SCIENTIFIC ABSTRACT ZARETSKIY, B.I. - ZARETSKIY, I.I.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001963820010-1
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 19, 2001
• Sequence Number: 10
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

------ -- --
ZARnSdI., Do 1.
Tractors. Moskva, Gz-;s. nauchno-tekhn. izd-vo "a hinostrolt.lit-ry,
1950. 135 P. (50-55251)
n233.Z3

KITHEV, Ye,N.-j inzh.; ZAMTSKIY, B.I.0 otv. red.,
(The boat cements.for the manufacture of asbootoo-cezent
materials] Optimalfrqe tsementy dlia proiz-vodstva asbeol;otse-
mentrqkh materialov. Moskvav'Otdol nauchno-tekhn.inforuntsii,
1959. 71 p. (MIRA 151l)
(cement) (Asbestos cement)
N-

KITAYEV, Ye.N., inzh.; GONCHARSKAYA, R.E.; ZAIRETSKIY, B.I.,, etv. red.;
ERLIKH, I.A.., red.
[Asbestos cement materials obtaimd from sa-M ce_-entE 14,-.7
autocle-ve treatment,$ and their chemical resistance to nor-
rosive solutions] Xhimichoskaia stoikost' v agressivnylch
ras-tvaralch asbestotsementnykh materialov., poluchaemykl iz
poschanistykh tserentov a prJneneiiiein avtokLavuoi obrabotki.
Moskva., Otdel nauchno-teklm. informalsii, 1960. 24 p.
(MIRA 15-.:1)
(ABbestos cement)

K'MLISKIKH, D.K.. prof.; APASHEY. M.D.. kand.tekhn.nauk; BARSKAY, I.B.,
kand.tekhn.nauk; ZAYCHIK, G.I., doktor tekhn.nauk, reteenzent;
ANOKHIH, V.I., kond-tekhmnauk, retsenzent;',~~~' 130iff
inzh., red.; POPOVA. S.M., tekbn.red. *wUmam"OL."
[Theory, design, and engineering analysis of tractors] Teoriia,
konstruktsiia I raschat traktoroT. Hoskva, Gos.nauchno-lekhn.
izd-vo mashinostroit. lit-17. (Pt-3- Theory and amalysits of
tractor chanslol Teorila i ranchet mhassi traktoroy. Poil obahchni
rod. D.K.Karollskikh. 1950. 144 p. (MI-AA 11:12)
(Tractors)

ZAH-!!-,rSKI
"TractorB. 1950, 1 f'opy.

4 A I u;ZA -A *.P-'kA a 1'~ffm-4
-L 29931v-66 -JD/IIM-
ACC NRi AP6018011 (A) SOURCE CODE: UR/0413/66/00/010/0126/4-i~-
INVENTOR, Voronin, G. I.'; Slotint V. I.;
Shvetsov: P. N.; Barannikov, G. I ; Eakin, G. Is
ORG: none
TITLE: Ultrasonic unit for fluxless brazing of metals, Class 49, No. 181967
SOURCEt Izobreteniyp, promyshlennyye obraztey, tovarnyye znaki, no. 10, 1966, 126
TOPIC TAGS: brazing, metal brazing, ultrasonic brazingg brazing unit:
ABSTRACT: This Author Certificate introduces a unit for fluxless brazing of metals
equipped with a heater and ultrasonic emitter. To increase efficiency$ Me ultrasotdc
Fig. 1. Fluxless brazing unit
1 - Crucible; 2 - brazing allay;
3 - ultrasonic emitter.
Card 1/2
UDC1
21,721.351A.03

ORM - -
L Ngll-M

BLTS, G.A.; ZARETSKIY, D.F.
[Solution of the generalized Yj-1ne problem) Resbenie dtobshebenr-
noi zadaebi Mi:ln--,. Moskvaq 1955- 15 P. (MIEU 24:7)
(NeutronB-Scattering) (Integral equations)

ZARNSKIT,D.P. --
[Iffective boundary con-ditions for Im""m bodies] Wwail-Are
granichriya unloviia dUa "Berykhm tel; daklady, predstavlonrWe
SSSR na Rezhdun rod=iu konferentsUn po mirnoun impolizovimitu
atomnoi energii. Hoskva,'1955. 17 P. [Kicrofilm]
(Nuclear physics) (KLRA 51:3)

tr Physid/s ermal neutron capture FD-326o
Ual uc ee
Card 1/1 Pub. 146- 19/44
Author : Shut1ko, A. V.; Zaretskiyy D. F.
Title z Capture of thermal neutrons by lead isotopes
Periodical* Zhur. eksp. i teor. fiz., 29, No 6(12), Dee 1955, 867468
Abstract The authors consider the isotopes Fb-207 and Fb-208 and. their ex-
citation levels) spins) parities, energies, etc. They compare the
theoretical evaluations of croso-section of thermal nett,.,ron cap-
ture by lead isotopes with data of experiments. They conclude that
captm-*e in Pb-206 is "less single-particle" than in the case of Pb-
207, and that the anomalous character of capture radiation in lead
isotopes is explained by proceeding from the single-paz"~icle pictare
of capture. The authors thank Professor A. S. Davydov tmd V. F.
Turchin for comments. Seven references Iq including one USSR: L. K.
Peker and L. A. Sliv, Izv. AN SSSR, ser. fiz., 17, 1953,
Institution
Submitted August 31j, 1955

ZARETSKIY, D. F. and SHUTKO, A. V.
"On the Thdrmal. Capture by Fb Isotopes" a paper presented at the Haternational.
Conference on Nuclear Reactions, Amsterdam, 2-7 July 34.956.
D551274

UrV 7
L

VOW

-- ZE

"1 75

AUTHOR ZARETSKIY, D.F-, SHUTKO, A-V- PA - 269o
TITLE Quisi-Magnetical, Interaction of the Nucleon Spin With the
Rotation of the Nucleus.
(0 kvazimagnitom vzaimodeystvii spina nukloica s vrashch,eniyam jradra-
Russian)
PERIODICAL Zhurnal Eksperim. i Teorst. Fiziki, 1957, Vol 32, Nr 2, PP 370-371,
(U.S.S.R.)
Received 5/1957 Revisived 6/1957
ABSTRACT It in possible to find a now interpretation for the rotational levels of
nuclei with spin 1/2 if we start out from the following promises: (1) In
These nuclei there wdst "tates. Then in first approx'Lmation the levels
with the total angular momentum I-K11/2 are degenerated. (Here K stands
for the rotational quantum number). (2) This degeneratiolk is eliminated
if we introduce into the Hamiltonian byBohr and Mottelvon an interaction
of the f orm of "R- - - ( X /mc 4) '1 j VU Ikoll] Hors ~.sitands for a non-
dimensional phenomenological constant with the same sigmificance and ma-
gnitude as in the normal (usual) spin-orbit coupling of the nucleus.
Furthermore the following denotations are usedi V'for the vector of the
nucleon spin. U(?) for the selfcoasisting potential of the nucleus. mea
for the velocit
for 4;$s ramt energy of the nucleon. and vkoll y witA which
the nucleon participates in the collective motion. First of all the sig-
Rific&ncg Of vkoll is clarified, and then the significance and the ori-
Card 1/2 gin of the above-mentioned interaction HR.. For the wave function we set

AMORS: BW , G.A.# Zmkret*lc~v D.Pa ZOV/09-4-6-2/30
TITIM The Effac-~i -TA B olmd Val a Conditions in the Dilfusion Theory
of Neutrons granicbnyye usloviya v teorii
difftzii ney-tromv Obzor))
PMODICAL: Atowcwya energiya, 1958, Vol 4, Nr 6, pp, W-519 (USSR)
ABSTRACT: In tha oam-se of a survRy the methods are describied by means of
which tha iffaotive boundary value conditions can be determined
which bring about agraement within the asymptotic range between
th-3 solution of the n=tvon diffusion equation and the solution
of the corr9aponaing kinatio equation.
The bounle..ary values ara described for monoenergetio neutrons;
some of them &r,4 vcmpu-ked~ and, especially, the o=rring ooeffi-
oienta az-a r-~rgistered in tables for the following cases:
1.) For an Infinitely thin "black" rod in a mediurA, in vddoh
souro.a;3 ari uniformly distributea.
2.) For & ple-ne boundary between medium and vacutus. by means of
the exact anal~dical method deveiopea by Wien-er and Hopf.
3.) Yor a "blaW ro,,md cylinder. The following m,.-thads of solv-
C erd 1/2 Ing ara mentioned for this purpose:

The Effeotixe Bouniary Valua Conditions in the SCIY/09-4-6-V30
Diffusion Theory of Neutrori
a The balance method developed by Bruano (1951)
b The -~,ariation meibod developed byZaretskiy'
01 The mathod of spherical harmonies by Galanan (Ref 6)
a Solution of P.-tiorlas (PayerVis) equtions for g~:mt and small
r,, according to the me*M developed by Davisori.
4.) For a "black' rod of any cross station by thn nethoa of
appxvixima,kion devo~loped by fi=vitz (Gurvits) ana Roe (Ref 8)
5.) For a "g~-,ayll rcd (only possible by approximatim). If it is
in~er4e3 io take the neutron apectnm into aoutiunt in oonnoo--
t,lm w1th Wt boun-Uxy value conditions, thia to possible
oal,y for some simpl-i boeler cases.
(A 1,ody u aesoribted as being either black or gray aczoraing to
whether tho nautronia Impinging upon its surface ars fu3ly or only
par,',17 absoxted). Theri ari 2 figures, 5 tables I and 10 references,
4 of whioN are Soviti.
SMUTTED: October 1,, ',957
1. Neutrons--Diffrusion 2. Diffusion--Theory 3. Mathematics
--Applications
Card 2/2

ZARV-TSKEY,, D. F.
"On -Masonic Fieeion."
paper to be presented at 2nd 'Un Intl. Conf. on the peaceful uses of Atomic
Energy, Geneva, 1 - 13 Sep 58.

~- 'r-!r. . - - . I -
_- MOV$- -S. J.'I' tM-1ShlY$ 0 1 - KWIN) L I P. I T. Kh.
DF D. F and SFMUIIKOV
"On the Formation of a Mermal Neutron Spectrum."
paper to be presontod at 2nd UN Pito. Conf. on the Peaceful uson of At,xic
EnerEy, Geneva, 1 - 13 Sep 53.

I-A- 'V-

Ursbal wlah.D
fn%z.. ?h. VIII Annual Congress of Nualear spectra-copy (TIrr
701h.codboya su'vahchanly. Y. 764.".y
PIDLIMICAL: Vap.kht fisich.skikh a.uk. 2~56, Vol 65, Xr 4.
Pp. 721 - 722 OUR)

ASSTR=t Th* Oth Congress or Nuclear Bpootromeopy took ;Iaa* Let
LenIz4r&d from January 27 to Ftbr"ry 3. 195a. It sras
&tt"dod by 300 scientists from %he CSSR. further by sclacti.%8
froo China. rrance, Poland, Cm*Qbo4lov&kts# HuneazY, Sawlext
Germany, Yugoslavia, "4 the Mangal Democratic lopubl$s. A
~i~ i22=-;- '4- ; -a'V.,;a "", h '-'" ,- 'em"s'
lecture. deal$ Ith problems concerning nuclear mc,dolo, %zo
and A-daaay# y-radlationo Internal conversion. and xo~lwox
Corraspandin; Member. Academy of
Sciences, 11351. opened the conference. Loctu~rsa more U*ZA
by: I.?-. 00-chsr, T-- V. I-ORIn. S.P.?-Ytka (2-I.LS Ma--JM3
on light nuclei -f -g..--r.Trx-oT-hacIsi mo4alsil..Z. F.kr
(SIX 3331-Llbrary AS U33S)i lu.X.3hlrokow (IMU-9004ow SLau
L.A ad PV-i-e- Rchnical.
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A-1khAsaw, A.P.Orimberg, G.M.Gusin.kly, X.I.Teraltblas A"
I.Kh.Lemb.rg (LFTI) on having found no rots-L-Al lovela
at Z(1 may In Crq In, and 31a auclol. The zam roats.not wor-ra
also ortd an
2p a&* discovery of vibraticnal 7~1*vwL#
l 4
.w - nuclei by %.-a at tt. owthxi or tis,
L..w
Coulomb (Kul.n) 6-Its,tien at I
(DAN 3333) gave a survey rmport~ "Concerning Saw hallem."re
in Vik-tion.1 Level. of Warned Twol.t". -&-t~qs soon
he'd alf 33 33 M) am rm,444%L.
1/21 Ia.
Shvin I- Z WIFI U3U Wd Sal.ctifla Sam ... CA Z..%I%4tq 4C
Phyalas, Xosoow State Univoralty) on tho '&T*l dimplocoese=
and %1he pro'bability of corres
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In add nual.11D rets"y J, 51 - AS MZ3) 04 $to
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man. a, the uu.L.t, (AX 521 -IS Z=) 4^ tt-
axls%er.ce of light nuclei with high neutron or proton re,voss;
T.A.Xrawt"v (LPI-L*nlnCr&4 Polytechnic initltutw) am t"
fornwtion of nucleon pairs In ouclol; L.L. ;QI'dtA* A. 2.
?illy.. K.A.T-Uart IroaX= (M AS SMAX)
on *lph4stay .. rotational level. of add Z=1.11 V.0,
s0.0, W 53511 - AS U3510 .. maPha decay -f
s.0101 (&-.y)1 A.I.Allkhano,. T.A..yukj,,..
'
rT.Itr. !aor (TTL AN SSSR) an polarlsation co,s-#ajV
at .1oalrons emitted in the O-d ... y of U17., Lm,177. A,
3.153. j.'a6 W. 0.1._x. _1) .8 wall am I. tant of *sjo sced _90
(&1. 2.- a. -I) IT.P.SudAkov (kn -SSR - IS US!2
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1
1
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.*at& of the (0-7) angular correlations In B. -4"aj I
"d Yu.T.T.rokh- CM AN IISSE) a* I ... sOld.91".
tron-neutran cor~rwl&tJodm and the resonance

go ao State University) CA this bromant:Lbluag *4'
lo-CIA.41-Ily pol&rls.d *l..tma.j *ad Vw,v.
P;ray (XZU) " the arfactive crom. section of zbo afOltertag
a*1"-.t*d electrons and poitrans at palarlsed tlea%~*,voj
Y-E.Chudar. and I.Y..T.wa (alffa) an %he 4t
the intensity Of the components of the complex :-02001r"
&a' ardif
wo the F.rat dl.gr"L I.N.Band, iw,4
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To P.3 '. , LOU (L-trigraid Us%. Vail.rotty) on %be 4#*.
4
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tion of the probabllttjr of the permitted and of In*
forbWou mApSarm of ol"trom bjL & analwoo.

Z'AdtET~Irll-ylp D. F.
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7t

1 2,60
Zaratskiy, D, F. SO V/56-3.5-3-54/7
On 'ha Theoi-y of Nuclear Magnetic Yoments
(x toorii magnitnykh momentov yader)
T i) _-.1 1 CA 1, ~7 hart~l cI.:;;pcrimcnInltnoy i teoretichaskoy
~959,7Vol -.-j'-6, !,r pp a69-873 (USSR)
_Aic imTxirtarit rin-r-11 played by spin-orbit coupling in 'the
of nu-,lovr zhells is, in.general, taken into acnount by(,)
s */m2c2 8
[v U~01
'Dhonomenolo3rical spin-orbit coupling cons-tan'
xluClo 04 snizi operator, U('?) = selfconoistunt nuclear
-f,otantial, j, ~, mumoitim operator of the(nucleon); if t,-ie
nucleun is in an A:,ctromagnotic field, 1) vithl-oc-ii/c
over into e .41ullc3) -4 -4
3 IV U a] (2)
Aiere a v,_--c~vor potential. Mayer and Jemien (r'
71crc the fi-I-ct to point out the necessity of takinG this
71 :tnin-orbit ci%.'uct into account withoutt howavex, using (2).

6 --6
--,i ooz- of ;,ucl~--.r ':-.s-watic 1,oments SOV/-
J). 1'. Grochu:"Iain (Ref 2) calculated the opin-c,r1bit -.uuplin~-
for Lr---xcitiono of the kind d *0a I n the
3/2--- 1/2 -
prc:,,an1- 7--Ter Ule effect is investigated by which (2) is
int::oduc,-~', into t1w, mag~-etic moment of spherical and ror-
spho;7ical -'uclei wi-th odd proton number. Althou!~h (2) is not
L'ho only cau-,c of the deviation of the observod madnetic
monon"U3 from the Schmidt (Shmidt) line, an initeotigation
(ost.imato) of (Z) is nevertheless of interest, because it
facilitates separation of the other effects. In some on--cs (2)
makes tlio contribution to the deviation of magnc ti c
momonto f -. on the Schmidt line as %,.oll as to th; probability of
forbidden 11al-Ornnaltiono for nuclei with nn odd proton nuribor.
In the caco of nuclei with odd neutron numborsq conoider:~.tion
of (2) ic of good purpose when there exists an effective charge
duo to irilr1raction lictwoon noutron and the care of the nuclous
(of- !'of 3). in t1he Proaent paper the additional f-"Ct(;,r
ocourrinj7, for otron- spin-orbit coupling by the intorc-otion
between ~ac llucloon~u' in the nucleus and the oloc tromf.,.(,w.- tic
field ic, o:,,nentially, calc~ulated for spherical and nonspherical
nuclei. Tor former the magnetic moment 113 J~z 1j, J>
Card 2/3 /A

On the Theory o*f Imolenr Lic L'Mmonts SOV/56-36-*-,-,~,i1
and, in co-LIsid
Icration of (2):
0 /(j + I)
nnd witj,. (2) ~or rrpin 1/2 also a formula,(21), iz ac-rivQd.
!'or V.1 Vlio rcoult'l ill ,&- -0-35 nucloar
a,-3ainot ci, (-~.:p,-r-incntnI value of 0.20
The author 'Limnally thanks P, E, Nemirovskiy for discuosionc.
There are 13 rofcronces, 7 of which are Soviet,
SUBMITTEND: September 16,
Card 3/3

24(5)
AUTHOR: Zaretskiy, D. F. SOV/56-'46-4-26/70
TITLE3 On the Radiative Transitions in the-System of
Rotational Levels of Nuclei With Spin 1/2 (0
radiatsionn,ykh perekhodakh v sisteme vrashchal;ellnykh
urovney yader so spinom 1/2)
PERIODICALj Zhurnal okoperimentallnoy i teoreticheskoy fizriki, 1959,
Vol 36, Nr 4, pp 1129-1132 (USSR)
ABSTRACT: For the purpose of calculating the probabilities of
magnetic dipole- and electric quadrupole transitions
between rotational levels of deformed.spin 1/2 nuclei, a
coupling system suggested by Hund and already previously
used, by the author (Ref 1) is used. A transformation of
coordinates (transition to the system of cooriinates of
the nuclear axes) is carried out in tha wave function,
and by using the relat-ion m I DM M 'm'
13 s s 13 s
Card 1/3

on the Radiative Transitions in the Syst= of SOV/!i6-16--4-26/70
Rotational Levels of Nuclei With Spin 112
a wavo function of the form
~2 J,
f(2 + 1)/8 Om I-x 411 Jm 'D ms'
Xs ME1
is obtaLned, which causes no difficulties with respect to
calculating the probabilities of electric quad:7upole
transitions, The result agrees with that obtained by
Bohr and Mottelson (Ref 2), Yo denotes the .iave function
desexibing the-motion of the nucleon with respect to the
nuclear axes, /,- the spin function of an odd nucleon
in the laboratory system, the rotation quantUHL number 'r-
I I I +-
assumes the values 0,2A...,. for the states and
1,3,5..,,, for T-U In the following the authors
calculate the probabilities of magnetic dipolo:transitions
-and show that transitions between components of different
doublets with A j - 1 occur mainly as magnetic dipole
transitions. The admixture of electric quadrupole
transitions amounts to not more than 1 V In
Card 2/3 0 - 2 0

On the Radiative Transitions in the System of I
Rotational Levels of Nuclei With Spin 1/2 SOV/56-36-4 26/70
conclusionthe nucleus'Tm 169 (and Tm171) is sho:~tly
investigated as an example, and a comparison is drawn
with the results obtained by references 7 and 8 with
respect to the nucleus Yb171, the daughter nuclous
originating from the (3-decay of Tml7l(Fig). The author
thanks S. A. Baranov for discussing experimental data,
and D. P. Grechukhin for his comments. There are 1
figure and 9 reforeinces,* 3 of which are Soviet,
SUBMITTEDt September 13 1958
Card 3/3

5
ZARITZZY,II, D. F.
Radiative capture of a neutron. Zhur.ekep.i teor-fiz. 3? no.4:
1084-1087 0 '59. OGRA 13:5)
(Neutrons--Capture)

16.8100,24.6720,-.4.6800,24.6810 77009
sov/r56 -37-6 -49/55
AUTHORS: ZaTe~sqy, D. F.,and Novikov, V. M.
TITLEt Letter to the Editor. Depolarization of Muons in
-Mesoatoms with Deformed Nuclei
PERIODICALi Zhurnal eksperimentallnoy I teoreticheskoy fiziki,
1959, Vol 37, Nr 6, pp 1824-1825 (USSR)
ABSTRACT: An. analysis wao made of the additional depolarization
caused by the interaction of muon with rcuclear deforma-
tion in ~L_mesoatoms. The effect was considered for
even-even nuclei. The Hamiltonian of the muort-nucleus
system was taken in the following form:
H = I/,, + 1/4 + Ill.
Here, H0 Is the Hamiltonian of the muon In the mono-
pole field; H. is operator of rotational'energy of the
Card 1/4

Letter to the Editor. Depolarization of 77009
Muono in -Mescatoma with Deformed SOV/56-37-6-49/55
Nuclei
nuc leus; Hq is operator of quadrupole interaction of
muon with nucleus. The diagonalization of the Hamil-
tonian shows that the quadrupole interaction consider-
ably changes the eigen functions of the system with
corresponding muon in the 2p-states (of, L. Wilets,
Kong. Dansk. Vidensk. Selak. Mat.-fys. Medd., 29, 3,
1954). The changes of the eigen functions of other
states can be neglected. In stAch an approximation
the polarization of muon in Is-states beoomes:
P A4 W11, (CIP't )0 IV-/. < OINS >0
Here W, and W are probabilities of the passing of
_ff 3/2
muon through states 2p, and 2p :p, and
Card 2/4 'ff 3/1; _ff

Lett-er to the Editor. Deepolarization of 77009
Muons in ~L -Mesoatoms with Deformed S6Y/5-6-37-6-49/55
Nuclei
,( a-2p3/2 ) 0 are polarization of muon in the above
S~viteB in the absence of quadrupole interactionj A
q
and B are factors compensative of the ELdditional
q
depolarization. The factor Bq was determined from
muon tran3ition.from the upper levels into the ls-
-state through the states that can be described by
the eigen function of the above given Hamiltonian:
B,j = 0,8 3 C,', +2 0.61
k- L
whe,e
r-2(E. + r-,--i
C2k E,- EIOI
E3 (ER+E, 2 EE. )!!+k'-(Eq + L -r/. V+ r
q P. - -1,q 3
E2 (Ell +-2 rj("j:-r-h)2
q
Ed (En 2 E/.,,v - El,)-r- q212
Card 3/4 3

Letter to the Editor. D~_-polarization of 77009
Muons in /i-Mesoatoms with Deformed SOV/56-37-6-49/55
Here, E~ is eigen values of the Hamiltonian which
correspond to muon in 2p-states and to the whole
momentum of the system 3/2, E f.8 is sp:Litting of
fine abructure or the 2p-level; ~R is energy of the
first rotational level of the nucleus; 13 q =< 2p IHq) 2 p).
The 'ollowing values of B and D. were calculated for
Gd 1,18 .1 W184'Th 232 , and U938, re spectively: 0.63, 0.64,
0.38, 0.38 and o.61, o.64, o.6, o.59. Thus, the
interaction of muon with nuclear quadrupole deforma-
tion can lead to a considerable additional depolariza-
tion of the muon. There are 4 references; 2 Soviet,
I Dutch, 1 U.S. The U.S. reference is: W. Ford,
C. J. Mullin, Phys. Rev., . 108, 477, 1957'.
SUBMITTED: August 21, 1959
Card 4/4

GRIN$, Yu.T.; DROZUV, S.I.;-ZARETSKIY, D.F.
Green's Pinction for odd nuclei. Zbur. eksp. i teor. fiz. 38
no.1:222-:228 Jan 160. OURA 14:9)
(Potential, Theory of) (Nuclei, Atomic)
F

27480
s/046/61/025/0051/005/007
B104/B1 02
AUTHO.RS 1* Grin', Yu. T.j and Zaretakiy, Fe
TITLEt, Collectivo excitations of non-spheric*al nuolul
11MIODICALt Akadomiya nauk 88811. Izventiya. Scriya z
,6hoskaya, v. 25,
no. 9, 1961, 1169 - 1175
TEXTt This paper %!,ras road at the 9th Annual Conferen, Nuclear
Spectroscopy. The authors generalize the thoory of a' ctive excitationo
of non-spherical nuclei. An equation is set up for the frequencies of'
collective nuclear oscillations, and a relation between the frequencies of
the excited .8(k-G) and J-(k.2) vibrational levels is derived in quasi-
classical approximation. Using the Green's two-particle function
K , the equation
1 2 3 4 0 2
(E1E1 -6 ~ +LV)
XF C432 1 2 1(q 2012 1,2 (9)
12 2E 1E2 (El + E 1)2]
Card 1/5

27480
5/048/61/025/c()9/005/007
Collective excitations of non . ..... B100102.
is obtained f or'Ithe f requoncies of., the bound states of,,two qLLasi-particles.
Within the framework of the Nilsson model Eqo (9) can only be solved
numerically for a real model. Using themodel of an axisyinmztrically
deformed oscillator potential., the authois attempt to find a solution to
this equation. Eq. (9)'is represented in the form
.X 2A2jqX).,j2+ (E)A6, - exev (Sh + EO
R (4 CZ - (02) 2L.-).E)L,I(L'
The first term is the sum over all transitions without onerF,), chanee, and
the second term is the sum over all other transitions, Since ci is
negligible in the latter sum, Eq. (15) can be reduced-to
AX, H. (4,V, -1XV
where (16).
+
)Ar
Card 2/5

3/04 &111/0u 5/00 ~VOO 5/007
Collective excitations of non- B104/B1O2
In oua si-clas3ical approximation, Eq. (16) leads to
4A 2 1 2 4
-rotan q 6(F, I) I ~.,,CO/AR
A
,The following explicit solutions are obtkained from this equationi
( f or &j 4 2 !N und
lo- 26 Y1 jq a (C
2 V~
tj . 2 LX -ZX,2 q 12 for 2A - Q&26-
An analysis of thes-i solutions indicates that collective excitations with
ener,-,ies much less than 2A may exist in deformed nuclei. and
vibratinns are inte:vrelated by
Card 3/5

27480
S/048/61/025/009i'005/007
Collective excitations..o.f.non- B104/BI02
CA - PAI
AM
(
(23
01AW 6010
2A
From this relation, it is concluded that the frequancioz of ind
vibrations agree within the framework of the model of an axisymme trio
oscillator potential, The agreement of the froquoncies is cl:zoly related
to the degeneracy of the levels in the occillator potential. 'Finally,
the Ifilsson model without spin-orbital coupling 16 briefly dii3cuased. The
following values art) obtained for the ratio CIA *r as a function of
o6_ 2D_,0/,)0
Ile 1.8 2.25 3-0 4-5
0.90 0.86 0.80 0'72
(1960))
i4i mantiona4.
S. T. Belya yov (Zh., ekeperim. i toor. fiz. 32, 1387
Card 4/5

27480
8/048/61/025/009/005/007
Collective excitations of non- B104/B102
There are 11 references: 7 Soviet and 4 non-Soviet. The references to
English-language publications read as followsi Marumori T., Progr. Theor.
Phys., 24, 331 (1960)1 Baraneer M., Phys. Rev., 120, 957 (1960)j Porlman
I., Proceedings oil the International Conference on Nuclear Structure,
P. 547, Kingston, Canada, 1960.
Card 5/5

DROZDOV, S.I.; ZARETSKIY, D.Fs
Effecto of pAir oorrolation near cloved aballa. Zbur, Oksp, i
teor. fiz. 40 no.IQ66-295 Ja 161. (KM 14t6)
(Potentialp Theory of) (Superconductivity)

2 AS I
S/056/61/040/003/031/031
'AUTH RSs Zaretskiy, D. F.9 Novikov, V. MO
TITLE: Nuclear fission by/.k-mesons
PERTODICALt Zhurnal eksperimentallnoy i teoretioheskoy MILki, v. 40,
no. 3, 1961, 982-983
TEXT: The effect of a meson on nuclear fission can be calculated for the
case of rigidly oriented nuclear axes. The energy E ? of a bound meson
depends on the deformation parameters of the nucleus. A solution of
SchrUdingerts equation for a meson in the Coulomb field of the deformed
nucleus is required for the determination of E It is assnmed in the
present paper that the nucleus has the form of an ellipsoid of rotation
up to its saddle point. The Coulomb potential of a homogeneously-charged
ellipsoid of rotation with the semiaxes a-and b has the formi
Card 1/3

2ZL52
S/056/61/646/()03/031/031
Nuclear fission by ... B112/B214
(p (a, P) I - P2 (ch at) Pg (Cos In c0l -20- + .1 C111 a
C 2 2 ch a0 P2 (COs
3 sh2 cc N sW 0 -Pr cb a < cli a0 -a
T W i -oi. ) Ti 13;-f '; I
(p (a, Z-0- [ I- P, (ell cc) P, (Cos P)l In ctli .1 + .1 ell otp, (Cos
C 2 2
for cli a >- a
C
2 2 2
Here, Ze is the nuclear charge, C . a b P is the Legenare poly-
nomial, and a,A are the degenerate elliptical coordinates. The
Schr5dinger equation for a bound meson in a nuclear field with such a
potential was solved numerically with the hel p of an electronic computer.
The value of E threfl6 for different values of a/b is given in the
following table (U .3 nucleus):
a/b a 1.2 1.4 1.6 1.8 2 2.2 2-5
E (Idev) . 11 .89 11-78 11.66 1"! -53 11.36 11.21 11.01
The increase 6E of the fission barrier for some nuclei is gJven in
another tables
Carol 2/3

Nuclear fiesion by ...
22151
S/056/61/040/0015/0-411/031
B112/D214
Nuclaus a/b a/b Ethreshold' Mev &E, Mev
statistical saddle point 1
5.8 0.6
e2 3a 1.30 2:24
35 1.25 2 2 5-75 o.6
PU239 1-30 2-17 -F 5-48 0-5
D. P. Grechukhin is thanked for his advice and V. K. Saullyev for
setting up the program and calculation with the electronic computer.
There are 2 tables and 7 referencess 2 Soviet-bl"oe and 3 non,.Soviet-bloo.
SUBMITTEDt Januarj 11, 1961
Card 3/3

ZARETSKIY., D.F.,-, NWIXCV2 V.14.
Excitation of nuclei in heavy,"mesic atoms. Zhur.eJcsp.i teor.fiz.
42 no.l.-214-221 JI 161. OUJU J-4-71)
(Naclei,, Atomic)

ZARETSKIY, D.F.; URIN, M.G.
Nature of collective levels in nonspherical nuclei. Maur.eksp.
i teordiz. la no-3.-898-906 S 161. 01MA L/*.-10)
1. ~bskovskiy inzhonerno-fizicheakiy instit,4t.
(Nuclei, Atomic)

! .1 IN
ZARETSKU. D.FA;.ARIN, M.G. -
q.- ~.O ~
I I ,
I Microscopic description of collective,igisle of nowphirical ~uqUjs
Zhur, eksp. i teor. fiz. 43 no.3:1021-100 162. (MIRA 15slO)
1. Moskowsk-ly inshonerno-fizichookly institut,
(Quantum theory) (Nuolle, Atomio)

3/056/62/042/001/046/048
B154/B112
AUTHORS: Zaretskiy_L D. F., Urin, M. G.
TITLE; Low levels with negative parity in nonspherical nuclei
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, V- 42)
no. 1, 1962, 304-305
TEXT: In deformed even-even nuclei, low levels with 0-3-1-3 Mev were
recently detected (Ref. 1). These 1- levels correspond to internal
excitations with K - 0 and negative parity. They cannot be explained by
the hydrodynamic model. Thereforep it was proposed that such levels ahould
be interpreted in terms of the superfluid model. Using the method of
approximate second quantization in the same way as in Ref. 1 (Zaretakiy,
D. F., Urin, It. G., ZhETF, A-1, 396, 1961), the excitation energy (h - 1)
is found to be 2 V/
X 7 n, P 1 (q30),kx 2E E 2 2
1XX I % Xv (EX + EX;) Q
Card 1/ 5

S/056/62/042/001/046/048
Low levels with negative ... B154/B112
where q30 r3.Y 30 (0) is the single operator for the octupole moment;
-7
E _V67 A 2 . The energy EX is substracted from the Fermi surfacel
Za - An(6 P) is a constant characterizing the energy of proton (neutron)
pair correlationj 6n , E"(Fp) is the energy of the Ferml boundary for
0 0 0
neutrons (protons)j x -C /AR6 is constant depending on the oatupole-
0
octupole interaction. The value of x is proposed to be the name for nn,
pp, and np interactions. (1) permits two solutions which, al;
correspond to the dissociation of a neutron or a proton pair. For a
given group of nuclei, x can be regarded as constant. If x ia therefore
determined for one group of nuclei from the position of the 1- level, it
will be possible to estimate 4) from Eq. (1) for the other nualei of this
group. The probab:Llity of electric dipole transition from the I- level
to the ground level is expressed by
Card 2/5

S/056/62/042/001/046/048
Low levels with negative B154/B112
B (E 1; 1 0*) =
en. p (qlo))LjL, (q3O)xj, - E).ex' +Ex + EV j2 X
2E E).,
XV X (Ex +:EX.), (2),
X 1 (q30)JXX'j' EAEX' - exem +.A2 Ex+ Ex, - 14-1 -
2-EXEX' -I (EX + ~V.)' 77
,where en Ze/&' ep . He/A, e is the proton charge, and Z(N) is the
number of protons (neutrons). In quasiclassical approximation, the
authors estimate B(El) for low 1- levels (w O with
respect to the occurring gamma quanta from the muon-transitLon,- There are
1 figure, 4 tables, and 13 referencess 8 Soviei and 5 norf---.3-oviet.
Card 2/3
S/05 62/042/002/032/055
-FOf collective nuclear... B108%104
The four referenoes-to English-languago publications read as j-011ows:
Jacobson. phyg. Rev., ~-6t 1637, 1954, D. 1j. Van Patter.
42, 1959;-1- M. Shmushkevich. 11,Ucl. phys. Nucl. Phys.j 14,
llucl, Phys-, 1, 569, 1956 419, 1959,
- - A. Z, Dol,',,inov.
SUBMITTEDs August 8, 1961
Table 1. Results.
Legendt (1) nucleus; (2) parameter Of axial symmetry;
Splitting; M-energy of the 2+ level; (3) 4111-orbital
(5) excitation probabili.ty.

Me Up" 4v

0~.110 '156
255
158
22
3
F
0,1
0,40*
H91" 113 .
4
2 3 0,1 0,3()

_- .
.04
Card 313

40429
B/056/62/043,/003/043/063
2q, ~,j~oo B108/B102
AUTHORS: Zareiskiy, D. F., Urin, M. G.
TITLES Microscopic description of collect'ive levels of nonspherical
nuclei
n
PERIOD AL Zhurnil eksperimentalinoy i tooreticheakoy.fiziki, v- 43,
Z
n
no. ~(q), 1962t 1021 - 1030
T~XTt Vlhen'ip ir correlations of nucleons are considered by the method of
1h
~ogolyulovis canonical transformation this leads to unphysical states.
u
0
_qere th Istructure of such collective states-in deformed nuolei is studied
h
1
by seco d quantizatiowapproximation (cf. ZhETF, 41, ~98, 1~)61). In this
0d
Jase th 'Hapiltonian f7or the collective excitations is represented in a
diagon*alizea form where~from'the collective unphysical state can be
eliminat d.. The unphysical states of the form A+,jC are orthogonal to
0
all PhYB Cal (real) states. The error which results from sl,~mplifying the
Hamilton, an H - HO + Hint to~: collective oscillations is of the
order ok (Q where a is a constant determining the pairing energy
0
Car
1/3

Microscopic description of...
S/056/62/043/003/'043/063
B108/B102
and Q0 is the energy density of the single-nucleon levels near the Fermi
level. The matrix element of tho electrical multipole moment for a
t,ransition between ground state and excitwa state with multipolarity >u
and projection K of the moment has the form,
V/
QC1
OK 0>'= [e7,,J%',)12J' 11, (a);.,K)]' Ja)xK (q),K)I, I'JI2(WXK
1.2
(24)
with J - (612 31 /ata 2; I +Y)E /2E E 2 2
12 12 12~107ud ' (E1E2_'-Y2 12 1 2(F'12_6'xK
+ A2 E E + E is the single-nucleon state energy. In
12 ~ 1 21 Ev
the.oase of ~-excitationsj Bq. (24) determines the reduced 233~-transition
probability B(FI),,j B sp (E ?v) Q0A2AIw 'XK with &n accuracy of ,~0" where ~ 0 is
the equilibrium deformation of the nucleus and B is the reduced single-
sp
pakrtiole transition probability.
2/3

_Z?ARET,)'KIY_ D. F.,_IUSHIMOV) A. A.
"Applications of the Theory of the Fermi Liquid to Nuclear PLotoabsorption."
report submitted for All-Union dn Nuclear Spectroscopy, Thilini, 14-22 Feb
64.
LAE (Inst Atomic Knergy)

; T
MJJGDAL, -A. B. LUSIMIKOV; A. A.; ZARETSKIY, D. F.
"Theory of nuclear dipole photoabsorption."
report'submitted for Intl Conf on Low & 14odium Energies Nuclear Physics,
Paris, 2-8 Tul 64.
Kurchatov Inst, Moscow.

ZAUTSKIY, D.F.; URIN, M.G.
Oscillations of nonspherical nmlei.
no.W18-126 Ja 064.
Izv. AN SSSR. Ser. fiz. 28
(MIRA 171l)

7"1-)r, i I A rj ow h 48

L 4817-6s
XCES.11:10,11 URIX AEWC441~
munber at
to U= L-I-LILL
It is
OTm-r Lt~o
rie:tb of the e:!.-jj.ttarz level by ;Vacl;w~ pr biona:
v il-h im irte re-, as eift the u
af-c~"ect:Lva nucle
the eutbe rc-c- i Tt-lizAlms DA i 6 a -.-Lble tp
rzl; am
-pj~- ekarr2iI b o 4-~7Li~ cl' m-mccb-r- ic am-ma fillarita aid tho 1-ifetirlas Of the
~
,
~
-d -
aced in a crys-I
-A
z
t
m-
,.
acc
r
n r
r LI
c
Cil, uz-12~1cit"t-6. o, ~hc 3j-.Mc Gort. "i1c thwnk F. - 6!iwDirc- '(-)r
-n (-A for discussion-s.
w:Z" 0 fc,

A fl 11 A M 7 r~---TnnZ, -14- T11git
Itute of Atcodic
4 CODE;

Cc::d 12

L 2752-66 Ev rr(rj)1T19aA (m) -2
!ACCESSION MR: AE15024345 UlUO361/65/002/002/0307/032
'AUTHOR., Zaretakly
D. F-j
io.-WIn'teraction and baryon masses
iTITILE:, The.four-ferm
,SOURCE: Yadernaya fizikaq v. 2. no. 2, 19 .51 307-314
.TOPIC TAGS: article, symmetry, witary symmetry, group theory, strong nuclear
I p
''Interaction, baryon, fermlon, pae~iclc physics
nterpret ng" he mass spectrum of
ABSTRACT: A simple dynamic..modal Is proposed for I' I i!t
baryons, (octet and decuplet). The. mathematical -analysis -is bal,`ed on a Hamiltonlain
with strong four-fermion interaction, which corresponds. to a s14.altz-x_- and to the
eighth component of an 8-vector S110) representation. The four'-fermion interaction!
iis made up of strongly Interacting baryon currents. This modeA is used as a basis 1
for determining the relationship Ivetween splitting of the maszi.~s of the baryons ~n*
the octet and corresponding splitting In the decuplet. Orig. Ort. has: 32 formul
j,
'ASSOCIATION: none
!SUBMITTED: 30Dec64 ENCIJ SUB CODE., UP,. MA
NO REF SOV#.' 002 016
=Ri

- 4;~Nll-
SHAPIRO, I.S..- ZAR4-T_qUX,,DJ,.,j LUSH1410'V) A.19
Nuclear pbysics; the mechanism underlying ruclear
reactions] IAdernaia fiZikaj mekhanizm iaderrjykh rea;ctsii.
Moskvaj AN SSSR, 1965, 88 P- (MIRA 18s.10)
1. Akademiya muk SSSR. Institut nauchnoy informatsil..

36377..66 Vdr(m)/T
7590
AUTHOR: zaretsgX, D. F., LQm=omt$-YY-,
.6
6
ORG: none
TITLE:~,Concerning certain features of the radiation of gaigna, IIMU~a!gom nuclei in a.
crystal, latt- ic e
SOURCE: Yadernaya Mika., v- 3, no. 2, 1966,, 263-267
TOPIC TAGS: gamma radiation, excited nucleua., nuclear isomer$ nuclear energy level)
crystal lattice structure, line width., spectral distribution, angulwe distribution
ABSTRACT: Mis is a continuation of earlier work by the authors (DEW v. 43, 36-8)
1965) where it is shorvni that under certain conditions collective nuclear excitation
(nuclear exciton) can exist in an ideal single crystal, and that tMa exciton has a
decay width which differs noticeablv from the natural width of the nuclear level. The
present article is devoted to a study of the singularitiea of radiative decay of nuc-
lear levels in the case when the conditions for the existence of a nuclear exciton
are present, and to a study of the spectral and angular dintributicii of the ga=n-
quantum fb= in this case. To this end, one of 'the methods of generation of nuclear
collective excitation and the effects associated with it is investigated, and th,-~
radiation from a recoilless nucleus placed in a definite crystal 13ttice point is dc-
termined. This recoJ.32ess nucleus is assumed for simplicity to be a two-level isc'--r.
All the nuclei in the crystal are assumed to be of the same kind en the radiating
Card

L 36377-66
ACC NRs Ar6o17590
nucleusp and line splitting is neglected. From the equations of motion the authors
determine the amplitude of the state corresponding to the case when thit isomer is
excited but the other nutlei are not, the time dependence of the deca3r. probability
of the isomer) and the spectral and angular distribution of the gum= quanta einitted
under definite relations between the wavejenFth of the radiation and tho lattice con-
stunts. The results are extended to a three-level isomer and to radiation of M~re
than one nucleus in the crystal. It is concluded that the existence of the nuclear
exciton can be ascertained by observation of the spectral and angulaT distribution
of the gamma-quantum flwc when the condition K - 2xb is satisfied (K - vave vector
of the radiation, b - reciprocal lattice vector). The authoro thank J~p_-&-Ygyt
vetakiy for useful discussions. Orig. art. has: 16 formul".
9UB CODE: 20/ SUBM DATE: o8,Tan65/ oRiG REF: oo2/ oTH RxF.. ool

Vio --fff3ctAL&fm=. tj.2_rj_n_p the correclor. of mitzile, Z2n3tv)dl. J.
C, -T.--*
Applied Chen. U.S.S.11, 24, 5214 rJO-MI(TTF-1. J- m, rn I r--tion
see G.A. 46P 49PNpa.
i=zdisto sourao cUpping
B.R,,
I tt~:~t +

ac of C!, C, a
cc

-7
RT-1237 Z7, w-)i, r.-orrosi
0 mcjejjan-L,,,,mo korroz-4oqnof.-O ra-trcsleivariiia a,'O v
E2~la dpTr-ii 607-610.,. 1947
~d, Alca IaW- SS3R, ~

:NNO000004111000606606
Iii-717". 1,10*1; ;;
I I loss it 91411U11MI; 1? 16 P, a I MuSASMIN-NIM-0 an on MAI NX6,11 ado
A L, 0 -&-j -A -1-A- -L-j~ -A ~ a F - a T I t I AA 111111% 0 zfs-k- 4-1-s- J-1 k A I a
0
0 A III A.0 J.0 C40901 ..1 to. C. go
r Aseflef,11 "A.
so .
~-W-ux Vag* 1i AiNOWSdAhmm mr "MMCM-COMPOMA,
-Tbe Rack"Un d C"N" of O"M ia golvitions of Ammonium Com-
pourtills. K. 3f. G. V., Aklinov (Zhur. Pril-hod. KAimii (J.
.4 r4iri (Am.). IL 47,9~. 1161-1170-11n lt~ian.j 1*1ii- -rn~i,,n
IT 41 ecipper at 'Un-
1irn4 below OWIN weir practically non-mmutive. enfftolon hw~1Ajk111g,r1vIv1'IIv
0 41 In morr concentraleti solut inno. I lw nim so In (hit raw of.N I 144 111 thmir N'll It').
Tkerv uiL* pr"Alortily no corrosion In the abarnm of air. Commloninvolvro
0921,
rkrtrot-hetrilval "utim of copper m culwouo amnionium minplex. 4,%i-L%tk,n
410,31 ,
n(the ittier in solution to the enivic mmpound, followed by nAm-fi,,ii 40',
0001 latter to the eupirous, compouivi at local cathodes sai "ilix-r xtjrfa4,-. sith
&a,-ompan3,ir%z stIlution of colippr. These "urtkins ixert- ronlinisoil aiA
amplified by mrottirerm-ita of currrnt and effective 1:!,tmlW (4`
plAtinurn MI.
' The solution potential of copper In Sil Oll a
w4utium broomes innir negative as the concentratit'n ol the P,fiatim L-
irwrranni. the rffcct twing gmat" in NH40H solution.4- .1. It.
A I a - I L aAtIALLURGICAL tITIRAILSIF C&ASSWICATION
4920t4 41P 04V 944
U.0 AV 10 It' it
0 '0 0 (IF n it N it it a of a ~ 01 ~61416'
0 O's 0 0 0 0 0 0 6 0 0 0 0 %
0 01*0 0 0 0 411 0 0 0 0 0 0 00
4 1 i7i,7a-d-vii -ti-t
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46,444 4OW'" ~41011011MAO' MA-3
(!4% 9t AD -WV*-W- ft*b- "M OVW4 to the W"IlW
latti"
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rising Imm'I day wndw:& lm4 of mm. to 32-43
dapandri it laid of 2-1 kg;-- Tbow v Isr, t*"ing
thmash ay"Am a Well as a5ml War ctucking
canuest be p"Mmew by,chataw or ekcftAytk Oxidation of the
surtacv. at by sambattl4d ck~ OmaW butment at the alloy.
Al. Zt Mir or MA-3 alley Amb do not crack durIng weathering
under tic Sum MA-6 ofty (10% of AQ emb readily under
the" c(McInkmo. but thla effect most 4Wppmn after annealing
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7
The effect of defamflon an tM coffoolon et molmic.
Z-M..Z&mWLJL-J, AAjWW C". V.5,S.R. 24. 821-9
1095MIngf. (r*aAWkm3).-.'ka C.A. 46,49Ma. 8 R.

14iTIL wor-nr# at Deformation an
the Corrosion of Metalli, f In flu"inn.)
F&Af,,.,Znr;tskl1. Zhurtiat 11riklifilital
in V, 1, Uny 1031, P. 477-484.
S" nbstrarts tit patip I and
VAeadrist Ago: firma 340t and M.
R, 1951.
(R general. R11, (424, Al. Zn. CU.
RTJ

.lr&e The Inflo"C" at Drforwillon
P.41.1bblo at MrtshL,I. ft.
"Imm) EL&~rrt;lclf, Zhurmal PAk.
ne 1931. P.
.400 .1.8tract of PlWismiattim nnd
CNimml.-n" Chimical Aye; Itvj#sA31#-
It and 3F,&Ib 1901
. R 11, q24, it, Al. Cu. Zn. 8TI

far 6-6-o-q-0-6 f 0 a-- o-OW-We 0 *a#*
of A/ or
All It A
fit t a 1 0 a if I a L A
004
POK11141S AND FJ`CfI#fllS 00
of reamal at oxides In the
rtf:.4".
so A
1 goal by adds. V. 0. Krvn* and H=_
.11 %U. Vo I Xwbd I Net S. No. :1 4. IS - 18(likon.- 00
I ormt iln-froviulls, nature 4 Attic twocrst of tilching. v id fir FrA h i i-ole
T6 be It,
clitifit. wvfr fivadr will% tile 414144 a Ilitclortrilterilt tior Clev,
frolic vi which was made of miM mill tit, fAhrr tit the Mir they Ir-wt to hvilm I'll?, I'llitillf III-Avr" I" tlvp 'kill' 00
1: ii-Ifited Mtmp 1mvitig the Venrial fi-frowittIA Fr.O,. Tile
00 ml, coulaoird C 0A. Cir Iffil, %in 1,01, S; charltv. TlICtvIQr, .."I It tit" Iwitill' Ill fifill Alill If- 0
Still 01 it I'll"' 'I I... ogid,s f,mill"I cm %Ili.
oi: lite talbillk, lhokilliAl All-I if,,- .11mm f 1111111
ocri milaill alitut INI.N. tit', 1 1.4% 4A F,4)
ir
11 .
40 dild W.1% of 111CIAllic F'. A, thl. pfove,4 goir. .111 file Ito. tile vil,%itk, o4 ill,- In-, e4tiAl WIt
0 ltf~ IV41W U the a110110 VIIASIC" Very b(tk-. 18111614 tile r"', 1111W lite Will 1( 1:0). dl~lljvjt. tit .,mv job All.11 its.,
plave; t1ft-11 the IK)Jeii. A,id Ill, Ilmh-11vold fital -4 h. If)"
10 min. a trms 1.4aligatittio takt, 1 roe
00 litit -1 the vatlitule ti~~ to a v-.111le %lightly a1mve the ittitt.11 "flit-it [IA. I& higher 1, 11delicy 1'. m0m.. fit I flit W
00 tvflc; filially it dit'p,s ititioll, alm"I I %:Admilt I lit ViAllit-4 I lie file 4'AJIHXIC J.11CIIIiAl 441111111 It I)-11iVV VAIIICI file
11"111 thrim."Ir :411.1 Ill" dth'.1c 1110cip. fL&I difftirtilev aml Ow v. J. tit, i-.i~ It'll Ille 6-11-11KIII If
00 0 1
In wiright lhilmit 0W. li"I two I.". of It "'Ittiv Ill ht 1. Oll- It Kl-
"a. lA"tVr'I 411441C I bell IbUIA1111% IWXAII lit 11W 101, 1. roe
aPPC&f oil tile CIIIII-Al" AIVIT1111411liCAl fly Willi. 14 tile 41jille entitc, vlv~,l lit (11" A. li'm j It.. .4, 1.1 lilt '111l'iti'm
tile lattic now 64 4)11 lite all'A'. 1`11114 1)11 file Illmo All,mll
Min from thr Fc all alutilt lite calluxle surface. fly tW thotle It but-blit apiwar jild fix gmitoimal
time thecurrvia mirtiXth fell ai.-ii(P-t tozVro. FLO IRN-Mi" celgion-, of the ca
drup, luck to Itte ame VaIll, a.,
v coniplettly dissAv"l isiall nii,tallic Fe dectmles to (1.17 mt tile
All" etchistit the 111,9110ill PITIlle, Ili 11W oxide cill't
hav- alluOlt vvioc I invaii4 that IC.(), WAI
Wifely redaevil during tlw jitmvio, while Fe" rentained
mwtk-~ay unchmuSed. The mechauLmn (A etching #.An
r !wee
me IrwrWriled sLi ftAtm%! (Sri 11k. A1111110 Fe, I itim vir
41 faftn"I. On 11W micitmealholk- ItziniviI of 11W allotle 11W ti
11 kist,' lm~,Rnr di-Imovilrd. Oil I IW-valt"fir rise If I k-14,
U1101AIVIIII foe
'is' tre
ISO., 0
t 1 491 milli, d.9 C., lot
alliti
is)
U14 AV "S W a to if it tm a left Ii rifilitt it of KW n i M
0 006 (if

00000 0. 0 0 0 0 0 of
-
4~4--
slkj: : 4 0 0 0 0 0 4i 0 0 0 0 4
4
4 0 0 0 0 0 0 0 0 0 0 0 0
10 if t) is 14 0
11 1 6
6
4
W
nu nuls-isnam r-11 R U m a mmawastoff a aco
I~ AL
&
"
.......
7 00
A '

CIO 00
so
00

Comments on the paper of V~ S. Zarin. cafradon
PTMII~ under dmps of scilutfams.
J~ PAY. Ch'rm. (U. A~ It.) 13. 4

'
-00
00 a 4 1A (1,
.
ROPI't, V. S. buitt 1
0o I - 11 -00
04 f .00
go 't me*
=00
06 a szoo
000
00,3 ago
Pro*
00 loo
6:00
S I L A 61TAILLUNG11CAL LITINATM CLAWIFICAMIN
-1-- - ~. - -- --- - , - - .
via., 1-.14"
ctf
U it AV on 11 (V tv Pt fe it P; ff x CIO It fl! tv It 1
000000!000 0 0 0 0 't 000,0001006000*40044000*04
Z:00
WOO
tj00
~-lv' i 1 woo
it, to*
11 fatI

0 off 0 0 a 0 0 Ill 0 0 0 0 0 0 1 0 0 a o
0 0 0 * 0 0 0 0 4 "V
f
B 14 V )q U 11 U k V
A 1, In P, 4
a- A
LL r U A I j &A W Q
0
to U
1
Ai 41
-
.
1
41

Cormalon of Come In sla"Us Mutfoul of ansmoaluns
tompounds, 1. Tho nw-Malso of W o"O". V
M.
Zsrelskil SCRI GL V. Akimov. J. ApWW C".
,

W. 8%. S. R.) It: ItOl-71(in IT'hh-h.
1 0 LU in solnl. of Nil. mnrxlq. i- allOwl-A
lit f to thl" (1) rkt-ttuchetAs, mtfit, ~-l -00
C11 wit h-1W I'malion of CapnXII-ammmlia rr, 00
1, , I"a ,, of emosinn prix"" with t1%- .
Chem. ori.uciun of the cornril"
4 :.410
111ed by tile 0 of the air to cliptic-4111mollis ")mple'l;
and (3) clectrochem. r"luction of the cupric-druntouia
go COMPICI to cuprou%-ammunia complex. The soln, of Cu

:
404 procceds rucilletically in promu (3). which toother with
'S M fonus an independent mle. Becalm of incomider-
Able &wxn. of the copMr-4mmook complex tation, thv
Ot potential shiftistro"ly totbenet.sideand thediffer-
trice bet-, t &"k and catho& rewhvq a considerable
value. The Cucorrosion islestintensive in NII.CI multi..
ptesuntably llecause the complex is partWly tirmtoyed and
therefore its potential is more Pos. and the difference IPC-
So ivtrrn the anode and mthode portion,; is matter. InOw
atr"Ure of air, Cu is pract"lly unaffected by corrtnion
00
ir the NIT.011 and NIIXI stArti, The velotity of Co -
j rotrusloil itwfmscs with the increase of 41411.olf ""bIll.:
'40
00 it increases with NII.Cl conen. In N unit then drt-rm%"
with further incrmsL of tile NIWI conen. NII.CI soln.
urrodrs Cu toasmalkrelegreethandnes N11401L
00 A. A. llmlvwny
00 S

00
V~ '-1 1
'

le 0 0 0 0 0 0
r
13
. It K it 4 Q
a 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 a 0 0 0 air
~
to 0 a 0 0 * 0 * 0 0 * * 0 6 0 0 ~ - -
: 0 a L It' 0 0 Q0 0 Q S f 0 9 0 # # 0 f 0 t.0

W14000* 0*000 o a fie is 0 6i i1i i ii i '41; 69 i 00 00 0
0 0 11 11 1) w I$ is a It it 111fuldo b~j 4194 01 till w is -0,
it p Is
00
Ilt --p -lip
00
00 r
00 1
00 a .00
11=1 Daormation & Cornmim. Part 11. Aluminfuns,
so Zinc, Capipwr & HIM. Chemical Age. v. U5, So 1, 1 En I
299-3W. (Bak-d on faix,r by E. Nil-Zarchri. 7%urnal
rikladnw Ithima (journa us Appbetl Chenustryl, v, 214. May
i31. p. 4TT4PA.) see
Outlines exie"iments on effects of deforming stremes on corro- =
tion of aboic materials In different media. so
i? .00
so
so 0
wee
to0
L-0 0
S L A -11ALLURGOCAL L119MAY01 C A SWKA;30.
L I
to 0
s ~4 8 4;x 4~' isi 4
U A, lua
126! Nil 9% It (I if Is a (W 0 0 0 1 Ar IN I d3 a 3 4
0 0 0 0 0 0 0 0 0 4 We 0 0 0 0 0 0 0 0 0 0 0 it * 0 0 0 0 0
0 0 0 e 0 0 0 0 : : ; 0 go 0 4 ojo 0 * 0 6 0 0 0 G * o o *so o 6 * 0

fif
00)#
1W
00 is
go

all
009 -

Oo
1

In
'

of A J
=M" Jrhtn" (Jour'
114 AmIstrY)
V. 20
Sept
.
,
.
rrosion resistance of 1-mm.

0.95% nt4lol 5.62 to ISM Al-
0.38T Un; 0.00% ana
SLO 0 05"
47
con Ill 0 WIN Investigated under

a
i t

t o
evalw stvas and at
empt
alr a
d ures from room to 4"- In
I
l
n
te Is
re n var
.
ous other madis. At.
tmProve atress-corrosion
b
l

A
tr y co
d worktag or heat
It were unvuccesotw.
L
_1111.4
141,341 01, 0.. dot 1431111
0 U W AT 10 1$10 it V 9 It 4 X S9 it
0 0 0 0 A 0 6 0 0 : : 0 * &0 :
00 No
k~M T~M
imp ~.5 0 1:44
400
. 4
roe
roe
:30 0
goo
:900
ISO*
ties
too
An L 1 4 Md 0 0 4 1 Mr It ID a 0 1 T
0 0 0 **see 0
0 0 & 0 *Ap 00000 0

lot 14 Oil 17011110161 11111414laU 6;0
00
94 C' CMcking of C"t M".
a
00 Ala
Z. ts L 1:~ (Win
00 to Prikladaw MAIM11
FIX 'A.
flour of
P:W4 Chemistry), v. 20.
00 it Hapt, 1 7, 0
7. P.
ran
at -currostolt r0414tancts
orcast
'n ""luw~ Of thO ^11-Y Mentilo,d
In
the
00 Plrmdlng alutract. and of "00
&no an* COntswal 10% At.
00, 0.
we ve 0.04%-Fe. an 0.9g% 81,
The first waj not
BenI5ttle"NotlLrefia-corroalon: the no*
c
rm Of the -and contrary
h
cc" worked form, Is Istoo not
G:Oo
k~ -x
00
"asitive; the lattukirwr 11110Y has U slight tendency tom"d roe
t
00
stress-corrosion, which can be eltainat*d by proper heat troat- 300
4900
Air
rcnt arA quenching procc St
Voo
looo
t1oo
A$11-11A 1111ALLU"ICAL LITIRATUIC CLASWOXCA cgs*
108 016
.1 To Md 0 a 1 3r 3 q
0-0 0 0 0 a a 0 0 0 0 40 0 0 0 0 a 0 0 0
Is
-00 V 00000 0 0 0 6,00 0 00 Ole 0 * 0 0 -0 0 0 0 0.0 ft. 0 Is 0 0 0 a ol~

linif, V. 24, MAY 1951, P. 477-M.
Hdo abstracta of parts I and 11,
A*=klW A##; items U4-It and US-
ML
1 gateral. R11. Q24. At Zn, Cu.

to it Is b If M it A SO It 41 U U w Is
AIJA_
oil
%*464 .,
so I
so
00
.00,
.00
(In Rua-
612Z Cact"Aaft CmCkIng at nedum Mays.
Mcnal Prikladmoi Khimli
sinn.) E. M. 7A"kil. Z I so
so (journal of AppI104 Chemistry), V. 20. SOPt. 1947,
p.
The cormlon resistance of I mm. sheet containing
5.62-5.84% Al; 0.95% Zn; 0,38% )fn; 0.09% S.,
Oi
snS 0.0511. Mg wu Investigated undtr conditions
of tensile stress and,,st temperatures from room
to 420* tn air and I various other medla. At- L go*
tempts to Improve stresa-corroslon resktance by
cold woridng or heot treatment were unsuccessful.
goo,
lid
we is
Use
too
ASS-ILA
.3. C- got -OCl Ire o
a" amp M
U U or 00
a a R IN R on I S a no 0 so 0 '1 5 a It
&-:.* 0 :~G 0060 so 0000 0 0 0i 06 s.
a Z'O 0- so 00010 000 000 000 00000 SOOL gigs go* W

A41
004
0*
100
~ve
OOX
002
I
90' k
64 Ir I
00 it
004
*0 01
00.)
OOW
00'4
00 .0 0 a 6, 0 0 0 0 0 0 10 0 0 0 6 0 0 0
101 uu~ldlj *!I mpg 41 aum
-A, P. 4-0-c-A.
10~ Oo_ A" !!I- ti,tol
A-D F*6*401141 o4ep
sla Cwtusioi-Creckbw of Owl Kaguslum Alloys. Vn
fX. 7^tVAWI, ZkmraW PriktW"
Russian.) I K .
a
mij (Journj 6r"Apolled Chemistry). v. 10, S*VL
1947. p. 930-340.
Strus-carradon re&tancn of cast Ug, of the
allay mentioned In the above sbatract~ and of an-
other an* containing 10% All 0.20% Un; 0.04%
Fr. and 0.09% Sl wore Investigatod. The first was
rot stnOtive to Otma Corrosion- the cost fnrnt of
Ow second, mntrageto the COM-worked form, Is
also not #oUsItIvo; ]Alter cut alloy hike a slIght
tendency toward streea corrosion. which con be
eliminated by prorr beat treatment and qtsc"h-
edurt. wh ch Is described. The mothanism
In# Prot el
of stress cortodon In cold-worlted and east UX
alloys Is uplaine& 12 rer.
OPO
A
"SO
-00
of
lee
:00
Solt
moo
46.0
00*
CO 0
009
so 0
49 0
ago
:60
Ala-ILA SITALLURCKAL LITINATL49 CLASIVICATION
Mff It IWO $1114 A 10. spow bodiftv 00
~ %jAJOj .4 -- S4340,1 WIP QkV 441 4"1"' 134111 OW O.V pit
u u AT -0 As t - I I - I I ' "
111 . ; ; ; I , r It ; ; ; a t", K . I.,. . . . .
0 0 :; 0 0 000 0 0 41 000 0 0 0 0 0 * 0 * 0 41 0 0 0 e
T4 661000060*09 0 0

Bases df 40(timatfois an the c9closica of tattab. K St.
A,o4:LiAjL_/ r~"Pttf~ihj& Kbip". (I. Apptwtl Chien
II" of (tilled full annralc4l hig Allnyb
%%Iih (1) 1 tls"~ %11l. 111). Al Wth, Ce 11,33, Ntn 1.677o.
1111 At.- IQ. %tit 0.:43. Ni 0. 1-4 %, anit I Tnm. lbk-k
,t 32
ed C it M. %fit it. . "A' 0.10. Ni Cc Mice,; I flint.
thh,k Cu; A tiiui thirk In; anit.1 lum. thkk Al Were sub.
1, AM lo knomil trn%ilr Allt'.srt 0, anti the deffirt of co"o-
-ion W41 littil. by the 14*0 of Wt in '214 hit. With 1, stress
to 111)", of file limit) h4if not t(lect on the coltmion lit a
It Na-0 MAII. Jbilliffell 1.0 pll 0 81; ill Ill"I. r1publife,
wm"k,o in-I ilvvirtw, With ,. pa,wi thron h
lims. lot at-ut * - 40") theu inviraws. With lit I.'
it, I At MICI.the r"Ul [Wa4ses thit"1111 a low l"all .
tlj,-n J'Alls tit about the %ziur value as with the unstressed
untal, Willi 11, "va;-4tmI incrrarm Aughtly will) 0. NO
latte vilivi .116 the Culit"m M th"r his mll"Y%' llwy ate
highly Itsia.111 to Corro-ion 11) rxloulc 1.1 all ilkil"llial
al m., The lins of tensile strength tit I Pum. thk k Strip* in '11
~CAFJ ILIVIIIS bee" 5, 16. anti 'Vlop, only fut, 11 It. *1141 Ill.
tesp, The cimicnityu of altmed V lit 11.4 .11 11C) illefral"
%ith v nip tit about '4;7o, then renusim conlt.; in 0.11 At
V.iCl. It I% von.t. oil to atiout a - 711e;. ilwn Inetra,,eo (in
1.190 ilss'i expis.). Willi Zn fit (012.1 At the lov of
"t. IncleAliet with 0, the km 44 troatir sirtogth 111-1 de-
(TOMS, fCMAlrs coast. betwiren d' to and &)V/;, thtts In
With Cu In 0.1 At (NIf':.;(N, baffrted to pil 2.
file rintosiou derFraws mmur"IlAt Willi infirit'ing 4; in
it 1913 At 1(0411, %fir." hot "to rffcvt an the fittloollm. With
~1~1 in I.F. At 11,4411. (fir CtIfful,14141 i"VICOW. willt 0 only
VA ty blifthtlY. UIUIC 1110MCAmly tit , - N. T.

Corrosional aackW&.of M!" allay AZM in viazious
Inedid, "l_O;tf Auju, - 11441dy Mad, N*.Ihk NX.S.R.
$8, 77. Me alk;j (AfC "tilt M. I lit, 0.0
IN) w" exattki. lit 110M. NaXth, an,] NaCl-KiCtiCh
stilris. Smd) concns. of IIjSO# atmIcrate cruking type of
co"Osiou powtily by acmtuatcd potcutL-d diffuences
betweto ;he &raise zones and the rest o( the material; in
0 4 X an-I IN(sh" 4M arnetal mmlakwl pfedmilin4les, I"
vo Nxt.41* whm Otat.-I
Wlua
InAve avvIrtmea a"WIS-munk"I hy NeVC1.41 Itul"lint
1%1111 uhvu ultlnl tu NACI Vitt&,; the 11141. ClIevi 4xvU111 at
alm-af (10.1.1 .11.

W, see
it )d 0 Is jP as is A; 41
It 11 11 14 1) 4 V 111 It 2D I I_& I... I.D 4, '?'-~ - # 0
V A.- t-j-11-Al ... A-
141 fte 1W,
00 07acking of mAgneglum, AUY-T.A. F, X. r-*
00 -i IV-8-s-H.) 20, K-6-9 1-1 4' cast tam. 00
J. Ap#wd Chem. U.
11414f= SUM, Ibid. 101 x
00 Aits! te"t" were run "a 15 X 3 min., cut ft
Mcf-11 cast in land Of 30-W' and
the Ug alloys Itlection UA-3 (A)
5.84, Za 1,10, Ain etched, bent under k~"nowu Ictids. ~Ntg ishowets 914) sires. I
tie Si 0,14, Ve Mir.'), I_ICCtMj AIA-I (0.15, U. 122
anrQr,~ romon. Likewise. and its Ltmitrast to iti tichl%itir in tht
o.oi,, and %I& (oz3, f).07,(1.03.0.02.0.05). rolled state, cast MA-3 proved t .'i%fa'lt: the lot I
00 at 420' and etched, its the f,irm of rolled ribbona I into. crack under I I ks./sq. mits., Olt 0 be it
00 thick, 13 mm. wide. IN) altu. lot'if. bent into 1000 I)f PrAfCd to still. CXpoince
only after W days. noue In 300 dAys under Una [Irv SITTS10es.
It radius 8 mm. And subjected to ditictrzit kmown 81"3143 it, t.p-water Spr.1y. th It
00 14 putting together of QjWt the ends of the loot). V Crack VIPPeilrell. under 11
. In kg After 11) IIIWfh4' RIO mily W"'.
eff a um. exinysture, the ]At crack allitcoml, III lkI %-;J,
if, under 15.9 1:1.1stil. film.. after 5-11) found under 9 film. A much
00 1! after 1-2 d* a
days undry 8, littile After 3W asys "ithout sigtis. trivy Its *firm rottusion wits Ij)ujId Kith cast MA-6 (Al
0 0 It, &wdu effects. but after Ittsiscir thurs. were observed in 10-0. Zil 0. %in 0.20, Fe tu", ,;j If.( 00
:W 0J), the lit crack, s
00 immersion in distd. 111,C), mind. even more slowly, its a tapI- in Alm e fire, appearing within 22-21) days under
water spray.. Vndcr the sartie conditions. gentital (non- 's 2.".()*kX1r Izoo
IT mM-; the cracks are m"nlY JJMK 9fRi13 =0 0
4640 Stress) Corrosion was itisignificiust; nor did any cracking b
o"and"'e". lit t&P-Wat" 213FAY. 'he 31WIF is; highly re. Zia a
occur in siantiples bent (Plastic-411Y) into & 100P but not silitant, no surfaft cracks bring vigibl, in 11) tricsithm, only
04 .3 subJected to an clAmic stress, In distd. Ils,01 in the All- rucroft-o0c Intemyit. Corroljon wit;% cininbliziff of ShI&
00~1 W= of (),' the tendency tt, streu cursicaLioti is dtata" -crYstiti"lls- fmtntl"indistil.ll-()c2u%c%tiuchn)(me
iftwkedly. The aspect 61 site%% cccr(llsim is very (blycl- filitill litt"ll CVrrGRi4X1 than WJW 4SIV4y. Cnt,ting wl
0041 rnt frots: utdinAfY turriju,'n; file &USIACe Of ecilCyLe't h
Plea often remained 1'right. 0 1 1Sun grease f"revente'd st"M costrusilln fill 3 Ye-4rit. 2~ 11
I stress- further contrast to the #,Lqkd alhqv. be.1-tIcAltnent If
corrosion cracks arc sects so pj.. IxAh skjos boundaries luve a '"Alked effect On the site'% cnittwinn of cjst NIA'Awi. 0
0 =it 0 . I through VIC ST41111. Annealing tollawcd by Three firs. annealing at Ala)% it followed by CMI:ng in the
= An,
under diflcrrnt cuuilitions. amd temPer"ill' had furnace, lowr" th"' r1mlista"Ic (the Ist. crack appearing. Zee
~ittk iauctscle all tisc Little of a;pearatice of stress-cot- in distd. Hit, in 54 lirs. under 9,11 kg./,q.
Ilwats cracks. Chem. surfacr tic-atments reurded some- MIT.), but, if
followed by quenching in seat" at 2[j, or at 1q)o It 11,
Are :31 gi whia the apprustatitV of the Ist C72 W t!e 0
ck without. however, -creases the r~wlsitajice (to &ssIjr3.). I"SaIllp in
1wevtoting hilarricolmy, Relatively best rewlts "ere at 3)', cracking will muce 11roflouncedly illerrryll,, -U'W I tie*
(kialesed by it odic ujidaliuli In a solts. X,CrXh 101) + with crumbling of inso Ile I Iuencbd " I - L-00
gra " relis n samples
I, SaII&M ,A) X.il. Soirface treatment with sit"I balLs was At 100* the cracks were moote nearly twiented in ti
.if no avail. The MA-I alloy alit] Mg arc to! stabir" to lion of the str-- 1'"Iticutar sensiti it dircc-
vity of I lit- stress. ik
e.1 01v il~
0 a a 2 1 it
-q1
U IS AV SO w 0 0 it 2l it is a It a PC n 1 00,600 0 0 IS
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-

AGRANAT, B.A.; ZAMTSKIY F L
Use of ultrasonic waves to prepare a stable drawing omulBion.
Sbor. nauch. trud. GINTSVETMET no.33s369-376 160. (MA 15:3)
(~btalworking lubricants)
(Ultrasonic waves-Industrial applications)

S/137/62/000/004/068/201
A052VA101
AUTHORS: Agranat, B. A., Zaretskiy, F. I.
TITLE: Application of ultrasound to the production of a stable drawing
emulsion
PERIODICAL:' Reforativnyy zhurnal, Metallurgiya, no. 4, 1962, 311: abstract 4D197
("Sb. nauchri. tr. In-t tsvet. met. im. M. I. Kalin1na", no. 33,
1960, 369-376)
TEXT: The investigation of the emulsification process acted upon by a
strong ultrasonic field was carried out on emulsion of the "Moskabel"' plant.
For drawing Cu- and Al-wire the'plant used to prepare emulsions by boiling a
soap solution and mechanical mixing with oil and water. These emulsions would
usually stratify in 5 - 10 days and proved unsuitable for further use. A
series of experiments carried out to produce a more stable emulsion by meana of
ultrasound has shown that the disperisty of the ultrasound treated emulsion
changes inconsiderably, and it preserves practic 'ally its stability during several
months. A description and diagram of the ultrasonic unit for producing emulsion
are given. K. Ursova
fAbstract6r's note: Complete translation]
Card 1/1

XOVILLENKO, D.H.; ZARMSKIY, G.M.
Bentonltes in the Lovushnianakoys deposit. Bent.glizW Ukr.
no.3:3-13 t59. (NIRIL 12:12)
1. Inatitut geologlebaskikh nauk 41 USSR i Ukrainskoye,
otdoloniyo Vanuayuznogo trosta stroltsllno-takhnichoultikh
insrulmniy.
(Dniester Valley-Bentonito)

SORKOVICH, S.V.- ZAREPISKIY, I.I.
Effect of immunotherapy on kidney function in burns. Xhirurgiia 35
no.7:16-21 J1 159. (MIRA 12:12)
1. Iz patofiziologicheekoy laboratorii (zav. - chlen-korrespondent
ANN SSSR prof. N.Aa Pedorov) TSentrallnogo Instituta ganatologii i
perelivaniYa krovi (dir. - deystvitel In" chlen AM SSSR prof. A.A.
Bagdasarov) Ministeretva zdravookhraneniya SSSR.
(BURNS, experimontal)
(KIMMS, physiology)
(Imm SmmS, pharmcology)

C,
Water motabolim isher I*qgonmw Wassil Uismaisiom-
Poltd,
T~,.LMilljXt9j MAIM, I
ra dro -un (AV.
at 11.0 coutient in the rwipkni's b6A 0m
U.;M!j.),,xhich Is ioUovml by a rW. fftchind 1.49."16 (aV,)
Axive sionlut Its %I-4N Ism Ci lavill (tsilows IhAf 0( 11.0.
Uryth"icytex jurtic*le In thechanctilfrivolmfo ax 4bowis
1,v enl4ancW ability for uptake of IIA) an4 Cl wiffila 1-2
tAY% Aft0f tMISAItOU"l. lthfiVidUAl WAI.O. 01 ttYlhF"C7lV-
inclum io 140 mullillulism pflvmtv. liNflorlary iLIKI
lW4101my Pg(%'t'WWt aj~) X" Olit"11111 A
itiff (ditimil afhf 1401k, P"I~fhpn
Lim 16iur acig a*,i irgul4w W k1w thosiges, whkis take
I-Live. C., M. KL"41msll

ZMTSKIY., 1. 1.
.., -heskogo sostava Krovi txlsle
35481. I=enehi,-e Khiricheskogo i morfologic
perelbraniya izogennoy kvovi. Vracheb. delop 19/.9, No. II, stbp 9E;5-88.
LetoDis' Zhurnallnykh Statey, Vol. 1p8, Moskva, 1949

WAI*r metabalim In healthy &4d artsmic subocts ilftot
bloott transfuWad. 1. 1. 1AFritkif (Mmi-Ity 4 JIL-ilm. I
Nt'iw"11 1. 1'etapest. IPW 2Z - Mi. .3. 65-xi lik*il); cf.
C.I. 44. -The cfytltrm;frs of tht- Imipient take
active p.irt in illo nictalio1hris in the Ist iliys after trani.
fu.-I,m. T'hcycnffgetk-Aflyrcl;iinfigOan,linervatinv.4,
Oil the day of trAftxfti,i(,n dittreii And elindmithm 4 C1.1e.
Ollie. Litter 24 4M hm Impth mr. Tranifum,ai fir.0i to I
Ir", Immaiv tLI -A dAyk) drefine lit volu-n. 4 1.4.4 twwria
ILUVIYOUNIIIII). III ittle"lic SlAtients I.Till'.41,111ty ,q Ilw
4.~ISAIIAry visdi3theliuns im-trAtics. TIw McClurc-Aldriche
tmt i'l tick-cleratril in the Ist .0-3 LILLY$ after tran"I'mion,
0. M. K-milawif

ZARLTSKI,Y., -1.[1-'jCandidate of Medical scienco
"Problems in Connection with Blood TramfUSiOd'
ModitAnokiy Rabotnik, No. ;3,, 1950
--W-11691, 5 Jul 1950

ZARM-TSKIT. 1. 1. 1
L.-
Present problems in hematoloor and blood transfusion. Sovet.
med. no.9:38-40 Sept 1951. (CULIL 21: 1)
1. Report on the 29th Nxpanded Plenary Session of the Learned
Council of the Central Order of Lenin Institute of Hemaiology
I and Blood Transfusion held in Pay 1951.

ZAB3TSKIY, I.I., kandidat meditsingicildi nwil: (Mwicow).
Certain remIts and -nrospecta in the developtent of hematolD~;r and bicc-d
tranufuoion. Sov.med. 17 no.8:4k-47 Ag 11)3. (?3-U 6: 8
(Blood--Transfusion)
1953 Seasion of the ScLentific COUW-U, rfentral. Order of Innin
ImUtute of Homtology and Blood Tgawfusion

UEETSKITPI.I. (Moscow); MIMUYLOVA,I.A. (Moscow); ROZANOVA,Y.S. (1405cov)
Ametional. state of the kidneys following tranaftelon of comati-
ble blood. Arkh.pat. 16 no.2:26-31 AP-Jo *54. (NT.R. ~.3)
1. Is patofiziologichookoy laboratoril (mv. prof.
TS,ontrallnogo Inatituta gomtologii i perelivantya krovi, Hini-
steratia zdravookhranonlya SSSR (dir. chlon-korrespondent AHN
SSSR prof. A.A.Bagdasarov).
(BLOOD TROS7USION, (KIDMB, physiology,
*off, on kidney funct.) *off. of blood transfusion)

I
ZA;'(,,T.SKIYj I.I. and FAYi13iiiiY6, F. P".
Some Jest ~,xperimental Ind Glinical Data on the Field of Hielliatolo,-y.
Voyenao-lieditsinakdy ,hurnal, 1,11c, 1) p 15) lq,~5-

TEDMOV, N.A.. professor; URZWKIT. 1-1- (Moskva)
Rama functibu following blood trawfuian; experimental and,
clinical investigations. Xllnmed.. 33 no.11:28-36 N 155,
(Ica& 9-.7)
1.-Iz patofixtologichookoy laboratorli (sav.rprof. H-A.Fodorov)
TSentrallnogo inatituta gematologil. i perelivaniya krovi,
Hinisterstva zdravookhranonlya SSSR (dir.-chlon-korrespoadent
ANN SSSSR prnf, A-A.Pagdamorov)
(mmusyss physiologyj,
off. of blood transfasion)
(BLOOD TRMFMIOH,
off. an kidney fanct.)

ZLRZSKIY, I ,I., Icandidat meditainskikh nauk
~~*,
New trends In the field of hematology and blood transfusLan.
Voen.-med. shur. no.6:8-16 je 156. (HIJIA 9:9)
(BLOCID)

USSR Human and Animal Physiology. Excretion. T
Abs Jour: Ref Zhur-19iol., No 22j 1958, 101947.
Abstract: activity of the tubules according to diodrast or
phenol red were determined. The investigations
were conducted on the day of transfusion after the
emergence of the animals franthe state of shock,
next day, and later every two days until return
to normal. In heterotransfusion and in isotrans-
fusion, a biphase change of the kidney function
occurred, sharper in the first case. During the
first phase (1-2 days) after blood infusion, the
excretory and concentrating powers of the kidneys
decreased, glomerulus filtration and the kidney
blood circulation decreased, the filtration frac-
tion and permeability of the glomerular membrane
increased. This was confirmed by histologic data
(edema of the medular layer of the kidneys, edema
of the glomerular capsule, constriction of the
Card 2/3

VINOEUROVA, G.~.,,,Q-AR3TSKIY, I.I.; MIKHAYLOTA, I.A.
The effect of blood transfusion. blood cozponents and plasma
substitutes on kidney functions. Problegemat. i perel.krovi I no.2:
48-~2 Mr-Ap 156. (MRA 10:1)
1, Iz TSentraltnogo ordena Lenina institute gematologii i perelivaniya
krovi--(dir. - chlon-korrespondent ARK SSSR prof. A.A.Badaserov)
Hiniaterstva sdravookhranentya BOSE.
(KIDIMT.S. physiol,
funot., off. of blood transfusion, blood components and
plasma substitutes)
(BIOM TRANSTUSIGH
tiff , on k:idney, f une to)
(FUHKA SUBSTITMS, off.
on kidney funct.)