SCIENTIFIC ABSTRACT KONONENKO, V.O. - KONESKA, SMILJA
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SCIENTIFIC ABSTRACT
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SUBJECT USSR/MATHEMATICS/Differential equations CARD 1/1 PG - 65
AUTHOR XONONZNKO V.0.
TITLE _~'n -the os6-illa-tions of non-linear systems with many degrees of
freedom.
PERIODICAL Doklady kkad. Nauk 105. 664-667 (1955)
reviewed 6/1956
A method is given for determining periodic solutions of a system of differential
equations of n degrees of freedom.the coefficients of which are slowly varying
almost periodic functions and the non-linear parts of which are multiplicated
with a small parameter C...The method is applicable if the stationary oscillat-
ions possible in the system essentially take place with one frequency. 'Oter
the transformation of the starting system which corresponds to a principle-
axes-transformation of the linear partial system, the solution is set up in
the form of an asymptotic series in terms of powers of E. Corresponding
series are found for the slowly varying phases and amplitudes of the wanted
solution. The coefficients of'the series expansions are given ias trigonometric
double series. If these are determined, then the problem is reduced to the
integration of the defining equations for phase and amplitude, a problem which
can be reduced to simple quadratures if amplitude and phase occur in separable
form. Slightly non-linear systems with purely periodic coefficients are con-
tained as a special case in the considered starting system and give certain
simplifications of the method of solution.
A) c rV e A) V_ U
j
25(2). PffASZ I BM EXPIDIMON BOV/2563
Akademiya.nauk Sam. institut Seminar Vo tearli Ynashin I
mekhanimoy'
Trudy,o tam 18.. vyp. T1 (Transactions of the Institute of Mechanical ngine",,
Academy of Sciences., USSR. - Seminar on the Theory of Machinery and Ylechanimbp
voi 18, No. 71) Moscow, Iz&vo AN SSSR.. 1958. 89 p. Errata slip inserted.
2,500 copies printed*
Ed. of PubUshing House: M.L, Dobsbits; Tech. Ed.t N.F.-Tegorova,*. Mtorial
Boaid- I.I. Artabolevskly., Academicism (Respe Ed.); G.G. B&ranov,, Doctor
of Technical Sciences., Professor; V,A. Gavrilenko., Doctor of:Tecbnieal
Sciences, Professor; VA& Zinov'yev,, Doctor of Technical Sciences, Profeqsor;
Aje. Kobrinskiy., Doctor of Te4ohnical Sciences; N&L levitshy., Doctor of
Technical Sciences, Professor; N.P. Rayevskly., Candidate of Technical Sciences;
L.N, Reshetov, DocWr of Technical Sciences., Professor; and M.Ap Skuridinj,
Doctor of Technical Sciences,, Professor.
PM3P=t This collection of articles Is intended for scientific research workers
and'etZineers.
Card 1/4
Transactions (cont.)
S(W/2563
OOVERAGE: This of articles deals with ~he following topics: thread
control in textile machines, pneumatic devices vith diaphragms, resonance J~k
cea~trifugftl pumps., the dynemdes of electrically driven machinery., synthesis,
of four-link transmisbion mechanism, and the design of link mechazdams. ft
personalities are mentioned, References follow sgvMl of the articles.
TAM 6F. CdNTEM:
Preface.
ICostitsyn.. V.T. (Deceased) Iftietor of Technical Sciences., Professor]. Design
of a Disk-type Thread Governor A
The author points out the interdependence betveezr:the tension in the thread
and,the angle of,contact betwegm thread and spindle,
Gertsp Ye.V. (Candidate of TedmIcal Sciences.]. Dynaimle Characteristics of
Pnemnatic bisphrqp-type Devices n
This- theoretical and experimental investigation deals vith the dynamic
characteristics of a single-action pneumatic device with a place diaphragm.
3
Card 2/4
Transactions (Cont.) SOV/2543
Exem.les of the calculations involved are presented,
JLononenko.,V.0. (Doctor of Technical Sciences], Resonance Properties of a
cenITEFERT-VIVrator 22
Equations for the motion of a ceutfl:fugal, vibrator are presented,, and the
basic interrelations between the parameters of the system and the regimes
of the motion we established. Simplified geometrical criteria for ste&4
motion and t2fe~*effeot of mechanical characteristics are presented.
Bykhovskiy.. M.L. [Doctor of Technical Sciences.]* Problem of the Dynmics of
Machinery With Electric Drives 43
The author derives a general equation for investigating the dynaades of d-c
electromechanical systems., vith consideration being given to electromagnetic
processes in the motor. A comparison is made vith other simplitied methods which
takef only the static characteristics of the motor into consideft-Cion.
Cherkudinovj S.Aop and N,V. Speranskiyo Synthesis of Four-bar Linkage Rechanints
by the Method of Interp&ative ApWaximation With One Node of High Iftitiplicity. 60
This article is the continuation of an article published by the authors in
Card 3/4
KOX04~~KO, V. 0.
V. 0. Konorfenkop
"Sam Now Problem of Vibration Theor7 in Machines."
papw pmseaW at the 2nd AU-WIon C=f - an Yupdamutal fftblsw In tha
TIwory of Wah1we and MmUnIamp Nbscow, MW, 24-28 Ywuh 19~8.
SOV/24-58-7-13/36
AUTHOR: Kononenko, V 0 (Moscow)
TITLE. Res3nance Vibrations of a Rotating Shaft Carrying a Disc
(Rezonansnyye koleba.niya vrashchayushchegosya vala s diskom)
FERIODICAL-. 'Izvestiya Akademii nauk SSSRI, Otdeleniye tekhnichesk1kh
nauk, 1958, Nr 6, pp, 87 - 90 (USSR)
ABSTRACT: Transverse vibrations of a rotating shaft carrying a disc
are considered. These vibrations occur when the system is
not balanced. The.system under consideration is illustrated
in Figure 1 and the equations describing its motion are
given by Ecp(l). In these equations m is the mass of the
discq I is its moment- of inertia, o is the rigidity
of the shaft and 0 is the off-ceittre distance. The
system of equationt is non-linear and an approximate method
Of solution (Ref 2) is used. It is assumed that the vibr-
ations do not differ very much from harmonic vibrations
and that the angular velocity changes very slowly. In that
case all the,terms on the right hand side of Eqs(l) can be
looked upon as small. Using the substitutions given by
Eqs (2), the s7stem. of Eqs (3) is obtained in which e is
a small parameter. The solution is given by Eqs (6) and
Card 1/2
SOV/24-58-7-13/36
Resonance Vibrationa of-a Rotating Shaft Carrying a Disc
An erpres3ion for L is given by Eq (8). Each'positive
root of Eq (8) corresponds to a stationary motion of the
rotor with a vibrationamplitude "all calculated from
Ea (7). A detailed discussion is given of the stability
of the motion desertbed, by the. above equations.
There are 3 figures and 3 Soviet references.
SUBMITTED~ April 18, -L9C3
5
Card 2/2
KONONE',TKOP V.o. (~blwe6w)
- ~ ~.- -
Resonance vibrations of a rotating shaft fitted with a dirk.
Izv. AN SSSR. Otd.takh.naul- no.7:87-90 JI '58. 04IRA 11:9)
(Shafting--Vibration)
AUTHOR: Kononenko V. 0. (I.Ioscow) SOV24-58-8-10/37
TITLE: On Parametric Resonance of Fractional Order
(0 parametricheskom. rezonanse drobuoGo poryadka)
PERIODICAL: Izvestiya Akademii Nauk SSSR, Otd.eleniye TekItnicheold'KII
Nauk, 1958, Nr 8, pp 62-65 (USSR)
ABSTRACT: The author considers resonance phenomena in oscillatory
systems whose motion is described by differential
equations with aLniost periodic coefficients when the
modulation para,aeter on the fundamental frequency is of
arbitrary depth. The investigated oscillatory systems
occur in the motions of mechanisms of instruments i-iorking
on a vibrating base (Ref 1) and in problems of the mot-ions
of charged particles in accelerators (Refs 2 and 3). The
fundamental differential equation discussed is:
d2x/dt2 + (b0 + b 1 Cos wt + c Cos-Vt) x = 0
in which the frequencies w and V may be incommensurable,
the positive coefficients b 0 and b, can take any
values and the coefficient c is assumed small in
Card 1/3 comparison with b 0 and b1, This eauation is solved
On Parametric Resonance of Fractional Order SOV/24-58-8-10/37
with the aid of Mathieu functions, and only those motions
?f the system are considered for which the frequency X1
is near to a where + ia are the characteristic
indices associated witF the Mathieu functions. For
a =.a and also for values of A near to a the motions
are unstable and the corresponding states of -the system
are resonance states. Resistive forces (friction) have
a considerable influence on processes characterised by
parametric resonance of fractional order. The solution
of the equation
d2x dx
= + k at + (b0 + b, cos 60t + c cos Vt) x = 0 (21),
dt
in which the second term is considered a small frictional
term proportional to the velocity can be obtained by the
same method as that for Eq.l. It is found that the
friction reduces the area of partunetric resonance. The
Card 2/3 phase difference 6 in the equation:
On Parametric Resongnce of Fractional Order SOV/24-58-8-10/37
d2x + [bo + bi Cos wt + c CO'S (-it + 6)] X = 0 (23)
=dt
causes the domain of parametric resonance to be
distorted.
There are 3 figures and 6 references, 4 of which are
Soviet, 1 German and one is a Russian translation of an
English textbook.
SUBMITTED: April 24, 1958
1. Resonance--Mathematical analysis 2. Instruments-Vibration
Card 3/3
49~ 0, V. 0.
Resonance properties of centrifugal vibrators. Trudy Inst.mash.;
Sem.po toor.mash, 18 no.71:22-42 158. (MIRA 12:1)
(Vibrators)
AJ I<
24(6); 25(2) PHASE I BOOK EXPLOITATION SOV13241
Akademiya nauk SSSR. Institut mashinovedeniya
Problemy prochndtti'v*niashiyi6stroyenii, VYP. 5 (Problems of Strength in Mechanical
Engineering, Nr 5) Moscow,'Iid-vo AN SSSR, 1959. 69 p. Errata slip inserted.
2,500 copies printed,
Ed.; F. M. Dimentberg, Doctor of Technical Sciences; Ed. of Publishing House:
G. B. Gorshkov; Tech. Ed.-. I.F. Kovallskaya.
PURPOSE: This book is intended for analysts and designers of turbomachines and
vibration machines, It will also be of.interest to teachers and students
working on the problems of vibrations in machines.
COVERAGE: This book contains,4 articles on vibrations in **Aines. An article
by V"O. Kononenko .discusses-the of nonstationary vibrations with
, pr
respect to a general vibrational'system, taking into account the cinmection
with the motor. Essentially the same problem but with respect to a rotating
shaft.is studied in the article by-L. A. Rastrigin. In the article by S. M.
Grinberg, a study is made of the nonstationary process in a case of an arbitrary
problem of the law of excitation frequency variation. Finally, in the article
Card 1/2
4-7-vv-
All
14
oil A
FA IJ
~1 OV ofy N
SOV/179-59-2--11/40
AUTHOR: Kononenko V.. 0. (Moscow)
TITLE: On Resonant Processes in the Vibrating System Containing a-
0' '0 rezonansnykh protsessak-li v kolebatellnoy sistemel
t r \'.
G
soderzhashchey dvigatel,')
PERIODICAL: Izvestiya Akademii nauk SSSR OTN, IMekhani-k-a i mashino-
stroyeniye, 195% Nr 29 PP ?5--80 (USSR)
ABSTRACT: Vibration of a system with n degrees of freedom is
described by the author. The vibration is produced by
rotation of the mass m . The whole system (Fig 1) con-
tains masses m,, ... I mn and rigid bodies r;1, ... en -
Oneof the masses, for instance. ml , coatains the mass
of a motor . the rotor of which has a moment of inertia
I and the mass m at the distance r from the axis of
rotation. It is assumed that the characteristics of the
motor L(~p) is known and that m/m i< I (i = 1, 21. a. n)
The resistance forces.of Vhe motion are proportional to
every coordinate of (P 7 Y19 ... ~n - The equation of motion
Card 1/4
SOV/179-59--2-11/40
On Resonant Processes in the Vibrating System Containing a Motor
of such a system is expressed by the Eq (1) (Refs 11, 2).
To find its solution and in order to minimise the values of
its right term, the following assumptions are made: the
vibrations are harmonic, the angular velocity * does not
(P
exceed the period, the frequency w 5 of the specific vib-
ration of the system is the root of its characteristic equs~t-
ion, and the value *k w (k -- 2, 3,...) does not apply.
The system (1) can be represented as a collection of indep-
endent vibrators, each satisfying the Eq (2). Then, from
Eqs (1) and (2), the expression (3) can be derived, where
the function 2 B is defined as Eq (4). If w S is the
specific frequency of the system, then Eq (5) can be defined,
the solution of which can be expressed as Eq (6). from which
the stationary vibration in the resonance region is obtained
as Eqs (7), (8) and (9). The solution of the problem can*be
expressed in the general form as Eq (10). As rl and a
can have several solutions, only those are chosen which
correspond to a stationary condition of the system. These
are expressed as Eqs (11), (12) and (13), from whir--h the
Card 2/4 Eq (13). written in the form of Eq (14), is the most signi-
30,i/179-c9-2-11/40
On Resonant 11r'ocesses in the Vibrating System Containing a L-Iotor
ficant. This is illustrated in Fig 2, where the graphs of
the engine characteristic L(CL) and of the function S
are shown. The points of interser;tion 1, 2 and 3 eharac-
terise the stationary values of J1 , acoording to Eq (9)
(the points 1 and 3 roprosent stable motion., point 2,
Luastable). A distribution of the stable and ntustable reg-
ions in the resonance zone characterizes the. motion of the
system. The most interesting cases are: a) recedJug stable
vibration and the curve (8) cannot be obtained; (--,) the
resonance curve (8) for stable drition at quaai-stationary
increase of SI ean differ greatly froia the resonance curve
at the diminishing value of I)- (Fig 3). In practice, 2 or
more resonance regions can occur, Therefore, the aharacter-
istic graphs of the motor and the graph 3 S' ~Q) for the
resonance zones (Fig 4) should be closely studied. The
calculations show that the charaoter of the resonance depends
on the properties of the mo`56r and on the reser-,e of power
of the motor , A part of the latter can transform into the
resonan-.e which can be satisfied by the velocity SI and
frequency a. as illustrated in Fig 4., where the graphs
Card 3/4
SOV/1'79-591-2-11/40
On Resonant Processes in the Vibrating Syster. Containing a Motor
S1 and S2 are shown. Here thii motc-i:, is taken with the
characteristic curve L(a) . Its stable motion is shown by
the point B . The transformation of -the system into the
second resonance is shown in Fig 5. This was obtained from
Eq (6) for s = 2 and for iiiitial conditions eorresponding
to ts N and P in Fig 4. Generally, the variations
of lin depend on the reserve of power of the motor . This
can be shown as a segment t in Fig 4. There are 5 figWes
and 8 references, of which 7 are Soviet and 1 is French.
SUBMITTED: December 3, 1958.
Card 4/4
,K01IONENKO,-1-9. --
Passing of a mechanical system containing an engine through the
resonance zone. Probl.proch.v mehinostr. no.5:5-9 159.
WIRA 13: 1)
(Vibration) (Resonance)
KDFONENKO. V.0., prof., doktor tekhn. nauk.
Effect of engine performance on the vibrational strals' of =chinos.
Vast. mash. 39 no-1:53-56 Ja '59-~ (MrM 22: 1)
(ftchine tools-Mrstion)
KONONEYKO, V.0. (Moskva)
A form of Routh-Hurwitz criteria. Izv.AN SSSR.Otd.tekh.nank.K~kh.
i mashinostr. no.4:125-128 Jl-Ag 160. (KERA 13:8)
(motion)
MDRONOW, Y.O. (moskva)
--------------------- I-------
Interaction of a parametric vibrating system with an energy source.
Izv.AN SSSR. Otd.tokh.nauk.Mel-h.i mshinostr. no.4:141-146 8-0 160,
(MIRA 13:9)
(Vibration)
58519
S/179/60/000/006/012/036
0~ 3 0 0 9191/E135
AUTHOR: .4ononeakol V.O., (Moscow)
TITLE: Forced Oscillations of a System Containing a Source of
Energy in the Presence of a Small Non-Linearity
PERIODICAL: Izvestiya Akademii nauk SSSR,Otdeleniye tekhnicheskikh
nauk, Mekhanika i mashinostroyeniye, 1960, No. 6,
PP. 80-85
TEXT: The mechanical system considered consists of a mase
represented by a slab mounted on a spring, whose characteristic
function contains a small non-linear term added to a large linear
term. The slab carries a motor, whose shaft has an unbalanced
mass and so produces unbalanced forces when rotating. The rotor
of the motor has a moment of inertia, a driving torque and a load
torque, both of which are functions of the shaft speed. The slab
motion against its spring constraint is assumed one-dimensional.
The driving torque, load torque and damping function of the linear
motion, are assumed known. The unbalance mass is-assumed small,
compared with the slab mass and the difference between the driving
and load torquesis assumed small. The equation of motion of this
Card 1/4
88519
S/179/60/000/006/011/036
E191/E135
Forced Oscillations of a System Containing a Source of Energy in
the Presence of a Small Non-Linearlty
system is formulated. It is assumed that the oscillations will be
near harmonic and the angular velocity of the motor shaft will vary
slowly compared with the period of oscillation. In the sense that
the system is mechanically self-contained, its oscillations can be
thought of as self-excited but the designation "forced oscillations"
is used to signify the similarity of systems which are examined
without consideration of the properties of the source of energy.
The solutions of the problem are stated (Eq. 2). The angle of
shaft rotation and the linear displacement of the slab as well as
its linear velocity are defined in terms of a basic uniform rotation
for the shaft and a basic harmonic oscillation for the slab on
which are superimposed additional small periodic functions.
Asymptotic methods of solutions are used to determine the parameters
(angular velocity, amplitudes) of the basic motions. Under steady
state conditions the angular velocity of shaft rotation is constant
as is the amplitude of slab motions This motion is sinusoidal with
Card 2/4
88519
S/179/60/000/006/012/036
2191/E135
Forced Oscillations of a,System Containing a Source of Energy in
the Presence of a Small Non-Linearity
a period exceeding that of the shaft rotation by a constant &mounte
The angular velocity of the shaft is not arbitrary but several
solutions exist determined by the properties of the motor. The
steady state solutions are examined for stability by the metho4n
of I.G. Malkin (Ref.12). It is shown that by changing the nature
of the torque as a function of the speed of the motor it is
possible to change stable into unstable states and vice versa.
An example is given wherein the non-linear term in the spring
characteristic is a cubic terms The motion of such a system has
been studied in detail when the frequency of the exciting force
is a given constant. In the present system, two cases of non-
linearity are considered, namely a stiffening spring and a
relaxing spring (cubic term positive or negative, respectively).
The differences between the present case and the well known
resonance curve of a non-linear system are discussed. The
discontinuous changeover between two states depends on the
Card 3/4
88519
S/179/60/000/006/011/036
El9JL/E135
Forced Oscillations of a System Containing a Source of Energy in
the Presence of a Small Non-Linearity
characteristics of the surplus torque as a function of the motor
speed. In the case of a relaxing spring, when the surplus torque
decreases with increasing motor speed, the unstable condition may
be transferred from the rising branch of the resonance curve to
its falling branch. The difference between the stability of the
system at a prescribed motor speed and a system with a self-
adjusting motor speed is discussed. A system unstable at a set
speed can become stable. The superimposed periodic deviations
from the basic motions are shown to be small for the system
considered.
There are 4 figures and 13 references: 12 Soviet and 1 English.
SUBMITTED: May 18, 1960
Card.4/4
XONORIM. T.O.,(Moakva); XQMLW. S.S. [Xorabllov, S.S.] (Hookwa)
Vibration of a shaft with dieks, allowing for the
Interaction of the engine with the vibratory system*
PrOd.mekh. 6 no.2o.129-137 160. (MM 13 3 8)
1. lwtltut mm~shluovedeniys AN SSR.
(1hifting-Vibratio,p)
KONONRIKOY V. 0.
"Some autonomous problems of the theory of' nonlinear vibrations."
Paper presented at the Int. Symposium on Nonlinear Vibrations, Kiev USSR,
9-19 Sep 61
Institute for the Research of Machines).Academy of Sciences of the USSR,
Moscow, USSR
XQNONEINKOIP V,O, (Moskva)
Interaction of a natural,*Lbration eyetem wA the power eouroes Isv*
AN SSSR.Otd.tekh.naukt!bkh.i. mashinostr. no.2:50-54 Mt%-Ap 161.
(MM 14:4)
(Vibration)
S/179/61/000/005/009/022
zl9l/z481
AUtIIORSI - Kononanko, Y.O. and Fralov, K.V. (Moscow)
TITLZs On the interaection between a nonlinear vibrating
system and an energy sourts-
PERIODICALs Akadtmiya nauk SSSR.
tekhni%-~hesk1kh nauk.
V'51 ijft, 69-76
Izvestiya. Otdeleniye:
MekhanIka i mashinostroyeniyo.
TZXT: Characteriatiz features of the interaction between ac-
nonlinear oacillating system and'a Bource of energy were examined'
by S.S.Korablev (Ref.13 Trudy IMASh AN SSSR, 1959, v.1) and one-
of the present authors, V.I.Kononenko (Ref.2: Izv. AN SSSR, 07W,
Makhanika i mashinomtroyeniye, 1960, no.6). Some of the results-
obtained wers veriflad- by 4xp-srimant with a machantcal model.
The pressint pap-or reporta the examination of ther,probles with the,
help of an oleztroniz madel &jzmxl.&tjng the nonlinear mechanical
oscillating systam zonaldarad7.Ln ths papers quoted above. Briefly,
the mechanical 4yetem has a nonlinear elastic for~ze obeying a law
with a linear and a cubic term. The vibrations are,excited by the
inertia fortea of wn unbalanced*masm rotateii-by a motor with
Card-1/4
S/179/61/000/003/009/022
On the intarattion betwaon OOP 2191/2481
wilh a kno-on torqut/Apeed'tharattaristiz. Changing over to
elaztronic models became possible after -rariftcation, furnished In
the earlier experiments-already quoted, that the static
.0haracteristics of entrgy sources could be substituted in solving
the dynamic probism. Although elettroniz models inherently
embody a convenient varisbiltty of parameters, the range-.
iw,restigated did not tz~,,eed that a~doptadl in ths, author's earlier
papar Mef.2) when i.,onstruzting thw approximate solutions of
nonlinear equations. -the only exception was the parameter of
nonlinearlty whLob ia the constant factor in the cubic term in tho,
.r.slation betwe,un the forz*~and the displacement. This was Yoried-.
in a larger rang-a:to reveal the behaviour of the system in the,
pres-en-ze Of a Bubatantial nonlinearity. The scale factors are
derived from the permissible maxima of the electrical variabjL6~.&ndL
introduced into the equations of motion of the mechanical system
thus deriving a system of two equations for which the analogue
circuit was devised. The mine and cosim-&-functions require& the.
special blozka designed by V.S.Tarasov and his team (Ref.3:
Nauzhn.-tekhn. informats. vyl. LPI, 1959, n0.51 and Ref.4:
Elektricheztvo, 1960, no.4), The programme of the investigation
Card 2/ 4
S/179/61/000/005/009/022
On the interattLon betvaen ... Eigi/s48i
had three aims. (a) The study of the steady--state conditions,
where it is describad by a harmonic dAlsplactment of the mass at the,
forced frequency on whi.--h a small periodic function of time is
superimposed and the motion ef the exciting unbalance has another
small periodlo funi_-tlon superimposed upon a uniform rotation.
In particular, the nature of stsady-state conditions with
substantially inrreased nonlinearity and at a substantial
departure from rem-anant-9 was of interest as representing a
vlolatlon of the condlclona on whIt.h the approximate analytic&1
solutlona were baaed, (b) The clarification of non-steady state
whith aris43 near the limits of the stability region when the
ayatem changes over from tne steady-state zondition to another.
(c) The discovery of any peculiarities in the motion of the system
when the steady-state ~~riterla establiahed analytically are not
fulfllled~ The eff,s.--t of the exalting motor characteristic was
the centre of attenTion, The slope of the characteristic curve
could be easily varied. The techuique of experimentation
permitted the z-onatrw--tion of rezonan~ze curveAr for rising and
falling valu-aa of the for^.ing friqubncy separately. Transient
Card 3/4
On the interattion batwzen
S/179/61/000/005/009/022
8191/S481
conditions arizing iA switthing on dLd not form part of the
_'nvestLgat_Ion but those which rc-..,.--urr6d bttween two steady states
were examined. Owing to tha pronounced differaxxc_e between the
resonance phenomena in systema with stiffening and unstiffening
nonkinearity terms In the restoring for(eje equation, each case was
examined aiaporataly. The rasults of the zxperimenta are given in
graphs whers the amplizuds ta plotted again3t the forcing frequency
and in oscillograms of liaplm.,smnt against time (for the non-steady
states). Without rt-realing &ny naw aalient ftatures, the results
of these 61e~.troniL simulator ia3ta confirm the basic proposLtions
about the propertiss of narillnear systems with nonideal sources
of energy found sarlibr (Ref.2). Emerging from tha limitations
imposed by the mathematital mA~hods used earlier did not yield
Substant4ally new re2ultz, There ars 12 figures and 4 Sovlet-bloc
-references.
SUBMITTED.- June 27, 1961
Card 4/4
..KONONENKO. V0,-. doktor tekhn.nauk, prof.
..........
Problems of general mechanics at the 10th International Congress
on Applied Nechaniqs. Vest. mash. 41 no.6:77-78 Je '61.t'
(MIRA 14:6)
(Mechanics, Applied-Congresses)
KONOIENKO I V. 0
"Vibration of a solid body about the center mans,"
Report presented at the Conference bni-A~plied Stability-of-Motion Theory and
Analytical Mechanics, Kakan Aviation Institute, 6-8 December 1962
39806
S/179/62/00o/oo3/606/015
Eigi/E413
AUTHORS: Kononenko,.V.O., Frolov, K.V..(Moscow)
TITLE: On the resonance properties of a parametric oscillating
system
PERIODICAL: Akademiya nauk SSSR. Izvestiya. Otdeleniye
tekhnicheskikh -nauk. Mekhanika i mashinastroyeniye,
no-3, 1962,.73-80
TEXT: * Reference is made to a pre'vious paper by the senior author
(Ref.l: Izv. AN SSSR, OTN, Mekhanika i mashinostroyeniye, no'.5,
1960) wherein steady-state conditions were examined subject to
limitations determined by the approximate methods of analysis
employed. In the present paper, a parametric oscillating system
with a low depth of parameter modulation is considered on the.
assumption that the source of energy which imposes the periodic
(or almost periodic) variation of the parameter of the system can
interact with the oscillating system so that the oscillations
become dependent-on the properties of the energy sourcei The
physical oscillating system considered is an elastic bar subject
to a periodic force in its axial direction, so that its bending
Card l/ 3
S/179/62/000/003/006/01.5
On the resonance properties E191/E413
stiffness changes periodically. Under certain conditions, as a
result of the periodic variations of stiffness, parametric
oscillations of the bar in the direction transverse to its axis
take place. Details of
the system are given in Ref.l. The
-
equations of motion are formulated, and its simulation by an
analogue computer is illustrated with the help of a block diagram
and discussed. The equations of motion contain a term with the
cubed transverse coordinate. The coefficient of this term is the
nonlinearity parameter which, in the present paper, is examined
within a wider range than before. The purposes of the simulator
studies were (a) to establish the motion of the system under
steady-state conditions at positive, negative and zero values
of nonlinearity; (b) to clarify the nature of the nonstationary
conditions of motion arising near the boundaries of stability and
corresponding to the transition from one steady state to another
dhd (6) tb 6boOrve the motion of the system when the conditions of
stability are not fulfilled. The energy source charnaterintis'
curve is conceived as a linear function of the torque against
speed of a motor which imposes a periodic force on the bar. The
Card 2/3
On the resonance properties 0*0
S/179/62/000/003/oo6/ol5
E191/E413
slope of this curve is among the important physical properties of
the system. The nonlinear restoring force is denoted as lfhardif
when the nonlinearity parameter is positive and as "soft" when
the parameter is negative. The results of the analogue computer
simulation are illustrated and discussed, selecting the behaviour
in -the resonance region where the interaction of the oscillating--
system with the source of energy is most pronounced. The three
cases of hard, soft and zero-restoring force arc considered
separately. The main result of the present investigation is a.
broader view of the nonlinearity parameter limiting the
amplitude of parametric oscillations. In systems considered
here, the factor which limits the amplitude of pArametric
ospillations is the nonlinear link between the energy source and
the oscillating system, This-link,varles with the variation of
the steepness of the cLracteriatic curve of the energy source,
so that parametric oscillations with*limited amplitudes can'be
obtained by an appropriate variation in the steepness of the
energy source curve. ~There are 11 figures.
SUBMITTED: December 26, 1961
Card 3/3
EWT(-j)1US AFnQ/V3D
L, !416
Ar'=-SIO" 11M, AF3004~9T S/OIT9/63/000/004/0023/0030
Al"MOR: flononanko, V. 0t (140800w)
TITLE, On oscillations of P_ b ~Lbout I~s ceatxoid
S OMCE : AN SSSR. 1Z76 otd. tekh, nauk; Mekhanika I mashinastroy-eniye, no . k-0
10,630 23-30
TOPIC TAGS: ciremeentrold oscillation, fdreed 002illation, nonlinear oscillation,'
oscillation-component interaction.,, system oscinetion, oscillation stabili
cillatift equation
ABSTRACT: The oscillation-of a body joined by elastic springs to a stations~
fre=e and
subjected to the action-OIL' external momments Is investigated, The
center of mass of the body is.4mmovable, and the mo=ents cause diriectly Cecil-
lations about only one'coordinate axle. The case of indirect excitatioa of
oscillations about other coordinate axee is discussed in nonlinear formvIation
(i.e., the Oscillation equations are not.lineer as related to coordinates aril
their derivatives). The mn3or emphasis is placed on the establisbment of con-~.
ditions under nhich oscillations are excited about those coordinate axer. about
Car
d .1/2
KONMOV, D.M.
Age and origin of whade of the PoltaTian stage. Biul.NOIP.Otd.
gaol. 29 no.6:98-100 31-D 154. (KWA 8:2)
'(Geoloff, Stratigraphic)
.I ~ -_- 1~,z I t
I V
....... ;~~ I
.". t
98-58-4-16/18
ATJTHORS: Konenkov, G.I., Sorokin, AN., Engineers
---------------------
TITLES: First Science and Technolo6y Conference of Young Specialists of the
"Gidroenergoprovekt" institute (Pervaya nauchno-tekhnicheskaya kon-
ferentsiy.- molodykh spetsialistov instituta "Gidroenergoproyekt")
PERIODICAL: Gidrotekbnicheskoye Stroitellstvo, 1958, Hr. 4, p 61 (USSR)
ABSTRACT: The authors briefly describe the conference which was arranged by
Komsomol organizations for the purpose of furthering and inter-
changing the scientific and technical knowledge of young
specialists. Prof. Voznesenskiy, A.R., director of the Institute,
and Makov, Yu. S., engineer, read reports entitled respectively:
"Problems of Gidroenergoproyekt in the Develolment of Soviet
Water PLver and in the participation of Youth in its Worle' and
"Particilation of Youth in the Public Works of Leningidep". Several,
other reports were made by unnamed leading specialists in the fields,
and 112 reports were read by unnamed young specialists.
AVAILABLE: Library of Congress
Card 1/1 1. Water power-Study and teaching 2. Study and teaching-USSR
USSR / Cultivated Plants. Fodders
Abs Jour: Ref ZhUr-Biol.j No 6, 1958, 25098
M-4
Author Konenkov. G.S4-
Inst o g~lven
Title Corn Stubble Sowing at the Benyakonskaya Agricul-
tural Experimental Station
Orig Pub: V ab.: Kukuruza V BSSR. Minsk, AN BSSR, 1957, 331-
334
Abstract: At the Benyakovskaya Experimental Station in
Grodnens*4aya Oblast' the Krasnodarskaya 1/49 corn
ield consisted of 205 centners per ha. of green stuff
f4lOO food units), yellow lupine-green mass 315
centners per ha, the food units were 3780. -- A.T.
Card 1/1
-,V
I ME1 I MEMBER
fNt~, 3w
SOV/32-24-10-41/70
AUTHORS: Slezinger, I. I., Konenkovr, K. Potrova, 0. P.
TITLE: An Apparatus for Determining the Mechanical Properties of Rocks
(Pribor dlya opredeleniya mekhanicheskikh svoystv gornykh po-rod)
PERIODICAL: Zavodskaya Laboratoriya, 1958s Vol 24, lir 10, pp 1270-1271 (USSR)
ABSTRACT: At the institute mentioned under Association together with the
Konstruktorskiy byurc neftyanogo priborostroyeniya, (0=1~xaeu=
Bureau of Petroleum Machinery) an apparatus was devised for the
determination of the hardness of rocks. At the same time also
the extent of the deformation of the sample can be determined.
An automatic recording of the data is made by the apparatus. As
may be Peen from a diagram given the apparatus consists of
three mair. parts: the loading device, the electrical indicator
for the deformation measurement, and a small stage for fixing
the sample. From a diagram of the deformation of a rook sample
as a function of the load it may be seen that in spite of a
step-wise displacement of the drum the recording is sufficiently
accurate. The apparatus described may also be used for testing
other non-metallic materials (rubber, ebonita, plastics etc.).
Card 1/2 There are 2 figures.
An Apparatus for Determining the Mechanical Properties SOV/32-24-10-41/70
of Rocks
ASSOCIATION: Institut nefti Akademii nauk SSSR (Institute of Petroleum,,
AS USSR)
Card 2/2
RATITER, S.B., kand.fix.-mt.nauk; NOSOV, Yu.A., insh.; KONEMY, K.S., Insh.
0
Measuring the radial compression force of rubber sealings
resulting from temperature drops. Vast. mash. 38 nq.9:24-26
S '58. OaRA.11:10)
(Sealing (Teebuoloff)) (Rubber goods--Testing) I
YUSHKIN, V.V.; KONENKOV. K,S4
Apparatus for studying gas-condinmate fields. Trudy VNIIGAZ no*17.'
33-51 162. IMIRA 15:12)
(condensate oil Vello-Equipment and supplies)
I
GUSHCHRIP N.S.; VYBDRNOVA, Ya.I.; STEPANuVA, G.S.; KONENKOV,-K.S.,
Modernization of the FIVT-7 "~. Trudy VNIIGA7& no.17:259-264 162.
(MIR& 15:12)
(Condensate oil wells-Equipment and supplies)
ALEKSANDROV, A.M., inah.,-WHEROV, V.S., Inzh.; BDBROVNIKOV, B.N.,
inzh.; VAGINOV, M.P., inzh.; GUREVICH, B.M., insh.;
.DZHIBELLI, V.S.j, inah.; DROBAKH., V.T,, inzh.; ISAKOVICH,
R.Ya., kand. tekhn. nauk; KAPUSTIN, A.G., inzh.; VIN"
insh.; MININ, A.A., kand.tekhn.nauk; PEVZNER, V.B.,
PESKIN, G.L.2 inzh.; PORTER, L.G., inzh.; IfYADILOV,
A.N., insh.; SLUTSKIY,-L.B., insh.; FEDOSOV, I.V., inzh.;
FRENKELI, B.A.,, insh.,j-,TSIMBLER, Yu.A., inzh.; SHULIGIN,
V.Kh., insh. ESKIN, M.G., kand. tekhn. nauk; VOROBIYEV,
D.T., insh. fdoceased],-,SINELINIKOV, A.V.s, kand. tekhn.
nauk; SHENDLER,.Yu.I., kand. tekhn. nauk, red.; NESMELOV.
S.V.,, insh., zam. glav. red.; NOVIKOVA, M.M., ved. red.;
RASTOVA, G.V,, ved. red.; SOILANIK, G.Ya., ved. red.;
VORONOVA, V.V.., tekhn*;-%ed.
(Automation and apparatus for controlling and regulating produc-
tion processes in the petroleum and petroleum chemical industries]
Avtomatizatsiia, pribor7 kontrolia i re"rovaniia proisvodstven-
nykh protsessov v neftianoi i ne~tekhimicheskoi promyshlenno3ti.
Moskva, Gostoptekhizdat. Book 3. (Control and automation of the
processes of well drilling, recovery, transportation, and storage
of oil'and gas] Kontroll i aytomatizatsiia protsessov bureniia
skvazhin., dobyehi, transporta i khraneniia nefti i gaza. 1963.
551 P. (Automation) (MIRA 16:7)
(Petroleum produ---"-,.4l.on.--Fqu~,]Rment and supplies)
ACCESSION NR: AR4025722 8/0081/64/000/002/DO46/DO46
SOURCE: RZh. Xhimlya, Abs. 2Dd2
AUTHOR: Tabunshchikov, 0. K-,_!~ _Ki_.Se
TITLE: An apparatus for In"atigotion of the phase equilibria of hydrocarbon systems
at low temperatures
bITED SOURCE: Tr. Vaes. n. -1. in-ta prirodn. gazov, vy dp. 17/25, 1962, 265-269
TOPIC TAGS: hydrocarbon, phase equilibrium, low temperature phase equilibrium,
gas Uquid equilibrium
TRANSLATION: An apparatus Is described which permits the study of the phase
equilibria of hydrocarbon systems at a pressure of 300 atmospheres and a temperature
1 up to -100C. The basic part of the instrurnent is a high pressure bomb, which is placed
In a cryostat with an adjustable temperature. The phase equilibrium of a gas-liquid
mixture is obtained by mixing the mixture with a TsEN-IM circulating pump. The
temperature is measured with a copper-constantan thermocouple. The optical 9yatern
permits the quantity of the liqtdd and gaseous phases which are formed in the bomb after
obtaining an equilibrium to be determined visually. The bomb to providwi with connect-
Card -1/2
A.ccFmioN NR: AR4025722
ing pipes, awovo WMoh b"s Ov P860d for'
L. Reznit&ldy UmPliOg the Aafts' during the awyals.
DATE ACQ: o3Mar64 SUB CODE: OC
ENCIg 00
Card 2/2
IONEhOVP S., narodnyy khudozh'nik SSSR, laureat Leninskoy premii
Man is the master of earth., IUn.nat, no*381-3 Mr 163.
(MM 16;4)
(Gonservation of natural resources)
S/046/60/006/01/09/033
B008/B011
AUTHOR; Konenkov, Yu. K.
MW
TITLE: On Normal Waves With Flexural Vibrations of a,Plate
PERIODICAL; Akusticheskiy zhurnalg 19609 vol. 6, No. 1, PP- 57 - 64
TEXT: The present paper deals with'.the investigation of the propagation
of flexural vibrations along an infinite elastic band with aidth K and
thickness h. The following cases are dealt with: the plate margins are
free, fixed, and with articulate support. Gorresponding dispersion equa-
tions are derived and solved (Figs. I - 6). In completion of theoretical
considerations, experiments were made on a 160 cm long aluminum- band. 2
The parameters of the band were: ?-= 2.65 g/cm3, E = 705 - 1011 dyn/cm
a-= 113, h = 0-3 cm, H = 5 cm. Q - thickness of the material)* The
method described by N. S. Ageyeva in Ref. 1 was applied. The excitation
of the band vibrations was made with the aid of a piezoelectric vibrator
with a frequency of 12 kc/sec. With an asymmetrical excitation the
author obtained the wave form of Fig- 7, and with a symmetrical one, the
Card 113
On- -Normal Waves With Flexural Vibrations S/046/60/006/01/09/033
of a Plate B008/BO11
wave form shown in Fig, 8. The normal zero wave was not established, as
the conditions for its excitation were unfavorable. Figs- 7 and 8 also
indicate the measurement results showing the distribution of the dis-
placement over the width of the plate. The coordinate x is plotted on
the vertical axis, and the amplitude of the displacement on the hori-
zontal one. The table contains.the distances between the nodes for dif-
ferent y-values (symmetrical excitation), and the calculated mean value
of-5-37 cm. The same distance determined theoretically is 5.4 cm. Thus
it was possible to establiab a good agreement between theory and experi-lzc
ment. The ocdamnce of waves of other orders of magnitude, which are in-
evitable under real condLtiona, was found to be the cause of a certain
dIvergence-This circumstance gave rise to a distortion of the node
lines.(Table). The occutrence of a.tranaversal resonance was observed,
as expected, on the frequency with a critical value for the wave shown
in Fig- 7. The wave did not'propagate under this frequency and entered
the class of inhomogeneous waves. The author thanks N. S. Ageyeva for
Card 2/3
(KOVENKOV Yu
2 RVK-A-
W20igh-tYps f:Lwmral wave. Akut.zbur. 6 Fol:.124-126 160,
(NM 14:5)
Is Akusticheskiy iustitut AN SSSR, Moskva, I
I (Sound wavei~)-
A
S/046/62/008/002/016/016
B104/B108
AUTHOR: Konenkov, Yu. K. (Moscow)
TITLE: Calculation of the phase,velocities of normal waves in
bending vibrations of elastic bands
PERIODICAL; Akusticheskiy zhurnal, v. 8, no. 2, 1962, 241-242
TEXT: In a previous article (Akust. zh., 1960, 5, Is 57-64) the author
derived a transcendent equation whose solution made it possible to find
the phase velocities of normal waves in bending vibrations of elastic bands.
In the propagation of waves (symmetricaa. and antiBymmetrical) in a plate
fixed at the edges, these equations are
Ira-.
Cthy2Q-Q.
21
Card 1/4
S/04 62/008/002/016/016
Calculation of the phase velocities ... B104YB106
tgy".
2
th
is the dimen'sionless frequency of the vibrations
h
72- . k and pare the Lame elastic constants;
h, H are density, thickness and width of the plate, Q is the
n
dimensionless natural frequency of the vibrations; (,j is their angular
frequency. The dimensionless phase velocity of the normal wave is
G The solutions of (1)-(2) in zeroth approximation are
n S?n
Card
S/04 62/008/002/016/016
Calculation of the phase velocities ... B104YB100
nlal< On< (a + t)';0-. n2k + t
2 coO (A)
nlAl< On< (n + i)':&'; n2k
A virtually exact solution can be obtained by one more step-of successive
approximation:
Card 3/4
5/046/62/008/003/005/007
B108/B104
AUTHORt ~-OnAnkAY-4-LkZ.1 Noscow)
TITLE t' Waves in a viscous liquid
PERIODIC,,',L.- Akusticheakiy zhurnal, v. 6, no. 3, 1962, 320 324
TEXTs The motion 'of a viscous -liquid subjected to a small perturbation
can be described by the equations
dp/at 0c2div
aG/at -grad p + 92U + (% + %/3)grad div 0.
Q IV
0
u is the velocity of displacement of the particles in the liquid, ~andq
2
are the coefficients of viscosity, Q 0 G is the modulus of compression.
This problem is solved for two concrete cases (free oscillations in a
liquid bounded by plane rigid walls, bending oscillations of thin plate
which is in contact with,a viscous liquid on one side) by introducing a-
scalar potential y and a vector potential which satisfy the condition
Card 1/2
S/046/62/008/003/005/007
Waves in a viscous liquid B108/B104
u - curil + grad and by a transition to the harmonic wavd equations.
Calculation by thTs method can also be used when heat-conduction louses
have to be taken into account. In such a case new solutions bf the wave
.equation are found. A real liquid has waves related to the thermal
processes caused by compression.and expansion of such a liq .uid. There is
-1 table.
SUb?AITTE,D; April 179 1961
,Card 2/2
.KTggff,_~g,_ ~(14?skva)
7-
Waves in a viscous fluids Akw~ozhur. 8 noo3s320-324 .162.
(NIRL 15:11)
(Fluid dyiamioo') (Vaves)
KONENKOV, Yu.K.
Diffraction of a deflective wave on a circular obstacle in a
plate, Akust. zhur. 10 no.2:186-190 164. (MIRA 17:6)
I..Vaeooyuznyy tsentralInyy nauchno-isoledovateltakiy institut
okhrarq truda,, Moskva,,
140 REr SOV 00
-ENCLi s IE
UB Co
OF
Ps
KONEV, F. A.
"Investigation of the Process of Filtration in Preparin.g solu-
tions for Injection." Cand Pharm Sel, 1~oscow Pharmaceutical Inst,
Min Health USSR, Moscow, 1955. (KL. No 11. Mar 55)
SO: Sm. No. 670, 29 Sep 55--Survey of Scientific and Technical
Dissertations Defended at USSR Higher Educational Institutions (15)
I... - - ,
1. -7~ -- ! , : - .1 1
I
KONEV, F.A.; OBUKROVSKIT, Ta.A.
Productivity of soniautomatic ampule machines. Med.prom. 12
no.4:27-32 Ap 158. (MIRA 11:5)
1. lhar'kovskiy nauchno-iseledovatellskiy khimiko-f9rmntsevticheskiy
institut.
(DRUG MUSTRY-sqummm Aim summs)
AUTHORS: Konev, F.A., Kolesnikov, N.A., Kolesnikov, D.G. 32-3-49/52
TITLE- The Automation of the Filtering Process of Injection Solutions
(Avtomatizatsiya protsessa fil'trovaniya in"yektsionnykhras 4-VO-OV
PERIODICAL: Zavodskaya Laboratoriya, 1958, Vol. 24, Nr 3, PP. 375-375 (USSR)
ABSTRACT: For the continuous and uniform feeding of suspensions onto the
filter when filtering injection solutions an automatic system was
developed. In principle the scheme consists of four coils, two
selenium rectifiers and two relays which form part of a common
circuit, which, by the rising or falling motion of an iron core
(which isenolosed in a glass ampule and generates induction Gar-
rent) opens and closes an electromagnetic three-way faucet. The
latter is mounted on the container of the liquid, Which, besides,
is connected with the vacuum as well as with the spare container
for the liquid and with the filter. By the interaction between the
vaaaum and the three-way faucet connected with the atmosphere,
which is connected with the level of the liquid (by a float), the
container is alvmys filled up again as soon as the level is reduced
Card 1/2 to a certain height, so that in this my a continuous feeding of
The Automation of the Filtering Process of 32-3-49/52
Injection Solutions
the filter is attained. There -is 1 figure, and 1 reference, I of
which is Slavic.
ASSMATION: Scientific Research Institute for Chemical Phamaceutics, Khar'kov
(Khar'kovskiy nauchno-issledovatel'skiy khimiko-farmatsevticheskiy
institut)
AVAILABLE: Library of Congress
1. Injection solutions-Fi-Itering processes
Card 2,/2
KONEV, ?.A.
Filtration of injection solutions. Apt.delo 8 no.5t64-71 S-0 159.
(KM 13 1. 1)
1. Is lrharOkwakogo nauchno-lealedovatel'olcogo khtmika-farmateevti-
ch.eskogo Instituta. (FIIIPARS An FILTRATION)
KOIOV F.A.
of the product17e capacity of apparatus in ampule
manufacture. Med. prom. 13 no.8148-53 Ag '59. (MIRA 131-80
1
1. Khartkoveldy nauchno-issledovatel skiy khimiko-farmatsevticheskiy
institut.
(DRUG INDUSTRY)
KOITIV, F.A.; OBUKHOVSKIT~ Ta.A.
Obtaining doozygenated distilled water. Med.prom. 13 no.11:28-31
IT '59. (Km 13:3)
1. Marikovskiy nauchno-lonledovatellskiy khtmiko-farmtsaytichookly
inatitut.
(WAMM, Dlsmm)
KOHN$ Pv**;: XUMUKHOTO Lwe
Filtration of Injection solutions and other liquids in pharma-
ceutical practice. Apt.delo 9 no.2t65-6? xr-AP 16o.
(KIRA 13:6)
1. Is lbartkovskogo nauchno-issledowatel'skogo khimiko-farmR-
tsevticbeokogo lustituta.
(731TIM AND FILIMION) (FELMCT)
KONEVp F.A.; KRAYNYUKOV9 N.I.; KOVALENKOp V.S.
Determination of the durability of the capillaries of amall ampulea.
Mod. prom. 14 no.5:42-" W 160. (MIRA 13:9)
I* Lbarikovskiy nauchno-iosledovatel'skiy lehimiko-farmatsikv~icheskiy
institut.
(DRUG INDUSTIM)
EDMIT, P.A.; OBUKHOVSKIT, YAL.A.
Determination of gas composition and pressure In ampules with
&.solution. Ned.prom. 14 no.6t38-41 An 160. (=A 13W
1. Kharlitovskly nauchno-Issledovatellskly khtmiko-farmatsevti-
Cheekly lustitut.
(SOLUTIONS (PRAMOr))
t~, Mt'!Pq
KONEV9 F.A. [Koniev, F.A.); KIJRCIfENKO, I.N.
V,~ ...... -
Studying the stability of ergotal injection Solution. Farmatsev.
zhur. 17 no.6:40-43 16L2. (MERA 17:6)
l.-Kharlkovskiy nauchno-issledovatelfskiy khimi\ko-farmatsevtic.heskiy
institut.
KONEV, F.A. (Koniev.. F.A.1; TIMOFEYEV,, V.V. (Tymofiievp V.V*j
Air purification from mechanical impurities. Xhim. prom. (Ukr*]
no.3S80-81 J1-S '63. (MIRA 17t8)
1. Kharlkovok:Ly- naachno-isaledovatellokiy lrbimiko-farmatesvti-
cheskiy institut.
KULF.SH, K.F.; KONEV, F.A. [Koniev, F.A.); BUGRIM, N.A. [Buhrim, N.A.1;
Prinimali uchastiye: LAPKINA, A.M.; GENDENSHTMI, Ye.I.
Increasing the production of prepared drugs by lowering the
number of extemporaneous prescriptions of pharmacies.
Farmatsev. zhur. 18 no.5:3-7 163. (KIRA 17:8)
1. K-arlkovskiy nauchno-issledovatel'skiy khimiko-farmtsevti-
cheskiy institut.
,.-KONEVt F.A.;,TIMOFETEV, V.V,; FEDORCHFIIKO, I.M.; ANDRIfEVSKIYO R.A.
Ceramic metal filters for the filtration of air and water.
Porosh. met. 4 no.604-88 N-D 164. (MIRA 180)
1. Kharlkovskiy nauchno-issledovatellakly khimiko-farmatsevti-
cheakiy institut i,Inatitut problem materialovedeniya AN UkrSSR.
KIJRCHENKO, LN.-_~Offl~~
, F.A,,
Study of the stability of * thiamine chloride solutions for
Injections. Apt. delo 13 60.4t27-30 Jl-Ag 164. (MIRA 180)
1. KharIkovskiy nauchno-issledovateliskiy khimiko-farmatsevti-
cheskly institut.
KONEV, F.A. (Kcniev, F.A.]
Liquid prepared druga and prospecta for their production.
Farmatsev.zhur. 19 no.lx6-9 164. (MIRA 18:5)
1. Kharlkovskiy nauchno-iseledovatellskiy Wmiko-famatsevticheskiy
institut.
KIJIF U., yj~-. -.1
of 6x-" dr-agii W"4'h tablbta. Apt,. d lo 14
W4-1 L' 9-15 A-P 16~. l8alo)
;shE,r,k!,.y
KIMCHENKO, KONEVj, F.A. [Koniev, F.A,I
Study of the stability of ergotamine solution for idjections.
I (MIPA- 18:.11)
armatsev. -zhur. 20 no.5-.13-16 165.
F
1. Kharlkovskiy muchno-issledovatellskiy khimiko-farmdtserti-
cheskiy institut. Subaitted March 29, 1965.
KOM OK OVA.N.; CHUBUKOVA.T.
------- m-lew"Mm
Factory production of gypsum fiber slabs. Stroi.mat., izdel. I
konstr. I no.8:24-26 A9155. (MLRA 8:11)
1. Eaveduyushchly laboratoriyey Danilowskogo alebastrovogo savoda
(for Xonenkova) 2, Nachallnik tsekha Dantlovskogo alebastrovogo
savads, (for Chubukowa)
(Wallboard)
KONEIIKOVA-DAVIDENKO T.D.
Some data on the clinical and experimental study of ganglionic, blocking
agents. Eksper. khir.,i anest. 9 no.1:77-80 Ja-F 164.
(WRA 17:12)
1. Kafedra gospitallnoy khirurgii No.2 (zav. - prof. D.P.Chukhriyenko)
Dnepropetrovskogo meditsinskogo institute.
COUNTRI :
CATEGORY : Chemical, Tecbnolopy. Chemical Products and
Their -'Applications. Leather. Pur. Gelatine.*
A
B3
JOUR
!
zt?,' in 0 1c;
X11 i
A
,
.
'nonert~, C.
2 i 2 Ppa.,~ons for '41'pnni(le T,osses Fncountpred in the
Vef-,et-able Tanninp Processes
ORIG. FUJ3 Intl. Usoars, 1958, 5, No 11, 410-417
ABO: ~'T C T A re-view of -liter-Lure en4 anmlysis of reasons
'i-11*1-taininp to losses of tatini0es, encotintered
in vc-(~Ctable, tanninf, proces-ses "Is a filixtion
tl~c aszvortme:it of riianu-
e tanninF met!-.od,
Tactured lpatN4r nroducti, the emnloyed tan-
ning mediurn, and. the sedimentation cliaracte-
ristics of titnninc, solutions. i~ theoretical
ex-Aanation c-f 'Uhe nature of losses is T)re-
sented. Methods of reilucing losses are j Ti ven
for cortain isolated cases. The 11)DA.i0f~rai,lby
covers 32 titles.- G. Narkus.
*Tnnninp! Materials. Indlistrial 1roteins.
ILIESCU, Ch., dr.t SBIERL,A,, ingel TOGANpM*p biolog.; KONERTH chim,
Study on the Rumanian hardwood as raw material for the
pu1p industry. Cel hirtie 10 n6.71&217~-225 JI-Ag"61.
FISCHGOI,DpS.p ing,j POPESCUtG,., biolog; AVTCE., I,p ing.; BUROVA,,T,,
candidat Atiinte tebnice; HERSCUO.,,. ohim.; POPMCIM., abig.;
PLATCK.,14.p irg.; KCLER!M,#,gkm_,qhim.
Some conaideratipsion the utilization of beochwood tar ob-
taining chemical pu* Cel hirtie 10 no,718:225-231 n-Ag'61-
PIAT(IffvK.v ing.1 CMUNTINESCOAp ing*II K(MMTH,,H,,, chimo
Use of waste materialo-fr6m-forestry operation and wood
industry mills, Gel birtie 10 no.7/6M5-2a JI-ACS61.
Ing.; BURGVA;~J.
CMSTANTII~-Cu 0., Ing. IHOTOPKMW,Aes~
Ing,; KOVERTH,H.&, chim.; POPOVICI,M.., chl-m.; RERSCU'Day chi$.;
PEIMpG*, inges, PLATON,U., Ing,-'.
Cbtaining SNS chemicafand semichekcal itndps\fram reed by
means of continuous digesting in thd,Pandia t7Pel, instRll&-
tione Cel bf 162
,Artie 11 no-3tlOO-101 Mr.
PLATMI,M., ing.; CONSWITMESCU,C., ing.; DRAGHICI,F., ing.; AM -
chim.; ANTCN~I.,,,ing.; BUROVA,T.0 inge; FISCHGOLD,S.., ing.;
HOTOPEIrOl."U,A., ing.
Induotrial, experiments in turning to account waste materialo
resulting fran the exploitation and industrialization of wood.
Cel hirtie 11 noOZ102-106 Mr'62.
ESAVU,F., ing.; 1UKW.V1,j1A, ing.; P11DRUCHOVICI, F., ing.; FISCHGOID,S.
ing.; POPESCU,G., biolog.; ANTON, Is. ing.; POPOVICI, M. ing.;
HOTOPELEAIIIJ,A., ing.;-REICHMAVN, E., ing.; COIISTANTINESCU,O.,
ing.
Studies o- how to obtain an alkaline pulp (sulfate and natron)
from strat by continuous digesting in a Pandia type installa-
tion. Col. hirtle U no,6t2O5-219 J062
1Y
ILIESCUpGh.,, dr.1 KCWHMjH-, chim; AVDRUCHOVICI, F., Ing.
Laboratory and Industrial tests to obtain pulp from beachwood.
Cel hirtie 11 noo7$245-252 R~62*
BUROVA,T., ing. POPOVICI,N., ing.; KCINERTH,H,,, ing.; IIOVODVORSKI.,L.,ing.
Some experiments for obtaining high grade chemical cellulose
from fir wood. Pt.2. Gel hirtie 12 no.5/6:169-175 MY-J9163.
FISCHGOLD28.9 ing., poMOU,G., Iliolog; HMSCUyO.,, chim.; XTERTIT.,11.chim.
Considerations on the utilization of the red heart beeohwood
in different alteration stages for obtaining chemiaal pulpo
Gel hirtie 12 no.112357-362 P63-
I A
Fig,'HGOLD, S., ing., YON-FWTH, If.,
Research on obtaining ray - -,ulp from be-achwood, Col
hirtie 13 no. 301-81 mr 64.
KONEF2A, M.
Some architectural problems concerning the construction of metallurgical
plants. p. 410. (Hutnicke Listy, Vol. 12, No. 5, May 1957, Brno, Czechoslovakia)
SO: Monthly List of East European Accessions (EEAL) LC, Vol. 6, No. 8, Aug 1957. Uncl.
VINZENZ, Zdenek, inz.; KONERZA, Miroslav, inz;
Development of the Czechoslovak metallurgical industry from
the viewpoint of territorial distribution. Hut listy 16
no.10:69&704 0 161.
1. Hutni projekt, Praha.
Increase of slectric.conductivity and ciiange In temperature of
the distilled water by.wire electrodes, Biltan mat fiz Mak 11:
27-32 160.
KONESTABR) V.
KONESTABR, V. The Yugozlav navy. p. 8.
Vol- 3a, No- 8, Aug- 1956.
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So: East ?European Aceessiong Vol* 6s No* 22 Feb. 1957