SCIENTIFIC ABSTRACT YEGOROV, V. P. - YEGOROV, V. V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001962510007-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 1, 2001
• Sequence Number: 7
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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ED,

YIDGORCV, V.P. (Sverdlovsk)
The seven-year plan in action. Zhel.dor.tranap. 44 no.6;20--24
Je 162. (MIRA 150)
1. Nachallnik Sverdlovskoy dorogi.
(Railroads)

BIRKINVAL11j, P.V.; BURDIN, M.P.; GORKIN. S.F.; )3Qf& "if Y_,Z,,- URZMS:91T,
V.A.; XOMODOV. A.A.; IAKTIOVOV, A.T.; LICUDINKO, D.P.; LINEVSXIY, A.A.;
LCBAZIOV, 0.7.; LTAKHOVJCTSKIT, Z.Ta.; MIROMSXATA, O.N., KIMT.1,07,
P.N.; RIKOLiTEV, S.V.; PAKHODZYEV. V.1.; SOKOU)V, G.T.; STRIZH17, N.I.;
SHAPOVAIDY, V.A.; TAVKIN, P.Te..- IVANIXIN, F.D.. rednktor; DROZPOV.
A.I., redaktor vypuska; SERGEYNYA, N.A., redaktor izdatel'stva;
BORISOV, A.S., tekbnicbeskiy redaktor
[Handbook of consolidated estimate norms for geological prospect.ing
operations] Spravochnik ukrupaeanvkh smetaykh norm aa geologo-
razvedochnys raboty (SUSN). Moskva. Goo. izd-vo geol. lit-ry. NG.?
[Rotary drilling] Rotornoe burenie. 1950. 175 P. (ICA 9: 12)
CMicrofilm]
1. Russia (1923- U.S.S.R.) Ministeretvo geologii.
(Bbring)

Subject USSR/Mining
Card 1/1 Pub. 78 - 3/27
AID P - 489
Author Yegorov, V. P.
Title Causes of delay in derrick-errecting work in the- oil
fields of the Main Western Petroleum Production Region
Periodical Neft. Khoz., v. 32, #6, 12-16, Ju 1954
Abstract The author discusses various causes of delay in the rigg-
ing and removing of derricks in the Western oll,field
region and the Increase of the cost of production from
140 to 186% over estimates, The use of high power pulley
installations and mechanical transport by caterp'-llers
will considerably reduce delay and the cost of production.
The author proposes the development of standard ';ypes of
derrick construction with standardized flooring, siding,
concrete work, and specially trained crews for h.!indling
heavy pulley equipment.
Institution : None
Submitted : No date

YEGORGV,V.P., inghener
Results of a review of efficiency suggestions in the organiza-
tions of the Main Administration of Highways. Avt.dor.18 no.5:2'.'
3 155. (MIRA 9:1)
(Highway departments)
-F3,
AF-5
FIE ~d

- I I "I I i . r- r-
YEGOHOV, V.P. "
Important mainline in the Urals. Zhel.dor.transp- 39 no.11:86-92
11 '57. (MIRA 10:10)
1.1fachallnik Sverdlovskoy dorogi.
(Ural Mountain region--Railroads)

SOV/4-59-1-6/,"2
AUTHORs Yegorov, Vladimir Petrovich, Chief Designer
TITLEs The Turbines- of the Seven-Year Plan (Turbiny semiletki)
PERIODICALi Znaniye - Bile, 1959, Nr 1, pp 6 - 9 (USSR)
ABSTRACTi' Thermal power engineering has begun to make more powerrul
turbines, and the problems involved are described in tnis
article. The 7-year plan provides for an increase of 0
million kw of turbine power plantat whereof 50 million are
thermoelectric power stations. The author explains hor
greater economy is achieved in building powerful plantt
which produce a much cheaper current. He also tells of' the
difficulties arising in consequence of the transition from
100,000 kw turbines to those of higher capacity, and of the
new way in which the problems of automatic control of hLgh-
power turbines will have to be solved, There in 1 photi.
ASSOCIATIONt Leningradskiy metalliohaskiy zavad (Leningrad Metal Plant)
Card 1/1

.,Pa- ~(4
RB 6o/o34/07/(.16/009
BS 00157 0 7 0
AUTHORS: Strakhov, B. V , Yegorov, V. P., Lebedev, V. P.~
Kobozev, N. I.
TITLE: The Pbysical Chemistry of Concentrated Ozone~\ IX. The
Dependence of the Yield of Nitric Oxide on the_Explouion
Temperature of Ozone -Nitmgen Mixtures
4
PERIODICAL: Zhurnal fizicheskoy khimii, 1960, Vol. 34, No. 7,
pp. 1524-1527
TEXT: Investigations were made on the dependence of NO yield on thEi com
o
position of ozone - nitrogen mixture for constant temperature of explo I n
and an initial pressure of 100 torr, as well as for constant oompos,~tiono
of the initial gaseous mixture. The experiments were performed in an
apparatus already described (Ref. 1). The temperature of the explosion
was controlled by introducing stoichiometric mixtures of methane and
ozone In the explosion pipette. The i8othemoofoNO yield (Fig. 4) obtained
for the constant temperatures of 3000 and 3500 K of explosion show a
maximum for a 40% ozone content in the mixture. If the composition of
Card 1/2

The Physical Chemistry of Concentrated Ozone. 3/076/60/034/07/0r)/009
IX, The Dependence of the Yield of Nitric Oxide B015/BO70
on the Explosion Temperature of Ozone - Nitrogen 81972,
Mixtures
the mixture is kept constant (65% 03 + 35% N2)f NO yield varies with
explosion temperatures from 0.6% at 250001C to 3% at 42500K, viz-, a J',ive-
fold increase in the yield for a 1-7-fold increase in temperature. Tl-;a
results obtained are explained on the assumption that the yield varie:
according to the change in the thermodynamic equilibriumlof the reaot'4,0n
N + 0 2 NO at the temperature of explosion. Ye. 11. Yeremin, A. 11,
2 2 - - i,
Mallteov Ya. Be Zelldovioh, P, Ya. SaJovnikov, D. A. Frank-Kamenotsk-I.y
are mentio~,Wdin the't-e*xi." There are 5 figures and 4 references: 3 Soliet
and I German.
ASSOCIATION: Moskovokiy gosudarstvennyy universitet im., Me V. Lomonc,sova
(Moscow state university_imeni Me V. Lomonoso
SUBMITTED: October 5, 1958
Card 2/2

EFR/EPF(c)AW(q)/W(m)/BDS AFM/APGC Ps-4/pr-4 BW,
S/076/63/037/004/025/0,,
AUTHOR: Yegorov, V. F.~ Lebodev, V. P., Ko'bozov, 11, 1
0 0"7XIV.- Interaction of
TITLE: Physical cbendstry of concentrated zon
ozone with hydrogen Earoxide at loli-t-emperatures
PEMODICAL: Zhurnal fizichaskoy khindi, V. 37, No. 4, 1963, 922-924
TEXT: Tests were conducted to deterrdne the possibility of a reaction ii
the case of the low temperature interaction of ozonellwith hydroren mroxiAellwitt
the fonnation of a higher peroxide-of hyd Two eerios of tests were con-
ducted: 1) bubbling pure ozone through a cooled 60% paroxido, and 2) freezin.g
pure ozone at the temperature of liquid nitrogen on preliminarily pulverized so]' -d
peroxide and holding the resulting mixture for a long period of tire (up to 76
hours). In bubbling the 100% ozone throuch the concentrated (6011) peroxide ther.
r~ IV
is a partial decomposition oj' the peroxide which increases as the temperature of
the solution goes up. In the case of the condensation oj~ pure, ozone no action W, S
--detecte-d-on-the pulverized -.alld peroxide There is 1 chart. The most importan,
sh~-language source reada as follows:-D.-H.. Y-olman,, J,_-_-Chem4,-Frjys-., 1/+~ 707,
___1946
-S-tii
ersity irgeni M., V. Lomonosov
Card 11il
- _7~ -

PINUS, EkUl Ruvimovich; RADIN, Anatoliy Nakeinavich;
red.; GORYACHKINA, R.A.9 tekhn. red.
(cement concrate.]TSementobeton. Moskva, Avtotransizdat, 1962.
59 P. WRA 16:3)
(concreta) (Pavements, Concreta)

YBOOROV, V.P.
Potentials for increasing traffic speeds and the weight of
trains* Zhol.dor.tranap. 42 no.703-36 Jl 160.
MR& 13:7)
1. Ikobalknik Sverdlovskoy dorogi.
(Railroads--Trains)

YEGOROVO V.1's (,Sverdlovsk)
Potentials for the reduction of labor and material expenditures.
Zhel,dorotranspo 46 no66tl9-23 Je 164o (MIRA :18:1)
1. Nachallnik Sverdlovskoy dorogi.

-~1~7 ~ --2
USSR/Metals - Freezing, Effects- Marter-site Feb 50
"Aj-.plication of t~e Diletometric Yethod to Invr.S+Ii-*Ir,,i- th.,~ Yarter.~Itlc
at Temperatur(is Below Freezing," 1. L. Mirkin, V. 3. Yeilzrov, C pp
IIZavod Lab" Vol No 2
PA 159T61

YB30ROV) V. So
"Lost Wax Method of Casting Metal Cutting Tools at the Sestrovetsk
Plant imeni Voskov," p. 211. in book Yechanization and Automatic Control
of Founding_Processes, leningrad, 1957, 22hpp.
77777777'77-7

SEREBUAKOV., Mikhail YaVgenlyevich. Prinimali uchantiye: VOROBIYEW,
P.A., kand. tekhn. nauk; SLROTINSM, V.F.j, kand. tekhn. nauk;
V.S. kand. tekhn. nauk; D14ITRIXEVSKIY, A.A.., do-.Ur
YEGONY j
'-t,eTdm. nauks prof,p reteenzont; USINNOV, V.F.9 kand. tokhn.
naukq dots.9 retsenzent; DEMUSYAK, A.G., inzh.,, nauchrWy red.;
MOJOZOVA, P.B., red. izd-va; KARPOV, I.I.,, tekhn. red.
(Interior ballistics of barrel systems and powder rockets]
Vnutrenniaia ballistika stvoltrykh sistem i porokhovykh raket.
3. izd., dop. i peror. Moskva, Oborongiz, 1962 703 p.
iKERA 15:12)
(Balliaticop Interior)
r

XEGORUV, V.S.. maahinist
What causes electric power losses? glek.i tepl.tiaga 6 no-5:19-'~20
My 162o (MIRA 15-.6r'
1. Depo Barabinsk Zapadno-Sibirskoy dorogi.
(Electric railioads-Management)

KOZHEVNIKOV., S.N.; KUKHTEVICH,, inzh,,- MUKOVj Ye.A., inzh.;
inzb.; KEVEnD, A.V., inzh.
Analyzing the accuracy of weighing on lover-type hopper ocales.
Trudy Instschern.met.AN URSR 16tl5-25 162. (MM l5sl2)
1. Chlen-korrespondent AN MaM (for Kozhevnikov).
(Blaat furnacee-Equipment and aupplies)
(Remote control)
Mr

KOZAI:VNIKOVF S.N.Lig~'~V ~V.S. , Inzh.
Frequency meters of speed and travel. Trudy Inst.chern.met.Aff
URSR 16:66-69 162, (MIRA 15x12)
1. Ghlen-korrespondent AS UlcrWR (for Koahevnikov).
(Machinery, Kinematics of)
(Electronic measurements)
4,0U, IMM

BEKINS N.G.; EPSHTEYN, V.G.; Prinimal uchastlye YEGOROV,, V.S., inzh.
Investigating the dependence of drive power and screw preisure
on the thrust'boaring on the technological parameters of the
rubber compound injection. Khim. i khim. tekh. 1:371-384 162.
(MIRA 17:2)

.: .:, -.. :,.~T : -~ ~~, ~!v ; ; ~:~ - I ~ . . ~ .1 . --
YEGOROV, V.S.; ANDREYEVA, A.G.; FOMENKO, G.D.
- -, Ga s , c ,y .aniding &,Id cewntation of Khl7N2 (E1268) stainlesis steel.
Metalloved. i term. obr. met. no.3:33-37 Mr 164. (KRA 17:0 1

AIZKSEYEVSKIYI ?I,Ys.; JTJF.RO'IIIT, A.V.;. YEOOR9Y;
Pulse mt%ods of 3twdying the superconducting proTerties of alloys.
DAL AN SSSR 163 m3#5:1121-IU3 Ag 165, (MIRA IWO)
1. Inatitut fivichrskilk-li problem im. S.I.Vavilava All 6SSR. Sub-
mittAd Janua-.7 16, 1965.

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AUTHORS; Grabovskiy,, M. A., and Yegorov, Vs. Be, 53-44-7/11
TITLE: Sam& Cafts,10g: 3VeAwzk~&k;j0=wjjAtjons for,rW*AeA*=l -0AAr9e, in
PbYsics (Neskollko demonstratsionnykh opytov po obahcheou kursu fizi,'Ci).
PERIODICAL: Uspekhi Fizicheskikh Nauk, 1957j Vol. 63, Nr 4, pp. 8"lf.; (USSR).
ABSTRACT: A device for the demonstration of the motion of the center, of mass
of a system "Falling Board": This device consists of a bow.!:d in
oblique position. one of the ends of this board is held Mimly by
means of an electromagnet, while the other end slides, nea-Ay
without friction, by means of balls on a slideway. For the.detern
mination of the path of the center of mass two brushes are;'fastened
on the system, which are in slight touch with a vertical s.~~ieet of
paper. One of the brushes is fastened to the center of mat:4 of the
system, the other somewhat higher. After switching off thi! electro-
magnet the brush located in the center of mass will draw it straight
line., and the brush located somewhat higher will draw a c,:,rved line
(with the curvature directed towards the center of mass).,:'Follawing
this, a weight is fastened to the upper end of the board.iThe upper
brush, is now in the center of mass. When the experiment vf~Ls repea-
ted it was found that the upper brush draws a straight U~ie, whereas
Card 1/4 now the lower brush draws a curved line the curvature of 4hich is

Sam 00ts,,6f ExperiwntalLDemnatrationtifgr-.Ltbe,,Generallcomse. 53.JW1111
in Physics
directed towards the center of mass* The authors give some practical
directions as to the construction of this device, 2# The resonance
of a motor suspended on a spring*' In the case of resonance motors
are able to loosen their fundament. These and similar phenomena can
be demonstrated as follows: A small motor is fastened on a cylindri-
cal sprine on a massive stand. On the axis of the motor a small
rod is asymmetrically fastened, which causes percussions, o_*f the
frequency of the motor. The first resonance at -- 85 rotations per
minute manifests itself by a periodical lifting and lowering of the
motor. The resonance frequency of the spring depends on th~ elastis
city coefficient of the spring and on the mass of the moto-r. In the
case of the second resonance, at about l7o rotations per minute,
the motor oscillated round a vertical axis. With an increase of the
number of rotations new frequencies occur. With the highest frequen-M
cy standing oscillati6ns occur on the cylindrical spring,, but the
motor remains in its position. In large lecture halls it is advisable
to project the shadow of the motor on to a screen* 3. The pheno-
menon of acoustic resonance on Helmholtz resonators: Four Helmholtz
resonators of different size are arranged in such a manner that the
holes are on 11-he same level. In front of these holes four iimilar
paper turn-wheels are fastened. In front of the large openings of
Card 2/4 the resonators a loudspeaker connected with a sound source is moum-

36m- Cases Experimental - Demonstrations -,for.! -the, General Couric. 12"ho-71 11
in Physics
ted. The turn-wheels which happen to be before the excited resonan
tor then rotate. The dimensions of the apparatus are given* 4o.
A small, ball in a gas- or liquid jet; A gLus. tube, one hall' of
which has a cross section that is about 16 times as great as that
of the other, Is connected by reans of a rubber tube with a 12alloon
which contains liTiid carbon dioxide under high pressure. In the
wider part there is a ball, the diameter of which is smaller by
about I - 1,5 mm than the inner diameter of the wider part cf the
tube. The gas flows from the narrower into the wider part o.-" the
tube. Because of the decrease of pressure occurring on the vider
part, it is possible to turn the tube with its wider part directed
downwards without the ball falling out. 5. A "cut" ball: A tennis
ball caused to rotate by an oblique impact is surrounded by rather
complicated currents of air. Therefore, a '?cut" ball may change
its direction during flight and may thus deceive the other tennis
partner. For the purpose of demonstrating this application of the
Magnus effect a special device is here described: A direct current
motor of 25 watt power in vertically fastened to a massive stand.,
On the motor axis a rubber tube is:fastened which is longe::- by
X - 2 mm than the axis protruding from the rotor, On to t:-te end
Card 3/4 of the rubber tube a celluloid table-tennis ball is fastent-.d..

Some C"es~ of-HicperimentaY Demonstrations for the Gefferal. Coii~~e
in Physics
A small disk Is pressed on to this ball from above by means of two
cylindrical springs. When the motor rotates the ball is tako~n along
by the rubber tubes and rotates -nth good regu1arity with tne fre-
quency of the motor. The resting as well,as the rotating te-mis baU
can be knocked out of its position.by means of a'spring, First, the
bal]L is knocked out several times while the motor is not rotatinj
and in this case it practically always flies ii. the same directiont
However " in the case of a rapidly rotating motor, it flies in anon
ther direction.
There are lo figures.
AVAILABLE*' Library of Congress*
Card W4

:~.. and GHUMITIN, A. M., 1-bacow
)MGOROV,_ Lt. -
"The Observation of Anomalous Dispersion in the 1,116mentary Processes,"
a paper presented at the Third Internotipnol Conference on Ionization
Phenomena.in Gases, Vcnice, 11-15 Jun 57.
SO: B-3,087,498.

(~ C) 1< -o \[I V, 5-.
AUTHORS: Shukhti n, A.M. and Yegorcv,! V. S. 51-4-25/25
TITLEj . An assembly for obser-Wallat-vt-the -anomalous dispe;.-sion
in processes of short duration. (Ustanovka dlya
nablyudeaiya anomallnoy disperaii pri kratkovremez;j3ykh
protsessakh).
PERIODICAL: 11ORtika i Spektroskopiyall (Optics and Spectroscopy"
' '' 19~1, Vo12, No.4 PP-543-544 (U.S.S.R.)
ABSrRACT: D.S.Rozhdestuen8kille "hook" method (Anomaloua Us-
persion, published by the.Acadamy )f Sciences of U.-S.S.R.,
1951) of observation of anomalous dispersion requircs ex-
posures from several seconds to several minutes. To study
transient processes (e.g. pulse discharges, shock waves,
wire explosions etc.) the present aqthors used the "hooic"
method with a strong-light-source of the pulse type. This
light-source was a glass (30 am long, 8 mm dia.) di~,c'harge
tube with hollow cathodes. It was filled with H2 or air at
several mm of Hg. The pulse was produced by 201.4,oF :apacit-
ors charged to. 9-11 M The pulse duration was less than
30-30,44,aec The pulse produced very bright continu:.us
spectrum fr;m.6500 to 2200 A (it is reported by othar
workers that such pulses produce also strong infra-red
radiation). Interference patterns in the visible region
Card 1/2 were studied.with a diffraction grating spectrograph while
Ilk.

51-4-25/25
An assembly for observation of the anomalous dispersi(5n
in processes of short duration. (Cont.)
for those in the ultraviolet a quartz priam spectrograph
was used. This source was used to study pulse discharges
in neon (at several mm of Hg) of about 300 see dura,,.ion.
The circuit for pulse synchronization of the light sc,urce
and the neon discharge is-given. Anomalous dispersiot.
"hooks" are shown in a plate a5ound lie I lines 6402 It
(3s3P2-- 3p3D3) and 6383 A UP P1 - 3P'Pl)- There ar 'It
four figures-and seven references, six of-which are ;4lavic.
ASSOCIATION: Physical Research Institute, Leningrad State,
University. (Hauchno-isaledovatellskiy fizicheskiy
institut, Leningradskogo gosydarstvennogo, urtiversUeta
SUBUITTED: November 30, 1956.
AVAILABLE: Library of Congress
Card 2/2

AUTHORS: Shukhtin, A.-M., regorov, V. S. SOV/48-22,6-18/28
TITLE: The Observation of Anomalous Dispersion In Proce3ses of 'hort
Duration (Nablyudeniya anomal'noy &Lspersii pri kratkovr-.-ms.,rwYkh
protsessakh)
FMIODICAL: Izvestiya Akademii nauk SSSR, Seriy& fizicheakaya, 1958, Vol. 22,
Nr 6, pp. 711-713 (USSR)
ABSTRACT: The so-called "oxotch" (kzyuk) method developed by D. S.
Rozhiestvenskiy concerns the obtaining of spectrogram3i.,ade in
interferometill.o ay_st~3m3 with low light intensity. The eAeavor
is Aadd here to use this methoi for speotrometrie inves-;igations
of processes having the character of an explosion and c her cases
iu whi:jh exposure is restricted to some milliseconds. Ilie light
source used vas a synchronized flashlight scurat as d"cribed in
this paper (Ref 1), and the spectrograph used is described by
reference 2. The authors emphasize the fact that only sim experi-
ment was intended to be carried out for the purpo3e of finding
aat whether it is possible to employ the method mentiored. In this
experiment a discharge tube (Fig 1) was used which was introduced
Card 113 in-;.,o the beam of the interfarometer. The tube waz filli,d with

The Observation of Anomalous Di3penion in SOYAB-22,.6-j8/28
processes of Shoe. Daration
r,eor-- or hydrogen gas. A oiaaa of sodium vapor w&s produ,r-a in
its center by meani of a heater' These vapors diffasel a A formed
a iret&! rrd,rror on the glass $Urfac,7 ne--tr the hiater~ A c!irrtnt
di,scharge pulse (AISOO A) was sent ttirough -the +,,.ibi, -;tiijoh vnois
iynahroL,12,ed veith tha flashlight. The "crotches" -near the lines
of the yellow do-ablet of dodium v.--re photographed be-
forty -the pulne, duri..ng the piAse, w will as several mi.5r%meconds
after ii. On this occasion it was found that the tuioma~e
van:'Is'hea during the carrent. Impulse, whereaa a-fttir the -;)ulse it
is 3everal times greater tlv= before, This is explaInid a3 a -.on-
seqaer.cz- of the stripping of X& &+.oma from the glaas iu.,,fa_--_.
Moreover. the lack of wAcmly during the pulie is -i-rpla!.n-,-a by
thi transition of atoms to 5ta-teb of higher energy a.-s vi-,.-11 as by
the effeot of negative dispersion, After -the pulse disfo!rsion :~n-
oreases rapidly and dies down again in the oourie of BCO-1000P-
seconds. This process corresponds to the theory of the. ooncentra-
tion of the excited atoms (Ref 3). In the sama marraer erperiments
Card 2/3 were carried out with mercury-- and magnesium -fapori th,~, resu3-4.3
PW

The Obsormtion of Anomalous Dispersion in SOV/48-22-6-!8/28
Processes of Short Duration
obtained do, however, not agree with those obtained prarviously
(with Ne). In conolusion the authors stress the neoe3sily of a
further investigation of this problem. There are 2 figurea and
3 referencts, 1 of which is Soviet.
ASSOCIATIOM Fizidhe3kiy institut Leningrtk%kogo gos. universiteta li3.
A. A. Zhdanova (Physios Instilate of Leningrad State Ur;Lversity
imeni A. A. Zhdanoi)
1. Spectroscopy 2. Interferometers-Performance
3. Flashlights--Applications 4. Discharge tubes-App.'iications
j

9(6)
AUTIIO~S: Shukhtlln, A. M., Yegorovr V. 3. S07154-59-3-1121
TITLE: Observation of Anodalous Dispersion by the Method of
D. S. Rozhdest-,renskiy in the Pulse Discharge in Veon
PERIODICAL: Ve3tnik Leningradikoge unizaraiteta. Serlya fiziki J_ khimii,
19599 Nr 3P pp 6!-66 (USS'17)
ABSTRACT: In strong gas discharges the atoms are in highly exci4;ed state
which may be determined from the energy distribution. The
concentration of the atoms in the various energetic i:tates may
be determined by various methods, the most important '-eing the
"hook"-method by Rozhdostvenskiy. This method was used. in the
present paper for s~ndensed ;.ulse aischarges. The ach:!me of the
apparatus is described in an earlier paper (Ref 2). The pulse
source for the continuous spectrum ic represented in,!.igure 1.
'
l
The square pulses and bell-shaped pulses with differe~i
amplitudes were investigated. Spectrograma were obtallaed which
correapond to varioua stages of the pulses, and the (Dncentrat-4on
of the absorbing atoms N and thair number f waro dotormined
herefrom. Figure 2 gives the results for an atom exc1tation in
Card 1/ 3 the 3P2-level. Maximum dispersion was attained at thi: end of the

Observation of Anomalous Dispersion by the Method of SOV154-59-3-11121
D* Be Rozhdestvonckiy in the Pulse Discharee in Heon
plane part of the pulse. Figure 3 shows Vic time dopenii.enco
of the occupation of a level after the s,ritching off of the
current for various levels. Moreover, V.e influence exercised by
the structure of the backside of the pi-.!.Je on the atom.
distribution is investigated. It was found that the cbange of
dispersion dependE on the steepness of the decrease of the dis-
charge current*After the switching off a strong rice takes
place. In the plane ranee of the pulse, however, no slLt:,.h
dependence was to be observed. In a bell-shaped pulse of a
duration of 16/4.see with an amplitude of 60 a a concentration
of the atoms excited in the 3 P2 leve). of 2.8.1013/cm3 -ould be
observed. Figure 4 shows the variation with time of th3.
concentration N for various levels. With an increase !Ln pres3ure
in the discharge tube frum 1-4 torr the value of dispersion
increased to a maximum. The concentration of the exci4ed atoms in
the first part of the excitation wave is very low and increases
onlj in the plane part. After the current has been switched off
it strongly increases. Thin nharp increase is explained by the
Card 2/3
7,

Observation of Anomalous Dispersion by the Method of SOV/54-59-3-1/21
D,89 Rozhdestvenskiy in the Pulse Discharge in Ron
recombination of ions with electrons. In conclusion, the authors
thank S. E. Frish for the supervision of the work. There are
4 figures and 7 references, 5 of which are Soviet.
SUBMITTEDt April 14, 1959
Card 3/3

SHUKHTIN, A.M.; YEGOROV, V.S.: TUMAKAYEV G.K.
Source of radiation with a continuous spectrum and with single ,'lashes
of short duration. Opt. i spektr. 8 no.3:423-424 Mr 160,
(MIRA 14: 5'd
(Radiation)

TEGOROV, V.B,: BOUTIN, A.M.
- -----------------
Afterglow and its relation to gas density in a pulse dischargo in
Me. Opt. i spektr. 9 no. 6:794-796 D 160. (MIRA 14:1:1
(Neon) (Blectric discharges through gases)

69845
s/o5l/6o/oo8/O3/O33/O38
a 0 0 E201/H191
AUTHORS: V.S. and Tumakayev, G.K.
TITLE: A. Continuous-Spectrum Emission Source Capable of Sinj-,le
Short-Duration Flashes Jt
PERIODICAL: Optika I spektroskopiyat 1960, Vol 81 Nr 3,
pp 423-424 (USSR)
ABSTRACT: The authors describe a.light source with continuous T
emission spectrum capable of 'single short-dura tion flashes
of great intensity. The main part of the source is ii
demountable capillary discharge tube (Fig 1). The aising A/
of the tube (13) is a.thick Pers ex cylinder inside -which
a porcelain capillary (14) of 3-& mm internal diameter is
fitted. Blectrodes.(l) and (10) are attached to the
cylinder and the outer ends of the electrodes are fitted
with windows (2). One of these windows is made of qaartz or
glass and is usqd for transmission of the flashes. Under
working conditions the windows become dimmed by depooits on
them and have to be cleaned or replaced regularly. A lens
Card (5) is used to produce a parallel light beam. An au;-:iliary
1/3 (s.tarting) electrode (9) is pla,,-ed In the middle 0f i;he
discharge capillary. To reduce the strong Inductanc~ of the

69845
S/051160/008/03/033/038
F.201/sigi
k Continuous-Spectrum Emission Source Capable of Single Short-'
Duration Flashes
~discharge circuit the electrodes were connected directly
to terminals of a capacitor (0.56 pr$ charged to 25-.10 kV)
used to produce the discharges. The air pressure in the
discharge capilla-A-y could be regulated so that at a given
steady potential difference across the tube spontaneous
discharges would not occur and that when a firing pulse
was fed to the tube the discharge would occur rapidly and
easily. In the tube described here the optimim air
pressure was 130-150 mm Hg. The electrical circuit is
shown in Fig 2. The authors used a hydrogen thyrat:-on
TGIl-400/16%which ensured that a discharge was prod::.ced
about 1 14 a after an appropriate positive signal wi.s
applied to the thyratron grid, Fig 31 1, shows thel
oscillograms of the discharge current (Gurve a) and,',,the
Optical flash (curve 6); the optical flash existed,!only
during the first half-period of the discharge2 i.e.~about
Card 3-5 Psec. Fig 3, 119 shows the osaillograms of the.
2/3 optical flash and time marks which represent Usec,each.
The spectra of the flashes were found to be co inu.*:3us

69845
8/05'1/60/008/03/033/038
H201/E191
k Continuous-Spectrum Emission Source Capable of Single Short-,;'
Duration Flashes
between 2200 and 6500
Card There are 3 figures.
3/3
SUBMITTED:
November 12, 1959

S/053/60/071/004/005/005/xx
B006/BO67
AUTHORS: Grabovskiy, M. A. and Yegorov, V. S.
TITLE: Some Experiments on the Topic "Rotational Motion"
PERIODICAL: Uspekhi fizicheskikh nauk, 1960, Vol. 71, No- 4, pp. 677-680
TEXT: The authors describe some demonstration experiments for physi-,,s
classes of demonstrating some rules governing the rotational motion.
The first device which Is described is a cylindrical double spiral viich
is perpendicularly fitted onto a stand and which can rotate about if.a
longitudinal axis. The instrument shown in Fig, 1 (photograph) is :
1.1 m high, and the distance between the two windings Is 55 mm. The *'two
spirals form rails on which a metal or wooden sphere may roll. The
uppermost part which is called the "accelerating part" is designed in Ll
such a way that the sphere is supported by the lower rail; as soon as
the speed of the sphere is high enough it rolls downward on the rails
which are nowlying on the waj~ of the cylinder ("perpendicular part of
the winding") (see Fig. 2). With this device a demonstration of the
rolling of the sphere on ihe perpendicular winding with braked rotation
Card 1/2

Some Experiments on the Topic "Rotational S/053/60/071/004/005/OCIVX X
Motion" B006/BO67
of the spiral, a demonstration of the law of the conservation of the
angular momentum~ and a demonstration of the motion of the sphere on ihe
spiral rails if the spiral is rotated (in- or opposite to the directi(,n
of motion of the sphere) are described. Furthermore, a similar device
(Fig. 2) is described which again consists of a double spiral running
at the lateral area of a truncated cone. The upper part of the rail is'!
considered to be the region of acceleration on which the sphere attain~i
the necessary speed in order to be able to continue its way on the re-"
maining perpendicular part of the spiral. This double spiral is fixed.'!
Experiments with spheres of different sizes and different weights are
discussed. There are 3 figures.
Card 2/2

20930
B/057/61/031/003/014,1'019
B125/B209
AUTHORj Yegorov, V. S.
TITLEt Measurement of the temperature of an electron gas and of
charged-particle concentration during a pulsed discharge in
neon
PERIODICALt Zhurnal tekhnicheskoy fiziki, v- 31, no- 3, 1961, 352-356
TEXTs The author has already made optical observations by the method of
"crooks" (established by Rozhdestvenskiy). In the present study, bo) makes
an attempt to measure parameters of a pulsed discharge, such as teu;?erature
of the electron gas and concentration of the charged particles. Tha con-
cept of electron temperature is meaningful only if the velocity distribu-
tion of electrons is Maxwellian. This is the case with the present con-
ditions, at least approximately. The electron concentration ne and the
temperature T 0 in a pulsed discharge in neon were measured by the tffo-probe
method for various amplitudes of the discharge current pulse and at
various initial gas pressures. The probes were placed in tubes of 14 and
Card 1/8

20930
S/057/61/031/003/014/019
Measurement of the temperature... B125/B209
60 mm diameter. The volt-ampere characteristic was ascertained frot-. the
points for several dozens of pulses of the discharge current. A collibina-
tion of all pulses belonging-to one cross section forms the volt-ampere
characteristic of the double probe with respect to a certain phase of the
pulsed discharge. Fig. 1 depicts the experimental arrangement. Fig. 2
shows an instance of a volt-ampere characteristic of the double probe as
taken by this method. In the 14-mm, tube, the ion current falling on the
probe exhibits no peculiarities in the case of high potential diffeXences
between the probes. On the oscillogram. of the ion current at the 60-mm
tube, periodic attenuated oscillations, whose amplitude and frequency in-
crease with the amplitude of the discharge current, can be observed. The
temperature of the electron gas was ascertained from the volt-amperif
characteristics of the double probe by semilogarithmic graphs. The
results of measurements of the electron gas temperature under varioas
conditions and at different times of the pulse discharge, as well a3 the
field-strength values on the discharge axis are compiled in Table 1. Te
varies only slightly during the short current pulse. The relativelj high
Te values during afterglow are explained by a remanent voltage acro:is the
Card 2/8

20930
8/057/61/031/003/014,'019
Measurement of the temperature ... B125/B209
capacitors and by the "tail" of the current pulses which is due to 'rhis
voltage. The concentration.of charged particles was determined by
evaluation of the ion fractions of the probe characteristics. At these
pressures, the following formula was ueedt n T a 2-10 12 a fAF i ln
e e IF +
(1), where X" denotes the mean free path, Q ithe cross section of charge 0
exchange of the neon ion at 1 mm Hg, A the atomic weight of the gas-, T the
gas temperature,.j the density of the saturation current to the probe, a
the radius of the probe, 1 the length of the probe, and x 0 is a correction
factor near 1. An inaccurate T value does not give rise to greater errors.
Data concerning the density of Ne were ascertained interferometrically.
Table 1 shows the concentrations of charged particles as calculated from
Eq. (1 ) . Under 'the conditions of the present study, the degree of Ioniza-
tion is very low. The greatest error in the n evalues is caused by the
influence of the photoelectric effect upon the'probes. When the potential
of the probe is highly negative with respect to the plasma, another current
appears besides the particle current, which is due to short-wave radiation
Card 3/8
V"
54u,

20930
S/057/61/031/003/014/1319
Measurement of the temperature... B125/B209
giving rise to-a photoelectric effect on the probes. This additional
photocurrent apparently increases the saturation current of the ions. The
author thanks,A. M. Shukhtin for guidance and Yu. M. Kagan for a din-
oussion. There are 3 figures, 2 tables, and 12 references, 7 Soviet-bloc
and 5 non-Soviet-bloo. The two references to English language publications
read as followas Champion, Proc.Phys-Soo., Beot.B#70,2,1957; J. B, Hasted,
J. Appl. Phys., 30$no.1#2291959-
ASSOCIATIONt Leningradekiy gosudarstvennyy universitet im. A. A. Zhdanova
(Leningrad.State University imeni A. A. Zhdanov)
SIJBMITTEDt February.24,.,1960
Card 4/8

2G9N
S/057/61/031/003/014/0-19
I 4easurement of the temperature... B125/3209
4
Legend to Fig. 1: Diagram of the arrange-
ment. 1 E 70 v, 2 - C 2000 micro-
3 Rogovskiy belt.
farads R 0.6 ohm, 4
I C-1
0.
7
Fig. I
Card 5/8
,-in

.5/057/61/031/003/014/C)19
Measurement of the temperature... B125/B209
Legend to Fig. 2s p0 4 mm Hg,
rectangular current pulse with an
7-
amplitude of 200 a; t 50 micro-
seconds.
10 10 10 /a zo jo 4
J
10.
29,
Fig. 2
Card 6/8,

20930
5/057/61/031/003/014/:)Ic

l4easurement of the temperature... .
B125/B209
HunyAbC TOXN, KOAOKOA006P42R*ll ftOpUbt, .(OHMrIyAbC TOX4 npXUOyr*Abtt*R IVOPUM.
npAy-isiembitl npH antpitoAnqec3com P03PRAt noAy4,%euoA Ilpit P13PAAG HCXYCCTOCII-
XMIAWICAITOPa 0.8 uscip a -rpyGxa 0 14 mm; uo;i Anunm a Tpyoxe 0 14 mu: AAwTcAb-
AAI4TtAb)tOCTh IWIYAWL 110 OCIIOD*IfHIO UOcTb DO CICHOSSURIO M MXceK...
16 mxcen., I = 60 - 70 &; pa 4 mu PT. CT. nAocxax DepmX1111 150 mxctx.
IX 4-6
-I mew
I- Mpa
3
t, NXCSO. X
rt.
9. 214H

.tog.

1l.

ICU
q r
A sr.
-test
4
3m
14
6 35000 12
8 37000 9
301 44000 6 30 3M 7.5 10 IM 5
100 40OW 6 100 40000 7.5 12 29000 2
140 40000 6 140 32000 7 20 =7000 < I

Card
MIMM

S/057/61/031/003/014/'019
Measurem.ent.of the temperature ... B1251B209
Legend to.Table Is I - Bell-shaped current pulse obtained from periodic
discharge of an 0.8-microf4rad capa citor in a tube of 14 mm diameter.
Length of the pulse at its base: 1 6 microseconds, 1.- 60 + 70 a;
Po 4 mm Hg. 2 - po 1 mm Hg,,l - 200 al 3 - Po M I mm Hg, I - 3C0 aj
0
4 t, microseconds; 5 T K; 6 0
E in v/cm; a - T in K; E in V/*Cm;

14 Po -.4 mm Hg, 1 -*200 a; 15 ti microsecondal 16 - T 1 0KI
e
IT - E,Y/cm; 18 - the same in a 60- mm. tube; 18 a p0 a 4 mm Hg,

1 600 a; 11 t,
microseconds, 12 0
T e, K? 13 E, V/cm.
.14 p0-4 UM PT. cT.. 1-200
..Jg Tomes T ORO AHaMOTPOM
14

r,, K
E. SAM NX
484tt)
I
6M
-
&q.. 4

so
25000
8 (A!1
85 26000 8
120 26000. 8
IS5 29000 8
172 21000 6 20
181 14000 5 90
1 25000 MI

Card 8/8 190
10000
4 ISO
200D0
=:I

193
9600
4 ". ,

207 9700 4

395o2,,
S/056j62/043/002/053/053
'? 0 B108/B102
illekseyevskiy, N. Ye.j Tegorov, V. S., Karatens, G. E.t
Xazak, B. N.
TITLE; Galvanoma,-,netic pi~operties of transition metal single cry5tals
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki,. V. 43,
no. 2(a), 1962, 731-733
TEXT:- The change in'resistivity of transition metal single crystals
Pd,'Re, Mo) with the change in field strength of a strong magnetic ffiiald
UP to some 150 koo) was studied at 4.20K. The results show that Pd t.nd
~
Re have open Fermi surfacep. The Fermi surface of ?cr is similar to that
of Pt. The square-law increase of resistivity of Mo with increasing
magnetic field strength is indicative of a closed Fermi surface. There
art: 2 figures and I table.
ASSOCIATION: Institut fizicheskikh problem Aka-demii nauk SSSR
(Institute of Physical Problems of the Academy of Scien,,,.es
USSR)
Card 1/2

1
Galvanomagnetic properties of ...
SUB'I'.ITTED: June 8, 1962
0
3/056/62/043/002/053/053
BIOS/BI02
41-

S/129/63/000/001/008/0-17
E073/035
AUTHORS: Fomenko, G.D., Engineer Y &9yo-y V.S. and Androyeva
A.G., Candidat,es of TecL4cal Sciences
igation of the contact strength of case-hardened
TITLE: Invest
stool, 12-",~3;, (12KhN3A)
PERIODICAL; Metallovedeniye* i tormi!ctloaka'ya obrabotka, Patallov.,
no. 1, 1963, 23 .- 25
TEAM The effedt of carbon cone _Mtration in the case-hardened'
14yer on the contact'- and fatigue-strength was,investigated on
so ecimens carburized'(for 4 h) to a depth.,of 1-2 mm in a 15-litre
capacity laboratory furnace. Sintin was used as a carburizer
and the carbon content of the surface layer was about 0.75c.. if
5 drops/min were applied and about 1.3% if,,20 drops/min wbre
applied. After cooling in air, the specimens were heated in a
0 0
saft,bath to 780-800 C, oil-quenched, cooled to -70 C and
tompered at 150 - 170 OC. The surface was then ground-off to a
as was '61-63 HRC. Th o
depth of 0#1 mm; the surface hardne
:,,specimens were made to rotate between clamping rings to !simulate
~'the loading conditions of gear teeth; thoy.ifere subjected during
Card 1/2

s/i2
Investigation of .... E073/E335
rotation to contact stress6s varying along tHe circumference,,
the maximum being 700 llcg,'As well as to abort 2% slip. The
maximum contact strength,-' about 3 350 lcg/cm " was obtained wi.th a
1.10% C content of the surAce layer. In thl; case, the stru:Aure
of the surface zone was acicular martenisitaiwith fine carbid.-i
figue strength indr
plates and grains. The fa eased almost lkLearly
2
from abort 68 kg/mm for W6111; C of the surface layer to ,bout
75 kg/mm -for 0.911. C and'rimained almost constant,with increasing,
C contents Therefore, to achieve the highest fatigue and contact.
strongth the surface layer,of case-hardenod steel should be flat-.
urated to contain 1
Card 2/2
7:

ACCESNION Nit: AP4000479 13/0051/63/015/006/083~/0840
AUM1011: Yegorov,V.S.; Koziov,Yu.G.; Shulchtin,A.M._
TITLU: Concentrations of excited atoms in pulse dischakgos in a mixture of tielium
and noon
kna.. Optilta I spoictroskopiya, v.15, no.G,,1063, 839-840
-'TOPIC YAGS: inert gas excitation, energy transfer, pulse discharge - , 1o% al popu-
lation, helium, noon, optical pumping
AiSTRACT: Earlier two of the authors (A.M.Shukhtin and V.S.Yogorov, Vestnil: LGU,
No.3,2149 and Opt.i spolctro.9,794,1900) studied the population of the uppor levels
of neon at different stages of a pulse discharge. The present paper gives some of
the results of a similar investigation, al~o'by the Rozhdostvenskiy method of hooks
of pulse discharges in mixtures of noon and helium. The discharges were ri.-alized
In a 15-mm diameter, 60-cm, long tuba.' It.was found that the introduction of He
results in increase of the peak concentration of No in the 2pbsXlistate; a-. the
same time the population of the ls2s3SA of He is reduced. The Inferred lo,tol popu-
lations for No and He separately at 0. and 4 mm lig pressure and in mixturo with
Card 1/2

ACC.NR-. AP4009479
the same pressure ratio are given in a table, The increase in the rolative number
of excited No atoms is attributed to energy transfer incident to elastic and inol-
astic collisions of the Ito atoms with the other particles of the decaying plasma.
The various possible energy transfer mechanisms are discussed. It is concluded
that a number of these mechanisms may play a significant role. Orig.art.haa: 8
formulas, 1 table and I figure.
ASSOCIATION: none
SUBMIMD: 25May63 DATZ ACQ.- 03Jan64 EXCL: 00
SUB CODEP PH NR REP SOV% 001 OTHER: 004
Card 2/2

1 17635-63 ErfT(1)/~WP(q)/EWT(m)/ S/056/63/044/003/048/0"
BD5 AFFFC/ASD IJP(C) JbIJG &
~AUTHOM Alokseyovskiyp No Yee YegorovA Ve So-, and Kazak,'B. 14.
.-TITLEs ~,GalvanomaMetio propertie cf rhenium
PERIODIOAL: Zhurnal oksperimentallnoy i takhnichookoy fiziki, v# 44# no@ 3t
1963, 1116-1119
TEXTs -The authors and 0, E. Karstens reported earlier (Ref. It ZhETF, 43, 73~#
1962) that rhonium has an open Fermi surface. To study the topological typo o
this surface the authors investigotod the galvanoM3VI13tiC properties of the Movo-
of pure rhanium having different ori 'ontation of crystallographic axes
with respect to the axis of the sample. They co-nclude-that the Re Fermi surfaia
consists of two independent parts, the vacancy surface and electron surface. iron
the measurements of the Fall affect it follows that the eloctronic surface Is ibe
open one with cpenings parallel* to the hexagonal axis and also in the dirocti(n
within the hexago nal plane. Thera are 3 figures and 1 table.
ASSOCIATIONs Institut fizichankikh problem Akadomii nauk SSSR (Inetitute for
SUNITMi Dec=bar 26j 1902
Card 1/1_
q1 _i-5
li_~' Vi3'

)/BDS AFFIC/A31) JD/JG
Ir 17218-63 T4P(q)/&,T(n T
---,.;-,ACCESSION NR: AP3005301 S/0056/63/045/002/0388/-:391
ADTHORS: -Alekseyevskiy, Ye. 1Yegorov, V. S.
'.TITLE: operties of beEyllium
Gaivanomagnetic PX r1
Z,
_~-(SOU~CE.- Zhur. eksper. i teoret. fiz., v. 45,, no. 2, 1963, 388-341
9;it-i-vano.macrne-ti-c-p-r-op-ert~
ABSTRACT: 0 f single- bexyl
-The variation f the resistance o 2ELstal
lium was.investigated in magnetic fields of higher intensity tha .1
1,hitherto~employed,. up to 50000 Oersted. In fields up to,35000
i':Oersted,;the increase in resistance in the field was found to be
fzcloseto,_quadratic for all-directions of the magnetic field, int icat-~
thatberyllium behaves like A metal with a closed Feimi suri aicd, J,,
but in'fields close to 50000 Oersted the dependence*of the resittancA
on the fields seems to saturate in*the (1000) direction.. This i,,an
be attributed-to the appearance.of open trajectories along the
i'Card 1/3
777

L ~17218-6.3
J.ACCESSiONijNR:. AP3005301
~:hexagonal axis. -The Fermi -surface of beryllium consists theref6ill:,I.
~of two parts --- hole and',electron --.with volumes that a
re equal,
to 35000 Oe,-above which open directions appear in the Fermi sur-,
_face. "The authors are ~ratefui to Academician P .L. KaRitsa for
1nterest inithe work and o G. E. Karstens, for help in the pre,j
tion of the
specimens and the determination of their orientatiorf~
,
IWe take thid o__ ortunity to-thank B.
G. Lazarev, who furnished th
pp
7
initial beryllium crystallites." r
6R~ t. has 3 figures and
table.

ASSOCIATION.-! Institut fizi6heskikh problem Akadem:H nauk SSSR
(I-nstitut' of Ph)Lsics Problems, Academy of Sciences'-SSSR)
e
__
:SUBMITTED! 16May63 DATE ACQ: 06Sep63 ENCL: 01!

-SUB' CODE: PIH NO REF.SOV: 004 OTHER.- JI

2/3
Card

ALEKSEYEVSKIY, N.Ye.; YWOROV9 V.S.
Measuring the resistance of single crystals,ln a pulsed magne,Ac
field. Zhur. eksp. i teor. fiz. 45 no.3t448-454 S 163.
(MBA 16:10)
1. Institut, fizicheskikh problem AN SSSR.
(crystals-Gaivanomagnetic Oropertios)
(Magnetic fields)
_U
S
P
_n"
~.tL-,S4

0M,
~g Ig ipx;i M ENER
1;

gf

e1!

-ZO

pi~axi.iwuw. conce ttr at ion of the exci-ted he I I tim- atrwmu 4r Is in-I a fl, e
r", ~ at of t -,e di S~hilrqp ir ; h,- 'h6-1 i um-ne-r, mi Y+- - r-P -irf- qma
with thit wncentrations of the atoms of
the-neon and coq
-i i nm ~~ rthn ~ r -es.4 rtj o
ASSOCTATI(M-4: none

- - - --= -- --- -
YEGOROV, V.S.; KOZLOV, YU.G.; SlIUKIMPI, A.M.
Concentrations of excited atoms in a pulse
helimm. Opt. i spektr. 17 no.1:154-156 i1 ',., ". (!,-~~JkA I
M~

FUTOYIIIN, N.I.
Thienyl aldehyde and its derivatives. 7,hur. (b. ~hlrn. 3 ro.12:
4084-4086 D 164 18tl)
1. Kuybyshevskiy politelzbnichoskiy institut.

REA

A . . . . . .. . . . . .

'
UY!"

Lg,

Arl.-

4; 6 AXI

E',,IT(m)/EPF(c)/i;WP(t)/r-,!;[P(b) IJP(c). JD/jG
NR: AP5016282 U/0386/65/ool/oo~/oc'i-1/0036'
---AUTHORS: AlekseyevskiX,_E. Ye.; --Yegorov V. S.
TITLE: Investigation of the galvanomagnetic properties of tra'
MsitlQ
~metalz in strong magnetic fields
V,
SOURCE., Zhurnal eicsperimentallnoy i tekhnicheskoy fiziki. Pifr1mav
Iredaktsiyu, Prilozheniye, v. 1, no. 5, 1965, 31-36
;TOPIC TAGS: magnetoresistance, vanadium titanium, t
_Lu ~stenL C-hrom-14-ml
igalvanomagnetic effect 6 tr-
ABSTRACT: The autborz present the results of measuremento of ;;be
igalvanomagnetic properties of W, V,.Ti, and Cr, carrIod out in large
:effoctive magnetic fields. The measurements were made with apparatus
;described earlier (ZbETF v. 45, 4118, 1963), on single crystals several
!millimeters long,with transverse dimensions approximately 0-5-0.3 mm-,---.
'.The use of the apparatus has made it possible to make measurem~-nts on!
~:transition metals in which the ratio of the resistance at roomi temper-',;
mature to the resistance at liquid helium temperature was relat:!.vely
Card
I- m m
777777W7

----------------- ----
L 3394-66
:!ACCESSION NRi AP5016282
~Gmall (130 -- 175). In spite of' this low ratio, the maximum val ',ues of
7~tbe effective fields were q"ite high, amounting to -.2 x 10 Vie
iresults are illustrated in Figa. I and 2 of the Enclosure. Whe::;. ana
Jyzed from the point cf view of modern ideas concerning the beh~!Vio..
j,
!of electrons in metals, the results indicate that vanadium and :!itan-i
lium have closed Fermi 3Urfaces and chromium has an open Fermi siWace.~
"bange
-rungaten, also has a closed surface, but Ite magnetoresistance
,is large, whereas for Ti and V the change Is small. Orig. art. !has:
ti2 figures.
;!ASSOCIATION: Institut fizicbeskikh problem-im. S. I. Vavilova
1Akademii nauk SSSR (Institute of Physics Problems AN SSS-R)
SUBMITTED: 23Apr65 ENCL: 02- SUB CODE:
.:NR REF SOV* 001 OTHER-- 002
Card 2/4

L 3394-66
ACCESSION IIRt AM16282 ENCLOSURE: 01
0
-,Y
Fig. 1. A and B Angular distributions
of the magnetoresiotance of aing;'Le-
cryatal Cr at 44 and 74 k0c, reapectively#
C and D - Magnetorsistance in the maximum
and in the minimum, respectively. The
scale for curves A and B if; on Vie right,~
and for C and D on the left.
3ff

~331,a3 oc,-wring in a disintegmting Pl&a:4&
foired in a, pul--3-n d-ig~~,harga through a-n lie No mixture during
generation. Opt. i sv3lktt~- 19 no-43T,'9'72.A. AP 165, (MIRA 18:8)

Its; t.4"i-T
Ut
3o56-46 _Eirl(i JJP(c) GO
iACCESSION NR: AP5021274 UR/0020/65/163/005/1121/11:1!3
iAUT110R: Alakoeyevskiy, N, Ye,; DubrovLn. A. V.; Yegorov, V9 so
'ITITLE: Pulse methods of investigating the a .uperconducting proLqr,i
!of alloys
SOURCE: AN SSSR. Doklady, v. 163. no. 5. 1965. 1121-1123
TOPIC TAGS: superconductivity, superconducting alloy. magnetic fl.eld'.'
measurement.
IABSTRACTI Two pulse methodo for mcaaurLng the critical magnetic
Ifield intensity of superconducting alloy wires are described. MI.-
first is deal ned for measurements at comparatively small current
idensitics (10 amp/cm2). An external magnetic field of 150 koe il
in a solenoid (ID 0.5 cm) by means of a discharge of a ba;::k
of capacitors (800 lif, 300 v); buildup time to maximum current is
4 mace. The winding of the solenoid is pure Al wire 0.3 mm in dl--
lameter, with P10004. 2r.,, - 300 and resistance at liquid helium tem.,
pevature 6f 2,;5 a~m.- voltage- prop-ort16ftal tv the turrent: in-
-Card J.
o

L 3056-66,
=ESSION NR: AP5021274
0
the coil, and consequently tothe magnetic fields in passed to t1tin
horizontal plate of an oscilloscope, and simultaneous scanning oU.
the magnetic-field is effected. A-given deviation of the beam from
the horizontal corresponds to a given field intensity. The irkstl;lnt~
of disruption of superconductivity of the sample is registered by
the appearance of a resistance between the potential electrodes cif
the sample. To record the resistance, a d-c measuring current
(several dozen milliamperes, 35kc) is passed through the sample.,
,The signal from the potential electrodes and a signal..compensatijig.
the measuring current are fed in -series to a tuned amplifie:!,
When the critical field intensity is reached, the resistance appnars.;
the compensating s.ignal is blocked out, and a curve of the trans:!,tion,
to the normal state appears on the scope, The second method is
designed for higher current densities in a stationary field. A ohortl
current pulse growing linearly with time is pnssed-through the stimples~
and a two-beam oscilloscope registers curves of current intensiv, andil-1--_
voltage at the potential outputs of the sample. Buildup time of"the
i
ivoltage pulses is adjustable from I msec to I min. Pulves from I~he
Igenerator pass to-the feed-circuit of the sample from the output of
a three~-otage transistorized amplifier (gains 105)# and a voltagii I
_-2/3-

~ 30,r'6_66
A
CCESSIOH NR: AP5021274
I'D

I proportional to the current intensi'ty is fed to one input of the
scopa, The voltage from the potential outputs of the sample are f~a d
to the second input, At the instant of disruption of ouporconduct';Lvity
.I
. a voltage pulse appears on the scope. The position of this pulse
l
relative to the current-intensity pulse determines the current int;en-
aity of the sample. The two pulse devices can be mated by subctillut-1
ing a current pulse from the generator for the d-c measuring currj;nt.~.-
I This pulse is fed to one input of the scope, while the second tnpt.ft
handles the unbalanced signal registering the appearance of the
resistance. The horizontal sweep is effected by a voltage proporl:.ional.
to the magnetic field. Orig* art. has: 2 figures. E PWI:
ASSOCIATION: Institut fizicheskikh problem im. S. 1.~Vavilova
Akademiinauk SSSR (Institute of Physical Problems, Academy of Sc Lencepj,
IS;SR)

SUBMITTED: 15Jan65 ENCL: 00 SUB CODES 1ZC
"(-OTHERS L.,000 ATD FIRESsl
NO REP S.OV0. 001
.
T3
Lqurj__3

ALEKSEYEVSKI'f, N.Ye..,;. YEGOROV, V.S.
Galvanomagnetic properties of tranaJtlon metals In high
magnetic fields. Fiat. v red. Zhur. ekepar, i teor. fiz, 1
no.501-36 Ja 165. (MIRA 18t11)
1, Institut fiziebeakikh problem imeni Vavilova AN SSSR.
Submitted April 23, 1965.

ACC NR, Awoo4136 SOURCE CODE: UR/
~-~UIMOR: Yegorov, V. S.; Skrebov,, V. ?1.; 6hukhtin, A. M.'
i ORG; none
TITLE: Concentrations of excited atoms in pulsed discharges in mercury vapor
SOURCE: Optika i splAtroskopiyal v. 22) no. lp 1967~ 9-13
1
TOM TAGS: mercury,, electric dischargep atomic speqtrum, excitation energy,, level
population.. radiativa recombination
ABSTRACT: Using an iixperimental vatup described earlier (Opt, i spektr. v. 2. 543#
1957) the authors usi-.d the Rozhdes-tyenskiy hook methdd to measure the populativas of
the first excited le,rels of mercury atoms 6s6p3,Po 1,~ in different phases of a short-
led near the visible triplet of
duration current pul,ie. The hooks were photogrWp
mercury (7r'sl - 63po 3.,,2) and also near certain lines lying in the near ultraviolet
region of the spectram and corresponding to the transitii)ns 63D1 2 3 - 63p0 2. 2. The
pressure range was'0.01 - 1 mm Hg,, with the most complete data o'n the conden'tr'ations
of the excited atoms obtained at 0.2, 0.5, and I mm. Hg. The population of the first
excited levels first. increases w:V,,,h the current and the discharge, reaches a certain
maximum value ahead of the maximwa of the current, and then decreases on approaching
the trailing edge of the pulse. At the instant of'termination of the discharg(!, a
sharp growth in the concentration of the atoms of mercury at the first excitedi-states
is observed. The resultant maxim= value of the concentration of atoms is muc~-k
C!nrd 1/2 UDC: 537-523/.527: 54'.';.49

NRt AP7004136
larger than the corresponding value in the discharge itself, after which, with in-
creasing'distance from the trailing edge of the pulse, the population of the levels
decreases more or less rapidly. The results are interpreted on the basis of drta
previously obtained by the authors (Opt. i spekbr. v; 2D, 382, 1966) regarding~the
mercury vapor density and the density of the charged particles in different plu,~-.es of
a pulsed discharge. A numerical estimate (-10-10 cm-1/sec) is obtained for thellcoef-
ficient of volume recombination at the typical values of the other parameters v.,f the
experiment. In addition to measurements by the hook method, the concentration f
the charged particlvs, the temperatures of the electron gast and the time vari.10ion
of the luminescence of many spectral lines of the mercury vere also measured. F%ese
observations have shown that although the population" of the different excited :Ig'evels
of mercury in a decaving discharge plasma is determihed essentially by impact-
radiative recombination,, there are other mechanisma influencing the population of at
least some of the levels. The relative i6portance of these processes calls for fur-
ther study. Orig. art. has: 3 figures and 2 formilas.
SUB CODE: 20/. SUBM DATEs 19Au-651 oraG Ym: too4/ oTH mw: oo4
Card 2/2
`0 11V__'.-1,!

ACCESSION NR: AP4020246 S/0129/64/000/003/0033/0037
AUTHOR: YeSorov, V. S.; Andreyeva, A. G.; Fomanko, 0, D.
TITLE: Gas cyaniding and carburizing of stainless Kbl7N2-(91268) steel
SOURCE: Metallovedeniye i termicheskaya obrabotka metallov, no. 3, 1964. 33-37,
and insert facing p. 41
TOPIC TAGS: diffusion layer, hardness, carburization, cyanidation, sub zero
treatment, 1(hl7N2 steel, stainless steel
ABSTRACT: The authors investigated the possibility of obtaining a thin layer
with a hardness higher than Rockwell hardness 58. -For that purpose,steel Khl7NZ
specimens were cyanided in a 10-liter laboratory muffle furnace into which pyro-
benzol and ammonia were introduced. Air cooling was followed by oil quenching
fro.m 1020 C. Finally, the specimens were treated at -70 C and.subsequently
tempered at -160 C. Hardness was highest after treatment at 3700-750 C.* The zone
with a hardness of H.A-700 was 0,075-0.12 mm deep. 40-45 cm /min a=onia and 15
to 18 drops pyrobenzol per minute incroduced into the furnace were found to
enhance hardness which reached H,,.-1040 without changing the depth of the active
Card. 1/2

ACCESSION NR: AP4020246
zone which was 0.5 = deep after a six-hour holding period. Sub-zero treatment
prior to high-temperature tempering did not affect the amount of residual
austenite in the layer and the temper hardness. The authors recommend the
application of sub-zero treatment at temperatures of -70 C or -120 C for case-
hardened Khl7N-2 steel parts. If the sub-zero treatment is applied for the
purpose of enhancing hardness characieristics of the carburized layer, the cooling
media should have a temperature of -70 C. Volumetric changes are effectively
prevented by the application of a sub-zero treatment at -120 C. Orig. art.
has; 9 figures.
ASSOCIATION: None
SULMITTED: 00 DATE ACQ: 3lMar64 ENCL: 00
SUB CODE: MM No REF SOV: 003 OMR.- 000
Card 2/2

ACCESSION NR:o AP4031138 S/0056/64/046/004/1205/1207
Alsksayevskiy, N. Ye.1 Yegorov, V. S.'
AUTHORSs
TITLE: Concerning magnetic breakdown in berylliurl
SOURCE: Zh. ekspjr. i teor. fiz., v. 46, no. 4, 1964, 1205-1207
TOPIC TAGS: beryllium, galvanomagnoticef:Bect, magnetic.field, re-
'"Slativity, magnetic breakdown
ABSTRACT: This-is a continuation of work.reported earlier (ZhETF
v. 45, 388, 1963) and aimed at checking the change in the variation
j,of resistance with the magnetic field above 50 kOe. The- measure-
ments were made on a single crystal of 1~eryllium in difEe~:ent effec-
tive fields at temperatures 4.2 and 7SX. Pulsed magnetic fields *
were used ~n a rp9asurement procedure Whichyas also deocribed earlier
(ZhETF 45, 448, 1963). The results are in good agreement with those
ob#ained earlier,, in that the change in thi~.law of resistance'rise
Card, 1/4

ACCESSION NR: AP4031138
I occurs at the sa6e value of the magneticifield (45 kOe at 4-2K and
40--50 koe at 78K). This behavior of resistance is attributed again
to magnetic breakdown. it is emphasizedi however, that this inter-
pretation of thd,iresults is only qualitative and cannot be used as
yet for quantitative estimates. Orig. art.~has; 2 figureis.
ASSOCIATION: InAtitut fizicheskikh problem AN SSSR (Institute of
Physics Problems AN SSSRY
SUBMITTED: 050ct63 DATE ACQ: 07May64* ENCL: 02
SUB CODE: EM, S~ NR REP SOV: 003 OT'HER: 002
Card
p, -v~ - n

ACCESSION NR. AP4031138
ENCLOSURE: 01
Angular diagrams showing the va-
riation of the resistance of be-
ryllium in a transverse magnetic
.-field. The hexagonal axis is per-
'pendicular to the current. H is
perpendicular to the hexagonal
axiu in the direction of the arrow
Cur~el (obtained in stationary
field) - T -_ 4. 2K, H - 5 k0e.
2 - 78K and 44 kOe; 3 - 4. 2K a:nd
34,kOe; -4 78K and 150 kOe
V, TMIT ~,T.

ACCES~10214 UR: API..0311138 ENCILOSURE 02

A/

Dependence of change in resist ance on the magnetic field when the
field is perpendicular to the (00011 axis. Curves T 4 2K, 2 `- 78K
l
;
(a, linear a;ith
icj
scale, b log
Card,.4/4

R"J,

Y7,
the zrrtact cf -,f* Fczf-rtiomeilters.
P.Hborost-Irclanio no.6.-19 -'e 16i. OMIRA 18!7)
Zz

Ila.
051 1-1,
IJ,

TUSUMICH, O.Ye.; YEGOROV, V.V.
Standardization of operations for preparing mixtures,
Mashinostroitell no.1209-40 D .163. (MIRA .17:1)
Y,

SKAfOV-.A-. I-.-, -dot s-ent -dot se n-t
-,kamd I da t-t-ekhn Ic heolf c ik li-
nauk, retsenzent; YRGOROV V.V. (deceased], dotasat, kandidat tekh-
nicheakikh nauk, retsenzenf-;'VIMODAROV, S.F., inzhener, retsenzent;
MAYKOPAR, M.B., doteent, kandidat takhnicheskikh nauk, nauchnyy re-
daktor; KOPrZVSKIY, D.Ya., redaktor; SUSWV, P.V., redaktor literatu-
ry po metalloobrabatyvayushchim professiyam, Inzhener; RAKOV, S.I.,
tekhnicheskiy redaktor.
(Problems in electrical engineering, electrical measurement, electric
machinery, and electrical equipment] Zadachnik po elektrotekhnike,
elektrichookim lzmareniiam, elektrichookim maohinam i elektrooboru-
doyanliu. Moskva, Vaea.uchebno-pedagog. izd-vo Trudreservisdat, 1954.
413 P. (MLRA ?:1l)
(Ilectric angineering-Problems, exercises, etc.)
4~- r

II V_T y I-
PRINTSEV, A.A., inzhener; PETRDV, V.Ta.; TZWRD.,V,,,j4V.; L&MMY, I.A.,
, _ iAe
inzhaner: KONSTANTINOV, B.A., kandida khnichemkM mauk.
Rates for electric power* Fromoenerg. 12 no.1:18-22 Ja 157.
(MLRA 10:2)
1. Inergoebyt'Laningradekoy alektroenergetichookoy mistemy
(for Printsev, Petrov) 2. Xnergoebyt Estonskoy alaktroenergetichaskoy
sist6my (for Yegorov) 3. Laningradskiy piyovarenny7 sayod
(for Lamanov) 4. Laningradakiy inzhenerno-takhnichookiy Inatitut
(for Konstantinov).
(Electric utilities--Rates)
Mr-
"4 7,
zi

MIKHALEVSKIYo A.1.1 STD4PNLrVBKTY, N.M. [doceased]j IkOOROVo V.V.9 dotsenti
SALENKOy S*V-.t red.; DEWATKOV, V,F,, red,
(Railroad car.P; structural features end repair techniques] VagorWj
ustroistvo i tekhnika remonta. Moskva, Goo. transp zhel-dor. izd-
Vot 1945. 814 P. ?MIRA 14t 8)
fiailroad,o-Cars)
V.

RKNOVA,
_kQROV, Vasiliy Vasillyevich; BACHININ, G.I., red.; YE
Md .
(Liberia after the Second World War, 1945-1962] Liberiia
posle Vtoroi Mirovoi voiny; 1945-1962 gg. Moskva, Izd-vo
IMO, 1963. 165 P. (MIRA 16:10)
(Liberia-Economic conditions)
(Liberia-Foreign relations)

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y .. V
Mbr., Soils Institute.. Aced. Sci. -1947-
"New Date on the Lower Levels of the Caspian Sea In Ue Past,n Dok. All, 58,
No. 8, 1947.

7-
The chiracter of I In the mloaralitation o( ground -
eoU moisture under I".. It'lons of the Solonchak vMcess in
the delta depression at the 844. V. V. 11
';~otcjv Pofh-
r(lerdrPtic (Pedology) IOSO, Q(H0L=-PMZift*txitul
watcrs of the arem aclMningsea ilcifatarco(rivrr and sca I
orijill. F. traers tile changes in the compri. (A the
Kfound * atersA t he "I areas bamd an the chein. "4 of
the wAters in the rivvi at different points. of the va water,
inirshes in the area. wells. and comiln. 4 parent matrriAl
alul geolock Ofl& (I this. .14. ]oat

YEE V. V
Dark mosaaw wils of alluvial valloys and their &Vo.
prodwavity charactortow. V, l -krowdeft 4
1931. SN"CA.-These "I IYOC Alf,"T54. arc (how
that are vib*t to x4liniu-tio". This Is especially true for
the delta regions and even above tbcse where thr hilgb d4upt
suce brincs la fine sediusent lato temporary rivtr ch4nfwlq.
I *' aditne, at the" "Is, R. gives them. slata gas she
U~ VO'~%.*d humus (011(ent as well as C(h. f1cch. Cl, 600
ca. 111g. ana Na In a water ext. S. Joffe