SCIENTIFIC ABSTRACT KUZNETSOV, A. V. - KUZNETSOV, A. V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000928110019-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 20, 2000
• Sequence Number: 19
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

S/182/62/000/012/001/005
Press forging in sectional dies D040/DI12
is made to non-Soviet special presses for sectional-die rorgingp such as the U.S,
Baldwin press, the Gorman "Siompolkamp", or the British Wilkins Mitchell.
There are 8 figures and I table.
Card 2/2

NIKOLISKIY, L.N.1 GAVRILOVO M.Ye.;, KIZNETSOV, A.V.; PANICHEV, F.P.
Experience in and ways 6f introdusing rotary swaging for further
forging. Kuz,-ahtam,proizv, 5 no.8:15-18 Ag 163* WRA 16:9)
hw

PHASE I BOOK EXPLOITATION SOV/5715
Kazandzhan, Pogost Karapetovich, and Andrey Vasillyevich Kuznetsov
Turbovintovyye dvigateli; rabochiy protsess I ekspluatatsionnyye
kharakterietiki (Turboprop Engines; Working Process and Oper-
ational Characteristics) Moscow, Voyenizdat M-va-obor.SSSR, 1961.
263 P. 10,000 copies printed.
Ed,: 0. 1. Kalashnik,, Engineer, Lieutenant Colonel; Tech. Ed.: R. L.
Solomonik.
PURPOSE: This book is intended for the engineering and technical
personnel of the Air Force and the Civil Air Fleet. It may also be
useful to students in aviation and technical Institutes and to
technical personnel operating gas-turbine power plants in trans-
port and under stationary conditions.
COVERAGE: The book deals with the design and operating principles of
turboprop engines and their components. Physical phenomena occur-
ring in the engine are described. Operational and regulation
Card-1/6'-

Turboprop Engines; (Cont.) SOV/5715
problems are treated in detail. Factual materialB are based on
non-Soviet practices in aviation-engine design, and questions of
future prospects reflect non-Soviet opinion. The authors thank
Yu. N. Nechayev, Doctor of Technical Sciences, and N. G. Smirnov,
Candidate of Technical Sciences. There are 11 references, all
Soviet.
TABLE OF CONTENTS-
IntroductJ,on 3
1. Basic requirements for aviation engines 3
2. Application of turboprop engines (TPE) in aviation 5
Ch. I. Principle of TPE Operation , 7
3. Diagram and principle of operation of TPE 7
4. Propeller, reactive, and total power. Specific para-
meters of TPE 13
5. Brief information on the design of existing TPE 19
Card 2/6

KUZNETSOVI A.V., starshiy tekbnik-leytenaat; LASHMICH, A.K.,, tekhaik-
---l-ei~ienant,
They did itthemoelves. Vevt.Vozd.F1. no.6:82 je 161.
(MIRL 14:8)
(Transport planes) (Slide rule)

KUZIZTSOV, k.; kand.tekhn.nauk
Negative thrust. Grazhd.av. IS no.5s26-27 My 161. (MIRA 14:5)
(Airplaneo-Turbine-propoller engines)

ACCESSION NRt AP4040585- S/0040/64/(P-8/003/0567/05U
AUTHORs Kuzneteov
A, V, (Kazan)
TITLEt flie P; 3119M Of jet
oblem of jet flow ovor a slightly oscillating contour
SOURCE: Prikladnaya matematika i mekhanikap ve, 28,, no* 3. 1964t 567-571 A
TOPIC TAGSt oscillating contourp translational oeoillationp flow velocity) radius
of curvaturep rotational osaillation, perturbation volooityp harmonic plate,,
!.anharmanic
ABSTRACTs The problem of an oscillating contour with given translational oscil-
lation OC(t) at a given angle W(t) relative to its principal position axiq was
discussed analytically. For small and i& the moving coordinate system can be'
related to the fixed system by,.
whoro.6 = cc Cr =OC + x The solid body contour is defined by F
x x
(xy,,t) = Op and for the flo%i 'velocity vector in the oscillating field n by
ive
+ +
Cc r-a-
113
vj

-7~
,.ACGESSION NRt AP4W585
:one has,, to first order
VP;Vr Oro, +,V X (6,x VS)) VF
i,If the radius of curvature of the contour is large, ~o(d% the above
expression yields for translational oscillations
6V
and for rotational oscillations
) ev
R as of
In the general case of a separated jet flow Taylor's theorem is used to expand
ithe velocity vector, thus V(x,,y) Vo +AVOv and the perturbation velocity is
:given by-the approximation
-&V. - 1W
which leads to a solution/for A This solution indicates that in harmonic.
Iplate oscillations the change'in the perturbation velocity is anharmonic In time,
Orige art* hass 23 equations and 1 figure,
CIATIONt none
7-7

KUZIrAi"C!3:OV) A.V., nspi-mnl;
at er,
~"-t r=.cg-&m3 for plotting axonometric projections. lz7.vvi3.
P
cbob. zav. ;mar, himno!,re noo5;5-12 164. (MIRA 163)
1. K~amrarslddy gornomtallurgicheskiy institut.

KUZITE.T:SC'V-',
Porameters of the elasr,!,ln O.ent;nts of car s.r 9pring eusvmelon.
Sbor. t--ud. 't.!T?HT na.22.5.,,99-109 164. OICRA 1?.-,12)

KUZNETZOV, A.V.
_...... -~IINIZI, 1 11--.1-11
etermination of the "dead time" of an X-ray counter of the
URS-501 apparatus. Zav. labs 30 no.5:629-61,0 164. (HIPA 17%5)
1. Petrozavodekly gosudarstvemW universitet.

U3ing coordinate tran3parencies in plotting axonometric
rr,prevmtations. Vest.mashinostr. 4.1 rio.3*87-89 Mr '64.
KF A 1-1 :4'j

r% 1 T
SUBJECT USSR/)IATHEMATICS/Functional analysis CARD 1/2 PG 305
AUTHOR KUZNECOV A.V., TRLCHTENBROT B.A.
TITLE Investigation of the partial recursive operators with the means
of the theory of the Bairs space.
PERIODICA1 Doklady Akad. Nauk 105, 897-900 (1955)
reviewed 10/1956
Theqperators considered are partial recursive operators g - Tff] where f is
a function of one variable and g is a function of one variable or a constant.
0T denotes the domain of full definition of the operator T, i.e. the met of
all those fully defined functions f for which T[f] is also fully defined.
The author given examples to show how diverse the sets 0 T can be. He then
correlates each fully defined function f with the point of
the Bair* space J. A, primitive recursive enumeration An of the Baire inter-
vals is given and a set in called effectively open if it is representable in
00
the form U 6a(") where &(n) in general recursive. Effective GS , F G
11-1 a, I
*to are defined similarly. Theorem 1. Every partial recursive operator
g - T[f] considered over j only, has a representation in the form

Doklady Akad. Nauk 897-900 (1955) CARD 2/2 PG 305
g(x) - b(,kt(f Z where a and b are primitive recursive. Theorem 2.
A necessary and sufficient condition that there exists a partial recursive
operator T such that 0T - N is that X be an effective GS . Effective con-
tinuity, uniform continuity, compactness and boundedness are then introduced
and their relations investigated, e.g. Theorem 3--Bvery p&rtial recursive
operator gives an effectively continuous mapping of its full definition into
J. Theorem 4. A mapping which is effectively continuous on an effectively
compact not is effectively uniformly continuous on it. Theorem 5. If T in a
partial recursive operator then on any effectively closed M SOT it is
general recursive. Finally various results are proved which bear on the problem
of whioh funotions are riduoible to effectively olosea points.
AM, ~_M
WE-

16(l) PHASE I BOOK EXPLOITATION SOV/1708
Akademiya nauk SSSR. Matematicheskiy institut
'Sbornik statey po matematicheskoy logike i yeye prilozheniyam k
nekotorym voprosam kibernetiki (Collection of Articles on Mathe-
matical Logic and Its Applications to Certain Problems of
Cybernetics) Moscow, Izd-vo AN SSSRj 1958. 362 p. (Seriess Itat
Trudy, t-. 51) 3,500 copies printed.
Rasp. Ed.: S.V. Yablonskiy., Candidate of Physical and Mathematical
Sciencesj Ed. of Publishing Housei A.Z. Ryvkin and L.K. Nikolayevaj
Tech, Ed.: T.P. Polenova.
PURPOSE: This collection of articles contains original contributions
of Soviet mathematicians in mathematical logic and is intended for
mathematicians working in this field.
COVERAM The articles deal with studies of problems connected with
mathematical logic and their applications to certain problems-of
cybernetics. Primarily, Switching circuits are studied, but many
Card 1A

Collection of Articles on Mathematical Logic (Cont.) 1 SOV/1706
of the results obtained are of a more general character. The
content of the collection of articles is closely conne7oted with
many branches of cybernetics which study the methods of describing
the processing of discrete information, problems of the analysis
and synthesis of control systems, and methods of controlling the
performance of control systems. The characteristic feature of
these articles is their connection with various fields of mathe-
matics such asjmathematical logic, combination analysis, set
theory, algebra, topology and theory or numbers. All articles
were written in the years 1954-3955)and the concepts presented are
arranged in the book in a systematic order. The first.articles
concern problems of mathematical logic, then problems of the
theory of the synthesis of circuits are examined, and finally
problems of the theory of controlling the performance of circuits
are considered. The editor thanks Professor A.A. Lyapunov,
Professor S.A. Yanovskiy$ B.Yu. Pillchak, A.P. Yershov,
V.A. Uspenskiy and Yu.I. Yanov for their remarks in connection
with the final editing of the collection.
TAKE OF CONTENTS:
Preface 3
Yablonakiy,, S.V,- Functional Construction in k-valued Logic 5
Card 2/7

Collection of Articles on Mathematical Logic (Cont.) SOV/1708
Introduction
Ch. I. Foundations of Logic Algebra and the Theory of
5
Switching Circuits 7
1. Functions of the logic algebra and some of their
properties 7
2. Criteria for the completeness of systems of functionaJ2
3. On the representation of a function from P2 by means
of normal forms 22
4. Techni ue of construction of simplified and minimal
d.n.f. Nisjunctive normal formal 29
Elements of the theory of awitching-eircuits 39
Functions of the logic algebra as a mean for a
definition of an n-place operator over a field of two
numbers (0, 11. Types of functions 52
Ch.1E. Functional Constructions in the Many-valued Logic 56
T. Systems of the Pk function. Superposition of
functions. Closed classes 56
8. Homomorphism of systems of functions 58
9. Duality 6o
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Collection of Articles on Mathematical Logic (Cont.)- SOV/1708
10. Complete systems. Theorem on functionally complete
systems 61
11. Basic lemma 68
12. Criterion of completeness 70
13. Closed classes with a finite basis. "Precomplete"
[predpolnyyel classes 17
14. Auxiliary lemma 1
15. Classes of monotone functions 82
16. Classes of functions of type T 85
ly. Classes of functions of type U 91
18. classes Lk.(x) of linear functions 93
19. Classes 8k, of self-binary functions 100
Ch. IIL Functional Completeness in Three-valued Logic log
20. "Precomplete" classes in P3 log
21. Formulation of a theorem on functional completeness
in P and consideration of a planfbr proof
h 113
22. Ce
ain lemmas for functions from P3 115
23. Proof of a theorem on functional completeness 123

L-31lection of Articles on Mathematical Logic (Cont.) SOV/1708
Lhuravlev, Yu.I.. On the Separability of Subsets of Vertices of
an n-dimenBional Unit Cube 143
introduction 143
1. Statement of Problem 143
2. Solution of Logical Separability Problem 145
3. On the Seleotion of Truth Variables 151
References 157
Lupanov, O.B. On the Possibilities of a Synthesis of Circuits
of Arbitrary Elements 158
References 173
KUzneteov,, A.V. On the Property of Functions Realized by
Nonplanar Circuits With Nonrepeating Contact 174
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Collection of Articles on Mathematical Logic (Cont.) SOV/1708
Kuznetsov, AN. On Nonrepeating Switching Circuits and Non-
repeating Superpositions of Functions in Logic Algebra 3.86
Trakhtenbrot, B.A. On the Theory of Nonrepeating Switching
Circuits 226
Introduction 226
1. Graphs, networks, and Circuits 226
2. Nonseparable networks, streamlined and homogeneous
subgraphs 232
3. Separation of separable networks 238
4. Separable circuits 245
5, Synthesis of nonrepeating circuits 255
References 269
Chegis, I.A.,~and S.V. Yablonskiy. Logical Means of Control
of Electrical Circuit Performance 270
Introduction 270
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Collection of Articles on Mathematical Logic (Cont.) SOV/1708
Ch. I. General Theory of the Construction of Testa 270
1. Tables of fault functions and means for their
construction 2~2
2. Tests and their construction 2 0
Certain rules for test construction 28
Construction of test for dual circuits 29~
5. Unit tests 304
Ch.31. Methods of Construction of Tests for Individual
Circuit Classes 307
6. Tests for circuits which realize the elementary
symmetric functions 308
Test for circuit which realizes the linear function 322
Test for comparison circuit 326
9. Ordered and conditional tests 334
10. Test for a binary adder circuit 339
References 360
AVAILABLEt Library.of Congress LK/ad
Card 7/7 6-16-59

KUMETSOV. A.-7
"The Impossibility of Constructing an Algebraic kDparatus with a Finite
Number of Functions."
report presented at A3-1-Union Conference on Problems in tbDTheory of Relay Devices,
Inst. for Automation wA Remote Control AN IBM. 3-9 Oct ~951-
Vestnik AN SSSR, 1958, No. 1, v. 28, pp. 131-132. (author Ostianu, V. M.)

AUTHORz SOV/42-13-3-29/41
TITLEt Algorithms as Operations in Algetraip Systems (Algoritmy kak
k
operataii v algebraicheakikh sistemakh)
PERIODICAL: Uspekhi matematicheskikh naukq 1958, Vol 13, Nr 3, pp 240-241 (USSR)
ABSTRACT: The author prdposes a general scheme according to which the
investigation of the existenos of algorithms can be-performed
on a purely algebraic way. The scheme bases on the general
theory of algebraic systems.
Card 1/1

KUZNIITSOV. A.V.
One property of functions realized by means of nonplane non-
repetitive circuits. Trudy Xnt.inst. 513174-185 '58.
(Boolean functions) (MIRA 11:11)
a. ..i

KUZNBTSOV. I.V.
Nonrepatitive contact circuits and nonrepatitive superpositions
of functions 'belonging to the algebra of loglo, Trudy Hateinste
51:186-225 158, (MIRA 11:11)
(Electric circuits) (Algebra, Boolean)

F11
11 i
jj 114 lit" 3 3111.1
Lob
m
44
Aj
JAN I

KUZKETSOV, A.V.; PADUCHEVA, Ye-V-; IMMOIA3ZVA, I.M.
InforWtional language for geometry and the algorim for
translation from the Russian to the informational language.
Boob. Otd.makh.i avtom.inform.rab. no.;40-73 161. (MIRA 15:2)
(programming languages (Elootronic Oomputers)-Goometry)

KMXETSOV A. V.; YUDITSKIY, M. M., kand. tekbn. nauko doteent
tric projections# Vent. mashinootre
Devioea for plotting axOnme
42 no.io:82-85 0 162. (MMA 15: 10)
(Ge=atrical drawing--Zquipment and supplies)

ACC NR1 AR6017338 SOURCE CODE: UR/0044/66/000/001/BO78/BO79
AUTHOR: Kuznetsov. A. V.
REr SOURCE: Tr. Seminars po obratn. krayev. zadacham. Kazansk. un-t, Vyp. 2, 194t
TITLE., Jet flow of a slightly fluctuating contour
SOURCE: Ref. zh. Hatematika, Abs. IB368
TOPIC TAGS: jet flow, boundary value problem, "61) U~Af
0
TRANSLATION: The plane problem %f small fluctuations of an arbitrary curvilinear arc
flowing with separation of the Jets is studied. The liquid is considered to be ideal
weightless and incompressible. The oncoming current may be unlimited and contained I
a channel having parallel rectilinear walls. A solution is given for the boundary
value problem and fbrmulas.are introduced for the forces acting on the fluctuating
contour. Considered in detail is the case of a plane disc which makes small high-fre
quency hamonic fluctuations in an unlimited flow. Hamonic fluctuations and pulse
motion of a disc In a channel are also considered. As a limiting case of pulse mo-
tion, the known solution of the contour shock-wave problem in the case of separated
jet flowia obtained. M. Gurevich.
SUB CODE:~Op/ UDC: 517.9:530.145.6
Card_ 1/1'MT

KUZNETSOV, A.V.1 TEMINASOV9 Tu.S.
Theor7 of X-ray scattering by mosaic er7stals. Iristallograrii'l 6
no*2il77-183 Nr-Ap 161. (MIM 14:9)
1. Petrozuvodaidy gosudaratvennyy universitet4
'(X rays--Scattering) (Crystals)

S/057/61/03VOO3/0i8/019-
B125/B209
AUTHORS: Kuznetsov, A. V., Terminasov, Yu. S.
TITLE: Consideration of secondary extinction
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 31, no. 3, 1961, 383-366
TEXT: The authors derive formulas for the integral reflection of a
massive specimen, taking into account secondary extinction and assuming
the mosaic blocks to have equal axes and equal probability of orientation.
On the same assumptiorethey derive the thickness of the elementary layer
as a function of the block size. In this casep the secondary extinction
of this layer is supposed to.be negligible. A correction for secondary
extinction has to be introduced if in every column of mosaic blocks in the
direction of the primary beam at least two blocks are aligned in reflect-
ing position. When the blocks are large and the probability that they
are aligned in reflecting position,is the same in every column, one
single block may appear in the center if the effect of secondary extinction
vanishes. In the case of smaller blocks,.m blocks in reflecting position
may appear in every column. In each case, the entire volume of the speci-'
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Consideration of secondary extinction 3/057/61/031/003/018/019
B125/B209
men may be divided into m layers, and in each of these layers the effect
of secondary extinction may be assumed to be of the same intensity. The
authors examined the diffraction at a thick polyoryptalline plate. The
angle between the primary beam and the plate surface is denoted by a;
denotes the corresponding angle for the diffracted beam. The total
energy scattered from the first layer into all rings of volume dV amountel.
to ZP PQOOS dV*o In the present paper, the same notations as
1 2 0 ~10
in the paper of P. James, Opticheskiye printsipy difraktaii rentgenovskikh
luchey, IL, M-t 499 1950, are used. Here and henceforward,the summatioll
sign without any indices denotes summation over all Debye-Scherrer rings.;
In the case of a massive specimen, the cumber of elementary layers may be
assumed to be infinite. For that casey
*XP _i' sing
P Pq Cos 60 1 -na
An a% (7~
2p (I -I- (Y'PQ '.' 8.) k
&XP
2 And E - (I
Card 2/ 5
OR',

Consideration of secondary extinction S/05 61/031/003/018/019
B125YB209
In the calculation of the energy falling upon the short region 1 (Which
is short with respect to the radius r of the ring) of the entire ring',
Eq. (7) has to be multiplied by
21%rsin 240
SIDG, d
P Pot 4XP 14 -4- -0170) fill a
A ilin d8
7 -f- OXP ming
BW sin 00 . ---I -I)
(I F(2PQcO'00);1 -in
A.
When small blocks are considered, the expression
P PQ1
err sin so 1 -4- sin a) -#- I 2PQ 403 (14),
5. ( Z -nP2
instead of Eq. (8),holds. for the dependence of the integral intensity on
the block size, when secondary extinction is taken into account (when
P . .1 i p qc 0 a ri~ dVI Eq. (14) may be regarded as a limit which,
1 2 0 o
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-J
T.
M

Consideration of secondary extinction S/05 61/031/003/018/019
Y
B125
B209

in the case of strong granulation of the blocks, is approached by the
integral intensity. Secondary ixtinotion lowers the integral intensity
to a considerable extentj if
+ a'n Z pqcoe This
a is of the same order of magnitude as 1 -$
.
0
8,
no 2
is probably the case only with hard radiation and weakly absorbing media.
But even for an Mo radiation,
I
sina 1 Z:pqcosO,-,,0.6 cm- holds for an Al sample when

(1 + 27 cm-
a)

a The effect of seqondary extinction for any size of the mosaic
0
blocks is only weak if the quantity I z7pqcos4 may be neglected as
2 0
+ Oin
compared to 1 For Mo radiation and an Al samplet the condi-
sinol
tion
+.
< 0. 1, (13)

4
holds up to a size of the mosaic blo&s of about 10 A. Thus, extinction
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Consideration of secondary extinction
3/057/61/031/003/018/019
B125/B209
does not change the ray intensity when the size of the blocks is about
10-4 A or lose. The size of the elementary layer, in the case of an Al
sample and Mo radiation is
dz L2 (A). This formula holds the more, the more mosaic blocks
71 Fna 14 0
are present in an elementary column. Allformulas of the present paper
were derived with regard to the secondary extinction in the primary
cell. More accurate formulas for the case examined here will be given in
a later paper. There are 1 figure and 1 Soviet-bloc reference.
ASSOCIATION: Petrozavodskiy gosudarstvennyy universitet
(Petrozavodsk State University)
SUBMITTED: April 4P 1960
Card 5/5

23735
S/'057/61/031/006/019/019
B116/B201
AUTHORSt Kuznetoov, A. V. an& Terminasov, Yu. S.
TITL.Es Consideration of secondary extinction. II.
PERIODICALi Zhurnal tekhnicheskoy fiziki, v. 31, no. 6, 1961, 757-759
TEXTs The formulas derived in the present paper take account of the effect
of secondary extinction in a polycrystal with mosaic blocks uniformly
distributed with respect to the angles of iotation taking multiple re-
flections into account. It is shown that existing formulas taking account
of secondary extinction are not applicable in the case of small crystallite
dimensions. The formulas derived in a previous paper by the authors
(Ref. 1t ZhTF, 30p no. 10, 1960) take account of the effect of secondary
extinction in the primary ray only (for a polycrystal with mosaic blocks
uniformly distributed with respect to the angles of rotation). With small
mosaic blocks, the integral reflection from a small, thick polycrystalline
plate (Ref. 1) is given by
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23735
S/057/61/031/006/019/019
Consideration of secondary... B116//B201
P PIQ
Bnr sin 41~ +sin a ) +
0 sin 2 T- pq coo %q
To take multiple reflections into account, it is sufficient to take account
of the attenuation of intensity due to extinction in the rays reflected
from the various elementary layers as they emerge from the specimen.
Further reflections will not play any role. According to the author's
estimates, their contribution is considerably below the accuracy of
existinp methods of measuring the intensities. On the basis of similar
considerations, the following formula is obtained for a polycrystal with
mosaic blocks uniformly distributed with respect to the angles of rotation:
P PlQ (2
I sin a) (4 1
8nr sin 0 sin pq coo
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23735
S/057/61/031/006/019/019
Consideration. of secondary... B116/B201
With an aluminum specimen exposed to Mo radiation the presence of a
secondary extinction reduceis the integral reflectlon of any interference
by 4%. It is pointed out that many papers (not specified here) make use
of formula P PQA(%%)
(3)
P + gQ
for taking secondary extinction in polycrystals into account. A (0) is
a factor depending on the geometrical conditions of the recording. In the
authors' opinion, the application of formula (3) to a polycrystal, regard-
less of whether the latter is compact or powdery, is in no way justified
with any crystallite dimensions. In fact, this formula is valid only if
in each column the mosaic blocks of a single crystallite reflect X-rays.
In other words, every ray is reflected only in the mosaic blocks of a
crystallite, with the mosaic blocks being so weakly disoriented that none
of them is reflected into any other ring (hkl). Under real conditions,
however, everything will be more complicated. The authors have examined
this problem more closely, namely, as applied to an aluminum specimen
exposed to Mo irradiation. They made the following assumptions for the
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23735
3/057/61/031/006/019/019
Consideration of secondary,.. B116/B201
polycrystal: It consists of crystallites of random orientation; each
crystallite consists of mosaic blocks which are not randomly oriented;
all normals to the reflecting planes of the mosaic blocks are concentrated
witin a small solid angle, and all mosaic blocks of the crystallite can be
reflected into a Debye ring only. It was shown in a previous 2paper o the
authors (Ref. 1) that in each column of a length dz/ain a -W 740 - i Wo
an aluminum specimen exposed to Mo radiation has, on the average, only a
single crystallite (as in the present case) in the reflection position.
The orystallits size is assumed'to be L 103 L The length of the
elementary column will then be 1.3*103 If the crystallites in the
column are assumed to disperse, in which case the column size is equal to
the half-aboorption thickness of the layer every ray will be reflected from
3.500 3 crystallites. Formula (3) cannot be used in this case; in faot,
if the crystallite is placed at some depth of the specimen, and not on
its surface, the X-rays reaching the oryotallite and those emerging from it
will be weakened due to crystallites reflected into entirely different
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23735
S/057/61/031/006/019/019
Consideration of secondary,to B116/B201
rings (hkl). In this case, formula (2) must be used in the crystallite
consists of one mosaic block only. If, however, it consists of some weakly
oriented Giosaic blocks, the second term in the denominator of (2) has to
be written as g.L T PQ cgs where the coeffJcient 1 takes account
2 1 1 4
of secondary extinction in the crystallites itself, Even if L - 10
the ray will be reflected in 30 crystallites, and formula (3) will there-
fore be inapplicable here, too. Only if L - 5.104 1, each ray will be
reflected in the specimen only once on the average. Formula (3) is
applicable only with such and larger crystallite dimensions. If, however,
the mosaic blocks of a crystallite are disoriented to a sufficient extent
so as to be reflected Into different rings, it is very doubtful even with
large crystallites whether formula (3) may be applied. When using another
radiation, the crystallite size beginning from which (3) may be used,
varies. The lesser the penetration depth of,X-rays, the smaller is the
crystallite size for which (3) may be used. A more accurate analysis must
bo performod by using (4). The interpratntion of effects of secondary
extinction is most difficult in cases Hiere each ray is reflee,~ted in soat
Card 5/6

Consideration of secondaryeas
23735
S/05 61/031/006/019/019
B116YB201
crystallites. Future calculations will show how things really are.
E Abstracter-s notes Essentially complete translation.] There is 1 Soviet-
bloc reference.
ASSOCIATION: Petrozavodskiy gosudaretvennyy universitet (Petrozavodsk
.State University)
SUBMITTEDt July 8, 1960
Card 616

S/070/62/007/001/013/022
E032/E3i4
AUTHOR: Kuzngtsov, A.V.
TITLE: The effect of secondary extinction in monocrystals
PERIODICAL: Kristallografiya, v. 7, no. 1, 1962, 121 - 123
TEXT: The author makes use of a discussion given in an
earlier paper (Ref. 1 - Zh. tekhn. fiz,, 31, 3, 1961) to derive
formulae which take into account the effect of secondary
extinction in the reflection of X-rays from the face of a
mosaic monocrystal. The monocrystal Is divided into elementary
layers, in each of which the secondary extinction effect is
zero. On the first approximation the thickness of such a layer
can be assumed to beequal to the average size of a mosaic block.
To begin with, an expression is derived for the energy scattered
by the first such layer when all the mosaic blocks within it
are parallel to the face of the crystal but are slightly dis-
placed relative to each other. Each of them then scatters
independently of its ntighbours and the energy scattered by the
entire layer is n times the energy scattered by a single
Card 1/2

S/070/62/007/001/013/022
The effect of .... 'E032/E314
mosaic block. Multiple reflections are neglected. The final
expression gives the total reflected intensity.
There are 2 Soviet-bloc references.
ASSOCIATION- Petrozavodskiy gosudarstvennyy universitet
(Petrozavod State University)
SUBMITTED: July 8, 1960
Card 2/2

KUZNETSOV, A,V,
Line displacement as dependent on the final dimensions of mosaic
blocks. Trudy LIM no.29sl25-129 [i.e. 391 162. (MIRA l6z6)
(X-ray crystallography)

NUZNETSOVP A,,V.
Theory of I-ra scattering by mosaic aryotals. Trudy LIEI
no,293137-145 ri.e. 391 162. (KMA l6s6)
(X-ray er7at-allography)

K,uzw4T4Qv-#-AaY.-;. SH
t IVRIN, O.N.
Mutual interference on X rays reflected by different mosaic
blocks ih a crystallite, K;istallografiia 7 no,1:134-136 Ja-F
162. (MIRA 15;2)
1. Petrozavodakiy gosudarstvennyy universitet.
(X-ray crystallography)

KUZNETSOV, A.V.
Applicability of correction formul4 for the calculation of
secondary extinction, Fis. met. i metalloved. 13 no.21
306-308 F 162. (NIRA 15:3)
1. Petrosavodskiy gosudaretvennyy universitet.
(X-ray crystallography)
13"

S/070/63/008/001/015/024
E132/E46o
AUTHOR: Kuznotsov, A.V.
TITLE: The broadening or X-ray lines due to secondary
extinction
PERIODICAL: Kristallografiya, v.8, no.1, 1963, 102-104
TUXT: Whon the di?tribution of blocks in a mosaic cryst~JL in
given by
~2 A-I
+ jT 2
(y) (21Tp2)
then the relationship between the line widths Pe and Pt with
and without secondary extinction are given by
2 2
Pe Pt [1 + (2TTY
where 1L is the coefficient of linear absorption, Q tho
integrated intensity of the reflection from unit volume,
(p is an angle and is the deviation from the Bragg angles
Card 1/2

5/07o/63/008/001/013/024
The broadening of X-rmy F,132/E46o
There are 2 figures.
ASSOCIATION: Petrozavodski.y gomudaretvennyy universitet
(Petrozavodak State University)
SUBMITTED: June 27, 1962
Card 2/2

KMNETSOVP A.V.
Measuring secondary ext4netkcm in po3ycryotala. Fix. met. I
metalloved. 15 no.213g&,-305 F 163. (MIRA 1624)
1. Petrosavodskiy goeudaretvennyy universitet.
(Metal arystals-Optical properties)

KUZNEETSOV, A.V.; F1LATOV, M.S.
Application of au=ary corrections of counting errors. Zav.lab.
30 no.3:300-301 164. (MIRA 17s4)
1. Patrozavodskiy gosudarstvennyy univernitat,

E-UZIMTSOV, A. V.
"Some Problems of Interru ted Flow." Cand Phys-Math Sci, Kazan' State U,
Kazan' 1954. (RZWIekh, Nov 54~
Survey of Scientific and Technical Mssortations Defonded at USM Higher
Educational Institutions (11)
SO: --=. 110. 521, 2 Jun 55

SOV/1 24-57-7-7621
Translation from: Referativnyy zhurnal. Mekhanika, 1957, Nr 7, p 22 (USSR)
AUTHOR: Kuznetsov, A. V.
TITLE: Concerning the Pressure Exerted by a Flowing Gas on Several Obsta-
cles With Flow Separation (0 davlenii gazovogo potoka na nekotoryye
prepyatstviya pri obtekanii s otryvom struy)
PERIODICAL: Uch. zap. Kazanskogo un-ta, 1956, Vol 116, Nr 1, pp 45-49
ABSTRACT: The author examines the plane problem of the steady separated
flow of an ideal compressible fluid (as defined by Kirchhoff) past a
plurality of obstacles consisting of straight-line segments. The paper
is based on ChaPlY8in's approximate equations. The problem is solved
by representing on the upper serniplane the regions 'of variation of the
complex potential and of the function w = a- + i 0(Lr being the Chap-
lygin variable and 0 the angle of inclination of the velocity vector with
respect to the axis of symmetry of the contour).
B. S. Kirnasov
Card 1/1

KMN-PTSOV, A.V.
Flow around a curvilinear are with separation of flow. Uch. zap.
KRz. un. 117 no.9:95-99 '57. (MIRA 13:1)
l.Kazanski7 gosudarstvennyy universitat im V.I. U117anova-Lenina.
Kafedra gidromekhaniki.
(Gas flow)

14
16(1),16(2),10(4)
AUTHOR: Xuznetsov#A.V. SOV/140-59-3-15/22
TITLEi ow Around With Separation of Rays of an Impediment Enclosed
in a Channel With Parallel Walls
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy. Matematika, 1959, Nr 3,
PP 159-167 (USSR)
ABSTRACT: The author considers the symmetrically plane flow around of a
curvilinear arc by an incompressible fluid. The arc lies between
two parallel walls and is symmetrical to the axis of the channel.
The curvature of the arc is a oontinuoua function; the are is
star-shaped with respect to a point of the axis. The existence
and uni eness of the solution are already proved by Serrin
fRef 4j. The author uses the method of Ya.Berman ZRef.12 t)
mapping of the lower part of the flow into the first u dran
and determines the form of the rays as well as the corresponding
potential flow. The author mentions M.A.Lavrentlyev.
There are 2 figures and 4 references, 3 of which are Soviet,
and I English.
ASSOCIATIONtKazanskiy gosudarstvennyy universitet imeni V.I.Ullyanova-Lenina
(Kazan, State University imeni V.I.Ullyanov-Lenin)
SUBMITTED: April 19, 1958
Card 1/1

B/140/61/000/004/004/013
CIII/C222
AVTAds i6ine'tibv', 'k, To
TITLEs Cavitation flow aroundja platId'iri 'the- ~ne!Vdhborhoo d 'of
the free surface of a :-MU!Ld e4 no w6i'~ht
PERIODICALs Izveatiya vysahikh uchebnykh'zavedihIY4.. Matematika,
no- 4, 1961o 39-50
TEXTj Under the assumption that the cavitation numbei zoe ii small
the author considers the cavitation flow around an infiryk-te ~ibhe
with the width 1 by a fluid of no weight in the neighborhood,4 ~Wb
free surface according to the scheme due to D. A. Efros (Ref. Is
Gidrodinamicheskaya teoriya plosko-parallellnogo kavitatsionnogo
techeniya [Hydrodynamic theory of a plane parallel cavitation flow]
DAN SSSRp v. 1, no- 4, 1946). The scheme is shown by figure 1
Card I"

Cavitation flow around a plate in ...
F;j VI

KI 0 M D C 9
0 in a at
Ic

K' OM'D' V
A B is the free surface, F--critical point, C--ramification point on
the plate, Ox 11 V.. The jet flowing into the cavern is directed
OD
exactly contrary to V06 J is the angle of inclination of the plate
with respect to V. .
For a given 1, of # H00 , ?e an d V00 the author seeks the form of the
Card 2/7
S/14o/61/000/004/004/013
CII1/C222

8/140/61/000/004/004/013
Cavitation flow around a plate in . . . 0111/0222
free surface and the cavern, the velocity field,-the buoyancy and
-esietance. The plane out along k is mapped onto the right angle of
figure 2 of the u-plane, and the Romplex potential w -,f + i4l and
the function X - 1n -I- dw are investigated. The solution of the
V dz
00
problem leads to the determination of Lw -f (u) and X(u)-f
du 1
With the aid of the elliptic functions G'(u), J(u) and - 2S
dw is represented by 13
TU dw - As - 13(OL _m) 6(u- 0c - to 2) G'(u_ 6' (u-
ru - T (u-m- to 2) 62 (u-2 ca,)
where A--real constant. For (u) the author obtains the representation
Card 3/7

S/140J61/000/004/004/013
Cavitation flow around a plate in 0111/0222
x (a) f InL'-g(aVt)d1-1f It--w-1fy)Jg+(u,t)dt-
0, va
a+m,
8+4% 20, *4%
la
_.i f A If (t)] V) d t11 ic jf(Ojg dj]+
FIn In c1W. (7)
where f(u) is defined by
241
Au) In. in 01F (4)
Card 4/1

S/140/61/000/004/004/013
Cavitation flow around a plate in . . . CI11/C222
and g(u, t) is defined by
g(u, t) = e I., (u- t) 6'(t-u+cl 6 3(t-b)6~(u-a) (5)
Lr7c) 6' (t-u) (r3(t-a) C (u-b)
3
71, ~2g(q), c=W1 + b 2a
The author establishes additional equations for the determination of
co
the constants A, 9 oL , a, bIM, Pil A2 , 2 of which can be pre-
scribed if the si u tion of K on the P ate is not fixed:
0) General condition
01+ 2P1 - M + 401 (2)
1) Direction of the velocity in the jet flowing into the cavern
Im (M+ (02) Or
Card 51~

Cavitation flow around a plate in . . .
2) Direction of the velocity in cD 3
Im ),(0) 0 .
3) Boundedness of X (u) in u b+ CO 2*
4) Width of the plate
~&414a
1
S/140J61/000/004/004/013
0111/C222
(10')
e- 1 (u) dw + e- X (u) dw
VI Im
00
c0, a+
2
Width H00 1
I sin S (14)
1
V Im Cm (2 W I w (of, + W2) Hoo .
a)
(15)
Card 6/7

S/140/61/000/004/004/013
Cavitation flow around a plate in . . . 0111/0222
Then the author determines the pressure R with which the flow acts on
the plate.
There are 3 figures and 4 Soviet-bloc references.
ASSOCIATIONt Kazanskiy gosudarstvennyy universitet im. V. J. Ullyanova-
Lenina (Kazan, State University im. V. J. Ullyanov-Lenin)
SUBMITTEDs December 6, 1959
Card 7/7

S/179/62/000/001/026/027
E191/E1135
AUTHOR: Kuznetsov, A.V. (Kazan')
TITLE: Flow of a 3et of finite width around a plate in the
presence of cavitation
PERIODICAL: Akademiya nauk SSSR. Izvestiya. Otdoleniye
tekhnichoskilch nauk. Mokhanika i mashinostroyenlye.
no.1, 1962, 174-177
TEXT: Cavitation flow of a jet of incompressible fluid of
finite width is considered wherein the plate is placed symmetrically
and at right angles in relation to the jot. The Cavitation Number
(defined as the square of the ratio of the velocity at the boundary
of the cavi4, to the velocity at InfinIty, less unity) is assumed
small. A stationary pattern of cavitation is assumed. The
complex potential in the plane of the flow is introduced and a
special function defined which is the natural logarithm of the
derivative of tho complex potential with respect to tho complex
position divided by the velocity at infinity. When this function
is found, the shape of the jet boundaries and of the cavity can be
plotted and the pressure of the flow on the plate can be computed.
Card 1/2

S/179/62/000/001/026/027
Flow of a jet of finite width ... E191/E435
The kinematic part of the problem is solved by conformal mapping.
In the physical plane, a semi-infinite cut is taken along the
streamline passing through the stagnation point (in the centre of
the plate). This streamline is taken as the zero streamline.
The singly connected region so obtained in the physical plane is
conformally mapped on the inside of a rectangle in an auxiliary
plane. In the analysis, reference is made to the pattern of
cavitation flow examinod*by'D.A.Efros (Ref.l: DAN SSSR, V-51, no.4,
1946) and the mathematical derivations of L.Woods (Ref.2:
Symposium of translations "Mekhanika", no.2, 1956) and thus the
present author's derivations are purely mathematical.
Instructions are given for determining the jet boundaries and the
shape of the cavity. The pressure on the plate is derived and it
is stated that the formula so obtained is valid also for curved
profiles.
ASSOCIATION: Kazanskiy gosudarstvennyy universitet
(Kazan' State University)
SUBM'ITTED: June 26, 1961
Card 2/2

KUZNETSOV, A.V. (Kazan')
Flow of a weightless fluid with a free boundary. PMTF
no. 604-99 N-D 163. (MIRA 17:7)

I,IJZNETSOVP A.V.
Oil reaerves in carbonate raservcir rocks. Trudy VNIH no.310-:
179-187 163. (mIRA 17;9)

n
Problem involving flow post a system performing minor vibra-
tions. Prikl. mat. i makh. 28 no.3067-M try,4064
(MIRA 17t7)

KUZMrZSOV, A.T.
Phyalcogeographical conditions of the Pashiya layer formations In
the southeastern Tatar A.S.S.E. Trudy 1311 no.11:15-25 157.
(Tatar A.S.S.R.-Potroleux geology) (KM 10111)
V1111 - All-Union Scientific Research Institute of Petroleun and Natural
Casio Poscow

T'' "..V.
0
--, lr'~~.,,,~~-.~"-_-- , .
-volr proparll~n of et Itatnnes from tho -,~-)ducin,-- ~-r' ir I n
Rrico7 4
t1m I!clo. Trucy YNJI n.i.ll;:hr--54 '57. (ri%-, 1".7)
MonL-.'-Llf,~Ino ra.,~71nn--Potrolonm, poolof-j)

A v
KENES9k~
Certain forms of arenaceous formations in the horizon DI of the
Romashkino field. Trudy VNII no.23:93-100 160. (MIRA 13:11)
(Romashkino region--Sanastone)

KMIMOVO A.V.
Systematio errors in calculatizg the size of o:Ll and gas pools
from isopaoh maps. Trudy VNII nn.As75-85 162. (WA 15 V )
(Petroleum geology--!'Apo)

GERASIMOVAj Ye.T.; KUZNETSOV$ A.V,; IATYPOV, N,G.
Lithological and mineralogical characterization of argiLlaceous rocks
of a Lower Carboniferous terrigenous layer of the eastern Russian
Platform., Dokle AN SSSR 151 no.2419-421 J1 163. (KIRA 16:7)
1. Geologichaskiy institut, Kazanskogo fWals. AN SSSR. Predstavleno
akademikom N,M.Strakhovym,
(Rusaian Platform-Clay)

KUZNETSOV, A.V.
Electric rock drill. Gor. zhur. no.8:61-62 Ag '58. (MIR& 11:9)
(Rock drills--Patents)

AUTHOR: Solomonov, M.S. SOII/180.59-1-28/29
TITLE: Conference on the Physics of the Disruption of Rock and
Tool Wear (Soveshchaniye po fizike razrusheniya gornykh
porod i iznosu instrumentov)
PERIODICAL: Izvestiya Akademil nauk SSSRI Otdeleniye tekhnicheskikh
nauk, Metallurgiya i topli-bo, 19,1~9?Nr 1,pp 123-124 (USSR)
ABSTRACT: On 18-20 November 1958 a conference was held at the
Institut gornogo dela AN SSSR (Mining Institute AS USSR).
One group on the physics of rock breakdoung heard the
following reports: A.N. Zelenin, (--rGD AN SSSA), on "Some
Investigations in the Field of Mohr's Ring Construction";
A.I. Beron, VUGI, on "Physical Nature of-Effects in the
Cutting of Brittle Rocks"; R.Ye. Zygeles, VNIIBT, on
"Mechanism of Rock Breakdown in Statio and Dynamic
Insertion of Punches"; V.P. Samoylovq NIIOSP7 and Shih
Chung--han- (MIIT) on "Experimental Investigation with the
Aid of Radioactive Isotopes of the Process of the
Introduction of Symmetrical Wedges (Stamps) into Rocks";
V.M. Matrosov~ Tomskiy politakhnicheskiy institut (Tomsk
Card 1/3 Polytechnieal Institute), on "The Breakdown of Rock in
Vibration-Rotation Dzilling by the Core Method".

SOV/180-59-1-28/29
Conference on the Physi6s of the Disruption of Rock and Tool Wear
The second group, dealing with tool durability, heard
the following reports: 416netsov (IUD AN USSR) on
Ku
"Abrasive Properties of Hoc s and Their Influence on
Drill-Edge Bluntins (in Perforation Drilling)";
M.I. Smorodinovq NIIOSPq on "Investigation of Rock-Cutting
Tool Wear with the Aid of Radioactive Isotopes";
V.V. Sevastlyanov, VUGI, on "Investigation of Tool
Durability in the Course of Impact Chipping of Rocksllj
I.A. Ter-Azarlyevq AISM, on "Main Stages in Cutting-Tool
Wear in Stone Cutting"; K.S. Vartanyan, AISM, on "Local
Tool-Wear in Stone Cutting arad Friction Work"; G.G.Karyuk,
Novocherkasskiy politekhnicheskiy institut (Novocherkassk
Polytechnical Instituta) on "Iwrestigation of ShBM-Combine
Cutting-Tool Wear"; V.F. Kiriyerko, Opytno-issledovatell -
skiy tsekh Norillskogo kombinata (Experimental-research
department of the Norillskiy coLabine) on "Increasing the
Durability of the Drilling Tool and the Drillability of
the Gabbrodiabases of the Norillsk., D6posits";
B.N. Lyubimov on the "Work of Giprouglemash"..
Afterwards comwaai-.ations wera presented by-representati-
Card 2/3 ves of tha Dnepropetrovskiy go:cnyy institut (Dnepropetrovsk
Mining Institute), Novooherkasskiy politakh-nicheskiy

-59-1-28/29
Conference on the Physics of the Disruption of Rock and Tool Wear
institut (Novochorkassk Polytechnical Institute),
Khartkovskiy gornyy in-stit-u-b (Kharlkov Hinin Institute),
Kazakhskiy gorno-metallurglchesk17 institut fKazakh
Mining and Metallurgical Institute) and others. The
conferen-.9 noted that littae work had been done on some
of the subjeots discusseA. It recommended that work on
the physics of rook disruption should be ~:arried out
mainly at the ICD AN USSR~ the Institut geologii i dobyehi
Polezwykh iskopayemykh AN SSSR (Institute of Geology and
of MA.nerals,AS USSR) T1UGI arA VNIBT;
and work on tool -dear and breakage preferentially at NPI,
AISM, Gidrouglemash., 71UGI. VNII5T and the Institut tverdykh
Card 3/3 splavov (Hard.-Alloyi lnstitat-~).

KUL -T, AeV,
ftperimental study of the effect of abrasive properties of rocks on
the dulling of bits in hammer drilling. Izv.1rar. i XD11.fil. AN SSSR
no.2:116-121 159. (KIRA 12:11)
1. Institut gornogo dela Alf SSSR.
Rock drills)

IOZESTSOV, A.T.; GIA-D", L.D.
Measuring the wear of cutters of sinking machines. Ism.
tekb. no.4:12 Ap '6o. (UL" 13:8)
(Xining machinery)
(Mechanical wear-Measurement)

BARON, Iesarl Israllevich, prof.$ doktor tekhn. nauk;
.Aleksandr Tasillysyl U-MMAY, L.M., red. isd-ve; ASTAY
G.A., tekbu. red#
(Abrasiveness of rooks in mining opeiotional Abrasivnost'
gornykh porod pri Aobyvanil. Hoskya, lzd-vo Akad. nauk
SSSR, 1961. 166 p. (MIRA 14:5)
1. Institut gorn*ogo dela Im. A.A.Skochiniskago Akodamii nauk
SSSR. Lyubertsy, Moskovskoy oblosti (for Baron. lusnateov)
(Mining engineering) (Rocks--Testing)

SIDOROV, I.N., inzh; KUZNETSOV, A.V., inzb..-,
Boring with a sinker dril.1 without axial force applied on the bit.
Clor. thur. no* 6:72 Je 1619 (MIRA 14:6)
1. Gorno-geologichesk Institut Urallskogo M."ala AN SSSR.
IlRock drUln)

BARON, L*I.y doktor ; GLNTMA.N-, - L. B. - --- - - -- ;
, gornyy inzh-,--_KUZNETSOV
A#V*j gornyy in*,
Determining the abrasive properties of rocks mined with cutters.
Ugoll Ukr. 5 no-4122-23 Ap 161. (MIRA .14":4)
1. Institut gornogo dela AN SSSR.
.(Abrasion) (Coal mining machinery-TeBting)

p 4-r.Vasillyevich;
DO-110CHKOP Ivan Ivanovich,- KUZZ,'ETLOVj Alo%-u
D'YAKCVA, G.B., re-d-.Tz-Z--v~; 6~~RKVA, Z.A., tekhn. red.;
LOMILINA, L.N.# takhn. red.
[BS-4 scraper hoists for filling materials) Butovye skreper-
nye lebedki BS-4. Moskva, Goagortekhizdat, 1962. 55 *Pi
(KIRA 15#5
(Hoisting machinery) (Mine fining)

RODIONOV, N.S., kand.takhn.nauk; KUZNETSOV, A.V., inzh.
Now design of a ppoh for estipating the hardness of rocks and
minerals. Nauchtisoob. IOD l7sl29-130 162. (MIRk 16s7)
I
(Roc 9--Testing) (4nerals-ke sting)

SIDOROV, I.N.; KUZtIETSOV_,_A,.V
Waing the efficioney of boring and blasting during mining in
hard rock. Trudy 1nst.gor.dela UFAN SSSR no,,7:125-129 163,
(MIRA 17:3)

KUZNETSOV, A.V., Inzh.
- ~.,- -
Comparative evaluation of the abrasive properties of some petro-
graphic rock groups. Nauch. soob. IGD 21:125-132 163. (KIRA 1712)

I K-UMETSOV, A.V,.-,, (Kommunarek, Luganakaya oblust' ), Yf,tzti?r")Vk , D.3.
(Kommunarsk, Lugunskaya oblast')
Nomographing two problems In mining engineuring. Nom abor.
no.2v54-59 164. iMIRA 180)

KUZNUSOV,__LV. (Kommunarsk, Luganskaya oblast')
Nomographing the construction of central axonometric -4aotimnq.
Nom. abor. no.2:60-70 164, .,." .
Nomographirg the construction of parallel standardized axonometric
projections. Ibid.:71-77 (MIRA 18:3)

ITINSKAYA, N.I'# kand.takhn.vauk, dotsenty DEGTEW, M.D.,, kand.tekhn.nauk,
assistentl KUZNETSOV,p.-,LV-..-aopLrant; TRETIYAKOV., B.S., assistant
Effect of the prolonged use of crankcase oil on the performance,of
DT-54 tractors. Trudy MIHESKH 6:351-364 159. (MIRA 14:5)
(Tractoro--Lubrication)

ITINSKAYA, II.I., kand.tekhn.nauk, do'-sent; DZISTSM ~-V.,
otarshly prepodavatel, u
Properties of aiesel oils in the operation of tractor
ongines. Izv. TSKIIA no.2:.U5-130 162. (KM 15:9)
(Tractora-Lubrication)

L 08463-67 JUP(m)/EWT(l) WV1
ODE: un/61-2-VN576-6
AUTHOR
TITLE: Flow of a weightless fluid with a free boundary.around a plate
SOURCE: Ref. zh. Mekhanika,; Abs. 12B612
REF SOURCE: Tr. Seminars, po obratn. krayev. zadacham. Kazansk. Ti--t, VYP 2, 1964,
84-87
1
ITOPIC TAGS: fluid flow, flat plate, streamline flow
ABSTRACT: A previously derived general solution (Kuznetsov,'A. V., Zh. Prikl. mekhan.
i tekhn. fiz., 1963, No. 6, 94-99-Rzbmekh, 1964, 4B378) is used as a basis for
numerical solutions on the "Ural-I" computer on determining the lift factor 0 of a
Y
plate of length Z moving under the free surface of a weightless fluid with velocity
VC.. In expressions for
in I dw- dz r,'H,
-P; W. 7v-, ,
where r is circulation, H is depth of immersion,.Y is lift v-v~+Ivg (0evj-c2,K; 0-4vg