SCIENTIFIC ABSTRACT VASILYEV, YE.N. - VASILYEV, YU.B.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001858920014-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 31, 2001
• Sequence Number: 14
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

69952
SOV/1111-
The Excitation of a Smooth, Perfectly-conducting i-olayiol
Revolution. Part 1.
The latter, as well as S m is a function of two points in
space whose separation is Eq (16). In the important case
of an axially symmetric field (m=O) , two of the kernels
(P2129 P 1) are zero and the equation system Eq (7)
be omes 2 o independent integral equations for TE an 'd
TM waves. The values of S m may be found by graphical
integration. As an example S 0 and 5 1 are shown as
-functions of P. in Figure 1. As (p 0 tends to zero'the
real part tends to infinity. The nature of the infinity is
examined by separating out the term giving rise to the
singularity, Eq (19). This integral may be solved in terms.-
of complete elliptic functions. For m = 0, 1 and 2 the
results are Eq (20) in terms of E(k), B(k) and K(k)
It follows, from their properties (Ref 8), that all the
S functions have the logarithmic singularity of Eq (2L,),
m
Card3/4 where po and oil are shown in F'igure 2. The derivatives

69952
SOV/141-2-4-7/19
The Excitation of a Smooth, Perfectly-conducting Solid of
Revolution. Part I.
appearing in the kerneliformulae offer no difficulty.
Thoseinvolving S M may be calculated using Eqs (23)
and (26), the latter having been partially tabulated by
the authors. Derivatives of coordinate functions involve
no more than trigonometry. Expr*osaions for the primary
field in terms of azimuthal harmonies are given in Eq (30),'
the harmonic functions being defined in Eqs (31) to (34).
The near field may be found from a formula similar to
Eq (30), while the distant field is described more simply
in Eqs (35) and (36).
There are 2 figures and 8 references, 5 of which are
Soviet, I English and 2 German.
ASSOCIATION: Moskovskiy energeticheskiy institut
(Moscow Power Institute)
SUBMITIED: Originally: January 8, 1958
Card 4/4 After revision: May 6, 1959

699' )3
.9000
AWHOM -Vasillyev, Ye.N. sov/i4l-2-4-8/1-9
TITLE: Smooth, Perfectly-conducting Solid
of Revolution, Part 11. E K\^/
PERIODICAL. Izvestiya vysshikh uchebnykh r-avedeniy, Radiofizika,
1959, Vol 2, Nr 4, pp 596 - 6o1 (USSR)
ABSTRACT: This is a continuation of the preceding paper. Two cases
of axi-symmetric excitation are treated. The equations for
electric flux are preferred since they give answers which
can be more easily realized physically. The first example
- a thin cylinder of finite lenAth - is excited by a
transverse slot. In Eq (7) of the preceding paper,
m = 0 and that equation is taken which corresponds to a
TM-wave, namely, Eq (1) of the present paper. The
numerical solution of thiA equation first requires its
substitution by that of Eq M, according to the method of
Krylov and Bogolyubov. The roijult is a set of linear
algebraic equations, Eqs (4) and (5), for the flux
density at each point on the curve which generates the
solid of revolution. The advantage of this method is
Cardl/4 its simplicity and the fact that it is applicable to

69953
SOV/141-2-4-8/19
The Excitation of a Smooth, Perfectly-conducting Solid of
Revolution. Part II.
equations whose kernels have singularities. The accuracy
is poor but this is not usually a disadvantage in the
problems where it is used. The non-diagonal elements of
C.1 in Eq (5) may be calculated as products of interval
lengths and the values of the integrand at the centre of
the interval. The diagonal elements must be separately
calculated as regular and singular parts. The latter is
best arrived at by elliptic functions as in the previous
paper. The nmmerical work has been done for cylinders
0.95 X long with hemispherical ends. The diameters were
0.287 XI 0.192X and 0.096 X . The interval length was
0.1 X o The results, from an electronic computer are
in Figures 1-3. As the diameter increases the attenuatif~i.
of the wave propagated along the cylInder increases, as
also does the maximum fieldat the slot. The radiation
diagrams, shown in Figures 1 and 2, are symmetrical
when the slot is symmetrically placed but are displaced
Card 2/4 oppositely from the slot when the latter is displaced.

69953
sov/14l-2-4-8/19
The Excitation of a Smooth, Perfectly-conducting Solid of
Revolution. Part II.
When the displacement is extreme, two lobes appear.
The accuracy of computation was verified, by an
alternative integration, as 2-3% at points other than the
slot and 7% at the slot. A similar calculation was made
on a cylinder 0.287 X in diameter when excited by a
magnetic dipole X/e away from one end. The result is
shown in Figure 4, where it is obvious that currents
are induced only at the excited end and the rest of the
cylinder is screened from the dipole. It is concluded
that the method of proper functions is probably simpler
for simpler structwres and comparable for symmetrical
spheroids but for more complicated arrangements is
inferior to the procedure outlined here.
G.T. Markov is thanked for advice. There are 4 figures
and 4 Soviet references.
Card3/4

69953
SOV/141-2-4-8/1,9
The Excitation of a Smooth, Perfectly-conducting Solid
of Revolution. Part 11.
ASSOCIATION: Moskovskiy energeticheskiy institut
(Moscow Power Insti-tute)
SUBMITTED: Originally: January 8, 1958
After revision: May 6, 1959
Card 4/4

HAFdCOV, Grigoriy Timofeyevich. Prinimali uchautiye: TMINSHIN, O.N.,
doteent;,rASIL'YEV, Ye.N., dotsent; DUMNKOV, D.A., aspirant;
SAZONOV, HOSOV, 0.11., inzh. PISTOLOURS, A.A.,
retsenzent; DOLUKMNOV, H.Pop prc.f.0 rsteenzent; KOCHMIZMSKIY,
G.N., doteent. red.; VORONIN, K.P., tekl~.red.
[Antennas) Antenny. Moskva, Gos.energ.izd-vo, 1960. 534 p.
(HIRA 14:4)
1. Chlen-korrespondent AN SSSR (for Pistollkors).
(Radio--Antennas)

DaWKHANOV, Mark Pnvlovich; GRUDINSKAYA, G.P., reteenzent;.VASI'L I YEV.
,Yo.N retsenzent; BARTEREV, G.M., rateen2ent; VOROHOVA, A.1
- 0 p
red.; rARA ILOVA, S.F.. tekhn.red.
(Prolmigation of radio waves] Rasprostranonie radiovoln. Izd.2.
Moskvv, Gos.izd-vo lit-ry po voprosam aviazi i radio. 1960.
390 P., (MIRA 14:2)
(Radio waves)

3/194/62/000/003/048/066
D201/D301
AUTHOR: Vasillyev, Ye. N.
TITLE: The vectorial wave equation in rotation coordinaZler,
PERIODICAL: Referativnyy zhurnal, Avtomatika i
no. 3, 1962, abstract 3zh131 (Tr. Mot3k. encrr,-. i-n-ta,
1961, no. 34, 206-211)
TEXT: The analysis of a vectorial wave equation in rotation cuordi-
,,iateo io prooented. In this coordinate oyE-,~(!m -thc. Larne coefficient
-is independent of the azimuthal coordinato (f. htl 1 roollit tile depell-
dence of the general solution on is given by a scalar function
itzid by the derivative of this funItion. It is shown that the azimu-
thal field harmonics in rotation coordinates are orthogonal. In a
particular case, when the field is independent of -~he azimuthal co-
ordinate, an equation is obtained which luis been derived in a diffe-
rent way earlier (RZhPiz, 1957g no. 4p 9584). Z-Abotracter's notei
Glomplete translation.
Card 1/1

S/058/61/000/0 11102210--2-51
A058/A10l
AUTHORS: Vasillyev, Ye. N., Seregina, A. R.
7ITLE: Current distributions on thick vibrators
PERIODICAL: Referativnyy zhurnal, Fizika, no. 11, 1961, 299, abstract 11Zh334
("Tr. Mosk. energ. in-ta", 1961, no. 34, 212-224)
TEXT: There are given some calculation details and the results of
calculating current distributions on thick vibrators by the method proposed in
an earlier work (RZhFiz, 1960, no. 7, 17891). Calculations were carried out for
cylinders with radius kR - 0.3, 0.5 and 0.9 for generatrix length kL - 2.8, 5.9
and 9.2. The effect of cylinder length and slit width on current distribution
was analyzed. Calculations were in good agreement with experiment.
Ye. Vasillyev
[Abstracter's note: Complete translation]
Card 1/1

-4b
s/18o/62/ooo/oWooi/oli
F,075/E435
AUTHORS: Nasonov, P.Ya., Va--til2-ye-v-,-YAN._,_Lur1ye, I.L.,
Knyazev, V.F. (Moscow)
TITLE: The reduction of iron oxides with hydrogen in a
fluidized bed at an elevated pressure
PERIODICAL: Akademiya nauk SSSR. Izvestiya.' Otdeleniye
tekhnicheskikh nauk.. Metallurgiya i toplivo, no-5, 1962,
29-36
TEXT: The reduction of mill scale and~a Krivoy Rog ore/-fines with
hydrogen in a fluidized bed at elevated pressures and low
temperatures was investigated in order to elucidate the influence
of pressure, the rate of feeding reducing,gas, particle size of
the starting material and temperature on the reduction process.
The experiments were carried out in a laboratory apparatus made
from stainless steel with a fluidized bed reactor,' operating
intermittently with 300 9 samples. Experimental conditions:
tear.perature from 490 to 650OC; pressure from 3 to 30 atm Zauge;-
two rates of feeding hydrogen - 2.5 and 4-5 litre/sec. The
pro~cess'of reduction was controlled by measuring the decrease in
Card 1/3

5/180/62/000/005/001/011
The reduction of iron ... E075/E435
the amount of hydrogen in the gas holder. In the lower pressure
range (up to about 9 atm) an increase in pressure was found to
load to an intensification of the process, even without an
increase in the rate of supply of hydrogen to the reactor.
An increase in pressure from 3 to 4 atm had a considerably higher
effect than an increase from 4 to 5 or from 5 to 6 atm (the
corresponding increases in the consumption of hydrogen read from
the graph were about 36, 14 and 13% respectively). In the
higher pressure range the increase in the rate of reduction is due
to an increase in the supply of hydrogen to the reactor which can
be made without increasing dust losses. Optimal reduction
temperatures at a pressure of the gaseous phase of 30 atm and a
hydrogen feed rate of 0.3 litre/sec per 1 cm2 of the free cross-
sectional area of the reactor are: to obtain 70 to 75~- reduction
500 to 520%; to complete the reduction process - 550 to 5600C.
Under the above temperature conditions neither sintering of ore
particles nor sticking of particles to the walls of thit reactor
was observed. For reducing scale the maximum temperature of the
process can be raised to 6500C. Within the rang e of 0.3 to
Card 2/3

S/180/62/000/005/001/011
The reduction of iron ... E075/E435
0.10 mat the particle size of the scale has no influence on the
reduction process. The iron powder produced is pyrophoric.
The minimum annealing temperature of the iron powder necessary to
remove its pyrophoricity without soaking and with a 30 minute
soaking was found to be 780 and 750*C respebtively. There are
4 figures.
SUBMITTED: March 15, 1962
Card 3/3

j.L_
ACCESSION NR: AP3004846
AUTHOR: Vacillyev* Ye. N.
TITLE: Ex citing a finite-length cylinder by a Hertzian dipole
SOURCE. IVUZ. Radiofizika, v. 6, no. 3, 1963, 591-607
TOPIC TAGS: Hertzian dipole, cylirder exciting
1ABSTRACT: This is a further development, of a previous authorts work (Tr.
Moskovskogo energ. in-ta, Radiotekhnika i elektronikas 34# 212F 1961). An
axially -nons y mmetric excitation of a finite-length cylinder by axial and radial
Hertzian dipoles is investigated mathematically. The boundary problem. Is
reduced to a number of independent integral equations that describe azimuth har-~,l
Monica of the density of the surface electric current. Then-, each Iniegral
equation 1.9 replaced by a act of linear algebraic equations and solved numericallyo
D! stribution of amplitude and pbase of the current (tensity for various harmonica
',Card
S/0141/63/006/003/0591/0607

and dipole-cylinder arrangements are presented in t0a form of 36 graphs. "Ia
conclusion, the author feels deeply grateful to L. N. Pokrovokaya, who actively
participated in calculations, and to Yu. P. Nikitin, who carried out a great deal
of work in programing the problem. 11 Orig. art. has: .19 figures and 6 formulas.,
ASSOCIATION: Moskovskiy energetichegkiy institut (Moscow Power-
Engineering Institute)
SUBMITTED: 05Oct6Z DATE ACQ: VAuS63 ENCL: 00
SUB CODE: PH
NO REP SOV: 003 OTHER: 000

VASILIYEV, Ya.N.; SEREGINA, A.R.
Excitation of a thick cylinder with finite length. fladiotekh. i
elektron. 8 no.12:1972-1979 D 163. (MIRA 16:12)

VASILIYEV, Ye.N.; SFMGINA, A.R.; KAMMEV, V.G.
Axisymmetrical excitation of a cone with finite length. Izv.
v7s. ucheb. zav,; radiotekh, 7 no.2:243-246 Mr-Ap 164,
(MIRA 17s8)

JkOCIEMSICH MR: AP40=99
a/oW/64/ooq/oo3/oi61/ol68
AUMCMj Ruatm., IS@ Le; VoAlllyav# yo. no
Nitriding omstenite stainless steel 25jQj8NW2
SOMCE: IVUZ. Chernaya, metallurgiya~ nos 3, 1964, 161-168
TOz--LC TAGS: steel, stainless steel 25Khl!%8V2, steel nitrlding,, nitrided layer
hardness, nitrided layer depth, corrosicn resistance, aitriding temperature,
nitriding time, ==onia dissociation
ABSTRACT: The properties of nitrided stainless steel 25MUMV2 (used in machine,
parts procluctica) have been inveztigated.~ Its conposition (in ~) Is: C--0.23,
Cr--17-04, H--7-97, Ma-0-35, W--2.15. 8=plez 10 mm in diamet6r and 20 = long
vere annealed for tvo hours at 8XC + 10., air coolecli, and ground to surface
smoorthness of v8 - vg. After degreaZing and reducing of the mcide ri2m, with anno-
nii--4 chlorideP the s=ples were suspended In a stainlx.-ss steel container within a
furnace. Ammonia vas next blown into the container, nnd the samples were heated to
530, 5Pj 560, 370, 580, and 6MC. They were nitrided for 20 hours and were
Card

ICCESMN n; AP4=899
air cooled to IM 15bC, At this point the flow of ammonia was stopped and the
sanplas removed. The depth of the nitrided layer,, the hardness, and the micro-
structure of metal wore then studied. It was found that with ammonia dissociation
of 2_r-3% the gmatest, depth of nitrided layer (0.15 mm) was attained at 6= and
the smallest depth (0909 um) at 530C. The maximam hardness (1180 HV) was reached
at 530C and the minimun (752 KV) at 600C. The temperature of 5600 was taken to I
be optimal, for the dasired combination of these properties. When the period of
nitriding was varied (20, 30, 40, 50, 100, and W hours), it waA determined that
the depth of the niU-JLdW layer inwe~ased parabolically with tho time of nitriding,,
reachin,gr its maxJmum of 0,29 ma in 245 hours, The hardness of metal,, however,
decreased an the tine lengthened (see Fig. I on the Emlosure), To establish the
relation betmew ths depth of layer and the degree of ammonia dissociation, the
latter process was varied (2S-25.%, 25-35%, 35-4A and 70-90%). The depth reached
its -mri-= (0,142!; ~n) at tha dissociation rate of 3S-25% and its mJnJm;1m
(0.215 =) at 70-9Q%. The most desirable hardness was attained at the dissociation'
.rate of 25-60%. For the beat coobination of depth and hardness, the dissociation
of 2544 was taken to be qpt1=1;-- TM-bhango of hardness through the depth of
vAtrided layer w" studied on the specimens processed for 30 hours at 5600 with
Card 2/43

!CCESSION HRs AP4022899
&n'tonium dissooietion of 23-35,4o. To determine the influence of nitriding on the i
corrosion resistance, V'-he samples were nitrided for 20 hours at 56OCs with
dissociation of 15-25%, 25-35%., 35-45/1., and 70-9Q-". In order to obtain comparative
data
similar specimens of stool 30KhGSA were also nitridod, Corrosion produced
by a*osure to fresh and to sea water was investigated by surface inspection) and
L.he time of exposure necessary to produce the first signs of corrosion was recorded.
St,eel 25M&W proved to be less resistant than steel 3OKhGSA. Samples nitrided
for 20 hours at 560C and at the dissociation rate of 25-35% showed no signs of
corrosion after being exposed to warm fresh water and to sea water for 11 days.
The greatest corrosion effects were noted on steel nitrided at 530, 580, and 600C.
Gi-aphs presented in Fig. 2 of the Enclosure give optimal conditions for nitriding
machine parts made of steel 25Khl8N8V2. For parts with the nitrided layer 0,10-0.33
Pra deep the aitriding should be continued for 20 hours at 560C with ammonia
dissociation of 20-Wo. For a depth of 0.3.4-0.20 mm, nitriding should be contimied
for 40 hours (with other conditions remaining unchanged). Parts so treated have
s,--face hardness of 960 HV and resist corrosion in either cold or warm fresh water
&a.--d in sea water vapor. Orig. art. lm: 6 graphs arA 1 table.
.A-0,3XLkTWX: Moskovskiy avbomekhanicheskiy institut (YAsoo-d Institute of Auto-
card

VASILIYEV, Ye.N.; SERLGINA, A.R.; KAMMIEV, V.G.
Excitation of an ideally conductive body of rotation with a
sphere on its axis. Radlotekh. i elaktron. 9 no.4:581-569
Ap, 164. (MIRA 17:7)

ACCESSION NR- AP4042016 3/0057/64/034/008/1341/1344
AUTHOR: Vasillyev, W.N.; Orlov, Yu.I.; Perayakov, V.A.
TITIZ: Boundary conditions at the surface of a plasma with rapidly changing--para-
1motors
SOURCE: Zhurnal takhnicheakoy fisiki, v.34, no.$, 19G4, '1341-1344
"plasma, plasma wave props-
TOPIC TAGS: plasma, plasma boundary layer, inhomogeneous
nation
ABSTRAM She authors discuss the boundary conditions for a plane ele6tromagnetic,
wave obliquely incident from the vacuum onto the plane surface of a plasma in which
the electron concentration is proportional to'the distance from the surface and the'
collision Irequonoy is independent of position. Under theme conditions the gradient'
of the dielectric constant is a complex function, a, of well-known form of the wave'
frequency, the collision frequency, and the electron concentration gradient. Max-
well's equation's are solved for plane waves incident on'the boundary at an arbitra--;
ry angle, and the ratio of the electric to the mognotic field components In the
boundary plane is calculated for two states of polarization of the Incident wavot
t2/2

ACCESSICK NR: AP4042916
with the electric vector, or with the magnetic vector parallel to the boundary. It
is found that for sufficiently small values of k/a (k is the wave number of the in-~
cident wave in vacuo), this impedance is the same for both polarization states, is
independent of the angle of incidence, and is proportional to (k/&)1/3. For larger
values of this parameter higher order terms become Important and the impedance vo-!
ries with the angle of Incidence and the state of polarization. The impedance was
calculated for several angles of incidence onto a plasma in which the collision fro-!
quency is zero, of waves with the electric vector parallel to the boundary, and the',
results are presen'~*ed graphically. Ostensibly the defined boundary conditions can
be extended to other than plane waves and to slightly curved boundaries*' Orig.art.!
has:'14 formulas and 2 figures.
ASSOCIATION: Moskovskiy ordena Lenina energeticheskly institut bloscor "Order of
Lenin" Power Engineering Institute)
SUBMITTEDs O8JulG3 ENCL: 00
Sim Cout.,ju.sm my sov, 001 0=R1 000
2/2

VASILIEV, Ye.N., 51-'.rd`,GINA, A.H.; KAMENEV, V.G.
. I - 11 I.,~' I ~~ :., - 4 ~- I I I " ~ I
Excitation of a thick cylinder with conical ends. Radictekh. i
elektron. 10 no.5t940-942 My 165. (MIRA 18:5)

h222--66 FWTVI)ITI"FOS (1, WR
410CESSION M AP501037t3 UR/0108/65/020/004/0027'/00'31
621-396
AUTHORt Vasillyev, Ye. N. (Active member)j Seregim, A. Re Aotive.member)
1TITUs Directional patterns of a slot antenna in a finite-length thick cylinder
SOURCE: Radiotekhnika, v. 201 no. 4, 1965, 27-31
TOPIC TAGS- slot antenna, antenna directivity
ABSTRACT: Directional patterns are calculated and plotted of the slot antennas
situated in the side and the end of a lo"g (length exceeds 1.5-2 di=stars)
der. The field within the slot iG asswiirl to bo oxinym7notricall the wirrow.
distribution over the cylVider rewamibies a braveling ;-mve with docronsing
,The ddirectional patterns for the nDar-end and conter ul.'-de slots and alao for thj
iond slots ara plotted for voveral. cylinder radill . I'Ln eonclilsion, tho autilors
i4lah Lo for his perusal of the -wmwoript wid co,%,mtv alf!
I ~i m a compufnr earl helped In cvloiLla"lor
J!.- A. Yu-rk-ov-, who rjoL up Lho prograi-
i Orig. art. has.- 7 figares, and 4 fonlaulas -
card 1/2

L U22-66
'1ACCESSION NR: AP5010378
IASSOCUTIONs Nauohno-tekhnicheskdye olishchostvo radiotekluliki i elektroavyazi
~:Im. A S. Popova (Sci6ntifia and Technical Society of Radio Engineering and
iElect;ocommunication)
SUBMITTEM 29Jan64 ENCLi 00 SUB COM. Ea
NO REF SOVt 002 (YrHm 1 000

L 16uo-66 34T(d)/T IJP(c:)
ACG NR: AP5025111 SOURCE CODE: UP,/0208/65/005/005/0841/0851
AUTHORt VagiViev, le,*,,N,,--(Mscow)
'7
ORGs none
TITLE: Function encountered in the theory of diffraction
SOURCE: Zhurnal vychislitellnoy matematiki i matematiabeskoy fiziki,*v. 5. no. 5"
1965# 841-851
TOPIC TAGSt integral equation., Fourier series, function theory
i PBSTRACT: The author studied the properties of the function which was the
~n
m-th term of the Fourier series expansion in terms of 'F of the function
-~~IDXP (-iYP,2 W cos rp) fPW --2v3 co3-fp
The expansion of Sm in terms of hypergeometric as woll as Logendre and Henkol
functions of half-integer indices were given. Some differential formulas and
,integral representations of % were also derived,, and E6 was tabulated to four
,decimal placese 7he function S6 often oecurr'M in connection with problems of
Card 1/2 UD03 517.564:535.4

L 16UO-66
ACO NR: AP5025132
diffraction on rotating bodies* It sorved to determine the kirnels of integral
equations encountered there. 'Die formulas obtained wore used for the numerical
computation of these integral equations. The author expresses his thanks to
B.L. Kogan,, A.Rt Sere j A.A* Falunin and G.M. Mlusl*ov for assistanoe.
Orig, art. hast 3 figures, 8 foiiiu-las and 1 table.
SUB CODE s12/ SUBM DATE: 11M&r64/ ORIG-REF: 009/ OTH REF: 003
Card, 2/2

VASILIYM' Ye,.-,--ci,iy Niholaycvich; 1:0~~"YASHEVA, F.I., red.;
SHCHM.~r.-A yIT.L., tekchn, rc-d.
[Capital investments financed from noncentralized fwidwl
Kapitallr.ye vlozheriia za scliet netsentrclizirovannykh
istochnikov. Foskva, Go.Aurizdat, 1963. 50 P.
(MIU 16: 12)
(Capital inveAments)

SHUM, Boris Maksimovich- VASILIY3 radaktor; IANOVSKAYA, H.P.,
redaktor izdatelletya: FAW&PE"S', takhnicheskiy redaktor
[The fittings of rail and structural steel, larga shape mills]
Armatura rellsobalochnvkh i krupnosortnykh stanoy. Moskva, Goa.
nauchno-takhn. izd-vo lit-ry po charnol i tavetnoi metallurgil,
1956. 218 p. (KLRA 9-10)
kRolling mills)

1331LISKIY, B.I. [deceased]; BURIYANOV, V.P.L.1,0IL! VITKINA, B.I.:
GALLAT, Ta. S. ; LEVIN, G. I.; KAMY)ff . Tu. M. ~, G MITUSTKIN, AJ e;
RCKOTTAN, U.S., red.; ISTOMIN, A.B., red.; red.;
NIPCKNUSHCHIT, N.I., red. Izd-va; KARASIV, A.I*.,~,tekhn. red.
[ferrous metallurgy in capitalistic countries) a-ernaia metallurgiia
kapitalisticheakikh stran. Pb.4. [Rolling mill produationj Prokatnoe
i trabnoe proizvodstvo. Bel'skii, B.Z. and others. Moskva, Goo.
nauchno-tekhn. izd-vo lit-ry Po chernoi i tavetnoi metallurgit.
1956. 627 p. (MIRA 11:7)
1 Moscow. TSentral'W nauchno-isaledovatellskiy In8titut chernoy
;;tallurgii.
(Forging) (Rolling (Metalwork)) (Pipe, Steel)

MOROZOV, N.G.; uchitall (selo Klyuchevki, Chelyabinakoy oblasti);
PRUDHIKOV, S., uchitell; GORB, Te.V.; SIDOREUKO, uchitell;
LAZARS-1, V.; SVIDOOVICH. A., uchitell ; JIUBIU, M., witorliat;
VASILIT~W, Yel.T..-,. uchit6l'
Letters to the editors. Geog. v shkole 23 no. 6:67-69 U-D
l6o. (MIRA 13:11)
1. 4-ya shkola shkoly g.Nevelya(for Prudnikov). 2. Direktor
16-y shkoly g. Vinnitay (for Gorb). 3. 81-ya shkola g.Baku
(for Sidoreako). 4. 11-ya shkola g.Tyumeni (for Lazarev).
5. TelemiClIBIMLya ahkola Brestakoy oblaatl (for Svidunovich),
6. Vinnitskiy oblastnoy institut usovershonstvovaniya
vrachey (for Rubin). 7.,Sanitorno-lesnaya shkola poselka
Klyuchi. Kamchatskoy oblasti (for Vasillyev).
(Geograpby)

VASILIYNV, Ye.V., arkhiteYtor
~
Modifications of stAndard specifications for designing railroad
stations. Transp.stroi. 7 no.5:23-26 My '57. (MIRA 10:11)
(Railroads--StRtions)

7ASILITEV, Te.V., arkhitektor.
Some trends In railroad station construction abroad. Zhel.dor.transp.
(MLRA 10-7;
39 no.6;80-84 Je 157,
(RailroAds-Stations)

I
t T jot so) 4*1 OV 401 *a 4090
t f 4 A. A -b
tx-lalb a a
kf I No ~"Pjq
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tF
1"U" at nwg-
a. Chun. J., 11KI4,
awe 0-71
91
K* see
Ito. and
00 &
6. ;j eq
60,3 f a BsO, a" 10 O.S. ON 9."L
I I t of
00.3
too
Oew
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COO
See
X*O
voe
it OJ L11100401 CtA ISWK ATO" It-
*saw A? 04V all I it,
An I I a fw 0 0 It I w It 0, a

VASILIYEV, Yu., ntarshina, sokrotarl partiynoy organizatsii batarei.
'We try to do our best. Komm.Vooruzh. Sil I no.1.3;49-50 J:L 161.
(M URA 14:d
(Russia-Army--Artillary)

VASILIYEV, Yu., starshina everkhsrochnoy sluzhby
We achieved our success this way. Kom Vooruzh.Sil 3 no.24:45-
48 D 162. (KMA 15s12)
(Russia-Army-Artillery)

VASILIYE,V,, Yu.
Communist Youth League should not stand apart. Prof.-tekli. obr.
20 no.12:9-11 D 163. (MIRA 17:1)
1. Otvetstvennyy organizator TSentrallnogo komiteta Vsesoyuznogo
Leninskogo soyuza molodezhi.

VASILIYEV, Yu.
Holding of several posts by pedagogical workers. Sots. trud 8
no.9tl33-139 3 163. (KERA 16:10)

VASILIYW, Tu., as rant
Increasing the power and the econocV of gas-turbine
plants with free-piston gas generators. Xor.flot. 20
no.8:28-30 Ag 160. WR& 13:8)
1. Leningradskoye vyssheye inzhenernoy morskoye uchilishche
Im. admirala Makarova.
(Marine gas turbines)

VASILIYEV, Tu.
"Inch-59" flashlamp. Sov.fGto 20 no.2:35 7 160.
(MM 13.7)
(Photography, Flashlight-Squipment and supplies)
,-.; - - - - -N
c I I I., - .1 . - I I -f: ,,, ~ :~i `
'a, , Ak-i"I -'-~ -
I. - - ---- - ''

VASILIYEV Yu
Practice in applying legislation on benefits to persors workir-E in
the Far Forth Pnd equivalent territories. Sots. trud 6 no.9:
129-137 S 161. (MIRA 14:9)
(Russiap Northern-Labor lava and legislation)

VASIL' -0-1-, U,-, -
Y%V _j
Connection of an additional pulse lamp. Sov. foto 19 no.5:57-58
M7 159. (MIRA 12:9)
(Photograpbq, Plashlight)

VASIL'-fr.V, Yu,
---
Fulso transformer. Bov,foto 20
(Photography--Lighting)
no.1!40 A 160.
(14M, 13:5)
(Ilectron tubes)

-42110-66 ~ - ZWT-(d wnAm- --- -
ACC MRs AP60236 SOURCE CODE: UR/0308/66/000/007/0024/00251
AUTHOR: Vasillyev, Yu. (Engineer); Belostotskiy, A..(Engineer)
ORG: non e
TITIE: Improving the pickup of-marim-divAglo with gas-turbine supercharging
SOURCE: Morskoy flot, no. 7, 19660 24-25
TOPIC TAGS: marine engine, diesel engine, supercharged engine, supercharger,
marine engineering
ABSTRACT: Engineers Yu. Vasilfyev and A. Belostotskiy, after discussing
American methoes for improving the pickup of diesels with supercharging,
describe a Soviet method developed by specialists bf the Machinebuilding
Plant im. Malyshev for which an Author Certificate has been issued.
This supercharginp method consists in the supoly of additional air directly
to the cylinders of the engine during a transition operation. The air
.can be supplied by control valves as well as by valves automatically
.operatinR during pressure drops. In the case of mecbnni.cally operated
valves, a camshaft comes into operation with increased loading and opens
air valves through which additional air enters the cylinders.
UDC: 621-436-001.6

L 42:UU-Ob
ACC NR. AP602j__6,_06_____
Experiments revealed that a pneumatic valve-control method using
the diesel's air-supply system was adequate only at rpm's near those
encountered when starting (n-90 rpm), and that at 500 rpm the valves did
not open. Therefore, a system of automatically operated valves was used
for improving the pickup of a D-100-type diesel generator ecuipped with
a 10 D-100-IA gas-turbine supercharger.
3" Fig. 1. Device for improving the pick-
up of a diesel with gas-turbine super-
L-
z charging
8
HO *5
0 a5

The pickup-improvement device of this 10"cylinder twocycle engine
with two-stage supercharging (first stage, a turbosupercharger 3; second
stage, a.centrifugal genr-driven supercharger 4) consists of automatic
,valves 5 located on each cylinder, a control valve 7, an air reducer 8,
cylinders with compressed air 9, and an air-supply line 10 (see Fig, 1).
When the engine I is runninR steadily, the control valve 7 is closed and
the pickup device is switched off. With a sudden increase in the load,
on the generator 2, an impulse is sent to the device which opens the conT
trol valve 7. Compressed air from the cylinder 9 is reduced to the pro-
per pressure in the reducer 8 and enters the air-supply line 10 through
the control valve7 and on into the chamber (a) of each automatic valve 5.
When the pressure In the cylinder drops below the pressure in the chamber
(at the beginning of the compression-cycle), an additional amount of air
enters the cylinders. This increases the filling of the cylinders and
raises the air-surplus coefficient in them during the transition operation
occurri6g with a sudden load increase, effectinp a significant reduction
in the transition period and an rpm loss and decreased smoke formation in
the exhaust gases. With the end of the transition operation, the device 6
closes the control valve 7 and cuts off the additional air supply. The
switching off of the control valve 7 by the device 6 can be accomplished
by means of a time swit6hine relay, the supercharging pressure, the rpm
of the turbosupercharger, or by the diesel's rpm. The debcribed device
was proved on.the plant's 10 D-100-la diesel generatorand the transition
Card 3/5

operation during the engine's loading between idling and 1600 kw at
750 rpm was studied. The fuel-supply checking device was advanced at a
1760-kw load, and additional air entered the recess (a) of the automatic
,,valve under a pressure of 7 kg/cm2.
A diagram (see Fig. 2) demonstrates the transition operation of the
rim

n,
n,
1
Y

m a a
to
too - - ;-S 2 - - - - ,
I
16
V

E

M
650

50
600
600

_

_
-

.

.
12 13 7,sec
8 9 10 ft
Fig. 2. Transition-operation
oscillograms of a D-100-type
-diesel with a gas-turbine super-
charger
n - rpm of diesel; hp - the rack
path of fuel pumps: - with ad-
ditional air supply: --- without
additional air supply.
5 6 7
engine with and without an additional air supply. In the latter case, the
transition period decreased f rom 14. 7 to 7. 5 secorxb ard the rpm drop decreased
a little; therefore, the time the centrifugal rpm controller held the
rack in a stop position decreased from 12.4 to 5.9 seconds. The rpm drop
occurs only during the first period of a transition operation, when the
Card

3-6b6
ACC NR. AP60~
controller's action is lagging. Using a two-impulse controller the retarda-
tion Is practically zero. Thus, by using a two-impulse speed controller
together with the device for additional supercharging, the transition
period is shortened and the rpm drop with increased loading is decreased.
The described method of improving the pickup of diesel generators with
turbosuperchargers is considered most promising since it makes it possible
,to maintain the necessary air-surplus coefficient in the cylinders during a
~itransition period,,significantly shortens it, and re-duc-es.the exhaust-smoke-.
formation. Orig. art. has: 2 figures. [ATD PRESS: 5052-F]
SUB CODE: 13 / SUBM DATE: none

ACC~!'N&- ARG022470 SOURCE-CODE: UR/0169/66/000/003/DO22/DO22
AUTHOR. Raykher, L. D. ;--YaaWyzv,.-Yu..-A. ; Xharaz, 1. 1.
iTITLE: The method of controlled flat front and its field procedure as a modification
of the MOV method of seismic prospecting
ISOUPdE: Ref. zh. Geofiz,'*Abs. '3D137
IREF SOURCE: Tr. Ukr. n.-i geologorazved. in-t, vyp. 11, 1965, 100-105
TOPIC TAGS: seismic prospecting, geologic survey
TRANSLATION: The method of controlled flat front essentially consists of turning the
flat front of the emitted seismic wave through a predetermined angle from the day 6ur-
face to insure the parallelism of this front to the reflecting surface. In such a
case, slopes of the line of shot moments and of the trace of the reflected wave are
equal, though opposite in sign. The total time of retardation produced by this method
i
mined frcm these two, provided that the principle of Symmetry is complied
_1may be deter,
with.."Distances 4 between the points of shots, which contribute to the formation of al
flat wave at depth H, can be determined from the formula;
TH-
W-
Cos a
UDC: 550.834
Card 112

'I-ACC-NR3 AR6022470------
where I is the wavelength, N is the number of flat waves in the emitted group, and a
is the angle of inclination of the flat front. Distances between the reception points
are selected in the same way as in the SPF method (RZh Gfiz, 1965, 2D160). As a rule
the bases of emission and reception are coincident. Neighboring setups are serviced
by one or more chann*ls. G. Sbakhtman.
SUB CODE: 08

Strr.cture )f the wave flell,l ~f a
discreet 11 B group. lzv. -S 7
1. Ukrainskiy nauchno-ia5-l6-J,-,vatr-11;3kly
in3titut.

VASILIUV. Yu.A.; ZAMYATIN. Yu.S.; SMOTININ, YeJ.; FOMUSBKIN, X.F.
Spectra of neutrons emitted in the fission of U235 at 0,45 and
qbP angles to the line-of flight of the fragmGnts. Atom. energ. 9
no.6:449-454 D 160. (MIRA 13:12)
(Neutrons-Spectra) (Uraniun-lootopeo)

S/056J60/038/03/02/033
B006/BC,14
AUTHORSt VasilIYeL&.jgj._A-., Kamyaji~in* Yu.. s.IIllin, Yu..~.,
Sirotinini-Ye. I., Toropov, P. V., PomuBhkin, E. F.
TITLEt Measurement of Spectra and the Average-Neutron 'Number in the
Fission of U 235 and U 238 by 14-3-Mev Neutrons
/7
PERIODICALs Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol- 38, No- 3, pp. 671-684
TEXTz The present article deals in detail with the experimental investi-
gations made in the energy range 0.4 - 5 Mev by means of the time-of-Elight
technique and a pulsed neutron source. The experimental arrangement is
schematically shown in Fig. 1. The reaction T(d,n)He4 served as primary neutroL
source in the target of an accelerator. The target was bombarded with 150-kev
deuterons. The time-of-flight determination was carried out electronically
by measuring the time integrals between the pulses in the detector. The
deuteron impulses were obtained by modulation; i.e., by means of a a soidal
inu
Card 1/4

8205
Measurement of spectra and the Average Neutron 3/056/60/036/03/02/033
Number in the Fission of U 235 and U238 by BOo6/BO14
14-3-Mev Neutrons
electric field (f - 2Mc/sec); the pulses of the 14-3-Mev neutrons lasted
3mtAsec and had a frequency of 4 Mc/sec. On the averaget 4 neutrons were ob-
tainedf~t-pulse. Two fission chambers were used (with U235 (go per cent) and
U238 (na~tural isotope composition ); the chambers were filled with a mixture
of argon and 002-gas (10 per cents at 760 torr. A tolan crystal (diameter
80 mm, t4iqk~ipps 25 mm) with a photomultiplier of the type FEU-33 served as
neutron detector. The efficiency of the detector was determined according to
Hardy. Fig. 2 shows the efficiency as a function of the energy of three
threshold energiess 0.2, 0.25, and 0-3 Mev. The electronic apparatus used to
measure the pulse distribution in the detector with respect to time is de-
scribed in detail. Pig, 3 illustrates a block scheme, Fig, 4 a recorded pulse
versus time diagram. Fig. 5 shows the time distribution of the pulses re-
corded with the measurement of the neutron spectrum of the U238 fission.
Besides neutrons and g--rays of the fission the following were also recordedt
14-Mev primary neutrons; neutrons, and r-quanta due to interaction between
primary neutrons and parts of the apparatus, radiations of the activated
Card 2/4 A-

~:'.V,L'
Measurement of Spectra and the Aver&Et. Neutron S/05 6/60/038/L)31/02/033
Number in the Fission of U 235 and U238 by B006/BO14
14.3-MOV Neutrons
1. i
substances, neutrons, and C-quanta due to primary neutron scattering, and
2-5-Mev neutrons krom the accelerator. Details and accuracy of the 118eparation"
of the measured values from the background are discussed. The neutron spectra
of U235 and U238 fission are shown in Figs- 7a and 7b. All curves show a
similar course: a steep ascent, a peak, and an even descent. Figs. 8a and 8b
show the diagrams made for the analysis of the spectra in the coordinates
1n (F(E)/E) and E . The spectra may be satisfactorily represented by
p (-~w/Tf) 2
qx" exp (-E/T.) sh
F(E) CK exp (-E/T) + (1
T2
The analytical results are listed in Table 1. The following parameter values
are indicated: for U235P Tf = ( 1 , o6~- W3), mev; T = (0 - 37 � O~ 04) Mev;
q (fraction of evaporated neutrons) = (0~16 + 0,02)~; for U238,
Tf . (1 .16 + 0- 03) Mev; T (0- 40 + ;0,04) Me~;; % - (0.21 + 0.02)9~. The average
number of neutrons emitted in the fis6on.V: 4-17 � 0-30 (U235) and
Card 3/4

82hO5
Measurement of Spectra and the Average Neutron SJ056/60/036/03/02/033
Number in the Fission of U 235 and U238 by B006/BO14
14-3-Mov Neutrons
4.28 � 0.30 (U 238), the ratio ~(U238)/~(U235) - 1-03 � 0-03. The following
data were obtained: U 2351 d~/dEn 0.112 + 0~011 and 'U 238: d'~/dEn
0-115 � 0-011; (E n - neutron energy). In conclusiong the authors thank
Yu. Ya. Glazunov, A. Njj~~sjcyj N. 1, Nemudrov, V. A. Parshina, A, I, Re-
shetov, V. S. Khorkhordin, for ).,:_vinr; p.-_rticiprited in the
measurements and for their assistanc6, V. A. Komi,.rova for:toiaputer ca-Icula-
tions. Mention is also made of the group of V. A. Ivanov, Yu. S, Zamyatnin,
G. A. Bat', and L. P. Kudrin. There are 9 figures, 2 tables, and-21 ref-
erences, 12 of which are Soviet.
SUBMITTEI)i August 5, 1959
Card 4/4

,RRIL~~~ZAJCATRIU, Yu.S.; ILRIN, YU.I.; SIROTININ, Te.I.;
TOROPOT, F.T.; FOKJSMN, Rjp.
Measuring the spectra and average number of neutrons in the
fission of U235 and U238 induced-by 14.3 May neutrons.
Zhur.ekop.i teor.fiz, 38 no-3:670-684 Mr 160.
(MIRA 13:7)
(Neutrons) (Nuclear fission) (Uranium--Ieotopes)

'AUTHORS: Vasillyev, Yu. A. , Zamyatnin, Yu. S., Toropov, P. V., 89-12-9129
Po shW~in~,.
TITLE: Measurement of the ifeutron Spectrum in the Area below 0,5%V bY
Means of the Tine of Flight Method (Izmereniye spektrov neytronov
v oblasti energiy nizhe 0,5 MeV metodom vremeni proleta)
PERIOLICAL: Atomnaya Energiya, 1957, Vol. 3 , Nr 12, PP, 542-544 (USSR)
ABSTRACTi By applying an impulse source of neutrons the secondary neutron
spectrum is aeasured, which develops, if 14 MeV neutrons pass
through layers of uranium. A fission chamber, which was connect-
ed with a 3o channel analyzer, was used as a neutron detector. The
distance between source and detector was 6 m.
The energy spectra for the following samples were shown by a
graph:
a) U235 ; 2,7 cm thick (, 1/5ilin)
b) U238 : 2,5 cm thick (,1/3 /-Lin)
c) U238 : 8 cm thick ( ^-in)
The spectra obtained from a) and b) originate from a simple
interaction between 14 MeV neutrons and the uranium nuclei; It
can be assumed that in the measured area of energy the develop-
Card 172 ment of the secondary neutrons originate from evaporization from

Measurement of the lieutron Spectrum in the Area 0,5 MeV by Means 89-12-9129
of the Time of Flight Method.
the stimulated conditions of the compound core.
For the case c) the development of a higher number of slow neut-
rons was ascertftined. These are the consequence of a multiple-
inelastic interaction which confirms the existence of low situa-
ted levels in the U238 nucleus. There are 3 figures and 3 refer-
ences, 2 of which are Slavic.
SUBMITTED: July 2o, 1957
AVAILABLE: Library of Congress
Card 2/2

VASIVYZV YK
Qraphic analytical method of solving spacial problems in seismic
prospecting by the reflection method. Izv. AN MR. Ser,geofix.
no.1158-67 A 163* MIRA 16z2)
1. Zapadno-M=ainskaya Goofizicheskaya razvedochnaya skepeditai-ya.
(Seismic prospecting-Gmphic methodff.)

1OFFE, A.Ya., kand. tokhn.nauk, red.; VASIL-IYEV, Yu.A., rod.;
GVIRTS, V.L., tokhn. red.
(Control of rejects and quality improvement of grp-y iron cast-
ings]Borlba s brakom I p~vyshenie kachestva otlivok iz serogo,
chuguna. Leningrad, 1962. 93 p. (14IRA 15:11)
(Iron founding) (Foundries--Quality control)

KP.'iHIRSKIY, V. G.,, ke-nd. tekhn. nauk; VASILIYLV, Yu. A., inzh.
Some results of the pyrolisis of brown coa-I from the Easiparn Fegions
of the U. S. S. R. Izv. vys. uch6b. zav.; energ. 7 no.5:122-126
My 164. (MMI 17:7)
1. Saratovskiy politekhaicheskly institut. Predstavlena kafedroy
promyshlennoy teplotekhnikl.

BARAYEV, S.G.; VASIL'TfV, Yu.A.
Lifetime of rotors and swivels. Mash. i neft. obor. no.9:3-7
1614- (MIFA 17:11)
1. VIIIIPTneftemash, Baku.

RAYKHER, L.D.; VASILIYEV, Yu.A.; KHAFAZ, I.I.
Method and technique of field work using the plane front method.
Neft. i gaz. prom. no.3:11-13 Jl-S 164. (MIRA 17:12)

RAIKIMR, L.D.; VASILIYEV, Yu.A.; KHAIILAZ, I.I.; SAGALOVA, Ye.l.
Disturbances in pattern shooting on larCe prospectling areas.
Razved. i okh. nedr. 30 no.3:44-48 Rr 164 (HIPA 18:1)
1. Ukrainskiy rauclmo-issledovatellskiy geologorazvedochnyy
inatitut.

ACCESSION R. APS0102ft UR/0307/65/000/006/0010/0022
5 rtf) . 3
AUTHOR-. Eende Ya. Vasil'yev, Yu. A. Raykher, - D. ; Yharaz, 1. 1.
TITLE: Elements of the theory of variable control of sei!imic wave fronts
.SOURCE: AN SSSR. Izvestiya. Fizika zen~li. nmo. &, 196-5, 10,02
7-
--TAGS~ loration, hodograph
seism'ic- wave,. shock wave -fronts geologic exp!
iABSTRACT: The theory of controlling the shape of seismic wave fronts by active in-
iterference of waves at the source of elastic vibrations -,- studied. This interfer-
I
-.ence is acconplished by grouping charges over short distarces, or by directed
jinear wave sources. An analytic solution is obtained for the Erect and inverse
three -dimens i onal problems of se smic prospecting by the reflec-ed wave inethod.
,Point, line, and surface sources am discussed in detail for an arbitra.-y configura-
tion of the reflecting surface. it is shown that a thme-dimensional travel-time
-,curve can be produced for a reflected wave with a predeternined shape by construct-
Ung a null la chron of the corresponding configuration. It is sho"n) that the coor-
!,dinates of tho null isochmn are continuous and single-valied flinctions :~f tho. -cor-
dinates of the re"'1--tIng surface anrl tra-el-time ciirve
Card 1/2

L 69_974-65
1ACCESSION I;R: AP501.8286
rcfl(~(Ac,d wav,~, Thi~ will izior-hroi-,, Fiurfacp, vi~ tra,'el-ime Curve 'Of the
Elect wljvf_~ iire of' a if I.Y') .14
Eire -given, the tbird can be uniquely detertained. An dnalj L JL'a
for the delay tirne which must be used with a grouD of charges in ordt-r to obtain
ithe travel-time curve in d given form. 'riF. irt, h-3~ : 31 f ormu ',3:-, f i F u-es
A,-,", Cf'A k-iv a--?oIIcpo~azv,?ri,)chry-j insli-ut
!SUBMITTED: 12,jun64 EN C L 00 E
JTO REF SOVi 006 OTHER! 000
--------- --

S I L
22U1
S/08 60/009/006/001/011
B102YB212
AUTHORS: 4611'yev, Yu. A., Zamyatnin, Yu. S., Sirotinin, Ye. I.,
Pomushkin-,--E-.-F-.-
TITLEt Spectra of fission neutrons from U 235 emitted at angles of
0, 45, and 900 to the direction of flight of the fragments
PERIODICAL: Atomnaya energiya, v. 9, no. 6, 1960, 449-454
TEXTt The results of previous measurements of spectra of fission neutrons
and their angular distribution with respect to the direction of flight of
the fragments agree well with theoretical data (based on an assumption of
isotropic neutron evaporation and Maxwell neutron distribution); but this
theory furnishes values for the mean kinetic eriergy of the fragments,
which are somewhat too low, and, therefore, th(! correctness of above X
assumptions may be doubted. In order to check it the authors have
measured again the neutron spectral and this paper r8ports on the results.
The spectra of the neutrons emitted at 0, 45, and 90 to the direction of
flight of the fragments in 14.3-Mev neutron induced U235 fissions have been
measured, and also their angular distribution has been determined. The
Card 1/7,

S/og;*0/009/006/001/011
Spectra of fission neutrons... B102 B212
time-of-flight method was utilized, the distance of flight was 75 cm and
the resolution time 7 m/tsec. A detailed description of this method and
the equipment used is given in Ref. 9 (Yu.A.Vasillyev idr. Zh.eksperim. i
teor.fiz. 38, 671 (1960)). However, the method employed here made use of
a multi-layer fission chamber with fragment collimation as a fission-
neutron source. A U235 layer had been deposited on both sides of an
aluminum fT (having a thickness of 0.5 mm); the thickness of the layer
was 6 mg/cm , and the total weight of the two layers amounted to 3.5 9-
0-75% of the fission taking place in the uranium have been recorded. The
chamber was filled with a mixture of argon and carbon dioxide 00%)
(pressure 760 mm Hg). The rise time of the pulnes was about 0.1/Lsec at a
1 kv electrode potential. Fig. 2 shows the experimental setup. 0Fig. 03
shows the neutron spectra F(En ) in arbitrary unIts measured at 0 , 45 , and
900. Fig- 5 shows the spectra of neutrons emitted from the fission frag-
ments. The angular distribution has been calculated by numerical integra-
tion with respect to the neutron energy (of. Table). The angular
distribution of the T rays (ET > 0-3 MOV) produced during fission has also
been c&jpulated by assuming an isotWpy relative to the direction of flight
im. i

t~ui' J11-J, "U. II T
Spectra -of fission neutrons... 3'102~3'212
(Ono
(45'),:n
of the fragments. Here are the values obtained: r-'~
(1-31+0-07);(1.22+0.o6):1.00. The neutron distribution showed a con-
siLderabYe anisotrop-y: b - N(O')IN(90') - 3.23-+0.12. The following
14
value has been obtained after subtracting the neutrons evaporated before
a fission bt -~ 4.03 :t 0.23; this value agreea within the limits of error
14
with that obtained for -thermal neutrons (b t . 4.35�0.19). In order to
describe these experimental results theoretically, calculations have beOn
done and various assumptions have been made regarding the neutron spectra
in the coordinate system of the fragments. However, no variant.was able
to yield satisfactory results that agreed with all thre e spectra which
have been examined. The authors thank P. V. Toropov, Yu. Ya. Glazunov,
A. N. Maslov, N. I. Nemudrov, V. A. Parshina, V. S. Khorkhordin,
V. A. Komarova, M. P. Novikova, G. A. Peretokina, and L. A. Chernova for
assistance. There are 6 figures, 1 table, and 14 references: 6 Soviet-
bloc and 8 non-Soviet-bloc. The three references to English-language
publications read as follows: Rbf. 7: W.Stefn.Phys.Rev. 108, 94 (1957);
Ref. 10. S. Whetstone. Phys.Rev., 114, 581 (1959); Ref. 12: J. Terrell,
Card 3/1&
ly

S10891601009100610011011
S-pectra of fissi n neatrons... B102/B212
Phys.Rev., 1.U9 127 (1959) -
SUBMITTED: Feb uary 29, 1960
235
Legend to Fig. 2t 1) U laydri
2 deuteron beam; 3) target;
4~ collimators.
CR
03yi<
so
M PT"
12
of 0
Card

L 217~,3-66
L,6002919
L. D,; Benderskjy, Ya.; I lu~ va-,7j-~~Otu) .,J, Do;
-arUZY 1. 1.; Ghervonskiy, 1.1,
nono
TI'kL,*-,*: A met-hod for seismic exT)loration. 'Class 42, ido. 177103 Zra-nnouncel
a -a Institute (Lv--rain3;ziy nauchno-
kra~nit-,n Sc`an~ific Ro5oarch Goo-logical ZxT lor tio
,eo1oGorazvedoChnY,-f in3ti'U
'OURCE: 3yullaten' izobreteniy i tovarrkvkh znakov, no. 21,, 1965, 82
TOPIC TAGS: seismo=-P~Y a smology
: This Author Certificate presents a method for seismic exploration with
tho use o--:' controlled directional excitation systuens (operating along any specified
pi-irc-Ijilo) and systeras of vibration reception. The method increases the e.'?GC'%,iVO-
A, -ion of seismic iravos from the irra-
noss o' ox.Dloration and provides a uniaue select
di,-,~od o*U-Jocts. The intorferonco oystoms in the vibration reception are coordinated
with lrt,~i-frjronce sYsteras of the vibration excitation. This is accomplished by
surzing, up displacemoats of any number of recordings based on a previously specified
rellit"Lonship which agrees with the vibration excitation principle.
SUB CODE: 08/ SUBM' DATE: 20Jul64
Card 1/., UDC: 550.834

VASILIYEV, Yu.A.; RATKILEM, L.D.; SAGALOVA, Ye.1,
Conditions of formation of a sun wave Induced b-
y a I in ear
arrangement of explosion points. Izv. All SSSR. Ser. geofiz.
no.8*-1195-1203 Ag 164 OMTRA 17t8)
1. Ukrainskiy nauchro-issledovateltakiy geologorazvedochn-
institut. yy

MAKAROV., Petr Vasillyevich, prof.; :VASIL'YEV, Yu.A., red.
(Chemistry of the cell) Khimiia kletki. Leningrad, Ob-
vo po rasprostraneniiu politicheskikh i nauchnykh znanii
RSFSR, 1963. 56 p. (MIRA 17:5)
1. Chlen-korrespondent P1411 SSSR (for Makarov).

VASILIYEV Yu A
Solution of the direct spatial problem in the reflection method
of seismic prospecting in the case of linear source of
vibrations. Izv. ?f SSSR. Ser. geofiz. no,3:397-405 Mr 163.
(MIRA 16:3)
1. Ukrainskiy nauchno-issledovatellskiy geologorazvedochnyy
institut.
(Seismic prospecting)

KISELI, F.M.; VASIL'YEV, Yu.A., elektromek-hanik
We have facilitated the servicing of long-distance communication
apparatus. Avtom. telem. i sviazt 8 no. 3:34-35 Mr 164.
(MIRA 17:5)
1. Starshiy elektromekhanik Leningrad-Vitebskoy distantsii
signalizatsii i svyazi Oktyabr'skoy dorogi (for.Kiself).

ZISILIYEV, Yu.A
Share of hcdographs of reflected waves in t2e case cf L 2Lne-~r
source of fluctuations. Geofiz. sbor, no-3:19-24 162.
(MIRA 1519)
(Sei3adc prospocting)

RAMER, L.D.; BENDERSKIYp V.Ya.; VAS11,1YL-V, Yu..k.; KMIZAZ, T.J.
Increasing tha goolrogical efficiency of' elsmic pronpecting Aln
the inner zone of the cis-CarIxithihn trvigh and the southwestern
part of the RiissUn Platform. Neft. i gaz. prom. 3:12-1-4
J:L-8 165- (MTRA 18:11.)

VASIP YEV. YXI .-.-A-.I- A T1711 .
FI-100 diesel electric.- rower plants, Enerpomashinozztroenle (
(fl-- !.: '~)
rIo.P:I..P Aff '(C ' . . -' .,-, .1
(Electric power plants) (DIPsel f-ni,.*,nvs)

VAsIT,,yHv,_.Yu.A..; PAYMER, L.D,; S.AGAIVIA., Ye.l.; KIIARA'/-', I.L
Thq flat frcnt techniqljo In t~.e method jlr reflected -wa-ires.
Prikl. geofiz. no-38:~5-"/ '64. 118: 11)

ACC NRI AR6016962 SOURCE CON: IJR/0169/65/000/012/DO22/DO22
AUTHOR: Raykher, L.D.; Yasillyev, Yu.A.; Kharaz, 1,1.; Gasilov6kiy, K.S.; Sagalova,
Ye. 1,
TITLH-. Methodology'of flat front (SPP),and central rays (STsL) work techniques for
regions with complex seismological conditions at depth
SOURCE: Ref. zh. Geofizlka, Abs. 12D146
R13F SOURCE: Tr. Mr. n.-i. geologoz:azved. in-t, vyp. 10, 19651 3-9
TOPIC TAGS: seismology, seismic prospecting, flat
front seismic prospecting, central rays seismic pro;pecting
ABSTRACT: Results of research for the establishment of theoretical bases, methodolojox
ind observation techniques for the use of the STsL anti the SPP methods for complex
seismological conditions are presented. The basic volume of STsL work was done within
the limits of the outer zone of the Precarpathian deflection (9.1 km) and in the Post~
carpathia (3.6 km). The distance between PB was taken as 100 m; a mixed grouping of 31
seismic dotectors on a base of 30 and 60 m. was used. Use of this method both for re-
con and for detailed search is noted. Combination of the method with ordinary profili.
ng is useful. Por SPP, theory of spacial interpretation was developed and optimum se-
quence of operations determined for field work, SPF can be used either with profiling
or independently in those cases where common methods do not guarantee the necez5ary
reliability of the results. [Translation of abstract].
Card IZI SUB CODEt 08 UDC: 550.834,5

ACC NR, AT6028962 SOURCH GODL: n/0000/65/000/000/00.Q3/0025
AUTHOR: Raykher, L. D.; Vasillyev, Yu. A.; Kharaz, 1. 1.
!ORG:. Ukrainian Scientific Research Institute of Geological Prospecting
(Ultrainskiy nauchno-issledovatellskiy geologorazyedochnyy ipAtltut)
;TITLE: Application of linear vibration sources in the method-of
;reflected waves
SOURCE: Vsesoyuznyy seminar po novoy metodike seysmorazvedVi',-'.
Seysmorazvedlca s. ~k imeneniyem gruppirovaniya vzryvov na dlinnykh bazakh
i sposoba tsentrallnykh luchey (Seismic prospecting using the.grouping
of shots on long bases and the method of central rays); trudy-aeminara,
Moscow, Izd-vo Nedra, 1965, 3-25
TOPIC TAGS: sciGmic modelinr,, seismic prospecting, seisjnori~hphy,
underground exploGion, geologic cxploi,atlon, seismic wave C
ABSTRACT: An analysis is made of travel-time curves of refl:ected waves
generated by linear sources obtained by the plane wave-front thethod
(SPF) and the directed plane wave-front method (UPF). It i&.-~pinted
out that the shifting of the reflected wave limits the uae of SPF, and
in regions with steeply sloping interfaces it is advantageoi4i.'- .to use
UPF. In tracing faults the use of SPF and UPF makes it posa-ible.to

ACC _R R:- AT 6-0- 2 8 9-6-2-
impr.ove detection of diffracted waves from the different sbapej-of the
tray4l-time curves for reflected and diffracted waves, The-choice o.L'
the:.thot-point parameters takes into account generation of int.er_.
ference and noise, the curvature of the reflecting interface.-b-a.nd the
specific characteristics of the amplitude field of the refldc''ted wave.
By varying the shot spread parameters, it is possible to attenuate the
even'waves in the upper part of the cross section. Under la*boratory
conditions SPF and UPF may be compared by summing using special vibra-
tion'patterns from single explosions within the geophone spz~ead.area.
Studies are made of the method of processing seismograms, tlie- inter-
pretation of observed travel-time curves and their corrections,.and
methods of compiling cross sections. Analysis is performed'of-.,the
accuracy of determination.of gootectonic structure by SPFA UPF;.and
profiling by MOV. An example of successful use of UPF is g~4enjor a
region with a complex geological structure, Orig, art. has-.,..*9 figures,
and 9 formulas.
SUB-,.&ODE: 08/ SUBM DATE: 30Apr65/ OHIG REP: 017
c,,,,' 2.12

ACC N.Rz AP6025661 SOURCE CODE: uR/A13/66/ooo/013/0126/0127
INVV,"IOR: VenedIiktov, V. A.; Yaqillyev, Yu. A.; Popov, N. 1,; 14arke1ov, Ye. V.;
1Veynblat, Mj. Kh.; D'yakov, A. P.; Shishakov, K. I.; Yusim, L. Ya.; Skyortsov, A. 114.
Xireyev, Yu. A.; Guzanov, G. N.; Gerasimovich, S. G.
ORG: None
TITLE: A fluid device for damping torsional vibrations. Class 47, No. 183539 (an-
nounced by the Turbine Motor Plant (Turbomotornyy zavod)]
SOURCE: Izobreteniya, prorpyshlennyye obraztsy, tovarnyye znaki, no. 13, 1966,
i126-127
TOPIC TAGS; vibration damping, ~Wdraulic device, torsional vibration
ABSILRACT: This Author's Certificate introduces a fluid device for damping torsional
vibrations. The unit consists of a housing with a hole for fluid delivery and a
movable annular disc with a compensating cavity set inside the housing. The instal-
lation is designed for more reliable and simpler filling of the unit with fluid by
providing the faces of the disc or the internal surface of the housing opposite the
hole for fluid delivery with at least one annular groove connected to the compensat-
ing cavity by channels in the disc body.
UDC; 621-752.2

!: ACC NJ I AP6025 61
i - !
N

GAGIMINA, Ye.G.
FIOSHIII, M.Ya. -, jA
Influence of the nature of the cation on the J5,olbe alectrosynthesis.
Dokl. Ali SSSR 135 no.4:909-912 160. 1 (MiRA 13:11)
1. Institut elektrokhimii Akademii nauk SSSR. Predstavleno
akademikom A.N.Frunmkinyri.
(Reduction, Slectrolytic) (Oxidation, Electrolytic);
(Acetates)

FIOSHIH, M.Ya.; GIRDIA. r..P.-. VASILIYEV, Yu.B..-_KHRULEV, M.V.; FOLIYEVKTOV,
M.K.; ARTEMIYEV,.-AXr. -
Additions of alcohols and their effect on Kobe's electrosynthesis.
Dokl. AN SSSH 140 no.6:138841391 0 161. (MIRA 14tll)
1. Institut elektrokhimii AN SSSR. Predstavleno akademikom A.N.
Frumkinym.
(Chemistry, Organic--Synthesis) (Blectolysis)

FIOSHIN, M.Ya.; VASILIYEV, Tu.B.
Kinetics of anodic and chemical reactions in Kolbe electrosynthesis.
Izv.AN SSSR.Otd.khim.nauk no.3s437-446 Mr 163. (MIRA 16.4)
1. Institut elektrokhimii AN SSSR.
(Chemistry, Organic--Synthesis) (tlectrolysis)

VASIPYEV, Yu.B.; BAGOTSM, V.S.
Electrolytic oxidation of formic acid and its oalts on a rotating
platinum electrodes Dokl. AN SSSR 148 no.ltl32-135 A 163.
(MIRA 16t2)
1. Institut elektrokhimii AN SSSR. Predstavleno akademikom
A.N. Frumkinym.
I(Formic acid) (Oxidation) (Electrodesj, Platin=)

VASILITEV, Y4,B., kand. khim. nauk; FSHENIGOIKOVO A.G,, kand.
nauk IF
International Congress on Electrocherdstry in Moscow. Vest.
AN SSM 33 no.12:55-57 D 163. (MIU 17:1)

YAO LU-ANI [Yao Lu-an]; VASILtYEV, Yu.B.; BAGOTSKIY, V.S.
Electrochemical processes in the system quinone - hydroquinone.
Zhur. fiz. khim. 38 no.1:205-208 JaI64. (MIRA 17.2)
1. Institut elektrokhimii All SSSR.

BESKOROVAYNAYA, S.S.1 VASILIYEV, -'- Yu'B.; BAGOTSXIY# V.S.
Adsorption of aliphatic alcohols on a smooth platinum electrode.
Elektrokhimiia I no.6x6q.1-695 is 165. (MA 18:7)
1. Institut elektrokhimii AN SSSR.

KHAZOV'~Ij O.A.4 VA.',11,'Y'l~,V, YU.B.j V.S.
y
Adsorption of ~Lthanol on a sm"th platin-um electrofle.
1 no.1:84-89 Ja 165. (AURA 18-5)
1. Institut elpktrokhimiJ. AN

MAZOVA, O.A.; VASILL'YEV, Yu.B.; BAGOTSKIY, V.S.
Effect of the adsorption of foreign ions and molecules an the
oxidation rate of organic substances on a platinum electrode.
Elektrokhimiia I no.4:430,-445 AP 165. (,MIRA 18:6)
1. Institut elektrokbiml.1 AN SSSR.

VA
a T I C, ,;
f
j t 1 TI! J.
al,lt:'-ries ani carlix--xYlit, Wit,, n
st,rfuce inh.cmogerle--Ly ufC Ule 1:1ritin'.-al.

MIAZOVA, O.A.; V~I'YIV,_.Yu,-B,.; BAGOTSKIY, V.S.
Electrolytic oxidation of organic subst-ences cn a platim=
electrode. Report 1: General aspect of potentiostatic Clarves
and the nature of inhibition of electrochemical oxidation processes.
Izv. AN SSSR. Ser. khim. n0.911531-1539 165. (MIRA 1819)
1. Inatitut elektrokhimli AN SS~SR.

YAO Ll.'-AW rYa.,,
0
K iw~ -i
nonpartio~ pat,"' ng in n.

YAO LU~I-AN' [Yao Lu-an]; KAZARINOV, V.Ye.; VASILIYFV, Yu.B.; BAGOTSKIY, V.S.
- "': "'. - -.4 ''
Effect of adsorption on the rate of processes taking place on a platinum
electrode in the system quinone - hydr~qidnone. Dokl. AN SSSR 151
no.IsI51-154 JI 163. (MA 16:9)
1. Institut elektrokhimii AN SSSR. Predstavleno akademikom
A.N.Frumkinym.
(Quinons) (Hydroquinone) (Adsorption)