SCIENTIFIC ABSTRACT ARTYM, A. D. - ARTYNSKIY, V.M.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000102310001-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 6, 2000
• Sequence Number: 1
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

-
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a
4 ~ 4oftio.
doz. ~:5

9R,
iussg/ Electronics ModUators
1/1 Pub.---133
5/19
Authors iAr A Do, Candidate-of-Engineer,ing Sciences and Leaturer-at
thn, -
affln" tnCIMechnic Institute of Leningrad
Title INew method of suppressing dynatron-oscillitions 6enerated in
powerful.
moclulator-installa.ti,ons (in. radio tranarlission)
Periodical IVest. svyazi 1, 10 11, San 1955
Abs lie- hod of auppressIng ovoillationo.when instability develops in:
-desoribied-
radioJxansazitters . operiting -with -powerful dynatron tubes, is
The method.consists in -e~ncorporating an anti-dynatron tube.
Elperimtnts
werc conducted to dete 'm~ine the stability of various modulation
systoms
equipped with and witUtf,11A.an, anti _dynatroo tube. OscilIoV,-EIXW
nhow the
advantages . of the projx~sod method which-also resultv in an
increeso in pow-
er eccmouW and reduction in non-linear dilstortions in the grid
airouit of
the modulator tube. Circuit diagram; gropbs.
Institutions
Submitted%
_3090 MIN
z

ARTIM) A-* D
"A New Method of Phase Modulation.," Radio Te).h., no 1, p
53, 1955

ACC' N.Rt-K-17002610
AUTHORS; Artykov, T. U.; Avazmukhamedova, K.
ORG: none
tITLE'i On two mothoda for solving 11olmholtz md Poianon. equations
SOURCE: AN U:.,SSR. Institvt matematiki. Resheniye uravneniy
gidr6termodinamiki
primenitellno k zadacham meteorolopi (,',olution of equations in
hydrothermodynamics
applied to problems in meteorology) Tashkent, Izd-vo PAN VzSSR,
1966, 33-39
TOPIC TAGS; Poisson equation, weather forecasting, approximation,
atmospheric
goopotenti&l, weather map, matrix element
JMTWLCTi An experimental study of numerical weather forecasting is
made. The work
was done to reduce the errors cauaed by insufficient description of
physical processes:
by matherLatical equations &Ad by calculation errors. The method of
planes is used.
T'he matrix of the known right sides of the Helmholtz equation
OH ki P, oH
a W -7 ~(H, AH)-~ VX-11
is found. Its Qlements are
1F (H,. AH)jI +
I (
Then the method of straight lines with rospect to the variable y is
used. The ?

ACC NR. AT7002810
obtained system of ordinary differential equations for x is put in
canonical form
(o + -L) (P'+ -LL (A) Al.
dx~ 1,2
The influence-funotion method'is examined. A working fomula foz
the, Helmholtz and
?oisson equations is found as
;OH
b AD
I
wherc b are the weighting factors and n 45 is the number of points
within the
i
selected domain. The Jacobians in this formula are datermined. The
results obtained
show that the Helmholtz equation gives a better description of the
prOgftO3tiO fields.
Orig. art. has, 71ormulas, 2 maps, and 2 tables.
SUB CODE: 12j 04/ SUBM DATEs 26M&y661 ORIG REP. 005
Ccrd 2/2

ARTM A.D#, kozdidat te!+-4.cKajcikh nauk.
Theorr of grid Tl3kh.televid ;.io.6:50-71 155. (MMA 10:3)
r'
N.-lectron tubes)

ARIII/fe`ct~ro"nics - Transmitter modulation FD-2293
Card 1/1 Pub 9o-6/12
Author Artym, A. D., Active Member VNORiE
Title New Method of Phase Modulation
Periodical Radiotekhnika 10, 53-60, Jan 1955
Abstract The article,:which was delivered as a rcport in April
1954 6t a VNCRiE
conference, examines a new method of pbetse modulation based
on use of
nonlinear amplitude modulation. The method makes it possible
to obtain
increased (in essence, non-limited) phave deviations. A
mock-up exciter
with FM, the schematic of whose phase wcdulator is reproduced
in the
text, was used for experimental checkingand gave a phase
deviation of
-'- 5400. Diagrams, graphs. 3 referencets, all USSR.
Institution: All-Union Scientific and Technical Socitty of
Radio Engineering and
Electric Communications imeni A. S. Popcv (VNORiE)
Submitted July 12, 1954

USSR/Electronics - Frequency Modulation FD-2500
Card 1/1 Pub. 90-819
Author : Artym, A. D., Active Member, VNORiE
Title : Increasing the effectiveness of reactance tubes
Feriodical : Radiot~khnika, 10, 67-77, Jun 55
Abstract : A method of Increasing the effectiveress of reactance
tubes used in
broadcasting frequency modulation is described. It is shown that
increasing the effectiveness of a reactance tube also increases
the
stability of operation in the medium-frequency range. It is shown
that the effectiveness of the reactance tube is proportional to
its
suseeptance. Results are cited of e;~perimental verification done
with an FM exciter using a waster oscillator built around 6Zh4
tubes and calculated for 5.4 Mc. Graphs. Four USSR refe'rences.
Institution : All-Union Scientific and Technical Society of Radio
Engineering and
Electric Ccmmunications imeni A. Popov (VNORiE)
Submitted : March 25, 1955

ARTYX, A. D.
~ -, -, i
11
-, ~ "e - ;4~ Uv "^i
Merating frequency modulated oscillations and
transmitting
them through linear networka. Trudy LPI no.181:111-123
153*
(Radio frequency modulation) (XIIRA 10:1)

ART 1,2&; Glyn, T.D*
W. W~
Now method of suppressing dynAtron oscillAtions in powerful
modulators. Trudy LPI no.181:124-130 155* Oan 10:1)
(Radio frequency modulation)
1;- ;1.11,

A ID P - 4561
Radlotekhnika, 5, 35-43, MY 1956
Card 2/2 Pub. go - 4/8
references (1953).
institution : None
Submitted : Jl 30, 1955

A,,-D-, kwAidat tekhnichoakikh nauk, dotsent.
Protection of plate circuits of powerful radio
transmitters. Test.
aviatt 16 no.5:9-11 My 156. OajU 9:8)
1. Leningradskly polltekhnicheekly Institut imeni K.I.
Winina.
(Redio-Transmitters and transmission) (31setron tubes)

17/7
CIRCUITS
"Thyratron Circuit for Disconnectdn~ Hiph-Volta e DC
Circuits," by
A.D. Arty,,n. Elelctrosvyaz' No 7, July 1957, PI) 39-41
Analysis of a thyratron circuit used to disconnect high
volti_,-
anode circuits of output tubes of high-power radio
transmitters in
the caste of braakdown of one of these tubes. It is shown
that the
disconnect time can be quite short (uslially fractions of a
milli-
second), and that the MaXiLMM current d!irg,ng the
disconnecting pro-
cess is insignificant (for exawr)le, 20-340% hig:ier than
the maximina
Dermissible current under normal conditions). Ucing
thyratrons de-
signed for hundreds of amperes and for breakdoim voltages of
15 kv~
it is possible to disconnect the anode-circuit of
transmitter tubes
ivith a rating on the order of I mvgawatt or more.
Card 1/1 - 3 -

M156
ft-3 7-7 0
S/112/59/000/01.3/055/067
A002/AO01
Translation from: Referativnyy zhurnal, Elektr~tekhnika,
1959, No..13, p. 264,
# 28077
AWHOR: Artym, A.D.
TlTlEi The Application of Frequency and Phase Modulation for
Wansmitting
the Television Image Signal
PERIODICAL: Tekhn. televidenlya. M-vc, radioteklui. prom-sti
SSSR, 1957, No. 23,
pp. 3-35
TEXT: Methods of obtaining frequency modulation developed for
broad
casting are practically unsuitable for television, where
frequency deviation and/
the range of modulated frequencies are oonsid:wably greater.
The metk~od based
on the application of the phase modulation is an f!ffective
method of cbtaining
a frequeney modulatlon in which the stability of the mean
modulation frequency
is ensured. As a rule, phase moduleors make it yossible to
obta.n a relative-
!-, small modulation index and for ita increase, it. is
ne-sessary to perform a
frequency multiplication. The pliase modulation index
requirkid"b obtain a given
frequency modulation is many"times higher in televiaion than
in broadcasting.
Card 1/2

84156
S/1 12/59/000/U l,i/055/067
AO02/AO0A
The Application of Frequency and Phase Moduls~tion f or
Transmitting the Television
image Signal
Owing to this fact, the conventional methods of ratising the
phase modi;,lation
index are unsuitable. The author describes an efficient method of
freque=y
module-ion of the quartz stabil:ized carrier frequency by a
wideband television
signal. The metbod Is based on the division of the spectrum of
module.ted
frequeno.ios. The relatively low carrier frequenoy is
phase-modulated by a tele-
vision signal, whose spectrum Is limited by the frequency Fl,
whic~h is lower
than the carrier frequency Fo. After the multiplicaticn cf the
frequency P. by
n times, It :Ls addil~ionally phase-modulated by a television
s�gnal, whose spec-
trum extends from Fl to F2. In this case, the signal F2 ir, n
ti:P.Gs learger than
the signal Pl. By it similar method, with an inercase in number
of' additional
phase modulators, it Is possible to obtain the reqjuired index of
the frequency
modulation with a relatively wide televielon signed Bp&otrum. lbe
author dis-
cusses conditions of matching several. pha-se modulstcr.v used In
t,he described
method of obtaining frequency modulation, and wayd; of the
prantical realization
of different variants of the aforementioned methoi.. M.N.T.
Tran6lat'01"a note., This ia 'the full trans4lation c-f the
original Russian
Card 2/2 abst-ract.

AUTHOR:
1'embar of the SOV/Io8-13-8-6/12
4XLUI A. L'A-

1
Society
TITLE:
The Use of the Phase Auto.-Trimming of Frequency
(Primeneniya

fazovoy avtopodstroyki chastoty)
PERIODICAL:
Hadiotokhnika, 1950, Vol- 13# 11r Op PP- 37 - 46 (MI113H)
ABSTRACT:
The author investigatris cases of the use of phase nuto-trimming

of
frequency, as of a band of filter, of a froquency modulator

and of
a phase dotector. The following in shoun: 1) When the

difference
between the noise frequency and the tuning frequ)ncy

of the
generator to be stabilizei is -Rufficiently groat the PAT

(phase-auto trimming) system leads to an increase (if the sig-nai_

-to-noise ratio which is proportional to the damping of the volt-

age level of the difference frequency in the filter as well as

to
the ratio between the double difference frequenoy to the

half-width
of the band of frequency synchronism AD)
. 2) At

,
the passage of the frequency-modulated oscillt,tion through the

PAT
system distortions are formed. They are similar to those

of the
modulated low-frequency voltage In the equivalent schene.
Card 1/2
3) The PAT system can also be ured as a phase modulator which

The Use of the Phase Auto-Trimming of Frequency
SOV/108-13-8-6/12
0
secures a modulation index within the borders of up to-90 .
The
non-linoar distortions are practically completely daterminod.
by
the characteristion of the phase detector. The frequency
distortions of the modulating siGnal are characterized by the
equivalent dia6ram in the modulation- 4) When usinG the PAT
system as a frequency detector the non-linear diatortions are
determined by the modulation characteristics of the reactance
tube. The important advantaje of this frequency detector type
is its cimple control and tuning. There are 4 figures and 4
references, " of which -is Soviet.
SUBMITTED: November 15, 1957
1. n-equency--Control 2. Phasemod.ulation--Equipment
3. Frequency analyzers--Equipment
Card 2/2

MDD1P,L', M.; ATMYM, A.D.
Using countercoupling for suppression of cross
distortion In
miAticbannal high-frequehey amplifiers of single-band
transmitters.
Trudy LP1 no.1941.3-1) 1 58. (MIRA 11111)
(Radio, Shortvave-Transmittere and transmission)

9(8) SOV/112-59-2-3781
Translation from- Referativnyy zhurnal. Elektrotekhnika, 1959,
Nr 2, p Z23 (USSR)
AUTHOR: Artym, A. D,
TITLE: Equivalent Circuit of Auto-Anodic Modulation
(Ekvivalentnaya 9khema avtoanodnoy modulyatsii)
PERIODICAL: Tr. Leningr. politakhn. -in-ta, 1958, Nr 194.. pp
26-35
ABSTRACT: It is pointed out that fundamental premises and the
equivalent circuit
of auto-anodic modulation: a,.3 set forth by Kruglov
(Radiotekhnilca, 1954, Nr 4),
are not substantiated and that khe results of sollition of his
differential equation
are devoid of any prartical value. The following
ttre~presented and explained:
(1) an audio-frequency eq7aivalent circuit and its parameters;
(Z) a. complete
equivalent circuit and its energy relations. It is shown that
the auto-anodic
modulation circuit can be replaced by its energywise
equivalent, i. e . . by a
simple anodic modulation scheme whose modulator operates in
class A. The
advantages of the auto-anodic modulation ci:rcuit as compared
to claBs-A
Card 1/2

SOVI 112-59 -2-3781
Equivalent Circuit of Auto-Anodic Modulation
parallel simple anodic modulation are: (1) automatically changing
energy
consumption that ensures the most economical operation, and (Z)
reduction of
the number of tubes, thanks to the joint use of one tube as a
modulator and ars
an oscillator. Class-B simple anodic modulation is more
ecano'mical than
auto-anodic raodulation to that degree in which the class-B
modulator is more
economical I..-ian the class-A modulator; thiij advantage,
however, is difficult to
realize fully in practice. Bibliography! 2 items.
V. M. L.
Card Z/2

9(0) SOV/11,Z-59-5-9960
Tianslation from: Reforativnyy zhurnal. Elektrotekhnika, 1959, Nr 5,
p 219 (USSR)
AUTHOR: Art J) ,W*d Tamm, D. L.
,4- Y
TITLE'.,. Selecting the Transmitting System for Stereophonic Radio
Broadcasting
PERIODICAL: Tr. Leningr. politekhn. in-ta, 1958, Nr 194, pp 41-53
ABSTRACT: From a consideration of the requirements of a stereophonic
radio-
transmission system, the following fundamental principles of the
systeyn have
been drawn: (1) transmitting both stereo-sound channelb an be,
realized 4y
or.e radio transmitter having a subcarrier; (2) stereophonic
progri-._m
tra.nsmission can be realized by FM in themicrowave bwid by using
standard
transmitters; (3) transmission -channel signals can be formed by thxv
Crosby
sum-difference Tnethod. The AM-subcarrier system has been selerAed
for its
simpler two-channel modulation and particl;Llarly for its simpter
ch&nnel
dilitaion. in the receiver, witl-. an Fhi systetri, a better (by 7
db) anti-noise
featurc could be obtained only by considerable complication of the
receiver
Card 1/2

SOV/ 112-59 -5-9960
Salacting the Transmitting System for Stereophoidc Radio
Broadcaoting
circuit. Experimental testing of an AM master oscillator (a
block iicheme is
pr e a ented) showed good quality in both chann els with only
I I tubes and a simple
alignment. The channel frequency characteristics show that
the nonlinear
disto;,,tion factor in any of the channels is not higher than
1. 51o with m z 100010.
The backgrownd-noise level lies lower by -65 db than the
signal level at
m - IOG%. The experiments have proven th.-,t: (1) the above
t:ransmission-
signal principle permits easy division of the two char..nels;
(2) the maf3ter
oscillator and the transmitter can secure a high quality of
reproduction of the
program. Bibliography: 5 items.
'If. M. I
Ca-rd Z/2

86,'73
S111216010(*102110011001
A005/AOOI
Translation from: Referativniry zhurnal, ElektroteklLnika, 1960,
No, 21, p. 41,
f 6.17288
ALUHORt Artym, A.D,
TITIE- A N.?w Method for Generating Powerful. Pulses
PERIODICAL: Nauchno-tekhn. inform. byul. Leningil. politekhn. in-t,
1959, No. 5,
pp. 63-73
TEXT: The imperfections of the usual eleol-ron-tube modulators are
consider-
ed which are used in radar stations- the low pulce intensity on
account of which
a pulse transformer is needed which raises the price and
complicates the modulator;
the infavorable conditiona of de-ionization of tho thyratron
whic'.i lindt the pulse
recurrence frequency. A new method is proposed for generating
powerful pulses
(charging & capacitance and discharge through a ttqratron and small
inductance).
The circuit diagram is presented and its operation is described;
experimental
results are considered which corroborate the possIbility of
generati.nLi pulses of
prescribed duration Tp whereat the duration of th( current pulse
through the
Card 1/2

8677.3
S/112/60/OIDO/021/001/001
A New Method for Generating Powerful Pulses A005/AO01
thyratron is .-;;7, T and the pulse magnitude in a load
minus the losjes Is Cqual to
the break down voTtage of the thyratron, The application of
a charging choke and
the selection of capacitances make it possible to reduce a
few Umes the supply
source voltage at the same pulse magnitude in the load.
V,I,Sh,
Tranelator's note: This is the full translation of the
original Russian abstract.
Card 2/2

80) SOV/105-60-1.-12/25
AUTHORS: Artymo A.De. Candidate of Technical Sciences,
Bon;k-0Y-.W---'q-. Doctor of Technical Sciences
TITLEs Generating Damped High-frequ9noy Oscillations by Meano of
Controlled Ionic Overvoltage Arresteis
PERIODICAL: Blektricheetvo, 1960, Nr 1, PP 59-63 (USSR)
kBSTRACTi The principles for the generation of damped
oscillations in
eirouits with controlled ionic overvoltage arresters, the
deionization time of which is much longer than the period of the
generated oscillations, are shown hexe. Circuits of generators
and the optimum conditions of their parameters are investigated.
The latter warrant the maximaim output at a predetermined ourrent
impulse and the existing electric strength of the discharger. The
poaitive properties of controlled ionio ovorvoltage arresters
%'%res
tho ability of letting pass large impulse currents, the high
elootric strength and the negligi'ble voltage drop at the
electrodes during operation. This permits under otherwise equal
conditions to oommutate currents which are a multiple of those
obtained in valve oirouits. The i,)nic overtroltage arresters in
Gard 1/3 particular can achieve a strong effect at an impulse
excitation

Generating Damped High-frequency Oscillatiou3 b& SOV/10j-060-1-U/25
Means of Controlled Ionic Ovorvoltage Arreetare
of the damped oscillations. The sjmpj6a-~ wiring diagram of an
impulsa excitation 1!3 given ~.n -f_tLvkre I ~.n%; 3yj,,~,%iiud.
The basiz
problem consists In c,eatinp~ ~:uaditiolla ~independeat 01, the
frequency of tho gon 'urated oacillations) at which the voltage
at the discharger-anode rezaa:;us nagative auflfiuit~ntlv long,
whilst.the rate at which bhe poaitiv%: voittige inoreaseei, remalas
sufficiently small. The simploat circuit nohemc which warrants
those conditions is shown in figure 5. Th- shortaomings of
thie o1rouit saheme are the nacenjity of solacting a mueh higher
frequency of the discharger-ci;:cuit tbar, thu, of 'the generated
oscillations, as well as the neoeisity of maintaining the con-
dition 0 '>Q Based or. the general investi-gation mentioned
P
here it is shown that the shoxteonings can be elimInated con-
siderably. The circuit scheme shown in figure 5 :Lu proposed as
one of the posuiblo circuit variams for it alld O;LplaiAad. All
basic theses of the paper undar roview w6re c)ieck(kd on the
simula-
tors of the Induction heatf7i, - ins-,~&Ilation in the re3earoh
labora-
tories of the kan-,s of' tae Laiiingiad*kiy
Card 2/3 politekhnicheskiy institu,,1_,_-.u,; KaUaina (Leningrad
Folyteohnic.

Generating Damped High-frequenoy Oscillations by
SOV/105-6o-1-12/25
Means of Controlled Ionic Overvoltage Arresters
Institute Imeni Kalinin) and tM OKB elektroteriaioheakogo
oborudovaniya Lensovna hoza (qrperimental Desiirn,_Office for
the Electrothermal JEgui ment of the kenin r
P.- &_q~d
The results oblalned thereby ag.ree with the computed data.
There are 8 figures and 4 Soviet references.
SUBMITTED: December 24, 1958
Card 3/3

30141
S,1194161/000/007,/07,1/b79
D.201/1)305
AUTHORS: Artym, A.D., Gomoyunov, K.K. and Kozhevn:LL-ov, A.N.
TITLE: A shift-pulse reactance generator with a thyratron
comutator
PERIODICAL: ReferativrWy zhurnal. Avtotantika i
radioe:Lektronika,
no. 7, 1961, 33, abstract 7 K195 (Nauchno.-tokhn.
infom. byul. Leningr. pol:Ltekhn. in-t, 1960, no,
3-12)
TEXT: Theoretical and experimental an.alysis has beerL made of a
circuit generating shift current pulses of magnetic elements.
The-
circuit consists of a capacitor C charged through a diode and an
inductance Ll from a d.c. source, the resonant frequency of the
cir-
6utt fomed ~by Ll and C being equal to the- shift pulse
repetition
frequency. C discharges through an inductance L, . connected in
ser
ice with the discharge thyratron and the load, t?e resonant
frequen:
cy of the L2-C circuit being determined by the required duration
of
C ard 1/2

30341
S/194Z61/000/007,/0711(079
A shift-pulse reactance generator... D201/L)305
the shift pulse. Special circuit is used for stabilizing the load
current within very wide limits. The circuit sh,,,jnts Ll when C
charges to a pre-determined value of voltage. The experiment has
proved the correctness of basic assumptions obtained in the
thegret-
ical analysis of the circuit. 4 references . Z Abstractex's note;
Complete translation2
Card 2/2

24848 3/106/60/OOCV004/003/007
A055/A133
7
AUMOR.- Artym, A. D.'
TITLE: Use of norminimum-phase c1rcuits in sane systems with
php.se can-
versions
PERIODICAL: Faektrosvyazt, no. 4, 196o,.14 - 2o
TEXT: The author examines several practical nonminimum-phase
circuits and,
in particular, the circuits suitable for wideband -ahaseshifters
ane. for phase
control or phase modulation. A "classical" exampl,~ of *a
norLminimum-rhase four.;
polesection is given, where- .0
zXzy R (1)
R being the load resistance., The transmission coefficient of
the circuit ii:
V(Z ZY
ZY R, ZY R
(2%
J.
+ 1~71-! -- I I + -'Y
+ + R
ZY R ZY R
Card 1/ 7

24848
S/106/60/000/004/003/007
Use of noriminimum-phase circuits in some...' A055/Al33
1
if Zx is iwL and ZY is TIC and if, according to (1)p R we havo-
R Z= 1-1l~CR (3)
+ I CR
The modulus of K is equal to one for all frequencies, and the phase
(varying
from 0 to 7:.,) is determined 15y the relation;
wL
arg K - 2 are. tg are tg w CR. (4)
One of the practical defects of sucha circuit is the presence of
irductrnces.-'
If Zx and Zy represent moi-e complicated reactances satisfying
condition (1), the:
amplitude characteristic will not ch&nge, but the phase vailations
will bo equal
to nl~ where n is the number of zeros or poles in or Z - Thus if Z.
consists
of parallel connected L and C (i.e. has zeros at frequencles 0 and-Y)
eaid Z Y con-
sists of serias connected L -and C (i.e. has poles ut these
frequencies) the oon-
dition (1) is satisfied if~:L R and, according to (2):..
C,-:,Yi 2/7

24843 ..3/106/60/COO/004/00-VO07
Use of nonminimum-phave circuits in some... A05.VA133
11K
ZY
+ 1+ 1
Z'
WO
where Ft
wo C
N LC
whereas the phase is:
2 arc,t,, W (8)
w w0
With increasing frequency, the phase.varies from 1) (for w 0)
to 2 7c (f~r W.0,,-),
its value being JT for w - wo. In the majority of practical
cases, the input and
output circuits must have a grounded point, owing to whibh a
transformer mist be
added to such circuits. To avoid the use of tran:-,formers, it
is expedient to
Card 3/1

2).30
Use of nonminimum-phase circuits in some ...
S/106/60/000/,DO4/00-1/007
A055/A133
choose circuits equivalent to crossed circuits. Iffien the
presence of a trans-
former is admissible, the circuit shoim in Fig. !5 can, for
instance, be used.
Application to v)ide-band phase shifters. - The ei:.-Ouit of
Fig. 5 can be used.as
the basic element of the wide-band phase shifter, i,e. as its
section passing ali
frequencies. If capacitance Ca. is used as the rimptance between
grid and anode
of the tube, the equivalent circuit will be that of Fig. 6.
Comparing this cir-
cuit with that of Fig. 5, wd find:
Z1 n w it .
i%'Cac' Z3
Z2 - Ra is - according to (12) - equal to Ra - A(-: so where S
is the steepness
of the tqbe. To reduce the circuit's sensitivity to variations
of tube-parameters
Ri and'a, it is expedient to provide .'negative current-feedback
by insert-ing ihto
the tube's cathode circuit a resistance not shuntod by a
capacitance. In this
case, the equivalent internal resitance of the t-.tbe becomes
11jeq - Ri (1+SRk) -
Usually it is possible to choose Rk so that SRk 5~- I., Then
Rioq --' P-18Rk Rk;
R aga
a :--NRk, and
Card 4/7

S/106/60/000/00VOOMW
Use of nonminimum-phase circuits in some... A055/A133
:A
I- I CarRI, I wCac Rr + 1 - I W c6'. (R, -I-
1+ +
I'd CaeRt, (R, + 1 C., -SO
S
If the capacitance of the output circuit is taken into account,
the modulus of K
becomes frequency-dependent. However, when the phase shifter is
intended to ope-
rate in the af-range, the influence of Cp can be neglected.
'rhe circuits of the
examined type have a certain.defect because of-the inconstancy
of the input im-
pedance, whiQh is very large at low frequencies and
comparatVely small at Kigh
frequencies, where it is nearing 1/2(Rk + I/S). To remove thLs
defeat ', it ii ap-
propriate to increase the input impedance of the circuit by
Increasing Rk,
to reduce the exciting circult impedance by using cathode
foLLowers. Applicak.1011
to phase contror circuits and to phase modulato~rs. - In the
circuits exdmined
above, the phase varies with the parameter, but the modulus
o:~" the transmission
coefficient remains constant. This property can obviously be
made use of in p1TW
control or in phase modulation of voltage at a gLven constant
frequency. The
Card 5/7*

S/1()6/60/000/004/003/007
Use of nonminimum-phase circuits in some... A05-5/A133
easiest solution is to choose as variable parame,~-Ier the variable
resistance R
.(rather than L or C). This variable resistance oan, for instance,
be the output
resistance of the grid modulated tube. In the case of Fig. .5, it is
convenient
that Z2 and Z31 should be capacitive, Then Z, rmist be a pure
resistance (vaxi-
able resistance. The input capacitance of the noxt stage cma be used
as C2. For
phase control or for pha;e modulation, it is con,renient to
c).-I'oose the circuit
shown in Fig. 11, where the variable resistance Ill is the output
resistance of
the cathode follower, varA-ig (depending on the cittoff
grid-voltage) from about
1/8 to aboih Rk (S being the steepness of the tul)l_!and*Rk the
cathode load;
Rk >> 11S)- Since, in this case, Zl - Rl, Z3 -ij;6 3 , we obtain:
2 are tg(nwC3Rl), (19)
where n is the transformation ratio between halvits of transformer
secondary.* In
th
.L e ideal case, Nhen the resistance varies from -0 too'-, the phase
varies from 0
to -,c. In other words, the maximum possible phaso modulation is
*7V2. There are
11 figures ani .5 references: 2 Soviet-bloc and 3 nori-Soliet-bloc.
The refererideb
to English-l&nguage publications read as follows:: Darlington.
"Realization of a
constant phase difference". BSTJ, v. 29, no. 1, :1954; Dome.
"Wideband phase
C ard 6/7

2-4848 S/106/60/000/004/003/0Cq'
Use of noraninimum-phase circuits in bome... A055^133
shift networks".' Electronics Dec. 1946; Weaver,, "Design of RC
widebeind 90!de!-
gree phase difference networ;~. Proc. IRE, v. 42, no. 4,,1954.
[Abstractert-s
note- Subscript lleqll (ecfaivalent) is the translatl.on of
SM=ED; january 6, 1960
Fig. 5. Fig. 6. Fig. :1.0~
z Us.
C.- Pl.
Zt
zt Ul Us
-A
Z3 4EQ
I EIZ3 Fig. 11. Uwmod
Card 7/7

ARTYM _Dmitriyevicli; MODEL'., A.Z., red.; SOBOL-EVA,
Ye.M., tel6hn.
j_AWmqliy
red,
(Theory and me#ods of frequency riodulation] Teorila
i metody
chastotnoi moduliataii, Moskva, Goo. cinerg. izd-vc.,
1961,9)w P.
NnA 24
(Radio frequency modulation)

,.A"ARTYMP A.Ds
Methodo for ou-rying out linear frequency modulation of
qwwts
oociUators, ElektrooviAzi 15 no.'i's23-29 n 161. (KM& UtO
(Oscillatorap CryBULI) (MDdulit,tion (Bleotronica))

33699
S11C61621000100210051010
A055/A 10 1
AUTHORS: Artym, A. D.!--t VZO)t V. V. .
TITLE: Frequency modulation of crystal oscillators
PERIODICAL: Ble ktrosvyazl, no. 2, 196P, 32 - 35
TEXT: This article concerns the methods of frequency modulation by
means
of direct action upon the frequency stabilizing et.ement, i.e.*;he
crystal. Only
one of such methods is (according to the-authors) used to-day for
high-quality
broadcasting. There are other methods which provad-to be simpler and
more effi-
cient. One of such methods is described in the p:!esent article.
Instead of the
usual circuit (Fig. 1a), the authors use the equi,rhlent circuit
ofFig. 1b, which
shows that the "superf luous" element in their prc,;)1em is C I. The
effect uf C I
can be compensated appreciably with the aid of Lcl, (Fig_2a~, tuned
with C'.1 toothe
mean oscillating frequency &)0. The capacitanc.e C.M. of the tube
part of the
system, Including the mean vaWe of the controlled capacitance Ccontrl
is compen-
sated by Lose, I.e.: 1 1 (1)
M0,870 ~ V-Los-ccosc
Card 1/

33699
S1 I C616 Pt,"0100210055-1010
Frequency modulation of crystal oscillators A055,/AlOl
Tha nonlinear distortions, conditioned by the difference of the
examined system
(Fig. ?a) from the antirezonance circuit (Fig. are given by
Kf _(4Tn)_2 - -
2u~ (2)
where &qm is the frequency deviation amplitude ' (41 and W, are,
respectively, the
crystal antiresonance and resonance frequency. Tge authors
reproduce the diagram
of their modulated crystal oscillator (Fig. 3)i -The parameters
of the chosen
crystal arej Co - 17.5 Pf, C, - 0.022 pf, L, - (~.Oql h, R, n
12ohms, f2 - 3.56
Me/s. , The nearest sphrious resonant frequency 04: the crystal
is removed by 36 kc/s
from :the fundamental one. Owing to the dependenc;.e ofthe
voltage across the 4K-
resistance upon the modulatirg voltage, the diodeis are
unblocked for a time equal
to a more or less considerable fraction of the period of the h-f
oscillations,
which causes a corresponding variation in the maittive component
of the conductance
(300 pf-capacitance in the circuit of the diodeit and of ~;he
crystal). The
equivalent reactive component of the modulated cupacitance
remains practically un-
changed at considerable variations of the diode parameters. The
described reac-
tive modulator Is therefore highly stable. The !.nductance i:.i
the anode circuit
Card al "3

33699
8/106/62/000/002/005/010
Frequency modulation of crystal oscillators .-~05~/AlOl
of the first tube plays the part of Lose of Fig. 2;!t. With the
aid Pf the parallel-
connectbd variable cappcitanoe, the -system i'3 --tu'hef~i s'b"
, 'that,' at thd mediu!m 'ue
of the controlled reactance and the crystal beifig"pulle 'the-
'AY~k
d out, freque y-.f,the
oscillations is about equal to the carrier frequen.:iy. The
inductance in the crys-
tal circuit (L; in Fig. 2a) is tuned to resonance with the
crystal capacitance
(CIO) (with the aid of the series -connected variabla
capacitor). The second stage
ensures the suppression -of spuilous frequencies. ::Iome
experimental results are
added. There are 4 figures, and 7 references: 5 Soviet-bloc and
2 non-Sovi et -bloc.
The references to the Englirh-language publication;ii read as.
follows,: Mortley.
FMQ. Wireless 'World, 1951, 57. Mortley. Frequency -modulated
quartz oscillators
for broadcasting equipment. Proc. IEE., 1957, v. 1.04, no. 15.
The Soviet authors
or scientists mentioned in the artigle are: M. G. Margolin, F.
V. Nushnir and I.
A. Shidlovskiy.
SUBMITTED: January 3, 1961
Figure 1. b~)
Card 3/1

AWN.M, A.D.
iI
Definition of an active electrical ne,tvorko
Radiotekbnika 20 no#7976'
ii 165, (MIRA 1818)

3 -g ~rj 1: 1
Artym,Anatoliy Dmitriyevich
Electric adjusting circuits and amplificr:ii; theory and design
(Elektricheakiye korrektiruyushchiyc.ts-!.,pi if4siliteli;
teoriya i
;; , ,, 418 P. illus.'
proyektirovanye),moscow, Izd-vo 4'Energlya 19)5.
biblio. .9000-ccipiea printed.
TOPIC TAGS: electronic amplifiez-, clectmnic circuit, ra~.io
communication
syst~em, radio engineering, negative feedback, frequency
conversion
PURPOSE AND COVERAGE: This book is inten(!~ed for scientific and
technical
personnel concerned with'the planning a"nd develo;ment of radio-
communication systems and equipment,puliie technique,automatic
con-
trol,etc.; it may also be used by aspirants and students in
advanced
courses at radio-engineering schools of higher education. The
book discusses methods ofanalyzing and synthesizing stabl4! linear
electric circuits of the active and pasiiive type, as well as the
the-
orems pertaining to the link between the real and imaginary-com-
ponents of the circuit function. Examples are presented, and
solutions are given for a series of pra(:tical problems connected
with
the planning of electrical systems pocedissing optimal
characteriLtics.
The general theory of multicta4a amplif-,Iiers with an absolutely
stable
UDC: 62k,_3T3;.+--.62l.3T5-139

SaNEVAM MOM"
ACC NRi
negative feedba;k in pres-anted.
TABLE~OF CONTENTS*.
3
Ch...I. Methods of Analyzing Electric Circuits With
~umpedj?&"r'&m-,.,
6ters -- ~
1. Elec'tric cirnuit components -- 9
.2. Differential equations of-e1ectric circuits -- 12
.3. Complex-frequency method- 13
.4. Properties of-linear circuits
5.~Prop6rties.of functions of linear circuits with lumped param-
eters -_ 29.
6. Stability.and physical fe'asibility -- 33
7. Transients in linear circuits 315
Ch.II. Properties of Two-Terminal Networka _- 42
'l,'. Some general*properties of the input-Injection function.-. 42

ACC NR, Am6olo603
2. Concept of energy function3 -- 44
3. Input injection 'of a minimally active type --
4. Input injections of act ive two-terminal networka -- 50
5. Inpitt injections of a minimallly reactive type -- 55
6.. Properties of two-terminal networks wilohout looses __ 6L)
7o Determination of the function of a two-termina:L network on the
basis of one of its components __67
8. Realization of functions.satisfyl:n6 th* conditi,onn of physical
feasibility __ 74
-Problem*a of the Planning of Two-Teirminal. Yetworks -- 82
1. Reverse circuits -- 82
2o*Synthesis of two-terminal, networks without loss.es -- 85
3. Distinguishing features of minimally resistive and minimally
reaciuirc
types of circuits -100
4. Synthesis of'two-terminal net-work's winh losses -- 107
5o Auxiliary two-terminal networks 11:1
6 Equivalent two-terminal networks 120
Ch.IV. Four-Terminal Networks -- 131
Cord

ACC NR3 Am6olo603
1. Parameters of four-terminal networks -- 131
2. Measures for a four-termi~al-network transmission -- 140
3.; Realization-of a four-terminal-network transmission
function in th
form of a lattice circuit -- 146
4. Mi'nimum attenuation and minimum phase circuits 151
5. Auxiliary four-terminal networks -- 3.56
6. Four-term'inal networks equivalent to lattice circuits --
159
T. Determination of transmission impedance on the basis of one
of its
components -- 170
Ch.V, Use '-of "Nonminimum-Phase" Circuits 174
l.' Functions of "nonmiminum-phase" circuits -- 179
.2. Types of "nonminimum-phase" circuits -- 179
3. "Nonminimum-phase" properties of an amplifying tube cascade
186
4. Linearization of phase-frequency characteriatice~by means of
of nonminimum-phase" circuits -- 193
5. Delay circuits with linear phaae-frequency characteristics
-- 202
6. Wideband frequency discriminators -- 211
7. Phase shifting circuits and phase mo4ulatore 229
Ch.VI. Frequency Conversions and Their Application 231

ACC NRI AM601o603
1. Frequency normalization 231
2. Calculation of losses in circuit components by menns of
frequencY
conyqrsion -- 236
3. Conversion of a 1-f circuit into h-f and passband circuits
-- 242
4. Transients in pasoband circuits -- 251
5. Analysis of transients in pasuband cl.rcuits -- 262
6. Link between a transient in a 1-f ci:t*cuit'and the
envelope in a
passband circuit obtained through fr-i.-quency conversion --
279
7, Synthesis of a pasaband circuit basei'i on a given envelope
of its
oscillations -- 289
Ch.VII. Theorems on the Connection Betwe,iin the Real and
Imaginary
Components of a Function and Their Application -- 308
1. Generalized function of a circuit and the limitations
imposed upon
it -- 308
2. Integral of a real component of the Tunction of a circuit
314
3. Optimum matching of a power amplifier with an active load
319
4. Phase dependence of a given f.requenc-.1, on the
attenuation given
in the entire frequency spectrum -- 141
Card

ACC NRI AM6010603
5. Graphoanalytical method of determining the phase-frequency
charac-1
teristic on the basis of a given ampl,itude.;frequency charac-
teristic -- 351
6. Attenuation dependence on the phase given in the entire
frequency
spectrum -- 360
T. Integral bond between attenuation and phase gi-iren in different
frequency bands -- 368
8. Optimum correcting circuits of videband amplifiers -- 377
Ch.VIII.Planning of Negative Feedback Amplifiers 392
1. General considerations --- 392
2. Optimum characteristics of the feedbvick loop 394
3. Maximal poisible feedback depth _- 401
4. Effect of amplifier tubes and number of stages -- 40T
Bibliography 415
SUB CODE: 09 SUBM DATRt 16 Oct 65 ORIG- REX:.032 OTH REF: 005
6 6

28 222
S/019 61/1000/005/063/0-78
(41t4 Ap"3101) D201YD303
-AUTHOR- _~jtym. D.
TITLE- Increasing the precision of the equation of fre-,
quency modulated oscillations
PERIODICAL: Referativnyy zhurnal, Avtomatika. i
radioelektronika,
no. 5, 1961, 9, abstract. 5 167 (Nauchno tekhn, in-
form, byul. Leningr. politeklin, in-t, 1960, no. 3.
84-93)
TEXT: More precise -solutions
the F11 oscillations. These
carrying out the exact analysis
quency is so great that it
by which the frequency is being
make it possible on the one
operation and consequently
the limits of applicability
Card 1/2
(P.) are given for the equation of
solutions arp required either when
or when the ratio of chzw4re of fre-
becomes necessary to consider the p.~occss
set up. The more precise solutions
hand to correct for the non-stationary
to determine the criteria determining
of this operation. On the other hand,

28 222
S/191t/61/000/005/063/0118
Increasing the precision... D201./U303
they permit the establishment of a stabiLity criterium with
the aim
of avoiding the danger of inducing paramatric oscillations.
The
solutions are found in the first, secon6i, third and fourth
approxi-
mations both for the particular case of a harmonic
modulating sig--
nal and for the general case of a harmonLc function which
may be
represented by the Fourier series., Thc Eirst approximation
of r,
of the M-1 equation is the quasi -stationvvy solution, From
the
second approximation the AN depth which i.s associated to
nl is
determined. The P in the third approximation permits
evalilatiorL
of the amount of linear distortions in F~f and the fourth -
tk-~at of
-.linear distortions- The more exact solution of the Mathieu
non
equation makes it possible to analyze the problem of
stabiLity and
to determine its corresponding criteria, 3 figures. 3
references..
/-Abstracter's note: Complete translaticn_,/
LX
Card 212-

HORYGANOV, P.V.; ARM, M.I.
-
Thermodynanic Investigation of the ci~llulosn fiber dvaing
process using vat dress Izvevysoucheib.zav.; takh.teksteprome
no.2:125-113 '59. (MIRA 12:6)
1. Ivanovekly khlmlko-tekhnologichee.lciy Institut.
(Dyes aW dyeing-uhemistry)

ARTrM. M.I.; 14DRYOANDV, P.V.
Kinetic investigation of dyeing cellulooo fibers
with vat dyea.
Izv.vys.ucheb.zav.; takh.luaket.prom. ut).6:107-113
159.
(MM 13:4)
1. Ivanovskiy khimiko-takhnologicheakiy institut.
(4,e6 and dyeing-Cellulooe)

ARTPI, M.I.; MORYGANOVI P.V.
Relationship between the structure and iiffiLI-ty
of vat dyes.
Izv.vys.ucheb.zav.; tekh.~okst.prom. noj:110-116
161.
(MM 14 - 7)
1. Ivanovskiy khimiko-tekhnologiclieskilr instittit.
(Dyes and dyeing--Toxtile fibers)

ARTIMp M.I.A MORlGANUV,, P.V.; KORO .0 A.N.
Irl
Investigating the migration of the louco-compounds of vat
dyes*
Izvovys.uchebosave; tokhoteksteprome no.l:nO-n7 163. (MIU
16:4)
1. Ivanovskiy khimtko-tekhnologicheiz'kiy institute
(Dyes and dyeitig-Textile fibers)
I
I

th&
',')u Maglli h- ir
n,
8,
lvanovsk-y

56-58.2-17/23
AUTHORS: Fastovskiy, V.G., Doctor of Technical SCM~iices,
T,, Engineer and Rovinskiy, A.Ye., Candidate of
_ArtYm, A.,
TecKi-cal Sciences
TITLE: The Boiling of Freon-11, Methylene Chloride and Benzene on
a Horizontal Tube (Kipeniye freona-11, kh1oristogo metilena
i benzola na gorizontallnoy trit'De)
PERIODICAL: Teploenergetika, 1958, . , No 2, pp- 80 (USSR)
ABSTRACT; The boiling equipment for cliese tests, which ig illus-
tratod in Fig.1, consisted of a steel tube 170 mm diameter and
280 mm long, closed at the ends and. enclosing a thick-walled,
Gcrman-silver tube 8 mm diameter and 200 nun long, heated by
electric current. The evaporated vapour was condensed and
ret'urned to the main tube, The thei7mal loading of the heating
lurface was determined from the ele(Itrical power consumed;
temperatures were measured by therm~)couples at appropriate places.
The substances tested were chemical'.'y pure methylene chloride
and nominally pure Freon-11 and benaene. Measurements of the
boiling points of these liquids at !itmospheric pressure showed
that the Freon-11 and benzene were also coikoaratively pure. At
the start of tests, the liquid was boiled for some hours to
remove gases from it and the equipmont. The heating tube surface
became contaminated and was cleaned from time to time.
Card 1/3

96-58-2-17/23
T1'e Boiling of Freon-11, Methylene Chloride and Benzene on a
Horizontal Tube
In the region of well-developed boiling, the experimental data
are co~rrectly represented by the eqi:iation:
a = Aqn
which is valid when q is greater than 6 020 kcal/m 2hour for
CC13F and q is Sreater than 12 000 kcal/m hour for CJ12C12
and C6H6. The values of the constants in this formula are
tabulated. The experimental results are also plotted in Fig.2,
which clearly indicates the conniencement of bubble formation.
The test results in term6 of the criterial3elationship of
Kruzhilin are graphed in Yig.3. It is noticeable that although
the physical properties of Freon-11 do not differ much from those
of the other liquids used, yet its heat-transfer coefficients cn
boiling are much hiGher at the same thermal loads. The article
then discusses bubble formation duri.ng different phases of
boiling and relates the results to the work of other authors.
There are 3 figures and 11 references, 4 of which are Russian,
4 English, 2 German and 1 Japanese.
(;ard2/3

96-58--'2-1?/23
The Boilin.- of Freon-11, Methylene Chloride and Benzene
j.,j a
Horizontal Tube
ASOCCIATIM. All-Union Electroteohnioal Institute
I ~Vsesoyuznyy elektrotelzriniel:ieskiy institut)
AVAILABIR: Library of Con-ress
Card 3/3
1. Methylene chloride-Boiling 2. Benzene-Boiling 3. Freon-
Boiliiag 4. Heating elements-Applications

SOV196-58-8-15122
AUTHORS: Fastovskiy7 V.G. (Doctor of Te(-,,hnical Science)
and
(Engineer)
Artym,
TITLE: An experimental Investigation of the Critical Thermal
Load
during, Boiling of Binary Mixtures (Eksperimentallnoye
i.ssledovaniye kriticheskoy teplovoy nagruzki pri kipenii
binarnykh smesey)
PERIODICAL.- Teploenergetikat 19587 1ir 87 PP 74-'78 (USSR)
ABSTRACT;This article reports an investigation of the
critical thermal
load at atmospheric pressure as a function of the comp~,-
sition for mixtures of methanol, propanol, iso-propanoll
n-butanoll methylethylketone and iso-amyl alcohol in wat9r.
The experimental equipment is first described and the
reasons why certain design features wero chosen are
explained., a scliamatic diagram appears in Fig 1. The
tests were made on & horizontal nickel wire 0.4 mm.
diame-4-'ar
and 50 mm long. An editorial note sbatos that becaria of'
the small size of the heating s~;irface) the tests are not
characteristic of industrial conditions. The chemicals
Card 1/1+used were chemically pure, except for the n-butanol
which
was of technical purity. The ~:~ritical point was d(?tprmingd

Soir/96-58-8-15le-2
An Experimental Investigation of Grit.lcal Therrial Load
diirin~
Roiling of Binary Mixtures
visually and by instruments. In the majority of aquerlus
solutions with small amounts of organic componentos the
wire usually burnt out wher. the :critical condition was
reached. The critical thermal load as a function of
composition for the system methancl/wat&r is plotted in
Fig 2. The broken line corresponds to water alone. The
maximum thermal load was obtainod with a composition of
18% by weigbt methanol, ar-(' -s double the load for water.
Figs 3 and 4 display corre. : nding curves for iso-propanol/
-propanol/water. Aq
wat?r and n :ajn the results depend on
tho ccmposition, and a,.-o -typical for scluticns rf unlimited
Yrut-aal solubili ty. Figs 5~ 6 and 7 give cort-esponding
graphs fo.- the binary systems comprising methylethylketona/
waters n-bntano1Arat;r and iso.-anyl alcohol/wa-ter, whi,~h
have linited. mutual solubility. The limits within which
single phase is not obtained aro indicated in Figs 5 and
by vertical dotted lip-as. ThuF in Fig 5 there are three
parts of the C'Lrva- the first corresponds to a solution of
Card 2/4 S.
nothylethyllcOtono In wato,-r-, t';10 third k'O a Soluticn, of

SOV/96-58-0~-15/22
An Experinental Investigation of the Crltiral
Boilinug of Binary Mixtures
water in methylethylketor,~-,~~ *iinc-ireao th-.1 ~iic,~nd
.1.3
transitional. Simila-_~ result-s wire obtained fo'--, the
system !soamyl-al.-ohclArat.Gr (FIC, IhQ (.urv%t in Fig
lor tho systnm ri-butanol/wator 1.9 i-jntlni~ci)s bocause the
Wiro was always in a solution of water In'n-batanol. For
all three systems there is a clearly-Gxpreissed maximum at
low concentrations of the organi-.- componont in water. As
the solubility of the organic, component i)ec3mes less, thIs
maximum benoraes higher and o:tcurs, at lower
conaentrar.-Ions.
Thus the critir-,F1 thermal. loading for the system iscamy!
a
.L
"cohol/water, tt an aj.c::Iic1 c~~rrtantratjxn of 0.5%
weight.
Uras th'-'Q4) times that f-:~r wateT' rhilse TaSults a-ra
gen,~rally i7i line uitb pibJish'-..,J Tbe zer-iiarLtsm
of tbe effoot o." small arw,.nx,.-.s of urga.--Jo solvent
O-n th~j
eritica'l thernal. loading at whi-;h L-abble boiling ,-eases
is
discussed. Awn the snlutlon bolIq J)s-J6dq a naiet3nt bubblt.
it is mainly the Iow-boili.n- -:~cmponent that b,-Ala~ the
film,
C'ard 3/1+ `)f "L""'d' onvFlopir,,g tbn steam, bubble is
anrir-hod with the
high-boiling comuonent and, therefore, bolls at a higher

Ail M-.porimental Investigail-ion of the CriticAl Taci-rial Load
durine
Boilii-,C of Binary 1',i%tures
toi-iporature than I't-'he initial comros"'Gion. Curvas of
t1iis 'l-anporaturo difforencc i:,, fimotiotis of c;orposition
aro giv,3n ill. FiGs 7 iliclunive. Of Courso , small
ai,iounts of organic liquids in wator have a considerable
offact on such other pro:,.orLics aa tho surface tension
and tho wettinE angle,
Thero aro 8 figures, 8 litorat'uro roferences (2 English,
1
3 Gol-I'lan, 3 Soviet)
ASSOCIATIOU: Vsosoylizzlyy olektrotuokhnichoskiy ins)titut (All-Union
Electrotechnical In~;titutc)
1. Cyclic compounds--Thermal effects 2. Cyclic compounds--Test
methods 3. Cyclic compounds--Phase studies 4. Laboratory equip-
ment--Applications

10(4); 28(5)
1:6302
SOV/170-59-8-13/18
AUTHOR. Artym, R.I.
TITLE: Formation of Nuclei of a Now Phase-in Diluted Binary
Solutions
PERrODICAL% Inzhenerno-fizicheskiy zhurnal, 1959, Nr 8, PP 103 --
107 (USSR)
AWIRACT. Some solutions, investigated In 11,eference 1, possesis
certain advantages in
comparison with pure water, in particulnr in cooling nuclear
reactors of
the boiling type. In view of insignifi,iant conventration of a
second com-
ponent in water, it is admissible to consider these systems as
diluted bi-
nary solutions. It is known that heat uchange during boiling is
deter-
mined by two individual processes: formation of rmolei of a new
phase and
their subsequent growth. This paper consider3 thet process of
formation of
nuclei by calculating the probability o:41 their orJAination from
the view-
point of the basic tenets of statistical physics. The principal
condition
for the formation of nuclei is formulati)d as followsi this
process will
occur when the gaseous phase is more atitble and liquid phase is
in a thermo-
dynamical metastable equilibrium. The author derives equations
for the
radluu of a nucleus, Formulae 10 and la, and for Uie probability
of their
Card 1/2 formation, Formula 11, and applies them to several
particular cases. Their

.32152 R
S/076/60/034/008/012/014
B101/b208
AUTHOR: _,ArtW"_R__1__
TITLE: Calculation of thermodynamic functions of ideal gases from
spectroscopic data
PERIODICAL: Zhurnal fizicheskoy khimii, V. 34, no. 6, 196o,
1816-1825
TEXT: Aim of the present study is the calculation of tj..3
statistical sum
0vj of vibrational and rotational 8tates, considering the
interaction
between rotation and vibrations, and, assuming that the quantum
numberf~ be
limited. 1) To calculate the sum of the vibrational states of a
multi-
atomic molecule the following is 'written downs 2 Q(v 11v2p ....
vk) 3
F_ exp(-hc 'Jokvk /kT)(P+lPivi + F-Piivi +Epij Vivi + 7 PiiiVi
vlt..,v k
-f tP 2v + Y-P + ...). The calculation of QV is reduced -to the
iijvi i ijkvivjvk
calculation of sums of the form: 2: exp(-hotjvAT); L v exp(-hcij
v/kT);
V V 0
Card 1/13

32152 R
S/076/60/034/OOt3/012/014
Calculation of thermodynamic... BlOi/13208
V2 exp(-heto v/kT); .... ; vnexp(-hctjOv/kT) (2). The denotations
are
0
substituted as follows: ho4jo/kT - u; r - exp(-u); a - 1/1 - r)
(3), givirg
00 exp(-UV) a (4). Consecutive differentiation of the series Eq.
(4)
1
V ;-
and changing of the sign gives the summation equations: v exp(-UV)
- sf;
V.0
2 2 3 3 00 n
v exp(-uv) - sf v exp(-uv) - sf r..... V exp(- uv) . ,n,
V-0 V-0 V-0
i 2 2 2
where the functions f are defined as: f - 1.11rs; f ~.
1.llrs+1.21r s
3 2 2 3 3 n k=n-1 kI k k n n
f _ 1.llrs+3.2tr 8 +1.31r a ; f , aln*lIrs + akn r 8 +annnIr 8
k-2
(5)j where al. Mannl holds (6). k1l other coefficients are
inter-related by
the equations: akn " kak(n-l)+a(k-1)(n-1) (7). As the vibrational
quantum
Card 2/13

32152 R
C)
S/076/60/034/008/012/'014
Calculation of thermodynamic... B101/B208
number cannot adopt infinitely high values, i-: holds:
v v +1 v
m M
exp(-UVI . S(i r' and, as v 1, as approxination: Zk axp(-Uv)
m
v v
SO - r m) (9). The followin6 summation equations are obtained by
consecutive differentiation
",d OM
V "C' s1 - srtm (v.A I v3e-uv sr"n (vin
.~j
t..t) V-0
0"1
+ 21-M/ v3e-up , S/3
vr'm (vm +
t'-0 "'n UI-IV
Sf' - sr'- (0, + ilt~ml + 3z,41.+ p).'
r-0
Card 3/13

312152 JA
S/076/60/034/008/012/014
Calculation of thermodynamic ... B101/B2108
s11- sr"In (v,, + s14 - srrl- (v4 + 40 / + G it'
In In in
vin
I Vne-Uv= n-Sr1vn(V.+/)n =Sin- Sr' n-,/ +
YJ s/ m (11,n, + n M
t-0
n (n - 1) Vn-2/2 n (n (n - in + i).Vn-fn/Tn
+ 21 M 101 M
where f, f2 f .... P f n are calculated from Eqs. (5). 11)
This method is
applied to calculate Qv in diatomic molecules. It is assumed
that:
v
2 3 4 (13). By
Qv exp -(he/kT)(,,6v - W 0x 0v +,~; OYOV 0 .10v ...
V-~
substituting the denotations from Eqs. (3), ant expansion in a
Mtoliturin's
series the following is obtained: Qv exl?(-uv) 1+ux v 2
+(1/21)u 2 x2V4
.0 0 0
Card 4/13

S/07 6 1 XM4 ~006,101"/01 4
Calculation of thermodynamic... B101/B208
2n 2n 4n 3 2 ,2 6 2,r, 2m 6r.".
+....+(1/2nl)u x V 11 - uy v +(1/21)u y V + (1/2mllu Y v
0 0
4 4 21 81
',2z2v8+. 21
XO+u, z0V +(1/21 ul~ 0 ..+(1/211)U z 0 V j(14). This equation
is
calculated by Eqs.'.,(io) and gives:
QV = S 16~ - r"-) + uxo jf2 - r'- (v2m+ 2v,,f + f2)) -
uyO 1/3 rum (v3,,, + M ,,/ + 3v,,,Is +
U24 + Uzo) (11 rum (4, + 44f + 6vmI2 4. 4vmf3 + 14)]
uxOyO rum (v. + 5v' / + IOvIp + 10v2 /3 + 5v,,114 +f5p +
M M M
+ U rum (I'm + j)2(In+3m+4111
2n I 2rn 1211
(15)
Card 5/13

Calculation of thermodynamic ...
32152 R
S/07 616010341008/0 12,'0 14
11101/11208
After rearrangement, it results therefrom:
2111-1 On- 3)
x + - - - + U !10 V"j x
21 61 X
-x (I + Uv4. U"S v + U201, (I + lix,14" U2
2n, 4
2T, 0 in
x UYOV, + 11'"Y""v6MN
. ) x
V-1
x
+ n+m+1 n m 2n+ 3MJ41
XDYO ZO x 0 Ux"v'111 +
III fill IF /it
tp it Yo V-sn-) x
x UY'O" +
x (I + UZOVm, + AQ
(O,HNIP~ = anharmonic); The following holds for it:
(16)
13'ard 6113

Calculation of tliprmodynamic...
32152 R
S/076/60/034/008/01 2,1014
B101/B206
aurap + UjOf2 UyOf3 2 2 +
00 4- U XU UZO p Uxyx
Q
Ullon-ft 11
T11TIT111- x0yo -0
Q (v,,,) = sr'- 2uxof - 3uy, (v!,./ + v,.11) + 20--.2
(v3,,.Il + v1 f- + v.f~ +
I m
V3
+2uzo(2 1+3v1/2+2v .. f3) uxy(, (5v' ./ +)VI jM +
,IV' /3 + 51)./,) +.
ml fn JTk m
2, n +m+ I)XO?71ylMZ21 X
2n I 2m 1211U
k-1
x Yj _i f- m
k-2
(18)
in
k-2n+3m+41
(17)
Card 7/ 13

32152 It
5/07 6/60/034/0013i'v` 12/014
Calculation of thermodynamic... B101/B208
The values for n, m, I ire chosen in auch a way that the
equation is
fulfilled with any a Driori accuracy:
-hcG.(Un)IkT r,- + fixel", - U21%xaln 11 4n)x
e,(p
2n In,
Urnyinivoin 4 V
0 - 11YV' k 11Z V",+...4- -L11212 L)
x in 0 V% 211
----! I ,2n-I -n-i
in x
r + zlxov~" (2:j --I
X UY,,V3 1 .1 in "' +.LU21z11V81
in +- -+ 2ntl U' Y; ?on ) (1 --, UZ 01-411t 0 in
+ Uxov, + i
in T,
3 1),n in
in _71_U Y, in it- 11 +... L 111-1 V .1
~x (I 1l?/,?: Z,. .y4, 1! '0 D (19)
Then kq. (16) may be representect as follows; Qv - lz~
exp;-hcG 0 (v Id /kT.
- Aq(v ) (20), where SQanharm (21).- If the term -1Qj(v ) is
neglected
m m
Q,V. !,- I
in Eq. (20), the following is obtained: (I -1-eyp -hcG (V )/kT
- (22),
V 0 m
Card 8/13

32152 R
S/076/60/'034/DA.'012-'014
Calculaz,ion of thermodynamic... B101/B206
where vm results from the oondition G(v m DC1,D0 being the
d1s.3ocittion
energy of the molecule. III) To calculate th,D statistical
au:-.: 0., of the
rotational energy of a 2-atomic molecule in the electr-,)n
sta,.(" the
im
following is written down: Q j=0 (2j+l)exp -(hcAT) -BVj(j,1)--
- D i2(j+1)2 + F i3(j+1)3 . ...... (26). In a similar way as
.4.(~r
v v ZV
it is obtained: Qj QOc-,07-hCF,,(vj,)jkT A111 (Y'n
j (Y.), (36)
where
V. (Y-) + 2y"') +
+ 262.e. (y3. + 2y'lln + 12y..) (5y'M + i8y,": d-
.3M 4n+om
+ 54y'. + 120y,,,)+ a qu x
2nl3tnl
kl 4-1 k-3 nl nil
x Y YJ ily?, 7,7. -1,, F,! (33)
Card 9/13 k-4n+6m A.-nn+sm

32152 R
S/076/60/034/008/012/014
Calculation of thermodynamic... B101/B200
Q~' = q. (1 +
d. + 3d.' -/,- Odd,
1)m (2n +3T) dn./m (37)
balds.
1.n (37), the relations d - 26 q2, fv = 6y q3 hold. 4NI (y ) and 5(y
v v v v v v m n
are neglected and ii is finally obtained, Q . Qj 1 expi --hcF )/1:T
(391/
j v m
IV) The following is written down for Qvi
vm im
Q~vj exp~-hcG (v)/kT; k2j+l) exp~-hcl' (J)/kT (42). Assuming
0 v
V-0 J-0
n
that q a,=q a (1+v . vk) (43), Qv6 1 exp(-heD /kT)
v 0 0 Pk rc t* (Z~nt 0
Card 10/13

Calculation of thermodynamic...
v
VM_ n P vk ) x exp(-hcD /kT)
I ( i +
rot "i._ ~-- k 0
=0 k-1
method. is calculated from E,-i. (21).
Q~
3 21 2 B~'
S, NO / 0 3 4/0 0b i ' 2,'0 14
Biol/B20e
(44) is obtain,.,d by thi.~
Q I,' t - q a (45) and i s
rcl 0 0
nt, vith '~.it be'ng
calculated from Eq. (37), where qv . q av - ac.Q~.
n
equal to (1+ Okfk) (46). The following equations are written
down for
the free energy, enthalpy, entropy, and specific heat
oVdiatorJ( id(!al
gases:
F-E 0
In Q' - Ina;
(47)
I &DO rJ00 1100)
:~`ft ~T ~R'-V - + ~7~j ' -j"Ilb
a
S
D (H00 F1 00)
~'-cj
'- "I"b
+ 0 e-hCDjj:T + 111 (40)
Card 11/1-

32152 R
S/076/60/034/008/01 2/014
Calculation of thtrmodynamic... Bioi/b,'m
coo ' ( hCDON2 (C~t'o - G-) b
!~ -.L b)
-it a 10 A- -kT
P) hcD,)- _~,:p) C-hcD,11-T
Rr k7l 117,
b)
11T
where the following holds:
QC* Q*) no 00
QOO
up +
I - (I + b)a-',cD.'kT, ~b (W
QOR
ri
(Index denotes rotation, index interaotion). B. 1.
Brounsht-~yn
is mentioned. There are 5 references: 2 Sov',et-bloc and 3
non-Sovi-at-
bloc. The three references to En-lish-language publications
read as
Card 12/13

Calculation of thormodynamid.,..
32102 R
S/076/60/034/08/012/014
B101/B208
follows: L. S. Kassel, J. Chem. Phys. -1, 576, 1933; L. S.
Kassel,
Chem. Rev. , 1-8, 277, 1936; A. R. Gordon, C. Barnes, J.
Chem.Phys. 1, 297,
1933-
ASSOCIATION- Vaesoyuznyy elektrotekhnicheaki,v institut.,
Moskva
(All-Union Electroengineering liastitute, Moscow)
SUBMITTED: November 26, 195a
Card 13/13

VUKALOVICH doktor tekhnenauky prof,; ARTYM R.I insh,
M.P.0
Calculation of thermo4yuamic function of polyatcaic moleculeo in
an
ideal gaseous',otate* Toploenergetika 10 not4t75-78 Ap 163.
(JMIRA
1. Moskovskiy onergeticheskiy institut.
(Steamr-Thermal lzoperties)

ACCESSTON NRt AP4042461 6/029IW64/002/003/0359/0366
R. IsI.Spiridonov, G. A.
AUTI ICBS ~Ft-Y!Mf
TITLE: Derivation of equation of state for binai7 particle mixture
by the
method of correlation functions
'SOURCE: Toplofizika vv*sokikh tomperatur, vo 29 no& 3p 1964p
359-366
TOPIC TAGS: equation of state, binary gas mixture,, interaction
potentialt
canonical distributiont correlation dietribution funotiont
intogro-difforential.
,equation, short-range interaction, series expansion, classical
equation, virial
coefficient
iABSTRACTt Bogoliubovlo method was used to determine the equation
of atate of a
binary gnu mixture N, and N under the potential anorgy
2 .........
fie No
uti - Tj I ' (D,,. (I q,t - qq+
j Yj 01, qjj - qjj
t4W