SCIENTIFIC ABSTRACT FR:MIASEK, M. TO:MGEBRISHVILI, I.M.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001033800035-6
• Release Decision: RIP
• Original Classification: U
• Document Page Count: 3
• Document Creation Date: November 2, 2016
• Sequence Number: 35
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTR

~, l4I,ASEK, M.
Tight binding method for white tin. Hul Ac Pol mat $ no.2:$9-93 '60.
(EEAI 9:12)
1. Institute of Physics, Polish Academy of $cience~;. Presented by
L.Infeld.
(Tin) (Crystal lattices)
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~bLAND~Solid State Physics -Solid State The~~ry. E
Crys~tallo~;raphy.
Abs Jour Ref ~~liur Fizika, No 11, 1959, 24$71
lluthor Miasek, Maria
I:lst : Warsaw University Poland
Title Ttie Application of tl~:e Ti~lit Bindi::C hietl:ac~ to the Txives-
tiG.atioil of E:1er(,y Bailds ii1 Hexa~;oiia.l Close-Packed Struc-
ture.
O:ri~ Pub Acta p~1ys. palor~,, 1958, 17, I~1o 6, 3'j1-387
Abstract : The author ca1c;,~l.ates the iute~mals eucuwit;ered i;~ the
expxessioil for the e:~er~;f of the sir.E;1.e-e~.E:ctro.~ spectrw~
oP liexa~onal close-packed structure in the tight-bii~dii7~
approxir.~atioii, as derived iia the preceding paper by the
author (Refera~t 7.nur Fizil~a, ]-958, No ;.~, X71}19). Aeco~uzt
is takea~ of paired i;:teraction not Duly between tho near-
est nei~'~bors, but also the iioxt to nearest nei~ibors kp
Cc~rcl l/l to the fourth order. -- K.P. Gurar
- 43 -
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POId-ND
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Ceatxal Labor+~-toxy a~ the Qa~ Industry (Ceutra;tne Laboacatoriea
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AN Gruz. SSR ;-1 yia. 3s5b5~-568 S '63. (MIRA 1;:7)
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~', aut~o~:~ calls ~rtis ~ ~,,.-~ior: of disloca ~io.t
'.~r";'.L"l;li ~-j-E' ~ Y,e~ ~'-L'c`3.::'r:`v O1 .v v `l.~e ;;~aC;rOSCOp=C
� ~~, ::lO.r y C~a.i1:�.C �l~ ~ r:~ it r, 'stic do or:ad~tion � 1 .~ ~ ~ yoo ``
i `'s r~re....,.,:1 rla.,~ ply. r on oi' isloc~.,,:~on ~ ,
~~~ tcie proceSS of to the :,oti
~.: m,- r uis,~lacci~~er~t due become yixed is equa..
de~or...~tiorl o- . - ~Jlhere ~hcy (~ ~' ~r~~
~ ~r So:~rC~3 to ~r.e points ~- ;;ne:~ trlc. width o~
pro::: ~ri~,_.. plastic ey;:ec ~.
in :..ao ytud~ to ~r~ secGndary .
-~
Ca.raA ~ ~
''~
~,fl
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~..
~,UTIi0R5
, 7'I~i'I~E:
PERIODICnL:
s/aa4 f~z,faca/t~~7/4a~/102
B1 b6~~181~
0. T., Dzhnnelidze~ R. B.
i~~ebryan, ~..~
~uestion~ concerning the crystallization of MoO~
Some i
17. 1962, S3 ~ ~.bstract
'tteferativnyy z'nurnal. Khimiyv. 86,. 19f0, 433437 '
17D199 (fir. `rbilissk'. un-ta,
`summary in Eng �~~ . .
large Mo03 single orystals
' for produging
TE}:`r: ;,i~: i,lioda are discussed, been found
The most efficient method haQ , ,
ro erties~ ~ timum sublimation
' witi~ semiconductiVe p puaa.�tz tube, for whioh the ap
to bo sublimation in a ~1 ' o uartz tube ~o ~
erntu~ce 850 C, inolif~ati.ori of tlg die in the
condition" wero. teralP orysl~~ ',
width 1 ~6 - 6'mm, thiokner~e ~,,
time 48 hl's� Tl~e dimennionsWaf~tmm,result rig
following ranges; length 15 J late trein'glat,lan�~ I..
IfAbstrE~oter~e nota: C~mP , ,,
..50 - 200 �
;,
1 "Cttrd 1~1 ... r. ~_..~e._w_..__.~-~..~~~. .. _ ...~. _ ,~ , .
_~..�.
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The Blocking of Dislocations on tYte Grain ~o~ande.r~t SO1J f ' 6 z-->~"2v 37~' !J
~, H
sha~aei the dependence of In ~ ~Ia on }~~ i'or t~~r.~ use i;s,]..~ ~ nv~~~,i ti,_
h
gated (Ha ~ change in microhardness of the top la,yer~ H~
microhardness of Lhe layer at a distance h from the su-�face)�
A tF~l~.le indicates the vt3.].ues f,or the ratio of di.sloc~:tio~t
I~
aens:tties ~~�- (I1o =dislocation density on the surfaces ~~m
m
di~~location density at a distance hm from the surfs.c ~~
The :following conclusions a.rP made: At the passage of dis~
locations through block and grain boundariesg their densit~r
decr~sasesa This decrease is marked by the coefficient a ~h:_ch
is ellual to the logarithm of the ratia between deformation
work and heat liberations The experimenta]. values fora 1Q~t
it seem iriprobable that the dis3.oc~ztions directly penetzat~~~
beyond the boundaries of mosaic blocks or grains The
disl.ocatiorts in the neip;hboring block originate by excif ation
of dislocation sources due to stress concentration, At
Card 2~3 condensation of 30~a0�Jo, the density of the checked
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,`a ~7)
AUTHOR: ~gebryang G:. I,
~~~i J "' J
TITLE: The Blocki n~; af. Dis:l.ecat~i.one on the Grain ~i~~zrc~'''y
)
(Blokirovka dislokatsl.Y na granitsc zern~r.

pERIpDICAL: r ~ ~ n i 1~~11~ �
Nauchny;,~e doklady "vysshey shkol n .+iE.t~lluxt~;ay' .,
qtr 2 q pp 2G7�~211 (US ]R)
ACT:
AB5TR Various disturbancw~t- of the ocatioil
ndo~ls~~~ the'` graf.r ~ ~~
l,1~
. K
.
s
atomsy inclusions, other disl 4
the mgtion of d:islocs.tians, The ~ner�;;; oz
t
o
bounclar~y~ resist
ises wit'n the approach of the dislc~cfstiun t{z
this resistance r
the obstacleo The p:cesent paper investigates the pcnEtra',:i~n
i
"
.r~e
.
of the ~rf~i n boundaries by dislocations - Thy p~:~lyc~ys taI
(iG o Zn I
l
Z
'
s
n
"
~' a A
pure metals and tl;e e.lloys Zn, Al, Cu; F
as wel'1 as zinc ~un~cry:~talsr ve7e
~ )
2
Q C q
C (0
F
.
y
,
~
~.~
ot~�brt~,8s and
Tile s.nn~s.1F~~. mf?ta1,s were I�;,~.a.a.y and pl~.st [call
stxgated~
ve
i
~
'~
,
n
Q
t
~ " a fine ;uttin nn ~~, tt.rrnzn~; lathe ,
deformed by det~zc.itng g
h oC ~;he
~
;
density of d~slocatinna; =tnd to{=ir ~han~~ ire ,h~; r}c~L,
the i~icronr~rdnes:z;; Aft~,r
metal, were determined by rneasurin~~
a th3.n layer was P1 cklea ~ a.nc!.
f hardness
t
,
o
each measu~�emen
the hardness of the uncovered layer was mes.sureda A diag~a.T.1
Card 1 ~3
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The Origin and Motion of :Dislocations in Nic~:el ;%GV~'~~~~`>j'�~'~'/j'
and in the Ni-Cr Alloy
In the alloy, the lattice
presenca of foreign atoms,
in pure nickel There are
which are Soviet.
of which :is much di ~torted by t~
this process is :Wore intense t
4 f igurF~; and 8 ref ex~ences y 5 0
ASSOCIATION: Tbiligskiy gosuds,rstvennyy un~,versi.tet (~~blis:i State
University
SUBMITTED:
Card 3/3
April 3, 1c'S8
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The ~Ox'igiri GriCI ~Oti.on /'." i`~:t~'r.~r�.t1Gri^ n itiC ... _- ~v'.r ~~ ~^ f;i~'~ t"
and in the 2di--Cr A11oy
phase tr�a.n5~'or:~l~~.tions~ eto�}, The pr^~ ~e:~t j,r.A;~,r .. -,~;;r~~"; ~~-ri .,~f�
invest~.g~~tic~n :.f thr> sccc~ndary p's au f;i.~ af:~'E c t i r~ ne harder:
ing of niccE~l s.nd :~. n~.cl:~:~i pchr' ~t~it~m ~.il5o;~ ~:fitt `~`- , 3 ~ I
~'~�43 ? Cr as wel~. ~s a 1..~~~ c~~ntPtit of ~,~. C rc? tr�?~e~ .,f 'rat-
The hardening was carried out at dif'fer�ent ';~:,.~p~~at;a:rF�^
(200800�) e Figures 2 and 3 snow the' deI-~end;;n,e c~z the
potent~.al on the hardening tempei'at3:uc:~ These ;,ur~e:.a are
characteristic for the or.gin of di:i~ooat:icns ~~~-co~.�aing Jc
Fe Ce Fr~,rk ~.nd '~Jo `.P~ Re~.d (Ref 3}, A secr>n,? sz;7~ies of
experiments oil the dependence of th~~ potenti~:~+i on thF
annealing temperature (F:Ig !~) conf'i~�mcd tr~`~ le~salto or~t~.i~u~d
by Ze Ido Clarebx~ough~ '+7_~ En ~Iargz=ears and G< 'T~ ;"lost (Refc- 7.8)
who found tha-~ the metastable dislocations in n,ck~1 disa;ypear
in 'the tempc3r~.t~xre i.ntex'~;~~.1 between X50 a,nd b~0~ ,^ that ;'i1e
jump in the curve of density ch~~.nge and the ~~J..mirt~tion o'
latent energy;yy observed at 2GUp3OO~' by t;h{~ ~i~ai,}:ur.i roentio ~e I y
is due to the dise.ppearanc::~ of vacanc;i~~~s,. Try Lhe nick~:~ (..~
chromiuum al:loy9 the dislceationc di.~nppo:~x� rra~:lrr~e.d~ bW~twEe �~
200 and ~50t>, The c~i.f mini;t:i,on o:f X-hc; mr~tr~,:�~tat;1.E� dzs:~ oc,n.t,~ any
Card '2~3 therefore dE~pc,:idsvery much on !;l�ic ~~ true tu.re o~:' l;he rsie t:z~l .
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AUTHOR: idgebryan ~ G a I ~ ._
The Orig.-n and Motion of Dislocations i.n ~i
tsli;~yv n~;l'~s1
loks
TITLE. s
.
lozniknoveniye i dvlzh~,na.y
NimCr Alloy (1
i v splave Ni-Cr}

Fl;RIODICAL: .~sh~=,y shl�:c,ly. ',~:ets.ll.~~r~,i.ys.Y 1 `~~9 ~~
Zdauchnyye doklady vY`
Nr 2 9 pp 2C)?_m20~ (US ~R)
ThQ method .3uggaated by the r~.ut}ior is b~tsr_:d c,n tkie foilowiri~,
e of nny
r
ABSTRACT: ..
n ~ earflnce ~~r~d da 9r~,p~~e~i.rr~.n
delib rations . At th , s.pp . �
efarmntf an
thrust d
)
.
disloca.tion~ the lattice- undr~rgoes a
tal shawfa mett3stable (check~;d
After cold ~+aorkingy the me
strip i3 cut atrt of the r~etns (e~,:g~ b;r nnneF..
be deter"n1rlc::d
due to plastic defarmFltion. This s~hi.ftir>.g can
otential dif
f the
tt
bc,
v
n
c
et
p
r r~~.
by the amount o
;
metu
the
g
ala
urrent
e of c
the two points at the pa$sag
gram of thE' experimer~ts.l p-.unto
cuit die
i
.
r
Figure 1 shouts the c
is termed by the author "seecndar~~ plastic
This phenomenon
c' Tt is only caused bar a. change in the density of
effect o
dislocn-tions but not by ather phen.omen3 (diff'usic;.1 pYOCe~se'~
Card 1/3
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]~B8X,1N~ _0. Y .
~eria~ental m~thod for 3ethrmining ~heSdSensil;y of clisl~tdlRA~11:7)
Soab. AiJ Druz. SSR ?.0 no. 2:151-15~
1~ Tbili~akiY goeudmrstvennyy un'iaersitet im. Stalia~a. prddsetavleno
chlenom-korresnondentam AN (Tr~lls~x~~~,)l~m~~+~khlizovvm.
(Met ~ p
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i ..rt -~sr7. r! ` it _ v~ r`i_.~ 't' ' ~ i I? ._ .,._
J.1 ii~l f;+~Je ~. (i1 � illti A~'T~l .X.~li 1. i.:{{ (.i.~. ~!�~.r l~~: l: ~~ .~ ~! i~ ~ (l :. ~.~~~'tr: ~+1
~. 4>y .~.`~+ I ~ "'''� ~ .C':.tl C~~ :~C~. s~?_v:: t . .~.tif' i" ~1 t ., ~..LC 'i , i_c ~ 1 -~'~. .:ti--
.- ~ ~--
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r4GEBRYAN, 0. I.
Determination of Penetration Depth of Plastic Dei'ormation by 13rinel~
Hardness Teat
Tr ~ 'bi ~ i sk. un-ta. 5~, ~-~'S~4, FF 47-53
.-rr-ax r
A formula sxpressing the p�nltration dsi~th of cold-working is der:ivsd�
p~z~,,,' (ho _ hl)/hl, whore .t"max is the maximum depth of penetratjan, h� and
the enetration depth of the hall in the hardness test of the .in.~tial xnd
h p
cold-worked specimen reapectj.vely. Experimental results carrjad out on Cu
and brass confirmed the validity of the formula. (RZh~'iz, Pda 5, 1955)
S0: Sum. No. 639, 2 Sep 55
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MGEBRYb1Q, O.I.; ~iDRONI&~SH.9IbT, E.D., chlen-koxraepondant.
feet of the compactness of dislocation on the pxoceas of creep. Soob.
$g ( 6:5)
AN Gruz.SSfi 23 no.8:45?-462 `52�
1 Tbilieakiy Gosudaratvennyy Uni~ersitet fa~eni Staiina (for 1~bryen}�
2, Alcademiya I~aiik Grux~.ngkoy SSR (for Andronikasl~vili).
(Creep of metals)
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r
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' 8 N r d Q ', `I 1{ ~ ~�' y, '~ r N �. M~ U i+ e i~ Q w C~
a ~ 0 a ~ M i~ 'l r< y w r, .i r i~ n a U
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