SCIENTIFIC ABSTRACT SIVOSHINSKIY, D.S - SIVTSOVA, E.V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001550920013-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 24, 2000
• Sequence Number: 13
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

S,LVOI~lm,~SL'i F.F.
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Ccz--~~ernirig F.F. Kaperkols art-icle "DeterraInation of heart
'VOlume and other indications of ceptral cardiac hamcdynamics
by means of radioactive krypton Kj, 5.,, Mled. rad. 10 no.6-.
621-68 Je 165. WRA 18:6)

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42123 32'1011, ~'- G. - Fermbrly I Dokembriy Zapadno.go Mayan;,. Trudy Oorno-geol. In-ta (-.Kad.
Nauk Zap.-33ib. F-- lial), VYI . 2, 1948. c 125-4*,'. - Bibliogr: 15 Nazv.
h v'-h '3tatey, Vol. 47, 1948
SO: Leto,,jS17 urnaltn r.

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31110V, A. 2^-
El--~ment3 of the Stratigr-pphy and Tectonics of the Devonian Deposits of
the Minusinsk Hollow
The application of the paleontological method to the analysis of
the Devonian of the Minusinsk hollow (syncline) permits one to establish
reliably only divisions. A more detailed analysis is made difficult by
the limitedness of the distribution of organic remains an0- by their in-
dependence of associations; here a local subdivision possesses the most
important significance. At the foundation of the Low~r Devonian of the
Minusinsk Hollcrd lies the Kharadzhul'sk effusive series (basic unit of
regional scale is in the authorts opinion formations limited below and
a,.~ove by nonconformities and divided into strata). (RZhGeol, No. 5,
1055) Tr, Tomskogo un-tg, ser, ze0l., 132, 1954, 239-260.
SO: Sum. No. 744, 8 Dee 55 - Supplementary Survey of Soviet Scientific
Abstracts (17)

Name: SIVOV, '.leksandr Grigorlyevich
Dissertation: The Cambrian Period of the Western
I
0ayan and its Adjacent Regions
Degree! Doe Geol-Min Sci
Affiliption: ~Iffot indicateg
Defense Date, Place: 12 Jan 55, Council of Tomsk Order of
Labor Red Banner Polytbch Inst imeni
Kirov
Certification Date: 29 SeP 56
Source: BMVO 6/57
2-1

AKSARIN.A.V.; ANANIYZV.A.P.; BIWBDIKTOVA,R.II.; GORBLIIIOV,M.G.; GRATSIANOVA,
R.T.; YBGCROVA,L.I.,, IVAUIYA.V.A.. )MATIffSKAYA.L.B.; KRA YXVA,
P.S.; IJBADNV,I.V.; LONOVITSKAYA.M.P.; POLWAYBYA,O.K.; ROGONII.L.A.,
RADCHRUKO.G.P.; I?ZHCKSNITSKAYA,M.A.- SIVOV A.G.; FONICHEV,V.D., IHAI-
FINA,V.K.; KHALFIR.L.L.; CHMYSi~X -~~ITRUJ.Jff., redaktor;
GUROVA,O.A., tekhnichaskiy redaktor
[Atlas of leading forms of fossils in the faun and flora of Western
Siberia] Atlas rukovodiashchikh form iskopaemykh fauny i flory zapad-
noi sibiri. Pod red. L.I.Khalfina. Moskva, Gos. nauchno-tt)khn.izd-vo
lit-ry po geologii i okhrane nedr, Vol-l- 1955. 498 p. Vol.2. 1955.
318 p. [Microfilm] (KLRA 9:3)
1. Tomsk. Politekhaicheski:
y institut imeni Kirova.
(Siberia, Westera-Palsontology)

SIVUV, It.G.; TUNWHPOLISK&YA, V.D.
Age of Sanasht7kgol archaeocyathid-tribolite
the Sayan-Altai area. Hat.po geol.Zap.Sib.
complexes In
no.61:40-48
158, (MIRA 12:8)
(Altai Howitains-Paleontolopy) (Sayan Mountains-Paleontolog3r)

D. Z. Katserielenuauvl, N. F. 11. V. 11,11alin, A. N. SIVCV:
a -caJ c .:a%,, ~1~ C.,e. 11 3,-ierlti_f4 C
IfFroLaCatiori of Ifol .-i.-cives -j.er- ; L: f -1 Ses-ion
Devoted to Rauio Ya-z- 155e, Tracli-e~:,xvizc;-t, 11-.-o ccw, 5 Sef..
50
Conditions for the propagation of a summetric magnetic Hol wave
in a rectilinear .,eriodic waveguide an(! tile trans,-,d-ssion of an Ifol wave
through a bend in a periodic waveguide are investigated.
The periodicity, shape and size of the conductor from it.,hich the
waveVuide is wound, the finite conductivity of the metal, the dielectric
shell of tile waveguide are taken into account in computin- the damping,
of the 11()l wave.
Tile comilin-, coefficients of the Hol wave with the parasitic E.
6
and Hl type waves which arise are found when analyzing the transmission
of the 110, wave through the bend.

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r0e. ~e e OV%. X.05e -4 (3) can be
e . . I ___-:ftis can be Used
e e e 06 e the resulting
01 _...4ce Eq (1) cannot be
-r-due to the dielectri(,
.--the hel
Ixi a special equation
derived. The resulting
,-length is given by Eq (1)+).
,-ernal dielectric sheath of t The
he waveguide
account by using Eqs (1) and (2).
Card 2/3 'GLPPlicable to helical as well as -ring-type
-cles. . The Presence of a s"all elipticitY in a

AUTHORS: - V.V. Malin, and A.N. Sivov '0V/109- - -4-3-12/38
TITLE: on the Theory of Propagati-o-ft of the Hol-Wave in a Helical
Waveguide (K teorii rasprostraneniya volny Hol v
spirallnom volnovode)
PERIODICAL: Radiotekhnika i Blektronika, Vol 4, Nr 3, 1959,
pp, 433-439 (USSR)
ABSTRACT: It was shown in the preceding paper (see this issue of the
journal, pages 1+28/432) that the attenuation due to the
radiation in a helical waveguide is given by Sq (1). On
the other hand,7 the attenuation due to the angle of
inclination of the turns of the helix is expressed by
Eq (2). The following notation is adopted in these
equations: a is the radius of the waveguide2 p is
the period of the helix, X is the wavelength in free
space, s = e' - is", Ho and Hl are Hankel functions
of the 2nd kind k = 2W/X and la = 3.83. Also in the
preceding article it was shown that the attenuation
caused by the finite conductivity of the conductor is
expressed by Eq (3) where a and t are the parameters
depending on the form of the conductor. Eq (3) is valid
Card 1/3 for a helix whose conductor is rectangular in cross

SOV/109 - -- 4-3-12/38
On the Theory of Propagation of the Hol-Wave in a Helical Waveguide
section. The parameters a and t can be evaluated on
the basis of the transformation defined by Eq (4). It
is shown that, if the wave of the conductor is 2b and
its height is 2c, the parameters a and t can be
evaluated from Eqs (5) and (6). The variations of these
parameters as a function of q 2b/p for a given We
are plotted in Fig (2). If a 0.9 an " % = 0.8 cm,
Eq (1) can be written as Eq (7). The results of Fig (2)
can be used to evaluate a parameter 1n a i the
resulting graphs are shown in Fif (3). Eq (3) can be
approximately represented by Eq 8). This can be used
to evaluate 4 as a function of q the resulting
curves are shown in Fig (5). Since Eq (1) cannot be
used for evaluating the losses due to the dielectric
situated in the vicinity of the helix, a spefAal equation
for this type of loss is derived. The resulting
attenuation per unit length is given by Eq (14). The
effect of the external dielectric sheath of the waveguide
can be taken into account by using Bqs (1) and (2).
Card 2/3 These are applicable to helical as well as ring-type
Waveguides. The presence of a small elipticity in a

SOV/109- --4-3-12/38
On the Theory of Propagation of the Hc)l-'dave in a helical Waveguide
waveguide can also be taken int"o ac,:,ount. The attenuation
produced by this effect is given by Eq (17)~ where &
denotes the difference in the semi-ax-es of the elipse.
The authors make acknowledoement- to B.Z. Katzenelenbaum
for his interest in this work and his valuable remarks.
Card 3/3 There are 7 figures, L~ tables and 8 references7 Lr of
w1iich are Soviet, 2 English, 1 French and 1 German.
C3
ASSOCIATION: Ins'L-litut Radiotekhniki i Blektronikil AN SSSR
(Institute of Radio Engineering and Ele-itron-ics of the
Academy of Sciences of the USSR)
SUBMITTED: Mlarch 1st, 1958

s/lo9/6i/oo6/ool/007/023
9~' E032/E114
AUTHORz Sivov, A N.
TITLE. Incidence of a plane electromagnetic wave on & plane
grid (H parallel to the conductors)
PERIODICAL~. Radiotekhnika i elektronika, 1961, Vol.69 No.1,
pp. 58-66
TEXT. The problem considered is that of a plane el*ctro-
magnetic wave incident obliquely on an infinite grid, the magnetic
vector being parallel to the conductors in the grid. The space is
filled uniformly with a dielectric although the dielectric is not,
in general, the same on either side of the grid. Assuming that
the grid spacing is small compared with the wavelength, formulae
are derived for the transmitted and reflected fields. It is
assumed that the magnetic permeability of the medium is equal to
unity and that the grid is formed by parallel and perfectly
conducting metal conductors having cross-sections of arbitrary form
with two symmetry axes ox and oy (ox is perpendicular to the
conductors and lies in the plane of the grid, and oy is normal
to the plane of the grid). The time dependence of the fields is
Card 1/2

s/io9/6i/oo6/ooI/G07/023
Incidence of a plane electromagnetic.E032/EI14
taken to be of the form exp(iwt). Since the directions of
propagation of the waves are perpendicular to the conductors and
the grid is uniform in one direction, the problem is essentially a
plane one. The paper is entirely theoretical and consists of the
following sections, 1) formulation of the problemg
2) expressions for the fields at large distances from the grid in
terms of the field on the conductors and in the plane y = 0,
3) the electromagnetic field in the neighbourhood of the
conductorB, 4) discussion of formulae, 5) asymptotic. forms,
6) circular and rectangular cross-section conductors,
7) equivalent boundary conditions for the grid, 8) calculation
of the effective reflection coefficient of a system consisting of
a grid and a parallel screen. Acknowledgements are expressed to
B.Z. Katsenelenbaum for his advice and attention to the work.
There are 4 figures and 7 references: 6 Soviet and 1 German.
SUBMITTEDt May 10 1960
Card 2/2

7
s/io9/6i/eo6/oo4/coi/c)-,.---1
E032/E314
AUTHOR: -Sivov. A.:,-.
TITLE: Electrodynamic, 'f'ktcory of a Plane Grid Consisting of
Parallel Conductors
PERIODICAL: Radiotekhnika i clelctronika, 1961, Vol. 6,
No. 4, pp. 483 - 495
TEYT: The probleat considered is formulated as follows.
The infinite grid lies in froe soace and the plane electro-
ma--ictic wave is obliquely incident u:3on it. The grid is
flr~aed by parallel conductors, whose cross -s'ections have
t,,,ro sy=aetry axes. Assuming that the period of the grid is
sinall compared with che wavelength it is required to determine
the transmitted and reflected fields in the immediate neigh-
bourhood of the conductors, and to obtnin the local boundary
conditions representing the action of tiie grid. The prcoblem is
investigated in connection vith the attenuaition and phase
charac II-ris tics of electromagnetir- wztves in periodic wave-
guides. Two cases of polarisatioi-, are distinguished, depcndi.~i--
on the -)rientation of the electric a-,.,d ima-netic vectorAll
Card 1/-

Lj r'7
relativc, U.o the :--ri-d -,n tj'ie case of
'I e vic rield, ii es i~-, ;-.11o pli ne .)f
'H-pol,tvisat ion" t, e I c c t,
"rid aiid is j-.er1)end.i(-L11.,.1r to thQ --O11dMCtOi7S '. ililO J--~ :Ifle C. --,e
of "E-polari-gatiou". t,i(-- ;-lagnetic fiol.d is _)erpen,11ic,i1ac L--) the"
coa,'mc tors . It is fwvid that Lamb I -I- restil tr. ( 11of. 7 ) (01A C, i;lvt~
for the aco:.jstic case of a -rid conz;`~z3tin,,, of ti~-,in c-ircitIrr!r
rods and the resultz-, of Von R. Gan,-3 (Rel-. 13) for a ziimilor- case
are incorrect. The~-,e atithor-s (lid not. L;-.,he into ac omit
Peripheral curro--c,-its aj)d their reflection ccefficica-ts are -)jit
by a factor of 1.5. T'he formoilao obtained iii t1lie pvezc.-~~ IL pap,01.
can be specialised to t~ie c3se ~Ianre the coi1c:ijc-tor3 toLch e.1ch
other. The obtaincri for fields in the i.-lu:1ediaLe
neighbourhoo,j of the conductors can be used to correct for losses
due to -the fact that the conductors are not perfect.
Acl~tiowled-monts to D.Z. RLatronelenbaum for irit(--rCst Cl..d al.~-vj.C(7.
There a!-(- 5 figires z.-ind 9 rv~L 8 Soviet and I
SUBMIWED: July 23, 1960
Card 2/-

AUTHORS:
TITLE:
30432
S/109/61/00b/012/00'1/u2O
D26b/D305
Kotikq I.P., and bivov, A*N.
Propagation of H On type waves in a ring waveguide
having a dielectric-metal jacket
PYRIMCAL: Radioteknnika i eiektronikar ve 6. no* 12t 1961t
2005 - 2011
TEXT: The purpose of the paper is to solve two closely related
problems; (1) to calculate the reflection and transmission coeffi-
cients of plane electromagnetic waves incident upon a set of para-
llei conducDors (E parallel to the conductorav distance between
the conductors is small in comparison with the wavelengthi the
upper half-spaces are filled with different dielectrics)# (2) to
calQulate the propagation and attenuation coefficients of a ring
waveguide half embedded into dielectric and the whole structure sur-
rounded by a metal wall (Fig, 5). The solution of the planar prob-
iem is again divided into two parts: (1) The fields near to the
conductors are obtained with the aid of the Laplace equation (solu-
Card 1/$.;

30432
Propag ation of H b1l0V 61/ u06/Ul 2/007/ U20
On 'uype waves D266/D305
lion given by A.h. Sivov (Ref. 5: Radiotekhnika i elektronika, 1961
Vo 6p no* 4p 483));(2) The fields further away frow 'uhe conductor
are related to those near Lo che conducLor by using the Lorentz
lemma (explained by L.A. Vaynshceyn (Ref. 2: Blektromagnitnye volny
(Electromagnetic Waves) Izv. Sovetskuye, raciio, 19579 418)). The
auxiliary fieids - required by the lenima - are -caken as the fields
in the absence of the conductors. kerforming uhe calculations The
reflection and iransmission coefficients are obtaineo in bhe fol-
lowing form - _- I- __ ____ - _
2 re-1pip (RI - R) ExHA,
r
(7)
2
p (T~ - T) E2Hds.
C
where E 21 61 -crJBlecz2,ic constants in the upper and lower half-spa7
ces, TlP T2 - angles of incidence and refracTion respectivelyg R.,
TI - reflection and transmission coe:r'ficients of piane, waves inci-
Card 210 :

3uh32
,/61/006/012/007/020
bliog
Propagation of H On type waves D2o6/1)305
dent upon the boundary of two dielectricsp p - distance between the
conductorsp E 10 E2 _ auxiliary fields corresponding to the reflec-
t I
ted and refracted waves respectively I if magnetic field on the
surface of the conductor# U - contour of the conductor. With the
aid of (7) equivalent boundary conditions are derived which are re-
presented by an electric current in the direction of the conductare
and by magnetic current perpendicularly to the conductors. These
boundary conditions are applied to the corresponding boundary of
the ring waveguide. In the region 0 --z r -- a the dielectric constant
is taken as unity whilst the dielectric surrounding the rings is
assumed lossy (F- = t' - jF_11). The propagation and attenuation co-
efficients of this composite waveguide are expressed in the follow-
ing iorm:
h'= h, + 0; ho 1~2
a p hoO
W = (13 - 12) IM
4 h0a4 Itg Pod + 001
(i9)
k2p
Card 3/5 -h20-.

3(--)432
S/109/61/006/012/007/020
Propagation of ff On type waves D266/D305
where h0 - propagation coefficient of the smooth waveguide (H Un Mo-
de)f p - root of the J1 function, 12and 13 depend on the shape and
dimensions of the conductors (obtained in Ref. J: Up.cit.), k =
= 21flk- If d oo the formulae agree with those of B.Z. Katsene-
lenbaum (Ref. 5: hadiotekhnika i elektronika, 1959, no& 3, ve 4,
428). If
d (M = 1, 2,
2 -
V
there is a sudden increase in attenuation due to resonance. There
are 4 figures and 5 Soviet-bloc references.
SUBMITTED: April 17, 1961
Card 4/5

KATSENELENBAR., B.Z.; SIVOV, R.N.
Lamb's error in a problem on diffraction on a lattice from thin
round rods. Wiotekh. i elektron. 9 no.2:360-361 F t64.
(MIRA 17:3)

L 13569-65 EWT(d)/EEC(k)-2/EEC-4 ft-4/Pg_4/Pt_l0/Pl_4 iSl)(a).OAS
A~L ~SS~DA~IFIID(t)/R~~(a)/ESD(gs)/ESD(t) WS
CESSION NR: AP404660Z 510109/641009/0101
A
A ESS 0
!AUTHOR: Sivov, As N,
TIT'LE: Reflection of electroma netic waves by a tihort-periad corrugated
9
surface Report at a session of the Scientific and Technical Society of Radio
Engineering and Electrocommunication, 1961
15 URCE: Radiotekhnika i elektronika, ve 9. no. 10, 1964, 18ZI-18V
T6PIC TAGS: electromamnetic-wrave, electromagnetic wave reflection
ABSTRACT: The reflection of electromagnetic waves by a corrugated conducting
surface whose corrugations are small as compared to the wavelength is
considered. These cases are dealt with: (1) An arbitrarily polarised plane W&Vei
falls at a slope angle on a shallow- corrugated surface; c 4