SCIENTIFIC ABSTRACT MOUREK, J. - MOVCHAN, B. A.
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CIA-RDP86-00513R001135420010-4
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S
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100
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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Body:
TRAVNICKOVA, E.; MOURSK, L.:,TROJAN, S.
The effect of repeated blood losses on resistance to nitrogen and
stagnation anoxia during postnatal development of the rat. Physiol.
babowslov. 11 no.3:231-235 162.
1. Institute of Physiology, Faculty of General Medicine, Charles Uni-
versity, Prague.
(HEMORRHAGE experimental) (NITROGEN pharmacology)
(ANOXIA experimental)
MOUREK, J.
Oxidative metabolim, its development and Influence in the ontogenesis
of mammals. Sborn. lek. 64 no.5:136-144 My 162.
1. Fyziologicky ustav fakulty vasobsonsho lekarstvi University Karlovy
v Praze, prednosta prof. dr. F. Karasek, DrSc.
(CERML MMM SYSM metabolism)
(OXYGEN metabolism) (STARVATION exper)
(AGING pbysiol)
MOUREK, J.
Development of oxygen requirement in ontogenesis in the dog.
Sborn. lok. 64 no.lOs3l6-320 0 162.
1. Fyziologicky ustav fakulty vseobeeneho lekarstvi University Karlovy
v Praze prednosta prof. dr. F. Karasek.
WIMAW NEWBORN) (TISSUE METABOLISM)
MOUREK, Jindrich
Fasinination of metabolic relations during the course of ontogenesis
vith the aid of anzymtic Inhibitors. Cas. lek. cesk. 101 no.29/302
918-922 20 J1 162.
1. Fyziologicky ustav fakulty vseobeeneho lekarstvi KTJ v Praze, pred-
nosta Prof. dr. F. Karasek, DrSc.
(TISSUE METABOLISM pharmacol)
(MALONATES pharmacol)
MOUREK, J.
The effect of 2: / din-i trophenol on oxygen conitopti cn and res ~s tanc ~
to nitrogen anoxia during the dev,~-.lopnent of tr.e rat. Physic-',
bohemoslov 12 no.1:70-75 16-11
I.Institutti of Physiology, Faculty of Medicine, Gharles UnIversity,
Frague. (111TROPH11101,S) (141TROG111) (ANOXIA) (TISSUE f-J-SPIRATION)
(GROWTH) (ANIMALS , NEWBO'101)
MOUREKI-'~~,
The effect of hypoxia on oxygen consumption of cerebral cortex,
liver slices and of diaphragm in vitro during postnatal
development of the rat. Phyaiol. Bohemoslov. 12 n0-42377-381
163o
1. Institute of Physiology, Faculty of General Hadicine, Charles
University Prague.
4NOXIA) (CEREBRAL CORTEX) (LIM)
(MUSCLES) (TISSUE METABOLISM) (GROWTH)
(MANOMETRY) (DIAPHRAGM)
MOUREKY Jj- PELISKOVA, M.
2,,4-,Dinitrophanol and its action in the ontogenesis of rats.
(LD50 of 2,,4- t (t E T),
is a process toc. 1.3 There exists a process z . z (t) defiAed on the
total interval T and which is denoted as undisturbed process.
Card 1/4
$8749
S/040/60/024/006/003/024
a ill/ C 333
Stability of Processes With Respect to two Metrics
If z belongs to a Process in the moment t, then it is said that the
pair (Z,t) belongs to the process.
To every pair (z,t) there are defined two metrics (distances)
S o(z, t), 3 (z, t) with the properties t
2.1 so(z,t) is real nonnegative, where 3 0(zo(t),t) =- 0, t e T.
2. 2 3 (z, t) is real nonnegative, where 3 (z0 (t), t) ~ 0, t e- T.
2.3 The distance 34z,t) is continuous with respect to the metric
g O(z,t) EuniformlyJ on T !:-~ T, i. e. to every E > 0 and
toe T 0 there exists a gof- 1t0) 71 o EJ(E) > ol so that
5 (z,t0 < 6 is satisfied for all (z,t 0) for which 30(z,to) <
2.4 For every process z(z 0, top t) defined on (t 0 , t00),
3(Z(Z0 t0, t), t) is continuous in t (here 5(z(zol top Opt)
is the distance from the undisturbed process up to the point z
of the process z(z,, t 0 , t) in the moment t.
Card 2/ 4
88749
B/040/60/024/006/003/024
C ill/ C 333
Stability of Processes With Respect to two Metrics
Theorem 5-1: In order that the undisturbed process zo(t) on T be
stable with respect to the me-trios SO'l , where the initial moment
t0belongs to T'5;i T, it is necepsary and sufficient that there is
an R N 0 so th1t on RZT there exists a functional f(z,t) positive-
definite in the metric I and non-increasing which is continuous
on T0 in the metric to.
Theorem 5.2 is an analogous statement for uniformly stable processes.
Theorem 6.1 is a generalization of the theorem of instability of
Chetayev (Ref.2) to the case of two metrics.
There are 14 references: 13 Soviet and 1 Japanese.
SUBMITTED: July 14, 1960
Card A14
MOVCHAN -A A 11-00C PHYS-MATH SCII "PROBLEMS OF STABILITY
I ~
OF THE DEFORMATION-V~ ~ Of SOLIDS." MOSCOw, 1961.
(MOSCOW URDER OF LENIN AND URGER OF LABOR RED BANNER STATE
UNIVERSITY OMEN# M. V, LOMONOSOV). (KL-OV, 11-61, 207).
-1-
M"CHA"T, A. A.
"Running Wa,res in the Problem of Hypersonic Flutter of Panels of
Finite length. 0
Paper presented at theThird International Congress in the Aeronautical
Sciences, Stockholm, 27-31 August 1962
IIOVCWT, A.A. (Moscow)
"The analogue of Kelvin theorem on the conservation of stability with the addition
of dissipative and gyroscipic forces for the case of arbitrary displace-ments; xid
deformations of solids".
report presented at the 2nd All-Union Congress on iheoretical and Applied
Mechanics, Moscowp 29 Jan - Feb 64.
~r, HO
ACCESSION NR: AT4039439 S/2879/64/000/000/0695/0701
AUTHOR: Movehan, A. L (Moscow); Movchan A A (Moscow)
TITLE: Vibration forms in the problem of supersonic panel flutter
SOURCE: Vsesoyuznaya konfereniiiya po teoril obolochek i plastin. 4th, Yerevan, 1962.
Teoriya obolochek i plastin (Theory of plates and films); trudy* konferentaff, 19G4, 695-701
TOPIC TAG: panel, panel flutter, wave propagation, supersonic- flutter, panel vibration, gas
flow, supersonic gas flow, flexure, damping, boundary problem.
ABSTRACT: Noting that the use of high-speed digital computers makes it possible to discover.
the characteristic peculiarities of the eigenforms of the vibrations of panels within a super-
sonic gas flow, the authors present several such peculiarities which are common to panels of
different configuraUons in a plane. For simplicity of exposition, the discussion in based on'.
the simple equation
J*W P.X dw dw N
D
dt* er &C
where w(x, t) Is the flexure of tbe'panel, occupying a region in We form of a band x4 0c;
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ACCESSION NR: AT4039439
The dimensionless values
x W
V, ID (4)
,are introduced in the solution of Eq. 1. Perturbed movements of a panel yield the form.
W (X, 1) X (X) e (5)
Function X (x), appearing In Eq. 5, is the eigenfunction (~on-trtviai solution) of the boundary
'Problem
L4X - A xx,
d~e dx (6)
1 1. V. L 4.
Lf (X)
,where Li(X) indicate linear homogeneous boundary conditions at the edps x0, x1. For
Card -3/6
'ACCEssioN NR: AT4039439
!the determ'ination of the eigenfunctions there is derived the following equation
L, (A') L, L.- (XJ) L, (X4)
F (A, X) so L, (XI') L, (XI) L, (X2) L, (XI) .0, (7)
La (XI) L, (XI) L- (XI) L, (P)
L, (XI) L4 (XI) L: (P) Lj (XI)
,the left-hand part of which is the whole analytical function of parameters A,
To each root
': A of this equation there corresponds, at least, one solution Cj of system 11 and eigenfunction
!10. If the eigenvalue A ia a simple root, one (with accuracy W constant factor) eigenfactor
,X(x) corresponds to it. If the eigenvalue X Is a double root and the rank of matrix 12 equals
two, two linearly Independent eigenfunctions correspond to it; if the matrix rank equals three'
,only one eigenfunction X(x) corresponds to eigenvalue ArW eigenfunction X(x).9f the
;boundary problem can be presented In the form
(8)
+ I"
!ACCESSION NR: AT4039439
where XI(x), X2(x) are real functions. It Is found that the natural vibrations are described
by the formulas
I X W I Cos It W + A 60 -
W ~X, t) X (A) I sin I? (X) + q11 do, (9)
For a real eigenfunction X(X) in continuity intervals 4) (k) condition V (k) constant is ful-
filled, thus providing a basis for calling the natural vibrations in this case standing waves.
It is shown that natural vibrations in the form of traveling waves. (for a complex eigenfunction
X(x) in continuity intervals V (x) with fulfillment of condition V (x) j const by analogy with
j equation (92)) are a typical phenomenon in the case of panel flutter. A theoretical qualitative'
investigation of the character of the traveUng waves in flutter, formerly involving extremely
cumbersome computations, has been facilitated through the use of high-speed computers.
The process of finding the eigenfunctions X(x) Consists primarily in the solution of rather
complex transcendental equations with respect to the parameters (r, 0 (which are complex
numbers for complex and In subsequent computation. In the final section of the article,
the computation resultar achieved on a "Strela!' computer, for the vibrations of an edge-
jammed pawl (x - 0, x - 1) are given and discussed. Orig. art. has: 4 figures and 21
formulas.,
,-Cord.5/6_
F
[ACCESSION NR: AT403"39
ASSOCIATION: none
SUBMrrTED: 00 DATE ACQ; 14May64 ENCL: 00
SUB CODE: AS NO REP SOV: 006 OTHER: 001
ACCESSION NR: AT4039439 S/2879/64/000/000/0696/0701
AUTHOR: Movch L (Moscow); Movchan, A. A. (Moscow)
TULE: Vibration forms in the problem of supersonic panel flutter
SOURCE: Vsesoyuznaya konferentelya po teorii obolochek i plastin. 4th, Yerevan, 1962.
Teoriya abolochok i plastin (Theory of plates and films); trudy* konferentaii, 1964, 695-701
TOPIC TAG: panel, panel flutter, wave propagation, supersonic, flutter, panel vibration, gas
flow, supersonic gas flow, flexure, damping, boundary problem
ABSTRACT: Noting that the use of high-speed digital computers makes it possible to discover.
the characteristic peculiarities of the eigenforms of the vibrations of panels within a super-
sonic gas flow, the authors present several such peculiarities which are common to panels of
different configurations in a plane. For simplicity of exposition, the discussion Is based on-
the simple equation
&W A0, dw dw
D t 1. 2- " -a
where w(x, is the flexure of the'panel, occupying a regton in the form of a band 0.~f x,,6 4%;
Lcard 1/6
r
ACCESSION NR: AT4039439
I
E is a dimensionless number indicating by how many times the full external damping exceeds
the aerodynamic damping, as calculated by the well-known formula of the piston theory
(A. A. 111yushin. Zakon ploskikh secherdy v aerodinamike bollshikh averkhzvukovykh
skorostey. PMM, 1956, 20, no. 6), while the other nomenclature coincides with that given
in A. A. Movchan (Ob ustoychivosti paneli, dvizhushcheysya v gaze. PMM, 1957, 21, no. 2).
(a panel moving in a gas in the direction of the positive axis x). The solutions of Eq.' 1,
which satisfy the boundary conditions at the edges x = 0, x = a, are compared with mcno-
chromatic waves of length a
I n 2x)y-L
rfW1,, (x~ i) - sin LX+
[a
which satisfy Eq. 1 without the right-hand part and derived without allowance for the boundary
conditions at the edges x 0, x a. The propagation velocity of the waves (Eq. 2) is given
by the formula-
2*
(3)
2/6
7
~ACCESSION NR.--A---T'4039439
The dimensionless values
x pa4
(4)
Rre introduced in the solution of Eq. 1. Perturbed movements of a panel yield the form,
w (x, i)'= x (X) (5)
iFunction X (k), appearing in Eq. 6, is the eigenfunction (non-trivial solution) of the boundary
problem
d4X dX
A
dx (6)
Lf (X) 4.
Where IaiM indicate linear homogeneous boundary conditions at the edges x 0, x 1. For
3/6
600CESSION NR: AT4039439
e determination of the eigenfunctions there is derived the following equation
L, (P) L, (XI) L, (P)
F (A. k)w L, (XI) L, (XI) Ll (XI) Ll (XI) _0' (7)
La (XI) La (XI) L (Xs) L, (X4)
L4 (XI) L, (XI) L: (XI) La (XI)
~e left-hand part of which is the whole analytical function of parameters A, )L To each root
A of this equation there corresponds, at least, one solution Cj of system 11 and eigenfunction
0. If the eigenvalue A is a simple root, one (with accuracy to constant factor) eigenfactor
'(x) corresponds to it. If the eigenvalue X Is a double root and the rank of matrix 12 equals
Aro, two linearly independent eigenfunctions correspond to it; If the matrix rank equals three,'
nly one eigenfunction X(x) corresponds to eigenvalue AzW eigenfunction X(x).gf the
oundary problem can be prmented In the form
+ I.,
IACCESSIONNR:
where X1(x), X2(x) are real functions.
by the formulas
It Is found that the natural vibrations are described
W (V, t) X (X) I Cos It (X) + qtJ CO.
W .(x, t) - I X (x) I sin 1~ (ic) + qt] 011
(9)
For a real eigenfunction X(x) in continuity intervals 4) (x) condition V (x) --t constant is f al-
filled, thus providing a basis for calling the natural vibrations in this case standing waves.
It is shown that natural vibrations in the form of traveling waves. (for a complex eigenftnction
X(x) in continuity intervals V (x) with fulfillment of condition V (x) ~ const by analogy with ,
equation (2)) are a typical phenomenon in the case of panel flutter. A theoretical qualitative'
investigation of the character of the traveling waves in flutter, formerly involving extremely
cumbersome computations, has been facilitated through the use of high-speed computers.
The process of finding the eigenfunctions X(x) consists primarily in the solution of rather
complex transcendental equations with respect to the parameters aC, P (which are complex
numbers for complex \ ) and in subsequent computation. In the final section of the article
the computation results, achieved on a "Strelall computer, for the vibrations of an edge-
jammed panel (k 0, x - 1) are given and discussed. Orig. art. has: 4 figures and 2jL
formulas..
LCard- 5
ACCESSION NR: AT4039439
ASSOCIATION: none
SUBMITTED: 00
SUB CODE: AS
L"M --- ?10
DATE ACQ-. 14May64
NO REF gov: 006
ENCL: 00
OTHER: 001
MOVCHAN, A.F.
Some types of polyclinical aid for thl rural population. Mad. sestra
20 no.7:23-27 JI 161. (MIRA WIC"
1. Zamestitell glavnogo vracha Kiyevskol oblastnoy bollnitsy.
(PUBLIC HEALTH, RURAL)
MOVCHANY A.P. (Juyev)
Hospital nurse. Had. sestra 22 no.6:206-21 Je'63- (MIRA 16:9)
(NURSES AND NURSIBG)
AUTIIORS~: 11olle-ri V, V, ana Movc~ian A. T.
TI'PLE: 'I"ethoets of Decreasin~- the Ash Content in Pitr-'--
U
(Puti snizheniya zol'nosti pekovogo koksa)
.!;ZRIODICAL: Koks i Khimiya, 1958, Nr E., PP 1?-"Il (UWMI~
ABSTRACT: The influence of various operatin6 factors oi., cl,.;2 a,~"
content of tar and tar-pitch is discus-,od --rL
by data on the ash content of tar, piLch and pitc.h coi:
produced on the Zaporozhsk coke oven vjorI:s (Tables 1,
The influence of tY,,,, followinb operatinf, factorc is
mentioned: 1) charfJ.nE conditions of co':e oven,
the degree of finenesc of the coal blend and thc
and duration of stuam injections; 2) condition of
operation of tar settling: tanks, intermediate aiid, stora, i
tanks and 3) additions of soda to tar before d_*._--I_-,I1--ti,_.
V:ere are 2 tabl~ac ~~nd. 1
ZnIx~roz,-EIrly zavrxi rr,-,.I.'.-e Coal-tar
Chezdcal PlanLi
i. Ovens--Performance 2 Coke--Combustion 3. Fue1s--Prc:-,)erti_e~-)
Z2 r~! 1 / 1
KULESHOV, P.Ta., kand.tekhn.nauk; MOVCHAS, A.T.
New system of processing the anthracene fraction. loks i khim. no.q:
36-37 160. (MIRA 13:9)
1. Zaporozhakiy koksokhimicheeldy zavod,
(Anthracens)
MOVCH M,-~-
Adoption of modern equipment and technology. Koks
5-9 163.
(Zaporozhlye--Coke industry)
khim. no-5:
OIIRA 160)
MOVCHAN .4 V.F.; LIVSHITS, B.Ya.; BUTUZOV, H.D.
- I A.T.; POPOV, K.P.; SOKOLGIi
Automation of sulfate recovery plants. Koks i khim. no-5:39-43
163. (Coke industry-By-products) (Automation) (MIRA 16:5)
KASATKII:, B. S. , -'IMCEMN, B. A.
Steel Alloys
Some data on the infl,uence of a metastable structure on the mechanic-tl pr(, erties (.f metal.
Avt(-m. svar., 4, No. 6 (21), 1951.
Monthl-v ILs_t 2L Russian Accessions, Library -f Congress, June 1952. Unclassified.
MOVCHAN, B. A.
Movehan, B. A. -- "Some Properties of Primary Crystallization in Automatic
"Ilding of Alloy Steel." GandTech Sci, Inst of Electric Welding, Acad Sci
Ukrainian SSR, Kiev 1953. (Ref era tivrWy-rhu -rnal--Xhimiya, No 1, Jan 54T-
So: SUM 166) 22 July 1M
KOTC11a, B.A.
Some characteristics of the primary crystallization process of alloy
steel. Avton.evar.6 no.3:3-15 NY-Je 153. (MMA 7:5)
1. Institut elektroevarkI im. Te.O.Patona Akadeall nauk USSR.
(steel alloys)
MOW@ Aa,?, AD.It-.
ussElphysics - alloy steel grains FD-1074
Card 1/1 Pub. 153 - 10/24
Author Svechnikov, V. N., and Movehan, B.
Title : Structure of the primary grains of alloy steels during heating to a
high temperature (i3oo-14oo0c)
Periodical : Zhur. tekh. fiz., 24, No 10, 1823-1829, Oct 1954
Abstract : The authors study by direct methods the structure of the grains and
the boundary zones of several alloy steels (results tabulated), namely
at temperatures of overheating. They find that chromium and wolfram
diffuse into the boundary zones of the grains and that man ese may
concentrate at internal defects because of rolling. They describe their
experimental procedures and evaluate their results.
Institution : -
Submitted : January 29, 1954
PARKOVSKIY. Yevpniy Adamovich; KOVCHAN. Boris Alsksoyevich; STITSINKO,
TwevDlod Ivenovich; SAEV1fjLUV,' T..Vvedushchly rodalctor; MOVIX, A.,
tokkmichookiy rodaktor
Lladioinotopes in metal reaearchl Radioaktivuye isotopy pri tooledo-
vanii metallov. Kiev, Goo. izd-vo takhn. lit-ry MSR. 1956. 87 p.
MaA 9:10)
(Radioisotopes--Industrial applications)
(Ketals)
AM P - 5254
Subject USSR/Engineering
Card 1/1 Pub. 11 - 5/15
Authors Gupalo, Yu. D., B. A. Movchan, and P. M. ShIrokovskiy
(Electrowelding lnstitute~'-Iml ~.' Paton)
Title Use of radioactive Isotopes to control the level of
metal melt in the resistance slag welding vat.
Periodical Avtom. svar,, 4, 67-69, Ap 1956
Abstract The authors describe the utilization of radioactive
isotopes for control of level of melting metal In the
vat of resistance slag welding. A special automatic
regulator was designed and tested by the Electrowelding
Institute Im, Paton, Two drawings; 3 Russian references
(1953-55).
Institution As above
Submitted No date
SrACHNIKOV, V.N*; HOTCHAN, BoA. .
Nquilibrium of chemical inhoagensity In allo7s at high temperature.
Sboy-. nauch. rab. Inst. metallofiz. AN USSR no.7.132-47 156.
(Metals at high te"raturoj) (MIRA 11:1)
(Ketallography)