SCIENTIFIC ABSTRACT KULAKOV, V. I. - KULAKOV, YU. I.
Document Type:
Collection:
Document Number (FOIA) /ESDN (CREST):
CIA-RDP86-00513R000927320015-2
Release Decision:
RIF
Original Classification:
S
Document Page Count:
100
Document Creation Date:
November 2, 2016
Document Release Date:
August 23, 2000
Sequence Number:
15
Case Number:
Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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CIA-RDP86-00513R000927320015-2.pdf | 3.53 MB |
Body:
Al-6036424
initial alloy after this aging had a tensile strength of 40.5 kg/mm2, a yield strength
of 37.0 kg/MM2, and an elongation of 17%. The tests*showed that homogenization had
little or no effect on the mechanical properties of Al--Zn-Mg alloys. Small quantities
of refractory elements added to the initial alloy had a small but noticeable effect on
the mechanical properties bul greatly improved the corrosion resistance, especially
zirconium and zirconium coml-ned with titanium. The mechanical properties of alloys
microalloyed with Zr or Zr + Ti were.-tensile strength 45.2 and-39.5 kg/MM2, yield
strength 39.0 and 35.8 kg/mm2, and elongation 14 and 17.22, respectively. The
initial A!-Zn-Mg alloy had a very low resistance to stress corrosion when naturally
aged (service life 6 days) and low corrosion resistance when artificially aged (ser-
vice life from 42 to 76 days). In the majority of cases, microalloying increased the
service life up to 200 days. The beneficial effect of refractory metals on corrosion
resistance increased with higher alloying. The effect of microalloying on the tem-
perature and kinetics of recrystallization was insignificant. in the Initial AI-Zn-ft
alloy the recrystallimation was completed during beating to About 320C. In alloys
containing zirconium, ihe recrystallization began at 310C and was not complete at SCOC
OrIg& art. hass 4 figures and 2 tables.,
SUB COM 11, 23/ SUBM DMl' none/ ORIG REFs 0031 ATD PRESSt 3107
ACC Kt, AT6036425 SOURCE CODE: UR/2536/66/000/06,-j/'01.-)'i/0',G~5
AUTHOR: 1~irpichnikov, X. S. (Candidate of technical sciences); Kulakov, V. I. (Engineer)
ORG: none
TITL LE: Effect of addu.- minute amounts of refractory elements on the stiucture and proper-
ties of ingots of aluminum alloy containing 5%' Zn and 2% -Ivlg
SOURCE: Moscow. Aviatsionnyy toldinologicheskiy institut. Trudy, no. 66, 1966. Struktura
i svoystva aviatsionny" staley i splavov (Structure and properties of aircraft steels and
alloys), 157-165
zinc containing alloy, magnesium containirf alloy,
TOPIC TAGS: aluminum base alloy, refractory metal, metz. grain structure, metal
property/AOO aluminum
A13STRACT: 25 ingots of AOO aluminum combined with 5% pure Zn and 2% pure -M- and minute
aniounts of various refractory elements (0. 005-0. 1% Zr, 0. 005-0. 1% Ti, 0. 005-0. 1% Be,
0. 005-0. 05001o Cr, 0. 005-0. 050% Mn) were subjected to microstructural analysis and mechani-
cal tests. Part of the ingots was homogenized in a furnace with forced air circulation at 450-
470'C. Itxas established that all these elements, even if added in minute amounts, maelcedly
1/3
TJDC: 669.017:669.71
f".J-
ACC NR; XI"6036425
influence the structure and properties of the incrot. Zr in amounts of up to 0. 05 at - % increases
the size of the macrograin, reduces the size of the dendritic cell, slightly enhances Uie hard-
ness of the ing-ot and inicrohardness of the solid solution in homogenized state, and reduces
hvinorunization time. TI, like Zr, also reduces the dimensions of the dendritic cell,
but unlike Zr, it has an opposite effect on macrograin size, hardness, microhardness of the
solid solution and homogenization time. Be sharply reduces the intracrystalline segreigation
and homogenization time of the ingot. The effect of Be in many cases coincides with the effect
of Zr and is opposite to the effect of Ti. Thus, e.g. Ti reduces the hardness of the iu-zn-Mg
alloy in cast state by 4-5 11 units, whereas Be increasas hardhass by 3-5 units and Zr also
D
increases it, though to a less significant extent (Fig. 1). This may be to some extent. attri-
butable to the fact that Zr and Be have metallic radii which sharply differ from the metallic
radius of Ti, whereas the metallic radius of Ti is similar to that of Al. Inthe ingots to which
rnoi-e than one refractory element was added, the observed effects were diluted if not
~.-neutfralized. Orig. art. has: 5 figures, 2 tables.
2/3
ACC NR: AT60364214
B
70
68
66'
A
62
8e
TI+Be
Zr
No additional elements
-Or
r +rl
0 0,07 40S 0,/,9
Content of refractory elements in at.%
Fi,,*. 1. Mean hardness of the Al-Zn-.Ni-Ig alloy in cast state as a function of its
content of additional elements
SUB CODE: Il/ SUBM DATE: none/ ORIG REP: 003
Card 3/3
KULAXOV, V.M.
welecting the safety factor In calculations of petrochemical
a-
,pparatus for strength. Mash. I neft. obor. no.3:10 164.
(MIRA 170)
1. Voronezhakiy filial Gosudarstvennogo proyektnogo I
nauchno-4-ssledovatellskogo inatituta promyshlennosti
sinteticheskogo kauchuka.
KULAKOV, V.M.
Reducing expenditures on stainless and acid-resistant steels
in mixing devices. Mash. i neft. obor. no.4:17-19 164.
(MIRA MO
1. Voronezhakiy filial Gosudarstvennogo proyektnogo i nauchno-
issledovatellskogo instituta promyshlennosti, Jinteticheskogo
kauchuka.
-Z,
ARKHAROV, Aleksey Mikhaylovich; BUTKEVICH, Konstantin Stefanovich;
GOLOVIETSOV, Andrey Grigorlyevich [deceased]; KULAKOV,
Viktor M.i.khay'lovich, MARFRIIINA, Irina Vasillyevna; MIKIJLITI,
Yevgeniy Ivanovich; STOLPER, Mikhail Borisovich; Prinimali
uchastiye: BAKLUIOVA, V.G.; GRIDIN, V.B.; PETROVSKIY, Yu.V.,
red.
Dow-temperature equipment] Tekhnika nizkikh temperatur.
li
Mosk-va, Energiia, 1964. 447 P. (MIRA 17:12)
83669
S/048/60/024/009/002/015
BO13/BO63
AUTHORS: Baranov, S. A., Zelenkov, A. G., Kulakov,-V. M.
TITLE: Investigation of the Fine Structure of the Alpha Radiation M
of U234 and U235
PERIODICAL; Izvestiya Akademii nauk SSSR. Seriya fizicheskaya, 1960,
Vol. 24, No. 9, pp. 1035 - 1040 234
TEXT:-The authors studied the fine structure of the alpha spectra of U
and U235 by means of a large magnetic spectrograph with double focusing
(Refs. 1 and 2) in the energy range 4150 !.- 4800 kev. A uranium target
235
enriched in U , which was produced by vacuum evaporation, served as the
source. The target had a thickness of "10 #g/cm2. The spectrograph was
calibrated with a group of U 234 alphas. This group corresponds to the
transition of Th 230 to the ground state. Three well-known groups
corresponding to the transitions to the rotational levels of
Card 1/3
83669
Investigation of the Fine Structure of S/048/60/02VO09/002/015
the Alpha Radiation of U234 and U235 B013/Bo63
Th 2,30 (0+- P+_ nnd 4+) wAra found in theoe-rav snectrum of U2.34 (Fix. I and
Table 1). The latter transition (4+) was observed for the first time by
means of a spectrograph. The values obtained for,the energies and the
relative intensities o-,^ the above-mentioned groups are in good agreement
with the results of Refs. 3 - 6. 'he results of the investigation of the
fine'structure of the oC-decay of U235 are given in Figs. 1 - 3 and Table 2.
13 groups of alphas were found altogether. The results published in the
present paper do not contradict those obtained by means of an ionization
chamber (Refs. ? and 8), but differ considerably from the results of Refs.
9 - 11. This is especially true of groups of high intensity (Fig. 2). The
analysis of the data obtained indicates that the fine-structure groups of
the d_~-spectrum of U235 correspond to the transitions to the levels of
23-1. An energy--level scheme of the
four- or five single-particle state's of Th
Th 231 nucleus is suggested (Fig- 3). However, this scheme cannot make a
claim to finality. The determination of a reliable scheme would require
Card 213
83669
Investigation of the Fine Structure of
the Alpha Radiation of U234 and U2315
s/048/60/Oa4/oo-,/oo2/015
B013/BO63
fuither experimental data, especially on the spectrum of conversion
electrons. The authors thank V. V. Beruchko and A. 1. Timo6hinov for their
assistance in the measurements, and V. F. Gorbunov, V. P. Zah~arova, and
V. K. Sel:Lkhov for their help in the preparation of sources. There are
3 figures, 2 tables, and 21 references: 7 Soviet.
Card 3/3
MRANOV, S.A.;. KULAKOVi-YL%; SAI'IOYLOV, P.S.; ZEL-ENKOV, A.G.;
RODIONOV) PIROZRKOV, S.V.
Fine stru e of CK' -radiation from Pa231 and eiaergy level scheme
of the Ac nucleus. Zhur. ekap. i teor. fiz. 41 no.5;1475-1483
N 16.1. (MIPJi 14:12)
(Ilrotactinium-Decay)
(Actinium) (Quantum theory)
3,[769
S/O 5 61/ 6 111 104 1 /006/008/0--5,1
00 BIOB/B! 38
AUTHORS: Baranov, S. A,, Kulakov, V M_" Samoylov, P_ S
Zelenkov, A. G., Rodionov, Yu. F.
TITLE: The radioactive decay of Np 237
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fizlka, v 4",
no, 602), ig6ij 1733-1739
TEXT: The authors studied the radioactive decay of Np 237 bY means of
magnetic double-focusing :x- and 0,-spectrometers.spectromp-t:-'.c pronrort.~_~'nal
counters, scintillation spectrometers, and other device desc-ri"'ad in
previous papers (e.g. P. S. Samoylov, PTE, 6, 53, 11959) The a-spect-uT.
from Np 237 is highly complex, consisting of 20 monoenergetic lines
(Table 1). The resolution of the 0-spectrum was rather poor owing to th's
low activity and thickness of the source, Data on new rtransitio7ts
Fa 233 as determined from the electron and gamma spectra are given in
233 4
Table 2, An energy level scheme for Pa Is ~onstzuct;~d on the baais of
Card 1
The radioactive decay of Np 237
31769
S/'056/61/041/006/008/054
B1081/B138
the data obtained (Fig. 2) which is not, however, regarded as complQte
The authors thank S. N, Belenikom, K I. Merkulova, A A Arutvuno-i~
Yii~, I, Dmitriyev.. and the student at MIFI, Yu I Filenk,~ for help as
well as G., I.. Khlebnikov for the radiochemical purification --.f
237 rie, -:~.
NP There are 2 figures, 2 tables, and 24 references: 6 So,, . an
18 non-Soviel., The four Lnost recent references to English- langaage
publications read as follons; D. Strominger., J M Hollande7- 1:11IRL-8--89i
Berk,~ley, California, i958t F. Stephens eL a 1, P'hys Re.-t 2'2, -q~~;
J. Hubbs, J Winicur,. Bull,Am,, Phys, Soc 5".9, 19~-)8;
et al,. UCRL-9438, Berkeley. Califoznia, 196o,
SUBMITTED: June 21, :96i
Legend to Table 1: (1) forbiddenness facto.-., (2) levoz--! rnergy, Kr--"
Sum J13 + i j ~ 2,178. " Sum of three .5 a a a,
14 f z X -5
2
Legend to Table 2: -t -transitl.on energies (ke,.,) cff -Pa 'D al
(1) Pz5pt--,r-trcmeter, (2) pzoprlrtional counter. T
(4) mult-1polarity,
Card 2/6
S/056/62/043/003/010/063
B'125/B102
AUT1111ORS: Baranov, S. A:, Kulakov, V. It., Zelenkov, A. G.,
Shatinskiy, V 11~7-
T 241
TITLE; -Lnvestigation of a-deoay of Am
PERIODICAL: Zhurnal ek3perimentallnoy i teoreticheskoy fiziki, V. 43,
no. 3(9), 1962, 795 - 799
TEXT: Alpha decay of Am 241 was studied with a double focusing a-spectro-
graph. At 4900 - 5560 kev more than 18 fine structure a-ray groups of Am., 241
were aacertained, most of them for the firot time. Tile sources were mad.?
by sputtering americium nitrate onto a thin film of aluminum oxide. Thel-
2 2
effecti've areas were 0.25; 0-5 and 1.5 cm with