SCIENTIFIC ABSTRACT SHIRYAYEV, B.A. - SHIRYAYEV, N.P.

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• Collection: Scientific Abstracts
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• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 23, 2000
• Sequence Number: 8
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SOV/138-.58-12-4/17
AUTHORS: Zall-arov, 11. D. and 34%iryayev, B.
TITLE: Vulcanisa.;1on of 0,'ofla Synthetic Rubbers Without Sulphur
(Nesernaya 1rulicanizatoiya nelcotorylch sinteticheskikh
kauchukov). First Comffranication. Thermo -Vulcanisat !on
of Butad'J.&ne-Styrena Rubbers. (Soobshchen-1ye 1.
,rulllcanizatsil.!a bul~adi-Yen-sl'irol'nykh kauchuh-ov)
PERIOD I CAL: Katio huk i Rezina, 1958, Mr 12, pp 11 - 15 (USSR)
ABSTRACT: B- A. Dog-adlikin et al. (Ref. 1) found that n~arbon black-
111ontaininE mixtures Of SKB, SKS-30 show the t-lypf-zal
effect of vul,.-anisation when heated-at 180 - 20000. Zx-
il OUL on o -iva'-on
perimen'.s vere carried t, , the thern, -,ruloa- - %,.L
of variou6 tyL)e.9 of nitrile rubbers '. and also on the
(,ffect of sorne additives 4rd conditions on the process
of vuleanisa-Uion and on the properties off the rubbers.
The rvbbers SKN-40, SKN-'E~ and SKN-18 containing 36-24,23f~-To
19. 10% acrylonitrile -respectively were tested. T he a e
vulcanised at 14*,'~, 153, 1663, 4nd for
20, 40, PO ani '41'0 ':E, n -1 -,nc-
1_1 Ij - are obtal-n~,l
an;j ZT 1'
I , ov " -- , A
Card 1/4 -L"r o m 3 K 1 i - 4 0 7., h e n h-r- t,, c, f r? o m CO t o 12, 01 nu, tz; On in-
firetu;ln,a ;ae tle::!peratt--~--L -.o 19'ZL'000 t.-e mocb~ltas ~nd the

SOV/138-58-12-1+/17
Vulcanisation of- Some Synthatic Rubbers Without SulphAlir
,itren~:t1a inorc-ase :ontirucualy, but relatlva and
e1c)-nCation No in thq
prope ri; ie wilen tzo 11~1171~,O. Zi
proper~;ies cf the vul-ani-
on the. time of ,-ulc_-anisati,_,n chanr_r-,:- in cnar~k%'.-er
'Fir-3. 4 _--nd 5), Thz ter.,pei-ature at viiii-h the ri;io_-~~-,_Ilcani -
aal-izen proreeds at sufficiently faat rat5, and the preper-
4-
eal of 4;he depend cn thq T,;,,j~e of. the rublcerj
or. the -Juntant of P.!Lrile Lroul,-s ir. thE rubber. Th 13
a ju- e I r. c r e, a 5 5 u o n I n, _~ T. e a s 1 t h- e t e r~.P rA'- u C e n th e :S a -,a
a-3 _1uv1rC vuli-anI.Sat Ion *;.,ith 3ulp1har. Table 1 --h.)7ts
LOMe of the thenic--7ul,,,an.3atenr?hVh here th-,~
hi-in- -t decra~ of st.rength. Sim'17.r rx~aults 7ere cbtain,~-~t
durirz the therrre.-vulcanisation of rubbar rIxturea which
did rc~t- con!:,-Ain fillers. The rmo-vulcani 3at ion can also
be c-6sQ-t7aq in rubble.rs oontainir,,~ othor filler,~. SKI;-Zfj
mi)ctluve. containinZ, -,,.aolin, was vulcartised. fur (30 minutea
Card 211+ at 196cb. and the the rnio=vulcani sate showed strenEth of
30 k ;,.nd 242--2' 'k_111rMe modulus at 300 elcnCiitt4.cn.
E/
CompLirutive tests carried cut with ,Palpliur 1~

SOV/138-58-12-1+/17
Viil ;aniz!at4-,-n cf Sorw-
of nitrAle r,.Aj",-r3 prepaze-CA fr= 2tandard
vvhI,-:hmre -.,,al,-anised for 40 mint-Jes at 143eC. Sam~ples
of the rmc--.iul,7ar--',sate s .-,ontaininZ fillers were also
repared 4--hese viers vul~anlsed for 60 mir,%tes at 16-30c;
Table 0 ~ V
- . Thcr-rioc-vu-'~anisates viere shown to havc
~
poorer, properties than the sulphur vul.;anisates ri"Lth
reapect to their strergth and relative elcrZation, and
also in their resistann-e t-oageinL;- They are of soft
ccr,sls,ken3y and less therTo-stable. intermoleoular
1,opda are of greaLer Iraportawle In these vul.-lanlaate.3
thar. in sulphur vulcarlaates. Testa were carried out
on --;capar-ir;,c I
_; the dagree of aLeirZ2 of the twc tyj~ea of
rubber vulnan'satG--- at 1200C for 72 hours. Their frost
resiatance and brittlenes-&-viere also inTrestiCatedv and
it vra-;a found t~7-~t therma ~--,,ul-lani sate a are Ecre frost-
,11evista-r-'L, than oulpnuryulcanisates. Metal oxide-z'
vli.sn used as addltiv~&j, ir,~,rease the rate oil %-alCani-
~'iation an'd improve the physico-mechani.,al %harasteria-
ti,,s of thermc-vulcanisates (FiL,.15). )..3jdjc% :ubstan-
fauch ae sulphurie aalu) and metal chlo-
'i
r ides (3U& as Zr,"12, AIC13 and FeC13) also ir-fluence
Card 3/4

SOV/138-58-12-4/17
Vul, '-anisatior,, ef Sorre Rubterc Without. Sul;,-ur
the -ir-aL~anisaticn process. Wher. -,q~xg ~.!-,6 latter -ub-
Stal'iO-6 vul-7anisation ccours a,, '43(-'C. Therv ari- 6 F'-r
L
2 Tatlos and I Refe-r6rIce'll". I EnLlish rAr,,,l
Iv
A33001ATION:
ln.~;titute of Te--,I',L~jc"Ac,-,y ard tto Tyr.: 11ant)
Card 1+/I+

SHIRT&YNV, B.I.
Grid-control system of the lashira-Moscow d.c. power line.
Izv.NIII?T no.3:181-196 '58. (MIU 12:1)
(Blectric power distribution--Direct current)

SHIRYATF.V,B.M., inzhener
Universal attachment for connecting MB or BB apparatuses to
standard tab hand operated stations. Nauch.rob. YUGI no.11:
142-152 154. (MLRA 8:11)
(Mine communication)

FMANDY, Boris Moloeyevich; SHIRrArW $ Boris Mikharlovich; JOHIN. G.M.
rf3daktor; NADAIRSKATA, M.A., tekhnlcheekly~redalrtor.
[Mine telepbone system] Sbakhtnala telefonnaia eviazt. Hookys.,
UGlatekhtsdat, 1955. 151 P- (KLRA 8:9)
(Hine communication)

GURIN. Nikelay Yef Imovich; HIKOTIV, Turiy Alaksandrovich; W-IRMI-wa
Boris Mikhaylovich; SHISHK13, Nikelay Federovich; W23TIVA,
X(ROnMOVA, Z.L., tokhatcheek-ly rodaLktor.
[Blectrical engineering in mining] Gernata alaktretakhnika.
Hookya, Uglatekhtsdat, 1955. 5o6 p. (XLRA 9:5)
(Blectricity In mining)

AUTHORS: Protopopov, A. N., Shiryaye-v-,..-13. L". 56-2-lo/51
TITLE: ThL Study of y-Rays Emitted in the Fission of U235
Induced by 2.5 and 14-7 MeV lieutrons (Issledovaniye
y-luchey soprovozhdayuchchikh deleniye U235 neytronami s
energiyey 2,0 1 14,7 MeV)
PERIODICAL: Churnal Eksperimentallnoy i Teoreticheskoy Fiziki, 1956,
vol 34, Nr 2, pp 331-333 (USSR)
ABSTRACT: By means of a coincidence apparatus the authors investiZated
the spectrum of y--, 12anta which coincide with the fission of
U235 under the action of fast and thermal neutrons. By
means of the comparison of experimentallL, obtained rpectra
none conclusions on y-rayB can be drawr occurin,; parallel
vith the fission of U235 under the action of fast nei-,trons.
A diag-ram shows the block ache.,.e of the apparctus usel for
the measurements. The y-quanta were recorded by means of a
scintillation counter with a IW(Tl)-crystal and rith a
spectrometric photomulti-lier of the,-413Y-C type. The
fission fra,3mente were recorded by moLn-- of a multila~-er
card 1/13 ionization cha.-.bort which vaG filled T.1th a mixti-re of

The Study if y-Rays Emitted in the Fission of U 235 56-2-10/51
Induced by 2.3 and 14-7 NeV Neutrons
argon (95';'.) and carbonic acid (5"') under a pressure of
P;
76o torr. The layers of uranium oxide (with 97,8 % U235)
vore deposited electrolytically on the electrodes of the
chamber. The impulses of the cha-iber were pasued on c-croas
a linear amplifier to the coincidence circuit. The
neutrons with the energy 2,3 and 14 " MeV were for-,,od in
the reactions D(d,n)lle.;' and TZd,n)H;A at an energy of the
bombarded deuterons of 18o kell. The thermal noutrono wer,
obtained by means of slowin- down the fast neutrons by
means of a lead layer (Io cm) and paraffine (25 cm). The
distributions of the impulses on the amplitudes obtained
by these measurements are shown in a dizL6-ram. The spectra
have the same shape within the ranoe of amplitudes
investigated. In the fission of U255 by thermal neutrons
this range of amplitudes covers about goiTa' of the total
amount and 65-7o~', of the total amount of momentary quanta.
The total energy of the y-quanta emitted in the fission is
proportional to the mean number of the y-quanta
corresponding to one of fission process. Within the
experimental accuracy ( 15%) the total energy of the
Card 2/3 fission of U235 by neutrons with 2,0 and 14,7 '.IeV-

The Study of y-Rays Emitted in the Fission of U235 c6-2-lo/51
.0
Induced by 2.8 and 14-7 MeV Neutrons
-accompanyinZ y-quanta is the same as in the fission of
U235 by thermal neutrons. There are 2 figures and 6
references, 3 of which are Slavic.
ASSOCIATION: Radium Institute AS USSR (Radiyevyy institut Akademii nauk
SSSR)
SUBMITTED: August 30, 1957
AVAILABLE: Library of ConGreas
1. Ionization chambers-Applications 2. ~F' -Rays-Study and
teaching 3. Scintillation counters-AppUcations
Card 3/3

:J4
1.
r1
.4 1 -A

ARTEMMV, N.M.; PROTOWWVY A.N.; SHMAYEV, B.M,
Gamma rays accompanying the thermal-neutron fission of u235. Trudy
Radiev.inst.AN SSSR 9:78-83 159. (KMA 14:6)
(Uranium) (Gamw rays)

21M SOY/56-36-3-63/71
AUTHORS: Protopopov, A. K.,
TITLE: y-Rays, Accompanying U 238 Fission by Neutrons of the Enerff

2.8 and 14
.7 Mev (y-luchi, soprovozhdayushchiye deleniye u 38
neytronami energii 2,8 1 14j7 MeV)
PERIODICkL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, Kr 3, pp 954 - 955 (USSR)
ABSTRACT: Determination of the average total energy of y-quanta originat-
ing from U238-fission by thermal neutrons gives approximately
7.5 Mev (Ref 1) and for the spontaneous fission of cf252
8.2 Mev was obtained (Ref 2). L?xperimentally it was found
that for the u235 fission by thermal neutrons and by 2.8 and
14.7 Mev neutrons the values obtained for the total y-energy
within the limits of + 15% coincide (Ref 3). The purpose of
the present paper (III7etter to the Editor ") was to obtain
data concerning the division of energy by y-rays in U238-
fission by fast neutrons. The same method and apparatus were
used as in the case of reference 3; the I-spectra of U238-
fission by fast neutrons and those of U235-fission by thermal
Card 1/3 neutrons were compared; 7-counting was carried out by means

Y-Rayn, Accompanying U238 Firsion by Neutrons of the SOV/56-36-3-63/71
Eneroy 2.8 and 14.7 Mev
of a scintillation counter with NaJ(Tl) crystal connected in
coincidence with a single-layer fission chamber. The chamber
contained, with conditions otherwise being the sa-ne, a U235-
target (1.6 mg/CM2) and also a U238-target (2.2 mg/cm2). The
results obtained by these investigations are shown by a
diagram showing the dependence of the ratio coincidence/
fissions on the impulse amplitude in v. Measuring values are
along a straight line which declines in the direction of
growing amplitudes. The ratio of coincidences between I-
quanta and fragments in the case of U238-fission by 2.8 and
14-7 Mev neutrons and the number of coincidenceain the case
of U235-fission by thermal neutrons is given as amounting to
1.03+0.03 and 1.00+ 0.02 respectively. The authors again
arriVe at the conc-lusion that for U238-fission by 2.8 and
14.7 Mev neutrons the average total energy of y-quanta
agrees up to + 15,14 with the values obtained for ~235_fission
by thermal ne7u-trons. A comparinon with the results obtained
by other papers shows tha4l) similar values are obtained
Card 2/3 per fission for all investigated nuclei (U 235 'U 238 'Cf 252)

238 ' /7 1
y-Rays, Accompanying U Fission by Neutrons of the SOV/56-36-3-63
Enerjy 2.8 and 14.7 "'ev
for the average total energy of y-quanta per fission process
and 2) the y-quanta energy depends only slightly on the ex-
citation energy of the compound nucleus before fianion. The
authors in conclusion thank Yu. I. Belyanin for supervising
the accelerator during the experiments. There are 1 figure
and 3 references, 2 of which are Soviet.
ASSOCIATION: Radiyevyy institut Akademii nauk SSSR (Radium Institute of the
Academy of Sciences, USSR)
SUB.',!ITTED: December 6, 1958
Card 3/3

ARTE-11M, Yu.M.; RARANOV, I.A.; BLINOVI M.V.; KUZNL7SOV, M.I.; PROTOPOPOV '
A N.; SELITSKIY, Yu.A.; SoLOVIYEV S.M.; SIIIRYAYLV,-,B.M.; EYSMONT; V.P.
0 0 - I- -- ---
I.,ow voltage neutron generator. Trudy Radiev.instki SSSR 9.-134,-
140 159. (KMA 14:6)
(Neutrons)

S/048/61/025/001/026/031
B029 B063
AUTHOR: (j~hirYaYeVB. M.
TITLE: Determination of the mean lifetime of excited states of
U235 fission fragments
PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheakaya,
v. 25, no. 1, 1961, 143-144
TEXT; The mean lifetime of excited states with respect to the emission
of gamma quanta has been determined by measuring the solid angles cal-
culated from excited fragments. According to V. V. Sklyarevskiy, D. Ye.
Fomenko, Ye. P. Stepanov (Ref. 2), the main fraction of gamma radiation
corresponds to a fragment lifetime of (0-5 - 2-5)*10-9 see. The afore-
mentioned authors, as well as A. B. Smith, P. R. Fields, and A. Mo
Friedman have come to the conclusion that the emission has, above all, a
dipole character. The ionization chamber shown in the accompanying figure
was placed in a current of thermal neutronu. The coinciding pulses
originating from gamma quanta and ionization chamber were determined.
When the distance between the layer of fissile material and the
Card 1/4

Determination of the mean lifetime ... S/048/61/025/001/026/031
B029/BO63
collecting electrode of the ionization chamber is increased, the number
of coincidences decreases owing to the emission of gamma quanta from
fragments traveling over a large distance, i.e., owing to the decrease
of the solid angle calculated from the fragments to the crystal. The
decrease occurs during the emission of gamma quanta from fragments. The
relation - 12N _
L = %N Y5 !Q)/vf(r)
holds for the mean lifetime. f(r) is a function of the distance between
the layer of fissile material and the collecting electrode of the
ionization chamber; N is the number of coincidences corresponding to one
fission event; N I is the number of gamma quanta emitted in one fission
event; f is the efficiency of the gamma counter; v is the mean fragment
velocity; and Q is the solid angle calculated from the layer of
fissile material to the gamma counter. The gamma quanta were recorded
by a scintillation counter with an NaI(Tl) crystal, and the fragments
were counted by a single-layer ionization chamber. A layer of uranium
oxide with 97.6;.o, U235 was applied to the chamber bottom by means of an
Card 214

81"60,
-----Determination of the mean lifetime 8/048/61 025/001/626/031
B02~/B%
Ai backing. The valuos of 11 andl found by Yu. M. Artemlyev,j A.N.
Frotdpopov, and B. M, Shiryayev -were used to calculate -7 . The solid
angles were calculated by methods of K. A. Petrzh&X and K. A. B4k (Ref.~O-
The values of the fragment.volooities were -taken from measurements of,
R. B. Leachman (Ref, 5). It has thus 'begm found thit the mean lifetime
of such fragments with rvs~ict to 'the smiision-o? gimma qu~Lntev is
2.0)-10-9
(0-5 sec. This value Is in good agreement with the results
obtained by other methods. According to this experimental lifetime, the
gamma quanta are chief'ly emitted from excited fragments after evaporation
of neutrons. Since several facts contradict the usually accepted theory
of neutron evaporationt a search for shorter emission periods of gamma
quanta during fission would be of particular interest, A, X. Protopopov
and V. F. Eyemont are thanked for discussions. This is the reproduction
of a lecture read at the Tenth All-Union Conference on Nuclear Spectro-
scopy, Moscows January 19-27, 1960. There are 1 figure and 5 references:
3 Soviet-bloc and 2 non-Soviet-bloc,.
ASSOCIATION: Radiyevyy institut im. B. G. Xhlopina Akademii nauk SSSR
(Radium Institute imeni B. G. Khlopinq Academy of Sciences
Card 3/4 USSR)

Determination of the mean lifetime ... S/048/61/02
3020063
Legend to Fig.:
1 PhotDelectronic multiplier;
2~ NaI(Tl) crystall
3 housing of the ionization
chamber; 4) uranium-oxide
layer; 5) bellows; 6) collect-
ing.electrode of thq ionization
chamber.
Card 4/4

SDZNOVP G.A.j TUIIKlNA# M.Ya,j SHIIIYEYLrV# B,V,
Istopic exchange during the decarboxylation of douterated
benzoic acid. Zhur. ob. khim. 31 no. 21641-644 F 161.
(Benzoic acid) (Deuterium) (MIRA 14:2)

h336h
S/056/62/043/005/012/058
B102/B104
AUTHOH6: Blinov, M. V.t Kazarinov, N. M., Frotopopovj A. Not
jhi ryayey
TITLE: The angular aninotropy of/-quanta accom panying the U235
fission
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheokoy fiziki, Y. 43,
no. 501), 1962, 1644-1648 '
TEXT: The angular anisotropy of/~-quanta emitted in thermal-neutron in-
235 v
duced fission of U was measured under optimum geometry. The
/-t-quantum detector, a atilbene crystal and an,03Y--35 (F4U-33) photo-
multiplier, was lead-shielded (1U cm) in'order to reduce the background
effect. The effects of prompt neutrons were eliminated by a multi-
channel time analyzer (resolution 3-5-10-9see). In previous measurements
made with a gas scintillation counter and a copper collimator the
anisotropy was found to be 25-30%. Control measurements showed that this
high value can be somewhat reduced if account in taken of the ',-quantum
Card 1/3 If

S/056/62/04 3/005/012/058
The angular anisotropy of ... B102/B104
absorption botri of the collimator and of the Al backing of the target.
In the following experiments these effects were eliminated with the help
of a apecial arrangement (Fig. 1). The fragments were detected by the
flashes in a thin nointillation foil. The time distributions of the gamma
counts taken at 0 and 90 0 angles to the chamber axis show a peak with a
half-widtn of 8-10-9sec. Records gave 19-5-10 6 fission events
(15,065 quanta) under 0 0 and 19.8-106 (12,069 quanta) under 900 to the
axis. Thus after all .corrections the anizotropy amounts to W(O-WOO)
. W(90)
-02+2)1~, i. e. the )*/-emission in the direction of flight of fragments is
high;r by (12+2)% than perpendicular thereto. Assuming it is the
fragment's angular momentum that causes the anisotropy its value can be
estimated. For L?/2, j -25 - 50, for L-3, J-15 - 20. The measurements
described have been made at the reactor of the F?I AN SSSR. There are 2
figures.
SUBMITTED: June 18, 1962
Card 2/5
The angular anisotropy of ... 3/056/62/043/005/012/058
BIOZ/B104
Apparatus for measuring thG/'-ray intensity along the chamber
axis. Legend: I - neutron beam; 2 FEU-33, 3 - TerPhenyj film,
4-uranium oxide layer IJ235'
crystal (97.9% 5 - vacuum chamber, 6 - atilbene
7 - lead shield.
/Nj
Card 3/3

44233
3/056j62/043/006/031/067
2~. 4640 B125/3102
AUTHOR: Shiry&Yevt Be Me
TITLE: The kinetic energy dispersion of fragments in the fission of
heavy nuclei
PERIODICAL: Zhuraal okeperimentallnoy i teor*tichaskoy fiaiki, v- 43,
no. 6 (12), 1962, 2150-2152
TEXT: Calculations are made of how energy fluctuations and the rotation
energy of fragments affect the dispersion of total kinetic energy. The
half-width of the total kinetic fragment energy distributions is
P- Fkin - ~(t' L"d2+ (6 Erot)2 + (aEd 2 +.(A Ed 23112 fle- 20 Hey. ASQ
denotes the spread of the kinetic fragment energy due to fluctuation of
the mean diGtAnce between the fragments at the instant of fission, AE,
denotes the balf-width due to the neutron recoil, &Z zdenotes the
half-width due to charge fluctuation of the fragments. From the rotation
energy Erot " 1 212/J it follows that AS rot A 2J-1 JAJ and for
ard T
Card 112

50) SOY/54-59-2-23/24
AUTHORS3 Tefremov# G. T.# Kim Gun On,- Ob
TITLEs Co-precipitation of Thallium With Copper and Mercury Iodides
(Soosazhdenlye talliya a iodidami medi i rtuti)
PERIODICAL: Veotnik Leningradskogo universiteta. Seriya fiziki i khimii,
1959P Nr 2, pp 152-155 (USSR)
ABs,rRACTs The co-precipitation proved to be one of the most promising
enrichment or concentration methods of separating thallium from
materials with a very low oontent of thallium. Poorly soluble
metal iodides are used as collectors for the thallium. Similar
investigations with copper and silver iodides are indicated in
publioations (Refs 1-2). Investigations with copper and mercury
iodides have not yet been carried out. This method tested in
this paper with the monovalent metal iodides of the mentioned
metals# proved to be particularly suitable for investigations
of mercury-containing materials on one hand; on the other hand,
the presence of copper does not disturb the final determination
of thallium by tho colorizetrio methyl violetzethod. In order
to prevent the formation of free iodine in the copper iodide
Card 1/3 solution, the presence of which disturbs the precipitation of

Co-precipitation of Thallium With Copper and SOV/54-59-2-23/24
Mercury Iodides
thallium, a reducer was introduced In the form of fresh-made
sulphuric acid. To investigate the optimum conditions for a
complete precipitation of thalliumt the copper iodide content
and the VH-value of the solution were varied in a solution
volume of 25 al at 180 and a thallium content of 501w Th. The
results of this investigation are compiled in a table. The
optimum conditions were attained at a pH-value of 2.9 and a
thallium-copper ratio of It200, At an increase in temperaturej,
the precipitation of thallium became worse. Investigations
with thinner solutions also yielded worse results. The
precipitation mechanism is considered as a surface adsorption
of the thallium on the copper iodide. Besides, the thallium is
determined In some natural compounds by means of this method,
For the precipitation of thallium, with mercury iodide, an
excess of potassium iodide had to be introduced to stabilize
the Hr-J in this way, it was possible to precipitate 95%
2 2;
of the thallium from 20 ml of solution (0.001 mol/l KJ excess)
with 254- thallium at a pH-valus of 3.3 - 4 and a mercury-
Card 2/3 thallium ratio of 111300- A further excess in KJ reduced the

Co-precipitation of Thallium With Copper and BOV/54-59-2-23/24
Mercury Iodides
yield. Toots with a boiling solution yielded worse results.
The precipitation mechanism H92J2 - Th is also considered as
a surface adsorption. There are 1 table and 5 Soviet references.
SUBMITTEDs December 22, 1958
Card 3/3

TIrAM4)V. G.T.: KIA (JUN ON; SHIIMAYF.V. B.
TnMaAL--l
Coprecipitatlqn of thallius with copper and mercury iodides, Vast.
LM 14 nr,.10:152-155 '59. (KIRA 12:6)
(Thalllux) (Iolidos)

21 4,
V
1-C
rl
t
at t4l.
lj53.
9' L Is t-0f Russian Accessions
Library Of Congress.
----- :_~1953. unclassified.

of Farm Animals - Diseases Caused' by Bacteria anol, R.
A-s Jour Ref aur - M.A., 11o 60 1953, 26236
.mtii:)r Shiryayev, D.T., Sha-povalov, ,.T.
In a t Rcstuv-,)n-the-Wn Goverimental Scientific Research
.Uitijil3j;ue Institute.
Titl,~- Faaminations of Antelopes (S3iLp tatarica) in the
M)rtheast Prckaspian Area fcr Dr-acellosis Infectirin.
Orir, Puli Tr. Rostovsk.-a.-Do L:css 1.-it protivochurai. in-taj,
1956, 10, 432-434
Atstract Vien the b1co--! rf antelon
-jes was seroloGically examined,
f,,r ',rucellosis (P%--Yt and 1Gie