SCIENTIFIC ABSTRACT KITAYEV-SMYK, L.A. - KITAYEVA, V.F.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000722920001-8
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 18, 2001
• Sequence Number: 1
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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ACC NR, ATG012903 SOURCE CODE; Ult/0000/05/000/000/0245/0252
AUTHOR: KltMev-Smyk, L.A.; Zverev, A.T.
ORG: none
@17
TITLE: The Influence of short-term elghtlefinness am the combined action of weight-
lessness and angular and Coriolis acceleratio on some functions of the human
operator 'k
SOURCE: Slatema chelovek I avtomat (Man-automaton systems), Moscow, ltd-vo Nauka,
19G5, 245-252
TOPIC TAGS: weightlessness, angular acceleration. Coriolis r4'dof C C ) man, man
i machine communication, automaton, human engineering, human physiology? VE S r,14444-e-
ABSTRACT: The progress of cosmonautics has posed the problem of development of an
optimal version for the inclusion of man in the cosmLe-apparatus system. In the
solution of this problem It will be necessary to take Into account some of the specific effects
to which the oporator-coamonaut will be subjected In flight, such" weloitla"ne 0. The pro-
I sent articlewas wri t ton as part of the program of Investigation of the activity of man-
operator subjected to weightlessness awl to the combined action of weightlessness and angular
and Coriolis acceleration. The conditions of weightlessness were created in an aircraft in
parabolic flight, with the duration of weightlessness lasting for 2s-30 see, preceded by and
followed by G force up to 15 see. In some tests, weightlessness was established without
L

L.- -31992-66
Ar-C NR- AT6012903
being preceded or followed by G force application. it vas found that an increase In the time
of motion reaction and a rise In the error during operation In weightlessness may be the
result of known disorders of the function of the visual and motor analyzer, as well as a
disorder in central ittegration. The difference In the direction of the variation In the time
of the motion reaction during weightlessness and G force may be compared to the con-
trasting variations In the muscular tonus in these conditions. The substantial decrease in
i the quality of work of the operators, and the appearance of vestibulovegetative disturbances
in them during the combined action of weightlessness and Coriolis acceleration,- which,
first of all, influences the vestibular apparatus, confirms the opinion of many authors that
weightlessness primarily promotes disorder in vestibular function,,
A reduction Intheperformance quality during weightlessness and angular and
Coriolis acceleration, furthermore, may promote a variation In the coupling between the
h=an body and the support, Le., the Best. Ile character of motion is undoubtedly
af fe,
cted by the absence of the weight of the extremities and the trunk.
This, accordifig to the authors, primarily explains the reduction In the time of putting on and
taking off the parachute harness In conditions of zero gravity. In an evaluation of the data.
obtained It is necessary to take into consideration the fact that during the first 30 see
Of wti L 8 h c I e s s n a a a, the processes of adaptation and stabilization occurring in the
neuropsycltc, cardiovascularl and other systems of the organism apparently-@'
are not completed. Orig, art. hast 3 figures and 2 tables. log)
SUB CODEt 05/,' SUBM DAM 02Aug6S/ ATD PRZSSst;*O;'1

SHAGILULLIN, H.R.; SAI-TAltoyA, F.K.; RAn.IISKIY, O.A.; M-MIrOll, G-4-;
KITAYLV, Yu.P.
, @t @ ..
Infrared absorption spoctra of semi and thiosemicartoatones of the
aldehyde and ketone series, ltv. AN SSSR. Ser. kh'Am. no.6:960-965
Je 164. (MTFA Vill)
1. Xhimicheakly Institut im. A.Ye. Arbuzova AN =SR.

RODUXOVA, Ye.O.; RUNTANTSITA. N.Y.; sortirovshchitaft plamennoy korres-
pondentsti; ICITATILL ALY., po.-htallon; ILDWA, L.T.; sortl-
rovshchitma plameanoy karrespondentsil; ZHALIWYA, H., bripAdir
pochtallpmov; ZUULLOVAs ?.I.; XWDIA, T.I., brItpdIr pochtall-
onovj TUMTA. O.A.. sortirovshchitea.
LeMing postal workers, are sharing their experiences* Test. eviast
20 no.Ilt22-24 N 160. (XIU 13:12)
1. Tachallulk 98-go oWeleulya avyasl g.Moskyy (for Rodedcom)o
2. LentngradskI7 pochtamt (for Raw7antseva). 3. Artanaeskaya
kontora avyazi Gorlkovsko7 oblasti (for litayeva). 4. Rinero-
3modskoye otdoleLlys parevozkl pochty (for Klimova). 5. 5-yv
otdolentys, eryazi g.Chel7abltska (for UAlilova). 6. Uchallnik
24-go otdolentva vvpzl golvanovit (for Ktrillova)o 7. Kuybyshevskly
pachtant (for Kharins). 8. Otdol obrabotki pisrermoy korrespondentalt
Sverdlovskogo otdeleyniya perayozki pochty (for Ttizova)o
(Postal service-Imployees)

AUTHORSj Sobolev, X.N., Potapov, A.Y.,t Fsyzullov,
F.S., Alyamovskiy, V.N., Antropov, Ye.T. and Isayev, I.L,
TITU: Spectrosoopic Studies of the State of Oas Behind a Shock
Wave. I (Spektroakopichoskoye isoledovaniya sontoyanlya
gaza za udarnoy volmoy. I)
PERIODICALs Optika I Spektroskopiya, 1959, Vol 6, Nr 3, pp 284-296
(USSR)
ABSTRACTs The paper describes attempts to measure the temperature
behind a shook wave using relative Intensities of two spectral
lines. Shook waves wero produced in a shook tube (Flg.b).
9.2 em In diameter and 4#5 m long. The high-pressure
chamber 1 (50 cm long) was filled with hydrogen at pressures
of 110-130 atm. The low-pressure chamber 11 (4 m long)
was filled with air or nitrogen at 10 mm Hg. The two
chambers were separated by an aluminum diaphragm, burstin.6 or
which produosd shock waves in the low-pressure chamber. The
spectrum of radiation emitted by the region behind a shock
wave was recorded either photographically or photoelectrically
Card 1/4 using a spectrooraph ISP-61. In the latter ease two photo-

Speotroscople Studies of the State of Ons bohind a Shook Wave. I
multipliers (FEU-17 or Fx;U-22, cf. Fig.6) were used to
register two speotral lines; the signals from the photo-
multipliers were amplified taf. circuit In Fig.7), displayed
on an osoillograph 01-17M and photographed. The shook-
wave velocity was found by measuring the timbwhich It took the
wave to travel between two Ionization counters, denotea by
lalt2 in Fig.5@ Experiments were carried out at shock-wave
velocities of 3-4 km/seo at which the tZmporatures behind
shook fronts were @6xpeoted to be 3500-450 OK, At these
temperatures neither air nor nitrogen emits atomio lines.
The authors consequently Introduced small amounts of Ll
and He In the form of LIG1 or NaCl. The temperatures
behind shook-wave frontsoalculated from the relative
intensities of Li &rd Na lineN were highly scattered
(Table 2) and the scatter varied from one line pair to
another and from one experiment to another. This scatter
was due to partial re-absorption, a3well as to disturbanoo
of the thermodynamio state of the gas by the comparatively
Card 2/4 large amounts of salts which had to be used. Moreover,

Spectroscopic Studies of the State of Oas behind a Shook Wave.
the salts settled on the cold walls of the shock tube and
their emission was consequently concentrated near the walls
(Fig.9). To ensure a uniform distribution of the emitting
substances behind a shock-wave front the authors used gaseous
dloyanogen In their second series of experiments. They
deduced temporatures from the relative Intensities of
vibrational bonds of cyanogen (dioyanogen dissociates at those
temperatures) using the method described by Brinkman (Ref.6)
and Smit (Ref.7). Again no reliable values of the temperature
behind wave fronts could be obtained (Tables 3,4) because of
the long time necessary to establish equilibrium distribution
In vibrational degrees of freedom of cyanogen. The authors
conclude that the method of ielative Intensities in suitable
only for determination of temperatures above b000011 between
1500 and 50000K the self-reversal method (Ref.6) should be
Card 3/4 employed. There are 10 figures, 4 tables and 9

Sovlbl-'@ -3-6/ 28
spectroscopic Studies of the State of GaG behind a Shook Wave.
references, of which 3 are Soviet, 2 hngliah, 1
translation of English into huasian and 3 Dutch.
BUUMBDt April 3, 1958.
Card 4/4

XITATSTA, X.
I-
Inspeollon cowittee of the primary organisation. WO 2 no*7s39-
60 JI 0601 (MMA 1317)
1, Zamestitoll predeedAtelya sovota *tuchno-tolchnicheskogo
obehaheatva strottelluo-sontashoogo tresta 16.16, S. Uroslavll.
(Technical soototles)
I -.t-

S/ I ?3/1S I /000/1D 22/0 13110 24
A004/AJOJ
AMHORS- Voytovich, V.A., Kitayeva, L,1., Bardinkova, V.V., Kuznetsova, T.V.
TITIZ: Anticorrosion protection of metal parts by plastics. Report 1,
Practice of using the r3H -150 ( B ) (M-150[V)) elastomer
PERIWICALs Roforativnyy shurnal. Hashinoatroyonlys, no. 22, 1961, 79, abstract
22B477 (qTr. Proyaktn. tokhnol. I n.-I. ln-ta. Gor'kovsk.aovnarkhci"
1960, no. 2 (4), 35 - 37)
TEM The authors describe a now anticorrosion coating, the OEN.150(V)
olastomer, representing a composition of n1tr1lo caoutchouc and a special synthe-
t1o resin. Prior to heat treatment the material dissolves well In acetone, ben-
zene, toluol or ethyl acetate. The elast4mor solution can be applied by a
brush, by pouring, spraying or dipping. ir the coating In applied by spraying
a 5% acetone solution of the elastomer Is used. @Iraying Is affected with a
sprayer designed by the Konstantinovka "Avtosteklo Plant. The application of
the coating by other methods requires a l5-2D% solution In benzene, toluol,
ethyl acetate or P -4 (R-4) solvent. The metal surface Is prepared for the coat-
ing In the following wayt sandpaper cleaning, degressing, careful drying. To
Card 1/2

3/1 2.3A l/UW11D22VV 1311024
Anticorrosion protectic-n A004/AIOI
obtain a donee coating, 4 5 elsatomer layers are applied. The first layer is
held at room temperature for 2 hours (at 500C for I hour), 7he second and su'r.
sequent layers are applied In the same way, the final top layer Is held in air
for 2 - 3 hours. at 500C for I hour and at 1500C for 2 ours. The obtained film
possesses an adhesion -to steel and aluminum of 35 kg/ca@, does not break at ro-
peated bending through 3600C and does not lose Its properties during a 200-h--jr
holding In oil at 1500C.
N. Savlna
[Abstracter's note. Complete translation)
Card 2/2

AR6035016' SOURCE CODE.- UR/0044/66/000/008/BO49/BO49
SOURCE: Ref. zh. Matematika, Abe. OB231
AUTHOR: Ved', Yu. A. Kitayeva, L. N.
TITLE: The assymptotic behavior of solutions of second-order differential
equations with delayed argument
REP SOURCE i Sb. Materialy Mn Nauchn. konferentsit prof, -pr"davat.
sostava Fiz. -matem. fak. Kirg. -un-t. Sekta. matem. Frunze, 1965, 20-29
TOPIC TAGS: second order differential equation, differential equation,
assymptotic behavior, delayed argument
ABSTRACT: Sufficient conditions for an "nearly -linear" behavior of solutions at
infinity of the equation
e(s)-yj P@cgw'1(61,00)+
are given. Under certain constraints for known functions (continuity, absolute
convergence of improper integrals'" I . the Lipshitz condition with an absolutely
rd 1/2 UDC: 517. 949.2

@kICC- NR.'-
integrable "constant" on the infinite interval), there exist equal limits for aU the
solutions of YW
Jim -LUX . f
IM
The sufficient condition in order for these limits to be distinct from zero is given.
Hh. Tavang. [Translation of abstract) [DW)
SUB CODE: 12/
2

KAIW.VSXAYAO S.M.j RADZYUXLVICH, T.M.; XlTAYbVAp L.N.; SOXOLOVA, N.N.
Introduatlon of a rapid drying SM-1 bindere Lit, prolm no.10s
5-6 0 163. WFA 16:12)

KITAYEVA, L.N.
Clinical evaluation of the indices of the cerebrospinal fluid
in treating children with tuberculous meningitis. Sovemedo
no.302-M 162. (HIPA 1595)
1, Is kliniki detskikh bolezney (zav. - prof. A.I. Miloserdova)
Kuyb7ohqvsko o med1tsinskogo, instituta (dir. - kand.med.nauk
D,A. Voronoyl.
(MOGNS-7UMMCULOSIS) (CMMMINAL ?MID),

SOV/1 57-58- 10-Z I SZ I
Tr a ns I at ion from: Refer at ivtiyy z1virtin I, Mt-ta I I urHiya I 4iW Nr 10. p 152 (USSR)
AUTHORS- MakoHon. M. B. , Panin, V. Ye@ . lKita ev Korotayek- A. D
Sukhovarov, V. F, , Shcherbakova. '. I
TITLE: The Effect of Annealing and Intermediate High -temperature
Deformation,on Compression Cur%es of Copper and its Alloys
(Vtiyaniye otzhiga i promezhutochnoy vysokotemperaturnoy
deformatsii nd krivyye izhatiya medi i yeye spln-.ov)
PERIODICAL: Dokl. 7-y Nauchn. konferentsil. posvyashch. 40-letiyu
Velikoy Oktyabr'sk. sots revolytitsii Nr 2 Tomsk Tomskiv
un-t. 1957. pp 59-60
ABSTRACT: The effect of plastic deformation (D) on the progress of
recovery processes in Cu and its alloys with Ni (5, 10, 15
atom-%). Al (5. 10, IS atom-%), and Zn (5 atom-'/0) was
investigated. Mechanical properties of metal which had been
subjected to deformation at room temperature were compared
after the metal had been annra)ro as well as _,ubjec(ed to slight
delormation under identical iemperaturr conditions It was
established that application of stress stimulates the recovery
Card IIZ processes, this is manifested by the fact thdt mvchaniLal

SOV/157 58-10-21521
The Effect of Annealing (cont.
properties of work-hardened specimens (S) which have been subsequently sub,
jected to mild deformation at elevated temperatures are lower than the prop-
erties of S's which have been annealed only at identical temperatures. A drop
in secondary reduction curves of S' 9 which have been preliminarily subjected
to deformation at room temperature is observed at elevated temperature.
The stimulating effect of loading, which becomes greater with increasing tem-
peratures, begins to diminish as the T point is approached and, finally, goes
down to zero. It Is shown that the D o?work -hardened S at temperatures
beyond the recrystallization threshold contributes to complete relief of work-
hardening stress achieved at room temperature and at the same time, pro-
duces new distortions which cannot be COMPICIC17 relieved during D at the given
temperature. Compared with pure Cu, other conditions being equal the inten-
sity of recovery processes under load is lower in the Cu alloys in--e3tigated.
As the concentration of Ni is increased and the concentration of Al in the Cu
alloy is reduced, the intensity of recovery diminishes. In alloys with relatively
small cohesive bonds (Cu-Al), the recovery processes occur more intensively
than in the case of alloys in which the cohesive forces aire greater (Cu-Ni).
Copper--Heat truatrent 2. Copper a1:oyc__Heat trcat,-ent
3. Copper-Cerorrration 4. V, N.
Card Z/Z

MAXOGONS, ".; MAMA, L.P.
Atudy of the kinatloo of ordering and nome mechanical properLies
of the Yg3Gd alloy, Mr. fis. shur. 8 no.2t233-238 F 163. (JUPIA l6s2)
It 81birskIr fisi*)-t*kWob@#kLY boUtut AX SM, Tomsk.
@(Wgnevius-cadxLua allop)

BUSHITEV, L*S.; KITAYEVAl L.P.
Electron microscope study of the domain and dialocation structure
of the ordered alloy YIg3Cd# Kristallograflia 9 no.6079-985 N-D
164. (WRA 1812)
1, Sibirskly flziko-tokhnicheekly nauchno-iosledavatollskiy Institut.

n a
I C@N_" Ul
do@ffia @JL UVV aawmium Pilo-. el"tric e---.
'nf' C @7
a v 0 -, , , 7'. 7,
A L I t h kl!-
r a ch ff r- ;4 4 t I'm nd h
A -near re lat 1,Lmshl[,, h@@xweeti 'he k- Lf-, t ri -,4 1-7n(tT;rtIvtt ,v
and the I-nme-rge of the k@@-_ *7m;- _" a r bl;
bebw, Wr-Rar
I n 4 e n c of thg- domain size is jzivs@n bv the equatinn
f ktO 3
7'rip aiittior-Q ;br-- gri- r
@tefu to I, S. Bushnev for help r1rig a r! ljvjr4@%q.

. . -, @i A F'4(14 8 'rj@i
I N" q i k i 6 1 r I @ i klv.-. 11 1, A
-n m I Tnku t I tutn
NP. RE-17 SOVf,06 CrMER- M

JD
AGCWSION NBt AP5025321 W01Z/65/020/003/0379/0383
539,22s661.W
t
AUTHORt Tukhrqju1l1nj A*OAoj Kit
L-P
TITLEs . Study of the character of orderiisordar tran3formation in alloy X930d
SOURM Fisika mstal3ov i metallovedenilep vo 20, no* 3, 1965# 379-383.
TOPIC TAGSt metal beat treatme'ntp metal analysis, x ray diffractiont
crystal etructure, Mae ium ))aso alloy, qftd%jYM ntaining alloy
ABSTRACTI Y.-ray dirfraotion studies of ordering in 1493 Cd allo" (2.2,30 atoa%
Cd) during slow cooling from above-crItical tnimperaturbs, cmdo by A. Moore
and G.V, Raynor (Act& metep 1957, 5j 10p 601)t revealed the coexletence of
or4ered and disordered regions in the samples. The present study was made to
deterraine if this coexistence was an equilibrium stato or an effect of the
unbalanced state of the alloy& The X-ray diffraction otudy of the Mg-Gd alloy
(25.2 atom% C4) was made after annealing at 350C for I hour, followed by order-
ing, consisting of annealing at 2750 for 2 hours, slow ooolinq during 5 hours
to 130 Cp annealing for 72 bourp at 1300, and subsequent cooling to riaon
cof"i 113

L h915-66
ACCMSION XRt LP5025321
temperature at the rato of 5 degrees per hour. 7he changes in the width of the
main (202) and superaLructure (M) lines In tho X-ray diffraction patterns#
vaken of the quenched samplest were measured and plottod in tho graph as func-
tions of the quenching temperatures. The equilibrium coaxistmee of 2 phases
ordered and disordered) was proven at the definite toperature Interval
-20C) after quenching from temperatures > 150C, At temperatures ;;P 170C the
N
Mg Cd allo:r was entirely in the disordered state. The destruction of long-range
orler occurred by the formation of dinordered regions In sn ordered matrix.
The volume of dizorderei regions increased with incroasad-quemehing temperature#
and at temperatures @;,170G the entire sample was converted into the disordered
state, It was shown by Z. A* Hatys"ag A. ro Mosar# and A# As Smirnoy
Okra, f1s. shurnal, 1963o So 3# 339) that 2lectria resistivity of alloys was
directly proportional to the value of (1-99,, Aare S was the degree of long-
range order# The degree of long-rang* order of the &lea after quenching
from tam erature T was determined by the author& from the ration of intensities
(is 1 1@3 of the suporstruoture (112) and main (2D2) lines by taking the 8
of the ordered sample at Sal and adculating the s or quenebed, emples by
-.=3ing the formulas
sT
T
Card 2/3.

L h915-66
ACCESSION NRs AP5025321
'The comparison or obtained data agreed well with the oorrespon4ing calculated
and measured resistiviti*ss Orig* arts bass 4 figures# 3 formulas, and 1 table,
ASSOCIATIONs Siblrskiy fiziko-tskhnIcheskiy institut rion FUAIc2t2CWL9.4.1-
n
-SUMITTED p-65" EXCLt 00 SUB COM MHO SS
OTHIRt OD5
NO RU SOVs 004

L 40-739-65 EWT (m)AWP(w'/EM(d)AmA/F-wP(t)/bw(b)/ENA(c) P*-A IJP(c)
F`.- C. @4-p kPS005 S/00 20 /F, S /1 /'0562/05 95
rj 7
L. P K
akogon, K . 4 Koby t e v S
'%nicai prop-mrties of the ordered alloy mq Cd
P rInk I 4dy. v . 160 no . I I w, FA) q
T'0@1 T T* LC' -rdqred a! la maqnesium alloy, ultimate atrprvgth.
A
_T 71hr muthors investigated the affect of ord-rinT on the
-.r-;>@ertles and on t -m i% t i on i n ^ r. Mq Cd
@ i_ he character of iefor 3
inq A hexr&qonal close packed (bcp) stnicture. The procedure
7 r- -. - : -, -i - I;. -:-- --Iloy and the sit lea wan des,7-rtberl in detail also-
I i me t a i I oved . v . 16, no S 14t,41 flvo caM-loso w*re
234K Por min"tA 10 %oft*
0 , . , I i I f tx rit
qN.1 if, photoqrmphic V%por T 1,k
quenrhed fr,fm @V)' w-1 ffir vart-
Card

L 40739@65
ACCESSION NR; AP5005SS7
t c. rn, at 8*111, after which they were doforv-u-d ftt roo-at te-rap4trature.
1!-14@rlA I on -rft-4% determined by x- r ev A i f f r act )v Mot A I I C@-
)f he v;tmple surfares wmere mAdp i r A rt
r r
r-, w i t h A Io -,,I r no
q -4 rp I s-- Fi d e f o rmefl a t t e-rpp i
Mq ICI exh ih it, ed r - AF. r,
r r% F;
i n s i n (11 deq ree of ordpr ,@r i r
hl@ I)L iero-d st ate . 7h e j I t i it, -. t e F@ r r- n r, ed
I -, q I ?.,-. and t he p 1 As t 1,- 1 1 , 1. --,1 1 , 1.)
r it, r '4 P'; A t r )(-Ar , -rr@@
,)r there phenow-ena. The metAlloqririphi t 1 0:19
'. 'k Tin hoth tho ord-prad and disorder"O at mtes -oitrso
1 '-tnp 4fte- 5'1@ defor-M'qtjon. Frr)trn a nf the
f i -tpnt 9 rind the character of he In f,)rT-n 1,4 t r i s
rna i n 7 nu a e o f t h-- I a I j f, F n A r I e- r, i 'Nq c'o of -
he disordered atate with domal n ql @-hc pre
Card 2/3

L 40739-65
ACCESSION N-Rs AP5005%87
-zence Olt wjrwq with- the olipi
Thin r@-port was pregeitted by G. V. Kurdyumov. Oriq. art. hast 4
N;,1.30C1AT101;t SibirukLy fLtiko-tekhn1cheskiy institut Lm. V. D.
(Sibtorian 1"hyxicotechnical Institute)
StMKI I 05A.-jq64 ENCLt 00 SUB CODEt MK
N' R PX,. F S 0 V009
OTHERI all
CA" 3/1

AP5027146 UR/0126/65/020/004/05ST/0591
AUTHOR: Kitays'ral L. P.; Bushnev, L. 8.4 Kakogon, X. B.,
44.5-, If f. t'@ -q-q' i, A
ORG: Physicoteahnical Institute in. V. D. Kusneteov (Sibirekly
fizirco-MMI-01101jKly
TITLE: Klcroe6oplo stud f deformation in an Hg Cd alloy
4t. 1 01,; q 3 -&-1
SOURCE: Fisike metall I mst&3-lovedeniye, V. 20, no. 4. 1965s
587-591
TOPIC TA08% aryotal'deformation# magnesium alloy, cadmium alloyl
twinning
ABSTRACT; The study was made on an alloy with a composition of
magnesium + 25.'2 at 199 cadmium. Samples with a diameter of 1 ma
and a calculated length of 50 mm were stretched on a UPR machine
at a rate of 0.23%/min. The elongation curve wao recorded auto-
matically. For electron microscope investigations, samples were
produced by rolling to a thickness of 0.27 mm. After annealing and
deformation by stretching, the samples were thinned down in an
el otrolyte (methyl alcohol and nitric acid in a 2:1 ratio), @The
thin toils were examined in a UMO-100 electron microscope at an
1/3 VDO: 539.292-;548,4

L 8936-66
ACC NAt A?5027146
accelerating voltage of 85 kilovolts. The grain size of all the
samples was about 20 microns, To obtain an ordered state, the
samples were subjected to prolonged heat treatment under the 0
following conditions: holding at 2700 for I hour coolinA to 170
in the furnace, cooling to 1300 at a rate of 10 degrees7hour and
holding at 1300 for 72 hours, and finally cooling to room tempera-
ture at a rate of 5 degrees/hour. The deformation chart was
studied after 0.2 and 5% deformatiou,and the dislocation diotri-
bution after 2-5% deformation. A figure shown the dependence of
the strength coefficient K on the degree of deformation for the
ordered and the unordered state. The strength coefficient In
determined as the difference In the flow stresses with a 1% change
In the deformation. US= 1%
0.6, (1)
where (r, and Ir are the flow stresses at = 0.2 and 1%, respeo-
tively.0'ihe valae of 6*, In takonbeyond the yield point. Ac-
cording to the authors,otge large coefficient of strain hardening
in the ordered allor in connected with the existence of superdis-
locations and with a breaking up of the antiphass domains during
2/3

C NN, AP5027146
the deformation. This x9ohantim Iq applicable also to the X Cd
alloyt since the supordislooationarbbeerved in the ordered #Uts
have a domain struoturs. Thi efiarp drop in K with an Increase in
the degree of deformation In the unorder6d alloy is probably
bound up with the development of mechanical jolygonization and
twinning, the Intensity of which depends on . At = 0.2% poly-
Sonization or twinning vers not observed. OrIg. art. has: 1
formula and 6 fig=ev.
SUB OODE.- MM, 10/, SUBM DATB: 308op64/ ORIG RLP?: 008/
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BLANK, L.Is,, Insh.; KITATEVA, X., inth.
Mechanized recording of the performance of coiiatruation
maohinee. Mekh. stroi. 20 no.8t9-11 Ag 163. (MIRA 161ll)

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Lj2AZjU_--Jj ,_#anltarnyy vrach
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KUSH=, 1h. F. KITATNIA, 0, U,
Measures In control of negative results of inbreeding In
poultry. Diklady Akad, nauk SM 79 no.4t665-668 1 Aug 1951#
(C1XL 2111)
1. Institute of Genetics, Academy of Sciences US=.
2, Presented 4 June 1951 bjv Academician K. 1. Skryabin.

1. c. N. K[rA-i--'IA
2. USSA (6CK)
h. Blood- Transfusion
7. Ex,-*rimnt in overcoming, negative effecU of Inb-rceMrw, atA effectivenens of
freoh blood transrusions in poultry breeding. Trudy Inrt. i-en. no. 19. 1952.
9. Monthl List of Russian Accessions, Library of Congress, 1953, Uncl.
X'-
R?,

KUSAN&R, Xh.1r., KITATOA, O.N.
IMMMIN
Xxperl-.iental ilats on the breading, value of crossbred chickens.
Trudy Inat.gen. no.20:225-236 13). (KLRA 7:1)
(Poultry)

UMHM, Kh.F.; IIUYVA, O.N.
Now experbwntal data on the problem of brooding related and
unrelated varieties of chickens. Tru4y Inst.gen. no.20237-248 053,
("a ?11)
(Poultry)

FU VVITTI, UTUV AD. - -it. , SIR=' - ff. - T
and NUVM,
"The Sterilizing Effect of Innizing Radiation on YAwals" Report n
TheEffect of X-and Gems-Irradlations on the Estrus Cycle of Penale
Xice." In the book "Collection of Works on Radlobiology" edited by
N. 1. Numbdin Publ. House of AS MM, MD5c0w 1955

MrWT Of IONIZINO RADIAMMS 0W THE ]VERTILITY 2114 vs A I r a r@'" WA fthi ba any @#vi %I, i'm * fri @" I'-
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SHAPIRO. U.1.1 MUZHDIN, X.Lt 11TATIVA, O.N.
Studying the reasons of disorders In the astrual cycle of nice
following total X irradiation. Ity. AN SSW. Sarsbiol. no,5i
537-355 8-0 '3?- (MIRA lOtIO)
le Institut biologichaskoy fiatki Akadexii nauk SSM I Institut
genstiki, Akadevii nouk SSSR.
(ASTRUS) (Z RAYS-MBIOLDOICAL XMCT)

AUTHOR 3 0 7/ 2 o - 1 2,-j - 3 - 2 1 A 7
TITLE: The Influence Exercised by Fractionated X-Ray Treatment on the
Ovary of Mice (Vliyaniye fraktalonirovannogo rent,,-,enovskoCo
oblucheniya na yaichniki myshey)
PERIODICAL: Doklady Akademii nauk SSSR, 1950, Voi. 12o, Nr 5,
PP. 514 - 517 (USSR)
ABSTRACT: This paper begins with a short discussion of earlier works
dealing with this topic. The author in thin cane used only co--
paratively weak irradiation doses @v 50 r). Three years old
female white mice were used as test nubjecto. They were nubjectod
to a total irradiation by X-rays, the dona,'@o being 30 to CO r
(with single and frq.,ctionated action). At the untie tine, a
group of fenak mice ran irradiated once with 1:@ r. Fracticination
wan carried out by dividine the doses ( 60 and 30 r) Into two
equid phrtn with nn interval of 1,2,4 nnd 0 4ays. Non-Irradijited
mice of one rind the name age were uned an control subjects. The
examination of the mice after treatment ic dinctin:.-.ed in short.
In the case of irradiated mice (an compared to not irrnidiated
Card 1/3 nni7: -1 considerable docronne of primor,l;al follicles in founi

The Influence Exercised by Fractionated X-Ray Treat-.erA BC@V/Zo-12o-21-21/67
on the Ovary of Nica
alrtsa-ly during t?,e firot few days follDwirf,@* treat--.ent. The rumter
of @'-rowini; follicles in not reduced until later. The destruction
of foll@clen of irradiated aninals shown a direct dependence
on the irradiation doza,,e. After a ningle irradiation with 60 r
tht, primordial follicles dioappear n1moot entirely (about 3 or
4 days after irradiation). The number of @,,rowinr@ follicles is
not reduced to the vnne extent no th-vt of t'%e primordial ones;
it occurs only after mnme loneth of ti-ie. In the cane of a
fratitionated X-ray Irradiation more follicles are conserved than
If irradiation taken place only once with the name dose. V,o
longer the interval between irrTidintiona the lar.@er will be the
number of conserved folliclen. If mice tire subjected to a single
irradiation with 60 r, the number or primordial follicles
decreases very considerably. but this In t1rie case to an even
f;reuter extent in the case of fractionated irradirtion with the
sm.-in done. In conclusion, the auth,r thanks '1.1.?.uzhdin, Corro,
sponding Member, AS USSR, and N.I.Shnpiro for their advice and
aid. There are I table and 13 referer.ces, 3 of whicl, are Soviet.
Card 2/3

The Influenco Exexcised by Fractimitel X-Ray Troatnet,t 3,0-7/2o- I 2o-3-2 1/67
on the Ovary of Mice
PRESENTED: February 17, 1958, by T.D.Lynenko, Ucm@crq Ac.-Ale-ty of Scic-r-cer,
UISH
SUB@IITTED: Feb@rtmry 13, 1953
1. Genital glanda-Effects or radiation 2. X-rays-PhysiologIcal
effects
Card 3/3

112690
.J/74'1/62/000/000/011/025
D296/D3U7
11. 1., ihapiro, N. I., Petrova, 0. Jj'. and_Xi-
T.,LL'i' influence of x and 6radiation. upon the oeu-11run of
mice
Hadiatsionnaya genctika; sbornik rabot. Otd. bi'
ol. nauk
;tN -*JzjJH, Moucow, Izd-vo Ali' SJ'.JR, 1,)62, 133-179
Hiotoloj;ical Lind croso-breeding methodu ati well its observa-
tion of tiie oeaLrua have boon extensively @uued to attuly the mecha-
-.Im reo,,on3ib e, for radiation-produced sterility. The authors cri-
_-_ze tochnical shortcomings of previous studies which led to
c,):i-.r!vi.Jctory ruoultuo I@heyatudicd tiie effect of ionizing radilation
up.m I.Lj fertillity of ferkile mice, by following up the oentrus us-
iot-tined vat,inal umo@@rs, taken daily in the first three months#
in UIC bixth minth ufter exposure to total body radiation.
p-ases of the cycle ware establiuhcd qualitatively nd quanti-
t a
on the basis of the relative )roportion of the 3 main ele-
1/3

S/7 4 1 62/u00/00/011/025
0@ x Y,
)296, ir',07
azinized flat(OO 'Irld leuc c As tho
it outiafactory but nevert'iL
-leju intlirect index
@;rtli-Li *.y, ,@f pre rt,aac,etj and of )ro;;eny was also re-
A.
.I @'Qlc t @:L@i ica,,. Ion af tor the irradiated femalea had been
@'Qr ,%j t, iyu. A exp)Gire to x rqu WaG found
naI-IULr o.,* cyclea @trid their frequency in the group
*.he c@feie the proi)ortion of the pro-)-utrus and oes-
were dl-iin ik; lied and the proportion of ti.e. met-ocstrus
uOrreapondir.i;ly increaued. %e de@-,ree of tl'-Aese
@iiroctLj depondant on the doi;e and or. the time since
-e- j@ueu ar,(4er 50 Ar had no effect upon the ocatrus al-
d A. &
_".y wiiz) -mptired even by douea of 15 - 25 r. After ex-
40
ij a I'latency dt:riod" of 6 weeKa during which
4 iiolvicod I;id 4/hIch becomes ohorter after exposure to
V -00 U'.j 00 - 4vO r). 3 months after the irradiation no cycles
@),J.JC@_VQd in of -.he animilo. The dinordera were irre-
ii fj;, period if observation (6 months). Nulli-
au woll au mice of different utraina
L);. A C j A ;i Oiral@.x i.i..awxr. ahronic expouure to r rayo, even in

0/747/62/000/000/011/025
influ@@nce U-1, x ... D296/1507
a,Ojeo, very clo-je to the maximum permiuoiblo dooet led to ci-
C,@L.Igcu uftur a lutency wriod of 12 montho (0.4 r daily -
klo-lic 11o.7 r) up to 15 monthe (0.2 r daily - total done 72.8 r
,D.L- J.1 r Liaily - !.otwal doue 36.4 r). 0.05 r daily had no effect upon
*i.e oe@,trus Therv are 13 figorcs and 12 ta'bles.
;,,"2 loN; Inuti tu'40 genotlyi AN jJJR (Inatitute of Gune'ticeq AS
U.JJ4) and Inatitut biologicheskoy fiziki Ali 63:jRj
kloijkva (Inutitute of @diological Physics, A@; USURg
MOBCOW)
Vard 3/5

h2691
3/747/62/000/000/012/025
D296/007
s Jlwplro, IS. I., iuzhdin, N. I. and Xitayeva, 0. N.
'.;tu(Ij of tiiu causes loading to diuorders of the oestruo
.@ra mice expoued to total body rad.iation
ftadiat"iunnaya genetika; abornik rabor. Otd, biol, nauk.
AN Jjjll, Njoucow, lzd-vrj Ali' 3-JjRj 1!),62, 180-210
1: In a prev."oua paper (jb. rabot po radiobiologii, Izd-vo AN
,;j-JR, 19j5, 113-14')) the authoru had uhown that the oestrual cycle
;.-ilce 18 iiij;hli radiojensitivo. In the present utudy tho authore
t,-4Led to eatabliuh. ahother the oterility qauued by ionizing radia-
-ij due a) to imijairnant of 1xiduction of the gonadotrophic
from the pitui,.ary gland, b) interference with the res'ponee
':,y t.',Ij va,,*ina.; opithelium to ocatrogeno, c) deutruction of the ova-
folliclea, or a) other cau,;es. '.&ey aluo tried to devine an
Qxdcr,4.-"cntul technique for tho restoration of the oestrus. flice were
exi)oz.od to total boay irradiation by means of x rays in a dooe of
WO .-; homoionatoo of tiie p1tuitary t;lande were then used to carry
G'Ard 1/3

3/747/(j2/00U/UU0/012/25
""tudy of thu C'1U;jCAj ... 'U2 jU/D5U7
Veaction On infantile Mice and were
.4
to Po.,;jeoj tie noma.L ;on:idotruphic activity. The va,,,inal
c:j'@I.clium o,' Liie lvr,tdiated .Uce gave a norzlal reUpoTISC to injCc-
A
IL L. 1
_)n3 of beatrol, as chown vtgina' mmears.
cunLuntj'.@on tiiat izter-vxp.)rure to radiation of the
foiiicloj Ij .,*-.e main cause of the oej'(.rual diaorderap the
*%.rW1Ud1anL-_-a nur..,;all ,varies into the Irradiuted Mice, where-
1101-mal 'ju-itrub cycle wau reutored. If transplanted
removed or under,.ent rLz,)retion the cycle
r. @,-z@caome lnvcatigal4on revealed com-
0.1, foilicieu and an almost cotlple*vr; lack. of corpora
C a -"Q ovari'.!a a" L""C irrudiated mice. '11,eae ovarieu mainly
J" olroml-. " jiuvoLio *%,;,.e transplanted ovaries showed a nor-
whether vory high douca of ,;onadotro-
cj,i.La roduce a response from my rcaidual ova-
n ii-r;ikilatcd ovarie3 the Mice were
6iven 60 mouse
Of J,ormone. The ovaries and uterus reoponded
@@n increnuc 'An @md size but no restoration of the atro-
cuA1,i oe oba,.rved. There are 13 fi-ures and 6
0
"t U
.'
C,,-rd 2/3

S/747/62/000/000/012/025
tud@r Of Cho C'AuBeO 1)296/D307
Ina-itut bialogicheakoy fiziki J Institut genetiki
All I .;.j
i ;@-H, Mloukva (ln-titutO Of BiOlogical Physics and
Inutitute of Genetics, AS USSR9 Moscow)
Ird

KITAYEVA. . R. 1.
Efrect or corchuroolds on the ewree and outcome of expoprimontal
myocardlUs and myocardial scleroalB. Farm. I toko. 27 no.l.-43-48
Ja-F 164. (MIRA 17:11)
1. Kafedra farmakologil (zav. - doktor md. nauk V.I. 7#vrazhnov)
Voronexhakogo gosudarstvennogo meditsinakogo itistitutA.

XITAYEVAt
I%,--
Effect of corchoroside in oxporimental myocarditte. Farm. i toks.
25 no.li62-66 Ja-? 062. (HIHA 1514)
1. Kafedra farmWwlogil (sav.-- dotsent V.I.Zavrastmay) Voronoshakogo
gosudaretvannogo me(UtsinsLklo instituta.
(MOT-DISFM (CARDIAC GUCOSIDES)

6ii-4 va, '). /r-A.
J:L1 ,i.A.; nUMA. 8.1h.
Photooleatrio dolorinster delornination
In cellulose. Pum.prom. 27 no.120-10 D
of Iron and sulfate content
152. (XLVA ?s1O)
1. Xoskovskly filial TsVIID,
(Cellulose) (Golorbmtry)

Sbidylujo the rrocess of woul;A111), elect r.
no.(::,-7 J* '57. -?A 10*8)
I.Mool-c-isk.11 filial TSentrallnn,", nauchno-io-~'ovd,-),inti"lskoeo 1"t t
A I 'its
bumagi i Institut gookhinii I t4ralitichookvy . d-iii ir. V.I. Torn&iskogo
Akadomit navik
(Woodpulp) @Elsotro4txlrvls)

MIUM, B.G., doktor takha. nauk;_XITAMKU* R Kh-
Reducing dielectric losses In cellulose for capacitor and
high-voltage cable papers. atm. prow. 34 no.5:4-7 My 159.
WIRA 12t6)
1.Koskovskly filtal ?Soutrallnogo nauchno-Issledovatel'skege
Instituta tsellyaosnow I bumchnor proWshlonnosti.
Oellulese) (Dielectric heating) tPaper)

KITAYEVAt S. Kh.
Cand Tech Sci - (dies) "Study of the effect of ash elements of
wood sulfate cellulose on its dielectric losses." Leningrad,
1961. 17 PP; (Ministry of Higher and Secondary Specialist Educ-
ation RSFSRj Leningrad Order of Lenin Forestry Engineering Acad-
emy imeni S. M. Kirov); 150 copies; free; (KL, 7-61 sup, 238)

MILDVO B.G.# doktor tekhnonaukoj XITATEVAj S.Kh.0 atarshly nsuchnyy sotrudnik
---
- 4 Ways of Improving the technology of the productIon of voodpulp for
, "... .oondenser paper. &s.prom. 36 no.ls9-12 Ja 161. (MM 1413)
.L-Hookovskiy filial Toosoyusnogo nauchno-issladovatellskogo Institut
bvmaWmoy prom7shlemosti. (Woodpulp) (Paper)

.@p nitlcn br tw-ri rnnynait Ir itrd 14,,t
Izv, SO A:!

KITAUVAj T.Q.
Studying the effect or nucleases on the capacity of the
influenza virus for the reaction of howagglutination. lay.
Sib. otd. AN SOR no.7slO6-108 162. (141.11A l7t8)
I* Institut taltologii i genatiki Sibirskogo otdeleni7a AN
SSSR, Novosibirsk.
6,i @

KITAYT,VAt V.
Th the State Co=itteo of tl,,.e Light bduatry A*.tacl.ed to t@o
State Planning Commission of the U.S.S.R. Yoz)i*--obuY- prom,
7 no. 1005-36 0 165 (Mll.RA 19il)

KITAYEVA, V.F.-.6jrve-stigations of the Yoms and Widths of Spectrum Lines
In a Constant Current Electric Arcs*j D1330rt&tlOng For
Degrees In Science And Engineering Defended At U33R Higher
Educational Institutions(34), Moscow State U Imeni. M.V.
Lmonosov, Physical Faculty, Moscow 1955
SO: jalahaM Lpto2is' No. 34. 20 August 1955
F r the Digren of C-indtfite In

StudyIng the shape and breadth of spectral lines In d.c.
olootrio &rem. 19W. AN SSSR. Ser. fit. 19 no.1:2?-28
ja-F 155. (KLU 8:9)
1. FlatchoskU lustitut laonl P.N.Lebodeva Akadeall n&uk
SSSR (Spectrun awlysim) (Spiectroustor)
7 4

AnI i--
t alM,
11:11 . I I ;; 15a j.
1 2 . ? '3 to &
1.74 1,
1-4
agil 1i I fill,
46411 11114 .I j I V
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fl-4 '11 91
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311 1
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41
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3 0: A.1
q ja q gi I

XITAMIYA, T97. I SMOLIY# Ist,
Broadening of Oeotrm line# In a Co. are. fix.sbor. no.4:
312-315 '58. (MIRA 120)
1. listchaskly institut tuent P-N-Lebodeva AN SM.
Olootric are) (Speetrw anal"Is)

AUTHORS: Sobnlev, X. N., POtapov, A. Y-t Kitayeva,*67A6" qn 6.4128
V , Fayzullov, F. S., Alyamovoilly;
, Antropov, Ye. T., Isayev, I. L.
TITLE. The Slectroscopioal Investigation of the State of the Gas
Behind the Shook-Wave (Spektrookoploheakoye loole4ovanlye
sostoyanlya gaza za udarnoy volnoy)
PERIODICAL: Izvestiya Akademii nauk SSSR, Seriya fizicheskayat 1958,
Vol. 22, Nr 6, PP. 730-736 (USSR)
ABSTRACT: This paper describes a practical method of obtaining a high-
temperature plasma for research work carried out In laboratories$
via. the method of the %hock tube" (Fie 1). The shock tube Is
divided by means of a diaphragm into two chazbers (for high-
and low pressure). An soon as high pressure develops in the
high-pressure chamber the diaphragm is caused to burst, and at
the same time a shock wave forms in the second chamber round the
shock center - 1. e. the rarefying ways. Between the fronts of
the shock wave and the contacting surface a layer of gas of
high t:Tporature to formed which Is here described as "lock"
Card 1/3 (probk . This "lock" moves with the velocity U 2, -which to

The Spectroscopical InvestiCatior of the State 307/46-22-6-23/20
of the Gas Behind the Shook-Ways
Card 2/3
somewhat lower than that of the shock wave U 2. The temperature
of the "lock" increases with a reduction of the molecular weight
of the gas. If the velocity U 8 is known, it Is possible, by
basing on the law of conservation of the mass, the impulse and
the energy, as well as on the strength of the ratio of enthelpy,
the degree of ionization, and the state of the gas, to determine
the 6 unknown quantities; p,O Q21 U20 H2 , T2 and a, relatine to
the state of the monoatomic gas located in the "lock". A
graphical illustration of 3 states of argon and 3 states in air
behind the shock wavo in given. The device Is described on the
basis of a schematical drawing. The chapter dealing with: The
Method of Relative Intensities describes the use of the
device mentioned for the purpose of obtaining the spectral lines
for Li and Na for measurinj; the 'temperature by the method of
relative Intenuition. Measurements were carried out photographical-
ly and photoelectrically, without as well as with full reOmMUM
of spectral lines. The chapterL The Generalized Methol of Re-
vereing the Spectral Lingo is based upon a paper (Ref 7j in-which
the said method to o.xplained *Ith respect to its application for

The Speotroscopical Investigation of the State SOY/48-22-6-23/28
of the Gas Behind the ShOck-v&vs
the purpose of measuring temperature without observing a moment
of reversal. In this case the optical scheme is used for carrying
or,at the following measurementas The radiation intensity,of the
gas in the spectral line, the intensity of the radiation of a
source employed for the purpose of comparison, and of temperature,
For measuring temperature a device was used which is described by
mvans of a schastical drawing (Fig 5). Finally, a graphical rt-
presentation of the results obtairA. by measuring the tempera-
t,ires of nitrogen arA the air behind the Impulse way* by means of
the photoelectric method of the reversal of spectral lines is
glTen. There an 6 figures and 7 Werenoes, 3of which axe Soviet.
ASSOCIATIONt Plzicheskiy institut im. P. N. Lebedeva Akadendi nauk SSSR
(Physion Institute imeni P. If. Lebedev. AS USSR)
1. Electron gas-Spectra 2. Electron gas-Radiation 3. SpecuVe-
COU 4. Shock tubes-Applications 5. Shock waves-Analysis
.Y
Carl W3

KITAYLVA, T.F.
Studying the forn and width of spectral lines in a doe* arn.
Trudy ris, Inmt, 11t3-64 159. (KIU 1313)
(spectroscopy)

80BOW. 11.11,; XITAMA&_Yo@o; RODIN. G.H.; FATZULLOV. Y.S.; 71MMY. A.10;
Temperature of the flame of a liquid-propellant rocket sr4ins#
Part 2, Zhurotakhfis. 29 no,.1:37-" Ja 159, (KIRA 12:4)
L lisicheekly institut in, Polio Lebodeve, AN SSSR, Koekvae
(Rockets (Aeronautics)) (71me) (Temperature-Moasurement)
.:.: @j ".;

@000 68381
,:;z j t/ 0 0 S/051/60/008/02/002/036
AUTHORSs - Alyamovskiy. V.N. and KitjY22g!3#!F.
TITLZt Contour of the It 0 tly@;Qgen Line in i@g_on Behind a
Shock Wave
PERIODICALs Optika I spektroskopiya, 196o, Vol 8, Nr 2,
pp 152 - 156 (USSR)
ABSTRACTs The present paper is part of the work carried out at the
Fizicheskiy institut AN SSSR (Physics Institute of the
Ac.Sc., USSR) on spectrosco ic, investigation of the state
of games behind shock wavesN." The authors studied the
contour of the H 0 hydrog-en line behind a reflected shock
wave (the intensity of hydrogen Lines behind an incident
shock wave was Insufficient for photographic recording).
This particular line was chosen because (in contrast to
Ha, HY *to), it does not possess a central Stark componon-
and therefore its theoretical 11oltsmark contour can be
calculated more reliably. Shock waves were produced in
a shock tube (Figure 1) described earlier (Ref 1). In
the high-pressure chamber hydrogen at 80-110 atm was use
Cardl/4 q/

Contoui the
PlAsma"behind a reflected shock wave (Figure 2) consists
of two clearly separate regions. The first region (up
to - 100 lie) represents emission after the first
reflection of the shock wave from the end of the tube an"
has a characteristic constant intensity; the second
68889
s/o5l/60/008/02/00.2/0@6
9201/9391
H0 Hydrogen Line in Argon Behind a Shock Vave
Tho low-pressure chamber was filled with argon at
~ 0.3 - 3 mm HS, to which 2-5% hydrogen was added.
Velocity of the incident shock wave varied from 3.6 to 4.8
km/soc and the corresponding calculAed values of tempera-
ture and pros ure bshind a reflected wave were
^- 12 000 - 1; 000 K and 095 - 1.5 atm. The H0- line
was recorded photographically (cameri! with r n 270 mm),
using a spectrograph I.SP-5i with 4o X/mm diaper ion
the H0- line region. The spectral alit width we: 0#81
Time-resolved spectra (resolution of - 25 ps) were obtained
using a rotating disc (- 1 500 rpm) in front of the
spectrograph alit. A typical emission spectrum of the
region represents emission after mubsequent reflections

68881
S/051/60/008/02/002/o36
Contour of the H P Hydrogen Line in Argon2HAORA91 Shock Wave
The authors analysed the H P_ lines in the first region
only; one of the contours obtained in this way in shown
in Figure 3 (circles represent the experimental points).
The observed H 0 contours had considerable half-widths
Oo-6o 1), central dips due to the absence of the Stark
component and a slight asymmetry (-.-6%) . These contours
agreed quite well with 11oltsmark's theoretical contours
(one such theoretical contour is shown as a continuous
curve in Figure 3). From the experimental contour and
the half-width of the H -line the authors deduced
concentration of charged particles in argon behind a
reflected-shock 'wave. The va 1@ as-3btained in this way
(they were of the order of 10 cm ) agreed quite well
with the values calculated using Saha's equation4 aszumin.@
that argon in an ideal San and that it is in thermal
equilibriums (a table on p 155). Acknowledgment is toad
Card3/4 to N.N. Sobolev for his advice.

68881
8/051/60/008/02/002/036
9201/9391
Contow- of the 11 p Ilydrogen Line in Argon Behind a Shock Ways
There are 4 figures, 1 table and 10 references, 2 or
SUBMITTEDt which are Soviet, 4 English and 4 German.
June 22, 1959
cilud lt/"

21-970
11 Y/)
4 "6
D ok. 1 adi 'j'.UdvMI 1 1."'. U% '4
TEXT: The 11rc-ent pu@(,,z , Jvo:-, a Ur.'j Cf t"
d CI C r:-4 I-,
ar'l if i r, c s exlvri-@V-'
40t al. 'Lof H. R. ;rloms A.
of .-J--Jro,-;cr. Linv@,- in
WanhinGton, 1960; iiiyv. aev., 116, j, (1'@59); ;i.
71-6
A hyr. 'Rev. '1-,14 1 lct,@r.Anvd
ClOritciura of t!ic *.! lia,@j emitted from a d.c. c,irlon 'r, rm
m
of ar'-ofl with 5/0' ji.2' jile half-width, 01* t@ict ;;-.s
Fig. 2 shown tilt) a '.'r g- line-, detercifle'l Q11 a o1io6. wa;.
ill kry@ ton with 1" -;i uni E. In ar,"4,n v6iti@ I ri
z 21 v k
cal.3 1/7

I 'A 3 1
is 1. 0 @7 0 1"'y
nati.-f:ictory
':trat--z fur, c t ii-t@ -in I o. ,.i ur eff ec, twii I c I. ii re nid@ rc .1 In -v
tnoary of jricL@ Ut U4 Al'O 0 @:.Ccnt r..t ion
of tac ciairt@vd pirtlelva dotorminel fr@ .7, t@,io c i,'
IL'Id ti",t daLur-inty I fro.-n t1w half-vi4ti. if y1roj.-, nI inva aj;rpe V, th
the valuva uxlic-rimuntilly determine-i tlait tbs.@ t.,.-iory jovolopel 1,y
,;riem vt aI. in caurnat. It In Lxr#-I'@,re t.) @i'@tr7-,.ne thf! C-In-
contr,ation of cb4a6od i,zirticl es fro:7@ tliv bronde;.in,, o.
by me4im ol tnio tixury. For this I.urpo3or, Fig. 3 f-It different
relativne between the concentration nf the rharsod ;.a.-t17'1- %rd t@ip
7-
"j.,'
of 11PI I., o For detez of ti.o p..rtlciv;@@q
the uuthor recommui-Ja the H line fir I C(Mcl!ntz-
15 17 p
-11 -.;leo -@Iti 0 @ e
2. 1 o 10 , wid tLe 11 1 Ine 1, - c n t I
asymmetry uf ti,t) it, 11rien (Figa. I anJ is f!x.1a1Y-x1 x !-@c to z-
P
quadratic S'v,,rk effect. Fivally, 'ar"!
experiment in tiift c,%,;p of tj,u Juj,cnde.--.cn of tr.i
maxilma of ifplinoo on the hal.'-wilt!, io ds!rAt w@,th t,ii3 t:.e rc:-;1t.,: u@.osn
"ard Z/ 7

219 70
3/02 6'1/137/005/913/026
Broadening of hyd.-ogen lines in ... B104%214
in Fig- 4 G.:0 discussed. There are 4 figures "nd 0 references;
4 Soviet-bloc and 4 non-Soviet-bloc.
ASSOCIATIOU: Fitichattkiy inutitut Im. 11. .11. Lobedeva Akrtdemti nau% SSSR
(Institute of Mysice imeni P. 'it. Lebodev, Academy of
Scionceit USSR)
?RESENTED: Decembor 159 1960# by L. As Artsimovicht Academician
SUBUITTED: December 3j 1960
Card 3/7

I Arjt ?a-4/Fd-,4/Pr-4 'WWIJD
ACCESSION M.- A11300296 8/0124/63/000/005/ao2k/1095
SOURCE: Rzb. Makhanitap Abe. 5B121
IAVrHOR: Alyawyokl _!.N. I Arom pot 11tayovat V9 ro
Yi- _4v. As I Bviridov, A. 0*
M. No . mwqm@ -
TITM Ex"rimuts-1 detemination of the eoneentration of-charged particles
In argon and krypto Inhind a shock wave
CMD ills 0b. _Qw. magdtus. g1drodirwath I diamiki plet'sy. Y. 2. Riot
AXITAtyMs 1962t 379-386
TOPIC TAGS: argon,, k37pton.. @book v*"# spectroscopy, contour line# electron
teVersture
TRANSLATION: ftectroficopic studies of the states of the inert pose art= and
krypton behind mbock waves waft mMo. The contour lines of hy&-ften in
krypton were studied lehisd the incident we"; In argon, bobind the reflected.
TbO hYdr*Pn aftixtvxt 'mw about 1-5%. The Initial pnosure "a ef the order
of 0.2-1 of wriur3r, 'In the argon behind the reflected vevep the calculated
[Card 1/2
-5S",
-4

ACCUSION M: A83002656
temperature was of the order*f 12=-130000 X. ?be concentration of electrons
was determined by the @sethod of aoqWlson of %be eqmrimental co2t4mw lines
with the theoretic*1 onesp and the teeparaturs was detemined using the ass=ip'tion
of thermodynamic equilibrium, Yu.R.
DATE ACQ: 1hJun63 OUB COM S ps IIICLt 00
Card 2/2

_1 i;' @,i 7
S/051/62/012/002/004/020
E032/ES14
AUTHORS: Kitisyevn. V.F., Obukhov-nonisov, V,V. and Sobolev,N.N.
TITLE: Concentration of charged particles in the plasma of
an are burning in an argon-helium atmosphere
PUMODICALi Optika I spoktroakopiya, v.12, no.2, 1962, 178-185
'rv'XT: The authors report an experimental study of the
profiles of the hydrogen line s It f and 11 6 emitted by the
plasma of an arc excited In an atmosphere In
the current rnnge 1-200 A. The arc was produced in a special
water-cooled chamber. Hydrogen was added to argon and helium
in amounts corresponding to 0.2-5,5' by pressure. The central
part of the arc was photographed with the grating spectrogr 'aph
,Q(5C-4 (DFS-4) whose dispersion In the second order was 6.@ A/mm.
The spectrograph alit was 0.025 mm and the corresponding half-
width of the instrumental function was 0*3 As This half-width
was determined experimentally from narrow lines emitted by a
Goisler hydrogon-filled discharge tube. The line profiles were
compared with the theoretical profiles based on the work of
H. R. Griem, A. C. Kolb, K. J. Shen (Rat-51 Stark broadening of
Card(@_l

Concentration or charged *so S/051/62/012/002/004/020
E032/E5i4
hydrogen linen in plasma. March 4, 1960, Non. Report 5455, U.S.
N.R. Los Washingtonj Phys. Rev., 116, 1960; A.C. Kolb, 11.1t.Griem.
Phys. Rev., 111, 5111, 1958). A satisractory agreement between
the theory and experiment was established. This comoarlson also
yielded the chnrged-particle concentrations for aremproduced in
argon and in helium in the current range 1-200 and 6-200 A,
respectively. The results obtained are shown in Fig.5. There
are 8 Vigurest
FIG.3 Legend. Concentration or charged particl 16 8 N in the
plasma of an arc nip a function of the arc
current.
a - neglecting the instrumental fNinctions and
Doppler broadening,
- n1lowing for these two offectst I - argon,
11 - helium.
The experimental points are identified an followst
Argon1 1;5%1112 flashed at 10 litrea/min, electrode
separati n 2 mmi 2-5% H 2 at 10 litres/min,
electrode sop ation 25 mm; 3-5% of It at
Card 2/4 3 litroo/min,111 a 12 mmi 4-2% H2 at Is litres/min,

Concentration of charged saa S/051/62/012/002/oo4/020
9032/E514
i = 12, 25 mm. The numb*rx on the curve
indicate the temperature in OK.
SUBMITTEDt JanuarY 30, 1961
I
Card 3/4

10025
S/057/62/052/009/008/04
Bi25/Bis6
AUTHORS., KitsZ!v@ It, F,j' Kol*snikovt To No, Obukhoi-Dentsont To Tot
-ain-d-Soboleyt-Wo No I G
TITLE: Structure of the positive column of an arc discharge In
argon. 1. The local electrical characteristics of the
column
PERIODICAL: Zhurnal tekhnicheskoy fisiki, v. 32, no. 9, 1962t 1084 - 1009
TEXT: The field strength and the radial distribution of the concentration
of charged particles are determined from the contour 9f the hydrogen line
Hot and the radial distribution of temperature, to measured for a non-
equilibrium plasma (I - 4a) and for an equilibrium plasma (I - 10 - 200a)
In an arc dlachnrge In a hydrogen-sr8on mixture (Arit94-0%, H2 -A st 0
-and C impurities). The volt-ampere characteristics (Fig. 2) are shifted
if there to a change In the diameter and material of the cathode# the
hydrogen concentrationp or the velocity of the gas flow. The general
!hap* of the characteristics is practically Independent of these quantities.
Card 1/4

S/05 62/032/,009/008/014
Structure of the positive... W25Y,186
The dashed line shove the extrapolated sum of anode and cathode drops. The
descending branch is due to the change in amperage of the columnj and the
ascending one to the increase of anode and cathode voltage drops# The
field strength is practically constant at 1 t5ft. The radial distributions
of the concentration N0 of charged particles (Fig. 3) and of the current
density J(r) - a(r)E (Fig. 4) in the column are calculated from the exact
formulas of the kinetic theory for the plasma conductivity o. The
concentration of charged particles and the column radius Increase with In-
creasing amperage. There is no indication ofo: pinch effect in air at
these amperages. The amperages calculated fr J(r) in a partially ionized
equilibrium plasma agree well with the amperagon measured. The formulas
here given for a In plasma hold as long as the Boltzmann equation Is
applicable to the plasma. the applicability of these formulas for
concentrations of It ion *1015 00-3 cannot be established yet, from lack of
experimental data. There are 4 figures and I table.
ASSOCIATIONi Fisicheakiy institut im. P. No Lobed va, Moskva (Physics
InstItute imeni P, No LebedeY9 Nosco:)
Card 2/4

S/057j62/032/009/008/014
Structure of the positive ... S125/B186
SUBMITTED: July 279 1961 initially)
January 29# 1912 (after revision)
Fig. 2. Volt-ampere characteristics, (1) Diameter of the cathode 2 ant
of the anode 6 mm; (2) diameter of the cathode 6 an, of the anode 12 m.
Fig# 3. Radial distributions of@th*.concsntration of cha rged particles
In the column of the aro
0 (1) 200al (2) 4dal (3) 10al (4) 4a.
Fig. 4. Radial distributions of the current density in the coluan of the
aro. Designations as in Fig. 3.
Card '3/4

Structure of the positive#&.
Fig. 2 Fig. 3
01
Card 4/4
3/057j62/032/009/008/014
B125/B186
Fig. 4

L 14526=kL Wr(l)/ZW(k)/8DS/1=(b)-2/ZS(V)-2 kFFTC/ASD/Y-cZ-3/
AFWLISM PI-4/Fo-4/Pab-4/Pz-4 AT/IJP(C)
ACCEMIO'l NRt AP30055:.5 9/0057/63/033/008/1011AM
AVISOR- Roomer, M. D I rrank, A. 0.1 Ki+W0Vft V.
TiTlZi Localization oil hIgh-frequency induction disch" 71
SOURCF,4 Zhurnal tekhW,ebeskoy f1siklo v. 33# no. 8o 1963,, 1011-1020
TOPIC TAO1- induction discharge, ht&.-frequency discharge, b1gb-froquency Induc-
tion discharge, plasmaj plasma discharge, hydrodynmic instability
AMSTRACT: A detailed Sw4estigatlon, has been %ado of conditions for the loaallm.
tion of high-frequency Induction discharge In H2, He, Ar, and idr at pressures
of 1.0 to @O m Eg, discharge frequencies of 5 to 16 Me, and discharge currents,
of 30 to 120 amp. It vas found that during an hf induction discharge in a bell-
Saw-
shaped magnetic field ct a gas pressure above 1.0 mm 11go a plearma coil is
ateil whic-h to separated from the valls of the vacinm chamber and VhIch Imts,
during the whole hr Vulse. The conductivity, terq)erature, and Ionization rau
of the plaxnOwere measured, and the abepe of the plwna coil -ins investigated
by means of hlgb-ape,@4 photography. A qualitative explanation of diacharge
localization Is given cn the basis of a hydrodynamic model of veeakI7 Ionized
Card 1/2
N'

L IA526-63
plems. "no autbors
AX!W and 1. __X,,_ghWkil_for help in per-
fomtng the *nortwouto and No 5j_AablMovlch and A. A. Rukhadze for Yaluable
ou"ostions." Orig. art. hii-F-4 figures agod
Card 2/2