SCIENTIFIC ABSTRACT OSTROVSKIY, L. A. - OSTROVSKIY, M. I.
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Collection:
Document Number (FOIA) /ESDN (CREST):
CIA-RDP86-00513R001238510019-1
Release Decision:
RIF
Original Classification:
S
Document Page Count:
100
Document Creation Date:
November 2, 2016
Sequence Number:
19
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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16 10207-63
AcamIct, NR: AP3000053
gmatly Indebted to A. V. P!~MOV and V, p, Dokuchayev for discussing the
results." orig. arto bm: 8 formiaso
ASSOC=on-. radiofizicheskiy Institut Gorlkovskogo gosudarstvannQgo
univeraiteta (]MiOPhYJ3iC3 InStitUte, Gorlkiy State UniversitY
22xov62 DATE ACQ: 12J=63 ENM: 00
an NR M? SDV: 005 000
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- ---------- - - -------------------- -----------
OSTROV6KIY, L.A.; STEIANOV, N.!~.
Paranel.ric Fenert!on of electrovignetic waven In a Mqi7np*.oa-t'vp
plasma. Zhur. eksp. i teor. fiz. 4111 n-,.5:1473-1478 N '0-~".
(AURA 1-,I)
1. Radiofizicheskly InstiLut Gorlkovskof7o i,osudarstvennogo
universi teta.
ACCESSION NRs AP4025929 6/0056/64/046/003/0963/0969
A.�..,j Yakubovich, Ye. I.
AUTHORS: 2R&LQmfl4Y,.
TITLEt Averaged laser equations and their stationary solutions
SOURCE: Zhurnal eksperimental'noy i teoreticheskoy fiziki, v. 46,
no. 3, 1964, 963-969
TOPIC TAGS: laser, laser nonlinear equations, laser rigorous non-
linear equations, laser averaged equations, two level laser, sta-
tionary nonlinear laser oscillations, oscillation frequency spec-
trum, field spatial distribution, nonlinear laser modes, periodical-
ly varying oscillation amplitude
ABSTRACT: The difficulties involved in solving the rigorous non-
linear laser equations are listed, and it is shown that some of the
solutions obtained are incorrect. Some laser theory aspects con-
nected with the influence of the nonlinear medium on the field struc-
Card, , 1/3
ACCESSION NR: AP4025929
ture are considered, and.it is shown that the initial equations can
be averaged under some general assump~Aons and reduced to a lower
order system for slow time-varying quantities. in particular,
averaged eq6ations are deriyed for the electromagnetic field in a
two-level ac'tive medium without expansion in the eiganfunctions of
the unperturbed system, and are solved for stationary nonlinear os-
cillations in a plane layei with arbitrarily reflecting boundaries,
which can be regarded as a one-dimensional laser model. The fre-
quency spectrum of such oscillations and the corresponding spatial
distributions of the field phase and amplitude are obtained. The
components obtained determine the finite number of possible non-
linear oscillations (modes) whose frequencies differ from the natural
frequencies of the unperturbed system, and whose amplitudes and
phases depend on the coordinates. it is emphasized that the super-
position of these modes is not the solution of the problem and that
the question oi existence of other stationary processes (auch as os-
cillations with periodically varying amplitudes) still remains open.
Orig. art. bast 2 rigoes ajA 19 fc=ulfts-
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ACCESSION NR: AP4025929
ASSOCIATIONs Radiofimicheakiy institut Gor'kovskogo gosudarstvennogo
universiteta (RadiophyaLcs Institute of the Gor'kiy State University)
SUBMITTEDs 09Aug63
SUB CODE: PH
DATE ACQ: 16Apr64
NO REP SOVt 008
ENCLs 00
0 THE Rs 001
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L6090-65 FL,,0-& Aem-""Ifz nw? '7; [k I- Ih i.;71 /FZ
AM5017153 BOOK MPLOITATION UR/
621.3-17-01.077
Ostrove Lev Aleksandrovich
Principles, of the general theory of e1eqtgi_a_WA-ijv1,! L
(Oanovy obahchey teoril elektrolzmEritelInykh ustroystv) P1.0scow,
lzd-vo ItEnergiya") 1965. 530 P. Illun., biblio., 1nde 2C *9500,
copies printed.
TOPIC TAGS: electric measuring instmment, transducer$ energy con-
versions electromechanical transducer., oscillatory circuit, fre-
quency response,error correction, servo measuring system, servo-
syatem, digital measuring circuit, astatic scrosyetem, servosyst%em
PMPOSE AND COVERAGE: This book is intended for technicians and
engineers. ooncerned with the development of methods of,electrical
measuring and with the computation and design of all types of
alan+vvinal measurinj% ectuipment. It can also be used as a textbook
Ca rd 1 /10
_7771
L. 60985*-Z5-
AN5017153
matchingt and their frequency and transient characteristics. The
structural forms of the basic types of various measuring circuits,
their special foaturec, specific errorej and some compn correction
methods are d1scusoed. The basic types of modulation ,tand demodula-
tion in open meaouring circuits, as well as t5e opirtloo of
^Innprt astatic and static measuring servosystems, are Investigated.
jut
.A.60989-65
AM5017153
-6, -Even and odd effects and their relation to-the linearity of
converters -- 42
'Ch'i n. Equations describing maauring converters 45
1, Genexiil considerations 45
Various types of converter equations -- 46
he relationships of reciprocity and the conversion
._-Seleotion-of-goneralized forces _iid__060rcKM_tbs-"--56-
Equations describing the basic typea of electromechanical-
7~---converters _t!! 60
6, Equations desmilbiht-a--thermoeleotrio --converter ~w-_71.
Ch, M*' Basic technical parameters of measuring converters 79
- 1, General considerations -- 79
_~_._I~,_-Converoion factors -- 80
Comiter reoistAnces -- 84
SenxitIvI of measuring converters --.94
.5. Basic origria. regarding the efficiency of converter
power transmission -- 102
to load
_05017153
Ch. XV. Conditions for obtaining optimal converter power 112
l,,_,'r1Genera1 considerations -- 112
2, Operation of a finite internal impedance source on a directly
connected load -- 115
3. Converter operation on a load under given voltage (given force)
conditions -- 123
Converter operation on load under given current (given velocity)
conditions -- 125
Converter operation on a load under given power (given energy
flux) oonditions -- 127
6, Operation of finite internal impedance sources on lo&d through
Intermediate converters -- 131
7, -Matching of load resistances and converters by means of
transformers -- 235
-Ch, V, Oonverter dynamic properties, Notion eq%~ations -- 144
-I& 0eneral considerations -i.- 144-
-2. Xnveotigation, of-the motion of a movable part of electro-
mechanical converters by the method of analogies -- 146
-cwd 4/10
-tr -6~-65
U5017153
3,. Series oscillatory circuit under the action or an external
sinusoidal emf
147
Basic,dynamic parameters of a converter characterizing
attenuation "" 152
Series oscillatory circuit under the action of an external
suddenly-varying emf -- 157
Parallel oscillator an external
circuit under the action of
-sin'usoidal emf 8
Engineering criteria for the stability of system equilibrium
and its phase picture -- 171
Phase-pioture of an oscillatory system in the absence of
175- -
9,, Phase picture of an ozoillatory-synfem with-ettenuation--177
Phase picture of an oscillatory system with negative
attenuation -- 179
-.11, Phase picture of a system in the presence of dry friction,
Error due to friction -- 181
40h VI, Frequency characteriatio,s of converter and measuring
..Instruments 186
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1 60989-65
AN5017253 0
Genera2 considerations 186
Frequency characteristics and mathematical methods of systemn
research'--- 189
'Various methods of frequency oharaoteriatio representation -398
4, Frequency characteristics of oscillatory systems, Converter
operation prior to resonance -- 205
!3, Frequency characteristics of oscillatory systems. Converter
operation during and after resonance -- 21T
6. Frequency characteristics of degenerating systems, Differenti-
atIng And integrating properties of a circuit -- 223
7, Frequency characteristics of aperiodic systems. Differentiating
and intograting converters -. 226
Ch. VII. Transient (time) characteristics of converters and measuring
i instruments 234
1, - General considerations 234
24--- Tranoie _(timo) characteristics and mathematioal-methoda of
nt-
systems reoearoh -- 236-
Transient characteristics of onoillatory ayesv-emu 244
Transient characteristics or some aperiodic aystems -- 250
09-
AX5017153
U
5. Interrelation between frequency and transient characteris-
tics 256
~Cho' VIII. Methods of correcting converters In measuring
oirouits .62
1, General considerationa -- 262
2, Distortions in the conversion process resulting in measurement
errors -- 263
30 :Stabilization of converter nensitivity during the action of
external factors and problezrLs of temperature correction -- 270
Basic methods for correcting the nonlinearity of measuring
convertcra -- 275
Methods of correcting frequency characteristics 288
Ch. 3X. Some operating principles and. basic struotural formtj of
modem measuring devices -- 302
General considerations -- 302
2,' Open measuring o1rcuito with direct evaluation -- 304
Pon automatic measuring circuits with time scanning 320
Closed servo manuring circuits vith discrete action 364
M -X ulto -- 369
Open measuring o1ro
- General considerations -- 369
'2t Parameters of circuits consisting of series connected
converters 310
Modulation of a sinusoidany varying oscillation -
376
Pulse sequence modulation -- 396
Criterion or information erficiency for measuring instruments
with varims forms of modulation -- 407
6. Basic methods of demodulation 418
7, Open measuring circuit errors 435
-Ch._n,_____Astat1c servo measuring comparison devices 443
-1. General oon"derati0n13_--- 443-
-20- Investigation-of the dynamic propertles of systems by sub-,
atitutlng standard sections L 445
36 Basic standa.rd oubstituting sections. Aperiodio type'o'f
.448
_6rd --ratio.n
1,-60989-65
AM5017153
Auxilary standard soctIons 453
5 Special features of input measuring circuits In Automatic
comparison devices -- 456
of closed automatic circuits and equ tions of
6. Sensitivit a
motion -- 459
Servosystem measuring errors under steady condition 466
S.
Ways of reducing servo measuring errors under steady con-
ditlons and the principles of correction __ 476
9, Stability of servo measuring devices _- 482
-.1. 10, Correction of the transient characteristics in aetatic meaeur.,,
Ing instruments -- 484
Ch# 11L - Static - se--rvo measuring devices with direct evaluation 491
1, General consideratIons __ 491
feedback."n static systems 492
2# 'Various types o.& A
-independent
3, Basic properties of static systems with frequency
feedback -- 497
4. Stabilizing action of negative feedback and errors of static
- servosystems -'" 507
5, Examples of the investigation of some statio servo measuring
dwatems 515
SqO_ 9 A
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uR/ol4l/65/oO8/ool/o09j/ocq7
AUMIORt Ootrovokiy, L. A.; Yakubrmich Ye. I.
TITLE: Steat'qr-state oscillation of a laser th distributed looses
SOURCE: IMs. Radiofi.&Uta, Y. 6, no. 1, 1965, 91-97
TOPIC TAGSi laser oscillation, laser loss, laser operating mode, laser active
medibm
~ABSTR=: This is. a continuationcC na eulier vork (zhm v. 46, 962, 1a.64) devoted
to possible stationary (monochromatic) processes in a laser. In the present
article the authors ptudy the bebwAor of electrorAgnetic oscillations in a plane
active medivn under the.aasumption that the enerMr losses are due not only-to ra-
diation through the layer boundary, but also to losses In the medlum iteelf, vhich
contains active molecules, The report conaMers the one-dimensional probum (f, oc~dlla-
+4rma in a nlane-bardalel 1wrer containing two~.level active molecules. A phants-
tC*_d_7_V_
-7-
L 48092-65
ACCMXON mRs AP5=68i
pbaae of the~field In space. It is shown that several stationary frequencies are
possible In the case of a thick but limited layer. If the layer is sumciently
thicks then to each frequency there corresponds also a finite number of modes vith
different field distributions in space 4nd with different values of outputpower.
-To determine the exact oscillation that will be produced it is necessary to win-
lyze the wnstationary processes in each case, including the initial disturbance
- - I- . -V V6. 1,564,r~ "Th* authnra thank A. V. namnav fnr In-
I UUc vu WRI&a
n -the-vork-and-for a MoMelon oi- the vemlltao-ll - OrUv- "t-a- ?%A*
st--l
tire
figures sad 2.6 formul4ed- [021
.ASSOCIATION, Muebno-inaledamtellakiy radiorizichaskiy institut pri Gorllwvakcm
uAiTerolteto (Scientific Research ties Institute attbe Gorlkiy Universi-
80MMMI 2&4u,64 EMLs OD SUB COM EC
30 mw OTEmi 000 XW PFMBS 1 1002
I I I I
- , . I . . I I
L 01178-66 EY1T(d)/EEC(k)-2/EED-2 WS-4
I
!ACCESSIM XRs AP5017654 LM/0109/65/010/007/1176/1180
621.391-814
MTHORt 09trovskin L, A,
freguenoy-imodulated signal
'T1Ms Emagation of s in dispersing systems
ISOURCE: Radiotekhnika I clektronika, Y. 10, no- 7, 1965, 1176-1180
iTOPIC TAGS% As the Fourier method is inadequate for analyzing the propagation of
IFM waves (com4ressed pulses) In dispersing systems, the present article offers a
imore general aolution based on a time-domain approach. Variation of frequency In
i
1.a frequency-modulated wave, propagating in a system having an arbitrary dispersion
characteristic, is described by a first-orxier nonlinear partial differential
equation. A Riemann Integral Is the solution of this equation In a aingle-variablo
case. The variation of the wave amplitude depends on the shape of the frequency
envelops. It Is found that, under certain conditions, the dispersion results In
la grouping cf the wave energy within narrow Intervals associated with 2brupt
ifrequency changes. A certain similarity between the propagation of group fronts
4'In a YN-wave and the travel of particles In a volocity-nodulated boam Is noted.
."The author wishes to thank A. Y. Gaponov for discussing the results." Orig. art.
jhaBs 16 formulas* q4
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L 01178-66
'ACCESSION Us
ASSMIATIONs none
SUB)117=t O4May6-4 ENCL 1 00 SUB CODn HO
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Card 2/2
0v.%. Im AttVJ3-j4U SOID(CE CODE: UR/oloh/b5/oDo/oDh/ooW/ouj3
AUTHOR3 ODtrOv3!dx%LoA6 (Engineer); Usykiyar, N.V.
Owl: none
TITL33 7YPe TPP-20D boiler for 800 Mw eyatem
SOURCEs Elektrichaskiye etantsii',~no, h, 1965t 6-13
70PIC TPS: electric power engineering, thermoelectric power, steam boiler
ABSTRJCT: A general deacrJption of the deai(:n,, construction And constructive
lessons learned in producing a series of power system baiAere, including the types
TPP-110 and TPP-210 of 300 Rx'cApncity ind the TPFL-20D, designed for use in power
systems capable of producing 8W Uw. The troup includes both sin&le and double
block boilers, the lptter having been found to be preferable, since r- breakdown
requires oray x tempDrprv reductioli tn power cmtput an one section is shut down, not
P complete abutoff. Croas-3ections and diagrma are presented to explain the
operatim and design fePtures of the TPP-200. Orig,, art. hPar 5 figures, Pnd 2
tables. TJMI
SUB CODE: 09 / SUM DATEt now
UDCI 621.18.65
L4 V,
I IM7 Vm)-V pf-.4/ _4/m-4/Pm_4/Pn-4/Po_4/P*b ii c WQ
M016 Pi
ACCE881011 Of o4 UR/OW~65)/C48/6(*/l()B7/101fi
AUTHOR: Ostrayakiy, Lo At
TITLE: Intiraction of oscillation modes in a laser
GOURM -Zhurnal eksp erimertallnoy I, teoreticheakoy firiki, v. 48, no. 4, 1965,
1087-1096-
TOPIC TAN: laserp one mode laser, two mode laser, laser cavity, laser atmbility
ABSTRACM It is pointed out in the introduction that the customary asetumption
made that Wer transients involve only one fundamental cavity mode are not al-
ways satisfied-in practice, and that more modes must be taken Into account. The
author then proceeds to obtain, within the framework of the model of a two-mode
laser cavity, a bufficiently complete picture of both the ataticnary and nonsta-
tio=7 processes occurring in the laser. The modes are assumed to have different
frequenpies and the lazer equations are redusced for this case, try an ave-raging
-metbod to &-system of dimensionless abbreviated equations of third order. The
A
phase pl=e method in used to Investigate the atability of the monochromatic end
tuo-mode operations and to describe the -transients In the laser. "The ttutlwr ia
Card
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____ACCMWCff RI - AP5016504
grateful t* A. Ve QsRMWqLnd Qt_j, ZXV&ULan_f_qr a discussion of the results.
OrIg. art.-bast 2 fisures and 17 formaas.
ASSOCTATIONt RadiotiticbeekLy inotitut G*rlkovskogo Sonudarstvennop univeralteta
(Radioplqsics Institute of the Gorlkiy State University)
SUMTM: 31juJ64 ENCL,. 00 m CODE: EC
MR MW EMS 007 omrm oo4 ATD PREWt h001
L 10261-66 FM/EWT(I)/EEC(k)-2ft/,EWPtk)/,EWA(M)-2 )VA(h) SCTP/
ACC NRj ApSOOD23.2 SOME CODE3 W0056/63/049/003/1535/1543
AMR: 2drovsLd& L. A.YY
OW: PRILdig2br-sice Institute ot the Gor"hix jalme Itan -'a1YFftdIof1zIchesk1y In-
titut GoOkovaUgo gosudarAvennogo universiteta)
TL193 Autanodulation of ratUation of a laser2-1