SCIENTIFIC ABSTRACT RUDAKOV, V.I. - RUDAKOV, V.V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001445910013-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 20, 2000
• Sequence Number: 13
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

RUDA inzh.; 3:ICIJ M"OV, T.
in7h.
-echr-.-ization of t~e workir Un
of frozc:. ground in the State ion
Tr=t for the DesiEn and Conotrunticn of Hydraulic Structures.
i dor. mash. 6 no.10:1.(--lu" 0 "al. (~m-u 14: 10)

SKABALIANOVIICH, I.A., kand.tekhn.nauk, dotsent; RUDAhOV,._,V.K., inzh.
Prediction of' tYe flooding and re!~haping of the tboresof the
reEnrvoir oil t~,e DneprodzerzhinE~ Pydroelectric Power btation. Izv.
vys. ucheb. zav.; energ. 4 no.lC:116-122 0 '61. (FIRA 14:11)
1. ilauchno-issledovatel'skiy institut geologii DnepropetrovsLogo,
govuniversiteta.
(Dneprodzerzhinsk Hydroelectric Power Station)

RUDAKOV, V.K., inzh.; TUMENKO, N.R.
Calculating the rise of ground water in a land mass between rivers
as a result yf the creation of a reservoir. Gidr. stroi. 32
no.2:35 F 62. (MIRA 15:7)
(Water, Underground)

14(6) SOV/98-59-4-7/17
AUTHOR,,, Gryaznov, V.I., Candidate of Geological and Minera-
logical Sciences, and Rudakov, V.K., Engineer
TITLE- The Rate of Washing-Away of Loess Banks of the Kakhov-
ka Reservoir (Razmyvayemost7 lessovykh beregov Kakhov-
skogo vodokhranilishcha)
PERIODICAL: Gidrotekhnicheskoye suroitellstuvo, 1959, Nr 4, pp
32-33 (USSR)
JLBSTRACTi The authors give a more precise definition of the
formula of Ye.G. Kachugin to determine the washing-
away grade of the above-mentioned banks. Proposed
Etb 9
in 1955, this formula looks as follows: Q=k
1
p
whereby Q is the volume of the washing-away rock in
cu M; k is the washability coefficient in cu m di-
vided bypton-meters; E is the wave energy per year.
in ton-meters; t is the number of years; b is the
power indicator,, less than 1. For loess-like ground-
F5
Ye.G. Kachugin cites the following values: k =25-l
-
p
0-5m'-'/to
47 x 1 n-meters. The correction was rendered
Card 112 possible by way of new kno,.,iledge gained through recent

SOV/98-,59-4-7/17
The Rate or Vlashlng,-Anay of Loens Banks of the Kakhovka Reser-
voir
observations on the washing-away phenomenon of the
Kakhovka reservoir. This study was carried out by
IV-he Nauchno-issledovatel7ski-Y institut geologii
Dnepropetrovskogo universitu'eta (Research Institute
Geology of the Dnepropetrovsk University) in. co-
operation with the Ukrainskoye otdeleniye instituta
"Gidroenergoprcyek,"*"' (Ukrainian Section of "Gidro-
energoproyekt" Instit~te') during the period 1955-
1957. The formula of Ye,G. Kachugin was incorrect
as it could only be used for calculation of low
banks with sand bars,, However, steep banks, as it
was learned meanwhile, are subject to a much strong-
er washing-away effec-"-. Therefore, the washing-
away data on the banks of another reservoir, the
Dnepropetrovskoye vodokhranilishche (Dnepropetrov-,9k
Reservoir), were ascertained by the newly-amended
formula. There is I graph and 1 table.
Card 2/2

(Sibay region-Breacia)

AID P 2157
Subject USSR/Engineering-Electricity
Card 1/1 Pub. 28 8/9
Author V. N. Rudakov
Title Automatic remote measuring instrument for weighing
and indicating level of liquid in tanks
Periodical: Energ. byul., no.5, 28-29, My 1955
Abstract This device is built on the principle of the changes
in the weight of a submerged body according to its
submersion. A floating vertical pipe is freely
suspended inside of a tank and connected with an
outside measuring instrument. The results are
telemetered to a galvanometer located in a control
point. Two sketches accompany the text. The author
was awarded second prize in a competition for
suggestions on the more economical consumption of
electric energy and fuel,
Institution: None
Submitted No date

GLUKHAHOV, N.P.; KOVAINVSKAYI. Ya.P.; KRYLOV, K.I., prof.; MURAVIYEVA, G.Ys.;
RUDAKOV, V.M.; SMIRNOV, P.S., tekhn.red.
[Ieboratory work on electromagnetic fields] Isboratornye raboty
po elektromagnitnomu poliu. Pod obahchei red. K.I.Kr7lovs. Lenin-
grad, leringr. elektrotekhnicheskii in-t im. V.I.Ullianova (Unins),
1957. 246 p. (KMA 11:7)
1. Zaveduyushchiy kafedroy "Teorii elektrichestva, magnetizma I
stroyeniya materiiw (for Krylov)
(Electromagnetic theory)

z - -T
AUTHOR: Dogramadzhi, M.F. and IxUdakov, V.N. 136-5-8/14
TITLE: Magnetic field and state of the surface of fused me-tal in
the electrolytic.bath. (Magnitnoe pole i sostoyanie pover-
khnosti rasplavlennogo metalla, v elektroliznoy vanne.).
P I-LIODICAL: "Tsvetnye Metall'711 (Non-ferrous Metals) 1957,-No.-
A
pp. 50 - 54 (U.S.S.R.)
ABSTRACT: The object of the work described was to-find ways of
reducing the influence of magnetic forces in electrolyzers.
The work was carried out jointly by the All-Union Aluminium-
Magnesium Institute, the Leningrad Section of the Tyazhprom-
elektroproekt Organisation and the Leningrad Electro-technical
Institute (Leningrad Elektrotekhnicheskoy Instuitut) in 1955-
1956. Part of the work consisted of an analytical calculation
of the magnetic fields in the electrolyzer bath. These calcu-
lations showed the part played by cur-rents in the different
parts of the bath in the generation of its general magnetic
field and suggested ways of finding rational lead designs. The
influence of current flowing in the leads is to disturb the
symmetry in the distribution of the magnetic field, this being
Card 1/2 more noticeable in lower-power baths. Direct measurements of
the magietic field on working alectrolyzers were made with the
aid of a graphite-cased, water-cooled instrument. Results are
tabulated for a 62 kA bath and similar measurements are said

SOV/137.-59-3-5513
Translation from- Referativnvy zhurnal, Metallurgiya, lq59,
Nr 3, p 82 fUSSR)
AUTHORS. Rudakov, V - N -, Murav'yeva, G - Y;~
TITLE: On the Effect of Magnetic Fields or; the Contour of the Surface of
Liquid Aluminum in Electrolytic for the Production of Aluminum
(0 vliyanii magnitnykh poley na fo-rnu poverkhnosti zhidkogo alvumi-
niya v elektroliznykh vannakh d1ya polucl-.eniya alyuminiya,l
PERIODICAL: Izv. Leningr. elektrotekhn. in-ia, 1958, Nr 34, pp 172-187
ABSTRACT: The author studied the effect of thc ma~znetic fields formed by the
electric current flowing through -1- busbars on the contour of the
surface of liquid Al during its el e.:- rol. vsis. The difference in Al
levels at the opposite ends of t~e el, -Jrolytic bath 11EB) on the average
is 2.5 crn but on certain occas:,-,r-s .-.t -ins ~;- 6 crn and even 9- 10 crn.
though for normal work of EB tl-,e dstnce from the lower surface
(base) of the anode to the surface of the Al (interpolar distance)
should be 4-4.5 c~m. Deviation in et.her sense causes an overheating
of EB and increases the specific consumption of energy. The inves-
tigation was carried out on an electrical analog of the electrolyzer bv
Card 112 using a sand bath. EB parts were prepared from a mixture of sand

SO V/13 7- 59-3 - 5513
On the Effect of Magnetic Fields on the Contour of the Surface of Liquid Al (cont.
and graphite. Recommendations for the design of busbars for EB in aluminum
plants are given.
V. A.
Card 212

84494
S11 12,/59/000/014/0,73/08-5/
7e6 0(/ 0 3,~-, Z, /,/,~ 2-) A052/AOO1
Translation from: Referativnyy zhurnal, Elektrotekhnika, 1959, No. 14, p. 245
30282
AUq.iORS- Krylov, K. I., Rudakov, V, N.
TITLE.- Application of Michelson's Interferometer for Determining Electri-,
Parameters of a Substance at Ultrahigh FrequenciesB
PERIODICAL: Izv. Leningr. elektrotekhn. in-ta, 1958, No. 36, pp. 139-149
th
T=.- Application of Michelson's interferometer for measuring ~ e
dielectric constant and tangent of dielectric loss angle in UHF band is described.
The measurements are carried out on a 3.2-cm wavelength. Calculation formulae,
are derived and an example of determining the parameters of a dielectri-r -fTDm
experimental data is given.
Ye. B. Z.
ranslator's note: This is the full translation of the original,Ru
T s San
abstract.
Card 1/1

S/105/60/000/07/09/027
B007/BOO5
AUTHOR: Rudakov, V. N., Docent
I 0:04419119:=A
TITLE- The d-c Magnetic Field in a Parallelepipedon
PERIODICAL: Elektrichestvo, 1960, No- 7, PP- 39-41
TEXT: The author points out that an accurate calculation of the d-c
magnetic field in a rectangular parallelepipedon leads to very
complicated formulas, and presents a special computing operation.
It facilitates considerably the computation without introducing simpli-
fying assumptions. The method is described with the aid of Fig. 1, It
is shown that the determination of the vector of the field intensity in
the d-a magnetic field in a rectangular parallelepipedon consists in the
calculation of extensive but equal functions. Thus, the calculation of
the magnetic field can be much simplified by compiling a table of these
functions., Fig. 2 shows the ~ (X, Y) curves drawn on the basis of.the
tables compiled by the author. S. K. Kalinkin and L. P. Konovalova
assisted the author in compiling the tables for the functions.
There are 2 figures and 2 Soviet references.

S ov/~T - 10 -1 1 ;-V1
~AUTHORS - N.1 BogovodskIY2 V. V.
T1 IV I _E, Moa,,Li!~oments, of' Glael.er ThIckrionss by Electromac-n'--tic
Ml ~ f hods
PFR [ OD EGA L: nurria I temit, i.chesto.,; N z.1 V-1 , 1c)60, Vol I,
-10,
pl)
ABSTRACT: Th-2 P-oblem ~,_iroote during measurerrients of Ice layers In
~~he AntactIc as a part of' the International Geophysical
Yoar progr-am. Gravimetric -and magnetometric irnethods are
on-ly relat-.Ivc- wh1le the seismic methods are Imprac t -Leal
du,:,~ to a thIck datripintf, layer of' Snow. Thc, authors dis-
cliss, ~h-i,efot-e, the pos~;Iblllty of urlng vetarded, re-
flected electromagnetic signals. (1) Electromagnetic
propertios and 111-he st ructur-e of Ice: The authors review
the data abOUt thQ dielectric pePmi11,-tivI1Cy C and the
an 8 of' the angle of electrical losses in the
- ctrlc obtalned by Eder
d-le LE, (Ann. d. Phys., 1, 7 C),

,d 1/8
C cc, I -98. 194 They compare them to those computed
a t using the Debye equation

of' Gla(,.Jer Thlclkriess by 7 7 3
E Ic trorn-agnetic Mi--,thods SOV/5-1-30-1-101/18
9fj 4. C,X2
2
(2)
x
fo
Ife re 0 -is value of at f Is valUe Of
;J1,- Op'--ICal t*V~.~CjUencles (tip to the stuart of' electronic
d1sperslon); f'. 113 fr-(~qt.lency atu which reaches its
max Imum va lue .Taking the values of "he constants from
the work by Eder, I'he al-11-hors COMPLIted Table A. Assuming
~1 lineav temper-atUre chatige in the deeper layers of the
Ice,
t* = t'-- b (It - z), (5)
!ahere z is the, coord.1natle pe, Pendicular to "he glac.ier;
is temiperl-.tuve of' the earth bencath: b Is tenriperature
Ca rr'!

Measurements of' Glacier Thickness by 773-33
Electromagnetic Methods .5 OV/5, 7 -3 2/1
Table A
Die,lectric permittivity and the tangent of the angle
of electric losses of insipid ice at t = -100 C
(a) Frequency-f,(c~cles; (b) computed using the
Debye equation; c experimental data by Eder;
(d) experiments data by Pasynkov, Rudalcov, and
KholUyanov.
0 80.0 0.000
10 80.0 0.004
102 80.0 0.011 80.0 0.167 -
103 68*0 0.410 6-1.3 0.695 -
101 6.2 2.8W 11.0 2.195 - -
103 2.0 OSSO 2.0 0.721 3.2 0.600
100 2.0 0.086 2.0 0.222 2.0 0.140
107 2.0 0.009 - - 2.0 0.014'
Iw 2.0 9-10-4 - - 2.0 -
109 2.0 9-10-5 - - -
C, a rd 3/8 1010 2.0 9 - 10-f) - - 2.0

Measurementr, of- Gl.acler ThickrIC33 bY 77
.Elec tu romagnet IC Wthods SOV/57-30-1-12/18
g-adlent. Taking b 0.02 deg/m and t = -30 C, they
u U
calculated the relationship between the dielectric
permittivity and the distance from the surface of the
glacier (see Fig. 3).
Fig. 3. DleluctrIc permittivity of
the glacier vs distance from the 10-
SLIrfaC- of' the glacier: (a) at
f = 104 cycles; (b) at f = 108 f6 -
cycles; h Is the glacier 16--hick-
ness.
L M
Card 11/8 47 J00 1000 fivo 1000

~2 of Thickneiss hy
7 7 3 3 3
Me t hods -9 OV/5 7 -30 -.1 - 12/18
Th,~, aCithoro also note thal, thE: -'c,--, at 8; to -10 irr,
mndf~- t-hp surfaco of' 'tic. f
I _~lacler Is made mostly out
oC cry,-,ta.1s of 1-21 cm s1ze. No dat-a are available
Cot, deptho. Eloetromagn(~t.lc inves t- Igalk-, Ions of
wevc- made. only In the region of' light waves.
Pmpa(ratlon of electromal-metle waves In Ice: Since
"in 0. permIttiv.11-y of' liun to be complex:
C = e -ji, =-- E (I - j Ig ('1). (7)
M; 1 tiL,, Maxwe I I I P, (- quations, the authors obtain an
- I u
,aqua' Lot
-j for the, electric vector E (E b.f.)
AE tE --f-grad (E grad F) =0. (9)
C2
A,'..'3Ut11lnr, a slow vai-lftlon o I.' ritid taklng the wave
pi,opai-,utlon to be along th(. flie solution can be
obtained in the Simplified Cut,m
Ca t,d 5/8 E (z) (16),

Thickness by 77'33
M., thods SOV/ 57-30-1-1 2/18
VU2 -f-
tgfp=
wh(~re W It-, Eq. was fIVS' SUbstltuted by I
a r i~- u U G
k (X, y, -z)
,and then k was wvlttnn in a complex form
k (Z) (Z) J.3 (Z), (13)
For the time of return of the signalat high frequencies and
~.-lfflclenl.ly low temperatures, title aLlthorr, derive an
uppr ma q i i a " 1 o n 2nh (19)
c
Is Intlex o" v(,~fractlon. For h Km; n z: vfE-
V7, -r c om e s c u -. 'L-1 o b e 18 . ~) 1-1 Sc-c There ezists one
-i e I o a bs on by ice. An approKi.-
J.nd ot"' dimplnu- di orp, I
ca0d mut.e ClUatlon at. hIgh freqUenclen Is
lV,lh,==8.65,"' V-ht
~c (22)

I'! M. 3 OV/ JO-1
vi I w~ Illd 1) dc, no tf o f v,~ numbr- r o I' d c I be I Fo r
> -10 ,.Yc k~2, 'Carl and n = conot, so
-Ing
tlia'~ for In Km, lidl) O.uc) dl). Vic., scatter
anolu.h~.~r damping grIven by
V,lb, 2!.!L (23)
SWI, 12-4v2 (24)
3C4
I's the croso :;uction of scalut-e-r-Ing, and V
is th~-- vc-itirrie of sin~_,l(z CPY.Stals. A3 is known,
3 11-1 (25)
4% -t-2
-d 7/8

M, Ulod:, nv/~y- jo- I - 1-/ /18
A-:, $j m ; rip'. cm Nd 1) 0 . 0.1 d b a t f. = 10 8 c Y c I e 3 ,
but. lncreus~~!.~ rapidly 11o Ndbp --100 for f = 109 cycles.
The ai,il, ,hor,,, otlh(-~,r contrIbult-Jons ',-,o the damping
(partial 01-1 the or- alr--~now t;urface,
ri-Nection t'vom the Ice-ground SUr-face, waves
not, plane) trid conclude that "orX= 1 m wavelength,
,;h(., damping does. rio'u exceed 100 db. Wituh a 10-11-:w
I~encrLltor, one needs a receive of I~L vol'. sensitivity and
a 0.1- ~, SCC iMPL1120 St--CILI(?nc(, with pauses larger than

sc
C) ac, which Is, all technically feasible. The
notc. that the effects di:35CLISsed in the Present
pap(,~r pi-obabily the cause of 100 to 120 m altimeter
r,~ in .-I-Ir-pla-ties landingr on glaciers of that
appr~oxlm;.itc, t-1hJck-ncs,;. The uo,,hors conclude that there
probabl' ,,f a po.--31b11Lty Of' Using highly directional
mil'llnletc,-i, but ~,hat One first needs, experimental
Inves',11cations- Of' of such waves in Ice. The re
!--Ah1(J-; "Ind 6 referencesY 4 Soviet, I German.
3 UBIM I TTE D July 11, -9~~8
Ca,rd 8/8

RIUDAKOV, Vsevolod Nikolayevich; FERSIM, Maya Vasillyevna; SYCHEV, V.V..
N.I., teidm.
red.
red.; BORUFOV,
[Use of atomic energy in electric power plants] Ispolizovarde atoms
noi energii na elektrostantsiiakh. Moskva3 Gos. energ.izd-voj 1961.
158 p. (Nuclearreactors) (MIRA 14:12)

MURAVIYEVA, G.Yaot doteent,.kand.tekhn.nauk; RUDAKOV, V.N., dotsents kand.tekhns
nauk
Principle of duality and electric models of magnetic shields. Izv.
vysouchebezav.; energ. 4 no.502-39 W 161. (MM 14&6)
1. Leningradskiy elektrotekhnicheskiy institut imeni V.I.
Ullyanova (Lenina). Predstavlena kafedroy teoreticheakikh osnov
alektrotekhniki.
(Shielding (Electricity)) (Mgnetic fields)

3 7 7 G
S/139/62/000/002/001/028
E114/E435
AUTHGR: Rudakov, V.N.
TITLE: Electromagnetic method of stress analysis
P2.*,'1GDIC,XL: Izvcstiya vysshilch uchebny1ch zavedeniy. Fizilca.
no.2, 1962, 7-14
TS"--%'T: 'Nethods of principal stress analysis in transparent bodies
using polarized light are well-known. A.Dietzel and E.Deeg
extended this method in 1954 to 3 cm electromagnetic waves for
bou~ies transparent to such waves. The present article describes
the work carried out in the.Leningrad Electrical Engineering
institute imen� V.I.Ullyanov (Lenin) extending such technique to-
bodies transparent to i-iiillimetre electromagnet:Lc waves. This
.i--s the advantage of dispensing with models which cannot reproduce
internal residual stresses, if any are present in the specimen.
Lon-er wavelength help to cope with the difficulties caused by
small discontinuities in the material but longer wavelength also
;-.-.eans -reater interference, diffraction phenomena and poorer
resolution. A good compromise was considered to lie in the
;:-..illimetre range, Assuming that the test piece is thin and
Card 1/3

S/139/62/000/002/001/02U0
Electromagnetic -,iethod ... E114/E435
thlerefore only two principal stresses are present, an expression
i,.,as derived for the difference in magnitude of thd two principal
stresses; this is a function of a multiplier, which is constant
for a given experiment, and arctan of a number, to be determined
by the experiment, which is proportional to the ratio of field
strengths in the two principal directions. The multiplier is
proportional to the wavelength and inversely proportional to the
thickness of the plate and the optical constant of its material.
I-n the experiment a thin high voltage porcelain plate was clamped
between the transmittin.- and receiving horn antennae. The
direction of major principal stress axis was found by rotating the
tiro antennae together i-tith the receiving antenna at right-angles
to the transmitting antenna. At the point of zero reception,
the principal stress axis will be in the plane of the emitted
polarized electromagnetic wave. By noting the angle of the
trans.:ii-Lting antenna as the plate is held in the beam in a number
of reguldrly spaced posi-ti-ons, Isocli-nes and isochromes can be
-apped, showin- the direction and intensity of principal stress at
each point in the plate. "'By rotating the transmitting aer.-Lal
Card 2/3

S/139/62/000/002/CO1/028
E'Iectro-m,agrnetic method ... E114/E435
throu_--h 450 to the principal stress axis, the intensity of
electro:;:z;~nctic field can be measured in the two planes of
prLncipal stresses by the receiving aerial which is rotated
su~~_-bly. Bv substitution of these quantities into the equation,
;.-.e difference of magnitude of the two principal stresses was
C:etermined. As an example, the magnitude of the difference of
-,c -Wo principal stresses is mapped for a fired thin porcelain
:)late, one side of which was heat treated. The gradients in 'the,
fired plate were found to be less steep than in anunfired plate.
Tlic non-uniforia heat treatment caused non-uniform distribution of
-1:-~Idients. The method was found to be suitable for qualitative
and quantitative testing of porcelain. There are 6 fligureS4
ASSOCIATION: Leningradskly elektrotekhnicheskly institut imeni
V.I.Ullyanova Menina)
(Leningrad Electrical Engineering Institute imeni
V.I.Ullyanov (Lenin)
SUB""ITTED: December 6, 1960
Card 3/3

BOGORODSKIYJ, V.V.; RUDAKOV, V.N.
Electromagnetic methods for determining the thickness of
floating ice. Zhur.tekh.fiz. 32 no.7:874-882 Jl 162.
OML 15:8)
(Electromagnetic waves)
(Ice)
-:- ~-q

RIRIAKOV~ V,N,, kand, tekhn. nauk, doteen,
u
rh:ee histor4~al phases and composing p5r's of present-day
al~m'trodynamlcs. -Tzv, LET! no.48:3-1-6 163. (rURA 17x12)

--- ~ I

w
%
L :3Z ~3-65 EWT(1)1EP%(S-)41#VVf(' )AIM( )/EPF(n)4.APA(ii)~-2/FtC(-t)/Eii0
lip(
ACCESSION XR: AP5005325 6/Ol8l/65/0OT/C-W/065q/11:"i:
AUTHOR: Bogoroditskiyq No Pol Rudakdvi, V..No; Tairova Do A,
TITLE: Electric anisotropy in polarized ceramic materialslelectrets)-
SOURCE: 'Fizika tverdogo tela, v, To no, .29 19655 659-661-
TOPIC TAGS i polari zation c eramic m"ateriAl'i, electric ani s6tr opy elactret-
polarized structure. dielectric constant
'TRACT: To study the anisotropy.in.ceramic electrets made of T-150 material- the
BS
A
on-
authors used an electromagnetic poltiioscope~vith B-mm operwti4-wv-;T~
ngth
.~-Zv. VUZi--Fizika'-
2,$-Ti--2962)-.-----Tht~-investigs edpamp e,-.
n-a specla7 oca
tveen t-wa -antennas one of -vhL o
ch-.rAdiated:WAth therl-tece v
elec-tromMnetic vaves. When the:antenfia polarization-planes crossed the
electrr4uLgnetie signal could be receLired only,.-if the Investig 's -e ro ted
the planar polarization of the electrasagnetic'-vives-ptasing through:ite The,-latt
occurred vf"-n the veyes vare diffracted by local defects# and al a-- 6--fin the Y-- r e-s' e.
of anisotropy of the dielectric.c6astant. it the tatenna polarizati6a planes Ifers.'...'.
7
J Ccird - 1/2 ------

T 51 V
in tr
TT
.W!FUR

L 31915-66 E",'ITW)
ACC NR: AP6010727 SOURCE CODE: UR/0142/66/009/001/0090/0096
AUTHOR: Rudakov, V, N.; Aleksandrova, M. G.
ORG: none
T11'LE: Interference of electromagnetic waves in the space between probes in
SiLr- outfits
SOURGE: IVUZ. Radiotekhnika, v. 9, no. 1, 1966, 90-96
TOPIC TA GS: radio int rascope, flaw detection , rtr 0 r-,ro ml-)6 A-,r r/c
ABSTRACT: Four apgioximate formulas are developed for the intensity of the
received signal in a SHF intrascope outfit (see
T- figure) in which the specimen is placed either
El E -nitter T and receiver R (transmis-
between tranar
-Z sion system) or near transrr-dtter-receiver TR
Ila 0 (reflection system). The formulas were experi-
LR I R TR
11.14V ~416 mentally verified on a universal SFIF Intrascope
a
Card 1/2 UDG: 621.372.85Z.3.018.2

L J-1915--66
AGG NR: AP6010727
with abrasive material, plexiglas, and nietal-coated plexiglas specimens; the
formulas proved to be in good qualitative agreement with the experimental data.
Utilization of the interference phenomena enhanced the sensitivity and resolution of
electromagnetic flaw detectors and polariscopes. Orig. art. has: 6 figures and
22 formulas.
SUB CODE: 13, 09 SUBM DATE: 30NoY64
Card 2/2

(Wp* (k) _2/T_4A(h)
ACC NR: AP6015572 SOURCE CODE: UR/0146/66/009/00210018/0020
AUTHOR: Aleksandrovaj Mi G.; Zelenkov, A..L.; dak d
RU gXj_Ve 14t; Lebe evp A. 1.
ORG* :_~enifigrad Electro!:echnical Institute im. V. 1. Ul'*Yano (Lenin),.(Leningradakiy,
elektrot-e-11-n-Ickeskiy insFitut)
TITLE: Universal device for observing and recording r-f fields
SOURCE: IVUZ.. Priborostroyeniye, v. 9, no. 2, 1966,18-20
TOPIC TAGS:. diffraction camera, millimeter wave generator
has been'developed at"
)e,
ABSTRACT: An r-f diffraction instrument, the.radiointroscol
the Leningrad Electrotechnical Ins!4,tute imeni Lenin.for revealing structural details
of test materials. The introscop4P"consists of amillimeter wave klystron, trans-
-mitting and receiving ant,-nnas, and the associated detection and display units (see
Fig. 1).' A test sample is placed between the antennas in a frame, which is scanned
according to the pattern shomto the right.of the figure. The resulting diffraction',.
pattern is detected and observed on a long-persistence scope or recorded on film..__
For a transmitted pattern the antennas are placed coaxially, as shown; for a reflee t8
pattern they are placed side by side, with suitable decoupling. Fig. 2 shows a
pattern received at X - 8 mm from a polished disk (material not given], showing
layering and acrack. Besides defect detection,-the device can be used as a.polarima.
scope in dielectric studies; wavelengths*of 4, 8 or 32 mm are obtained by.changing.- -7-.,
Lgard IL3~ UDC: -620.179.18

I -
'L 2075-66
ACC NR: AP6015572
klystrons and antennas.- The authors regard the introscope a.powerful tool in
as
near-field diffraction studies, since theoretical analysis _
of this phenomenon. is
~
possible for only the most-tsimple obj ect geometries. Orig. ,,:-
. hasi
.A figures&
art
'
.
(SHI,

SUB CODE! 09/ SUBM DATE: l2Apr65/ ATD PRESS:

Card 3/3 FtA

L 11205-66 F-W~(d)/M(k)-2
ACC - NRt AP5026214 SOURCE CODEt UR/0381/65/000/004/0038/0040
AUTHOR: Rudakovs V. N.; Aleksandr1o4at M. Go

Ora: Leningrad Electrical Engineering Institute imeni V. 1. Ullyanov Lenin (aln-
gradskiy elektrotekhnicheskiy inatitut)
TITLE: Radiovave endoscopy of bodies with complex profile
;SOURCE; Defektosko n
piya, 6,4i,1965, 38-40
:TOPIC TAGS: radio wave absorpt an ric material,
I electronic tEst equipment, dielecii
set e diation a tug
niconducting mat rial, irra ppara
'ABST e ciibe~ a simple method of'investigating.the gross structure,
RACT: Th authors des'
'dj' a

I i centimeter. and kilimete, ra ow ves Jt
of bodies with complex prof le us ngi r
i ustrial
_o reveal various kinds of-deficts n- Ind dlelectilc's. and seiiic6ndItetois.
ar I el by the
,their method, objects with complex*profile,must'first be,made plane p a
l.1t
l
addition of special attachmenti having the same dielectric'perneability as the spec.i-"
pen being tested (figure 1). The roblem consists of direct.
,p Ing the emitted itave withm
in the specimen parallel to the-upper boundary surface of the specimen. The angles oi
d
refraction 0 and incidence 0 are Interrelated by the formula
d
sine/sine n
,
(n21--index of refraction of second sodium relative.
to the first).' According to the
formula, the requir-emut that:the radl ation be-parallel to the upper boundary, neceisI7-

620.179.414.*621.396.99
Card .1 2 UDC;

. ~- ~ ~~ Ff - - -. -,; - - -

SOV-98-58-2-2/21
AUTHORS: Vorc-Likin, I,N.~ and Rudakov, V~N., Engineers
TITLE. On the Pousibility of ErectinK-b,,,z-Without Cofferdams (C
vozmozhnoz!t-.L stroitel'stva plotin bez peremychek)

PERIODICALi Gidrotekhriicheskoye stroitelistvo, 1958;Allr 2, pp 6-11 (USSR)
ABSTRACT: Vie article deals with posaible methods of erecting hydro-
teshnical siructures without a cofferdam. These methods are
based on exp6riense gained in the construction of the bridge
over the Yarg.-ze river at the town Ukhan' in Red China$ where
reinforced concrete pipes were used for erecting bridge
pillars- The essence of the method and the sequence of
operations are described, A metal spatial framework is
placed betweer~ the pontoons. The framework serves to set
the reinforced concrete pipes and to establish a cylindrical
pLle fencing, Vte pipes, of an outer diameter of 155 ems
are lowered through the framework to the alltivium and the
bedrock (Diagram 1).. The author describes the use3 made of
submerged concrete, concreting, etc. By using the above-
mentioned method, cne may in a number of cases dispense
with erecting the usual cofferdam (Dia6-ram 3). Diagram 2
Card 1/2 pictures th.e possible construction for a dam and screen when

on the Possibility of Erecting Dams Without Cofferdams SOV-98-58-2-2/21
using concrete buttresses erected on the principles used in
the Ukhan! bridge. Such buttresses establish a reliable
junction of the dam screen with the underwater foundation
at any depth, The author also gives tI-e sequence of oper-
ations by which such a dam is to be constructed. Figures
4 - 7 show how the problem of linking a cofferdam with the
foundation is being solved.
There are 23 diagrams.
1. Dams--Construction 2. Reinforced concrete--Applications
3. Pipes--Aop.lications
Card 212

10(4), 24(5) SOV/98-r59-0-8/29
AUTHOR: Golltsman, V.Kh., Rudakov, V.N. and Rubina, A.L.7
Engineers
TITLE: Determination of Vertical Reactions on Flexible Grounds
PERIODICAL: Gidrotekhnicheskoye stroitellstvo, 1959, Nr 9,
pp 27-33 (USSR)
ABSTRACT: The authors consider conventional statistical methods
for computation of reactive forces caused by pad foun-
dation pressure as idealized. They try to bring some
new ideas to this field of theoretical mechanics, -
usin~,also' preceeding works prepared by P.L. Paster-
nak _ef 1), P.P. Laupman and V.S. Eristov, (Ref 2),
by taking into account bending of the foundation and
the plasticity and non-uniformity of the ground. Se-
veral formulas based on these principles are given.
There are 3 graphs, 1 set of diagrams and 3 Soviet
references.
Card 1/1

L-21582-661
ACC NR.- AT6008387 SOURGE,COM UR/0000/65/000/000/0145/0
AUTHOR: Meshcherskiy, V. Yu. (Kiev),_Audakov, V. P. (Kiev)
ORGi none.
TITLE: Scanning large linear fields in photoelectric conversion of optical-senm
information
SOURCE: AN UkrSSR. Povysheniye,tochnosti i avtomatizatsiya izmeritelinykh sisten
(Automating and increasing the accuracy of measuring systems). Kiev, Naukova.
dumka, 1965, 145-151,
TOPIC TAGS: photoelectric sensor, nonelectric quantity instrument
ABSTRACT: In measuring nonelectric quantities Photoelectric sensors, the
resulting pattern is scanned by an optical-to-electrical-signal converter. The,
scanners that realize pulse-time conv remote me s
ersion (for asurement ) include
either a disk with a read slit moving along an Archimedes spiral or a drum with
'a helical read slit. Formulas for errors involved in both systems are developed.
~To minimize the error, a modified system is suggested in which the scanning field
is subdivided into n areas analyzed simultaneously by n read slits. This modifica-
tion promises scanning large fields by curvilinear read slits with much reduced

L 2761-;66- ._EWt(d)/FSS;-2/EWT(1 )/EEC (k);-2 GW/AST
1ACCESSION NR: AP502126i
UR/0293/65/obj/664/O66o/o662
55i.50.94:629.192.2:550-j
AUTHOR:
hyarts. Ya. M.; M%rkCh2v,-N, T.; Petunin, A. N.; Rudakov, V, P'..
Skvorteor, V. V.0 4%55
TITLE: Testing of rocket electrostatic fluxmeter Ca
SOURM Koomicheskiye issledovaniya, v. 3, no. 1965, 66o-662
TOPIC TAGS- electri field# epaceborne ionizatIIon measurement, ionization detector[
radiation detection
ABSTRACT: Laboratory.tests of an electrostatic fluxmeter of the rotary type with
thin wire ineshes and a synchronous detector are reported. The meter is designed
1for measuring the electric field intqnsity at the surface of a probing rocket and,
indirectly, the external electri,
c-fibld of the upper atmosphere. The sensor was
placed in a chamber under vacuum of 10-4_10-5 mm 11g and subjected to bombardment
of argon ions with energies tcf 1000 ev or less. Determipatione were made of mesh per-,
meability for streams bf charged particles and of the effectiveness of the screen I
plates and synchronous detector as noise suppressors. The'coefficient of optical- 1;'
i transparency of the screen was 0.87, while t~e electrical permeability for an ion
I Card 1/2

ACCESSION INR: AP4033108 VOIZ016410001002/0061/0063
AUTHOR: Larnunin, V. L; Rudakov, V. P.; Serikov, L N.; Sokolov,~ N. I*;
Khaldin. N. N.
TITLE: Vacuum scatter chamber for studying charged -particle reactions
SOURCE: Pribory* i tekhnika. eksperimenta, no. 2, 1964, 61-63
TOPIC TAGS: scatter chamber, vacuum scatter chamber, nuclear measurement,
particle reaction. particle scattering
ABSTRACT'.- A scatter chamber (see Enclosure 1) consists of a steel housing 1,
lower lid 2. and upper movable lid 3. The primary particle beam. restricted by
c1raphite dia-p"aragms 4 and 5, passes the filter chamber 6 and is collimated by a
set of tantalum diaphragms. Then, the beam strikes the target and goes into the
Faraday cylinder. Filter disks 7 are remote-operated by ShI-11 step-by-step
telephone-type switches located inside the filter chamber. Diaphragms 8 and 10
e134 1/3

ACCESSION MR: -AP4033108
belong with the collimator, while diaphragms 9 and 11 remove fringe particles.
Detectors are faLitened to the movable lid 3~ by means of a nipple 15 which is
positioned at an angle of 100 from the central plane of the chamber. The
recording angle can be varied within 100-1701 without disturbing the vacuum.
Remote control is provided for the detector position, target replacement, and
filter,changes in the primary and secondary beams. Orig. art. has; figureR.
ASSOCIATION: none
SUBMITTED: 0lJun63 DATEACQ-. 1IM4y64 MNCL; 0 1
SUB CODE: NS NO REF SOV: 004 OTHER: 001
Cord 2/3

AUTHOR: V.r.halo,lch, D.
TITLI: The VIII Annual Congress of Nuc.'e*r Spectroscopy (V1:1
y.sh.godncy. o,.sh.h-i7. p- Y-&-r-0y
MIODICLL: Usp.kki fIxIch.ekt4h n.4k, 1958, Vol 65. 1qr 4,
pP721 - 722 (USSR)
A13TRACTt The 6th Congress of Nuclear Spectroscopy took place Sr.
Lotilagriod from January 27 to P-tr~ry 3. 1958, It *As
attended by 300 scientists from tht USSR, fqrther by oz.
froa China, Prance, Poland. Cxecbowlcv&k%a, Hungary. Eastern
Germany, Yugoslavia. and the Mongol Democratic Republic. 4
-In I:cl":* Ndt,.b.-.1bS,0.,.prl or: 1,.*:r 4' in
on N,
r A.:r n t
u'r
a- a 0- 7-,.d ll*rnl u.
-dI"'on' '.P-lI
lea ri. R.S.Dah.l. me, Corr 4 ..b r,
opened %he conference. Licitut,** were hold'
by; V.Tu. 4onch~, Y.. V. In.p1n. S.P.T.ytko (FTZ.AS UkrSSR)
&t light nuclei and P.k.r
(SAS SSSR-Library AS ussa), Yu.U.Shirokov (=C-Uoa- SL&%*
University), L.A.Sli. (Lni-L*%ir:d th c4l nl!al
m V.I~
institute) at .1. .. level. I M 4 me- " ISI
IP Ortaberd, G.U.Gusindkly, X.I.Yerakhtna =4
A
IKh L:vb..A.
.1 r, LFTI).:..h.vIng found no rotazlon.l I .,a'.
kh
In Cr, Ind Un n4olel. Tnq s- ri.sw.ron wori-ra S
I.. ad an the discovery of vibrational y-jewo.4
Wipport
18 tn.
1. W 41 go- n4o'.% by ..An- of the .*tA.,4 ..
Coulomb (gulon) excitation at X,xcei.i I NOV.. L.K.?4-fi
(W 3333) gave & survey roporti "Concernirt; Some Panl-lars
in Vibrational Levels of Deforced guclwt-. L.ctmrom war*
bU
11;ld.,I,c. yj P.Z.r.t.kly (AN SSSR - A*SSR) on r.41,tlon
-tInidIr-d nuclei with in* *pIn - 1/211 V.S.
Shpla.11 RIP MZU (2nd scientific Research Institute of
Physics. No.c.. St4t- Unt..r.1ty) on th. 1*,.l 4t.pl-c ... nt
and the probability of corresponding /3 - and f - tran.ttl-4
In odd noalal I D.P. Zaret.kty (All SSSA - IS USSR) on %I..
influence of the spin-orbit.1 coupling upon %he m&,jn*tjc
moment. of the nuclei, A.I.BW (Ali BUSH -AS USSH) on the
light nuclei with high neutron or proton *%case,
(ox-L.nine-d poly-..h.f. r.4tlt"a.) - tn*
.;f Amcloon pairs In nucloll L.L. GoI6.114. A.
fo r-tlon D.
illy0Xowlkova. X.A.Ter-Martiro&yan (TTL AN 3=)-
;a alpha decay on rotational level. of odd nuclei, Via.
coal (AN 3351t - As USSR)
h:n .1ph. decay of
u,clet (surv*y)l A.I.Allk ft-', W-4.1q.bimo,,
(TTL IS )b:n,polarl.&t1on,Eassur*oon
1:r I ST 177
- tr.. ..It ad In t-decay of To 1-. Lu
0.153, R.'Z (4 0., a. _1 9 fj
I- ) so -.11 .4 In %net f Sr ' and I
(AX- 2, a %. -I)IV.P.Rudmkow (As sm - AS U3SS;9on .... . ..
son%& Of the (P-'yT-Wn-dur&-r correlations In BeI-d-yj
XB:rg,:.^nd 1u;V Lbov (TTL IN 11E.) .. I.v.stlj&tlq~s
jA;h .1 t.. ;T:,*I. ti.l
r n r -%Son. n4 the r ... n-
c.%t.rLng or y-r.dl.t1onj B5K;X.rtxo, and
(MOU ;Mo.i... state I,y I the b,.a..tr.hl..j of
td.U*ll :,I T rl.,
21:1ral In
(.)Yis I. r A of t ~1.
of Vol-ria.4 .1!.r:f& and positron@ at polarl;o4 oloct-61
YA.Zi.Chu4ara and 1. Ys Taurn (Rigs) an the lat-Inatton of
%h*tonxlty or the component. of the complex iliispec%mm
.4.r 41n 9 to the ?.-1 41.gr..j I M.bon4, L.H.ZZyr,
LOU (Lanintrad State University) on the
Potation f the probability or the permitted and of the
fcTbLdd"-opturs of el"tromm b,

21(8)
AUTHORS: Vlasov
111. A., Rudakov, V. P. SOV/56-36-1-4/62
,

TITLE: 139
~'Angular Correlation in 'the Decay of Ba and the Sign
of the Rntio of the /3-Interaction Constants (Uglovaya
A -,r korrelyatsiya pri rnspade Ba139 i znak otnosheniya
konstant /3-vzaimodeystviya)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, Ur 1, pp 24-27 (USSR)
ABSTRACT: In the introduction the results obtained by several investi-
gations of the ratio of interaction constants (9S/9T or gV/gA)
carried out by several authors are discussed. 'With respect to
the connection between angular correlation and the ratio of
these constants, A. Z. Dolginov (Ref 7) showed that the aniso-
tropy coefficient a can be represented in the expression of the
angular /~ - e correlation W(g) _ I+a cos2e as a function of this
ratio Pnd some ratios of matrix elements of /3-transition. The
latter are written down for the case A J = 1(cf. Ref 7) and di~-
cussed. Further, the results obtained by a number of other
papers are discussed (Refs 8-12). In reference 8 the angular
/3-r-correlation was investigated for the cascade transition
Card 1/3 between the states (7/2 /.Z0,(5/2+) T, )(7/2+) at

139
Angular Correlation in the Decay of Ba SOV/56-76-1-4/62
and the Sign of the Ratio-of the 1PI Interaction Constants
E/3 = 2.23 and Ev = 0.163 IfieV,, The authors investigated it
in the decay of ja139 (from the reaction Ba138(d,D)Ba139).
A statistical evaluation of 30 measuring series resulted.in
the following values for the anisotropy coefficient%
a = fN('r,) - N(ri/2)j /N(7/2) = 0.058-+0.023
(Ba139 has a half-life of 85 minutes).
Control measurements were carried out with the preparations
SC461 and Sb 124 the results of which are also given. Calculation
of the anisotropy coefficient was carried out both on the
assumption of a mixed vectorial and axial interaction and
for a scalar-vectorial mixture. The following was obtained
for the constants: g. = -g '; 9T = _gT'; gV = gV; gA = gJA,
3
where the quantities with a prime relate to the non-con-
servation of parity. Calculations were carried out for the
case of a mixture of magnetic dipole (96.%)- and electric
quadrupole (4 ~Q-radiation. The dependence of P_ on the ratio
Card 2/3 9S/gT or gV/9A and on only one ratio of matrix elements was

139 SOV/56-36-1
Angular Correlation in the Decay of Ba -4/62
and the Sign of the Ratio of the /3 Interaction Constants
calculated; the functions obtained are given in figures
2 and 3. Theoretical results agree with experimental ones
only for 9VI /- < 0. The authors finally thank A. 'I. Dolginov
~Aem know calculatio'n restilts and fc-. eiscussions,
for letting t
and they express their gratitude to S. P. Kalinin for his
interest, and to L. A. Sliv and I. S. Shapiro for discussing
results. There are 3 figures and 13 references# 1 of which
is Soviet.
SUBMITTED: July 11, 1958
Card 3/3

RUDAKOV, V. P. , C,ind Phys-1--lath Sci (Giss) "Angular correla-
tion." Leningrad, 1P60. 6 Dr,; Order of Lenin State Univ
im A. A. Zhdanov); 200 copies; price not given; (KL, 27-60, 148)

RUDAKOV.-Y.P.-
Distribution of the number of fission neutrons. Atom. energ. 4 no-3:
315-320 Mr '58. (VIRA 12:3)
(Neutrons) (Nuclear reactions)
M

VLASOV. N.A.; RUDAKOV, V.P.
Angular 15-2(-correlation in the decar c-I 3al30, pn& 'he sign Of the
ration of the -interaction constants Lwith summarv in English].
ZhurZeksp. i teor.fiz. '36 no.1:24-27 Ja '59. MRA 12:
Barium-Decay) (Beta rays) (Gama rays)

FT
Hudakov, V. J_. 89-3-25/30
T!TLE: Distribution of Fission Jleu~crons (Rasrredeleniye chislan
neytronov deleniya)
PERIODICALt Atomnaya Energiya, 1956. Vol- 4, Tir 3, pp. 315-320 (1133R)
A '13 3 TA C '1' In Septe,,,-iber 1957, at the Neutron Conference at the
Columbia University, D.Terel (USA) held a lecture on the
mathematical determination of the number of neutrons set free
at the fi3SiOn from which an extract is given here.
A simplified process of calculation with a reduced number of
parameters is given. It is assumed that the fission products
emit neutrons only if this is energetically possible. Further
it is assumed~ for the sake of simplicity, that the emiss�on of
any neutron from any fission product reduces the excitation
enerL-,j of this by the quantity AE, which on the average
amounts to about E = LE and that the total excitation
0
energy of two primary fission products at the double fission
has a Gaussian error-distribution. Thereby the mean quadratic
Card 1/2 deviation from the mean energy E is (5 E. Both these assumptions

U
j-'stribulion of FissJon Neutrons B9--3-25/30
are, ac~~ord4ng to experimental investigations, permissible.
-2 -2
As a measure of comparison the quantities D = r- r
-2
r - r
and r2 7z7- are computed as well from the experimental
data as from the given assumptions and an asceptable con-
formity ha3 been achieved. There are 5 figures, 1 table, and
7 references, 0 of which are Slavic.
AVAILABLE: Library of Congress
Fis-tio:: neutrens-DistributJon 2. Mathematics-Theory
Card 2/2

ACCESSION NR: AP4043632
AUTHORS: Golldberg, V. Z.,i Rudakov, V. P.; Serikov, I. N.
TITLE: Analysis of elastic scattering of He-3 and Alpha particles
an the basis of the optical model of the nucleus
SOURCE: Zh. eksper. i teor. fiz., v. 47, no. 2, 1964, 571-576
TOPIC TAGS: helium, elastic scattering, alpha particle reaction,
.,differential cross section, optical potential
ABSTRACT: Although.a detailed.analysis of elastic scattering of
alpha particles by many nuclei from C12'to Th232
was made by Igo
and Thaler (Phys. Rev. v. 106, 126, 1957), no such analysis was
3
made for the elastic scattering of He Earlier calculations, made
.on the basis of a limited experimental material, have led to para-
meters that vary erratically from nucleus to nucleus. The.authors
have therefore used the optical model to attempt a more systematic
Card 1/2 J,

ACCESSION NR: AP4043632
analysis on the data concerning elastic scattering of He 3 by differ-
ent nuclei, and calculated the differential cross sections for this
scattering. 'New data obtained on the differential cross sections at
the laboratory of the authors (V. M. Pankratov and I. N. Serikov,
ZhETF, v. 44, 187, 1963) and by Gonzalez-Vidal et al. (UCRL-9566,
1961) have been used in the calculations. The results show that a
single set of parameters for the obtical potential can be used to
describe satisfactorily.the experimental data over.the wide range
of nuclei from Be9 to Bi209. A comparison is given of the parameters
of the potentials describing the elastic scattering of He 3 and of
alpha particles by A127. "The authors thank V. A. 1~elyakov, P. E.
Nemirovskiy, and I. S. Shapiro.for useful discussions." Orig. art.
has: 3 figures and 3 tables.
ASSOCIATION's None
SUBMITTEDs- 2Wan64 ENCL: 00
SUB CODE: NP NR REP SOV: 002 OTHER: 010
Card 2/2

G(j IDURG 11 T, tjr)," KOV V . p
Wide-focus magnetic betp--spectrog7p-r~-.. ekap. Fs
no.6i36-37 11-D 163.

-,.TL

2, (7), 21 (8)
AWHOR - Rudodcov, V. P.
'TITLE: IX 11-1--union on TTU--.~leftr
(IX Vsesnywr-o-ye s,D-.reshdh,-.uiiy~R nc yadei-no-i ovktr:~.-sk-r1i)
P&MDICAL: Atounaya energlya, 195~,, Vr,l 'I., 'Or '. p-~ 7(-,-"'J11 (Tj:;-j.?)
ABSTIUCT; TEs IX Ccafercri..;e vw) frolm jtuol~'-7y to
Februar,, 2,, 19,59 at Khar'ko-,.,-. th~nn 700 p,:L,--ti:Apan1;s heard
.00 11-ecture3, the most ir-noc;:~ti~c:t .,f dle.-~11 .v5 th the
fall-owing fields. Theory, GenT:ral CA-I il-iei-,ay.
A. j. Da:.rydov (1,11U)
excited zmzlear states. L. ". Pa-':Cer- fleformo.,! n-u,~-Pi. P.. L.
Birbpair- L. X. Peke-,; L. A. Sliv (L:-`T1) -
Oocillzt-iono :,f defrr-med nuclei. Ye. V. Ir)ypin, V. Y,.-. Gcnchar,
S. F Tsy-11-kc, ( I," -) : "I I
1.11ITT Calolation ~f the ft-values matrix
'y
elements f~r ur,'U'AltIOnZ 1 IIIE-a7_3 cf genera., -z.Eo- nu--ea.
- - --) : C, - r- r tion
--c-leI. S. T. Ue'''.y ay e L-k -, n. s11 e i ~ z- t ir- C-f Pai Cc rala
i n nu Q I e i . A. P . 11--- ~,,d a-- ( 1A E) . T'he -app]L1--,~z,-,;-.--,r- of the sia-per-
condu!~t-'--vity av.;ds-1 to au;'l-e-i fcx- the of
thei- P,-,ients 3f* iric3rti,,~. r. -1". IN .-,-Li.~x~.-vokiy of
the -ei-trcn cf nnj,~Iei Ya. (IA---) -, The
Card 1/3 present sta;~-e in the thec.I,;- c-f V. V. V1,-.dim2,Tskiy,.

IX. All-Union Conference on Nuclear Sjpectro,.3r,,)-.;y v,lr),) 6/2 6
V. K. Grigcirlyev- V. A. Yer-ak,;v, u. V. TrebukIlc%rzkiy (ITZI-,"
Yea3urement of the ani-,Ilar norrelation *~etwean electron and
neutrino in the deoV of the rie-it rou. V. 1.~- V. A.
Nazarenko, L. I. Ruainov Mrsasurement cof Lhe ccrrelation
between the transversal election polar~.,zation tind circular
polw,ization of ~-quanta =:urring in the defmy of
" 46 6o. ',)n of Nuzdei. Yu- P.
0c and C o Decay Schemes. ~--radiatL,
Anufriyev, A. K. Vallter, Yu. V. Gorichar, Ye. G. Kepa.,leyte,
A. N. LIvov, P. M. Tutakir, S. P. Tsytkc, P. V. Sz~rokin, A. S.
Deyneko, 1. Ya. Malakhov, A. Y2.. Taranov (Fizikc-tekhnizhesk 4 y
Kharlkovskiy injtitt,,Zt- Institute, Kharlkov)):
311-34(P,7), Ar 41(p,.r) arj N11 (p,h
The
reaction3. D. G. Alkhazov, A. P. Gruiberg, 0. M.
11-!,~ Kh. Lemberg,, V. V. Rozhde3tvem*jj., T. 11. YerokIline of the
Lenizigradskiy fizikc--tekbn_J.-,heskiy instit-ut (Leningrad Physi-30-
u
ten,hnical Institute): Iliveotigaticn of the Coulr,,mb exaitat:.on
(.,f the lower levels of some nuelsi duripg V~eir bombardmer'; by
multiply charged ir)ILS (C., N; 0-,. M.1 lt-~). A. V. Kalyamin, A. N.
1--'urin. V. it. rokro-skiy, V. A. Yjkc~vlev PLAN); New isotores
Card 2/3

IX. All-Union Conference on NuJeax
KI
Tu Ho 11r,' B. V. A.
Se.rgi enko (LOW); De;;a.-j schemes cf soms lou',1.,cm-defic;ient,
0 y
isotopes, set up ca the basis c-f mea*-,~remoz~n,8 of the
den,.:e of the electr-,-.ns.
Engi-neering. B. S..Dzhelepmr, R. '_E. V. G. IN, ed*ve 3cv.,
V. G. Chum-in (HIATT': %-spe-:,t_-omater double fo,.~UO-111g.
S. A. Baranov, V_ V. Parucir.-k-D, A. G. Zelenk-;v, A. F. Tf.Tallcv,
G. Ya. Sholiepicin (11E'i: Ii,~Iprovt~d I. F.
Barchuk. G. V. Belylch, V. 1. Gol-shkin.. V. A. -L.-,~rvzn (IFAN
UkrSSR) Magneti~-, spectro-varh for 11E?avy charged parti::;les.
The repveoentatives of the radlictekh-nicheskoy
Prromyghlenricsti cf the fladic~--engineeririe industry)
gave a repoi,t about rv~,w Lmltiplliex-s. The Cmference was
clcsed ty B. J. Dzhelepc,v, who streszed the falct that nu,--Iear
tables wid :reference viorks ou.-Int -%-, 17-3 publi_--!-:!d Lm-.~h more
quickly in or-der tn be of raal -joe to tlf;e .7~xysrimsntsr.
Card 3/3

Y V. P. pand VIASOV, N. A.
!fCorrelation angulaire beta-go dans is desintegration do 139 Ba et signs
uotient, 0," constantes do la desintegration beta."
preseni.-.i at the Intl. Congress for Nucloor Energy) and
lear StxIIucture'(Intl. Union Pure esd Applied Physics,) Paris, 7-12 July 1959.

AUTAOR- Rudakov, V. P. BOV/89-5-1-13/28
TITLE: VIII. All-Union Conference of Nuclear Spectroscopy
(VIII Vsesoyuznoye soveshchaniye po yadernoy spektraskopii)
PERIODICAL: Atomnaya energiya, 1958, Vol. 5, Nr i, PP. 78-80 (USSR)
ABSTRACT: From January 27 to February 3, 1958 the VIII. All-Union
Conference of Nuclear Spectroscopy was held at Leningrad. It was
attended by a total of more than 500 representatives of the various
institutes of the USSR, Poland, Czechoslovakia, the German
Democratic Republic, Yugoslavia, and France. 100 lectures were
delivered in the course of 10 sessions. The material of this con-
ference is described in detail in Journal I. The following
principal problems were dealt with:
1. General problems of beta decay, nuclear shells, c( -decay.
2. Decay schemes. The r-radiation of nuclei.
3.~ The technology of spectroscopy.

VIII. All-Union Conference of Nuclear Spectroscopy SOV/89-5-1-ly 28
1. Nuclear physics 2. Spectrosc6py
Card 212
-.Fg,-j LIN

ARTEMOV, K.P.; GOLIDBERG, V.Z.; RUDAKOV, V.P.
Elastic and inelastic scatteri ng of alpha particles an A127.
Atom. energ. 14 no.5:482-04 My ~163. (MIRA 16i6)
(Alpha rays%~'-Scattering)

L ii qnh.~A*i
ACCESSION MR: AP3001178 0089/63/014/005/0482/0484
S/
AUTHOR: Artemov. K. P.; Golldbe V. Z.; Rudakov, V. P.
TITLE: Elastic and inelastic scattering-of Alp par by Al sup 27
SOURCE: Atomnaya energiya, v. 14, no, 31P 1963. 482-484,
TOPIC TAGS-. elastic scattering, inelastic scattering, Alpha particles,~excitqd
states of Al sup 27
ABSTRACT: The Alpha particles were accelerated to 40,.380 and 36 Mev in the 10-5
M
cyclotron of the Institute for Atomic Ene A high pressure ionization chamber.--,,:':
was used for detection of Alpha particles. In agreement with the results of other
workers, the angular distribution of scattered particles showed a "diffraction
pattern," the maxima of the inelasticaLLy scattered particles coincided with the
minima of those scattered elastically. The results are interpreted on the basis-of
theory by other authors, among them S. 1. Drosdov (Zh. experim. i theoret. fiz.
)11 901, 1956). The radius of interaction of the Alpha particlevith the Al-
nucleus is found to be 5.5 fermi. Conclusions are made concerning the excited
states in Al sup 27. "The authors are grateful to S. I. Drosdov for the discussion,'.
of results of the work." Orig. art. hass .3 figures and -references.
Card
----------------

GOLIDBERG, V.Z.; RUDAKOV, V.P.; SERIKOV, I.N.
Use oK an optical nuclear model in analyzing the elastic scattering
of He-' and alpha particles. Zhur. eksp. i teor. fiz. 47 no.2:571-576
Ag 164. (MIRA 17:10)

h2912
5/250/62/006/012/001/003
A0O1/A1OI
AUTHOR: Rudakov. V. P.
TITLE: On one sufficient condition of motion stability during a finite
time Interval
PERIODICAL- Akademiya nauk BSSR, Doklady, v. 6, n~. 12, 1962, 757- 759
TEXT: The author considers the problem*ot.motion stability of a system
Which looks as follows:
dx
P (t) x + X (t,x~
where P(t) x (xj (1,k I .... n)
p (t)j! x(t,x) x (t,x))
Ik 1.
It is azsumed that within the region
to t T x, a (to T, a 0)
Card. 1/~

P)/,,?5o/62/oc6/o i2/oo I /ouj
on one sufficient condition of... A001/A101
natrix P D-S a r(!al and rontinuous function of tim n. v ctor X i-; a re
e t. a d e al
and continuous ftinrtion of time t and real perturbation vector x. The author
cttes a definition of :itability.given by G. V. Kamenkov and A. A. Lebedev (P.1".4,
v. 18, no. ~~, IJIP, 1954) : The unperturbed motion is stable over 'the finite timp
Interval I t0 ]. it' in space x can be found cycle V (t,x) = A which possesses,
within this interval, the following properties: 1) diameter of the region
V ( t, x) s~, A (2)
doei not ex~-f?d initlai dianeter D (t 0),
D (tj (3)
D (t 0
2) at any initial perturbations x x satisfying condition V (t YX
0 101 0 0
perturbations x(t) satisify inequality (P). The author introduces the concept of
a regular bundle of quadratic forms K ~LV and determines its characteristIc
numbers, I.e., roots of equation
det (C fA-E~) 0
Ca rd P/3

MW
S12501621(YO6101210011003
on one sufficient condition of... AOO1/A1Ol
where C is matrix of coefficients of form K; E is unitary matrix. The maximum
root, at any time instant, of equation (7) is denoted by p,(t). Then the -.uthor
proves two theorems to the effect that the following conditions are necessary
and sufficient for the motion to be stable within the finite time interval:
P- B(t 0)