SCIENTIFIC ABSTRACT AKSENOV, V. - AKSENOV, V.S.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000100720008-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 5, 2000
• Sequence Number: 8
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

AKSBNOV, V..# insh..
Electric lack for Tqagnetic starters* Stroitall no.6:15 Je '59.
(MIRA 12:9)
(Electric cutouts)

AKSINOV, V. , inzh.
Now cutting 'head for fininhipg moulded products. Stroitell no-1:13
Ja '59- (MIRA 12:3)
(Planing machines)

AKSENOVj, V.
......
Concerning the design of a controlling rectifier with consideration
of the effect of phase overlap. Elektrosviaz' 16 no.5:76 My 162,
(Electric current rectifiers) (MIM 13:5)

ZU41N, M.., Imnd.tekhnsnauk;-A-W_OV, V tekhnAuk;
. [Ake I onov., V. I., kand
HINIDZE I K. . gornyy Inzho; DUMOVN7Y,, S. , gornyy inzhe
Pay more attention to the extraction of building materials in the
,republic, Bud* mate i konstn I+ t6,1:9-33 JA-F 162. (MIPA 15:7)
(Ukraine-Quarries and quarrying)

AKS~NOVj V.., zerzhant
liblie teachingp I tra~no,.Starsb.-serzb. no,W4,45 Je '629
(Militax7 edueation)

S11 12/59/000/0 13/048/067
AOO2/AOO 1
Translation fromt Referativnyy zhurnal, Elektrotekhnika, 1959, No, 13, p..227-,
f 27797
AUTHOR Aksenov, V.A.
TITLE: "te Introduction of Holes in n-type Germanium
by a Pulse Method
PERIODICAL: Sb. statey nauohn. stud. o-va Mosk. energ. in-ta, 1957, No. 10,
pp, 12-20.
TEXT: A conventional pulse method of measuring the lifetime and mobilit
of charge carriers is discussed and an experimental apparatus is described.
Translator's note: This is the full translation of the original Russian
abstract.
Card 1/1

S/089/62/013/003/004/007
B102/B104
AUTJIORV~ Aksenov, Brodkin, E, B., Buahujov, A* V*, Pollk4rpov,
_ ___j
.V. r
139
TITLE: CS gamma radiation
PERIODIC~L: Atomhaya Pnergiyap v- 13p no. 3p 1962, 271-274
139-
TEXT: No detailed d*ta for the jamma radiation spectrum of Go being
availablb apart from--thoqe of Perkins and Xing (Nuol. Sol. and Engng.
VIIP 3P*1958), exact measurements were madep and some new lines discovered.,Z_
The isotope was separ"ed from the deoay.products of Xr and X contained in.-'
the gas channel of a r4search reactor by means of an aerosol filter. A.
acint~llatiod spectrometer was used for studying the y-spectrum, while
N
f(Tl) 'and CsI(Tl) crystals with IDJ-13 (FEU-13) photomultipliers were
al
used as detectors. The pulses from these were fed into a 100-channel
pulse-height analyzer. At E - 9.661 Mev (Cs137) the energy resolution wal_'.
9-5A and the non-linearity 1A. The background produced by the cs138
spectrui was measuredp giving results in good agreement with the data of'-'-'.
Strominger et al, (Rev* Mod. Phys. 30t no. 2j part 119 1958). The 08138
Card 1/2

KLINKOVSHTEYN, G.I., kand. tekhn. naukl; ALW.QY.,_
Vj.j, inzh.;
SA19MSIYANTS2 B.G.., inzh.,- SHUMOV, A.V., inzh.;
MANUSADZRYANTS, Zh.G., inzh.; TROSHINA, M.Ya., inzh.;
STETSYUKI L.S., inzh.j PARSHIN, M.A., inzh.; KARPINSKAYA,
I.M., inzh.; FALIKEVICH, B.S., doktor tekhn. nauk;
ILARIONOV, V.A., kand. tekhn. nauk; POLTEV, M.K.2 inzh.,-
KOGAN, E.I., inzh.; CHIGARKO, G.T., inzh.; KONONOVA, V.S.,
red.
[Traffic safety and safety measures in automotive transporta-
tion] Bezopasntst' dvizheniia i tekhnika bezopasnosti na av-
tomobillnom transporte. Moskva) Transport., 1964. 74 p.
(MIRA 18:1)
. institut avto-
1. Moscow. Gosudarstvennyy nauchno-issledovatellski-
mobillnogo transporta. 2. Moskovskiy avtomekhanicheskiy
institut (for Fallkevich). 3. Moskovskiy avtomobillno-
dorozhrjyy institut imeni Molotova. (for Ilarionov). 4. Vse-
soyuznyy zaoclmn politekhnicheskiy institut (for Poltev).

KrNKIN,--A.Te.; PONGHABDV, T.K., elaktromakhanik; AKSEROV, V.D.
Semiconductor converters for supplying on tug,
Avtom.. telem. i aviaz' 2 no.10:25-28 '58. (MIRA, 11:10)
1,Nachallnik laboratorii signalizateii i svyazi Yugo-Vostochnoy
dorogi (for Mynkin). 2*'Nachallnik otdala evyazi Tugo-Vostoohnoy
dorogi (for Aksenqv).
(Mleidtrio current converters)

NMIN, A-To,; GCHCHAROV,.T.X*, elektromekbanik; AEZUOV$, V.D.
Nodernizing low-piwer rectifiers. i~tom.telem* I eviazi
3 no*12:24-25 D 159' (XI 13:4)
1..Nacbo,l'nlk laboraltorli signalizatell avyazi Yugo-Vostochnoy
dorogi (for Nvnk;:i)*- 2. -Na6clialln:Lk otdela svyazi lugo-Vostochnoy
dorogi (for Aksenov).
Oclectric current rectifiers)

AESINOV, V.I., sturshiy inghener.
m twm~%WaNift
From the manory of the engineer in charge of the Novorossiyok electric
power plant. Xlektriohestvo~no.12:68-69 D 153. (MM 6:11)
L'Tekhotdel V/0 Voutoksagotserno. (Novorossiyok electric power plants)

i
I
z,, ~i-ri-ninirT. 11- 'I'd-tlic "
I . .

li7'1~ 6
109-1-13/M
AUTHOR: Aksenov, V.I.
TITILE: Determination of the Losses of Magneto-Dielectric Materials
at Ultrahigh Frequencies (K opredeleniyu poter' magnito-
dielektricheskilth materialov na sverkhvysokildi chastotakh)
PERIODICAL: Radiotekhnika i Elektronika, 1958, Vol.III, Vr 1,
PP-156-157 (USSR)
ABSTRACT: Formulae for the determination of the overall losses of
magneto-dielectric materials are given. The formulae are
valid for the case when the losses are low. If the losses
are determined e3j7perimentally by the short circuit test in
a measuring waveguide section, the resultant loss tanSents

are expressed b BE 1
( ), where parameters x and y are
determined by Eqs. ~) and (3); X and X are wavelengths
9 IZ
in the free space and in the waveguide respectively, X,p
is the critical wavelength for the waveguide, d is the
thickness of the measured sample, k is the standing wave
ratio, t is the distance between the surface of the
magneto-dielectric sample and the first minimum of the
C;)
standing wave. If the overall losses are to be determined
from an open circuit test, the loss tangents are also ex-
Card 1/2 r-

Determination of the Losses of I-Aagneto-Dielectric Materials at
Ultrahigh Frequencies
pressed by %(l) but parameters x -and y are given by
Eqs.(5) and ) respectively, The author expresses his
gratitude to Prof. L. A. Zhekulin for his valuable advice.
There are 2 English and 3 Russian references.
SUBMITTED: March 13, 1957
AITAIIABLE: Library of Congress
Card 2/2

SOV-109-3-4-1/28
AUTHOR: Aksenov, V. I.
TITLE: Scatterin-6-orElectromagnetid,Waves from Sinusoidal and
Trochoidal Surfaces having Finite Conductivity (0 rasseyanii
elektromagnitn,vkh valn na sinusoidal'nykh i trokhoidal'nvkh
poverkhnostyakh a konechnoy provodimostlyu)
PERIODICAL: Radiotekhnika i Blektronika, 1958, Vol 3, Nr 4,
pp 459-466 (USSR)
ABSTRACT: The scattering of electromagnetic waves from a limited
area of an irregular surface is considered. The surface is
assumed to be rectangular, and has dimensions d and X
For the purpose of analysis, the rectangular system of
co-ordinates x, y, z is chosen in such a manner that its
origin coincides with the centre of the "illuminated" area
and the axes x and y are parallel to the sides d and
A of.the.rect&ngle.The.-irr6gularity. of-the surface is described
by a periodic function z = Z(x) , having a period A . The
dimensions d and I are assumed to be much greater than
the wave length X of the incident radiation and d is
also greater than the periodicity A of the surface. It
is further assumed that the electrical properties of the
scattering surface can be described by a complex permea-
Card 1/5 bility ~L and a complex permittivity F_ *_ . The

SOV-109-3-4-1/28
Scattering of Blectromagnetic Waves from Sinusoidal and Trochoidal
Surfaces having Finite Conductivity.
incident wave _*pjnging on the surface is monochromatic and
its wave vector X lies in the plane xz The problem
0
consists of determining the scattered field at a point P
situated at a distance R from the origin of the co-
ordinates (see the figure on p 460). It is assumed that
R is comparatively large. The scattered field at a large
distanc:4'from the origin can be expressed by the complex
Kirchhof integral:
-JkR
J eA)po e 4
r _*JR1
trnl] - R, ~An e aS
47r R S Wo
where -8 the it vector of the internal normal-to the
surface; are the values of the field at the
Card 2/5

SOV-109-3-4-1/28
Scattering of Electromagnetic Waves from Sinusoidal and Trochoidal
Surfaces having Finite Conductivity
surface, ix +-jy -1-kZ(x) is a vector drawn from the
origin of the co-ordinates to a surface element dS;
R1 sin a -k cos a is a unit vector directed from the
Card 3/5
origin of the co-ordinates to point P . Integration of
Eq(l) is carried out over the whole "illuminated" area. If
the incident wave is vertically polarised, its field compon-
ents can be expressed by Eqs 5) from which it follows that
the solution of Eqkl) is in the form of Eq~6), where
f -7
p -I /1~, In a horizontally polarised incident wave,
V 7
having components expressed b~ Eq(7), the scattered field
is expressed by Eq48). Eqs(6 and ( ) are the basic ex-
pressionsfor the evaluation of the scattered fields. If
it is assumed that the scattering surface is described by
Z(x) =:-a cos Xx , where a is the "undulation" amplitude
and K - 2rj/A I the scattered field of a vertically polari-
sed wave is expressed by Eq410) where KX and P
and y are expressed by Bqr:k.(113 and (12i;12if is a
periodic function expressed by Eqkl3) which can be expanded

SOV-109-3-4-1/28
-Scattering of Electromagnetic Waves from Sinusoidal and Trochoidal
Surfaces having Finite Conductivity
into the Fourier series, as shown by Eq~14). The second
part of the integral in Eq(,10)can be expanded into a
Bessel function series as given by Eq(15) from which the
integral can be written in the form of Q16). The solution
of the integral is given by Eqkl8). For a horizontally
polarised wave, the periodic function of the integral of
Eq(8) ls represented by Eq419), whose solution is given by
Eq421). For a trochoidal surface which is described by
Eqs423), the scattered field from a vertically polariBed
wave is expressed by Eq(25). The solution of these is in
the form of Eq(28). A similar solution can be found for
a horizontally polarised incident wave; the periodic funct-
ion to be expanded into the Fourier series is in the form of
Eq.(28). The above theoretical formulep,, in particular, Eqs,
(17)? (21)$ (27) and (28) can be used to evaluate the
amplitudes of the scattered waves for the surfaces having a
finite conductivity., A numerical example of such a calcula-
tion is given for a sinusoidal surface having the following
Card 4/5

i. SOV-109-3-4-1/28
Scattering of Electromagnetic Waves from Sinusoidal and Trochoidal
Surfaces having Finite Conductivity
characteristic parameters: A/a ~ 10t AA =, 3.75 and
p = 0.2 +AO-65. The author expresses his deep gratitude
to Prof. L. A. Zhekulin for his constant attention and
help. There is 1 figure and 5 references, 1 of which is
English and 4 Soviet.
SUBMITTED: July 25, 195?
1. Electromagnetic waves--Scattering 2. Electromagnetic waves--Theory
3. Surfaces--Electrical properties 4. Functions--Applications
5. Kirchhof integrals--Applications 6. Fourier's Series--Applications
Card 5/5

5 W
AUTHORS: Kuznetsov, V. A., Akeenovs V. I.p SOV/20-128-4-35/65
Klevtsova, M. P. %
TITLE: Zero Charge Potentials of Tellurium-Thallium Alloys
PERIODICAL: Doklady Akademii nauk SSSR, 1959, Vol 128f Nr 4,
PP 763-766 (USSR)
ABSTRACT.~ The system Te-T1 was chQsen because the two components,
- according to data by S. Karpachev and A. Stromberg (Ref 1)
have very different zero charge potentials facillitating the
determination of the dependence of the zero charge potential
of an alloy on its composition. The zero charge.potentials
were determined by investigating the electrocapillary
properties of the liquid metals and alloys. The potential
of the capillary electrodes was referred to an electrode of
fused lead, the experimental temperatrxe was 4750. Figure 1
shows the electrocapillary curves of the two components and
their alloys. An addition of T1 (up to 25 atom%) to Te
lowers the maxima a max of the electrocapillary curves. At
a high content of Tl, a max increases again. Similar observa-
Card 1/3 tions were made by A. N. Frumkin and A. V. Gorodetskaya (Ref 4)
N

Zero Charge Potentials of Tellurium-Thallium Alloys SOV/20-128-4-35/65
on the electrocapillary curves of Hg and T1 amalgam. They
explained this phenomenon by the fact that the field of
the electric double layer influences the adsorption of the
alloying constituents in the surface film. Figure 2 shows
the dependence of the zero charge potential on the composi-
tion of the alloy. With an increasing content of Tl, the
zero charge potential shifts in the negative direction.
According to A. N. Frumkin, this is explained by a varying
charge of the T1 adsorbed on the surface film. E) 2 is
determined - the fraction of the surface film occupied by
particles of the second component (T1). From the equation
da ' - r dg, - 11 dli,;, ( r = Gibbs' surface density of
max 1 2 .. 1
Te, P = the same for -2*-1, chemical potentials for
2 IL1 I tL2 da
max
Te and TI), an equation is derived for P 0.
1 2 dA2
The activity of T1 was determined by measuring the el*ctro-,
motive force of the concentration chain Tl/eutectic mixture
LiCl +KC1 + 2% by weight of TlCl/alloy Tl-Te. The measure-
Card 2/3 ment results are given in table 1. Figure 3 shows the

Zero Charge Potentials of Tellurium-Thallium Alloys BOV/20-128-4-35/65
dbpendence of F(1) on the alloy composition. A: strong
2
deviation from Raoult's law is ascertained. This suggests
that the surface film consists of dipoles and is not mono-
molecular. Similar phenomena were observed for the Tl amalgam
by A. N. Frumkin and N. S. Polyanovskaya (Ref 6). Therefore,
the potential shift for mono- and bimolecular layers was
computed (Table 2), the assumption of a bimolecular layer
showing a better agreement with the experimental data. The
computation of ()2 confirms the assumption made by A. N. Frum-
kin (Ref 4) stating that the shift of the zero chargo
potential is directly proportional to the fraction of the
surface film occupied by the metal added. There are 3 figures,
2 tables, and 7 referencesq 6 of which are Soviet.
ASSOCIATION: Urallskiy gosudarstvennyy universitet im. A. M. Gor1kogo
(Ural State University imeni A. M. Gor'kiy)
PRESENTED: April 13, 1959, by A. N. Prumkin, Academician
SUBMITTED: March 5, 1959
Card 3/3

69919
S/109/60/005/05/007/021
X 2. q o o F-140/E435
AUTHOR: Aks2nov. V.1.
TITLE: Application of the Method of Variable Reactive Load to
Measure the Dielectric Properties of Materials
PERIODICAL: Radiotekhnika I elektronika, 19601"V'ol 5, Nr 5,
PP 771-781 (USSR)
ABSTRACT; The method employs impedance,eirele-diagrams to
determine the dielectric parameters of non-ferromagnetic
materials with medium and high losses. Nomographs are
given for rapid calculation.of the diqlectric parameters.
Acknowledgements are expressed to L.A.Zhekulin for his
interest in the work and to'K.P.Moiseyeva and
Yu.A.Aleksandrov for calculating the nomograms. There
are 9 f1gures, .2 tables.and 6 referencesq 3 of which are
Soviet, 2 English and 1 French.
SUBMITTED: JulY 30, 1959
Card 1/1

s/ioq/6l/oo6/oO3/0U1/0l8
r-,032/r.,314

-10 _,~Aksenov,

-.-App icat1oh:,of the~.Kirchhoff Approximation.to the
.
-.Scatte i f~'Elec.tromagn6tic Waves by Periodi ally'
c
r. n&:o 7
tneven'.3 rface- ithla--Finite Condu%.tivity
U 8 w
-1961, :voi. 6, 'No.-3,i
Uiekhiiiia~..i elektronika,

%
4
T" 35
_
i
` "I -io s
3T uthor used
; paper,.-(Ref.' 3)-th6 presenta
kk
E n a prev u

27. t he' K r

chhoff:appr*oxitfiation-to'discuss the scattering of.
lectromagnet'ic waves by A:finite portion;of a periodically
urface,-having, a.f were
uneven-s inite,conductivity. Solutions
ta-IT ' ' " 11* '
ob ied,-:Cor i a 1 sxi%-:Cgce which is periodically uneven in one
dirociion only;. ;,In the presentpaper, tlie the6ry is extended_ ~
ureace which"' is periodir, in two directions.
P-.'the-. case, of a. s
t
' ,
-an expression of them
e-.s
Th cattering sUrface,-is-given by
.
m z -assumed that the wave vector of
f or y)
,
the incident, plarxe; monochromatic wave and-the point of
observatioij, p ~,lie:,in.-,the plane xz At large distances
from,,.the scattering*'surf ace the field for:a surface periodic
Card.,.1/6-,

_7
21647
S/109/61/006/003/001/018
Appl-ication of......, E032/E314

L.4
P

T4 -,COqCt)j -
Pn, (sill (2)

n cos (T - a
j(COSO+P)(1-prksI ot' pW cos a) - pn' (1 M) X
Cos 0
___exp(jkj~(sInT+ III ot) + Z (cosr + cosot))) dS.
(I.+ P Cos 0) (CM 0 + A
(2y

band a are the angles of-
`lh tfidse expressions,
intid6nce and scattering -measured from the z-axis

I the relative complex magnetic and dielectric
And: e Are
J permeabilities of the scattering surface,
p
n arei the components- bf the -unit vector -n-
n n
X y z
:
it:
i
th
e un
s
the surfa.ces,,, k
~along the. inward-normal to
0
wave:vector of the incident.wave and cos E) = -(n
-
0
The.assumptions made in the,'derivation of the above two'

a
rd
C
3/6,
,

I:Ez
PF Off I., -

-
- , 'S,

Application of ....
(n ~2A,. JE gol must cover only the ionization
time of the valve 'T , i.e. be not less than 10 -6 Sec.
u
Thus, tU. > u (Figure 3, Curve a)
In the second case, due to operation of two valves,
successively with 60 0phase change the duration of the
upper part of the pulse should be greater than 600, i.e*
1
tv - + TU
u 6f
Card9/ll and the horizontal part of the pulse should not fall lower

sov/lo6-59-7-7/16
Control Accuracy Criteria of Ionic Rectifiers
than 1.2B go (Figure 3, Curve 4 ) . Also when the-pulse
Width is small, the grid of the valve is negative for a
large part of the t1me.and it suffers from ion bombardment.
Thus, the opt1mum pulae shape during the time anode current
flows is as shown in Figure 4 and:
tu I/mf see
The duration of the leading edge of the pulse can be found
frorp:
tCP SeC
2M S
op
The slope and duration of the tra iling edge are not
critical.
Card 10/11

S/194,/61/000/007/075/079
D201/D305
AUTHOR: Aksenov, V.N.
TITIZ: The relationship between the background noise level'-'
of broadcasting installations and the ripple of
their power supplies
PERIODICAL: Referativnvy zhurnal. Avtomatika i radioelektronika,
no. 7. 1961, 54, abstract 7 K365 (V sb. 100 let so
dnya rozhd. A.S. Popova, M., AN SSSR, 1960, 294-310)
TW.r: Design formulae are derived and given for determining the
allowable'ripple level (at the output of the smoothing filters) of
the anode and grid supply circuits, as depending on the allowable
background noise in the following cases: The stages of transmitters
with anode or grid modulation, intermediate HF-stages, modulated
signal amplification and LF. 4 references. Z-Abstracter's note:
Complete translatiou-7
Card Vl

fill
lot

AKSENOV Vladim ;-TZIWT%7KVj B.P., otv. red.; POVINOVI, Ye.5.1
red.; MARKOCH, K.G., tekhn. red.
[Rectifiers and transformer substations] Vypriamiteli i transforms-
tornye podstanteiis Moskva, Goo' izd-vo lit-ry po voprosam eviazi i
radio, 1961. 439 p, (MIRA 14t. 11)
(Electric substations) (Electric current rectifiers)
f,

7/003/005
B/jIo6/62/00()/W
P'lo,55/p,101
a. ystems
Itistage bro
in Mk, I I
noise 32 le 51.101Ate between
PIUVOI, 19622, 2B - redi-01 hips C) f tI-A
no. 7, urovnem f ona ti-OD5
'rTrjz Z,~eni 1181-OL Ltions Nil BSSR,
il a ne 7-11d" f PAJ~E
,Slel~trosvy" Bootnoanen hio naprya level 0 it iza. I or
4 the OV5 1 1,
VF -j0'D-ICXL' Ty. itavsllo level an Ive
'R P, Pop d noise - f the
his mo I tall P noise Zyicle n il a Ur Our' atiOns 0 tems.
Invnem Vail sa round, dn-JOI 'r0 the bac -PUI-Si -age Sis a
TEV Uro bacy-S let SO between f
tv I stem %11()0 t e-st systlext
~al ionships Ievel 0 sills, ta9p
u5troys deasting SbOrniy- rela tems and 'the OS 0 f or maltis d effeOt
ed t
ti-ie brOa )Itage ~' ) , led -the SU P 00111biDe , rms
IV deduc sting sis .1, were tne
onsh
supply author . a Vjjj4,c at t a giving
the dL brOadca 10 Ous 0
d no'
isteul 9
,9601, idell use thesO 6 duces aneL 6 bacl(gro f
d Of
tre most 104 i_ied to he de urces Of ai
3 app A
voltaSe, article te& so d, Vith
,Prpsen no correla atimatp vol toge
in the !more n Carl be. e 'noise
9 ,,ined SteLge bacMroxm
?or two 0
0 on the e tae re s"Itant
val'o Of --ationshIps
and card 1/3 Kbackgr 2 (3)
x-ces -
n
Card 0~~F~backgr K lackgI. i
4)
T'I -M
-P,
N

Background noise .....
8/106/6 2/000/00 7/003/005
A055/A101
In the above mentioned work, the coefficients Kbackgr i were determined as functims
of the pulsation coefficients of anode and grid voltages. No satisfactory method
exists as yet for calculating the dependence Of Kbackgr on the heating circuit con-
ditions, but experimental data are available for tungsten-cathode tubes, that per-
mit the determination of the coefficient of the background noise in the anode cir-
cuit -if the heating conditions are known. A table containing these data is repro-
duced in the article. The author deduces next a formula giving the resultant
Kbackgr in the case of a multistage 1-f amplifier. A numerical example - calcula-
tion of the resultant Kbackgr in the case of a three-stage modulator with tungsten
triodes is given at the end of the article. There are 1 figure and I table. 1000
SUBMI March 27, 1962
Card .3/3

122-57-8-17662
Translation ~.rom: Referativnyy zhurnal, Elektrotekhnika, 1957, Nr 8,
pp 255-256 (USSR)
AUTHOR: AksenQy. V. P.
TITIZ: On the Design of a Parallel Balanced DC Voltage Amplifier (K
raschetu parallellnogo balananogo usilitelya postoyannogo napryazhoniya)
PERIODICAL: Tr. Mosk. energ. in-ta (Transactions of the Moscow Power-
Engineering Institute), 1956, Nr 18, pp 344-358
ABSTRACT: Design f&rmulae are presented for determining anode currents in a
symmetrical.parallel balanced DC-amplification stage; the formulae allow
for variations in tube parameters and in load resistances of both halves
of the stage. Equations of the differential amplification factor and
the level-amplification factor are given; a numerical example of ampli-
fier design having 3 parallel balanced stages is presented.
A. A. S.
Card 1/1

AKSMOV., V. P,, Candidate of Tech Sol (diss) -- "Investigation of the assembly of
instruments for dynamic impulse testing of receiver amplifier tubesy Moscow, 1959.
16 pp (Min. Higher Edue uSSR, Moscow order of lonin Power Engineering Jnst)~ 150
copies (KL., No 22., 1959., 113)

77.
"The investi-rati o, of th tcc',~n.*,que o' t, m of
r ilnil-s!.- j~;A ----~n-7
,--:cc (Uncl concli4-1 onr o f' -a! O-l-lr--l-~--'--
-nf-- urown--c
"'min lil--F,-~er 'I-ducat-i--n T"'::i-ninn -111R. 17-eir Cyrder of
cl- -I! c st r .0 01" Df,
--jlF 1, iev, l'-, 34~
r, scitn", on for
'fechn--c-z~1 Sciences)
1.2tonis" 1~,.,O IP I~i,6)

_MWLZZU,Xg,n,l.telrhn.nauk; ORVINKHOVSKAYA, LA., in2h. -
4
Methods for substantiating paramater determination of open- .
pit mining equipment with continuoiis action. Ugall Ukr- 3 no.6*.
44 Je 159. (MIRA 12:11)
1. Kiyevskiy politekbuicbeskly institut (for Aknenov). 2. Ukrgipro-
shakht (for Orzhekhovokaya).
(Mining machinery)

AKSENOV, V.P., kand.tekhn.nauk; SBPFYTOROV, Yu.Z., inzh.
Fvaluating the effectiveness of opcn-pit mininF of the Stebnik deposit
of potassium salts. flauch. zap. Ukrniiproekta no.2:92-98 160.
(MIRA 15: 1)
(Ukraine--Potassium salts)

AKSENOV, V.P., kand.tekbn.nauk; MELINIK, N.A., inzh.
Establishing the optimum length of the front of an open pit when
usin.- conveyer haulage of the overturden. Nauch. zap. Ukrniiproekta
,.n�Artoq-1i7 16o. (Conveying machinery) (MIRA 15:1)

ZHERBIN, M.M.0 kand.takhn.nauk; NINIDZE, K.K., gornyy inzhener; AKSENOV,
v kand.takhn.nauk; DUKHOVNYY, S.D., gornyy inzhener
'Y_LL~
Urgent tasks in the field of open-pit mining.of mineral deposits
in the Ukraine. Ugoll Ukr. 5 no-11:30-33 N 161. (MIRA 14:11)
1. UkrNIIproyekt.
(Ukraine--Mines and mineral resources) (Strip mining)

AXSENOV-,V.-,P*,.kand-tckhn.nauk; TSIVnZV, V.A*, inzh.; BUDYKA, V.10) inzh.
". I , ~ - ~- --,
Analysis of the present state of and outlook for quarrying
building Materials in the Ukraine. Nauch.zap.Ukrniiproekta
z
no.5 s8l~-95 161. t- 04IRA .15,7i
(U~a:ine-!Quax-ries and quarrying)

AKSENGfV., V.P.., kand.takhn.nauk; NELINIK, N.A.,v.in-zh.
Establisbment of an.efficient annual rate of production in
manganese pits of the Nikopoll deposit. Nauch.zap.Inamll roekta
no*5:96-104 161. MU 1537)
(Nikopol I region-Strip, mining)
q-%,
I ,

ALSENOVY V. P,, kand. tekhn. nauk
Determining the weight characteristics of continuous mine
transportation equipment and efficient mine parameters in using
it. Sbor. trud. MISI no.39:285-287 161, (MIRA 16s4)
1. Gosudarstvennyy nauchno-issledovatelOskiy i proyektnyy
institut ugollnoy', rudnoy, neftyanoy i gazovoy promysb-
lennosti.
(Ukraine--Mine haulage)

AKSENOV V. P.$ kind. takhn. nauk; EZLYAKOV, Yu. I,,, kand. tekhn. nauk;
-:7:~~NENKOI A. A* , insh,
Continuous aotion equipcent oomplex for "n-pit mininge Ugoll
ukr. 6 no.10:22-25 0 162. (MIRA 15S10)
(Coal mining ma&inery) (Strip mining)

IVONINP Ivan Pavlovich; DAVYDOV, Viktor Viktorovich; ZORIN, Leonid
Fedorovich; IVANNIKOVp Ivan Andreyevich; AM
kand. tekhn. nauk y - ,
.. retsenzent; BY1010VSKAYA, S.N. p red.
izd-va; MAKSIMOVA, V.V.., tekhn. red.
[Open pit mining of native sulfur deposits] Otkrytaia raz-
rabotka mestorozbdenii samorodnoi sery. Moskvaj Gosgortekh-
izdat 1963. 303 p- (MIRA 17:1)
~Sulfur minos and mining) (Strip mining)

Z= kan&t6khnnauk; ERLYAKOV.
Yu.l,j, kand.tekbnnauk;
FBGWK, AcIlop inshe
ProMmato for using continuoue equipment in open pits of the
Uo$*SoRe Gor6zhure noe2slO-13~7 163. (MIRA 16s2)
1. GDsudarst7ennyy naucbno-issledovatel'skiy i proyektnyy insti-
tut ugollnoy,, rudnoy, neftyanoy i gasovoy promyshlennostip Kiyev.
(strip mining-Fiquipment and supplies)

RODIONOV, GRo, doktor tekhn,vaukl AXSENOV, VJe, kand,takhn,nauk;
nOWWVj V.H..* kand.tekb-n.-naa-;PROWUT, O.Y., insh.
Reomt traMs in developing highly efficient excavators and
loadw~% Cor.,zhur. no.2s" F 163. (MIU l6s2)
I* Gosudarstvennyy -quelmo-3seledoratel'skiy I. proyektnyy institut,
ugolluoy., rudnoy,, neftyanoy i gazovoy promynblentosti.. Kiyer (for
Prisedskiz),
tftearating machinery) (Mining machinery)

BUYANOV., Yuriy Dmitriyevich,, kand. tekhn. nauk; AVERCHENKOV,
Anatoliy Favlovich., gornyy inzh.; BESSMEMNYY, Konstantin
Sergeyevich, gornyy inzh.; AKSENOV, V.P., kand. tekhn.
nauk, retsenzent; BELYAKOV'x'TT."f"
tekhn. nauk.,
retsenzent; GEYMAN, L.M.., red.izd-4a;'LAVRENTIYEVA, L.G.p
tekhn. red.
[Sand, gravel, crushed stone and clay quarries] Peschano-
graviinye, shchebonocbnye i glinianye karlery. Moskva., Izd-
vo "Ne#W' -1964. 358 p. (MIRA 1713)

AKSWOV, V ~~_ kand. tekbn. naukl YMYAKOV, Yu.I., kand. tekbne nauk
Nine transportation equipment of continuous operation used
in strip mine construction. Shakht. stroi. 7 no.3t6-11 Hr'63
(KW 17 t7l
1. Gosudarstvennyy nauchno-issledovatellskiy i proyektnyy in-
stitut ugol',,,aoy.. rudnoyp neftyanoy i gazovoy promyshlennosti
UkrSSR,
ii.

AKSENOVI-Y.P.; ROZENPLENTER, A.E., kand. tekhn. naukg CHERNYAVSKIY, A.T.
Efficient correlation between the height of the top and bottom
scooping of rotary excavators. Met. i gornorud. prom. no.2:67-69
Mr-Ap 165. (MM 18:5)

LEPILKINV N.M.Y inzh.; AKSENOV V.P kand tekhn. nauk; KUKHARCHUX, N.N.,
inzh.; KABYSH, V.L., In-A.; ~?A IN, iu.K., inzh.
Method of laying out quarries for the quarrying of rock products.
Gor. zhur. no.6:53-55 Je 165. (MIRA 18:7)
1. Gosudarstvennyy nauchno-iseledovatellskiy i proyektnyy institut
ugollnoy, rudnoy, neftyanoy i gazovoy promyshlennosti UkrSSR, Kiyev.

L 39042-66 saT(i )/Ewp (e )/F:i."T (M)/T/Elvp
ACC NR: AR6022896 SOURCE CODE: Ua/oo81/66/OOO/OO5/IO12/IO12
AUTHOR: Aksonov, V. P.; Blinov, L. M.; Marin, V. P.; Polak, L. S.; ShchiDachovt V& So
rITLIE: PHF plasmatron and some possible areas of its application in chemistry
SOUR4 Ref. zh. Xhimiyal Part 1-1,, Abs- 51iOl
REF SOURCE9 Sb. Kinematika i termodinamika khim. reaktsiy v nitkotemperaturn. platmfjy
X., Vaukat 1965, 233-237
TOPIC TAGS: plasmatrong SHF, chemical synthesisp ionizing iPZd&ab.',an
ABSTMCT: It is shown that by using the ionizing effect of SHF radiation lonle can carry
out the following processes: synthesis of ammonia, recovery of nitrogen oxides from
air (in the production of nitric acid); synthesis of hydrochloric acid, hydrooyanic
i pro
acid; recovery of sulfur from hydrogen sulfide and flue gases; a~ro;~oum cracking1f
aration of acetyle 9~
rom methaneV production of alcohols; chlorination, nitration) hy-
droxylation., carboxylition reactions; synthesis of benzene, biphe7~., phenol; polymeri-
zation of ethylene into polyethylene;'~Xoreparation of pyroceramics;l,!preparation of ul-
trapure films and metals. A diagram of the pulsed SH97a-vice is given, and certain
characteristics of the SHF discharge are described. Results of measurements of the
temperatures and concentrations of electrons and ions in the SHF discharge and of pre-
liminary experiments on the formation of nitrogen oxides in the SEF plasmatron are
,given. G~tL-;-tTrahslati6a of abstract) F
07
~r " .1

r 1; 17738-63 EWT(1)/EWpLqj_/E-WT(M)jDD3 AFFTO/ASn D Pq_4 _)~M_
ACCESSION NRj AP3007174 S/0072/63/000/009/0015/00 6&
AUTHORi Lipchanskaya, R._V. (Enginser)l Aksenov, Ve S, (Engina~er)
TZ TILE aEff t of uniform heating rate on the therpolunineecen4~_si
of glass
15-16
TOP I C ~-TAGB_V7~g I-BB A-1 Wt
gift a a0 --the rmol Umines C 0--0- -----g
silicate
heating rateg Irradiated glas i00'
a
;~~jUS7-RAift -beirmoluminescence of a ceirium-containing.sLlic a
The _t t
gl'~ a 1-2 --B-- 0 ---J-9-412I~BpO 561K
a 6 0 2 4% Na'O
2
-Ws
5%* SbjO iiz~.i 07
-me'thod od -can-: a1d*-be~-_us*_
d formul I
curve -dav
Thi tit -eloo,
for glasewhich would not exhibit:thermoluaLueseence--a-ft-e'r-irrika-CA.
tion with hard-rays. Samp'les of the glass were Irradiated with
x-rays and then heated steadily to 350C at rates varying from 2 t~
5OC/min., A photomultiplier, a cathode follower, and a recording,,,
Card 1/j$

IT
ACCESSION NR4 AP3007174
potentiometer were used' Readings were taken at regular inter-
En-
vale and plotted as the glow curves shown In Fig. I of the
closure. It was concluded that heating rate significantly af
fects the thermolumineacence Intensity, the optimum rate being
20-30C/min. Orig. art. has: 1 figure.
ASSOCIATIONt Saratovskiy filial Institute stekla (Saratov Branchii
Institute of Glass)
SUBMITTEDi 00 DATE ACQ: 30Sep63 ENCL: 01
-SUB CODE: PH NO REF SOVs- 003 OTHERs 000
cara 2/14

9 1 - I . - -
I . - Fr - -.7- ; 7' W - . . -

,~k
O"ATION:
Cord 2/2

7~h , hYSENU)T V S n-.h.
iv., jwl v tar of
of the tPeed of urilrom heating UpOn th6 charfic
gl,s 20 nu.9~1 .5-16
~6)
c- .,jkil scinL.Ill ation of ker,,
sar--tollskiy filial Grjru-4p-rfj,.venrogv nauc"bnc,--~sr,.-3dOvatel'-
-kogo lristitllta atekla.