SCIENTIFIC ABSTRACT ZELDOVICH, V.I. - ZELDOVICH, YA.B.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001964220011-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 15, 2001
• Sequence Number: 11
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

ACC NR- AP7002739
deviation from this ratio is termed a dilatometric anomaly (ZeYdovich, V. L, Sorokin, 1. P.
FALM, 1966, 21, 223). The difference between the dilatometric effect of the transformation of
textured (deformed) alloy versus that of a statistically isotropic (nondeformed) alloy re e-
pr
sents the measure of the dilatometric anomaly, on taking into account the amount of the trans-
forming phase. I n this connection, on the basis of an analysis of dilatometric anomalies and i
changes in texture due to a-y transformation, as well as on the basis of the change in trans-
formation temperature owing to prior plastic deformation (92% reduction in area), the nature
of a- y transformation during continuous heating is discussed with respect to N23, N28, N32
and N27T2 ferronickel alloys and G7 and G14 ferromanganese alloys. The temperatures at the
beginning and and of We transformation were taken as the temperatures at which the dilatome-
tric curve began to markedly deviate from its rectilinear couse. The dilatometric curves were
plotted with the aid of a differential optical dilatometer, and the phase composition was deter-
mined by the magnetometric method. Findings: in ferronickel alloys with 0. low Ni content --
N12 (12. 0% NI), N15 (15. 1% Ni), N23 (23. 17o Ni) -- the decisive role in transformation is played
by diffusion processes (the austenite texture becomes dispersed to a much greater extent),
whereas in the alloys with a higher Ni content the martensitic mechanism Is largely respon-
Sible for this transformation. The addition of Ti (1. 9%) to the alloy with 27% Ni (N27T2) inhibits
the recrystailization of asutenite and the development of disordered diffusion processes during
transformation. This may be a -definite factor in enhancing the strength of Fe-Ni-Ti alloys
Card 2/3

ACC NR. AP7002739
owing to phase strain hardening compared With Fe-blli alloys. In ferromanganese alloys the
I initial temperature of ce-y transformation markedly decreases izader the influence of deform-
h ation, which points to a diffusion mechanism of cf-y transformation in these alloys during
their continuous heating. Orig. art. has; 2 tables, 2 figures.
SUB CODE: 13, 20/ SUBMT DATE: 20Apr66/ ORIG REF-. OOV OTH REF, 002
Card 3/3

- ------------------------
ACCESSION NRs AR4027681 3/0276/64/000/ool/GO08/GO08
SOURCE: RZh. Tokhnologiya mashinostroyonip, Aba, IG60
AUTHORs Golldshtoyn Yat Yoe; Zoltdovich. Vo 1.1 Shmatkop Ke Se
TITLEs Foculiaz~ities of,the effoot of ra" iarth F'etals on the struoture am
properties of,structural stools
CIM SOURCE: Sb4, Teoriya ipraktika motanurgli. Vy*p. 5i Chelyabinsk,
196.3s' 12-3-131:
TOPIC TAGS: rare earth metal,, structural stool, stool motallurgyq rare metal
admixture, rare metal anoy
TRANSLATION:' The authors havo ostablished the possibility of immudzing'stool,
from flake formation by increased additions of RM (rare earoh metals). Such
treatment simultaneously increases the resistance to brittleness and hardenability
oll' the stool. The-mechanism of long-term effects of REK additions is associated
with the high absorptive ability, of cerium with respect to hydrogen. and possibly
with the fomation of stable cerium hydridos. The introduction of 0.23% IRM
Card

ACCES'SION NR: AR027681
steel leads to the redistribution.of sulfied in microvolumes of steolg as a
result of which the high-melting corium sulfides are looalized in the dendrite,
axos.and not in the intoraxial spaces. The concomitant fragmentation of the
dendrito crystallization is explained by the modification effect' as well as the
purification of the melt of hydrogen, sulfur, and other admixtures. 'Tho maximum
dogroo of disorganization of the dondritio crystallization is noted upon the
introduction of increased portions of REM (0.0)o The purification of stools
likewise prcmotoo the removal of spot inhomogeneities. An important
characteristic of steel,treated with FM is the increased isotropism of its,
mechanical properties (yield point)* The best results (the minimum anisotropy
factor) are-achieved upon the introduction of 0.25% forrocerium. It was found
that the optimal amount of REM additions depends on the thermal processing
regime and the purpose of the steel; in the state Zollowing annealing and high-
temperature tempering, ari addition of 0.1% is optimal; in the state of low-
temperature tempering it is 0~23% REK* The introduction of increased amounts
of REM on the order of 0,.4-0.6% for the elimination of flaking sensitivity Of
'steel is permitted and is recommended only for alloyed stools to be annealed
and quenched to low and medium temperatures* Such a dependence of the optimal
R34 -addition an the oomUtions of -subsequent thermal treatment is associated
t. C.-rd 2/3

ACCESSION AR4027681
-with the variable solubility of ceriumi - In d%-Fe Studies have confirmod the
theoretioLl possibility of active extra-furnace dasulfuration of steel throu
gh
the addition of TIM. The introduction of 0.6% forrocerium loads to a drop in
thosulfur content ( in tho main ingot body) by a factor of 4.5. A disadvantage
of the treatment of steel with rare-earth elements with the usual technology of
their introddotion and deoxidation of steel is tho;incomplete evacuation ofthe
treatment products into,the slag.and the head motii of the ingot. The succassAa
solution of the problo~t of the completeness of flotation of these products will
essentially doteraina the rates of introduation ofREK into structural steel
production.
!DATE ACQ:03W 64 SUB CODEs ML WMI, 00
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AP6023699 CODE: UR/0126/66/021/W4/0541/0545
AUTHORS: Zelldovichl V. Lj Sadova*, V. ID
ORGi Institute oi' Physics, AN SSSR
Ins titut fiziki A11 SSSR)
TITLE: Vemperature'dependence of the magnotic'propertioa of iron-nickel alloys
S,
OURCE: Fizika ze~allov--j me'talloveideniye, v. 21, no. 1966
541-545
TOPIC TAGS: iron 9-1loy.. nickel alloy,, magnetic metal,, magnetization, magnetization'.
curve
ABSTRACT: The temperature dependence of the magnetic saturation., magnetization, and
..coercivity of iron-nickel alloys containing 27.9% Ni and 27,0% Ni plus 1,9% Ti resp99-
-tively was studied, The study supplements the results of V. I. Zelldovich and V. Dj
Sadovskiy (FM 3.965p 20 416). The experimental procedure followod In dencribod in
t-,,-tho reference above, and the experimental results are nun
wrizod in graphs and tabloo
(see Fig. 1). It was found thato, an a result of annealing, the auBtonito phaco be-'
4,-- comes enriched with nickel to the extent that the specimen acquires forromagnotic
properties at 200. It is conclud d that the chief difference in the*
.0 coorcivity of
Ve-Ni and Fe-Mn alloys Is due to the ferromagnetism of the austenito component of the.
foriner,
Card 1/2 UDOj 669.15:538*24

A116023699
0602-3~99

Figs': 1, The dependenco of the magnotization moo
(1) and coerciv#y (2) of an iron-w'

niokel allcq on' the annealing "D
.0
.temperature@;
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rig. art, hass 1 table an4 6 graphs.

Tm COMs 32/ 11RUBM D= i O&Tun65/ ORM, REP t 009/~ OTH REFs' 003

CHROMIUNI-INICKEL STEEL WITH CERIUM (TJSSR)
Y,~ V I Z--`ij 1. Koniis!;arov, and Yo, I-
J
no. 4, Apr 1,963, 354-358
S/133/63/0001004/007101
effects of the addition of ferrocerium containing 947/o rare- earth metals
on the mechanical properties of 4OXH (0. 37,16 C, 1. 03% Ni, 0. 57% Cr) s-ee'L
we-Te 7a* ea a* the Chel-,,-,abi-sk Scientific Research Ins-litute of Metal-
"-e Che--yab-nsk Nletallurcrical Plant. The hardenability of steel
iurgy an-`- A. C,
increased only with the addition of 0. 06 Fe-Ce (smaller additions did not
iffect th~-, hardenability). Fe-Ce has little or no effect on austenite grain
size or the rate of grain growth at high temperature. The addition of O~ 10
and 0. 255o Fe-Ce had a positive effect on notch Loughness. With low-tempera-
ture tempering a ma-.,nmum notch toughness of 5 kgm/cm2 was obtained in
Card 1/2

FAY
CHROMdUM-NIC=- LS-ZEIM [Contl(j] S/133/631000/004/oo7/o-u
-'st'661-With 0, 2517o Fe-Ce; with high- temperature tempering a maximum of
22 kgm/crn2 was obtained in steel with 0. 1% Fe-Ce, Fe-Ce lowered the sus-
ceptibility of 40XH steel to temper br-ttleness. An addition of 0. 2510 Fe-Ce
reduced the anisotropy of mechanical properties, 0. 10% Fe-Ce had no effect,
and 0. 6% Fe- Ce ;Increased the anisotropy. The addition of 0. 6116 Fe-Ce lowered
e
the temperature of transition to brittle behavior by 30 to 40*C, which can b
attributed to the purifying and refining effect of Fe-Ce. [WW
Card 2/2

V/(')
AUTHORS:
TITLE:
82642
B/126/60/010/02/012/020
E021/E335
Gavranek, V. Bol'shutkin, D.N. and Zeltdovich, V.I.
Thermal and Mechanical Action of a Ca;Tt__ntion.Zone
on the Surface of a Metal
i metallovedeniye, 1960, Vol. 10,
PERIODICAL: Fizika metallov
No. 21 pp 262 - 268
TEXT: The present work is an attempt to examine the change in
temporature and pressure impulses arising in the surface layers
of a solid in the onvitation zono. A magnetostriction vibrator
was used in the experiments with a constant amplitudo of 0.06 ium
and a frequency of 7.5 kc/s. Phase changes in a quenched U7
steel and DI duralumin were investigated in the cavitation zone
by microhardness and X-ray investigations. Fig. 2 shoifs the
relation of microhardness with time of cavitation erosion.
Fig. 2a is for the steel and 2b for dural%~min. The changes in
hardness show that the temperature of micro-volumes during
cavitation erosion reaches 470 OC. Fig- 3 shows the effect of
.a_preliminary tempering treatment at various temperatures on
ht..rdness (Curve 2) and rate oftrosion (Curve 1). The rate of
erosion is practically-unchanged by preliminary heat treatments
Card 1/3

82642
S/126/60/010/02/012/020
E021/E335
Thermal and Mechanical Action of a Cavitation Zone on the
Surface of, a Metal
up to 400 OC. This shows that the damage occurs on micro-
volumes of metal, the temperature of which is up to 400 0C.
X-ray investigations show that the internal stresses arising
in the steel in the process of quenching are removed by
cavitation eroslon. Similar results were obtained for duralumin.
During the experiments, the duralumin became artificially aged,
showing that high temperatures are reached during cavitation
erosion.
The obtained results can be summarised thus:
1) the mechanical and the thermal effects in the cavitation
zone produced by the magnetobtrictionavibrator were calculated.
It was found that in the-dase of using/7-5 k2ls vibrator, the
pressure increases periodically to 550 kg/cm during a period
-5 5 2
of about 10 see and acts on an area of about 10- mm The
micro-volumesof the metal bordering on the cavitation bubble
are heated to 300 - 500 'C-
2) It was established that during the process of cavitation
erosion, hardened steel is being tempered at temperatures up
Card V3

82642
S/126/60/010/02/012/020
E021/E335
Thermal and Mechanical Action of a Cavitation Zone on the
Surface of a Metal
to 470 OC.
3) The speed3of cavitation erosion of steel hardoned to obtabi
a martensitic structure and of atool tompored at temperatures
below 400 OC are practically equal.
There are 4 figures and 10 Soviet references.
ASSOCIATION: Kharlkovskiy politelchnichaskiy institut im.
V.I. Lenina (Khar4kov Polytechnical Institute
im. V.I. Lenin
SUBMITTED: June 26, 1959, originally,
February 17, 1960, after revision.
Card 3/3

34M
B/I 331662100010031C,0410081
A054/A127
AUTHORS: Golldshteyn, Ya. Ye., Candidate of Technical Sciences, Zelldovich,
VA-I.'s Keys, N. V., Kossovskiy, L. D., Vaynshteyn, 0. Ya., Shmattko,
K. S., Engineers
TITLE: Theeffect of treating liquid chrome-nickel steel with cerium on its
crystallization
PERIODICAL: Stall, no. 3, 1962, 258 - 261
TM; Tests were carried out to study tho effect of adding ferrocerium to
chro.-ie-nickel.structural,steel on the flake formationland crystallization. The
tests were based on the chemical affinity of cerium to hydrogen, whi:!h increases
when the temperature is raised. As rare-earth metals mostly tend to adsorb hydro-
gen in the 200 - 6000C range, where the hydrogen separation from the metal is par-
ticularly intensive, this phenomenon can be used to reduce flaking. Four 40'.,L-~
(40KhN) steel ingots of the same melt were tested: one, checking specimen, with-
out ferrocerium.. the others containing 0.1, 0.25 and 0.6p,7" ferrocerium, respective-
ly. Lumps of ferrocerium, containing 94% rare-earth metal (primarily cerium)
were used. The ingots were top-cast and weighed 2-65 ton. Lateral macrotemplates,
Card 1/'~

The effect of treating...
S/133/62/000/003/0011/008
A054/A127
cut from blooms rolled fro m the test ingots, (air-dried after rolling, non-anneal-4
were analyzed after 1 and 6 months. Flakes were hot found in templates from steel-
to which at lea!A 0.6,5 ferrocerium was added. The analysis also showed that the
effect of cerium (lanthanum, etc.) actually does not manifest itself in the ad-
sorption of hydrogen, but rather in boSding it in the form of stable hydrides.
In steel, containing as much as 3.7 cm hydrogen/100 g, there was no flaking, due'
to the addition of 0.6,,ro' ferrocerium, while flakes were found in steel containing
not more than 0 56 em3/100 L., drogen, if not treated with cerium. When ferro
hi
cerium is added to the liquid steel in amounts above 0.25%, the pattern of den-
dritic crystallization changes and sulfur will be re-distributed in the micro-
areas of the metal. High-smelting cerium-sulfides pass from the interaxial areas
into the dendritic a;-es. When ferrocerium .is added in amounts of up to 0.6%,
dendritic crystallization disappears, and, under the effect of cerium, the steel
is cleaned from sulfur, antimony, stannum, bismuth, lead, etc. 0.6% ferrocerium
reduces the sulfur-content of the metal 5 times. However, when ferrocerium is
added in the ingot mald., the cerium-sulfides (=j-sulfides) cannot entirely be
removed into the slag and the feeding head. This results in a nonhomogencity of
the boundary zone. The high-temiperature cerium-sulfides (oxy-sulfides of in-
tricate composition).are forming already in the period prior to crystallization
Card :2/3

S/133/62/000/003/004/0c"
The effect of treating... A054/A127
and are moved to the inGot surface during the casting. The liquation in the
Doundary zone can be prevented by smooth, rather slow filling of the ingot mold
fro.m the bottom and by an Increase of the head temperature. Cerium containinrr
steel t-:Ith a liquation in the boundary zono shows a tendency to red shortness.
This exi be reduced by adding ferrocerium in the ladle instead of in the ingot
mold, or by roughing the ingot before rolling. The addition of forrocerium in
amounts of at least 0.25%' prevents spotty liquation, because a greater part of
sulfur is bonded in the form of cerium-sulfides with a high melting point. There
are 5 figures and 9 references: 8 Soviet-bloc and 1 non-Soviet-bloc. The ref-
erence to the English-language publication reads as follows: Russel, Journal of
Metals, no. 4, 1954, 438 - 442.
ASSOCIATION: Chelyabinskiy nauchno-issledovatellzl-iyinstitut metallurgii
(Chelyabinsk Scientific Research Institute of Metallurgy) and
Chelyabinskiy metallurgicheskty zavod (Chelyabinsk Metallurgical
Plant
Card 3/3-

ZBODOVICHI V.1.1 SADOVSXIY, V.D,
V~~, ~, ~~-
Effect of beat treatment on tho inagnetia proportion rl Q,)PtAln
Oloyn In tho nyutAmn Fo - Mh sAnd Fj - R. y1s, met* I
metalloved. 20 no.3.-406--411 S 165.
(MIRA 18:11)
I, Tnstitut fiziki metallov JUT SSSR.

ABDULIN, A.; ALEKSEYEV, I.; BANTLE, 0.; BOBROV, L.; BOZHANOV, B.;
BOyKOt V.;, BONDAREV, K.- BORZOV, V.; VERKHOVSKIY, N.; GUBAREV, V.;
.0
GUSHCHEV,.S.,- DEBABOVP V.; DIKS, R.1 DMITRIYEV, A.; ZHIGAREV, A.;
ZELIDOVICH. Ya.; ZUBKOV, B.; IRININ, A.; IORDANSKIY, A.;
ItAlmA6i5gKlYp P.; KLY'UYEV, Ye.: KLYACHKO, V.; KOVALEVSKIY, V.;
KNORRE) Ye.; KONSTANTINOVSKIY, M.; LOIN, V.; LITVIN-SEDOY, M.;
HALEVANCHIK, B.; MANICHEV, G.; MEDVEDEV, Yu.; MELINIKOV, I.;
MUSLIN Ye.; NATARIUS Ya.; NEYFAKH, A.; NIKOLAYEV, G.1 NOVOMEYSKIYp A.;
OLISHANSKIY, N.; OSIMINp S.; PODOLINYY, R.; RAKHMANOV, N.; REPIN. L.;
RFSHETOV, Yu.; RYBCHINSKIY, Yu.; SVOREN', R.; SIFOROV, V.; SOKOLISKIY, A.;
SPITSYN,l V.; TEREKHOV, V.; TEPLOV, L.; KHARIKOVSKIY, A.; CHERNYAYEV, I.;
SHAROLI, L.; SHIRANOV, A.; SHIBNEV, V.; SHUKIN, N.1 SHCHUKIN, 0.;
ELISHANSKIY, I.; YURIYEV, A.; IVAHOV, N.; LIVANOV, A.; FEDCHENKO, V.;
DANIN, D., red.
(Eureka] Evrika. Moskva, Molodaia gvardiia, 1964. 278 p.
(MULA 18: 3)

~WUKUri WUNt
AMOR: Zeltdovich, To, Bo; Okunt, Lo 9.1 PUml hier 3 B
ORGi none
TITIE t Quarks t Astropf*mical mid pbysical-chemical dopc to
SOURM :Uspoktd fjzjoh4skjkhh&ukj' v
9 S?t not 1,, 1965s U3.124
MPIG TAGS S hueldoh cosmic ray
wson
baryon, mass spectroscopy
Vd.r ous7appio for now stable p
AIPMOT: achei~to.tfia- see'rah arti
oleo are !,reviewed s,. namely, throb assumed: quarkal having charges
-W3891-4/38,* asid'!11/301*20 ad well as others having Integral
~-oharges. The 11ehtest fraotional-charge quark to supposed to be
stable In vacuum as well an In contact with ordInary matter
,(nuclei$ electrons), ConditIons are given under which Integral-
'charge particles can be stable. Various possible sources of quarks.
are reviewed, the most powerful being cosmic rays from superstars
or quasistars. The annihilation of quarks Is then discussed In
detail. Since quarks a" heavier than nucleons, the process
,q1 + q, -9 q3 + q-1 Is possilgle # followed by q, + q_1 -.v nqo (vhere
ithe subscript Indicates the number oC quarks and the minus sign
1ndioates an antipartioles) q3 Is thits an ordinary baryon of threej
'quarkag and qO Is a meson* QUarke are therefore annIhIlated via:-,*-,,
.~6_ - I Mr rx __ - .I . - 0)

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~~t h6282-66 aq (m)/ZW'P (w) /T/-w,P (t)/ETI M(O ;D/Mi
;~~CC NRI AP5025326 -SOURCE CODE: UR/0126/65/020/003/0406/0411
~.;~AUTHOR: Zelldovich, V. I.; Sadovskly, V. Do
ORG: Institute of Physics of Metals, 6rN SSSR (Institut RAM metW-lov AN SSSR)
'V
TITLE: The effect of heat treatment on. the magnetic prok)ertle Is of some Fe-Ma and Fe-N1
alloys
SOURCE: Fizika metallov i metallovedenlye, v. 20, no. 3, 1965, 4063-411
TOPIC TAGS: ferrous alloy, nickel containing alloy, manganese containing alloy,
metal phase system, phase transition )9'VX"-/9t./'Va InAq;,Vc -ri(1. SAr0R41-.,0A1
ABSTRACT: The effect of annealing temperatures on the mB gaetic satura tion intensity and
coercive force of tempered and stressed ferrous UIIOYB waB studied. The samples, containing
0.5-10.6wt% Yin, 0.1-31.8wt% N1, and 0.05wi% C and 0.15-0.35 wt% Si, were tempered
30 min at 1180C, quenched in water, and annealed at temperatures toj120C in a salt bath.
During annealing at temperatures corresponding to cL-*y transitionsla high dispersion of
magnetic martensite and nonmagnetic austenite Is formed. Ma,,', etic saturation Intensity
reaches a minimum. and the coercive force a maximum, due to the appearance of an ATn- or
an Ni-enriched austenite phase which Is stable to a-t transitions close to room temperature.
tMCi 539,202:536:538

L 46282-66
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Deformation of the tempered Fe-N1 samph, '.,y rolling at room temperiLture prior to annealing
DO
caused a sharper decrease and increase of ..japetic saturation and coercive force, respective-,
1y, during annealing at temperatures of co-Y transition. For the alloy of 3 1. 8 wt% Ni content,
a decrease of magnetic saturation intensity but no essential Increase of the coercive force was
observed at a-)~y transition temperatures; a peak of the latter parameter appeared at 250C
and on approach to the Curie point of the ferromagnetic auBtenite phase of this alloy. Orig.
art. has: 5 figures and 1 table.
SUB CODE:I/,O/ SUBM DATE: 18Jan65 ORIG REF: 006/ OTH REF: 001
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mogirmkif wo Va. ?W*rtkh. Atid
rhytkarkin. U. P.S.S~ 1,
=tk invtatigation od the adsorption oFC0, Oo and
catalytic MnOt wal Made by MrAtts of a AlWe
ipp. whivit allowed the study of the isotherms over a le
nessure range (10-10W trun. fig) p ad the 60bux AM also
he adsorption kinetics of gaset at comt. prcszwr. The -so
emp. change of the MnCh powder an adsorptim was -00
howetically calcd. and mesAwred by me&= of a thermo-
-00
vu te. The adsorption of CO and Ot wra found to be
ME mal, mW active. The Isotherm d mol, adsorption NO*
ollowrd FrituMfich's rute (or km Pfessuis dad [Ang-
nWr's rule for medium and high press". The heats of zoo
not. adsorption of various cases on MnO~ were found to coo
oe . (h 23W. CO 26W, COs 55M, N, 34W, HYO 12,M).
~Jl~ 12,000 W./mol. The ratios of heats of mol. ad- coo
=.,V-d with Lnndon's theory. The delayed es-
of
for mul. advxptlon was traced
a heating of th:iU.It.4yot let first and to the slownr" of
as islion throughout the ratelpt, 11w heats of
CtI=of 01 and CO on the catalyst were found to be
MW and 73W W., rT. The activg adsorption of
4 spiwared to be a In the WO, lattice. The
ctive adsmptiorl of the CO (heat of adwptkm 40,(M-
''so
5.000 W.) appeared due to an irrevmible chtm. tt-
ction with the 0j of the lattice surface by which the tie*
1116 10
mely bound C(h was formed. The abs. speed of ad-
Wptjou JULboth Cases Was Smaller than
that elided. an 0 a
MP[q mal. kinctle considerations. It. H. Rowley
400
9-1 1 tie W
-4x,
.1 W IM
a. . . . i z I J;ilo
U Ct (I it a[ n 1 114
00 0 10 o 0 0
OOoOo6O::: 0000000 0*0090,1,
0000900
q W 00000:::00e0000;

j t i f 4 11 it 11 It
A 11-IL
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46
00
lee st
so A
it
C:1 Z
Y f:
:V
LIATIOAT
0- 49 4 4 0 0 * 0 0 0 , o * 0 -00-,
-
I to V 4 It a W
U is mt) Fill oil,
F 4NO, of it $I
Y
LA T. 1 -1)
00

the -gch..i at t!jis catabtia oiddadm Fd Carbon
monoxide. It. S. Roginak-if and ye. 7e - rkb, Add
Or
l, G"man);
Phyicodin. U. R. S. S. 1, WS am
cf. preceding abstr-Atlaxption messurentents Indicated
that there was notinie lag hetweta tbeartiveadsorption of
O
..
CO and the reaction: CO + SlaO, - CO~ + NIn
The speed of ibe CO adsorption with coast. autts. of C(h
at the surface Is proportional to the amt. of accessible
In the sturface. The speed of OF reCeneratiott by OlidAtiOn
of the reduced Ma0i, Is much slower than the speed with
which the 0. is uq"I in the catalys6. It. H. Rowlev

=00
zo 0

oill

.00
fro 0

,4-11 A 5 4 . t L AMETSWIRGICAL
It CL.11WICATION
S
t1l;NJI..
,~T
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U a AT PO As AA K
-! j;qp
IF
tv rf IF to 4( Or an
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AM 'FAY:kKMm. ot X S. J. 1. W74
&so
ft
.00
am, *qwlm 9 W
.so dC
09
SUM t by a Prw" Z;mm of poicits .00
to. be" ad admPticao tba FmOM& imothum
*00
so It. Raishmoltift
2doe
Soo doe
00 '3
0 it
has
J:7
4160011.4 "TAkk~"KA& killoAlly"'A 6116FICATION off-
too
I iiio-or/ .4 OAV o" 441 M POO
IS AT so, at 04 0 14 a I N a a u a ~l
to It It It It 14
is 000 00060 66-00
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a
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o
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P
t
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n
do h and V. S. ft
. Zcl
. _j* Mn, J.
-8 41 R ) 4 1*0(1934),- -
rhfmw
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-pirls? n Alai %ties life
' iiW
P. H. Rialitnamn

00

400 ts

of
eat 0
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of 0
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9

L
if. A OETALLUNCKAL LITINATURI CLAI$WPCATION 0
plant sivisslytt 114.1 00.01
:m t
111041 MAP

r--v
)NV dal
*'a

f a a It K K a AM A s 1 00 0 9 1 w 14 1 oll 0 1
" i ' 0, A u
R a K a a it w
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0 0 0 0 0

at 0
0
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Owl Isis$ to IS tj 11 " 0 It u n &30-- all U831416 bux
v x v
YI. -144: 11 - I
CA 00
of.
004,
006 00
004 Actin a Vat. J. Pbys. "90
Ck 0. 92Q(123lT:=-Acti-tcd ad- -00
10; vrith the wb* Crow tot-
008 cbctgl, read
as& ., mid it owtilut" the Wad Ww"a 414- .00
It. pathmam
SMP
00 a =00
0 3 as 0
000 see
0ou
7. coo
Oo croo
SO
Af i-4
coo
600'
I ZOO
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15 t:00
tie 0
U00
_~~GKAL UUMAT CLA$11FICATIC14
to". 51--fill. I low 40.07 NO*
SIX&JUNt 411111 (W ON-L'sk
u ImAloo III,, 1 0 1 S. A 1 9 ew a 0 a I If if I A a 3 t I
a it at 0 9
0 a 0 0 010 & 0 0 0 0 0 0 0 0 0 0 ~ 0 0 0 0 0
0
AILM 0 0 0 0 * a 0 0 0 0 0 0 000000*000000 0 01

-lit
-Thowy,of the PcoundUch s4sarpUM ig*tksrm
J.. ZzLtpdvrnm (AqfW Phydoochim U.Rss., 1936,
60 a Inunmudw of
es f devistimw fnm-thg *0*
the condi.
a US w0 *
00
r*
I
goo
A
Aid-ILA MULLINIGICAL LiTfuTual CLASINFICATION cro
Mamo Mse 4xv cot VIL131 616 Ofty III
low
4 q F
U :~A"Onj; R' pop ;n
0 a 0.0M 0 0 a 's 's 0 0 0 0 0
0 0 0 0 * 0 * 0 * 0 0 0

6 0 0 0
4 1 4 It 1; It 14 1$116 11 It it 11 fli-d' It, 1XII V11 14111 bit Milo of 041 6646,46
A 4 A 1-1-4- J, AL-k- I-J,-AA_ 1G.", W (I A
ctI Is "41 11colif fit I,
ov
theory of Lateractim of atom mad weltall. Va. B.
2 1 ick. A Fxpd. Morar. P,4ys. (U. 8. S. R.) S.
(1035).-The latemaian of the atom with IT" clec-
s of the metal is found to the 2nd
proximation of
00 perturbation theory. The tbtra ad intirmtion, is
in ersely proportiottal to the square of the distaom train
Eh surface of the metal. F. H.. Rathmann -00
J
of a 06
no 0
00 000
o0 coo
60
00 x
1400
tee0
o
t
ASK-$LA 61TALLUKKAL LITERATURE A111MADGM
1 -1 -All I I I Oj 0 0 v I W 04 1 it
it
tv lei lit to It Do it OR it It OF 111 1. an 1 4114
0 0 9010 000*0000 00 00 0 01 9 0 0 o 0 * 0 6 0 e 0 0
* 0 0 *1* 11111 0 0 111 * * 00 0 4111 00 0 11111: 0 0 0 0 00 0 009 0000 61

m Is m u a a 6 41 a -.1 -.imli
T~. *1 A,* a a' M U A,o 0
oo
4 .00
UmftlM law of bvdjr awatidbig convection cufft-3cm.
-Vm.-B.ZWdLT"-, - J. Expit. I'Awaffl- PhYl. (U. H. H. Rj
7, 14IM-6. 146"(1937).-Iniffnal heat trAnAltr at low
vViocitirs and 0 fuwim of viuvwly of the liquitl is
00 "mside". P. If. Rathinatin -00
'00
*0
so 4 .00
00 4p .00
do*
CIS 0
a 00
00 0
.00
too
_0
041 '90
14
'00
A 11~~Ay C~A~s V-
too
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P
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0 0 0 * 0 0 0
0 000 00 00 0 001

00
11 a U
I IA P AL F it 99 K
of's
oj -j'.Wwiv yo Cv vk,h.
Aldlo"It "uf&Lvi*4Cf~W44PAoW&t Whk-hp(E~ 11 the =Me
foe ad wAtfwo tkmots. ma" p(r%)JR Is tW prob&bWy -00
-tvwn
I kct itor bftt tif wb"two on a Ilwo ckmmt 14 bt
K mW E +48. "is b "fid ma ubte Owtitial allit-
a k d6mewd Imm the vkwpoint of the vw~mo See
**,a mumlins ft tft" of "faxot6o a the luffut
arid, the t1meoladourption. H. C. P. A.
see
got
!*04
ASP-$LA MITALLU44KAL LITINAIMIll CL41WKATCH fit-
"OD
114"1 51"Nal" Igoe
I
taloso "it o"T cat - "T
* 4 T q - j I v- 00
41 IQ L, at ffK 12 It IN t 00 L I I Od 0 It I N a 5 a 4 3 1 1
N s
: * a 0 0 0 9 0 0 0 0 0 0 0 0 0

0 0 0 0 0 0 0 0 *'*~q 0 a o- A
val t I I 1 0 10 11 U 11 4 11 16 11 -it. 100 V" Jim my 111"o#1 041A*~V'O
fk_~L 'j- A~ r, a I is
XV, N_'Ok A-1. Ak 9 OR 0 JL-1 i 4.A _4 -I,
13W. Propetatim of Fhme. J,,M~7Atd4wUwb._*n4 D.
AO
00 Frank-Karnetittski. AeM Pkyllkwh6vike. 9. 2. PjO. 341-360. 11138.
0* A ExjrUA,-Tb* otbr' fbemits of the MmiW pm"tim of MUDO by
successive Ignition of the gas mixtum by the bat liberated in the reaction
.00
aft unsatisfactmV in that they use the Conceptim of ** ipititvn ttfflrera-
.00
W ture " of the mixture. This ignition toinivratuft is delwadent on the
properties of the mixture ItleR &M the alse and form of tM coataining
0 a vessel. A, ristional theory must therefom give the velocity of propagation
60 0 as a function of the temperature and concentration of the reacting suh,
sism", Working with this object In view. formtO Itre ifedeced for the
so -00
%vkx-.ity of p"qugation in the cam of fint, anti
00 They am somewhat complicate4. but are In (mns of Utertual comfuctivity.
00
heat of activation, density. Wori& value. sfvcific rate of reaction, the
90 gas constant and.temperature. The presence of paralW reactions and the '00
so formflon of interme4flate Products grestly restrict Use APPkation of these
himplil formuLT,
'1100
00
e 11.2"r
Yam iia4imv
103061) 91# 4.V Qvi I Floe
or of , a
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o
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ciples 441bamodpA t"k's (bat 1h4 at"It 01 ON [me awly
F at 0, m 96CIC, AM Of AM thOrMMYCAMIC WACIIIIII # At .00
10 - cis", dwelt bm 0" (WW am Qwy) Miss., And have
Willer a Mx. um any Otber ptationny powt. 'rho
investi
milou cO ne
witl complex k4utions of the man. -00
g.
s
s
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bmum the
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40
i
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I L A 04TALLUIIGKAL L"9110441 CLASIVICATICIN'.
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~' im'& 400
o *.~j J. A afid 0. A.' FAAu-KA1iZXXTiX1
IZAOO~-104- 1*0
6t diallwim-am hewit, c6duction in a .00
To) age
de),im (b --m-~44)Ab 'W' he T. a
,.W re
a, 6".:. are the temp. and, cvwn. In a' nt of the
1-b"I " AX... "0 0
1..-7 -! beNti Aand aftw' the reactim, voo
trely"'"d 7~:tht temp. befm the mwtin.
_J. J. B.
OOV
goo
we, 0,
COO
goo
goo
ago
64-ILA SUALLMICAL UTERAT409 CLAUVICATCR
Isom NOVOW if Woo
gala" Hit (my a" all"10"i mum COG.. us to
. , 9 0 '- , , , q r v cc a ZIN
u is Is I ; a a T 11A An I sa Ow 0 0
& w cl a It O'K m it it Cwt if ft I a a 3 6
0
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is 0--o' 0-0-0 Ce 0-0 -:10-0 0 0 0 - O'e's 0 0 a a 0 0 0 61

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0 0 0 0 o 0, 0 0 0 0 0,
it jo it 61 ink It Ifli
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00
60.
0o it
Sol
1*1011 MR Jim IOU owed, Q'i
lie ..;I 10, *of

004 Md D. A. Frank-Kammock4, ComPks Riodw ("lady) Ae I'Acod.
00 1 d#j ScOws, U.S.S.& 19. 9, pp. "3-M. IM In EwjhA.-4X the
exittin tboorla a( Sam. pmpaption. only that of LAwls &W v. Ulbe
Is" Abstnict 4347 111401 takes into A" Attb*k1aeWuf,tbAdwmW
proom, And they assum,that up to a given tempgMure Of Ignition no
reactionoccure, Actually the nwdou w1ocity-Is not aRexplidt tuaction
of ti-i but of the tempemtum and concentration of the rawtants
.
The Mann" In wbkb it dOPends On Uld time and On Uw distam front the
001 d4nw front cannot be obWned. tniom injeMilgg jh~ vqu&jjQn jw
60 propaptlon, and the multiag exprmwn must, in Particular. contain the
0 MufFed
vVWty Of PrOpdptkm, A paml, meti-I of solving jh~

0
0 0; ,
comill" lififftutW equat" Involved is now suatattd. It. If. Ito.
CTALLUPSOCAL UTINAT1,81 CLASSIFICADC"
OW
64 It
V
U $I AV $0 11:
. it to -1W It iN It Of Vr a ic a
:0 0
100 0 00 6 0 0 9 0 0 0 If 0
0:0 0000000 0 0
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--iiiiii
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U3 A I Kit
0 600*440*066000**00
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~00
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LIM

0 a: i s 9"oullutsuly is Pt a i s 2) i 1310 10 H P 13 it A 36 V Is 30 4 41 Q 41 40 6 2
'.
4 1.0CCjUt A-4 C 'I Ns
Thelma! exPlOCICS Of nitrOM Oxide. -Yj6-JJ,.-,7AT--
clo
Vakoviev
ich and B
1
rtnd
romps
d
i

j .
.
.
.
. nea
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v
.
-At
S
19
li
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S
M(19M
li
h
(i
ff
i
.
n
s
.
su
.
u
,
ng
).
ently
)
hills temps. and corTegboudinsc rate of heat liberatkni
from The eXachermic reacticra, decompa. of INO Nrmnes
of explosive. accompanied by a blue game and a diurp rise
so a in prt"urt. The following limiting temps. wrre fixitul

fe v in a quarti vr~wl 2,3 cm. diam. by IS cm. I(mig.
0
i
P. In now T. Imod
T, esi-d.
.00
171) 12W 12M
00 Uf IM: jl-,5-
590 11W 1110* ago
~

06 The calcu. was carried. out according to the Frank.
00 j Kanscactskif chewy W, oreceding abar.). G. At. Evans coo
*0
0
0
L
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age

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ASIR.ILA afTALtURCICAL WilAYL,11 CLASSIPICA1101,
r3o", 11valiv. C-17
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0 u In Aw is

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to
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sted vvmd cWtalped sk wasa
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7~
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i tmp. by bmt ' Am witb the wells al thQ
M%wtd bf the Pce"We
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ibe cowis M The I
thmncd.~ ,The repliu wro the saint (Of the 2 9900 -d 9
lie in iia falwPAaam Owmisla. U. M.

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A a - I L A IIIIALMICAL LITINAT(All CLAIMPICATION CIO 0
room laolftv
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millal OR ~v All
AT 10 As~l w ax mii s a aki o a w i v so 9 a a 31 T
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MUM GwAwgmwu 09 t5s acdoWl s"Us"40"'

a
l 1425-7(IW9); cf. C- A - 34- '1734'-
h 'jU S S R ) 9
r ,
Kh. cocusida the mt-d-tiOn 'A
neutrms fomed in U disintesmlion AM tht utcvst&ry

, rivndifliotm for the dWattuation. F. it. Rathmants
,
go j 1 Zoo
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,
Tkwn4. Pbr; (V. S. S. it.)
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m
e I
i r
j
j
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er
a
m
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cg
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betarrva rjr unequally heated wW% h discutwd., Tual
crinditkon B
w
e
ttin
i
ti

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g it v
s
onary smia or kad.
o
p
199 t0 11MIAMMAtton. tho ilhope **j dhMA"S W %be
11
th
i

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e MW
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da of tbf tutf, itit., "a eft4dVied and a
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00.3
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zast. Chemical Physics
Aca(I
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PO -3 reacts with a gaa or catalymm & gas readi- the zoo

06- supellkW part has nume n1ty for Traction than
which a Traction
t
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00 ;1 o
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that underneath.
e tg*tm in cale.; it is inversely 0C the a To root
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be 0
tie 0
to 0

via.,
via., 95. are is
SS146.4 -IF *~v gas ad 4"l is .I
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o -ft&Ii-(651WdTZ-tvxrstIo* of uranium under the ac,
tion of slow neutrons. Ys. D. Zrl*dqykb and Yu. R
Khwiton. J. Expl. Mord"PNWIWS~.18.- R') 10,
'Z1,4910940).-Tht poWbility of jauclc4r chain-rrartlons
(explonions) In the system U-11,K) were studied, taking
into account that after the collWon with a proton, the

energy of neutron can lie with equal probability anjwherr
ttccwvcn its original value and zero. and siting Ortit.
%%'irxnrr'4 tewrinner formula for Ilse last of 26-c, Y. neu.
Irons In she CtAlwous with the heavier U Isotope. They
cale. the value of P#,P,, where P Is the numbcr of neutrons
emitted pcr U nucleus 0 the capture probability of neutron,
and lp the probability th it the neutron will be slowed down
Without being captured on the tt!konance level of Ulm.

Under ismst favorable fulzing ratio W V and 160
.40 w 0.00, The condition nect-&ury for the chain reac.
tion is #0v > 1. It isconcluded that thersplosive liberit.
tion of nuclear energy in ibis system is inspossiJbIc. If the
concentration of U14 can be increased by, a factor of 2,
Ap becomes equal to unity and the esplosion can take

place. The cawns. have been c"cd out for infinite me.
dia; in the caft of small volumes the rated, value of reop is

considerably reduced, and, In order to obtain the explosion
it Is twt&wy to Increase the corseentsatiou of Us* still
I(okkiland (Asslow
u)(We. -00

-so
-00

0

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000

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tiL L I
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or K CC Vt U n Ct n 11 CC A* A 1.
V~
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-4 ~,N -.4
ZEWDOVICII, IAO-B.--
RT-963 (Kinetics of chain decomposition of uranium) Kinetika tsepnogo raspada urana.
ZHURNAL EKSPERD=ALIKOI I TEORETICHESKOI FIZIXI, 10(5): 477-482, 1940.

poll 9111 -00640
I a fluum"Is fly," l"Wa8l" it is it a RU a 14a At It x a 40 41 v a a 4 0
T u I I M IN I- A
00 0
law" of uts
*Ms. Ye. B.PC711-Tvvdiftch. of d4EftTP&dtI*U I& CU*h*YUJS
00 .00
0 jr divoisses the talc pill ptutuptiou, sekdoikol the Built. -00
vulue, inflantmdon by coinprcmion, propagation In a
04 1H In .0
be with correction for Impmlanm and thenual lows,
conditions for the prove" of Chem. rtaxtlotls Mid the spin -60
of Ebe detbdation wave and ounol&rs sovue cxpil, data
lot H-air dctoustion, concludes that Icultion results .00
00 It= a temp. Lacrejume produced by touldpir raleated cow. .00
00 pression produced by the exploviou wave. Diffusiou of
WiVe Centers COUU01 &"OUnt (09 400011tWO Ion 000
0 * 'j For last chew, reactions the ckulca! thcory =k., '40
F. it. Rathmann
66
of COO
W
Lab. of Combustion of Gases, Inst. Chemical Physics
Acad. Sci. Ma
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ttrn lure, compt"sixtoro fit the V44 lititsture. and the laws
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tor thedetmational2flo+ Oandil + Cholixta.arecom.
I with rxpil. dais. The best *1 d6som. of CO Is
to toe over 210 ks.-Coil, F. It, Rathmnit -
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-Phyeice, Acad. Sci. LssR
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4~11 1;10R--0111
40 mixtures in a veokAj tube can be ignited at the bottom but not tit .00
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W supply to the dame (determined by the dMuslon corfl. of the 0
so
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eurr. After a eltort di4cussion of the ditIrrence
the two t)TAs for a ren subot&nm Is rwokirred. At low tvtnpvralunv~
06 A
transition of a metdl eta a dielectric form would be a phase ch&tW. with 4
.00
latent beat and R discontinuous ehwW of projwrtho; 4-vatinuoua tranxithm is
ony ible at very h~h tensperatures and lirt-mures, where the excitation
y Thmi calwo am,
an electric4l covuluctiv t of tile dielectric form am, high.
0 0 $see
seem.
panW by liquid ---)-gas transition. (b) onheatingstawtulantp"urr, =go
liquid metal changem into a " metallic gas," W)104 at high temperatuirs.
changes into a normal gas; (c) an heating at a constant pressure, liquid nietal
ChangvS Into a non-vowtuvtIng liquid, Which on further hoating is trawrormed
0OU Into a normal gas. (a) is expected for non-volatile metals, (6) Is improbable. SOO
%,4whfle (c) to expce" for subnanm lihe mereury-G. V. ft.
_2 'ACad
Inet. Pbpical Problems, -901- U&S and
.06 LISt- Chemical Physica, Acad. Sci. trM ZOO
ISO
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ZEL I DOV IGji OVIGIL
Teori.ia goreniia i detonatsii gazov. klos?va, Izd-vo Akadem-i-i 6auk SS41 15411)
70 p., diagrs.
Bibliography: p.60,-70.
Title tr.: Theory' of combustion and detohtion of gases
QD516.Z4
SO: Aeronautical Sciences and Aviation in the Soviet Union, Library of
Congress, 1955.

~-A I,

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ar
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MOCA L"tRAIM CUUNremin

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ZELIDOVICH, YA. B.
Teoriya undarTikh voln i vvedeniVe v gazodinamiku.
(Theory of Shock Telaves and Introduction to Gas Dmamics)
1946. 186 p.
~IN This monographIspecial care was given to the accurate
presentation of basic laws of the dynamics of gases and
tothe methods of calculation of simple problems.
Aranslation 5 52464

-SELIPOVICH9 YA
-Jul
Rarefaction 'Waves
Shook Waves
"The Poobibility of the Rarefaction Shook Waves,"-
Ya,. Zelldovich, Inat Chem Phys, Acad Sci USSR) 2 pp
"Journal of Physics USSR" Vol 1, No 4
Damonstraten that for gaaeo with large molar heat
capacity 0 there exists a region vhere the rarefac-
tion waves must -propagate in the fozi2 of shook waves
add ccmpression waves must bo blurred In the course
.of propagation. Received, -5 Sep 1945.

2ELIDOVIOHP YA.
jaix* 19
Shook Waves
Wave Propagation
"The Propagation of Shock Waves in Gas With ReverAbld
6
Ch6mieal Reactions," Ya. Zelldovich, Inat Chem Phye,
Aced Sci USSR, 4 pp
"Journal of PbyaioB UM" Vol X, No 4
Study of propagation of shock waves in gas with re
versible chemical reactiono or retarded excitation of
the part of the heat capacity which Induces a mat
expansion of the shock wave front, structure of vb1ch
depends on wave amplitdde.-Mis Webt used'in In-
vestigstion of e*erMr transfer ~ to Inner deases of
freedom of,zolsoulas-, :Racelved, 5 Sep 1945-
54T88

pov"Olles 0h"&
Axi* wini& -Ts"M'dow
J. EVA It. Pt
h
i
d
on
r C-mcfas
ke
to t
tts as abqu t shmk
11331 raref3dion in
ams
ropm
p
S
p
"nalm, waves blurml with
and em
p
lti
f t
ons o
Uad" mm cow
emp,
-1wid premtv "1 (6401*9. b bm than 0 (at mut. en-
tropy lumch sunterkd take.. & comt. bcat Co-
'
i
"
rquAt
m
I Strict Todity 4 yaw tkf XVAAU
ity C.
M
dask are'amnicd, %bon this to oomw for C.
*1 cal./
111CAC. JIM
ww

sell

41
41

~
1*14*4 olp Q%0`44f
9 A WA
8.*-(*
lop" _A~ a--* ol~CWWI
*00
**a
lot .
moo
wee
:00
U* I*
w0

ZELIDOVICH, YA.
USSR/Shook Waves Prop2jptlon Apr 1946
Gases
"The Propagati- o of Shock Waves in Gases with a
Reversible Chemical Reaction.," Ya. Zellclovich, 4 pp
"Zhur Eksp i Teor Fiz" Vol XVI, No 4
Consideration of the propagation of chock waves 1n a
gas with a,reversible chemical reaction or a delayed
excitation of part of its specific heat, which
peculiarities cause a sharply pronounced expansion
of the shook wave front.
13T52

A
Combusum of methyl nitrate Topm, Va. 11.2d'.jovich
**A And Vu. Kh. Shaulov, (Inst. Chens. Phy~., Acad. *vi.
U.S.S.R., Mtpwow). J. Pkys. Ckes". (U-S.S.R.) 20.
of 1.359-020940)(1n Rumbn).- -Photographs of ignition #4
SON WOSO~ vapor In a g1am vemel by & spmrk show that it
fianic ftA]4mn M Apark &Itet a tinte Int"val of 0.01 w.'
*OA for a vessel 15 cm. in diem., aml UAW 4vc. for a 5-cm.
vr.let. It was concluded that the %park cauw3 the mar.
tion CIII.Voi - CO + 1110 + 0.5 11, + SO which 41-
velevs too fit(ke rwUliou to affect the ph(Angraphic-
Pta r. I owrv", thii trartkm rai-* the jw ~- within 'too
**-I Ihe'vetsell, and the heat III the adi4bath, cornprmiun in-
j Ulit dum4a sermil dame in whicht),5 CO 1- 11.5 111 + Xotivv zoo
0.5 C(h + 0.3 UvO + Thi,;awchanistnumsproml
by Copts. In a Kim vesstj %cpd. Itom another vr*-tl filk-d
with inert g" by a thin membrane which broke during $,he a
first reaction and eliminated the adiabatic conipt",itm. too
T'herv was no smodary flaniv in this arrangrinent. The.
6fter deconip". In The pin-A."Ce 0( a me"Ibratir Cm.
*sit gas a WOO
tainqt(I emi ninre than the thrvictical aint. o(NO, and the
xa* after a he vetwad Nine Its a clowd vemel rem
taltird mily
about 1% of NO. 1. 1. hilimitan 40*
777= see
'A
%JMAL~ "TALLURGICAL UTCRATUNI CLASSOtCATIC*
glow 61"914W. slam VU&AV
MJAW ow GOV All
%$Java At 04V Got
go 0 , , , . 1 0 F A a ?W 0 of a I Iff It I A a 3 1 v
r
4 x a x 0 En I YA
vs 0 0 0 0 6 6 0 0 0.0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 111 0

0 0 0 0 0 0 0 0 0 0 0 0 0 a 0 0 ;jr; -0
11 or 13 W4 is 4 11 it I- I U .3 24 AS h a A Z Is V Is M 11 14 11, 9 so 4j 'I
.4-1- 1 - t ~ i -1 9 _ a % A t 1 1 7 1 so
L
6. The oxidation of nitrogen In construction and arplodonse.
Va._1I_ZcVdavkh%(In*t. Client. Plin., Mwcow). Arta
phyfSearhift. V.R.S.S. 21, 5-714US(1940) (in F-sifush);
cf, Cal. 40, Wl~-The &nit. of NO formed In tile cx-
00 Is. Itim"t tof inists. of Ilr4h-Nj. v"ttg from 28~-q to 48%
Ill. anti of Coliti-Or-Ni. cuntx. 6-81" W14, was mix.
halfway between am toncrui. of N's ;~rcxccw 0, owr the
o0 'IS' rtViirensent fcpr complete oxitlation. NO ykid torsis detil.
Z' after exid,rdlin for inixts. of Ifor-Ch-Ni with No equal it)
it; ctive" Ov. I(vair, with Ni equal
ii 1 1- to) excezu 0,., artil (901*oCO- 1017a1 Is) -air at 200 min.
p(Miure Anil initial tellip. from -100" to 3MI. The :6,6
r(juil. con,ot. C'its the equation, [NOI - C'
'31 1, tore 1(ill Is the excess 0 after conslainstion, Is Intle deist
tkil the iVl '"lif 0" ention". last Ilt 1'rola'ationAl tit t cons Cog
it Itible lit the 111111. Fur rise d1kWW_ olipt.*. tile curves (if ago
I" plotted as a fulwti.sn (4 the beat (it cluillnistiou Islui a
ciorwWasi for tile winsible licat of the utlit. Mudde,
'rhe utoervird yields art tU)-'7U','e of the caled. ther"listly-
goll
ItAillic cillill. if the exploolon tvillp, Is coartrick(l (Ur the
I
alatche r(Iret I-W lentil. disititnition 1011 athill'of varying anih. lit N011111o lit 111111" Wollift'l:
One its the little effret inyiolv~l its the 1,rojoasistion of 11601", A, v -41 an't Lho JWT Ill'ol. wet.
.11 n1j", roortillr4 'd
A inlost. 14 coal stas-01-dir "a% buruct In it opecial IMill'u. 119;1111 IOW tile IWAt 44 111"1'411111-11. And holinAlblil. to--It.
!
1e. low. Virtaturi-tylie burner *it% nit "Id. troult. of 'K~ rhe ilr;k-ndrih-c of the reat-th.st vrincity (as 0, colnen.
"anspim of 1.400
jibe gas at a writs of joitints starting from the. predictril by the chairt arrvitanitim watt c%infinned tryorajois.
Onus of 0 r Iturner %huwrJ an Inervam in NO conen. up Wit is ritcV4, (Joel. The ellwrmolnil JIS01/41 - 0 X 11114/
tit a rn-ix. The rmlis coisfirin the therinal formation of
So fr'sul 'q1 and Ol wt a rmilt (of t tic high (emp. prfxfticr4 I its WtI10% 411.1 Vlown'. ilk H144. L. Was dtflMl 1101'
ion toxidati,"i id the cornbu.tible. The anti. of NO on I rcactit'll A. Fleiwhrr juee
vxpl~bris of inkis.-4 tit
-lit AS&~$L& a[TALLVRCKAL &ITIRAYWC CLASUPICATICH
4, to .161 444141 1:19 4.- it,
Joe
TA'
W
U Va to (1, It a 1W of A R It $1 n of 0 41) A 1 1"
9!o 0 9
0 0; 0 00 0 0000 000 0 0 0.4 0 '0 0 :10 _6 0 0_09 06 so 0 0 a 0 0 *A

API i to j-0- -0
109,11"? 1 to I
oft I T T ?'.&
A -A. L 0 r .1 1 IL
Plac-CiMl Ago #*"Fsl;tf vis
00
0& A'
00 106
A
00
00 4!
O%idaIff-vt af Nitrogtil During COmbusilkm and Expl~-
zoo
iiar. la, Zeldrivitch, Reports of W .11'ade,wl 4,
51, no. 3, 1916, p. 213-2fill. Cleo
002 Sciences PT'US.S.R., V.
0 43 ,
9 00
001,
goes
AA
X00
w0 s
uoo
4.1LA AlITIRLURGICAL UfflIATUA9 tLAMOICAIJOW tso
~MOOO -A ago IV C%W 049
1041
$_jb U 9 a 10 is to if to (11 OC 'K if ft CC It Ot ZI u IX
o 0 0 *1* 0 9 0 0 0 0 0 0 0 0 a
A."AL-0--s e : : : :
0 0 010 0 * 0 0 o_* 0 0 0 W 0

0 0 0 It -1 0 11 V- 0 a 0
0 a J# b x v m m Ao R Ij JI M 14 30 Is P AV 4 v .1
Is4 Is &I R It to x k q 0
~A A-.X- i-I
0 A
00 . .... ....
to, A
00
'016.61 j.00
*0 0
00 It j!
eo a
(5midation of ni"m bx combustion and SK00alan.
0 Zv&luvich. .
acod, mi. V.R.S.S. 51.
0 'imory(may--rGo. on th~ uAturc and IftIvItsulull ol r0 0
00 this rtwti4xi Show It to be a thtflital INIC. with the Ist-at
=06
produced by the tsirni!iS piv"ii:ig a high trmp.. IghcrVAS
so 0 01 the N atidatiou rtaction jimmeds a% it 'AmM UnAlpr 1 460
00 %3 any pitur twoul-i of hestarig. 'nse all, totior t4 the
IR4 *Xtcf %lilt thr avullilption klf d
60~ 1411101. SlIt-ChAlliMIS. Init dt~ AjtVV "ith tile CUP$ lJKVhA- X0
0* nisin: 0 + N. - NO + N. N I- Ot - NO #- 0. Sisim 0
the dre%mim. velocity 1% toutxwtiotutl to the 4quare of tile 0
00- "Mcn. of NO all the irmilts uq fiattiAl k0actic computa. -0 49
tit"is uUMIC ou tile a-mumptioll of a himul. Tracti.ml Frislain 0
ill 1.1fer. -111V c1laill ulmhalli'm 1% not at Variance With
1110 C0IIVj)ti0n of thl' 01CF1110 SIA11114' Of tile teACtido,
A. 8, Mwotan
200
IMI
!:0 0
st?ALLUStGICAL LITIRAILM CLAt$tFKATIZI. life
:010
IfflaNj oil CII 4.( 41 Wckr'
. I i~4~
u AT p0 Ls It im two GIwI45A3d 34V
; I 1 91 a It of 01W ?I
61 It 0 14
0 0 0 * 0 0 0 0 0 0 0 * 0 0 0
0 Ole 0 0 00 00 0 0 a 0 40 0 * 000910 a 0 0 0 a 0 0 ~ 0 ** so 90 111"~

Am
PaBchety teplovykh protseusov
pri vyskoi temperature (Calculatiorw of thermal -processes at laigh
temperatures), Izd. Byuro Novoi Tekh. bez Goroda, Moscow, 1947, 66
pp. 16 rdforences.
Reviewed in Uspekhl Fiz. Nauk, Vol. 34, 11946, pp. 462-463.

ZILIDOVICH,Ya.B.; SADOVNIKOV.P.Ya. (deceased]; FRANK-KAHNUZSXIY,D.A.;
*"p~""*~0I)~St'IY.V.V.,rodaktor; SEMOV,N.N.0 akademik, redaktor;
44LYSHK1ffA,O.V., tekhnicheskiy redaktor
(Oxidation of nitrogen during combustion] Okielonie azota pri
gorenli. Moskva, lzd-vo Akademii nauk SSSR, 1947. 144 p,
(Nitrogen) (MI2A 9-3)

41* A'
06
.3
to
0 0 0-0 0 0 0-0-0 - 0 ,*--0 0 -0- OC
0 7q
*to o#&# bill mumostedi ado ot 0
Mm

(A Ctxttw tit
KnLla I
Trpiov%A vat" I vA"O%ATSnvAc PL
.
(;,ArA%h (ThvnWI ffxpk rtkm of Mium
14km awl 11,111M
m Y
Voo"odookU
In ll
Ya
~

o ois
.
.
,
y
,
130
Kni" 11. TurW -WM Wleftigrnnue (koctuic Moo.
=00
1
11111clit musl By Va. 11,
6,1
l 1)
nk Mwmws
F
Z
IM
A ve 0
.
1 013t
.
ra
T
UY
U400, Upskuy. hickhan. Inst. 1017. RX) pp. ReJ .
ro.
VICIMI III fliftiki NAim. 17. M-8(1900.
goo
400
goo
voo
use
so v
u fA AV to i. Al a 1 4 04 0, 14 9 a 3 4
o W000"A sit ";Ft
is Co. Lt. 4i I& i's I R
00-000 0

00
"00
00 00
a' as
Theory of Aletonad-
J. 7'"'1'k" S.S.R.) ItMil)417"
ogs -p ;g,3 hich W bee
& i a( a strasight cyfiikbicLl tube was studied. In o:
0 the &= surfacc is F - (Sht-Jer. A .0
0
0019 1j=h1chc15 Is the CTM-SOCtin"All am 01 the
tube, W. Is tile IUALIL- V'eWty of the gas. M. is the Horinal 00
vitlocity Of thee gas. wO ri is the av. WtIocity of the gL% =00
000 a givvn croAs sedion. The disphectn"It Of
V:. T tile tube sit* due to tutbultwt PubAtIM3
amounts to 7% (A the tube diam.; It dtffcAAA,% near the
Wells. The value of the pullation velority rt"hca 11%
of the av. VvltxitY In stn(KAh tubes and 17% In foush
tubec In lantluAir dow the time requilt4l for ilttWM6011,
of the flamt front Is A, . RO/20 v In which R is the tube
radius and A, to the kinematic Viscosity of th4t K"- Titne
:nd length of path of detonation onwt, ecArAing time od the
opment of the flame front lue- 1100
as. anit the lime for tlcvvl No
cakil. R. W. Runker
a see 0
!:08
Lre 0
A
9 z7r- doe
411111 ow "W Ali- ]to 0
I F
U A, x It or it It 4 t Run 1A A I V Od 0 AS a i ar w 9 a a 3 0 K V
0 It . I
0 0 0 0 0 0 Q 0 0 0 0 0 0 0 0 9 19 0 0 0 9 0 0
;T.4 00000
0-0 000 0 0-0

'ICY
Formation of IUVtc*n
stridild tube. IL =Cdarill *to*"= 14 is con
Zh%r. Fliptt. re". Fit. M
Autles III the moment of trAniltion Into detonation, the
wrlocity Incrraws from a rclottlye value of 0.."4).4.1 in III
r0AtlYO VAllit Of 1. 10 nAff*W 1141W0 1114P Pf"OfMIAMM VTItW'
lly prior to transition Is the same, wlthirl ezptl. evor, oil the
i1clonatl(lit velocity fit widic tutics. An exp1l. arranievirrit
WAO maile lit whk-h prolmiltillaii was Initleteol ct the wWt
elid of a tube 14) t-111. 14MIg MISIStIlle of a W-cm, kvilem,
1.3-5.0 rin. In diam. and a 30-cm. section 0.8-1.0 cru. lit
.1i4m. Elementary inethods of c-Ak-n. for irtleett4l and
irunsli4knal waves Indicated that In the narrow tube the
pressure in ritflection was 2.5 times greater. The c&W. m
milm agr"4 with expt. H. K. tjvfnxstcm

1111P wig His 149 spell dtk **'PO
00
00

0.4
:
0

lt

00 f

O*s
00
-00
so A
00
534=
-00
;
0400 44M.

.
-
, vww.

'
OM '
V

0 4
3
i -0%
OVO." T
N
dom . .at-on -wan
00
di
0
mc
0 r
thma of
ft=
to be dai*d fi4f, =00

"=ft W4
of swcuad .00

on frd OOMY 060
.
Anwaft 00"' COORL Ba Q*
ro 0
0 a bid aw J04 tbw H*
"
0 SAV did am dliefvhy

L 0. T.- gee

woo
VII !10*
~
:00
A!,!-.lL& PITALLIONGICAL CITINATURE CLASSWICATICII g-2 too
loci., 1:96

-
y
1
IMI&II Ole amv Ill
-
0
LV 10 Ll l
-II In a, X, IKI a,
n, In, I Ali L S 6 cd a I No a 43 0 3 1 9
m
~
000 0 *41411100000,000000
' ~
0,00094POO0600000000900
'' 4
p
~
60
000 0000000000000 00 000000000*000.410*449,000

C'A
Conditions for establishment of instability of normal Calls-
bustlon. Transition of spherical Itame into dotonstfoo.
B. 7el'd-vich anA A. 1. RnzInv4it, POkfoldy .04d~
1917) -h
,Van& t.1;..1L-SzRVAb7F'.'"'-1 N. - -Ilarning 1114
twith C.% added for vic-urvii definition (if pholopiphy) in
a %t"1 bonih with a I X III cim lit 'A.11 rcv.wdetl Ily Ilith.
%pMI pholography. At ;I total pt-urr of alumil I Alto
, liking Such a mixt. 3e.441.1 11) .1 irgion of propag-stion of
tric bme with "Scillially ctmount vVIncily (;I% we" throux))
the 40 of 8100cm./see. After travern-ulticul. and cool-
buttion o(670of the rnixt. the lore-tAurv riws tip 1.7atm., near
the end of combustion tile pressure d" In III atin, and
intensity of radiation ri~" sharply. No autoturbulcoce 6
observed. At an Initial pressure of 10 atnt. the comunt
flanit! propaptioll velocity 1122.091 cnI./-%rc. for a 2A Col.
path, after which deton3tion is mcht-.1,(Mobably as a relult
of autnturbulctice, St. KnioUloff

41
oi
1
foe'lat'if
:~if
(loot., Mto.
11hyrs, ('414, U. 27-0004M)OR RUN"")
l(quisticas an givirn for beat cmd.. dilfw4w, ArAl C4100h.
00 is in fitro" smoving In an TIPWVT Mixt. The
400
KCAMI disiributioct of temp. in the datrie and the -it-
:; 00
tigms wkkh must he futOetj by * them. teadlutt to amble
IMI, "0 rao o(-
to Inovit at a "M%%1. fulf 410 Ili
~""fistkm 44 Olitme Iscollml. lot silifoolke WOW twist 0
dilfusion and heq it-Ouctalke. Tht differoth" bttw"n
r of propetca" 1A
ttw upper slut 1hoi kmer utrift of the -it,
x"wiff The grak"t ill* letup. coed. of The rate of chan. is
The effect ce ellitin rvotcttms an kbe VOPOPtim
rescitkos. Wertol IF
J. J.
rvaluatird.
1.F
1110114.4% WAL&VOrOCAt. LryffaTtidlif CLASIMPIC&TJOx
Ai ------ ---
to sat., a., Zat
lot 1,
VU 0 P4*11r4M2dJG,)
U 911 0 go It Or it _1111, a it tt
00 tt " "r"
0
0 1 0 0 0
**1*,* 0 0 4111,001
0 0
LL
~54~ff

7

Va. B. Zdldovkb (lot. Cbm. ftys., Amd. Sel. U.S.
I
;
ILR MMA-1 ). .1. FAV. 11~. MJAR.) V 427-
- t
r
dimt w5L tbo
r#
.-
a
A
mV. C
"ampia agm ho At mx. at a dk"JK4 4
ew
th
C
u
vu* *
m
f u
fi
f
h
d 4m
e
.
m
fom t
e ta
o
gem.
=p
V
'
svA the dfinessio" of the butia.
of tM gsik Its vd*dAr. 160
This ms. cutm a =ax. of do gritdimt GO d. p wit" tat"
Plow at ftm=- do first-olmd Max. wbu so

0 imbutim oo=s.,:A bem of thgodA
doug
Lmxu
1
f
m ft
4
m t
w
s
l
a
CIO =tbP 41/
)om
fdm dw temp. NNW" wkWo the
go can be calml. '11m equatim reclubcd m duived.
87
h
f
k
ith M ro o
d. o
s
Rxpts. wem ma& by uslas a w
%) w
(
matff. @=A no (13%) xwwiu " a mft of 10-a cm./wc.
Tu rem&s wm fe avo4mt wM cbe ti=".
94t
w="

ve

woo

Full
q1-_: -s * Im
Km
0: -AO
-01

X 1~
00 -;-,-------M ~_4*6 1 _114- 111-6 f-W,
-00
"a 0
00
00
'a 0
as 1401
De4onittion of &%soon$ milluriss. 8,
1,14. Is. ,~jjended from 19.0 to M-K~ Il. I file wwr tUIW*,
Silskvich_ Diktadv Mad. Vawk S..V.S.R. 63, datonation was observed from 15 " '00,
00 '"1 o(TOR -lituditl of ticinnition fit w6le fishes were In IL For all
file tAliCCt Of ICAIllitig 11)(Yet AIXMI, the KAtUrV of olixts. from 25 to W; If* file Frcuriled tmxuufc was in i's 0
*a ,-It "is,,
he v( cocidem9ml gais in thew Ave (runt. Theoretical C"I QUee"lect, with the prewirr cakd. for the traction
00 if itmis %hawrif that by uw of larger tut" it wcmld PCOdUCts Ill flwAns 'A fh~ rl4sicil theory of detonation. 'E 1-00
fer,"; -put near the lower Jbilit. the rocalsturd pressure was
a, 0 C to (Ictonate mixts, thit, hA- Rwh it VrAt time =11. a tinsel the calelf. Value awl nftf flit UI4W1 Hillit '00
for chem. rrartion that they wrAtkt not dclonate in narrow
a vil pristsurr was approx. tivict as Lust " ca", to 0
it
60 1 tut". I'liv app. cvmisisted of steel tubes W mm. in in- me"Ur
00 0 frets $I diam. and 12.2 m. long. equipped with a ittrain r,!gr The explanation for this dillerrisce is as follows: For mixt1k. ~*e
Thc,it!to;i-.ttionvr.Aiiniti.,ttdvnth near stokitionsetric, the time from the conspression of the
00 j fill,, %a
A M, I. rltmst 4 fliph"I"V. I'Le Int)e dtiltl%. were PI its t. fly the shock w2sir until the end of clital. rimctiou is
Ah - W is tillics ft~Atcr than MOW of tilfw* 11.4mily UwA in drwivi. t4i inuill as to be negligible in cim)parisort with the reironsve r-O 0,
00 11 f Lt. The uft- o( (fit Wide, tutet im-rica-Ad Ili, little Of list Arpin fluxt, Which lj~ about 0.1 "Imisec. FCK r* a
floss ii Ili $
fang* of 11 catu*"$. in It-air Inixt6, over which detonAtfoll very loan or very skil, milt", the velocity tif tvActiR,4% be-
cotM to obw1W. In narrow tubts. detatizublif inuu. comes compaublewhIs the list r'spoun firm the ft- too
cord;d rcsitutgels newirs, to the pressure Of =rawtbm
'too thf W Prodoets. Con.
a to pft~Aurt of the react .1-60
shirrafkm of the theory for florists! dettivition waves (Z.,-
CA 33 =') jind spinning detonation wamis M. C.A.
41, 11.1 113 rithrr cupr the limits of dvtm4- t"be
h
t
fWa, were extrmird and flit mass. rewtion firm At the a
L
litill IncrMsird with
tv a
too
Ajs1.jCA 61YALLORCOCAL WINATunt CLA$j#K,sTr
1111108a "is Qv ONC flow OVIRV
:U:19,1*10 14 too'. CW 4Wv Lit
7 7A *A L I a ad a
OF is a It 09 If A I 'a a
00 0 000 0000,0
, I to 0 O,e 0 a 0 0 as 0 0 0 0-0 00 a 9 .0 0 41 46 as 'a
0 4 0 0 40 0
so
00 00 0

00 d
M 31 a 13 w 10 36
.1 el .1 11 _12 1-JuL LA"A 1
A
9-1 -1-
Ail
4Mk
&Stgo, 1IM4. Air Mat. Comam. WrigAt-PaUftvan Air Pocc
8-- D0100". OW, Tsck ReP. m F-TS-IMIA, 118 pp.. May
1M.
7.7= :I-
*I*., 11TI&SIV.
iiiabi Mir 44T ant
* 1i T i I I
IL : AT 43 to Ivis waft* Ifult 110M,04
0 0 40 0
0 0 0, 0 040 0 Wo 00 so 000000
114" Oman-
P it 4 a a Q 41 d'4
=00
use
Ras C,
00
goo
gOO
M
An & S a cw a 9 A a
0 0 0 0 0 0 0 0 0 0 0 0 a
0 4 4:0. 0 0 a 4 00006946

P 'D
k~ -9~01
i -Co' i,
Af
w
ZTE TIC71-YA-i-B.
25533. O.Fovyerkhnost Nom Vatyazhyenin Granitsy Fm7dyela Vzaimno Vsstucv-Izykh-
Zhidkostyey. Zhurnal Fiz. Yhirr5i, 10,49o VfP- 8o c 931-35
SO: Letopis' Zhi)rnallnykh Statey, Vol. 34, Mmsleva, 1949

7EL'DOVICH,-Ya4--B*---
L I
36594. ZELIDOUCH, Ya. B. i'SIKO11OVI I.T. N K Teorii Iski-ovogo Vosplp-mnoniya
Gazovy1ch Vzry-vehatylch Smsey. Zhurnal riz: KhLrrdio 1949, vyp. 11, c. 1361-74 - Bibliogr:
12 Ilazv.
SO: Letopisf ZhurnalfrWkh Statey, Vol. 50, Vloskva, 1949
ME

O-V/ )Y.qkv v _[Z~Orvl ISO V~ C.
!/vi'dilvith. /Avr~ &AA. VIA!. 10 'No ltkloltlt~ V-10.
.ljrfw.v,v0~.. Aerewful. TMA, uga ::o vi.-
(lik,l): -A tttNwvtk.Al StWIT it UmIttAt J0.
111,ic"I ItAI1IC* With IIIV ~~IUI'1111441 Of 1,111id (VACtiOU FAI"
and no Iola of glivittv Ily Ta,IWiwt (cf. 14%VAII. 6.1skjarst.
114. 1048). CIE11.1114wil aw lit-
Nth 1.11I.Wilu, Jmlwof
01 1tit. 4410 111V thime It.41111, 1110 lAwl It vAid III lw
Iirld VVIIII lite Irulls. III it pfe-IOW11 114111'. Of 111, mw
CUI vit.. whith is aviarAry to espi. This is dite it) the fAct
III the rA61km loss III rut diflusiott (Lunes 6 not neg-
lisible. Rx Is4� twett wOmmed firfe. Until. Of (visibumitma Of
ulamixed jw~ .$IV III.) cuu4i.irred. I lerv III,- bet th4t rede-
IkXI VrI(Witit's dir ACILWIIY IhIIIC Alki 111110
toe 14ken l"Isp 'tt'"Int. sind vtpr~kml% Aw tjplwr and km"
n"11 IIFISSIM"I IiII014 C.111 111011 I~ delly"l. C~ I'AIdOt1I

00 .00
Oe A
.40

.00 imbdum, It. A Anaa-iv.

'
vil" it, "d M TtAirs XAmr. Pis, Shim.
914" .40

00 - 11m. .1, lk-
He a7gifiHO).~
vvd r"the OpaptIft of the torm ption. In a dAt
so C8011"y Ili vrXib'duNiow 9(2 callints. takes III,"* In dw
d
(
d

A s Lmi
~74ptkwi depen
l,~~k it, ~09 0
diflu
"i coeffs
f
_in% h
5
00 e
s
, o .00

8
00 el 1.1.
~ pcotiuct ut thq ppt. We
I:b Y.
:
t
4
. j the cupIlLitry m1w stra calcd.
~
ni. .1 th. .0as 0
00 it 1 0
so 900
0 0. coo
00.4
Cos
LA

goo
goo
Is
too

Wo
a - -~~!IIAI !~111111,1149- CLISWIC01"

"14-1110" Ow 9"1 111
1
'

0 AI
;

k r
,17r
Ap 1 0 fw a 10 1 1 IF 0 0 a 0 2
Ii, "1 4111
low A 10 4 ;T W;
F
0. 0 00 4
L 0 see O's 4 o ww* is 0 to a 0 0 6 0 0.4 0 so 000600 00 0 00
-
2
l
A
-a * 0
0 0-04 0 0-0-0-0 0 6: o
0 as o so 0 6-6 o a a
0. 10 *so 0 0 10
*

LI-1 l
fi
Ms O
o
n
4

-kftdm,- Ya. B. Zet'do*h aW 0. if.
-
Fis. Kkiol,(J. ftl9tca
aw.1 Ud. pre-
cedlux awes that the time
ol fmwoon ig 0. to P. Was the
Is r- -
Omd
pr
-_dlmawe- of tbv
. boun"y, and Ibmt
4 W.
qw- thedblium (r.. -- r.) ire In &cmnmrkAlprmrmhm.
"v ratict v%tild(tv 4 the illwxwy 1*18(wined. U.
ear -00

, too
00 43
00 to 0

be*

IN8461, "1# 4%t 0#4 Mail 40 cv ask
1-
is Is, to 1% at
It -T --- 0 x 9 1 w"
Ot g g 6
itWki
of 4000 Of 0 We 0, OL 0', 4Qait0 0 wo 00 0 0 0 00.00 00 0
'
f'o Q
* Q OL 9 'S00 00
way

zeluovich, Ia. B., -'~n the surface tension of ~h,:- border of division of r.utually
soluble lie,,Ads. F. 931
The i.ordler of division of irixing liquids haa a p9sitive surface tension
(that is, h~~s the same sign -'as the non-mix-ing liquids have). T.I.Iis surface tension
is inversly pro-ort.~onal to the thickness of the layer of the mixture formed on the
border of division in the process of diffusion.and therefore decreases -Ath time.
Inst, of O'hemical Physics
Acad. of Sci., USSR
Oct. 10, 1948
SO: Journal of thysical Chemistry, (WISR11 23, No. 8, (1949)

11401 ON dw iq~ Won of Sq'614
H. Somw jAcad. &J, US,
Yvs, KAAX. 2j, 341-TRIML-
.011114# riWolon is Inda"d by omit whm twiv b No
9 as QW/WC200" k Is ewt., 0 (he bft( 4f twtbo.
it] Isa"M of the Rativ. a the 14wvt"y.
Saing pWWtIon, C, the but c*padty;-,A the hat
cond.. and 0 As bw 4. of the ctddW P!9dWq.' TlW
atibel" dbcnuv volt= through If P-A(fin"Wer
mm. Its) 00 usbuildne anit. of Nils decamial. m-,
sundes tbAt 23.0w cal./cad, are spent an The decocupil. I
The 9 w" Sodepewdout ON the no. Awl Of the leveh of t2W
%Wk gap. was pcom tiotW to C-'-" wbM C Vacicd IMM
OAX to U, OW W. what IrKruse-d with P (40-74M); It
a". e.g.. 0.11 of C - O.OWS and P - 40 an4 OMS at
C - 4 and P - 7(k). The tion was Applied to M1114.4
of CO (97-80%) with 0. (111r) W Ils (o-3%) -W t. Ils,
0, mists 0 A. Cs, and P weic e*W. Fair a (cm./sec.) of.
D*nkil (cad 81 111.1.
istbellcown.lu%. Thsm1c.RwavdtW.atjva(W-
7M. k Pic to be about 12 w, it. the cakd. mdkn R
of the sPhm raised by The spark to the dame temp. was.1
tin" as citat " the width I of the heated none In the
statkaurylUter, Tberulck-381sapprox,sotisfiedalso
by the expis-of Lewis and Vba 61W (C.A. 41. 7WJ)
wbase tbtwy Is hicavvec .. On pbotocra of the It
in CO-Itro, Mists. the MON of the Ftkusts =
was atxmt 1,3 R while the owrespondAnS sadius in CO~-Ifvo
atlitz. (qt the mame P), wa 0.7 R. flumrmdn

t4i 41- 1". "WAS "lit
Ipjam of *xPlowtv Salvoul miltur" In gh"It. wave*.
1
Y
Shl
i
kh
D
kkd
a.
nto
.
,
o
yAlt
y.
'
00 A 43 871-40010); cf. Z. and LcIpuo-,
4RIt'-Sl~k Wa mmit rApid twilng
skil
~.A. M
i ,
.
of the ext"Ve usixt. anti tfunufulle al(frAtimill rg
00 the chem. tkostripti. during the CN'40 MW
P
1n I=
=

00 coultilkatkilim due to CAt4lytiC AWI
T1
1
A .00
t4inistritent tutthull cif prothmsti; %i &Iwwk wave lit to dre
b
if
h
llel
h
h
h
0
-00
00 -A 'A
u
d t
roux
o
l
t
e pwomis mlitt, A
1.
:111. ~Vzt 1+1 d thi order ni Ili 440 The phoustrApIrt
/wc. itsiltrs a ittlit
the liclocily r - 2 kin
sell .
.
M r. fultIM-1, I",, trculiAliti Ili the iltuitiOn. At
Th,4t the Ignition, ii thtic t,oldy to the tbwk viuve, lcmled, .0
-rr to
1144 its heat livotfurrd by ftiviion on She bullet, Is Provo ileltit-itics diltifictly Krrmtr Miss the "tin. W HrC
*
,
IjC dAiLhe% latl break.
h
11119C %
.
J 1. 0, Which 6 d4j. jWqk,,htV,, thrle site jWt
[IV etpia. iallil a 11111it, C,44
taltdal
4-1) 4,6 insit. Wk% lonlirt at the mln~ r - 13M kjoilitus 14 %he t-oininmion. Ailh it fietWiWY r 4(
Irk the "' 'U + I'll 14 life lullit.; 0 1% a fum,110"
but vtbk,b a Inslict L4 the mint 0 X 11PIPM

lk Itils, is) tguite evitu at 7 - 17511 mitv., as thsi of the tjUts, a tA the dAt lilt of the Witt the 114rerso4oti-
rAlliset
:
10-
within lim Unsilis 0
in
i
t

300
0013 .
n
/e trilm
g
IwAt duc Its frielkni I# the mitir lit both ea". and the Im% inaltnitutle ti
Shwk wave Amplittlidst Is Krimict in the raw. %A the 04t. 0A1. rise ottwir Indridrot pheltimi'toom 14 the I"t
nI in
live I-ractitmi prodw
.
-mly I'T slit alkitit 11 jinvinte t4 the Airtz Tx tonr
014ml butirl, the likill It rViAt I'n y
ml wc~ A ofteralow. Alui Ind"tess
Irl. troot .4 th
wcthl In ti
t
unnin
In
li
INA "
th
wav
t
bkh o
'
e
i
t
.
0 4
e
e F
uty
i
f
d4ft of J'Alft. 9, the ttlop. ilitAll"l, asul thr "it'; I
lo A pelloilk. 0~ili is 0

4
A In
is I^ Initial d.), are. 21 to + th 4- TAI, IF I
7
1
%
S
- Jim, T - I "t
0
p. o, 42; 2C0 +
, p
at
OF (SAId. with lip
zi + 0# 79%, 13.1), 1.111 1%sliVrApIlk fro 0
t recording oil a tevisiving filin 4 it 111111ri firril ImiritinstAlly
through ON jailer oall. 11"Wing volkidly, frons Ili*
, ZOO
Witold up, at Lit- L-, Iminlilled licirs. ot lim
lbm lag r 0.1 the ignition; at r I&X? fro) Wo*
use

cl**

(*W 40 13111 an "V sit
9AL 41 two 4 4 lif*o"4 36,T,jlA5_.__
as pit" *0 sit Will Pill.
~
o *40
1
o a 0,0 o o 0 a a 0 0 0 a o o a a (it 0 o 0 o a 0 0 0 0 * 0 0 0 0 0 0 0 0 0 70i
0-0-0-0- 60
a 0 0 40 * a 0 * a 0 0 0 0 a 0 0
0 0 0 0.0 0 1A a *,0,0 0 0 0 4D 0 A 10 0 0 o1

Adkl1iads rtion of rsXPj bw" gat calstwoo. Va.
T. Gentian . Va 8, 1' (Mch, and A. 1. Rodo"ki!
Acad Sci U S S ---- 7J4k6w)-.'- Zkow. ivis. Miss. M.
b
l
h IY
l
a" tu
1 cm., In-
east
e (
g
ternal diam. 2.1 cm.), stated at the bottom and stoppered I
at the upper rad, was fitled with a gas inixt. at a low pmv-

and heated to tvalp. T. Then the stopper was!
wa, and the air rushing In compressed the mixt.
=
to at v PS (temporarily also to Walter Pressures)
and 4~40fin=ly mised its temp
to To (called
from Pat$- (by a device described) at a qonoli:4 mjwc. and the
.
.
sm'sequaticm). 'nsensixt.dWordidnotignite. lithe sksmovedin this agovensent.Witim amidtVi-ible br tormine
3fM
f 10
ft
d
h
k
/
=

Ignitim was caused by adiabatic heating only, the Hot -
tn.
o
.
e s
o
a in t
) at septe
Imatal vapor
The ladinction perlod of tlw ndxt. 211, + (14 is about 0.01
"Ignition'* from "no (gultion" in a PW UK $410 -
S
angast log 1- should be straight and have the taaVmt - sec. Coatroy to Rakipora. es at, (cf. prmtding abstr.)
(I Is the ratio of ttw heat especitin at coast. sphim"I detotualm of I in their expis, could not be
caused hy adialinfir heating. 1. J. Wherman
prtvme and mist. vol. Uxtrapolstion of this Hat to -
jil - p would givv,the ignition temp. Ti. The tbftwy
proven correct extept at very low P, at which the allaw,
'wits dild. with. rather than compressed by, air. Tiwu
5771 for 211s + Oj between p - 0.124 and Oa44 stmi
r
W70 for W
'D IS + 39% Ok,
+ 2Z% CS6 40D
- Th
40
d
f
49D f
I
M
O
or
or
approx.
,; an
e +
t.
e,
t
deth. of Tg for this kSt Mist. Was djSCUIt.r becou the
tubeburst. A deposit of KCI on tbeglasswa madvarta-
Han of the shape of the makil end did not &&ct 7-j.
Moving pictures showed that tbe stopm was withdruwn
film
221M

CA-
Slow propalcatim d darner In tultims. G. A. Bankil and
Y.. H. Zei'dovich (Aczd. SH. USS.R., Moscow).
8SD-W(l9W).-Wbrn gas In a hori-
mantal tube clased at one tati is Wttd at the opm tad.'
the thme famst'la concitive toward Ibc Iritwo Point.
This 6 so bemust of convvetim: hot 1% %h "I
Nawstwitatthe *r wull, vind The mhl P"11M down
tit tlW lKtitum 1=11far Which t1try, burn. ~ It a to the
IKWIIIAI VVIOCIty Of OAt"t (ilimilardhis corivKtion), w the
vOm-ItY of, am Parallel to the axis at a given point. wo the
test m Me. along the axis). S the ama o( the darne
r
.t. a" F the crams-section of the tubc. then the gas.
vrA. buming at any point Is mdS - (m + ss% - w)JF;
ni the bottoon wall v b neg. arAl the rate tit cumimsthan Is
awrot, Thr sbml* of the donte dependo oto the illitirn.
iiiis"Irm Witt WS/Op., g is amirmlim dur to gr-Ovily
itFut d i* Iliv diam. of the tube. 11te qttAlkml Itaitte'l
IL
Arc C(IIIIIIIrMl (m bunting mists of C) Cill with Ut
(11tersturr d4ta) when st vwini from Omto 50 tindsm,
lk"IyV Increstag in N Inay cause retsirtl4tion of Coltilmis.
1W. A IWIW (of drig. lk ItAfiw ffout Imin pbotft-
of the turns 6 41"Oritted, Phot Its of vibral.
Biktrmsn

2- ODE) I -it 0000101#91
Goa 4521o DETONATION OF 1i'-.DR6GEN AIR MIXTURES. Brodsky. A. H. and
I
60A
6*2 Zeldovitch, B. (ZhurDLI Fiz. Xhims, (Journal of Phytjioal Chemistry), 1960,
00A
*9.8 -7-78-786; abstr. in chem. abstr., 1961, vol. 45, 862)o The compositions of
0 0r the &&sea at various points on the ways front of detonations of H air minturej
u
0*0 and the atop wise kinotion ot the detonation aro calculated. Caloulations
000
&~rce with exporSmental data.
vie I I t!
LUNW-AL LITINA7141 CLAISWWATION
NVOW lifts#& it" 14*44T
VC 64j00,> 040 Cott, 0#4 4111$1 61C *-* 491
- I -I N 0 It 0 1 V 41 0 m 0 75 s I 'a
1) U a -A11aV1 rim -t
GIN
*0 0 a 0 0 * 0 0 * a * 0 0 : ~ * 6000,0 ooo*ooWioo* 004
. I I : : 0 to 0 0 *Go-go-** (., 6 0 9 10 0 *0 0 0 0 64 0.0 419 a *ad
00
I**
'00
-01
as*
Coto
ttoo

$41.127 64"
W*dm Magda- tlgit no vcwt~ .a
.Oa.wavts is. put wrward
of P04!4 zCkjovkh POLIts
tt4,v dta to
of 4110
06 dis A, SOKOLM' C051) lit forguation erm ilngc~,O#Vlmion
do Of 2 Oww' I=', attention to in *tkh tm
Zk. FAJPT. Tnw dmWs -A bif~ b*lm 'to
9014110'. is sea-wed S*WkIfk lu Unto tug wvxwt 11"I O&OK,
4 that a It&"% Ot"d of I% attfibuW4 10 'a It% womwo
pis w"WO 60'"tum am he unwat P, baW1O that tM Ti ..
f by wition of IM v0d " not a twn Of the
tho raw; Ww'd 11A shoa-w'" Ult ik bJ&
0" &rA b" Sokol
10 the Sato jo On.^ to that. hock is y use It, Ong woul, 0,
nw*Anhn ,,I
Zdty M.,kv "Ild've susoted
tm sagg"'VI It lomki'sm mifitht " ps, it It". tom do*"
&kb H 1,W4 rwm itself cak I of 4don'do". ,e in the &IOgg"
to dw so in I rw am&" shm-kwavel itto h%% dvo 'lot Of J*Kh
,00,0)l bys(I
In ttA tubV*%N- "W of wok I
(ame, by s0"% I'SM " PC vitt waadf
raffam 0 gicii(ronse Lt 2=
WAII dW Ur&srut Jowly A&I'le ouk Intatiots tV
Cdt
tw sw - ftnvA as
Odom$, consom Sok
,,,Watt*
don its IM mly 'imil all dw i-u -akcc carliff Of atom
"agma mcgi-IntlOg . u&--- -At this has
4=91im
OWIL.Vay, ~k tup umb! tw fts-c- ramber is not %h" 00
bOM obw"md.
into V*ve is wt up. sine,) ceaws"d SIbdkin bat for
adstolgaiiion14 ,.His-IOtTv, bc as a* o*
&OVO to dw PS ( Ito go. it wo,14 its &w in Ito gictow
~wd ewity 1A.M p--deo-All?" tMI do is Ito t%WY
with Ito f- 04
gr%PC04 on Ih6 themy, igga dw 4 tbo gavwvwly Ong is twiell I In 0,41 too" tonli tund fcnvunt4
W"m sivrox, OV witich Im f- a Id Vgoj. to hal
iii~ r, a wide tOS4 to dUW C'~~ _ -L
It, &tWMkll %Wl('fmnt' An,916CCOOn Jbil, in th"S ""Wk LO
Lac A. INCH"
it of it
r"j %be lim jItugv. dd-A"On
(c,tlr4)1 It (,,t that in this ictongion
jut,t6goed to I tcs a, OfKt of
-60. tao placv. I ignition *hcW of 0-
twouOt Stmt by ion of
4LO to the "Roc, n, of th, LVISIAW66
inw gatfs cd nw-W
On dw VAMW
tub.,

CA
mom
-1 il"plih
'AIM!
b =i.rslo S71;rj riOncl. 40
I
9crc,
-4
it no
rj
.9 El
tat
Ir

U5S�/Fhyaics Compton Scattering 1 Mar .52
"Polarization of Gamma Quanta During Compton scatter-,~
W) im, at 1800, Ya. B Zel I dovich, Corr Mem, Acad Sci
9*,
PDA- Ak Nauk SSSR" Vol 83, No 1, pp 63 -66
Considers the backward scattering of quanta polarizecL~
in a circie. Depolarization does not occur 'for any.
valtie of the quanta. Considers the scattering an
oriented electrons. The cross section of scattering
depends on the direction of rotation of the pol~ris-
tion plane. Proposes that'the scattering or ganm-
234T93
-data by magnetized iron be employed for meaburing.
q
the '.circular polarization of the gamma quanta. ~G:Lves
a descriptive explanation of the results obtained'.
Sub~aitted 8 Jan 52.
23~ 3.~'
C-)

L) V 14--- Vt
nuc litar ch-.rq-- t~ thm ba~4 -t; thr lu,-t mat trtz tiltd n,l e,
tyrm~ns i.d n~utm- r am, ~s, With-ut such pr~
nol, the
2ut if th~ -n h
ess li 1,

ZELIDOTICH, Ya. B,
111sobar of a Nucleon as an Intermediate State of the Beta Processes.." Dok AN
SSSR, Vol. 89, No Ij pp, 33-361 53.
Cor. Mbr,, Acad. Scips SSSR; Inst. Chem. Phys., AS USSR*
Four fermions simultaneously take part in beta processes. Author attempts
to prove deficiency of meson theory and to explain beta decay from viewpoint of his
isobar theory. Indebted to Prof. L.D.Landau and V.V.Sudakov. Received 9 Jan 53
259T74