Brain and Machine
SOV/29-59-2-4/41
the brain. In modern calculators, the occurrence of
accidental signal combinations is avoided. But it is not
impossible that such "senseless" combinations play an important
part in the activity of thoughts by supplying material for
intelligent constructions. If all remembrance cells of the
calculator are filled with signals it cannot receive any more
informations. A quite specific property of the brain, however,
is the ability of comparing the signal combinations stored up
at any time, creating economical connections between them and
thus making the remembrance susceptible for new informations.
Man receives during his life such an abundance Of signals that
billions of cells would not suffice to keep them in their
original form. A generalization of the connections between
signals, and the removal of superfluous repetitions, is the
aim of the logical function of the brain. A machine capable
of removing superfluous repetitions from the stored-up signal
combinations without interrupting the connections between them,
cannot be designed yet. Besides, the brain can remember its own
actions which cannot be achieved by the most perfect machine.
The opinion that the principal difference between brain and
Card 2/3 machine is the fact that the machine works according to a
Brain and Machine
SOV129-59-2-4141
program is not correct. Also the brain receives orders and
instructions from the body and subordinate parts of the nervous
system. The statement that the brain is a machine and that the
machine is capable of thinking has to be rejected too. Such
statement is an unpardonable depreciation of mental qualities.
It justifies imbecility and mental poverty, cruelty and
heartlessness toward other people by insisting that there
are only reflexes instead of a soul. There are 6 figures.
Card 3/3
29(0) SOV/29-59-3-8/23
AUTHORS: Gushchev, S., Teplov, L.
TITLEs How Was It ...? (Kak eto bylo ... ?)
M 0
PERIODICAL: Tekhnika molodezhi, 1959, Nr 3, pp 14-17 (USSR)
ABSTRACT: In this article the au ,thors report on the successful launching
of the space rocket on January 2, 1959. Before the rocket was
launched, accurate computations of the proper time of launching
and the trajectory had to be made with complicated electronic
computers. The rocket could not be seen when it took off and on-
ly a weak earthquake was noticed. Its flight was watched by
locators and in the middle of the aoreen there was a small
bright spot to be seen. After leaving the troposphere the top of
the rocket inclined toward the east and the first stage was de-
tached. After the first thirty minutes the rocket had also croa-
sed the ionosphere. Now it was difficult to determine the motion
of the rocket from the earth curvature. The computers now did
not calculate the trajectory with respect to the earth's surface
but with respect to the orbit of the earth. The trajectory of
the rocket somewhat declined below this plane. In this moment
Card 1/3 the next stage was detached and the rocket lost its flashing
How Was It ... ?
SOV/29-59-3-8/23
tail. It had attained the parabolic speed of 11.2 km sec. When
the motors stopped, also the last stage weighing 1 1~2 t had
reached its trajectory. The top was detached and a rotating ball
with aerials and a magnetic feeler on a long rod was hurled out.
Each part of the disassembling rocket had the came speed and
therefore they flew side by side. Suddenly a aeoming deviation
from the trajectory was observed on the projection set up ac-
cording to data calculated by the computers. Yet this was again
a paradox of space travelling. Due to the different directions
of motion, the projection of the rocket lagged behind the rota-
tion of the earth. After one hour of flight the rocket had al-
ready covered a distance of more than 10000 km from the earth.
The data of the magnetometer gradually became inaccurate and the
magnetic field of the earth became weaker. At a distance of more
than 30000 km the rocket had already left the magnetic field of
the earth. The instruments in the rocket could only measure
cosmic radiation in its original state. Two counters recorded
the number of charged particles hitting the rocket, while two
photomultipliers analyzed the composition of radiation. After
eight hours the rocket had already covered a distance of more
Card 2/3 than 100000 km. At a distance of 113000 km the quartz clock had
How Was It ...?
SOV/29-59-3-8/23
released the fuse of the vaporizer in the right moment, whereby
the metallic sodium evaporated in the space as a yellowish cloud
several 100 km long. Although radio locators can record the dis-
tance from the earth every second, it is yet very difficult to
determine the accurate position by radio location. The flash of
the sodium cloud that was observed for several minutes permitted
a precise determination of the trajectory. Meanwhile the preci-
sion instruments in the rocket communicated their observations to
the earth. They served the purpose of measuring the degree of
density of cosmic gases, and should answer the question whether
they are less dense farther from the sun. Further, they recorded
the number of corpusculee emitted by the sun. A man, whatever
his intelligence, health and reactivity, could never observe and
record everything as precisely as these instruments. Therefore,
it is unnecessary to risk casualties. At a distance of about
400OOkm the attractive force of the moon becomes effective. If
this line were crossed, the rocket would fall on the moon. The
Soviet rocket had another program, however. The instruments com-
municated the size of the magnetic field and the radioactive in-
tensity of the moon. Communications of the rocket were received
still for a long time until it was fully integrated by the solar
d 3/3 sphere and became an artificial planet. There are 8 figures.
TBPWV, L.
Invisible printing plants. Tekh.mol. 28 no.4:25-26 '60.
(MIRA 13:11)
(Ruesia-Underground literature) (Printing plants)
I
I I -V L
I -` 0 r,:r.. njt. no.10:2 0 161-
.1-r-f our ki~vr'l ~-'- sPr-, ('rapi, lio lo)
T~10, il.
)
I TEPI'Ov ~ Lt
Dreaming about a selfptyping typewriter, Znan. eila 36 no. 4:26-29
Ap 161o (Cybernetics) (Typewriters) (MIRA 14:4)
TEPWV~ L.
The seeing machine, Tokh.mol, 30 no.190-6 162. (MIRA 15:12)
(Pereeptrons) %
TEPLOV, Lev
Inform Lion, life,, death, luunortality, Tauka i takh ml.adazh
15 no. 11: 3-6 N 163.
..I;--
I
ABDULIN, A.; ALEKSEYEV, I.; BANTLE, 0.; BOBROV? L.; BOZHANOV, B.;
BOYKOI V.; BONDAREV, X.; BORZOV, V.; VERKHOVSKlY, N.; GUBAREV, V.;
GUSHCHEV, S.; DEBABOV, V.; DIKS, R.; DMITRIYFV, A.; ZHIGARFV, A.;
ZELIDOVICH, Ya.; ZUBKOV, B.; IRININ, A.; IORDANSKIY, A.;
KITAYGORODSKIT, P.; KLTUYEV, Ye.: KLYACHKO, V.; KOVALEVSKIY, V.;
KNORRE, Ye.; KONSTANTINOVSKIY, M.; LADIN, V.; LITVIN-SEDOY, M.;
MALEVANCHIK, B.; MANICHEV, G.; MEDVEI)EV, Yu.; MELINIKOV, I.;
MLINP Ye.1 NATARIUS Ya.; NEYFAKH, A.; NIKOLATFV, G.; NOVOWYSKIY, A.;
OLISIIANSKIY, N.; OSIMIN, S.; PODOLINYY, R.-, RAKHMANOV, H.; REPIN. L.;
RESHETOV, Yu.; RYBCIIINSKIY, Yu.; SVOREHI, R.; SIFOROV, V.; SOKOL'SKIY, A.;
SPITSYNI V.; TEREKHOV, V.; TEFLOV, L.; KHARIKOVSKIY, A.; CHFRNYAYEV, I.;
SHAROLIp L.; SHIBANOV, A.; SHIBNFV, V.; SHUYKIN, N.; SHCHUKIN, 0.;
ELISHMKIY, I.; YURIYEV, A.; IVANOV, N.; LIVANOV, A.; FEDCHENKO, V.;
DANIN, D., red.
[Eureka) Evrika. Moskva, Molodala gvardiia, 1964. 278 p.
(MIRA 18:3)
71PWV. L.P. (Koscow).
History of Russian printing and publishing; 120 years from the discovery of
milticolor planography. Polipgr.proizv. no-7:23-24 Jl-Ag '5). (MLRA 6:9)
(Printing-press-History)
TEPWV. L , .inshener.
-". ''
Together forever. 29kh.sol. 22 no,5:12-13 My 134. (MM 7:6)
(Printlng-Histary)
U-PLOV I L.
SPLOT, Lq, inshoner.
~,:~ ~
The machine writes
(Typewriters)
letters. Takhsol. 22 no.6:33-33 Jo 034. (NLRA 7:6)
TIIPLOV, L.
Science and technology in countries of people's democracy.
Tekh. nol. 23 nn.4:26-27 Ap 155. OGRA 8:6)
(Europe, Eastern--Technology) (China--Nuclear physics)
I
TIPLOV,L., inzhener
Electronic photography. Tekh.mol.23 no.7:12-15 Jl'55- (MM 8:10)
(Printing) (Photography)
7EPI,Ov,q V,
C7bemetics. (To be contd.) Ilauka i takh mla&zh noO3.-25-26 Yr 157a
TSPLOV,L., inshaner
Inventor@ and inventions. Takh.mo.23 no-9:&10 S'55. (MLRA 8:12)
(inventions)
TEPIOV. L,. inshoner.
Tolellbrary. Tekh.mol.24 no.6:13 Ja '56. OaaA 9:9)
(Scianco fiction)
TIOPLOY. L.
-
Yrom goose quill to charactron. Takh.mol. 24 no.11:26-28 N '56.
(Typesetting machines) (KM 9:12)
TWWV L
Yhat Is cybernetlcs?
Tokh. mol. 24 no.12:30-32 D 156.
(MLRA 10:2)
(Cybernetics)
'F-J~ f ~C 6VL- .
TEPL Ok , 11 "
w4 .
Ronding machines. Tekh.mol. 25 no.8:24 Ag '57. (MIRA 10;9)
(Readir--, machines)
6(o); 27(o) MWE I BOOK M-EPLOITATION sov/3)464
Teplov, Lev Paylovich
I, ................ .........................,
Ocherki o kibernetike (Essays On Cybernetics) (Moseav] Moskovskiy rabochiy,
1959- 229 p. 30,000 copies printed.
Ed.: S.Gurov
PURPOSE: This book is intended for the layman interested in the science of
cybernetics.
COVERAGE: The book discusses such subjects as the theory of signals, probability
theory, biology, physiology of the nervous system, psychology, theory of auto-
matic control, and theory of automatic machines, all of which contribute to the
new field of science known as cybernetics. No personalities are mentioned.
There are no references.
TABLE OF CONTENTS:
Control 5
card V3
Essays On Cybernetics
Deformation
Sampling [of signals) FrCM Noise
Feedback
Logic
The Brain
Mach1nes-automatons
Signal Machines
Elements of Signal lachines
Double Calculation
Electronic Ccmputers
Card 2/3
sav/Yi64
15
37
54
67
67
106
119
136
164
175
Essays On Cybernetics
"Higher" Automatons'
Cybernetics and Hunanity
AVAILABIZ: Lfbrary'of Congress (Q31,5.T4)
Card 3/3
sov/yI64
193
216
AC/gmp
4-26-6o
Teplovo Lev Pavlovich
Ocherkl o kibernetike. Moskva, Foskovskiy Rabochiys 1959-
V. ijIus.
Bibliographical footnotes,
FOR C%IPLETE HOLDINGS CONSULT SHBlY LIST
1. Cybernetics. 2. Russia - Cybernetics. 1, Titles
M.2E I 30,Y EXPWITATIM Sal/0484
Teplov, Lev Pavlovich
Ocherki o kiberrietike-(~'ssays on Cybernetics). 2d ed., rev. [MQ3COVI Moskovskiy
rabochly, 1963. 413 P. 50,000 copir-3 printed.
Ed.: S. Gmrov; Teeh. r3d.,. Ye. YF-kc-,-rI-,)va
RWI)'E: TTiis 'took is fo-r 9-,,~ reader.
CGIEPUAGE: A popular-.3tyle des-'ription is given of the origin, history, and pre-
llen"- state-of-the-art of Various autmatic machines are described,
with emphnzi.3 ca sir-ilaritles trt:we,~!a and things in nature, and various
methods, of u-aing, controllinj,,, and a-~cm.,ulating information are outlined. Refer-
enceG and reccmmend~-td rending ax- giw~n fcr chapter and are more or less
evenly divided between Soviet nc~n-,Svdet aources.
TATIM
, OF CONTF.17TS:
CyberneT.Ics', its PInce 1-.-L Lif-~ 3rcL Amcxig S(Aences
3
ALIFEROVICH, Yu.I.; GUTCHIP, I.B.; KAYBYS , A, L.S.;
HEV _Z4~4p~j L.P.;
BOGDANOVI G.G.; DROBYSHEV, Yu.G.; WIRNOV, G.V.;
TRETIYAYGOV, V.S.; BREYDO, M.I.; YEIVS-EYEN, L.A.; ')TEBAFrjVp
S.A.; FEDCHENKO, V., red.
[The ABC's of automation; collected articles] Azbuka avto-
matiki; sbornik. Moskva, Molodala gvardiial 1964. 349 p.
WMA 17:7)
TIPLOV, N.M.
Practical experience in the control of rabies in Stalino Province,
Ukrainian S.S.R. Yeter$mriia 36 no.11:20-21 N 159 (KIRA 1):))
1, Glavrqy vetvrach Stalinskogo oblastnogo upravlonlya sel'skogo
khosyaystva.
(Stalluo Province-Rablee)
A 2,
AUMOR: TEPWV, N. L.
TITLE: A-U Sci Conf dedicated to "Radio Day", Moscow, 20-25 MMY 1957.
"Basic Correlations in SignalIntegration and Fluctuating Inter-
ference in the Radio Receiver Channel."
PERIODICAL: Radiotekhnik i Elektronika, Vol. 2, No. 9, pp. 1221-1224,
1957, * (USSR).
Vor abstract see L.G. Stolyarov.
rswz 4
AUTHOR: Teplov, N. L. 108-9-1/11
TITLE: On the Evaluation of the Noise Strength of the Radio Reception
Methods Based upon the Keane of Signal- and Noise Functions
(K oteenke pomekhoustoychivosti metodov radiopriyemat osnovannykh
na usrednenii funktsiy signala i pomekbi)
PERIODICAL: Hadiotekhnika, 1~571 Vol, 12, Nr 9g pp. 3-11 (USSR)
ABSTRACT: The investigation of the question is bore restricted to tho gener-
al case of an averaging linear on principle as the result of a
summation of the values (discrete and continuous) of the input
function signal noise with the weight function of the adding
(averaging) devicat whereby the latter has a constant value which
is here assumed to be equal to 1. The physical supposition for
a yield with regard to noise strength when the mean of the signal
and the chance noise is taken is practically the complete co-
herence of the signal and an essentially lower coherence of the
noise which degree# however, is determined by the selectivity
of the total receiver-traot. The preponderating of the signal
over the noise which is guarante4d by a concrete receiver scheme
at the input of the recording device is used as the most general
Card 1/3 criterion for the evaluation of the different methods of re-
On the Ivaluation of the Noise Strength of the Radio 108-9-1/11
Reception Methods Based upon the Means of Signal.- and Noise Functions.
oeption from the point of view of reliability. Following methods
are discussed:
1) Method of repeated repetition realizes the idea of accumulation
in the most simple way. The single measurements or the readings
of every mixture of signal and noise at all which repeat with a
period T are added and the mean is teaken. It is shown that the
yield in the case of a reponderance of the signal over the noise
is equal to the number of the repetitions n.
2) The integrating of the signal and the noise can from the
physical point of view be described as a continuous summation
of all instantaneous values of the function signal noise within
the effective range of the signal. A formula is derivated which
explains the physically obvious result: the relative yield with
regard to the noise strength in the case of integrating is direct-
ly proportional to the ratio between the signal duration and the
noise correlation interval which is determined by the breadth of
the band of the total receiver tract.
3) Discrete taking of the mean of the signal and the chance
noise. The investigation is restricted here to the case of a
Card 2/3 constant signal level.
On the Evaluation of the Noise Strength of the Radio 108-9-1/11
Reception Methods Based upon the Keane of Signal- and Noise Functions.
4) Method of accumulation. This is considered as a pairing
of the repeated repetition with the integrating of the
signal and the noise within the effective range of the single-
signal. It is shown that in the case of broad bands the efficiency
of the method of taking the mean in a concrete apparatus is de-
termined only by the total signal effective time T N and does
not depend practically upon the fact wether the signal is trans-
mitted discretely or continuously. There are 8 figures and 2
Slavic references.
SUBMITTED: October 31, 1956 (initially) and January 17, 1957 (after revision)
AVAILAPLE: Library of Congress
Card 313
TEPMV, 11. L.
N. L. Teplov, "Certain questions of the theory and computation of the interference
imminity of impulse radio reception." Scientific Session Devoted to "Radio D&I,
May 1958, Trudrezervizdat, Moscow, 9 Sep 58.
Questions of tho maximum approximation of interference-immuiity of the radio
reception of impulse signals to the potential interference immunity are analyzod
as is also a general method to analyze and compute the interference imminity of
impulse rauio reception circuits.
TEPLOVS H.L,
Fundamental relationahipe during the Integration and filtra-
tion of a signal and fluctuation noise In the channel of a
radio receiving system. Sbor. trud. 11TORIN no.2:35-55 '58
(MIRA 16:6)
Radio-Interference)
dio--Recelveto and reception)
t
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ablu 2016111lowl" ad slooftiftl 0911111141"Momme Ia. A. 0. PoWr (VMS). moom,
&32 Nw.
AUTHOR: Ze4o v N sov/lo6-59-1-4/12
TITLE: The Maximum Noise Stability of Radio Reception of Signals
with Amplitude, Frequency and Phase Keying (Maksimaltnaya
pomekhoustoychivost' radiopriyema si nalov s amplitudnoy7
chastotnoy i fazovoy manipulyatsiyey5
PERIODICAL: Blektrosvyazl/131959, Nr 1, pp 28-37 (USSR)
ABSTRACT: Fig 1 shows a typical AM receiver, while (1) are equations
for the mark and space versions of the signal. The
receiver is working correctly when its output is greater
than a certain threshold value during the signal period
and less during the space period. Errors occur when the
situation is reversed. The probability density of the
envelope of the sum of sinusoidal signal of fluctuation
noise is given by (2). The mean square value of the noise
in the effective receiver bandwidth is (3) and the
probability density of the noise in the absence of signal
is given by (4). For equal a priori probabilities of mark
and space the probability of error during reception is
given by (5). Combining (3) and (4) into this last
equation gives 1.6). The error probability is reduced by
Card 115 increasing the signal/noise ratio at the input to thp
detector and for a given signal/noise ratio thb
SOV/106-59-1-4/12
The Kaximum Noise Stability of Radio Reception of Signals with
Amplitude, Frequency and Phase Keying
probability of error depends on the threshold value. A
study of the minima of the function in (6) reveals an
optimum value for the threshold (8) for a sufficiently
large signal/noise ratio. This gives the commonly used
design value in (10) (limiting level equal to one half
expected signal level). Eq (8) is plotted in Fig 2. The
minimum probability of error when receiving AM signals
with an optimum threshold value is given by (11). it
will be seen that this probability is uniquely determined
by the signal/noise ratio at the input to the detector.
The action of frequency shift keying is defined in (12)
and a block diagram of a suitable receiving system is in
Fig 3. Errors occur in the system when the value of the
noise envelope coming out of one separating filter
through which there is no signal exceeds the value of the
total. envelope for signal-plus-noise coming out of the
filter in which there is a signal. The analysis proceeds
as before and the probability of error is given by (16).
Card 2/5 Frequency shift keying is defined in (17) and a block
diagram of a suitable receiver Is in Fig 4, The
sov/lo6-59-1-V12
The Maximum Noise Stability of Radio Reception of Signals with
Amplitudet Frequency and Phase Keying
fluctuation noise at the input to the separating circuit
takes the form of a sinusoidal oscillation whose envelope
and phase are slowly varying functions of time. The
corresponding probability of error is given b~ (24). It
is stated by the author that the formulae (11 7 (16) and
(21+) were obtained by him in 1954 in fulfilment of his
dissertation work. The penultimate section is devoted
to a calculation of the maximum noise stability of radio
reception of signals with these various forms of keying.
Eq (27) is the expression of the square of the signal/
noise ratio. The optimum bandwidth of the filter for
passing a rectangular pulse has been found. by Siforov
(Ref 4) as (30), while the optimum bandwidth for a single
tuned circuit is given by Teplov (Ref 5) as (31). The
corresponding maximum signal/noise ratios are (32) and
(33). The formulae are repeated in (34) and (35) in
terms of Q2, which is the ratio of the energy in an
elementary signal to the noise density at the input. A
useful concept is introduced which is the limiting
Card 3/5 signal/noise ratio in reception obtained by integrating
soVlo6-59-1-4/12
The Maximum Noise Stability of Radio Reception of Signals with
Amplitude7 Frequency and Phase Keying
for the duration of the signal. It is shown in the
simple analysis in the top half of page 34 that th-,
limiting signal/noise ratio is in fact equal to Q- (Eq 4-2).
Applying this last exprossion to the throe parti,--ular
cases the noise stability for each is given by (43)7 (44)
and (45) for AM, FM and PM respectively. The last
section gives formal solutions to the problem of radio
reception in such a way as to realise the potential noise
stability as defined by Kotefnikov (Ref 6). Block
diagrams for PM FYI and AM are Figs 5, 6 and 7
respectively. 6orres onding expressions for tential
noise stability are NO, (52) and (56). Grappoh of Fig 8
shows the dependence of the probability of error on Q
Card 4/5 'hen receiving the three kinds of signal with synchronous
sov/lo6_59-1-4/i2
The Maximum Noise Stability of Radio Reception of Signals with
Amplitude, Frequency and Phase Keying
and amplitude detectors. By using coherent detection
the maximum noise stability equals the so called
potential value.
There are 8 figures and 6 Soviet references.
SUBMITTED: June 30t 1958
Card 515
2o475
9, 3,Z 2,5' (41so JO 3/) 7 3/106/61/000/004/002/004
iyd 0 A055/A1 33
AUTHORs
TITLEt The noiseproof feature of integrated reception of signals in
the case of fluctuation noises and of sinunoidal interferences
/Sl-
PERIODICALt Elektrosvyazl, no. 4, 1961, 9-iB
TEXT. Integrated reception is compared, as a rule, to the usual nar-
row-band reception. Such a comparison is natural enough, since integration
averaging~, considered as a physical process, is equivalent to filtration
smoothing). By narrow-band reception is usually understood the reception
~
with the most advantageous pass-bards corresponding to the optimum noiseproof
feature of reception. As to fluctuation noises, the most advantageous pass-
bands, for reception of single pulses, are the so-called optimum frequency-
banda (V. 1. Siforov - Ref. 1: "Influence of Noises on the Reception of Fula_-
Signals", Radlotekhnika, 1946, no. 1). The author of the prenent article be-
gins with some general considerations regarding the main features of the in-
tegrated reception, as compared to the usual narrow-band reception. He points
out thatt 1) the noises exert an effect upon the integrating circuit only
Card 1/5
2o475
5/106/61/000/004/002/004
The noiseproof feature of integrated... A055/A133
within the duration of the signal, which is not the case in the usual narrow-
band reception, where filters are "static" or permanently switched on; 2)
in integrated reception, the superposition of adjacent pulses, due to resid-
ual oscillations, is eliminated; 3) the salient difference between the two
reception methods is the fact that, in the integrated reception, the frequen-
cy selectivity is determined, not by "static", but by "dynamic" resonance
characteristics and pass-bands of the.integrating circuits. After these ge-
neral considerations, the author proceeds to a comparative theoretical ana-
lysiB of the noiseproof feature in both reception methods. He first examines
the case of fluctuation noises. The principal formula used by him is the
formula giving the ratio of the signal-power to the noise-power at the output
of the integra'Ling circulti
h2 !1 a2,r (14)
b2 2V2
T, 0
where ar is the amplitude of the signal at the output of the circuit, T is
the duration of the signalt Vg is the intensity of the noise in the 1-cycle
band (specific intensity), and brrexpresses quantitatively the amplitude of
Card 2/ 5
20475
S/106/61/000/004/002/004
The noiseproof feature of integrated... A055/A133
the noise. For the usual narrow-band reception, the corresponding formula
is h2 - 0.82 a2lr (16)
Opt 2 =1
0
This formula (16) is valid for the reception of single pulses and for any
filter with the optimum frequency-band. For the extreme cases of an ideal
filter and of a single oscillatin ircuit, formula (16) becomes
h2 a9vo (21)
opt.id.f. ' 0.825=29-
0
and 2 a2,.
h 0.815-- c (19)
opt.single osc. 292
respectively. Taking the ratio of (14)oto (16), the author finds:
h 2
-zz*-)fluct. = 1.22 (22)
(
hOpt.
For the reception of single, widely spaced pulses, the integrating reception
method is, therefore, almost equivalent to the usual narrow-band method with
optimum f requency- bands. But the advantage offered by the integrating method
Card 3/5
204,75
5/106/61/000/004/002/004
The noiaeproof feature of integrated... A055/A133
proves more substantial in the case of an uninterrupted sequence of nignal-
pulses (for instance, in radiotelegraphy). In this caooa short mathematical
demonstration shows thatt 2r-
h 2 0 a (26)
opt., '5=2j
The ratio of (14) to (26) ist
h* 2
(hopt.)Iluct. '_ 2 (27)
As to the ratio of signal-pcwer to noise-power, the integrated reception of
an uninterrupted train of pulses ensures thus a gain practically equal to
two, in comparison with the usual narrow-band reception. Thia gain proves
still greater in the case of signals subject to fading. In the last part of
the article, the author examines the noiseproof feature of both reception
methods in the 2case of sinusoidal interferences. Here also, he deduces for-
mulae giving, h*, h2 and h pti, and finds thats
opt, h* 9
_), , - 1.22 (39)
hopt sin
Card 4/5
4 5
S/106 '601 000/004/002/004
6
The noiseproof feature of integrated... A055~A133
and h* )2 -2 (40)
(FO-Pt, sin --
There are 6 figures and 5 Soviet-bloc references.
SUBMITTED: April 12, 1960
Card 5/5
80162
3/108/60/015/04/04/()07
6,1000 B014/BO14
kUTHORt -Teplov, N. L.., Member of the Society
TITLEs The Maximum Noiseproof Feature in Systems With Discrete Signals'b
PERIODICkLi Radiotekhnika, 1960, Vol. 15, No* 4Y PP- 27 - 55
TEXTs In the article under review, the author studies the maximum noiseproof
feature of systems having discrete signals in the case of coherent and incoherent
reception. Formula (2) is written down for the probability of regular signal de-
tection. The fluctuating noise5is expressed by formula (3) which is split up into
its components according to 4 . Then, the author gives formula (8) for the
correlation function between the amplitudes of formula (4). Formula (8) is used
to determine the energy spectrum of the fluctuating noise. The relation between
the signal expressed by (1) and the fluctuating noise may be represented by the
vector diagram shown in Fig. 2. Next, the author carries out a general estimation
of the noiseproof features of systems with discrete signals in the case of co-
herent and incoherent reception. In both cases he proceeds from the probability
that the amplitude of the noise in branches without signals is not larger than the
amplitude of signal plus noise in branches with signals. This is described by
1K
Card 1/3
The Maximum Noiseproof Feature in Systems With Dia-
crete Signals
80162
3/108/60/015/04/04/007
B014/BO14
formulas (13) and (20). Subsequently, he develops formulas (18) and (24) for the
probability of regular signal detection for the two cases under consideration.
The two formulas assume their definite form with formulae (27) and (28). When
investigating the maximum noiseproof feature the author first studies the
maximum surpassing of the signal over the noise. Integrals (43) and (44) are given
for the determination of the maximum noiseproof feature. Formula (47) is used to
determine the relative error arising in the estimation of the noiseproof feature.
In conclusion, the author compares the noiseproof features in systems with dis-
crete signals in the case of coherent and incoherent reception. Table 2 indicates
that the greatestdifferenoe in the noieeproof features of the two modes of re-
ception is obtained in the range of the highest values of error probability. As
compared to incoherent reception, the greatest gain of signal power in the case
of coherent reception is equal to 2. Hence, when signals with a given error pro-
bability are received, the signal voltage at the input of an incoherent receiver
must be higher than that at the input of a coherent receiver. The respective
factor between the two input voltages varies from 1 to 2. In conclusion, the
author gives the formulas for the maximum noiseproof feature and those for the
probability of detecting signals for the case in which fluctuating noise occurs
only in one part of the branches of this systems formulas (56), (58), and (60).
Card 2/3
The Maximum Noiseproof Feature in Systems With Dis- S/108 jo~'115&4/04/007
crete Signals B014YBB014
This article was read at the All-Union Anniversary Session of the NTORiE imani
A. S. Popov in June 1959. There'are 5 figures, 2 tables, and 3 Soviet references, I
SUBMITTEDs March 6, 1958 (initially) and July 24, 1959 (after revision)
Card 3/3
61
AUTHbR: Teplov, N. L
311)7
S11061611000101210011010
A055/A127
TITLEt Noise iimmnity In integrated rt,,ception of ~Ienalzi in the presence of
impulse or transient sinusoidal Interferences
PERIODICAL: Elcktrosvyaz'~,~j. 12P 1961, 3 - 12
TEXT: This article is a theoretical comparison of the noise immunity of the
integrated reception method and the usual narrow-band reception method in the
case of: 1) impulse interferences, 2) transient (short-term) sinusoidal inttr_
ferences. 1) Impulse interferences. a) Narrow-bami reception. - The impulse Intei-
ferences at the filter output are given by the expression:
C(t) - cWcos(Wot+%).
WO is here the angular frequency of the tuned filter; ~po is determined by the mo-
ment when interferences appear; c(t) Is the amplitude (envelope) of the oscilla-
tions, whose time-variation determines the shape of the impulse interference at
the filter output. Starting from this formula, the author finds the ratio between
the maximum amplitudes of the signal and the impulse:hterference single pulses at
Card 1/6
"'11)?
'3/ 1
, DS/6j/()00/()j2/fo 3/0 In_
Noise immunity In integrated reception of... A055/A 127
the output of the narrow-band filter. In the case of a single oscillating cir-
cuit, this ratio is:
faoutp max ?6feffT)
~coutp max1ingle circ ~ 2 SoMeff P (5)
where So in the modulus of the spectral density of the Impulse Interference at the
filter input; Afeff is the effective frequency-band of the filter; T is the du-
ration of the signal pulse. At 6f pt. = D~~ (for single signal pulses):
eff.o
aoutp max a
= -g-- 0 .56 (7)
Coutp max)opt. single circ. 00 2 - o.65 - 3 0
At Aft 1.1 (for reception of an uninterrupted train of pulses):
eff opt - C
aQ"P_.M't& = 0.36
(
coutp max)opt'single circ. 30
Analogous formulae are then derived for ideal band-filters. in the general and
average case, It can be assumed that:
Card PA
31-1)7
3/106/61/000/012/001/010
Noise immunity in integrated reception of... A055/A127
fac~utp max Wr
-,,,0.5 (12)
~Ooutp max)opt. so
outp max arc
-,0.3 (13)
(a, I
coutp max ptV S0
b) Integrated reception: afeff being here the effective static band of the inte-
grator filter, the author shows that the maximum ratio between the signal and
the Impulse interference is determined by the formula:
(ic )integr. (14)
TO
Comparing (14) with (12) and (13), the author obtains: for the reception of
single pulsest
31197
-9/106/61/000/012,/001/010
Noise immunity in integrated reception of,,,. A055/A127
for the reception of an-uninterrupted train of pulsesl
a
(
10 intejzr 96 3. (21)
tA)
kc opt,
This comparison shows the advantage of using the integrated reception. 2) Tran-
sient (short-term) sinusoidal interferences. a) InteXrated reception: The.avera4p
statistical amplitude of the interference is assumed to be the same and equal to
einterf - The ratio between the signal and the transient sinusoidal interference
Is giveA byl 2 qntegr a2q- a2,Z- -
- :: - 21 2 Ir __ t_j (23)
h; elinterf rf interf o interf
where 'rinterf is the duration of each interference and 12 iatho square of the ef-
0
fective value of the interference, assumed to be the same a*y frequency. b)
Narrow-band receptionj The signal-to-interferenoe ratio at output af1he nar-
row-band resonance circuit is determined by# IT
card 4/6
31197
S/106/61/000/012/001/010
Noise iffminity in integrated reception of.;; A055/A127
a2(1-8-26feff") 2 (29)
8~2tq.~f -,'4bfeffTinterf)
)Outp * 4fef,f, 0
where Afeff is the effective Prequency-ba~d of the circuit,* if &f o.65
effoopt
a2 2(j.0-1.3)2 2
outy a a ec 0.82
9.65 I_e-2.6rinte e 1-e * &
nterf outp ei2 . ;?Fl - # 2 -2 6vint
)Opt, nt rf 7 T_( interf
(31)
Comparing formulae (23) and (31), the author writest
A 1,*22(1-0.2.6p
(33)
_(3-1T'! p
whare,p rri or ~V Formula (33) permits to rate the advantages of the integrat-
ed receptionr,it Me; examinIng-t1seff9ot of the irregular variations of the signal
pulse amplitude, the author draws the following conolusionxt The noise Immunity
of the integrated reception, an compared to the narrow-band reception, is the
greatest in the case of impulse interferonoes and transient sinusoidal interferen-
C ard 5/6
3U97
5/io6/6i/ooo/oiP_/ooi/o1o
Noise immunity-in integrated reception ofe~j, A055/A127
des. In the~reception of single signal pulses, the immunity of the integrated re-
ception as regards fluctuation and "undamped" sinusoidal interferences is but
little different from that of the usual narrow-band reception with optimum fre-
quenoy-bands. The integrated reception noise immunity for each kind of inter-
ferences is determined by the magnitude of the signal-to-interference ratioj these
magnitudes,-suoh as computed by the author', are listed in two tables. There are
2 fi gure's'., ~ tables and 3 Soviet-bloc references. The names of Soviet scientists
mantl'oned In the arti,,ole are, Koteltnikov.and Oonoroyakiy.
SUEMITTED: April 18th, 1960
Card 6/6
Dot 'rmiwttion of the of an i,-Iea2 receiver.
16 no.3:31-39 'Ir 101. (:,(1 A 1.";2)
1. Doyrjtvltolln;rj chlon ob.')Iic',,.oatva r;,.dtc-
ta!dhniki i clolftrourfazi i.,n, A.5 4Popovr%.
. v --) (In.Cozmation tl,.cor,,)
(Radic-Recievors and recc.,lio,
AUTHORS: Teplov, N.L., Shmatchenko, V.P.
39466
5/106/62/00Q/608/001/009
A055/A101
TITLE: Analysis of the Integrator of rectangular radio pulses
AV -
PERIODICAL: Elektrosvyaz', no. 8, 1962, 3 - 12
TEXT: The authors determine the parameters of the ideal integrator (with
linear integration) and of the integrator with a single oscillating circuit.
Ideal integrator: The equation of the integrator resonance characteristic is:
(6 f a (A f )Ir sin TG Af lu (9)
a (0). it 6 f Ir
where 4Lf 2,, and AW -0-00, C is the duration of the integration.
The effective frequency-band of the integrator is
00 Go
?r,6 f C
Y2 g,n2_
A f (,&f)- dAf - 2 d6f (12)
eff T OrAf;Y
-00 0
Card 1/4
S/1 06/6Z/OW/008/W1/GV9
Analysis of the integrator of rectangular .... A055/A101
Assuming that the signal is A-(t) - ao sin Gio t at 0 4 t (13)
(-- being the duration of the signal), the excess of the signal over the inter-
ference at-the output of the integrator will be
a 2
0 2
h2 2 so T (14)
id Integr -V ;d 'A f 2
0 eff T 2 v 0
where ~~ 0 is the specific intensity of the interferences (in the 1-cycle-band).
Integrator with a single oscillating circuit: The authors obtain the dynamic
resonance characteristic of the intergrating circuit:
z 2 4y;
y (A O'c a W 1/1 - 2 e Cos 2 it x + e- (21)
a ( v, f 0 + ( Tt e-2y
where Y- z.&fff; x- AfIr. At V 7--) 00 ,
lim y (A f)_~ - y (,& f) - (22)
r -4 00 + x )2
Card 2/4 Y
sli o6/62/0OQ/008/(;,U1/0O9
Analysis of the integrator of rectangular .... A055/A101
which is the equation of the static reAonance characteristic. On the basis of
(21), the authors calculate the ordinates corresponding to the minima and -naxima
of the dynamic characteristic. They next give the formula for the effective dy-
namic frequency-band of the integrator;
c0
Af y 2(Aqt dLf 2 e-2y Cos 2n&f-V + e_4y~ d A f - (28)
eff z (,_t 6 f ,~ )2) .-21 2
-00
This formula shows that, at an unlimited narrowing of the static band, the dyna-
mic frequency-band of the Integrating circuit tends towards the effective fre-
quency-band of the ideal integrator. The excess of the signal over the interfer-
ences at the output of the Integrating circuit is:
2 2
h2 ao so , 1 1 - e-2y 2 1 1 - e -2-1 (32)
integr 2 2 -21
2 v0 Af eff 'U 2 vo + e
where q2 . h2 is the limit-value of the excess, and a0 is the input signal ampli-
Card 3/4
S11 06/62/GCO/O08/001 /0G9
Analysis of the integrator of rectangular .... A055/A101
h~
tude. The analysis of the curve showing the dependence of intexr on y per-
h2
mit6 formulating the requirements set upon the parameters of the single-oscil-
lating circuit. The ratio of the amplitudes at the beginning and the end of the
(4Eb1c damp
damping of the oscillations is k = e , where cc_r- a, + 1:(,2 (ckj boing
the attenuation of the circuit in the integration period, and oL2 the additional
attenuation:br the damping of the oscillations), and A 'r- damp is the damping
time. Designating by ilfeff z the effective frequency-band of the circuit in
damping operation, ihe authors write: 1n k - 2 Lfeff z 4 "~damp, or (replacing
Y - ln k (36)
L fef f Z L Tdamp by F_ 2
A graph illustrates the dependence (36). The Soviet personalities mentioned In'
the article are: V.A. Kotel'nikov, I.S. Gonorovskiy. There are 11 figures.
,51JU1,1TTMr.D; January 13, 1962
Card 4/4
I I
I 'n- I. i~ ,, ..~ r ! - ce 7t I I ' - **
--- ~-- , r, , -E! re n
- - - -I - . I --, r~
- ,;!! HV-
, 1 - - * - , I , M;l o - L , ~,U,7 - '~- - - -r -4 -n-1 1: vii th f~s-
-1*- , ;, .1 .- i
L 7646-66 EWM)A!.JA(h)
ACC Mt AP502/,996 SOURCE CODEt UR/0286/65/CW/016/0059/0060
AUTHORz 11 TepLon -No - Lo- 19
ORG: none
TITLEi Kinematic filter, Class 21, *qo. 17,3857
SOURCE: Byulleten' izobreteniy I tovarpykh %nakov, no. 16, 1965, 59-60
TOPIC TAGS: filter circuit, rosom~or
ABSTRACT: Thi;3 Author Certificate presents a kinenatic filter made of a quartz
resonator connocted to the load and yTovided with an active resistance for sup-
pressing rosidaal oscillations. lo increase the effectiveness of residual oscil-
lation suppression, the active resistance Is connected in series with a switching
unit and in parallel with the load rosistarce (see Fig. 1). A negative feedback
circuit is connected botwoon the output and input of the filter,
Card 112 UDC: 621.372.543.2
S>
L 7646-66
A= 1IRt AP50ZI+996
Fig. 1. 1- active resistance; 2- switching unit; 3- load resistance;
4- filter input terminals; 5- negative feedback cirovit
Orig. art. has! 1 diagram.
SUB COIEs EGI SUBMDATEi OlAug6O
Card 212
ACC NR,AT6022363 SOURCE CODE: UR/0000/66/000/000/0012/0016
AUTHOR:
ORG: none
TITLE: Potential noise rejection ability and mothods of realization of optimal codes
I
SOURCE: Vsesoyuznaya nauchnaya sessiya, posvyashchonnaya Dnyu radio. 22d, 1966.
SaktsV,a teorii informatsii. Doklady. Moscow, 1966, 12-16
TOPIC TAGS: signal noise separation, signal coding
ABSTRZT: ExamLnation of known thooratical formulas for errors In code-transxlsuion
,systenz shows that: (1) The noise-rejection ability of an optimal (equidistant)
binary code is determined only by its base n, and is independent of the number n of
its used; (2) Within acceptable error-probability values (1073-10-6), the
~ortnogonal code having mmax ensuros a probability of information-trarAsmis5ion error
;by three or%ders of magnitude lower than ihat of the optimal binary code..Mothods of
D
~constructing orthogonal codes are briefly discussed in general terms. Orl.g. art. has:
.1 figure and 12 formulas.
,SU-B CODE: 17, 09 / SU&X DATE: 28Apr66 ORIG REF: 004 OTH REF: 000
Cord 1/1
JAI
uo
0 19
10 jot
to
a
ij
7
c 0 d L) a v ii V.F. ycpl(~V.
sffccr of gas-aaturateG ~n, cl,;ran3ch and ~:~:Ctility
.:L,;a oi titanitun 4alloyj
-;PCZ! AN SSSR. institut L yego -)Ii"vy%*, no. 10, 1963.
1:ialedcvanlya titanovy*',,Ii splavov, i
"I C 'TAGS: t i
ti 0, i: LC -I I -a I ILI
r-nd zeduced L, L L-L. U-
D 7 1
1~ C~ 11 Iv T;'ll.-', ~z
U'i
ca t;1,.2 ot:'Iizr il-~,
'bi rice. 1'.
c o
7 cablczi ove
s s () Cfiil- -iii i inct"Allurc."
Kim
ri r.' fl
11 (A
47
,)/1q1/61/OO0/006/002/oo6,
13 L) B110113201
--------------
AUTHORS: Kamenskiy, I. V., Itinskiy, V. I., Teplov, N. Ye.
'b-idrianov, B. V.
TITLE: Synthesis and study of monomeric and polymeric reaction
product6 of acetophenone -aith furfurole
PERIODICAL: Plasticheakiye massy, no. 8, 1961, 12 15
TEXT: Reaction Droducts of acetODhenone with furfurole are as follows:
-1120
0 \CHO + aico-qli,
=Cti-CO--qH,
0 \CH
_H10 (A)
k0)\01O+2CH3-CO-q11,
ai,co-C,11,
0
-Card 1/8
S/191/61/000/008/002/006
Synthesis and study of monomeric ... B11CIB201
(II) is obtained with considerable excess of acetophenone only. (1)'is
prepared by condensation of equimolecular amounts of furfurole and
acet6phenone by means of sodium eth~~late in alcohol in a yield of 60 - 80 elb.
In-consideration of the fact that the production of resins by means -df
benzene sulfonic acid catalysts and resulting resin products had be6n
hitherto insufficiently desc~?ibed, their descriptioh was the aim o~..the
present work. The authors used (l)-furfurole, (2) a'cetophenone. The
polymers were obtained (1).directly from the reaction mass without
separation from monofurfurylidene acetophenone (1,1FAP), (II) by way of
resinifict,.tio'n of ;tFAP. The product produced-by Harvey's method (Ref. at
USA Patent 2,461,510 (1949)) loses fluidity on, the passage to the B stage..
nardening takes plac~e ~' 2500C during 30 minutes with the separation of
t
50 ~j of volatile parts. The authors ,-rashed the reaction mass with cold
water, dried it at 1000C~Ind 15 mm H& during 3 hr, thus obtainin a brorrn
14 ~~ furfurole, 16~!.
oily liquid. A vacuum distillation yielded: , 0
acetophenone, 60-1/'0 I-WAP, 10 c' resin. After 3.5 hr of heatine at 250 C a
fusible black resin (dropping point 6500 was obtained. On addition of
benzene sulfonic aci acetone solution) th~ resin is hardened
9 (5 0
during 19 minutes at 250 C under separation of 40 % of volatile Darts and
Card 2/6
2 5596
S/1C, 1 /6 1
Synthesis and study of monorrE!ric-... B110/B261
formation of foaming products~ Table I shows that in :-iiAP producLior,
under optimum, equimolecular conditions, a temperature drop
I reduces the resin formation ard a,, the same time i-E;tar.*,,s thc ~-,-.FAP
formation. An increase of the catalyst amount (experi,-.ents 4?'~"'-l '2)'
and a concentration IncreaBe of its aqueous solution (exp'ril~,erts -io - -,I),
however, speed it up. At room temperature (experiments b - 12), !,1FAP is
obtained without resin, 20 g KOH in 20 g H 0 were added ~,y drops to 1,6 j-,
furfurole and 120 g acetophenone within 20 ? .50 minutes, neutralized /kith
0.5 11 HC1, washed with H20 until Cl ions were removed completely, and drit-i
in vacuum. "'IFAP is briCht-yeljow, f ine-crys tali lir~e 'i-ith the meltin,~~ p3int
41.80C, and 89 ~- of the yieid, soluble in ail
(to 12 ~(. in petroleum eth~,-r),, Its specific grit-ilty Ya6
point 166 0Cat 11 mm Ht.~, 18100 at 9 ht- The 'molecular weiilf-t.
cryoscopically deteri;;Jned in dioxan Vi"s 19~"E~' tJ~'-'
since benzylid~.,.ne auetopkienon~-- compounus auc two 11,y(jr-nYy1 al-uinf~-
Resinification took place (I) thermally, (11) in thL. Pruzer:c. of a
According to Table 5, rf.-;inific~itiorl
(25000 with 95 - 97 ~,' yield, jince Lvrzene null"unic acioi (111,~;Aj '11.j
Card 3/8
I /CjoU/u(j,: A~u
Synthesis and study of mono:..eric
(Table 4)dinoolvu in tho rionvmF:r, tii,~, I%ttur wo to n a h r
necked flask, and 1 - 5 catal.-/ot w,',-. add~--d ~,'!Aer v4:'-~ 1
f -, 1) 1*
rosin obtained in a y i e 16- of 1~6 s Ib r i t1 ea tro o ;i. p
W-5 9) monomer in -wG al to ~ uerie -1 el'];"a w~
monomer) a viscous, rut-I-er-like maSZ3 wi.;,Ch
Melting, ~.inssolutle polymf-r. All w-1,
and a sl-ecific gravity ~f 1 ~1 The ~iro:,Pir!F
Obtain,-d witiout B!;A w;.is 7) C; 0'at Of r~.,,njr, ijz3;, w;,~l
The resins w,!re found to be well. soluble in I ',,I (k,*rl VIktiVI,:; , (j
chlorohydroc arbor., various %etonic.-, (~~yclrLexanune). iscar,-,ely in
and others. FractionL.Lini; reco,-razing a polya rot,
Four fractions were separated frow -1 10 % acetorit; !.joluticln: i
residue, (2) and (3) wt.-re separat-fd by adi.i tion of' 10 -1111 II)o to a !".-0 -,,;1
solution, (4) by means of' 1W0 ml Irl 20 Infrared apct;tra 16r
produced without (1) and with (11) catalyat y1oldQq CO t,%nd.,j
1 1.
(1685 1665 cm- ) and double *Lond bands (1047 1621 cm- ) 1.11 tile -,;O1ljUgatc
-11=C-O-system. The double pea',.,; lvc-re. howe-or. foan~t to 'ce weaker
particularly with (1). The pe~,k of othylene Lond(121(4~ - 1~lo exists
only witI, monomer tend (1j),. The abzjorrtion b~.tnd of' the fz;rP--I r;.nir
Card 418
Synthesis and study of monomeric...
-2-5596 7
S/19 61/000/000/002/006
Bi 1 OXV2011
(1131 - 1189 cm is weaker with (I) and (II) than with the monomer. The
pea%s of the benzene nucleus (1110 - 1070 cm- appear in the three spectra,.
1
whereas the furan ring-bound in o~ p(I -pooition .(1378 cm- ) was found only
with (1) and (i1). There are 1 figure, 5 tables, and 15 referencesi
6Soviet-bloc and 9 non-Soviet-bloc. The references to ~nglish-lanruage
publicatione read as follows; Ref. 71 US Patent 2,4611508 (19A9); Ref.. 8t
US Patent 2,461,510 (1949);' Ref. 9: US-Patent 2,768,406 (1956)
.i - - - I . t
tiN
. --- I - I .
- ---- - - --- -.- - - - - - - - -- --. ---- - - ---- -,-- - -- -, - - - - - I- I- - kw
I.,
5LL
Agm
tz-,
N-Yes; KABACHNIK,
th
r-, thy
A.1:164-166
ganichesidkh
Trj.,-.tjtv1, el,mentoor
ri'au"e'l IlLy 17, 1965-
TEPLOV, O.V... mladshiy nauchnyy ootrudnik
Role of human ascarids in the epizootiology of ascariasic in
piglets. Trudy VIGIS 11:156-160 164. (MIRA 18:12)
ABUSITOV, S.K., Izobratatell; THPLOV, P.V.. izobrntntn11j GOGULIN. I.Ta.,
loobretatell
r- ' Dealgning now loomo. Izobr.v SSSR 2 no.2:5-6 7 '57. (MIRA 12:3)
1. Gavrilovo-Poaadakaya tkatakaya fabrika.
(loons)
TVIOV. S.I., kandidat meditsinskikh nauk (leningrad); SCKOLOVA, To.A.
tZftlngrad)
Iffects of the cerebral cortex on the cardiovascular system connected
vith imminent surgery. Klin.med. 34 no#9s4l-4? S 156# (MLRA 9:11)
I* Iz teraparticheekogo sektore (zav. daystvitaltayy cholon AKK SSSR
profs H.T.Chernorutakiy) Institute fistologii im. I.P.Pavloya AN 6SSR
(dir; akad. K.H.Bykov) J Gospiralluoy khtrurgichoskoy kliniki (dir.
profa- F.G.Uglov) I leningradekogo meditsinskogo, Instituts iment I.P.
Favlova (dir. A.I.Ivaaov)
(SMXRT. GPXRATIVA. psychol.
off. of cerebral cortex activity on cardiovasc. system)
(CUR RAL COMIX. physiol.
off, of cortical activity on cardiovase. syntem before
imminent surg.)
(CARDIOTASCUIAR SYSTIM, physiol.
off. of cortical activity- befor imminent surg.
EXC",RPTIA =CA Scc.18 V01.1/0' Cardiovascular Jimo 57
1795. TEPLOV S. 1. I-ab. of Elect rophysiol., 'I.P Pavlov' Inst. of Physir"..'
Lening-ra-T ~-xeri~mcntal coronayy insufficiency and its Yeproduction as condilioned
-Ycllcx (Russian text) Fiziol. Z. 1956, 42/9 (7115-751) Illus. 5
Lv. injection of posterior pituitary extract (3 units in a dog of 21.5 kg. and 5 iinit,
in another dog, of 13 kg.) produced within 30-45 sec. sinus bradycardia ('10 to 110
beatsIn-iin.), prolongation of the P-R interval (by 0.02 to 0.03 sec.) and of the Q-T
interval (by 0.04 to 0.05 sec.) and an increase of the T wave by about 3 times the
orivinal amplitude. The peak amplitude occurred 2.5 to 3 min. after injection and
disappeared in the 6th to 7th min. These changes, interpreted as due to coronary
insufficiency, could be reproduced by a conditioned acoustic signal applied 30 sec.
before injection of the extract. Conditioned bradycardia appeared after 80 repeats,
prolongation of the P-R interval after 120-130 repeats and conditioned increase of
the T wave after 100 repeats. Although the number of repeats necessary for the
iormation of the conditioned reflex was unusually large, the conditioned response
was in no way different from the direct effect. Once established, the conditioned
reflex was very stable; it disappeared only after 150-160 repeats without reinforce-
ment. Simonson -'Minneapolis, Minn. (11, 18)
EXCERKA MEDICA Sec 18 Vol 3/6 Cardiovascular June 59
V323. Alechanism of electrocardiographic changes produced by pain stimulation
(Russian text) ILJINA A. 1. and Trm.ov S.I. 1.P. Pa% I,)%- inst, of Phviol. and iab,
of Pathol. Physiol., District 31ilit.-TPTs~peningratl A. 4'*,S (7211-;26)
11111S. 5
Electrical stimulation of the sciatic nerve in a curarized cat produced a slight STS
elevation within 5 to l0min., and a more pronounced s'r, cievation several hour--.
after stimulation, coinciding with the first and second phase of blood pressure
elevation. These changes were prevented by bilateral denervation of the adrenals.
Simonson - Minneapolis, Minn. (11, 18)
1 71T-
TEPLO7, S I.
Reflex renctions from the stomach on the blood in exDerimental
gnstritis [with summnry in BzWIishj. Biul.eksp. biol. i med. 46
no.7120-23 Je 158 (MIRA 11:7)
1. 1% ekeDArimentallnoy lAborntorii (nach. - knnd.med.nauk S.I.
TA2-1-OVj Leningradekogo okruzhnago voyenno-Co
Sokolov). Predstavlena deyetvitelinym chlenom SSSR M.D. TuBhinakim.
(GASTRITIS, exnartmentnl,
eff, on 1e*ukocyte count (Bus))
(LMKOGYTE COMIT,
exper. gnatritis (Run))
IRCLIKIS, A.V., TEFLOV, S.I.
Chazges in the 9ecretomotor activity of the stomach In experimental
gastritie [with aummaz7 in Znglish]. Biulfekspblol. I med. 46
no.831A-48 Ag '58 (MIRA 11:10)
1. Iz Leningradskogo okruzhuogo voyennogo gospitalya (nach. NOS*
Sokolov) Prodstavlena deystvitellrqm chlenom AMU SSSR N.D. Tushinskimo'
(GISTRITIS, exper,
off. on secrotomotor activity of stomach in dogg (Rua))
(STORACH, physiol.
off. Of expero gantritis on searetomotor activity In
dogas (rluu))
TOWNE, A.V,; IL'INA, A.1.1 TITWV, M.
A'---,-
Nechanisms umderl7lng changes In coronary blood flow accompanying
pOn stimuUtion. Fiziol,zhur.SSSR 45 no.71753-76o 11 159.
i (KM 13 -4)
1. 1aborator1ya*nervno7 trofiki Inatituta fisiologii im. I.P.
Pavlova AN SSSR, i Pitofiziologichask&ya laboratortya Okruzhnogo
vo7eunogo gospitalya, Uningrad.
(OORORART VMS= physiology)
(PAIN pbysi6logy)
I
T0NKIKHv L.V.; ILIINAV A.I.;_ TFJ'LGVg S.I.
Pharmacological analyeic of the mochanim of changes in the blood
pressure and coronary circulation folloving painful oti-Ilations.
Fiziol. zhur. a no.120-456-1462 D 160. (MIM 14: 1)
1, Laboratoriya nervnoy trofiki. Institute, fiziologii im. I.P.Pavlov,a
iii SSSR# Leningrad*
(BLOOD PRESSURE) (COROHLRY VESSELS)
(PHAF14ACOLOGY)
TONUKHj A.Y.; IL1111AV A.I.; TEPLOV, 3.1.
Chan,jes in the coronary circulation and blood pressure during
Btimilation of the hypothalamus region. Fiziol. zhur. 47 no.7:
801-105 J1 161. (MIA l5sl)
1, From the Laboratory of Tropic Innervation; I.P.Pavlov Institute
of Physiolo y Leningrad.
MR&M nskz) (BLOOD PIMSSURE)
(HIFOTHALAWS)
TEPWq, Ser s
:&~, Iv novich- VA ILEVSKIf, N.14., red.1 W110110VA, 1,M,j
"OHM "
. _- vl---T , G.A., tekhn. red.
te . red., MA aSH
(lieure-I and hormonal regulation of coronary blood circulation]
Nervna:Ia i gormonalInaia reguliatsiia koronamogo kroboobrashche-
niia. Leningrad, Medgizp 1962. 142 p. (MBU 15:6)
(CORONARY VE&SLS)
L 29213-66
ACC NR, AF6019078 SOURCE COEE: WV023916510511005105541056.3
OTf,: laboratorf of' the Physiology of thei Vegetativa Mirvwus System and Nervo TTo ci.
P4
Institute cf Physiolo L.P. Pav3nv,, All SSS.R,_jqn-L d(Laboratorlya fizio-
paA
loif1__v"c__go1_.,a_t_ivnoy nervnoy siste,--rf i Tervnoy trofikl Instituta fiziologii A-14 S&Z)
TITIE: Role of ach-enargic vechaniar,3 In tim dovaloS~wit of prolonged changes ir, the
olectrocardi,igram and blood pressure following stipulation of the hypoth4.J4r,-qJ_
SOURCM FizioloGicheskiy,zhurnal SSSR, v. 51, ao. 59 J,965,9 $514 -563
70PIC TAGSt EKG., blood pressure,, catp vasopressin., horrone
ABSTRACT: 'Alit experimonta conaucxen an cato, atirrulation of the anterior regions
of the hypothalamus produced a two-phano (dopreanoi-preanor) reaction of the blood
prenaure followed by dovelopcont of a prolon,-ed (up to 3 hours) wave of blood
proeoure increase. Pirthermore, pronounced und ntablo charGes in the EKG, spec-
ifically in the ST ael,,,ment and T wnve, wc~rc obaerved. Upon an intravenous inject-
ion of nhlorrromazine (largnctyl) or dene:-vation of the auprarenalo# the prolonced
pressor reaction and 'the pressor phase of thv Initial reaction were abeent, while
no changes in the FXG occurred. Irritntion of tho poaterior-median hypothala=s
generally produced either no change or a 1,Tadual de,.renoe in the blood pressure,
while the changes in 'the LXG were minor, In three axporimente out of 12, a pro-
cipitato drop In the 1;1ood presoure took place. Th3 effects of the Mainietrat-
ion of chlorpromazine or donervation of the cuprarcim13 indicated that the pro-
longed preanor reacticn. produced by irriltE.tian of the anterior hypothalamm was
due to a horm,)nal reaction initiatad by adranalin mid remating in the evolution
of vnaopreasin by the anterior hypophyoto 4 Blocking qf~ -the Jaupply. of adrenealn
eliminated Ahq preaeor reactl "n" haut 6 f1meas
115IJB CQEt 0/sum rMt 2~JanX)4 Oq~J( - 8 02F
'fff7gO9 / 0711 REF
U Dr,
L 28045-66
ACC NRj J
AUTHOH: Ton1':ikb. A. V.;
, 0239 6)/0
T
111ina, A. I.; IePlov) S. 1.
ORG: Laboratory of Phyviology of the Vegetation Nervous Syaten and Nerve
Trophism, Instituto of I-V im. I In
_FjiLqiolo F. Pav GV _AjjjS~ft Leninj~r
Ad
slatenry I nervnoy trofikd
(Laboratoriya fiziologii vegetativncy nervnoy
Instituta fiziologii All SSSH)
n)ot i upon Irritation
TITLE: Changes in the electrical activity of the h
jAjazaL
of a sensory nerve or administration of adrenaline
SOURCE: Fiziologicheskiy zhurnalt v. 51,*no. 6, 1965p 755-761
TOPIC TAG3., pharmacoloUt electrophysiology, catp EEG, brain# blood pressure,,
rasoprcssln, animal .physiology
ABSTRACT: _Ln experiments on catst Irritation of the central end
oi a severcd sciatic nerve (a pain Irritation) and Intravenous
in~ectlon cf adrenaline had the s.:uae effect on the electric acti-
vity of the hypothalamus: the activity In both the anterior and
posterior divisions of 1-1he hypothrtlomus was Increa-sed (desynchro-
nlZatlon of EEG rhythris took rjlaoj~ ~rjjjA t'410 fjj[jpjj~V,.ds~, Of
1.,'a'. I j-..o r"a "; ei I F, r ca c 'L, 1. c n c o: L i,, c 10, (1 w I F,, i an I x 10 ro I t;,,
1.5'-" lirs. afte:~ t-h" prl."-ary effect; (al-iLlulution
jof thc-! elea.trlcal cLativity-of the hypothalamus *following the-pa-kn-_.,,.
.CLa-rdy U
-----------
1, 28045-66
ACC NRs A.P6018179
jrr~tat.,~,on- or- injection-of a r
al Intl R-detiond I-nerease in the,
'lc . ti inc, I -
_0 t cai a'c Vity,of the hypothalnnun, took place, c0
ed I','I'th the pxolonged wave of blood pressure increase described
In the authors' earlier work. One may assume that a chain neuro-
,hormonal reaction Involving stimulation of the hypothalamus do-
-veloped both in responso to Irritatiop of the selatio nerve and
I
ito injection of adrenaline. Irritation of the sciatic nerve
I
Istimulated the sympathico-adrenal system; vavooonstriction under
the effect of nerve action and also release Into the blood of
i
adrenaline and vasopressin, which was oontrolled by the vegetative
icenters of the hypothalamus, took placo. The initially released
Jadrenaline stimulated the hypothalamus, with the result that
::vasopressin was releasedo producing the seoondl prolonged Increase
orig,
,in blood pressure, whieh was of purely hormonal orISI4. ........
---- art. -hdd':__ 6 figures. lin..S7
SUB CODE: 06/ SUBM DATE: 3OJan64/ ORIG REF: 0051 OTH REF: 009
2/2 e_ ~,
VALSWYEVA, L.f.; TECU;'j,
Changes 'in "'ne coronary b-ioccl fl()~~; In
fibers of the vap-l-In n,?,rves Fi7iol.--'!~ur. 51 165.
18:10)
1, laborato-Hy-, f,7--*r,-.'u--71i W!,,-?,tAat,lvnoy nerjnc~v i nervrioy
trofjlki !*i-,,,,~-:3--)z:-'li I.P.Ilavlovr., AN Lcnin~rad.
-~r -- .-), ~~i ~111 6" Iv.
f , YSLIZAROV,P.P., kandidat takhnicheakikh nauk; TEPLOV,S.V.. inzhener
*W.V.
Heat losses during the starting and shutdown of the TP-170
boiler. Teploenergetika 2 n0-7:38-44 Jl 155.' (KLRA 8:10)
1. Moskovskly anergetichookiy institut
(Boilers)
BLOKHIN, V.N.; GRIGORIYEV, M.G.- KOZIMUIXCV, A.I.- KOROLEV, B.A.j MATYUSItIN,
I.F.- PARIN, B.V.; TSIWUW, I.L.; KALIHIRA, G.V.1 FEDOROV, A.M.;
KOLOkOLITSE;V., M.V.; SOKOUN, V.V.; PRILUCHRAYA, O.A.; SHUMIUDIA,
Ye.I.; ABRAMOV., Yu.G.; FUMOV, A.Kh.; IKONNIKOV, P.I.; VOZ!-iz.3Z.'!SKIYJ,
I.Ya.; TUk2~~; NIZINGVp N.H.; KUKOSH, V.I.
V.M.Durmaohkin; obituar7. Ortop., travm. i protez. 21 no.801 Ag
160. (DURMHKIN,, VIKTOR MARKOVICHp d. 1960) (MIRL 1311-1)
ACCESSION NR: AP4004156 S/0294/63/001/002/0318/0320
AUT11OR* Filimonov, S. S.; Kryukova, M..G.-, Toplov, S. V.; AyrJqtov,
A. A.
TITLE# Test stand for studying heat transfer in the flow of liquid
aluminum in a pipe
SOURCE: Teplofizika vy*sokikh temperatur, V. 1, no. 2, 1963.
318-320
TOPIC TAGS: heat transfer, liquid aluminum heat.exchanper, liquid
metal, liquid aluminum, aluminum hent.trnnsfar, heat exchnnper,
liquid metal coolant, coolant, fluid flow
ABSTRAM A test stand has been designectifor beat-transfe.r studies
with liquid aluminum. The use of liquid-aluminum an a heat-trans-
fer agent in heat exchangers operating at tempornitureetexceading
1200C is being investigated since difficultion*are encountered
with alkali metals at such temperatures. Fig. .1 of the Enclosure
shows the test assembly. An induction-type'electromagnetic pump
with a traveling magnetic field (capacity 3 m3/hr) was specially
Card