SCIENTIFIC ABSTRACT ZHUKOVSKIY, V.B. - ZHUKOVSKIY, V.S.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R002065010015-1
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: July 16, 2001
• Sequence Number: 15
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

HIP 4"
ACC NR: AP7003222 SOURCE CODE: UiV66-~-t)7667ii5:Vo-66;rl;52~1183;r
I AUTHOR: Sokolov; A. A.; nukove!& V. Ch.; Korovin,# Yu. A.;
ORG: Moscow State University (moskovskiy gosudarstVennyy. universitet)
TITLE: Stimulated transitions in the radiation from a relativiatlc~electronln an
inhomogeneous magnetic field
SOURCE: Zh ek6per i teor fiz v. 51; no. 6, 1966~ 1829-1832
TOPIC TAGS: relativistic electron electron radiation, ptithulated emission axial
C-L ?C rqOV 7WdA1J1r,1f.W
magnetic field, maser theory,
ABSTRACT: The authors consider stimulated transitions of relativistic electionsi
moving in a constant but inhomogeneous magnetic field. In particle tltir., the r6diation
from an electron placed in,an axially symmetrical focusing magnetic field is~Jnyeisti-
gated. The probability of the stimulated remission is obtained for an externa elec-
tromagnetic wave which is linearly polarized and which propa:aates at a certain angle
to the magnetic field direction. From this probabi ty, the*authora determine the
power radiated by the electron in the case of ~t trAnbitibna.1nduced by.thp
external electromagnetic field at various harmonicsp and thei pcfwdr'of the dipole';
radiation. The region of variation of the harmonics., at which the stimulated emis-
sion should prevail over absorption, and is thus of,interest. in maser applications,
is determined. Two conditions for emission are formulated1n th4 form of ineqpali-
ties relating the different parameters of the problem. Origs arts has: 16 ro=04AS.
SUB CODE: 20/ SUBM DATE: 15aui66/ Ono Rul: 001/ oTE .9a: 001

_.L 29671-66... EWT(1)/ETC(f)-----1JP(c-) ---,.AT
fACC NR*.- AT6012691
SOME CODE: UR131361651or-OlWI000 00221.
AUTHOR: Bo AbLikov A., V.; Brevnov' No N V
Zhukovskiyy Go po R10TWAirkwisft M. Ift
ORG: SJ
qu Uog og At MMI,
e -COMMWge omig Dner" MCA* of Atomic Energy I
im. I, Vs Kurchatov, Moscow (GosudarstvalhW komitatpo, ispolIzavalyu atomoy
energiip Institut atomnoy energii)
'AS" installation
TITIZ: Investigation of plasma in the
wma: Moscow. T=titut atomnoy energii. Dok1&()y#, noo' 988, 3~65., Issiedova-
in1ye p3.aznW v ustanovke AS, 1-22
TOPIC TAGS. plasma research, p*lasma compression, plasms, #jectioln.. plasnold ac:
celeration, plasma stability, cyclotron reso
nancep. magneti,6 mirror
ABSTRACT: The authors describe the "AS" (adiabAie c2Meqaion):: Weirratus: for the I
study of a plasma produced by injection of fast ions,, An axially-centered cylin-
drical plasmoid is detached from the injector by means of
,pulsed magnetic
is accelerated toward a stationary magnetic mirror$ aiA is'~iccqpreaved by &'t
increasing magnetic field of mirror configuration. The ihiti&L Ion energy can
reach 30 kev. The article contains a descriptioi, of the insUllation (Fig4 ~1)
the awd1lary apparatus., and the measurements details*, Measurements were made of
the density and potential of the plasma.. the, 31fetimes of the fest ionsp ar4 the
Cwd 2/3

L 29671-66
ACC BR: A76o:L2691
Fig. 1. Schematic diagram of "AS installation.-:I - Magnetic leFx,,2 - ch4nnel~
azotite, 4 : titanium evaporators) 5 - chmb'er) 6 7,8,io,11 '": iltationary' mag-
3 1
hetic field coils, 9 - copper screen) 12 - detachment coil)', 13pt - cemprCasion:
coils$ 15 - neutral particle detector) 16 - secondary ion energyn
pectrum rialyz ens'
IT - current receiver.. 18 - rod probe) 19 - palladium leakNalve,
onset and development of oscillations at the ion-cyclotron1requen al
cy, Theiniti i
plasma density was found to be proportional to the injection curireht and amounted
to 1016 cirl fast ions at a current of 5 ma. In the absence of Injection- ourrent
pulsations, the plasma potential did not exceed +30-40 Y and vae, independent of
the injection current or of the neutral-gas pressure* Cyclotron inatabilit~ with
an increment time of 20-30 psec developed in the plasma after detachment from the
sourse, lasted for about 100 psecp after which it decreased exponentially,,4ippar- !
ently as a result of self-stabilization. The lifetime of the fast ions depended
only on the charge exchange with the neutron molecules. The development of pyclo-1
tron instability did not cause additional ion losses. The plasma decayed after
compression with a characteristic time of 500 psec. This is several times smaller-,-e.,P~
a beha~vior is!not yet,clear. I
..than the charge exchange timej and the reason for thi
The experimental plasma lifetime of the fast ions increased an?ribodmately in prc~-
portion to the pressure* Orig. art. bas: U figures and 8 foivulao,,
SU3 CQDE 2D/ SUBM11ATE: 00/ 01IMBU: 0051 OTH REF%~~ 005
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(/0 Y31 IIYS-1115 3) ~S/040 6qtq2~/01010271033
B01 3XBO61
AUTHORS: Andreyeval N. A.p Grushevskaya, 0. and
Zhuk2vi3kiyt V. I.-
TITLE:. Some Considerations on the Methods bf Producing Materials
With a Smooth Temperature:Dependehob of the Dielec'tricl~
Constant
1A
PERIODICAL: Izvestiya Akademii nauk SSSR. Seriyk filti0heskayat ~1 960 9
Vol.. 24, No. 10, pp. 1285 - 1288
TEXT: In order to obtain a smooth temperature dependehoe of the ,dielec-
tric constant, the authors looked for an efficient admix'ture totaT102-
For this purpose, they chose bismuth. titanium, and irsirconium oxideaiin
different ratios and combinations. The system BaTiO -131 Ti 0 was given
. ~ 3 : 4 3 12
special attention. Fig.1 shows the temperature dependence of theAielec-
tric constants of various samples. It may be seen thiLt; they bec6mie fair-
ly smooth by the addition of BaTiO -Bi Ti 0 The maximum (curie po3-Lnt)
3. 4 3 12*
characteristic of barium titanate, is, however, not affected. Phenomena
Card 1/3

Some Considerations,on the Methods of S/04,8 60/024/0'10/027 3
roducing Materials With..a Smooth 3 2
P
Temperature.Dependence of the Dielectric Constant~
of the same quali,tative:character may be also found in':iamplea of the
system BaTiO -Bi 0 -ZrO (Fig.2). Fig.3 illustrates th.e temperatu re and.
3 2 3 2
frequency dependences of E and tan 6,for one sample of the system
BaTiO -Bi Ti 0 a illustration indicates Thai pres4nee of relaxation
12* Thi
3 4 3
properties. An X-ray analysis performed by V. 0. Prolchvatilov and
Ye. I.,Gindin has shown that various compositions of the systems
BaTiO -Bi 0 _TiO and BaTiO Bi 0 ZrO P besides :,a phaGe having the
3 2 3 2 3- 2 3-. 2
structure.of barium titanate with changed lattice pa-rameters (not per-
fectly cubic), exhibit another phase .which might be held responsible.
for the relaxation properties ofthe. material..Solid solutional,which
can be formed presumably only in a very small range of'cioncentra4tiong'
were not detected in the systems examined. The authors$ studies 14ad'to
the conclusion that the materials of the two systems under consideration
contain a piezoelectric and a relaxation phase. The vom~osition of the
latter has not yet been determined so far. The dielectric constants of
several samples showed two maxima. It is assumed that the low-temperature
Card 2/3

-1,1,7~600(loq31114'O 107S-) 8/040/60/024/010/030/033
B0131DO63:
AUTHORS; Zhukovskiy,-V. 1,, Dorokhova, 1. P.`1 Uromba, N . Ye't 0
Dykman, D. G., Boye, G. V .
TITLE: Data of a Thermographic Study of Bariuta Ti.tanad~ , h
Certain Admixtures
PERIODICAL: Izvestiya Akademii:nauk SSSR. Seriia f1micheskaya, 19609
Vol. 24, No. 10, Pp. 1,294 1295
TEXT: The authors examined the effect of commonly ulled admixtures upon
the sintering procese.of barium titanate.- These a4mixtures includie U02,
Bi 203 . Ti 02' CaC 03' MgC.03' BaC ~03 ~ et,c. For this ~purpose,, they made use
of a complex thermal analyais which4as cond,ucted.Ton an apparatus;of~
the type YKTA-58 (UKTA-58)0.3 Barium ~itanate was :synthenized:at 1$00d.
The samples were produced by the conventional ceramic proo see. Thie ther-
mogram of barium titanate is shown in.Pig.l. The firot.exothermicleffect
appears at 3000C and is related to the burning out of the plasticizer;
the second effect occurs at 13000C and is due to the tormination 'of the
Card 1/3

Data of a Thermographic Study of Barium S/048M/0201 01010301~33
Titanate With,Certain Admixtures B013/Bo63
production process of barium titanate. The endothelrmic~effect oba'ervable
at 8700C may be explained by the conversion of BaCO contained in the
3
material used. on the addition of TO and ZrO two other thermal ef-
2 2P
0
fects are visible in the temperature range 1250+~~.I 2!)Ol C - an endo.thermic
effect on heating and an exothermic effect on cooling (Pig.2). This is
presumably due to the formation of an eutectic BaTIO, 'Melt withitita-
3
nates of higher acidity andtheir, subsequent crystallization. An X-ray
analysisoperformed by Ye. I.-Gindin, of the systemiBdTiO'-ZrO indicated
3, 2
the existence of a solid solution. with a per 'ovskite latti-ceo This: fact
is indicative of an excessive.amount of titanate dioxide.. The above-
mentioned thermal effects are probably relatedto,~tha presence OfIthe
latter. However, the data available do not indicate the compounds that
form an eutectic melt. The authors established thiLt a liquid phase
exists when sintering a material on the basis of. barium titanate i9ith
the addition of Tto and ZrO 2# in the presence of,MgM CaCO 3aCO
~2 3' 3
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~kCc NRo AiMO30730 SOURCE CODES M/00-5V66/000/0O4/Oi17/0128
AUTHOR.: Kalinin, q., V., 21~91qk
ORGt -Dop'artment'of lbeoretioal and Applied Mechanics NI3M (Otdol teoretichdikoy~i
prikladnoy makhaniA NIJM)
TITISs Conditional stability of motion of an object -trith an automatic control Ovice
in some critic'al'aas4s
SOURCEi Moscow* Universiteto Vestnike" Seriya fiziki i. kh'imlit' nos 4, 1966s, 117-128
TOPIC TAGSs servomotor, motion stability, aircraft stability
ABSTRACTt 'The system of equations forthe motion of an objoot (Aircraft) viih 1
automatic control is given by
T + IVIT + kly
~+A=,py,n "M
+
a
Zia first equation in that of the object the motion of uhichAs to;bo regulated;!the
second is the equation of the servomotor& Here is the deviation from the,state
Card 1/2
I UDCs .531 6391 a 5

ACC NRj
AP6030730
prescribed for the system, angle ofthe rudder rotation. is the argument'of
the rudder regulation, F(t,J) ) in the characteristics of the seiromotor which
determines the rate of readjustment.of steering. The authors cotoider the odso, vhen
F(t, is not linear. A linear approximation rosults in a characteristio:oquationo
of which the following cases are consider6dt 0 one zero root, 2) one zero~and two
imaginary roots, 3) two zero roots, 4) three zero roots* A casD ;Ojr a small:lviaas 'of
the servomechanism Is also considered. The general conclusion .1s: that in oiddr to
have a stable motion, the nonlinear characteristics of the:servomotor can bo given not
only by an equation of an odd order, but also,,under certain conditIA)ns, by.an
equation of en order* Origo,art, bass 23 equationse
N
OjZ
SUB C 13 UBK DATBS MAY651. QIM REFs 014
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MONO

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O-AR6017333
;-NMOURCE CODE.; UR/0044/66/000/00:L /B046/BO46 ~~a
~d
AUTHOR: Zhukovskiy,-,
IhTLE: Some instailbility conditions sufIficient for a trivial'[ solution of a sy;siem:of
two linear differential ~equations
SOURCE: Ref. zh. Matmatika,- Abs. lB205
REF SOURCE: Uch. zap. Orekhovo-Zuyevsk. ped. in-t, v. 22, no. 3, 1964, 36-34
TOPIC TAGS: linear equation, differential equation,-:kuW=Ut"-g1 "9=2"
ABISTRACT~ Results obtained in the paper are based on a modification of N.G.
Chetayevl s~-ilstabllity theorem The proof of sufficient conditions of instab
~lity has
been demonstrated by means of linear forms. V. Toloknov. [Translation of
abstract) (KP]
SUB.CODE: 12/
.L-Card 1/1 11b UDC; 517. 917

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- -------- -----
I IJPW
L 43131t-66 ENT I
;*#t~'~~P6014168 ~-70N-TKA-f~.Tld-O-ViM
SOURCE com:
AUTHOR: Zhukovskly, V. 1.
ORG: All-UnIon Correspondence DwtItute of Textile and Light MftAusPL0!L(Vsesoyuzn)T
zaoehnyy ~wmut ~teks ~Inoy I blennosti)
promys
TITLE-. Instability and conditional stability in th6 critical case of n verb roots
SOURCE: DiffereittaWthyyouravnenlya, v* 1,, no, 12, 1965, 1601-1605.
TOPIC TAGS: differential equation system,,'differential eqt3atlon iolution Mor"04);
ABSTRACT: The fundamental theorem of motlon instability duet.0 N. Gi. Cheitnyev (TJoh.zap.
Kazansk. un-ta, 3btematika,, kn. 9, 98$ vyp. 3, 1938) and the theorein of stability Otte to
P. 'A. Kuzlniin (PMM, t. XVM, VYP. 1, 1954) allow the establiolunent of sufflolent conditions
for instability and conditional stability In critical ba.
cases. The ai -yestigates an antono-
mous differential equation system of perturbed motion with it holomorWaright-handisIde,
and with a characteristic equation of the linear system in thofirst approximation with n zero
roots to which correspond simple elementary denominators of thechameteristIc matrix, :The
author derives sufficient Instability conditions (tifforent from those found in the literature (A.
A. Shestakcv, DAN SM, 79, No 1, 1951; G. V j Kamenkov, Sb. trudov KAI, No 9, 1939).
Card 1/2

5/195/62/003/006/007/61V
EOWEW
AUTHORSs Vlasovi V#Goo Zhukovs1qy. ',V.M,
TITLE: Reductiq'h of uranium trioxide with~ammonia,
jPERIODICALt Kinatika i kataliz,
V*3, no 4.6, 1962 882-~-886
The kinetics of reductions % investigated in the
;,TEXT: Of U03 wal
temperature range 300 to 1k25*C..und0r.l0 to 600 mm KS'partial N1113
pressure a heated aft'~r dr~ying* in high",
% a 7 Amorphous U03 (0 .5 g) wa
vacuum,in a circulatory apparatus with;'a clontinuous recording-of
As weight.losses. The composition of, ep s wash checked,''
I ,d,. producti.
0 4n alr'~And by.Debye-Shereri.
by their *ireZd*-6m#OsA:r0ii t U308'' 'at, 0I.C
fixed M
X-ray anal5#sis. Fdf, a 113 pre3~iure, the.roduction rat
~'decreas6a with decreasing'temperature-~thile the4nduction, period
t
The dependence of th ratii ok the reaction w an
increases. e,
partial; NH' is given b
3 P.ressu", Pr4H3
b PN
H3
k,
CI)
P14H3
wh re'- ~k and b are, constants (k
e 0,89%/min and
Card,1/2.

5/195/62/003/006/007/011
Reduction of uraniuw
b 0-00312 mm- 1 fig at-4000c). The apparent activation energy
for the process is 45.3 kcal/mole and practicall:~ does 'not depand'.~'_-
on the degree of U03^reductio .n..: The authors concludii that,.the-'-^
reduction-islreal-i~md in:the-following stages: '1) adsorption of
gaseous NH3'-oh-UO3 surface, 2) docomposition of, adsorbed NH
3#~
N"3 ads -4 NH2ads ~Hads N11
2ads NHads + Ndss.
n of U6*~,t U4+
-:~Nfl' Nads + Hads; 3) reduciio 0
ad
02- + H OH + -:e,, OH_ + H
-~4 f120ads +,:8;
ads adili
41+
~U6+ + 2e
----r> U 4) rearrangement of crystalline lattice of ithw~ i
oxidized phase; .5).dosorption of Pi from the surfacet;.
2Na ds' -4 N N2 gas; desorotiow of H20~ formed during',
2ads
-the reduction, The.'slowest stage in this procesaji'stage
5,
There are 5 ~figures.
ASSOCIATION! Urallskiy politekhnicheakiy institut im. S'4M,Kirova
(Ural' Polytechnic Institui~iM_eni*S.M,,K1rov)
March 24, ig6i (initially)'
SUBMITTED.$,
(after revision)
Card 2/2 September 11, 1961

'23
1!i
4
ML26/62/014/003/020/022
E039/t420~;
AUTHORS: Zhukovskiy, V.M., Vlasov, V.G,,,Lebod-av,,A.G,
TITLE, Electrical properties or'the uraniuiai-oxygen system in
the ran'ge of composition U03-to U30~11
PERIODICAL: Fizika metallov i metallovedeniyeo,vdi4t no&39 .1962,
475-478
TEXT: The range of uranium-oxygpn c.ampounds:UO2ito U307r
investigated by other workers' is.bxtended t0l~cover'U03 to U308'-
Electrical conductivity Is measured in the temperature range
25 to 200*C. -Samples are prepared from U03'~by dissociation in a
muffle furnace. Spectroscopic measurements.~show~the presence of
impurities Na, K, Mn, Fe, Skand Al, the largest component being
Na at 3.8 x 10-2%. Debye-Scherrer,X-:ray:analysis indicates that
U03 is amorphous while U 08 has.a~hexagonal lattice. Intermediate.
3
compounds show a mixture of the two phases, Eden UO' xhibits
2 37,et
Yeak lines of the U308 structure. Samples are form; n o,
tablets 14.5 mm in diaMeter and-7 mm thick at~a pressure oC
3000 kg/cm2. Densities after compression arn,3,13,9/cO (for U03)
and 3.65 g/cm3 (for U308).. Resistances in the ran'Se 106 to
Card 1q,;&

s/126/62/6W 03/QgO/022
Electricalproperties,
E
Oj9/
7,
011 ohms,are measured using aconstant current megohmmeter'~with
-1
an uracy of 2 to 2-00%. Resistances in th~range~lo tW
10 ohm are measured using an ate* bridge at~JODO C/s wit~'!an~
accuracy of better
than 5%. Samples are measured tinder vacuum
(10-3 to 10-4 mm HS) Values of.the specifie,electrical
conductivity x (ohm-lem-1) for U03 and U02~; nd tOOOC
67 at 25 a
are given in the table. The temperature dependenc'e' (if the
electrical conductivity in given by
x A exp(- AF./2kT)
-10 where jaE is the activation.energy. Isotherms,df%' x aro'~Si4en
I't is shod t~ t
and also the, dependence of, 6E on ~compoxitionl.~ A
all samples have a negative thermal emf with r4papoct 1o coppdr.~
Both the electrical meAsurements and X-ray analysi.s,,shbw tha~t.-
or to greater
there is a transition from a state oflow ord for'U03
order for There are 2 figures and 1 table.
U308'
ASSOCIATIONt Ural'skiy politekhnichoskiy-Anstitu't im.,S.M.Kir~val~
(Ural Polytechnical Institute AM97 i SMAir 'Y).
Card :2

/62/01;5/010/001/012
S1080
D204/1)307
-AYMORS %hukovskiy :V.11. and V3.6 0v V.G
s
'T I IME .,The offect.OC,alkali:metal earboUates1w.01% the rAte
of reduction of,uranium trioxi&v
PERIODICAL: Zbu r n a I prikladnoy Ithimii, v.' 35'~ ~noji,!Oi 19 2i
2131-2134
Na-q -Z
CO
TZXT: Theeffects of analytical pi~rity~iLi,P~,.
and K CO- were. observed, on the rated of reduction: of : dm6rpholu
2 Z.)
2
M '3 nt
U03 (Specific surface 15,0. /g, dencity:6..5 9
~Cj
-2 - -10-4 'ia.amounta of K In 170 1 '
about 10 Ila M i Al arid
d frix4 the c~1~41y~-
rwith a dry, 1,116-free mixture of H2 and 142 1 derIve..
tic decompositfon of azmionia. The c4rbonates wdx-al .46d' a 171
roin-&;togeig
~n amounts of 0.2 - 10 mol.5 (W.r. t. ~ U00 I tiara t r trith
SU, the oxide, and were preheated for 2 hourjs at 3809C beto'rc the ireduc:-
tion. T lie prod Gure of (311,) + -142) was 200 m 11g;:, awl t.he temp~iitture
PAIdition slo~r
was 4000C in all cases . It was found that carbonat1%.
Card 1/2
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2
Mill

SAM=
ms
m
'AUTHORSt Via mov V.S., Z V
TITLEs Iteductign 0,C uramium trloXidla by a,
PUZODICAL: Kinetika L katalim, 4i
TEXTI ~ r, ~-I--
Thie wor C,. a a: Coll ftwi
tion at kiddtI16, altudles- of the
Aim antarplimtv U V
radtidtiam qf U03 with various gasas~ 03 itl
the surface area aC 19 uj% and density (~r 6.5 gletzt? %-ao raduaad
with a mixt,tre Of N2 a" U2 reumlt"L& from the reductiam of W13
over Ni at 930-C. Full. tranmition from UO> to U01,1 wal; colUaidetred
as 100% reduction. The redixctiort was studied b,styo,(Ion 30-0 and
500% at a pressure or P 31i?-.N , 200 mm Hg, mad at 425"C, vith
2
preasures ranging Crom 25 to 6013 mm HE,# The rato of reduatlon~
increased rapidly ic:Lth tomporature, nO indU0t40,n p0t'iads beillig
noticed.. The effoct of pralsstu*o an the reduotion v~r. t vv f. a
expressed by v a kpH pj~ boing the partial, prtils'amr-ov of
hydrogen. The vatluai be mrs m?P12-oxiarately C.111,15. Tho
roductian is thereCore iadopend-vat OC M2 uhich 4kctm only a a a
diluent. The pracesm takes place In the follmrimjr tita.gesl
Card 1/2

Reduction or urdlitum
E077,/EI43(1
1) U03 -) U02'.92 reducticiu ratm constdint;
Z) an auteentalytic pro'ceslis IJkI
UO '44H UO 141,- 0
2.92 aaorph. 2; C'm a 2.67 CrYgil 11 &AIS
3) UO H UO H 0.
2.55 cryst. * 2 gas 2.125 2 get a
4) UO
2-55 U02+x U02
The first atage takes ploce Ln the pVesen(llm Of two solid phaten and
the second. in the presence of oine itolid pimse or rhallaing com-Ooffitim
with the roduction rate fallinig continuounsly. Tl,.v, mpparent
activation anergiam for the various stagea of j,*dkttA3cm vary er-cam
26.5 to 31.7 kcal/mole. In jranarail, the rediuctimi with N2 + H2
ocemrrad more easiLy and to a futleir sxtent 11-haml A1,1'.111 qtth NH3.
There are 4 figure4i,
ASSOCIATIONs Uralltslciy poIiIP4chn;,cheaItiy institut 1.113. S.M.Ktrava',
(Ural POlYtOO.IhILiC TVkOJtit%'t0 11IM111. 11.)1.311rCIVI
SUBMITTED: May 1,;, 1961 (initiflIly)
Card 2/2 Septomber 26, 1.961 (aftor rayls:Lon)

AUTHORS: Zhukovskiy, VVM.-, Tkaicheinko, Ye.V. Vlavov,, VA.
TXTLE.- On the quastion~ of~:pbwtsq -conversioil: in
PEAIODICAL: Fiiika: metal 110V~, 1.1 tie ta llovad4raylo, 11 15,1 visa.22, 1~63,
:77
210-214
TE.' o,. contra d Let ~46~k 4'hc.4411 ~`Ori ~ith!t t1s
h
is
ions In -the tl'- 0 daysteva Cori thit
and
range U02- U02.25 is examined. The dependonce of tLte density anfl
parameters of.the cubic lattice on the. compogition ot the raoli.V
phase formed in reduced U4.09.,i%,rhen decomposed by ammwida and $6 ,id
carbon is invostigated. With increase in quantity of introduced
oxygen the density of the oxide is increased and the lattllce
parameter decreased. When the oxygdn content of t,tia omide is
changed it is necessary to alter the charge on some of tho urartiuai
ions in order'to maintain electrical neutrality. In particulAr
in U02 uranium is found only in the torm of Uk+ ionm (ac.-cordin$, to
the authors' data), the lattice parameter is 5-417 X and the donsit 'y
is 10 7 j1cm3. In the ease of U~'39 Yhich has a lattloo pararito-tov,
of 5.44 and a density ot'll.4 S/I;m3'0 it is noodinsairly to altai the
Card 1/2
F

S /.19 -rddt~bos
th u a ~90 2TO
-On, e, q e ti46n. of,phas 3 :1
+
n soma of the.. utartiuaA -ii6tid frbui ~U ~:~to~ V,
harge. o
it
substitution Q f, -some: 4+ ~ ~ - * , 5+
i-I ons ~b~r~ the I sriaillei~ U. ions Yt
-1ea
d- to, a decrease
in: the 14t:tiii~b pa'x~aaetor.:for. U40
,the introduction ~of m re'ioxyzen.: j th 6 radil 1 V5 n
0 a 41 u6i
ions are 1.05, 0,91 and 0.79 X respectively) . 0onsitios maa,#~rO4
-experimentally compare well with thosie detersaine.4 f i:.mii X - ra y
diffraction arutlysis. The resultis are in agreeiviani. with the
statement that the phase of U02+x has a cubic lattic-4L~ at' the
fluorite type with disordered introduction of surplus oxygen wid
four atoms of uranium in the elemoxxtar.y call. There are is fiAiAreal.
ASSOCIATION: Urallskiy palitelchticheskiy insti'ttM ilrl~ 8*J1.X r0
Wral Polytechn:;icia ~ III
f T:ztitute imeni S.M.3:irov)

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Call. 1164 AY55iOW C 6 0 0 CA 3
BOOK
Axithor: ZHUKOVSKIY, V.S.
ftn' Titli--.--TEM=AL7THERMODYfl~AkiS (3rd ed Io
Transliterated Title: Tekhnieheskaya Term6dinamiM.
Publishing Data
Originating Agencyi. None
Publishing House: State Publishing,House 'of Teehlifcal-ThboreticAl Liter~iureo;
0!
'Datei. 1952 No. pp.: 408 (text).and 29 tables No 4! cc i ple a: l5jOO1
Editorial Staff
Teohniciil Mitor: None~
Editor; None. r
14)praio" None i
Editor-in-Chief: None*
Text Data
Ooverage: -The third revised edition.is supplemented by he following newl,
-subjects-, tendency of isolated s7;stems Ao this; Ma~6:'of eqaili~wii~ft;
differential thermodynazie equatione ail
q poteatial~~ O~Oles
Of*gas turbine-and refrigerating initallatlonh* 1i the ~ chapt4is on
technical application'of:thermod
ynamics. only eseon~#1, in
given and details are: referred :to
--The main object -of ithe -is prlxwuy to i*ineg q. clear understanding
~Adq itio he. ~9'
ofthe basic subject of, the problem ~ under coniq rr n' t - Pecific
methods of its solution,:: and interrelation ok~ ~th-i O*en met-ha, of
scieittific.:analysis with otlwr,metfiods&~:
Purpose: A textbook for students in institutions of higher Uaining and 6, t~ermo-
chemical in titut ons.
1/2

U-
O-VS7, Fl-
AID P 1256
Subject USSR/tngineering
Card 1/1 Pub. 110-a 17AT
,Authors Zhukovskiy, V. S., Doc. of Tech. Sci.i., et~ al.
Title Deych, M. Ye,, Technical Gas Dynamics. Gosenergoizdat):
1953- (Revi w)
Periodical Teploenergetika, 1 62-64,
Ja. 1955
Abstract The book of,M. Ye. Dey~ch.outlines the principles of gas ,
dynamics of the sections of turbines between the inlets:
and outlet valve through which steam passes~. It tou;chtp's
also upon the theory of turbines. It! is Intended as a:
textbook for students.
Institution None
Submitted No date

AID P 1333
Subject USSR/Engineering
Card 1/1 Pub. 110-a 15/19
Authors Kazavchinskiy, Ya. Z., Kand. of Tech. Sci. and
Martynovski-y., V. S.,, Doc. of Tech. Set,
Title Zhukovskiy, V. S., Engineering Thermoclynamics.(Review)
Periodical Teploenergetika, 2, 5T-59s F 1955
Abstract The textbook on engineering thermodynamics of,
Zhukovskiy, V. S., 3 rd.: ed., revided, published -by
Gostekhizdat in 1952, iolreviewed.
Institution None
Submitted No date

I ?I , , III 1- -11":P1 1
--- --------------
ZHUMSKIT -- ToSe-.-prof,-- rat senzent; --KNCM --red. ;-BOH1SWW1T, ~I-Xq- ---
re'd.;Z&M~MMp A.A., takhn. reds
[Problems of aerodynamies.arict hea~b transmission in boiler farnace
processes] Voprosy derodinamiki i toploperedaefil v 6tallao-
t6ocbm7kh protseseakht abornik statei, goakrao'Goo.' anere. izd-
vo, 1958* 329 P. (HIU lltltO)
(3krwass--Mrodymmics) (Heat-Tmnsmieffion)

GMSOVA, Tekaterina Aleksandroyna; ZEUKOVSKIY, Mikhail Isaakovich;
ZATADOVSKIY, Anatoliy Klkhaylovich,, ZYSIRA,-MCLOZM, Larjea
Mikhaylovna; SMRI, likolay Akimovich; TYRY=IJr, Ve'Isvolod
Georgiyovich; ZMOVMY, V.S.4 prof., doktor tekhn.wiuk* red.;
KWATMADZE, B. # prof,,`-'d'6ktbr tekhn.nauk, red,;, ZHITNIXOVA,
O.B., teklm.red,
[Aerodynamic improvement of bladed apparatus!,of atealm and gas:
turbines] Aerodin'amichookoe sovershenstvovanie lopatochaykh~,
apparatov parovykh i gazovykh turbin. Pod red. 7,8.23mkovskogo
I S.S.Kutateladze. Moskva, Gos*energ.izd-vo, 19,50. 340 p.
(HIRA 13:7)
(Steam turbines) (Gas turbines)

S/170/62/0'05/-3q7/005/010
B10,1 /3112

k~,.TIMR: S.
T ITLE isothermal flow of g-,as throug1h pire-i
FZ7~ IOD ICAL; Inzhencrno-fizicheakiy zhurnal v- 5, no. 1962
45-51
TZXT' The h:r2othasis of L. A. Zalmanzon (Protochnyye ej'&-qnty
ikh priborov kontrolya.i upravleniya - Floivo ments ofi
pnevma'ichesk cle
pneumatic control instruments, Izd. AN sssia, 1961) and ~ SISM .
Thristianovich et al. 'Prikladraya gazovaya dinamika - Ap,)Ved Gas
dyna, 71 cas in a
,j mics,. 1940-that t-lie .11sach number of an isothermal flD Of!
pi.ie can approach unity, and some conclusiond"I(lerived therefrom, are
.4:
V
reiuted. Under conditions of convective hea'k; transfer 'n ii3othermal flo's ~
izA
oe gas in-a pipe can occur in a completely determinea relationship of

number 11 at the input of the pipe and M'ach number it at., the out
,:a c h u
Pt:
1 2
t-
4+(2-r)11)/(4+r~-'i), where r is the reduction factor,, and
"
%
1
2 1

- Ps In
+ ( P1
WM 2
A P,
Card 1/2

/170/62/005/007/005/6101
Isothermal flow of gas tbrough pipes B'104/3j12
As this relationship is close to unity, the~interval of possible 11-iach.
numbers that fulfill this relation becomes extremely narrow. Hence, an!
isothermal flow of gas in a pipe can be nbtained only-if1the pr4agure
drop is very small. There is 1 figure.
ASSOCIATION: Vysaheyo voyenno-morskoye inzhenornoye uchilishche imeni
P. E.-Dzerzhinako.-of g. Leningrad (Higher Naval ~3ngin'eering:
School imeni F. E. Dzerzhinskiy, Leningrad)
SUM'
'D: October 25,
JTT! -61
Card 2/2

1. Vaesoyumnyy zaochnyy onergeticheakiy inatit-ut.

9-L~
, , T "Ijw~4 -1 , H- "
, ril, I r
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. I - I . -i ~ 1 .2

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III;. A.A If I I;

T~-
AO~)9,(A U: C6
AUM0113; ZhukovskAy, V.S., Hatnikovich, K. 1. (Leniugrud)
TITLE: He&t wd masex trarnsfer in air codlers wit2i spirthl-l'iiowd tubas
SOURCE: Teplo- i massoperenos. t. 2: Teplo- i wmssapeTonas pri fazovytdi i
khImichealkildi prevrmshcheniyaldi. Ed. by A.V. LOto% arxi. B.M. &W-
skiy. Mins%, jzd-voAUI 391M, 1962. a06 - 214
TF..Vr z With respect to the 'aoeTfi(Aetut cif heat tvatisfew frotA th,,~ air !iA
spiral-finned tubes produced by rolling-on di ffer only 14.1 ttdo f T ov. (-j rcular-
-ribbed tubes with wound-on spirale mr:er ~he conditions of jrooc ccntict of the
ribs with the supporting surface. Stability of the hea.t conuftict ijiclr.-~endently
of the operating conditions is &u &dvantago of rAie rolltng-ou rwthad. The coef-
ficient of heat transfer can be ca-lexilated from the dependenaes
Nu im,7;0*077. tdO*7!
T~ tUIL-voi=6
_._~.:,::.developied by the authors-~ anti 111if
ture contents up to 10% should be deteridned on tbe assumptbon or it a1ridlarity
----------- 7.7 .177-7.
77
7
41
I I Mill

Heat and masa transfer in air cooleva ....
_t Idh from MY oq110:11t,r:1 Wti-L) o Nu,
of the partial preissitre and tomp ratu" rie i
where NuD is the Plusualt diffusion ariterlon. 7he hydmu1i(!: re-ifit"tarl-.0 of Qpt-
ral-finned tubes at which moistura conden-,ration ocours Is in ox xt 1:_s C,f -he nl~-
sis"nce uf circul.ar-fluied tubas in. di7 air, and In appraxlimtt 11
- '
_e
o.417
Eu n Re-
where n' is the number, of longitudinal rows of tubes in the d:1ivA;1s)n of flovi.
The entrainment of miisture at velocitier:, of flow exceltiding 145 :V~mo is extrn*m-
ly great and attains 60,15" of 'hat candensed in the cooltyr. In Ud,1 oase, partj-
cularly efficient viater separator-:-, should be uaed which, la m-did t1on '~.o a ocale-
-up of the device, results In a ftart1m,-r Increane of the roaial-A: cats whir.~h wet-q
contviderable a-*z;o wi~hoi~t 'U-As faraz Lnterienlng. An approprIal, ~Appar limit of
velocity is 10 - 12 a/sec idiich ia usually rehoonimDrided and &L wi loti a sci' paraLl.on
t'0 "'r- - -,0% of the s-appl-led rnis-~-Lire Is obtal--iea the mo. t i-iin:110 separa-
-~,bes
,,r.. '. s iti-, riba sho-ji a ro-ug~) in-~ernal surfa.,cirj 11. t,'h ;ff Ie r-a ti ri~lj
f !a% depress'lan.5 &rid pro.)ef3tlona r,_5k:imb.L1.-4T, 1~he -,hraad o' ii, t;ci'~ -4. D-Le -n rsi~ah
an rouFPLrjeqs", Lne oom_ffIclianT, of ne&T transf,ir, frrr ~111!a !alter n1do
is twice th&t calculated from the current dependonees. This af-ert !E partle~ij-
Card 2/3
US !"ME. ~MFM
1:S' I I

S/8 5Q eA.10 2- /M 0/02 V029
Heat and mans trmnst'er !n air coolers .... A05-11/lk 12-6
larly us-aful far finned Vibes. V.Mo Anturlyev, G.S. SebmsXly, mid lAw Too-
trallnyy InstItut tokhnologil nmahlriastroyoniya (Oantvttl InAltitt ".mchra'.ovzr
of MaclUne Dullding) (Ts3'L-L7R-"'h) are ii;entioned. There ar-P It luld I
t-P ble.

. . : . . . I T I !. I I , :1 1 ~; . 's
- - - --- -- -- .. - . - - - - -1

OW." I I I I 1311M,
i . : ; . . I I . VIN. i
. :i I I I 1111 11 ~; I Mi ! 1;,[: 11 . ,

AUTHOR: Zhukovskiy, V.S. (Moscow). 24-7-19/28
TITLE: Distribution of stresses in notched rods during elastic'
plastic deformation. (Rappredeleniye napryazheni-y v
nadrezannZ(kh sterzhnyakh pri uprugo-plast.icheskom
deformirovanii).
PERIODICAL:"Izvesti.va Akademii Nauk,Otdeleniye Tekhaicheskikh Nauk".
(Bulletin of the Ac.Sc., Technical Sciences,Section)t.
1957, NO.7, PP-132-136 (U.S.S.R.)
ABSTRACT: Solutions of the problem, published b ]Jzhik, G-V-.~Ms
Grubin, A.N. and Likhachev, Yu. 1. (2) 6ynd Likhachev, Yuj.(3)
of the distribution of the stress inside the narrow cross
section of a deeply notched.specimen under tensile Stress
in the case,of elastic-plastic deformation are approximate
and the importance of a number of the assumptions made is
not quite clear. The results published in this paper aimed
at clarifying some of the problems involved. Due to the'
existing analogy between the problems of plane and axis-.
symmetrical deformation, it is possible~to verify certain
conceptions relating to the elastic-plastio deformation
deri-ved by means of the axi4-symmetrical problem by
1/3 experimental results obtained on plane specimens. In a
series of experiments the deformations were measured after

Distribution of stresses iyotched rods during elastic-
plastic deformation. (Cont.
21~1-19/28
successive loading steps at various points z the-axis BB,
FiS.1 (axis connecting the roots of the,notches of the front
surface of the specimens subjected to tensile-stresses in a
test machine. The shape and the dimensions of the notches
were,the same as those used by Uzhik (1). In the graph,,
Fig.1, the stress distribution in the narrow cross section
of a deeply notched tensile specimen isicompared for,axis-
symmetrical deformation and~for plane deformation. Fig.21
gives the dependence on the~specimen thickness of theAnerease
of the curvature radius, of.the axial deformation and:the
stresses at the apex of the notch at the instant preceding
failure. Pig-3 gives the dependence of.the axial deformation,
the stresses and curvature radii relations at the apex of the
notch of a thick specimen on the nominal stress in the ~
narrow cross section. Fig.4 gives the stress distribution
in the case of plane deformation calculated.by various.methods;
Fi&.5 gives calculated values of the stress distribution'for
the case of axis-symetrical defotmatioft:, usbig the same,
solutions as were used to determine thecurves of Fig.14.,
2/3 The available results are compared. For the case of plane
deformation the results are considered which were obtained

Distribution. of stresses in notched rods'during elastic-
plastic deformation. (Cont.)
0/28
IrSt24-J-19
n
by,B. P. Kishkin in his dissertation res :e neentration.
in the case of plane deformation and failure of a beam~with
deep notches", who used the theory of small elastic-plastie
deformations for determining the stress state of a tensile
stressed steel rod under plane deformation with a specimen
configuration similar to that shown in Fig.1, P.132; the
stress epures in the narrow cross section cbtained by this
author for the fracturing load are plotted in Fig.4. For.
the axis-symmetrical deformation the results of Likhachev,
Yu. 1. (2 and 3) are discussed, who gave an approximate
solution and considered the large plastic,deformationsoand
the increase in the curvature radiusat the apex of the
notch; tho stress epures obtained by him~are plotted in
Fig-5 and relate to cylindrical steel speciinens with a,deep
notch of hyperbolic profile subjected to:tensile stresses.
Grubin, A.N. and Likhachev, Yu.I. (2) did not take
adequately into consideration the change in the curvature.
radius at the apex of the notch at the in'stant of beginning
of failure. The author thanks G. V. Uzhik for his advice
3/3 in carrying out the here described work.There are 5 figures
and 9 references, all of which are 61aviot
SUBMITTED: November P-81 19566
AVAII&BLE:

AUTHOR: Zhukovskiy, V. S. (Moscow) SOV/24-58-5-21/31'
TITLE: -0 -tE6,,c-ourrxcxenv-W-Mtrengthening and tha Character of
Propagation of Plastic Zones in Notched Bars
(0 koeffits:bente usileniya'i kharaktere rasprostraneniya
plasticheskikh zon v nadrezaimykh sterzhnyalch)
PERIODICAL: IzveBtiya Akademii Nauk;SSBR, Otdeleniye Tekhnich6skikh
Nauk, 1958, Ir 5t pp 116-120 (USSR)
ABSTRACT: The coefficient of strenthening f of a notched bar is
the ratio PiP,, i.e. the ratio of the load at whi.6h.
a
plastic defo at ons in the weakened cross..section ate for
the first time larger than the elastio~def6rm*ationsl-,-bo~-the
,smooth bar,
yield point of a, the cross section of which~is
equivalent to the narrow cross seetion:,of the notch6d
bar. Study of this coefficient is of.defibite inter6st~'
s'ince it provides additional possibilitieB.oi verifying,
experimentally certain assumptions of-the theory ofj,',
plasticity. -Uzhik (Ref 2).has shown that9' due to three-
dimensional non-uniform tension which ?~in the case of a~
deep notch, takes place along the entire narTow cross
section of the cylindrical or plane deformed bar the
Card 1/4 development of plastic deformation which Btarts at the

807/24-158-5-21/31
On the Coefficient of Strengthening and the Ch6racter of
Propagation of Plastic Zones in Notched Bars
apex of the notch and extends towardsthe narrow cross
section will be braked, whereby in the.ci".e of a
sufficiently sharp notch the na row.'cross s-ection will be
subjected to elastic-plabvic deformation until the ' ~
specimen fails. The deformation of tensile stressed
bars in the case of.a bilateral notch,~ Fig'.1. was studied
by Southwell and Allen (Ref 3) within,the framework of .
the plane problem by means of the relaxation- (,numerical)
method andl in the same way as in thelother quoted~
theoretical work, they did not take into consideration
work hardening. Hill (Ref 5) assumes t1tat plastics
deformation develops rightacross the narrow cross section
of the bar,and this prevents formation of an elastic core;
according to the formula of Hill the r~espedtive numercial
values are calculated and entered-in a table, p.ll~'in .
which theoretical results are also given of Southwell and
Allen (Ref 3), Jacobs (Ref,4) and-Hill (Refs 5,6). The
greatest divergence between the f values'pertain to
plane deformation which is also confirmed by the data of
Card 2/4 Jacobs; for the plane stress state when there is either.

80V/.'?4-58-5-2l/3l
On the Coefficient of Strengthening and the Character of
Pr6pagation of Plastic Zones in Notched Bars
no elastic core at all or the elastic core is very small
(Fig 2), the divergence in the f val-~es is small.
As the basic assumptionwhich justified them character of
the propagation of the plastic zone, Hill considers the
requirement that the notch should be sufficiently deep;
this contradicts the results obtained by Jacobs (Ref.4)
according to which the character of ~he deformationidoes
not change right up.to values of b/2a -~ 8. There is~alio
a contradiction between the results ot:Hill.and the data'
of Green (Ref 8). Equally, available 93q.,erimental data~,
do not confirm the views expressed by Hill.;.it can be
assumed that the views of Hill are correct for certain
types of notchesi for instance, forvery obtuse-angled
notches. In the latter part of -the p&per the author;
deals with the approximate nature of producing the plane'
state of deformation experimentally and refers the reader
to the Candidate Dissertation of B. P. Kishkin I'Stres~s
Concentration in the Case of Plane Deformation and
Failure in a Beam with Deep Notches". furthbrmore, he
Card 3/4 gives experimental results obtained for 70 mm. long notch'e.d

Oil the Coefficient of Strengthening and the Character of
Propagation of Plastic Zones in Notched Bars
specimens of various thicknesses with'varl6us character~-
istics as enumerated on p 118. The experimental results,
graphed in Fig 5, show that for very thick:specimenB'.the
transverse contraction is small partielularly in the, case
of sharp notches which contradicts E0 results of
Lee (Ref 11). The experimentally obtained-values of~. f
are shifted towards lower values as colapared -to those
calculated by means of the.Hill formula~'a; the greateA
divergence is obtained for specimens with a sharp notch,
of considerable depth. It,was fovnd that the sharpnoss'~
of the notch did not affect appreciably the-values of. f
and this is in a reeme .nt with the results of Allen and
Southwell (Ref 35. For thin apscimens the data graphed.
in Fig 5 are in agreement with the data of Siebel and
Hosang (Ref 19). There are 5 figureel 1 table and
19 references, 11 of which are Soviet,,? 19nglish, I German.
SUBMITTED: December 2, 1957
Card 4/4

Y PHASE I BOOK EXPLOITATION SOT/2566
J.
Akademiya nauk SSSR. Institut mashinovedeniya
Problemy prochnosti v mashinostroyenii, vyp.,2(Problemil of Strength''In
Moscow, Izd-vo
Machinery Design, No. 2) AN SSSR, 1959. 97 pe-
Errata slip inserted. 3,000 copies printed.
Resp. Ed.: N.I. Prigorovskiyt Doctor of Technical! sciences Profes4*
sor; Ed. of Publishing House: V. M. Klennikov; Tech* Edt: O:;*M*
Gus1kova.
PURPOSE: This collection of articles is Intended for scientificj
research workers, engineers, and designers.
COVERAGE: This collection of articles,deals with stress concentra-1
tions. The topics.discussed Include stress concentrations in.,
holes of equal and unequal ratio, stress and strain distribution
In flat notched bars, residual stresses during heat treatment, and
stress distribution in a wide strip with a hole,near the edged No
personalities are mentioned. References follow each articlee.
Card 1/4

Problems of Strength (Cont.) ")OV/2566
TABLE OF CONTENTS:
Preface
Vagapov, R.D.0 0.1. Shishorina,.and L.A. Khripind. Method of a
Superposition of Kiiown Contour Functions for Evaluation of
Stress Concentration for Several Holes of Equal Radii (Plane
Symmetrical Problems) 5
Vagapovp R.D., 0.1. Shishorina, and L.A. Khripiria. Approxi-
mWVe'-E-v~-1-ua-Elon of Stress Concentration at Mutual, Effiect of
Holes of Unequal Radii ~31
The fore-going articles are discussions of investigations
made by the author at the Laboratory of Dynamic Strength of
Machine Parts, Institute of Mechanical Engineering, Academy
of Sciences, USSR. In these articles the authors develop a
method of linear superposition of known exact.solutions for
stress concentrations for each individual hole with aDproxi..
mate stress concentration due to mutual effect of neighboring
holes. An experimental check showed full agreement with the
approximate analytical solution.
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Problems of Strength (Cont.) SOV12566
Zhukovsk,iy, V,.S. Stress and Strain Distribution.in Flat Notched
Ba___
rs fn O~ne
Bars n onnection With the Three-dimensional Character of the,
State of Stress 54
The author investigates stress distribution and concentra-
tion in flat steel specimens of varying thiaknesses with
deep notches. The relationship between strelss concentration
and the thickness of the specimens is shown in diagrams.
Lomakin, V.A. Theoretical Determination:of Residual Stresses
During Heat Treatment of Metals 72
In this investigation residual stresses accompazlying heat
treatment are determined by evaluating plastic deformations
occurring during the process and establishing a strass-strain
relationship by means of the theory of alasb0plasfto strains.-
,Test calculations of residual stress diatributioit In a
quenched cylinder fully agreed with other experimental data.
Vagapov# R.D., and 0.1. Shishorina. LateralCompresiqlon of a.
Wide Strip With a Hole Near the Edge 84
The work described in this article was done at the Lab-
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Problems of Strength (Cont.) SO.V/2366
oratory for Dynamic Strength of Machine Parts Institute of
Mechanical Engineering, Academy of Soiencest &'3S;RQ B. I.
Rus1kin participated In the experiment. Determination of.the,
lateral compression was obtained by a method of superposition
involving the solutions for omAidirectional compression and
lo4gitudinal tension. An experimental check fully agreed.with
the results of the theoretical solution.
AVAILABLE: Library of Congress
GO/eO
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3/572/60/000/006/009/018
D224/1)304
AUTHORs Zhukovskiy, Ve $0, Candidate,of:Technical Sciencesi
----------------------
TITLE; The stressed state and strength of ai'flat steel bar
e a
of considerable thicknessin the presenc,' of conc,ehtr.'
tion of stresses
SOURCE: Raschety na prochnost'j- teoreticheskiye:i eksperimen-'
tallnyye issledovaniya-p Irochnosti.mash-inostroitellnykh
konstruktsiy. Sbornik atatey. No, 6* Moscow, 196o.,
145-154
TEXT: After static fracture of a flat steel bar having dee~~and
,sharp cuts on both sides, two.different zones,:.are obeervedoil the
surfaceg one of which (central) indicates failure of:material in
the elastic domain (brittle failure), It*ie of intbrest to'com-
pare the dimensions of the zones with the results of approximat 'e
calculation of stress distribution in the weakene&oross-seation,
The author gives a graph of stress distributions calculated from
experimental values of deformationsg.with reference' -to previous
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3/572I60/000/006/009/01'8
The stressed state ... D224YD304
publications by himself and others, There are 6~Xigures and 17 re:-
ferences: 16 Soviet-bloc and 1 non-Soviet-bloo.;The-reference~to
the English-language publication reads as follows: M,.' L. Pried and
G Sachs, Notched bar.tension tests on annealed carbon steel sipe-
cimens of various sizes and contours. Symposium on deformation ofi
metals as related to forming and service. ASTM,'Speoial Technical
Publication N87, 1949.
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ACC NR1 AT602 /6317/0323
1846 (IV SOURCE CODE: UR/0000/65;/000/000
AUTHOR: ~hjkovskiyft V 3 Madiyevskiy, Ve L; Reznikovicbs K. 1. 34 7
ORG: Hiaher Naval Engineering School im. F4 E. Dz6rzhinskiy(Vysshe-Ye
voyenno-morsko,ye inzhenernoye uchilishche)
TITLE: The true wall temperature In a stream of superanturated
SOURCOE: Teplo- I ina'sooperenos. t. III: Teplo- I me asoporenos
famykb prevrasbcheni-yokb (Heat and mass transferoNs 3:- Heat and mass
transfer in phase transformations). MInskp Nauke*1 tekhnikap 19650
317-323
TOPIC TAGS: steam power plant, temperature measurement.
ABSTRACT: The experimental "nit employed was.fe&fron-sn industrial'
boiler which produced slightly moist steam at a pressure.of 16 to 20
atmospheres, After throttling$ this steem4 wbicb was somewhat .~
superheated, was led through a spray type umidifier into a horizontal
tank to which was attached the experimental round*noz-,,.10, wbich;bad
along its length seven outlets for sampling the pressure at tbelwall:9
The experimental results are presented in the form.of a figure which
shows the distribution of the relative tempersturep? p/jO. Further
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11 ACC NR. AT6021846 9::p

A)
AP6021217 R'C'E CODE: UR/0294/661004/003/0399/0406
AUTHOR: Zhukovskiy.- V. S. (Leningrad); Mad~yevskiy,__X, L.' (Leningrad); Reznikovich.~
K. 1. (L ingrad)
ORG: none
TITLE: On the characteristic temperature of a wall in a stream of supersaturate~d*steam
SOURCE: Teplofizika vysokikh temperatur, v. 4, no. 3, 1966, 399-406
TOPIC TAGS: steam superheater,'Laval nozzlep supersonic flow,liquid flow
ABSTRACT: The flow of a saturated steam in a Laval nozzle is investigated.by deter-
mining the characteristic wall temperature and e femper4ture stagnation coefficient.
The review of literature covering such flows indicates incomplete underst a-h.ding of the
problem which has been attacked by authors by developing a splacial apparatus allowing
stagnation and wall temperature measurements to be made at anY point in the flow. This~.
system is described with special attantion paid to the sup~ersonic Ix--gime of tho flow.
The measurements have been tabulated for two-to-one relative pr4issure range and sev~-
ral superheating conditions. The results satisfy a simple relation for the tempera,-
ture dependence of the stagnation coefficient. The characteristic wall temperature
corresponds to the results of D. J. Riley in Engineer, 210, 1960. The divergence of
results from the theoretical predictions is due to flow conditions where the steam is
UDC: 536.423.4:532.5
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ACC NRt AP6021217
near the phase-transition state and such initial parameter'-a aa the degree of satura-
tions are critical. This has been confirmed by observing.the behavior offlow with
artificially introduced liquid phase. It was established 1hal: 'the surface effects
which determine the stagnation coefficient are also strongly dependent on the proximi-
ty of equilibrium transition point and influence the flow chavacteristics. Orig. art,
has: 4 figures, 1 table.
SUB COM, 20/ SUBM DATE 05Jan651 ORIG REF: 007/ OTH IM F tQ03

AP 92 66/cOO/006/0018/0021
ACC NRI SOURCE CODE: UR/012ii'
AUTHOR; Zhukovskiy, V. S. (Candidate of technical sciences'LLecturer); Surkov,~A. 1.
(Candidate of tec 6ai_8'6iences); Morozov, B. A. (Doctor of technical sciehces)
-7
ORG: None
''TITLE: Using the net-point method for dqtermining stresses in Lpal. td Vith complex
shapes
SOURCE: Vestnik mast-linostroyeniyall no. 6, 1966, 18-21
TOPIC TAGS: stress analysis stress concentration stress distribution
ABSTRACT: Expressions are given for calculating stresses in,pIrta of.various cbnfig-
urations. The net-point method is used for calculating stresses -"n,flat parts.~ A6
example is given for using this method to calculate stresses:ih a blooming millframe.
The frame was ass,,uned to be loaded.only- vertically, horizontal, forc6s ~being disregwrde
as insignificant. The stress curves obtained by the net point:melhod are comp Iar.ed withi
results for a flat frame model studied by the photoelastic method. :The:two metho
show satisfactory.agreement. Although the net-point method is-normlilly used for cal-
culations where the parts are uniform in thickness, it may be lused for approximate
stress determination in parts of nonuniform thickness as well Orig. sit. has:
figures, 1 table, 8Lformulas.
13
SUB CODE: 20/ SUBM DATE: none ORIG REP: 007/ OTH IM: 001
L _jr-
;j;
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