"SCIENTIFIC ABSTRACT LYAPICHEV, P.A. - LYAPIN, A.G."

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001031020018-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Sequence Number: 18
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

- LYAPICT ~11 V, -P. A. - Cand. Tech. Sci.
Dis,sertation: "Basic T~jprzq of Run-off Ref,uliAlnn for a Several-Year Period." Mo3scow
Order of Lenin Power Enf,fineering Init imeril V. M. Yoloto-i, 10 Oct 47.
SO: Vechernvaya Mloskya, Oct, 1947 (Project #17836)

0
1. LYVI * 11"! L' - V, P. .1.
2. USSR (600)
4. Technologi
7. 'Water power regime in a hydroelectric oower station with amnual regulation of flow.
I
Moskva
, Gosenergoizdat, 1952.
9. Monthly List of Russian Accessions, Library of Congress, April -1953. Unclassified.

LYAPICFW Petr Andreyevich KAPLINSKIY,S.V., kandidnt tekhnicheskikh
nat r. dAkt or; BARSOV,M.Y., redaktor; MLTVRW,L.Yq., teani-
cheskiy redaktor
[Method of controlling river flow] Metodika regulirovaniia. rech-
nogo stoka. Moskva, Gos.izd-vo lit-ry po Btroit. i arkhitekture,
1955. 389 P. (MIRA 9:2)
(Rivers--Regulation)

SIDORDY, A.A., kandidat tekbnicheakikh nauk, redaktor; BLIZWAK, Ye.T.
doktor tekhnicheakikh nm3 , professor; OLESHKEVICH, L.V., kandi-
dat tekhnicbeekikh rail , doteent; AKUTIN, A.R., doktor tekhai-
cheskikh nauk, professor; BMWINSKIY, A.R., doktor tekhnicheskikh
nauk, professor; GRISHIN, K.H., doktor tekhnichookikh nauk, pro-
foosor; DZHUNKOVSKIY. N.N., doktor tekhnlehkeskikh nauk, professor;
ZHM6GHKIN, B.H.. laureat Stalinskoy prenii, doktor tekhnicheakikh
nauk, professor; MIKAYLOV, K.A., doktor tekhnicheakikh nauk, pro-
fessor; NICHIPEROVICH, A.A., doktor tekhnicbeekikh nauk. professor;
NESDUM, F.Ta., doktor tekhnicheakikh nauk; NBDRIGA. V.P., kan
didat tekbnicheskikh nauk; SAMNOV, P.V.. inzhener; LATTSHMOV
A.M., kandidat tekbnicbeskikb riauk,dotsent, redaktor; MUROMOV,
V.S., kandidat tekhnicheakikh nan , dotsent, redaktor; BARSOV,
M.V., inzbener, redaktor; MNSTIM, V.A., kandidat tekhnicheakikh
nauk, redaktor; LIPKIED, H.V., kandidat tekhaichesklkh nauk,
redaktor; LYAPICHEV, P.A., kandidat tePhnicbeekikh nauk, redaktor;
P.BPOV, I.M.- [Knnicheakikh asuk, dotsent, redaktor;
IN, V.P., insbener, redaktor; M3DV3DlV. L.Ya., tekhnichaskiy
redaktor.
[Wdraulic englneerlng handbook]Spravochnik po, gidrotekbnike,
Moskva, GosAzd-vo lit-ry, po utrolt. i arkbit.1955. 828 p.
(MIRA 8:10)
1. Moscow. V9esoyuzWy usuchno-issladovatellskiy institut
vodoenabzhenlya, kanalizateii,, --idrotekhnicheakikh soorazhegiy
i inzbenernrT gldrngemlogii. 2. ZasluzhezWy deyatell mu i i
(Continued on next card)

SIIY)ROV, A.A., kandidat tekhnicheskikh nauk, redaktor,and otberm... (Card 2)
Ellydraulic engineering handbook]Spravochnik to gidrotelchnike,
Moskva Gos,izd-vo lit-ry, po stroit i arkbit. 1955. 828 p.
(Card 25 (MLILk 8: 10)
2. ZasluzheMy deyatell nauki I tekhniki RSFSR(for Blionyak)
3.-Deystvitellmy chlen Akademli nauk AzSSR(for Milckylov)
(Elydraulic engineering)

LYAPICHEV, Ye.G., starshiy elektromakhanik
This yields good results. Avtom., telem. i sviaz, 4 no. 12:26
D 160. (MIRA 14:1)
1. Kotallnikovskaya distantsiya signalizatsii i avyazi Severo-
i KaAmzekoy dorogi.
i - (Electric lines--Poles)
--;;, - -

LYAPICHEV, Ye.G.,, starshiy elektromakhaaik
------------------------
Change in the design of a welding clamp. Avtoa.- telem,i sviaz~
6 no.4;39 AP 262. 0141PA 15t4)
1. Kotellnikovskaya distantaiya signalizatsil, i svyazi
Severo.,Kavkazakoy dorogi.
(Welding-Equipment and supplies)

WT 'T' -jp(c~ jpl
o46 X /L*
ACC NRz
AP6010099
SOURCE CODE: UR/0129/66/C,00/003/0060/0062
/V )i
AUTHORS: Arkovenko, G. I.; G37,ekov, N. A.; Lyapicheva) N, F,; Sazonovaj T, u,
ORG: none
TITLE: Relaxation.~6f tensions in titanium alloys, as a function of.hot deformation
conditigns . j -t) -1-1 1 ~/
SOURCE: Metallovedeniye I termicheskaya obrabotka metallovp no. 3, 1966) 60-62
TOPIC TAGS: titanium alloy, metal grain structure, metal deformation / VT3-1
titanium alloy, VT-2J+ titanium alloy
ABSTRACT: The influence of temperatureend degree f deformation on the relaxation
of tensions in the titanium alloys VT141and VT3-llwoas studied. The chemica
'I composi-
tion, the usual mechanical proporties, tho grain s
ize and grain structurej$and the
microstructure of the alloys were investigated. The exporimental results'are pre-
sented in graphs and tables (see Fig. 1). It was found that the deformation of
alloys VT3-1 and VT-14 specimens in tho P -region leads to a formation of coarse
grains and to a decrease in the relaxation stability. Lowering tho daformation tom-
parature to the ('A + P )-region yields, upon deformation, a more homogeneous s tx%cture
and leads to an increase in the relaxational stability. The alloy VT14 Is more
sensitive to hot deformations than is alloy VT3-1.
1/2
UDC: C-69.245:539.371

L o4631-67
[-A'CC NR: AP6010099
Fig. 1. Relaxation of tensions (for
cylindrical specimens) at 100C and
C-0 = 0.65UO.2 for VT3-1 and
0.70 0'0.2' for VTIJ+ as a function of
the testing time, heating temperature
during forging, and degree of deforma-
tion during final heating stage: dashed
curve allay VT3-1; solid curve - alloy
Orig. art. has: 2 tables and 3 graphs.
SUB CODE: l1/ SUBM DATE: none
13/
11~ - M

14 .
12
10
1
8. >0
-
6
.
4

tesiting-. time
awm
rd 2/2

LAKHINO P LYAPIDEVSKIYY O.P. [!Aapidevs'W,,, O.P.1; VETaov, O.P. [Vietrov,
O:vp: I -- -
Methodology of the graphic recording of the quantity of biological
fluids. Fiziol.zhur. [Ukr.] 10 no.1,2558-560 Jl--Ag .164-
(MIRA 18:11)
1, Ins titut fiziologii im. Bogomoll tea AN WzSSR, Klyev.

LYAPIDU,VSKIY. S.S.; SIDME'Ll, A.G.
Stammering. Med.Bestra 18 no.9:30-35 S '59. (MM 12.':Ll)
1. Iz Goaudaratvennogo nauchno-iseledavatelolkofo instituta
ukha, gorla i nose, Ifini8terstva zdravookhraneniya lib'PSI1, Moskva.
(STAMERING)

PRAVDINA, O.V.; MKLMOVA. L.V.,* IVANOVSKAYA, V.A.; TAPTAPOYA, S.I.;
ALKAZOVA, A.I.; LTAPIIM'MIT, S.S., red.; NOVIKOV, Ya.A., red.;
DRANNIKOVA, M.S. ;--V6Rb-n-.r-e-cT.-
[Essays on the pathology of speech and of the voice] Ocherki po
patologil rechi i golosa. Pod red. S.B.Liapidevokogo. Moskva,
Gon.uchebno-pedagog.Izd-vo H-va proov.RVSR. No.l. 1960. 148 p.
(MIRA 13:12)
1. Moscow. Moskovskiy gosudarstvennyy pedagogicheskiy institut.
(Speech, Disorders of)

ZEYEMAN, Miloslav[Seeman Miloslav] prof doktor med. nauk;
SOKOLOVA, Ye.o.ttranslatori; TRUT'NEV, V.K., zasl. deyatell
nauki, prof. (deceased], red.; LYLPJJA_V~KjY, _S,.S._' dots.,
red.; YAKOBSON, I.S., red.; ROMANOVA, Z.A., tekhn. red.
[Speech disorders in children] Rasstroistva rechi v detskom
vozraste. Pod red. i s predisl. V.K.Tintheva i S.S.
Liapidevskogo. Moskva, Medgiz, 1962. 298 p. (MIRA 16:6)
Translated from the Czech.
(SPEECHj DISORDERS OF) (CHILDREN--DISEASES)

LYRND-VS-Kly V K: FD 412
USSR/Physics Ph6toconductivity
Card 1/1
Author : Krongaus, A. N., and Lyapidevskiy, V. K.
Title : Negative photoconductivity of cuprite
Periodical : Zhur. eksp. i teor. fiz. 26J. 115-119, Jan 1954
Abstract : Investigate the influence of an electric field and intensity of light on
the photoconductivity of cuprite. Establish the presence in cuprite of
both negative and positive photoconductivity. For increasing light in-
tensity at given voltage in a crystal the negative photoconductivity
increases, reaching its maximum value. Increasing the electric field
with light intensity unchanged leads to increased values of negative
photoconductivity. Results of a study of the temperature dependence will
be published in separate articles.
Institution : State Scientific-Research Institute of Roentgenology and Radiology
~Submitted : March 17, 1953

_ZqQ~ 0
USSF/Playsics Ionization cbamber
Card 1/1 Pub 146-13/22
Author Lyapide,vskij, V. K., and Shcherbakov, Yu. A.
Title Study of the operation of a diffusion-condensation chamber
Periodical Zhur. ek6p. I teor. fiz.) 27, 103-109, Jul 1954
FD-7113
Abstract The operation of a rectangular diffusion-condensation chamber
filled with air and alcohol vapor at atmospheric pressure was
studied. Analysis of the vertical temperature distribution re-
vealed that the heat exchange with the side walls of the chamber
is a decisive factor. The chamber was found to work steadily at
various temperatures. Photographs of ionizing particles are pre-
sented. Indebted to M. S. Kozodayev. 6 foreign references.
Institution Moscow Engineering Pbysics Institute
Submitted August 5, 1953

LUPDAVSKIT V Allww,:
I
Instrument for the observation of ionized particle tracks. Fiz.
v shkole 15 no.lt47-50 Ja-F 155. (MLU 8:2)
l.' In2henerno-fizicheakiy institut, g.Mosk7a.
(Ionization chambers)

-)IN I IV T
USSR/Pfi-ysics- Diffusion-condensation chamber FD-2i-.,65
Card 1/1 Pub. 146 - 26/26
Author : Lyapidevskiy, V. K.
Title : Investigation of the field of partial pressures in a diffusion-
condensation chamber
Periodical : Zhur. eksp. i teor. fiz., 29, August 1955, 263-264
Abstract : The saturation distribution in the volume of diffusion chamber, and
consequently the height and quality of the sensitive layer, depend
upon the temperature field and upon the partial pressures field. The
temperature field in the volume of a diffusion chamber was investigated
by the writer (co-author Yu. A. Shcherbakov, ibid., 27, 103, 1954) and
others (H. Morrison, G. Plain, Rev. Sci. Instr.' 23, 1952). In the
present note the writer describes the procedure and results of measure-
ments of the field of partial pressures, for which a special device was
constructed, a diffusion chamber with expansion (cylindrical vessel with
glass walls, the bottom of the chamber consisting of two brass disks
held by screws,and cooled by liquid nitrogen passing through a spiral
channel cut out in the upper disk). He thanks M. S. Kozodayev and
Professor M. F. Shirokov. Two references.
Institution : Moscow Engineering Physics Institute
Submitted : November 1, 1954

LYAPIDT;VSKIYJ# V. K.
Lyapudevski-r., V. K. -- "Investigation of the Physical ProcesseS in a
Diffusion-Condensation Chamber." Min Higher Education USSF. Moscow Engi-
neering-Physics Inst. Moscow, 1956. (Disseration for the Degree of Candi-
date in Physicomathematical Eciences).
So: Knizhm,,,a Letopis', No. 11, 1956, PP 103-114

'
711
lard coord
d toi, -
~
V;esdt- Lhamt mra. in diam., wul I
,
and-M mra, L.A-, IL: 46ftorm J w4icfft wai cvur Wit
"
Ili Gi;&. "pts., tbx a W.
cooted to voxj,~s timmps,. th-.~ bo-tum Lciri& lidd at a Corst.
bight-T"t=lp".
tho 6'm'm c3t'--J t- ttr-,p-.
Tilii:eoiZio caa~;Ci air-~ vaptir in Oie

-1 SWIW't te
The pmsitlm vval deul. at which
'hiatian atia a c%3nit. typc of Czitivect6a were ferLched.
dh#n
ush v~
cfepeadlxls".em me W~ tliulp- a - dx.
- '
k-it hidka* -; it, wis

pte,~Yfth3v Or ~:&amuictL, '0.
aiir
u
found (1) kt a given Of UiC with

vapur r~ula d fb~"u it 1-nual ImIIT~S'
the temp, C t ~~C
of tilt, tGp~ and b~z t~~ az. V~c it aihnol y C~C-Ci iriz:;' ~'~S w 1-th

the 1:tizi .(:L)-at a gitr-a b:!iz1tt- Olf 0!e
Of 06 dwifli-K".r,
-d a L
c1l'imbtr az tl=-11'~ (fie (fq, thi, ktaliffity vrt~iurc
j
q. -W increase,- wit'; flie. terup. Of tcq~ (ffcccaiZ7' 0.1 tht~ temp,
dielit in tb~ 0113ru Lt. 2~ lt:u! d

bwlpw~ the
'
,
et, a pum=. t"WUL.
The- Hquid Ili
ofjhava% *Ad a

st
tux
betO

u
id thi
bouam. abauba.-Teathava'aft

ev
M4 *a

,
WO.X am- st

-
.~

LYAPIDBVK V.-YIX6 ......
Formation of a cellular structure in
i teor. fiz. )0 no.2:399-400 7 136.
lo Hookovskly Ins ener-n--6--Micheskiy
(Oondensation trail)
fog or smoke layers. Zhmr. eksp
(MLRA 9:M
inatitut.

/- y

LYAPIDEVSK.IY.1- V-LLWTIS11INP V.-M.
Investigating partial pressure fields in diffusion cloud chambers.
Prib..i.tekh. eksp_.-no.1:48-49 Ja-F t57. (M12A 10:6)
1. Moskovskiy inzhenerno-fizicheokiy institut.
(Cloud chamber)

AUTHOR: Lyapidevskiy, V. K. 120-2-10/37
TITIZ:-3~A~_plfication of Th-e-D-iffusion Chamber to the Determina-
tion of Small Activities. (Primeneniye Diffuzionnoy
Kamery dlya Opredeleniya h1alykh Aktivnostey.)
PERIODICAL: Pribory i Tekhnika Eksperimenta, 1957, No.2,
pp. 37 - 39 (USSR).
ABSTPACT: The difficulties in determining small activities when
using particle counters may, to a large extent, be avoided
by using the diffusion chamber for recording radiation.
The author gives results of measurements of a-activity
using a diffusion chamber. Two mthods are described:
in one the sample is at the bottom of the chamber, in
the second it is placed in the region where supersaturation
is less than unity. It is shown that using the first
method, both the absolute sample activity and the vapour
stream may be determined; the second method per *ts the
de termination of activities of the order of 10 iL~ curies
both for a- and P-preparations. A formula for the evalua-
tion of the particle stream with the camera in a stationary
regime is given by equation 1, where C is the act~'Vlty
of the sample, It is the a particle range in mG,/cm , h is
Card 1/2 the distance from the source plane to the sensitive layer

120-2-10/37
-An Application of the Diffusion Chamber to the Determination of
Small Activities.
in mg/cm2sec., t i2 the time in seconds and f is the flow
of vapour in mg/cm see. Schematic drawings of the diffu-
sion chamber and of the chamber for determining the activity
of the sources and two graphs of the counting speed versus
time for two measured samples are given. Wil. f~artishin
has helped in cons-traction of the apparatus, PA.S. Kosodayev
has assisted in the theoretical side of the Work. There
are 3 Slavic references.
SUBMITTED: May 11, 1956.
ASSOCIATION: Moscow Institute of Engineering and Physics.
(bloskovskiy Inzhenerno-Fizicheskiy Institut.)
AVAIIABLE: Library of Congress.
Card 2/2

AUTHOR: Lyapidevskiy, V.~~.
1'0-3-30/11.0
TITLE: Diffusion Chamber with a Transparent Base (Diffuzionnaya
kamera s prozrachaym dnom)
PERIODICAL: Pribory i Tekhnika Dilks-perimenta, 1957,. Nr 3, p.103 (USSR)
ABSTRACT: The instrument is designed for the observation of tracks
of ionising particles. In order to be able to project the
0
tracks-on a screen the base'and the cover of the chamber
are made from transparent materials. The diffusion cham-
ber (Fig.1) is in the form of a cylindrical vessel 100 mm
in diameter and 60 am high. The base of the chamber con-
sists of a layer of liquid, 6 (ethyl aicohol), which is
poured onto the glass plate, 7. The liquid is cooled by
special.walls made of copper (lower part, 5) and of plexi-
glass (upper part, 4). The walls of the chamber are cooled
by solid carbon dioxide placed in the container, JL~. The
lid of the chamber is made of brass and contains a -lass
window. The temperature of the lid is controlled by an
electrical heater. In order to prevent icing of'the outer
surfacel special thermal insulation is provided in the form
of three closed air spaces, 8. A humidity transmitting
material (filter paper) is used as the source of va-pour and
is placed on the inner side of the cylinder. Tlie liquid at
Card 19:

120-3-30/110
Diffusion Chamber with a Transparent Base.
the bottom of the chamber rises up the filter paper, evap-
orates and diffuses dovmviards, making sure of a continuous
functioning of the instrument. The chamber is illuminated
by means of a 300 watt lamp. It is placed at a distance of
5 to 6 meters from the screen. When the liquid layer is
cooled, convection takes place and is clearly visible on
the screen. In the steady state (10 to 15 minutes after the
introduction of the solid carbon dioxide) the supersaturat-
ion near the bottom of the chamber becomes sufficient for
the condensation of drops on ions to take place. Using
this instrument it is possible to observe on a screen seD-
arate drops formed on condensation centres, as well as
tracks of a and 0 particles. Trials carried out at indus-
trial exhibitions have shown that it is possible to ob-
serve (x-particle tracks on a screen in an auditorium in
daylight. The author wishes to acknoviled-e the i,,'U'-erest
of M.S.Kozodayev in this work and to thank A.M.Konstantinov
for 11is help in the construction of the instrument.
Card 2~1'

V
AUTHOR: -_LYAPIDEVSKIY_,V. ERGLIS,K. PA - 2319
TITLEs Devices for Nuclear Physics. (Pribory dlya yadernoy fisiki,
Russian). -
PERIODICAL: Atomnnia Energiia, 1957, Vol 2, Nr 3, pp 291 - 292 (U.S.S.R.).
Received: 4 / 1957 Reviewedt 5 / 1957
ABSTRLCTt At the department for experimental methods of Nuclear Physics
of the Moscow Institute for Physical Engineering investigations
have been carried out for some years which concern the registration
devices serving the purpose of ionizing radiation.
The most important properties of the diffusion chambers were in-
vestigated, and some types of chambers for physical investigations,
measuring of small activities and for purposes of demonstration
were developed and built.
As a device for demonstration the diffusion chamber, if compared
with the WILSON chamber, offers the advantage of uninterrupted
action. The chamber with a transparent bottom developed by the
above mentioned department permits the observation of traces of
c(-particles and electrons on a -6 m2 screen.
A new type of diffusion chambers permits the measuring of radio-
activities of the order of magnitude of 10-12 curie with high
statistical accuracy because these chambers concentrate concen-
Card 1/2 tration onto the surface of a preparation introduced into the

Devices for Nuclear Physics.
PA - 2319
chamber. One of these chambers for the determination of low
activities will be on show at the All-Soviet Industrial Ex-
hibition as well as at international exhibitions.
ASSOCIATIONt
FUSEN= ZY:
SU13MITTEDi
AVAILABLEt
Card 2/2
The development of large diffusion chambers raises several problems.
At the department mentioned above the2construction of a diffusion
chamber with a surface o5 6oo x 900 m (the reviewer believes that
this should read 6 x 9 m ) was developed in which an uninter-
rupted vapor flow is supposed to act. This chamber contains plates
on two walls opposite to each other which conduct the moisture.
Furthermore, an experimental amplifier with drive correction was
developed by means of an ampiifier with contact transformer by the
department mentioned above. he application of contact transformers
in electrometric amplifiers is useful only in the case of using
current intensities of at least 10-11 a (with respect to the full
scale of the device). (No illustrations).
Not given
Library of Congress.

14A P ip E Vs K 1,/
AUri-1116R: KRONGAUZ,A.N., LYAPIDEVSKIY,V-K., DEYEV,-'1-S- 56-5-10/55
TITLEt The Pho tocondue-f-i~v~-y--o-r-Cu-,-O-.--tPo to pro v oJimo st I kuprita, Russian)
PERIODICAL: Zhurnal Eksperim. i Teoret. 2.1q ziki,1957, Vol 32, Nr 5,
pp 1012 - 1017 (U-6-6-R-)
ABSTRACT: '2he light of a mercury vapor lamp is sent through a monochromator
with quartz optics and focussed on a Cu 20 crystal which is fixed
between two electrodes, which are connected by a sort of bridge
circuit with a rectifier as current source and an oscillograph
and a galvanometer as indicating- and measuring device respective-
ly.
The curves concerning the photoconductivity in dependence on the
wavelength of the inciding light show for negative conductivity
a maximum at 6400 R and for positive conductivity a maximum at
4200 R, inasmuch as the crystal was illuminated with low intensity.
Also in the case of the investiCation of the temperature dependence
of photoconductivity a maximum could be found both for positive
and for negative conductivity.
It was further found that if a Cu 0 crystal that had already
been irradiated with li,,,,ht and which has a maximum negative photocon-
ductivity is additionally irradiated with X-rays, its negative
Card 1/2 conductivity diminishes, and even positive conductivity may de-

The Photoconductivity of Cu 20.
56-5-10/55
velop. If irradiation is carried out in the reversed order, an
increase of negative photoconductivity is observed.
-Y and Radiology
ASSOCIATION: State Institute for Roezituefjolog
PRESENTED BYP
SUB:JITTED:
AVAILABLE: Library of Congress
Card 2/2

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GUSAROV, IsIo. aspirant., LYAPIDEVSKIY, V.K., kand.fize-mat.nauk
Method for measuring natural radioactivity of the air by products
of radon fission. [with summary in Suglish]. Gig. i Gen, 23
no.10:10-16 0 158 (MIRA llsll)
1. Is I Moskovskogo ordena. Lenina meditsinskogo inatitut imeni
I.M. Sechenova i Moskovskogo inzhenerno-fizicheakogo instituta.
CAm,
natural radioactivity determs by rAdon fission
products (Rua))
(RADIUM, radon fission prod. in determ.. natural
radioactivity of air (Rua))

AUTHOR: Lyapidevskiy, V. K. SOV/53-66-1-6/ii
4.~
TITLE: The T~s ~a~.er-~Diffuzionnaya kamera)
FiMIODICAL: Uspekhi fizicheskikh nauk, 10,58, Vol. 66, 1[r 1,
pp. 111 - 129 (USSR)
ABSTRACT; By means of foreign publications and by his o,,-.,n numerous.
papers in this field the author gives a survey in the
present article on the problems of recordinG ioniziriC
particles in diffusion arid cloud chambers. The first section
deals with the physical processes in dii'fucion chambers, the
influence of the condeiisation upon the temperature distribtition
and the distribution of the partial pressures; the effects are
discussed by means of many diagrams. The followinC sections
deal with the char,-e of the ions and the dead time, the
direction of diffusion, similar chambers, low pressure cha,,.-ibers
20 - 30 torr), the sensitive stratum, the control system
photomultipliers FEU), arid the constractive particul-ars of diffu-
~
sion chambers (the coolin(, of the bottom of the chamber, t1te
vialls of the chamber, the steam source, the chamber illumination,
Card 1/2 the application of photo-plates in the diffusion cha-~iber)-

The Diffusion Chamber
SOV/53-66-1 -6/11
Finally it is stated that the diffusion charabers comparei ;vith
th+loud chambers exhibit a number of advanta.-es, i.articularly
in work with accelerators and for absolute measure!-.ients of a-
and P-activitics of an order of 10-12 Curie. They are api-li-
cable in many ways, above all for investiaations of .-as dis-
charges, for the investi-ation of t,!e behaviour of charL:ed
droplets in the electric and in the -ravitational field,
for the investi,,~ation of the process of formation Lind growth
of droplets or also of monocr,,3tals in the seed of condensation,
for the investio-ation of the scaLterin- of lilght, at dropl~!ts,
of the interaction of accelerated particles -.Ath matter, etc,
There are 15 figures and 41 references, 19 of which are Soviet-
1. Cloud chambers--Design 2. Cloud chambers--Performarice
3. Cloud chambers--Control systems 4. Particles--Recording devices
TITLE: Diffusion Chambers
Card 2/2

30/120-59-41-8/50
KUTHOR: Lyapidevskiy V K.
TITLE: The Convection Chamber -' a New Instrument for the Observabion
of Charged Paxticle Tracks
PERIODICAL: Pribory i tekhnika ek5perimerta, 1959. Nr 4, pp 49-53
and 1 plate (USSR)
ABSTRACT: A description is given of a r;onvection chamber whose
principle is similar- to that of the diffusion chamber. The
difference between the two lies in the fact that in the case
of the convection, chamber ther-. is a temperature difference of
up to 8000 across the bottom of the chamber. As a result of
this temperature difference cowj-ective motion is set up and
the vapour is moved from tLe periphery to the central portion
of the bottom and forms a sensitive lsj~-,r a few mm high. The
chamber is shown scab emat "'L -ally ir. Fig 1. The bottom of the
chamber consists of two parts. The central part 1 is made
of a good conductor and is cooled to -600C. Wear the walls
the bottom of the chamber 3 is marle of a bad conductor.
The walls of the chamber 2 are at approximarely room tem-
perature. The vapour is provided by a layer of alcohol 7
Card 1/3

SOV/120-59-4-8/50
The Convection Chamber -- a New Instrument for the Observation of
Charged Particle Tracks
The vapour is transferred from the periphery to the centre
of the chamber by convection and the liquid condensed on
the central part collects near the walls. Data are given
on the temperature distribution (Fig 2), the partial pressure
distribution (Fig 3), super saturation, and the rate of flow
of the gas. The chamber can be used for the demonstration and
measurement of low-.activity solid, liquid and gaseous speci-
mens. Figs 5-9 give typical photographs obtained with the
chamber. The chamber can be used 'to record both very high
and very low particle fluxes. The chamber may.be modified
so that the wox-king volume is in contact with the atmosphere.
In the latter case it jgy be i:zed to determine the activity
of the atmcephere (10- a curie/litre or more). Acknowledgments
Card 2/3

SOV/120-59-4-8/50
The Conve-c-tion Chamber - a New instrument for the Observation of
Charged Particle Traoks.
are madp,.to M1. S. Kozodayev, A. M. Konstantinov, V. I. Ani-
simuvp-, T. M. Bogacheva and Ye. Ye. Minayeva. There are 11
figures and 2 Soviet raferen,3es.
ASSOCIATION: Moskcvsk-iy 1nzhenerro-fiz-L!iheski,7 tasidut-C Moscow Institute
of Enginevring and Physics',
SUBMITTED: -Ame 69 1958.
Card 3/3

AUTHOR: Lyapidevskiy, V.K. SOV/120-59-5-34/46
TITLE: On the Work of a Low-pressure Diffusion Chamber
PERIODICAL: Pribory i tekhnika eksperimenta, 1959, Nr 5,
pp 131 - 132 + I plate (USSR)
ABSTRACT: The diffusion chamber which was studied was described
by the author in Ref 1. It was shown that a reduction
in the height of the sensitive layer, as the presnure
decreases, is connected with a change in the partial
pressure and the temperature distribution. The first
is important in chambers with a very non-linear tempera-
ture distribution along the walls and the second fri
chambers with almost linear distributions. Figure 1
shows the distribution of temperature in the chamber.
Curve 1 refers to atmospheric pressure inside the
chamber and Curve 2 to a pressure of 20 mm. Hg.(the
temperature is plotted along the vertical axis and the
distance from the bottom along the horizontal axis).
Curve 2 shows a similar plot for another temperature
distribution over the walls (non-linear). Another effect
Cardl/2 discovered was that at low pressures inside the chamber
>_11,

SOV/120-59-5--34/46
On the Work of a Low-pressure Diffusion Chamber
fluctuations in the drop background took place. The
sensitive layer divides up into cells. A typical i '3hoto-
graph of the sensitive layer is shown in Figure 3 (opposite
P 134). The cells appear at pressures lower than
200 nwi H9. When the pressure is reduced to 30 nua 11g,
the size of the calls is reduced and then begins to
increase again, At a rxesBuro of about 10 nim HS, both
charged-particle tracks and the cells are absent. In
diatinction to 'high-pressure chambers, this effect cannot
b3a removed since the temperature distribution in the low-
pressure chamber cannot be regulated. Acknowledgments are
made to M.S. Kozodayev and V.I. Anisimova.
There are 3 figures, and 3 Soviet references.
ASSOCIATION: Moskovskly inzhenerno-fizicheskiy institut
(Moscow Engineering-physIcal Institute)
SUBMITTED: June 19, 1958
Card 2/2

21 (0), 24 (0)
A7rMR, Tyarozow, C. A. 30T/89-7-2-t6/24
Tr?=. Saientifle Conference of the =M (Natchraja kotforent.1ya Klrl~p
PIQXODICALI AtOo4sq- 0-91Y-, 1959, Vol 7, J1r 2, pp 176-ITT <
A33-UCT. The ;.-iy scientific -tinc .- h.Ld rroz 17 Wil to 15 may
1919 in the Mo.kovskly IAtxh*n*r-fiztch*oklj InaLltut (KOSCOw
rb.-i-I Fulgimearlng institute). Lorv th= 600 7~tjclpmt. frm
100 different institutes att-dd the 2 pl--7 -d 10 venti.."I I-V
w"feromo.s. A total of 148 lectures war. hold. T~.. following
1.0turoa ar speoially mentionedz --. K. R=!~!IZrSW oq
the na-~(_ on
pbyst..l facmd.U." of -I.cul- C 5; 'Plif,
t
_hi~akiy onthIts conatrut,tion of . foot "Actor,
- the ovf of the p*riph,ral collision or mesons
and moLsomm, ja~ on amparriuldity dud moment= of
i--rti. of the nuclei, A. tm 4=4
City sv.. Y. 1. Gorr, ca Is er. ...It.d -it
ra
g
the -.1- hall and nethods of comprehan4inc thea. _L_L.
.Lux:LL&Z.w&d L. j.. Prokb- wo tb .17 1. f -be p ... ibl.
scsp.rixent. for the o; ~thm M-racenta of the
Card 1/~ P.A.momm. m the spectrum of I lq.Ld =4
crystalline hydrogen ujor pr-:ur. an
instrument for ... V--Jtr
the b,or,-lon Mr`*c, T. 7%
Q-7. Glmc~-dLm. on r-Ic.rfW__p-o..LbLlitio
..thdo
for llzsa~ Jgctj~p moovlerat- with al atary wavon,.E. A.
PZALIZ. - ~rl and A. !rZb new, -th.
under betalrom CondIt MAs of the &cc*lvr&tLqm, I
On OPtim=_ v-" 14-Cth f-r - S. r.
and 0. A. Tyo~~. fo"e- --z-
C 1,.A in.
el.atr= accelerator, LjI
Zorl th- 3 m- It- Of the ialpl,
&w
no acesninotio-'-', om ="easnt In the '.Y.t-
or . ,:.r
of t';& olutron with consideration, of the mc3-%:rLA,, fL.1d.-O, L.
L-P-1-a mthol for -~Iuj t:~. he .. conduction
iv...7-Of LiR-idc AM JtO tb---7 Of t-'4* =.thd, YA__!Z~_
XIAb - 't- - ~ -
f=.:. A. Ct
~1-1' whl~ in . cir-Isr apoo.. y_j__
b0moctron~l-ion to circulatLmE zorcur7. v t-
59 LIS
~Qjs~
Card Z/3 sp::Ial aditIonap ban eorj~lC with a flat triode In
the L-;,Ll-- technique. IeZ- F-C-OY-1 c- C-I..l.-Lon ..th.de d
construction of an ln;uloe t-sFo'-r Zm icn-rAcento with
.octi-conduator els~smta, on a p - ibilLt"
L.a
le~ent vyctw for a itii
0.1 mate;'-* ccmtrol OFthe r=aoet.rd or
P. I. To Of .... ral
system. i-.h hih Shymi Cy a; -t~ cam be autcmatically
v m 3 =q.
started, zga~ hol-?t- the quality of
.rawtor contro!. rhea the reActivity chAneas wto"~ or
,inarL!7. 0. A. L...-17gT -4 A. r. 7r.,. In on examination
of the Lod!ne nethod ef refining vtiobi= =4 -h--acteristice
of the metal obtln.d, Z. L. Gruzlz -d C. G. ]~-.b- On
examinatitux f th =icro-dlotribu-.Im of -=bon~,u-48ten- iron
0
and otb~ .1..-t: I= circonicom and its .11~. b;- ... of -t,-
redioCraphy, P. P. Foderor ca datermlAmtion cf -he swbli..tj~o
heat of xirvoctl~- I by u-inC rcdioact-'v* LmAL-t,ca
and 0. D. Fad..--- and .4 d.tarnlooti- of the
diffmaloco coefficient. Of chromium. nickel. lm. ond chrociun
nickel ate.13. The literature for al! tbel- 10cturs- will be
Card 3/3 published by the VIn in a s7.pmiun.

S lo 3 C) /6 J./C -, C) 10 C, Ito 10 ;' C
I C
50' POO 022" 113 Y/ /,S- -2 0) BOO C/"~n
AUTHORS: Gusarov, 1. 1., Lyapidev~3kiy, V. K4
TITLE: Determination of Inhaled Doses of Radon Decay ProductG
PERIODICAL., Atomnaya energiya, 1960, Vol. 10, No. 1, pp. 64-67
TEXT: A new method is suggested for detormining the inhalation of radon
decay products. The method is based on the counting of alpha particles
per liter of air, which are produced by a complete decay of radon daughter
products. In view of its relative exiguity, beta activity is neglected.
The amount of energy released by a complete decay of the a-a,7tive atoms
contained in 1 liter of air is given as E 1 = a(ERaA + ERaCI),~(b+c)ERaCl.
where a, b, and c are the numbers of RaA, RaB, and RaC atoms, respectively,
per 1 1 of air; ER&A and ERaC are the energies released per decay of the
respective element. Denoting their mean value by E a, one obtains: E 2
= Ea(2a+b+c) - E an, where n is the number of alphas produced per 1 of air.
The error due to averaging is insignificant,. If it is further assumed
Card 1/5

Determination of Inhaled Doses oil Radon S/OP'9 60101010-0-1/cO91020
Boo6 Bo63
Decay Products YB
that the absorption coefficient ^9 is equal for all inhaled rador decay
products, E = ~nE will hold. In addition to the commonly accepted filter
method, there are some other methods available for the determination of
the unknown n: Supposing that for a certain pumping rate v, the number
np of alphas recorded per unit time remains constant within a long time
interval, the number of radioactive atoms will remain constant within the
time At of this interval, that is to say, the number of radioactive atoms
retained by the filter during the time 6 t is equal to the number of atoms
decaying in the same time. In the time 8t, exactly 1 1 of air is to be
pumped through the filter. For RaA, RaB, and RaC, the number of atoms
retained by the filter is yl(a+b+c), where 'y, is the known filtration
efficiency. The total number of decay events is 91(2a+b+c) = y1n and, -thus,
n is equal to np/vyly2' where T2 is the recording efficiency; the counting
rate nP is expressed in pulses/mini v is given in 1/min, A device with
continuous recording of the alphas emitted by the filter was developed by
the authors jointly with A. M. Konstantinov for dose measurement by this
Card 2/5

Determination of Inhaled Doses of Radon S108,016JI010100110091020
Decay Products BC06/BO63
method. This device was used for two series of experiments, the first of
which corresponded to a short-period exposure of the organism to a
contaminated atmosphere, whereas the second series corresponded to a
longer exposure, in which radioactive substances are' concentrated in the
organism. This concentration differs from the concentration of these
substances in the atmos;here. On account of the fluctuations in time of the
quantities of substanceu contained in the air, simultaneous measurements
viere made with two devices of the same type. The number of a-particles
recorded in a complete decay of the daughter products proved to be largely
independent of the method-applied and of the concentration ratio of
daughter products. The radon concentration may be determined from the
number of recorded alphas. Fig. 2 shoas accumulation and decay curves of
daughter products retained by filter 1 and filter 2 (for v = 151/min,
A = 11). The authors thank A. V. Bykhovskiy, M. S. Kozodayev, and Ye. V.
Shchepotlyeva for discussions, and A. A. Titov -for assistance in measure-
ment3. There are 2 fiCures and .3 refezvcnees: 2 Soviet and I US.
SUBMITTED: January 12, 1960
Card 3/5

310691601010100110V
-9/020
B0061 '063
Legend to Fig. 1: 1), and 2) filters; 3), 4) scintillation counters; the
arrows indicate the direction of air movement
Legend to Fig. 2: np counting rate, t pumping time
Card 4/5
2
A
), t 123
4 3
r
r~- 4

np, Uj(17/J(Uti
201
S108916-blO10100110091020
B00613CO-3
np, uxnlxuAt (pLlso-s

2

Card 5/5

~2/. 5~200 67826
SOV/47-60-1-20/46
AUTHOR: Lyapidevskiy, V.K.
TITLE: A New Apparatus for Observing the Tracks of Charged
Particles (Convection Chamber)j
2.Z)
PERIODICAL: Fizika v shkole, 1960,ANr 1, PP 70-72 (USSR)
ABSTRACT: This is a detailed description of the above-men-
tioned apparatus (Figure 1), and of how experiments
on.4, and A radiation should be conducted using it.
A convection chamber can work under ionic loads ex-
ceeding thousands of times the natural background.
This permits alpha-sources of great activity (hun-
dreds of particles per second) to be introduced
into the chamber, which was impossible with a dif-
fusion chamber. It is also more reliable., as the
entrance of 8utside air into it does not affect its
work. An 80 C difference in temperatures is main-
tained at the bottom level, and the intensive move-
ment of gas caused by this accomplishes the transfer
Card 1/4 of steam from the source. It is situated near the I/

67826
SOV/47-60-1-20/4165
A New Apparatus for Observing the Tracks of Charged Particles
(Convection Chamber)
central part of the bottom near which a sensitive
layer, several mm high, is formed. The gas attains
a speed of several cm per second. The bottom of
the chamber consists of two parts. Its central
part is of a good heat-conducting material which
is cooled to a temperature of -40 to -60 C. The
part of the bottom near the sides of the chamber
is made of a poor heat conductor. The sides are
at a temperature approaching room temperature.
Alcohol serves as a source of steam. Convection
transfers the steam from the periphery to the cen-
ter of the chamber. The liquid which has condensed
in the center part of the bottom, which is elevated,
runs off to the sides where it is warmed and again
evaporates. The apparatus, filled with air and
ethyl alcohol vapour at 1 atm pressure, starts to
work when the temperature of the central bottom
Card 2/4 part is below -20 0. Theofj and /S particle tracks

6ye'216
SOV/47-60-1-20/46
A New Apparatus for Observing the Tracks of Charged Particles
(Convection Chamber)
are observed through the transparent cover and sides.
The radioactive preparation is introduced into the
sensitive layer in the chamber by means of a special
holder through an aperture in the side of the appa-
ratus. To increase the number of tracks ofcZ par-
ticles in the sensitive layer, an electric field
is created between the cover and the bottom. The
sensitive layer is illuminated through the sides of
the chamber, and it is best to use for this purpose
a PR-115 projector. The tracks of the particles
can be observed in an undarkened room. With the
aid of this convection chamber it is possible to
conduct all the main experiments with 0& and t3 ra-
diation. to demonstrate the -tracks, measure the ac-
tivity of preparations, obtain absorption curves
and measure the length of the run ofU particles.
Instructions how to conduct these experiments are
Card 3/4 given. There are 2 diagrams, 1 chart, 1 photo- q1

6 7 82 6
SOV/47-60-1-20/46
A New Apparatus for Observing the Tracks of Charged Particles
(Convection Chamber)
graph and 1 Soviet reference.
ASSOCIATION: Inzhenerno-fizicheskiy institu4TUA-Oscow
Card 4/4 Engineering-Physics Institute)

LYAPIDEVSKIX.,.V.K,
godel for the study of color vision. Dokl-AU SSSR 134 no.2:
463-466 S 160. (MIRA 13:9)
(GOLOR SENSE) (PHYSIOLOGICAL APPARATUS)

LYAPIDEVSKIY, V.K.; PAVLOVAp T.G.
Vlffual method for the determination of law activitie-3. Yled.rad*
no.Ut66-171 961. (IMU 14 :11)
1. Iz dozimetricheskoy laboratoril Gosudarstvennogo nauchno---
issledovatel2skogo rt~-,zitgeno-radiologlcheskogo instituta Mini-
sterstva. zdra,7ookhraneniya RSFSR.
(RADIATIOli-ICASUREMENT)

2Pj3l5
s/cal
BI 06~31 01
AUTHORS; Gusarov., I.. I, Lyapidevskiy, V.. K.
TITLE; 1-Tew methods of determining atmosrheric pcllution by radon
daughter products
PERIODICAL; Referatiunyy zhurnal. Khimiya, no. 16, 1961, 32' '1, abstract
16 W 356 (Med. radiologiya, v. 6, no. 1 1~61 . ':
~)2-57)
TEXT: A method of total counting and an equilibrium method are described
which are suffioiently accurate and can be employed in practice. The
principle of both methods consists in determining the total number of
a decays from the Rd daughter products which were isolated from a certain
volume of the air to be examined. The principle of the equilibrium method,
consists in measuring the a activity of a filter under conditions at which
the equilibrium was established between the number of the atoms in,3ident.
and those decaying on the filter. EAtstracter!s note: Comolete transla-
tion.]
Card 1/1

I.YAPILEVSKIY, V.K.; OBODOVSKIY, M.M.
Diffusion claud chamber controlled by a photoelectric multiplier.
Prib. i tekh.eksp. 6 no.6:38-40 N-D 161. (MIRA 14:12)
1. 14ookovskiy inzhenerno-fizicheski institut.
(Cloud chambeJ
(Photoelectric multipliers)

S/12o/62/000/001/007/o6i
E032/E514
AUTHORS: and Obodovskiy, I.M.
TITLE: A convection chamber with a honeycomb base
PERIODICAL: Pribory i telchnika eksperimeAta, no.1, 1962, 41-42
TEXT: It is pointed out that the convection chamber
described by the first ~f the present authors in Ref.1 (RTE, 1999,
No.4, 119) has a relatively small base area (up to 100 cm ). In
the present paper the authors describe a chamber whose.base area
can be made as large as desired without affecting its performance.
The base consists of isolated prisms 1 (Fig.1), each of which
functions as an ordinary convection chamber. The top ends of the
prisms lie in a single plane and the prisms themselves are cooled
down to -40 to -600C by thermal contact with the plate. 2 xjhich
in turn is cooled by solid CO.. The upper part of the chamber
(walls and lid) is maintained at room temperature. The working
vapour eiraporates from the surface of the source 3 and is
brought up by the gas flow into the upper region of the chamber,
.. a nd then' down towards the prisms 1. Near the surface of
the prisms there is a sensitive layer with a super-saturation
Card'1/3

A convection chamber with a 5/12o/62/000/001/007/061
E032/E514
greater than the super-saturation at which droplets begin to form
on ions. The cooled gas-vapour mixture becomes heated on
approaching the walls and moves in the upward direction, thereby
producing a closed convective flow of the gas-vapour mixture.
The chamber operates continuously so long as the temperature
difference h-etween the bottom and the top parts is maintained at
the necessary value. In the honeycomb chamber the gas motion
can be made to proceed in a single direction so that the diameter
of the chamber can be reduced to the diameter of its working
region. In order to achieve this, the prisms were laid over the
entire base area, while the upper part of the chamber carried
peripheral windows which were cDvered with the Petryanov (~nn-ig
(FPP-15) filter. Air at room temperature was drawn into the
chamber through the filter by a backing pump and after reaching
the prism surface was ejected back into the atmosphere through
an aperture in the bottom plate. There are 2 figures.
ASSOCIATION: Moskovskiy inzhenerno-fizicheskiy institut
(Moscow Engineering Physics Institute)
SUBMITTED: May 17, 1961
Card 2/3

A convection chamber with a ... S/120/62/000/001/007/o6i
E032/F-514
I
Fig.1
I
II f 1 11
f I
i
f i
;..
Card 3/3

S/04 62/008/00-3/007/007
7 0 0 0 B108YB104
AUTHORS: Lyapidevskiy, V. X., Falomkin, i. r.
TITLZ: Effect of ultrasound on the process of directed arystdllizaticn
PERIODICAL: Akusticheskiy zhurnal, v. 8, no. 3, 1962, 369 - 370
TLXT: The effect of ultrasound on the redistribution of impurities between
the liquid and solid phases during directed crystallization was examined
in a glass tube closed below by a nitrogen-cooled steel plate. Ultra-
sound cxerts its principal effect upon the region near the boundary to
the solid phase. This region is enriched in impurities; ultrasound'
accelerates the transfer of substance. It probably a,1so accelerates the
diffusion of dissolved substance into the liquid. The result of ultra-
sonic treatment is an increase in the output rate of pure substance from
the solution. There is 1 figure.
ASSOCIATICV: Ob"yedinennyy institut yadernykh issledovaniy g. Dubna
(Joint Inititute of Nuclear Research, Dubna)
SUBLITTZ-0: January 15, 1962
Card 1/1

will
'LYAPIDEVSM. V. 'K.
019/02
8/089/62/013/006/ 7
B102/BW
AUTHORS# 0. T. and M. R.
TITLEs Nauchnaya konforentsiya Mookovskogo inshenernovfixioheekogo,
Institute (Scientific Oonferenoe of the Moscow Engineering
,no
Physics titilts) 1962
PERIODICALi Atomnaya energiya, Y. 13j nce 69 1962, 603 - 6o6
TEXT j' The annual oonfarence took place In May 1962 with more than 400
delegates participating. A review Is given of these lectures that are
assumed to be of Interest for the readers of Atomnaya energlya. They are
follovingo A.-I. Loypunskiy, future of fast reactoral A. A. Vasillyevp
design of accelerators for superhigh energies*1 1. Y&. Poseranahuk,
-.analyti6ityt unitarity, and asymptotic behavior of strong Interactions at
high onergioal A. B. Migdals.phonomenological theory for the many-body
prcbleml Yu.'D. Fiveyekiy, deceleration of m*dium-energy antiprotons in
matterl Yu. . ogan, Ya. A. losilevskiyp theory of the Rdsobauer effeatj
M. L4 Ryasanovp theory of ionization,lossee in nonhomogenoous; mediual
Yu. B. Ivanovq A..A. Rukhadse, h-f conductivity of-suboritical plasma;

S/089/62/03/006/09/027
Nauchnaya konferentritya... B1021BIS6
To. To. Loystakiy, A. A. Rukh4dze, electromagnetic waves in nonhomogeneous
1. L. Rozentalf, the origin of fast cosmic muons;
plasmal Yu. D. Kotov
Yu. M. Ivanov, muon depolarization in solids; V 0. Varlemov, Yu. M. Grashin,,
B. A. Dolgoshein, V. 0. Kirillov-UMumov, V. 5, Roganov, k. V. Samoylov,
p- capture by various nuclail V. S. Domidov, V. G. Kirillov-tjgryumov,
A. K. Ponosov, V. P. Protanov, F. M. Sargeyov, soittaring of 9- me
5 , 15 Rev in a propane bubble chacberl S. Ya. Nikitin, M. S. Aynu d
Ya. 14. Selektor, S. M. Zombkovskiy, A. F. Grashin, muon production in X'p
interactional B. A. Dolgothein, spark chamberal N. 0. Volkov,
I. M.* Obodovskiy, study of operation of a convection
ohamber-FT-. G. Finogenov, production of square voltage_pulaa"f-high
amplitudeal G. M. Alekeekov, problems of color via ion j'-V--Xc_Ly&pidevsk _j-,-/
13
ant 0 oral
relation between number of receivers and number of Indepand
To. M. Xudryavtoov, N. N. Sobolov, X. I. TIzongauzen, L. N. Tunitskiy,
Y. S. Paysulov, determination of the moment of electron transition of os-
oillator forces and the widths of the Schuhsan-Rungs bands of molecular
oxygen; B. Y*. Gavrilov, A. V. Zharikov, V. 1. Riyko; decomposition of the
volume charge of intense ion beamal Ye. A. Kramer-Agoyvv~j V. S. Troshin,
moasurenent of neutron spectral 0. 0. Doroshonko$ now methods of fast -
noutroq recardin8o V. 1. Ivancy, doolnetry torninclog7j. R. X. Voicnkvt
0
ar4L.2/4...

1-YAPIDEVSKIY, V.K.; FALOWIN, I.V.
-------- ~ I
Effect of ultrasound on oriented crystallization. Akust-zhur. 8
no.3:369-370 162. CIP.A 15;11)
1. Ob"yedinennyy institut, yadernykh issledovaniyf g. Dubna.
(Ultrasonic waves-Industrial applications)
(Cryotallization)

LYAPjDaVS-KIY,__Viktor Konstantinovich, kand. fiz.-mat. nauk; LYUSTIBERG,
V.F.9 inzh., ved. red.; LEVIN, G.E., kand. tekhn. nauk, red.;
SHVETSOV,, G.V., tekhn. red.
[=X".ion chamber for determining slight o-(.- and (3-activities)
Diffuzionnaia kamera dlia opredeleniia malykh O