SCIENTIFIC ABSTRACT KATSEN, L. - KATSENELENBAUM, Z.

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• Collection: Scientific Abstracts
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• Release Decision: RIF
• Original Classification: S
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• Document Creation Date: November 2, 2016
• Document Release Date: June 13, 2000
• Sequence Number: 3
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

APTMIARI, S,; KATSEN, L.
A norm plan for metallurgical machinery unitso SotB.trud 4
W.9:87-91 6 159. (HIBA 1321)
(Steel industr7--Production'iitandarde)

KARMAZIN -V -I-ddktor-tekhn-.naukc
9 0 elp p
UT~~ kand.tekhn.nauk; ITANOV, ~Ll., inzh.; OSTAPMO,
--PsYiep inzh.
Magnetized roasting of Krivoy Rog qUar'tsites in a fluidized bed.
Stall 20 no. 12:1057-1060 D 160. (MMA 13:12)
1. Mekbanobrehermet.
(Kriovy Rog--44uartsiete) (Fluidization)

KATSEN, Leontiy Grigor!yevlch LUPYANOV1. Mikli-iil Razlinovich;
AMEXAW, Snveliy Semenovich; TEMSHOHENHO, P.A. , inzh.,
retsenzent, C11UMkCHENKO, T.I., red.izd-va; BEREZOVYI, V.N.,
tekhn, red.
(Labor productivity in ferrous metallurgy in the Ukrainian
S.S.R.] Proizvoditellnost' tmda v cbernoi metallurgii
USSR. Kiev, Gostekhizdat USSR, 1963. 2_18 p. (mirvi 16:4)
(Ukraine--Iron industry--Labor productivity)

KAZANTSEV, Yevgeniy Ivenovich. Prinimali uchastlye- ZEI-11,YANYY.
kand. tekhri. nauk,
11.G., inzh.; UTW - SDIIKIN,
I.D., prof., retsenzent; STEPNIOV, Ye.S., red.;
SHKLOVSMA, I.Yu.p rod.izd-va; KOROVINA, N.A., tekbn.red.
(Industrial furnaces; handbook for their calculation and de-
sign] ProvWshlenxWe pechij spravochnoe rukovoOstvo dlia rasche-
tov i proektirovaniia. Moskvla,, Izd-vo "Metallurgiia," 1964.
1+51 P. (MIRA 17:4)
1. Dnopropotrovf3kiy motallurgicheakiy institut (for Somikin).

33325 KATSEN. L. YA,
NakrovatrWy stolik dlya bol'rWkh v kostnotifoerkuleznykh sanatoriyakh.
Problemy tuberkuleza, 19490 No 6. a. 61-62

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L :8408'-66 WR
E~IT( I ),/FSS
ACC MR, R`b U I V
Charactexistics of detect-lo'n Kh-wcu' terlatiki obnarazl-senlya) Moscow, Izd-vo "Sovet-
. skoys-radio", 1965. 95 p. illus., biblio.., &4agrs. 7500 copies printed
TOPIC TAGS: radar detection, radar engireering, radar siEpal processing, pulsed,
radar, coherent radar, oontinuous radar,
PUFME AND COVERAGE- Ttiis booklet is intended for engineers concerned with calcula-
tim, desigi, and operation of radar equipment. It mV also.be useful for students
In this field. The booklet discusses detection characteristics of radar stations,
su&i as relationships betweeen the probability of correct detection and the nor-
malized range for a widle, ran8p of valms of Integrable pulses and of -T'alse alar-in
pmtebilities. Flickers of signals reflected from real targets and the various
rethods of transmitted pue;er-pulse aid sigial-processing techniques are taken into
emsicbration. Theoretical mterial is presented in two chEpters In ortl-er to ex-
plaf-n the principles used to obtain tb~ graphs. T. S. Zotava and M. P, Zhurolay
participated in the calculation of deb~cticn characteristics. G. M. Zemlyanski
ccnstructed the range -cal culat ion nomp-am V. D. Zubakov and B. A. Suftrenin
maji and corrected the nmuscript. A. E. Basharinov, L. D. Goll~r.-zhteyn, aid V, I,_
_J~gqv provicbd commnts and ad-Ace.
TABIE CF ODNTEM
Cam ux: 621.4.o2i

ACC: NR,
Foreword -- 5
Ch. 1. Detection4ameterlstics of the radar station for single-tigial. taript.
detection --;; 8
1. Probable estimtion nethods of radai%-&Aection range evaluation
2. Selection er-mrs md niles of acceptance of the solution In problem of radar
detection - 15
-tection of a single sigial on the badq~rotmd of noncon-elated noise - 22
3~ DL
Ch. Ii. retectim characteristics of -the Taear station for sigial-pocket tarVt
cetection - 35
1. Detection of incoherent packet reflected ftom a static taxWt 35
2. Detection of flicker taiVt 40
3. Detection of col)erent packet 47
4. Target detection duAng contInuous. radiation - 52
5. Probability of detection during cyclic scannDig - 53
6. Exarrples of calculation 57
Ccnelusion - 67
Bibliography -- 68
AppendAxes 71
CC-";', 17/ sLram nni o6veW/ MIG Ws 014/ OTH RU 1 011

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Waves, neotrompetio
Dieleotrion
"'Ths-DIstribution of Blectrccagnetio Waves )Aong In.
finite DI'oleatrical Cylinders at low 7requenclea,"
B, Ze Weenouift4us, 4 pp
"Dok AksA iiauk SM., Nova Ser" Vol Min, No 7
With very broad 8-~ -s~pt".Jql-
above that two polarized
vaves,, with different forms, can be Ustributed alioug-
an Infinite dielectrIcal bar. In general their speeds
are different, ftWtted by Acadesiolan M, A, Leonto-
TIcho 26 Jun 194T.:
6Mni

USM/Pbysics - Dielectrics
Wave Gulde
Oct 49
Symmetrical Excitation of an Infinite Dielectric
Cylinder," B. Z. Kateenelenbamm, 10 pp,
"Zhur Tekh Fiz" Vol XIX, No 10
Discusses electromagnetic oscillationn arising ~1~
an infinite dielectric cylinder is excited by an
elementary dipole situated on. its axis. In a c~Lv-
ity, the dipole creates a spherical wave throug)i-
out the space. In the presence of an infinite
cylinder, plane waves form along with the spherical
wave. Plane- waves may be propagated along the d:L-
electric cylinder under certain conditions. Slti~,44-~L
151T88
USSR/Physics - Dielectrics (Contud) Oct 4q,
structure of these waves, region of their for-
mation, and distribution of enerey between them.
This problem is closely associated with Noether
cmd Vladimirskiy Is work on the excitation of a
tallic cylinder and with Pistollkors' work on -,2*
excitation of a cylinAer made from magnetic materi-,
al. Submitted 18 Oct 43.
F

JSSR/Physics - Dielectrics Oct 49
Wave Guide
"Nonsymmetrical Oscillations of an Infinite Dielec-
tric Cylinder," B. Z. Katsenelenbaum, 10 pp
"Mur Tekh Fiz" Vol XIX, No 10
Discusses free and forced nonsymmetrical oscillations
Of~.sn infinite dielectric cylinder. Studied charac-
t;r-istic eq-aation for nonsymmetrical plane waves
propagated along the cylinder and structure of the
'wave field, classifying them completely. Solved
problem on excitation of the cylinder by an elemen-
tary electric dipole placed on its axis for vhicli
a ymmetrical plane waves are propagated along the
151T89
USSR/Ph-ysics'- Dielectrics (Contd) Oct
cylinder along with the spherical wave. Deri-ved a
genexal expression for the radiation resistance of a
ddpole placed in an arbitrary dielectric body whose
d1mensions are small compared with the wave length.
Submitted 18 Oct 48.
151T89.

jj-r~) NEI P-111-.Uf p
tv
Z. WiltaS4"ps with nonfileal mills,
Dolklady Akad. Nauk SSSR (N.S.) 88, 37-40 (1953).
Ved. 'H
SopL. VP"', The nuthor (Ictermineq the w lority (himping ana fimtj
configuration of cleclummignelilt'. wayvq III a of
arbitrary cross-section, the ivalk of whichare good, bilt nol
jx-fect, Conductors. I I is analysis is based oil the sllrce~sivv,
expansi6n of the field% in powcrs of the complex wave re.
sistance of the wayiguide walls. This permits the aj;plication
of Lcont6vicl'i's b(;undary condition [im-pstigations hito the
Picipagation of Radio Wavesi, Vol. 2, 19-18 (in Russian)]
and the consideration of only the interior iegion of the
Wavegilide. C 11. Papq (Pa-,adei.:i, Calif.).

USSR/Engineering - Radio FD-3221
Card 1/1 Pub. 41-2/22
Author : Katsenelenbaum, B. Z., Moscow
Title : Degenerate modes in wave guides
Periodical : Izv. AN SSSR, Otd. Tekh. Nauk 7, 9-22, Jul 55
Abstract : Investigates disturbances produced by small sloping deformations
of the boundaries of wave guideFi with finite conductivity. Es-
tablishes an equivalent boundary condition in the form of small
slanting discontinuities in the path of magnetic currents along
an undeformed surface. Applies usual methods of the theory of
disturbances to the case of degenerate electromagnetic oscil-
lations in wave guides. Concludes with investigation of certain
questions on non-sloping local disturbances. Four graphs; formu-
lae. Eighteen references, eight USSR.
Institution t Institute of Radio Engineering and Electronics, Academy of
Sciences USSR
Submitted : 18 February 1955

t2'
L
-SHTEYNSHIRYGER, Vollf-Bentsionovich; 1OKSHINA,T.A., redaktor; NNYMO,
H.S., profeasor, doktor tekhnicheskikh nauk, rateentent;
SKRFJ&ENBAUM,B.Z.. kandidat tekhAichaokikh nauk, rateenzent;
redaktor
(Phenomena of Interaction of waves in electromagnetic resonators]
lArleniiavsalmodeletvits. voln v alektromagnitnykh razonatorakh.
Moskva, Gos.1zd-vo obor.promysh., 1955- Ill P. (MLRA 9:2)
(Electric resonators)

Pe7-iodlcal Do~,~. A'. 1102/4; 7-11-7,14, Jun 1, IQ5S

OPSENETENTHUM J I .
_9 6-~Z-
Cate'-~ory USSR/Radiophysics - Radiation of Radio Waves. Antennas 1-5
Abs Jour Ref 7hil - Fizika, No 2, 1957, No 4510
Author Katsenetenbaum, B.Z.
Inst 'Tiia-t-i-t-u-t-e-o-f-FA-Za-o-bigineering and Electronics, Academy of Sciences, USSR
Title Bent Waveguides of Constwit Cross Sections
Orig Fab Radiotekbaika i elektroulka,, 1956,, 11 No 21 171-185
Abstract Solution of the problem of the passage of an electromagnetic wave
through a bent waveguide of any cross section. The walls of the wave-
guide are assumed perfectly conducting. The field in any section is
represented as the superposition of waves that can propagate in a
straight-line'-4aveguide of the same section. The amplituaes of these
waves depend on the angle of the cylirAiical system of coordinates, the
axis of which agrees with the'axis of,the-bend iii the given section. A
first-order system of differential equations'is established for these am-
plitudes; the amplitudes are continuous in'the junction between sections
that have different duivatur6s; this determines the values of these
functions on the boundariis-of'flie bent portion of the waveguide. The
coefficients of the system of equations depend on the shape of the
Card 1/2

CatUorr: UM/Radiophysics - Radiation of Radio Waves. Antenaw 1-5
Abs Jaw Ref Zhur Fizika No 4510
., No 21 195",,
transverse cross section, on the diractiono and on the nadi~ftucle of the
curvature. The syst6m-of equatinns.deschbes the coupling produced by
the4curiping of the vs:vegLAde between vaves that are independent of each
other in the straight vaveguide. In the case of a bend having a short,
el6ctric_length_(bi6ak) &A bf'6 bend hivb* a large radiu's of cur*ature,
the syst6i' is-i6lve4l'in 'qua ~ituiei, and 6x]~Ucit'ixpressi6zis are obtii~~d
for -the -6mplitudes of alX"th6 -w9v6s' - A detailed * analysis is mad6 of the
case-Wher-e-a wav6 in a round w0eguid6 is incidnet'on a section that
is 'bent'ifi a` ~rhglAr4xc. .A digeneracy occurs in'this case, the Z
wave'bas the'skie velocity as -the AO'J"'and therefore after' passing 4woush
~ - finit6 angle it as 6=6a fbAte values even if the - radius of curvature -
is lirge. The'nethod develop6d in thei-'afticle'leads to the'known results
by .Jouguet '(J6u~et * IC- Ciblii 6t Wan~mds gi6n, - 1947, 1, No 2, 133)
for the - i&me'pr6ble_m~'Q__t6_ gexiekaliz6 these results in many'respects
The _IdAs6s - due 'to the - transforimatioh of -the Eb, wave by- a- b 'reak of
i6E43id'drd 6alculatbd. The t1al re3Ati*e'_loss'6s* .of ener- are equal
9y
appr6ximiLte- ly'16 -.- 6 10 )'(k'is the vavi*niunber in vacuum and-
&_th6-_radiub_bf the__ii-4egtiide)_. .. AppFoximtely-315 of -the energy'is
carried-6~'the' ii~_Ae' while the Hil carry 1/5 each.
and 'Eli modes
H12 - *
Bibliography, 6 titles.
Card 2p

_i~_, ~09 _T_,-~ 00~&:7
Category USSR/Audiophysics - Radiation of radio waves. Antenn s 1-5
Abs Jour Ref Mmi - Fizika, No 1) 1957/ No 1864
Author Katsene-lenbaum, B.Z.
Title -.-eymmetrIt-InIT6c-t-r-Ic-TFansition in Round Waveguide for Hol Mode.
l
Orig Pub : Hadiotekha. i elektronika, 1956, 1, No 3, 3-19-343
Abstract : Explanation of an example of the application of the transverpe-cross sec-
tion method to the problem of the incidence of a Rol mode irx a round vave-
guide on a long symmetrical dielectric tranaition. A general equation is
established for the determination of the r6flection coefficient of such a
transition.
Card 1/1

-T- S C A) ~_:7 J~
T)IT
kUTHORt KAT SEITEIM, NBAUM 0 B. Z. '109-5-3/22
TITLEt --L-on-g--By-m-m-el-ric-a-1--Wa-ve guide Transition for the Wave H01.
(Diinnyy.simmetriohnyy volnovodnyy perekhod d1ya
volhy H,,, Russian)
PERIODICALt Radiotekhnika i 41ektronika, 19571 Vol 2, Nr 5, PP 531 - 546
(U.S.S.R.)
ABSTRACT: Two wilveauides with circular cross section and common axia
but with different radii, are connected with each other by a
waveguide transition which is a body of rotation. The angle
which is formed by the generatrix of the waveguide with the
axis is a small quantity which has everywhere one and the same
order of magnitude. The wave H I impinges upon the non-regular
waveguide. The amplitudes of tfie reflected wave and thoso of
the parasitic H n- type waves are determined here. From the
mathematical po?nt of view an ordinary homogeneous differential
equation of second order and special type is investigated in
the first case, namely in the determination of the coefficient
of reflection of the impinging wave. For determining the
amplitude of the parasitic wave H , a non-homogenoous equation
is solved. The formulae derived A% can also be applied to
the case in which the wave numberof one of the waves, which is
Card 1/2 calculated for a regular waveguide, becomes equal to zero

109-5-'1/22
Lone Symmetrical Waveguide Transition for the 'gave H 01.
in any'cross section of the waveguide transition.
Ojith 1 table, 2 illustrations and 7 61avic references)
ASSOCIAEION: Institute for Radio Engineering and Blectronics of the Academy
of Science of the U.S.S.R. (Institut radiotekhniki i elektroniki
AN SSSR, Russian)
PRESENTED BY:
SUBMITTED: 29.8.1956
AVAILABLE: Library of Congress
Card 2/2

20-2-9150
AUTHOR. Katsenelenbaum, B. Z.
~TIT!St On the General Theory of Non-Regular Wave Guides (K obshchey teorii
nerogulyarnykii volnovodov)
PERIODICALs DokladY AN SSSR, 1957, Vol. 116, Nr 2, pp. 203 - 206 (USSR)
ABSTRAM In a previous work (rep. 1) the author developed a nethod by which
the problem of the propagation of radiawaves in EL non-regular wave
guide is reduced to a system of ordinary differential equation3.
Further previous works by the author dealing with this method are
mentionsd. In the present paper this method is applied to the
problem of the symmetric electric wave in a symmetric wave transi-
tion with a circular cross section. Here a restriction assumed in
a previous paper is omitted. In the case of cylindrical coordinates
and a dependence with respect to time exp(i 63 t) the Maxwell equa-
tions give the following relations for the field to be investigated
here the line denotes ;3/a z)t E
= (1/ik)HI, E -(1/ik)(1/r)b

r.
rH)/b r; k = W/C. A formula is g2ven also for ihe azimuthal com-
~
ponent H(r, z) of the magnetic field. The cross sections of the
wave guide through the planes z = const are circles with the radius
Card 1/2 (r,z) are introduced which at any z =
a(z). Next, the functions H
M

On the General Theory of Non-Regular Wave Guidec
20-2-4/50
const represent the ma8metic field of the waves E om in a regular
wave Side with the radius a(z). The further course of computationa
isfollowed. In the general case the field are expressed by two po-
tential functions. Next, the author discusses yet another method,
which is not quite as rigorous, but very illustrative, with the
help of which all most interesting properties of a non-homogeneous
wave guide can be determined in an elementary manner. The expres-
sions for the amplitudes of the parasitic electric waves in wave
transition computed with the help of this method are given. There
are 10 references, 7 of which are Slavic.
ASSOCIATION: Radiotechnical and Electronic Institute AN USSR
(Institut radiotekhniki i elektroniki Akademii nauk SSSR)
PRESENTED: May 11, 1957, by B. A. Vvedenskiy, Academician
SUBMITTEDt May 11, 1957.
AVAILABLE: Library of Congress
Card 2/2

B. Z. KATSMIMMM-1, IN. P. Nehzhentseva, V. V. Malin, A. X. Sivov-
waves in a,periodic waveguide." Scientific Seasion
"Frop~gation of 901.4
Devoted to Radio Day, Itay i958, Trudrazervizdat,, Mos,;ow, 9 Sep. 5F--
Conditions for the propagation of a summetric magnetic Hol wave
in'a rectilinear periodic waveguide and the transmission of an H01 wave
through a bend in a periodic waveguide are investigated,
The periodicity, shape and size of the conductor from which the
waveguide is wound, the finite conductivity of the metal, the dielectric
shell of the waveguide are taken into account in computing the damping
of the Hol wave.
The coupling coefficients of the Ho~ wave with the parasitic E
and Hj_ type waves which arise are foundNben analyzing the transmission
of the H()l wave through the bend.

109-1-4/18
AUTHOR: Katsenelenbaum B Z
TITLE: Influence of the Dielectric Film on the A'tenua`ion of the
u
Hol Wave in a Straight, Nearly Circular Wa-ve'-uide
(Vliyaniye dielektricheskoy planki na zatulzhaniye
V
volny H 01 v pryamolineynom volnovode, blizkom k 1:ruz;ovoM1_0
PERIODICAL: Radiotelchnika i Elektronika, 1958, Vol.III, lir
pp-38-45 (USSR)
ABSTRACT: A thin serai-conductinr" film. derosited on the innez sur-
face of a wave-uide results in tie at"i-enuation of the waves
C.3
propagated in the Suidle. For the waves of H., tud-pe, the
0
attenuation is proportional to the cube of the film t1hick-
ness, 8 , and it is much lower than the attenuation for
other waves, which is proportional to 6 . If the valls
of the waveguide are deformed or distorted, the field be-
comes distorted and a normal component of the electric
field appears. This results in an additional attenuation
of H Ora waves, which is proportional to 6 . The atten-
uation increases with the deCree of the deformation. The
Card 1/4

U-1
Influence of the Dieloctric Film on the Attanual-4
Wave in a Strai-ht, Nearly Circular Waveguidc
0
aim of this woric is to determine the additional attenuation
in slightly deformed wave guides, provided t-heir axes are
rectilinear. A circular waveguide, coated internally with
a semi-conducting layer having a dielectric -Vonstamrt
e = e - ie" is considered. It is assumed that in the
presence of a normal electric field component, B n ~ the
attenuation coefficient of the system can be expressed by:
k6r;,11 PEn12 ds
e R e ~ [111% d S
where k w/c The evaluation of the additional atten-
uation of the Ho, wave due to the deviation of the
cross section of the waveguide from an ideal circle can
be determined from the so-called diaphragm fu-ac-'k-lion, whhich
can be evaluated by findi.n7 the eigen-function of the
boundary equation given by Formula From this, it is
0
Card 2/4 found that the contour integral of Eq.(6) is by

109-1-4/18
Influence of the Dielectric Film on the Attenuation of the H
01
Wave in a Straight, Nearly Ciicular Waveguide
0
Eq.(20). Since the integral enters into the expression for
the additional attenuation of the viavegW 'del as can be seen
from Eq.(6), the solution of the inte-ral car- be used to
determine the value of the attenuation. It is found thlat
the additional attenuation is expressed by E-.(27) where
PO_ is given by Bq.(L~). If t1le ljaV(-(,rU:L(-I(- as subject to an
elliptical defor.-iiiation such that A represents the eliff-
erence between the maximum and the iiinimuln rac'li4-7 the
additional attenuation is exprosood by:
2
P = 2P0
a
where a is the radius of the waveguide. From the Eq.(29)
it can be shown that,if it is necessary to restrict P to
less than 10-3po should be smaller than 2.2xlO-2
a
In this case, if a 25 mm , the difference between the
Card 3/4

109-1-4/18
Influence of the Dielectric Film on the Attenuation of the h-01
Wave in a Straight, Nearly Circular Waveguide
0
semi-axes should not exceed 0.6 mm. The most important
result of the above analysis is Eq.(27), which can be ex-
tended to the evaluation of the attenuation in waveguides
with appreciable deformations, in pazticular, in thle Sys-
tems in which the cross section varies as a function of
length. The paper contains 7 references, 3 of which are
Russian and 4 English.
ASSOCIATION: The Institute of Radio Engincerin- and Electronics
of the Soviet Academy of Sciences (Institut radioteklmill:11
i elektronikil, Ali SGSR)
SUBMITTED: February 13, 195?
AVAILABLE: Library of Congress
Card 4/4

KRTSENEA_aN51AVfv1, B,-Z
108-13-3-10/13
AUTHOR: None Given
TITLE- Inter national-Congrpos for High-Frequency Circuits and
Antennae (I!ezhdunarbdrqy kongress po tsepyam i antennam
sverkhvysokoy chastoty)
PERIODICAL: Radiotekhnika, 1958, Vol. 131 Nr 3, PP- 73 - 75 (USSR)
ABSTRACTi This are transactions of the congress which took place
in Paris from October 21 - 26 1957. It was organized
by the French Society f_or~_T=chni~caEngineering and
Radio Engineering and was supported by the government, the
trade unions and a number of companies. 166 lectures
were held. In two commissions the membera of the
Soviet delegation Professor A, L. Yikaelyan and the
Corresponding Member of the At USSR A. A. Pistollkors
were elected chairmen. Of the Soviet delegates B. Z.
-Katsenelenbaum spoke on the theory of wave guid-e-s with
slowly chan-(-;1n-g pakameters, and Yu. I. Kazziacheyev
on works and sucess'in the theoretical field of tele-
communication over great distances by means of the
Card I/ Hol-wave.

AUTHOR: Katsenelenbaum, B.Z. 109-3-5-6/17
TIM: Bent Waveguides with a Von-homogeneous Medium (IzolDrnutyye
volnovody s neoclnorodUm zapolneniyem)
YERIODICAL: Radiotekhnika i Elekt-ronika, 1958, Vol III Nr 5
Pp 634 - 640 ~U&ssll)'
ABSTRACT: The work is a generalisation of the results obtained
by the author in an earlier article (Ref.1). The solution
is based on the concept (Ref.1) that the field in a bent
waveguide can be represented as a super-position of the fields
whi--h exist in rectilinear waveguides; the coefficients of
the super-position br this solution are expressed by a system
of differential equations. The boundary conditions at the
surface of the waveguide must be satisfied by each term of the
super-position. First, a regular, rectilinear waveguide, filled
with an arbitrary medium is considered. The fields at the wall-s
of the guide should satisfy the conditions expressed by Fos,(l)
and (2), where s and z denote the direc'Ui--)P-s tah-ent to
the waveguide and; 1 + i
W - kd1
2
uhere k is the wave number and d. is the thickness of te
surface layer. The waves propagating in the positive direction
Ca.rdl/30f the z- axis can be written in the form of Eq.(3',;, where

Bent Tylaveguides with a non-homoGeneous Medium
1 is the wave index and h ~i is the pve number. The
components of the vectors and I should satisfy Ecf,(5)
which are derived from the Maxwell equations (Boo.(4) ).
The fields propagating in the positive direction can be
determined from Eq.(6~, while the components of the two,waves
differing by the sign of the index are related by Eqs.(?).
can be express6A -in terms of two diaphragm
The fields E I
functions, as given by Eo.(8). The fields of different waves
are mutually orthogonal so that the integral ., taken over
the transverse cross-section of the waveguide, is equal to
zero. The fields in a bent waveguide (Ref.1) shouldh1fil
the conditions expressed by Eqs.(10), where the functions
Pi((3) are determined by the system of Eqs.(14). The functions
Pi(;~) can finally be expressed in the form of Eq.(17), in
I
which ir, = iF The coefficients F and 1,1 are expressed
by Egs.(19) and (20), respectively, in which N is ~.ven
by Eq.(21). The above analytical results are used to determine
the fields ia an empty waveguide and it is shown that they
lead to the same final expressions (see Eqs.(29) ) as those
Oard2/3

Bent Waveguides Twith a Non-h- or.,io gene ous Medium
109-3-5-6/1r,
obtained in the earlier vork
There are 1 fiGure and 8 references, 5 of which are Soviet,
2 English and 1 German.
ASSOCIATION: Institut radiotekhniki i elektronik-ti AN SSSR
(Institute of Radio-RigineerinG and Electronics
of th~- , AS . USSR)
SUBMITTED: February 13, 195?
AVAILABIE: Library of Congress
- LD
Card 3/3 1. Waveguides-theor7

SOV-109-3-6-3/27
-AUTHORS:KatsenelenbaiLm, B. Z. and Malin, V. V.
"-7
TITLE: Formation of the Side Flow in a Long.Wave-uide Line: Part I
(Formi--ovaniye poputnogo potoka v dlinnoy C.) volnovodnoy
linii, Ch.I.)
PERIODICAL: Radiotekhnika i Elektronik.a, 19r-8, Vol 51 Nr 6,
pp 750-755 (USSR)
ABSTRACT: The side flow in a wave&uide is defineu as the energy of
the principal wave propagating in the T.,iain direction but
lagging in time behind the principal vianve. This -,,phenomenon
is caused by the presence of various irre-~,'ulariticS in the
waveguide which result in conversion losses -and Dultiple
reflections. The problem was first studied b,,,, X"ierce and
here his basic idea is extended in so far that a relation-
ship is found between the geometrical parameters of the line-
and the side flow. For the purpose of anal.,sis it is assumed
that a is the attenuation coefficient of the main waire
in the i4ide, a ih is the attenuation coefficien'u-for a
parasitic wavel Ili is the coefficient of conversion of
the principal wave into a parasitic wave. THe reverse con-
version coefficient, that is, the coefficient of conversion
Card 1/4 of a parasitic wave into the principal wave, is asstuied to

Formation of the Side Flow in a Long Waveguide Line: Part I
be equal to a li 11 It is further asswded that the principal
wave propagates in the direction of the axis z ~ By means
of a simple analysis (see Fig.1). it is shown that the
relative energy of the side flow at a distetnco z cali be
exp2essed by:
T
_02 [2 uqj (5)
where m. qi and -a are defined by Eas.(6). The
-Daramete_- u in Ea.(5) denotes the length of the line in
of the
normalised units he parameter m i defines t1l_e typ-c I
waveguide irregularity, while qi is a para.motor -dependent,
on the attenuation coefficients of -the T)rinci-oal and the
parasitic waves. The side flow equation can also be derived
more rigorously on the basis of Eqs.(?), where P is the
Card 2/4

10"-'5- -0-3/27
Formation of the Side Flow j-n a Long 1,11aveguide Line: Part I
energy of the principal wave, 1~1 is the ener- of the
Sy
parasitic Nvave and Pn relates to the side flow. Solution
of Eq.(7) for the boundary conditions expressed by Eq.(8) is
in the form of Eq.(9). From Eq.(9) it follows that Eq.(5)
is accurate provided it fulfils the condition expressed by
Eq.(10). The.density distribution of the side flow can be
expressed by Eq.(11), in which the variable ~ =~L/z ,
where z is the length of the wave guide and L is the
position of a cross-seotion; the function C in Eq~(ll) is
defined by Eq.(12). A graph of Bq.(,-II) is given in Fi-,2.
The distribution density of the partial side flow as a
function of its time lag Te is expressed by Eq.(17), where
Ti is defined by Eq.(15); v, and vi in Dlq.(15) denote
the group velocities of the.principal and the parasitAc waves,
respectively. In certain cases, it is more convenient to
employ a non-normalised expression forthe partial side flow
density distribution. which is in the form:
-2uq,.~-
(2m U)2 1- (1 e (18)
Card 3/4 i Ti T,

,- 3 /C"' 7
SOV-1 13
Formation of the Side Flow in a Long Waveguide Line; Part I
where the term 2m.iu = aliz denotes the conversion. losses
for the principal wave. and t~ is expressed by Eq.(14),
There are 2 figures and l.En-l-*Lsh reference,
0
ASSOCIATION: Institut radiotekhniki i elektroniki All SS,3)R
(Institute of Radio Engineering and Electronics of the
Soviet Academy of Scienoes)
SUBMITTED: November 21,, 1956
1. Waveguides - Psx9o,-m&=* 2. Wa-veis- - P~~qpaga-'EAL %P-
Card 4/4 3. Mathematics - ApplicationB

C~
307/100/-3-7-4/23
AUTHOR: Katsenelenbaum B
TITLE: Irregular Waveguides with Variable Dielectric Filling
(Neregulyarn,Tye volnovody s peremennym dielektricheskim
zapolneniyem) 3
PERIODICA1: Radiotekhnika i Elektronika, 1958,.,-,Nr 7, pp 890-895
(USSR)
ABSTRACT: The paper deals with the propagation of the electro-
magnetic waves in a waveguide which is obtained when a
regular waveguide is filled with a material having a permit-
tivity e and a permeability g which are functions of all
the three coordinates.The.analvsis is based on the followin---.
at a point x, y, z the fields 2 and it are assumed to
consist of a set. , of wavesihich would exist in a regular
waveguide where z and ji are the same functions of the
coordinates x and y in the transverse cross-section,
as= ~).and It in an irregular waveguide (for a given
z The coefficienta of this set' are functions of
and it is possible to determine for them a system of differ-
ential equations of the first order. In some cases it is
Card 1/4

30V/109-3-7-4/23
Irregular Waveguides with Variable Dielectric Filling
possible to find an explicit solution of such a syste~i. By
employing conformal transformation, various cases dealing
with local irregularities in a waveguide can also be con-
sidered as a problem of a waveguide with a non-uniform di-
olectric. It is assumed that the fields in a regular wave-
guide are in the form of:
y, z) - 2'(x, y) exp (,- ihiz), ~ (x, Y, Z) Y)
exp (- ihiZ)
where the various components should fulfil the conditions
imposed by Eqs.(2). The fields of Eqs.(l) can be deter-
mined from the Maxwell equations and they should satisfy
the orthogonality condition as expressed by Eqs.(4), where
the integrals are taken over the transverse cross-section.
0
The transverse components of the field at an arbitrary
cross-section z =-~ can be expressed in terms of the
series given b.Y Eqs.(5). This can also be v..-ritten in the
form of Eqs.(6). On the basis of Eqs.(6) and (3) it is
possible to obtain a system of equations which describe the
Card 21L~ interaction of various types of waves in an irreSular wave-

SOV/109-3-7-4/23
Irregular Waveguides with Variable Dielectric Filling
guide. This system is expressed by Eq.(8), where Si~ is
the so-called coupling coefficient. The coefficients can
be expressed by the integral of Eq.(9) or by Eqs.(10) _md
(11) )Iq~(ll) can also be represented in the form given by
Eq.(i2 o by Eq.(14), where S refers to the tangent com-
ponent and n denotes the normal components. When e 4 oo
the coupling coefficients can be expressed by Eq.(16). rrom
the above it is concluded that a general expression for the
coupling coefficients in a waveguide of variable cross-
section can be obtained from the analysis of the electro-
magnetic field in a waveguide having a constant cross-section
but filled with a non-uniform dielectric. The paper contains
Card 3/4

30V/101.)-3-7-4/23
lrx~egular Waveguides with Variable Dielectric Filling
13 references, 4 of which are English and 9 Soviet. 5 of
the references relate to the works of the author.
ASSOCIATION: Institut radiotekhniki i elektroniki All SSSR (Institute
of Radio Enpneering and Electronics of the Soviet Acadeirq
of Sciences)
SUBMITTED: December 31, 1957.
l..Waveguides--Electr,llcal properties 2. Electromagnetic waves
--Propagation 3. Electric fields--Analysis 4. MAgnetic fields
--Analysis 5. Mathematics
Card 4/4

AVTHORS:
TITLE;
PERIODICAL:
ABSTRACT:
SOV/109-3-11-7./13
Xatsenelenbaum, B.Z. _4Lnd Malin, V.V.
Formation of the Side-flow in a Long Waveguide Line,
Part 2 (Formirovaniye poputnogo potoka v dlinnoy
volnovodnoy linii, Ch. 2.)
Radiotekhnika i Blektronika,,1958, Vol 3, Nr 11,
pp 1389 - 1398 (USSR)
In an earlier work by the authors (this journal, 1958,
Vol 3, Ar 6, P 750), an equation was derived for a
coefficient mi which determines the magnitude of the
transt6rmation losses in a waveguide and which plays
a substantial part in the formation of the side flow.
In the following, the coefficient is evaluated for
several caBes of waveguide discontinuities. It is
assumed that the deformation of a waveguide, which does
not involve the bending of the waveguide axis, can be
described by an equation r = a + J(z, where a is
the radius of an ideal waveguide and is the defor-
mation (discontinuity) which varies at various points
of the waveguide surface. If the waveguide is operating
with an 1101-wave, the amplitudes of the prasitic
Cardl/5 H-waves can be described by (Ref 3):

SOV/109-3-11-7/13
Formation of the Side-flow in a long Waveguide Line, Part 2
L
+ -J)10)li ep -js i z
ep
a (z)e dz (3)
2
F
O~h_ohj I p7 2 p
i
where it.is assumed that the deformation extends over
a distance z = 0 to z = L ; i is the number of the
parasitic wave, Ili is the root of the derivative
of the Bessel filn tion (sach that, 2tra/Iii it, the
critical wavelength for a given type), h i is the wave
number for the %-wave The coefficient a P(Z)
in Eq (3) denotes either ap(z) or bp(z) from Eqs (2),
depending on the polariEation of the wave. The quantity
81 is defined by Eq (4). Eq (3) can be written as
Card2/5 Bq (8) in which the factor B i is defined by Eq (7).

SOV/109-3-11-7/13
Formation of the Side-flow in a Iong Waveguide Line, Part 2
The energy of a parasitic wave can be expressed.by a
function P i which is defined by Eq (5). On the basis
of Eq (8), the energy carried by the parasitic waves
causod by the waveguide junctions of the type illustrated
in Figures 1, can be expressed by Bqs (9),-(10) and (11).
In a practical waveguideq the discontinuity parameters
a, vary as a function of distance and it is therefore
ne essary to evaluate the averages of the functions
defined by Eqs (9), (.10) and (11). The resulting
expressions for the 3 cases illustrated in Figure 1 are
given by Eqs (12) and (13). If the axis of the waveguide
is curvilinear, the amplitudes of the parasitic waves
can be expressed by Eqs (17), where R is the radius of
curvature and B i is the amplitude of a parasitic wave
of the same type (H14) which is produced by curvature;
Bi is calculated for 1 radian. The above formulae,
as well-as the formulae from the earlier work, were employed
to investigate the sideflow in three particular cases.
Card3/5 'Aln the first case, it was assumed that a 2.5 cm,

SOV/109-3-11-V13
Formation of the Side-flow in a Long,Waveguide Line, Part 2
X = 0.8 cm, the height ok the discontinuity is 6 = 0.005 cm
and that the main wave Is of the H 01 type; the dis-
continuities are due to junctions; these are assumed to
be symmetrical and spa"d at a distance of 150 cm. The
amplitudes of the parasitic H 01 waves for this case were
evaluated by using Eq (?) and the results are shown in
Table 2. The attenuation coefficients for these waves
can be found from Lrq (21); the results are given in
Table 3. The additional parameters for the system are
.given in Table 4. The above numerical results were
employed to construct a ni=ber of graphs; these are shown
in Figures 3 and 4, where the curves of Figure 2 illustrate
the distribution densities of the partial sideflows for
various waves, while Figure 3 illustrates the overall
distribution density for various lengths of the waveguide.
In the second case, it is assumed that the sideflow is due
to the displacement of the axes of the waveguide sections;
again it is assumed that 6 = 0.005 cm. The amplitudes
of the parasitic waves fox this case are shown in T~des 5
Card4/5 and 6, while the-total sideflow as the function of the

SOV/109-3-11-2/13
Formation of the Side-flow in a Long Waveguide Line, Part 2
overall waveguide length is represented by Curve 2 in
Figure 4. The third case refers t8 a waveguide having
a bend with an angle,equalling 0.1 . Various relevant
parameters for this case.are given in Table 7, while
the total sideflow is illustrated by Curve 3 of Figure 4.
There are 4 figures, 8 tables and 8 Soviet references.
In AN SSSR
att*t t udio~ekhnikl i elekt
ASSOCIATION: (In Mte o a io EngIneering KaaikeUtronics
of the Ac.Sc.USSR)-
SUBMITTED: November 21, 1956
Card 5/5

I ~
9(6),9(9)
AUTHOR: SOV/20-123-1-13/56
Abaum B. 7
TITLEs Tho Critical Cross Sections in Non-Regular Wave Guides
(Xritiohoskiye secheniya v neregulyarrqkh volnovodakh)
PERIODICAL: Doklady Akademii nauk SSSR, 1958, Vol 123, Nr 1, PP 53-56
(USSR)
ABSTRACT: In one of the author's previous papers (Ref 1) the amplitude of
the wave H on produced by the incidence of a wave Rol on to a
symmetric wave guide transition is calculated. In an arbitrary
cross section of this transition the wave number h of the
n
wave Hon becomes equal to zero. In this paper the same problem
is solved for an arbitrary wave in a rectangular non-regular
oblique wave guide of any shape with ideal walls. The eleotro-
magnetic field in an irregular ware guide is explicitly
described in the case of a dependence with respect to time by
the infinite system of equations
1 00
Pj + ih P i M 1 8 iv PV
Card 1 A (the prime denotes the derivalt"i-ocon according to the coordinate

The.Critical Cross Sections in Non-Regular SOV/20-123-1-13/56
Wave Guides
Z along the wave-gulde) and by the boundary conditions 0
and z - L at the ends of the nona-regular domain. These boundary
conditions are determined by the nature of the wave inciding
upon the aforementioned domain. Pi(z) denotes the amplitudes of
the waves of various types whioh may exist in a regular wave
guide with a cross aeotion equal to that of the non-regalar
wave guide. A general expression is written down for the
coupling coefficients S im (z) and is Bpeoialized for elentric
and magnetic waves. Wear the critical arose section the field
cannot be represented as a sum of the fields of direct and
inverse wavest and new critieal variables must be introduced.
Also equations of second order are written down for these
variables. Also in the general case investigated herat the
problem is reduced to the integration of the equation
investigated in the aforementioned paper (Ref 1) for a special
case. In the case i - 1 (i.e. if in the critical crosb section
the wave number of the inciding wave becomes equal to zero) the
field is described by a Pomogneous equation in the highest
Card 2/4 order with respect to 1~. 0 denotes a certain average

The Critical Gross Sections in Non-Regular SOV/20-123-1-13/56
Wave Guides
cross section of 1~(S,Z)l , and 4(s,z) denotes the tang of
the angle between the tangent to the wave guide (which is
vertical to the edge of the cross section) and the z-axis.
In the case i ~ 1 inhomogeneous equations given by the author
are to be solved. For the system of differential equations it
is possible to give a boundary condition (or more exactly
expressed, a condition for the end of the wave guide), which is
equivalent to the existence of a critical cross section: in
this way the critical domain can be eliminated from the
investigation. These "end conditions" are then explicitly
written down for magnetic and electric waves. Outside the
critical domain the direct and inverse waves form independently
of one another. However, in the critical domain the parasitic
field forms as a whole. The use of the "end condition" derived
in the present paper permits a uniform analysis of the field in
the entire non-regular wave guide.
Card 3/4

fte Critical Cross Sections in Non-Regular SOV/20-123-1-13/56
Wave Quides
There are 6 references, 6 of which are Soviet.
ASSOCIATION: Institut radiotekhniki i elektroniki Akademii nauk SSSR
(institute for Radio Engineering and Electronics of the Academy
of Sciences, USSR),
PRESENTED: June 20, 1958, by B. A. Vvedenakiy, Academician
SUBMITTED: June 17t 1958
Card 4/4

i~V(V,11Tl',T!BAUV',j B.Z., Doc Phyr,-Ya%li Soi f
bi i rhi ii-r
irrc.,,,:ulgLr vnvok~aw with slo-~~!ly all-nCinC p- U
T QUCe Of t, pp soi ussj,~. t of
B iv; Acnd of Sci USK; 1959 - 16
fiadiol~[ZineerinC and tloctronics) - 175 cOrie9, ~iblio,-r~q)hy A end
of toyt (10 titL:2) (K-1,08-59, 113)

SHIRMAN, Yakov Davidovich; KATSMaMMAUMV. B.Z., kand.takhn.nauk, reteenzent;
DOMBROVSKIY, I.A., kand.takhn.nauk, retsenzent; PZRSIXOT. N.Y.,
kand.tekhn.nauk, otv.red.; NOTIKOTA, Ye.S., red.; KARABILOVA, S.F.,
tekhn.red.
LRadio wave guides and-cavity resonators] Radiovolnovody i obwem-
nye rezonatory. Moskva, Gos.izd-vo lit-ry po voprosam sviazi i
radio, 1959. 378 P. WRA 12:4)
(Wave guides)
I

sov/log- --4-3-11/38
AUTHORz B.Z. Katsenelenbaum
TITLE: emation of Hon-waves in a Helical Waveguide
(Zat-akhaniye voln Hon V spirallnom volnovode)
PERIODICAL: Radiotekhnika i Elektronika~ 1959, Vol 42 Nr 3,
pp 428-432 (USSR)
ABSTRACT: The following notation is adopted; the radius of the
waveguide is a', the angle between the axis of the
waveguide x and the wire of the helix is 1V/2 - V I
the "period" of the helix is d and the wave number is
k = 2 WA . First, a ring-type of the waveguide is
considered; in this case V = o . The expression for
the attenuation due to the radiation losses is given by:
h" ICL12 ,)2 IM yaH(02) (ya)
7
k2hoa
H (ya)
CL T2 k2e h2
HXO 0

12
Card 1
10) = 0. Ho is
where ~ is the root of the equation J
, 0
the electric field component while Ht,. is the magnetic
MMM

SOV/109- -4-3-11/38
Attenuation of Hon-waves in a Helical Waveguide
field component. Eq (1) does not take into account the
losses due to the dielectric. These additional losses
can be expressed by Eq (5), where ell is the imaginary
component of the permittivity of the-dielectric material
(which surrounds the wire of the waveguide). The
attenuation losses due to the radiation in a helical
waveguide, (V rA 0) are given by Eq (8).
There are 2 figures and 10 references, 7 of which are
Card 2/2 Soviet, 2 English and 1 German.
ASSOCIATION: Institut Radiotekhniki i elektroniki AN SSSR
(Institute of Radio Engineering and Electronics of the
Academy of Sciences of the USSR)
SIMMITTED: October 24, 1957

214385'
S/142/60/003/005/012/015
911-760 11,192/E382
AUTHOR: Katsenelenbaum., B.Z.
TITLE: Reflection of the H -wave in a Rectangular
10
.Waveguide from a Thin Circular Metal Rod Which is
Perpendicular to the Electric Field
PERIODICAL: Izvestiya vysshikh uchebnylch zavedeniys
Radiotekhnika, 1960, Vol. 3, No. 5. PP. 517 - 518
TEXT: The above problem for a rod perpendicular to the
narrow walls of the waveguide was solved in Ref. I (L. Levin
Modern Theory of Waveguides, izd.vo in. lit-ry, 1954) and
Ref. 2 (Handbook of Uaveguides, ed. Ya. Felld. Izd-vo Sovetikoye
radio, 1952) and it was found that the refie'ction coefficient
is given by:
3i S
R - ah - .. (1)
2 S
0
where S is the cross-Bection area of the rod,
Card 1/4

S/142/60/0037 W/01-0/015
Reflection of .... B192/E382
S ab is the cross-section of the waveguide,
0
a is the width,and
b the height of the waveguide.
h 2 Tr/k is the wave number and
is the wavelength in the guide.
In the following an'attempt is made to determine R for an
arbitrary position of the rod provided it is parallel to the
wider walls of the system, During the incidence of the
H 0-wave onto the rod an azimuthal current component flows on
its surface and this produces a reflected wave. The current is
determined by the longitudinal component of the magnetic.field
H and this can be expressed by:.
air-
Hz HO. + 2o -r ,sin
! COs T + w"
Y
where x and y are the rectangular coordinates in the
Card 2/4

Reflection of ... 1
24385-
S/142/60/003/005/012/015
B192/E382
..transverse cross-section of the rod, r and ~O are the
cylindrical coordinates and. (a is the radius of the rod.
The reflected field produced by the-azimuthal current
''proportional to H z can be determined by the waveguide
excitation theory. The reflection coefficient R is
proportional to the integral of the magnetic field given by
Eq. (2) over the surface area of the rod, the integral being
multiplied by the azimuthal component of the electric field
of the incident wave in the absence of the rod. Eq. (2) is
~valid for the rod provided its axis ia perpendicular to the
electric field E The expression for the reflection
coefficient is:
COSCO26 1
R - 30 cos 0 (1 - e-WIL)
S, VIP _7n, TIWW) (3)
where is the angle between the rod and the narrow walls
of the waveguide,
L is the distance between.the "inlet" and "outlet"'
Care 3/4.

s/142/60/003/005/012/015
Reflection of E192/E382
points of the rod in the waveguide, i.e.
L = a ctg_9
For Y --tr/2 , Eq. (3) is identical V;ith.Eq. (1).
There are 3 references: 2 Soviet and 1 non-Soviet.. The
Englisb-language references quoted is: Ref. 3 J. Lane
PIEB,-1955, B 102, No. 6, 8i9.
ASSOCIATION: Vsesdyuznyy N11 fiziko-tekhnicheskikh i radio-
tekhnicheskikh izmereniy (All-Union Scientific
Research Institute of Physicotechnical and
Radiotechnical Measurements)
SUBMITTED: January 19, 1959 (to the editor of the journal
NDVSh)
February 4,1960 to thi#3 journal.
Card 4/4

204
s/iog/60/005/012/009/035
~t 9 U0 E032/E514
AUTHOR: Katsenelenbaum, B.Z.
TITLE: On the Normal Incidence of a Plane Electromagnetic Wave
on a Periodic Separation Boundary of Two Dielectrics
PERIODICALgRadiotekhnika i elektronika, 1960, Vol.5, No.12,
pp.1929-1932.
TEXT- The problem is formulated as follows. A plane electro-
magn;tic wave is incident normally on the separation boundary between
two dielectrics. The separation boundary is a "wavy" surface. The
problem is to determine the amplitudes of reflected, transmitted and
diffracted waves for any values of the wavelength and the height
and period of the surface periodicity. The method put forward in-\)
the present paper is a generalization of the "cross-section method",
which was reported by the present author in Ref.l. The problem is
reduced to determination of the proper waves in the so-called
comparison medium whose properties are independent of one of the
coordinates (corresponding to the direction of propagation of the
wave) and are periodic in two other coordinates. In the final
stage an infinite system of ordinary first order differential
Card 1/2

20411
S/109/60/005/012/009/035
E032/E514
On the Normal Incidence of a Plane Electromagnetic Wave on a
Periodic Separation Boundary of Two Dielectrics
equations has to be solved. There are 1 figure and 6 referencest
5 Soviet and I English.
ASSOCIATIONa Institut radiotekhniki i elektroniki AN SSSR
(Institute of Radio Engineering and Electronics,
AS USSR)
SUBMITTED3 May 9, 1960
Card 2/2

AUTHOR:
TITLE:
PERIODICAL:
S/108/60/015/05/08/008
B007/BO14
Katsenelenbaum, B. Member of the Society
Letter to the Editor. Wave Impedance of a Right-angled WavagtAde
Radiotekhnika, 19609 Vol. 15, No- 5, P. 79
TEXT: According to many authors (Refs. 1-3) it is possible to use formula
(1) for calculating the reflection coefficient R of the H 10 wave of two
right-angled waveguides which are joined together and whose cross sections
differ but little from each otherp if formula (2) is assumed for the
wave impedance W.'(1) and (2) lead to formula (3) (Ref. 3)- It is pointed
out that this formula is not exact, and that formula (4) is correct, It
was published in the papers of Refs. 4 and 5, and is obtained from
formula (1) by assuming (5). R may be determined from.formula (6) especial-
ly in reflection from a wav'eguide with slowly changing oross-sectional
areas. Finally, it is noted that on the basis of the paper of Ref. 6 it
is possible to determine W for any waveguide of any cross section in such
Card 1/2

. Letier to the Editor. Wave Impedance of a S/108/60/015/05/08/008
Right-angled Waveguide B007/BO14
a vay that both (6) and (1) are valid. There are 6 references: 5 Soviet
and I German.
SUBMITTED: September 4, 1959
Card 2/2 4

PHASE I BOOK EXPLOITATION SOV/5876
Katsonelenbaum, Boris Zakharovich
Teoriya neregulyarnykh volno-vodov a medlenno menyayushohimisya parametrami
(Theroy of Nonuniform Waveguides With Slowly Changing Parameter,s)
Moseowp Izd-vo AN SSSRp 1961. 215 P. Errata slip Inserted. 2500
copies printed.
Sponsoring Agency: Akademiya nauk SSSR. Institut ra:diotekhaiki I elektroniki.
Resp. Ed.: V. I. Siforov, Corresponding Member, Academy of Sciences USSR:
Ed. of Publishing Houset V. V. Shmidt; Tech. Ed.: Yu. V. Rylina.
PUUOSE i The book is intended for scientific personnel, aspirants) and ad-
vanced students dealing with electrpdynamic calculations and related problems
in mathematical physics. It may also be used by specialists in Zraveguide
communications.
Card I/#

Theor7 of Nonuniform Waveguides (Cont.) SOV/5876
COVERAGE': 'The book contains a systematic exposition of the calculation method
for fields in nonuniform radio and acoustic waveguides. Bent and tapered
waveguides. and wa*eguldeo with filler material whose parameters vary~ along
the axis of the guide are discussed. Attention is given to waveguides con-
taining campensating.and matching inserts. Large-radius.. waveguide bends,
slight waveguide tapets., and gradual variation of material parameters ire
studied in detail. No personalities are mentioned. There are 114 references:
65 Sovietj 39 English, 5 French, and 5 German.
TABLE OF CONTENTSt
Introduction
1. Content of the' book
2. Survey of litfwature in the field
3. The uniform wgveguide
3
3
7
13
Ch. 1. Metho4 of Minor Discontinuities 20
"Waveguide curvature* Bent.waveguiden as a limit of
waveguides having a laFge number of bends 20
Card 2/5

20576
s/log/61/006/002/008/023
/_3 0 a (a 3 0) E140/E435
AUTHORS: Katsenelenbaum,_D_Z~ and Malina, Z,A.
TITLE: The Design of Tapers for the Symmetrical Magnetic Wave
in a Circular Waveguide --
PERIODICAL: Radiotekhnika i elektronika, 1961, vol.6, No.2,
pp.228-233
TEXT: The problem is to design waveguide tapers for transmission
of the Hol-wave in circular waveguide with minimum conversion loss.
The method used is based on the authors' previous results (Refs.l.
and 3) (studied also by H.Unger, Ref.2). The treatment of
critical sections is based on the authors' previous work (Ref.4).
The method is based on the now well-known analogy applying to a
certain approximation between the problem considered and that of
finding the optimum form of variation of transmission line wave
impedance for a matching section between two lines with differing
wave impedances. The precision of the method depends on
neglecting the difference between the wave length of the Hol-
and H02-waves in the waveguide and in free space. Under these
conditions, the waveguide taper is calculated on the basis of
optimal results known from transmission line theory. Two cases
Card 1/2

20576
The Design of Tapers
S/109/61/006/002/008/023
E140/E435
are considered, one with the absence of critical sections, the
other in their presence. The results obtained show that the
approximation used is valid in the former case. To handle the
latter case a more exact al)proximation, involving greater
calculations, is given. This modification, being more general, is
also applicable to the case of absence of critical sections but the results
are not more satisfactory than the simplified method applicable to
that case. There are 4 figures, I table and 8 references:
4 Soviet and 4 non-Soviet.
ASSOCIATION: Institut radiotekhniki i elektroniki AN SSSR
(Inaiitute of Radioengineering and Electronics AS USSR)
SUBMITTED: June 24, ig6o
Card 2/2

-kATSEMMMAUM.. B.Z.
TheorY bf irregular acoustic u~ve guides. A)aMt*ZhUre 7 no*2:201-
209 161. (MM 14:7)
1. Ingtitut 3?~LdjOtekhnjkj J elaktroniki AN SSSR, Mskva,
(Sound--qransmission)

KATSENELENRAUM) B. Z.
"Diffraction on a broad aperture in broad wave-guide"
Paper to be presented on RADIO (SCIEN=IC) UNION, INTERNATIONAL
(URSI)- Symposium on Electromagnetic theory and Antennas - Copenhagen,
Denmark, 25-30 Jun 62
1. Int3titute of Radio Engineering and Electronics, Academy
of Sciences USSR

V A ro K 4.4, V19rvrYrVYw
a. VA Fnzlt and L& Vpinnt,~I.n -'Crocu-SecLionak
Diffurion in ShorL-Wava Mffrrction on Convex
Cylinder.'
44. MokVULYAW
b. AL Itichn 'Plicnomenoa of Interconnection
of Hapatizod Forrita Pattcrns.,
c. _jZ_&L2pnp Ion', ftLin - 'Diffraction On WidaAperturo
in Mi do-'lave Cuida.1
d. Yah Mononov - 'On Theory of ParcmotrLc Rc:ionanco
in
GI Nakarav - "The rrop.-~ation of Elcctrms:~uotic Vivaa in
Smooth XonosipharLc Zzycro."
re;orts to be submittcd for the Intl. Sytmcaliw on Blectrolzec;naic zleon.
and AbterLnes, Copewhagen, Denmark, Juno lqfL0.

810191621000100810261121
A154/A126
AW11011t Kattonolonbaum, B.Z.
TITLE: 'An image transmission line consisting of a mirror system
POITODICAL: Byullotenl izobrotenly, no. 8, 1962, 30
TEXT: Class 21a4, 4868. No. 146362 (732170/26-9 of May 26, 1961). An
image transmission line consisting of a mirror system differs from others in
that, to reduce losses and to compensate for diffraction widening of the wave
band, a planely-polarized wave is used directed at the mirrors at a small angle,
the electrical vector of which is parallel to the surface of the mirrors. The
latter are either of an almost plane or an almost cylindrical form, and have
periodic surface discontinuities, e.g., corrugations.
Card 1/1

S/020/62/144/002/012/028
00 B104/B102
AUTHOR: Katsenelen~baum, B. Z.
TTTL-7: Diffraction at a large aperture in a wide waveguide
u(x,z)
whichsfor x = d (Fig. 1) and the lines in semi-planes x = 0, z < 0 and
x = 0, z' L, sat-isfies the boundary condition u = 0 or du/dn = o. one of
the poss.-Lble waves,iixing* a wavelength which is small compared with d,
impinges from the left-hand side (27-,/Ic~ d, kdzl) 1, kL ~I). By the method
presented here the field on the slit (x - 0, 0 L) is sought first 'and
the solution obtained is urged to deter-mine the -field at the ri,~it_hand side of
the slit. The field on the slit is calculated from formulas based on the
huyjezs principle and the zolutions for the riGht-hand side of the slit
are obtained by applying the perturbation theory to waveguides. The wave
aziplitudes in the right-hand part of the waveguide depend on the effect
of all parts of the slit; hence the effects from thb slit corners can be
bypassed. The largest portion of the energy of the incident wave passes
over to the right-hand part of the waveguide. With u =, 0, the relative
Card 113
PERLIODICAL: Akademiya nauk SSSR. DoIclady, v. 144, no. 2, 196e"', 322-324
of the wave equation F 2u + k2u = 0 is sought,
TEXT: A solution

S/020/6',?/144/002/012/028.
n at a large aperture in a B104/BlO~
Diffractio
3 d2)1/2.
energy decrease is 21L /3, where Ii, nL/k Eal fof this energy
passes out i-hrough the slit while the other half is transformed into
dary-condition
par-sitic waves. The energy loss is g-reate= under-the boun
0',u/(/'n = 0. Expressions for the parasitic wave amplitudes are presented
for both boundary conditions: The results here given are applicable.to
symmetric and magnetic waves in plane and circular waveguides'. Moreover,
they can be extended to asymptotic diffraction problems (optics) apart
from wave guides. There 4S 1 figure.
ASSOCIATION: institut radiotekhniki i.elektroniki Akademii nauk-SSSR
(Institute of Radio Engineering and Electronics of the
Academy of Sciences USSR)
D December 27, 1961, by B. A. Yvedenskiy, Academician
5U3',1I-'-,~T ED December 20, 1961
Card 2/3

'7. 10;7o-6; -01
AC=XCW NR: AP3001010 s/0109/6:)/oo8/oo6/lo87/1088
5`11
AUTHOR: Xatsenelenbaimj Bo Z,
rk,
TME: semirlwr auasi- ItD [held at the Institut radlotekhniki i
elektronilki AN SSM t of Radio.~~-eeriag and r-Lectron.Lcs iul swPO
S(YJRCE: RwUcteWmika i elellftronilm, v. 8, no. 6, 1963, JC87-icM
TOPIC TAGS: quasi-optics, wsweeguides
ABSTRACT: Qiutsi-cptics deal:-3 mainly with centL-neter- ana YaMimeter-wa"
charmeling by optical meaw. L. A. Vayn:-7hteyn of the Institut fizicheskikh
problem 40 SSSUR (Institute o:,! Physical Problems AN BEER) submitted a method
for determining the r-a-tural :1're-quency characteristics of a lasex-type
resonator by :3imple calculatlcins made on -a usveguide model. A new mz!thod
for computing plane and ax-JaLly symet-ric horns and i4vuriction tW>es beetween
waveguides off various cross ~3ectlons wa-- aescrilbed by its crig'na-,cr,
B. Ye. Kinber of VI?IIFMI. Nher reportz dealt with the prinei-ples
the Go~~-~beam vaveguide and other channeling systems, a new type of int-7-
feromter, ard an integrator for solving various Oiffraction oroblems bV the use
-'P?-OX'M
tion

L 18~96-Q BDS/EEC-2- AFFTC/ASD/ESD-3/APGC Pi-4/Pi-4
1ACCESSIONNR: AP3003711 S/0109/63/008100711111/1119
AUTHOR: Katsenelenbaum
TITLE:, Diffraction by a flat mirror at a wide-waveguide bend
SOURCE: Radiotakhaika i elektronilra, v. 8, no. 7, 1963, 1111-1119
TOPIC TAGS: waveguide, diffraction
ABSTRACT: As wave propagation in wide waveguides obeys the laws intermediate
between the wave guide -proper laws and the optical laws, electrodynamical calcu-
lation of diffraction by a mirror can be reduced to an asymptotic diffraction
problem. A mat -iematical method used in tht: article combines the theory of
diffraction in ope a systems with the theory of waveguides. The transformation
loss or energy oj undesirable modes is calculated .or a flat wiveguide (two p3lari-
i zation.5 of the incident wave) and for a Hoj mode ir a circular waveguide. In the
latter case, the loss is 6;55 where iv is the wavelength, a is the
Card 1/2

L 18396-63
ACCESSION NR: AP3003711
waveguide radius is the angle between the waveguide sections. Inthe
above method, first the field in the waveguide slots (equivalent to the bead with a
mirror) is determined by essentially optical techniques. Then, conventional
waveguide methods are applied to find the amplitudes of the dominant and undesir-
Orig. art. has: 5 figures and 18 formulas.
able modes outgoing from the bend.
ASSOCIATION: Institut radiotekhniki. i elektroniki AN SSSR (Institute of Radio
Engineering and Electronics, AN SSaa)
SUBMrrTED: 283un62 DATE ACQ: OZAug63 ENC L: 0 0
.SUB CODE: CO NO REF SOV: 002 OTHER: 003
Card 2/2

L 1qj9?-6-5 BDS/EEC-Z-,...,AFF=/E$,D-3/RADC/~PGC
ACCF4ION NR: AP3006453 310109163100810091151611522
AUTHOi: Katsenelenbaum,'B. Z.
/17)
-~~gr reflections from several focusing
TITLV: Transmission of millimeter waves
mirr6rs
SO'URCE:'Radiotekhnika i elektronika, v. 8, Ono, 9, 1963, 1516-1522
TOPIC TAGS: transmission, millimeter wave focusing mirror, reflection, millimetezv~'
wave 'transmission
ABSTRACT: An approximate theory is offered for a transmission Une that consists
of a series of f1confocal" mirrors; the mirrors are so arranged as if they were
represented by spots on the internal surfaces of barrel-sha?ad solids of revolutio
a series of such solids forming the transmission line. The series of mirrors can
be considered as a phase-corrooting system which provides a periodical correction
for phasei'distribution in the wave thus prpyenting divergence of the beam.in its
.propagati O'n along thq lifie. A millimeter-w-ave beam witli an azimuthal component
of electric field is propagated by.consecutive reflectioxi from one mirror to
another. Near-graz~,ng slip angles are used, and an'.attenuation of about a few
Card 1/2

L 19697-63
ACCESSION RR-. APW6453
db/km is 'expected. IThe transmission-line pek:I~Drmanoe is similar,," physically and
;mathematically -- tp ~,that of Fabry-Perot op9q,resonators-.. Advptages and
disadvantages of thepiew transmission line compared to the conventional circular'
waveguide will becqjm~ clear "af tei6 a clarif~qation of the problem of necessary
:precision of manuf4p~ure and adjustment of ~49 mirror system.01 ,grig.. art. has.-
i 4 figures and 20 Virmulas'
;ASSOCIATION: none-
SUBMITTED: O6Aug62 Dki ACQ: 3OSep63 ENCL: 60
SUB CODE: C0 NO REF,~OV: 002 OTHM: 004
4
n
Card 2/2

KATSENELENBAUM, B.Z.; SIVOV, A.N.
Lamb's error in a problem on diffraction on a lattice from thin
round rods. Niftotekh. I elektron. 9 no.2060-361 F 164.
(MIRA 17:3)

- - - - . - -- .1 - - ~~ " --- ~ - -- I , ~
11 - C 1, . - . I
". -," , - -
- ~-, , 1~ -, , -,v , i~ , ~ ~
: - .: ". t~~ ~ : ~ --5. . ~1, . I
,,j.: ~
: --- z 7:-1 . .- .
--, - - . I,-- - I"i.-.. - - 1

21 ~, I- Ll~ , ~ I I ~ -1 . i. t- ~ 1,

- - - ~ln . A k-

ACCEMON MR; AP40385SO S/0053/64/083/00110001/0105
AMOR: Katsenelenbatnj B. Z,
TITLE: Quasioprtical methods of formation and transmission of millimeter waves
SoURCE: Uspekhi fizicheskikh nauk, v. 83t no. 19 19649 81-105
TDPIC TAGS: waveguide bends waveguide mirrors waveguide slots millimeter wave,
resonators quasioptics, beam waveguide
ABSTRAM 7he application of optiml rethods to redio-wave propagation is dis-
cussed as applied to three new technical problems in the propagation of MiMiw-
ter and submillimeter wavelengths* where geometrical, optics.and wave theory over-
lap. These concern the use of optical devices (mirrors, prismsq lenses) in wave-.;
guides, the theory of open rescnatms such as are used in lasersq.and lens-type or',
mirTm-type Lines for low-loss transmission of narrow radio beams. The first of
these problems necessitates the unification of the mathematical methods used in !:I
optics and in waveguide theory. The second and third problems are matlrjnatically'~
similar and their distinguishing feature. is that the ratio of the tmsvarse beaTk
dimension to the wavelwjtI4 which ia large In ordinary optics$ * not v
in quasloptics. The iopitical system considered are waveguide Ump which
quas
1/2

ACCESSION NR: AP4038550
the bean is bent by mirrors or by prism, large slots in waveguides, microwave
lens systems mirmr transmission lines, and open resonators. A section headed
'Confocal phase correctors' analyzes.all the ray-bending devicer, from a unified
q, point of view, since the net effect of all of thm is to deflect the ray (correct
A the phase of the wave), with special attentim paid to confocal. systems. 7he rela-
1 ticn between the acneentration produoed by the phase correctors and the losses in
I i the systern is discussed. Since quasioptics entails foruall:y an asymptotic appro- I
I
ach to diffraction problems9 and sinoe an asymptotic treatnent of wave t"
well Is equations) is very cmbersam 0 it is concluded that an asynptotic modi
1: tion of ray optics should serve as the starting point in the develowwt of a
11ished theory of,quasioptical devioes. orig. art& -Mil 12 fiVxw and 54 fe"MIlas.
ASSOCIA17ON: None
SUBMUrm'. 00 ATD PRESSt 3080, ENMI 00
SLO ODDE: OP EC NR REF SM 026 OIHERt 020
d . . . . ......
C
or

KATSENELLeNBAUM, B.Z.
Diffraction on flattened transparent bodies. Radiotekh. i elektron.
10 no,,3:550-552 Mr 165. (MIRA 18:3)

L 8242-66
AC%7~' NR: AP502243Z SOURCE. CODE: UR/0109/65/010/00911672/1675
AUTHOR: Vaganov, R. B.. DogadkM, A. B.; Kateenelenbaurn, B. Z.
CIL)
ORG. Institut radiotekhniki i clektroniki AN SSSR (Institute of Radio Engineering
and Electronics, AN SSSR)
TITLE., Periscopic mirror line
SOURCE: Radiotekhnika i elektroLka, v. 10, no. 9, 1965, 1672-1675
TOPIC TAGS: beam waveguide, periscopic waveguide
ABSTRACT: It-is-proven that the use of spherical- surface mirrors, desirable for
praCtical reasons in rrjrror beam waveguides, instead of the theoretically optimal
ellipsoid - ourface mirrors. does not seriously impair the waveguide parameters.
Two mirrors with a apacing small in comparison with their focal lengths are
regarded as a single phase corrector, and the radiation loss therein is evaluated
after A. Fox and T. Lt (IEEE, 1961, 51, 1, 80). Based on this evaluation and on
card 112 UDC: 621.372.218:535.312

,L 8242-66
ACC NR: APS022432
the G. Boyd and J. Gordon loss /beam-cross -section curves (BSTJ, 1?63, 40, 2,
489), a method for designing periscopic mirror lines I~s indicated. The radius of
mirror curvature and the diffraction loss can be calculated from the formulas
given. Orig. art. h": I f.',.,-,ure and 11 formulae.
SUB CODE: 09 / SU13M DATE: 06Jun64 / ORIG REF: 004 OTH REF: 003
Card 212

3553
JRCE C6DE: UR/0109/66/011/001/0042/0050
AUTHOR: Gorshkova, N. K. Dyachenko, A. A.; Zyatitakiy, V. A.;
Katsenelenbaum, B. Z.; Kolesnikova, N. A._
ORG: none
TITLE: Principles of a statistical analysis of the propagation of a light beam in
slightly deformed round mirror pipe ;z
SOURCE: Radiotekhnika i clektronika, v. 11, no. 1, 1966, 42-50
TOPIC TAGS: Bight pipe, light propagation
ABSTRACT: Plots of per-unit-length loss vs. sliding angle for 5-80-cm diameter
ideal aluminum pipes and light wavelengths of 0. 6 and 3 p are constructed on the
basis of theoretical formulas develop.-d by G. Eaglesfield (Proc. IR.E, p. B., 1962,
109, 43, 26). In considering rough-surface real pipes, the interaction of beam-
parameter variations and the beam diffraction divergence caused by the finite
wavelength-to-bearn- section ratio are neglected. The real-pipe deformations are
responsible fOr the increase in the average beam-sliding angle, for its divergence,
Card 1
17A f) 1

'-ACC _NR.'AP6003553_
and for its deviation from the meridional plane ("helixing"). The latter phenomenon
results in nonlinear increase of losses with the light-pipe length, in azimuth
divergence oi the beam, and (in the case of thin beams) in azimuth uncerta.Iinty of
bearn position. A statistical connection is established between (a) average squares
of waU-deformation angles and (b) average values of the sliding angle, helixincy,
additional loss, and beam divergence. Orig. art. has: 6 figures, 16 formulas, and
I table. [03)
SUB CODE: 20 SUBM DATE: i8sep64 ORIG REF: 001 OTH REF: 002/
ATD PRESS: ItIl

DIJBROVSKAYA~ ?.I.; DYUZHEVA, Yu.V*!,-XATSEnFMBAUM, M.S.~ YUSHKO,Ya.K.,-,
KOROLBVAp V,A.; BULICHEV, G.V.
Disoharge into the atmosphere or waotes from the pruduc4llon of
synthetic fatty acids and theiz, effe,," cm publi-~ health. Tjl-~.
zap. Mosk. nau-1h.-isal. inst. ~~wn. ~', gig. 261
(MIlu a6ai)

KA-TSMMFMAUM, M. S. (Moskva)
Study of morbidity among workers on the basis of incapacity
for work andthe number of sick persons. Sov.sdray. 14 n0-5:
22-26 s-0 '55. OILRA 8:12)
1. Is naucbno-issladovatells.kogo sanitarnogo, instituta imeni
Brismana.
(INDUSTRIAL HrGIM
In Russia, morbidity among workers)
(VITAL STATISTICS,
morbidity of workers in lbasia)

,,-1,7-,S "41) /V !~ ,
I .
SOSNOVIX, I.Ya.- KATSBNELENBAUM, M.S.; LUKIYANOV, V.S.; PIAKKII-111, A.S.;
TOLKA C I -
Methods for organizing and carrying out complete dispensary services
for workers. Zdrav.Ros.Feder. 1 no.11:31-35 N 157. (MIRA 10:12)
(MEDICINE, INDUSTRIAL)

BAYKOVI B.N.; MLKHDIAO V.P.; Prinimali uchastiye; VASILIMV, A.S.;
,,_41SENUENUtR4, M.S.; KOMAROVA, A.A.; ZHIGULINAp L.A.; TERNMUM,
K.I.; GUSELINIKOVA, E.L.; KETOVA, O.N.
Hygienic characteristics of air po3lution ij~ Gubakha and its effect
on health of the popitlation. Uch. zap. Mosk. nauch.-issl. inst. pan.
i gig. no.6:21-25 160. (IUPA 14: 11)
(NIZHMYA GUBAKHA-AIR-PoLLuTION)

DUBROVSKAYA, F.I.; KATSENELENBAUM, M.S.; YUSHKO, Ya.K.; BULYCHEV, G.V.;
KOROLEVAt
Air pollution with wastes from syiithetic fatty acids and alcohols
and their effect on publio health. Gig.i san. 26 no.12:3-8 D 161.
(MIRA 15:9)
1. Iz Moskovskogo nauchno-isaledovatellskogo instituta gigiyeny
imeni F.F.Erismarna.
(SHEBEKINO--AIR POLLUTION)

KATSBNKENt3AUM, N.A.
Superstructures in intermetallic
atoms. Vestnik Moskov. Univi 7,
Ho.5, 181-6 152. 1
INCA 47 no.22:11865 153)
compounds with densest packings of the
No.8, Ser. Fiz.-Mat. i Estestvan. Nauk
(MLRA 5:12)

KATSEMELENEIM, N. D.
USSR/Physics - Crystallography Apr 53
IlReview of 'New Investigations in Crystallography and Crystallocherds try,"' (V. A. Frank-
.Kamenetskiy., reviewer)
Usp Fiz Nauk, Vol 149, No 4, pp 628-630
Reviewed buok presents abridged translations of foreign articles processed by G. D. Vigdoro-
vich, A. S. Anishkina, B. V. Nenart,, T. L. Khotsyanova, V. M. Koshin, N. D. Katsenelenbaum,,
Yu. G. Zagalskiy,, and N. A. Pobedimskaya, with preface by Prof. G. B. Bokiya the editor.
267T92

USSR/Geophysics Crystallography Aug 52
"Super Structures in intermetallic Compounds With
Densest Packing of Atom-),"'N. L, Katsenelenbaum,
.CYAir of Crystallography and Crystallochemistry
Vest Mos Univ, Ser Fizikowat i.Yest Nauk, No 5,
pp
Discusses structural types of binary alloys with
densest packings of atoms and super structures.
Establishes the following superstructure: MgjCd
(hexagonal packing of atoms), Cu',Ai.-. AlTi, AIZr,
275T68
Pt3cu, CuAu, CuPt, Curt7 (cub ic packing of atoms)
and Ni~ri (four layer packing of atoms).

1. UTSENELENBAUM, N. L.
2. USSR (600)
4. Stereochemistry
7. Super structures in intermetallic compounds with dense pac)dng of atoms.
Vast. Mosk. un. 7 No. 8. 1952
9. Monthly Lists of Russian Accessions, Library of Congress, March 1953, Unclassified.

XATSENELENMUM, Z., prof.
~tu'~rfiover of checks and clearing payments in the U.S. Don. i kred. 16
no.4:-17-87 Ap 158. (MIRA 11:5)
(United States--Banks and banking)