SCIENTIFIC ABSTRACT GUSEVA, L.G. - GUSEVA, L.N.

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• Collection: Scientific Abstracts
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• Original Classification: S
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• Document Creation Date: November 2, 2016
• Document Release Date: September 21, 2001
• Sequence Number: 10
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

sov/log-4-8-6/35
Ignition of Discharges in the Non-uniform Fields at Low Gas
Pressures
and the curves were taken for various depth$ h of the
lower channel. The curves illustrating the breakdown
voltages of configurations IV and V are given in
Figures 5. From the investigation, it is concluded that,
in non-uniform fields, when the two electrodes have a
different shape, the breakdown voltage is strongly
dependent on the polarity. Secondly, the breakdown
voltage is determined not by the longest distance between
the electrodes bit by the length of that path which meets
the condition of the self-maintenance of the discharge*
The electrical strength of the discharge gap, as the
pressure is reduced, is limited by the field-emission
phenomena which appear at the cathode when the field
reachesE-.200-500 kV/cm.
There are 5 figures and 5 Soviet references; one of the
references is translated ftom English.
WO,
Card 3/4

SOV/109-4-8-6/3
Ignition of Discharges in the Non-un1form Fields at Low Zs
Pressures
ASSOCATION: Vsesoyuznyy elektrotekhnicheskiy institut im.
V.I. Lenina (All-Union Electrotechnical Institute
- imeni V.I. Lenin) L/
SUBMITTED: March 5, 1959
Card 4/4

G.V. ad
AUTHORS: Gra.no-kir. Y.L.. Luk~ymnov, . u-, I,.
3Lrot.nko Z.G.
TITLIt _jj~~~O.d All-U.J.. C.cf.r.ilc. a Gas
Blectroul.s
I 4L*kt1-ajk., 1959, 1.1 4, Wr
,
i
tokhn k
PSUODICALt RAdi
USSR)
5B
(
pp 133 - 13
;
Ac-So.US3R, the
AwraAcT I Th. confer .... 0 --- organised by th:
.
t Ministry of Higher Education and Ho a. 3 tat. University.
It was opened by ir"&n o f tile rgmal.lnij; connitt
*;
:
h
.
Ni.n. D~rizlg the plenary .... L
4-A L* 9~ 1c:dc
_Rj
toar.r... a, a number of survey papers were delivered.
.r_j..
A -high
road a paper an "Production of Ultra
plam..".
~
A survey of the optical method of measurements was given

A
r, by
in th
pap
,
y
- Me AmhAtt I ti u . rT:,hmo!*
;
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:
3*Dr
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.
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,.,* """ of the high-frequency method. f th
.
.-tion of stationary and non-stationary pi..- (a.. p 12441
I. this Issue 0 f the journal).
N.Y. Fedoranko read a paper entitled wIani-ation and
Crdl/.15 ~ao&* ~ ~tt4rLnX Ch~ng.Atomxic Colli.Ic..".
deal with 'Clecientary Processes
the t~ or 4ons in use-.
A paper by To. Otdareu (Rumania) dealt with "The Role of
the line tin' of !"a'.
StAk2j_'_n_i.kOv considered the &I &gas of the
5-

h*..i and the
_4t
P-.nt of park. (coroua-l*^d*r, -In
,
fin, ch-2 ).
: i
11, t gnit n process..
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rs.Isilly rarift.d Same..
.1 dis .
.kd." Of . high-..Ou- gap vs.
br
f
th
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Th
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ation Of
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y
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rants In a =arn
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p N
An 4*xdot.~ R. JLo=p ( Zest rn Germany) described . n"b.r
:
:
&
experimento an non-stationary plasma conducted by
of
la
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M. 3taftbock (Eastern G rama r...-Itsed theory or

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d
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Th: first section was r ~.r I,
y
cm-.d with the elementary processes In gas discharge*.
;
DIIOw`IAX Papers we- read in this emotions

Transf mation of positive I... at.
o
:
n Razi
ied G......
f
Ta.
'
ogel. .1th V. -AQkM"jq"_.^. D.V. Pitipociw
C
t a
;C. And Los. Al.ctro.. D-Ld Ch.
P
t Atoma of Carbon and Hydrogen with the Molecules or

-
--~o at .2.
,-
:o or
1
,
I!
of Hydrogen D%Wjag Cc IOm .
_111, 'd Tit-5- alar_~X~- "C:Piure Cross-..cti...
.1"
j or Blectroom in Multlc~srz one In Inert Q......
At 1. - r~p I
of the
R:chrglog in Certain Games -d
metal Y.Pur.
O.S. Fir.or -
.Qualitative or Inelastic
ZilCif-u-1i - Ato.
,
-
~Y9xkaTA_x "Rff:c;ive Excitation Cr ...... cti." of the
_
-
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-
A~
':
R-11- of In.
S-
E
C.rd3/1 A.Pj .. tInyy ad _S.H. JSLft~-
5
=
Investigation of the optical F ctions Or the 9x.Lt.tion
Deads of & Negative sy.t....
A.A. V CQWYr ad A.G.
,

Scattering . . X
r th Z-,
;,- I -nt On 'hAmb r.
Th - :"c"d motion a. pr..Ld.d -- by O.N. KiY-1f.I'd
And am devoted to the praillms or tile electrical break
down In rarigi.d gas.. ad
in IlLsh v-um. Tile f.Il.wj.'
ra
re read In this -.ctL.nt
p p
:
.:m
Gr ._rfLIisan9v And 'gLactr-tatic
C;ntrol of the Ignition or GIO-JLsQhArX* Tub,sw(mm.
p 22716.rthe J. --I).
PtItay" At a" war& cOuc1ru1J litts the Ut,akdowle
tiLfh-1-It-go mercury ro4tifl,r p 1278 of the
jo.raal .
1-ftr Ignition of th,e Dt,cjj,rS, in Mon-unif_
M-
:
I .
n.
Gas (
.. p !L60 of the jouroal).
A.5. .-d 3.N. 11 rf. d- Tile Discharge ph.no..c.
,
Between a Point And A PI-n- At G- Pr....,.. or
10"3 ame HE..
-- --------

AP4010309 *100"164VMA0lA14lA146
AUTHOR: Guseva, L.O.
TITLI: Influence of Individual ols"stary proosesep an the chwmateristica of high
voltage discharges ffisport, 5 an nd All-Union Conference an the Physics of Zlectro-
nic and Atomic Collisions hold In Ushgorod, 2-9 Ootj'"27
SOURCE: AN SSSR, Izvestiya. Seri3~*'hxicheskaya, v.it, no.1, 1964, 141-146
_TOPId'TAGS: high voltage discharge' discharge mechanism, electric b.reakdown, resti-
tution coefficient, electron prb0u~tlon, ionization, electron reflection, multiple
ionization,'- electron multiplication
ABSTRACT:- Many aspects of the mechanism of high vottage dischax*ei is still ob-
scure~. It is often assumed that' only two processes:lare significint where ignition
of &-discharge under the conditionalcorresponding t6-theFleft-hand,branch of the
Paschen' curve are concerned, namely, ionization of the gas in the gap by primary
electrox a and gamma processes on'the cathode, Howe*er. analyses'-cirried out by the
author'indicate that these two processes alone do not satisfactorily explain the
behavior of high voltage discharges.i There must alto be considered the contributim
Card 1/3
min

AP40 10309
from Ionization by positive-ions, charge exchange, additional Ionization produced
.by electrons reflected from the anode and by electron ejected froet the atone of the
gas in the process of primary ionization. The probable roles of these different
processes in high voltage discharges are estimated by evaluating the electron restL-
tutIon (multiplication) coefficients associated with these processes. Specifically,
calculations are carried out for the coefficients connected with the Ionization of
the gas by the primary electrons, the ionization produced by electrons released tm
atom Ionized by primary electrons and ionization produced by electrons reflected
from the anode. The values of the calculated electron restitution coefficients are
tabulated for the cases of high voltage discharges In nitrogen and mercury vapor.
It is concluded that the production of now electrons in the discharge gap due to
reflection of electrons from the anode is often comparable to and sometimes greater
than,the.effect of primary elec~-.rons. The fact that the effect of reflection of
electrons from.the anode may be significant in the Ignition of high voltage dis--t-
charges to also indicated by studies of the influence of the material of the anode
on the breakdown voltage. 'the author is grateful to Prof.B.H.Klyarfei'd for valu-
abLe advice and suggestions in the course of carrying out the invowtigation.0,
Orig.art.has: 7 formulas, 3 tables and 2 figures.
2/3
card

AP4010309
ASSOCIATION: Vaesoyum)0y elektrotekhnichoskiy lastitut ImN.I.Lanins. (All-Union
Electric Engineering Institute)
SUBMITTED: 00 DATE ACQ: 1OFeb64 ZMCL: 00
SUB CODE: PH NR REP SOV: 005 007
Card 3/3

EOF IN' n)-2/2"IR/En-A (w)_21Z,3C
&_;p (b) IJO(o)_ _JD
ACCESSION IfR- AP5005233
AUTHOR- Klyarfol'd, V.N.: Gusova. L.G. 1
4
r ?5
TITLE. On the. nature. of -the -pos itive qurrent-wvolta~d chara6t6rist a:!ot. v lov S
sure. eleotric, discharge
;2 3o6 .
SOURCE- Zhurnal telchnichoskoy-fiziki, ~v.~5,: 0*
TOPIC TAGS: gas discharge, glow d
Ischarge, pl"ma low prasp~re did-hargg halium
argon
-111gh-voltage discharges in a betifei6n. pit, xrb_oni7~,d
AD.~TRACT:: holiuk ~d.argon.~ AD V.
iron el2ctrodes were investigated experimentally and. th6 r4a~j'IU ~T- i
~jr~ haliun at.0.08
mm lfg with 8 m electrode saparation are A 3 the
,presented; graphically. t: low eurre~~
potential-rom.^tined*constant-at 4.6 Wj~ but w1hen: tlte~ cuktont:. roacheti A cartain!
I threshold the potential increased, and plasma could, be observv in! the vicinii~,:of 1
the anode. Wi "I h further increase of current the plasma layar~~becaivt thlckar,4d
;I_jhe potantial continued to rise, This increasa* In, potent iMl to tha;.09-~
fpctive debrease in the length of tho discharge gap as mora 9-1 the' Interclectrode
apace becomes oocupied by essentially equipotential plasma. The thlc-Luiass of the
Qrdl/2

~_-L 41e!42_65
ACCESS 1011~ NR: AP5005233
j 'plasma at the anode and the potential dro
p weri:~ measured as _.*ictipn~s ot lie pros
t
wuro for fixed current and electrode ;Spacing.. Fiorl the :resulli ing the 1-14-t0!
of -the ion ow-rent, -to the - elee'ron curront was estimated an&140und to be smaLl
-coneltded -that -the hic 4-ria anod(i
From this-it is pii~_ - at- thc.'
arid the anomalous- glow discharge area "qualitatively Idqntiaa3..:, d~'~fUoriftg oul in.,
the ratio of -he ion to the olectron-curIvont. As this:ratia, -the _pot_(Ik_iiI
drop approaches- a 11miting value. This is ascribed either,ioii ~Caki.1:11 - -an i;I the!
=ti j
negative glow plasma or to a shif t oi the position ot maxim'Wt potwitLal in thd nn~-
ode plasina toward the region of the cathode drop. "V.V.VjasoV, A.Y,,~.J~tljj.kov ItIld 14
Z..Shapiro- articipated in the experimental portion of the
4 figures.
-ASSOCIATION. Vsesoyuznyy Elektrotakliniche Uy"nstitut ImVV.:)'4Laniin;L 011-Uni~,n
i Electrotechnical InstAute)
.30jl:pr64,---.-- --EIM-L:__OO
NR REP SOV: 003
MMER:' 004
Card
f ~4

ACC NR3 AP6013126 SOURCE CODE: UR/0057/66/036/004/0704/071:1
AUTHOR: Klyarfel Id,,B.N.; Guseva, L.G.; Pokrovskaya-Soboleva,A.'s,
ORG: All-Union Blectrotechnical Institute im. Vtl,Leninjlos~aw (Vaesoyuznyy elek-
trotekhnichoskiy institut)
TITLE: Glovi disAarge at low pressures and current densities up to 0.1 A/cm2
SOURCE! Zhurnal tekhnicheskoy fiziki, v. 36, no. 4, 1966, 704-73.3
,TOPIC TAGS:, glow discharge, hydrogen, nitrogen, neon# laon, gam discharge,plasmal
A13STRACT: Current-voltage characteristics of glow discharges between plane parallel
electrodes in H21 W21 NO, and Ar have been measured at voltages Xrom 0.2 to 30 XV,
currents from 10-9 to 10 A. and values of the pd product (pressure times electrode
distance) corresponding to the left-hand branch*, the miniumm, and n portion.of the
right-hand branch, of the Paschen curve. The diameter of the electrodes was.always
greater than the distance between them, and care was taken to assure purity of the
gases and to avoid distortion of the curves due to thermal effects. The high curren*i .7
discharges were pulsed, tho data being recorded on the fall of the pulse. measure-
ments at intermediate currents by both the pulse and continuous techniques gave con-
cordant results. Many of the recorded current-voltuge characteristics are present
Praphically, and they are discussed at some length. Glow discharges are classigied
I
nto three groups, for which there are proposed the following designations: Simple
UDCt 537.525
Card 1/2

L 28485-66
ACC NR, AP6013126
(or Simplest) Glow Discharge; Dense Glow Discharge; and Normal Glow Discharge. 7be
simple glow discharges comprise the Townsend dischargei which Is thus regarded as a
kind of glow discharge, and the high voltage discharge; they are characterized by
absence of space charge between the electrodes and a potential that is independent of
the current over a very wide range. The dense glow discharges are characterized by
increase of the voltage with increasing current, decrease of the voltage (at constant
current) with increasing value of the pd product, and the presence beyond the cathode
fall region of plasma, the potential of which is close to that of the anode and which
exhibits a typical negative glow. In the normal glow discharge the potential is
almost independent of the value of -the pd product) the curront density at tho.cathodo
is nearly indopandont of tho current (and not proportional to it as in the simple and
dense glow discharges), and a negative glow plasma fills only part of the inter-
electrode region. As the current is increased at low pressures a simple glow dis-
charge passes directly into a dense glow discharge; at higher pressures there is an
intermediate range in which the glow discharge is normal. It is suggested that it
may prove necessary to introduce further new terms to describe the still insuffici-
ently investigated glow discharges for values of the pd product exceeding 100 mm lig
x cm. V,V. Vlasov, A.Ye.Kulikov, and A.T.Pavlova participatvd in the experimental
'work. Orig, art, hab: 7 figures.'
SUB CODE: 20 SUBM DATE: 16Jul65 ORIG, REF, 005 (YW REF: 008
Card 2/2

1 2, ~-3
r ACC NR: AP60187,46 SOURCE CODE: UR/0057/66/036/006/1140/1143
~AUINOR: Udris, Ya. Ya.; Gusova L Q.i
__Phornov, V,A. 57
f........ .
ORG: All-Union Blectrotechnical Institute im. V,I.Lenint'..Moscow (Vsesoyuznyy elektro-
tekhnichoskiy Institut)
i
TITLE:(ka some propeiLl--)s of a high voltage hollow anode glow discharge
SOURCE: Zhurnal tekhnicheskoy fisikip v. 36, no. 6, 1960, 1140-1143
TOPIC TAGS: glow Oisc]Large, electric discharge, electrode, hollow anode, air,
inert gas
ABSTRACT: The authors have investigated high voltage (3 to 25 kV) glow ddcharges In
air and different inert gases at pressures from 0.001 to 0.1 am Hg ind -currents from
0.0001 to I A between 6 'to 35 cm diameter plane cathodes and plane or hollow anodes
of the same diameter (the hollow anodes were from 15 to 100 cm deep). 7be current
distribution on the plane end of a hollow anode waa the same as on a plane anode,thus
confirming the conclusion of G.W,.McClure (Phys.Rev., 124, 696, 1961) that the glass
tube confining the discharge in the case of plane electrodeslbecomes charged to ap-
proximately the anode potential and so gives rise to conditions approximating those
within a hollow anode. The discharge curront was found to be focused onto'.tho central
portion of the plane end of the hollow anode. The current to the cathode surface, on
the other hand, was not concentrated in the central region of the electrode, the
Cqrd 1/2 UDC! 537.525

L 41005-66
ACC NR; AP6018746
current density was actually somewhat lower in the center of the cathode than at sow
distance from the center. 7be focusing of the current on the anode and its defocusing!
on the cathode were enhanced by a longitudinal magnetic field. The enhancement of the
current focusing duo to the field of a short solenoid depended strongly on the axial
position of the solenoid. Particles were withdrawn from the discharge region through
holes in the electrodes. Difficulty was experienced with discharges through the
openings in the electrodes when the pressure In the regions beyond the electrodes was
the same as in the interelectrode region, but such discharges could be avoided by
maintaining a low pressure in the regions beyond the electrodes. From measurements
of the particles withdrawn from the discharge region through holes in the electrodes
it was concluded, in agreement with the findings of McClure (loc.cit.) and D.Kamko
and F.W.Richter (Ann, d. Physo~ 10l 3609 1963)v that 75-90%7.of the energy of the
hollow anode discharge is carried by the electron current to the anode. The authors
thankl.V,L,Gra (deceased) and B.N,Klyarfelld for val"ble advice and dis-
cussions. Or has: 3 figures.
SUB CODE: 20,0S/ SM DATE: 22Oct65/ OR1G.R1Wz 003/ OTH RV: 002

I. GUSFVA, L. 1.
2. USSR (6oo)
4. Moths
7. Some data on the b1olo&r of the moth. a raw fur nest. Trudy VNIO. no- 10, 1951.
9. Monthl jistaf Russian Accessions, Library of Congreez, Febru 1953. Unclassified.

WOMYANOV, A.H.;GUSEVA, L.I.;TMONOVA, L.I.;ZABCRSKIY, A.K.
_a
Chemical state of atoms resulting from nuclear transformation@.
Dokl.AN SSSR 103 no.6:1041-lo43 Ag 155. (KLRA 9:1)
1.Hoalwynkiy gosudarstyenW univernitat beeni M.Lomonoxava.
Predstavleno akad*mikcm A I.YrwWVu.
(;Zto&hOMI�try) ,

Category : USdR/Nuclear Physics - Structure and Properties of Nuclei c-4
Abs Jour : Ref Zhur - Fizika, No 2, 1957 No 3216
Author : Guseva, L.I., Filippava) K.V., Gerlit, YU.B., Druin, V.A.,
MyasFy-e-dov, B.F., Tarantin, N.I.
Title Experiments on Obtaining En and Fm with a Cyclotron.
Orig lk-kb Atom. energiya, 1956, No 2, 50-54
Abstract Report of production of transplutonian elements by bombarding U with
nuclei of N and 0. Quintupli-charged ions of N and sextuple-charged
ions of 0 were accelerated with a cyclotron having a magnet with pole
diameters of 150 cm. The transplutonian elements were deparated by
the fluoride method using Ia as a carrier. The half lives and the
energies of the q particles were measured with the aid of photographic
plates and an ionization chamber with a spherical electrode. The quin-
tuple-charged ions of N were obtained in a specially developed slit-type
source. The energy of the N ions at the maximum radius was 105 Mev, and
the ion current was 5 X 10-7 amp. Irradiation of U by N ions produced
the isotope En.2117, identified by the value of T and by the energy of the
,.-z, particles. Sextuple-charged 0 ions were obtained by "stripping"
double-charged 0 ions on molecules of the residual gas in the cyclotron
Card 1/2

Category USSR/Nuclear Physics - Structure and Properties of Ruclei c-4
Abs Jour Ref Zhur - Fizika, No 2, 1957 No 3216
chamber. The maximum energy of the accelerated 8extuple-charged ions
of 0 at the maximum radius was 120 Mev. The current of ions with
energies exceeding 100 Mev was 3 X 10-9 amp. The isotope Fm was ob-
tained by exposing U to ions of 0 and was identified by the value of T
and by the energy of the-4 particles. Several hundriAs of atoms each
of isotopes of Cf, Bk, and Cm were separated by the chromatographic
method.
Card 2/2

i~- 41~

r r1

U. G T, Yu. B., 'V, -n. F.
GUETh L I KLIII~ UVA, K. V. , FL -"V
and Ta.%`:T1 I. (Acad. O'ci. TUSISR~
"Mass Distribution of Fission Fragments Formvited by Nitrogen Ions on Gold
and Uranium Nuclei,"
paFfir submitted at the A-U Conf. on " clear Retictions in -'edium and T OW er
4~u gy
Plkvsics, MOSCOW, 19-27 Nov 57.

56-2-4/47
~WTHOR GERLIT, Yu.D., GUS"-JA L.T.. MWOYJMDV,B.F., TARANTIN, N.I.,
FILIPFOVA, K.i., , ~RW
TITLE Yield of Californium isotopvb. ivi,outiced in t.),e inLeraction between
Carbon Isotopes and Urani-Lun Nuclei
(Vykhody isotopov kaliforniya. v reaktsiyakh waimodeystviya IDnov
ugleroda s yadrami urana. Russian)
PMIODICAL Zhurnal Eksperim. i leoret. -Viziki 1957, liol 33, ';r 2 (8), 1,1, 33?
- 342 (U.S.S.R.)
ABSTRACT In a 67 cm cyclotron rour-fold charged carbon ions are acaierated tip
to go ~LeV. Vlith this energy they inpinge upon a thick uraiiilm target
and cause the reaction U(C, n)Cf. The absolute yields per impinging
carbon ion and the following reactions are:
U239 (G-'", 4n) Cf 246 1,5 - 10-9
U239 W", 5n) Cf 245 3,0 . 10-9
U239(c 6n) Cf 244 9 . lo-11
The fissioning of uranium bombarded with carbon was found to be
3~8 . 103 times more probable than the 2pvaporation process of neu.-
trons from the intermediary nucleus Cf ~O .

AUTHORS: Tarantin, 1'. 1., Oerlit, Yu. 11.,_1VuzeYaj L. 1., 56-2-7/51
Myasoyedov,' B. F. , Fili'ppova, K. V.
TITLE: The Mass Distribution of Fission Products 2roduced by the
Irradiation of Gold and Uranium by Nitrojen Ions
(Raspredelaniye po massam produktov deleniya,
obrazuyushchikhsya pri obluchenii zolota i uraaa ionami
azota)
PERIODICAL: Zhurnal Eksperimentallnoy i Teoreticheakoy Fizil:i, 1958,
Vol 34, Nr 2, PP 316-321 (USSR)
ABSTRACT: The present rork investiCates the mass spectrum of the
fission fragments of radon and einsteiniu2 uhich are formed
in the irradiation of jold and uranium with nitrogen ions.
First the ex-.ierimental method is disclissed. Gall- and
uranium plates of a thickness of 30 p were irradiated with
five-times char-ed nitro-en ions from a slit source at the
inner ray of an 150 cm cyclotron. The ezierU of the nitrogen
ions was 11.5 ?A---V. After the dissolution of the irradiated
tar-et the different radioactive elements on the
Card corresponding carriers were dissolved. The radioactive
1/3

The Mass Distribution of Fission ProductsProduced by the 6) - 2 - 7 /5 1
Irradiatiun of Gold and Uranium by Nitro"en Ions
0
isotopes were identified accordinC; to their half life. The
relative yields of the nuclei identified this Nvay are
listed in a table. A aiau-ra~-, shows the vields of t.-.e nuclei
k;iven in this table an a function of t,,.(., ~,:ass number A. The
inain part of the yield of fission products is concentrated
within a comparatively narrow interval of mass numbers. The
yield of fission fragments increases rather C;reatly with an
increase of the class number froi 7o to loo, and with still
greater mass numbers it decreases to the same extent. From
the experimental values of the yields of single nuclei the
total yields of tile correspondint,: mass series (massovaya
tsepochka) were computed. The additional taking into account
of the yields of nuclei not identified in these experiments
changes only little the character of the distribution of
experimental points. The curve of the distribution of
fission fragments in relation to -the mass with the values
& - 85 to 115 has tile shape of a narroyr peak with a half
width of about 2o mass units. The yields of Ga72,73, Se123,
Sb122 and the yields of thu aeries of decays corresponding
to these nuclei do not coincide with the monotonous course
Card 2/3 of tile curve and are a little greater as normal. About 2o

The Mass Diatribution of Fission Products PrDduced by thle 56-2-7/51
Irradiation of Gold and Uranium by Hitroggen Ions
different isotopes were identified anions; the fission
products forming in the irradiation of uranium with nitro,-,en
ions. The yields of the accumulateO nuclei are collected in
a table. The fission of nuclei under the action of heavy
particles can be represented by the followine scheme:
Formation of a compound muclaus, emission of neutrons and
fission. The half width of the curve of the distribution of
fission fragments on the mass is considerably smaller in the
fission of radon than in the fission of einsteinium. There
are 2 figures, 2 tables, and lo references, 4 of which are
sl~:-vic.
SUBMITTED: August 2o, 1957
AVAILABLE: Library of ConGress
1. Gold-Irradiation 2. 3. Nitrogen ions-
Applications 4. Isotopes-Detemirw-tion
Card 3/3

GUSEVA, L.I. (Moskva); OVECHKIN, B,,I. (Moskva)
--------- _-,
Atomic X-ray scattering on solid solutions of copper and nickel.
Izv. AN SSSR. Otd. tekh. nauk Met. i topl. no.2-.82-85 Kr-Ap 159.
(MIRA 12:6)
U rays--Scattering) (Copper-nickel allo7s--Ketallographr)

5(2) SOVI/'18-4-9-38/44
kUTHORB: Grigorlyev, A. T.y Guseva, L. I., Sokolovskaya, Ye. 26.,
Maksimova, M.V.
TITLE: On Polymorphous Transformations of Chromium in Alloys With
Tantalum
PERIODICAL: Zhurnal neorganicheskoy khimii, 1959, Vol 4, fir 9, pp 2166-2169
(USSR)
ABSTRACT: The cooling curve for liquid chromium determined by N.A. Nedumov
(Ref 4) exhibits, in the vicinity of the very distinct maximum
corresponding to the crystallization temperature, a second
maximum which relates to the transition of chromium into another
modification at 18150. By means of microscopic, thermalp and
X-ray analyses the chromium-tantalum alloy was investigated in
the range rich in chromium after hardening; The location of the
solidus and the lizits of solubility of Ta in Cr were checked.
16300 was found to be the temperature of transition between the
modifications E and d . In contrast with the data obtained by
N. Grant (Refs 1, 2) it was found that immediately after freezing
chromium does not possesd a face-centered but a cubic body-cenUred
Card 1/2

On Polymorphous Transformations of Chromium in SOV/78-4-9-38/44
Alloys-With Tantalum
crystal lattice, which is in agreement with the fact that a
continuous series of solid solutions of chromitun and e-iron
form. There are 1 figure and 4 references, 1 oY which is Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet im. M. V. Lomonosova
Kafedra obahchey khimii (Moscow State University imeni
M.V. Lomonosov, Chair of General Chemistry)
SUBMITTED: January 12, 1959
Card 2/2

210) SOV/56-2/6-j2-17/71
M
AUTHORS: Volkovp V. V., Gunevii, L. I., Pasyul A. 3 i12
Filippova, K. V.
TITLE: The Production Cross Sections for Californiurr. Isotoi)es by
the Irradiation of U238 With Accelerated Carton Ions
(Secheniya obrazovaniya izotopov kaliforniya rri obluchenii
U238 uskorennymi ionami ugleroda)
PERIODICAL: Zhurnal eksperimentallnoy i tooreticheskoy fiziki, 1959,
Vol 36, Nr 3, pp 762-765 (USSR)
ABSTRACT: In the course of the irradiation of heavy elements with multi-
charged ions compound nuclei are formed, Yhicn decay aEain
as the result of fission or neutron evaporation. Important
conclusions may be drawn with respect to new transuranium
synthesis from the ratio of the two decay processes in ciepen-
dence on the excitation energy.and the parameters of the com-
pound nucleus. In the present paper results obtained concern-
ing the energy-dapendence of the cross sectiorio of the reactions

ard 1/3 U238(C12 , 4n -5n) Cf246-245
238 13 246-245 (cf. alBo references 1-3)
U (C , 5n - 6n)Cf
are discussed. The +4612 and _'_4C 13-ions were accelerated on

SOV/'J:',- -31 - 5-17/71
The Production Cross Sections for Californium Isotopes b7 the Irradiation
of U238 With Accelerated Carbon Iona
the 150 cm. cyclotron of the AS USSR up to 76 and 84 1.1ev re-
spectively (with an accuracy of 31,16). Energy measurement was
carried out by absorption in aluminum, measu-_-ement of the ion
flux on the target was carried out by means of an inte.-rator
(0.2 - 0.3 pa). The results obtained byhese measurements are
given in figures 1 and 2 in form of diagrams. Figure 3 allows
the cross section of the reaci-lons (C12, 4n - 5n) and
(C13 . 5n - 6n) referred to -the total production cross section
far the comnound nucleus in dependonce on excitation energy.
Each of the curves shovis a characteriTtic maximum. The shift-
ing of the maximum of the reaction (C 2 , 5n) towardo that of
the reaction (C13' 5n) iO assumed to be due to an inaccuracy
of ion energy measurement. For the connection between the
decay probabilities and the cross sections it holds that
0n = at(i ntWn + Tjf))n
0 = total cross section of the nauhron emisuion reaction in
n
the case of a fj,,i-ven energ,'r.6f = cross section for the formation
Card 2/3 of a compound nucleus at 'the 3LMe onergy. n = averag
,e number

11/56--'6-3-17/71
The Production Cross Sections for Californium Ijotope~ by the Irradiation
of U238 With Accelerated Carbon Ions
of emitted neutrons. Wn = probability of neutron ez.-.ir~sion.
Wf = fission Drobability; (W denoteo t.-ie mean value)
.:inl-wf for californium is - 1/4 and varies only little in the
interval of the excitatian oneru Of 35 - 55 ~10v.
Cf2,16 ' r f '3.
Wn/'Wf for (4n -- '5~1) is '-_' 1/2 and fo C ""'On - 6n)
The authors finally thank Professor G. N. Flerov for super-
vising work, and they- also thank the cyclotron to,--im i,,nilor
Yu. 71J. Pustovoyt and L. K. Tarasov for their collaboration in
the chemical part of this work. There are 3 figures and 9
references, 5 of which are Soviet.
SUBMITTED: September 16, 1958
Card 3/3

GUSEVA, L.I.; MYASOYNDOV, B.F.; TARANTIN, N.I.; FILIPPOVA, K.Y.
Cross sections of the formation of CM 240 by the radiation of
Th 232 with C12 alA c13 ions. Zhur.okup.1 teor.fiz- 37 no.4:
973-977 0 '59. 04IRA 13:5)
(Curium-Isotopes) (Thorium-Inotopes)
(Carbon-Isotopes)

GUSEVA, L.I.
Obtaining female lines of cucumbers. Sbor. trud. zinp. i Mol.
nauch. sotr. VIR no.5tlll-ll3 164. (MIRA 18:3)

e; ii z,j
~-%,oprecipitation of "WCke an cmmt-j, tnalsturni Ana ztac
IN t
iththen t I MIMV 0Wk en admao up, ZT_-i_
Aliniarin, it( nev, and
AfCchenykh Olnev v lial. Xh*MW-tr,1d-_=0 S.S.S.R.,
Iasi. Cicakkint, i Anal. Mat. IQSS, 1,~-23; cf. C-4. 4T.
469&-t.-Copptn. of these metals with members of tile 1\1
and V groups was studied with the aid of Ntn", M,", Zn
and TI-44. Pptn. with 11-S vms carried obit in 0.3N acid
solns. , Tn the sohis. contg. Ni there was 101. -f Ni and tile
Ni:M ratio ums 1:58, The Afn solns. contained III y Ain
-anti the'.1,1n;*M ratio wits 1:49. NI and Mn coppid. only
slightly with tile sulfides, except fit tile vasca of Bils, anti
SnS, where coppm. of Ni was 1.24 and 2.80%, resp., and
HgS and Sit% where coppta. of Ma was 1.0 and 1,5 resp.,
in the TI-contg. sohis. There was 2.00 -( and the'Tl:1,,1
ratio was 1:6.95 X 101. Copptn. in these sollis. was very
high, co ptn. was smallest with Ag,S (2S.0) and highest
p
(96.0%) with H&S in. soins. where the mol. ratio of Tltht
was 1*1 copptn. was appreciably smaller; - in these sollis.
coprtn. was smallest (1.9 and 2.0% with HgS and A&S,
resp.) and h1glic-st (48.2%) with As,%,~ The Zrx whis. con-
tained 660 -1 of Za and the Zn:M ratio was 1- 12. WItenthe
HtS was passed at the mine rate as fit jlt~ other eipts. (50-430
bubbles/min.) cfjpptn. of Zn was small and re;1ched "i Ile
with US and 100 wtthS,,S,-
ing was raised to 500 cc./min. the coppta, of Zn went tip
from 7.0 to W d0,' with CdS from 10.0 to 47.7170 with SnElt,
from 0.8 to 4i.i.t with HgS'. and froin 0.4 to 11 with
Bit%. Copptn. with CuSt PbS, Agtq, AsA, arlif Sb,'q,
remained unaffected. Delay between pptu. anti filterijt97
caused more Zn to be pl)td. with US. In changing tiltz
acidity between 0.05 and 0.41V the anit. of Zo copptd. with
_.S~S and SnSj dropped with inercusing acidity. M-J1oVJ6#,.v&'

~01' dcqdoa of souse surface-"ic dyes by. iqmtaw
caurse of their a"; N. A. Ruilnev and L, 1. Gusevis
~J 2V. 1. Vernadskil Inst, Gcochetn. and Anal. Cf-rnr,-XfWV'
1. U.S.S.R., Moscow). Zhap. A#W. Khi*. 11, 44-64
(1956),-The adairption ota dye (neutrid red) by frahly
ptd. and ikgcd amtst xulfidcs was studied with the vkw of
elucidating the structure of suMde ppts. and the ehanges
t~tat they may undergo with thne. Into a IW-wJ. dask
were addR a solo.-Of the-M-etal "LIU Sucli-114IMantitY(hat
the sulfide ppt. would be 0.1 X., IICI (1, 1) tv tuake it O.3N,
10 mt. of 0.5% sots. of neutral red, and lfjO to a total vol.
of IW tW. The dask was pUced in a thermostat at 28-
and afur 10 win. HaS -vas passed for 5 suln, at Approx.
.ce.lmhs. To the &e wis then addtd 10 mt. 11*0 sat&
with HDS mud shaken I w 20 adn. After definite tiam Inter-
vals 3-5 mt. of solo. was centrifuged and the amt. of dye
senizining was cktd. calorimetrically. In 4nother series of
cxpts. the dye was added after ppta., In which am It was
Udded after psasial; HaS and to place of tile 10 ml. 1410
patd. with H.S. Mter 36 rain. the Woos, vAsarplion w"
by Ass%, 97,217g; lean by HgS. PUB. SuSj, and 111*%, 40.0,
44.0, 48.8, and W.0%, -p.; mud In between were COS,
A&S; and Sbv%. 79-0, 58,2, and 60.4%. resp. Withrespect
to t1rue the suirides were divided itito 3 voops:, the adauep.,
tion of dye by HgS, Discl, sbkl%. and SA fi!crcm" with
ti=; adsorption Y CuS tutcl AW dccm2scd with titce; and
"Asmption by CdS. PbS. and A%Sp rcrmained practically the
same. Ad*wptica by Hc, Cu. and As sulfides was not a(.
feettil by the time when the dye was added. Thu4 the
aging of these sulfides Is " affected by the dye. An lit-
crease or decrease lit the amt. of dye ad*mbcd an 60 1
attributed to cibnottation or aggregation of tht x2de
with thuc. An elmtrott-micrukow study of All.% Sn!6
CuS, As.%, and Sb&% gets shuwed Own t~ have a-purm..
cellular structure. The structure of Ag~S was (lemqtr OUL11
thatol the othersulfi&3; PI)SuiitlCdSliaditclyst.sourtmfu.
Id. 11(M-11

AVRAKENKO, L.F.; VILENSKIY, Tu.B.; GUSEVA, L.K.; IVANOV, B.M.;POCHINOK,
V.Ta.; ST39MUMIKOVA,
Stabilizing effect of thiazolotetrazoles and tatrazolobeazo-
thiazoles on silver chloride photographic emulsions. Zhur.nauch.
i prikl.fot.i kin. 5 no.4:2~4-295 Jl-'Ag 160. (KIRL 13:8)
1. Gosudarstvenuyy universitet Kiyev, Filial Hauchno-isaledovatell-
skogo kino-fotoiastituta, Shostka i inatitut kino-inshenerov,
Leningrad.
(Photographic emulsions) (Tetrazole)

BLOOVA. V.A.; PLOTNIKOVA, N.V.; VOLKOV, N.M.; SYSOYNA. A.V.; AVDINW, P.P.;
aTSEYMAN, Kh.A.; RODINA, P.M.; GUSEVA, L.L.-, KAKMISKIT, V.I., red..;
BYKOV, A.H., tekhn.red.
(Economy of Tambov Province; a s%atiqt1Cal manual] Narodnoe khoziai-
stvo Tambovskoi oblasti; statisticheskii abornik. (Tambov] lid-vo
"Tambovskais pravda," 1957. 187 P. (MIRA 11:3)
1. Tabmovekaya oblast'. Statisticheskoye upravlenlye. 2. Statieti-
cheakoye upravleniye Tambovskoy oblasti (for all except Kamenekiy.
Bykov). 3. Nachallnik Statiaticheekogo upravioniya (for Namenakiy)
(Tambov Province--Statistics)

GUSEVA, L.L., (Moskva)
Clinical picture of dystrophic myotonia. Klin.med. :16 no.9193-97
S 158 (MIRA 11:10)
1. Iz nerrologicheakov kliniki (zav. - prof. Iq,A. Ponova)
Koskovskogo oblastnogo nauchno-isoledovatellskogo imitituta imeni
Vladimirskop.n.
(my6TCNIA, ASTROPHICA, clin manifest,
(Rug)) ,

GUSEVA, L.L.
------&h--~~acteristics of massage in hemiplegia of vascular origin. Vop.
kur., fizioter. i lech. fiz. kul't. 26 no-4:312-315 JI-A 161
(MYR~ 1;:l)
1. Iz otdeleniya fizioterapii i lechebnoy fizichaskoy Rulltury (zav.
dotsent N.P.Krylov) Moskovskogo oblastnogo nauchno-issladovatellskogo
klinicheskogo instituta imeni M.F.Vladimirskogo.
(PARALMIS) (MASSAGE)

GUSVVA, L.L., nauchnyy sotrudrlik
Massage in spastic paralysi3. Mod. sestra 21 n-j-5:53-56 My 162-
(MIRA 15:5)
1. Iz kliniki nervnykh bolezney Moskovskogo oblastnago nauchno-
issledovatellskogo klinichaskago instituta imeni m.F.nadimirskogo,
14oskva.
(MASSAGE) (PARALYSIS, SPASTIC)

SDMOV, V.A.; GUSEVA, L.L.; SMIPMOVA, G.G. (Moakva)
Clinical picture and morphology of defects of de"lopnen' of
the blood vessels of the spinal cords"VbP. neirokhir,26 no.58
22-25 S-0062 I(MIR9 17t4)
1. KII-nika nervnykh bole2ney i patomorfolog-Icheakogo otdela
Oblastnogo nauchno-isaledovateliskogo instituta imeni M.T.
Vladimirskago, Hoskva. *

SEMIOV.0 V.A.; IOFFH, Yu.A.; GUSEVA, L.L.
Clinteal aspects of Dera=ls syndrme. Sov.med. 26 no.12:102-
106 D 162, (MMA l6s2)
1. Iz kliniki nervnykh bolemey (zav. IoM. GDrtachaft) Mookovskogo
oblastnogo nauchno-isoledovatellskogo klinicheakogo Instituta
imet4 M.V. Yladimirskogo (dir. - zasluzhwm7y vrach FWM PeNo
Imonimko). ~
(CORFUMCS)

SEM, NOV, V.A.; GUSEVA, L.L.; IOFFL, Yu.A.
Clinical aspects of Ifelkernson-Hosentiml uyndrome.
Zhxtr. nevr. i peM. 62 ,c.2:2734176 162. (141RA 15:6)
1. Klinika iiervnykh bolozney (zav. U-11. Gorbacheva)
Noskovskogo oblastnogo nauclino-is.-,IcdrvL,-tt-l:.5kc.-Eo Idinicheskoso
instituta imeni M.F. VladLrdrskogo,
(PARALYSIS, FACIAL) %EDEMA)
1
(TONGUZ---DISEA.'~E'L; )'

- G.US EVA IL. L.
Exercise therapy in postlnsult, motor disordera. Vop. kur.,
fizioter. i lech. fiz. kullt 29 no.1:8-11-1 164.
(MIRA 17:9)
1. Klinika nervnykh bolezney (zav.- pro.f. N.A. Popova) I
otdeleniye fiziloterapil i lechebnoy fizicheskoy kulltury
(ispolnyayushchiy obyazannosti zaveduyushchogo Ye.O. Chernomordik)
Moskovskogo oblastnogo klinicheskogo instituta imeni M.F.
Vladimirskogo (dir. P.M. Loonenku),

i'l, Ij
kho 65 13
Vedr-,
Kv kc-linyk-In i v(,,
.
I
7;
of. -3 .1 !3a b'~
Ir'. n, "-.%i
mc

STOYANOV, B.G.; SEMENOV, V.A.; GUSEVA, L.L.; IOFII,, Yu.L.
Melkers son- Rosenthal syndrome. Sov. med. 28 no.K;61-67
0 '65. (MIRA 18: 11)
1. Kafedra. koztinykh i venericheskikh bolezney (zav.- prof.
B.M. Pashkov) Moskovskogo meditsinskogo stomatologicheskego
instituta i klinika nervnykh bolezney (zav.- prof. F.A.
Poyemnyy) Moskovskogo oblastnogo klinJcheskogo institu"a
imeni Vladimirokogo (dir.- P.M. Leononko).

19.36-
Translation from: Referativnyy zhurnal, Metallurgiya, 1958, N r 2, p 6 (USSR)
AUTHORS: Pevzner, M.L., Guseva, L.M.
TITLE: The Formation of Magnetic Amalgams in the Amalgamation Process
(Obrazovaniye magnitnykh amal'gam v protsesse aniallgai-natsii)
PERIODICAL: Kollyma, 1957, Nr 7, pp 38-39
ABSTRACT: A study was made of the principles of formation of a magnetic
amalgam. It was established that the cause of the formation of a
magnetic amalgam is the medium. During inO~rnal amalgamation
of the concentrates in vats without any CaO or Na0l-I (i.e., in an
acid medium) and when Cu ions were present in the liquid portion
of the Pulp, a so-called "iron amalgam" formed which, in addition
to an Au amalgarn, contained a considerable quanLitv (up to 50%)
of amalgamated particles of copper-clad Fe, as a result of which
the iron amalgam acquired magnetic properties. To avoid losses
of the extracted metal the magnetic fraction had to be treated with
HN03 ; the Fe scrap, which was obtained during the finishing
treatment by the amalgams, had to be collected and treated separately.
The CaO concentration in the liquid portion of the pulp was as high as
Card 1/ 1 0.15%. A. Sh.
1. Amaigams-Xagnetic-Formation 2. Amalva-mation processes-A pr,21-
cations

..GUS11VL-1-M1; SOKOLOV, B.K.; KRASIN, A.G.; LTSMKO, A.K.; MMO`ZOV, G.A.,
red.
Clor high corn yields] Za vyaokle urozhai kukuruzy.
Knizhnaia red.gazaty "Noygorodskata pravda,w 1960.
(corn (maize))
Novgorod,
59 P.
(MIRA 14:12)

VORONOV, B.G.; GUSEVA, L.M.
Spectrum analycis of deposited high "ed steel- Avtom.
svar. 16 no.U-.84-85 D 163. (MIRA 1'7-. 1)

VORONOV, B.G.; GUSEVA, L.M.; KURDYUMOVA, A.M.; KRASNOPROS11D., V.A.
Spectrum analysis of girth joints in high-alloy steel. Avtom.
svar. 17 n0-4:94-95 AP t64 (MIRA 18:1)

GUSEVA, L.N.
Phase transitions in alloys of chromium with tantalum and
nioblum. Izv.AN SSSR.Noorg.niat. 1 no.10:1743-1'746 0 165.
(MIRA 16:12)
1. Institut metallurgii A.A.Baykova, Moskva. Submitted July
5, 1965.

GUSEVA, L. N.
"Esophagogastro- and Esophago-Intestinal Anustomosis." Cand Med Scl,
S6cond Moscow State Medical Inst imeni I. V. Stalin, Moscow, 1954. (E, No
3, Jan 55)
Survey of Scientific and Technical Dissertations Defended at WZR Higher
Educational Institutions (12)
SO: Sum. No. 556, 24 Jun 55

QUSSVA, L.N., kandidat uieditsinBkIkh nauk- (Moskva, Goo()Itxjllxiyy val.
17, k-v. 86)
Morphologic examination of esophagogastric and esophagointestirial
anastomosis following radical surgery for exophageal and cardial
cancer [with au-mmary in Pinglish P-1571. Vest.khir. 78 ao.6:23-34
JS '57- (KLRb 10:8)
1. Iz fak-ulltetakoy khirurgicheakoy kliniki (zav. - prof. B.V.
Petrovskiy) 2-go Moskovskogo meditsinskogo institute
(ISOPHAGUS, neoplasms
surg.. morphol. of esophago-gastric & eaophago-intestinal
anastomosis)
S,2 OKACH NEOPLASMS, surg.
morphol. of esophago-gastric intestinal anastomosis in
cancer of cardia)
(IMSTINSS. surg.
morphol. of esophago-intestinal anasbomosiB in cancer of
cardia)

30NDALEVICH, V.Ya.; OSEVA, L.N.,--,. -
Work of +16- '4hite Russian Republic Surgical Society. Zdrav. Belor.
5 no.9.'77'S !59. (WHITE RUSSIA--SURGICAL SOCIMMES) (MIRA 12:12)

--- GUSEVA, L.N.
Sarcoma of retroperitoneal space in complete reverse location of the
internal organs. Zdrav. Belor. 6 no.9:69 S 160.' (MIRA 13:9)
1. Iz kafedry fakulltetakoy khirurgii (zaveduyushc'hiy - professor ,
P.N. Maslov) Minskogo, meditsinskogo institata.
(VIGERA,ABNORMITIES AND DEFOWITIES) (ABDOMEN--TUMORS)

GUSEVA, L.N.
In the Society of Surgeons and Therapeutists. Zdrav* Belor. 6
no. 10:68-69 0 160. (~MIA 13:10)
(WHITE RUSSIA--SURGICAL SOCIETIES)
(WHITE RUSSIA-THERAPEUTIC SOCIETIES)

GUSEVA, L.
Meeting of the Surgical Society. Zdrav. Bel. 7 no. 5:71-72 My 161.
OGRA 14:6)
(WITH RUSSU-SURGICAL SOCIETIES)

, - 1 1-1- . .....
GUSEVAJ, L.N.
Nitritometric titration of some secondary amrq:3 !~~Hh iriLl,nla'l
indicators. Sbor. nauch. trud. TSANII 6:103-1001 U~
(141PA 19:1)
1. Laboratoriya farmatsevtichesko.go analiza (nikovotlite-il - kand,
farm. nauk M.I. KuleshOva) TSentrallnogo apt%echnogo nauellno-
issledovatellskogo instituta.

KORNILOV, I.I. (Moskva.); MINTS, R.S. (Moakva); GUSFVi~, L.N. (.Moak,,ra);
MALKOV, Yu.S. (Moskva)
Interaction of' the NiAl compound with niobiiim. Izv. AN' SSSR.
Met. no.6:132-136 N-D 165. (MIRA 19:1)
1. Submitted Ally 30, 1964.

:T1
410'
TITLE: X-ray di ffract ion anal of the, Cr-T& s'ystem
A. j
SOURCE: AN SSM- Izvestiya. Veorganicheskiye m tatia 1,?,-:v4
no.. 64~ 1965,
880-634
TOPIC-LTAGS - alloy-s 'heat -resis*
tant~alloy 'chromiud.Ajloy.~
A
-tantalum -system system phase, d 16 Pase cop
chromium h
structure "A
W.
talum al ont t%' re 4evi-.4! in'
ABSTRACT: Cbromlwm-tan it h6. tant~aum C elit
-AOYB W 17
tation - melted from >99-97% purflCr -and > Xd -sit,11di'J'a%.
99.9%-mp~ire/Ta~ in'*purified htliud.
by x-ray diffraction and zri;`r-os~ruc:tura1 a4talysi '. ne phase ~Ia,:;i7l:'~;7o~ tCr,-Tii 31--
system (see Fig. 1 of the. sure) vag. plotted~oa the basii;, of obteined dp-tq..;, ~ 1t;!--,
-was found that the maximn solubility of Ta in Cr ~em'pq_',It'atuvei'-~
s 5-Z at% 4t
and drops to less -then 1 at% ih st 14ooc. About 13 at% Cr dissol,,;~es bi Te:. 80W~ili~j
decreezes witb decreesing -temperatures. The existence of two modifications oj':TaCq.
compound was confirmed, the high-temperature modification with a, hexagonal 1--truct,
Card 04;
L'.

I I I . - - ~ ~ I:- " iiii" 1:1 j ill:
-65
L' 63497t
ACCESSION NR: AP5018921 Mc 0I
1 7 1-i. 1:

1 0 41fe To,
:at~!

i9.
the,:
Phase :diagtad of d
. ;A:

em-
Cr-Ta sys
V !It

Cav-d 3/3

AUTHORS: Shifrin, K. S. and Guseva, L. N. 49-6-18/21
TITLE: Forecasting of the natura 1 illumination intensity.
(Prognoz yeq~testvennoy oaVeshcheiuioxti)-.?
PERIODICAL- "Izvestiva kicademii NaWc, Seriya Geofizichesk a"
(Bulletin of the Ac.Sc . Geo hysics Series), 1 0,6,
pp. 82~-830 ~U.S.S.R.)
ABSTRACT: It is now known that the regime of the natural illumination.
intensity is independent of the geographical latitude of the
observation point. AccordinG -to data published by
Sharonov, V.V. (1) and particularly data published by
Barteneva, O.D. and Guseva, L.N. (2), the natural intensity
of illumination in a given point is an unequivocal
function of the height of the Sun and the degree of cloudi-
ness, i.e. it depends only on the character and intensity
of the flux irradiating the lower layers of the atmosphere.
The chan6es in natural illumination intensity caused by
fluctuations by the transparency of the atmosphere are
smaller than the accuracy of observations of the illumination
intensity. Therefore, it is possible to forecast the
illumination intensity by utilising the existing scheme
of forecasting cloudiness. The aim of this paper is to
cardl/3 develop a method of forecasting of the local illumination

49-,6-18/21
Forecasting of the natural iliumination intensity. (Cont.)
intensity on the basis of cloudiness forecasts. It is
thereby assumed that the success of the forecasting will
depend on the success of forecasting the cloudiness and
also on the probability of existence of -the above mentioned
unequivocal relation between illumination intensity and
cloudiness. The data given in Table 1 show that the
illumination intensity changes relatively I-Ittle with
changes in the shape of the cloudiness for various cumulus
clouds. On the basis of the data Civen in Table 1,
Table 2 gives data on the total illumination intensity in
terms of variations of 'the natural illumination intensity
between given limitua of maxima and minima. Table 3
contains data on the scattered light (illumination in the
shade) corresponding to seven forecasting classifications
of cloudiness. On the basis of analysis of the data of
Table 2 and 3, it is stated -that in the case of a clear
sky the fluctuations will be small and the total illumina-
tion intensify will increase from 5000 Lux for a height of
the Sun of 5 above the 0horizon and to 90 000 Lux for a
height of the Sun of 55 above the horizon. The respective
Card 2/3 values of the scattered illumination will be 3000 and
40 000 Lux. The author also mentions the work of

49-6-18/21
Forecasting of the natural illumination intensity. (Cont.)
IMUrner, H. (4) and states that WOrner tries to circumvent
the necessity of forecasting cloudiness and considers that
that is not justified and that to be effective the method
of W?Jrner requires accumulation of illl'~mination intensity
data over many years for all the points of interest.
There are 3 tables and 4 references, 3 of which are Slavic.
SUBMITTED: November 19, 1956.
ASSOCIATION: Chief Geophysics Observatory imeni A.I. Voyeykov.
(Glavnaya Geofizicheskaya Observatoriya im. A.I.Voyeykova).
AVAILABLE: Library of Congress
Card 3/3

f
36-68-7/18
AUTHOR: Barteneva, O.D. and Guseva, L,N.
TITLE: The Effect of Meteorological Conditions on Natural
Illumination. (Rezhim yestestvennoy osveshchennosti v
zavisimosti ot meteorologicheskikh usloviy)
PERIODICA,L: Trudy Glavnoy geofizicheskoy observatorii
1957, Nr 68, pp. 120-131 (USSR)
ABSTRACT:- The article summarizes the pesults of observations on
-the interrelationship between natural illumination,
degree of cloudiness and the elevation of the sun.
It was found that the correlation between variations in
total and scattered illumination i~emains constant for any
latitude in Russia provided that the sun's elevation and
the type of clouds are the same. Hence, the information
obtained by V.V. Sharonov for the area of Slutsk is of
a general nature and has been confirmed by observations
made at Irkutsk, Tashkent, Yalta, Nikollsk and Lisino.
The article mentions Ya.A, Lopukhin and N.N. Kalitin.
There are 8 diagrams, 3 tables, and 32 references, of
which 27 are USSR.
AVAILABLE: Library of Congress
Card 1/1

ASHIROV, K.B.; GUBANOV, A.I.; SURGUCHEV, M.L.; GUSEVA, L.N.; GPURlN, N.V.;
YUGB, L.G.
Geology and development of the Tarkhany oil field of the Oil Field
Administration of the Bugunuslan Petroleum Trust. Trudy Ciprovo-
stoknefti no.3:165-182 161. (MIRA 14:12)
(Bugurusian region--Oil reservoir engineering)

ASHIROVY K.B.; GUBANOVA, A.I.; SURGUCHEV, H.L.; GUSEVA~ L.N.; OPURIN,
N.V.; YUGIN, L.G.
Geology and development of the Tar)d*my-field of the Oil
Field Administration of the Buguruslan Petroleum Trust* Trudy
Giprovostoknefti no.3.,165-182 161. (MIRA 1.6.'7)
(Buguruslan region--Oil reservoir engineering)

ASHIROV9 K.B.; GURANOV, A.I.'; GUSEVA, L.N.; OPMUN, N.V.; YUGLI, L.G.
Geology and flow diagrams of the development of the Alakayevka
field. Trudy Giprovostoknefti no.5:197-208 162. (MBA 16.-8)
(Kuv.bshev Province-Petroleum geology)

ASHIROVP K.B.; GUBANOV, A.I.; GUSEVA, L.N.; OPURIN, N.V.; SHALIANOV, V.A.
Geology and oil potential of Devonian layers in the 14ikhaylovskoye-
Kokhany field and basic prerequisites for its development.
Trudy Giprovostoknefti no.5:209-221 162. (MRA 16:8)
(Kinell-Gherkasay District--Oil reservoir engineering)

ASHIROV, K.B.; GUB UO V9 A.I.; Q L.N.; OPURINV N.V.
_q]~7A 2, .1 -
Practice in the development of the pool in the layer B of the
Radayevskoye field. Trudy Giprovostoknefti no.5t24O.,X 162.
(HIM 16:8)
(Kuybyshev Province-Oil reservoir engineering)

GUSEVA, L. N.
Physico-Chemical Investigation of Ferro-Silicon. N. V. Ageev, N. N. Kurnak~~v,
L. N. Guseva and 0. K. Konenko-Gracheva. (Mletallurg, 1940, No. J, 1~!,- 5-12). (In Russian).
The authors describe an investigation of the physical properties of Cerro-5ilicon. Alloy-fi
with silicon contents of 43-5-66-ut were prepared by melting, castinS into heated moulds
and coaling slowly to avoid cracking. In alloys with 43-53k Cf silicon, the structure
consisted of FeSi dendrites against a backgronnd ol' large Oon8ated orystals of thel:-phase.
The structure suggests that the,&-Fhase is formed by a periteetLe reaction between the
molten alloy and the f_-phase. Alloys annealed for seven days at 950C C. showed decompo-
sition of the r, -phase into a eutectoid type of phase. Commercial Verrc,-silicon had a
peritectic struc- ture made up of crystals of the 6 -phase surrowided by the Ys -phase.
Measurements of the electrical resistance and the temperature coefficient of electrical
resistance of cast ferro-silicon showed no anomalies. The; -phase hr~s a higher electrical
resistance than the t-Fhase. Microscopic and X-ray examination show that the; -phase has
a homogeneity range of 53-54,5% silicon. The crystal strvicture iDf this phase was determined
The X-ray examination showed that on annealing the amount of the;-phase Is reduced due to
decomposition into silicon, f-phase and an unidentified phase.

00 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
a 0 0 a 0 0 0 o 0 0 e 0 o 0 4 0 0 1 4
03 1 1 4 1 6 1 A 9 IQ 11 it 11 W is bs, 1) to " It
A I f. 12 It. L_ _L a ft r 9 A I - I __ 9
g 4 Co"M
-A!
11-My lovemisMiom of OA AhupJalum-fth Al Me Cu Alloys. V. G.
Killiti-toov. &lilt I.- S. -1 Ux Sri.
0 . ~*), IN2k,.v, i;.A. RI[IR 1111mim), I The IN-I've X rav
I " ffs"S.). low 1(lim
00 s Ik.'Atit'r U411114061. Its- filicniat"pit. e%attlill4tion. "to., Im'I
ifi-termine the ph"m in aluminium-munesium-t
0 &M 51) %t,% magneeiltus. The X-rav J."A'Irr
0 hV'rrt. ., m. the Chang" in IsItal. 1161101110-ter 'AMA U*ll
0 devel, Ite,
00 to tirtermilte, the "ubility imicithrmis of magnmiunt ant mlilwr Ill Allifflill-
illill at 445'. *41'. 31101", atui 2(111' C. ; file 5191- C. imothmn amA ,I,tnir.,f hv
The sense nk-tkmxi was tja%i to determine the Immiularies ;(
so the phameo amijuilling thr temary *AW ollutital at the x1m),re Ipluls-raturrit,
fit.. investightiona In-inu earrivil out with alkiya having "millitmitRim ititiviteil
of a;
I u1mg Iteven Hines rimlisting fmm the aluininium mnier. 11wirrart-mvenphaar
60 a! fit-his neightmiuring on to the tOnUWV SOIW K4UtkM rt'gk)fi. ISAIUCIV : 2
Go x L. x + L, 2 f- + T, 2 + T. 2 1- 7' i. M,Ag, AIR]
Mir, where L Is the mmlit,tAnil AJ.VuMu.ssmI 7'i.M.CuMg, When
Ai..
04 the teluilwiratuirr is Iowemi tc)2NItp'C. thu tuo-lilum- n-gions Airiuk. hit.- ti-
lhlrve-pham- rrgimts. mitivially t6- m + T i. M.Mg, n-gion. r%imud. [it
;%1hWmofIIw lIumbilmin i.vix-falliall ifull contrilt),it is like CUAI, 41.1M.Cu'Itlit,
TO g mlijklAICRIS thfil An' MIKIIIAlble for T).. a xillilint
rfrev( PIRPLIM be ObtAint'd in Sitil Ull ill O'S,~,R fultiowsium and 3 41.4,2"
,~ . .......
4) 1
Co 0 I's 0 4 a 6 0 * 111 0 Is 0 0 0 0 0
U n It b )6 17 2 It N 11 1? U 34 U ~11 V N V 40 it 4;
1-1 1 _M~ a % ;~,(L It_ lt~ -c-A 2
I
43 M Of:*
s o
t_oo
1.00
-00
-00
.0 .6
goo
=06
00
a
izo a
goo
00
Argo
.00
lilt quetwhing firum It.
14,00
oto
06 00
At& ILA 00
60 8 WOO
it,
10 .0
Is a Iflittl It mmwn I'l
00 0 111, goo goo 00,111, 0006 6 00 0 ,0 0 0 0000 00 fees 0 09 0
00 go 00 so 000 * 0 0 0 0 * 0 4 0 a 0 0 0 0:0 4-0 a _0 0- 0_0 0 -0 0 0 0 4 0 0

A,A 16 11 to it Of so 0 0 a 00 00
I,I- 1--k.- " 1, Z
,, "'m -_t__k_AA,,0 M.M.Mt-C-11 I I I L
Dieftibution of the electma density I. metillic aluml-
nun N V Axovv 4m1 I.- N Gu-%o ..... . L.. so
Imis lo--tx~ Vlwoi., A,-,,.I 1~ 1 14 , 1401
U.N.A.V.. iL.", .., IV41 . ..... 0 ot. 4111
I'mol slata 0 )aole,. lit 111JIVY, aild - 1. t .1
stilt! thodc of Prindley slid Ri,llcy I& C.A. 3j, towhij...o
the at."'It"inglactof Fcurvr, And Willi tile
4.141 A., the electron d. .1mrilmom it, lite .%I
is lattice hiLi been ralcd. by 3~liloelwmlml 14.4irt~r
Calm. lit thediimi-ml 11001 at !Nl* yj"hi, 11,K
the it. o%ing totupturvol th, wise.,
of F for higher lemp.. the elvtross'll. %%m hoth'-r
lost"I. front 0.2 1-, 0.2 A.. Im I I(m) 1. Willi the "Svc kilgill
%t,, Ko. Ill 7M' sold 10,111', and %%ilh Ille wivu It.,11CIll.
09 llltA)* the orit. Valor, 111.1111%V1 and tile 11,10,111 w1i
k~,Kor. oullmot: dawtumi..". .I tile
noticeable at 71110% Vani'll lit I(MA1,;
that telop rupture of the Wiled ha, o., C114NI.
At *till blilie; Imp., 1&0. trrwo~ W11--l-mlioll t.~
retlection% have valov, *hieh fallAithiii the
lonits us error; h4he't Scroravy i. 11111, ol.14411"I at tile
valen, temp. of Ka wave lenvit, -4 Fe, Co_oul
TV writs. It is con-equently "labli,li"t that its vi... .4 it 1,.w
LaIcn. temp. it is priefemble to tia tile As-i-t --
length.. With h1o Ka, mic-n. tetop. UNW. it,.. di,mbo-
tion curvest It"I: contputest told tol.,lint lot the 1111'r.lark, -
Imms 11001, 11111. anil I I fill. Flom th'.-
iaidsu of else loss. in the AT IAIW~
0.95 1. Its the &;mkv lwsw~n tou%. Ilso h,tnbots-at s.
even. Curnpairiwn between the exptl. einve, mul ih,
PIFTALLIFOCK&A. LIT Ihewl kid curves almwn for AV and LIT Al I,a,l, to
the conclusion that lit the sitelal cfy%tal Litti-, At I. Fr
Io", It
-~w d. N
1_-....-
U TL '. No, 1% -sr V
dMO,
0 see** 0 60 0000 0 0 0 0 0 0 see"
Is a 06999 0 as 9900 ,_~S* 0 :: : : *0 0 0 00 0 0 0 0 * 000,

0 111111_d~" 6,tilais,ittim, go 0 0 * 00 0 0
.?O?O-,6rOOOO *Osseo 00

1,
i 0:
If 1 goo q 0
Is
0
t u S) is 0 - a 0 111 V 13 us )IIII)
i
% lilt 46
. .
so .1. , 1. . I
A
I-V -Fi !A! , !Lt
!% . 8 -A .1
-
-
AND r&Cff.ll(4 -.1.
I rich alloys Of maposium with kduvtsinuaw- -
t
I u r
-fi
- A
M
440' 5% Ii
fir tr
ut
1
u
ol .Rquillbirlictu oll"frosat of the system Mg
I
I :F,:; 1
t, ril
.
r
er
l
Mp.
t
The - MO.Al. I~
AS US N1170. witin, NltoA%
MSAg Ma.M.. V. G. liniontiativ ofnit L, N, (N.
11I
';d
ad
S
G
l
Cl
A
I 1.111(trv ... flon I'lle Is- III M Vs'. 4o". I iot_
`
:f;
so
.-
.
.
nti,
n
ient.,
r
.
kninaktiv
uinfl. 4 glMill"I ..I V,Ifl
it. At III
u loil
"Iss. If).. trol,l) I
4111"

fee. C14SI& Ifl. thim. 1943,
h
f
i
h
M f
I.P, 1 425* and t tell tlisr;l tit &II " al ~ MA'All
so i
11k
"Int
3117 rhe aris-'r plortsil.
roill
t
S " This% at 42NN". file ctir%vot lot IN-Kinjil"t Cls"fli. z1f 'vs Mill
&,I.[ So, pillar As still At igith 0A.M,. Thr, "*iln,l ikrrv,l at 1:17, If V

so A
I~e astj lpii;~' . Phaw diallfaini, Weir sr'lablib.41 fly
%I I
"
It(
h
t
l
i fit 'Intillialirial. twilts. "r t,afl plia- to I , at lots is, 44%
'so

00 .
st-lav
oo. saw
Imm" .( th's
mal soina
., Illwit-ilap
y
'
-1
I'l
11111tid it, %lilt tilt
Are dMI
1
I Imin
'
s-
-so
8 latlo!
ll
10
1.
FNIC
111
nisitiffissis wiled in the hinaty PIlls As &oil %IS -At systlomm: In
A thitsi ri-t at ul,l
I-m
-
l
4
i
00 Al
i
NI tit
tant
tsill ilm, .
fflu

0 t
flit -y phow I)( MI-Al lwovwil on the c*mlxl.
.
S.
's
-
.
-A
haw of 161
(looll
fil
fl
ht
h)
lt
d
f~ I- A. The ~vlllln %foliAX-NIII.M. Ileft'liti flaw -
~`n
gee

9 J; iort
, t
s
e
sa
aug
e v
,
is (
p
1
l
As) Is )I (flaughwAV, to,). The triple gs,lit ft ". i's a rt (he line is( the peritiviW ittonlifolinarion If j- milit -
- I
lot til
~41116

so III! (in'tra.1 Ill sall. Ubs, notation &I is trwtvr.t tit Crystalli .4
rimsi
WNO
whi
il
d
hl
h
O l
rrilory it At Ill
,Ill' I it, loss, hilvi- 1. ifir Nil;, kg %1,~. lil
pt.-~
e.
,
t i
ll.
n elc
nill *l
~
Alt
oor.
-
-
,
nlaill
hi
h
k
th
h
h
d ,
41 flit- n'llipl.. Mg"J" %K
"."
Al
00 a s
re
ar
er
an
c
I t
e
&w sl4wars
1, W
" p
di
i
l
i ,
L.
.
12.3% 161S. I'll, Islas, Sir
l
r
I ,so

1 menskInal me
t
alfratits,
. lighwor throlushout. Two-d
ng l$, "
al"
I
r,
-
i
f
l
z
00- air Own for three radial liertions ctroorrespanding to con't ti
ornwirt, I
ist platte at :I 7..V7S, Ag.
I "I A[, NIM,
" 00
raliStS At At - resist. 1: 4. 1: 1. and 4: 1, for (As + At) firistir trillp 125
, S.-lill-11113- ""(I- I,rd. I'S, Itiv.1"
-00
tie, IW)7 -irtsphorsilroorsphi
" to.Uj~ ( Nf from 110%ta, 0). Mk
itstroil r A At has 8 + (A + -,,) + (3
str
l"
am is
"'roly IIw alld 1111"t"graphy, p"I
&lilt (111, lit 3.101 % ;~fkl
goo
S
+ -1. + -1.); 110 4NIC RI 7 Al
s + 0 + -0 + A +
-
+ -Y2); JIM sl` M is+ 11 agrettlit-lit with 1141loilli'lls. lii,-
shows thre" si"9111 PhAle vtorra~ ,( the ternary .,list -111,
Z;O0
11
244.1 "' As. 25.96
i-va + .11 + 4); Al. -ri + (Ti + 70 +
1
AT11 .
, -n and -n, ran tior"hiL, ar,, , + 6- -f- V7. &till
Dole thr
l not
1 (A + -") + (A +
(,to I- -rl f- 1) 1, 5,11,79,
1y. A.517.
-
A A re-p
otoom area a + -,, + ,,. 1(,,Iatiw i's
fnl,s dititill
.
s
I
ha- Ill"Ifulgiri" off
loo
h
,
hif
p
!x00
n +
+ -,,); 441% AS. 10;,, At, 4- 4) + (
Surface Consists tol
hl
Ii
t
h
l
h ,
m"
t
'
,
.
fed lit
h
ot
fifrmgs~nt 11mitisix r-jell
.4 1),,. 6-1"1
us
flis
a
e
ese (
e, t
-vs Proust t
four firlda "Wr"r ling to wpn. of the temory mislid .
"All' C"'I'ligooli"In Sit the dAtA (IN file t4loil Stills, ri,th
t:
in ?.IgAl, (-vs), in MaOlg (-n) and in
ailing In 'Mg (1) d'its obtained lilt he 00
.
Ilan. the ternary
In ary"Inent wi*b Itinfill Willing diffrorene". 1. the "Illil.
tale, rise junis"Istry Iw_
t
h

3oo
I L A -IIETALL(MCKAIL LIVEO&Tifft CLASSOICATOOOI
A S 9 weet' t
e wilid vills. J arul thr tn'tv-phow arta, it vit,ilgiv too a
- sq.. roe

-
31 u 14 LT f,
e IS'

F An j I a rill 0 a a I ill lt!pa,2
too
.14,
Pill#, IWAIC on to plan
l
ifesooosefoooose
e
1
Z ess
1
a 0 go 0 is 0 0 0 0 0 0 0 0 0 so
: : : : :
o 0 000
0 0 0 0 0 0 * 0 0 a a 0 * 0

4-o
UF
hiftm to hisItet voovus. ill tAg + U) as compArttl with 00
the nonequil. cmulm-ot. At ill, rath, Aj.,Al - 1: 1. the 00
hoinclitenvott, IMd ill the rquil. thagrato Inchm" conipus.
114 which ill the flollutillil. oate the ternary tulerlic Is *0
vixt. lt,mmlsri,~ 1vt%vivit the two-phaw anti thv three.
phaw arm err hill-wi- trot,stly shilit-41 Ill the %more three.
00 th'". Tho,, &I AA:Al - 1:4. without rqulL. the tmm-
dary 1- 4tuatell at the tvmp. d the tt"ary eutectle at
9*1 sivout 27~`e (Ax t- At I; at etrull.. at as it,* 4% 31a), do
-
whole wctiml jus-~ mly thimigir live tsme of rise jl~hwm 00
into the two-pha- more A + -wi- Th, Isoutuli" line I*-
twrm thc two-phaw atut the Ilmv-phaw arew th"4pistal" 90
&jut the whogelielti i.,veupicil fly& +-ft. Oijillisoretion, 410
in the equil state. ill%! three-phase rwdm appears only at
00
temp. atmitst 2oW &tilt belim; hem tire boundary Une be-
flitten 8 +- It anti a + -it + -ft lw&"nf nearly parallel to the 411
cosupti.m%is. A third anvit ill the coolinscurve wa% only
Go
oftwrved tat rumcquil. symcniv; at equil.. the line c(wrr-
$WAfiI19 to PTIM. Ol the tCfn*rY VUtrCtiC it ftl-~Vllt MA 90
the diagmm appea" as that of a bioary systern. Ascons-
00
pamt with flalighli"t's date. the Nnindary lines between
the (WO-1111A,e Ault the tht%C-1111ALW dtt-4% 111tel'StICt tilt title
4 ppin, clif she terumv rult-clic. on the sections AS:Ai ~
'
psod bfl%(As +All.&, against
1: 1 anti 4: 1,,st. rr-11. 111.5!
llaUghttAl's 17~7,, Alld V.%. A4 A ctlawquruce, the regimi
of wtin. of Our, pha-, &I Ilse cut'vsk. temp is oulliclabst
Ita"ower. that 01 A 'ji ftliorwhat brostler. N.'rhan

00
*0

o,
,Zz-
N
44.
USSR/Chemistry - Nickel, Electron i %[ Sep/Oct 48
-~Density
Chemistry - Density, Electronic Structure and
"Experimental Study of Electron Nnsity in
Crystal.3: No 3, Electron Density of Nickel,"
N. V, Areyev, L. N. Guseva, Inst Gen and Inorg
Chem tmeni N. S. Rurnakov, Acad Sci USSR, 9 pp
i
It I% Ak Nauk SSSRY Otdel Khtm Nauk" No
Conducted experimental determination of the atoale
factor of diffusion in nickel by method of substi-
tuting an aluminum standard in cobalt and copper
radiatlons. Calculated electron density for six
Am 27/49T39
USSR/Chemistry - Nickel, Electron Sep/Oct 48
Density (Contd)
directions of the elementary nickel cell by method
of Fourier's triple series for calculated
temperature of 810000. Each atom of nickel is
j9ined with 12 close neighbors by "bridgbe""of-thle-
Increased electron density, which Implies the
presence of exchanging forces between atoms.
Submitted 22 Sep 47.
27/49T39~

10
all 1 00 0 0 1 0 0 0 a 0 0 09
I ft Is 14 Is WI? I. P x p x J~ V " 0 a . I it V
A A L- a L_j-j r Q. P I - , 11-1 04 M M U it), 41,1-4
oe A ItF4ht) 1,,,, alt'lli P111,01ill
so a

a
i l
00
so .3
00
00
0

Mectma dowillily of akkel. N. V, Apev And L. N
Ndish 59, 65 it
t*.IIWVA. flobhudy Mad
110,101. Alonif lr%vtal plAtf... it-I.
al,A. I.Y Footiri rli- llool ills I %Iol
at. Icate"Ing factur curve obtaillell V01111 fillkly vfy,t. N1.
by u-ing Co and Cu radiation And mjvwting to Alm, vulfiv. .
with Al I-owder imptanihird. KmwhNialonikfink~.Iwiih
iti 12 urtit"I neighbl" by briliget of bi4hrr elmirmi,L. I 1
rlrrlrun~ cu. A., a% rualparrd with shout 0. 1 rl-~trtrli~
cu. A. bw thr intrrlotik- -pace. Thr 6-troo d. 11,10111.
N. mon
tion in the i(M) plAtic 14 shown.
'i
8 1 1
400
.00
Vo
go
0
0
coo
49i
AN.*
400
t
00
AID.%LA StTAILURCKAL LIT(NAT641 CLASSIFICATION :Z. tie 0
U," 49 03 A-1 I m# (1 4
10 0 It It ;V Ad 9 a A 11 11 n o v!
we 00
0 0 Ole 4 000 0 0 0 60 00 0

oktm derwily b crywWo. TV.
11
1
4
111110 6111 N.V.AjmvwvIL.X.Gmrv;&.
_T
10"t. Aba
1'"k S
S
S
M
i
(W
Kki
-
.
.
.
e
.
.,
at.
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