SCIENTIFIC ABSTRACT PARAMONOV, V. F. - PARAMONOV, V. S.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001239210012-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 15, 2000
• Sequence Number: 12
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

S/221/60/000/608/013/014/)Fy
D040/D113
AUTHOR v Paramonov, V.F.
TITLE: The running-in and power testing of machine tools without
metal cutting
PMIODICAL: Stanki i instrument, no. 89 1960, 14-15
TKKT: Detailed illustrated description is given of a running-in and test
device for lathes (Fig-3), which can also be applied to milling and drilling
man.hines. This device eliminates the considerable metal losses in the for-
mation of chips during ordinary standard tests by roughly cutting the blanks
with the maximum cutting force, The device* which is shown diagrammatically
(rig.1), consists of a long helical gear (zl) installed on the machine, and
a mating helical gear (z 2) which is coupled with a loading and braking unit
f1red on the saddle. The length of the gear is chosen according to the
work length and the length of the guide :brew or rack to be run in. The
saddle is loaded with'three components of the butting forest circumferential
Pz (Fig.2), radial Pyg which is proportional to P 2 and depends-on the pres-
sure angle and the vertical position of the axesq and axial P x, which is
Card 1/6

S/121/60/000/008/013/014/xx
The running-in and power testing D040/D113
proportional to the circumferential force and depends on the helix angle,,
P
The required ratio at the standard pressure angle is obtained by placing
2
the axis of the z gear above that of the z, gear. The height differenceg
x, is determined ?y the W angle from the 0 1 02C triangle (Fig.2)9 using the
following formula:
(dnol 0 d n02) sin
X =
2
Rotation is transmitted from the z 2 gear to the loading and braking device.
Bra:king can be accomplished by a mechanical friction brake, a magnetic
powder clutch, or by loading with the aid of an electric generator or an air
compressor. The application of electric generators of thel-C (GS) type
praires most convenient for braking purposes;using these generatorst the load
capacity can easily be adjusted and the current in the stator shunt winding
alt9red. The GS type generators operate at 360D-9000 rpm. Thereforeq a
multiplier (reducer) of three gear couples (z 4- z5; 26_Z7 ; ZB_z9) is used
Card 2A

S/121/60/000/008/013/014AG!,
The rmining-in and power testing D04O/.Dll3
between the z2 gear and the generators Any reducer design including plane-
tary may be used* The loading unit on the saddle renlaces the tool holder,
or it Mn be held in the tool holder. The z 3car is made of pla,..ic in
order to reduce noise. The total weight of he device together. i~,rith a Fc P
3000 (GOIR-3000) generator is 25 Icg. A photoCraph showing the device on a
IIIA61611 screwouttinG lathe is included. There are 4 figures.
V//
Card 316

PAFW4DNOv.-UAdjMjL,Ejdoroidch, kand. tekbn. nauk,- PETYMPOLISKAYA,
'-~N.Ye., red.; DURASOVA, V.M., tekbn. red...
[New dynamometric equipment and the measurement of cutting
forces]No,mia dinammetricheskais apparatura i lzmerenie oil
rezaniia. luibyshev, Kuibyahevskoe knizbnoe izd-vo,, 1962.
48 P. OURA 16:3)
(Dynamometer) (Metal cutting-Measurement)

PARAMADY. T.F.
EmmmiWit and efficiency tests of machine toolp without cuttimg
metlas. Stan-i instr- 31 n9.8:14-15 Ag 166.
(MM 13 '- 8)
(N&cbi,ne tools-Testing)

IPARAmauov. v.F.
Graduation of three-component dynamometern. Its.takh. no.3,15-16
Mr 160. (min 13..6)
(Dynamometer)

A k p) !~-I, C) t') c-, vf~ t/~, (~-~ ,
7JYONCHKOVSKIY, A.D.; YABED, U.N.; MIKHAYLOV, N.A.; 37,01TISTOV, V.I.;
SHMLUND, E.g.; HIMMYN, M.Kh.; GUS IKOV, F.G.: PARMONOV,V.G.;
GLUMUN, G.M.; GRIGORIIDI, M.T.
Polyamide treatment of Imitation kidskin and flesh layer splits.
Leg.prom. 16 no.10:22-26 0 156. (MIRA 10:12)
(Rides and skins) (Amides)

EJAORIKIYAN, S.Kh., inzh.; PAR&kRNOT, V.I., inzh.
Remulte of the testing of mobile nechanined supports for stopes.
Ugoll 34 no.8:27-32 Ag 159. (MM 12:12)
Is Giprouglemsak ZPAne timbering)

ITANDY, I., Inshener; P, . " .. Anshener: SHILINW, I.. Inshenero
.-MINOMMMU141k &
fletal props for this seem. Maetougla 5 noo.?':23-24 A 156.
f,'Xne timbering) (=A 919)

PAUNONOV, T. 3P. (Aspirant)
*An Investigation of the 0[ittiza Voross In the Rich-Speed Nechizing of Carbon Steel
with a Recently Developed DymmuetrIcal Apparatue.10 Cam I*eh Sol, Moscow AvI-
ation 2babsological, Imst, 24 Dec 54. (VM, 14 Doe 54)
Survey of Selontific and Technical Dissertations Defended aft USSR Higher Ifteational
InstitmtIons (12)
SO: SU ND. 3513. 24 Jun 55

PARAMONGV, V. F.
"Investi.mation of the Cuttin;~ Forces in High-Speed Turning of Carbon Steels
on the Basis of Newly Developed Dynamometric Apparatus." Gand Toch Sci, Kuypyshev
Aviation Inst, Kuybyshev, 1954. (RZInNekh, Apr 55)
SO: Swi. No. 704, 2 Nov 55 - Survey of Scientific and Technical Dissertations
Defended at USSR Higher Educational Institutions (16).

Sh _kand. tekhn. nauk; SO
UMVML--V1adbntr-FedoOch "LOMONOVp
ro 'era
AIMMA'ar ivzm a -novator; MINHEYEV,
6 ahllfovshchik
N.I., "d.; DURASOVA, V.M., tekhn. red.
[Machining profile parts on surface-grinding machines]
Obrabotka proftlInykh detalei us plookoshl.ifovallnykh
stankakh. Kuity-shev, Ruibyshevskoe kn1zhnoe izd-vo,
1963. 73 P. (MIRA 16:9)
1. Srednevol2liskiy stankostroitellnyy zavDd (for SolomDnov,
Paramonov).
(Grinding and polishing)

takhnicheskikh nauk.
PAW!RNDY
Interrelations of cutting paranetars. Vent.vAuh. 36 no-7:45-49
ii 156. (m,tal cutting) (Him 9: 9)

7
wder loading. Stan. i
(mm 1818)

F.ARAMONOV,V.F.
1--_ ~- ~ - -71 ~ I ~ -, - ~: I
Cutting forces In large-feed machining. Stan. I instr.26 no.10:
24-26 0155. (9w 9: 1)
(Metal cutting)

16.3200 77604
SOV/133-6c-2-4/2-5
AUmHOR: Kotrovskiy, M. M., Paramonov, V. G. (Engineers)
TITLE: Effect of Port Size on Produc'41.vity of Open-hearth
Furnaces Output
F'RRjCMI'^4AL: Stal " 19b6, Nr'2' Pp (USSR)
ABSTRACTi The Invest1gation of performance of the 370-ton
open-hearth furnace ports of various designs, when
feedtn oxygen into the flame (with air enrichment uD
to 24%1 was carried cut on two groups of furnaces "A
and "B". Group "A": charge 370 ton, volume of gas
checkers 116 m3, volume of air checkers 165 m3. roup
"B", rharge 370 ton, volume of gas checkers !63 r5)
volume of air checkers 224 m ~i' the height of smoke-
stack 100m. rPo determine the most rational dimensions
of the port the following po'.nts were Investigatedr
(1) The area of gas outlet into the flue; (2) height
Card 1/7 of gas port over threshold of the door; (3) angle

Effect of Dort Size on Productivity of 77604
Open-hearth Furnaces Output SOV/133-6o-2-4/25
of inclinatlon of the roof (in the air duct);
(4) angle of inclination of the gas po.rt bottom in
the flue; '5) the angle of Incidence of air flow and
gas flow; 'o angle of Inclination of' flue roof along
the generatrix; 7) distance to the point of contact of
gas floiq with the bath; (8) height of air gap between
the roof of ports and the flue,;(9) length of "fore-
cham~er1j;('1,O) ratio of cross sectional areas of flame
and gas door;(11) ratio of flame door height to Its
average width;(12) height of "air dam" over charge
door's bridge. As a result of Investigation the most
rational d1mensions are given in Table 1. The estab-
lished correlations are only effective under analo-
gous working conditions. At p:~esent the ports of 370-
ton furnaces are designed with consideration for the
established optimum parameters for both groups "A"
and "B". 7he design of pcrts s shown In Fig. 6.
Research continues to determine, the effects 01'
Individual parameters of ports on the productivity
of open-hearth furnaces.
Card 2/7

Effect of Pqrt Size on Productivity of 776o4
open-hearth FurnaceB Output SOV/133-60-2,-4/25

C IN
m 0

4.'j co
%_q ;4 0
94
l'
C
U
ll
let
Ll~
0
ll~
> m ~ ~
N ~
m ~
m N 0 ~
- C4 0
-ri 10,
.
4_1 IL.
0U

0
CV

f,4 m F.
0

0

4-4

o 4-) q..,
r 0,-

;~ 1
Ll I
: .1

0 - tin C4 1
-_ !e

CO 0
4

~
? IQ
C) X
V
!2
IS 12
Ul Doi d
Card
Ul Et J rl (-) S.4 U U 4 -a

Effect of Port Size on Pgoductivity of 776o4
Open-hearth Furnaces Output SOV/133-6o-2-4./25
Table 1. The effect of main rational
parameters of "Venturi-type" i~oxts on
productivity of 370-ton open-hearth
furnaces, and a comparison of these
parameters with typical parameters
(Giprostal') and with those used by
the plant.
MA.rea of gas door, m 2 (2) ratio of gas door height
to its width (3) height of gas hearth bottom over
the bridge (hh) (4) angle of Inclination of rhomb1c
roof of port (~p ) (5) angle of inclination of gas
hearth bottom and flue (-~ ) (6) angle of inclination
of flue roof along generatri), ( cL (7) angle of
incidenae of air flow and gas flow tj (8) height
of air gap between the roof of poxts d the flue,
Card 4/7 mm (9) length of "forechamber", mm (LF) (10) flame

Effect Of Port Si:~e on Protiuctivilty C)f, 776o,'~
open--hearth Furnace,,; oiitp~,,t
So V/-L , -6n,-2 /2,
wIr 1-11,
tIOOI~ 01) (b) ~le!.LJit,. min (11) (c)
'lull 1OWQ-P WIdth, mm
door height to
Of f*jIjjn(, I.,, rioov:;
~Jjj(j jr.,,
ch,cirge doov la,
of' gm,, 1.110w colit'ict WIAII 1;
are 1 t.,ible;and 6 ill[rtwo"I.
(U) (11) ratio of
vildill. (12) vai 1.0 of'
Of "n,
hn-11"Ilt 1-1.
dl o tiln(,.P, from W"? no I
w Nith to rluca, M. T!,-,
Card

Effect of Fort Size on Productivity of
ODen-hearth FurnaceB Output

, P

~o,

K~

776ol~
SSOV/133-6a,-2-4/?--'/
JT-71
Card b/7 F i fD

Effect of Port Size on ()!* U ~D () -4
Open-hearth Furnace.,, OutpUl, ISIOV/ I I I - 60 - 2 - li /2'~
I
Fig. 6. Design of' '~JO-ton open-hearth furnace porl-
with vatLonal parameters.(D)WIldth of gas door. F C),I~
other deslgnatLons see Taule 1.
Z-131
C,--,,,d '(11Y

KOTROVSKIT, H.M., Inxii.; PAMMNC)V, Y.G., inxh.
Effect of port dinenslons on the performance of open-hearth
furnaces. SUll 20 no.2:111-117 F 160. (WRL 13:5)
(open-hearth furnaces)

A,
EOPIM. A.A. [deceneed]; ZAYONCHXOVSYIY, A.D.: YABKO. Yrk.M.; PARINI, V.P.;
PAIIAKONOV V....G.; GLUZM, G.M.; GRIGORIADI, M.G.
Increasing, water repellency in leatnor bjr means of P velnn-tyne
Y
COMI-Potind. Leg.prom. 17 no-7:23-25 .1 (MLRA 10: 9)
(Leather Industry)

PARAMONOV, V.I., inzh.; KOWASIN, G.M., In2h.: VJLVILOY, V.V., in2h.
Unit of equipmert with the M-9 suprnort. Ne)ffi.trpd.rab. 11
no.8:17-21 Ag 157. (MIRA 10:11)
(Coal mines and mining-Equioment aAd supplies)

ALEKSANMOV, B.F., inzh..; BALYKOV, V.K.. inzh.; BARANOVSKIY, F.I., inzh.;
BOGUTSKIY, N.V., inzh.; BUHIKO, V.A., ka,nd.tekhn.nauk, dotsent;
VAVILOV, V.V., inzh.; VOLOTTKOVMT, S.A., prof., doktor tekhn.nauk;
GRIGORIYEV, L.7s., inzh.; GRIDIN, A.D., inzh.; ZARMAN, L.N., inzh.;
KOVALIV, P.F.. kand.tekhn.nauk; KWHETTSOV, B.A., kand.tekhn.nauk,
dotsent; KUSH TSTH, G.I., inzh.; LATYSOW, A.F., inzh.; LEYBOV.
R.N.. doktor tf)khn.nauk, prof.; LSYTZS, Z.H., inzh.; LISITSYN, A.A..
inzh.; LOKHANIII, K.A.. inzh.; LYUBIMOV, B.H.. inzh.; KAsm'-bTICH,
K.S., inzh.; RUKHASIYAN, R.V.; MILOSWIN, N.M., inzh.; KITNIK,
V.B., kand.tek2n.nauk; MIKHEYEV, Tu.A., inzh.; PARAM019OV,.V.I._,
inzh.; ROKANOTMIT, Tu.G.. inzh.; RIUBINOVICH, 76.76., in2h.;
SAMOILYUK, N.D., kand.tekhn.nauk; 30MOV, V.K., inzh.; SHOLDY-
RXV, A.Ye., ka:2d.tekhn.nauk; SHAGIN, V.T., inzh.; SHAGOVSKIY,
Ye.S., kand.teithn.nauk; FZYGIN, L.M., insh.; FREHMI, B.B., inzh.;
FORM, A.A., Inzh.; LIORIN, V.N.. dotsent. lmnd.tekhn.nauk; CHET-
VFaOY. B.M., i:azh.; CHUGUHIKHIN, S.I., inzh.; IKOV, V.N.'
inzh.; WMYAT3V, B.M., inzh.; SHIMMIN, N.F., kand,tekhn.nauk;
SHPILIBERG, 1.:6.. inzh.; WORIN, V.G., dotsent, kand.takhn.nauk;
SMOOW, I.G.. doktor tekhn.nauk; &WRIS, N.A., inzh.; TMIPIGCPXV.
A.M., glevnvy red.; TOPCHIYEV, A.V., otv.red.toms; LIVSHITS, I.I..
zamostitell otw.rod.; ABRMOV, V.I., red.; LADYGIN. A.M., red.;
MOROZOV, R.N., red.; OZMWOY, H.I., red.; SPIVAKOVSEIY, A.O.,
red.; FAYBISOVICH, I.L.. red.-, ARJUlANGELISKIT, A.S., inzh.. red.;
(Continued on next card)

JECIESARMV, B.F.---(coutinued) Card 2.
EMYATEV. V.S. Inzh., red., BUKHANOY.A. L.1., In2h., red.; TLASOV,
V.M., inzh.. rvd.; GLADILIN, L.V., prof., doktor tekhn.nauk. red.;
GNOTSOV, N.V., inzh.. red.; GRECHISHKIR, F.G., inzh.. red.; GON-
CHAREVICH, I.F., kand.tekhn.nouk, red.; CUDALOY. V.P., kand.tekhn.
nauk, red.; DRIATOT, H.E., inzh., red.; 10MIR, S.M., doteent, kand.
tekhn.nauk, rei..; MMUOV, N.V., dotsent, kand.tekhn.nauk, red.;
POV013,--v:-=ITq I.A.p inzh., red.; SMLICHNYY, P.L., in2h., red.;SALI-
TSIVICH, L.A., kBnd.tekhn.nauk. red.; MRANTOV, A.V., kand.takhn.
neuk. red'- SUTLiM G.A.. inzh., red.; JBARBARCHUK. F.1., rod.izrl-va;
PROZOROVSKAYA, V.L.: tekhn.red.; KOHMATIYSVA, N.A., tekhn.red.
[Mining; an encyclopedic handbook) Gornoe delo-, entaiklopedichoskii
spravochnik. G-lav.red.A.M.Terpigorev. Chleny glav.redaktoii A.I.
]Baranov i dr. Moskva, Gqs.nauchno-tekhn.izd-vo lit-ry po gornoma delu.
V01-7- (Mining machimaryi Gornye maBhiny. Redkol.toms A.V.Topchiev i
dr. 1959. 638 p. (Mining machinery) (MIRA 13:1)

PARMIUY, V.I..- TMRDV, N.K.
CO-- " M F idw
Conference on metallic supports. Ugol' 31 no-11:43
N 156. (MLRA 10:2)
(Mna timbering)

-
np f4 -- --- -, - &~ I
~T " 1e,"
0,
q . I ~,e-

sInAL, v.S., inzh.; PA.ILMNOV V I.., inzh.
Unit for heating winter shelters* Avtodore 26 no.10:26 0 163o
(MIRA 16.21)

PARMNOV, V. 1.
~,.,
Vibrating device for cleaning mine wra. Ugoll 33 no.9:29-30 5
158. (MIRA 12..1)
(Mine railroads--Cars)
(Coal mines and mining-Equipment and supplies)

LISITSYN, A.A., inzhener; PARAMONDV, V.I.. Inzhener.
m-PNMVA--NNW
Rkparience in introducing MPK mechan12ed moveable mine supports.
Mekb. trud. rab. 10 no.8:11-15 Ag '56. (HLRK QtlO)
(Mine timbering)

LISITSYN, A.A., inzhener; PAMQNOV,.-,.VJ,,, juzhener; SUILIBFM, I.L.,
-11-~I~k-;.n,'-.1- -I"":, . 11
inzhener,
New met of eqaipment for the complete mechanization of longwall
mining operations. Nekh.trud.rab. 8 no.8:5-10 D 154.(KLRA 8-1)
(Mining mRch Ine27)

FARWONOV, V.I., IMShOn8r; KORZHIKOV, X.I.. Insbaner.
Rkporience In using 01 argsapips, post. Mokh.trod.rab. 8 no.3:36-37
Ap-My (154. (MM 7:6)
Mine timbering)

PAM ------

V' T-,
amo
TF

~~,Ikpbr4jnlen_ ton.-IPW6-atl:o~ V~aljlng- Scaffolds

!'J6 - !~J),
A, r, Y-1954,.-
p

-testing ~oiai' tyN. OK~-15O.:.
g sea
~ifdaii6n. and,
*
'

h autho _l
hd tYp6 _Z~150-scaff`Ad~ are cas to pro
a t o
I ccor ng e
y
'
-

_iiAn* 0" M
to- Advantages
etil:* -
esult bAhe
ahd r_ 600%8
ducef-
-
.:Tabl s;
andaid"MOS-50U,.scaffold~ are inted; out a
ovir -the st

-7 diagrams,
gr#b
j;
j
no t
lt
Oll

See
a"
use
%Saari

4,
PARPMONOV,V.1., in2hener
Mechanization of coal mining in lbgland. Nekh.trud.rab.9 no.8:
41-45 Ag'55- (MLIRA 8:10)
(Great Britain--Mining engineering)

KLOR',"KIYAN, S.Kh.; GRIDIN, A.D.; PARAMONOV V.I.
At the Scientific Technical Ccrancil of the State Experimental
Institute of Design and Construction for the Coal Machinery
Industry. Ugol' 39 no.11:66-69 N 164. (MIRA 18-2)

~- -7
V. K.
PAR.01011OV, V. K. -- "Investigation Of 'fie Influence of Atmospheric
~ U L,
Precipitaticin on the Function of Radio Station Antenms.11 11in Ccv--,munlica-
tions USSR, Mosccw Electrical Engineering Institute of Communication,
Moscow, 1956. (Dissertation for the Degree of Candidate of Technical
Sciences)
SO.- Knizhraya Letolpis' 'No 43, Octolber 1956. 'wIoEcow

SUBJECT uss / PRYSICS CARD I / 2 PA - 1492
AUTHOR PARAMOKOV,V.K.
TITLE The Influence exercised by Precipitation on the Electric Proper-
ties of the Surfaces of Nets of Wire.
PER16DICAL Radiotechnikat 11, fuse.9, 12-20 (1956)
Issued: 10 IT52 reviewed: 11 1956
This work deals with the problem of the influenos exercised by precipitation on
the electrlic properties of a network of line wires with round cross section. It
is assumed that wire of this network Is covered by a uniform coating of ice, i.e.
that the.-oleotric line and the coating of Ice form coaxial cylinders. In spite of
a certain ldeali2ution this case is a very near approach to conditions actually
existing in practice and therefore of practical interest. The first case to be
investigated is that of a plane wave ineiaing upon the wire net which is covered
by a coaxial coating of ice. This wire net is assumed to consist of an infinite
numter of infinitely long conducting wires arranged at equal distances from one
another. On the basis of these conditions a system of equations is derived which
~contains the unknown quantities Qm R S and coefficients which are determined
by the boundary conditione and do noT dmepend on the ordinal number of the conduc-
ting wire. (All conducting wires were numbered in consecutive order from - coto
+ oci). Next, the solution of this system with respect to Q_ is carried out. Com-
putations show that in the case of such wavelengths, wire Wiameters, and distances
between wires as occur in practice, the quantity q. suffers a sharp decline if
the summation index m (M W ... increases. This makes it possible,

PARAMOROV, V.K., inzhoner.
C 'I i~dio relay line antennas from the effects of precipitation.
W M fig
Vert.svlazi 17 no.2:9-10 P 057. (MLRA 10:3)
(Radio-Antennas)

SOV/106-58-5--5/13
AUTHORS~: Paretmonoit, V.K., Metrikin, A.A. and Fel,,, N.A~
m ~,o Small Reflection Coeffic~ients in a
TITLE;
Wide Frequency Band with the Aid of a T-bridge kIzmereniye
malykh koe-Ifitsiyentov c)trazheniya v shirokom diapazoLe
chastot s pomoshchtyu T--mosta)
PERIODICAL-. Blektrcsvyazl, 1958,r%Nr 5, 28 - 34 (USSR).
ABSTRACIT; The equ-';_pmr--&. is intended for the measurement of sidall
1?eflecticn coefficients (less than 1 - 1.50/6) in the frecuen3y
band 3400 - 3900 Mc/s. The arrangement is shown J n Fie-,,_Lre I
and consists essentially of a hybrid-T. The co-linear arms are
i.,onnected to an adjustable termination and to the elemenl~ under
:est backed by a standard termination. respectively. Me
13-arm is fed from the source; the ouiput krom the H-aTm may be
seleGted at one position of a 2-way switch before detec~:ioL.
The other position of the switch samples the output from a
dire,:~tional coupler connected to the source. The output from
--he switch gces to a detector via an attenuator and then to an
implifier and indicator. The detector consists of a cartridge-
--lype crystal mount with a Drobe extending into the guide. The
f~rystqi return path is a thin length of wire whose i_ndu-,tqn,,;e
In conjunction with the probe capacitance tunes tc the mean
Card 1/3

SOVAC6-58-5-5/1 3
The Measurement of Small Reflection Coef ficients in a Wide
Band with th,~ Aid of a T-bridge
operating frequency. The crystal is a DKI-_1 with an ef fer-tive
:resistance cf 300 Q. The matching over the band is nr w-~rs-
-than 0.5. Figu-Te 2 shows the variation in s.T,.r. ov,-r the ba_,acl
at the E- I H- and test-arms. The H-axm matching is
-Drovided by a tapered rod mounted eccentrically on a rctatiLrr
arm. The E-arm matching requires both a peg and a diaph-r-a6m.
4 shows a drawing of the adjustable termination.,
.the absorbing part of which is made of two thin vedges of
laminated insulatin:- material coated with aquadeg, m-ounted
.in the central ;)lane of the guide parallel to the E-ve%,,t.~r.
At their "dead" end, the wedges are secured to a movable
short-3-i-rcuit which also supports a thin rcd which moves
axially between the wedges. The -rod protrudes at the sl~,arp
ends of the viedges and is T-shaped at the ends Independent.
adjustment of wedges and rod enable the reflection coeff.-I-c-Lent
of the combination to be v-.ried.. irigulre 5 shows t1ne standa-r,,
This is a thin vredge of the same abso_rb_!::i,-
inaterial used above, supported in the ct-ntr-e of the --21-d--,
betweentvo taperint, blocks, of foajpod plaf~tic. The -f,
~,ard 2/3

SOV/106-58 ... 5--5/---3
The Measurement of Small Reflection Coeffisients in a -71-:de
Band w-il-.1 the Aid cf a T-brid,7e
0
rieasurem-ent. is :;onventfcnal; the necessary adjac,"x-en-'s
des,-,ribed -in detail. Seven sour3es of error are
and their pro'balDle values -tabulated. The total eErizate-d
ezror ir. measureffent varies from 0.065% -with a
ffi-lient of 0.11; tuo 0.2?50,'o' Tith an of 1.51/L TI-ere are
figures.. 1 table and I :5o-.iet reference.
q, jqr-r7
SUBMITTIM: July
~;ard 3/3

SOV/111-r--li-7/36
AUTTOR!3: Metrikin, A.A., Chief Designer; Paramonov, V.K., CanZi~---E
of Technical Sciences
TITLE: Parabolic Horn Antenna for Radio Communication P'elay '-l-ne-z
with "Vesna" EaUiDment (Ruporno-parabolicheskaye antennn dlya
radioreleynykh liniy svyazi n8 apparature "Vesna")
3
PERIODICAL: Vestnik svyazi, lq58'~Jlr 11, pp 4-6 (USSR)
ABSTRACT: The article contains basic construction data and electrical
characteristics of a parabolic horn antenna, developed by
the Scientific Research Institute of the USSR Ministry of
Communications, for radio communication relay lines using
the "Vesna" equipment. The antenna has the following dimen-
sions; height 620 cm, width 390 cm, depth 32C cm; area of
opening 7.5 sq m; antenna volume 11 cu m; weight 990 kg;
weight with rotnting device 1,37 kg. The opening of the an-
tenna is covered by plastic sheets (penoplast) in one version
(Figure la). However, a honeycomb type cover made of glass
cloth is more effective. The "Denoplast" cover reduces the
output only to a negligible extent, while the ~rlass wool
Carr, 112 cover reduces the output by 0.7 db compared with an uncovered

SOV/11 1 -'~ 9-11- 7/36
Parabolic Horn Antenna for Radio Communication Relay Lines with "Vesna"
Ecuipment
antenna. The dehydrator "AD-4" is used to
of dry sir at a low pressure inside of the
3 and 4 ere diagrams of the lirectivity in
and vertical planes. Further, the authors
formulas for calculating the various electrical
tics. There are 2 photos and 5 graphs.
produce an excess
antenna. Figures
the horizontal
present se's -~f
chRracteris-
AISSOCIATTONt Nff Minis tort, tvii tivyrizi SMSU ("WiOntifia Nonotirch lnot,0-0,e
of the (11,73B I'linintry of Communicti t ions)
Card 21:?

Pi 4"
ft-- JL 0. 6--p
(c ID A~ Ile -mm)
11 AL My~
A. MLA~
LX A.$-
P-W-b--
IN, L No-
61, 1
11 in B. 22
A. AL S-P..
It
I
=-Z -"- -~- M-
a
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tb-~ .?- P-- P-- -p-
It A ll~
sop" Somme tw *0 ambam" smol" or am edn"m 2numusloa smsft of
Swap s"Nowks wig 13DOWS-1 611111111111401113- 216 A. a. PIMP- (mn), 01110-1
am.

~j 0.) SOV/111-59-10-5/'v
AUTHOR.- Metrikin, A.A., Chief Designer, Paraponov,_Y.K_,, CanJi-
date of Technical Sciences
TITLE.- Waveguide Systems for Radio-Relay Lines Using the I'Vesnall
Apparatus
PERIODICAL. Vestnik svyazi, 1359, Nr 10, pp B-10 (USSR)
.A3STRACT- This article presents electrical characteristicz and
construction data for the elements of the waveguide Sys-
tem for radio-,relay lines using the "Vesnall apparatus..
Opening with a brief discussion of waveguide design and
construction, the authoiBstate that the afticle will'. con-
sider rectangular waveguides in use on several radio-re-
lay lines under construction. Choice of waveguide dimen-
sions, assuring the absence of higher order waves and a
sufficiently low attenuation of energy in the waveguide,
is discussed; the operating range in this particular case
is 7~7 to 8.8 cm, and future expansion of this range a--
the upper end is taken into account; thus dimensions of
58 and 25 mm are selected for the walls of the waveguide
Card 1/5 In dealing with the materials for waveguide construction

BOV/111-59-10-5/23
WaveguLde Systems for Radio-relay Lines Using thes I'Vesnall Apparatus
the autho3isstate that pure copper is best, but too
soft; brass, containing 96% pure copper, has suffi-
ciently high conductivity and, experiments show, suffi-
L
cient rigidity. Construction of waveguides out of a'u-
min-um, containing a very low percentage (1 - 2%) of im-
purities is also mentioned. It is noted that industrial-
ly produced aluminum waveguides are anodized by the chro-
mic acid method and have good anti-corrosion character-
istics, while brass waveguides are produced without a
protective covering; protective measures for the latter
are very briefly discussed. The author states that this
article considers rectangular (58 x 25 mm) waveguids,
manufactured from L-96 brass, containing 96% pure copper,
and that information on rectangular (58 x 25 mm) wave-
guids of aluminum, in which the content of admixtures of
magnesium and manganese does not exceed 1%, is presented.
Flange joints, and their requirements, in the waveguide
system of the "Vesna" apparatus, for both internal and
external installation, are treated, flanges for internal
Card 2/5 use are stamped from 5-millimeter brass, and brazed to

SOV/111-59--10--5/23
Wavegulde Systems for Radio-relay Lines Using the "Vesna" Apparatus
the waveguide using POS-40 solder. Requirements for
flanges used in external installations, determined by
conditions such as temperatuibdeformation and icing, de-
manding additional load carrying capability, are also
discussed; such flanges are cast from brass and brazed
to the waveguide with POS-40 solder; a rubber gasket pro--
vides the necessary hermetic seal. Such flanges, states
the author, can, under test, withstand lDads of about
7-8 tons. Both types of flanges are illustrated (Fig 1~.
Two types of curved waveguide are described- bent and
turned (P.-Lg 2); in order to keep the reflection coeffi-
cient from the curve in the former to a minimum, the ra-
dius of curvature is taken equal to no less than 0.5 m,
and the angle of rotation no more than 900. Twis-ted wave-
mAdes and their construction are briefly dealt with,,
T~e angle of twist is kept under 10-150 to minimize re-
flection of energy in such waveguides. Flexible wave-
guide inserts, their construction and use, are also
treated; -the reflection coefficient it is stated, does
Card 3/5 not exceed 3-4% in flexible waveguide inserts. Two types

SOV/l 11-5/9 -10- 515/2 3
Waveguide Systems for Radio-relay Lines Using the "Vesna" Apparatus
of hermeticizing inserts are described: a lower such
insert, -for separation of the hermeticized antenna-wave-
guide system from the rest of the apparatus, and an upper
such insert (Fig 4) to guarantee stable operation of the
antenna-waveguide system when antenna hermetization -Ls
disrupted; the latter is equipped with an electric hea-
ter and insulated cover to avoid freezing in winter; one
heating element consumes 70-100 watts. Measurements of
attenuation over the frequency range of 3300-4300 mc in
a rectangular brass waveguide (58 x 25 mm) 100 m long were
made, and the experimentally obtained values compared to
those computed by formula (given); experimental and com-
uted values sufficiently coincided for the most part
g 5). Measurement of attenuation in an aluminum wave-
M
guide (A-00 alloy) showed that it is 0.5 db greater ', on
the average, than the attenuation in a similar brass
waveguide. Matching of long waveguideB was studied expe-
rimentally on an experimental wavegulde 70 m long as well
as on standard waveguide systems of various lengths, pro--
Card 4/5 duced fox, one of the radio-relay lines, all mathing mea-

SO V, 1111 -59' - 10. 34
Apparatus
Waveguide Systems for Radio-reiay Lines Using the "Vesna~~
surements were made with a waveguide measuring line, and
the end of the wavegulde being studied coupled to a we.11
matched load. Repepted measurements showed that in see-
tions of waveguide systems 710-100 m 1ong with a well mat-
ched load,, the travelling wave coefficient over the ope-
rating frequency range has a value on the order of 0,95-
0.0.8. The results of one such measurement are illustra-
ted (Fig 15). A waveguide T-bridge, specially 2onstructed
for measurement of small reflection coefficients over a
wide frequency range, was used to measure the degree o1
matching between separate elements of the wavegulde 3ys-
tem; studied were: reflection coefficients from one wave-
guide Joint, of waveguide curves (bent and turned) of
twisted waveguides and hermetically sealed inserts, Mea-
surements showed that in the operating frequency range
the reflel-tion coefficient from one joint does not ex-
ceed 0.2-0.3%: Measurement of the iterative attenuation
between waveguides showed it to be no lower than 120 db
.Ln the operating frequency range. In conclusion the au-
thoisnote that on the basis of the data presented, these
Card 5/5 systems satisfy all the necessary requirements.

0 A-, o
For
8 2178
S110616010()0107102VO05
AVMOIRS: Kuzuetsov, V.D., Paramonov, V.K.
TI ME A Highly Effective VHF Antenna With a Low Fringe Radiation Level
and a Controllable Radiation Pattern
N
PERIODICAL: Elektroavyazl, 1960,'\No. 7, pp. 18 - 2.8
TEM: The authors describe methods and results of piklaulations and the
experimental investigation of a wideband reflector t' ifff esigned for use
an enn . d
on VEI? comMiLnication lines
3with atmospheric scattering The antenna (Fig. 1)
16 PtA of a horizontal parabolic cylinder. The exciter consists of a system
of Nadenko dipole vibrators and one reflector. The vibrators are suspended on
the metallized surface of the earth in such a way that the reflector, together
with the earth's burface forms the 900 V-reflector of the exciter. The latt--
is arranged in auch a way th# its line of phase centers coincides with the
focal line of the'pAraboiie cylinder. The antenna produoes a directivity pat-
term. in the vertical plane with small side lobes. The looation of the exciter
In the Immediate vicinity of the earth's surface simplifies the antenna feed
system and reduces the Influence of the exciter on the antenna directivity pat-
tern. Using a linear exciter in the form of a horizontal vibrator row pro-
Carl 1/3

82:L78 S/1%/60/000/07/024/005
A Hig12ly Effective VHF Antenna With a Low Fringe Radiation Level and a Controlla-
ble Radiation Pattern
vides a control of the antenna directivity pattern in the 'horizontal plane by
ph"Ing the vibrator currents. This also pemits the multiple use of one an-
tenne, for reception. The necessity of using cuirred supports is one of the dis-
advantages of the antenna. Preliminary calculations show that this does not
eauso extraordinary difficulties In the antenna desIgn, since only two or three
supports are required. 7he basic antenna dimensions are selected according to
the 'required antenna gain, the width of the direativity patterns in horizontal
and-vertical planes and the angle of main lobe inclination in the vertical plane.
For oommunicatlon lines operating in the 5 - 10 m range over distances of 1,000
1,5CO km, the following antenna dimensions are reoommendeds height of the
apeiture, H - 40 m; focal distance, f a 20 m; width. of the aperture, a -;~-,045
50 n (eight vibrators in the exciter); height of the exciter reflector, hr =
= 4 m. In practice, the basic antenna reflector and the exciter reflector are
a single-line wire lattice. The distance between the wires is determined by
the required re-radiation attenuation magaitude. To ob ain. an essential re-
duction of the side lobe level of the directivity pattern in the horizontal
plane, the vibrators of the exciter must be fed with an amplitude drop from the
Caid 2/3

82178
S/106/60/000/07/02/005
A Highly Effective VHF Antenna With a Low Fringe Radiation Level and a Controlla-
ble 11adiation Pattern
center to the borders of the exciter. Vibrators having an equal distance from
the tmbiter center are connected in parallel (Fig. 2) to provide a control of
the directivity pattern. The mathematical analysis of this antenna is given.
Equations are given for the directivity patterns in the vertical and horizontal
planes, the directive gain and the antenna gain. The experimental investigations
were performed on a centimeter model (1 z 2DO), on a decimeter model (I : 17)
and on a model of the excit6r in actual dimensions. All measurements confirmed
the correctness of the basic theoretical assumptions and calculations. The
experimental results are shown in graphs (Fig. 8 - 11). Urnere are 11 diagrams
and 1. Soviet reference.
SUEIG7M: January 25, 1960
Card 3/3

KIJZNETSOV, V.D.,- PAAP-&HONQVT-VJ4--
Control mystem for the directivity pattern of
hand antenna with a low level of minor lobes.
no.2t23-30 F 160.
(Antennse(Electronics))
, craplex wide-
Elektrosviaz' 15
(MIRA 24:3)

24074
9// AO55/AI33
AUTHORS: Kuznetsov, V. D. and Paramonov, V. K.
TITIZ: Device for controlling the radiation pattern of a multiple wide-
band antenna with a low side-lobe level
PERIODICAL: Elektrosvyazl, no. 2, 1961# 23 - 30
TEXT: One of the main components of a steerable antenna - or rather of
itz feeding system - is the phasing device. The practical setup of this device
depends on the particular features of the feeding system. The authors describe
in the present article a phasing device designed for an eight-unit recei-ing an-
tenna, whose feeding system uses unbalanced coaxial cables with wave impedance W
'P~ 75 ohms. This device is intended-for operation on wavelengthsA = 5 - 10 m.
.',.t allows to control the antenna radiation pattern within the angle-limits T, +
240 (the distance between the centers of the outermost antenna-units being ig.~ml
rhis phasing device (see Fig. 3) consists of four unbalanced artificial lines 1
with 75-ohm wave impedance. These lines are formed by identicallr-shaped ele-
mentary cells C.,, the radius-ratio of the four concentric semi-~circumferences be-
ing 1, 3, 5 and 7 respectively. Every cell is connected to a knob-shaped contact
S,/106/61/000/002/003/006
Card 1/4

24074
B11061611000100210031006
Device for controlling the radiation pattern ... AD55/A133
'K,Alie brushes of the slider 81 sliding on these contacts. The slider is also an
unbalanced line. To-ensure matching in the points of the Moving contacts, the
wave impedance of this line varies by steps (from brush to brush), its value beirg
respectively 37-5, 18-75, 12-5 and 9.4 ohms. The matchirg of the receivers is
er=,red by a special transformer Tr. Attenuators A are inserted, for simplex
operation,:between'the ends of the artificial lines and the output plugs p. (�ome
thei>retical and practical data are given by the author wLth-respeet to the para-
meters of the elementary cells, of the artificial lines and of transformer TO.
Besides the problem-of matching the antenna-units to'3he 75-obA:wave impedance
cable... there arises the problem of balancing, an unbalanced coaxial cable being
cormected to-the symmetrical, antenria-system. The solution of these problems in-
veives difficulties in the case of ultrashort waves. A device permitting to over%-
come these difficUlties is desciibed in the second part of the present article.
This~ matching and balan-aing de'vice (see Fig. 8) is bascd upon. the use of the shart-
wsive-transformer described,by 0. Z. Aisenberg [Ref, 1: Antenny, d1ya magistrall-
n.irkh radiosvyaz,ey("Antennae for national radio-communicationsI, Svypz'Izdat.,
PAS].. Figure 8a shows the connecting diagram ot this device, the following
method being used for a symmetrical introduction of the emf dnto the diagram: the
Inductance L2 of the correbtion circuit is divided into.two equal parts q, each
of these two parts having the form of a separate coil made with a thin 75-ohm cc-
Card 2/4

24c)74
S/106/6 1 /CM/Y-;VY-- 3.1~,
for controlling the radiation pattern ... 1,.055/A133
w:ial cabl,:). The coils are connected to the (.1dagram by the end.- of the br,-AdiriL~,
as shoun in Fig. 8c, whereas Fig. 8b show.,; the way used to couple thr-, t,-,o coLir,,
the emf being introduced through the inner conductor of the cable. '!~Lis devic,~,
proves entirely satisfactory from the point of view of both ma-tchin6 and balanc-
ing, within a wide band of short and ultrashort iaves. The author then dezcrib.~!_-
the equipment used for testing the phasin.- device. Radiation patterns in Ithe
horizontal plane were plotted for various sbttings of the slider. The tests prov-
ed that this phasing device allows to control the radiation pattern ..!ithin a suf-
f'.cient range of angles. Three radiation patterns are reproduced in the article,
for the central setting of the slider and for the 240-setting (extreme sottin.g).
A slight increase in the level of the side-lobes is exTlained by certain inac-
curacies in the length of the artificial lines of tt:rie phasing device and of the
connectiri,-, cables. In the case of transmission antennae, the control of radia-
tion pattems is more complicated. One of the possible controlling devices is
briefly described, its deficiencies pointed out, and a method permitting to eli-
minate theso deficiencies is suggested. There are 1~, figures and 4 Soviet-bloc
references. [Abstracter's note: in Figure 3 1 (line) stands for the Russian /7
(liniya), C (cell) for the Russian -'t(yacheyka) and Tr (transformer) for the
'~transformator); but K (standing for 1mobj and Sl (standing for --li
Russian Tp
Card 3/4

24074
S110616110001002100,31006
I)evice for controlling the radiation pattern ... A055/A133
tire not translations of the Russian symbols, but an ada:Ption of them, the Russian
B standing "vykhod" (leadout) and nT for "PDlzun-tokos"emniX" (brash
slider)]., Indeed for
SUgv',ITT M: February 25, 1.950.
Figure 3:
1) - 1
2) C
3) K
4) Sl
5) Tr
Figure 8:
1) b
2) c
iOMBEfBE~ BWE
6)
P., 8
card 4A

29552
s/1O6/6i/Ooo/oi1/Oo4/Oo6
6,1g-00 (11S9 A055/A127
AUTHORS: Kuznetsov, V. D. and Paramonov, V.K.
TITLE: Broadband stub in superhigh-frequency systems.
PERIODICAL- Blektroavyaz', no. 11, 1961, 30 - 34
T M : In antenna feeding systems, it is often necessary to ground a d-c
or a 1-f circuit without deteriorating the h-f circuit; parameters. The use of an
ordinary quarter-wave stub is possible only in systems operating on one single
frequency. In superhigh-frequency work, "metallic insulators" are used. The
present article is a short analysis of this broadband insulator or stub in the
general case, i.e. not considering the relations between the wave Impedances Zo
(of the line) and 7T and . The stub being symmetrioal, only one half of it
(Figure 2) will be ex ~e here. The input admittance of the transforming part
of the Stub (from the side of point A) at frequency f corresponding to the wave-
length Ais given by::
Y ZT + izo W
inp T i 2P
Ca--d 1/ 5 ZTZO + ZT

29552
3/106/61/000/011/004/006.
.Broadband stub in superhigh-frequenoy systems A055/AI27
or 2 2 2 2
Zoz~ 0 + PYZ 0 Y
Y inp T ' ginp T + ib inp T ' 2 2 4 2 + 1 2 2 4 2 (2)
ZOZt + ZT Zoz~ + Z~~
-where P= tg9.1; 2f(
A I Analogously, the input admittance of the correcting
short-circuited part of the stub in the same point A is,
Y ib - - i
inp K inp K 2 ZKO
The absol4te value of the total reactive admittance of the stub in point A is thus
Z (Z2-
T 0 1
by = b + b (4)
inp T inp K Z2 2 4 2 Z
oz~ + ZT ~
Thrt normalized value of this admittance (:an be written as follows:
C ard 2/5

29552
,9/106/61/000/011/004/006
Broadband stub in superhigh-frequenoy systems A055/A127
bj = 1: = 0 m - n (5)
91 2 P (1+e)
where z0
m = 2(Z0 - ZT) - (ZT~ (6)
ZT Zo zo ZK,
The matching (traveling wave coefficient) ELt frequency f is:
1,,, 2+ 4 -IblI
K V ku.0 (7)
f (bT'Y + 4 + jbj':j
Let the working frequency range of the stub be the frequency range within which
b.' does not exceed the Magnitude IF, corresponding to the inflections of function
br' in points/31,2 (Figure 3). The coordinates of the inflection points are:
2m + 6n + If (2n + 6n)2 + 16mn (8)
~1, 2 M
Card 2/5

29552
s/lo6/6i/ooo/o1i/oo4/co6
Broadband stub in superhigh-frequency systems A055/A127
The coordinates of the two other points whfjre the function is equal to are:
1 2
P3.4 ~ 2 01,2 (10)
1,2
The working frequency range of the stub is-
arctg P4 1800 - arctgP
max/"min - arctg~ are __
1 3 tgP 3
The calculation of the stub is effected a:s follows: m and n are determined by
Eq. (6). Substitution of the thus found magnitudes in Eq. (8) gives /3,,~. For-
mula (10) is then used to calculate f33 4. Substitution of /13 4 in Eq. 5)
gives P~ . Formula (7) permits then to End the minimum matchil% in the working
frequency range; the width of this range Is determined by means of (11). A graph
permitting to calculate K and q is given. The length I must be chosen equal to
~meanAj Amean being determined by the ar:' thmetical mean frequency of the working
range. The phase characteristic of the stub can tie computed with the aid of for-
mula:
card 4/5

Broadband stub in superhigh-frequency systems
2 !KP2
tg ZT
2 ZK + I
V
ZT
251552 s/io6/61/oDo/oil/oo4/oD6
A055/A127
(12)
An experimental check proved that the results olwtvined with the above set of for-
mulae are sufficiently correct. Mere are 9 figures and I Soviet-bloc reference.
SUBMITrED: Jannary 20, 1961.
Figure 2: Figure 3:
0 Z,
2M,
"
Card 5/5

25520 S/1.08/61/016/008/002/006
D21*-iO/D304
AUTHORS: Kuznetsov, V.D., and Paramonov, V.K. Members of
Society (See Associatl_o~n
TITLE: Installation for studying directional properties of
antennae
PERIODICAL- Radiotekhnika, v. 16, no. 8, 1961, 25-32
TEXT: The authors describe a simple arrangement for studying direction-
al properties of antennae. The results are displayed on a C.R.T. in a
polar system of coordinates. The &splay sh-DWS either the directional
distribution of the field strength or power and permits evaluation of
the directive gain of the antennae by means of integration of the polar
graphs. ;he installation has been developed for the study of direct-
ional properties of broadcast, TV and communication antennae, whose
directional properties have to be taken withAn a narrow frequency band
and are usually given in a linear scale. Tho bloc diagram of the
arrangement is shown in Fig. 1. In taking polar diagrams it works as
follows: A h.f. sine or pulse amplitude modulated signal, received by
a revolving antenna A is applied through a h.f. filter F to a detector
Card 1/5

25520
S/108/61/016/008/002/006
Instal2ation for.*. D280/q)304
D1* The I.f. detected signal (1000cls) is applied to the amplifier K,
whose load consists of the moving coil of the lphase splitter PS syn-
chronized with the motor. The two signals from the fixed coils of PS
are detected by a second detector D2 and through a phase switch are
applied to the inputs of the DC channels of the horizontal and vertical
deflection systems of CRO type 3 0-7, (ED-7) with a long persistance
screen. The diagram of the phasing switch and of the second detector
is also given. The amplifier used has the output voltage proportional,
within a certain range, to the square root of the input voltage which
for small amplitudes of the signal gives a directional diagram of the
field intensity produced by the aerial. Its cct diagram is shown.
The anode cct of the last tube has a transformer matching the amplifier
output to the inductance of the moving co:11 of the phase Splitter. The
primary of this transformer is tuned to 1000ey's. The required amplitude
characteristic is obtained as follows: the second tube of the amplifier
has its operating point adjusted very near the cut-off. The voltage
Card 2/5

S/102./61/016/008/002/006
Installation for... 25520 11280/b304
obtained by the rectification of the output is-supplied to the grid
ihrough a high resistance, (switch Swl open). With the increasing
grid current the grid-cathode resistance decreases in proportion to the
output voltage of the amplifier. Hence the amplification of the
first stage, whose load consists of the grid-cathode resistance, varies
inversely proportionally to the output voltage Uout , so that Uout =
C'V -Ui. (IL) where C - constant. For better smoothing and stability
the output signal is rectified in a bridge circuit and applied to the
grid of the second tube through an RC filter. The feed back loop has
a small time conotant and a pass band of tieveral tens of c/so In this
manner, with the speed of antenna revolut;1on corresponding to 15-20
rpm, the beam width of 5-70 of the directional pattern lobes is faiths
fully reproduced. The frequency response of the amplifier is given in
Fig. 5. the 3db points corresponding to approx. 600c/s. For 55db change
in input voltage and 27.5 db change in output voltage the amplifier
characteristic coincides with the the-aretic-al response. The gain
Card 3/5

25520 S/IOEI/61/016/008/002/006
Installation for.9o D28OyV304
of the amplifier is 90 db. at IODOc/s for maximum input voltage. The
noise level. at the output is 35 db below the naximun output signal.
The dynam.4c, range of observations is thus of the order of 30 db. If
the study of the side lobes is required with the corresponding radiation
below 30 db with respect to that of the main lobe, the generator power
should be increased accordingly. Amplifier type 28-OM (IM) was used.
The phase splitter was a goniometer, consisting of two perpendicular
to each other coils, built as two rectangular frames, with a third
coil ofthe same shape inside the two. A more judicious choice of the
phase splitter would be a two-phase variablc transformer of type
4L'-,,7%kjO 5 ri (4VTM5P) which has a longer gain and a better sinusoidal dis-
tribution of voltage in the stator. The above installation permits
also the determination of the directive gain of antennae by simple in-
tegration of the directional diagrams. The integrating cct consists of
the integrating network proper (C=2DDO V F and resistors 950,65 and
3*9 kOhm), a 30'$ A ammeter and switches S'N 2 amd SW3 . The procedure of
measuring directive gain is given and it is stated that the same reason-
ing and procedure can be applied to rectangular aperture antennae.
Card 4/5

25520 S/108/161/016/ocs/002/006
Installation for..e D280/11304
In conclusion, the authors state that the described installation is
.easy, 4uick and accurate in actual separation. There are 8 fligures and
2 Soviet-bloc references*
ASSOCIATION: Nauchno-tokhnicheskoye obshchestiro radiotelthniki, i
SUBMITTED:
C;%rd 5/5
elektrosvyazi im. A.S. Popova (Scientific and Technical
Society of Rndio Engineering iI. ind Electrical Communications
im. A.S. Popov). Abstractor's note: Name of association
taken from first page of j)urnal
March 28, 1961
4e4l'
t wo -..--L LN I I
ct,vt P&I CA,
6v, 4rh
, ""'
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.ikCCESSION NR: AP4037396 S/0106/64/,000/005/000910013
AUTHOR: Kuznetsov-, V. D.; Paramonov, V. K.
TITLE: Selection of antenna height for ionosp1heric -scatter lines
SOURCE: Elektrosvyaz',;no. .5. 1964, 9-13
TOPIC TAGS: radio communicalion, ionospheric scatter, ionospheric scatter
p.ropagation, ionospheric scatter antenna, ionospheric scatter communication
ABSTRACT: Reasons for selecting the antenna m(;an height H and antenna-
aperture height H0% for ionospheric -scatter radio -communication lines are
considered. Curves and formulas are given for computing the mean antenna
height for any ratio HA /H. It is found that: (1) With a specified (where
is the angle of max vertical-plane radiation) in an antenna with the cosine
law of aperture vertical excitation. the mean -antenna height decreases and the
mi-st utilization factor grows with HA /H up to N /H a 1; hence, the antenna gain
Card 112

ACCILSSION PIR: AP4037396
growis more quickly than the total antenna height; in an antenna with a uniform
law of aperture excitation, the gain increases only up to HA /H a 0.85 and the
mast utilization factor only up to H,,,~ /H. a 0. 80; (2) Using antennas with
H,4 /1-1 - 0. 25 -0. 35, as is often the case on 1. 800 -Z. 000 -km lines, results in a
poor utilization of the mast height; increasing 11, /H to 0.7-0.8 would add 3-4 db
to the antenna gain at a cost of adding only 20-30% to the mast height. Orig, art.
has: 6 figures and 10 formulas.
ASSOCIATION: none
SUBMITTED: 30Dec63 DATE ACQ: 09jwa64 ENCL: 00
SUB CODE: 5 r. NO REF SOV: 000 OTHER: 000
Card Z/Z

i-ACCESSION NR: AP4014672 S/0108164/019/001/0018/0030
AUTHOlt: Xuznefsov, V. D. (Active member). Paramonov, V. X. (Active
member)
Tr.CLE: Stepped directional couplers
SOURCE: Radiotekhaika, v. 19, no. 1. 1964, 18-30
TOPIC TAGS: directional coupler, multistep directional coupler, directional
coupler theory, 2 step directional coupler, 3 step eirectional coupler, power
;dividing directional co er
U?i
ABSTFUCT: A theoretical analysi's and the design -techniques of multistep
directional couplers are presented. The coupler is regarded as a stepped line in.
which the coefficient of reflection from thfi !nput enddetern-AineB the coupling
faqtor. Formulas for calculating a directional coupler with any relation between
the" impedances of the principal and the branched ci:rcuits. are gkr~en. An n-step
Ih.
ard

ACCESSZON NR: AP4014672
directional coupler having an optimum characteristic: Is analyzed by means of a
Zn-power Tchebycheff's polynomial; the extreme case of this characteristic, the
so-called mraximum-flat characteristic, is also consi4ered. Two- and three-step',
couplers with the above characteristics are used to illustrate the method Of
calculation and procedures involved. It its recommended that directional couplers
be used in cases requiring power division in a specified ratio (e.g.. a multi
:element antenna with a controlled radiation pattern). Orig. art. has: 7 figur
and 67 formula*. es
ASSOCIATION: Nauchno-tekhaicheskoye obshchestva radiotekhaiki i
elektrosvyazi (Scientific and Technical Society of Radio Engineering and.
Electrocommunication)
SUBMITTED: 253an63 DATE ACQ: O7Feb64 EN'rL; 00
SUB~CODE: CO, GE NO REF SOY; 003 OTHER: 003
212
Ord.

Kuz,n~'Psov, V.i).; V.K.
Da.id h,-dancing- anao,,terz. i-adlote~!xdka I,,? no,,'):20--l-, -~~ Iti-
(."LtA 1'!. 10,
I. Dey.-tiritel lny,,,e chleny I'lau chno- tu~drli c lie skogo ooshch-~ stva
-L
radiotekliniki i elel~,.trusvyazi im. A.3. POPOW1.

Lhala=UL WT11) Ila
-A NRa AP6019010 SOURCE CODEA UR/0106/66/000/OD6/0020/0027
AUTHOR: Kuznetsov, V. D.; Faramonov, V. K.
ORG: nom
TITLE: Coph sed antennewith an active broadband reflector
SOURCE: AN SSSR. Vestnik, no. 6, 19066, 20-27
TOPIC TAG,3: antenna array, dipole antenna, antenna radiation pattern, broadband
communication
ABSTRACT: A unidirectional cophased dipole antenna array with an active reflector
fed by~a directional coupler is analyzed. It is shown that, with certain chosen
parameteri3 (coupling coefficient, dipole and feeder characteristic impedances),
this antenna maintains high directivity with good matching, and efficiency characte
tics in a wide frequency band without re-adjustments.
Cophased dipole antenna-arrays are usually constructed iri two sections,
an active section fed by the transmitter and a passive reflector section in
.which the amplitude and phase of the currents are stub tuned to adjust the
.*reactive part of the antenna impedance. Antenna current components from
the active and passive sections add in the forward direction and cancel each
other in the opposite direction, giving rise to antenna directivity. In other
fyPes of systems the reflector may also be active, but special transformers
,piust be used to insure proper amplitude and phase relationships between

L 42112-66
ACC NRt AF6019010
the currents. - In both types the antennas are directional at the operating
frequency only. At frequencies slightly removed from the optimum, the
front-to-back directj,~-ity ratio deteriorates, the antennas are no longer
properly matched to the feed system, and the efficiency decreases accord-
ingly.
. The authors report on a new driven cophased dipole antenna system
comprising two arrays, each containing two sections of four horizontal
two-section dipoles placed one above another. Each. dipole section con-
sists of four conductors which form the corners of a parallelepiped. In-
dividual antenna down-leads are used for each dipole arraky, and the cur-
rent phases are therefore equal. The opposite ends of these down-leads
are connected to a directional coupler which channels the currents with
proper amplitudes to corresponding dipoles.
ThiE; antenna system may be analyzed by assuming that each array
may be replaced by an equivalent dipole with a corresponding radiation
impedance equal to the sum of all actual dipole impedances, including the
effect.of mutual interaction between the main dipoles and the directors.
For purteses of analysis, the reflector dipoles may a1sco be analogously
treated sLa one dipole. The calculations performed by the! authors apply
Card

NRt
'to an ant 'nna
e jqstem with the following parameters:. distance M between
the center lines of adjoining four-dipole columns, 430 mm; diameter of
each conductor used to form a dipole arm, 0. 00093 t; diagonal of the trans -
conductors,
verise cross section of the parallelepiped formed by the c
~0.0745 t; length of each dipole arm, 0.42 t; vertical distance between dipoles,
0.581t; distance between the two arrays, 0.337 t; characteristic impedance
of each dipole feeder, 300 ohm; directional coupler length, 0. 3 t; maxi -
~,muzn directional coupler current splitting factor, 0.2.
The authors develop expressions for the resistive and reactive compo-
nents of self - and mutual impedances of the equivalent dipoles as functions
of 1/A ilwhere 1 is the dipole arm length and x the wavelength). From these
expressions and the directional coupler parameters, the basic antenna
performance factors such as the antenna radiation patterns, the input
traveling wave ratio, the antenna efficiency, and the back-to-front ratio
are determined. The deviations are based on a previous work on a
driven cophased two-dipole antenna fed through a directional coupler.
The theoretical and experimental curves for the traveling wave ratio
(TVVR), efficiency (n), and back-to-front ratio (B/F) are shown in Figs.
1, 2, and 3, respectively. The experimental results were obtained for the
Card

L 42112-f
F FC-N R.
F,U
46
QL
UIZ UIZD UP gj:) U11 U"#3 (43
Fig. 1. Traveling wave
ratio as a function of
l/A
Solid line - theoretical;
dots - experimental.
Fig. 2,, Efficiency as a
function of l/X
4-~Ll i - S I
98 olid 'ine - theoretical;
0.- 0.2 025 0,3 0.35 0,4 C.45 Ob dots - experimental.
-B/F
42
U~- U," LW WO Wr
Fig. 3. Bar-k-to-front
directivity ratio as a
function of 1/X
Solid line - theoretical;
dots experimental; broken
line antenna with nonperiodic
reflector.
C,,d 4/6

NN AP6019010
antenne. whose dimensions were given above. Each array in the experi-
mental setup was fed by a coaxial cable, and the dilwles were driven
through's symmetric 30D-ohm. KATV cable. The frequency range used
in the test was limited to the band between 300 and 000 Mc. Both the
general. pattern shape and the half-power beam widths of the radiation
patterns [not supplied] are said to conform to the theoretical patterns.
It is apparent from the theoretical curves that the antenne. is highly uni-
directional (the B/F ratio does not exceed 0.1, 0.2, or 0.3 in the 1.6:1,
2.1:1, or 2.5:1 frequency ranges, respectively). A good match between the
antenna proper and the feed system is evident from the high TWR
,(0.7 for most of the range). The efficiency is 9016 at short wavelengths
and 707a at longer wavelengths.
One of the salient features of the antenna systej.-n is its ability to
maintainits performance level even when the parameters of its compo-
nents are sub-optimal. For example, the length of the directional coupler
does no-t affect the basic antenna characte ris tics. The dipole array dimen-
sions are not critical and may be made equal to the corresponding dimen-
sions of typical cophased dipole arrays, i. e., distance between arrays,
AO/4; vertical distance between individual dipoles, ;k,/2; and dipole arm
length,. 0.42)~ (where X. is the fundamental antenna Wavelength). The only

L 42112-66
ACC NRj AP6019010
relativ(dy critical parameter is the dipole impedance, which tends to
extend ---.-he antenna frequency range and assures a good match between
components if it is low.
For comparison, the broken line in Fig. 3 represents the B/F directiv-
ity ratio of a cophased antenna with nonperiodic reflector, i. e. , a reflector
in the form of a curtain of parallel conductors separated by a distance of
0.035 t. From this and other comparisons, it was concluded that the per-
formance of the new antenna is equal to or better than that of an array with
nonperiodic reflector or a cophased dipole antenna array in which the re-
flectcr is tuned at each frequency. Orig. art. has: 11 formulas and
12 figures. [FSB: v. 2, no. 81
SUB CODE: 09, 17 / SUBM DATE: 090ct65 / ORIG REF: 002
af

L 39678-66 EWT(1)/T WR/GD-2
ACC NR: AP6009497 SOURCE CODE- UR/O 106/1,6 /000 /003/0026 /003Z
AUTHOR: -Kuznetsov, V. D.; Paramonov, V. K.
ORG: noae
TITLE: Radiator with a reflector supplied through a directional coupler
SOURCE: Elektrosvyaz', no. 3, 1966, 26-32
TOPIC TAGS: antenna, radio antenna, broadband antenna, UHF antenna
ABSTRACT: The radiator -reflector antenna element ensures good directional
pattern b%it has a narrow-band characteristic. To widen its band, insertion of a
suitable directional coupler between the radiator and reflector is suggested.
Formulak. are developed which determine the conditions (coupling factor,
characteristic impedances of the rods and feederE., etc.) under which such an
element possesses good directivity, good matching, and high efficiency.
Card 1/2 UDC: 621.396.677.81

L 39678-66
ACC NR: AP6009497
Experimental verification of the new formulas included measuring the TW factor,
efficiency, and front-to-back ratio of a 4-prong antenna system within a
300-800-Mc band. The experimental data was slightly better than estimated;
hence, the new formulas are recommended for rough estimation of such antenna
systems. Orig. art. has: 6 figures and 33 formulas.
SUB CODE: 09 / SUBM DATE: 090ct65 ORIG REF: 00 1
Card 2/2

ACC NR3 APO
1) /T Wa
SOURCE CODE:
AYJTHM: Kuznatsov, V. D ; ParamogM.,&
MG: none
TIM: Remodeling of tuned CoL)hfieal amys Into broadband antennas
SOMICE: Elektrosvyazt, no, 7# 1966, 17-24
TOPIC TAGS: phased ax-ray antenna, broadband antenna, antenna engineering
ABSTRACT: A tuned-reflector cophaBal array can
be re-conne,.-ted into an active-reflector
broadband antenna; the reflector 1B fed via
a directional coupler. The mothod of
connection of four tiers of radiating
elements ofa stacked antenna Is shown
%see Fig. 3) for (a) multiple-feed
array and (b) paired-feed array. A
model of #%"-type antenna w&B tested
at 36D-6D) Me; plots of ite traveling-
wave ratio, efficiency, and back-to-front ratio
vs. frequency are shown. A scheme fc:~ remodeling
a tuned cophasal array with a controllable
pattern is given. Four transmitting
directional
(b)
Fi 1. Multiple-feed array and
FW 2 .39 r7%,2.,2
'[00 10

Lt~.-- 4b
ri Mi
The-
ig - lm :t -an a PhL~Lsi
ont;6 ng- -

40 mw66 E il /i
WR

MANOWN.V.P., arkhitaktor; KABTA K.J., inzhener; ZYSX&N,G.Ya..
-~~ ~-,-4nzbawr
Plans for apartment houses designed ty GIPRMIS. Rate. i izobr.
predl. v stroi. no.102:10-14 155. (MM 8:10)
(Buildings. Prefabricated)

1. PAR64[ONOV, V. P. SOKOLOV. L. A. ENG.
2. ussR (6oo)
4. Building - Standards
7, Standard plans for small residential buildings designed by '3tate Institute for
Planning of Standard Industrial Constructiom Biul. stroi. tekh, 9 no. 24. 1952.
9. R~ontbly List of itussian Accessions, Lib-ary of Gongress, March 19,r). Unclassified.

087ROVSKIT, H.T990 arkbitektor; PARMDNDV,, V-F-, arkh-itektor; YUSOVv
S.A., arkbitektor;
.6.1
Standardisation at seconlary and &=IlIsa7 bulldings and
structures In aU brawhes of Industry. Prou.strol. 38
no.6:6-13 '60. W" 13:7)
(Factories-Design and construction)

PARANOROV, T.P., arkbitaktor; KLEBANOV, P.N., inshener.
Planning apartment houses with small apartments. Stret.pron. 35
no.4:17-20 Ap '57. (KL2A 10:3)
(Apartment houses)

FARAMNOV, V*S*
Increasing the service period of t1w lini of a cooling drum.
TSement 28 no.2:22 M-Ap 162. (MIRA 15:8)
1. Kosogorskiy metallurgicheskiy i tsementnyy zavod.
(Kilns.. Rotary-Cooling)

PARAT-MiN, V.S.
AOR rurcbino. no.?:311-36 J1
041R~,~ L-A'l)
(Loatlier Indus try-F/lizipment and aimpliaij)