SCIENTIFIC ABSTRACT BESPALOV, V. I. - BESPALOVA, V. G.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000205110020-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 8, 2000
• Sequence Number: 20
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

0 'c) 764
5.,.11k1/6"1/004/003/015/020
Experimental investigation EiWp-i82
in Fig. 1. The equivalent quadripole of a sespaTated by
sections W and BBI is also sholen in the fi.gure,, The
matrix of this system is (Ref. 4A~ Blo-zh, F.J,, FiEher and
G.J. Hunt - Proc. IEE. loo, 64. i9.5',)
z
cosOc?) 4- --c-09(u~1 - .,C
Z2 T
it
(k
j sin~ke.)
j(.0cTc os (k t
z Z' (h
where w is the opera-i.:ing frequer)r,~-
k 46~1 "
~, is the length of the lir)t
Card 2/ P/;~

i~OOV003/0,15/020
Experimental investAgation E. P,
1/Z2 = 1/Zj '/Z2'
z1f = V~Wc:
Z 2' = V-C~/C2
Z = 4 CII/C0 are wavc~ imp--d-inc-as 1-f the. lzries
formed by a stub and the Lower bas, 4~,r"AL,- a ;-tut- a-nd
upper
base and by two neAghbouring stiA,s r -:~S F'. #,: ~ ie I v
C, C' and C are ihe c orret-p,:-ndiriv -. apac it.anc es per
.1 2 0 unit 1.engtb~
CTis the caparl;v boween the end of a stub
and the ba~,,- ('f tht- C11POSIte comb structure.
The scattering equation for a chain cor)wi,~%t-ing of such
quadripoles Is Siven by.,
C ay d 3

4'/(-- 1/004/003 /015/020
Experimental investxgatlon
A A22
Cos (P0 c o s (k Z' WC.TZ
wh er e (p0 a.s the pha.-.ie of the wa-... Thq :;,.att6ring
character-
istics were taken experimenta.1.11y b\, 115"T151 tv'r.
d6mountable inter-
digital. structurea, consist-Ing of -~;im-_~ar elemen-ts. The
system
'was designed for operation at de,)m"Trc- wo-%es and had the
following dimensioxj.q-~ period of iha D - A 0 mru
diameter of a 9tub 4 mm-, leng!h ol' a itut; 90 mm,
the gap between the at~ibs h ~ 2 be-Eueen the base
and the stub S could be -varied f,onl 0 to 15 mm. The measured
results are illustrated in Fig. '; Ism-All . -L-.-Ae!4)
together with
the calculated -urve;j (solid lino5). 5i ngt e di~. ont i.AuiJ
i es
in the system were produced by uciiric; npe. ial czOls in which
the
position of a stub could be varied Thi~ theoreli-,al -alue of
the modulus of the refle~'rion due to various types
of disconfijiuity can be fourid frori foinoi-1,ic- given in
Ref. 1~
Card 4/1/z, 6~-'

/(,i /oo4/003/015/020
Experimental in~vestigati.on V, E~-, 8 2
Experimental l.y ~ the fol.lcwiric.~ types ot ~2i r, f . rAu I
t v wer e
investigated,. displacement. of the ~r, -ans-erse
direction (g changes by changos -.n the SOF. Jr~t-een the
stubs; displacement. of the P-vub in th~ of the. structure
and changes of the length t of the ~tLib, Ilis -alui3 of the
reflection c oaf fici ant as a func t ior; cf g/D ~-;
Illustrated
in Fig. 4, together wiih the calculati~d r,:Ompat I ~Son of
the calculated and theoretical resuIts ,bow, rha' If the.
reflection coefficient produced by the is small.
this value can be found as a superpo_~-,titn --' thi-
refle-_-tion
coefficients due to individual discontinittio-, The. equivalent
circuit of a metal -plat e(comb- type) i~tru~tur+., !P in the
rorm of
a chain of F-type quadripoles whosj~- matr)-t~-2 ar,- In the
formR
A'~
w CZ tg(k'
Card 7'

,,-il?i/61/0011/003/015/020
Experimental investigation
where k -r w \Fc-ii I
z Is the wave impedance of the- !~tr)p lin,~ formed
by the neigbbouring plettt~!~ a r) d
is the helght of the plat,~,~;
is the capacit&nce between Ili, mid of a plate and
the cot-er,
The phase changes of the wave over a i di~,5~:rjbed by,,
COS W0 z I ... w CZ tg(kE)/2 (2.2)
The experimental system investigated conqi-~i~d of' two metal
surfaces, one of, which carried a number of
t~quidistanr.Ay-spaced
metal slabs (parallelopipeds) having diinrrozicns d 2 cm
s = 1.7 cat and 9.0 cm, The tipper of the t6ystem was
parallel to the lower iurface and it~! dint~jn-*-,- From the
metal
slabs could be varied. The non-homogz-nf-;ti-L- in the ey~toEm
were
produced by filling the gaps with metal plcilr,~z inserting
piece.-
of metal under individual slabs oz li-,ji,;Jrjr 'he i--pacing
between
the slabs. The results of the expi- illustrated In
Card 6/~~ ~'

Experimental invf:stigation
1. 17f)4
c; t 4 -.,/6.i/oWoo/ol
E -9 ZI/ EI 8 2
three figures, In part, i cul ~ir. F-i g~ 1 0 z;hows the value
o f
reflection coe~'fi.cieiit ai; a fun~rioj) of ibt- change. of
the
distan-~e between ~ wo tie i ghbour ing = I ab.~ The straight
lines
of Fig. 10 wer;:: basA on calrulationQ- while *he c-irc.les
sh6,
the experimental pc,.int~;~ From these ~.K~,eritfients- it -Ls
seen
that. for small inhomogeneitiez T h - a i~ r ~ em ev r b etwe
en exp.eri
On t h
and app.roximaur - al~Tilaltad r'e-,"Jr~. j, iat 1Qfa"tcsr e;.
other hand., for h/h and b/b
considerabl e dtev x -)t i onQ f rom the the(,rev.ical
s(.ra.kghx 14-nes ;~I
ob5 erved. The tiaxt =yz~eni to be irr, ~~ai ed --ons:isted
OfA,
number of recxangular rescnaior.~. t)-y means of nar
slot.S4 the i~y~--tem j-,, illustratA in Fig. !2 , The
equation of su(.h :Bv~Etem Is in the fovn~,
.0
impedance and xhe
wl~i-h is equi-aLlent- to..
beaked experimenta
r,~-,angular- channel.
where B and X r~-present tl)e
shunting aclmitt~~ri-e of a qu6drApcli
re-,t-angular ie-~onat.or- Tht, foimula w-s
by empl ing equipment consi:3iing of a
Card

"it
Ali.
3,D764
s 4i-/6.-i.,/oo4/003/01 511
Experim ent aJ I rju e i t Iai on .... r 19 2.1 E3 8 2
~ depth of 68 mm and wiilh of 1-2 mm. Tyarjbverse slota
havil&.'
~ depth of 3 trim and wi i, h of 1. mm ar)d -- pac. ed at 3
mm were Q%KV
at the wall-? tind the boi tom of thr- : ljartni-- , Metal.
plate
small. slots iri-it-s) werc, AnSer-tOJ AT0.0 ibcse slots, Th:
alet e 1
vras then covered with a plait? wht(h li,)rl correF4pon.ding
Blo
small apertuye" for measuring the in the resonat era It
The inhomogenei(,Le~~ III tlit~, Sy9tem Wei..'i produced by
changini"L:L, he
parameters of a c~ell, i.e. it., dimej)!~iolis Id and I% and
its.:,'
position (a The rcsults of lh,~ exp-~,viment~.,
il1ustrar-ijgt-,-,,t;he
L
change of the natur~tl frequervv of ilim ~-ystem are illustrat
in two figures~ rn particular. Fis, !b show,~ the frequency
deviation as a function of Lala aDo The straight
lines in the figure were obtained -h-ctetically, From the
above results. it is concluded that the periodic delay
structures
can be represented by the -ideal-Jied quodripolas provided the
non-homogeneities are not ex,..ess1vf--,, Tii mcst practizal.
cases,
the results of experiment and theory ore in satisfactory
quantitata--e agr&ement.
Card 8/1
Z/-, ~

3 0 7,~4'
1/oo4/oO3/015/020
Experimental investigation .... E192/E382
There are 16 figures and 7 rcCcrellces: 6 Soviet-bloc and
I non-Soviet-bloc. The English-language roference quoted is:
Ref. 4 - A. Bloch, F.J. Fisher and G.J. Hunt - Proc. IEE, 100,
64, 1953.
ASSOCIATION
SUBMITTED:
Fig. 1:
Card 9111Y
'7-
Nauchno-issledovatel'skiy radiofiziclieskiy institut
pri Gorlkovskom universitete (Scientific Research
Radioph3aLcs Institute of Gorlkiy University)
December 15, 196o

ALIBER., S.I.; BESPALOV, V.I.
Diffusion equation for a statistically nonhomogenous wave
guide. Radiotekh. i elektron. 6,no.3:448-449 Mr 161.
(MIRA 14:3)
-Nkvi pides)

1 12471-63. B/lo8/63/018/004/004/008 #
AUTHORS: Bespalov, V.I. and Kubarev, A.M., Active Members
of the Society
TITLE: Calculution of losses for design of circuits
forming
pulsations of the current in induction loads
PERIODICAL: Radiotekhnika, v. 18, no. 4, 1963, 22-30
TEXT: A system of linear algebraic equations is obtained
by a method
of perturbation. They permit waking corrections, which
are stipulated by
the presence of losses in inductions of the system, to
the reactive elements
of the forming dipole. The reactive parameters of the
circuitg forming
a prescribed pulsation of the current in induction loads
without losses,
are assumed to be known. Coefficients for the system of
equations are ex-
pressed within parameters of an ideal circuit (without
loss) and within para-
meters of the original pulsation. This work is a
continuation of that reported
in reference 2: V.I. Bespalov, A.M. Xubarev,
Radiotekhnika, v. 17, no. 7,
1962. The presentation considers the approximation of the
pulsation with
Card 1/2

-L 12471-63 s/io8/63/018/004/004/008
Calculation of losses for design... 0
a final total of transient harmonics, the parameters of
the forming dipole,
and the formation of a quasi right angled pulsation
consisting of two
harmonics (N=2). There are 3 figures and 4 foreign
language references.
SUBM=D: January 27, 1962
tf
Card 2/2

L 7'. ~4' M112FC(Q-21~'IDi) 'F,-(. /T/E-EC' 1--2/
ACCESSION NR: AP5=679 tIR/0141/65/o08/001/0070/0080
F
ATMOR: Bes~palov, V. I.; Gaponav, A. V.
TITLE: Statistical characteristics of automodulation of solid-state
laser emission
SOUIRCE: IVUZ. Rudlofizi v. 8, no- 1, 1965, 70-80
'~_statistical property, -two level- laser, relaxationlAme,
TOPIC TAGS: solid laser,
I ser automzodW,ation, laser spike sequcnce~ laser spike intensity
ABSTTUXT: The authors -consider the Influence of spontaneous emiGslon
an the be-
havior of a system of two-level objectB with different times of
longaitudinal (T
and transverse (T2) relaxation situated in a single-mode reconator
(T2. 00/005/0073/(>0744j.,
AUTHORS: Chicherin, Yu.. 1.j Abrosimov, Yu. V.; Bespalova, L. T.
TITLE% Use of glass wool filters for trapping potassium tetroxide
dust
SOURCE: Khimicheskaya promy*shlennost', no. 5, 1963, 73-74
TOPIC TAOS: glass wool filter, potassium, potassium tetroxide,
FS-8.5 filter
ABSTRACT: Authors describe a new design of glass wool filter and
its behavior when used to trap potassium tetroxide dust. This com-i
pound was selected to test the filter on account of its ability to
create very severe operating conditions for the filter. Authors
state that product losses amount to about 6.5 g per normal cubic
meter without the use of this FS-8.5 filter. 'Use of this filter
greatly reduces these losses. Authors then give a detailed des-
cription of the construction of this filter. Authors state that
their tests showed that these filters can be effectively used for
trapping different kinds of industrial dusts, including those with
d .1
/2

L 17."7-63
ACCFSSION NR: AP3004301
increased coalescence, at agas temperature lap to 300C. Orig.
art.
has: 3 figures.
ASSOCIATION: none
SUBMITTED: 00 DATE ACQ: 15Aug63 ENCL: 00
SUB CODE: CH NO REP SOV: DOO OTHER: 000

CHICHERIN, Yu.I.; ABROSIMOV, Yu.V.; BESPALOVA,
L.T.
Use of glass fiber filters for collecting dust of
potassium
peroxide. Khim. prom. no.5:393-394 My 163. (MIRA
16:8)

AUTHOR: Bespalova, L. V. (Gorky). 24-5-1/25
TITLE; n the theory of impact controlled vibration mechanism.
(K teorii vibroudarnogo mekhanizma).
PERIODICAL: "IzveBtiya Akademii Nauk, Otdeleniye
Tekhnichaskikh Nauk",
(Bulletin -of the -Ac.Sc.-, Technical -Scienca-s- -Sectio-ji)-,
1957, No-5, pp. 3-14 (U.S.S.R.)
ABSTRACT: A model of the mechanism considered is shown-in
Fig.l.
This consists of a mass M suspended on a spring and having
one degree of freedom. An external sinusoidal force
IF sin wt acts on the mass M and the spring constant is k.
The motion of the mass M is limited by a stationary plane
with which it makes inelastic collisions. It is assumed
that: 1) energy dissipation takes place only during
collisions with the plane, 2) the sprinG is linear,
3) collisions are instantaneous, 4) displacement of the
-ion
limiting plane may be neglected. The equation of mot
of the mass M is given by (eq.1):
16E + kx = P + F sin wt (x < x0)
Card 1/5 where P - a constant force, in general 94 Mg, and k -
the spring constant. x is measured from the point at
which the lower end of the spring is situated when the

On the theory of impact controlled vibration mechanism.(Cont.)
24-5-X/25
latter is unstrained. Impact takes place at x = X05
and a coefficient R (coefficient of restitution) is
defined by i1 ~ -R~01 where io is the velocity just
before the collision and ;c is the velocity just after the
collision. The equation il transformed by the substitutions:
~ = F-1 (MW2x_ A-2 ); T = Wt; N2 = kM-1 W-2
and takes the form
+ k2f = sin T (f 0)
114 1%'-11 -
1 L1+R2 ctg2in nX
1~4 - x2 _1 1 + (1_R) X2 (10 ctgltn%