SCIENTIFIC ABSTRACT GOLDFARB, R. - GOLDFARB, YA.
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December 31, 1967
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SCIENTIFIC ABSTRACT
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GOLIDFAI~B, R.I.; DANIISNKO, P.,L.
Determining the raffinose content of --molasses hy irean.3 of rancr
chromAtol-It,aphy. Sakli.j)rom. .34 no;5121-23 MY ',")0. (M:ll i/," 5)
1. Ukrainskdy iapaucLno-Issledovatells-kiy insti-Ilut spl-rtovoy i
likero-,;odocl-moy prormyshlennosti.
(Raffinose) Omo sses)
(Paper chromn _ . Y~
ROVENSi,~IYAY GOLIDFAM, ".N.; VA3".,%.OVSkAYA, I-II.A.
Resistance of dysenteric bacteria and ente X pa tho -genic'Eticherichia
coli to some antlinicrobic proparations. LalT.do-lo'7 no.9:53 l) 161.
(mll,-k ly~: 10)
1. Sanitarno-epi-de.,~uolo-iches:caya stantsiyu Lenins:,(,go rayona
Dnepropetrovska.
(ESCH"iaCIIIA GOLI) (DYSENT"-:~,*Y)
ACCESSION NR: AP4041363 510048/61t/0281006/0998/0999
AUTHOR: Ugay, Ya, A.; Averbakh, Ye. M.; Fogel'son, R. L.,
Gol'dfarb, V. A.
TITLE: Some properties of thin indium phosphide layers
SOURCE: AN SSSR. Izvestiya. Scriya fizichaskaya, V. 28, no. 6.,
19640 998-999
TOPIC TAGS: indium, indium phosphide , indium phosphi.de f1. In, indiura
phosphide property, film property, film alectrLe conducci.vity
ABSTRACT: The temperature dependence of electric cimiductivity of in-
dium. phosphide twin films and of their limit of absorptton in the
longwave range have been investigated. Films were prodticed by a
separate vacuum vapor deposition of components, first: of' fildium and,
then of phosphorus. under pressure of about 10-5 mm lip at 400C.
Electron diffraction patterns of the films corresponded to those of
the InP compound. The temperature dependence of eloccric conductivity
of InP films 0.55-0.06 v thick was determined at 20-500C. One of
the two films investigated was first annealed in vacuum at 2,50C
-:1/3
ACCESSION NR: AP4041363
for 3 hr. As shown in the diapram (see Fig.'l of the Enclosure),
the electric conductivity of the films at high temperature is almost
identical. The width of the forbidden zone determined from this
diagram is 1.42 ev. The width of the forbidden zone detevmLned from
;the longwave absorption edge wan 1.27 ev. The higher value obtained
~from the temperature dependence of electric conductivity is explained
by partial decomposition of indiurri phosphide at. high temperatures.
'Orig. art. has: 2 figures.
ASSOCIATION: Voronezhskiy gosudarstveny*y univeraLtet
~(Voronezh State University)~
SUBMITTED: 00 ATD PRESS: 3058 ENCLi 01
SUB CODE: SS,IG NO REF SOV: 002 OTHER: 001
co i
:2/3
L 5423-66 Ez1iT (I )/E P./EriG (m)/E lvA (%w)-2 I j 'H r, AT
ACCESSION NR-. AP5019764 uVoo 5 1/6 5/0 19/002/028h /0285
rt, 533-9
AUTHOR: Gol'dfarb, 1. _M. Ljq1
TITIE: A simple technique for determining the temperatwe u-nd elt'ctTon density of
a one-component plasma
SOURCE: Optika i spekt .roskopiya, v. .19, no. 2, 1965, 284-285
TOPIC TAGS: plasma temperature, electron denrity, line sp#ectrum, gats discharge
plasma, continuous spectrumy radiation intensity
ABSTRACT: The technique described is based an isolating the intervals in -which
the intensity of the continu-um of a nitrogen or argon plasma, is anky slightly de-
pendent on the wavelength and exceeds substantially the intenaity of' the line apec-
trum. It is then possible to forego the use of ppectrcy.,rraph and photograph -the
process through light filters. The measurement A411tere made Tor the following
sources-. (a) 25-amp are strength 1O6W1oRj_Vx&_ning in a strealn of' axSon bet-veen
tungsten electrodes in a quartz tube, (b) 2bO-amp pinched ar., fr(M am argon welding
torch with water-cooled copper anode, (c) 10-amp arc 20 mtk long between carbon
electrodes in a weak stream of nitrogen. The fornw1a used for the oxgon plasillp- was
5.9 x 10-"I,
Card 1/2
L 5423-66
ACCESSION NR.- AP5019764
where ne is the electron density, T the plasma temperature, and I the intensity of
emission (w/Cnr3Sr-1A-1). The formula for nitrogen is
I - 3 X 10-35 n2 T-1/2 + 8 X 10-17 n& T---1 X,
e
where x is the degree of dissociation of the nitrogen. The results are compared
with published data and some of the differences explained. Advantages claimed for
the method are the possibility of determining plasma parameters wil;bout complicated
spectral equipment, higher luminosity, ease of conparison with a standard source,
lower errors in the measurement of radial diatributions due to plasme, displacement,
and smallness uf reabsorption effect. The electron density and teii(perature errors
are estimated at 25% and 200K, respectively. Orig. art. has: 2 fiewes and 2
formulas.
ASSOCIATION: none
SUBMITTED: 21jui64 ENCL: 00 67JB CODE: NE, OP
NR UF SOV: 005 OTHER-. 007
L/ i/)
2/2
S/124/61/000/012/033/038
t2-'37/D304
AUTHORS: Gol dfarb., V. M, , a-.rid Stepanov, A11
TITLE: Elastic, constants and strecs of
stratiform heterogenous riedi~l
PERIODIC~.L,-. Referativnyy zhurnal, Mlekhanikrt, no~ 12,, 1961~
6. abstract 12V33 (V sb, Vopr., ddw~,,iki. 1
prochnosti, no,, ':.., Riga, AN Latv`)SR, 127-
158)
TEM A stratif'orm medium -is considered, -where each layer
consists of a different material,, The medium is put under streS~':
in such a manner that mean stresses in each layer ore con!,tant.
It vias sliown that the given medium ca-~i be coji9jd,?1:-ed anisotroDic,
and the method for determining elastic constants in an aniso-
tropic medium ;kith elastic constants of each layer kno~vn ~,,as
given, As an example, stretching of a stratifor-, model was con..
sidered. Each layer, in this case, is shown to be undc-r
Card 1/2
S/1241161
Elastic conslants and D237/D304
three -directional stress. ard the layers %,;ith hi;-:her Youn:~ s
modulus are comDressed, ~;hile the ones ,dth modulus are
stretched- Distribut-ion o~' stresses in separate layprs ,,ias in-
vestigated for the case -wh~ln dimensions of the la-er,-3 ~`Ile COM-
parable .,ii'L-.h other di~menslons of the model under inv.':?-;ti.-aticn,,
Experimental determination of noduli of elastic~_,ty of some
stratiform materials confirmed theoretical calculations,, it
wag found that the distribution of stresses in stratiform media
foun.d. by photo-elastio, methods -~(!Lncides with the di,~trJ.bution
found theoretic,all.y. 1, C 0!11 1_' IA
Abstracl~er o nott- A(?
tion
Card 212
S/051/6i/oi1/004/002/OO-'
E202/1-"592
,J
AUTHORS Gol'dfarb, V.M. and 1L'ina, Ye.V.
I I TLE: Determination of the moan residence time of atorlis and
the Coefficient of diffusion in an arc disch.11-ge pl.-Illil-M
PE,RIODICAL: Optika i spektroskopiya, v.L1, rio.4, P)O1, 1115-1151
1 LXT: High Speed Pilo tographic "ittidil'-s of' Carbon Zli-C
discharges,8 mm long, were carried otit by introducing firle needlos
carrying 0.1- to 0.3 iniii diameter beads of NaNO,, B;xCO I and Li~,:O-
These needles were either stationary, or traversed tho plas rltt -)
channel, at midpoint between the electrodes at a consta;lt Velocity
of 60 ciii/sec. Tlie high speed cine' camera was synchrollised with t.hc
entry of the beads into the plasma. Background arc luminosity was
rejected by suitable cut-off filters. Two independent methods were
used to determine the coefficient of diffusion D. The fir-st
method was based oil plotting the rate of blackening of the film
against the time lapse, and thus lead to the evaluation of the Me,"ll
residence time T of the atoms introduced into ,,he plasmix an (i
hence to the detAnination of the diffusion coefficie t D 1* In t 1--j-
second method, the coefficient of diffusion D,, was :Ili,-ter-mined
from the rate of propagation of the luminous f.~ont within the plasitia,
Card 1/3
-7
Determination of the mean residence ... S/051/61/011/0011/002/004
E202/E592
using a sequence of high speed photographs 1-ind I)Lotti.ng, witil the
help of a microphotomotor, a series of curves rel.atin,~- the
blackening to the distances from the axis at each particular
instance. 'Flip results given by these two method~m ar,-.i smmm%r-Izk!d
below: Table 2
Metal T (sec) D D,
2
(cm /sec) (cin /-;cc)
Li 0.002(0.0014-0-0027) :18 4o
Na 0.003(0.0022-0.0031;) 19 21
Ba 0.005(0.0037-O.oo6o) 11. 13
V
The authors found that the evaporation of the bead starts within
a few thousandths of a second after introduction and that the
luminous region surrounding the bead grows preferentially in the
direction of the cathode where it is retained for, 0.01 sec after
Card 2/3
Determination of the mean residence ...
E202/E992
the main part of tile luminous cloild is dirrused. During Ch,,- ducay
t, il tile hi,~~Ilvs t 111ru i 110.91 ty wa.,l ob!wrved not a 1olig (-he it xI ~. [)It T.
along tile peripheries of the discharge. There are 6 figures,
2 tables and 9 references: 2 Soviet and 7 non-Soviet. The Englizih-
language references read ab follows: Ref.l; V. 1. Symon. Proc. Zoy.
Soc., 46, 153, 1925; Ref.2: G. E. Davis. Phys,Rev., 24,2d)3,1924;
24, 168, 1912, Ref-5: A.Arnoid .
Ref-3; H. A. Wilson. Phil.Mag., J . I
lrid.Eng.Chem., 22, 1091, 1930.
SUBMITTED: November 19, 1960
Card 3/3
3/0 8/i~ 22/326/C37/024 '65C
B 12 /Ij 1 4
7. -knl Gol, I '--trb V. M.
i na t r. o f e . a a a n r a 13 n o f e om 5 nd
iin !rc :]Jschu~-L;Fj
.-L--jion coefiicicnt in D,
v e iya . sor4yii
2 no. 7, 1)'2,
n 0 f - t 3,.-, S i n t e a 3 f an v c 4 11 S C "Izi
t'- a 0 ex,C I t~Z
- e: 1. ; ly":7e
&n arc r-sch
31, ;c):-'s~ ~,nt t tire t S
cent er of '-i i a i-iliare'. 2:-. e i e
2 o I c, c e n t r, i n ::,,L, t r-r ij i f ',a o n
L-, eleCI c i-
.1,4 C f' 4,1 kd n ve c o
- -1 4
nd D ij t
r, c
I C C, I I t or. s 'D e b r, e to b e 0 r
2
S 4- n n p /2 . 3 follows for the e a n a t i o n o f a e
4-,. t 1 L; S D and of Li, ",Ta, and Ba are deterrained 'c,, .7.eans
y
B I
Second) :'o va
c 0
U- ou ic,rl c Oe~ 1 ic
C, 1,?~ermined by
Of
S C. c
J
r e f
t --k
1,,:,l y e Lo na V i La I , vevila 60 1, 1 D.111~113 )
V-, LO I !a
V,
[1-'utu~!l effe(-t of elr!,7,t!nt.s in the rpectrurr.
rar.jles in a i~rbon arcl Vzairrmyo vl.iiil::~ia
,anizi:ov, rio.5) I (A 1"': 15
AID Nr. 586-7 10 juae
T:L,%STIC DAECHP.11NITCAL PROPERTIES OF LA~JATINIATED "IMHOMOGENEOUS
E D LA. (U S S
Goi'ff~r;D., V, M, and A. V. Stepanov. Zhurnal prikladn,:)y mekhaniki i
no. 2, Mar-AprI963, 100-107.
S/207163/000/002101';.1025
The of "..hornogenecus "thin-laminated" media under arbi-
U'ary is 6.J*,Zcuss_,d. The term "thin-larninated" mleans that there are
any iaye:rs a vou-:n, e e, ement in .vhich the state D st:rcl-ss is close to a
tenSion, Vomures,2_ion, Otc. ). Tl'e layers are assumed
7c) Oe an-' ri -,.i -:1y In-rercornected; ziiel'r -hicknes!; es are small rclative
and the S~reSS f4e'd Nvi~hin each laye-r is homo-
L
-.a is treated as hornoseneous and ani~*.;otropic, with -sym -
:--,etry a'_-,~ut an ncrrnal to the planes of Le L~~%ers, so that: -the elastic constants
of can '--e '_-*_---__~_-~-~,ined by -using the equations oi the generalized Hooke
ia%%r :o tha avera-;,:~c' ,,alues o-1 .3tresses and strains of the volume ele-
ment. stresses in an -Individual layer are determined in terms of the com-
ponen~s o"its avera.ced state of stress. The awraged elaat~c conotants and
. Card V2
A :D,
OF TIM [Con-t1d] S/:20'r/6" /OI)0/0D2/OU/O25
S S Z th(-. C-,,., a-i-i'sotro-pic layc:rs are also d--'s(nssed, and associated
fornaulz~s .,Or the -zt:~~ss aralysis o-f polycrystalltne media. are
T -7"Ive results, are in, r,,ood agreement with experi-
nncrit--l Tha, depe.~---'e-acc of the clastic constants of a t"hin-1:irninated medium
on its er~~o-netry e. , --~~Iative thickness o;-.' layers) is discussed. Because of the.
d f-icu:---Ias in investgating this dependence theo.ret4cally, a method of using em-
pirical daza to obt-nin coz-rections for aria-I'Lytical formulas is outlined. [ vic I
Cz,~rd 2/:?
VATZ.;WY-1,11, D,I.j' irc-h.; GOLIL)FAiLE, '.7,".., ral.J'
Calculating the depth of tulle fusion zom3 in wel-iing
with carbon dioxide. SIvar. proinv. no.8-18-11 IY 16.3'
(VIRA
-'~ ";,10' ' P.)II IF i 11 ~" 4 Lilt,
I A -~ . K .' L I-
L ~6929-65
ACC&iSSION NR: AR4039898
ZnX 3072.06 and 3075.90 At. Call 226. 4n CMIX
distance between the carbon a lectroidliaii i4as 6: MM
I ': drate
41 the
salts of the basic metal were placed . n:
electrode (anode) mixed wi.tb:Lcq4l dust.; I%e ziPc id
on the bottom of a deep bole inth anode., Time s0
e
trum made it possible to chooseicOnditiOnaluber b~
the "influencing" metal, zinc, land callcium'!ent~rej
into the discharge channel. The, 6btai!4~4 Ci ti
and concentration of the electi!o,xi6 ard Ovet~jes ~.oVi0
posure time. The results of the measurbmexits havei
wit
plasma temperature decreases LhAedreasi:64~ iohii,
J
of-the metal and with increasiniq~concentkation:o~f I t!
of ionization of calcium.~Odroaa~o;09:,tbo. is
degree d
duced, and the concentratiOnLj6'j:tbe 6X60 ~6n 0 inct6
of the decrease in te ",rature.!, This. r0sult: haim
control measurements based
roaden r*:,of:,theA d
characteristics and f rom the b
Card 2/3
6929-65
:ACCF.SSION:NRt AR4039898
'7228 an
d 6214
1, witb
juat
1 i;
j!j, j--
T;
i
r
f 1 11
i T. H i
t
!
!1-1 '~A
i Ell
Card 3/3
ACCESSION NR: AP4043025 S/005'L/6,1/017/002/0302/0304
AUTHORS; Gol'dfarb, V. M.; Il'ina, Ye. V.
TITLE: Cesium line broadening in the plasi-iia- of a dc arc:
SOURCE: Optik'a i spektroskopiya, v. 17, no. 2, 1964, 302-304
TOPIC TAGS: arc discharge radiation, dc arc discharge, cesium,
line broadening, alkali metal, electron concentratton, Stark effect,
spectrum analysis
ABSTRACT: The electron concentration n e of a dc carbon arc was
determined from the line broadening of Cs lines, the St-ark constants
Zor which were calculated by H. B. Griem (Phys. Rev. v. 128, 515,
k
1962). The use of cesium was dictated b,/ the insufficient intensitv
of the customarily used hydrogen lines in weak arcs. Tests with a
KS-55 spectrogra-ph were made to chec'r'. that the line broadening is
indeed due to the Stark mechanism. The dependence of n. on the
Card 1/2
ACCESSION NR: AP4043025
amount of metal introduced was also measured and the possibility
of determining ne from the metal concentration was verifted. The
variation ofn 1~ along the arc was found to follo~v t',1(? variation in
the metal density. Deviations occurring on the boundary of the
radiating region are explained. It is also pointed out that the
variation of line broadening of alkali metals, fteqiiently used as
buffers in spectral analysis, can be used to judge Lhe stability of
the excitation and ionization conditions. Orig. art. has: 2
figures and 3 tables.
ASSOCIATION: None
SUBMI'ITED: 09Dec63
ENCL: 00
SUB CODE: OP NR REF SOV: 006 OTHER: 006
Card 2/2
4
L 2350-66 ~,/ENG (m)/~ PA (w)-.2/E1iP(t)/EWP(b) lip(c)
ENT ( I )/E irr PF c
:ACCESSION NR: APS016688 J6/.vT Ult/0294/6510031003/0333/0339-'I
S33.0.082.5:546.293
'AUTHOR: Golldfarb, V. M.; Dresvin, S. V.
,TITLE: Optical investigation of temperature and electron concentration distribu-
tions in argon plasma
,e
:SOURCE: Teplofizika vysokikh temperatur, v. 3, no. 3, 1965, 333-a39
iTOPIC TAGS: high temperature plasma, plasma heating, argon
i I
!ABSTRACT: Argon plasma burners (high frequency electrodeless heating of gas at at-1
I -
mospheric*pressure) with water-cooled quartz walls of various diameters are studied.'
;The electron temperature and electron density distributions are determined. These
I
iresults were obtained by observations (with in situ carbon arc calibration) of ab-
isolute line and continuum intensities and measurement of 11 broadening, relative
:i1ne to continuum intensity, and continuum photography. The electron density of
about 1016 cm-3 in the burner assured the existence of equilLbrium, which is re-
lected in the small deviation between values obtained by thili abova methods. It In
I
,noted that sometimes when larger diameter tubes were used, the planmin column wa-ndera--,-
L 2350-w-66-
!ACCESSION NR: AP5016688
I from wall to wall. The temperature profile for such plastna was found to have only
~slightly lower average temperatures as compared with symmetric discharges. OrIg.
!art. has: 5 figures, I formula.
ASSOCIATION: Leningradskiy pedagogicheskiy institut im. A. X. Gertsena (Leningrad
Pedagogical Institute)
Y
SUBHITTED: 27Jul64 ENCL: 00 SUB CODE: KE
NO REF SOV: 006 OTHER; 012
I-COM-2/2-
, ) jj-J/,Tf
L 5138-66 1)1:-,WT (M) /T/E-,Tp WAE"Jp Ob ) /ZWk ( C) T,T-.1 (,-
ACCESSION NR- AP5018723 Uli/C
IN
R.
CNW > R(A'.
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a I I 0! T I 'A td IX (k Ct
L I I IS. 4A L a A F9 ItI TU I
41
basis at carbail ca
ThA,
_:"
d,,' rrurionicocAnts Ill. The actica of hromalpyr"Ic
n
and . amin.mmUnts YA 1. -4
'
Ater tt
.4 ~~, R. 1 10,
M. S K ul.k-a. .1. (4-, (W,~~ W
%;
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It c1fill cit'El ill m It t ()I. Fit Ili -*4
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-00
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d Wi
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ll 1, .star. CIli dim 1, 11 mi zoo
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.
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of ~J. It Ij jf%,"]" '
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11 U 11 W 1 % 11 4 1. x 11 IT
j L
11 11 6 il 1? 41 .1 1; a 6. go
I AA 0 U X 11
1A# action acid ITAUdirs an tetrallydroturAn. and 14DIIIr
der, TAIlves at 4-diVtbYI1LM1JIG I bUIA1101 1. NI
"",,kd Vg. I.. (;j:I,(jfUtj, j t" IT """ ~I ~ ~, 1,
It I Iw liw. IP-NIIA:jI,CfK'I If
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AIR -k.j. Mf
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1.1, -1 1) INIP) IT". IIIN K"
67. -111, TI'a Imn in NIt I'll gl%. , .11, 61:
Wll,n IV I, heated with W`,' Kill, :1 AT---
t-d!,slillim-1-1pulaziol IV , h, ~%, ~Kj' (plcr.)I,jjjAj, I,
's". P-NOTC,JIXOIJr and 11 ;iv, -41-, 1
%ilh Ill 11(, p-t,,6e-.,We, I"
a, Ih, If( 11,111 (VI,), in. 1.-~4 9 !'It _'
Irt ~I, v,-r y 11 yst,-pi, VI 11 .111) Iltlt,kimd Ii
yi, 1.1 frum I ~nd V. Wdu, I ",1. 4 VI It 1, IICI , I I f
_',~ 40' gm-, 4 &i.1hylaminoli,I)i p-.j,n,x.oe, .,;:,
171A tf'j,j,, R,... t,,,n,
_4110
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jZ041.
1,
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JIIITI'11111~11T'
LO
1.UICA TIC-
rx
IT
u it IT) IT
0 go 0 41 Q
0 0 0 a 0 go
0 0 0 g00 41 0 0 0 0
0 0 0 0 go, 0 0 0 0 0 0
,
0
0
O 1
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T 0
1
1
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1
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11p 9 1 1 1 w I A 1, t Po t4 It, It
O
4
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0 Tho attivill of cl ba,"alzrione Da and JuDiAll"34OVIC4
-A 11 A I- 11, 31 k., C.,mlov #,,.I
045 .......... t
Im "'I'd. I-V fr~lilm.l 010
llou,
09
N. 1:, 1,,, ~1 k,, I. 01)
Ht t
oil
k t
Os l..1 A Ill.,
Ole
. ...........l
al ..... .I h, l'L
.. ...... . ....
f
I
, 10 0
0
I lt~%Ilgl. 114 Mill
~16 0
1, t.-n-i 4 and dicil
;00
it, -qd thAll ill hw
OF 0:j if l,- -0 . ....... . n-0 0
PO 0~: hil gli, .%00
I. i,ith I
l
ti ts Alf .0
11 11 v &
i
00 00 40 Of 40066~00004610MON* %* 00 1*6 :1 Ald
GOLTFARB, Ya. L.
"P-cw,ylation of iviAiil-s bir lr'(-~,'uls CC ";i-tern," C,.),:hch.
12, Nc- 5-6, 1,1-42.
Inst. Org. Cheri. SSSR.
.A. -Un
00 A
N F
as A
*0
00
Go
09
'o 0
A IM-SLA .9 ULLURG KAL LITI14TUAICLAMIF)C Ll DOW
wit
0 o
~2 12-
o0000000 o 0 0 A 00
0 e
lei lot 0 Q it in 4 6
L. L
1w, ~
-100
file
.119
-100
-100
W06-
IWI; -" 4400
zip 0
Roo
0
qpo
All 0
sive
tigo
ate
An L s a -.1 11 9 A (1 3 a v
111 41 o 0
00 see 0 OlIP0414) 41 16 9 0 0
e
0
rf
fff7fl/Irr
*
#
o
0i op; i 0 0 . . - -
a t k. i~ U 11 w If 4 il 4 " x , 21 12 to Id A A r? IS ?1 13 P U U A 0 a 11 0
l balides on amino Ovilvatives of nicadalt.
a( atk
y
Vs. L 13"'ilfall, Afid M S K-likkovi" ~ l"if ()r$- Ch"'
If
~
R S
J 1-00
--
-
li-l-
,
AcM. Sti. U.SS.R,). C-Pi. re-i. L1-I
. .
I
I
Wh
4.1A-7(IQ4S).-In the formulas bdow
48 ,
'
..
. .....
m
, fach 1, fl,01, I ........ I j,"I AI)P.111. ". -00
cift--cill 1~- 1RCIck 11cil" I lift "id M,i vild a
` .00
It ,% Ouch fiwm, ,' ~tdlldwg.
110" IV* w Vbj, h., K
N.) \ N.%fe -1111ak flint ript,11Y in air. %WhC(41t jo,,-
a , ty'l 11.114 1 Aij~j ~% I ji,c Va w Vb --,Iv
e it
I'hr jit'l -11 j R R (1), and AcC I I,C I i .00
00 (11) Stvv ~ imwh better yi,rld ~l it' .04 1
*0
(lei lei
"
trrnko, C.A. 35. 21191) fit,"' I And It, st'Pluitting the It
-whe product% are Irtrined sit the rearth",
aimitripticin th4t
S 1,
N1, NIF
:
,I a-h.l.warix~tivi tumlxls~ with aininonicutinics, particii- itaf (Vbl a
ally L I to -W, NIVOII sill". is treated with I
; gir
111.4t, Md, th,r null IwatM bir ~wral units , amt lit,O is kmv,.,
hv
*
4,filed it? inve le~ thina ~-10,7c tif a ba- and Aixut 136%*( an 1111-ilft!" k V11 Mid \111 41"! i I Vt. a*
which CVellttlAIIY rry.tAlliltes, In. 1-19 1141' "irthi-I'd u,, !!_,; A J, N,widakmM art,,.
I" h,n hrall-.1 %],,.Iy), after '~' , ryOns. (totil Air 01, tire C .1 35, 111-111) 'j, ~, .-1:4. to )lot-
1.., .1 it, Witlity w nli,ahct and artalyst.4, It I, &"I td 11, 1., u I'a- ., " '), , :~O% ar"I 7:*
or-t-, 11,101 Cff,CIf,CII,-NN1e,j11 O-Mllo X11), "iG of a ha~, 1,, INJ 4 ' tall, r t 11-trm Iiv cr-lit: o, .0 fit
-Alt Willi 11000, 41(11( I'm- 1~ I WN1 Vila i,,4--J
-'I; t,f . . ..... i~ 114' Ill and Art,(). y3firtirs) but c"ut'i I~ Vilb ow Sil, f~ fi;rawif on NAI K 4
h,ti, m -.-. iti, 141.11
qh-tr~l 1,v
rvill) alkah-) Vt wid I, if Kiv, 0)1~ ,[ the 1-~ dffjr
00
rIV). it ..... K-1,- 10. ; IV, (VIII). b, It-,, Vt hir lfl;(h tnatillp"t,
Z's 0
1
111..
101
10
0 U Is T I j 4-A1 41
v 44 ff a list nall It X .0
a 41 M
1 0 0 6 0 0
-11 ~4~ 4 Ul4d
':;I; ,u"41 ~Iv lAd Ju 1,1 4p. 1 lani.,4,1 uo!j.ps,
IAJ 1!111 Alth, aAll j41 1.11
IIA ... . ...
IIU -All HA
I
(qllA) I -11A)
IN 411
'11j
0 0 0 0 0 41 0 0 0 0
0 0_0 0 0-0 0 0 0 Q 10 0 0 0 0 0 0 0 0 0
so
06
0*
00
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0 0 * 0 a a a a 0 0 0 0 0 0
0 TI
M
w 16 11
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1
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, j.
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R.
.% 49, I_
I t P-15); If 1 1 40. "
so
go iri Iv III, h"':'I 1-41" is., 1., -00
III it'. ..... . I. I'f'. I -
go
I it, I i L I ~Jl .11 tl,I~I M It"ild III t Ile It, Old I I !I f,, I so
go !111'. "t !~.I! -;:, !'so
M1 kit" 111.1jiji'l it 1. 1. 1, -so
set floe
13, VIA t, pi't.1 In C, I,
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0
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.
se ... .. .....
go, V,
t h C,
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pj~td it,, ,,I
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IV) ("mi "Ifl. '111f.I1111Y. thr 6
IV
fc,,., a I-c. 11.2161S_ 2 11 ,vri- i;eo
tit, amm,,p%Ti,hile
f"ItIllf IV r..%Cll .1:!l filif 111L1
L A
afTALL49GACAL LITERATURE CLASIIPKAY#Ck ri
110.1 1111,1311.
- . .
.1 - , _-_T_ ____ !i, , .).".
i 19410
C S.".0 W4.3 A, 011,,, cot !.Mll, a. a
L I A 'A 0 9 1 1 If 14 5 it] 0 3 9
u is ity 00 11 Fw A,
Ib
so**
iT, lip
41
0 0 0 0 a 0 0 0 0 00 00 0
II ~It I -]A 1. )9 it 11n A 2. : r X 1, 1; t I, is v
I A L. AI I V v t- A
JL-" I , L a m 1~ L -0 0 'IC UP til A
A ,
00 I c:fbazo tondense4 ysterno ltom ud, 410
d ct th. 4) to
00 it aunintmucolln
*,,,I blunt "Acatulifetic
N , -1 .11 Ill. I l, -I Mid A.-t .41 0
N . 0.4, hh-, A ".1i 194n
".,.I hill,
.
0 .1 37, Amm-mimim, t~l) I ) an.1 2,,) jr 41
A,0114CIIJ. -
11
' IA M A1111W111 tl) 11AIld
2 " !
:
m.11)IIIIII. ill, I aWill, after -hwh
Al I Ile V,(011 1, n ..-I AW T, dll~. tArli up in 11A 1,
r W Ill K h-I .-d I:,
I t h 1:, 1 :0
.
dr, 4
0
qa' it
1111
I A
I i 1.1 d~
,u
,pn to dr
.
y
Ir-un-t ulill K, ill. in,l ~vu, III, ~.t:kj zib 0
'
a I M', p,,,,,.,e. 1:
2111 ift ... n aq
;
Nimit-11 .,I 1 1.% Li'lot'g 11M). 11;~~A 1. ill ill,- c.lid (,0, d 0
,so f to I~ L, I'l.- 11. -1 th'. oll"I lIx"I. C'Adllv AkVr a Ill!,
0
hot ~1, KO t 1:
Gal Kroup p-1ml,1v t, ill the 't-l-tion. C.. M. Koullaj~ff
* U
-Chlaro
-0-methoxy-S-nitirequinoline. lUrry L Yale 00
(Sujuibb lust Im M,d. K,
-,carch. Ntw flmn~wlck. N.J.).
1. A.i. Ch- .\., 70, 1~1,1,-' 191S~ 3A 0,N(ll,N)-
Q.11,0M, 4 it ), S2 it 16AW.. aml 3,N) ml. c-1
110 at lir ~ttb ill
t
-
"
U n It INa U It 11 14 A
4 4
.1,
0 0 to to .0 0 0 40 41 0 0 0 0
I to u W LE
r A 1 0 to
oo-, a it
$10
oil
Ilk I
Oly l
j
00 '
,
io,
fill j -00
,d) "Ift, It,,.I
00 t
to
i I ..... .. ..
*
0
0
M
0
;0
9
9 4
) 4
1
0
*
GOLIDFARB, Ya. L.
"The '-~nseirble' a-rid '~,-r%,ra,~ati(-,n' Princi-iles in CatEL1~sis," - i,~I- :" "r '
- - . , - ~ ;, ('. 2, 1 I.J- .
2L,
1
DePlu. of -~IhysiceLL Chem., Lab. of C.;talysis and !.-Ilectrcclie~,.istry of Gases.. ll.'~sccw Stat~-- U.
0 6 a * 0 0 0 0 a * 0 #-w-oci-
10 M " 0 *OID (I Goa 4 0041
00 0 00 000 0 9 0 * 0 0
4
q 4) 41 0 0 0a09 0
Ia 1 4 1 11 1 It 1. It 11 u 11 111 14 t o J. to 9 it z if Ll 9 It a III vw10 4 at Q ii 4. a ce
L0 1 u A 5 1 Lot v If 'I Ir I m ON IV 11 j It III
rA I", r'. to , ,
_& 0 41,
-11 -1. 1
Amfn',) derivall- it I pirridyl) 1
1 buladlotio, I
.
-14 "old d"Id
Y, 11, 1.4, L."t 11'. v. 1. 11.1"1 ... 1-1, , I.J.
40 1. 1~* 1pr-', I--- I I..) I, I I, -
IWII~Ill .. I
I
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L,I
)
1
:
11"I k
a Co. auld .
"
'
,
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1
0
Imt III, ;,l,
Ll ")
,1 14 1", I- 4
00 It C1 I i w'.t I I.!; "ofl f......
I ICHOI 111, 1,. l-,l ; 11'. 'l-ol I, II .'
00 J( vId'I' Im '.it, , Il' A .. I, I"'NI, Ali 41
Go a th,s uk-I O"dial'N tut, vA.",
76 1 "t a Ivav'11'r 4 11 'll"i (O'Lllwd %V!wl' I 'I I
so
11 "- in Ilit.g.
CS, .0.-
'
ClIk
.4 1 1-1-- of 11. 1, 1 1.,
. ...... . ..... 41, 1 1'. , "'0. ,
00 a Aipl it S Ilk I w -20
41)
"I", h "T"'o .:"I H.'S f-n'd I A-p It.
t~' g"'. Nl.,N Ind I~l
"I't A .... .I 'It I ".K ""I.] fi"':' 4
eloj"' ze It
,
ho-I 1,, 1,, AV, IV lot i ". 14" 4'L*"!) " I " I '( I
rvapc too . I,
'. '111-1
41 .ht'mlrd m _,I m vidd I-- I", K I!IYI I"",
C..4. 15, '1 Voi). lot) it. 1"~' 1; 111'
~
c*
at 105 Atilt.. b. 1"0-0)"
N IV) EMIL ind ..Oi-l ilh Vill)", it., '0", "t V 41
* f bad h,~A~ I I'L h,,. Ati-pl. V 1%, a* 41
9 -111 14 111 .1111 .%A,4 1 .111 A ItIA111 kith. IV 1-1% it" it" I1 1; "'Ily "', I---
~o
A, n
'tAlodmx III,, _',i - IV) '4 IV.
III-I M Ise 'j V. 41DO
.A. "bum'd. .6'.14 '1 1-1 1 lit . 1"I'. -I IjIjL'
1
e
:
w
, 1'~" _' I., %%
isio If Poriolwation of crclic thiosmideri. I V-h-ka IN- 0
Ich in'tiltite I)( flic lim., /60. k "'U., -
Ch
C
'%
"
S~
to,
oi$ob It I IIIIA-110C.1, 'III t3
41 1 0 It A) 1 4
Du 11 10 11 to
~
a It n q K n rt it ot 6UD n
1) 0 0
T 17
V L
i n t
of
and,.-Ya. L Dan 1% ~ ,
Opp- &37
Ahson. (J. Lien. IkAlem.1 I R-31 048 ... ~~jpft~, - ior dts. 1 i
trum of I-inethyl-2-Midon C (1) In a.kbows. U-40
R; at raft%. Lit 3400 and at M A.. am V
mg.11.), soln In EtOH ' t In (OiDlIp 31 1 VVU; 0,
he inax. are shifted to and th 1111di Va. ! L~ Gt
.; the 0
deviation from Eleer's Ill
's Ill In a1c. b not cleitr.' In speliOn of jhd follij
.In. in EtOH. 2
-arnhiopyr1dint (11) thiml a hand
with ninx. -it .00,10 A., log E - 3.6, I.e. the fWntoland as uble~ ~injr td"
In CIII,q (1;piersand Wibaut, C.A.31,52726 ;~ jdj
C411A the band is shifted to longer wam 41. Ott
.
A
The khift is not to be attributed t6 Uubvititii6i;~ bit. (I 2M 0-8);
cause a-dinicthyLiminopyridine (W), which, to itiot cap. 1-0 tb I 240ina
'able of tnutomerism, shows, In sk. goln., a further shift In ~ I
to inax. 31200 A., log E 3.8. the spectitum dmwbqW clam
q
kIo that of 1. The shifts are hitierpreted by all Illcreatted
wt, of Volair structures in the Ist kxcited state ont, Vitt a
U,
result al which the double-band character nt C:R la,.M. t~.24n"-I,$4hOr
00 hattred. this effect b increased by sub-titution art jhie aktillhe withiodid
Wall
NN- gruup with Met. Substitution with the !electtti. Met I III
de X~11
i~ nophilic groups Ph or Ae. give-s rise to a shift in ithe op-
1-2
q positeditect-lon, 2-diplietiyl,,tntitiol-)-ri(line(IV I WeLMAX. Ca te
V (iv am
i Lit 2.170 A., log E 3.4, and 2-acetatuidopynd rr (V) - flal
: iy tod 0, 'Pat]
Pl;~ Max. 2470 A. log E 3.8, tit
dit ?j dqW
Wide (Vi), in whiell the N atom of the NOI10i #OSIP iaritli!~(Xv
laethl
cannot patticipAte In resonance with the Ting, tht-je atj 3 t1vt to nicatime ati
close inax. at 2600, 1-1;M, and 2,M A.j log B 33, 333, "-dines telativi to
and 3.65, M~P,, i.c.005'! to the spectrum of C41(5N (ritin. am &tit. by re3on
Ttl!l at 2520 A.), as exty-vted, lit 1.111
tte NIr,
groa is free to take p1trt in ruollarwz with tltc Anx. the
- P
CIO
1K,
ss; xy I -a I `7~
~$t tv W. 1k or - it ~t -K St It. V. 2t '11 -M
66-~iWjis~
e
j(Utk4j jt~ hit rlalt Ij j V&
qlj~jj Off! C
I W Ot
al,
kit
141 1
do
t
-57. 511
q .4. A.-V
T-
L,;t
in uitravioLet )f ctuo
10
Dct'dwl" CU. nyx..
ba-
;I
-A.'x
s Ll'i-,- ol"
of i d ln-,nlmnico~
jail
Action of alkyl baLides on - and amitionicotines
V, 1. C. K."A 'k,'- I..'t I ",i C I-u
1!Tv'I ,,,'!, k,, ~ .~ H . I lid, t it, w.,
1049. 101, 47 M,I 12 ', g ) ,,,I U, K -,, -
ni-lin, m 21) itil fl,, 0.,11,11119 1 fit i! I,-
fluxing mm. K;Av, In. 14111 NI fw:"
Ftolf). v.mIX 1) !t If;( ). -th Ih, XIvI it the 1)vrrf,l,- N
Mom. a, it t' w"+.- Kv, I!- mw'! X..I I i ; it i I IC I ~I! I, m,
I -''j - ~ ) , . P.-Ition "f Mirl -11, 1 -'Ill it 1.4.
I-vd by vir"t I"'.1ki't 'Itth 11'a
171 In I-.,t fr~ I
th,"Im-ftlit, "t.0 "" I im,n I "I.w I,-- bv
-0-imi.m. - 1 1,, , wit (,~nn , c;,rhimat,. I IICI wh
M, I g imikir I, ull
aivi r0lu-i :1 hir., I.".
g '22; 7' f-m N1,0111, , wjig _%I~ I
I'VI-1, it r, i:, I!- fit, 't "Imic
'ith A. I. I '( I to I I., t It, 11i"t h~ , 1.~ ......
f...... t I., . I . " , , it , I I ". . 1'~ II. I- - .-1 1" 1k.,!,.
.'( ,,, fli'l p-h~ t'. I, I ; ~ ~'; . f'.."t
s-1 , t, d 12 K 1., 1 2 1, ,111,, 1
1-1:0 m.d th. tv"ts-i ';-1
It"r ALA' -mId- ':",t1
h."'I hp 11 .1 it,
%1~ I it Ow I'v".1mv N. in 171
Vl,'. of 11 A wiLm,,ii trit, ttiti. vid t
11TIN-0.11.11-11' Of 11. M '2 , 11 If\ Ot, ire iltn~t in
'01., t,~J h, NJ,-: . 0 1 4 2. :,',1 N I K, -A., poll
1.
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