SCIENTIFIC ABSTRACT -

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000308510009-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 12, 2000
• Sequence Number: 9
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

CHEFICHP I.B.
Granioplasty in large osseous trepanation defect of the skull ulth
organic glass Voen.-med. zhur. no.6.,82 Je Y61. (HIRA 14~:8)
iSKIJLI~ZURGEHY) (PLUIGLAS-THERAPEUTIC USENI

EAUSTINGp Ye*A.; L37Wp I.Mo; SABIXEVp M.F.1 IMSfZX9TSKrY0 V.I.;
,1.; Primim3i uchastiyes FIKULIN, S.A.;
PHEAW4 M
NONSTAMINOVA$ T.A.1 KOVAL', F.Ya.; KRYZH&POLlSKAYAg.:, P.P.;
SHULIGAO Ye.A.; NIKITIN., V.N.; DOROFEYEVA, A.N.
From practices of producing 19G steel at the Komna skiy
Metallurgical Plant, Stall 22 no,2:155-159 F 162. (MIRA 15:2)
1. TSentrallM nauchno-issledovatelvaldy institut chexmoy
metallurgii i Kommmrskiy metaIlurgicheshy mod,
(Ko=marokiy--Steel alloys-Metallurgy)
(Rolling - jMetalwork) )

~TIMDFEM, D.I.; .!~~ M.P.
. - ,! SABIYEV,
Effsot of defeats in side and end edges of vlaba on the
quality of the sheet. Met. i gornorud. proz. no.3&36-
37 Itr-Je 164. (MIRA 17g10)

KHOROSHILOVI N.M.;.CHERIJER,,. M.I..; LOXTIONOV, P.Ya.
Effect of the rolling scheme on plate steel quality. Stall 24
no.6:524-527 Je 164. (KRA 17:9)
1. Kommunarskiy-notallurgicheskiy zavod.

SEMEYEV~ YU.V.,- ANTONOVICH, V.I.;
POrtal pressure in acute experimental lasion of the liver. Trudy
Inst. kraev. med. Ali Tadzh. SSR no.D164-177 162,
(MIRA 17.5)

NIKOLkYHVj, V.A.,-.C NEFEDOVY A.A.
Regularities of advance changing in grooves for the rolling
of angles, Izv,k vys, ucheb, zav.; chern. met. 6 n0-4:83-87-1.63.
.(MIRA 1615)
1.4 Dneprodzerzhinsldy motaIlurgich k' zavod-vtuz.
es
(Rqlling (Mpt,alwo

NEFEDOV~ A.A., kand,tekhn.nauk;_CHERNETA, A.P., inzh.; DZIGVASHVILI, G.A.,
insh.; ZASLAVSKIY, G,P., inzh.
Inte'rnal ..'tures in'low'-carbon steel pipe billets. Stall 23
no.5:441- 2 W *163. (MIRA 16:5)
1. Dneprodzerzhinakiy metallurgichaskiy zavod-vtuz i Zakavkazskiy
metallurgioheskiy zavod. I
(Rolling (Metalwork)) (Steel ingots-Defects)

BESEDIN, P.T.; SOROKIN, A.A.; FILONOV, I.G.; KARPUNIN, A.M.;
CHEPELEV, P.M.; SHCHERBINA, P.A.; AVDEYEV, M.G.; KUTSENKO,
A.D.; TSELYUYO, V.I.; CHERNEVICH, Ye.M.; ORGIYAN, V.S.;
CHERNETA, Z.A.
Improving the technology of the heat treatment of rails
at the Dzerzhinskii Plant for the purpose of increasing
their durability in tracks. Stall 24 no.5:445-448 My 164.
(MIRA 17:12)
1. Dneprovskiy metallurgicheskiy zavod im. Dzerzhinskogo i
Ukrainskiy nauchno-issledovateliskiy institut metallov.

KATS, M.E., inzh.; CHERZTENKO, B.N., inzb,
Experimental industrial production of two-layer ceramics. SteU.i
ker. 22 no*10%30-33 0 165. (MIRA 18:12)
1. Kombinat stroitellnykh materialov "Fobedalle

I
COMTRY WO-i
ivrit L
r
t h--i T, I f
I 1z nre
.-N!,skmelort ~W-vi4ards Far~,-l
I.', Z 1 Gui:3' . ia. tr 111'.1- iln-
4
Gjioj~%- jjt~-I~atar,, iurv(,y nii 1-1vi of'-
i2ne-a-". ar,,~ ul--,ganic thlo
- w- I ' T
,;~'vity of 1,110.)tllm 'ea.
~lucoivxodatlr,ns jr Oho
-u e Li
and llotutoe,,~,.

0 D D I - RATS, IM.E.
G 1 i i~E IE; NK,
1,11.fit delays the adopt-lon of the mani"facture of caot fitiirling tiles.
mat. 11 no.5:3 My 165. 0-11"A 18:9)
1. T)irtaktor Leningradskogo komb*a'u!A stroitellrrjkh riatar~.rmlc,,V
"Pobc-dall (for Chernetenko). 2. GlLvny-,f inzhener Leningrad,-kc-C.,
korpbinata stroitellnylch iraterialav "Pobedall (fcr Kats).

DREVICH-SVIRIDYUK, L.S.; OWMICTS, A.N.
Shelterbelto. Put' J putakhoss 4 no.3:44 Mr 160.
(MIR& 13:5)
1. Nachallnik distantali rashchitufth lesomoazhaeay,Brest
(for Drovich-Sviriayuk). 2. Nachallnik proizvocletvannogo uchastka
zaabehitnykh lesonaeazbdeniy.-stantsiy-a Spue-Damansk,
Kalininakoy, dorog-I (for Chernets).
(Windbreaks. shelterbelts. etc.)

ACCMSIDF NRK AP5D,')5 268
AUTHORt Yeru, 1. 1. ; Pesk-matakiy, S.
TITLE: Sr)lri latti~_-e r-e-laxation of Fe_A_ a
stures
MIRCE, Ftzika trer-dogo tela., V. 7, n.,
TOPIC TACS, spi,,~ rebLxation, t
relaxation prob&billity
ABSTRACT., !Tv-,P investigqtion irp made
perature interv&I 1.4--'F. Fit-54 ionI6
they can yleld the necessaxy lata on
sition probabilities, avlnZ to the lax~
vw ure.,i vith thYee crygt&la rrce diff;
I to 10 W. It is concluded frm the
ence of the relaxation nn the field a---- r1', rt 7 1~
theories of spin-lattice relaxation.
ca ~j 1/2
,Q

ACCESSION ni
the spin-lattice relaxatlxi probabilitl'
nd
so that rio other possible me-chanigm o'
ch&ag~- pr.,,rs or po~kets~ '1_vP-C,1tLy axle-
for suppllyllng the r-.vr-tCo amu' nngiiieo,
ASS,&~7 'LATN nst~ --it. e-
Rad,' lcii iturid AN UI.TS-
ca--~,tr= 0C-L.
0 F-FF ISOV
4- I-IMA-
0, "N'114

S/18 b W~/004/003/01 5/04 5
L;~00 BI 02YB11 04
q 0 0
AUT12s: Peskovatskiyj S. A., and Chernets, A .N
TITLE: Spin-lattice relaxation in gadolinium ethyl sulfate
PERIODICAL. Fizika tverdogo tela., v~.*~4, no. 31 1962, 657-664'
TMT: In view of the contradictory results published up to now, the relaxa-
tion processes in gadolinium ethyl sulfate (gee) were studied i- detail.
From theoretical considerations it follows that the observed relaxation
time.will in all cases be greater than the real one by a factor
P = (I-x)/(1-xy); x - 6n/,an01 y = nf/nfol nf . (exp(hV/kT-1))-1; An is the
difference of the spin level population density, 6no is the same for
thermal equilibrium. An estimate showe that in ges with & Gd concentration
of 0.56,,-' and x --:~ 0, the frequency band width of the oscillators is between
70 and 100 Mc/sec, which is far from band overlapping. At 9000 Mc/sec the
peculiarities of the spin-lattice relaxation of gee were studied
experimentally. The measurements were made at helium temperature with
pulse durations of 400-500 9sec and a maximum error of V- It was found
that in general.,the relaxation curves were not exponential. The curves have
Card 1/2

S/18 62/004/003/015/045
Spin-lattice relaxation in B102YB104
not one but two characteristic times T 0.65 and 4-5 msec, and can be
approximated by'
4n 4n, 11 0.5 0XP Hd 675 0.5 OXI)
A special study shows that heating of the lattice oscillators has virtually
no effect on the relaxation rate. En&ineer 0. M. Blagyy and Technician
Yu. G.'Zvegintsev are,thanked for.help. There are 4.figure;, 1 table, and
7 non-Soviet references. The four most recent references to English-
langua~e` -publications read as follows: N. Bloembergen. Phys. Rev. j_01!
2209, 1958il- P- Bowern, W. B. Mime. Phys. Rev. =, 285, 1959; Quantum
Electronics, Columbia University Press, New York' 1960; G. V. Marr, P.,~
Swarup. Canad. Journ.-of-Physical ~_By 4959 1960.
ASSOCIATIONz Inatitut-radiofiziki-i elektroniki AN USSR Khar1kov (Institute
of Radiophysice-and Electronics AS UkrSSR, Xharikov)
J, ~6UBMITTBD: October 27, -'1'961
Card 2/2

- 1 36476
01) S/1 81 /62/004/1003/016/045
B1 17/B 108
AUTHORS: Peskovatskiy, S. A., and Chernets, A. N.
TITLE: Dependence of the'relaxa-tion time in gadolinium ethyl
sulfate on the concentration at helium temporatures
PERIODICAL: Fizika tverdogo tela, v. 4, no. 3, 1962, 665 - 667
TEXT: The authors studied the dependence of the paramagnetic relaxation
time of gadolinium ions in lanthanum ethyl sulfate -(les) on the concentration
of gadolinium ethyl sulfate (ges) and cerium ethyl sulfate (ces) impurities
at liquid-helium temperatures and a frequency of 9000 Mcps by the pulse
method on crystals grown from solutions. In most cases, the relaxat *ion
curves showed a cour5c divergina from the exponential law. This became par-
ticularly evident when the concentration increased, particularly in the
middle of the spectral range. The curves showed a rapid decrease of satura-
tion at the beginning.which became slower toward the end. The rate of
decrease of the fast components of the relaxation curves was independent of
temperature which is indicative of cross relaxation. A change in the ges
concentration from 0-5 to 0.25% slowed down these components which were
Card 1/3

S11 81 /62/004/003/016/45
Dependence of the relaxation ... B117/BlO8
no longer observed at a concentration of 0.1%. The time of spin-lattice
relaxation is inversely proportional to the power 2 + 0.5 of the overall ges
and ces concentration. Cerium impurities (up to 0.27,) had a uniform effect
on all the lines of the electron paramagnetic resonance spectrum if the
difference between'the resonant frequencies of the Gd and Ce lines did not
exceed 300-400 iAcps. The results obtained have not confirmed the hypothesis
of "exchange pockets" (Ref. 1, see below) explaining spin-lattice relaxation
at low temperatures. Conclusions: In spite of their strongly different
magnetic and relaxation properties, Gd3+ and Ce3+ ions have tiie same effect
on the mOB.xetion~rate. The ratio of the relaxation time-- of transitions
m 4---> m + I and m t ~- (m+l) is only slightly influenced by changes in
temperature which lead to a redistribution of the paramagnetic ions. This
behavior is consistent with the assumption of lattice defects due to impuri-
t;~es taking a great part in relaxation. This assumption was treated theo-
retically by B. I. Kochelayev (DAN SSSR, L-1, -1053, 1960). There are 2
figures, 2 tables, and 3 references: 2 Soviet and 1 non'Soviat. The refer-
ence to the English-language publication reads as followsi Ref. 1t Quantum
Electronics, Columbia University Press, Nwe York, 1960,
Card 2/3

S/18 62/004/003/016/045
Dependence of the relaxation ... B117XB108
ASSOCIATIOR: Institut radiofiziki i olektroniki AN USSR, Khar1kov
(Institute of Radiophysics and Electronics AS UkrSSR,
Khar1kov)
SUBMITTED: October 27, 1961
r
Card 3/3

35095
S/185/62/007/001/003/01-'
")209/D302
AUTHO]'S: ",PyesIcovatsIkyyt S.A., Q -4"gts'. A.E., llostohvax~dl, H.I.,
Sheyina, T.H., and Oliynyk, I.El.
TITL:`,: tirowing of lanth-_nnum ethyl sul4late single crystals viit*:i
0
gadolinium- end cerium ethyl sui-fate impurituies and
some of their physical properties
PBRIODICAL: U-Krayinslkyy fizychnyy zhurnall V. 7, 1,0. 1,1962,
22 - 29
T-r,'XT: The method of preparation, growinco., technique and measurement
of the dielectrical constants of lanthantua ethyl-sulfate with Cado-
linium- and cerium eihyl-sulfate impurities, is 6escribed. These Cry
stals are paranagneTic substances by- means of which ultva-hi-h fre-
LD
quencies can be amplified. The salts of the rare-earth elements of
ethylsulfuric acid were prepared by mixing equivalent al:iounts of t1ne
rare-eari;h element sulfate and barium ethylsulfiate in a solution. Tha
single crystals were grown by gradually cooling the saiurated soiu-
tion, over a period of 10 - 12 days; the crystals vrere 15 - 20 ,Im.
Card 1/3

3/165/62/007/001/003/04
Growing of lanthanua,, ethyl sui-fate ... D299/D302
long and 12 - 15 mn tnick. It is important ,o properiy selecT, the
rate of temperature decrease, as at hi-h rates an opaque solution is
formed and the ccystal becomes inhomogeneous. The shape of the cl-y-
stuals depends on the concentration of the solution; t-~us, some of
the crystals viere hexagonal prisms and (with higher gadolinium-ethy-
sulfate concentration) others were hexagonal double-p,,rramids.. The
crystals grown from pure solutions were stable in air and ina va-
cuum, during repeated cooling from room teviperature to t'lat of 11-
quid helium, followed by heating to the original temperature. The
Lelectric constants (permittivity &I and the tangens of the dielec!-
t-irc-loss angle tg 6 = were measured at a freauency f of
9000 11c, over a temperature range of 290 - 4.20K. In--'U-he literaturE!,
no'such data were previously given. The method of measurement was
based on the perturbation of the resonator through introducing- ~niali-
size specimens into its high--f-recraency field. This pernitted neasu----
ing at each temperature point the perturbed and unperturbed values
of the natural frequency and Q-factor of the reson,:~tor by simply mcu-
ving the specimen from the region with maximum 'Lield-strength to
that where the field practically vanishes. The permittivity z' va-
Gard 2/3

S/185/62/007/001/"!03/014
Growing of lanthanum ethyl sllfate ... D2 9 9/ D3 0 2
ried from 3.4 (at, 200 C) to 2.7 (at liquid-hel'Jur ten-peratire):
iaeasux,ement error did not exceed 3 ~;. The
CU-Ave of -tg 6 showed that 'ug o decreas-es -ELj-,Jy
rature, 8-10 2 (at, room temDerature) to 1.5 2-10-3 at 1 i buid-
helium '5emperature). There are 5 figures and 9 refe-rences: 5 So-~-?iet-
u
bloc and 'A non-Soviet-bloc (includins, 1 translation). T1ie re-feren-
ces to the Bnglish-language public~-tions r,~~ad as follov-,,: R.77 -'I-
C, - I ~--' UC
Grass~ B.O. Schulz-DuBoisi 11.2-D. Scovil, Bell Sys-,- T-e--hun., 33,
J
305, 1959; J-H. Sine-er, Ph.D. , "Masers", NeviYor'--, London, ','C'5,-
ASSOCIATION: instytUt radio'Lizy-ky -.-a elektroniky AN U--,"S.R ( In s t i ti ~1 'te
.p ~
of Hadiophysics and Electronics of the AS UlkrRSR)
Kharkiv
SUB',-7ITTED: I-elarch 14, 1961
Card 3,13

33990
S/056/62/042/001/002/048
j4 71 /419 2-) B125/BlOB
AUTHORS: Ganapollskiy, Ye. M., Chernets, A. N.
TITLE; Excitation of hypersound in quartz
PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fiziki, v. 42,
no. 1, 1962, 12 - 15
TEXT: The coaxial resonator with inhomogeneous h.f. electric field (Fig.1)
can simultaneously produce longitudinal and transverse hypersound waves If
10 10 cps. The hypersound was excited in a helium cryostat at 4.20K to
reduce attenuation. The generator produced 0.8psec-pulses, the receiver
had a sensitivity of 5-10- 13 watts, the transmission band was 6 Mcps.
The longitudinal and transverse deformation components, resulting from the
action of the v.h.f. electric field, produce one longitudinal and two LY
coupled transverse waves which propagate in the x-direction of the quartz,
The velocities of these waves agree aside from a measuring error of 5~;,
with the velocities calculated from the elastic constants for quartz.
Liquid helium was supplied by the FTI AN USSR for which B. G,. Lazarev,
Card 1/3

33990
S/056/62/042/001/002/048
Excitation of hypersound in quartz B125/~108
Academician AS UkrSSR, is thanked. There are 3 figures and 5 referencess
1 Soviet and 4 non-Soviet. The four references to English-language publica-
tions read as followss E. H. Jakobsen. Phys, Ilev. Lett,, 2, 249i 1959;
E. H. Jakobsen. Proceedings of the International Conference on ~Juantum
Electronics, September, 1959. Columbia University Prk-,cs, Iflew York, 1960;
H. E. BO"mmel, K. Dransfeld. Phys. Rev., ja, 1245, 1960; i~ E, Borgnis.
Phys. Rev., 98, 1000, 1955-
ASSOCIATIONt Institut radiofiziki i elektroniki Akademii nauk 'Ukrainskoy SSR
(Institute of Radiophysics and Electronics of the Academy of
Sciences Ukrain8kaya SSR)
SUBMITTED: May 27, 1961
Fig. 1 . Resonator.
Legendt (1) Cone, (2)thin diaphragm, (3) quartz, (4) metal screen-,
(5) waveguide, (6) coincident quarter-wave transformer, (7) co=ecting
hole, (A,B) quartz surfaces.
Cakd 2/3

0
Excitation of hypersound in quartz
Figi I
33990
S/056/62/642/00t/:002/048
B125/BIOB
0~
.; L-lem M
Gard 3/3

M KOVATSKIY~ S.A. [Fieskovatolkyi, S.A.]; CHER N Chernets'. A,N,];
POSTOGVARD, G.l.'[Postohyard R.I. ; SHEINA, T.G. Sheina, T.H.1;
OIZYNIK, I.R. [Oliinyk, I.M.1
Growing lanthanum ethyl sulfate single crystals with gadolinium
and cerium ethyl sulfate impurities and their physical
properties. Ukr.fiz.zhur. 7 no.1:22-30 Ja 162. (MIRA 15:11)
1. Inatitilt radiofiziki i Olektroniki AN UkrSSR, Khar1kov.
(Crystalo-Growth)
(Ethanol)

TEXT: The minimum observed value of the imaginary component
of magnetic susceptibility of a paramagnetic sample situated in
the resonator of a radiospectroscope is given by:(J.G. Foher
Bell Syst. Techn.J., 36, 449, 1957):
- 1 'a ""
V --T ( 2P"
0
where y 4PQ Al + P) 2V44) for a reflecting resonator,
P)2V
Y 4PQ V2(10 + 2 for a transmission resonator,
0

A certain type of .... E192/E382
1 2
V* = H 0- H dy , where H is the magnetic field, P is the
V
coupling parameter and Q 0 is the quality factor of the
resonator without load; the other symbols are: T - noise
temperature, A-j - operating bandwidth, P - power of the
signal Itlystron, V s volume of the sampleo V - volume of the
resonator and V~~14 effective volume of the resonator.
_(l). show;s_that-the scns:Ltivity of the spectroscope increases
va th`izicreasing* the -sensitivity-, can -be increased b
y
increasing Q 0 0ii them other hand, can be increased by
concentrating the high-frequency magnetic field in a small
volume. This can be done in coaxial or strip resonators bu-~ in
such systems the effective volume is still comparatively large.
!'his difficulty is overcome in the resonators represented in
Fig. 1, -Where the electromagnetic field is concentr*ated in a
narrow slot fomied by the wide wall of a waveguide in a rect-
qn-lular step inside it. Such a system behaves as a resonator and
can be referred to as a Uslot resonator". It can be iri the form
Card 2/3

_65/666/06VO18/018
Cc rak E192/E382
of a transmission~_reso2x'ai~'Or, as shown in Fig. IS, or a reflection
resonator Ps in Fig. lae The quality factor of such resonators is
100 to 300* This is exproBsed as Q = h/6 , xthere h is the
width of the slot and 6 is the dep?h of the skin-affect layer.
Since such resonators have a comparatively low Qo , .he frequencies
of the signal and local oscillator klystrons do not have to be
particularly stable. Thero are 2 figures and I table.
-aktronikj-.-_AN -USSR-
ON t1tU41~-YaCT: ~-~Jr al
eG
crS!;R)-
suBmrrTED: )iay i9, 3.962
Card 3/3
Bi&. 1:1 -------

PODGAYETSKIY . V. M. ; CHIMNETS,#. A. N.
Spectrophotcaetric study of the
and IFK-2000 pulsed tubes. Opt.
(Electron tubes)
radiation energy distribution in IFK-2000
i spektr. 14 no-3:424-426 Mr t63.
(MLU 16:4)
(SFectrophotometry)

TEXTs Since the.*uBual raethod of produoin8 hypereound, based on the pi.ezo-
effect in thin quartz rods or bars plRced in the electric field of a cavity
resonator, has met with serious difficulties above 2.4-10 10 cps, mainly
arising due to a reduction in dimensions and quality of the resonator, the
hypersound excitation by Blow electromagnctic surface waves is of great
interest. It is very effective and ca-Akea it possible to reach higher fre-
quencies (> 10 10 cps). The present paper gives a theoretics! analysis of
this method. A quartz single crystal 13 placed in the field (frequency w,
-wave number h) so that the coordinate systea, coincides with the crystallo-
graphic directions (X,Y,Z) and x C) forms the surface plane at which the
au du du 3U
boundary condi ions X x + ~V - 2 L:L - 2
t ax )r, , l "X Oy dx r2 2 1 EX ax .2 3 1 FY
are assumed to holds The kinetic equations are solved in first approximatim
1/4

5/020/63/149/001/006/023
Hypervound excitation by slow ... B102/B186
with respect to the small parameterj,,=h/k1 V(')/,e9 the ratio of sonic
a
velocity in the quartz to the propagation rate of the electromagnetic sur-
face wave. The solution reads
u, = u,, P, + 0 OL) P, 4- 0 01) P, + P. PA;
UY - 0 (P) PI + OUGI P2 + PUDI P3 + PARA, 4), where
0 (A P1 + PUOM PS - (LUI)ZP3 + P.A.
P, i = 1, 2, 3; P,
aD + 02
U U , u are the projections of the deformation vector, X Is the
Y iklm
tengor of the elastic moduli, Pl,ik; rl,ik acre the piezoelectric tensors
2 2 '2
(Al,ik Q the density of the quartzi p . h _K, k 0 . C i~6'
nn mn, ik 0
~61v(i)' V(i) is the sonic velocity alol.~; X;
e-velocity of light; k
A
a, PE112)2 4-- (X"~"
The hypersonic 'wave amplitudes are obtD-j.ne~' no
ard
C
2/,j

J
0-
S/020/63/149/0 bbibi~
Hypersound excitation, by slow... B102/Ble6
L"; UOY~Utw alnl+0701 UOS Orma -arm
UGz Till k, a, + Of (6)
and the p-oomponents, are eiven by
PS PP P
P, = P (7).
In the Case of t-0 three types of pure sonic waves are exciteds a longitu-
dinal one (V(1~1 (2), (5)
a ), and tvo crossed transverse ones (V a vB The powers
of these waves are
- i X Ts E3 v(,')S,
W" - -2
MIS
+ P72n I
~40' ) N21ill + + ~1213r) Us 03))
2
Card 3/4 0 zi-9 (L121%A2 - )-1.1.4 + )12134') V1
W- -2.

s/020/63/149/001/008/023
B102/B186
Hypersound excitation by slow...
where 5 is the cross-sectional area of the hypersonic ray. The power ratio
bet,ween the longitudinal wave and the electromagnetic wave is
>' 1W2
In i/w e X11,11 111 2 2 Where Xs is the hypersonic wave length,
71A C
e
e a VVC,.L is the length of the crystal along y. This method was used for
exciting hypersonic waves in a quartz rod at 4.20K. The frequency reached
was 4-10 10 cps and the power ratio agreed with the theoretical one
2
W --,I (R.) . (P-)~C),6
n t1 t2 h h
There are 2 figures.
ASSOCIATIONt Institut radiofiziki i elektroniki Akademii nauk 'K_c_'R (institute
of Radiophysics and Electronics of the Acsdem,~ of
UkrSSR)
PRESEFTFD; September 12t 1962) by N. IN. AyAreyev,
S UB M 1T T/L D t':~epteinber 12, 19oc
L_ Card 4/4

ACCESSION NR: AP4032871 S/0051A/016/004/0674/067 6
O.G.
AUDIOR: Fodgayetskiy, V-14.; Cho
T1921M, : Sane characteristics of a ruby laser with two reflecting prisms
SOURCE: Optika i spolctroskopiya,, v. 16, no. -4,, 1964, 674-676
TOPIC TAGS: larer,- ruby.laser, laser reflector, reflecting prism laser, laser
emission polarization
ABSTRhCT: Recently V. Bernstein, 1-1. and Shu3nan (Proc-IRE,50,1835,i962;
Electronics, No. 9,14,1953) and IN. Bertolotti, L. Musii, and.D. Sette (Nuovo
cimento, 26, 401, 1962) proposed the use of total internal reClection priGms
as the reflectors in lasers and pe3~foracd scme preliminary experiments. How-
ever, the characteristics.of such syctemc are still inadequately imawa. Accord-
in.crly, the present work was devoted to investigation of the lvrfomance of a
ruby ro& laser with two exten-ial triGonal glass prisms in the arrangenent dia-
gramea in Fig. I of the Enclosure, 7he ruby rod (about 0.05ri', Cr203) (3 in the
figure) w;Ls 8.5 = in diameter and~120 mm long; the angle between the geanetric
and optical axes of the rod was Lbout 70* - The distance between the prisma (2)
~Card 1/4

ACCESSIM WH: AP11032871
was about one meter. The results as regards variation in the intenbity ratio
of the beams (indications of the intensity detecting; ,knhotocells) as a function
of the angle of the analyzer are shown in FiG. 2. The ex-parimental data intUcate
that in the case of reflection fran the side of the crystal (Fig. 2ya) the main
part of the radiation has virtually plane polarization, whereas in the case of
reflection fr'a-4i the side of the prism 21b) the polarization of ~he main
Part of Vhe radiation is ncar4 circular. A posdible explanation is suggested.
The laser output varies with rotation of the ruby rod about its gecmetric axis.
The investigated laser set-up with the pump' power 10 to 30,ja above threshold
yielded a radiation line width of 0.1-0.2 cm and a divergence angle of 10 to
30 min. Origs art. has: 2 figures.
ASSOCIATIOM ncne
SMMTTM: O~J=63
NO REP SOV4. 001
Card 2A,
ENCL: 02 SUB CCDE: OP
OTW 003

ACCLWION NRt Ap4032ap. ENGLOSUREs. 01
Via. I, Experbnental laser set-up.
Pard 3/4
I - Pwition of plate for measure-
ments in the right axm of the system;
1.1 - position ot plate for measure-
ments in the lef"t am.

ENCLOSURE%
A00FISSIM M Ap4o32871 02
CL
Fig. 2. Variation of the intensity
ratio of the beams a3 a functim of
the analyzer anGle:
a - plate (FiG.1) reflecting frcm
W. W- v- the side of the prism; b -~plate 4
1.00- A reflecting from the side of the
crystal; 1 - main part of the emis-
0.15. ars sion 1 2 - part of the eMiGoion having
a polarization different from Thai of
040- the main-part.
W
-Its
-89 Ir -4r V 0 4r W 80,
Card 4/4

GANAPOLISKIYP Ye.M.; CHERIIETS, A.N.
-- ----- e- -
Resonance absorption of hypersound of frequency 1010 cps
in ruby. Zhur. eksp. i teor. fiz. 47 no-5:1677-1682 N 164.
(MIRA 18:2)
1. Institut radiofiziki i elektroniki AN UkrSSR.

YMU, LI.; PESKI'VATSM, S.A.; ~',HERNETS A.N.
zpin."Iattine relaxatinn of Ft,3r ions in natural andalusita at low
temperatures, Fly,. tver. tcla 7 nD.2:363-366 F 165.
(MIRA 1818)
1. Institut radioftzlki i. eaektruniki A' UkrS~'-R., n2arlkcv.

L :L5982 66. EEC (k)-2/V.VA(h)/EWP(k)/.EWT (1)/E'kVT(m)/FBD/T/VJP(e) SCIT-33/1JP(c)
ACC NR: Ap6oo4415 WG/10 SOURCE CODE: UR/0051/66/0'20/001/0138/0142
AUTHOR: Podgayetskiy, V. M.; Korneyeva, 0. G.; Che~e~ ~,A_
ORG: none
TITLE: The angular distribution of the ager radiation ener
'SOURCE: Optika i spektroskopiya, v. 20, no. 1, 1966, 138-142
TOPIC TAGS: angular distribution, ruby laser, laser energy, laser beam
ABSTRACT: The authors measured the angular distribution of the radiation energy
in a ruby laser with several types of resonators with external reflectors (either
two plane mirrors with 20% and 2% transmission or two 900 total-internal-reflection
prisms with various orientations relative to the electric vector). A rose-ruby_j,,,
~crystal rod 45 mm.long and 6 mm in diameter was used, the optical and geomit-ric
axes being at an '820 angle. The pumping was dmelcyWo IFK-2000 lamps, placed
~against the-rod and the forced air-was used for cooling. The setup used for the
:plane mirrors is shown in Fig. 1, and that used for the prisms was described by
-,the authors elsewhere (Opt. i spek1r. v. 16, 6741 -1964). rhe angular distribution
iwas measured by a standard photometric techniques. The widths of the directivity
Card 1/3
UDC; 62.1-375-9:535

7
~. I ~.Card 2/3 ..- - - I . - - --.. - - -- ~. . . I ~ .- - I I .

L 15982-66
ACC NR: Ap6ooh415
.patterns at half-intensity level in the E and H planes varied very liitid~-Jith
the type of resonator or with the operating mode of the laser (from 2.5 to 7 min-
utes of angle). A difference was observed, however', in the nature of the dis-
tribution of the intensity when mirrors and prisms were used as reflectors. When
prisms with parallel right-oxgle edges are used, the photographs show an inter-
:ference-fringe structure which depends on the laser operating mode. Orig. art.
has: 4 figures, 4 formulas, and 1 table. [021
SUB CODE: 20/ SUBM DATE: 2IOct64/ ORIG REF: 0031 OTH REF: 005/ ATD PRESS:
2,
~Card 3/3

70-66 EVIT (1)/EIVT (m)/EVIP (k)/T/MP(e)/E1VP (w) IJP(c) "AM
NR_-_AP603l43O SOURCE CODE: UR/0056/66/051/002/0383/0393
AUTHOR. GanaRol'skiy. Ye. M ; Chernatil N_ (3
ORG; Institute of Radiophysics and Electronics. Academy of Sci
(Institut radofiziki i elektroniki Akademii nauk UkrainsRoy SSR
TITLE: Hypersound absorption in quart nd rystals
SOURCE: Zh eksper i teor fiz* v. 51, no. 2, 1966, 383-393
Ukrainian SSR
TOPIC TAGS: hypersound, hypersound absorptioq quartz crystal. ruby crystal.
hypersonic wave
ABSTRACT: The frequency-temperature dependences f absorption coefficients of a
longitudinal and two transverse hyperso - 11
1, irected along the binary x-axis of
a quartz crystal have been measured at temperatures between 10 and 300F, at a frequen,
of 109-cps and between 10 and 40K at frequencies of 9.4-109 and 4-1010 cps. Absorp-
tion of a longitudinal hypersonic wave was measured along the trigonal. Z-axis of
quartz and ruby at frequencies of 109 and 9.4-109 cps. It was found that three-phoni
scattering of longitudinal and transverse external bypersonic phonons on correspondt
longitudinal and transverse thermal phonons, are responsible for hypersound absorptii
at low temperatures. This process can be used in explaining the fan-shaped frequenc:
temperature variation of the hypersound absorption coefficient. Orig. art. has:
10 formulas, 4 figures, and I table. ICS]
SUB CODE: 20/ SUIM DATE: 25Feb66/ ORIG REF: 004/ OTR REF; 014/ ATD PRESS:
:ard I/, hS 5083

24(0); 5(4); 6(2) rWE I BOOK EXPLOITATION 307/2215
Vsenoyuznyy nauchno-lealedovatellakly inatitut metrologii Imeni
. D.1. Mendeloyeva .
Reforaty nauchno-ineledovatollaklkh robot; abornik No.2 (Sclent-Irld
Research Abstracts; Collection of Articles, Xr 2) Moscow.
3tandartgiz, 1958. 139 p. 1,000 copies printed.
Additional Sponsoring Agencyt USSR. Koaltot standArtav, mer I
izmaritellnykh priborov.
Zd.s 3. V. Reshotina; Tech. Fd.t M. A. Kond:ratlyev&.
PURPOSEs These reports are Intended for scientists, researchers,
and engineers engaged in developing standards# seaSurta, and
gages for the various Industries.
COVERAGEt The volume contains 128 reports on otaM&rds of measure-
ment and control. The reports were prepared by scientists of
Institutes of the Koositet standartov, ner I lZoneritolInykh
prIborov pri Sovete Ministrov SSSR (Comodsolon on Standardap
Measures, and Measuring Instruments under the USSR Council of
Ministers). The participating Instltutez aret VVIIN -
Voonoyuznyy nauchno-inaledovatal-skly metroloat Intent D.I.
Mendeleyeva (All-Union Scientific Research Inazitule of met-
rology Imeni D.I.-Mandeleycv) In Uningrad; Sverdlovsk branch
f this Institute; VNIIX - Voenoyuznyy nauchno-IssledoTatellskly
~.tltut Komiteta otand&rtov, ser 1 Lzmeriteltr3ykh prLoorev
Z
(All-Union Scientific Research Institute of the Commission
an Standards, Xemsurea~ and Measuring instruments), created
from M0IMZP - Moskovskly go3udarstvannyy 1notitut nor I
i=eritellnykh prlboroy (Moscow State Institute of Measures
and Measuring Instruments) October 1, 1,955; VNIIPTRI -
Vaesoyuznyy nauchno-laBledovatellakiy Institut flzlko-takhni-
chask.tkh I radlotakhnIcho5kikh L=ereniy (All-UnIon Scientirle
Research Institute of Physicotechnlcal and Radlo-onglneering
Measurements) in Moscow, KhOIMIP 7 Kh&r'k0vck1y gosuda"tvennyy
institut mer I I=eriteltnykh pr1borov (Khartkoy State Institute
of Measures and Measuring Instruments); and XGZMIP - Hovosi-
birskiy gosudarstvenry Institut mer I icneritellrykh prlborov
(Novosibirsk State Inatitute or Measures and Measuring Xnatru-
s~eLitq). No personalities are mentioned. There are no references.
00;=!gfonand A 5 3
It
ru IQ a 0JrAR-b1_n'gn2sY_ooVf1nffr (Nl'vezPr0m)- Studying the Reason&
Scales
Mark9-L-A-and S N 26
WoRd for Chao , __ . C
e!:9
h n:rt6~(Kh"M1p)- Developing a Simplified
XG VNIIM IX to Used In Analysis 2S
in 'Z~uhd a' IThermostatic Apparatus for Metrological
nd 301 d Density M ... urazents
'Time and 29
.dldAtO Or Vrequency Measurements (T"ch1iPr0chko, 3.3., FALtor. Can
Tochn1dal Spionoeaj Tkhorzhavskly, O.A., Candidate or
Tochvio&l Solonaeli)
Toych
C1661'51 ~-theg-ta~jcn(P,','.Mn; Studying A.,tr,,n .. Ic,l Pendulum
Thai,,- Dally not. and Reducing the Varlatlons prom
to 4 0-003 Seconds
-aQlQX-'--_Z A 32
. _ __ (VNIIM). Temperature Studios of Astronomical
Pendulum Clocks or the AChH Type
Card 7/27 33
0

%
LITVININKO, L.M.; POLYAKOV. V.P.; GREKOV, A.P.; CHERNBMAYA.A.M.
Analysis of aminoantipyrine in t8Bting aminopyrine production.
Med.pro*. 11 no.1:46-4B Ja 157. (MLRA 10:2)
1. Kafedra organicheakoy khimii kharlkovskogo univerviteta imeni
A.M.Gorlkogo i TSentrallnaya laboratoriya Eharlkovskogo khimiko-
farmatoevticheakogo savoda mKrasnaya zvezdam
(PYWIDOM) (ANT IPYRIW

USSR /Analytical Chemistry. E-3
ill Analysis of Organic Substances.
Abs Jour: Ref. Zhur - Khimiya No. 2, 1958, 4358
Author Litvinenko, L.M., Polakov, V.P., Grekov, A,P.,
,Czernetska
Title Analysis of the Chloranhydride of Acetylsalicylic
Acid.
Orig Pub: Med. prom-st SSSR,, 1957,,\No. 4, 42-43
Abstract: The method consists of the mixing of the chlor-
anhydride of acetylsalicylic acid solution (1) in
78 with a benzene solution of C6H5NH2; the amount
0 6H NH exce Ieds by- 3 times (in a mol. ratio)
that oP (i). The excess of C611c5NH2 is backtitrated
potentiometrically with a solut"'on of NaN02 using
a Pt indicator electrode. The presence of the
N-phenylamide of acetylsalicylic acid in the mix-
C ard lp2

CHMETSKAYA, M.
~ .
400 1.. ork of oar geographical group. Geog. v shkole 21 no. 4:61
Jl-Ag '58. (MIRA 11:7)
1. Shkols Ilo. 2 g. Razanke.
(Geography--Study and teaching)

KORS&KOVA, A.S.; CIMRNETSKAYA, S.G.
.1al-W
Duration of excretion of dysentery bacteriophage in children in
preventive administration of the phage. Zhur.nikrobiol.epid.i
immun. no.2:70 F '54. (MIRA 7:3)
1. Iz Instituta apidemiologii i mikrobiologii im. Gamalei Akademii
meditsinakikh nauk SSSR. (Dysentery) (Bacteriophage)

C!rMMSKAYA,-U,---
MM - -
See the now. SOT.foto 17 no.5:28 Mv. 157. (MIRA 1e: 7)
(Photoigra,ohy, Journalistic)

C I iLll i 4-1 T,3,,:AYA p Z . .~ .
511.iycoflora of the Forests of North Ossetia and Their Phytopatholooi-c-rd
Condition," DnevnEI.Vgcsoiuzno.,,,o Slgzda- 3otanikov, 1923, pp. 13~-lZc). (31.11.i.
Translation 2135)
30: SIRA, SI 90-~3, 15 December 1953

CHERIZ MUYA., ::. .3.
"The Fun,;?us Diplodia pinea (Desm.) Y~irks as a Dan,lerous Parasite on Pine,"
- j I
C :p. 24-23 464-:~! R r2xv~
I-Aterialy r,o Eikolo.--~ii i Fitopatolo~:U, vol. 5, no. 2, 192', 1
60: jUlk, 61 90-53, 15 Doccraber 1953

CHMMETSKArA, Z. S.
CHERMMAIA, Z. S. "Diseases of Maize," Nauchpye Trudy Gol:slcQi Zonaltnoi
KI&uruzm-Soevo-Kartofellnoi C?Dytnoi Stantsii Seriia 1, no. 4, 1932, pp. 6-78.
106 G682.
SO: SIRA - SI - 90 - 53t 15 Dec. 1953o

Name: CHWJIRTSKIr., A. 1.
Dissertation: Main problems in the cultivation of buckwheat in
northern steppe districts of the Ukraine east of the
Dnieper
Degree: Cand Agr Sci
~ Min Agriculture USSR, Belaya Tserkov' Agricultural Inat
Defense Date, Place: 1956, Belaya Tserkov'
Source: Knizbnaya letopis', Wo 2, 1957

Auth6r-s
h9o 7z;eded Dltcharo in a Magnetic Field Za He Reikhrudel
U4080RO for a Special Configurifl-C-n-O-f%'Tw- Ig V* Vasileva
Disobarge Gap I A. V. CbernetskW,
2h. Te3ch. pis., Vol 22, 17o..12, 2. M. RIO-=ME
pq 2954--,1966, 1952
Scuroev Index Jk9r*=ut1a=jq Vol 11, No* 12, December, 1955, p 111~e'

.) . I ~ -
RZTKHRUI13L',.B.X.,; GHKRNNMKIT, A.Y.; XIMMVIOH, V.V.; VASIL'YEVA, I.A.
Mechanism of discharge in a magnetic ionized manometer. Vest.Mook.un. 8
no.8;87-100 Ag '53. (MIU 6:11)
1. Fisicheekly fakulltet.
(Sleatric discharges through gases) (Manometer)

a! e
1 14.
tam.
-r- ~,"Tn ut higb inteawy (up
us~ of tmj,A~ it-eding mtsu the maic -t~,
A ; ~!q , r 1~ -.~ --'Illtl"l L, tV.1t ncr~sswy' ll;ilr
'~d I
."t-f
"fg oau
.c tl~ Qd M.'i
I ~-~wt:'p to u,- . - t~
i fS) The magrict,,
thu, t~,ajq 11),
catW anil, ilit W1, ',I)t ) c4 01~ t-lnt
meat 0 lQw 1'-dylfl

A V FD-67i
USSR/Nuclear Physics - Ion sources
Card 1/1 : pub. 129 - 6/25
Author : Reykbrudel', E. M.; and Chernetskiy, A. V.
Title : Certain characteristics of a gas discharge source of ions
Periodical : Vest. Mosk. un., Ser. fizikomat. i yest. nauk, Vol. 9, No S1_
47-54, May 1954
Abstract : The authors describe a gas-discharge ion source in which the ions
are obtained from a low-pressure impeded glow discharge under
the action of an axially symmetric electric field, and in which
use is made of a gap having a particular shape that brings about
electron oscillations and hence effective ionization of the gas.
The ions are emitted through an aperture in the cathode and are
already directional in the discharge. The characteristics of
the ion current as a function of the various parameters and the
role of the electron-optical system are investigated. Refer to
A. Guthrie and W. Wakerling's "Characteristic of electrical
discharges in magnetic fields," Nat. Nuclear Energy Ser., 5,
1949
Institution : Chair of Electron Cptics
Submitted : July 11, 1952

A
(71,1el9AJ ~'t~3
AUTHORS: Vozneaen*aXiyjV-1-p Korotkikh, N.V., 53-4-9/1o
Chernetskiy, A-V., Koporskiy A.S.
Recording
TITLE: Oscillographical Tubes for/Rapidly Occurring Processes (Ostsil-
lograficheskiye trubki dlya zapisi bystroprotekayushchikh pro-
tsessov)
PERIODICAL: Uspekhi Fiz. Nauk, 1957, Vol. 62, Nr 4, PP. 497-522 (USSR)
ABSTRACT: The present survey comprises the last decade; it comprises the
main methods of oscillographics of processes taking place rapid-
ly and also some characteristic problems on rapidly acting elec-
tron-beam tubes (for instance for the production of a thin elec-
tron-beam post-acceleration.,etc.). The survey is arranged as fol-
lows; 1: The methods of velocity oscillo.-raphy. The deflecting
systems, the limitations of the usual deflecting systems for high
frequency. 2: The electron beam tubes with deflecting system in
form of a line with two conductions. 3: The electron beam tubes
for the investigation of phenomena taking place rapidly with high
efficiency. 4: Microoscillographical tubes- 5: Tubes with a re-
flecting system for a travelling wave. 6: The investigation of
the ultrashort electronic blobs. 7: The diameter of the spot. 8:
The velocity of registration. 91 The dependence of brightness on
Card 1/2 current density and on the accelerati6.d voltage. lo: The constrast.

Oscillographical Tubes for Rep6rdingRapidly Occuriing Frocessea 53-4-9/10
11: Photography. Summarized survey; Up to now the width of the
band of the frequencies to be investigated was increased to loooo
megacycles. Tubes with such a_band permit the investigation of
processes of a duration of lo 9 see. Most of the tubes have a
goud resolving power. The signal to be resolved must have at least
1 V. The registration velocity of 1010 cm/sec obtained for some
tubes is in fact a realizable value for serial devices. Frequency
distortions in deflecting systems, however, hitherto prevented
the sufficiently accurate investigation of those transition pro-
cesses the spectra of which exceeded looo megacycles. At present
oscillographical tubes are needed by means pf-which transition
processes of a duration of from 10-9 to 5A0--Lsec and with ampli-
tudes of some tenths of a volt can be investigated. Accordinglyj
improvements of the frequency characteristic of the deviations
and the resolving power of the oscillographic tubes has to be
aimed at when developing new tubes. There are 19 figures, 3 tab-
les and 55 references, 13 of which are Slavic.
AYAILA13LE.- Library of Congress
Card 2/2

tj E TS K, ~ 4. V
AUTHORS: Chernetskiy. A. V., Korotkikh, N. V., 53-4-6111
KonorsIdy, A. S..
.
Voznesenskiy., V.-T.
TITLE" The Electronic Methods of the Production of Ultrashort Pulses
(Elektronnyya metody generatsii sverkhkorotkikh Impullsov)e
PERIODICAL** Uspekhi Fizicheskikh Nauk, 1957, Vol. 63, Nr 4, pp. 801-812 (USSR).
ABSTRACT.,, The present survey is arranged as follows: Introduction., the pro-
blems occurring in connection with the production of pulses by
electronic methods (destruction of a "packet"*,excitation of the
output device), the pulse generator of the klystron type, a tube
with transversal deflection of the beam as generator for very
short pulses, the combined generator, a pulse generator with magm
netic deceleration; summary: The electron generators have a good
future. Their main advantages are simplicity, stable operation,
the possibility of producing very short pulses in a wide range of
frequency* The fact that a present these devices are only rarely
used may be explained by the novelty of the methods of electronic
pulse production. They are still not known to a wide circle of
specialists. Besides, the generators used at present are mostly
of low efficiency and their applicability is limited. However
,
Card 1/2 .
the development of the methods discussed here as well as of that

The Electronic Methods of the Production of Ultrashort Pulses. 53-4-6/11
of methods still to come opens up,new possibilities for pulse
technics.
There are 7 figures, 1 table, and 9 references# 3 of which are
Slavic.
AVAILABLE: Library of Congress,
Card 2/2

I
CU,METSKIY,, A.V. _kard.- fiz.-mat. nauk., red.; LMIIZE, L.G., insh.,
AVDRETMKO, Z.D., red.; VLASOVA, W.A., tekhn. red.
[Some problems of physical experimental technique in studying
gas discharges] Nekotorye voprosy tekbnik-i fizicheskogo eksperi-
ments. pri issledovanii gazovogo razriada; nauchno-tekhnicheskii
sbornik, Moskvaj Gosatomizdate RoO. 1961. 120 (MPIRA 1515)
(Electric discharges thropgh gases)

S/i25/61/000/003/0011/008
AUTHORS: A-P-~ Zinov'yev, O.A , Cherne-tskiv, A.V
T IT LE: ii~i,_rnwave method.-j for the a-easti-en"Ont oi electron, concclitra-
on ;1~a~;Llla.
SOURCE: Nckoto) Y%;!-, ~,,q;_rosy tekhmki iiz;. 3!~(~go eksj:-erinienla pri ..ssledovan";
~?,a Z OV Og C, Z' Va da; nauc hno -i y s bo rn it-_ n o. 3. A. V . C h er -
neLskiy C-:: L.,G. Lornize, eds. Mosc,,-~;, Ciosatomizdat, 1961, 3-30.
TEXT: This is a state - of - Lhe- -art report on 'lit of microwave methods for
the x-r-easurerrient of varl,)~-, -. parameters (elect-z-,A1 temperature, c fli~i7,--
en i? r g ylosses, etc.) ot' tlx~~ plas-cria, of a gaseous dischar~)e without introducing i.`-
6itional clectrojx~; an-3, hon~:c, perturbations into the. plzisn-ia. The primary ob,iect-
ive of this paper is t.!,(. detern-iiniition by nwans of (1) micro-
,Y.!ave t ri-ris illurn i nation, and (11) by interferoryieLry. Macroscopic Maxwellian theory
of electromagnetic waves in an ionized gas is expounded in conformity with Al'pert,
Ya. L., Gir]-ZlAlrg, V. L., Feynbc-1--? Ye. L. Rasprotitran-niye radiovoln (RaO'oY--,jv&
propagatiori). Moscow. Gosticldhi~-dat, t953. In the rc..;u1iing equition for the pru-
pagation of' ;i normally in- iden.' plaiie olectrun,agnetic the dependence of the
glo'bal -_puk.:ifi(_ .~,rln or the projwf-tivs of the plasl~na renlains
C;k rd 1 /3

Some inicrowave nie-thods ~5/7.~'.---,1611'000/003/001/008
to be explored. This i,,i in term-,; ,-.1 the rati,_i between the in-plasma
wavellength and thi, wiivclr~ngtil, 1) and of the absorption inclex, -y . The
effect of elf, C-Xru _iii ionized gas, Whit-- ki Cause s the
electrons ;o thf~ i -1 n ,! k~ct wave to foiloxv curvilinear
trajeLLO-rlc~l the -A the Lorent... 1'.1rcu, is investigated, and it is con-
cluded that the _,;r;E~c:f4C capacitance ..' in ioniLed gas is linearly dependent
on the electron density 'iWz presence a:iil in the absence oi an e.-,-ternal mag-
netic field. A ,ujn~ria Cl.,tioi~ oi the metho_-i js
given with ~o v.--..A:.: :-_, 'Ool~~oy-'Savelyev, G.G., ZhETF, v.38. n-).

1~,&O, 39-1,
1 on -it,~ Pe,
aceful Uses of Atomic EnercFN
SoN -t papc--- 7
;I, IWb8WI!_1, !~A~_,scow. Atornizdat, 1959, 8~;;
Vvt- ~onov, f~, r%-~a~_ ' I Co-f . p. 1,13; Harding et al., ibid.,
foreign 3. 1. T.r~r p n, n ne -n. onzz c) e a r r ea Cti On S , P.
also ct S -72 5 ~6 1
1 'Abst_ - I

003 /002 _!OM~) T In nri r ) () er ra 0 s
rtaias r i lie ele ct c n c nc a L" n i-
Srnal':el" 0.''1 ..~I
-,!) the w,.~Lvt; 13,Y the t*.-.--iti~:;!',.t,,.-iii,,,a~~ic)ii
.
device) ci g ~,cLnce ceases b!~cause the refraction index and
.
and the :_-,!r0) than the criticall coric ent ration, but does
n6t indicate it~, 1~:_J~S- T-lar&nq inultiple -frequency method is not
viewed as advI--,I-. tmultaneous us,,- of several microwave
Card Z/3

S0111t. MiCrOwavt~ Inothods ... S/71.nl/h 1 /000/003/001
generators appears tw-diffictilt an Lo.OC practicable. Tht.,
of the adaptation of -neth-_),ds previoui;ly useu in opz~cs to th,.~ dett--rmination 01
microwave- propagation characteristic~i b,'.. -.71d .-kniplitude comparison is
briefly reviewed and major attention is f-cused on the microwave Interferollieter
described by Wharton, C.B., &, Slager.. D,*M., ir, IRE Trans.Nuci.Sci., v.NS-6,
no.3, 1959, 20, and in J.Appl.Phys., v.31, nc-!, 1960, 428. This systeni, which
comprises a ineastiring and a refe"el-1U., channel, serves well with relatively ~-it:ak
discharges in a gas, but is iiicrvasingly affected by noise'at greater disk.h~,Lrvge in-
tensities. The devIce proposed by Dropkin,H.A., IRENat.-Gonv.Rec-, v.b, r10. 1,
1958, 57, which employs a frequency shifter, is described and terrrLed more! nois~-
proof and more accurate. 'rhe inadequate tirne-resolving power of this devic_,2 is
said to be overcome by the employment of auper-HF generato,.-S as propose-d
by Thompson, M.G., &. Vetter,M.J.-, 1",ev,Scient.histrurn., %!.29, no.Z, 195'~' 1.1i"
which is described in detail, and operational p-k-,~edureS speCif-led by Wharton,
Howard, et al., in the Trans. Zd Internatl Gonf. aLc. , 1959, 67 5, are reported.
There are I I figures and 23 references ( U, ~ viet, 7 Engli sh- language, and 9
English-language papers in their Russian 'ri
ASSC-CIA"I Nione
Card 3 /3

-7
S/725/61/0001!003/003/008
AUTHORS: Voznesenskiy, V.I., Chernetskiy, A. V., Sere~,riyskiy, I. N.
TITLE: The blurring of electron clusters due to Coulomb forces under the c(-,2;,-
pensating effect of an initial velocity modulation.
SOURCE: Nekotoryye voprosy tekhniki fizicheskogo eksperimenta pri issledovanii
gazovogo razryada; nauchno-telrhnicheskiy sbornik, no. 3. A. V.
Chernetskiy & L.G.Lomize, eds. Moscow, Gosatornizdzit, 1961, 53-59.
TEXT: This theoretical analysis of the changes occurring in short freely-
moving electron clusters - whether monochromatic or initially velocity- scattered -
is of value in the generation of electron clusters for the creation of ultra-short
(10-9 to 10- 12 sec) pulse voltages with gr eat iteration frequency, attaining hundreds
of mcps, which is useful in the generation of 'electromagnetic waves, in accelerator
design, etc. It is important to know how rapidly the electron clusters will blur
under the effect of their own space charge and to try to find a method for their
conservation over a relatively long distance. Short-wave generation by means of
the Vavilov-Cherenkov effect and transient or bremsstrahlen radiation (for non-
relativistic beams) can produce a noticeable effect only if this problem is overcome.
The Coulomb- force- produc ed blurring of electron clusters was investigated by
Card 1/3

The blurring of electron clusters ... S/725/61/0001'003/0031008
GA. Zhi I eyl~,, (ZhT F, -~ 31, no.4, 1961, 508) for spherically shaped clusters, and
the repulsive'lurces %4'cre found to be dxcleedingly significant for small cluster
sizes. The present study examines the blurring of cylindrically- shaped clusters;
in this case the repulsivo forces are found to be not overly great and are, in any
event, finite even for infinitely small longitudinal cluster dimensions (for a given
transverse size). The change of the spatial density of the cluster in the course of
its motion is accounted for approximately. It is shown that the shape of a cluster
may be regarded as invariable, so long as the longitudinal cluster diniension is
considerably smaller than the transverse dimensions. For short cluster "durations"
(ratios of the longitudinal dimension by its mean velocity), 10- 11 to 10- 12 sec. this
requirement is satisfied (e. g., if v= 5- 109 cm/sec, the cluster length is 5 - 10-2 to
5 - 10-3cm with a diameter of a few mm). The influence of the metallic or dielect-
ric walls is disregarded. This is justified for most practical applications, namely,
in linear accelerators, electronic ultra-short pulse generators, etc., where the
tube diameter is fairly large. The calculation comprises the determination of the
longitudinal size of a cluster as a function of the space-charge density (assumed to
be uniformly distributed over the cluster), the time, and the magnitude of the initial
velocity scatter; the radial spread is assumed to be counteracted by a magnetic
field. Cylindrical coordinates art: used, with the origin at the center of the cluster.
The calculation (and grapluc representatio,i) of the timewise chan 'ge of the longitudi-
nal dimensions of th.- cluster shows that, when the initial relative velocity is
Card 2/3

The b!urein~, of clearon clusters ... S/7Z5/611 '000/00.i/00" /00b
nonzero, the cluster initially shrinks to a certain inirilinal length anci then hef-"!~ to
blur out. Thiti approximate calculation shows that Fi cyl-indric-a' -f
cally very sniall dimensions is, in principle, achievable, since the replllsi"rt~ fc-l-ce
rernains finite. A comparison of the caseii in -swhich the initial relative velo-ity is
zero and no-azero, ri~Fpectively, shows that an initial velocity Modulation !7
lengthen the distance ovr-r which the cluster is conserved. There are 2 fligur-~-s --iriG
6 references~ including 3 recent Soviet references (Koporskiy, A.S., et al., Us~-~.
fiz. nauk, 1957, 601; Zhileyko,G.I., Cand. Diss., Iri-t Radioelektr., AN SSSR.
1959, and ZhTF, v.31, no.4, 1961, 508) and 3 earlier English- language refe-~-Ciices
(Enslein, Rev. Sci. Instrum., v.Z5, 1954, 574; Hastid, D., Phis. (sic!) Soc., 'Proc
V.00? 1948, 340; and Grant, R., et al., J. Appl. Phys., v.25, 1954, 574).
ASSOCIATION; None given.
C-ard 3 /3

h2h55
S/7Z5/63 /000 ;W-)`
AUTHOR: Ghernetskiy,,A, V,
TITL.E: The high-voltage pillse regime of a Penning-type 1-wi sourct!.
SOURCE: vopro-,y tekhrtiki fizicheskogo P";
~11~JZ 10" Og,~) iazi-yada; nauchno-tekhnicheskiy sbornii-, no-5. A.V.Cht~r-
ni-t~ikiv & -",.G.Lornize, eds. Moscow. Gos-,itom,zdat, 1961, 1-05-;~"
T;. --the-art report, accompanttad hy exporiniental
T f Is a Mate of
On it) the development Of PUlSe-tyjW iOll SOUI-CCS. WiliCh a"
pfAu,-iLi'-',7Z value in thermonuclear devices and accelerators. An-lon ther essentl
'koi as yet fulfilled is an irnpulse ion source easy nianufacture
endl~w-d with (i~~siral (e operating characteristics. Much promise. is st~cn in tht'.
lligh-v'-Atange palse-fed "Penning tube" (Penning, F., Physica, vA, 1937, 1190)
was first t(-.sted by R. Keller (HeIv.Phys.Acta, v. ~"'. j?49. -((3; v. Z3, 1950,
T[w nias~ylitm,i imi cori t~jits achieved were Z2 Illa. ITI 19~2 Ow present author
atta i ne,d ion curre~its of 130 ma at a pressure of 10--~turr (nini Hg) and 0. 5 a at
9 10-` torr, vvitn a pull-ie duration of a few (appx. 5) fnici-csec and a repetition ratu
i" 50 cps. CqllipTnent c-f R..N.Aeyer~rid and S.Brtj%vr~
The more recent experimental I
v.30, 1959, 2) is criticized as incapablt~ of producing ion
currenti:. grf,p_tcr than 20 to 30 ma and of operating at pressures below 10-3
Card I I'll

T~f! lilgh-voltage pull,,e rf--girne of a Penning-type. 5/17Z5/61/000/00311007/00~,'
The d0l.thOT ' S 195Z equipment is described in detail, including the rnanufacture of tht-
Pczining tube (anode wire ring, two cathodes, all electrodes made of HF-dcaassed
rnolybcl(muni, the tube itself of molybdenurn glass oven- annt.-aled at 4000C) and the
accessorle,s Gin ion-beam focusing lens electrode, the extornal rnagnetic.-fieid coi"'
and a pulse oscilloscope used for measurement. The physical phenon-iena occurring
durin,2 the discharges within the Penning tube are des'crii)cd (cf. Reykhrudel' , E. M.
et al., ZhTF, v. 12, no. 12, 1952; Smirnitskaya, G. V ., et 'Al., ZhTF, v. 29, no. 2.
19-59), includii)g the Jon - flow- aug menting effect of ;.~ pulhng fieW and tht~ beneficial
effect of an e~'-ternal magnetic field. High-voltage pLikst: op(-3-tion was performed
without application of a pulling field, since the ions .vere being accelerated sufficient-
ly by the cathode poti_nttial drop of the discharge. lon-currvrit vs. pre9sure graphs
show a sharp, current increase at higher pressures, tbiil, ,.tvt-n at pressurt-s-
(10-1 to 10- torr) appreciable ion currents %vt-re at'ani~t(J with a tubt- voltagi-I of 6
(rnagnetic "ield stIrf.-rigth: 570 oe). The Penning tube, Operatco in a hici- vo!Lag-_-
PLI15C reg.-'rnel as regardud as one of the mo!A effectivp. ~~Jd vet sim"Plest. io" sourc~_~_.
The reasoli~.. are as follows: (1) The high ene!:~,v J -rie electrons and their effcc--jv~_
confinernent, iii the discharge space yields an inLtnse of the gas wlucri is
hv secondary processes, such as 'he of electrc'ns in ti-e
space and knoclking-out of electron8 froni Hitt s~,rfac.(!-' (, -ation t)f
Z) loc
the r-iost ation near the cathode.~; fZj(:jj.I,;kft- fGj'tj.jjji()jj;
Card 2/3

The high-voltage pulse regime of a Penning-type. S""74'5/61 /G00/003 /007/008
(3) high- anode -voltage operations yield adequate flux at low ressur :--n-4
p e
to 10-5
torr) without differential pumping; (4) at higher pressures (110- to 10 _torr)
appreciable currents (up to 0. 5 a) are achieved inore easily and in":xPk~11si".e1v tIL3-;;,
for example, with arc sources; the construction of he Pennirig-tzbc~ de%,ice is
practicable for any average laboratory; (5) tht'. Ievi f, 1'."' Suitable for 10119-tern)
stable operation; (6) according to the Meycrilid Pi-,- p_ipei- th- Peiming pulse
sources yield up to ;507o more atomic ions.
(3 Soviet and 5 English- language).
ASSOCIATION: None given.
Card 3/3

ACCESSION URI AT4025310' 8/0000/63/000/000/0199/0211.'
AUTHORSs Kozlove 0. V.1 Rodin, A. M.r Rusanov, V. D.# 8kablor We
Aq Chernetskiye A. V.
TITLEs Plasma diagnostics by atom and ion beams
SOURCEt Diagnbstika plammy* (Plasma diacjnostics)l eb. statey.
Moscow, Gosatomizdat, 1963, 199-211
TOPIC TAGS: plasma interaction, discharge plasma, gas discharge,
magnetic analysis, charge exchange, plasma research, ion beam, atom
beam
ABSTRACT: Apparatus is described for the prcbing of a plasma of an
oscillating diadbarge in gas by means of accelerated and focused
ioji beams or by means of cbarge-exchanged atom beam . Formulas are
derived for the'attenuation of ion beanas in gases and are fouiid to
be in good agreement with eVerimente for the pairs Ae Ar. He*

ACCESSION NR% AT4025310
He, H +-o, Hw, He+-v- Ar andothers. The discrepancy between the
experimental'and calculated data becomes appreciable at high pres-
sures. The limiting pressure amounted to (2--3) x 1015 cm-2 for
the pair Ar+-.+ Ar with Ar+ energy 10 keV and about 1016 cm-2 for
the H+ -,.H2 pair. Analogous results were obtained by measuring the
broadening of the lines of the magnetic-analyzer spectrum. Mea-
surements were also Made of the dependence of the ion density on
the discharge current. Apparatus wag; developed for the study of
magnetosonic resonance and used to measure the attenuation of atomic
argon beams in a hydrogen plasma, atomic helium beams in a helium
plasma, and atomic argon beams in helium plasma. It is concluded
that in spite of certain dkfficulties, the method of determining
plasma parameters by means of beams of fast particles is worthy of
serious a-Ltention, since it has undisputed advantages (practical
elimination,\of contacts, locality of probing, wide range of measured
quantities,,and possibility of quantitative determination of the
plasma composition), It in also concluded that atomic beams are

ACCESSION URt AT4025310
more suitable for the determination of characteristics of charged
particles. The operating speed of measurements with particle bemw
can be made quite high# with a low resolution time* Orig. ari.
has: 7 figures and 6 formulas.
ASSOCIATIONs None
SUBMITTEDs 190ct63 DATE ACQ t.16Apr64 ENCL: 02
BUD -.6iDE tME OR REP SM 00.4' 07FRi '004

_mo
PION M:-AT400~~iO RNCLODSURR:,O
InstAllation with, magnetic -analyzer
M Y17
source, II focusing electrode'system,
III -\ 'gas discharge chamber,, IV - magnetic analyzer
V - oolleotorp VI vacuum pump unit

1-UMBSION NRs AT4025310
4
164
$FROM,
14
.0
Sounding of a plasma with a high-frequency pulsed
Installation:
1 ion source, 2 charge exchange chambers 3 transition tube,
4 bellows connections 5.- gas discharge glass tube, 6 plasma
pinch, 7 - screens 8 - magnetic core, 9 - bellows connection,
10 - deflecting platesp 11 collector units 12 -cathode followers
13 - to registration block, 14 - to pump, 15 - to leak valve,
cow sA 16 to supply. block

IWIV~PIP .- ~* " I -- 1-.1 - - ~ I, ~ 1.
------ - -- -
E
I'tt - , -!~ --, , .., j-,-. -.- ,lf,

3. L 1",
MINE=

-:., ...1.:- 1-1 ...
2
t--
.- - , J~
" i_

If
'
87/6
CC NRz AP6011913 SOURFE'CODE: UR/0141/96/009TO52/02

AUTHOR: Illin, S. D., Petrusev S. S., Che sk y, A., V.
titut) Ell
ORG: Moscow Aviation Institute(Mkakcvskiy aviatsionnn, ins

TITIS: Separating device for multifrequency Slip plasma Probing

SOURCE: 1VUZ.- Radipfizika, v. 9, no. 2, 1966, 287-291

TOPIC TAGS: superhigh frequency, frequency selection, plasma probe
ABSTRACT: A powe.rdistribution system for simUltane`bim; multifrequency plasma prob
ing is described. It operates over a wide frequency range and is provided with
sequential separation of the channels for each frequency. The system (shown in
Fig. 1) consists of a single mi-crowave track with frequency separator elements each I

Fig. 1. Microwave signal separator I
!5*'
-j
F

consisting of one Cht7byshev bandpass filter and one high-pass filter. The filter
arrangement is such, that the lower frequency spectrum is separated and branched out
Card 1/2 UDC: 533.9-07

L, 22880-66
ACC NRs Ap6o-- 1913
of the-track as the signal progresses from element to element. Design f o mul as are
given for calculating thenecessary, filter parameters of a sample system operating on.
Table
ncr
Iter el/C- calc measured, calc. meas ed
a3 ur
05 30 30
2 1.710 0,96 0,80 30 30
7 10 0,96 0,76 30
the 3-cm wavelength. A numNer of filters were ciesigned for frequencies covering the
range of critical plasma paxticle con cent rat ,,,n from 1012 to 7 x 1013/cm3. The
characteristics for three f'ilters are shrjw.,-. accompanying table. where rier is
the critical electron concentration a: - /P: is the output to innzut power
L ~n
ratio -for a filter whose passband is w,, pllasma frequen-Y) _~Ln C;, th e
attenuation of a particular signal 'n - n= ad~ a,-e,-,,, h ann e I s i-S
5 formulas and 5 figures. LBDJ,
-)7
-A' H RE CK A77-
_I'F nonc
Cc;rd

.i'ACC NW
Ukhachev,V.M.; Petru3ev,8.9.;Clierrwtskt-vA.V_.
Ano:
T 1TIZ Location of moving plasmn bursts Irm a conxinl injector
SO'Oj-LrE: Zhurnal tekhnichesltoy fiziki, v. 36, no. 1, 1966, 53-57
TOPIC TAGS: plasma diagnostics, plasma velocity, Doppler shift, microwave
hydrogen plasma A ~~
ABSTRACT: The authors have employed a micrownve Doppler shift rada technique to
m0a.913re III'-- yels~rktlea Q1 h-zdrPeeX1 nIn-mg htxrqt-; injected at velocities from 3.6 x 106
to 1.5 x 10' cm/sec into a 10 cm di=eter 130 cm long glass drift tube by a conical
plnsma gun powered with a 6 RV 20 pF capacitor bank. The measurenents were undertaken
to explore the possibilities of the Doppler shift technique. For control purposes the
velocities of the plasma bursts were also measured with two microwave transmission
cutoff setups located at different positions along the drift tube. microwaves in the
3 cm rnnge were employed for both the cutoff and the Doppler shift measurements. In
the Doppler shift measurements a single dielectric antenna, coupled with n 10 db direc-
tional coupler with a directionality of 25 db, was employed for both radiation and
reception. In order to determine the influence of the fluctuations of the rellecting
surface of the plasma burst on the frequency of the reflected signal, Doppler shift
Card 1/2 UDCt 533.2

'ACC: 004078
R1
measurements were made at several angles .(up to 400) to the line of flight. Good
agreement was obtained among all the velocity measurements, and it Is concluded that
the Doppler shift technique can be used to measure the velocities of plasma bursts
With further development the method will provide other data, Including the time varia-
tion of the velocity, tho trajector# the direction of flight,-and information concern-
ing the internal structure of the-plasma burst. The authors thank Professor M.S.
Rnbipovich and the staff of the laboratory for valuable discussions, and A.N.Pa tvuBhi
and G.I.Ochinnikov for assistance with the experiment. Orig. art. has: I formula,
5 ligureB and I table.-
SUB CCDR: 20/ SUBM DATE: 25Jan65/ ORIG MW: 002 OnI REF: ODO
2/2

Ysr.'
ACC NR: AM6023687 Monograph
U-"/
.:-~,179hernetakiy,,.-.Alekep,ndrV g Anbto4lyevich; Kozlov, Oleg
Uoillyevichi Zinov'Yev, Ole
!Vasillyevich
!AA
Apparatus and methods for plasma,"ludies (Apparatura i metody plazmennykh issledovaniy)
a
*Moscow, Atomizdatj 65- .0363 P. illus., biblio, 3,190 copies printed.
TOPIC TAGS: plasma measurement, plasma radiation, plasma research, plasma diagnostics
PURPOSE AND COVERAGE: The techniques and equipment for investigating the basic
,paremeters of a plas le.g., charged particle density, particle temperature, degree
of ionization, etc, are considered. After a brief discussion of the properties of a
plasma, superhigh frequency techniques a-ad apparatus are described, including antenna,
waveguide, and oscillator systems. Measurements of plasma radiation in the radio and
submillimeter regions are discussed together with the instrumentation requirements. i
The final section of the book is devoted to corpuecular properties of a plasma:
neutral and charged particle flux, pressure, and composition of the plasma. The use
of tritium, atomic, and molecular beams for probing plasmas is discussed'. The book
concludes with two appendices; the first contains tables describing equipment used for
plasma measurements, the second contains discharge and stripping cross section and
energy tables.
TABLE OF CONTENTS Za-bridged7:
F
-Card 113 UDGI 533-9-071

L 01999 6 7
_Acc'i4k~__kf6df36bf_
Foreword - - 3
Introduction - - 9
Section I. General problems of superhigh frequency diagnostics of plasma 13
Ch. 1. Electromagnetic properties of plaBma - - 13
Ch. 2. Basic superhigt. frequency units of diagnostic apparatus - -.21
Bibliography for Section I - - 46
Section II.. Superhigh frequency apparatus for active diagnostics of plasma 54
Ch. 3. Measurement of plasma parameters by the cutoff and "two-frequency" methods
54
Ch- 4- Measurement of plasma electron density by the resonator method 66
Ch- 5. Phase-measuring devices .,'or studying plasma parameters with carrier phase
measurement 74
Ch. 6. Phase-measuring devices with frequency conversion 93
Ch- 7-- Plasma locators - - 131
Bibliography for Section II - - 142
Supplementary bibliography for Section 11 146
Section III. Apparatus for Measuring natural plasma radiation - - 149
Introduction 149
Ch. 8. Measurements in the radio region 154
Ch. 9. Measurements in the submillimeter region,- - 198
Bibliography for Section III - - 210
Section IV. Apparatus and methods of corpUBoular diagnostics of plasma 212
Ch. 10. Investigation of corpuscular fluxes of plasma 213
Card

L 01999-67
ACC NR: AL"6025687
Ch. 11. Particle beam soundings of plasma - - 253
Ch. 12. Apparatus for investigating pressure and ga3 composition - - 316,
Bibliography for Section IV 333
App~ndix 1 - - 344
Appendix 2 - - 353
SUB CODEs 20/- SUBM DATEs 25Nov65/ ORIG REP: 310/ OTH REFt 102
V,
1,4
Lard 3/3

CHERNLTSKn, F. [ChernetsIcyi, F.1
Pulse of the sever-year plan.-Znan; ta pratsia no;294-5 F.462.
(MMA 15s2)
(Kharkov-Turbines) I

DEMIDYUK, F.; CtMMTSKIY, G.; BEMIS, A.
In the struggle for the title of enterprise, shop, brigade,
and shook worker of communist labor. Muk.--elev. prom.
28 no.7:22-24 JI 162. (MIRA 15:9)
1. Umanskaya realizatsionnaya baza Cherkasskoy oblasti (for
Demidyuk, Chernetski , 2. Nizbnetagillskiy mellnichnyy
Kambinat (for Neyms)~)
(Grain handling)

SIPITINER, Yu.B., inzh.; CHERNCTSKIY, Mop Inzhe
Standardixed parts of founding equipment. Stroi.1 dor.
mashinoetr. If n0-8:34-35 Ag 159- (MIR& 12:12)
(Foundry machinery and suppllea)

CIMMUETSKIY, G.I., inzb.; SIPITINER, Tu.B., inzh.
1. -1 .-1.: 4:. - , , ".
Combination die for banding clampa. Stroi.i dor.mashinostr.
n0-7:29-30 Jl 159. (MIRIL 121-11)
(Dies(Mntalworking))

CHERIIETSKIY, I.G., inzh.; SIPITINFAR, YU.B., inzh.
Universal device for gear milling designed at
Voestanic" Plant. Stroi.i dor.mashinostr. 4
S '5 9.
(Gear-cutting machinos)
the "Lknvarskoe
no-9:31-32
(141RA 12:11)

GHW SKIY, Gol.; SIPITIMM. Yu.B.
lathe operator and innovator. Yashinostroltall no.10:30-31 0
159. (Turd w -Technological innovations) (mu 13:2)

CHERIMSKIY, G.I.; SIPITIIM, Yu.B.; SHVARTSBURD, Mo-P.
Readjuxtable universal pneumatic attachments. Hashinstroitell
no.8:27 Ag 160. (MIRA 13:9)
(M4chine tools-Attachmente)

SIPITINER, Yu.B., inzh. CHIUM~T
1~ ~., lnzh.
Devices for turners-innovators. Stroi. i dor. mashinostr. 5
no.4:36-37 Ap 160. (MIRA 13:9)
(2brnlA,-:,Technologleal innovations)

8/193/60/000/009/009/013
A004/AO01
AVEHORS: Sipitiner, Yu.B., Chernetskiy,_gj,
TITLE: The K-401 Diesel-Electric Crane, A
PERIODICAL: Byulleten' tekhniko-ekonomicheskoi informatsii, 196o, No. 9,
pp. 43-45
TEXT- Based on the design of a team of designers of the OGK, the zavod
(Plant) im. Yanvarskogo vosstaniya in 1959, manufactured a pilbt model and pre-
pared the serial production of UFe 7K-401 diesel-electric crane on pneumatic
tires, possessing a lifting capacity of 40 tons. The power equipment of the
crane consists of a 100-hp KAM -100 (KDM-100) diesel engine and an a-c generator.
The costs of the KDM-100 diesel engine are by 2.4 times lower than those of the
2A -6 (2D-6) diesel engines used on the K-252 and K-501 cranes. A serial reduce
of the PM (RM) series is used for the drive of the main, bucket and jib winches.
A new feature of this crane model is an additional jib of 10 m length which is
mounted on the main jib of 25 m length. The jib projection is 14 m while the
lifting height amounts to 30 m (at a lifting capacity of 5 tons). The author
presents a description of the crane design and points out that the application
Card 1/2

S1193160100010091009A13
The K-401 Diesel-Eleotric Crane Aoo4/Aooi
of an electric a-cdrive, using standard big-series electric equipment, instead
of a d-c drive, makes.it possible to decrease th6 cost of electric equipment by
30%, to reduce the'weight and overall dimensions of the electric equipment, to
ensure the power supply of the electromotor from the 3-phase main*, to use the
crane as a movable power station for the supply of the outdour mains and lighting
network, to facilitate the replacement and repair of broken down electric equip-
ment. Since the use of an a-c drive reduces the speed ;.egulation range of t-he
motors, a dynamic-brake is provided for, which operates during the lowering of
loads. The direct current necessary for the supply of two phases of the electro-
motor during the braking process is obtained from selenium rectifiers fed through
a steD-down transformer. The following technical data are given; longitudi-
chassis base - 4,440 mm; height during transportation = 4,195 mm, maximum width
of crane - 3,950 mm; radius described by the slewing part of crane = 4,250 mm,
width of wheel track = 3,210 mm, wheel diameter - 1,220 mm; speeds: lift of
maximum load = 5 m/min, load lift by auxiliary hook = 14 m/min, lift of loaded
bucket = 28 m/min, turning of the slewing part = 0.5-1.5 rpm, travel = 6-14 km/
hour; weight of additional 10 m Jib = 450 kg, weight of crane with 15 m Jib and
hook = 49,500 kg. There is 1 figure.
Card 2/2

s/iq3/6o/6oo/oio/bli/bl5
AOO4/AOOl
AUTHOR: Chernetskiy, G. I
TITLE: The Pneumatic-Tyre K-124 Crane With Hydraulic Controls
14
PERIODICAL: Byulletent tekhniko-ekonomicheskoy informatsii, 1960,'No.!O,pp. 41-42
TEM The Odesskiy zavod im. Yanvarskogo vosstan~iya (.Odessa Plant im. Yan-
varskoye vosstaniye) has designed and manufactured a pilot model of the new self-
propelled full 'revolving K-124 crane with a lifting capacity of 12 tons, which is
hydraulically controlled. The crane is intended for loading and unloading opera-
tions, structural and mounting works and for the handling of loose material with
the aid of a 1. 5 m3 grab bucket. For structural =d. mount ing operations the boom
length can be extended from 10 m to 18 and 22 m by insertion pieces of 8 and 4 m
length. For the handling of large-sized loads the crane is fitted with a tandem,
having an operational boom of 2.2 m. The crane mechanisms are driven by the
(SMD-7) diesel engine of 55 hp and a three-gear transmission box. The use of the
diesel engine lowers the fuel consumption by 9 kg per shift. All units of the era
crane are hydraulically controlled, except the brakes of tAie load and bucket
winches. Control is effected with the aid of three handles and four pedals. The
Card 1/4

s/193/6o/Ooo/bio/On/015
The Pneumatic-Tyre X-124 Crane With Hydraulic Controls A004/AO01
traveling mechanism of the crane is equipped with antifriction bearings mounted
in the H-shaped lower frame with the aid of two barrels:. In this way t1he ground
clearance of the crane and its passability are increased. The loading character-
istics of the crane are shown ih the following table:
rpy3oaast xapaitTepHcTnua xpatia
A
rpY3. M
q.a AonojillIfTelth- joe3 AonomutTexh- BbzAeT. .9 :F BUCOTa noxbema'
xplaxa, At
Hux Onopax jiwx onop
CTPCJIA AARNOR M .9
12,0 10.0 4,2 9.0
9.0 7.5 5 0 8.6
515 4.5 7:0 7.85
-3.0 2.5 10.0 4,6
CTpenft'AA11HOA 18 x (6e3 ryebtia)
5.15 5.0 6.0
4.0 3.0 8 0
2.0 .1.5 12:0 14.0
card ~/4

S/193/60/000/010/011/015
The Pneumatic-T)rre K-124 Crane With Hydraulic.Controls A004/AOOl
Table continued:
CTPCqa AAHaoA IS x (c ryebicom)
2,6 2,0 17
CTpeita MnioA 22 At MC3 ryCbKa)
3,6 3.0 7.0 20.1
115 1,2 12.0 19.0
17.0
0,7 M 15.0
0.4 0,3 20.0 11,5
CTpeits AAHnoil 22 x (c rycuvom)
1.5 21.2
A loading characteristics of the crane; B - load in 'tons; C - with additional
props; D - without additional props; E.- boom in m; ;F - lifting height of hook
in m; 1 - boom of 10 m length; 2 - boom of 18 m length (without tandem); 3
boom of 18 m length (with tandeml 4 - boom of 22 m length (without tandem)
5 - boom of 22 m length (with tandem).
Card 3/4