SCIENTIFIC ABSTRACT NIKOLSKIY, V. V. - NIKOLYUK, V. F.
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CIA-RDP86-00513R001137220005-0
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RIF
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S
Document Page Count:
100
Document Creation Date:
January 3, 2017
Document Release Date:
August 1, 2000
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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Body:
Liv-c-av i.lf Forromagnel,ic kr~pllfit,r.3
oil the D.1sturbance Principle
SUBMITTED:
alao has a wave cha'ra'ctor. Vw
Parts 11 and 5 are :Amil"11, to thf~
Parts 2 and 3, rr~npective-ly. In th-!
said that the resuRn obtalned are valld Jn&-p~?ndvn~ I
of the type of natm,al o,~,Iclllatlow; '111
initial quality Qc,, the a ttenu,,i t Ions
and fill-in flictors ~ can be calculate-ld or m-aslirf-A.
There are 7 references, It ."Joviet, 3 11-:73. T1 U. S.
referenceo are: It. Suhl, Fyvz- Rev., 1957., 394;
H. Suhl, J. Appl. Phys. 1951 1225; P. K. TIQ11,
If. Suhl, Proc. I.R.E. 1958, 462,8-'foo.
February 23, 1959
Card6/6
5JUN/006/0L4
s/iog/Woo I
F140/E433
AUT11014 t NIkol'skiv- V_V_
T ITLE: The Investigation of' Holtow Systems With Animotropic
Regions by the ~.,ethod of Vtrenftin tions
Pt.l. Ifesonatoro
PEUIODICAL: Radioteklinika i eicktronika, 1960, V01.5' N".1t,
pp.1802-1810
TRXT: This paper wan propented at the Session of the Section for
Ferrites of the Society of Vadi(pengincering and Telecommunications
imoni A.S.Popov, January 13. 1960. and also at the Jubilee Session
of the Society(May it), L960).
Three groups of problems have been posed in applied electra-
dynamics; study of the general properties or holtow systems
containing gyrotropic bodies, to determine their possible
applications in radioengincering, and methods or realizing the
corresponding devLceiv. the detailed analysis of' specific devfcos
for the purpose of engineering design and problens in connection
with ferrite-parameter measurement. Problems or the first two
groups have not as yot been solved to a satisfactory completeness.
Card t/3
88158
S/109/60/005/OLI/006/ot4
E140/F485
The Itivestigation of Hollow Systems With Anisotropic Ilegionx by the
Mothod of Eigonfunctions. 11t. I .Resonators
Aftor Walker's (Ref.14) contribution. the lack of information on
the elgenvalue spectra of gyrotrople systems has been particularly
strangLy felt. An for the calculation of mpeciCLC devices,
their irregularity constitutes an obstacle In view of the non-
quasi-stationarity of ferrite elements. For generality. this
article applies to antsotropic regions the ordinary method of
eigenfunctions, in resonators, waveguide and a particular type of
wavegulde transformer. The problem is reduced to an infinite
5ystem or equations frnm which numerical methods are derived for
une with electronic computers. The methods developed permit, in
principle, consideration of all geometricaL features or real
microwave devices. The derivation leads to matrix equations with
the unknown frequencies in-the principle diagonal if the dimpersiun
of the antsotropic medium to neglected. In the presence of
dispersion. the unknnwn" alsn enter into the remaining elements of
the determinant. The example or a generalized cylindrical
resonator completely filled by ferrite in presented to illustrate
Card 2/3
88158
S/109/60/005/0LI/006/014
E140/R483
The Invtstigation of' Hollow Systems With Anixotroptc PegLans by the
Mothad of Cigenrunctions. Pt.l. Resonators
certain poLnts of the article. Thor* or@ I figuro and
15 reraroncess 9 Sovt*t and 6 English.
SUBMITTEDs rebruary 15. 1960
Card 1/3
2 o4. 16
s/ i (,r)/w,/oo5/ol2/Ol&/O35
47, /.400 ca/so IJ04) Eiga/E382
AUTHORt Niko I IskLY, V. V.
TITUS Investigation of tlia Cavi!y Systems wLth
Anisotropic Regions by the Method of Eigen
Funct tons. 11. Waveguide Transformer
PERIODICAL: Rtadiotekhtstka i elektronika, 1960, Vol. 51
No. 12, pp. 1960 - 196 7
TEXTv The first part of this work (Ref. 0 was concerned
with the problem of a resonator with an anisotropic regLan
so that it is now possible to consider a waveguide trans-
former based on such a resonator (or equivalent to it). rhe
transformer ts shown dtmgrairunattcally in Fig. 1. This is
a cavity containing one or sevoral anis,.%1tropLc regions
V and having N external 1~ort--% through which waveguides
are connected to the system. ir otay a basic rieLd exists
In each waveguide, the system can be regarded as a 2N-pole
relative to far objects. The problem of the transformer
differs from that considered tti the first part of this work
by virtue of the nonhotnoKetteity of the boundary conditions.
Card 1/8
2OU16
s/loq/6o/oo5/ol2/0I4/035
E192/E382
Invostigation of the Cavity Systems with AntsotrG-4c Regions
by the Method of Eigen Functions. 11. W&veKuide Transformer
Here, It is necessary to know the tangential components of
the vector or ie at the terminal cross-sections
(S10 S in Fig. 1). If F-1, and H are not
LP SN 171
given on all thecross-sections. on the remaining ones it La
necessary to know the relationship between E _1:~ a nd H Ir I
i.e. the external loads of the corresponding waveguides.
In this case, the solution of the problem leads to the
determination of the field of the transformer L Pand RP
and the matrices of Its input admittance* which relate the
fields at all the terminal croqn-sections. First, an
auxiliary problem relating to a resonator with a nonuniform
anisotropic medium, which Is excited through one or several
apertures in its envelope 50 is considered. It is shown
Card 2/8
j t.-~/oo/oo5/olz/G14/m
Investigation of the Cavity Systems with Anixotropic Regions
by the Eethod of Ligen Functions. 11. Waveguide Tran*Corm*r
that the 6ystem is described by (see Part 1. of the articlo)t
A j 1POL"llk.1 + Wal) Q gRk,. I -
The expressions defined by:
A j Qij F. B j TJk F
are also introduced, where A and 0 re composed oC the
coefficients,of expansion of ? and -14 and the matrices
(likll and lTikjj are expressed on the basis oC Eqs.
Card
s/log/60/005/012/014/055
E192/E382
Investigation or the Cavity Systems with Anixotropic Regions
by the Method of Eigen Functions. II. Waveguid* TrKnsCormor
The problem of a waveguide transformer with t~o perts was
solved by G.V. Kisunlko (Ref. 2). by using the above results
It is now possib.le to Investigate such a transformer when It
contains a nonhomogeheous aninotropic medium. The transverse
eigen functions or the waveguldes are chosen so that tho
coaditionst
t - h on S
h on 5
t
[n
2
1
i
1(2
o
(2)
are fulfiLled,where a, are eLectrical tranavorso Cunctions
are magnotLc
of the rirst and second waveguides and h
,
transverse functions. It in shown that t a solution is
it% the C*rm:
Card
2W416
Investigation (of the Cavity ~,)Y,,,tvms with Antsotroptc RogLons
by the Method of Ligen Function-'. 11. Wavegutdc TransCorner
11 Y !, A
IL - Y 1. ( I I I kAl i ( 12k 2
B2 = Yt~21)kl, AI Y If, 2~.,kA,
where j
i. Y 14 T 1.2) (16)
tl i(tiolk k(-0JI
are the admittance watricen of' thq- transformer and 0 1.2
are the vectors with components If 11 b2-, ... (which are
eLements of the proliminary matricem). Eqs. (15) can be
extended to a mystem with N exteutuil p rts (Fig. 1). On*
Card 5/8
20&16
5/109/60/005/012/014/035
E192/E382
Investigation ot' the Cavity Sy.,~tem,,% with Aninotropic Regions
by the Method of Eigen tutictions, 11. Waveguide Transformer
of the simplest traneformerA k3 the system based on a
regular waveguitW the waveguide in tasually such that It
can contain only the fiandismental fin)(1. In the case of an
arbitrary waveguide, tranat'vraier as Shown In Fig. 1, the
ficild can be approximated bv tlip eigen funstions of the
corresponding E-problem, for wliicls E - 0 on S 0 .
However, for r, %imple rrgijlor-wavejtuiolo~ traneCormer It to
possible to choose much a syslt,m of eigen functtons that
they havo n tangentiaL cnwjwonent of the vector C' at the
terminal cross-sect&tons. There exist other methods of
invostigating the vavegutde traw,4former by employing eigen
functions. Otte of thesc wettwam., which to based on 4
different solution of the a~sxilirtry probleta of the resonator
excitation, iv dtacusse(J. it &:s ziww Assumed that the field
g"', -W of' the resoviestor wAth rjowinsform anioctropic medium
con be expressed In torms of tho elg-ii functions byt
Card 6/8
Investigation of the Cavity Systerr- eith Aninotropic flexions
by the Yethod of Ligen Function.%. it. Wavcguide TransCormar
rot fi:
rot fw~ &(r-)
E, - 0 sa S.
It in shown that the solution obtetined by this method is
identical with t1tat expressed by Lqs. (6). Thtw above methods
of calculation are suitable for the investigation of yarious
Waveguide problems such an circulators. phase-shifters.
directional attenuators and other devices which contain mag-
netised forrites of comparatively large dimensions.
Card 7/8
t
s/iog/60/005/012/014,(035
E192/C582
Investigati on or the Cavity Systems with Aninotropic Region*
by the Yethod of Eigen Functions. II. Waxeguide Transformer
Nil- There are figures and 3 Soviet references.
jj
SUBMITTED: March 14,
ig6o
Card 9/6
204 29
s/io9/6o/oo5/012/0271035
(/1 yo, E192/E582
AUTRORt Nikollskiy, Vo Y.
ii_ethod_~_f Eigenfunctions for-the &xtern&L
TITLEt On the
Problem, of t1octrodynamice
PERIODICALt Udiotakhnika i alektronika, 1960, Vo:1.5). No.12,
pp.2055-2054
TEXTt The,mothad of eigenfunctions is widely, used in the
solution or the internal problems of electrodynamics and it is
thought that it could be applied successfully to the external,
dicrraction problems. In order to apply the method to, & diffraction
problem (see Fig.1, where A, is a body and F is a source),, the
external space S to limited artiCicially by a sheath whose Corn.
'
O
(Car instance a cube?. The field produced by
can be very simpL
O
the source is expressed in. terms of the eigenfunctiona'ar tho
region V thus produced. As the region is expanded, tho affect
or its bogndary on the process is reduced until an inatint L4
reached when the solution does not differ significantly fron'the
true solution (in the absence or the boundary). The very princip
or the artificial limit of the region is known in quantum stechanL
The question or a suitable chaLc* or the boundary is quit* important
Card 1/2
S/109/60/005/012/027/035
E192/Z,982
On the Method 'of Rigenfunctions for the External Problem of
Electrodynamics
since, an exaggerated extension of the region V, , is undesirable
.from tho point of view of the c&lculation ties* Thor
diffigul % are
I rijure and I Soviet re,for*ncew.
SUBMZTTZVt April 'it,I
-960,
r- - - - - - - - - - -
t
...Car-d _2/2-..-
KIKOLISM', FEDOROV, F.P., dota., rotoolazent)
BUM;SKIr, V.B.t kaM. fizih-matem. nauki red.; FERKCVSUYk,
G.Te,, red, izd-va,# GARINA., T.D.j, ukha, red,
(Zlectromagnatic field tbeorr) Teorift eleictrawpitnoCo polia.
Koskvag, Goa. izd-vo *V~rsshaia shkolap-10 1961. 370 p.
(KIRA, I~cZ)
1. Kafodr& tooraticheakikh opow redlotakWki Koskovskola
anergeticbetskojo inatituta im. Kal*tova (for Worov).
(zlectromgmtic tboary)
S/Laq/61/oo,6/ool/009/023
CJL40/ZL63
el-3304`419W 11310)
AUTHORt K ~* I
TITLAt Investigation at hollow systems wLtk aninatropLe
regions by the method of eigonfunctionso Part 111,
WavegoLdso
PERIODICAL: RadLotekhalks, L slektronika. val.6, I(o.1, 1961,
pp. 74-80
TILM This to a continuation of the authorls previous work
(an resonators. ReC.L. and an wavegulde, transformers. RoC.3).
The formnlaa are derived with a view to calculation an digital
computers. The waveguLds considered consists of an ideally
conducting tube of crass-eection So with arbitrary contour floe
containing an anisatropic cylinder of croas-4oction S. Tile
propagation constants of the possible wave modes of the system or*
Cound, The results arrived at or* simpUr than Car the case of
th* waveguido transformer (Rtf,3) for a number of practical cases,
Car example, the propagation constants oC wav*guLdes completely
filled by anisatropic (oog., gyromagnetLc) media. Two notes are
attached to the article discussing points raised by the
card 1/2
2U31
S/109/61/006/001/009/023
Ic 140/1c IL63
investigation of hollow systems with onlaotropic region* by the
method of eigenfunationse Part 111, Waveguides
preceding two parts.
Thor* are I figure and 3 Soviet references.
SUBMITT&Ds may 13 196o
Card 2/2
, i I
NMLIIM IT.-,
~*-T
Variatien principle for hollow-opaeo gptw&, vith aninotropic
madiun. Raclictekh. i alaktron. 6,no.9tl583-1595 9 161.
(MIRk 14t9)
(Wave guidoo)
t1loatric romotators)
(Ificrawaves)
. NUOLSKIYo V-V-l SUKRY(l Y.G.
jtj~, mr~h,~d for hollov cy tent with Anl5o*Mjc "djupl,, Wi,3tekl-..
R a - (KIU 14-.9)
i elaktron. 6 no.10,.16 16&4 0 161.
(Wave. iruide7s- (Liectric resonators)
6
S/1 09/62/007/OU4/C,~)`O/G It,
-3 L D230/D302
L 10
AUTHOR: 'ikollskiz, V.V.
N
1.~TLE: Double-aided evaluation of the resonant .,rreq!1O!!c4;eL
of hollow electromagnetic cavities with an
non-homogeneoue medium
PERIODICAM Radiotekhnika i elektronikap v* 7. no. 4, 1962,
601 - 616
T:XT: The double-sided method of evaluation Civec a relatively
simple Yjay of designing irregular resonators. The-accuracy -.f t*,.
Tesults in simpler form is satisfactory for most aptiIications; in
principle, it can be extended indefinitely. In the case of c'cc-
tric-mode ercitation (dielectric body In the waveguide') it ib
tively easy to prepare a table of the resonant frequencies in ter.-,7,
of the parameters q# r. and 02/p1, where q - a form facto.-O F - di-
electric permeability of the mediumt P, and P2 -spectra of the cor-
responding reciprocal operators (the square of tho ratio of t'Ee
first two resonant frequencies of an unfilled cavity). These valuen
Card 1/3
/62/007/004/003/013
S/109
Double-aided evaluation or the B230/D302
fully define both limits of the dominant frequency lndepen~cnt of
the type of irreGularity. In order to use the tabulated results In
the design of a reaonatoAr of any type the value of its form factor
is required beforehand. A test function f I is introduced au a spe-
cial caae of the normalized intrinsic field; bece.-use of "r. simpli-
city it is convenient to use; it, has, howevere no absolizle aftinta-
E:eu. It is possible, in principlerto evaluate not orly t4c
r,* " also other resonant frequencies. Analorous Probie:.~s ofv L~ i i
d,~ resonators are examined. In all complex cases considerel f,c,~r-
ttlin cases of non-reciprocity) the cutl-off waveruide frequcrc_-_-:,
-are determined. Using this nothodr it In also poc_-ible 'LD
the accuracy of a Creat variety of approximations in ry
A. & w
excitation. In all cases conaidered the niximun obtaiialbl e o r
~.Iho ayeMge resuit .%Tau found; as an example, tabulcted --a
coz,g~daon between the calculated and eX arAMertQ1 racul t'l
oaua or r**tanguiar roaOn&tOr rully M?21 with. In
appendix the following special canea of cavity re~-_natr,:,
nod: 1) Rectangular resonator with a cen'.rally-p2acad
cylinder; 2) Cylin4rical resonator with a cylindrical
Card 2/3
6/109/62/007/005/019/021
NikoVskly, T.T.
AUTRORx
"TITLIs 7-on--the--problen of :two side estimation of natural
4requenclas of hollow elect tic reso
PER =2 Radlateklialka. I elektranikag To 7# ILO* 50 19620
907..- 911
=Tc A further contribution to a pr*vloux paper (T.T. llkollakiyo,
.Rad&pt*khn1k& I elektronikap vs. 7P no. 4,, 19620 601) canc*ming the
2
upper lialt of the lowest natural frtquoncy v of a resonator with
an Inhomogensous antsotrop1b medium. A special a"* of a cavity fil-
lad with-foalte dielectriple consUarede The upper limit of w2 In
I
de''tormined using the elgenfunctions of an empty resonator. The case
of a oubio resonator containing a dielectric parallelepiped with
e/ro at 10 Is exam1neds The resul too can also be applied to a oylla-
drical cavity with a dielectric diae at the bottom for the ass* of
Card 1/4
3/109,/62/007/005/019/021
On the probles of two old* D230/D306
an Soo-fiold. Izaet results are'compartd graphically with those ob-
tafted from a functional Po ?or the 2,io-fleld the functional P gi-
ven excess values of cavity volume* The author also considers cylin-
drical cavity:contalaing a coaxial dielectric cylinder (EA. N 10)v
whose diameter Is equal tog or lose than# the cavity dlamot*rt res-
!,:poctively. In both cases the fundamental field in Effil, and the 3111-
field of an emptt cavity Is taken as the test functiono In both ca-
ses# when the dielectric filling exceeds 20 % of total cavity volu-
me# the funationil 7 given excess values with a relatively small .
error* The functional 7 can only be used for the caicuiation or W,
in a quasi-static.regi-ne for which the quasi-static approximate theo-
ry of e3 illation appli.-so If the,fundazental. field Is substituted
into the functional 1, the resulting w2_valuoo are less than the
I
exact values If the dielectric filling Is 5 to 20 % of total volumes
This law should be valid for different forms of cavity and dieloc-
trio filling* There are 3 figures and I table.
SUIC11ITT:M: or 29, 1991-
Card 2/2 Pot~
liggiAULA&
CamernInC the OTarlatlotma squivalence* of gyrotrople wave
guides and cavitLes. lUdiotakh. L elektron 7 no.7tl249-1250
9620 OURA l5s6)
(Wave g,.ddes) (ClactrIc tvaonators)
NIKOVSKU, Y.Y., lnz!;.
Ralsinor the height of a bmah with tims-bap of a r1we-o
mm"A. strait 7 noollt 36-Z? 1063 (iaRA 1.1c')
1. Dkitrcinkly s&%-" mastovykh zholezobetcrailth kcnutrukts!jo
ACCESSION NR.- AP4038613 S/0109164/0091004/06ZS/0633
AUTHOR: Nikollskii, V. V.
TITLE: Fourier niethod for hollow shap4d systoom with an anisocropin
4aterogeneous medium
:SOURCE: Radiotekhaika L slaktronika. v. 9, no. 4, 1964, 6ZS -633
TOPIC TAGS: SHF resonator, waveguide, waveguide transformer. microwaves.
resonator theory
ABSTRACT: The Fourier mn4thad of determining natural fraquencies. propagation
constants, and admittance matrices was developed earlier by the author for
resonators. waveguldes. and wavegulds, transformers. Its Limitation has boon the
fact that a total set of vector functions obtained from the problem of a nonfiLled
resonator had to be known. The present article to free from this litrdtation: no
got of analytically specified vector functions for the region in question is needed.
Card
:ACCESMON NR: AP4039613
'An expansion into vector oigen-functions of the electromagnetic field of a shaped-
envelope hollow system is wade. The get of eigen-functione to found from a
~problem dealing with a region that encompasses the hollow tystern. The applica-
bility of the Rita and Galarkin unthods to demonstrated In a resonator example.
"The author is thankful to V. G. Feaktistow for useful discussions of the above
problems. 11 Orig. art. h": 40 fornvAas.
ASSOCIATION: none
;SUBMITTED: 13Fsb63 I
:SUB COIDE: WoM
DATE ACQ: 05Jun64
NO REF SOV: 007
ENCL: 00
OTHER: 000
Card Z/Z
St0l09164t0091Q06/tJ4S,/t356'
ACCESSION NR: AP4043666
AUTHOR: Nikol'skiv, V. V.; Sukhav. V. G.; Karniy*nko, 0. to I Ortov$ y4 P,
TITLE: Calculation of a rec
"Ular waveguide containing a lon.g(tud(na
magnetized ferrite by the eig4efunct(on method
I SOURCE: Radlotekhnika i elektronfkA. v. 9,. no. 6. 1964, 134S-1356
TOPIC TAGS: wavegulde, ferrite, longitudinally magnatised ferrite, ferrito
containing wavegulde
ADSTRACTs Sao'ad an the Galorkin-Rits theory, a method for calculating the
propagation constants of and fields in a rectangular waveguide partially filled W1
a longitudinally-magnatized ferrite is developed* The problem to valved as
boundary problem for the wavtguide cross-aection; Ma"ell's equations are
used. Phase shift and attenuation are calculated for a wide range of, ferrite
characteristlego'faixte and c6nfigurations of the systotn* Programing tinn and,
Card I /Z
'ACCESSION "it, AP404968
techniques ate discuosed-is.'"tt as the accuracy of calculation'. rundanwataU.
characteristics of- the system are t1aillied by isolating various awdes and by
anaLysing their spectral composition," A few nuawric*1 W'MMVLOIF are calculat"
and data presented in graphical, form, Orig. art. hsav 15 figures forawlssp
and t table.
A=MATIONt none
SUBbQTTICDt ZZA"T6S, E N C UP 00
SUB Colm: ic NO REr SOVi 005 OTHERt 005
Card /Z
HIKOLISKAP V.V.; SU;~ICV, V.G.; D.I.; V.~.
--- F-. nV WA WJ WI OW -.t' Wft%g~,
Calculation of a. recfAmgular wavegjide wIth a lorgitudinal'A7 zagnetized
forrite using an e1goinfunctIon mt~:;d. Wintekh. I elektrcn. 9 no.gs
1345-1356 Ag '64. (MIRA 17:10)
'KA)USLEY, dlk ,;~ j, i iw~.; ""I '' ' '
_: i A r ~ 1 - 1 ;, , i~ . ; 0 , I !,r I . - - 1. . . - p
;. 4,0
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Nirlba s sil. 02?7-,!~~') 164 C, ~ '. .;, I r:.:)
I
1. Rn 0 t I-) V~,'~ I y 4.1 t it ; " n ~, " I t..~A t.
0 0 0 0 0 0 0
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t7e, A J
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94,10,;Mjm age
ODMITU DI'T ul *T'403ft DT.%l
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1~"j vcc7:::r tq qsj=v* oev"19 &maTZ*ajM - opft
CC
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ad *21 .10M;DODT4 FM jo Orvjzq&W44
Mr. Vtm slaxuml -10 00-mog 76 p"'I acxas&~R6
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YA. D. Sulliu~ -in, c,,j
h c: r a,- r 11 t u ra Ia n Ini.. 1f, rid,
r: D,- It. r, i,7
ti
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USSR / Diseases of Farm Animals. Disaaaes Cituxed, R-2
by Helminths.
Ab5 Jour: Ref Zhur-Biol-, No 2, 1958, 7370
Author : H. V. Badanin,,-YA-k_-Nikol1ek1y
Inst i Not (liven
Title Pecularitles, of the Measures For Fighting H*lmintht,-..
aim of Farm Animals In Vzbekiston.
Orig Pub: Hauchn. tr. Uzb. a-kh. in-ta 1956, lo, 63-73.
Abstract: Measures In the tight against the basic helmirths
of sheep are examined.
Card 1/1
119OLISKIT To 0 bW~T*t*rLn&rFM* Sauk
=L==
methods or 41121041 lmwiml di"als of Nalodso Thymalosla
Sled Avlt*lUmfa. Infectlaw of Wwop ad Coate wider fleld coadl.
tloms. Trudy Vx.mmb,-Ivvl.ln~t,v*t* UtUL-W 161o
(=A 1612)
(lubeldetan-Gootada) (Skomp-j~araol""")
(Goats-ftraolted-4"ts)
I KIM -D k"WT*teriwwppWW nauk
SIWUfted =AW of mdaroseWle dl&Wsls 3f Nml*sla 10sation
In shmsp ad pats. Trvo W16SAW
0610 (KIPA 16 t2)
(Ilzbeldst4a-Zestoda) (ftrasit4"hoop) (ftrealtes-4mts)
"RwAwt F'S.I~K9010,89up ra'D,
Im"Lelm or dm" IW tm"t~ trf~sphldm In Um ban.
Trmft 24114-175 t6l* (P=- I~CO
(TabskisUa-Zoolmorm) Wrtalts"")
"Diagrosis of ir rheen."
Vetertnartya, Vol. 34, Uo.5, Vbi
L ; i ~rr of
,,!kr,j'jqkjy, Ta. D.- Institute cS
Uzbck Acarinoy of AIrrimiltur-al Saic-,!rr.
VIKOLISM, Y&*Dev k"o vetar, muk
Therapeutic affectivVneds of calcium arvenate in agearlasis
of hions and chicket. Sbore natichp rab, Sar. NIVS 6tI73-184
163- (KIRA 18i11)
aoRxsmcm, ru.r.; Yt*OIFAMOV, G.F.; MELINIXOTp P.; MMLYWO, T*.5.;
SMIENYAO R.; rROUNp L.; IDDYAW)VO V.; KUM, ISM, Ta.D.1
LUZIAMINO D.; AZMV, D.
Inrormation and brior news. Utorinariia 40 no.201-96 F 163.
(MIRA 17t2)
N tmat cd I ru s I n f P on ,a t. or in I a - bs .Vet-rin.,irl"a 41
61 Js 164. (VIPA 6)
1. 3aratovskaya niu7!,r.-- !n-sledovatt-lskaya veterinar-na-ya
stantalya (for Nikollakly'l. 2. Ralakovskaya, rayo"-iayw
veterinarnaya lab-natorlya (for Plskunav).
UwHlff, P.M.F Ex SKIT
i Th*k
GLIculation of antematia errors for leysts vith self-adjuirting
ill&t linfw. Gso4i kart, no.1&18-22 Ja 161. (Km 1692),
(ravel (bavvying instment))
IZ4-57-Z-Z459
Translation from: Referativnyy zhurnal, Mekhanika, 1957, Nr Z, p 133 (USSR)
AUTHOR- Nikol' skiy. Ye. N.
TITLE: Calculation of the Body Shell of an All-metal Passenger Car for
Torsion (Raschet kuzova tsellnometallicheskogo passathirskogo
vagona na krucheniye)
PERIODICAL: Tr. Bezhitsk. in-ta transp. mashinostr. , 1955, Nr 13, pp IZ5-
149
ABSTRACT: Description of an approximate calculation method. relative to
torsion, for the body shell of a passenger car which is considered
as a closed shell with cut-outs. The theory of thin-walled beams
with open profile is employed. The sckematic calculation model
consists of two thin-walled, trough-shaped beams, connected to
one another by means of elastic partitions stressed by shear.
The contour of the cross section of the stringers is considered
nondeformable. The rigidity of the stringers under pure tors.:~,%
is assumed to be negligibly small in comparison to the sectorial
rigidity of the stringers. The terminal-walls are assumed to
remain undeformed within their plane. The calculation is per-
Card 1/1 formed by means of a combined method. 0. V. Bychkov
1. Passenger vehlclea--Torque 2. Mathematics
AL
i
7
lid
NO;
,
, , ., -;
v4il T
WA41
flat
tb p MLWWJ b lbb
MA
Ttd r, CaUl.
, WIMLISKIT. U.N.. d*ts., kuCtskhn.mult
UslffC F.F.Falkwleble metbod ts amsljrxlmjC %bo strossed stato
to tho Umer seettas of the body of a closed-sholl type of
passefter car. Trudy DITM no.17:13-31 157. (MIRA 11110)
(ftl1roade-ftmeowr cars)
KIKDLISXIT reg. data., kkad.telrba.0fluic
0.0~~~~te of n -*hapsi abstio: applicable to the If,wer
seetion of the body of a Clogod-ghell type of pasim *r car,
Trudy SITX #57s WPA litio)
(Rallroods--Fassonor cars)
I GKITL P.
muffiaNSKIT, Sargay faitillyevich, doktor takha.nauk; 04-c-L(WIT, reyvair
xlkolay%vLch, prof.0 daktar Ukhs,ssako NIUVWXY, Low Rik-olIP---
jovick. prof.0 daktor tokhm.mmk; ;;;i. AUkmW Alebwadrawlsk.
prof,, daktor toakhmeamak; SUVIRO FamId Abramoviob, prof,* doktor
takhm.amki IARAKWK. U.S.. md.: SOMMA, Te.N.0 Ukha.rado
[Daslgm of rallroad care for strsv4thj lAschat vmouaw as pracb-
nost'. ftd red. A.A.Fopows. M~Wm. T"olsdatellsko-pollas
ob%dlnenle X-ve ptttel saabehahmalls. 1960. 359 P.
(Rallnedo-Cers-Coustruct Lou)
I 1#75D BOTW807T
Nikallskiy, re. K.
TITL&t The Schwarz Algorithm in the Problem of the Thvory of
Elasticity of Stresses
PERIODICLLs Doklady kkadecxii nauk SSSR, 1960. Vol, 135, No. 5,
pp. 549 - 552
TEXTt S. L. Sobolev (Ref. 1) proved the convergence or the Schwarz
algoritha using the displacement problem of the theory of elasticity. Kere
the application of the Schwarz algorithm is investigated for the stresses
in the: region DI which can be reprea4nted at the auz of the two partially
12
overlapping region# D, and DZ" The existence of the limit or a function
and its agreement with the solution& of' the theory of elasticity in the,
region D, is proved with the Schwarz algorithm. and the exclusion
12
principle. rn the stress problem the freedom of choice of the, original
vectorial 4trese function in the region D . located within DI is limited
Card 1/2
191OLISfAr ra_lr_g prof., doktor tekhn.nauki VERSHIIVSKIT,S.V., doktor
r.mm. mauk,, retsens*xt; GAUXOTA, ILS.0 Lash., red.
DMINA, CF.,, tokhn.red.; TUMMY, A.Ye., tedw.rod.
(Railroad-car-typo mh*11s W'I;Wopen1ngs; theorstioal bases
for stress Investigation] Obolochkl a vyresaul tips vagom-
alth kusovow; toorsticheakle oanovy lesledovaulta sapriashouil.
Moskva,, Ylashest 1963. 311 P WRA 16&9)
(Slastic plates and shelis) (RuIlroade-Cars)
.1yly dckU KOV,
TIE, t,
a.1
(IMIRA
Acc Nitt
Ghadurp Loonid Abramovich (Doctor of Technical Sciences; Professor); Chelnikarv Iva"
Ivanovich (Doctor of Technical Sciences; Professor); Mikollsklyp raw Nik*Uyevlch
(Doctor of Technical Geienceep Professor)# ff1kol'skiy,,YL1vgen1y Mikolayevich (Doctor
of Technical Sciences; Professor); Tech-
n1cal Sciences# Docent); Kazansk1yi, Gcorgiy, A.1ekseyevich (Candidate of TechnicaL
Sciences); DMatkav# Vladlisir Fedoravich (Candidate of Technical Sciences)
Railroad cars; constructlono theory# and design (Vagony; korAtruktstya teorlys, I
raschet) Kadcove rx&yo "Ttamyort"t 1965. 459 p. 111u4., biblife 60000 copies
printed. Textbook for rallroad transportation Institutes.
TOPIC TACO: railway equlpment,, railway rolling stock, milmy transportationp raU-
WW Vehicle dAtA
MR111WE AND COVERAGEt The book deals with the conatructionp strength calculationsp
dynomicap choice of technical-ecunoodc pmrameters, " sizes of rallimad cars. It
Is intended for courses on "Railroad Cars" (constructionp thearyp calculation) far
those specializing In "Railroad Car Construction and RailrorA4 Car YKnagementa of
h1gher tedmIcal In4itutes for railway trwwport. It to destgoed to be a baste
course for furtbar specialization Is special-purpose cars such " refrigerator carep
electric equipeent, of railroad care# techno1W of construction and repair of rall-
road carev mad other s"claLties. It to degigmA for gtudowto itw bove some almAnt-
ary lacrusition an car construction and car strangth,
Card 1/2 UDC: 425123/,24
MC404824
TABM OF COSTEN (abrifted] i
Introduction - - 3
Ch, I. General information on railroad cars 7
Ch. 11. Dimensions - - is
Ch. III. Technical mid economical paremeters of freight cars 30
Ch, IV* Principal diate for strength calculAtIons of railzomid care -
Ch. V. Wheel pairs - - 55
Ch. VI. We boxes - - 69
Ch. VIIO' Springs and &hock sbiorbers - - 105
Ch. VIII. Trucks 142
Ch. IX. Frams wd bodies - _ 187
Ch. X. Ghock-couplir4: devlc*d - - 2w
Ch. X1* Principles or' railroad Qnsalce - 252
Ch. Me Freight cars - - 337
Ch* Mlo Dulk Care - - VO
Ch* wo ftsimuger cue - - 3m
Ch., XV* PrImIpIss of 4se4p# caustruettoup and tectift of care h23
BUS COM - IV WM MUs 2UUYW ORM RM 218/ OU JUWc 010
- MIZOLISM, is. (Ifflamcmd)
A 163.
With Ntwo mblirim eirfloors. Toes. NO& 10 --It
116ii-1611P
(Ndmulm warfmv)
A
NUKOLISKIT, Yu. (Tula)
V*luAwr beglamlage In the club for wat4r @parts* Toom. smm.
39 no.3o27-28 NO 163. (MIRA 160)
(Aq=tle sports)
AY.I.IJUEV, V.L .
Cc., ff
SOURCZ, CODEC M, 1OW01661OW10WI027310302,
0"07.4.103s AkulaySv.. oklyp No A
(Leningrad); Rkolf
J.t (Leningrad); Sborovskiyp At r.'
(-=ingrad)
CIO: none
T! 'LLE: Danping of forced vibrations in tho hull of a sh1p
institut problem materiiLlovedeniyao Rasseyaniye energii pri
kolobaniyakh ulprugikh sist4m (Ehargy dissipation during vibrations of elastic systs").1
aukova duaka, 1966# 292-302
Kiev, N
TOPIC TAGSs vibration analysis,, marine engineering
ABS-ZLIC.-IL: Calculations of forced vibrations using data from previously publishea-
Iit,eraituro yield calculated values of the amplitudes which# as a rule# are con3iderabl
lovar than experimental valua3v that is, there is an error on the side of danger* 'Ine
experiments described in the present article were conducted under deep w4ter condition4
which eliminated the effect of factors such as shallow waterp mooring walls " cther
~ch-'Pa. Yfeasura=ents ware made of the forced vibrations of the hull of a ship at
'differant values of the eccentricity,, in the presence of vertically directed anid
.undirected forces, Based an the experimental data,, curves were plotted of the zhan
iin the amplitude of the forced vibrations as a function of tbAir frequoncre rn
iwor;dng up the data# the decrements In the free damped vibration@ wwo determined from
I
i C.'j 112
A 07569-6-7-
ACC N14 V6029373
the resonance curves by the knoun forwAA
where b - (~24,)Alfis the relative width of the resorwce peak, found with the
of the Co cad vibrations equal too half t1w mucimm values In the proseneo
r0
of resonance,, the value of the dynamic coefficient is cargmted vith the deasment,6
~by the following relationship
A. --' (2)
6
A f igure shaws values of A for ships of various confioxationso After an wrtanded,
:athazatical davelopsent.' the article arrives at tbe, followlag formla for
deterainati(a of the dynamic coefficients
10000
:Orige art. bass 15 formulass 4 figures and 2 tables,
:So CODSs 13,, 20/ SM DAM 2V*b"/ =IQ RZfe 007/ IM We ow/ am asrs ooz
Y r I
It
MIX ;,K
111KOL.'sKly, YU.I.
...
Sone, problems In the xet~-od if In"-rpretingr graylty .2nonalier, in
reolorically, closed areas of the westprn Pirt of Central Asia.
Trudy VSEGEI 42-70-64- "(0. (MIRA 14:9)
(Kara Kun-Gravity prospecting)
ESILYAND, H.G.j HIKPIo'Mr, rit.Le
Evaluation of the methods of quantitative Interpret-stion of gravit&-
tional ammalies above a vertical shelf. Izv. AN Turk. SSR.3ar. fiz.-
takh., khim. I geol. nauk ro.467-65 163o (MIRA l7t2)
1. Mel ranyodochnoy geofizlkt L seygwlogit AN Turkamnskoy SM.
TAWTP 9-9-0 PNW=MSKITp X.X.; POL&TAYA, X.I.; MMU, G.A.;
MIKIMO S.L.1 ISAMOMA, A.0,; TWIMFO K.P.1
=of Ivy-Vzy (ChIls 15-weLls TITOW, X.T4.0 ?Mf?U&Mp A.1,;
UMMORA# T.T.1 GIRFAKMAO OXI ZUxEVq A.V.l II ~ISKIYp Tuatel
Wme O.N.
ftablem of the wthods of pological Is"sUgations. (TruOyl
TOM 92g91-98 163. OGRA 17W
IWT( 1
~191 NR: AR4044?V' S! 0) 6 96 4000,'005 fM 2 1 DOI 2
L4 1-i
Ref. th. Ge-oftaila, AIPH
F
11RAt P_'
P W:
The -.jae of spectal-i-ed -nmplitern ir
~~;(_)U'RCr! Tr. Vsss. n i wool- inAa, v 12, 19fil. 100
Tr")MC TALUM 11cophysics, wentlM rJoci, regional component. locux companent/
ttlym
~IILA110N- Repot to cm the !;-I riltimb-It'n-7 dr-"-loper" In 19SQ-1960
All-la'nlan Sete imww, this complitor in based
n, if H, I' ""r
prift, 11,10 In lomign"I for 9t, ~riansforrm lion
.w,owlal flelrb, ~ncludfiiR 07~e breukdorwn al the
!Ield bAo leml arw] r6~gjciinRi -ornpow~-,ts. for ~~onvertfisgthe Initial field
novi )evel, Or. The ipoU-in-n-w wp,~* ~jx7pr-,)v-d, qrml re(ornmended lor serifti.
lt~~ ti,yn 4n 19PI.
AR4044203
ES, Op
C 1.1 )o
MKOLISKIT, lit. la
Nottiods to allow for the zero creo-p '.r, TirAy
VSEGEI 104s74-82 164. (Y-6 RA -,, 8 ~ - ~.
Y~Sjr. A.R,,Lz
uzmcxixg T.G.
fis"Gurist," of 56 dhr~sww soWdiplold wboat feme
ftvU U4, blelo AN MM nao5s2W-M 160* (ML, 24M
(WMT BX=M)
ZXWU, A.Ro I 9sur ru MaWK, L.K..
0
AsmlU of Us stu(tr of pro&wtive lims of the sq&MplofA
bytrid Tritiew dur%WX, Tr, vul#aso Diul, lftt. biol,
AS US mG'l,5s28%-29d f60. (MBA 14L7)
~ (WMT SF89030) I I
-NUOLISKITp U.K.; KUMKHIKj, T.Cls
Yaterials an tho stOy of the inheritanoo of quentitative
sharacters in maphidiploid Iinse. Biul, Inst, blol, IN, HM
W*5t299-3M 160. (KML 240)
9=1 9SUrg U.K.; VAMIIMCII, 0.1.
ft~-
Galculation of the heridity of qwmtltative features of wheat
1dIVIoUW b7 dispersion analysis. Rule Insto biol, AN
~ vo.6439-2" 161. (KIM 15t3)
(WINAT 1 16)
UUMISKIY, Yu.5,
Th4ory of the welem clmv!es of 41,'I'srentisity1r, fwrl"A~:ra V11
s 33: 17. '04
Wd. Fit -1141, Sauk 1951, 21'.: 1
HWIMAq. fit i 1"f #s Art jwIn
wit, V-11,0 latt~-- 4 ~A X :3 X W tr. (CYI'Wirii~ 14KA4
C4 b, (XiMary 11.0) Ift a Irwir's 4a-'d rcr elfwTi-
intlom) U-IfOresct(cl, Ifit nvIl itith
IM (OUO*iug b-f-W.UIA 1A vatA J. - I + I IV-
MIZI)JIMMpowl, wh"f is tile rmin r'1
fix"tuco.fiv thtntvki If"llan'l 1"n All'i P'.Mvinis rft life
t
t
th tv". of felt n"troan U-Ainz in Un filwin CA fil. uwcb i
We *Ad L"- tfsp. ZIzt tis the rit4n r2u) C4 ti"16ti-m
callIttax and ,"a crovs scrIL-mil f-r Wn, T. ,) rr~-Cs-ij
ImArts. NoI/Artnive pm-TfArd Ja v-so ottb--xl ft!;Tncqtv
arv ZI-PeItted an p&gvr In the olb--r =~?I'M an kou".
tioik ch;umt~,r is uv4 lot c-untLrig rJ jA;c lr~grrmvws. [a
ticxib mfthr~ls laytrs & %sturld V Awl U L~ in U.- "r
C4 V~'t L-
knold. vfhkb "t plac-A in 6 wot of t4e 1: .Itkv. a, I
---livitkii alm C*Lupwtef- wur-r ls-.4-W 1.
--.kwa-
11r\
Category : USM/'K=le&r Ettysics - Nuclear Reactions C-5
Abe Jour ;Rot Zhur - rizika, Wo 1, 1957 So 558
Author :Katkov,,, V.P.,, Nikollskly, Yu.V., cd Stolyarov, G.A.
Title :Determination or taf-Ilatto orthe Average Fiselon Cross Sections of
P" SM U235 In Uranium-Water lattice Blocks
Orig Pub Atoni. mergiya, 1956, No 3, 61-64
Abstract fte ratio of the average fission cross sections of Pu:239 and U235 me
determined in uramiun-vater lattices of natural uranium and ordinary vater.
For the sake of comparison, this ratio vas mq%sure$ far a uranium-graWto
reactor. It is established that the ratio