SCIENTIFIC ABSTRACT OSIPOV, I.O. - OSIPOV, K.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001238410002-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 3, 2017
• Document Release Date: June 21, 2000
• Sequence Number: 2
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

OSIPOV p 1.0.
Ralleigh-type waves at the interfhce of two medi-i of cubia
anisotropy. Izv. AN SSSR. Ser; geofiz. no.91lI70-1190 S 't)4,.
OIURA 15:8)
1. Petrozavodskiy goeudaratvenny-i universitet.
(3einmic waves)

OSIPOV,
Reflection ,ind rpfraction of rlastic planp wav-s at
b-tween n liuuid arv-1 a soli'd ;nisitrotic todv. Izv. ,Ii S-&t. '.~er.
gpofi7. n,-).12:1768-1783 I) '(d. (M.-At 1-4:12)
1. Pet?'07avod5~iy r,osunarstvennyy universitet.
(Elastic waves)

OSIPOV -1.0.
Naturo of chanCen in the propagation volocity of elastle waves In
anisotropic modla, Izv, .1; SSSR. Ser. goofiz. no.1-1--10 Jil '0:,:~
(MIRA 113.-2)
11 Petrozavodskly go3uda-ratvenn7 universitet,
(Elfistle Wave'll

nJ :r)trol).' c med'a. i.:v.
+ rc, zij -,r-,i 7,1..--.,, T
S t I W,

OSIPOV, 1.0. _
Reflection and refr;.ction of elastic plane waves at the boundary
between two anisotropic media. Izv.AN SSSR.Ser.geo;iz. no.5i
649-665 ?t~ 161. (MM 14:4)
1. Petrozavodekiy gosudarstvennyy universitet.
(Elastic waves)

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ACC NR' AP6035598
SOURCE CODE: UR/0387/66/000/010/0062/0068
AUTHO11i Ouipov, 1. 0.
ORGi Petrozavodak State Univeraity imeni 0. V. Kuaoinon (Petrozavodakiy
gosudaretvennyy univeraitet)
TITLE: Love waves in the layer separating two anisotropic media of monoclinic
symmetry
SOURCE: AAN SSSR. Izvestiya. Fizika Zemli, no. lo, 1966, 62-6a
TO?IC TAGS: seismic wave, aninotropic medium, phaae velocity, propagation velocity j
ABSTRACTz The present work is an extcnaion of previoun studies by 1. 0. Ocipov
(Volny Lyava v anizotropnom aloye monoklinnoy nimmotrii. Izv. MN SSSH, Ser. (;eofiz.,
No- 5v 1963). The author investigates the dispersion of Love waves in a monoclinic
layer separating two aniaotropic media of monoclinic symmetry but with different
elastic constants. Dispersion curves are plotted for phase and group velocitiea%for
0, 1, and 2 nodal planoe. The three monoclinic media employed are aegorinot potassium,
tartrate, and tartaric acid. 11"ho Love waves under the stipulated conditions must
satisfy the conditionst
Cord
WSJ'
X13 < C < %is - -. q
XIS
211~
UDC' 534.222:

ACC NRs
where each X represents the ratio of tne corresponding elastic constant Uc to the
density of thb medium. The dispersion is represented by
Zn YD2
(20 (1)
C66 (CG6 Yni + C"
nn + arctg
4. C,:"
3, yD,
where n defines the number of nodal planes. It is f(hmd that when the ratio~,~/H
chanCeB at che site (O,q) the phase velocity of the Love wave at any value of n
changes within the intervals indicated above. The velocity increases with increaec!
,A/H. when the value of A/H tends toward zero or toward q9 the gro velocities tenddl
toward the phase velocities as defined above. At other values of ;k7a, the group
velocity exceedo phase velocity. From a consideration of the oonditiono for mono-
clinio media and other media, it followa W.t the phase velocity of Love waves for a
monoolinic layer at the contact between anisotropic media of the same Bymmetry--in
contrast to the case when the media hays orthorhombic symmetry or are iaotropic--has
*lower and higher lunmdariee that are less than the velocities of SN waves along the x
axis for a layer and a half space y > H under the conditions of
us# mass < mot -will
Card

ACC NR, AP60355A
11%. was found that the diaporoion curves for tho monoclinic and orthorhombic media
have the same form an for isotropic media. Orig. cLrt. has, 4 figureno 1 table, and
36 formulas.
SUB CODFo 06/ SUBM DATEj 270ot64/ ORIG RU-i 005/ OTH RUI 004
Cord

OSTMV, T. P.
091pov, T.P. -- *Mcrpholory of the Vepetativ3 Nervous System of LarFe-Porned Cattle.
Dr Blol Sci, Moscow Technological Inst of the 114pat and Dairy Indurtry, 2j Jan 54.
(Vechernyaye Moskva, 13 Jan W
SO: SIN 168, 22 July 1954

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:':erf- rirp - ref-re,ices.
c r
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SHCHERMOV, V.N.,- NAGOVITSYIIA, L.N.; OSIPOV, - X.S.
X-ray investigation of structural chUgev and mutual arrangement
of individual grains in specimens of low-alloy iron in the process
of deformation by pure terwion. Fiz. met. i metalloved. 9
no* 4:510-514 AP 060. (14In 14: 5)
1. Gorlkovskiy issledovatel'skiy fiziko-tekhnichoskly institut.
(Iron alloys--Metallography) (Deformations (Mechanics))

PETROV, V.A.; 0SIPOV, I.S.; FIVANOVA, P.S.; NOVIKOVA, R.E.
Distribution of doses in the surface layers of the t"
along the beam axis of the GUT-Co-400-1 gamia apparattis.
Ned. rad. 8 no.7:78-81 JI 163. (MIRA 17:1)
1. 1z TSentrallnogo nauchno-issledovatelliskogo instituts,
meditsinskoy radiologil (dir. Ye.l. Voroblyev) Ministerstva
adravookhraneniya SSSR.

PETROV, V.A.; OSIFOV, I.S.; PIVANOVA, NOVIKOVA, R.E.
Relation of *Ihp surface dose dintribution in ga=u. therapy
to the state of collimation. Med. rad. 9 no.2:86-89 F 164.
(HIRA 17., 9)
1. Mentrallnyy naucluio-issintiovatellakiy institut meditsinskoy
radiologii (dAr. Ye.l. Voroblyov) M-Inlaterstva Mravookhraneniya

7
7FDG-11"N' I UZ F, -, A.; C's I . M, , '-I ~ .
Internstiona: on ,vjluht.-)n cf *.ne, - - ~l ~ ~ 7~ ~ ' '. f V ~
oubstanons in %he hurrnn body. Med. rad. 9 N ")4.
(M-iql~ 'ao ,,

WIMP A.Ya.
finrlim" C,
f :1'0~~"V cf th;~~Icrar Ye-d!,!'nf,
(Muntreted, Carinda). K-41. rAd. 10 rio.504n-91 MY ' 6 5 -
(m;!iA '9t6)

OSIPOV. Ivan Tersot'yevtcli
[From two centnere to rocord rrops; practices of a flax crew]
Ot dvukh tsentneroy do rokordnykh uro2haev; 12 opyto llouvodnogo
svens. [Moskva] Hookovskit rabochil. 1957. 30 p. (MIRA 11:4)
(Flax)

OSIFOT, lovif Zinoviyovich
(Tateria-a treasure] Soirrovishcho Taterii. Kasen', Tatarelcoe
knishnoe izd-vo. 1959. 246 p. (MIRA 13:7)
(Tatar A.S.S.R.--Petroleum)

A
--I0,"-TpnV- Twif Zinov,yevich; S01A)VITIV. B.I.. redaktor-, KAMAKANOVA. I.N.,
teES-ETT-2911196swiskbor
LLong journeys; notes on the Maritime Territory] Dallnie dorogi:
iz primorzkot totradt. Moskva. Sovetskil pientel'. 1957. 156 p.
(KLRA 10:7)
(Karitims Torritory-Description and travel)

KRASVDV, A.I.; OSIWV, I.Z., rodaktor; TERSHOV. P.R., rodaktor; TROFIROV,
A.V., tegftnM 9MY-redaktor.
[Drop of gasolinej Kaplia benzina. Moskva, Gos.nauchnc-tekhnicheskoe
Izd-vo neftianoi i gorno-toplivnoi lit-r7, 1955. 47 P. (MLRA 8:4)
(Gasoline)

o.-J. , V, Losir ~,-'n(ylyevjch
-IyovichsBOWKINA. V., redaktor; MCIROZOVA, G..
teVhnicheskiy redaktor
[From a tourist's notebook] 12 putevogo bloknota turists. (Moskva)
12d-vo TsK VLXSM "Holodais gverdiia,' 1957. 83 P. (MLRA 10ig)
(Burope-Descrintion and travel)

-PLLLQI,.Iosif Zinov'yevich; ROTAPIKINA. V., redaktor; TERTUSHIIN, M..
tekhnicheskiy redektor
[Sak.halin notesj Saichalinskie zapisi. LNoskvaj Izd-vo ToK VUSH
ONolodeis gvardiia.0 1956. 285 p. (MLRA 9:10)
(Sak-halin--Description and travel)

OSIPOVO I. Z.
"In Zhirul; on the oil 3hore5 of the Volpa," ?-',OSCOW, 19148
xxx

PALMOS I.. kpnd.f-owrnf.nnuk: RIVI.M. A., Omrwillot-, OSIPOV. K.,
zhurnallet; OVSCIIKINA, L.S.. red. ---l-
(Blagpovephchon;k is 100 years old] Blao,oveshchensIni 100 let.
Blagoveshchensk. Amurakoe knizhnoo izd-vo, IQ58. 5-3 P.
(Blat,,ove,.ihchanak--Description) (MIIIA 12:2)

KEDVEDEV, N., RARTSINYUK, V., OSIPOV, K.
Operative electrified model of a "regulating relae atand.
Avt.tranatl. 39 no.2:44-45 F 16, , (MIRA 14;3)
(Vioual aids)
(Highway tranaportation workers-Education and training)

NIXITIN, I., SLAVUTSKIT, S.; 1119LENIKIT, V.; LAVRIMIYEV. V., konRtr-jiktor:
Os 1POV, insh.
Alorki, the rnad of tochnical prngrons. Hast,ugl. no.4:16-17
159. (MIRA 12:6)
1. Nachal'nik tokhnicheakogo otdAla Ralakhovskogo ekeperimental'-
nogo tavadn (for Hikitin). 2. Glavrqy inzh. kontory Proyektgid-
romakhaniontsiya (for Slavutskiy). 3. GlnvW konstruk-tor kontory
"Prnyektgidro,nni-hanizAtsiya" (for Bolen'kiy). 4. Stalinognrskiy
filial CriproiWhlenssha (for Lavrentyov). S. Proyoktnn]rn
Irontnra trnsta Sn3ruz9hFkkbtonsxishen1.ve (for ORipov).
(Coal mininr machinery)

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Or"tILUIzation
M%6ftotIC FIS1dA3
"017otallizat Iona of the Chemical Umpound Alfl 11rCA
7uslon in a Cocatant Magnetic Field," K. A. 06, pov,
A. V. Miz $m1n, Ihot General and Inorg Chem Imant N.
Mumakov, Acad Sol WW, 2 pp
"Dok Akad M= SSM, Nor& Ser" Val LIZ, No 2
Autbors comfteted. aawa 4xperiumts cc crystallizaAloA
of choolool compounds of metals from fuslm In can-
stwt magnetic held. All prIor study on cx7st&3.U-
"aim of motall1o allo7s In altsmating mometio
flo2d. Describes acparimmt with nickel-aluninua &I-
437103
OW/ftyalas (Ccutd) ll Jan 1948
1Ws ccotaluing 20% uIckel. Uperiusats show that In
amstant -gastle field, oriented or7stallIzatIon or
chmical ompaunds of metals take place. Subvittol 1w
AcadmIcIan G. 0. Urazm, 28 Sep 1947.
Ca
0

I
I IR
0 P I It 11 au
I
.
~
t
':
4 L I[ I I tj 1. f
L "I (1 11 4 L a p 'r I. -k I L INA it lk W 11 1 1

N 60, W!, WHIM r - snalv-i~ 0 In,"I (mi the
Mc) curves (" cd OKIrcins ha no the cnetgy r) for a- *00
and W-trxin~ The hiShri li,it strength III the -t-lmwe I,
CX11141""I bY 116 10*17F (IVn%lIV (A t-Wif(In %tAtel 01 the till,
-it tbv imvujv~l Irvek I'vider III.L%IIC d0cWT714114011 the
:ftrFly And disiributil", 4 the ihor-i% in the litlim~
nust ~h.mjr The pt.Ax;il)jljly N rethitritmilKin o loviry
0 the fr." !br twimits"I wi.t- I,, the Ic,miy I III,
curr"r
mdloaeresl
7
I.mm . h. , no the
6, lice And an N(F) uFvr tilmilar'..
tb~ ol -P -ir,"i have little ef?mt on the hot strength ,f ;40 0
;VC)" hen WI-Y fmn a -I)d "n with it Thi, I.
00 lialned by the m,ignpIw&,.t chAtige III the Ni I urge vi
this rau L-inimnrilts h4vino an -IattKv and an A-
00 curve ,,fr,retIt Imm th.- .4 1 nicreA- the h.t
0 w) There I, %hirp vinnimOnmov vI
oI
r
,
,,
,:
'j," 1, 1 - llh- the .-I III- -I-u
:

= t",n f-, fl~, metAllic Imynd
;
9 1010~11- .,I 1-1-n "m- 'W"-fing O'rph
h.tv, 4 1
fvwn M. '11.1f.1"Itlem ... I Ir-, ,III ".. I. I.e he I-I Coo
0-ngth 4 ) IFIM Often 3 -1111 11,11,
I, 111- .4
thl, j.h,n-j-- 1. -0,11 In tie 0
j do,
5
S
U
-
-
c
ats, I CL.SSWKAVK. is

I r
11 ID 0
a tj 1 11 lid G 0 - I Is 1. 1 611 1 3
va 4
103
tV I# M at g a a, g It
e 0 0o0 00 00 00 000 0 q 00
j
000
0
: : : 00 000 00 00 0 *06 0 0 oo(/
.
0

Jul 48
Alloys, FAgb-TmVerature
Melting Points
"The Relation Between the Malting Point and the
lut Resistance of Metal Alloys," K. A. Osipov,
Inst Gen and Inorg Chem iment N. S. X=Aakov, Aced
Sol UM, 31 PP
"Dok Ak Ifauk SSW" Vol LZI, No I
D"cribes, experiments on beat resistance of various
anoye--tron-ohromium, Iron-nickel, cobalt-nickel,
amd mwVanese -nickel. Discusses relation between
h9st resistance and melting point. Bubmitted 7 Apr
48 8/49193

Usim/metals oct 48
Alloya, High Temperature
BUtectiCe
"Beat Resistance Factors of Heterogeneous
Metallic Alloys," YL. A. Osipov, Inst of Cryst,
Acad Scl UMR, 3 PP
"Dok Ak Nauk SSSR" Vol IXn, No 4
Dincusses factors which prcmote viscous flow in
transition regions and, consequently, increase
plasticity of alloys. Conclud"s that, at high
tomperatures, heterogenization of alloys in
arat=s with a eutectic must lower their heat
resistance, while, in systms with a peritectio,
-m - 33149TSO
USSR/Metals (Contd) oct 48
heterogeneous alloys must have greater heat
resistance than do phases with a lower melt-
ing point, and snaller heat resistance than do
phases vitb a higher melting point. Submitted
by Acad G. G. Urazov, 17 Jul 48.
33A9TBO

2711"
AnLl it ichop~myp I t ro.,, 1,.1, .,1 vr,lyrt r,, r

USSR/Physica Plasticity Sep 49
Metals Alloya
"Mechuni6m of the Piusticity )f Humogeneaus
Metallic Aj.Luyr. at H.Igb Temperatures," K A.
Obipov InBt .;f Cryst, Acaa Sc! USSR, pp
"1Z Ak Nauk SSSR, Utdel Te&n Naux" Nc,
EXperimented study ~:,f binary and quaternary
Metallic confirmed that one of the basic
factors in suUject mechanism is Intensific&tion
of heterogeneous distribution ~;f components-a
process involving different degrees of stratifi-
Cation of the components until a uev phase in
15 Cfr 82
am/physics - plasl~city Sep 49
Metals - Alioys tContd)
created. Concluded that solid soluti,.~,ns most
resistant to plastic flow 3hcuid ut those for
WhIch z&ximum s~iubillty is CIniy 5i;ghtly changed
with t-----rRture increase. Submitted 21 Dec 48.
150T82

- - . a a a 9 w tr1-?N,1;T-~1, W
f Ohl

Pam#*'
i
A 1, -
~

210, 21t.
2 FA I)o 9"
1949.bP- (),( - ca r of
V, of t ci Its
N do

l
Ilsovol n saw,. X
R 110 a" V
0441fol
ha 1Aplallie zee
t
I t
a The Is on
I 11CA st"" tu
Of 16,
I the ip
,
coo-
JUVIO ;i,;Pe-tu- -tr
N
Ju Y
I
the see
00. f T&Ynpe"
A
th 0
C-1 l-
sttnv
t." in th i2
udies
.
t
.,
A Y
and Us 110 6 elpe en I
and elLpe I
ror
k - goe

Z-
I

ooret
nal
t
"too of (01i
Res t2 p,,Oibk
p
the
t C* 0,

o
h
1. Ica at
f Of
1l 9 of u
C
0 a**

7
ob,
0 a
y
ro vious,
Pape

tic 0
Lo 0
"Do
woo
041

;~-
14
Do**
010 0 1 0
:0

UM/Metals - Alloys" Metallic sop 49
Melsim ftlAt
"An Analytical loression for the Rotation
ft an the Xelti% Point and the Realt-Resistwas
of aktalUc Alloysj, n X. A. Osl;ovp 2 py
'Mak Ak Xauk "MA' Vol 1=11, So I
Uses a formula obtained by Xott, for sUp valveltr
on boundarlse of graim of monostainic metals and
a formula obt&imd by Kelley for ratLa of beal
of ftsion to Doltumm's constant to find a
formula vhich saw nes-ralaticm betwmm sUp
Telocity on boundaries of Srslss of solid solu.
CV
-.4 t4oa and liquid OW 80"d %VMW.', 0*9 *nUcIft
P4 2/M"
UM/Ikt&2a7 - Alloys,, Metallic Sep'
Point (Coutd)
St.' be-lovvy tko Am I w ft adUdUsperstwe .#pd
Vw vider t4o &Uo7l * ar7stallization iuterm2,
DIAR TVIOCI-ty also depeads up= such Talues as
frequency of atoaLc oxcillatiow., parameters 2f
lattless dUmuLona of atoms, and maLber of
&Wm WbIch t"a part IA slIpping process.
ftbgtted by Ac*d 1. T. OudUov 6 ju 49.

It

OSMV, K. A.
USSR/Metals - Alloys, Structure Jun 51
"Investigation of Plastic and Othcr Properties of
Alloys in Iron-Nickel-Tantalum System," K. A.
Osipov
"Iz Ak Nauk SSSR, Otdel Tekh Nauk" No 6, pp 848-851
Studies microstructure, elec cond, hardness and
deflection of alloys using specimens 2.6 mm In diaim
and 85 mm long. Outlines expansion of lambda-
solid soln in Fe-NI-T& system at definite temp.
Resistance to plastic deformation of ternary gama-
solid soln in Fe-Ni-Ta system increases with ap-
proach of alloys to boundary of max soly. Sub-
mitted by Acad W. T. Oudtoov.
20"77

am 111DIGUOIL A.
X,
ID,15r IV
usiii..)! 0. "a ),. tZW the binary
alloys of I th 5 at..% of W, Mo. Nb. Ti, and Tn. as pi-Ile
phase soN solln. Using tlectrolytin Ni and the orimmrrrially
'

I
re me", 100-g. Ingots wo, Pam) from Alloys nielt
I
t
T
in
, ooruudurn crucibles in a H
F furnam. Coarse gra
a
l
d b
l
utie
were proi
ow ooolin durin the t,.r_yvtn. iind by
y s
d IM' C
"-025
l
Ii
t 9W
i
A
Ob
an annea
-
an
s
rnyr..
.
a
n8 a
thI&
hi
k
ft
dl
h
d
I
irl
(near to t
e t
c
ness o
n
na no) were limpaml
t
from the undefortned blinp d Mier
oRraphit obtained
'
ith F
di
f 24 kN
ti
li
A
f
00 h
Journal of the Institute of Metals w
e ra
a
m o
.
nnea
or
r. at 050
mg
'
S.O.
Vol. 21 Part 7 -1- 50 hr~ at 1100
C. did not homogenize the dendritic gratnt;
l
C in cut Ni-W alloy. The dpndrite axe;
Ppeqrod lighter In
a Mar. 1954 the rwhogniphs, being enriched in 11'. grain hnundnripA
~,

Properties of Alloym ppear as broken tints, X-rays being weakly Rhpiotb~l I)v
&2
P
15O
/Oofthewhoisgrainourface. ThIsweskabonrplitinfail
be attributed to the p ownce of easily melting Ittipitriti-.
firinkAgs porosity, or solid soln. low In W. In Ni-Sto alkv
0' C
:
W f
90 h
9
fl
k
)
nne&
or
r. at
~s ant
ne,,Illea enrich-i I,,
3
a
..
Mo were observed. Microxcopic inveotigation Phowed that
the reedies represent an inarlIendrnt phww, "nih1v a
compound of Mn and N or one of Mo and N1. linwover, the
flaki-A were not observed tinder the mit-MArOpe. The part.
of the grains near the boundarita were also enriched in Slo.
A
Ni
Nb
1l
h
d
d
t
-
n-cut
a
i
a
a core
endritic structure, but
oy
'
b
ecame homogenized aRer 60 hr. at 1100
C., although the
cdgea of the gruint -rm still enriched in Nh and the grain
boundaries abqvrbed X-rays weakly. The NI-Ti alln v u,ted
contamml only 1-8 Ti. find --&a prepared from Ni-
O
4 wt..
/, Ti manter alloy ~ annealing for rin lit. at I IWIC.
A
f
remov
arem o
a weakly abionthing pha*r. but not the
id
h
l
i
l
d

cor
ins
e t
i
w)
e gr&W of sa
ng
n. The heterogeneity of
NN
i
the
-Tp. mile)- was i9l
redured on annealing. Nlicro.
,
ficopir investigation d*j%
:varlnum Riloys Indicated hettro.
'
nn,
livit w)f

"Thermodynamic Criterion of the Resistivity to
Plastic Deformation of Completely Saturated Solid
IWI'Aions of Metal-s," K. A. Osipov, B. P. StoyW=n
Discusses meeban' sm of plasticity and introduces
concept of thermodynamic criterion, ar-lysis of
which shmm that, solid solus near satn limit my
possess high resistivity to plastic deformation
When 2d phase, coexistent with the solid solms a
cording to phase diagram or sepd. from them in
process, considerably differs from th
by its c1mm c qj , cryst str=ture
vol. Submitted by Acad G. G. Urazov

Restr

I , r~ I I r-r 11,
13 1 1 K. A. , ~nj;.
2. USS)p ~()O
L. lllinin~., Machinos
7. Wori( t,)Tpri(,nce cf Yl:. an ifficir,)t oianirw, ripOinr rperAtvy-, Vest.
rmas~,, 32, Nl.-. 1?, 11412:
9. MontYly lirt r)f llu~3.slpn Arct!sqionzi, Library of Congm.9s, A~rll 1~'J, '.;rcl.

Tbvrrnodysomk anstyals of the foo6taAct of 11ro-pb4st
'"etal odilays to p6Ok 4milmmalitam, K A 4 K~I-v aml 11 11
~4- " It It I,, P41.adv ANW Vajot ~' .1; ~ R 83, 4.19 4j
I t$%', It, b1fre-I Ilfwphsw alliols, t1w firre riwfg% I,
m.mll thr'.41ch detiNwalm .I Ow ph&-. fh~f .I,
the lij"-l .141, O".0ke.,ibm 44 Ow It,,
offiallm 4 on " And a I ph"W. In .11-.1
0"1" ." . I'm, 1%- 4 Ow .I -"p.,
Ih, ".1t, .4 111, g"'I" .1". "1 llw I.I.-
t" " A ? ... I ph,4. -... Iml v, i hm,l,mrig .41- 1 -.4,
lwd, dl~joorf-l ..".1 it, 'fv.lal wor '%.W. 11'.4 '1-1 .
'49 offierallow. diffu4'" fu ftw torms"dAt".. .I it.,
it. ph.- mir-- 'j th. -, is,
it,. t-wanve it. tt6.IW OC110-M-1. 1h....

USSR
J Inval3lifallan of the d!
a..w
gjrLnjjlb' of tb slormary gyp ali
gad
V In.
A
AV.

Oul)-ov, x.n.; Irs1XII'Ov. S.G.; LOZINSKIY. N.G.
A, now mechanism of plastioity of metallic solid solutions. Doklady
A)md. Nauk S.B.S.R. 89, 57-60 '53. lyngl. translation issued b7 Natl.
Sol. Foundatiog, Wash., D.C. as NSY-tr-19, 5 pp. (June 153)].
(CA 48 no.1:93 '54) (MLRA 6:2)
1. Inst. KachItie Pract~oe. Aced. Sol. U.S.S.R.
Authors s,,=-iarize conclisions of several 3ritish investiFators whose works
on "new" mechanism of plasticity in Al and Zn when they are deformed with low rates at
elevated terms were published in "Jo,u-nal of the Inst of -etals" for 1949-1952. They
discuss exptl data which corroborate possibility of similar mechanism of plaEticity in
solid soln of Cu-Sn system., considering 2 ponsible interpretations of the nature of this
mechanism and disputing assinription that this mechanism in "new". not actually represent-
ing phenomenon of recr-ystallization. Four micrographs accompany articl?. Pre-gented
by Acad. N.T.Gudtsov, 12 Dec 52. 25,9T15
- 8 - I I.Aj-

two b& at ths t40114 44'
VOW, kl9b4.ofm"ttlw* bafb
-r4g
I tE
ka *'fl!o
t
WM:
A

OSIPA/
fta P', v
IK *
N&A Sjj am E. At. j
Mlod
Studies Amr, F-, 01,411,
P. 005.W
'r'd Fe wfth 0'36 ' '
A abd 0.2D to 0 33% to 1.041 C, o-1.3 to 0.2",
T66. pa 4 j rel. at hmpf-raturej from 910 to 1100 C.1

C'11' 1 1, 1 PUL'
Author Osipov, K. A. and Fedotov, S. G., Moscow
Title The heat content and mechanical propertie& of metals
Periodical Izv. A14 SSSR, Otd. Tekh. Nauk 2, 98-104, Feb 1955
Abstract Cites expertmental data on the relationship between the heat cor.tent and
the mechanical properties of various metals. Diagrams, tables. Thirty
reference3, 10 USSR
In!ititution: Institute cf Wtallurgy A. A. Baykov and Institute of Machine Sci-
ence, Academy of SQien(:es USSR
Submitted : November 22, 1)~-4

" ' ~ '7, f- A.
R. ;'. , '*~! : -, .,)!
I . , 1 71
1 1- - '. , - I' A, 'r. I .. " ", ra , 7 -

K. A.
~io.-it (,r A, tiv n t f'-Di
,In i-ov , K. A.
in Pand
n Aliloys Ac Sc S
in
MOSCOW$ Dr.
r C1 )'., t a I o tuld E
I Y. ,I ti II I C. Lulk"Widt,
AL,9 Jotu lip f Ltur - Fizika, No 2, 1997 No ~9(.)4
Au t h~, r Osipov K,A
.1j --_
Title ~flipage Al rig Grain Boundaries In Metals at Ifigh Temperatureo
-*r i g F~ub Pal,~-dovwjiya pc zharoprochri,)m aplavam M. , AN SSSR; 1956, 48-51
Abstract Further modifications are made to the theory of inter-crystallite
slIppage in metals, proposed by Mott (Mott, N.F., Proc. Fhys. Soc.,
1948. 60, 34o, 391). It is proposed that In the islets located at the
place of mutual contact between the grains, where the atomic surfacer,
show good adhesion, the potential-energy barrier, overcme by a group
of n atcas as they aproach the liquid state, is determined by the value
ofthe energy E::! n (we -v,T/T )y where We Is the heat content of the
liquid metal, and w 8 is the he& content of the solid metal at the
melti-tg point (per atom). Calculations made for alwairium on the basis
of this ass=ption give results that are In satisfactory agreement vith
the experiments.
Card
Orig Pub Prochnost' met-allov. M., AV SWR, 1956, 55-57
Abstract In an earlier work (Referat Zhur Fizika, 1957, No 2,
3882) it was shown that for many metals there takes place
the relation Q ;;L 4ge-, wtere Q Is the h,-nt- -f'

t f it I I vr, I I~n 3,, 1t' Dt r fuel i orl I 11 3 o I I dMe t- I L;
Or i gPub [)'-. zhar-pro -finym ~;plavium I.I., AN SSSH, I 4~6,
I" I- t r tI c~ t;fi h,it f,,r nioj t rn.,~ta i srctgu-d 1 (.-Gs of the t ylv of the -ryt;-
I It 'e the re lat Ionshl p 4w holds quite well (~4 is the energ-3,
of !1#?' f-I! ffu~iicn, wi the-heat content of the liquid
metik.' F%t tue meltAng point) This Indicates a close connection between
the 3-117-diffusion in solid meta.13 and melting from the energy point of
view. It is possible that the aeLf-diffusion mechanism contains the same
d1st,,;.r',-an--e tD the order in the crystalline lattices as the meltLELg pro-
cess This agrees vith the ideas introduced by Ya.l. Frenkel' (Kinett-
-htsshn~,a t~-oriya zh1d1,o.,Aey 'Kinetic Theory of Liquidr,/, Publ. by Aoademy
of Sciences, USSR, 1945). Bibliography, 55 titles.
Caxd i 1

0131PCYV, K. A. (Waaaw)
"A#,tlvntl4m Kiworay 1,1011t 91,011 V-1no 1--tt Vo%lllfwo ..f' Otool'it'o 0t,"% 041*-1
40%0 144 Q-.1 1.1 ,
1-1,"i pt vd"ttl @.-I . i I $-- A# ..... . I lf.~ I I I , 4 ~ # 1 1'. to- I .. I . , , f It., Oft . ~t . . . - , . f
. . . . . .I I t, ". . t . t " t to , i I - , - t s . 6 '. * , . i , ,
I I , 10 . .

Pus i on and no] f -d i r r,jr, j or, 111cli.1, 1$4,
lip ti I IIIII'l i It Ott
ti 0 1
(ActivitY coefficlOtnts) (Diffusion) (Solutions. Solid)

OSIPOV. K.A.: IfIRDSHKIIIA. Te.k.: SOTNICHINKO, A.N.
)font rpplntnn,,n rif NI-Cii nirntnm nillays. Trudy lmit.not.
I .,It. (MIRA 1.'l 1)
1 11 ... it 1, .1 it 1 .4 1 it 111 it I I , ~ V it )
I , I - 1, ,, .. I , I , I " I I " V I )

OSIJPOV, K.A.1 MIROSHKINA, Te.M.
Investigating nickel-chromium system alloys by the hot hardness method.
Trudy Inst.met. no.3:160-164 '58. (MIRA 120)
(Nickel-chromium alloys-Testing)
(Metals at high tanporaturee)

, ~ ) I V, - V . 0. 1, . , f I I It, - .I I r i I , , V '. , 1i ,
I tivnot trat i ne tt)si ros I a t it iwe to p In p t I c dq~ fnrewit I on ~f t, I I opi of
the nickel - iron system. leal. po zharopr. splav. 1: 388-191 ' ~8.
(MIRA 11:11)
(Nickel-iron allnys--Tneting) (Deformations 04echanics))

0 C)
A
L 1, 1 t I'l. I
t 1:3 1 n ik ro kocurli o 1~ ~,nn or. A-- r
the c Is, the activated st-tte of the aturis is ::(-nt!t,',
same for all the above-mentioned phenomena : it Is ~ln -)~trt-
Card 1/3 critical state of the theri~,clynatnic in!,tabillty of *.. , . , . --

SOV/ " (.) - I - I ~: ,
The Calculation of the Linit Values of t~,e Activ-, tion Zner,~-.- :f
Procasseg in Solil
in the cryotal. SOMe 3T~eCill Clgt'E3 Of t1iis ~-,tate ,ro
the:7 r.",:y occl.r se.,aratp'-Y or simiiltarernisl. . For
tivation enei.,y one mly write 6 ',1 = nq , whqre ii ~> ' t
the number of tl,.p 9 .mul taneou!i1y act iv;it(,d FitoT.,zi i;.
and t~ie a,~tiv ition ener-y of the forr.at on f
of the exti-ei-,e
one actav,ted atDir.,'. The iut~,or
(for t:,e same ;avtal iml for L:ie jame si-eci,il --aou rf
vation' variez) on1v slilrhtly if the 3xturnal , urA i
chunee~. The variety of the eK; crinental va:u-9 (,f
y c iiu sed :.-. i i ri I t lie 11 fferen~- e betw(~en t
e n,-! r fr
n, e. 1~y t:~e Lfference letween t!iu uctiv,it-~ a
3,)m- !i ~ c I ;t , -,~ ~n t ro I i [I -,,I j ~) i-~l . n ;i for . . n o:i .
, I- I im- n Lk I i ii t 1~ I - i r~- . r.or, t n i n rfl v or r I ho I
:I C, t I I 0.'j I ~I !1:11 t!lvy I t. oll.l t I- I t t. L 11 " 1. ! I(-
:onol ivrc,i ivr, t,.(, lir,-it v (3 f t~-,

SCV" 2 o-1 2 1 17 - 4
The Calculation of the Limit Valuesof the Activation -:-'ner~7j of Various
FrooeBses in Solid Ketala
perio4ic functlon of the atomic nnmber of the element. "~~ere
are I fig-ure, 1 tablet and 5 referencee, 3 of whi2~. are
Soviet.
ASSOCIATION : Institut rietallurgii im. A. t~. Ba~,kova Akademii nauk SS31~
(Institute of Metallurgy imeni A. A. Bnykov,AS "SSR)
PRESENTED: April 11, 1)513p by 1. P. Barlin, Academician
SUBMITTED: April 1, 1958
Card 3/3

A I ITI h ) k
it!
Cardl/6
k )( , It,
A
tit leilikrl tit T I
thertllu(lyrlam], r titat, II I1'j till liaij cf,iliq 1lit- 1A ...
state. In metals in wi-ict,
occur, deviations of d if fei rnt typEu may take place L~, ~,e
by side with those describc-d at,ove. I r, ti.i!3 c~a.-,e
given temperature T 4 T OLO (where T CX0 I-Le
temperature at which the low-tempei-t)ture mo(iif1(-,Ji-,I OL
changes into 0 ) some atoms may attain the !Aate t 'v -;;J~ 11,
they are normally charactei~sed at TOLO * These Jevi~itions

Activation Energy for CreeD and Other Processe-:
0 In clid L'etals
from the ideal structure, called by the
of limiting thermodynamic instability', may be aiso
referred to as domains of "local fusion" or "locaj
phormous transformation". To each of such ,omair.s a
certain average number, n , of etoms can be as-:-.bP6,
which can vary depending e temperature, applied streEs
and other factors. lt wavW111 h
y t e author in one )c hi_s
earlier works (Ref 4) that in solid metals witll: t,',-,e f,-ace-
centred cubic crystal structure, the experimental
of 6H , the energy of activition of vol-_Lme sf`if-
diffusion, obey the law 6H = nq , where n e
number of atoms, _1t r, f " I -I I,
q i -, t 1, e 1. ( 'I'll" ~ I: I , ~
of limit irl, 1, F. T1,11(), I Y I III III IIrl-110 lilt_'/ p, 1"1!
V~i I ti (I rlfonh. 11 1("l I,.%. I ! c !1111 1'( 1 1. ,
I A,, ilk ili%~N

A.,i I I n Env i-Fyf r C rr. c-,' i,1 r
in every case, be e-%q resoed ty the e,~- -3-, iAl~ ~i
by a simila,~- eountion of the same tyl e. The activ,~te~
state of atoms in each of these pr,,cesses is
identical: it reprebents the limiti-4-, critical state -f
thermal instability in the crystal. In Farti.:,iiar
this state corresponds to that which is chara:terlsti: ~f
a transition from the soiid to the iiq-)id state, or of a
solid state transformation of the cL---),0 type, where
a and 0 are the low a-nd high-temperatu2e mcdifi.LatioaEz.
The critical state of elastic stabilJty car, aisD rep-resent
the activated state. Dependir-g on the coaeitioni~,, ali
these cases of activated state may 9xist separateiy cr
jointly. The limiting state of thermodyaamical ~Jrstability
of the activated group of ELtoms may be z~aueed bv the acti (: n
of various factors such as tLermai fiu--tua-..on-9, appiie(~
stresses or various types of radiaticn. 1n any given
metal, the quantity q is hardly affected by the ;Fi.-'.!4tion
of the external factors governinj.~ the course of trie studied
phenomenon and it appears to be a link conzic-ctink,
different phenomenn tind rofloctln~T, thp i(iont-i* -I 11-~
nature of [ACtIvAlorl (-)I WIF)f3e AI; lt~#' (I"r!*(- "r,cfl,
Car(13/0 in the viiiiieti of tlie activ!it'lull oilrr-~r'y 'A'taIrif~d

A
f
I
I

y
F ~P,lircn I, ti I I d
a I UMi 111 UM H 0 It f U I 1" 11 f t IIe tA 1) 1'
the tpmper ;At ure (Rof 51) IR a 1 1 t!'eso :,I r, al a
(D v a 1 u e o f Ali I V 0 T'y TW ~1 T' ()r P -1 1 1 N I T, ( ~ t, t . C,

A, I I v!1 I 111 1" 1 it, i
it
IY
I b j1 LI c) ~j u It. t- dhy t. t
o f defo rinti Iuri I n c ro, o 1) ii, ned
Ellie rby c t i i1 Liol t. t , I, I ii, It 1, T I
Kfited tc ml , 4, r e r c ri I

A I , - .. I , 1, , , , I I . . I . I I
A - -- 1, 1 A I I i I i . . I I - , , ... . . . I !% I 1 1. 1 1
I . I ~ I . . I . .
I . I I
. I - ~, .. , ., ,

18(7)
..M:OR K. A.
y of F r- litJon of Vpic~u--,, r
TITLE: uln
~,'et rl (0 iyFi v-t)- -ir r, i y vvf- r,
PEli I AL D k y A ~i
A'-~STRACT: "any acknowled,-P~l the imi~ )rt,-.:.t ir~flr
t v -n on
r- t lll~ E E df.r~ te!l t',,, act -t
an c r,-.y o:' vol,i-.e nplffliffui~-.or rl d d i f f,
r,- of twit, I' r-,;ltior of V%-11"cit.r.E

t 1
h, i r, t c 0 1, 1 e r e d a 7,, re jl-e:,eral iii,ii,ti ty, t:.'! t
i s as t ~-x r t I v t i or. e:,e r,- . - , f-
o f t h e a p i~, -ri!.r - f
of t.,.ermodyvamic ity (Or as "Cf-f,terr, 'If
11 o f-, ; e c i a Im tiel was a.,it~ui,,i(~d 71 ~('
f D r t , e 9 o c e r i t t - r 9 . I
Val -1e s of q cal cula ted accord inE, to the rtbove me!, t , , r~- I
expression, aril also come vaiiies of the f-,o-ca~ I o d e T- e r -y
of "hole formation" (found by various methods for t..e
experi!nental invest igrati on of 5 met E, 1 .9 ) are gi ver, i r i
tai,l o. According to this table, the results of U'-s i,n: -r
and of some previous paprr3 on tt,is aul ,Qct otv;w v(lry
good aFreement. F--)r mQtals ;Yith polymori hous conv;~rLiio~,.,i,
the cotice-ti on of the cc-titers of t ~(,rmod
t Y t 1i t y
may be Feneralized for the cane ti at the rtate in
centers correspot, ds to t~ie t2on of a I
mol i f i c,t t i on into an )t:,t-r high-temporntiire
T:.e valuo q 0 f t h o i, - # I v% t I o ii o n f, r ry -, r r~ ~ it p) r, d n t
this state. T:, author found t~,.e values 11-01, 1 1, ~-,
11162 lkal.mol- for the a-mod lfic-~tions )f ir)r., t-,t-i, 7_
Card 2/3 and ei,tiv. I.,/. The :iwt:~or tnor rot r~iq t,,

I ~ . I . .1 .
1 1. , 1: . 1'.:
S L, lj.,: I . 'l, E")
I . I .
it ~ , - 1 1. 1
A I z ~ ; I, I , ""~
. I
m . . . . I I . .% I I . I
1 1 ., ~ . I . lil I I , - . " . " , -, I I ~
Card 5/ 3

IB(O)
AUTHOR 08 1! Ov, Y.
TITLE: Ie Values of
Liquid ..etala 10
v zhidkik-h 1.'etallakh,
PERIODICAL: Dc)klil,,, i,kndernii
I ussfi )
tne ;,ctivation Enerry of Selfliff~;~-,iozi ~n
-,:,,-.tc1icniyakh ener",ii klivatsii P,
nauk SSSR, 1 ,',f3, Vol 1 -1 y 1 1 2
ABSTRACT: Accordin,-, to a 1 rpvioug ,;,, er L,, tlie sn;ae aut:,ur
values of t~ie ctivation ener,-,v of the vol~.ime .:01 f ~on
F in 101 id me ta Is (w~Ach were le hi -ed f!- cj,,, e e x p, rI. en. I;
ent.9 of tile qelfd~ f fition -~oef f ic i~-nts~
In t
'IV
f

SOV " o - I ~, I -, - I i , ,,
On the Value-3 of t~e ctivat4or Enerr.-y of Self diffus i4on in Let-c
which (,ccur it) ooli] metalo. i'lle e.i,0.rimVFA"t: 1!1 tb'~
t, o :i v;~ i la b I p ; e r:- i t t h e f ul i c, wi ng - Dric I ufi i on vii : -at, ~3
tho activation onor~,,,, oil t~iv tlolf-diffii,iion ff
lijuid rietala near meltiti~-, point have to ,intinf tho o,ilmtlon
'q - L where L denotes the latent lent of fllgior~.
I iquid
A tl,')le -ives the v,ilues ct-lculated by moans of thin! equati,~r,
for o elements . According to the data of t is pi -,er, t~.e
rzethol c!' vioco.,3ity it, no cacti I,ermitg a jro,~Pr leter-minat
of L :1 liquid , F,) iI r o Y, , j n, 1 41 r o n - c a r b o n a 11 oy s , *. I-. - r, c- t ~, o I
of viscosity ~-,nd t~.(! metAd of the raiionctive isato-,ei-, -- v.?
equal vh,.Ues of .~atiirrAlly, the ubove-Jis-i;,5~ea
e,:,,erJ,r,entaI dzAa are 4nguffir--ient for tI.e aj:flic,~tion
equati on L 'I q', i L for any
equations 6H - nq and L 11 liquid ' q - L the ronci,lisi-)n
be drawn that the celf-diffuqion in licuil metaii
frog.-. t!.e self-liffut3ion in sclil rittals) is conj,-cted wit,.
an inlividual fictiv-Ition (t,nd not with It 70"11 ;!Ctiv---
Card 2,' of e ;i t or:i3 . There are I f i r-., re , I ta ~11 p , an I I I -,e C

. I . . .
.. I , " , , ..
. . I ! . , ~ I , 1. .1 1 . ( ')~, 1 1 1 ( . I -
,, ,, . 11 1 . i , i .. I .
1 .1 ' A ' ' 11 1 1 . , I. I , 1 1, 1 .. I , , , . I , , , , ,~ I . 11 .. ~ I I I I . , '' I . . h
I I .. ,t L , ,t , . I I. " I " I I . . , y I "', I A . f. . , a - - v , f, ~ 1 :1:111
ITE")LIITED: d'i ' I. iI I I ' 1 ~~; t 1 0 " Y I - ) - - I'll '.A 111 , " li I etP, i - i a n
TIBLIITTIED: 1 ,, 1) "t,
Card 3/3

I ul =14.T-T:
po" 701-d0 ~l ;IV
.1.
s,4-
A=V" W" ;o UC-.
COT
jo f~.qv it
Aq
it -I-- ~.ll
al Uto
X-mv u?-V ;c "-y
PUTI"Imov .1 r-~ .-m-4 V~-
21 IIT-.r it 1~. -,7=
Lq rTm s,41
Zel ftll"o ftil-cat: it
-6v~y T *,4;V4.
---Wj
I'm
.7-4
.07
it
J.j
66 -.Z"
it -ouv~os-v Uft-.i:
it
~,~Ttrv4:- I
Oul it
tvrTVWmqom 30 6612j.dc-Ld
W ..T.Ivv
"V.Mtvw TUT.Tw--..c J-j SIM
.2 T,
iy-mu~ lt~ -
Q~ ~.v
rv, 81"4
p"u3s"d
T'm
UT pOftft* 10=02Jd rVOMZ4n jC; I,
joad egopueTvb Tv2TUWX*lL it atsom 'mm
"0900
.29-41"s *d CRT "6-;,fT
uvjjdvv it Tvp PUS
In j. Lun-V
it guoI%:Vvvs.Ll)
*ZTq%u&js;-
*xTu.p .. W-.-Wft --..Xmw
.zv,L,.o"JZX r-
xv

180) PHASE I ~MK EXIWITATION WV12103
Tsentmllnyy nauchno-Issledovatel'Gkiy iriwitut tekhnologil i mashinostroyQrAya
StrluktuM I evoystva zharoprochr,ykh materialov; (sbornik] (Structure and Prop-
erties of Heat-resisting Materialsj Collection of Articles) Moscow, M%shgiz,
1959. (Series: Its: [Trudy] kn. 93) Errata slip inserted. 4,000 copies
printed.
Additional Sponsoring Agencies: USSR. Gosudarstvennayn plaiiovaya komiesiya and
Glavnoye upravleniye nauchno-Issledovatellskikh t proyektnykh rrga,ilzatsiy.
Ed.: Z.N. Petropavlovskaya, Caadidate of Tecibitcal Scienseq; Ed. of Publishing
House: N.A. r-n--tova; Tech. Ed.: A. F. Uvarove,; Managing Ed. for Literature on
M&tal Working Fad Tool Making: R. D. 11eyzellman.
FURMSE: This cook is intended for workers of scientific research institutes and
for engineering staffs of plp-nt laboratories of the boiler and turbine
industries and power stations. It may also be useful to staff members of
hig:r.er educational institutions studying problems of physical metallurgy.
Card .119

Rd
.r,d,,, ...1; d
V &A.Ye., Co rr$.P-dl~4 Mest,.r, M's" A d..; of
1" 11, 1 031~A. 1, fl~ ravlov, NO I P Zudin, Cardidato
31c...
MR ?U~ E ,Thle book to Intended for we t*llurgtets concerned with
th. tr.ct.-I of alloy.
COWRAOR. This Is & collection Of Opecialit.8 ,tudI,9 of various
~rohle�O 1~ the Otructurtl PlIallurgy of h~mt-rasiblant alloy*.
0" or* eoncornvil 0 1in in* Or~t!.,6Icpr1Pc1PI.a. am* sit h6 0, -
cripti-a of now equIp-oM .hl h a, othero with propertleD
or owlete wo t.rials. VmrtOuD patenomena " eurrt~g under
Poll"" Cold'":
no am O1u:1vd,8n,1 r:,.rtO on. For details,
New b,. f 0 1
'tO 0 C n n to rtI ION 4. seco.Varldl by a num-
bar or reforom caa, bot h Soviet and non-3ovlot.
TA" ON COXTENTS,
001mg, 1. A p T. 3. IvAnove, 6nd Tu. P, Ltb*rov. Role of the
Surface Of Separation In Creep-rupture palluro Of MotAlO 3
twividankov. P. 1. On One Contradletion In the Theory of Cold
I
13
C21?,a:.,JL..A,_0iLth9 Diffuston and Ust PlealotAftee Of metal
PI
-ftylov, V A It 'I Q4yd11kQ;. 0. 1. Pattwo, 0, 1, 4914.
gr oat- tr steurtw"i Pecullialrition
he, Behavior of mistale at slaw To"Oraturge
Card 2/11
77

VOL, Abran Yevgen'yevich; A(ZTNV, N.V.. red.; ABRIKOSOV, N.Kh.. doktor
tekhrl.nauk. red.; KORNILOV, I.I.. red.; SAVITSKIY. Te.M., red.;
0.5jFQY,-X.A.. doktor tekhn.nauk, red.; GUMA, L.JW.. kand.khim.
nauk. red.; MIRGALOVSLATA, H.S., kand.khim.nauk. red.; S1Da,0V-
SKATA, 1.7u.. red.; MURA:kiOVA, N.Ta., telchn.red.
[structure and properties of binary metal systems] Stroenie i avoistva
dvoinykh metallicheakikh niatem. Pod rukovodatvom N.V.Ageeva. Moskva.
11on.jad-vo fi21ko-irvitom.11t-ry. Vol.l. (Physicochomical properties of
not.lidim. nlmnimim. imnriotim. hnrtim. bnryllhim,
.... .. 1f% Ott- 1-1,11 -1 -1-t- In V " 1 0 1 0 1 " lww 11 1 4, V n "IV
I list 1... 6 '1 1 1 1 Im I I I I I I .. I I .
1. Gill nit-korrn Ilpfill-if, fit All :;:I:;1( (r,,r Ajnvt,v).
(YetA18) (Plinne nila and equilibrium)

SOV/180-59-3-L'7/4-i
AUTHORS: Osipov, K.A. and Sotnichenko, A.L. (Moscow)
TITLE: Values of the Activation Energy of Creep and Fracture
for Aluminium During Tension
I;ERIODICAL:Izvestiya Akademii nauk SSSR, Otdeleniye teklinickkeskikh
nauk, Metallurgiya i toplivo, 1959, Nr 3, pp 139-141(USSR)
ABSTRACT: Previous work is briefly discussed. The present work
was carried out on 99.99% Al after rolling at- oom
temperature. Testing took place in vacuo (10 ~ MM fig)
and at temperatures of up to 550*C. The specimen was
80 itim lotig w1th a gnuge length of 22 min and diameter 3mm.
The results confirm the relationship:
x = voexp(,&HI/RT)
where T is time to fracture, 'to is a constant,
A111 is the activation energy of the process, and
R and T have the usual meanings. Fig I shows the straight
line graphs obtained for log tinie against inverse
temperature for different stresses. Fig 2 shows the
relationship between 4111 and the applied stress. The
ctirve im not linear and &III approaches a limiting value,
no -1 1 IV 1-1 lov-1 f- ho 7.,.! k cn)/R ntom (the theoretically

OSIPOV. K.A.
Diffusion and bent resistance of metal phases. IsBl.po zhuropr.
splav. 4:21-25 159. (MM 13:5)
(Hoat-resiatant alloys) (Diffusion)

'jo I ti t Iullb 1)YtI I t3
PERIODICALt Izvestiya Akademii nauk SSSR, Otdolenlye teklinicheskikh
nauk, Metallurgiya i toplivo, 1959, Nr 4, PP 77-81 (USSR)
ABSTRACT: Binary alloys of nickel with iron, chromium, vanadium,
titanium, molybdenum, tungsten and tantalum were made
from metals of high purity and heated in vacuo at 1150 to
1200*C for 40 to 48 hours. The hardness was determined on
polished samples using VIN-1 apparatus with a diamond
pyramid and a load of I kg at 850 and 1000*C for one to
twenty minutes. The diagonal M of the impression varied
with time W as followst
it U atb
where a and b depend on the alloy composition,
temperature and load. Fig 1 and 2 show typical curves
for the relation of d And t for NI-Mo and NI-W alloys.
Fig 3 shows the rolation of' (n) with alloy compositionj
a is the characteristic ptirameter for short-term hardness.
Card 1/2 Fig 4 shows the relation of rate of plastic deformation V

~6(6) SOV,120-128-2-1-7, r9
AUTHOR: Osipov, K. A.
TITLE: Structure and Enerry of Grain Boundaries in Metals
PER10DICAL: Doklady hkademii nauk SS3R, 1959, Vol 128, Nr 2, pis 284-287
(USSR)
All 1111 A ('T t )is, I has, r Y o r -1 1 1 --1 t I ii is H r n I t wno li-,wti I tin t t ho
.11fin I nilp I no,
defint-d a,~ fillowei A b
the energy per unit of area of the bounlary, tl the shear
modulus under the assumption of an elaatic-isotropic medium,
Card 1/3 b the Burgers vector, -) the Poisnon coefficient, 6 the an,-le

Structure and Ener(,-y of Grain Bourd'Lries in Metals SOV/20-129-2-17,59
of' disorientation or the tingle of' relative rotation of the
crystals which tire in contact with one ariother round the cum-
mnn axis in the boundary plane, A a parameter dependent 3n the
nonelastic enerLTy of' the center of dislocation. Theory restricts
the applicability 3f the above equation to the range of' small
angles of' disorientation (no more than 15 0 if h )~> b holds for
the distance h between the diolocatione, but also at relatively
large angles (25-300) (if h -,,b) this equation is in agree-
ment with experimental data. This agreement indicates that the
erroro partly cancel at large angles. R. Smolukhovskiy's dis-
location model (Ref 5) permits an explanation of this agree-
ment. With the help of metals with face-centered and cubic
Lody-centered lattice, the author demonstrates that the energ-y
at grain boundaries with large disorientation anCles as cal-
culated b~ the above equation agree, with respect to the quan-
tity, very accurately with the activation energy of --ortain
I.rocuasee in the crystals. These processes mean the development
of centers with extrouie thermodynamic Instability of the crystal
atoms or of centerv of "local melting" Otefs 6-10). Unaer the
ii-no annum-1 t,., ths, ;k~jth,,r, E ~-` I. ~1, 0 (1 - In 9' pr i F,

18(10 SOV/20-126-3-26/58
AUTHOR: Osi.Rqv_,__K. A.
TITLE: Grain Growth and Creep in Metals
eEJ11ODICAL: Doklady Akademii nauk SSSR, 1959, Vol 120, Nr 3, pp 521-1-551
(USSR)
A14STRACT: P. Feitham (Refs 1, 2) showed that isothermal grain growth
in recrystallized metals of - very high degree of purity mby
be defined by the equation D2_ D2 - K exp(-h H,/kT)I, where
0 0
D0 and D denote the average values of the initial and variable
diameter of tL- grains (measured at the instant t of isothermal
annealing). K denotes a parameter defined by the values of
atomic volumeo, lattice constant, and surface tension at
the grain boundaries. L H I denotes activation energy, k Boltz-
mann's constant, T the temperature in 0K. In pure metals# the
deformation E satisfies the equation F_ - 00 at high tem-
peratures vithin the unsteady range of the creep curve with
one rotation. 0 and n denote temperature-dependent constants,
t the period of isothermal creep. Thelbretical investigations
Card 1/3 in accordance with experiments yielded the relation

Grain Growth and Creep in Metals SOV/2o-128-3-26/58
0 - 00 exp(- AR./kT)sin h(va/kT), where Po denotes a constant,
AH2the creep activation energy, v the activated volume, 0 the
voltage applied during expansion. In a previous article (Ref 5)
the author showed that the maximum values E m of energy of the
grain boundaries (determined at great values of their disorienta-
tion) for metals with face-centered and cubic body-3entered
lattice may be defined by the formulae E m '~' 1.35 gr or
Em '~ pr , where p denotes the s:aear modulus at moderate tempera-
tures. Tn the same previous paper, the author proved the
existence of the relation E m -z q, where q denotes the limiting
energy of the occurrence of shifts within the crystal lattice.
The quantity q represents the activation energy of those proces-
ses in which centers of extreme thermodynamic instability are
formed in the crystal or in the metals without polymorphous
transformations of the center;i of "local melting". q is cal-
culated by the formula q a -T HTS- 112 80 (6-7 - 1n T )-8 *ICV
6 T 3 - 2900 5 296 O~
Carl 2/3 11TS_H2 ,, denotes the difference in heat content of !he solid

Grair. Growth and Creep in Metals SOV/2 -128-3-26/58
metal at the melting point T S t,nl standard temperature 2~_~'.lr0K;
S2980 denotes the entropy of the solid metal at the latter
temperature. LH 1 = LH 2 = E M *= q holds for metals of a high
degree of purity. The following experimental values of activa-
tion energy (in kcal-9-at-1) are obtained for lead: AH1 - 6.7
(Pb 99.9)99%) and AH 2 ' 7.7 (Pb 99.99~). The validity of the
above relations confirms the aunumption that with increaning
grain size and also with unsteady creep the activated atate
represen'j the state of maximum disorder in the crystal lattice
(or the state of "local flow", or the "origin of the transition
to melting" according to N. 11. Nachtrieb's terminology (Ref 11)).
The vacancies, which are 11centern of local melting", may form
activated sites within the lattice. There 'Ire 13 referanc !s,
of which are Soviet.
ASSOCIATION: Institut metallurgii im. A. A. Baykova Aksdemii nauk SSSR
(Institute of-Metallurgy imeni AO_ A. Baykov of the Academy of
Sciences, USSR)
PRESENTED: May 27, 1959, by I. P. Bardin, Academician
SUBMITTED: May 22, 1959
Card 3/3

FLWX I BWX MIMITATION SOV/3880
Osiyov., Kirill Afene3tyevicb
Voprosy teoril zharoprochnoett uetaUov I splavoy (Beat Resistance of Metals and
Alloys) Moscow, AN SM, 1960. 284 p. 3,500 copies printed.
Sponsoring Agency: Akadeziya nmik GM. Institut neteUurgli ineni A.A. Baykova.
Beep. Ed.: I.A. Oding, Correeyonding Menber, AcaLleny of Sciences MM;
Ed. .5f Pablishing Ho4se: G.B. Gorshkov; Tech. Ed.: Te.V. ftkuni.
PURPOSI: This book is intended for met&Uurgical engineers and scientific research
v-3rkere studying proble= of heat resistance of wtals and eLUoys.
COVIOLWXc Tho bcok doeLls vith thooretleiLl problems of heat roviaLower or WtIOP Cum
wital phases In various combinations. Atomic bondinav the distortion of the
rryvital lettlev, otrarturo of ^1loyv, r"l.fttton between the strongth and the
plAntiolty obararterlativo aji(g malting towl-wratut-a 4alwondanou of wohnMeeLl
-if swtai phIM004, lVDI"M11141311 Ifolweletel MrAl"14111 n1lel hent, I-00101all'",

65657
S/180/60/000/02/013/028
/Y ")SY 0 Elll/E135
AUTHORSs Ivanov, V.I., and Osipov, K.A,--(Moscow)
TITLEs Investigation of the Kinetics of Recrystallization of
Technically Pure Iron during Rapid Electric Heating
PERIODICAL: Izvestiya Akademii nauk SSSR,Otdelenlye tekhnicheskikh
nauk, Metallurgiya i toplivo, 1960,Nr 2, pp 87-92 (USSR)
ABSTRACT: The authors point out that recent investigations
(Refs 1-8) of the recrystallization of cold-worked metal
at high rates of heating have enabled recrystallization
ttmv f() ho roducod to fractions of a -,ocand.. But the
%,tif-IIIII'l (1Xj,1t4nt%(I(,nn (tlor!i 14, H) havo not botin
rIjIIII't'vIcId by !4dwitlillo (IXI,f,r1I(I,IlIt!t1
III !h(1
Wol-It tlm ntt[Iwl.:i (ItIlIc.1.11141 tholl IIIvt):)I,Ijf.1I1 It'll I I
recry:it,,i111;,nt1on )t1notic.) uIltiol.
iron (0.016% C, 0.1% Vill, 0.06% 31, 0.008% P, 0.01% 3)
in relation to heating rate,, Ring specimens, 50 mm in
diameter, and I mm wall thic,,kness. were machined from a
deep-drawn cup. During deformation and machirii 'ng the
Card specimens were carefully cooled and kept at below -.10 IDC
between operations. Heating In the experiments was in a
1/3 single-coll inductor at 2500 c.p,s. and In a salt bath;

69657
8/180/60/000/02/013/028
E111/9135
Investigation of the Kinetics of Beerystallization of Technically
Pure Iron during Rapid Electric Heating
heating rates were 500 and 0.5 OC/sec respectively,
The temperature was measured with 0.08 mm diameter
chromel-alumel thermocouples welded to the specimen,
On reac:hing the required temperature the specimen was
kept at tI.At temperature ! 3 0C. Fig 1 shows a typic-al
ostAllograph, After the isothermal he:~lding the
specimen was quenched in watGr aftgr Induction heating
or in an air iet after salt-.bath Leating. Fig 2- shows
the logarithm of time of start of recrystallization as a
function of, annealing tGmperature in the salt-bath
(ouvio 1) and inductor 0-urve 2). In Fig 3 the same
rolat lorn!ihlp~~. aro qhown for a hoatlng rato. of 500 o("'/_-e,i
r(,,. i t t' i'(it,ont imik t.ir nit t vic, r, t rj itornp(trinp, itt. 1#50 CIC
111111 1 ) I1111"i t ~ I))'
A

69657
S/180/60/000/02/013/028
Elll/E135
Investigation of the Kinetics of Recrystallization of Technically
Pure Iron during Rapid Electric Heating
fractions of a second of the time of start of
recrystallization nd a reduction In the activation
energy of the initial Stage from 5?.25 to 26.9 kcal/g
atom, The main cause of these changes is the
coexistence of the reversion and recrystallization in
time and temperature (a schematic representation Is
given In Fig 4 In terms of the relations illustrated
previously), Preliminary reversion can have a
Card different effe3t on recrystallization kinetics
depending on heating rate and annealing temperature.
3/3 There are 4 figures, 2- tables and 18 references, of
which 13 are Soviet, 2 English, 2 German and 1 Czech.
SUBEITTED: November 15, 1959