SCIENTIFIC ABSTRACT TYAPKIN, YU.D. - TYAPUNINA, N.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001757710012-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 31, 2001
• Sequence Number: 12
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

AucC23~lcj lp'.: A104034035
essential featuzm~s o
by thev structure were 5imilar to those observed Previously
the agIng of.Ni-Be and CU-Ba. Orig. art. has: 4 figuxes.
ASSOCLI.'10,N: None
SMMITIM: o&7ov63
SUB CODE: SS,ZIM
DATE ACQ: -20:,,aA
NO FW SOV: 004
ENCL: 00
OIRM: 004
CON; 2/2
0 w

TYAPUT, YL.D., -,I-nd Phyv--b'.f,.th -"ci - (di.--u)
ral study of.,,-.Cing of nickcl nlloys." Los, 19510. 15 pp (Glavnii-
,~royckt under Go.,,pl,,-.n USSR. ~;cnt.al Scia.;6~ of
Ilerrolls T',Jt,-LIlUrL--y). 1)0 colpicri. Biblio-r.,phy -t ,,,n(1 of t--,:t
0M,39-59) 101)

CC NRo AR6013666 SOURCE CODEI UR 0050 65 000 010/E031/031
-AUTHOR: Gavrilova, A. V.; Tyapkin, Yu. D.
TITLE: Changes in crystal structure with age hardening in ni-:Uel-beryllium and cop-
per-beryllium alloys
SOURCE: Ref. zh. Fizika, Abs. 10E241
REF SOURCE: Sb. tr. In-t metalloved. i fiz. metallov Tsentr. n.-i. in-ta chernoy
metallurgii, vyp. 36, 10,64, 326-354
tOPIC TAGS: hardness, strain hardening, beryllium containing alloy, metal aging
TRANSLATION: Be atoms collect into monatomic layers parallel to the crystallographic
planes of the (1001 matrix in the initiall hardening stages of Cu-Be (150-2000C) and
Ni-Be (400-4500C) (Guinier-Preston zones). When the Guinier-Preston zones combine
with the surrounding matrix, a mixing of atoms occurs in the matrix which..can be re-
presented as an elastic shift in the [3_103.planes in the [1101 direction. These shifts-
produce I'monoclinic" changes in the initial cubic lattice. A metastable phase occurs
.in the alloys when the time lag increases or the hardening temperature rises to 3000C
(for Cu-Be) and 5000C (for Ni-Be) due to an extension of the Guinier-Preston zone. The
sti7u~qtural relationship between the metastable phase and the solid solution is similar
io_.thatbetween ordered and unordered phases in the ordering of an AuCu alloy. The -N

ACc - NR,... AR601366
!1motoclinic" changes in the matrix with the aging of Ni-Be and Cu-Be alloys are do,-
to the character of the stress state in submicrovolumes of the alloy and to the ani-
sotropy of -the elastic constants of the cubic matrix. Large elastic distortions
(stresses) with the aging of Ni-Be and Cu-Be alloys do not considerable increase the
hardness. The hardness increases only at the stage at which these stresses begin a
turn in the blocks of the matrix solid solution. 30 references. I. Tulupova.
SUB CODE: 11

GAMMA)
irrvastiga-I.Ing t~,c qglr~g of martcmit~- I'll A ror-:11 P.] !,-Yi vlth,
additions of aluminLIM. FJZ. Mit, I MOVillOW-fle ,,,j
Ag 165. (,',I-iPA 18:'-))
1. TSentralinyy mw:hnc--issledovat--A1--kiy iristJl.,-,t chernoy metal-
lurgii imeni I.P.Bardime

L 1939-6 UIT(m)/t"WP(w)/T/E.IP(t)/tiiP(z)/EWP(b)/E.YA(C-) IJP(c) hU11 (CL)/JD/HU
'ACCESSION MR: AP5021946
UR/0126/65/020/002/0313/03W;
548-53
A
AUTHOR: Gavrilova, A. V.
,~,Tyapkin, Y u. D.
TITLE: Aging of martensite of iron-nickel alloys having aluminum additions
ISOURCE: Fizika metallov i metallovedeniye, v. 20, no. 2, 1965, 313-315
TOPIC TAGS: iron base alloy, nickel ontaining alloy, aluminum containing alloy.
~iron nickel aluminum alloy # marag ng alloy, maraging t I
ee
~ABSTRACT: Three iron-base alloys, contaigdng 8 'i_1. 5 Al, 29 Ni-2.0 Al, and 29 MY
!3.5 Al, were investigated in order to deA?rmine the mechanism of structural changes
responsible for the significant strengthl%i e under the effect of heat treatmend
th pcreas
!The specimens vere cooled to -1-916C ,and a&t , at 4oo-450C. Aging brought
!ataut precipitation of a secondary phase %aving a CaCl-type structure and a composi-
,tion close to (Fe, Hi)Al. This phase then decomposes in Wo phases: HiAl and a-Fe.
*In spite of the small change in volume, the decomposition causes significant streng:th-
,ening, Orig. art. has: 1 table. [WWI
iASSOCIATION: TsNIIChERKRTjm. I. P. Bardina

L 1939-wO
946
ACCESSION n: AP5021
!SUBMITTED: i3jul64
,No REP SOV: 007
ENCL: 00
OTHER: 001
J
SUB CODE: MM
ATD PRESS:
c 2 2

RABIN'KIN., A.U., 1YAl"KiN., Yu.f).:
..'ances in 'ne --hr
1'n-Pt alloy thtj or4ter pi-c1ce."o. v4, t 19
r-,j.)r360-3b6 Mr It,5. "PIRA 18--4)
t 7llial T1
,,a AN SSSR
-chno --~irrncy- :m-zallurg-1-i `~m'?m

JYMIKIN Yu.D.;
. - - - ;P
Modulated peen-odi c 5-1i7icture in !a - Ni - Al base alloys
with a body-centered cubic IaLtice. DokI. Ali S-SSR 160 no.2:325-
328 Ja 165. (HIPA IP:2)
1. TSentrallnyy Islily i-Y -titut chernoy me-
tallurgil. im. 1.11. &-irdina. Submitted July A 1~164.

IR

.t I I . .
.. - . - . - .1, 1
E -.

TYAPKIN, Yu.D.; YAMALEYEV, K.M.
. Character of crystal lattice defects at the initial stage of ordering
of a CoPt alloy. Dokl. AN SSSR 155 no.6sI310-1313 Ap 164,
(MIRA 17:4)
1. Predstavleno akademikom G.V.Kurdyumovym.

YAMALEYEV, K.M.,j~(APKIN,Yu.D.- .-
X-ray exandna t4 cn of structural :,hanges during 'he- cr`srinz z~l
- I
F
single crystals of the KiPt alloy. vi_z. met. i rzn~talloved. I-,
no.1t141-144 Ja 165. (MIRA 18:.",
1. In3titUt metallofiziki Minz;~Ilrmgo nnuc 1,.n-)- I s _q led ovq te I I.---
instituta chernoy metallurgic imeril Fardina.

- - . - 1 .1.: ~ ~l ~- 'T ; IzI. ~i ,.~ I .- - '- '- , .- - i
7~= -7=~
, - - . . Z~~
A- ---~ Z - I - e--a 'n -
n nnn-ri untig-f-edu-c- i
a i i ov a r-~, .1 - - ..-- . . I ..-

ACCESSION NR: AP4013329 S/0020/64/154/003/0578/0581
AUTHOR: Tyapkin, Yu. D.
TITLE: "Monoclinic" distortion of the cubic lattice during the
aging of Ni-Be and Cu-Be alloys
SOURCE: AN SSSR. Doklady*, V. 154, no.-3, 1964, 578-581
TOPIC TAGS: cubi:c lattice distortion, aging, Ni-Be alloy, Ci-Be
alloy, nickel berillium, copper berillium
1 kBSTRACT: In the investigation of the nature of the chnages
occurring in the crystal structure of the matrix, Guinier-Preston
zones appeared at the initial stage of aging Cu-Be and Ni-Be
alloys. After a five-hour tempering period at 200C single cry-
stals of Cu-2% Be specimens were submitted to X-ray analysis.
Length.and arrangement of diffusion rods along the planes and the
region of anomalous scattering were investigated. Some rods were
not centrosymmetrical. Submicroscopic berillium-depleted or en-
riched regions were identified. The period of the Be-depletion of
Card 1/2-

ACCESSION NR:
AP4013329
2
the matrix, readily determined from reflections with a large h
showed an excess of 0.5 to 1% over the mean period. At a later
stap of aging, the dislocation of atomic planes Lioij towards
U011by means of 'r causes the transformation of the cubic lattice
into a "monoolinic" lattice. The value of the dislocation is equal
i to a minimum of �50 which corresponds to r- 0.1. In aging Al-Cu
specimens Guinier-Preston zones are also identified. However, mono-:
clinic distortions were not observed. charac-1
The difference in the
ter of the matrix distortion in Al-Cu, Cu-Be and Ni-Be specimens was
due to different elastic properties of the solid solution. Orig.
art. has: 3 figures.
ASSOCIATION: Institut metallovedeniya I fiziki metallov Tsentrall
nogo nauchno-issledovatel'skogo instituta chernoy metallurgii
imeni I.P. Bardina. (Institute of Metallurgy and Physics of Metals
of the Central Research Institute of Ferrous.Metallurgy)
SUBMIr.111TED,
26ju163 DATE ACQ% 26Feb64, ENCL: 00.
SUB CODE: ME NO REP-SOV: .008 OTHER% 008
Card 2/2

TYAPKIN, Yu.D.; USIKOV, M.P.
Comparison of X-ray and electronographic data on the dimensions
of crystal blocks in deformed stainless steel and nickel.
Fiz. met. i metalloved. 14 no.1:85-91 JI 162. (MIRA 15:7)
1. Institut metallovedeniya i fiziki metallov TSentrallnogo
nauchno-isaledovatell.skogo instituta chernoy metallurgii.
(Steel, Stainleso-Metallography)
(Nickel-Hetall.ography)
(Electron microscopy)

SIMONOVICH) Ye. N.; TYAPKINA, N. P.
Handy modification of Fulleborn',s method. Red. Daraz. i paraz.
bol, no.6:677-680 161, tMi~i 15:6)
1. Iz parazitologicheskogo otdola (zav, A. G. Revzina) sanitarno-
epidemiologichesRoy stantaii (glavnyy vrach L. K. Sakharova)
Leningradskogo rayona Moskvy,
(HPININTHOLOGY) (FECES-ANALYSIS)

MARYAlBU19 yu.A.; TYAPKIN~ Yu.D-
.gthe effect of the ye, lomponent
'2Kris*a.Uograf i1a
simple device for elitinati ngle Crystals*
in reversal X-ray photographs Of si
6 no.5:774-775 S-0 161. (~MIRA 14.10)
1. Institut metallovedeni i fiziki metallov.
M
(Radlographyr (Crystals--Spectra)

S/126/62/014/001/007/018
Elli/E135
AUTHORS: Tyapktn, Yu.D., and Usikov, M.P.
TITLE: Comparison of X-ray and electron-diffractlon data on
the size of crystal blocks in deformed stainless
steel And nickel
PERIODICAL: Fizika metallov i metallovedeniye, v.14, no.1, 1962,
85-91
TEXT: In X-ray diffraction determinations of the size of
crystal blocks with the aid of analysis of the width or form of
interference lines the size referred to is that of "regions of
coherent L;catterlngff. The question arises as to whether this
characterises a dimension of the crystal structuxle or is associated
with an optical effect. To solve this problem the authors have
compared X-ray results with those of electron microdiffraction from
thin foils of the test samples, simultaneous electron-microscopic
investigation of these foils being carried out. The samples
studied were of an 18-8 type stainless steel and pure nickel,
subjecte*d to cold-rolling with 96% reduction combined with heat
treatment and, where appropriate, electrolytic thinning. Some
Card 1/2

Comparison of X-ray and .electron- S/126/62/ol4/001/007/ol8
Elll/E135
electron micros-copic pictures (generally at 15000 magnification)
were also obtained. The authors conclude that, allowing for
svstematic errors, the block-size determinations by electron-
and X-ray diffraction give practically the same values.. The
greatest difference is with nickel, probably because the foil
thickness could not be determined with sufficient accuracy. Thus,
for deformed stainless steel and pure nickel the dimensions of
coherent-scattering regions found from measurements of X-ray
interference-line width determination correspond to dimensions of
real crystal blocks having a relatively correct internal structure
and disorientated relative to each other.
There are 2 figures and 2 tables, '
ASSOCIATION: Institut metallovedeniya i fiziki metallov TsNIIChM
(Institute of Science of M4tals and Physics of
Metals, TsDiIIChM)
OUBMITTOD1 October la, 1961
Card 2/2

,.TYAPKIN, YU,D,; BAGARYATSKIY, Yu.A.; GAVRILOVA, A.V.
Study of changes in the crystalline structure (,f the alloy
nickel-beryllium at an early stage of aging. Kristallografila
6 no.4:560-567 Jl-Aa 161. (IMU 14:8)
Inatitut metallovedeniya i fiziki metaUov TSentrallnogo
nauchno-iseledovatellskogo inatituta chernoy metallurgii.
(Nickel-beryllium alloys)

12 ~-D J~Lo&, ILI 1(a Zgog
WO 0 WdO , //'f 2/ 11,:~'3)
AUTHORS: Tyapkin, Yu.D.,
25892
S/07o/6i/oo6/oc4/oo4/OO7
E021/E406
Bagaryatskiy, Yu.A. and Gavrilova, A.V.
TITLE- Study of the changes in crystal structure of nickel-
beryllium alloys in the early stages of ageing
PERIODICAL: Kristallograf iya, 1961, voi. 6, No. 4, PP - 560-567 + 3 Plates
TEXT: Single crystals of Ni-Be alloys containing 2.2% Be were
quenc~hed from 11000C and aged at 425 or 5000C. The change in
hardness (Rockwell B) with the total soaking time during tempering
(in minutes and hours) is shown in Fig.l. The alloys were
studied by X-ray analysis to elucidate the changes in structure.
In the early stages of ageing (30 min to 2 hours at 4259C) the
formation of Guinier-Preston zones considerably enriched in
beryllium occurs. They are in a plate-form of 1 to 2 atomic layers
thick and parallel to the (100) planes in the matrix. At the same
time all the solid solution is less-rich in beryllium and
approaches to the equilibrium state. The depleted matrix divides
Into separate blocks which at first have different orientations one
from another. The blocks are elastically distorted. There are
cracks with thickness of the order of 20 to 30 A in the matrix
Card 1/3

25892
S/07o/6i/oo6/oo4/oo4/o07
Study of the changes in crystal ... E02l/E4o6
along the (110) planes. At 500*C, the G.P. zones increase in size,
regions with structure close to P phase appear and orientated
rotation of the blocks occurs around one axis of the CILOO] type.
This rotation reaches 8 to 100 after 32 hours at 5000C. The high
hardness values of aged Ni-Be alloys is connected not with elastic
distortion in the matrix but, in the main, with the division of the
matrix into blocks and with their rotation relative to one another.
All the observed changes result from the large difference in
atomic volumes of the matrix and the precipitating phase (NiBe)
which reaches 20%. There are 10 figures and 22 references.
16 Soviet and 6 non-Soviet. The three references to English
language publications read as follows: M.Hansen, K.Anderko.
Constitution of Binary Alloys. 290. New York - London, 1958;
A.H.Geisler. Phase Transformation in Solids, 454. New York -
London, 1951; R.B.Nicholson, G.Thoma, J.Natting. J,Inst.Metals,
87, 12, 429, 1959.
ASSOCIATION: Institut metallovedeniya i fiziki metallov TsNIIChM
(Institute of Metals Science and Physics of Metals,
Card 2/3 TsNIIChM)

BAGARTATSKITO Yu.A.; TTAPKIN, Tti.D.
Supplementary structural data oft the decomposition of
supersaturated solid solutions of titanium in nickel
and nichrome. Kri-stallograMa 5 no. 6:882-890 N-D 160.
(MIRA 13-12)
1. Institut metallovedenlya i fiziki metallov OTSentrallnogo
nauabno-iseledovateliskogo instituta chernoy metallurgii.
(Chromium-titanium-nickel alloys)
(Titanium-nickel alloys)

6780-5
S/07o/60/005/oo6/003/009
E021/E306
AUTHORS:- Bagaryatskiyj Yu.A. and T zaQin'; Yu.D.
TITLED. Additional Structural Data on the Decomposition
of Supersaturated Solid Solutions of Titanium in
Nickel and Nichrome
PERIODICAL: Kristallografiya,'196o, Vol. 5, No.
pp. 882 - 890 + I plate
TEXT: A detailed study has been carried out of the crystal
structure of nickel-titanium and nickel-chromium-titanium
alloys during the decomposition of the supersaturated solid
solutions from the initial stage when the titanium distribution
is nonuniform, to the final stage when a hexagonal phase is
precipitated, The binary alloys containing 11.8 and 14.1 at.%
titanium and the ternary alloys containing 16.5 at.% chromium
and 8,5 at.% titanium were investigated by ageing at 700 and
8oo 0 C for various times. In the initial stage of
decomposition, microregions rich and poor in titanium were
formed, Both the titanium-rich and titanium-poor regions
Card 1/4

67805
S/07o/60/005/oo6/ow/009
E021/E3o6
Additional Structural Data on the Decomposition of Super-
saturated Solid Solutions of' Titanium in Niclc(~l and Nichi,om!,
could deviate from cubic symmetry and could become tctragonal,
the binary alloy containing 14 at.~4 titanium and in the
,-,rnary alloy, the titanium,-poor regions be-,~ame tetragonal
with a c/a ratio of 0.999 + 0.001, In the binary alloy
containing 12% titanium, tRe t�tanium-rich regions were
tetragonal with c/a = 1.003 + 0.001. Thus, the tetragonal
structure was not caused by metastable Ni 3Ti compound, as has
been proposed (Refs. 3; 7), When the precipitate of the
hexagonal q-phase Ni 3Ti first appears, the regions of bcth
types became tetragonal with the above axial ratios, The
c-axes of all the regions were in the same direction so that
the initial monocrystal as a whole appeared to be tetragonal,
As precipitation of' the hexagonal phase occurred,
recrystallisation of the ,gions poor in titanium also o1ccurred,
which resulted in part or the whole of the monocrystal becoming
Ca.id 2/4

67W
S/07o/60/005/oo6/oo3/ooq
E021/E306
Additional Structural Data on the Decomposition of Super-
saturated Solid Solutions of Titanium in Nickel and Nichrome
polycrystalline. Afte- several thousand hours the binary
alloy with 14% titaniu.; remained monocrystalline but, the
ternary alloy did not. The transformation to a polycrystal
did not occur for the ternary alloy at 850 'C.
Recrystallisation was explained by stresses arising in the
monocrystal.
Acknowledgments are made to B.A. Mellnikov for his assistance
in the experimental part of this work.
There are 5 figures, 1 table and 20 references; 10 Soviet
and 10 non-Soviet.
Card 3/4

S/07o/60/005/oo6/oo3/ooq
E021/E3o6
Additional Structural Data on the Decomposition of Super-
saturated Solid Solutions of Titanium in Nickel and Nichrome
ASSOCIATION,a Institut metallovedeniya i fiziki metallov
TsNIlCh?-,, (Institute of' Metallurgy ind
Physics of Metals oF Ts'NtlChjNj) \X~
SUBMITTLD. April 19, 1960
Card 4/4

BAGARYATSKIY, Yu.A.; ITYAPKIN. Yu.D.
More on X-ray diagrams vith gatellites. Kristallografiia 5 no.4:
535-539 JI-Ag 160. (MIU 13:9)
S 1. Institut metallovedeniya I fixiki metallov TSentrallnogo nauchno-
istledovatellskogo institut chernoy metallurgii.
(Solutions, Solid-spectra) (Alloya-Spectra)

TYAKWINA. N.A.; k2EDVODITZUV, A.A.
Investigations of spiral etching figures in cadmium polycrystals.
Izv. Ali SSSR. ber. fiz. 22 no.10:184-189 0 158. (MUU 12:3)
I.Mookovskly gosudarstvennyy universitste im. M.V. Lomonosova.
k0admium-Atching)

- ------------------------------------ -------------------- .- -----------
USSR/Statis ical Physics - H~at D-4
Abs Jour : Referat Zhur - Fizika, No 5, 1957, 11455
Author : Mikryukov, V.Ye.i,,Tyapunina,
Inst : Moscow State University, USSR
Title : Investigation of the Temperature Dependence of Heat Conduc-
tion, Electric Conductivity, and Specific Heat of Bi and
Pb in a System of Bi-Fb Alloys.
Orig Puz : Fiz. metallov i metallovedenuye, 1956, 3, No 1, 31-41
Abstract : The heat conduction X and the electric conductivity XL-
were measured by the Kohlrausch method by means of a setup,
described earlier by one of the authors (Midryukov, V.Ye.
uch. zap mm, 1944, No 74, Vestn. MGU, 1949, No 3). The
use of a balanced method for the measurement of the elec,2.
tric quantities made it possible to bring the accuracy of
measurement of X to 3%,. and that of x to 1%. Alloys of
Card 1/3

USSR/Statistical Physics - Heat D-4
Abs Jour Ref Zhur - Fizika, No 5, 1957, 11455
22 different concentrations were investigated at temperqtu-
res to 2420. The alloys with a lead concentration up to
33.67% have (at various temperature ranges for various con-
centrations) a positive temperature coefficient at a value
of ;,Lless than that of pure bismuth. These phenomena are
explained by the presence of a solid solution of lead in
the bismuth, and obviously, by the presence of an o,% phase.
The dependence of N on the temperature differs from the
dependence of ~C on the temperature, this being explained
by the heat transfer not only the electrons, but also by
the lattice. Assuming that for the electronic portion of
the conduction the Wiedemann-Franz law is valid, the au-
thors have subdivided the obtained values of ;~ into A ell
vhich in pure metals diminishes, and increases in alloys,
an0lat, 'which always diminishes with increasing tempera-
ture. However, this separation leads to the conclusions
that A lat predominates over A ell and consequently
Card 2/3

USSR/Statistical Physics - Heat D-4
Abs Jour Ref Zhur - Fizika, No 5, J-957, 11455
doubt is expressed concerning the applicability of the
Wiedemann-Franz law for this system. The experimental
values of are in good agreement with the equation
>-%IC - A � B/T, where A and B are constants, C is the
atomic heat capacity, T the absolute temperature. C was
measured by the method of cooling in a Torovskiy-Bartenev
type setup. A slow increase in C of lead and bismuth with
increasing temperature was obtained. The isotherm of C
has a minimum at 4.82% and a maximum at 65.70~ lead.
This can be explained by the influence of the V~, phase for
small concentrations of lead and of the P phase for large
concentrations of lead (C of the ck, phase is smaller than
C of lead and bismuth, and that of the F phase is greater.)
Card 3/3

MIKEIYUKOV, V.Ye.-, TY-APUNINA CHERPAKOV, V.P.
Thermal and electric conductivities of biamth-cadmium 811075.
Vest.Hook.un.Ser.mat.,mekh.,astron%,fiz.,khim.11 no.1:127-136 156
(KIRA 10:12)
1. Xafedra molekulyarnoy fiziki MoskovBkogo universiteta.
(Heat--Conduction) (Bismuth-cadmii;n alloys--Electric properties)

!-ACC-NRI-' AP6036999-----
SIon, C-E C.O~t: --~R/0181/66/coo/oll/34112/3444'
ORG: Moscow State University im. M. V. Lomonosov (Moskovskiy go&udarz'#,vehnyy univer-
J' sitet)
TITLE: Electric properties of p-type germanium strongly doped with beryllium
SOURCE: rizilm tverdogo tela, v. 8, no. 11, 1966, 3442-3444
IOPIC TAGS. germanium semiconductor, beryllium, impurity level, ionization, carrier-
T
density, impurity center, Hall effect, temperature dependence
ABST.UCT: This i7s a continuation of earlier investigations of the propei-ties of
beryl I ium.-doped germanium (r.TT v. 6, 2193, 1964, and earlier). The present investi-
gation was aimed at determining the influence of the.compensating impurity on the
ionization energy of the impurity conductivi-kity of the upper acceptor level (for non-
hydrogenlike centers). To this end, temperature measurements were made of the car-
rier density and the electric conductivity in the temperature faterval 300 - 55K.
The procedure far obtaining the samples and of the temperature measurements was de-
scribed in the earlier paper. The results show that for most samples the carrier
density depends exponentially on the reciprocal temperature. The ionization energy.
of these samples at higher temperatures is calculated and the values are listed in
a table. An ana3.ysis of the temperature dependence of the Hall mobility has shown I
that-,at-low.temperatures scattering of the carriers by charge centers predominates.
.Card-

ACC NRt AP6036999
The densities of the beryllium and of the phosphorus calculated from there data are
also listed. In spite of the fact that the ionization energies were obtained for
samples with different acceptor densities, the dependence of the ionization energy
of the impurity conductivity on the concentration of the donor impurity agrees well
with the standard theoretical formula. It is proposed on this basis that. the change
of the ionization energy occurring with increasing donor density is due to the action
of the negatively sing2y-charged acceptors. At higher temperatures~ the ionization
energy is a'function,of the temperature, this being due,-to a reduction in the screen-
ing of the acceptors. The author thanks V. S. Vavilov,.N. A. Penin, and V. V. Ostro-
borodova for a discussion of the results. Orig. art. has:' 2 figures, 1 formula, andl
I table.
SUB CODE: 20/ SUBM DATE-.,',.3OMay66/ ORIC4i REP: 0051 OTH MF: 003

KUROVA, I.A.; KALASHNIKOV, S.G.; TYAPKINA, N.D.
Kinetics of extrinsic photoconductivity in n-ger-,qnii,- with gold.
Fiz. tver. tela 4 no.631,503-1509 Je 162. (MM 160)
1. Moskovskiy gosudarstvennyy universitet imeni M.V.Lomonosova.
(Germanium) (Gold) (Photoconductivity)

.,-c curren c wCn
a nunber Of mlnl-ma
-qQ Or ljv-.,-

S/18 62/C04/006/019/051
gJ77 0 0 B10 4XBI 12
AUTHORS: Kurova, 1. A., Kalashnikov, S. G., and Tyapkina, V. D.-_
TITLE: The kinetics of impurity conduction in Au-doped n-type
germanium
PERIODICALi Fizika tverdogo tela, v- 4, no. 6, 1962, 1503 - 1509
TEXT: The trapping of electrons on the E 4 level of gold in Au-doped
n-type germanium was investigated at hydrogen temperature. The
photoconduction of single-crystal specimens was determined in a He
cryostat evacuated to -10-2 mm, Hg. The heat emission of a crucible furnace
was filtered through Ge and Sb-In filters. The damping periods of the
photoconduction of the specimens were measured for two different directionW
of current passage. If the contacts of the samples are_of,high qualityp
the damping of photocanduction can be described by exp( t/,'~). The
c;_efficients--O of electron trapping on the E level of gold were-
n 4 1
determined from measured values of'-,., using the relation
Card 11.W

S/181/62/004/006/019/051
The kinetics of... B104/B112
(Table), where N3 is the dark concentration of Au~ ions. The temperature
dependence of the trapping cross section is described by s*exp(-F,/kT),
where E is the activation energy. The dependence of'~on T increases
with increasing Sb content. This confirms the authors' conclusions
as to the effect of electron adhesion to Sb ions. The temperature
dependence of the trapping cross section shows no signs of a strong,
influence of the potential barrier around the centers upon the trapping
processes. There are 5 figures and I table.
ASSOCIATION: bloakovskiy gosudarstvennyy universitet im. M. V. Lomonosova
(Moscow State University imeni M. V.' Lomonosov)
SUBMITTED: January 25, 1962'
Card 2/1

UROVIL, I.A.; TYAPI'llLi Y.D.
corctc--.,~4- rif containing littit-I i--
t I Ow tc, ;.- 1; a Y- t, z, 0F." zo tv,;r tala 3 no . 12 Olr(-.31C~ L'C
1- FfLiclloWdY f .11,11tat 11 o~;kovskop LgoordarstvennoCo vrivr,-rr,,
properties)

ACCESSION NR: AP4041733 S/0161/64/006/007/2192/2194
AUTHORSt Tyapkina, N.D.; Krivopolenova, M.*M.; Vavilov, V. S.
,.TITLE: Electric properties of beryllium doped p-type germanium
SOURCE: Fizika tverdogo tela, v. 6, no. 7, 1964, 2192-2194
1TOPIC TAGS: germanium, beryllium, electric conductivity, carrier
density, temperature dependence
!ABSTRACT: In order to determine the upper acceptor energy level of
;'beryllium in compensated and higher-resistivity-,germanium specimens,.
Ithe authors measured the temperature dependence of the carrier den-
isity-and of the electric conductivity of doped-germanium plates 2 x,
:x 3 x 15 mm in the temperature range 300--55K. The compensating im-
:purity was phosphorus. The plates were cut from the ingot perpen-
" '4
tdicular to the (1111 crystal growth axis. The measurements were
~mZe in a double metallic cryostat. A null method was used with a
C.,
d
.1/4

ACCESSION NR: AP4041733
'high-resistance potentiometer. The magnetic field reached 4600 Oe.
-Eight samples from four ingots were tested. The results show that
in all samples the carrier density is exponential in the reciprocal
temperature. The ionization energy was determined from the slope of
)3/2 103
1plots of 1n(pT against /T, and its value (0.064 � 0.003 eV)
iis close to that obtained by others and also close to that calcula-
Ition by the "helium" model, which is thus shown to be applicable to
beryllium in germanium. Orig. art. hass I figure and 1 table.
ASSOCIATION: MOBkovskiy gosudarstvenny*y universitet im. M. V.
Lomonosova (Moscow Statcuniversity)
,SUBMITTEDs- l3Feb64
3SUB CODE: SS, EC NR REP SOVt 002
C?~~ ..2/4 -
EVCLs 02
OTHER: 004

ar-LALMM v M ;MN rid . . . . . . . . .
ACCESSION NRs AP4041733 ENCLOSUREs 01
P,
lots
Dependence of carrier density on
the tempamture for different
samples
Sam

.i:ar .3/4 F

0 6.0 Lot
fag. W Me NO 1&0
AO T 'K
ACCESSIM NR s A4041733 ENGWSUPJS 02
Values of ionization energy in the
investigated samples

.1 .2 3 4

T

W
I
I L
.-
32 t
157(2) 0.8 1.4 , 1.7S 0.064
1691 1) 0.83 1.5 1.81 0.064
1691 5) 0.75 0.9 1.20 0.063
184 5) 1.2 .
1.4 1.17 0.064
181(6) 6.8 8.4 124 0.064

1 - sample no.. 2w- beryllim density in -5 -3
10 an 8 - phosg~iorus density
4 - ionization energy, eV

---------------------- -----

ow
EM6
q,4t3oo
2 Li -7 -7 00
AUTHORS: Kurova, I. A. and Tyapkina, N. D,
S11-5 1/60/002/0 1210 6/01.9
v
B006/BO63
TITLE: Electrical Conductivity of Lithium-doped Gprmanium at Lcw
Temperatures
PERIODICAL: Fizika tverdogo tela, 1960, Vol. 2, No. 12, Pp. 3106-3109
TEXT: Germanium specimens containing impurities of elements of the
third and fifth groups have been studied repeatedly at the temperatures
of liquid helium (Refs. 1-9), but there are no data available on the
variations of ionization energy of lithium in germanium and on the electri-
cal conductivity of lithium-doped germanium at low temperatures, This
work was intended-go fill this gap. As Li in Ge has a diffusion coef-
ficient of D=1.10 cm2 /sec at 5000C, diffusion of Li into Ge at
elevated temperature is the best method of introducing lithium. The
germanium specimens were ground, etched, purified, and annealed in vauo
at 4900C for 4-8 hrs, depending on the size of the specimen. The annealing
was done with an Li-Fb alloy, from which Li diffused into Ge. Starting
materials were p-type and n-type germanium having a resistivity of
Card 1/3

A
87916
Electrical Conductivity of Lithium-doped 3/181/60/002/012/010'/018
Germanium at Low Temperatures B006/BO63
-50 ohm.cm. The specimens were cut perpendicularly to the growth ax's
11113 , and had a size of 3-4-15 mm. After the diffusion, the specimens
were ground anew and etched with boiline H202' Lj-Pb spots were left. a3
contacts. Lithium concentration varied from 2.3-1014 and 2.9-1015 cm-3i
resistivity at 3000K from 6.5 to 0.58 ohm.cm, and ionization energy from
9.3 to 9.4 kev. The Hall constant (R) and the variation of resi3tivity
under the action of a magnetic field were measured as well. This was done
in liquid helium; the temperature of the specimens was determined from the
saturation pressure. The measurements in the magnetic field were made a+
1200 oe; the electric field inside the specimens did not exceed 0.2 -.,/CM
and thus remained within the range of validity of Ohm's law. Th,~ curves
9 = f(I/t) and R = f(I/T) are reproduced here. They show that only
specimens with 6.5 and 4.45 ohm.cm and lithium ecncentrationo of
(2.3-3.9).1014CM-3 have regular (exponential) functio!Ls, wh~-reas
specimens with higher lithium concentrations und resi=" +
an anzmalous temperature dependence of ? and R, R(1/T) curves, for -xample,
have peaks. The authors thank S. G, Kalashnikov for dis-c-ass:.ons, and
A. 1. Shallnikov for puttine his laborat,.ry at th,~ir d..sro!j,-:,_I The-_-
Card 2/3

871 916
Electrical Conductivity of Lithium-d3ped
Germanium at Low Temperatures
. ! " t, ~ /(( 12 "0, VO ; 5
-a/ I /
B006/B063
2 figures, I table, and 23 references: 2 Soviet, 16 US, 1 Germun, I
1 French, 1 Canadian, and 1 Czechoslovakian..
ASSOCIATION: Fizicheskiy fakul'tet Moskovskogo universiteta (Division
of Physics of Moscow State University)
SUBMITTED: May 5, 1960
Card 3/3

TYA~~NA,. N..D.3 KRIVOPOLENOVA, M.M.; VA"111,OV, V.S.
Electric prspart~as of FgermariJum with !=Purity. F4-z. tver.
tela 6 no.7*2192-2194 JI 164. (Yji(A I-1:10)
1. Moskovskiy gosudarstvanny-y universitat imeni M.V.Iomonosova.
0

STURAK, N.X.; TYAPKINA, X.F.
Logaritmic ovarlay for determining the depth of occurence of
magnetized r9ak seams. Razved.i ohr.nedr 22 no-3:39-41 Mr 156.
(Prospecting-Geophysical methods) (MIRA 9:7)

BM4YA.N. E.G., inzh.; MOROZ, A.P,, inzh.; TYRYSIIKIN,, V.G.-, kand.takhn.nauk
Principal results of testing experimental and in-austrip-I GT-700-5 gas
turbine systems manufactured by the V.I.Lenin Neva Machinery Plant.
Energomashinostroenie 9 no.12:24-28 D '63. (MIRA 17: 1)

TYAPKINAp V. V. Cand. Chera. Sci.
Dissertation: "btructure of the Primary Layers on Silver and the
Mechanism of Their Formation." Inst of Physical Chemistry, Acad Sci
USSRp 5 May 47.
SO: Vechernyaya Moskva, i4ay, 1947 (Project #17836)

1 ".4 T P
Pei
4[
41 diver a d at WAUhM b"
on Taks. K. K!s=hJ.M. Ine a" Js**
P. D. Aw. 7
1341011= ft,". Cbto.V' V - 891U.S.W. 104111
So c ma"aw). y Ads N"A SASY it, 45-14 lot
(1948).-Blectrom Terms by
Sol a( 20-100-A. A# ==d In 0 high sea m as
unheated mks freshly deavecl under water. showed, be.
sides the Debye dop of tw-mured table t. 92 eve
on the ( g Indlesdag orientatiou I to 11 11,
nommil to sumfift atThe ades; the plame of Ag
lies paralld to the (001) plane of the odes. Another t
at diffracdom pattern showed tht presence of a s(alyr.
004 Crystal As " with a bualloclal lattice wItImml dmp
of the at. r"us 1.44 A.. the (WA of the
004 Ag Ike P"Iell to (WO of mks. W-W Ali
490 bution whavelm All atom we disposed = 0 atcams
the (ODO pla" of the momockink museavits U &17. %o
0040 9.94. c 2112 A.. 0 WAII) in each a way That each AS
occupies a bok (onmed by 3 or 6 0 Imes the 6 We of Uq
Iftics all$ is PUWW to oaf of the own *1 *0 blamodli
AAL! comfiguratim famed zt stow, wberm OW a a* rams Coo
ju of 300 with other 2 sides. In the am of K1.
C9 odes train a 0. 1 N mato., the gee
441011 p, p 4 In each a way that ove=971.1"W: rikel 4V*
to the a "k. the other two teem an angle at 3(10 with the 1141114111
6 axis. In this came. I- Ions occupy only holes for=d
Icais In thepImm of the'ns". N. Than -400
floe
-flow Wmi 'lee
fly
His COOV OM4 sails? M Oftf sit
8 ad 0 a 9 1 w Im 5 a dftaf
To
To
oe 'a
0 to
4*6 000 ST1940 0 0 **go 0o6 00

*~/Chemlotrjv - silver 3. mar 1948
Chemistry - Oxidation
"M ~nstics of the Oxidation of Silver by Molecular
C-
4 0irgen in Electrical Gaseous Discharge," V. V. Tyap-
ti. kini, P. D. Dankov, Lab Structures of Surface Layers,
M=t Pbys Chm, Aced Sol USSR, 3 pp
*1)6k Akad Bank SSW, Nova Ser- Vol. LIX, No 7
Au.t*bors' experiments shov that in =Idatlcn of layers:
cr~silver, previously condensed in volume in slectri-
wa gas discharge, film of cubic oxide of Ag;,0 fomed
VIth cuprite-type lattice. Thus discovered that ac-
U've particles arising In conditions of electrical
dlischarge in oxygen capable of leading to~ thorough
UM/Chemint'ry - Silver (Contd) 1 mar 1948
oxIdation of silver. To explain mechanism of phe-
namemcm of formation of polytoleoular layers of the
M~da, authors studied dependence of the speed of
amidation of silver an the time of processing it In
the electrical discharge. Submitted by Academician
A. Kistyakovskly, 20 Doc 1947.
L'M

Mob= mmum k=l= pal
1) = SWOM.
Film an Abw. V. V. TY&PkIva . . T (Do"y
Akad-Vauk S.S.S.R, 1949. W (8). 1461-IOU-0n RuNdAml-
Thin pDlycrvst. Ag Illms tordenood ijt wnw on rellu"I
were expLwa for a ww hr. at 2W e to wet Ht$ contaminated
by air. Films IOD A. thick entirely converted to sulphide
were studied by electron diffraction (olectem velocity 40-
45 kV.). It wm found that the pria3&ry sulphide has the
fimn of ruirulle crivialt of the avonthite type (rhombie
mmlifivati-mi of Asr,$). W)Wreas the orientation of A$ stom*
In the tosidablitm of Ec.c. Ag vr~axls t4i AgOO rvaiains un.
changed. the cubic structum in changed to rliombic in the-
hirmation of Ax~;. Tliua, even the appam I LMbic
,14) In always A In the
Armentite (Mineml fiwm (if ~L
rhombic scanthite form the cubic form unly 41mvp
18W C. This differeave between A#.0 and IN awt tu a
ehaW in the magnitude of the "us of the =1 (r, -- 0-34).
whereby the non-cubic modification becomes the equilibrium
form. 10 irf.-A. G.

-- 1-1 -'~ I r I r LY. " r -1 7. D7
L ; fir
"Kinetic of Oxydation of :SlUver
D! schar~7e Lr. -a Dasec,:;,-, T-Fn-%, a. re-~ c-,-, a -L

L 36440-66 W(m)ITIEWP(t)ISTI Ijp(c) jwljD
ACC NR: AP6018070 SOURCE CODE: UR/0076/66/040/005/1064/1069
AUTHOR: Tyapkina, V. V.; Guseva, N. S.
.ORG: Institute of Physical Chemistry, Academy of Sciences SSSR (Institut
fizicheskoy khimii akademii nauk SSSRT
TITLE: Investigation of the interaction processes between the surface'lof silicon
and fluorine and hydrogen fluoride ill
SOURCE: Zhurnal fizicheskoy khimii, v. 40, no. 5, 1966, 1064-1069
TOPIC TAGS: surface property, silicon, nonferrous metal, fluorine, fluorine com-
pound, silicon single crystal
ABSTRACT! The kinetics of interaction of the oxidized silicon surfdCCS with fluo-
rine and hydrogen fluoride was studied atr M temperature using the microbalance
fi
technique.41The object of the work was t fi7l the gap in the pertinent literature.
4e
'Samples of silicon n-type single crystal here cut out along the 111-plane,
polished, ei-ched with a IINCV-HF mixture, and washed with double distIlled water.
3-
The surface of the silicon samples was oxidized either by treatment with dry oxygen
Card 1/2 UDC: 541.124/.128

L 36440-66
ACC NR: AP6018070 CD
,at 11000C (oxide layer thickness 0.15-0.20 v) or treatment with steam in argon at
;,12000C (oxide layer thickness 1-2 p). Fluorine pressures varied from 11 to 44 mm Hg
and the EF pressure was less than 100 mm Hg. In the range up to 0.5 g, the accuracy
iof the microbalance measurements were approximately 1.8-2xlO-6 g. Prior to treat-
ment with Hr, samples of oxidized silicon were treated with fluorine. The depend-
ence of the removal of the oxide layer from the silic6n surface upon the duration of
ithe HF treatments is graphed. In the case of surface oxidation with dry oxygen,
with fluorine had very small effect on the rate of oxide removal by
pretreatment
treatment with HF. In the case of surface oxidized with steam in argon,
:the average rate of oxide removal was 0.04.10-6 g/CM2imin in the case of pretreat-
,ment with fluorine and 12.10-6 g/cm-min without such pretreatment. The effect of
,the. pretreatment with fluorine is traced to the removal of moisture from the oxide
.layer. Orig. art. has: 7 figures.
,SUB CODE: 07/ SUBM DATE: l9Dec64/ ORIG REF: 003/ OTH REF: 003
'Card 2/2.1121IR"r

. TYAPKINA, Ye.
Problems in the further intensification of agricultural production.
Vop. ekon. no-207-45 F '(2. ( KIRA i 51: 1)
(Agriculture)

TYAPKINA, Ye.
Differentiation of purchase prices b7 Zones. Vop. ek-on. :ic.7:
~v
143-148 JI 161. (MUU 14 -,7)
(Produco trade)

TYAPKINA', Yevdokiya Petrovna; RYBAKOVA, V.D. . red.
- - ~ - --:; _. I I
-
[Collective-farm incme and Its distribution] Y-olkhnnye
dokhody I ikh raspredelenie. Xbskvap Ekonomika) 1964. 15E P.
(MIRA 17:3)

Iff.m
Increasing the efficiency of drqwing machines. Biul. TSIIN tevet.
met. no.9t23-30 158. (KIRA 1116)
(Drawing (Metalwork))

VULITSKIY. Z.; TTAPTIN, A.
More about interdepartmental control. 7in.SSSR 21 no.6:
73-v75 JS 160. (MIBA 13:6)
1. Revisor' Krymskoy kontorv Gosbanka (for Vulitskly)* 2. Gjavrvy
kontroler-revizor.Kontrollno-revizionnogo upravleniya Ministerstva
finanoov USM -po Kry-makoy oblasti (for Tyaptia).
(Crimea-AuditingY

arf A. F T 'T, I. -T.
Fishcric ----:SstcTlla
On 19521 s quota. Ilyb.khoz. C03, no. 2,, 1952.
9. Monthl List of Russian Accessions, Library of Congress,
ElAy 1952
. M Uncl.
0:5a

KOLYAHM, L.Ya.- TYAPTINA M.Ie* FOKEMt GeM.
Composition and yibld of coal-tar xylene. Xoks i khis. no.8:
41-44 160. (MMA 13:8)
1. KharIkovskiy nauchno-looledovatellskiy uglekhimicheekly institut.
(Xylene)

s/o,68-x/60/000/008/001/003
E071/E435
AUTHORS: Kolyandr, L.Ya., Tyaptina, M.I. and Fomenko, G.M.
TITLEs The Composition and Y!"eTa'of XyloleA a By-Product of
the Coal Carbonization Process
PERIODICALt Koks i khimiya, 1960, No.8, PP-41-44
TEXT: The composition of technical xylole, a by-product of the
coal carbonization process, was little investigated, mainly due to
lack of reliable methods and the lack of demand for the individual
isomers. In the paper, the yield and composition of xylole
produced on 9 coking works was investigated using mean dynamic
samples for the fourth quarter of 1957. In addition to xylole
fraction a part of xylole remains in heavy benzole and solvent
naphtha; it was therefore necessary to determine the content of
xylole in the above two products (Table 1). The determination of
the xylole content was done by careful rectificationusing a
column equivalent to 30 theoretical plates at reflux ratio of 5-6.
whereupon the fraction boiling at 135.0 to 144-5*C was considered
as xylole. The distribution of xylole between the individual
products was found to be as followst 78.8% pure xylole fraction
Card 1/3

S/068-x/60/000/008/001/003
E071/E435
The Composition and Yield of Xylole, a By-Product of the Coal
Carbonization Process
(GOST io465-39), 13.1% solvent naphtha (GOST 1923-50) and
8.1% heavy benzole. The content of the individual isomers in
technical xylole as well as in xylole separated from solvent
naphtha and heavy benzole was determined by the spectrophotometric
method. In addition, paraxylole was determined cryostopically
and wethaxylole was determined by the usual method through
trinitromethaxylole. Non-aromatic admixtures (paraffins and
naphthenes) were determined spectrophotometrically (the difference
between 100 and the sum of determined aromatics) and by the usual
method; sulphonation with 98% sulphuric acid (at 200 for 20 min).
The zontent of toluol was determined by rectification. The
composition of xyloles from the individual works was found to be
similar and is given in Table 2. on the averagc-, the composition
of technical xylole was as follows, in % a ethylbenzene 4.8;
paraxylene 21.1; methaxylene 58.0; orthoxylene 13.5;
t-oluene 1.1~1; non-aromatic and other admixtures 1.3. The
composition of xyloles separated from solvent naphtha and heavy
benzole was, on average, as follows~. 3.6% ethylben-zenei
Card 2/3

S/O68-.v/6O/0OO/Oo8/ool/O03
E071/E435
The ComposItion and Yield of Xylole, a By-Product of the Coal
Carbonization Pr cess
16-5% paraxylene; 48.5% methaxylene; 28.5% orthoxylene;
2.9% unsaturated and other admixtures (for individual work see
Table 3). The average overall composition of xylole was:
4-5% ethylbenzene; 20.1% paraxylene; 56% methaxylene;
17% orthoxylene; 2.4% unsaturated and other admixtures; it
differs from the equilibrium composition (given in Table 4).
The following yield of the individual isomers was obtained from
raw benzole (mean sample for the fourth quarter 1957)3
0.23% ethylbenzene; 0.97% paraxylene; 2.70% methaxylene;
0.82% orthoxylene. There are 4 tables and 5 referencess
3 Soviet, I English and I German.
ASSOCIATION: MIN
Card 3/3

KOLTANDR, L. T&.; TrAPTINA, M.I.. YCKINKO, G.K.
Impurities In pure benzene. Koko I khim. no-3:42-47 l6o.
(KIRA, 1~76)
1. Ukrainskiy uglekhimicheakiy inatitut.
(Benzene)
. rj -
r.-. , ,

68-58-2-10/21
AUTZRS': Kolyandr, L.Ya., Orlov, Y.L., Tyaptina, II.I. and
Fomenko, G.11,
TITLE: Production of High-quality Benzole for Oroanic Synthesis
(Polucheniye vysokokachestvennogo benzola dlya
organicheskogo sinteza)
PEPRIODICAL: Koks i Khimiya, 1958, Nr 2, pp 44 - 46 (USSR)
ABSTRACT: A new standard for benzole for synthesis I, introduced
in September, 1957, required a very low concentration of
thiophene (0.005Pilo). An investigation was carried out in order
to study the process of purification of benzole-toluole fracti
L
up to the limits required for the benzole synthesis I and to
develop the optimum scheme for the production of such benzole.
The investigation of the appropriate fractions from Zaporozhe
T
and Bagleysk Coke Oven 470 rks (Table 1) under laboratory
conditions was carried out. At first 7 a direct Tuiashing of the
whole fractions was tested (Table 2); the results obtained
indicated that this method of purification is unprofitable.
Therefore, the following investigations were carried out:
1) Separation of BTX (mixed) fraction into a narrow benzole
fraction and a toluole-xylole fraction with their subsequent
treatment to a --equired purity; 2) The usual washing of
mixed fraction to limits required to obtain pure products
Uardl/2

68-58-2-10/21
Production of High-qual-ity Benzole for Organic Synthesis
(bromine numbers benzoleAKO.6- toluole