a akin
- Note the ..tire asterior sa,not
So har ct.ri.tio Fast---. of IAducti,. Go. 5/057/60/030/o5/10/014
0I::hCrd.: 012/1056
f the &shot- At h h discharge fr:quenalea
:d tii of (300~ 700 Order that
uffItIf 'I," ..!a ty k./*) N,
CI:h
ki. layer he" -9 thin---. th.Iti. in
.be.b.r. -I
he P.
2 to 5 shoo 1:ttaimod afther gth of the
Conduati,ity
Now Ihl. .8h th: .c "u"'".
thicka-4- -k th-*:ki. lay-r Ir.: Of 60-100/h
I umf !~ --rI-h I,1t of the ..u_
:hambor ad '."It" It:,-infestigat'lhon anh other papers (11
In the 4" ran;
Ad. . ..to
be ..A,4 nof
. . .... BI" of the out or field. Zno
'd ":.rIusIt-tt,. relation to
th-t 1. the t,:,. " -Ib-d -P- 14-A q 1an..
1/2
IN observed. to sort aocurst* d&%* could be
thl-ku... Of the ki. layer, the frwq~ ... y of th 1:, d. 1~,, the
!,."k1lal i:.th- k.-t a,- ". Id.
No%..rnad for
3 f d~ and 5 r.f-xw.C- 5 Salt End .h
ASSOCIATIONs risich No
lu. t Itn W. Labodeva A$ $331t MC.k,.
aP. X. L.b.d. of the AS LM51t,
saber 4, 1959
LF

KOV.,'LIZ1fl1YKfl, L.M.(txanslatorl; RAYZE11, M.D. [translator];-SHP IGEL I ,
I.S.[translatorl; RABINOVIGH, M.S., red.; BUIITSEV,-A-.r.-,-
- ff-
re ; FOTAPENKOVA, Ye.S., tekhn. red,
(Plasma physics and magnetohydrodynamics] Fizika plazmy i mag-
nitnaia gidrodinamika; sbornik statei. I-,oskva, Izd-vo inostr.
lit-ry, 1961. 302 p. Translated articles. (MIRA 15:3)
Plasma (Ionized gases)) (MagnetolWdrodynamics)

20711
S/l2o/61/oOO/OOl/O53/o62
E032/E114*
M5
AUTHORS: Andryukhina, E.D., Safronov, A.Ya., and Shpigell, I.S.
TITLE: Characteristics of a Fast Vacuum Valve
PERIODICAL: Pribory I teldinika eksperimenta, 1961,No.l,pp-174-177
TEXT The last of the present authors has described an
electrodynamic vacuum valve in Ref.l. This valve is illustrated
schematically in Fig.l. In this figure the disc 2 is brought
into motion by the forces F4 due to the interaction betweell a
current pulse in the coil 3 and the current induced in the disc.
As soon as the disc rises, gas passes from the region 5 into the
high vacuum region I and the disc returns under the action of the
force Fp which is due to the pressure of the gas. In this way
an adjustable gas "pulse" can be produced. The present paper
rvports a simple theory of the valve and some of its experimentally
determined characteristics. The pressure distribution on the high
vacuum side was measured with the aid of-a miniature ionization
gauge, having a working volume of 0.2 cm->. It was found that a
directed motion of the gas can be obtained with sufficiently long
channels, the gas velocity being higher than the velocity of sound.
Card 1/2

20711
S/12o/61/000/001/053/o62
Characteristics of a Fast Vacuum Valve. E032/E114
Space and time gas pressure distributions are given.
There are 9 figures and 5 references: 4 Soviet and 1 non-Soviet.
SUBMITTED: December 14, 1959
Fig. I
Card 2/2

20666
S/057/61/031/001/011/017
B104/B204
AUTHORS: Mo ro z ,Ye. M. and ~,hpLj~ei I. S.
TITLE: Calculation of the electrodynamic pushing out of a non-deform-
ed plasma ring from a magnetic mirror trap
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 31, no. 1, 1061, 78-83
TEXT: One of the methods of accelerating plasmatic formations is the
acceleration of plasma rings in magnetic mirror traps. A. I. Morozov
(Ref. 3) was the first to investigate this process theoretically; in
experimental investigations, a maximum energy transfer to the accelerated
ring presents difficulties. Detailed investigations showed that the
energy transferred to the ring depends on the ratio between the build-up
time of the magnetic field in the mirror trap and the interaction time
of the plasma ring with this field, as well as on the ratio between active
inductivity and the parasitic inductivity etc. For improving this
knowledge, the authors carried out calculations of the motion of a
perfectly conducting ring in the magnetic field of a mirror trap, which
..is variable in time. Deformations of the ring radii and proximity effects
Card 1/5

20666
Calculation of the electrodynamic S/057/61/031/001/011/017
B104/B204
were neglected. The two former assumptions increase the results, the
latter assumption diminishes them. Nonetheless, the results obtained
make it possible to estimate the dependence of the energy of the progres-
sive motion of the ring on the parameters of the experi:mental apparatus.
The authors studied a system of two rings, A and B; A produces the
magnetic mirror trap, and B is accelerated. If A is a metal ring, through
which an electric current flows, an opposed current is generated in the
plasma ring B. The electrodynamic repulsion thus produced moves B in the
direction of the x-axis (Fig. 1). On the basis of an idealized circuit
diagram, the coupling between the two rings is discussed, and the equation
of motion for the plasma ring 2nR
mx H (1)
c 2 r
is set up. Here, 1 2 is the current in the plasma ring; H r is the radial
component of the magnetic field generated by current I in metal ring A at
the pl ce of B; m is the mass of B. (1) is transformed into
11 dif2
X__ 2mc2L2 dx (5); 11 is the current in A; L 2 is the inductivity of
Card 2/5

20666
Calculation of the electrodynamic ... S/05-71611103!100110111017
B1041B204
B; M is the interaction factor between the two rings. . The time dependence
of I is obtained by.integration of the differential equatiorl for electric
1 2 2 2
resonant circuits, and thus. U.t c d
X=
L)
2m dx
is obtained. U is the input voltage; L is the total inductivity of the
system; and t is the time. For the purpose of integrating this differen-
tial eauation,
~,he authors proceed to the following reduced parameter:
__ I[, = d,~/d J i~L~j
L L11
0 =fc/2RT
Solution is then carried out with L1 ~ L 2' Fig. 4 shows (dr/dr) maxy
5
max' and -r ax as functions of A with 0.02 for different conditions.
m
It is noted that these results have been obtained on the assumption of
U = const. This makes particular demands on the capacitor battery. For
the capacity of this battery, the authors obtain the relation
Card 3/5

20666
Calculation of the electrodynamic S/057/6i/031/001/011/017
B104/B204
C >> m 2 (19). Finally, a numerical example is calculated.
U2 dt max
There are 4 figures and 6 references: 5 Soviet-bloc and 1 non-Soviet-bloc.
ASSOCIATION: Fizicheskiy institut im. P. N. Lebedeva AN SSSR Moskva'-
(Institute of Physics imeni P. N. Lebedev AS USSR, Moscow)
SUBMITTED: May 24, 19060
Legend to Fig. 1: Arrangement of the
conducting rings.
X
Card 4/5

20666
Calculation of the electrodynamic
Legend to Fig. 2:
Idealized scheme of tbp Pyrprimental
System. F1, 2.
LO
Legend to Fig. 4:
DeDendence of WdT )maxy
.and T on ~'f or
>Max mak
0.02. Curves 1: 2~
Curves 2: r
5 Curves 3'
or
0 Curves 4: ro
20f
/2R.
X0
S/057/61/031/001/011/017
B104/B204
Card 5/5
-03
N~ .
fr . . I I
3 S

ACCESSION NR: AT4025317 S/0000/63/000/000/0263/0269
AUTHORS: Batanov, G. M.,- Ivanovskiy, M. A.; Fedyanin, 0. 1.;
TITLE: Use of a lumineacent probe to record a moving plasma
SOURCE: Diagnostika plazmy* (Plasma diagnostics); sb. statey.
Moscow, Gosatomizdat, 1963, 2.63-269
TOPIC TAGS: plasma, plasma diagnostics, luminescent probe, plasma.-
scope, moving plasma configuration, plasma electronimage, plasma
ion image, plasma configuration
ABSTRACT: The luminescent probe ("plasmoscope") method developed
by L. I. Yelizarov and A. V. Zharinov and reported by them at the
Nuclear Fusion Conference in Salzburg (4--9 September 1961) is used
to study the transverse motion of a plasma jet in a magnetic field
in the presence of translational velocity perpendicular to the sur-
Card

'ACCESSION NR: AT4025317
face of the screen. The results are compared with data obtained by
local density measurements~. The characteristics of the apparatus and,
of the plasma are described. it is concluded that at a plasma den-
sity _1011 cm-3 _107
and a translational beam velocity cm/sec the
luminescent probe yields correct information on the plasma configura-~
tion in a longitudinal magnetic field. Reflection of the plasma
from the screen surface does not distort the results, and there is
no luminor persistence. The density of the measured plasma is not
confined to the condition that the grid cell dimension be smaller
than the Debye radius. To obtain a sharp image it is merely neces-
sary that the pulse on the grid be of sufficient magnitude. If the
screen is not-illuminated by the plasma radiation, it is possible to
obtain an ion image without using electron*secondary emission. -Orig.,
art. has: 6 figures.
ASSOCIATION: None
Card 2/4'i,.-,

GKIDNA, V.P., m1ad. nauclui. sutr., st&rshiy bibiiograf; RAYZER,
M.D.Y kand. fiz.-mat. nauk; KOLESNIKOV, V.N., kand. fiz.-
matem. nauk; AJITROPOV, Ye.T., ml. nauchn. sotr.; SHPIGELI,
I.S.J. kand. tekhn. nauk, otv. red.; KOVRIZMIYKH, L.M.,
kand. fiz.-matem. nauk, otv. red.
(Plasma plUsics; bibliographic index, 1955-1961] Fizika
plazTmj; bibliograficheskii ukazatell, 1955-1961. Moskva.
Na-uka, 1964- 354P. (MIRA 17:11) 1
1. Moscow. Fizicheskiy institut. Biblioteka.

VORONIOVY G.S.; POPRYPiDUKHD%, A.P.; SHPIGELI, I.S.
Gas delay line. Prib. i tekh. eksp. 9 no.3:200-203 My-Je 164
(MIRA 18:1)

ACCESSION UR: AP4037614 S/0056/64/046/005/1915/1917
04'.) 1
lf
AUIEOR: Batanov , G. M. Ivanovskiy, M. A. ; WR6 9 1* so
4 T=: Particle losses and configuration of plasm jet mwing thrvugh a
!curvilinear magnetic field
SOURCE: Zh. eksper. i teor. fiz.9 v. 46, no. 59 19649 1915-1917
i
TOPIC TAGS: plasma, plasma in curved field, plasma in hanop
I eneous fields plasma
,particle loss, plasma jet nucleus, plasma jet tcngue, plasma ion distribution
ABSTRAM Unlike in earlier investigationss the parameters of a plasma jet passing
through a curvilinear magnetic field were studied further by letting the jet ccn-
tinue to move in a hanogeneous magnetic field, The plasma jet mDved from the gtm
first in a hanogeneous field (3 k0e) for 50 an, then thragh a curved field of
6 an.radius, and then again through a 120 cin hanogeneous field (1 k0e). The plasm
density was approximately 1012crd-3and the electici tenperature 5 - 10 eV. 7he
~,Measurvnent procedures are described briefly. The tests have shown that some 1-2:
microseccnds its passage through the curwd field the plasm jet ~~q
I It in
'tongue f1i ge plasma drifts towards the dkvbw wallsq alcing win the
a
rd 1/3 7-7

ACO~SSION NR: AP4037614
:main nucleus" of the plasma jet, which ccntinues to nxwe alcng the magnetic
!field and has a high density (dielectric constant close to 1000). This is in
~qualitative agreement with the dependence of the icn distributicn cn the n~agmtic
;,field (cf. figure) and is confirred by masurenent of the electric field ro-ar
~the plasma jet llnucleus~ Ori e art* has: 2 figures*
9
iASSOCIATION: Fizicheskiy institut im. P. N. Lebedeva M SSSR (Physics Instituteg
'AN SSSR)
iSUMI=., 03,Jan64 ENCLI. 01
ISUB CODEI ME HR FZF SOV: 002 01M: 004
'Card

tLPYJ._V.AJXVALPAVAA$ CUM LV%.V_6 J.VA vxjv'~
ties are established. Effective stabilization is shown to be possible when the
dimension of the inhomogeneity of the electr C field is smaller than the char-
inhoMOL ii y the transverse plasma.
1 acteristic dimension of the plasma gene
dimension)., if the field itself in larger than: or comparable with the thermalL
field. The stabilization does not dependLon the of the electric field and
-flute witinin a
is due to the fact that the field is capable ot-deforming the
time
time that is much shorter than the necessaryfor the flute instability to
develop. It is stated in the conclusion that~some experimentally observed
-devices may be connected with.t e
i1
stabilizations of flute instab ity in various h
stabilization mechanism described-in'the present article# "The.auth6ks thank-
S. Rabinovich.1. P. Silin, and 1. S. Danilkin,for valuable advice and dis-
cussion." Orig. art. has, -17 formlas.
ASSOCIATION: Fizicheskiy institut imi PO'.1-Nt Lebedeva AkademA nauk GSSR
(Physics Institute, Academr of Sqiences.,~~
-Card 2/3

~5~_9_2'_ EPA - -2/rr,(l)/EEC(t)/EPA(Bp)-2/T/L,-,IA(=)-2 PI_h/Fo_4/pz_6/Pab_10
rjp~'~ AT
ACGFZSIOII NR: AP5007656 S/0020/65/160/006/1293/1295~0
AUTHORS: Datanov, (). M.; ~erazhetskiyj H. S.; Grjgbenshchikov, S. To.; Zverey,
N. M.; Popr.7ndiftin, A. P.; Rabinovich, H. S.; SbitgLkova,_I.S.;
4. it
TITLEt M"GnOtic surfaces and the helical field of a
stellorator with external injection
SOURM AN SSSR. Doklady, ve 160, no-. 6, 19650 1293-1295
TOPIG TAGS: stellarator, plasma trapping, plasma injection, magnetic field,
helical magnetic field, resonance excitation, controlled fusion
ABSTIUM Magnetic surfaces and external injection techniques in a 10 000-oorated
longitudinal field stellerator (1200 mm large diameter and 100 mm small diameter)
are discussed briefly. The parameter 8, equal to the ratio fundamental harmonic
of field over longitudinal field, varies within the limits of 0.71-0.33, and the
helical winding is at 450. To verify the existence of magnetic surfaces, a
pulsod electron gun is used as wall as a 3 x 3 m2 probe. The results show an
unporturbed magnotio surface at E - 0.40, a resonance excitation of the second
kind Qt.F- " 0.37 with an external undisturbed surface,and an internal undisturbed
Card 1/2

L 35592-65
AGGWSION ?JR, AP5007656
surface with a resonance of the third kind at 0.39. The external injection
wa3 accomplished by means or rour plasma spark injector's operating simultaneously
for 0.4 /.k see. Oscillograph atudies indicato that the time for attaining a
steady state distribution in density across the chamber corresponds to R/YTI wherel
R is the largo chamber radius and vT is the ionie thermal velocity. Comparing
den3ity distributions in the helical field to those or a toroidal field, the
distinct influence of the former on the density distribution becomes obvious.
Orig. art. hast 2 figures.
ASSOCIATIONt none
aimmwt o9jul64 ML: 00 SUB CODES OP
NO M7 Sov , oo4 OTHERS 002
'tCard

Ut(c) AT
C NRj AP6015310 (91 S
) OU1?CE CODE: UR/0057/66/036/005/0881/0891
AUTHOR: Kossyy, I-A-; Shpigell, I.S.; Dorofeyev, Ye-V-
ORG: Physics Institute im. P.N.Lebedev, Moscow (Fizicheskiy institut)
TITLE: Investigation of a conical induction plasma source
SOURCE: Zhurnal tekhnicheskoy fiziki, v. 36, no. 5, 1966, 881-891
TOPIC TAGS: plasma gun, plasma source, plasma jet
ABSTRACT: A two-stage electrodeless conical plasma gun was investigated in an effort
to achieve a more efficient induction plasma source and to learn something about the
operating mechanism of conical plasma guns. A diagram of the apparatus is shown in th
figure. The capacity of C and C 3 was 0.6 and 2.8 ~Lr, respectively, and both capaci-
tors were charged to a mriximum,'potential of 22 W. The auxiliary cone was 7 cm long
with base diameters of 2.4 and 4 cm; the main cone was 20 cm long with base diameters
of 4.7 and 11.4 cm. The distribution of both the longitudinal and radial components
of the magnetic field in the main cone was measured with a --'- 2 mm diameter magnetic
probe, and the distribution of neutral gas on the axis of the system was determined
with an ionization manometer. The properties of Elie plasmas were determined with a
double electrostatic probe. The plasma source operated most efficiently when dis-
charge through the main cone was delayed until plasma from the auxiliary cone had
Card 1/s upco 533.9.

L 33387-66
ACC NRt AP6015310
4
3
7 8
T
JDiagram of the apparatus. 1 quick:-acting valve;
2 - auxiliary cone; 3 - main cone; 4 - winding for
compensating magnetic field; 5 - vacuum chamber;
C 6 - probe; 7,8 - pumps; 9,10 - vacuum gaps; 11 -
C, CZ - 3 '
gap; 12 control block.
7 L~j
reached it. Under these conditions a current sheet was formed in the main cone
0.28 microsec after initiation of the discharge (the period of the oscillating dis-
charge was approximately 2 microsec), whereas in single-stage operation the current
sheet was not formed until the third half-period. The charged particle density in
Card 2/3

L 33337-66
ACC NR. %PGO15310
14 3
the plasma at the mouth of the gun was 3 x 10 cm- and the electron temperature was
13 eV; the conductivity of the plasma in the main cone was of the order of 1014 cgs
units . The plasma left the gun as a jet with a velocitT of the order of 10 6 cm/sec,
pi-ecceded by a leader in which the velocity exceeded 10 cm/sec. The charged particle
density in the plasma produced by optimum two-stage operation was an order of magni-
tude greater than that in the plasma produced by single-stnge operation with the
same discharge energy. It is concluded that preliminary ionization considerably im-
poves the operation of conical inducWn pinsma guns. The processes taking place dur-
in-- operation of the gun are discussed briefly. Magnetic flux was entrained by the
curronts induced in the plasma, and during the second half-period the magnetic field
on the axis of the gun was directed oppositely to the external field. Orig. art.
has: 7 foimulas, 9 figures, and 1 table.
SUB CCDE: 20/ SUEM DATE: l3Mar65/ ORIG REP: 008/ (MI REF: 012
C.,d 3/3

L U4610-67
ACC NR: AP6033416
reduces admixtures. The effect of the magnetic field is explained by the reduction
of the diffusion of the plasma in the instrument's channel and, consequently, the
reduction of gas generation on the titanium surface, Orig. art. has: 3 figures.
SUB CODE: 20/ SUBM DATE: 29Nov65/ ORIG REF: 002/ OTH REF: 001/ ATD PRESS: 5100
Card 2/2

AC~~3 bwT(1)---1J1J(c)-- AT
3031 SOME CODEs UR/2504/6-.)32/000/0007 9
AUTHOR: Ba ov, 6. M.; Grebenshchikor. So Is., Ivanovskly. K@ I 5bJ Ik T S. f-
tan 9V&
in I.; Ahpigell, I. So
ORG: none
TITIS: Injection of a plasma into a closed magnetic trap a two phase helical
field
SOURCE: AN SSSR. Fizicheskiy institut. Trudy, v- 32, 1966. Fizilta plazmy (Plasma
physics), 7-19
TOPIC TAGS: plasma injection#* magnetic trap, helical magnistic field
ABSTRACT: A plasma injected into a closed magnetic trap must have the following
properties: 1) it must be sufficiently homogeneous in composition (hydrogen or
deuterium), it must contain a minimum number of impurities, and the percent ionization
must be close to 100; 2) its temperature must.be high enough to exclude loses due to
normal diffusion in the magnetic fie3d; 3) it must have a high conductivity to
eliminate polarization due to the toroidal effect; 4) the plasma,-fillin the toroidal
trap, must not contain marked longitudinal electric fields. The' article presents the
results of an Investigation of several methods of injections The experiments were
carried out in laboratory scale models. The first method tested VU Injection of the

6 -LV4U ( --0
ACC NR' Al~~:6 31
plasma into a "programmed" magnetic field; this method is based on the irreversible
change in the configuration of the magnetic field into a determined region of a closed
field. The behavior of a plasma was studied under rapid compression by an external
azimuthal magnetic field. The method proposed in the article involves injection of
the plasma along the tube of the lines of force of a magnetic field extracted from the
volume of the trap. Particular attenti3n is id to the problem of the movement of a
sufficiently den . -Irin a curvilinear magnetic channel. The
so plasma (n = 1012-10 cm
article concludes with a consideration of the collision of plasma flows in the
transvorso magnetic field of the trap. "In conclusion the authors consider it their
duty to thank M, S. Rabinovich for his continuing interest in the progress of the work
and for his helpful discussions of the experimental results and of the selection of
the basic directions of the investigationo Ihey also thank all their coworkerewho
took part in setting up the physical equipment and in carrying out the experimentst
Ye. P. Aleksandrov, M. S. Berezhetakiy, N, M. Zverer, luo G. Kruti ,kay, N. Ve Perow, as
well as all the workers of the workshop headed by V. P. Soloylyeve" drig.. art* has, 3
13 figures.
SUB COS: 20/ SUOK DAM' nons/ MM RM
0151 OM, MM :00?
Cwd 2/2"*

L 10406-67 EWT(!)--l P(c) AT
ACC NR: AT6
033032 SOURCE CODE: UR/2504/66/032/000/oo2o/do_4
AUTHOR: Berezhetskiy, M, S.; ~webenshchikov, S. Ye.; Zverev, No M9; ~-hpigell, L SO-4
none
TITLE: Toroidal magnetic trap of the stellarator type with external injection o the
plasma
SOURCE: AN SSSR. Fizicheskiy institut. Trudy, v. 32, 1966a Fizika plazmy (F"sma
physics), 20-28
TOPIC TAGS: magnetic trap, plasma injection
ABSTRACT: The vacuum chamber of the magnetic trap un er consideration was in the form
of a torus with a diameter of 120 cm and a cross section diameter of t0 cm. A-
magnetic field of the stellara r type (without taking the toroidal characterinto
account) has the following form:
co