SCIENTIFIC ABSTRACT KOCHANOV, N. - KOCHANOVA, YE.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000723420015-7
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 19, 2001
• Sequence Number: 15
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

-86270
ANothod for the Interpolation of Functions 8/ioe/60/015/008/009/010/XX
b.v loans of Exponential Polynomials and Its B019/B063
lpplio&tion In the Synthesis of Electric Cir*nts
is taken to be the solution of a homogeneous dIfferontial equation
0 ) n-i) (n)
so J(x) + &I I . ..... a ~~X) - ~ (z) - 0, Using this dif-
n-1
forential equation, a set of algebraic oquations Is obtalnods
olo + '111 ' * "n-lyn-I * ?n
+ a
A * "112 + n-11n * 1n+1 (6)
m + M ac
0 1 + a2m + an-1 VK
Thus, it is possible to determine VX) and represent 1(t) as followas
I - I
Mi x2 Mn
M Ck OPk+. 1 (9)
wn ,n-I mn-1 Mn- -
2 n n-11
SpIt 0 p2t e-Pnt 0
Card 2/3

t)3
AUTHOR: lot
AMM44
011 the COMICOLIC)II &Itwee-i Tr;jnorer F-jIIf*tAf)w, if' 1,111o.1t.
Systems and Their Dtplaci~
Avt,,,)mttlica I telemeldinni(a, 11,~160, Vol ?-11, lir 1, pp
0-28 033fl)
tn the study a method Is gJven of uoln, rec-,wrent
c-xpresiloni and ot' doublIng the pitf,11 oi* dclso-rete
values In their applicat, Lori to the analysl.-~ ,)r
the dlocrete magnItuden of trArisfer
DerInition of Problem. The it-imer.1cal mt,-Uvjd.,,, of
Bolving Lranalon't itate baoed ori discrete
magriltudes of' the tr,,.insf-~r furiction, do not rCquire
any calculation of roott (-W the chttraicterI.Ale eq,.ja-
tion. or any Fraphical m~thrjd..;4 Llnear zystcmo with
lumped coniUtzit..- are bel iv di~,.cw-mcd. Furintlon
Jet thc lmpull,;e trirtnoff;~,r V~uitutlrjn or-
pavi, of a Lr,tnnI'(- l'unf,tIon o!' 't .,,yrft~,M lrivl~ a

t t_. r.1 i t I lp I a c I., L; (.I. t,
fvac Lton, atv fol tlo,.-~
+
Sovies expar-sion of' th!!7i ;.'rav! 1-:i~ -~Itli
r(.110
negative degrees of' 1), 1:1
(21
Hero

On the Connection Between Transfer FuncC[onts 7-1472
of Linear Systems and Their laplace Reprooenta- SOV/103-21-1-3/22
tions
This equation in obtained rrom:
r 4- aa~-* + 0--e-2 + - - - + 4- - 0 (4)
u3ing the following systew of' correapondence botween
p and a symbols:
I-lift-Sof
1f,the transfer function of the ayztem is do.,;cribed by
means of discrete magnltude3 Fo, Fill F20 ..., F2r.-11 ... p
corresponding to equidistanL valves of the argument t,
then the following series may be written:
+ F, .~ F1, A...+ (6)
;;;r WIS M" .
Card 3/6 wherem - J77and T In apacIng or disevete valur;:3. Tran-
vrorminp, this series Into a continued rraction, a

0o "lic, Cortnection Between Transfer FuncU)nu 71111'2
ol' lAw-ur Sy:jtems arid Thelt, Laplace RCPI'C.30tlt,'I-- SOV/1 C-3 -2! -1 -3/24"
1'ra!,- t. lon can be found which corvespond:; to thl~,;
CIS,
(7)
If the equidistant.magnitudlea P I Fit
0
are valueo of an exponenti-:1 polyncrila,'- of the n-th
order, then the equIdlatant magnltudcz- ol' the f*l 'inctlon
may be obtuincd using the recurrent
Thlo ,quation I.-, obtalried on the bazlo ol':
+

tho lk-twcen TrInst"'j,
Milf.."It. .11y(II-cirm and laplacc.
I Io
la-011jr, opecial exprel."lown of'
j bur a(;'vr~-J
tile mand F symbola. Timu, tl-o-.- px,nt,I.(-rr m*i,,
of' extrapplation ol' c.xpenentlal poIjIlorn,111I.-, (JoAcm, ined
by 211 e(IIII(IlOtill"It, V[lJII(-I';. mctllod (~,I*
Fe(~urrent Equation foi, Ecj,iIdI,:A,.,jrit or
Time PurictIon. The approxImate n~~t h- A (-)1, -1--, tc- m. 'All I rkj:~,
the A-parameters ot' 01. (,,3) 1., a t I ,; I I
(9) representa a combination of' vooLOP
PIC 2p k7
C MakIng a almllar combination of ruot3 , tile
eqtiation ror doublIng, the pItch of di-crete valuea 13
obtalued. The covMclew'-s ot' the tn',trijfornfri -cquatlon
ave determIned by tnvans o-' 11. 1. Ioobx,!hcvnk! n m-thod
for ilulvlm equatlow;. TI-X equatic,.,
41

Between Transfer
and Thelt, Uaplaee
03 - 21 - 1/22
atid the re,.urrent vxIlves.91con L.; In th-- Corn:
1~~- ~ I 1' 1, 11 lv-,~ :10-, sit .., I'l."t"i - to.
Irt thetic equatlows the quant-Ity 1(1~ Is a comblriat1cr.
ol' several A-quantitlev. the doliblIn,; ullethi-M
veveral times, It Is possible ""o Increase by 4,8,16
timett the pitch of discret-2 valtica wIthout lowe.-Ing
the accuracy of the revurri-rit The
InItlal equidistant mtjjilt.jdo~j of the looked-for
time function are dlzeusseJ. Trajialo,,iit stalte cal(!ulatlem
li; given on art vxkmplt, - tif in tlectrohydi'aulle --ervo-
ayotem under the- Int' luc- rice of a -Ini-Ic Curiction.
s f,un 1, 11 1,,,:
A Mplaclan traivif'otin t,il. t 0
W -
Method of Determinattriti ()I' the cl* *Lh,~

On the Connection Between Transfer Functlons 77472
of Linear Systems and Their Laplace Repri!senta- SOV/103-21-1-3/22
tions
Card 7/8
Representation of the Approximating Function. A
Laplace transformed functlon must be derived expressing
the exponential polynomial used to approximate the
temporary characteristic Df the system. Let the
temporary characteristic be approximated by an exponential
polynomial at 2n equidistant nodes of Interpolation.
Then function (7) may be round. By means of this
function an arbitrary number of equidistant values
of the n-th order exponential polynomial may be
determined. To this purpDse this function may be ex-
panded Into a series of negative m-orders, or else
the recurrent equation (8) may be applied. The re-
lationship between symbols A and a is found., where a
are coefficients of the ciaracterietit equation (4).
Method of Determination or the Numerhtor of the
Transformed Function. To this purpose series are
used, the coefficients of which are Initial values
of the looked-for approximating function and of its

On the Connection Between Transfer Functions 77472
of Linear Systems and Their Laplace 'Representa- SOV/103-21-1-3/22
tions
derivativeso or else Initial-moments of this function.
An example Illustrating tae proposed method Is given.
In conclusion, the author says that: (1) A method Is
given of calculating the transient states by means of
recurrent equations obtained uslng the approximate ex-
pressions for the operator of differentiation and the
method of doubling the pitch of discrete values. The
method gives a high degree of accuracy. (2) The method
Is given of obtaining Laplace transformed functions
corresponding to exponential polynomials which Inter-
polate the given temporar7 characteristics at equidistant
nodes. This method may be used for graphically given
functions. There are 4 references, 2 Soviet, 2 U.S,
The U.S. references are: Boxer, R,, Thaler., S.# A
Simplified Method of Solving Linear and Nonlinear Systet-
PIRE, Nr 1, 1956; Boxer, :1., A Note on Numerical Transf.-!'-,%
Calculus, PIRE, Nr 10, 1957.
SUBMITTED; April 23, 1959
Card 8/8

ZDCR&NDY, 1. S.
Nothod of Interpolating funotlows using exponential
polynomials and application of Ols netW to problems
of the synthesis of time char"Oristics of electric net-
works. Wlotskbniks 15 no.8151-66 160.
SKIM 1318)
(Alectria networks)

S/142/60/003/004/009/013
sl92/s382
AUTHORt Kochanovo M.S.
TITLEt Interpolation of a Periodic Train of Rectangular
Pulses
PERIODICALi Izvsstiya vysxhikh uch~bnykh zavedeniy,
Radiotakhnika, 1960, Val- 3, No- 4, pp. 506 - 508
TEXT: A periodic train of rectangular pulses (FIX* 1) is
to be approximated by a trigonometric polynomial. A sequence
of valuex'of a given function corresp*nding to the equidistant
values of t can be written &at F M r a 1 /0
0 1
F2 = 2, *0* F2n a 1, F2n+1 0 0, F2n+2 a -1 From these
values of the function It Is possible to construct a fraction
which is in the form oft'.
Xta-1 + MU-4 +
N-i + in +
Card 14

Interpolation of a
S/142/60/003/004/009/013
9192/9382
Since the zeros of the denominator of -this fraction are known,
Eq, (1) can be written as:
2x-1 .4 CO
1 (2)
2m 005 + u
From this it is possible to determine a trigonometric
polynomial which interpolates the train of rectangular pulses.
This is given byt
2q-1
ctg -31n"Ot (3)
2n 2(2n + 1)
where n in the number of the terms in the polynomial. If
the interpolaiion nodes are chosen differently, the
fractional function can be written In the form:
Card 2/5

S/142/60/003/004/009/013
interpolation of a C192/2382
4
2n - I
iib (M) =~71 2n+1 'oSI-2(2j#-0)*
.5 MI - 2m cos +1 (.4)
2n + I
and the corresponding trigonometric polynomial is given by:
2n-I 2 Ix RK il
f M 2n + 1 2 (2fi + 1) ' 2 (5 + 1)
Fig. 2 shows a graph of Eq. for n a 4 1 the figure also
shows the form of ther first four Fourier terms (see the
dotted curve in the figure). By using Eq. (4) it is possible
to construct a bipole, for producing rectangular pulses.
There are 4 figures and 3 Soviet refor*nceso
Card 3/5
'9

S/142/60/003/004/009/013
InterpolAion of a o... 'E192/2382
ASSOCIATIONs Kaf*dra Akademii avyazi (Chair.of the
Communications Academy)
SUBMITrED: June 4t 1959 (initially)
February 29, 1960 (after revision)
I
Card 4/5

tk
KOCHANOV# Nq So Doc Tech Sot -- " Study of " poeblaims-of 1, amlysis end s3mthests
of linear electric circuits with lumped constants In a time region*" Lou, 1961
(min of Higher and Secondary Specialized Rduoation RSFSR. Len Bleatrtoal
Engineering Inst im V., 1. Ullyauovl~nln)).f KL, 4-61, 194)
_04,

IOGHUOV~ #J.,
'."ology for oonatructing tables for use in calmUting
the trapter Obaracteristicis of slectrioal filters.
ElskWorrias' 16 no,903-1A 8 -162. (MIR& 15s9)
(Zloctric filters) (Radio filters)

SOBEMIXv Takov Androyeviahl JOCHANOV. M.S., oti, rod.; VIZIFOYA,
V.V., red.1 CHUMXOVA,, V.A.t tekNi. red.
(Desip of,multinomial filters] Raschat polinomiallnykb
fil'trov. Moskyat SvIas'Isdat, 1%3. 207 p. (MRA 16s7)
(Zloctric filters) (Radio filters)

KOCHANOVp N.S.
Syntheali of liwar tlectriokl netuorks In respect to timel ap-
proximation problue Maktrcavias' 19 no#931-7-23 6 165.
(141PA is a 9)

KOCHANOVS-,fi.S.~
Approximation of given time funotione using exponential polynomials*
Radiotakhnika 20 noo5elO-19 W 065*
(MIRA 18ilO)
1. Doystviteltnyy oblen Hauchno-tekhnichaskogo obs~c)-Astva
radlotakhniki I. alektrosvyasi -imeni Popova.

.Al
KOCRANOV, N.Td. Cand vat ml . (dies) 'ftu4Y of the funotional stato of
the oardlowasoular sys4to bloodl- oatoreLan4 urine/ in highly produoti"
-44 Gv~,-~
Gows of 2nd, 3rd and 4th Galving M Voncentrate type7of foodings'
A
Nose 1959s 21 pp (Moe'Vet Aaad of the Idn of Agr RS?SR). 160 ooples
M, 49-69, 142)
-63-

KOCUNOVI X. (Candidate of Vet*rinary Sciences, Koni Branch of the AcadoW
of Sciences (ISSM
Methods of daterimnation of acidity and &11-11nity of cattle urine aw
their comlation
Voterinariya vol. 35: no- 9, September 1961, pp. 81.

XOCHANOV9 Most kand. voter, nnk
..=a 0, -
Methods for dotorminim the acidity and alkalinity of the
urine of cattle and finding their relationship Voterinarlis.
38 no.901-82 8 161. WRA 1638)
1. KORL filial AM SSSR.

TIEHOKIROVAl Angelina TeigenlysYnal TIMIROT, Patr Laonidwrl
Prininal uchastlyo KOCRAWY, P.D., nsuohnyy sotroWk.
MYSMo DePat kmnd*%0kbnnAt&q namohn" rod,: 109ARVA9
Tal,j, wedushchiy redol FRUMM, P.8,9 tekhA.rade
[91mciallsed course in electrical engineering, radio engineering#
@A4 41441ronlall ftetsisllnyi ken el*ktrotAkhnlkl# radlotakhalki
I slaktronW. Leningradp Oosons=hnq-t*khn,lzd-To-n6ft9 I corno-
toplivaoi lit-ryt l6sulwootd-ale, 1960, 483 p,
!(KIU IN12)
1. Xafedrs rudnoy Meofisiki Zeningradskogo gornogo institute In*
GaTePlakhanova (for toobanov).
(Ilectric engineering)

Pa-W-242-D-
Using the wthod of amplitude-phase wastw9ments to "loot
the paramiaters of appoatus. Geofis. pribo no 9$94-99
161. iMIRA 15:11)
(Meatromagastio prompeating-3quipwnt, and supplies)

.KOCHAMOV P D
Construction of Induction magneti: transducers for electric
prospecting apparatus. Georiz. prib. no.l9s86-92 164.
(MIPA 1819)

IOCHAHOV, P.D.
Selsating the optimal loop site for the exploration of
a spherical ore body. Up. LOX 46 rbo.2:121-112 163.
(MIRA 17t6)
I I.
t A
I

1WHAXOV, Y.H.
Device for X-ray exudnation of the foot and the wikle joint in
stada d conditions. lost. rent* I ral, 36 no,6:" N-D 161.
kmLl 15s2)
1, Is fotalaboratorii (sav. Y.R.Kmhmyv) Havosibirskop nauabio.-
iseledontallskogo imatituta trawatoL)gii i ortopedii (dir. -
dotsent DePtNetelk
7=.!SIOGRAPHY) (AJWXMlX-.MDIOGM?ffl)
(PADIOOMPHL-EWIHMAND SUPPLIM)
I

AURMCRODSXIY,. A.0., Amud. tokbn.wL*k -- JU)CRAXOT, TcL.P., lush.
Sifatlating the stability of f IM s;an cavors. Uvb. vys, nabob*
savol manblaostro so* 10148-55 160. (mm 1411)
likolayevelly karablestrottellmly Imatitato
(Itrutural framoo-Nodels)

it. 01PO
AUTHORSs
TITLEt
3/145/60/000/010/002/014
D262/D304
Arkhangorodskiy# A.G.# Candidate of Technical Sciences
and Kochanovji_)UP!j Enginver
Modelling the stability of flat docks
PERIODICALs Izvestiya vyaahikh uchabnylh zavedeniy. Mashino-
atroyeniyep no. '109 1960# 48 - 55
TECT3 The purpose of this study is to examine the possibility of
determining the.stability of decks on specially built modelling in-
stallations. The principle is based on the known relationship bet-
ween loads and deformations of rods at the moment when their stabi-
lity is disturbed. The utilisation of the installation is based on
the theor of similarity, The phenomenon of the lose of stability
is descrited by the general equations
4 2
Ei_ R ~ 8 TV 0 (at Y - Ym)
- Ti -
ex bX
Card 1/4

3/145/60/000/010/002/014
Modelling the stability of flat decks D262/D304
%.+0-
k..
OY4 X, lit-to (2)
114-0
di
-a Y2 i7y- (*Y"~ Ox ZRy', = L
(3 Y
a+
and U.E1, OV dv " Y.Y., (4)
-jW -~ T(x.oV'x
for the case shown In Fig. 1 (v - area# sectional moment of in-
ertia of a longitudinal beamp I - sectional moment of inertia of-a-
transverse beamt T - contracting force of a longitudinal beamp U -
coefficient of yieldingnees of elastic mid fittings of a beam; in-
dexee: m - succoosive number of a longitudinal beam, n - successive
number of a transverse beam) the constants of simllailty are given
by
Card 2/4

8/145/60/000/010/002/014
Modelling the stability of flat docks D262/D304
C'

C'- CV0
U..
U-1.
L C U. JU-2- . . ~L_-
L. U., U.L.
-L.-
(5),
CTQ
T..
C1.
the conditions of similarity# derived from equations 0 - 4) are al-
so given in equation form, The maximum size of the installation can
be 1600 mm x 900 mm. The results obtained from a test show that the
errors do not exceed 10 % in comparison with the theoretical calcu-
lations. It is stated that this method can be used on an equal foot-
ing with the existing methods of calculatLone and also could be
Card 3/4

8/145/60/000/010/002/014
Modelling the otability of flat decke D262/D304
used to solve more Involved problemst for, example when longitudinal
and transverse beams are not equidistant and their moments of Iner-
tia vary. There are 3 figures and 4 Soviet-bloc references,
ASSOCIATION: Nikolayevskiy korablestroitolnyy inatitut (Nikolayev
Shipbuilding Institute)
SUBMITTEDs December 26j 1959
Fig# 10
Card 4/4

S/145/62/000/002/005/009
D262/D306
U A, HORS: Arkhangorodskiyo A.G.g Candidate of Technical Sciencest
and Kochanovp Yu.P.p Engineer
TITLE: Y;odellinZ of bending of frames with fixed joints
P.73RIODICALi Izvestiya vysshikh uchebnykh zavedeniy. Mashinostroye-
niye, no* 2, 1962t 86 - 95
T--'XT: The work principle of the new device designed by the author
is based on the relationship between angles of rotation of ~ointa
and moments about the points of support of the frame rods. The condi-
tions of similarity are studied and a detailed description of the
device is given. A numerical example is given of design of a stati-
cally undeterminable flat frame. The err-or in design does not exceed
5 %. The device can be used in calculating ship frames and is recom-
mended for laboratory work. There are 5 figures and 2 tables.
A 0
,ASSOCIATION: Nikolayevskiy korablestroit,ellnyy institut (Nikolayev
Shipbuilding Institute)
SUBMITTED: December 26# 1959
1/1
Card

ARSHANWRODSKIYO A.0.0 kand.tokhn.nauk; IOCHMOVp lu,Pot-insho
MD&Iing the banding of Trams vith fixed units, Izv,vys#Uclwb.-
say. I naeldnostr..no.2s"45 162, ~ (mm 1515)
1, Nikol"evskly korablestroltallmrr institut.
(Structurml rrams)

[ACCESSION NN AP4037234
ALITHORs Nochanoyp Yu. P. (Niknayff)
TITLSj Plans problem in elasticity theory for variable thickness plat"
SDU11CZ1 InSh6n*rMM ShWnUap Ye ho no* 2jo 1VAp 368-375
TOPIC TAGSt plane e1"tic1tjr#,vsrJ,&bls thickness platep plans forcep stressed
statep rectangular plate
AWRACTs The author Investigates the problem of the stressed at"* of pUt"
of varisb2e thickness, applicable to bulkheadas dock@# eta. in ship. The plate
is subJected to stresses In its plMso After deriving the basic eqastions which
characterise the stressed state of the plAtep the "bor gives Ww solution for
rectawAlar plates of variable and pukated thicknessess Origo arte but
figures wA 33 fornAUms
AWOCIATION s
Cw
,A,--

I
M111.11ION', L&I's klo, I kcs, wri
N,.%-4imwstonml probl om Ln the thectry c f R'ftil i. i - ~,-r r lites
(~! .nr!i%ble thh~vi%oo Tnzhs thire 4 'f-'
,"I %; 'ryls)

NRI AR6035382 SOURCM CCDEs UR/0398/66/000/009/AO21/AO21
AUTHOR t , KochFTnju~- Pf
.LITLEs Equation or the plans problem of elasticity theory for stiffened rfatandular
plates of variable thickness
souRat Refs zhe Vodqy transportgAbas 9A129
MY. SGURCEa Budostre L sank* Noorushe Beeps moshv6d, nauohno-tekbn. obeg vpo 1#
1965, 13-16
TOPIC TAGS: compressed stiffened plateg elasticity theorrg variational nethodg stres
distribution, strain
ABSTR=s The problem Is solved by a variational method* Expressions an sat up for
the potential energy of the deformation of the plate and of the stiffeners, and ex-
pressions are obtained for the virtual vork done by the external forces, under the
assumption that the plate in acted on by volume for,,.cs and by forces applied to the
stiffeners in the direction of the latter. The dis;placements V and Y isre determined
on the basis of the principle of the possible displacements, accordiag to vhIch the
force function should Siva a minimum in the equilibrium position,, 1 Illustrations
Bibliography, 7 titloso Yee gukacheva, (Translaticm of abstract]
SUB CODES 20
Card 111 UDCs 629.12i62hs

ACC Nli, AM4015 8=0 COM to/3239/66/000/002/0094/0100
rN)
AMNOR: Suslovs V, P. I Kochanov, YUG P.
ORG: None
TITLE: On the problem of determining the loads an the bottom plates vhen a sbip is
launched from a longitudinal slip
SOURCE: Nikolayev. Xbrablestroitellayy institut. Sudostroyeniye L morskiye
socrusheniya, no, 2, 1966. Budostroyonlys (ShIpbuildinS), 9h-lOO
TOPIC TAGS: shipbuilding engineering, compressive stress, dynamic stress, stress
,distribution
i
tABSTRACT: An approximate method Is proposed for determining the loads acting on the
,bottom plates of a vessel during launching from a longitudinal slip. The procedure
,Is convenient from the computational standpoint and.conaLderation is given within cer-.
tain limits to structural flexure of the ship and to various other factors Involving
reactions of the launching ways In the second period. The ",actions between the slLd-1
.ing and ground ways in the second period of the launching operation an given tW the
lexpressiont
Cotd 1/3

ACC N1h AT7004015
Ubere s Is the distance from the cross section of the ship passing over the throshol4
lof the launching vays to the cross section being considered, r(s) is the intensity of
the reactions in the launching wsys during the second period of the W, bins opera-
~Ion, ro(x) Is the intensity of rewtAcus, in the launching vays after the vessel has
ibeen transferred from the building w4yi to the launching ways, r(P, M, 2) Is the in-
tensity of the reactions in the launching ways due to the concentrated force P and
the concentrated moment N in the cross section of the ship passing over the threshold
of the launching vays. Accuracy In determination of r(s) by this formula depends
l
lbasically on the degree of accuracy in determination of reactions ro(s) after transfer
of the vessel to the launching vars. Uperinental data on ro(s) for six ships vith
launch veights from 1500 to 4500 tons and lengths free 85 to 140 meters show that the
actual distribution of these reactions differs considerably from the theoretical dis-
tribution based on representation of the vessel during launching as a girder on ar.
elastic base under the effect of the launching load. Contrary to theoretical predic-
tions, no significant reaction pes1w were observed in W of the six experimental
leases considered. Reactions of the launching vays after transfer may be considered
japproximately uniformly distributed on the section of those wiqs wbich Is q~trlc
ivith respect to tho center of gravity of the shipr. giving the forwa&
to
2/3

ACC NRt AT70014015
;where D. to the launch weight of the vessel and Iis twice the distance from the cong
ter of gravity of the ship to the stern end of the unbroken section of the launching
,ways. This formula is used for derivation of equations expressing P and M and for
'finding the intensity of reactions r an a function of these Wo factors and the dis-
:tance z. It Is found that the curve for reactions of the launching track& is fairly
closely approximated by Wo types of l9ads: Q1 uniformly distributed with -respect to
the length of the bottom plates and Q2 with variation according to a triangular '14v
cover half the length of the bottom. ]Pormdas are derived for calculating qj and q2
and graphs are given for determining the coefficients appearing in these forxulaz.
The formulas are recommended for practical calculations, especially in cases where the
jaunching vays are not provided vitii girders under the keel and the continuous section
As symmetric with respect to the center of gravity of the ship, providing as
"Ure" "I
~taken to "sure uniform distribution of reactions in the launching vays after trans-
:.-er of the vessel from its structural supports to the launching ways. Orig. art.
~has : 3 figures, 15 formulas.
SUB CODE: 13/ SM DATE: Xone/ ORIO MWj 005
card

ACC NRi AT7004016 /V) SMCz-0ODZ: UR/3239/66/000/002/0113/0118
'AUTHOR: _Kochanoy Yq~, F.; Spikhtareakoo V. K,
A-
ORO: None
~TITLE: On the strength of bottaw plates during launching of ships
.SOURCE: Nikolayev. KorablestroitelOnyy Institut. Sudostroyeniye I morskiye
~sooruzheniya, no. 2, 1966. Sudostroyanlys (Shipbuilding), 113-118
!TOPIC TAGS: shipbuilding engineering, yield stress, compressive stress, plastic
i deformation
~ABSTRACT: The authors consider the problem of the strength of bottom plates during
launching of ships from a longitudinal slip on ground ways with discontinuous wooden
sliding ways. Expressions are derived for determining the compressive stresses in the
i
4
,sliding ways resulting In stresses equal to the yield stress of the material for the
I
.bottom plates. It to shown that compressive stresses or 10-12 kg/c&2, which are
.average for sliding ways made from boons with a cross section of 25x25 ca, produce no
plastic deformations in plates vith a yield stress of 4000 kg/cm2 and a thickness
.greater than .10-12 mm. However, thin plates my be subject to plastic deformations
~vlnce compressive stresses in the sliding ways mW exceed 10-12 kg/cm2 during trans-
~fer of the ship from the building vap to the launching ways as well " in the second
1period of the launching operation. Kites thicker than 22 = show no plastic dsforna-~~
Card 1/2

ACC Wo AT1604018
;tion since the yield stress.of 4000 kg/cn2 Is reached at compressive stresses greater
'.than the yield stress of the pine timbers used in the sliding ways. 7be effect of-
the spaces between the timbers on stresses in the plates shove up only in the case of
extremely thin plates (5 = -in thickness or less) and my be disregarded since these
'plates are subjected to plastic deformation during transfer of the ship from the
building ways to the launching ways. *It is recommended that discontinuous sliding
'ways should be used in launching ships since the stresses in bottom plates are not
'increased significantly oyer the case vhers unbroken vays are used vhile the savings
Jin materials and labor my be considerable. OrIg. art. bass f igureep I tableo
:17 formulas.
IMB CODE: 13/ SM DATIs None/ MIO RM 002

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Dissertationt . *An Imestiption of the Irnlomes of Surfaco-Active AgenU on the
PlAirtle. Flow of PoUcrptn'ni Alumbta St Various Degmes of Surface OztWianst
Cod Chm Scit Ploscow urthw'of lowin State Vbml X* Vo loomms"s 18 Jum 34.
(Vechellov~ MolkVis &soowe 9 Jun 54)
SOt SM 318s 23 Dec 1954

-00
I 1A

507/2o- 121)-4-15//67
AqPO1i;;: LLkhtman, Vo Top Kochanovno L, A.# Dryuk~ainovno Lo 39o

TTT.LY.: Thp Prittle Destruction of Dingle Zino Cryntaln (0 khrupk9m
rourushenii monokristallov tsinks)
Mi-RIODICAL: Doklady Akedomii nauk 555R, 1958* Vol. 12o, Vr 4, PP-757-760
.(USSR)
ARSTRACT., The single-crystal samples were produced from pure zinc
(99t99 %) by the method of zone-cr/stallization which had
been developed in the authors' laboratory, The rulen govern-
Ing the brittle de;.-truction of single zinc cryatals with
different Initial orientations or tq
basic plgno with
respect to the axis of the wire (13 80 ) were invon-
~
t1gated by means of uniaxial Totation with constant velocity
-
of the extension (rv12 % min
) of the sAmples In inactive
ond surface-activi media. A diagram shown the results of the
experiments carried out with oingle zinc cryetala at the
temperature of liquid nitrogen. The plastic 41arlacemont Pre-
-
ceding the destruction in all the greater the sma Iler X
.
Card 1/3 Besides# the normal tenalono neceavary for the break in 1h9

The Brittle Demtruction of Single Zinc Crystals SOV/20-'120-4-19/67
banal plane decrease considerably with increasing X The
brittle breaking off on the banal plant to facilitats; by a
previous displaaament in this plans, At relatively -high normal
tensions in the basal plans a slight displacement will al-
ready be sufficient to cause elastic breaking off. The ex-
perimental data obtained gave the following results;
The so-called Zonke Law of the constancy of vertical normal
tensions does not apply to single zinc crystals in a brittle
state* rlastic displacement causes defects in crystal struc-
ture which prove to be the originil cause of destruction. No
"consolidation when breaking off" was observed In the case'
of single zinc crystals* The rules governing the brittle d*-
struotion in single stho orystals at low temperatures apply
also if transition to the brittle state occurs under the
inflikqnoe-of a strong surface-active medium (tog* mercury).
A brittle'state of a single zino aryAtal that Is caused by
mercury satlsfl*a the same general regular rules as the via-
cosity due to low temperatures* Thor* are 4 figurts, -1 tablet'
and 15 references, 8 of which are Soviet.
Card 2/1

- The Brittle Watruction of Siftele ZiftO Crystals GOT/20-i2o-4-19/61
. . ASnIOCIATION: Inatitut fisicheskoy khtmit AWooll nauk SSSH
(Institute of 1,hysical Chemistry 1,3 USSR)
,R on Ift: Jonuary U,, IWp by P.A. Robind*r,, Academician
BEOMPiUs Jenuary 22, 1958
1, Single orystals-Mobanioal, properties 2. Slagle
metwo -3. 21no-cryst"SatIM 40 ZIM-Motwe
~vrd 3/~

AM"
Effect of fusible metal welts on the mechanical properties d
ingle crystals d higher melting metals. Bial. lost.
etaloker. i spots. splay* AN URID. no. 402-78 059.
:
(MMA 13sll)
(Metal crystals-Therviel properties)

67397
'2 00
A LF1 HORS s JjLtWjh*Dov*. L. S. 0 J&ochanovat L. A., Likhtuant V4_ I.
7 14
TITM The Rules Governing the Brittle Doetruct of single-Zito---
PERIODICALs' Fizika tvardogo tela, 1959, Vol 1. Ir 9. PP 1448 - 1456 (USSR)
ABSTRAM Tho.present paper offers a contribution to the problem
related to modern technical requirements concerning the
Investigation of the relationship existing between the
sechanloal.properties of-metals and the chemicophysical
influence exerted by the medium surrounding them during
deformation. ?trot, a number of pertinent papers to partly
dealt with In detail, among others, publications by ,
Academician P. A. Rebinder at al., Kishkin, Nikolenkoi.Ratner,
Potaks, Shchoglakoval Roshanskiy, Pertsoyl and Shchukint The
authors of the present paper investigated the rules governing
the brittle destruction of a single zinc crystal wire at
difierent orJoStaftone of the bass plant to the Wiro %Zia
(13 4'80 ) at liquid nitrogen temperature ( 6
0 , -19 C) at
Cord 1/4 elongation at a constant rate HO/min). The single crystals

67397
The Rules governing the Brittle Destruction of Single SOT/181-1-9-21/31
Zino Crystals
were pure to a degrse-of 99.99%, and were prepared in the
authors' laboratory by zonal crystallization. The crilical
shearing stress in the bass' plans attained ~ 130 6/20 at
these temperatures and was Independent of the orientation of
this plans to the crystal axis, as shown by special expert-
seats. Mercury was used *a surface-active material. figure I
shows the measuring values and the calculated dependence of
the limit of the plast-lo dislocation (a a) of the sAngle, zinc
crystals on the orientation angle of the base plane ( TO).The
steep decline of a is described by'formula a. 0 (E +I )s WT6-~)7
sin 2
]TO --
where F is the limit of elongation before tearing, k, to the
final orientation of the bass plane before tearing. Figure 2
shows the dependence of the normal tensiod N, acting upon the
base plane, an the displacement a during deformation at
different )'o values. The following holdsi 9 P sin sin
Card 2/4

67397
The Rules Governing the Brittle Destruction of Single 501/181-1.9-21/31
Zinc Crystals
P is the indication of the dynamometer, proportional to the
degree of elongation.-Table I contains the values of a 2I 110,0
,and Sa (shearing stress) for 6 TO values in the moment of
'brittle tearing. Figure 3 shown thedopendence of-the yield
limit Psfand the critical normal tension N oat the yield
limit at constant $- and figure 4 the dependence of
&a I V t 8108 a on ~O . P0('rol shove a symmetrical cours*9 first
dro with growing , a minimum at - 450 and another risel
a
0 0) drops
(10 rises oap--- hally with groving,to; am(~
exponentially# Xa(~O) rises and Sm(ko) shows a linear drop
with growing XO_ figure 5 shows the drop of N a with rising
pro-deformation (E%ro) at 200C. (The samples were first
elongated at rooa *nperatur*, only th*r*after cooled, and
a
further elongated to the tearing point). All these experiments
were also carried out under other conditions,# the transition
into-the brittle state was not attained byoool-Inp ~ut by
Card 3/4 the action of a strongly surface-active agent (Hg). Table 2 Ij

67397
The Rules Ooverning the Brittle Destruction of Single SOY/181-1.9-21/31
zinc crystals
shows the measured %-# Na-9 and Sm values for this casep and
figure 6 the function P(&) for nonanalgazated (full circles)
and amaiga"ted (empty circles) single *Ina crystals at
Yj . 48 and T - 201C (the values coincide within the
slasurins acouraoy). Figure 7 shows am(~O) for amalgamated
and nonamalgamated samples at 20 OCI in the first case %
decreases with X09 In thi latter case it rise@ stronglyo
Figure 8 shows %(Xo)o NaQo), and Sm(TO) for asalga-
sated crystals only# figure 9 P(e,) for both types at
X. - 4;4naCn1d* T - -19600, figure 10 for amalgamated
samples at 200 and nonanalgasated at 185 C. Shchukin (Itef 15)
Is mentioned to the text, There are 10 figures, 2 tables# and
17 references, 9 of which are Soviet.
iSSOCIATI01r: Inatitut fisichoskoy khiaii AN SSSR Moskva (Institute of
-Physical Chemistry of-tho AS USSR Moscow)
S'UBWTTn: February 20t 1958
Card 4/4

05276
18(4), 24(2) SOV/170-59-7-7/2D
AUTHORSs Koohanova, L.A., Andreyeva, I.A., Shchukin, Ye.D., Ll khtaw, V. I.
TMX: Regularities in the BrIttle Fracture of Pure and Alloyed Single Crystals
of Zinc
PERIODICAL: Inthenerno-fizicheakly zhurnal, 1959, Nr 7, pp 45 - 52 (U33H)
ABSTRAM The authors studied regularities In the fracture of Pure and alloyed
single crystals of zinc along the cleavage plane (0001). Pure crystals
were taken of 3 kinds: containing 99.999% of elemental zinc, containing
99.99% of it and commercial zinci those of alloyed specimens contained
0.2 and 0.5% of cadmium. Experiments were carried out in two versionst
in the absence of an active absorption medium at a temperature of -1960c
and with a thin mercury film of about 5A,.thick applied to the specimen,
at room temperature. Crystals were produced by the zonal crystalliza-
tion method and were 0.54 to 0.9 mm in diameter and about 10 mm long.
The fracture of crystals was performed on the Polyany device at a con-
stant stretching rate of 10 to 15% per minute. The authors formulated a
"condition of the constancy of the product of nomal by shearing stresses",
which is expressed by Formula 1. pc Tc' - const . K2. By &n&lyzing &
Card 1/3 considerable amount of experimental data the authors have established that

05276
3OV/170-59-7-7/20
Regularities In the Brittle Fracture of Pure and Alloyed Single Crystals or zinc
this condition is fulfilled within a wide range or orientations or
single crystals for both pure and alloyed specimens. As the quantity
of the admixture increases, the value of X also increases. The authors
explain this by'& hypothesis an th* origination of heterogeneities In
the shearing process and oacurreaos of plastic deforwation during a
phase immediately preaWng fracture. The value of X for amalgamated
speolmens Is Wee as lot com$" to - . non-amalgamated
ones,, both for pure and alloyed crystals. 'This is explained by the
lowering of the surface energy of s1no in the presence of mercury.
Tht condition formulated by the authors agrees well also with the ex-
perimental data of the other investigators In this field, such as
Deruyttere and Or*"o4gh Aef 17, wA In consistent with the theory
Card Z/3 of P.A, Rebinder Aefs 7-1q7 an -the effect of "sorption-sative asedla

05276
'SM/170-59-7-7/2D
Regularities in the Brittle Fracture of Pure and Alloyed Single Cr7SWS of Zino
on deformation and strength properties of solid bodies.
There are: 4 grapbs, 2 tables and 13 references, 12 of which are Soviet
end 1-uniftntiflod.
ASSOCIATIONt Institut fitIcheskoy Wall AN SSSR (Institute of Physical Chemistry of
the AS USSR), Moscow.
Card 3/3

2A S300 68783 '
18 (6) 8/170/59/002'/12/013/021
AUTHORS* Povtooz- W- 2014*14

TITLEs The Influence Exerted by the Deformation Rat* and Temperature Upon
the Amount of the Adsorption Effect of Reduction In the Strength
and PIA-4ticity.bf Metals and Easily Fusible Metallic Nolte
PERIODICALi
r
Inshenorno-fisichookly shurnal, 1959, 55R)

ABSTRACT& In the experiments described amalgamated tin single crystals (pu-
gt room tempera-
rity of 99.9991A) about I " thick were d*formod
o
tur thirl, % per minute).
~& wide velocity range (from 102 to I
.
In :r:!r to-study the offset of temperature, experiments were
carried out In the temperature range 1 400 0 and at - 1960 0. The
dependence of the elongation and actual breaking stress of amal
;
hm
ganated and non-analgazated tin single crystals upon the logarl
of the reciprocal deformation rat* to diagrammatically shown in
figure 1. The diagram of figure 2 illustrates the elongation of
pure and amalgamated tin crystals at 250 C and -1960!C. Hero the
deformation rate woo 15%/sin. These and further experiments indi-
cated that, If the rate of deformation Is low, amalgamation does
Card V2 not effect the mechanical properties. It say be seen from figure I

68783 ,
The Influence Exerted by the Deformation Rate and 5/170/59/001/12/013/021
Temperature Upon the Amount of the Adsorption Effect B014/BO14
of Reduction In the Strength and PmtIcIty of Metals
and Easily Pusible Metallic Melte
that at room temperature the action of mercury manifests itself
only at a rate of i04%/mIn. The dependence of the actual breaking
stress, elongation, and yield point of amalgamated andmon-aaal-
psated tin single crystals upon temperature at a deformation rate
of 15%/ain In graphically represented In figure 3- Below -390 C it
is no more possible to observe an effect of mercury, which to ex-
plained by its solidification. It was further shown that the tem-
perature dependenas of the above-4smaribed effects has the same
character as their dependence on the deformation rate. The part
played by surface-active mercury in the#* effects is explained by
the fact that It facilitates the further development of alcrocracks
into macrosoopio cracks. There are 3 figures and 13 referenosal 12
of which are Soviet.
ASSOCILTIONs Inatitut fisioh*skoy khIaII AN 3381, g. Moskva (institute Of
Physical Chemistry of the 13 'USSR, City of Moscow)
Card 2/2

SOV/lz6-8-2-19/26
AVrHORSi Kochanovs, L*Ao, Likhtmant V.I. and R*b1nder, P.A.
TITLE: ___T_aluon1-o__of_L-8W Malting-point Fused Metal on the
Mechanical Properties of Monocrystals of Higher Melting-
point Metals
PZRIODICALt metallov i metallovodoniyog 1959, Vol 8, Nr 2,
pp 288 - 293 (USSR)
ABSTRACTs Single crystals of mine (99,99%) and cadmium (99,99%)
were used in fused tin and lead. Samples were deformed
at 18-13% per minute with a temperature constant to
+ 3 C. The metallic =odium (Sn or Pb) was deposited
on the sample electrolytically (thickness 5 p)# which
was then placed in a tube with powdered graphite to
prevent oxidation, Figure 1 shows true stress-strain
diagrams for pure zinc and zinc with a coating of tin.
At room temperature the influence of tin is small but
at higher temperatures tin causes a decrees* in strength
and plasticity* The relation betw on temperature and
magnitude of the effect of tin is :howg in Figure 2. -The
sharp increase in effect at 300 - 400 C is connected
Cardl/3 with an Increase in solubility of zinc in tin. The

SOV/126-8-2-19/26
Influence of Low MoltIng-point ?used Metal on the Mechanical
Proportion of Monocrystals of Higher Mdting-point Metals
character of the fracture also changes from plastic in
air to brittle in tin* Lead-tin mixtures were also used*
The effect of pur* lead I* very slight but with increase
of tin content in the lead up to 20%, there is a sharp
decrease in strength and plasticity of zinc (Figure 3).
With further Increase or tin content, the affect is much
slighter. It was ehgwn that it zinc coated with tin is
held in lead at 400 C for long priods, the strength of
the zinc recovers (Figure 4). This shows the absence of
any marked diffusion of tin in zinc. A decrease in
plasticity and strength of cadmium in tin was also found
~(Figures 5$6). The results on single crystals show that
the decrease in strength is not connected with any grain-
boundary effect.
There are 6 figures and 21 references, of which 12 at*
tnglish and 9 Soviet.
Card2/3

Ilk- -2-19/h2lMochancal
Influence of Low Melting-point JP S05V(j?
a 0
us a A on
Properties of Monocrystals of Higher Melting-point Metals
ASSOCIATION1 Institut fistahtskoy khiaiiAN SSSR (Institute of
Physical Chemistry of the Ac,3c., USSR)
SUBMITTID: October 15, 1957
Card 3/3

50)
AUTHORS: KochanAvap L, A,# Andr#yova# Is Aot SOT/20-126-6-44/67
lb-0-h-u-il-ni Yes D,
TITLE: On the Brittle Rupture of Pure and Alloyed Zinc Single Crys-
tals (0 khru kou rasryve chistykh i legirovannykh sonokrist-
alloy tainkal
PERIODICAL: Doklady Akadealt nauk SSSRf 19599 Vol 126, Ir 6, pp 1304-1307
(USSR)
ABSTRACT: In the papers (Rafe 1-4) the authors investigated the rupture
of pure sino single crystals along the cleavage face (0001)
and found that the product of normal and cleavage tensions in
constant - poto a donat a XF. The results are given for tech-
nical zinc and for zinc alloyed up to 0.5 % with Cd and com-
pared with the results obtained for pure zinc (Table 1).
Figure I shows the values -of rupture tension for pure zinc at
-1960 C and various angles botween crystal axis and face
(0001) as Well as the effect of a mercury film upon the
strength at +200 C. Table I shows that X increases with in-
creasing amount of additions, Figure 2 shows the values of
Card 1/3 rupture tension Ir for amalgamated and non amalgamated pure

On the Brittle Rupture of Par* and Alloyed Zinc SOT/20-126-6-44/67
Wagle Crystals
zinc single crystal In deptndence on the crystallographic
~shear a, The characteristit break of the deformation curve
at so (flow limit) as well as the Increase in strength for
a < a. connected with the latter are due to the increase of
the incomplete shears (dislocation accumulation). a. d*-
creases with increasing amount of alloy components. Uble I
gives the degree of InhonogerAty f a a 0/a; (a; refers to pure
2ino). An shown 'by figures 3 and 4P the experimental results
are In good agreement with those obtained by A. Deruyttiltre
and G# Do Orsonough (R*f 5). parc a X2 holds for both astalpa-
ated and not a"lgoisated sinc single crystals of varying
purity. The values for X &rot reduced by 50 % as a result or
the reduction of the free surface activity a. The authors
thank V. 1. Likhtman for hiii advice. There are 4 figures,
I tableo, and 13 references, 12 of which are Soviet.
Card 2/3

On the Brittle Rupture of Pure and Alloy4od Zinc 301/20-126-6-44/67
Single Crystals
ASSOCIATION- Inatitut fialcheskoy khimli Akadenii nauk SSSR .(Institute of
Physical Chemistry of the Academy of Sciencess USSR)
PRESENTED,. February 17# 19590 by P. A. Rebindere Academician
SUBVITTED: February 10# 1959
Card 3/3

31603
3/137/6 If OW/t 12/124/149
9 Arbo AC*6/A 10 1
AUTHORS j Plabinder, P.A., Ukhtman, V.I., Mchakin, Y*.D., Koohanova, L.A..
Perteov, N.V., Ooryunov, TM,V,
T1=1 llegul&rltlea and 64* wohantsm of the offW. or suall surfave ao-
tive admixtures on Isforme.lon &M strer4th propertUs of singla
arystal matals
PMUCOIC&Lt ReferatIrAyy shurnal. Ybtallurgiya, no. 12 1961 3k.35, abstraot
;W 0'
izwiO ("Tr. in-ta fix. vot4aiov. Ali i& 116 - no. 23, 147-161)
TMI Experiments wotv made with lifferimtly crlent*d Zn ad Cd single
orystols of I = In d1ametAr, ao&'A-4 wI%h a thin film of surtsoo active an anid
.HS metals. It is shown that at tompersturse over ?a of Otasp metal.zoatine
euteatics, tk* presence of a molton surfac,* -jko Uve metal layer strongly reduoss
deformability ani strength of tho speaimen &:-A prtmotes brIt'.1a failure. ?ho
brittle effoot of the surfe-n active ff*141 Is mainly a t4nitton of temperature
and the d8formation rate, Embrittlemorit ard rolu"-d strengt), are nA comwated
.with corrzsion proc*sses tut ar* caused ty a d#creaso of the wcrk whlzh Is
necessary for tk* dev*lo;wnt of crack tucl*11. due to tt* adsorption of surface.
Card 1/2

32803
8/1.)7/6 I/DW/1) 12/124/149
Reg-.zlaritios %nI -the mechanism A006/AIOI
a,)Uve metal atoms on Um Intornal mior.-surfazae. At a drop of the test too-
peraturs bel.zw T of thop "base: 4etal-coat! ne outeotics, trWambrittling offeat
vanIshes gr&4,10,111, d,.& to a reiuoad mor,111ty of ads 2i-pvLon-ao"Livo atams. The
ombrIttlIng effect vaLaIshot also at iniffialently high ton;oratures and low
t*nsl,,,n rates, when tkw resor-ptiov of deformation sloro-hetercgerelt'49a and local
stresses p,*vents the failure nu,.Oel to -davolo; W4 dangerous craoks, own at
a o-twisi:lerable doirease of free surfsoo *nor". -There a.-* 21 roferenoes.
V. st*rmov
(Abstracter'& notei Complete translation)
Card 2/2

3/020J60/133/01/19/070
SO14/BOi1
AMORSi ~-nahsxovaj L..AojL_ Shahakin, Yes Da~ Likhtman, V. 1,
9 Academician
TITLE: Origin and Development of Cracks in Deformod CrystalJ
PXRIODICALs Doklady Akadomli nauk 38829 1960, Vol. 133, No. 1,
pp. 71-73
TEXT: By way of Introduction# the authors subdivide the cracking of a
crystal an stretching Into two stages depending 0A the *our** of deforma-
tion. In the stage A there oocurs a 4169 formation and a gradual grouth of
the cracks at sites with high -tonsionj in the stage B the crack quickly ox-
toads over the sntiro cross section of the crystal, The authors discuss the
basic role of shear in stage A# and explain the origin of alcrocracke In
this stage by the unification of dislocations and the formation of bollow
nuclei* The mechanism of the development of crack# is closely exmined, and
V. Y. loshinakiy (Ref. 7) Is mentioned In a discussion of the position of
the cracks in the lattioss The most probable arrangement Is regarded to be
the serial arrangement of dislocations in a -lattice plane, which develop to
Card 1/2

origin and Development of Cracks In Deformed 3/02Y6033/01/19/070
Crystals B014 1011
a crack on further deformation* rorsula (1) is given for the length a of a
crack# and formula (2) for the normal tonsions From those formulas the
authors derive the condition for the constancy of the product from normal
tension and shear str*sol this constancy Is well proven by experiments, The
authors toslod the Independence of expression (1) of expression (2). ?or
this purpose they studied the development of cracks In amalgamated %Lao
single crystals, Riaroscopto analysts revealed Inner cracks in the orystal
plans ~(0001) of all samples. Relation (1) and (2) by Criffith were tested
experimentally$ and a few relative results are given, The authors state
finally that the results obtalnod by then prove The universaltharactor of
the scheme worked out by them for the analysis of a crack-4 olopeont'A
Thor* are 3 figures and 14 references: 10 Soviet* 3 British, and I Japanese.
ASSOCIATION: Inatilut fisiabookoy khiaii Akad*aii nauk 333R
(Inotituteof Physical Ch*ulstry_of the Academy of Scionaeop
1133R) - - -
OVDMIMDt April 7# 1960
Card 2/2

83131
8/020/60/155/005/0()8/019
/P. 1.200 B019/BO54
IUMORS1 Shchukin, Yo. D.. Koch&nov&jU.-.A , Likhtman, V~ 1.
TITLEt some Special Features of Brittle Destruction of Metallic
Crystals
PERIODICAL# Doklady Akadsaii nauk SSSR, 1960, Vol. M, No. 5,
pp. 1064 - 1066
TEXTs In the introduction, the authors refer to some of their own
previous papers (Refs. 1 and 2). There, it had boon clearly established
that in the rupture of amalgamated single zinc crystals a spread of
rupture stresses occurs along the basic plans (0001). If, for a given
angle Xo between the plans (0001) and the sample axis, P.,,(Zo) and
Pm,XQo) are the minimum and maximum rupture stresses for the angle
then the relative quantity (P... - Pain,)/Pmax strongly increases with0
Increasing To . For Xo) 500, this quantity remains below 10%. for Xo< 30
It attains a value of more than 25%. To clarify theme relations. the
Card 1/3

83131
Some Special Features of Brittle Destruction 8/020/60/133/005/00e/019
of Metallic Crystals B019/BO54
authors carried out microscopic investigations of the basic planes (0001)
of the fragments obtained in the rupture of many amalgamated single zinc
,crystals. The diameter of the single crystals L 0 was about I an, 10 was
0
between 20 and 70 , Many steps were found (fig. 1) in the surfaces of
fracture which were caused by cracks on the transition from one (0001)
plane into the other. Thorough investigations showed that the main steps
appe r In the of origin of rupture cracks. In previous papers
(Ref:- 3 and 451,aothese authors gave a detailed theory of the origin of
cracks, and here they quote formula (1) obtained herej
IT )1121(p It )1/2 (P sin 3/2 Xcos 1/2 ~),/(Pcaid/ coo 112 Va - sin 112
(90 a A 0 0 B a ZO.
Here, p. Is the normal stress to the basic plans, t o is the shearing strew
the Indices A and B refer to the type of fragment, and P. is the break
stress. Fig. 2 shove the experimental data, corresponding to (1), for six
differently oriented samples. It appears that~l) is fulfilled in a wide
range of orientation with an error of about I . From the results
obtained, the authors infer the difference between the roles played by the
Card 2/3

83131
Some Special Features of Brittle Destruction of 5/02Y60/133/005/008/019
Metallic Crystals B019 B054
outer and helical dislocations.in the mechanism of destruction. By a
further investigation of normal and shearing strtsees In the rupture of a
,crystal 1t should be possible to solve a number of problems which are
connected with the temperature- and velocity dependence of 4*struction..
There are 2 figures and 11 Wersnoeso 8 Soviet. 2 Oerman, and I US.
ASSOCIATIONs Institut fitioheakoy khiaii Akadeaii nauk SSSR (Institute
of Physical Chemistry of the Academy of Sciences, USSR)
PRESENTED# April 7, 19600 by P. A. Robinder, Academician
SUBMITTEDs -March 29, 1960
Card 3/3

20797
4 114 8/1 SY6 1/003/003/023/030
07 B102 B205
AUTHORS: Xochanoval L. A,p Shchukin, Yo. D-j and Likhtman, V. 1.
TITLE: Mechanism of coarse destruction of metallic crystals
PERIODICAL: Yisiks, tyardogo tols, Y. 3p no. 3, 1961, 902-910
TEXT: Studios conducted by the authors in their laboratory hay* shown that
the mechanical proportion of metals can be strongly Influenced by placing
them in highly adsorbing media (fusion of fusible metals). such a treatment
results in a considerable decrease in plasticity and strength. In the
papers of Academician P. A. Robinder at &I. on the affect produced by advorp...
%ion from the ambient sodium upon the moobantoal properties of solids, thosi Ix
effects have been ascribed to the considerable decrease in free surface
energy on the boundary between the deformed metal and its saturated solution
in the other liquid metal. This effect of the metal melt occurs immediately.
Experiments have shown that the rule governing -the deformation and coarse
destruction of metals is not altered by the presence of the liquid n*tal.
The study of the mechanism of coarse destruction of metals in, however,
considerably facilitated by the use of active metal molts. The present
Card 114

20797
3/16 61/003/003/023/030
Moohanisa of BI 02YI1205
pap*r includes a detailed discussion of experimental data relating to this
subject. The data were obtained at room temperature for amalgamated single
crystals of zinc. Theoretical investigations have shown that the destruc-
tion (rupture on elongation) of single crystals of metals can be divided
into two stages; Stage A: More or lose slow formation and extension of
"embryonic" cracks at points of elevated concentration of strossoo. causod
by inhoaogen9ities of plastic deformation. In this stage, the shear stress
i plays the most significant roloo Tho.growth of the cracks to accompanied
by the occurrence of now dislocations. Stage B: Rapid extension of an
unbalanced crack over the entire cross section of the crystal. This process
in predominated by the normal stress p. The critical relation between nor-
mal stress and shear stress is given by p 010 a 7 2Gd/L, where y is a dimen-
sionless coefficient which differs only slightly from 11 0 Is the shear
aodulus~ L the cross section of the single crystal, and (F the specific free
surface energy. Furthermorst the relations
0 r2L2 11~~ (1) and p. a a(ZO/o )1/2 to-O I (GcF/o,,,) 1/2 (2) holdl
aax"Fut 0 50 max
c is the length of the crack, E the elastic mR4%tius, and 0 a dimensionless
Card 2/4

20797
Mechanism of
8/181 61/003/00~/023/030
BI 02X205
coefficient of the order of unity. The two last-mentioned relations which
characterize A and B# respectively# are experimentally verified independent-
ly of each other. This was done by,:,study of the formation of cracks on
an increase in P9;nd i. The speoin (amalgamated single crystals of zinc)
had a purity of 99~1 a diameter of 1 mat a length of 10 am, and showed
different angles of inclination of the basal planes toward the axis of the
specimens. The rate of elongation was constant and amounted to 12%/mln.
The stresses were determined from the relations
To a PosinX0cos~, Po - Posinl(cslnX, where P.0 Is the tonsil* stress referred
to the initial cross section, and X is the angle of inclination of the basal
plans toward the axis of the spoolmonfor a given deformation E. The valid-
ity of the function amax(t) was proved by a series of specimens with
X;1 a 210p and specimens with Xo varying from 16 to 670 showed the correct-
ness of the relation (2) by Griffith. A study of cracks of destroyed
!,,!Pecimens has shown that the predominant role in the formation of destruc-
,ve cracks is presumably played by angular or screw dislocations.
V. N. Rozhanakiy is mentioned. There are 5 figures and 31 references:
21 Soviet-bloc and 10 non-Soviet-bloo.
Card 3/4
X~

20797
8/181/61/003/003/023/030
Mechanism of ... B102/B205
ASSOCIATION: Otdol disperanykh sistem Instituts fitichookoy khiaii AN
SSSR Moskva (Department of Disperse Systems of the Institute
of Physical Chemistry of the AS USSR, Moscow)
SUBMITTED: July 28, 1960
Card 4/4

5/070/63/008/001/011/024
9132/z46o
AUTHORS: Shch,ukin, To.D., Kochanova L A , Portsov, A.Y.
TITLE: The temperature at which the transition from
brittleness to plasticity occurs when the strouSth Is
lowered by absorption effects
PERIODICAL: Kristallografiyo, Y.8, no.1, 1963, 69-74
TEXT: It won shown earlier that single crystals or Zug coat d
with a thin layer of 11SO show a brittle fracture
at room temperature for very low *train* because of the reducla
In strength by the absorption effect, Without 11g, brittle , '4/
-fracture occurs only at low temperatures, 'The brittleness to
related to the stability of a crack. Here. rods of Zu of
varying purity,*with and without amalgamation, have bo*n pulled at
a constant rate of darormation (10%/min) at temperatures from
-200 to +200*C. The p1naticity (limiting crystallographic slip)
and strength K a (pct )1/2 where the critical normal
strain and t the cr tical shear Patrols
0 1 in, are plotted against
temperature. It seemn that the differences or* connected with the
,groater strength or tho planing of dislocations in amalgamated
'Card 1/2

5/07o/63/008/001/011/024
The temperature at which 2132/946o
crystals as a result of the absorption on to the dislocations at
atoms of fig. However, the matter to not simple on4 it may be that
Jig only-fixes dislocations near growing cracks Into which HS atoms
penetrate from tho surface, the effects In the bulk of tho;materlal
being aniall. Similar phenomena have boon observed with Zn V.0
crystaAs coated with Ga but an accompanying development of
plasticity dAd not take place. There are 4 figures.
ASSOCIATION: Inatitut fizicheakoy khixdl AN SSSR
(Institute of Physical Chemixtry AS USSR)
SUHMfTTED: February l4$ 1962
Card 2/2

SHCWXIXs YO.D.1 XOCRANOVAo L.A*j PIMOV# I*T.
I
Temporaftrwdepandant transition from brIttleness to phati-
city under sanditions of the adsorption *ffoat of reduced
strength. Xrist&UografBA 8 no,1&69-74 ;&-T'63 (MIRA 17t7)
1. lhatitut f1slobsekoy thJuji a am

A -A?
cooe i uit/0126/63/020/W/0555/05
AUTHOR., -Le A,-1--lanosInA, _x_Nj shelmAla'--ye. M; WhCOM-11-
f r. fy 77
41 -Tr
ORG: Institute of Phystr&I QWgiry An SSSR (lastitut figicheskoy khtott AN USK)
00r.r
TITM Use of amul.sification for rtflning the stigetuto of allolp with a limited
solubility of co"mients in the liquid otate- ;!r Il
RC1t"ft-Lka__v*t a "7-j__met*lI6vW*nt ir. :20s_ not-
TOPIC 1A4$ t 1 -L
A 16
_.i Wail' O!Opp
v bra
haft:4 tv ,J!
-I ~o* 0 ~ ~- - -
to Wan-carri ~ikie4ttk:
U,
T "CM11
bilk
A WAWZ.W.
vat thik''4" ;4A
4M
jielj~4- fij 4 t,
asaft
of
:pW
water tt", raft"
U 00 %tsa at, 41011.0
wig
try I1i 11 d of metal
possibUlty of tt*16 actenco re
Lc-cro-4/2 owl -548.2

L 10771-66
ACC We Ap5027140
FC,C-N
such as ~1 Cu.
such 4
T&#>'Ukn8 nickel $ad.lp --ss,the.third compommt in Order
to lot
to lower the interphase tengiol It. Orig. &rt. bee,Ip4 figures. (AZI
I
SUB CODEI II/ SUBM DATE: 2*iikt64/ ORIC ARIPI 003/ OTH AM 002/ ATO pMS3

IN,m M 71
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. i a it hor ~ 2 f udicid Lh-a an& a I .~ i : i r. , ' ,, . I - . , -.- I A - -

L;4--- -- -- - .-,-

04

3/1-91/60/000/(jor,/0, Wo;'(i
W
0004/BO64
AUTHORS: Taipse, L. Ya., Sokolov, A. D., Kochanoy Lyakina. Z.N.
TITLEt Molding of Products Trom Novolak Molding Material
PERIODICALi Plastloheskiyo massy, 1960, No. 5, pp. 67-69
TEXTs It is the aia of the present paper to raise the efficiency of pres-
ses by increasing the molding temperature for the Troduction of materials
from novolakzolding powders of the-K-15-2 (K_ 15-2 , K-17-2 (K-17-2).
K-20-2 (K-20-2), K-119-2 (1-119-2), and K-118-2 (1-116-2) types, The labo--
ratory of the zavod "Karbolit" ("Narbolit" Plant) d8veloped It 1938-1939
a procedure to render molding possible at 175 - 185 C with the molding
material being preheated. Ex9erisonts with material preheated in a high-
frequency field to 100 - 110 C shoved that the product"No. 3388/1 (safeSY
cartridge), 46 an high, wall thickness 6 me, can be molded elk 205 - 215 C,
and the product No- 3388/2 (incandescent lgap socket) 28 an high, wall
thickness 4 am, can be molded at 215 - 230 C. Thus, the time of 2olding was
reduced without any change in strength, heat resistance, and water ad-
orption. M. 0. Gurariy is mentioned. There are 5 tables and 6 references:
Soviqt and 1 British.
ar
Wo, VO
N
1_1 ltofxx: 1~N

(MXZL'l P.A*j prof4s otv* rod.1 HATMUK, L.S., kwd,, sellkhos. aw*,
%am. red.; D1109 N.A.# M, (dooessedli DIRSAA1.j I.G.9 doktor
soVkhos. nauk# red.1 YAROSMSDi Morop daktor biol. nmk# r*d.;
ROVARSM 9 A.To.,, doktor sellkhos. naukj, red.; ZUIXUV,,A*Aog doktor
mod. mukg red.; PRINTSP Ya.1.9 doktor biol. nauke red.j GIMM,
T.S.# kand. biol, rAuko red.1 IYAWYj S.M.p kwW. bil. rAuk,, red.;
USMSXIY# Q#A.p kwO, biol. vaukj red.1 GIRGUMMOV, A.K.,g kan&
tokbn. nsuk,, red.1 FITOVA#.L.9 red.; XWAKINAp L, rodel
XOCHAVM, N.p red.1 MIFIS, V.,p tokhn. red.
[Papers of the Uni'tod SaisnUfle Session of the Department of
Biologidal Soiences of the Acade:Y7 of Sciences of the U.S.S.Re
tba Department of Agriaultu-9 of the VJ.Lonin AIIAnion AwdoW
of Agricultural Solences and the Moldavian Section of tta'Acadow
of Salomon of the TJ*S*S.R.] T2-i* obwedinenooi nauabnoi sesaiii
Melanin biologicheakikh nauk AN MO Otdolonis, sexledeliia
VASKMIL, Moldavskil, filial AN SM. KiishineT. Kartia Moldvimniaaks.
Vol*2. 1959. 483 p. (MIRA 150)
I* Ob"edinsansys, mohnqa aseslyal Kishonev, 1957. Zwestitall
"ezika-vokre"a Otdaloniya biologichaskikh nauk Aktd*MU
nauk SMR (for Gonkol'). 2. Doystvitel'My chl*n V8000YU= aka-
domil eel I skokhogyaystvemVkh nauk Is, V.1.1anina (for DiM10.
(Moldavia-Agrlcultural researah-Coom goes)

OZAWA, ~9*1*1 ITAWTA, I.N.
DquIlibriun to systems Consisting of Isonorphic sohonlto-tM oome,
ponents, and a thernograpbla study of double salts and their isonorphic
mixtures. Test. Xosk an Sere 21 Div. 15 no.403-35 il-4 160.
(KM 13:9)
1. Zafedra obshohojr kblwU Xomkovskop u2dyeretteta.
(Systens (Chemistry)) (salts)

S/i53j6O/O03/OO4/O1O/O40/kX
.B023/DO54
AUTHORS: Chirkov# S. I., 'Braynina, 1%. Z., Xachanovs, 0. V.
TITLX: Use of Polyvinyl Alcohol iv Polarography
PniODICIL: Isvestiya vysshikh uchobnykh savedenly. Xhiaiya I
kbinlohoskaya takhnologlya, 1960, Vol. 3, go. 4,
pp. 600 - 603
HIT: The authors studied the offset of polyvi nyl alcohol on the r*- w/
duetion of Cu-, Cd-, and Za tons on a dropping mercury electrode from A
chloride ammonium solution. The investigation of the applicability of
polyvinyl alcohol for this purpose was suggested by Professor A.A. Tag*rj
who in thanked by the authors. The studies were conducted on a visual
polarograph of the YIAH(UPAN) system* The amperage was measured with a
reflecting galvanometer of the typo M-21 (M-21). The potential of the
mercury electrode was measured by the compensating a*thod referred to a
saturated colonel electrode. This calomel electrode, which was oonnoot-
ed with the sleatrolyter by a low-resistamoo electrolytic bridge, served
as anode. The mercury vat previously distilled in vaouo. All solutions
ftrd 1/3

use of Polyvinyl Alcohol in Polarography 8/153/60/003/004/010/04
B023/BO54 O/XX
w;r;,prefared with doubly distilled water. The salts of the minerals
a u ed copper-i oadmius-, and stuo sulfates) were twice roorystallis4d
from the doubly distilled water. After previous avelling in a small
amount of water, the polyvinyl alcohol(mcilooular weight 25,000) was dis-
solved. The cations were polarographed ov a ehloride-assonium background
(1.51 NH C11 1.5N is OH) with an addition, of 4.0 9 of crystalline sodium
aUlf1te in 100 ml of4solution. The ammonia -was distilled In a glass ap-
paratus. Ammonium chloride and sodium sulfite were recrystallized from
doubly distilled water. Figs. 1-3 show the results. The upper curve
(Fig.1) has two maxima whose character has not yet been determined. Poly-
vinyl alcohol suppresses current maxima on all curves studied. A table
.shows that, In the presence of polyvinyl alcohol, the reduction of oop-
per- and zinc ions on the mercury *16otroi* proceeds irreversibly. The
reduction of cadmium Is not so much influ,enced by polyvinyl alcohol.
There are 3 figures, D1 table, and 5 reforisnats., 2 Soviet and 2 US.
Card 2/3

go* of Polyvinyl Aloohol in Polarogr&phy S/l53j6O/OO5/OO4/010/040/XX
B023/BO54
ABSOCIATION: Urallskly gosudarstvennyy -aniversitot, in. A~ X. GorIkogo
Kafedra analttich#skoy khijett (Ural State Untyersity
laeni A. X. Gorikly, Department of Lnalytical Chemistry)
SUENITTED: November 21, 1958
Card 3/3

7WN,Ylu., ref.; ROOMOVA,Y*#Do, ref.; MAEM,O-So, rof o
Prom the pages of Journals, 18amt 21 no.4i29-32 A&155.
(0essat Uftstrlos) (MM Bill)
. r . I ~ I "

IDCRAMA, To.B. I.. MABKt I O.S.
0~, &,0* ~;- -
Cement laftstry in the Valtal Btaton: from the "a of
foreign Jourwdes 100mout 22 aools28-31 Ja-7 156.
(UMted States-Cavent ladustries) (XIMA 9s6)

WOMMU, TOOBO, Inhour.
Cement Industries In France. "event 22 so,2132 Mr-AP 156,
(Frasoo-Comeat Industries) (XMA 9:9)

10CPANOVAS Yell', inshanor*
--- - -
osmat WUNUT In amdoze ?a""% 23 A6.1130-31,44 057.
(Swado"owat Industrios) (mm 1014)
. I
o

ilA~HI,KiA. YO.A., I.nshener.
% Iffent c,f vooltn7 -nditions
crushing (from
no.4.-IJI. Jt-Ag 157,
and minerAlogIcAl coomosItion on clinker
Zeitung" no. 1/2. 1957). Useent -23
NLRA 10.11).
(Cement)