SCIENTIFIC ABSTRACT SKOBELKIN, O.K. - SKOVELTSYN*, D.V.

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• Collection: Scientific Abstracts
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• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SKOBELKLTI, O.K., kand.med. nauk (Kalinin)
Surgical complicationo In ascarlasis. Mod. sestra 22 n,).IC,-.
30-32 0163 (MIRA 16t1.2)

SKOBELKIN., O.K. (Kalinin, 2-ya ul. Shevchanko., d.40, k-v.25)
.- - -- - Extenaive trawratiu- diaphragmatic hernia in a child. Vestn.
kh1r. Grekov. 90 110-4.91 AP163 (MIRA 17t2)
1. Iz fakulltetskoy khimrgicheakoy kliniki ( zav. - prof. A.G.
Karavanov) Kalininskogo meditsinskogo Instituta na bane Kali-
ninskoy oblastnoy bollnits7 No.! (glavny-y v-rach - sasluzbennyy
v-rach RSFSR A.A. Sokolw).

1 1 1 lit i v 1--~ I- 1. - qp "". . ...... 11 -.1-1... -, 1. 1-1. 1-11- -, ..". . , -
3 KO EK-,~LK 1:~`K -:anL;*. naWc (Kaiili-ln, 5, 2-Ya ulitza Shev--i-enko,
kv. 2 ; ~
C hol e d 0 c i-.cL oder-al fistulas. Vest. Khir. 91 no.I-C:113-114
0 1 63- (1-11-RA 17:7)
1. Iz fakul'tletskoy kh-irurgicheskoy kliniki (ispolnyayushchiy
ob~,azannGsul zaveduyushchego - dotsent N.V. Zavadovskaya)
K,tlLninol,oi,o r-raditsinskogo instituta (rokl.or - dotne-nt, A.1%
nil bnzu oblantnoy klAnicheakoy bollnitoy (glalmrj
vrat:h - zasluzhennyy itrach RZF31t A.A. Sokolov).

SKOBELEIN, O.K., kand.med,nauk
Revasculari7atica of -a mobilized stomacl: U:e ald of the
splenic artery. Trudy KGMI no.10:372-371." '63. 0, 11 ru~ -, C, . 1 )
1. 1z kafedry faku?",e skoy khirurgil (zav. ka-redr;-y ZaSILLZilell-
n.,rj deyatell nauki RSFSR - prof. V.S.Semenov) I kafedry tcral~,912-
noy khirurgii i anesteziologii Ukrainskogo tsentrallnogc, InstItuta
usovf--rshenstvovaniya vra(.-hey (zav. kafedroy - prof. A.A,Shalimc,,r)U

L 202ZO-~2 A"
ACCESSTON KH: AM4045869
Vo 00/001/1(oavloa
SOUCE: Ref. sh. Biologiya., SmIn-IC11 tons, Alba, J#J~M%i
AMHOil: Skobalkin,, 0, K,,
TTTLE: CL-cular defeat eaophagoplasty wltlh a stoomkoh sm.ablon cin a
,tascular pediols
CITED SOURCE: Sb- 3 Vaes. konterantal po vierg 8 lp!1122~'41; may I
or mov, 1963 yerevmn, 19&TFT,751

Ard doO 1t; 1
TIRAMSLATION: In exp(ji-Imentis mit la dog cddav~rd
was drinonstrated that it is more offeative to makh a al-himach tubo
resect-ton from the large eurvature of the atomadli Uujume of itli
8rcazer length and size and higj4ly audoquaits ritumbeir of vsssels,j After
mobilization and spleen remavml, the Vascular arathda, Rode it POOSLUIS
to bring the transplant into the thoracia cavity' L;o the lairel of' the
arch of the aorta and hip~aer. The distal end of the tr=,sp1ant

L 20270-65
ACCESSION NR
AR4045869
started 2 to 3 am hlgftor than Vie pylaoua awl the
-0 64-- evindal varb of tbo stoinach. An ingi J,
6111, 1!, OM

d1aphr1kgM'OpG=n
resultse
---
------ ...

SUB CODES.!: LS EMOL: 00

Card 2/2

Examination of labor disputes in the factory and plant local
committee. Okhr. truda i sots. strakh. 3 no. 10:65-67 0 160.
(MIRA 13:11)
1. Zaveduyushchiy yuridicheskoy konsulltatsiyoy UllyanovBkogo
oblastaogo soveta profsoyuzov.
(Ullyanovsk Province--Grievance procedures)

I'31KOBELKIN, V.
Seasonal and temporary work. Okhr. truda i sots. strakh. 3
no. 12:62 . D 160. (MMA 13:12)
1. Zaveduvushchiy yuridicheskoy konsulltatslyey U11yanovskogo
sovprofa.
(Iabor laws and legislation)

GYRS[WIOV, To.; SKOBEMIN, V.
Commission for labor Disputes at enterprised and inatitntions. Sots.
trud 5 no.1:140-145 Ja f60. (1411A 13*-6)
(Grievance procedures)

SKOBELKIN. V.
Printing estab2ishmenta are needed by Armenian industries. From.
Arm. 4 no.5:21-24 I,V 161. 0,13A 14 t8)
(Armenia-Frinting industr7)

SKOBELKIN, V.
Consulation by the Ullyanov Province Trade-Un-ion Council. Okhr.
truda, i sots. strakh. 4 no-5:53-54 My 161. (MIFA 14:5)
1. Zaveduyushchiy yuridicheskoy konsulttatsiyey Ullyanovskogo
oblsovprofa.
(Labor laws and legislation)

SKOEELKIN, V.
Is the court right? Olkhr.truda i sots.strakh. 5 no.4t42-43
Ap 62. (bgRA 15:4)
1. Zaveduy-ushchiy yuridicheskoy konsulltatsiyey U11yanovskogo
oblsovprofa.
(Maternal and Want welfare) (Employeea, Diamisadl of)

.. .... ......
SKOMLKIN, V.
Visiting our friends in Azerbaijan. FMm.Arm- 5,n"o.6:75-76 Je 162,
(Mil", 15:7)
(Azerbaijan-Economic conditions)

SKOBELKIN V.
~-- . - - -
Liability responsibility of the person reponsible for an
industrial acciedent and illegal dismissal. Okhr.truda i sots
strakh. 5 no.10:42 0 162. (MIRA 15:11)
1. Zaveduyushchiy yuridicheskoy konsulltatsiyey Ullyanovskogo
oblastnogo soveta professionaltnykh soyuzov.
(Employers' liability) (Employees, Dismissal of)

SKOBELKIN, V., kand.yuridicheskik-h nauk
Procedure for bringing a damage suit against a defendant who caused
an industrial accident. Okhr. truda i sots. strakh. 6 no.9:43-45
S 163. (MIRA 16:10)

SKOBELKIN, V. I.
and A.G. Shafigullin- authors of a-
Review & Smwnry of "Theory of Chain Processes" by N.S. Akulov State Pub. House of
Tech ?A Theoret. Lit., Moscow, 1951,
Zhur Fiz Khizn, Vol XXVII, A, PP 151-2
W-30868, 18 Auff 51,

r-7' n

SKOBELKIN, V. I. Sr. Sci. Colleague
"Some Questions of Non-Linear Electrodynamics,," a paper given at the
All-University Scientific Conference I'Lomonosov Lectures". Vest. Mask. Un.,
No.8., 1953.
Trabslation U07895p 1 Mar 56

-1. 17~-tO.-DEQ---Dl, V. I,, 31LIFTOTILIVI, A. rl,
2. ussm (6r2o)
4. Akulov, Nilcolai Sorgeevich
7. N. S. Akulov's book "Theory of chain reactions." Reviewed by V. I. SkobeLkin,
A. G. Slinfipillin. Zhur. fiz. khim. 27, no. 1, 1953.
9.- Monthly List of Russian Accessions, Library of Congress, may -1953. Unclassified.

USSR/Physics - Vacuum pump FD_lC93
Card 1/1 Pub. 153 - 19/24
Author Skobelkin, V. I., and Yushchenkova, It. I.
Title Theory of tLe vapor-jet vacuum pump
Periodical Zhur. tekh. fiz., 24, No lo, 1379-1891, Oct 1954
Abstract The authors investigate the interaction between the gas to be pumped
out and the supersonic vapor jet. They clarify the mechanism governing
the process and thus are enabled to calculate the speed of pumping out
of the gas and to determine the influence of the various parameters upon
this speed. They note that their results differ from those obtained by
the USSR authors Lifshits and Rozentsveyg (ibid., No 8, 1952).
Institution : -
Submitted : April 3, 1953

A
5086. -Oil N. S, Milll'IYN flleu~y of
_
-
j
1 27 Na,
V. 1. SKOHELM IN. A. dkyprr, le(
r. P
400)

A clificism of tbt~ 1heorl Ill
Divils:iia paper.
kinetics of chemical rcufl* pitiblishoJ W
Tite futulmlientais of cbMdea~ i1prarrivy [A(CAJ, J.
Moicow, 19401 and Thr threiry ;a/ 04tht prvrv.,:-,~r
(Gild, M.-L., 19511, which, in 1plaut of the U%v (it
s- aciflull,IproptM4 OTI Cl(fim-mlori for the im tc of a
ilia j
*
Raclion dt:pending explicitly on; time and implying af
A)xord-: `ij
ing to Skot4lkin dim pb~noiu~na
arc tiltimly the Ivitill-i of niattictnafiml errom
IV. 1, 3%YIATIJ'411~~

j

. .... ....... ......... ....... .....
- ---------- - -- -- -------
14F,
:6733. Dircrangency in nim-IftKar 4:Wrodpwiden.
V. 1. SKOULKIN, A. Ayper. ieor. F7z., 27. 111o, ii
It is phown that aniong all the non-linear systentt of
c1ccirodynarnks that of Born-Infeld is the only one in
whi h birefringency is abscra In directions normal to
C
the collinear elect romagnctic fields. It Is also shown
that the light may, in-it non-linear clectrodynantics, in I
general be rcsolved into four componcrits Rawly,
polarizcd in four different planes. B. F.
00
t lump. 111"m

Category USSR/Atomic and molecular PbyGics - Gases D-7
Abs Jour Ref Zhur - Fizik&, No 1, 1957 No 932
Author Skobelkin, V.I., Yushchenkova, N.I.
Title rrecti6ns to Article "Theory of Vapor-Jet Vacuum p."
Pam
Orig Pub Zh. ti--khn. fiziki, 11955, 25, No 2, 66
Abstract Refen; to Ref. Zhur. FIz. 1955~ 8952
Card 1/1

U SS Rj
5---9-3-(1-9-5-!;-) in-R-
The variational principla of magrictostaticn with
ferromagnefics in the field of efecirk: currents is
formulated, hviding to a solution of the general
Problem which could not be obtained by integration
of MaxweVs equations owing to the non-lincar
relation between B and H. A sysftm: of xxial sym-
metry is first comidered. and then a planar system.
Vic authors then -derive 4he "complete &systrm" of
functions and introduce direct methods ol7determining:
the magnetic flux. E:xcTiucALKmAKc:rtAssom-rtoN
JIM INIFIR E, I
- - IIV I Iff . .......

SU3JECT USSR / PHYSIC3 C,.RD 1 2 PA - 1,537
AUTHOR SKOKLKIN, 7. 1.
TITLE On Various P~rinciples in Hydrodynamics
PE11IODICAL ~urn.ek3p.i teor.fis,31, fasn-.2,317-321, (1956)
Issued: 5.10-1956
In the aorks by several authors the variation functional contained some field
parameters which were then varied independently (density, velocity, pressure,
and others, eg. density and stream functions). Tlowever, the number of para-
meters used on this occasion is not minimal. It is shown that for the construction
of the functional in the -eneral case of a threedimensional motion two defining
quantities of the field (stream-functions) suffle-3.
The principle of the lowest flow potential: 7 are assumed to be the parameters
for the determination of a certain streamline of a steady hydrodynamic field.
An orthogonal turihedron I i is constructed at each point of the streamline, and to
each trihedron an energy-momentum-tensor T ik is assignear The quantities
'f(xi), /V' (xi) of the field satisfy the relatione
Q7I . D(31, ,~QID(x 2fx3); QV2 - D(T,,5-)/D(x 31 Xd; QV 3- D(V,'; )111)(x1x2). For the
modification of the mechanic energy in a real steady field along the streamline
it is then true that: aT / - 2/2)+ Here R
f klaxkdS - (V
is the work of friction forces per unit of measure of the liquid. The LAMMIAN
is L = T Ss and the integral I = f Tss dw must be extremal for a real stabilized
sa

Zurn.eksp.i teor.fis,31,'Lasc.2,317-323 (1,056) CARD 2 / 2 PA - 1537
field, Herefrom follows:
aT ss /n -(alax ia) (aT 88 /(av,/axi 0; aT ss /a !~ -(alaxia)(aT ss I(OA-,~157j)) = 0.
Next follows the relativistic generalization of the principle of the smallest
flow potentia 1 for a stationary field. In relativiotic bydrodynamics it is
true that T (P+Qc2)U U +P6 Here u. is the four-volocity of the gas
ik i k ik' I 2(p+Qcl) VI + p.
motion. It then applies that: L = T29 t- P
The unsteady field: The principle ot he smallest action. Here three "stream
functions" T,,tr, a are introduced in the fourdimensional space-time-manifold.
For an ideal gas it is true that L - P + (WO 2) + QU2. The variation principle
consists in the fact that the integral S T- - asa'F/axi , a a xi, a Cr/a xi)d
ss
for a real field assumed a stationary value.
In conclusion the existence of a strong minimur. for steady adiabatic subsonic
motions of a gas is proved.
INSTITUTION: 'Moscow State University.

SUBJECT USSR / PHYSICS CARD 1 / 2 PA - 1218
AUTHOR _SKOBELKIN, V.I.
TITLE The Principle of the Smallest Flow Potential.
PERIODICAL Dokl. Akad. Nauk, 108, 787-790 (1956)
Publ. 6 / 1956 reviewed 8 / 1956
The present work establishes and formulates a variation principle for the
solution of various boundary value problems of gas dynamics by means of new
and partly direct methods. The parameters 7 and ~' are assumed to define a
certain streamline in a steady flow of a perfect gas. The surfaces 7 = const
and 115' = const form the flow surfaces. 7 and 0- are chosen in such a manner
that QVx . D(1F,n'j)/D(y,z), QVy= D(IF,,~-)/D(z,x), QV, - D(1F,N')/D(x,y).
The couple of functions (7,, ) may be considered to be the flow functions in
a threedimensional motion. The continuity equation div Q V~= 0 is satisfied
identically for any 7,;~. If on a boundary surface a the distribution of the
flow (the distribution of T and ) and the distribution of the total mechan-
ical energy E (T,qc,~ referred to units of measure of the gas are known, the
BERNOULLI equation has the form (v 2/2) +f dP/q Here P is `.-he
gas pressure, and integration is carried out along the streamline. Further-
more, it applies for the energy theorem (i.principal theorem) that
dQ = dU + P d(I/Q). Here Q denotes the quantity of heat and U the inner
energy. .
if T and-.~' are varied within the domain 2 (in which the motion of the gas

Dokl. Akad. Nauk, 108, 787-790 (1956) CARD 2 / 2 PA - 1218
has no strong or slight discontinuities) while their values are maintained on
the surface a the following principle of variation applies for the motion of
the gas in ')e : The integral I (p+QV2)d u.) , which is equal to the work
performed by the entire impulse flow of the directioned motion of gas (flow
potential), assumes a steady value in the case of an actual motion of a per-
fect gas which has become steady.
We now introduce the eometrical characteristic of flow:
9 = (D(1F,,15_)/D(y,z))5+ (D /D ( z, x) )2+(D(T,k-)/D(x,y))2and restrict our
attention to the motion which is barotropic for a given gas particle. The
OSTROGRADSKIJ equations corresponding to the equation 61 - 0 are given,
several times transformed, and specialized for an adiabatic motion. It is
shown that, in the case of adiabatic subsonic motions of the gas (which are
usually vortex-like), the solution of the equations represents a sharp mini um
of the functional I. Proof bases upon WEIERSTRASS function of the calculus of
variations, and is followed step by step. In the case of a subsonic motion the
phase surface Z=L is convex, but in the case of supersonic motions
without strong or slight discontinuities the phase surface has a saddle at all
of its points. If boundary conditions for 7 and on the surface a are given,
there is only one solution.
INSTITUTION: Moscow State University "M.V.LOMONOSOV"

7 IT,
I 24-11-12524D
Translation from: Referativnyy Zhurnal, Mekhanika, 1957,Nr I I, p 31 (USSR)
AUTHOR: Skobelkin, V. 1.
T IT LE: The Principle of the Minimal Stream Potential and its Application to
Problems in Gasdynamics, Electrodynamics, "and Combustion.
(Printsip naimen'sheg6 potentsiala toka i yego prilozhenij- kzadacharn
gazovoy dinamiki, elektrodinamiki i goreniya)
ABSTRACT: Bibliographic entry of the Author's dissertation for the degree of
Doctor of Physical-Mathematical Sciences, InstitLte of Mechanics,
Academy of Sciences, USSR, Moscow, 1957.
ASSOCIATION: Institute of Mechanics, Academy of Sciences, USSR, Moscow
Card 1/1

D-c
CC, 3-~ 0 1 i'-! -T
195~
Ily
2" op ~-~~d Sci
21-22
ri
Sil -

AUTHORS: Kogarko, S. M., Skobelkin, V. I. SOV/2o,12o-6-32/~9

TITLE: Relaxation Interaction Between Shock Waves and the Combusti~a
Zone (Relaksatsionnoye vzaimodeystviye udarnykh voln s zcnr,
goreniya)
PERIODICAL: Doklady Akademii nnuk SSSRO 1958, Vol 12o., lir 6,
pp 128o - 1203 (USSR)
ABSTRACT: The paper under review presents an investigation of the ir-
fluence of the kinetics of the combustion upon the structure
and the intensity of a shock wave when it passes through "he
(the period durlng
combustion zone. The relaxation time t
r
which no noticeable influence is exerted upon the diffusion
currents and the heat currents in the reaction zone by the
reaction conditions suddenly modified by the shock wave) is of
the same order as the reaction period V (10-3 - 10-5 sec),,c
is defined as the ratio of the width of the combustion zone
i and the normal expansion velocity of the flame. During t
r
the temperature and the pressure within the reaction zone 11n-
Card 1/3 crease. During the relaxation time the excess momentum in the

Relaxation Interaction Between Shock Waves and the SOV/2o-12o-6-32/'59
Combustion Zone
reaction zone is tranaformed into a ohock wave propae-ating
forward and backward from the reaction zone, Equatiors giving
the state in the shock wave are written down, The whole amount
of heat liberated In the passage of the shock wave is expended
for the iricreaoe of the internal energy of the gas ir. tho
veart Lori zorie.~ Vb donotes the diirtation of the pass_-w:e of th&
ohock wave through the combustion zone, IfT_ the reaction
b
is not completed during the passage of the wave through the
front of the flame and only a certa 4
I In proportion of the
chemical energy which is expended for the Increase of the
momentum of the wave is Imported to the wave. If't' ~'rb the
reaction is completed within the periodr . The total momentum
of the shock wave after passing the combustion zone is combined
from the interest momentum I and the relaxation momentum I.,
The maximum amplification of the momentum of -the shock Nave at
b may be termed momentum resonance. Finally a method for
Card 2/3 the determination of the index of refraction is presented,

Relaxation Interaction Between Shock Waves and the SOV/2o-12o-6-32/59
Combustion Zone
There is 1 figure.
ASSOCIATION: Institut khimicheskoy fiziki Akademii nauk SSSR (Institute of
Chemical Physics AS USSR)
PRESENTED: March 6, 1958, by N. N. Semenov, Member, Academy of Sciences,
USSR
SUBMITTED: February 25, 1958
1. Shock waves--Analysis 2, Combustion-.-Analysis 3 , Mp.the
Card 3/3

" ( 4 ) , 2 4 ( '~ )' SOV/2u- 122-3- " j/`~7
_'XTHOR: Skobelkin, V. 1.
TIT LE: ~the ~Therm~cjynamic Equilibrium of the Surfaces of a Stron,.;
Explosion (0 termodinamicheskom ravnoveeii Poverkhnostey
.lillnogo ra-.:ryva)
PERIODIC,%L: Doklady Akademii nauk SSSR, 1958, Vol 122, Nr 3, Pr 431-433
(USSR)
ABSTRACT: In hydrodynamics, the problem of the thermodynamic equilibrium
appears as often as a variation principle is formulated for
the description of the Cas motion. The infinitely small de-
flectiornfrom the actual motion for given boundary and initial
conditions must satisfy not only the raviation equation -uhich
is equivalent to the equation of motion but also to the
variation equation AQ - T6S = 0. This equation is equivalent
to the second law of thermodynamics for a real state of a
Jas in thermodynamic equilibrium. The above-iven equation,
therefore, limits the class of the permicovible variations.
This paper deals with the greneral case in which the -as moves
in the presence of a shock wave or of a oharply defined front
Card 1/3 of reaction (which divides the initial gas from the burnt

SOV 12o- I 22-7-7o/57
the T;e:,.-,1o!Jyn,-T-.ic Equilibrium of the Surfaces o-F a Stron- 7xrlosian
L
.,as). The laws for the conservation of r:iaSS, MOMentum, and
ener,-,,ty are 4-iven explicitly and then the !TU,-oniot (Gyugonio)
e~iuation is derived from them and a variation equation is
1 _~as. ~'o 'his
J:ven for the real subsonic flow of an ideal g - U -
variation equation, the initially ;iven variation equation
21q - T63 hao to be added. As an example, tho author inves-
tigates the subsonic flow of a perfect r-,as in a tube in the
presence of a flame front which propa,;ates with a Given
velocity in an isentropic f-as with a ~Jven Poisson (Puasson)
constant. A fil,,-ure shows the Hu,~nniot adiahates for the
2hock wavefor the detonation wave, and for a weak defia.,_~ra-
tion. :'.. ccording, to the deliberations of this paper, the model
of the motion of 2 incompres!,ible liquids does not satisfy
the equation of the thermodynamic equilibrium of the flame
front. If, however, the f-as moves in the presence of a shock
wave, Cie non-equilibrium conditions in a transition layer
of the order of the free length of pat1h of the gas molecules
has to be Investii3ated for the determination of A Q of an
elementary particle behind the shock wave. "here are 1 fi,,rLre
Card 2/3 anj 12 references, It of which are Soviet. L,

SC'N",12o- 122-3-3 / 57,
On t,'-,e Tliermorlyziarndc Equilibrium of the Surfaces of a Strong Exr1o.9-ion
ASSOCIATION: Yoskovskiy ~osudarstvennvy universitet 1,:. V. Lomionosova
(Moacow State Univernity imeni 1,.1. V. Lomoriosov)
PRESEN7'ED: June 30, 1958, by S. A. Vekslhinskiy, Academician
11
SUMITTED: P!ay 20, 1958
Card 3/3

5(4), 10M FOV/2o-122-6-25/49
AUTHORS: Fogarko, 5. 1M., , Skobelkin, Kazakov, A. N
TITLE: The Interaction Between Shock Waves and the Front of a Flame
(Vzainodeystviye udarnykh voln s frontom plameni)
PERIODICAL: Doklady 2.kademii nauk SSSR, 1958, Vol 122, 11r 6, pp 1o46-1048
(USSR)
ABSTRACT: The present paper investigates the intensification of shock
waves in their interaction with thefront of a flame by
variation of the normal combustion proces2 in the shock wave.
The length of the shock wave is assumed to be sufficient
in the direction of the reaction zone. For the interaction
between such a shock wave and the flame front the following
applies: I,' The shock wave is transformed at the flame front
(like on the boundary dividing two media). In this way a re-
fractcd and a reflected wave are formed. The flame front can
by approximation be considered to be a contact-discontinuity.
The expressions for the refraction coefficient are written
down. 2) When pasaing through the flame front the shock wave
compresses the Cas in the reaction zone, whereby temperature
Card 113 rises. 'fhis temperature rise increases reaction velocity, so

SOV/20-1 22-G-25/4)
The Interaction Between Shock Waves and the Front of a Flame
that the propagation velocity of the flame is also increased.
This propagation velocity increases very rapidly, and tAhere-
fore this process may be looked upon as a 3ort of explosion
in the gas current behind the shock wave; it causes the forma-
tion of 2 additional (intensifying) shock waves. The shock
wave front noves with sub!3cnic velocity in relation to the
disturbed ~,,as, and therefore any kind of disturbance is able
to catch up with this front in the current behind the shock
front, thus cmnging its structure. The propagation velocity
of the flame is not increased immediately upon arrival of the
shock wave, but only after a certain relaxation time. The
latter is of the same order of magnitude as the duration of
reaction. A diagram schematically shows the intensification
of the shock wave when pas:7ingr through the flane front. Ex-
pressions for shock front calculation are given. The new pro-
paGation velocity of the flame is calculated according to
the theory developed by Zelldovich. rhe amplitude of the
intensifying shock wave depends upon the amplitude of the
initial shock wave as well as on the kinetic properties (re-
action velocity, calorific value, activation energy, etc.) of
Card 2/3 the fuel. '.he second diagram shows the amplitude of the inten-

SOV/2o-122-6-25/49
The Interaction Between Shock Waves and the Front of a Flame
sifyin '- shock wave of compression in the reaction zone for
2 different propagation velocities. There are 2 fi,-,ures and
5 Soviet references.
ASSOCIATION: Inatitut khimicheskoy fiziki Akademii nauk SSSR
(Institute for Chemical Physics of the Academy of Sciences,,
USSR)
PRESENTED: June 21, 1958y by V. ff. Kondratlyev, Academician
SUBMITTED; June 11, 1956
Card 3/3

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240)
AUTHOR:
TITLE:
.. . ...... .. . . . .. . .
SOV/20-128-2-16/59
Skobelkin, V.I..__
On the Function of Magnetic Flux in a Three-dimensional Field
PERIODICAL: Duklady Akademii nauk SSSR, 1959, Vol 128, fir 2, pp 280-283
(USS'a)
ABSTRACT: In an article by V. I. Skobelkin and R. N. Solomko (Ref 1) a
principle of variation wasformulated according to which a method
was devised which permits an approximate solution of boundary
problems of two-dimensional and axially symmetrical ferro-
magnetic systems within the current field. In both cases, the
field was determined by one single function of the magnetic
flux I (which is similar to the method employed in hydro-
dynamics). In the case of two-dimensional ranges, in which
magnetic permeability is constant and no currents are present,
the function of magnetic flux may be regarded as the imaginary
part of the complex potential (which satisfies the conditions
of Riemann-Cauchy). In the general case, two everywhere steady
functions + and 1~ of the magnetic flux are to be introduced
for a description of the three-dimensional-,field. The latter
Card 1/4 are connected with the magnetic induction B by the relation

SOV/20-128-2-16/59
On the Function of Magnetic Flux in a Three-dimensional Field
B = 7+XV4. The planes const and 4 - const are the Planes
of' magnetic flux. The intersections of any two planes ~ and 4
form force lines in the field. 'Nith the help of the functions
and ON it is possible to plot a LaGrangian for the three-dimen-
fjional field, and the variation principle formulated in the
afore-mentioned previouu article can be explained for the
general case. For the plotting of the Larraneian the "vector of
magnetic flux" it = (1/2c)(+V-&--&,V+) and-.14e "density of the
potential function of the currents" u - -jR are introduced,
where denotes the vector of current density. If the density
of magnetic energy of the field is expressed by
w = ~B2 IT
0 H dl, L = w + u holds for the Lagrangian. The varia-
tion principle may be formulated in the following manner:
Among, all solenoidal fields of magnetic induction possible
(when the given boundary conditions for the real field of the
closed magnetostatic system are satisfied), the space integral
E = ~a L do~3 assumes the least value. The mathematical formula-
Card 2/4 tion of this equation is reduced to the equation SE = 0 under

... ... . . . ..... ......
SOV/20-128-2-16/59
On the Function of Magnetic Flux in a Three-dimensional Field
the condition div B 0, which is satisfied in a similar way if
,~ and 4 are chosen as the field-determinant quantities. L may
be expressed by B2 2
L = - -L +
J and it
2c 4!,-L ~ _2Y(B2
is possible to choose such a plane 6 that n A 0 holds. n de-
notes the normal on those planes on which the magnetic per-
meability 14 or the current density j are unsteady. As a result,
elliptical equations are obtained for the determination of."The
and i% as well as the pertinent natural boundary conditions
above equations fort and -(~ determine the projections of the
curl of magnetic field strength to the lines which are per-
pendicular to the surface of magnetic flux. To prove the exist-
ence of a distinct minimum of E and of the exclusion principle
for the field 5trength T?, the weierstrans function E of the
variation problem must be constructed. The article is concluded
with a discusaion of the required conditions. There are 6 ref-
erences, 5 of which are Soviet.
Card 3/4

SO'1/20-128-2-16/59
On the Function of Magnetic Flux in a Three-dimensional Field
ASSOCIATION: Uoskovskiy gosudarstvennyy universitet im. M. V. Lamonosova
(Aloscow State University imeni M. V. Lomonosov)
PRE3ENTED: May la, 1959, by S. A. Vekshiriskiy-, Academician
SUBMITTED: MaY 18, 1959
Card 4/4

24(5) SOV/20-128-3-22/58
AUTHOR: Skobelkin, V. I
TITLE: Propagation of Vector-Waves in Nonlinear Mesodynanics
PERIODICAL: Doklady Akademii nauk SSSR, 1959, Vol 128, Ur 3, PP rill-51-
(TJSSR)
ABSTRACT: The nonlinear mesodynamics of the scalar and paeudosc&!A.r
field was investigated in an article by D. I. Dlokhintse-
The generalization of linear vectorial mesodynanics rono:,~r,:,
in an investigation of the arbitrary function t ~N2
_
*
LQ ) + I of the three Invariants
E 1 ,
j- (
_L_ (,,;2 - B2), ig ( T2 - A2), (where it holds:
8TI
k
= 2-njic/li) instead of the Lagrangian L + + I (whero I
o
denotes the invariant part of the LagranZian, which
the interaction of the meson field with the nucleons). The
equations of the nonlinear meson field may be ascertained from
the variational method 6 div = 0. They have the form
1 al
L g + 2 4
1. .1 0~
curl H -
l
A
0
=
.
4nj , cur
,
at 7 7r.
a at 0
div ~ +k 2 T0 = 4nQ, div 1.0, 1-curl _T, 1-4n IL +

Card 1/ 4 0

Propagation of Vector Waves in Nonlinear Mesodynamice SOV/2o-128-3-22/56
. 14 ILI +8K(jj) jL-
+ 8 n (I + 4n 4
H a
a~ a al
81 -to 8L al
- 4n I I it - - -Z' T
IT _-~ a ~ IJ
The totality J, iQ (where Q denotes the density of distribution
of the electrons) forms a four-dimensional current which satis-
fies the equation of continuity 29- + div 'j -- 0.
The velocity of propagation of the at small distiitbations of
the meson field may be calculated by the method of character-
istics (e.g. by the method of Y~eak unateadinesses b~ Levi-f"_`7ita
(Ref 3), or by the method of wave equations (Ref 4) . All
these methods are adequate and deliver the same formulas for
the velocity of propagation of the disturbances. The following
expression is obtained from the above set of equation3:
cvx n + X-V 0, 04- A,n v 0, where it holds:
r aB I
-11 = [v
A-V - 2
L.-a _tj D
B
The vectors XE, X-t, X- are the vectors with the componant's
4 B D_,,.
Card 2/4 XHx 9 AHy' XH z , etc, and n denotes the unit vector perpe-ldicu-

Propagation of Vector 'Naves in Nonlinear Meaodynamios 3OV12o-129-1--:" !:`
lar to the surface of weak un34eadiness. Fuzrther4 t~a fol2r."..
ing relations are obtained: A-�n X--n - 0, X- x n - 09 a7v~
D A
V -L + 8, -LL
at
E -LL -
[a IL
of this set is equal to zero, which leadc tc
The determinan
an algebraic equation of fourth order with respect to v. Tho
only nonlinear mesodynamics which does not exhibit double
refraction or polarization of vector w.%ves iij the directionj
perpendicular to the collinear fields E and H has the form
L - C (1 - 1 - 8T( - a ' + C-,, rhere C and C, in general
4n D C2
are functions of Hence, experimental investigation of the
polarization of vectorial meson waves may indicate the physical
reality of the electrodynamics and mesodynamics of Bonn-Infeld.
If the mass and charge of the meson are known, the actual
field radius and the maximum field strength may be determined
Card 3/4 in this nonlinear mesodynamics. There are 5 Soviet references.

Propagation of Vector Waves in Nonlinear Mesodynamics. SOV/2o-128-3-22/58
ASSOCIATION: Moskovskiy gosudarstvannyy universitat im. M. V. Lomonosova
(Moscow state University imeni M. V. Lomonoso-r)
PRESENTED: May 18, 1959, by S. A. Vekshinskiy, Academician
SUBMITTED: May 18, 1959
Card 4/4

S/020/60/130/05/016/061
AUTHOR- Skobelkin, V. I, BC13/90-14
~"'PPLE. Variational Principles of the Deterpination of the Pi:incipall
CharacteriBtics of a FerKoaajEn ctbody on the Basis of the
~q_
Calculation of Its flys~7e~esis Loop
PERIODTCAL: Doklady Akademli nauk SSSR, 1960, Vol 130, Nr 5, pp 1012-1014
(USSR)
ABSTRACT: The theory discussed in the present paper permits a quantitative
calculation of the configuration of the whole hysteresis loop.
Furthermore, it connects the pr 'operties (constants) of the
ferromagnetic body with the shape of this hyate.-resis loop.
In the case of irreversible magnetization the entropy S of
a ferromagnetic body varies, so that the process of magnetiza-
tion is to be described by the use of the seconi law of thermo-
dynamics. The existence of magnetostrictive phenomena in a
ferromagnetic body changes its surface a so that in this case
an improper problem of variation (with variable limits) is
obtained~ Here, the field is assumed to be detarmined by the
Cartesian coordinates Y., Z~ x, t~ V are chosen as independent
Card 1/5 coordinates~ In this case, the variational equation of the VI,/

(A60
Variational Principles of the Determination S/020/60/130/05/016/061
of the Principal Characteristics of a Ferro- 13013//-B014
magnetic Body on the Basis of the Calculation
of Its Hysteresis Loop
field reads !i(Y,Z)=6E a + 6 S d 6) L+ D(Y.Z 6(1~4)dx - 0.
D(i~ pi~
I denotes the boundary of the surface a, L w + u
d) -#-
B d"fl the generalized Lagrangian of the field, and it holds
TrI 'B'
that d9 is equal to the magnetic pressure
0 A
acting upon the surface 0 of the ferromagnetic body. 6E de-
notes the complete variation in consideration of the variation
in entropy and in the magnetic induction flux an the surface 6.
The above equation is satisfied with any surface I irrespective
of its variation during magnetization. The variation in a is
to be considered by introducing an additional condition inferred
Card 2/5 from the second law of thermodynamics, The entropy variationy"

Variational Principles of the Determination
of the Principal Characteristics of a Ferro-
magnati.r. ,ody on the Basis of the Calculation
of Its Hysteresis Loop
S/020/60/1'301'0:~/C! "J'/061
entering into the above equation must vanish for a tr,.,? state,
The infizaitely small deviations from the true state may be re-
garded as possible non-equilibrium states of the ferromagnetic
body. With 6S = 0, the positive magnetic flux through %he
surface a has a maximum. It further holds that (1+ f3oEld,
with 1~ = 1 for
f B n ,, 0 and with E, - 0 for n < 0. In the gene-
ral case, the thermodynamic potential of the unit of volume
of a ferromagnetic body reads ('m) + 6 - -g m- -H2 + 8 -
0 an 8n Mel
6e1' H denotes magnetic field strength within the ferro-
magnetic body, N1, the magnetization of the unit of volume,
~an anisotropy energy. 68 1. ,lastic energy, and Sm. 3agnet~_"_
elastic energy, ~ is explicitly written down for nn.~'axial
an +
Card 5/5 and cubic crystals., If 4p is assumed to be a maximum, it holds,

Variational Principles of the Determination
of the Principal Characteristics of a Ferro-
magnetic Body on the Basisof the Calculation
of Its Hysteresis Loop
that 6 (-H4+ O~M) n dc+ - 0
S/020/60/130/05/016/061
B013/:BO14
with the auxiliary conditions
uik A UA denotes the deformation tensor of
the ferroma body. With V0 + i~ (where ito is the magneti-
zation determined by the initial magnetization curve, and A the
deviation of magnetization in the inverse process as a result
of hysteresis), it follows from the equation 65 - 0 that either
dS/dll+ - 0 (initial magnetization curve) or 61j+ - 0 (metastable
states corresponding to hysteresis). The hysteresis curve ob-
tained corresponds to the metastable states possible within
the range of irreversible magnetization. The conditions for
adiabatic insulation of the system are satii.-_ed. There are
5 Soviet references.
ASSOCIATION, Moskovskiy gosudarstvennyy universitet im. M. V. Lomonosova
Card 4/5 ~Moscow State University imeni M. V. Lomonosov) V

o
z

WO r
L: 01

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to
0
-:a Corr.
tioll
t4
ic-36
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t
ty 0-
an
r b
I s a t i -, , j C
,-,.Ctr)r
is C-1

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rr.
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f-) r p
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T h i~
n
arfL ar-e coefficients
1
2 ~~)
2
j. c tcrs of' thc 'FlIfA mi-, tUrc.
nn a.-, c t
c-jt4 c-11 fraqiaencics a n e-,,?
r~ Z; tv; o r o c
It_-nzth L' coTre37-niin_- to the co:r.-) ..on 2.s
r -A t* "or L L" howev~2r, Jl~ is only,
o I y for ccrt:iin harmonic!i. Foz L;~~L"
Ca

:71
n:3 v'~r, not
s EL 'on,
C'.7 ro no
w; ti o ca
ri-v;
-31on,

J/07 6/6 21"0'-* 6/~3f-'
la X, t i I t c t i f)!-l 10,11
of t"1(" ;:J ' 11r"; vi t~,r: r-ictirm; cffcc~ive %---idth of
'--"I'Ir"y t ' re lax-i ti~n
-
r
t 1. n I to i~-, 1 to burn t The resu!t
I z c' L') -"o1'. ','nr ii,' -;-,11d l'u,21o ... ith co:iibu5tion in tkc,
-5. 70 com.-,u-.~tion inst-i-in,iiity in rocket
',I(, 'IC
r tj. c to , '7--lint

e n L;3 -; I. ty t --a
o 7'L'7(~ t i-- u hc: t c onduc t- vi s cas A and rela..
t i on r ~7- C 1) n
-on zonc. ..ave i"'cur7Aion may b,'. impo--t-Mt
in c j- -ind vAll *rlc s;)Pcitilly Pxaminp-~I.
A- j ".)R, V,', t khiii-dc*-,es' ov f 4 ~-.4 A c
C- -~ cr. Z 1 n: i t e 0 f C ", Q i c -. 1. P " I," o i c
r (I

I I I! lmf I 1511 1~ I I v I, Uni, I v I mw I I -IT 1,
SKOBELKINI, V.I.; BOLDIN, A.A.
Functions of the distribution of concentrations within 'the cell.
Dokl.AN SSSH 145 no.6:1396-1399 Ag 162. (11MA 15:8)
1. Institut khimicheskoy fiziki All SSSR. Predstavleno akademikom
V.N.Kondratlyevym.
(CELLS)

SM)TELKIN) VA., red.; BADEYAN, A., toktm. red
(Dairy industry of the Amenian S.S.R. during the last
forty, years] 1volochnaia promyshlennost' Armianskoi SSR
za 40 let. Erevan, Armianskaia SSR. Sovet narodnogo kho-
ziaistva, 1961. 17 p. (MIRA 16:11)
1. Erivan. Vystavka dostizheniy narodnogo khozyaystva
Amyanskoy SSR.
(Amenia-Dairy industry)

GINDINA. R.M.; KOGANOVA. G.V., LARICINVA, G.H.; KFIKOVA, A.Te.-, POLYAKOVA,
M.G.; SKOBSUINA, I.F. : IKOHNIKOV. V.V., pror. otvetstvennyy red.
LW49DIV, A., te'khn.riqd.
[State Bank of the U.S.S.R.; a brief account on the fortieth
RILniversary of the October Revolution] Gosudarstyannyi bank SSSR;
kratkii ocherk k sorokaletiiu Oktiabria. Moskva, Gosfinizdat,
1957. 254 p. (MIERA 11:2)
1. Gosudarstvennyy bank, Moscow.
(Banks and banking)

USSR/optics Photometry, Colorimetry, and I'llumination Engineering, K-10
Abst Journal: Referat Zhur - Fizika, No 12, 1956,, 35944
Author: Ryabov, 1. 1*, Skobelev, V. M.
Institutiont None
Title: New Starting-Regulating Apparatus for Luminescent Lemps
Original
Periodical: Svetotekhnika, 1956, No 1, 22-23
Abstract: None
Card 1/1

BOKUCHkVA, N.A.; SKOBILIVA, N-I-
Study of volatile aldshydes of the bee, plant. DoU. AN SM 112
no.5:896-898 7 '57. Nuu lo: 4)
1. Institut biokhinii in. A.N. B-L-U& AkRdenii nauk SSSR. Pred-
stavieno akademikon A.I. O?ariAyu.
(Tea) (Aldehydes)

EX=A 1-=1icA sec.6 Voiao/jz Intemal Medicine D156
7422.SKOBELSKAJAI.B. Inst.otExp.Endocrinot.. USSR. *The cortical
regulation of the thyrotropic function of the hypophysis
and the thyroid gland (Russian text) PROBLEMSENDOCR.
HORINIONOTHERAPY 1955, 1/2 (9-15) Tables 2 Illus. 2
The author succeeded-in developing conditioned reflexes in male rats ih response
to the decrease and Increase or the th
ensuing changes In the f Yrotropic
Cornbining th unctional stat
irritants (the funct
e adMinistrat e Of the thyroid ton Of the Plypo
or methyl.thi setting of th 'on Of tyrox gland 1j, Physis And the
e 'n Or nieth I ~,, e achieved
ed thei ouracil h exPerfrnent, the Mo - Y 'thiOura this by
ra by r extinctio t). That the de of th With a
reflexes w e adrninistraticOMPleitity of
ere conditiOned ha on of tyro-vin
n alter the reinforcernent b an a been cOnfirrn-
d wn, The results obta;zied are regarded Proof that the f
Physis is regulated by ' Y absolute Irrit
the cerebral cortex. t3 has been with.
unction Of the hypo.
Tendler Leningrad nTT at

PAVLOV, Ye.-, SKODFLISKAYA, Yti.) SAKHATSKAYA, T.
S~mmpcsilxm on the formation of endocrine funct.iofts In ottogeny.
Usp. sovr. biol. 60 no.2:316-319 S-0 165. (MPRA 18: 10)

Vt r n
of .'ertain
r;3 tc s ~,Or
C ~il r T n Cn I-ioscow ~,jty
d_ ~
n!- ti ni~_ n i
T-A
Pa,f!-
'-nce! aril -,njn,,er:p:*
tt,! r 4n Sc^l
T7-- - - )';j
n r o i r
Mn

S -1, 1 1 r'. 2-',
ra t Ln- :3 if
p p

L .......... . ..............
S1
Development of vaccinta viznis outside of the organism. Blul. ekgp.
biol. i med. 38 no.11:66-70 N 154. (MIRA 8:1)
1. Iz Instituta virUB010gii imeni D.I.Ivanovskogo (dir. deystvitell-
nyy chlen AM21 SSSR prof. M.P.Chumakov) AMN SSSR, Koskva.
(VACCINIA, virus,
develop. outside of organism)
(VIRUSICS0
vaccinia, virus, develop. outside of organism)

BKOBILISM, M.D.
"--"--w4.%"XWA5arOi ! , ~ -
Possibilities of light optics applicable to the study of virus
particles. Biofizika I ao.4:379-382 '56. (KIRA 9:9)
1. Institat virusologii imeni D.I.Ivanovskogo AMU SSSR. Moskva.
(KICROSCOPY) (VIRUS R31SBARCH)

USSR/Virology Human and Animal Viruses E-3
Abs Jour : Referat Zhurn - Biol. No 16, 25 Aug 1957, 68242
Author : Skobelskiy,_M.D., Avakyan, A.A., Burak, A.I.
Title ; Use of the Luminescent Method of Microscopy for
Perfecting of Laboratory Diagnosis of Poliomyelitis.
Orig Pub : Vopr. Virusologiy, 1956, m 6, 58.
Abstract : Hela(?) cells were cultured on cover glasses, filtrated,
treated with acridine yellow (1:1000) and studied
through a luminescent microscope. Regardless of the age
of the culture, the protoplasm luminesced by a dull-green
light, surrounding the far more luminous nucleus and
small nuclei. Six hours after infection of the poliomye-
lite by the virus, thin sprouts of cells begin to mani-
fest orange-yellov illumination, which further enveloped
adjacent portions of the protoplasm spreading from the
periphery of the cell toward the nucleus. On the second
day after the infection of the protoplasm, the nucleus
Card 1/2 - 10 -

USSR/ViroloMr - Human and Animal Viruses E-3
Abs Jour : Referat Zhurn - Biol. No 161, 25 Aug 1957, 68242
also began to luminesce with a flaming-yellow light.
This luminescence did not arise when the specific
immunizing serum was introduced into the culture
together with the virus.
Card 2/2 - U -

SKOBELISKlYp M.D.; BURAKj A,I*
Method of arranging tissue culture for morphological awly-sis.
Vop. virus 5 no./p1+94-496 Je-Ag 160, (MIRL 14:1)
1. Institut virusologii imeni D.I.Ivanovskogo AHN SSSRp Mask7a.
(TISSUE CULTPRE)

KHONDKARIAN, O.A.; SKOBELISKIY, M.D.; KHVAN, L.M.; BURAK, A.I.
Clinical aspects and etiology of acute serous meningitis. Vest.
AMN SSSR 17 no.7:13-17 162. (MIRA 15:10)
1. Institut nevrologii AMN SSSR.
(MENINGITIS) (VIRUS DISEASES)

KI I uUMAR! AN A.-,
Clin-1 cal anti e ~t F13 ,~i B ~-,2 nr -~e r 9 phtt
Ve 2 + . ANUI -S 9 r, 11 1 4
I. Ins ti tu t ni a ,rr,:) c;i7 rkw~

RITKALMINY, V.I., kand.tekhn.nauk; MLCI-W.OV, 11.G.Y kand.tekhu.nauk,
Prinimali ucha:3tiye. 101---DOM~F-A.YA, I.N.; SHKOLINIKOV, YU.M.3
VOLVEMKIN) V.K.; PAYSUY, H.U.; BELENIKIY, A.M.; MbELITSIN,
FEY GZHU-,',11,Ll; CHAHAO TIN'-YUANJ
V.- -
Laprovomont of bell-type furnaces for bright annealing. Stall
22 110-4065-367 Ap 162.. (IMU 15:5)
1. Mookovokly Institut stali.
(Furnaces, Heat-treating) (fumealing of taotalo)

I loss if I VIIUUWIJ
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ILL AT 00 is IT ty 1, v set x a
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lignsinnabolul a so Alit 1:.u on bu into& it u4i .44VID
1--L- -11- V I V I I I JA ~M-M . 0. U
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POSidf* CkCtrild tMEJES. 1). Sknw- llyn, Sailor 133.
I 4(llk34).-Twv pairs of photographs (sterroocopit-) tire
!pr,kJuctd showing pairs of oppositely curvet[ eltr1ron ~619
;wits. In 3 of 4 cases in which the cricilics; were calcol., .40
ie energy ratio **/*- lies between 2 and 4; in the 4th
0
Ise it is about 0.1%. Calctim. indicate that the r4tit) no. .
0
airs/no. of Compton elections. is proportional to the at. 0

I. In the 2nd pair of photographs h(
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0

le
ectrons of Mthvr low energy (10
It,
V.) r
Wttle. at-io showifix evicirriev of the titivivar nvoil, A" 0
Annihilation rad6t%,is" iS 110 be TIpMIT11 (Tout An It-I*Y-
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with calculations be" *a Nukes space distribuki.ii equAtion,
pw - pe I A, relatin the no. of particles (p) fiammin through unit
crms'4ection with I~ distance (#,) from centre of fitower smil the
- halt-taflue " IN) of the shower. I.- J. I.

Altitude-depeadmos of Aaw @Mom mW ibs WinW swtma of
oosuderammuos. 1) V.SkOlwljAtn"c.,Mpl.rf"j..4caj ". I C US % . 11
87. 32-- S' ; vi A; 1943. 1,294).-Matheinatical.
_2
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T-1-IF . I' I F i I - I
TV! flit
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00 A P40141
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in: A~
1 1) %* *k,,It,I,j..y,j. M.U. a-4. ui. U.N.S.S.. Vr. C
C St. 2t.l., rviom.-The Impulses" registered fly
h-
oe 9 Walt C anibi-ts at we leve Indicate the lifts"ce Of large-
00 A value Auger ihowers. The no. o( "imPulws" Per unit 01
junr coijicides approx. with that obtained by calcus. in
conformity with file no. of showers resiAtcred by the
Inethod of sirrwrients. The catirly of the primary par-
47 tit Ic% proting Ing cffectivc showers is of the order 1019 e.y.
At high attitudes (IM) 4UPP in.), however. the CAN.
value. air greater liters the ("A. values by up to 20M
tittles, depending oil the dinitnsions of the chamber. A
0~ cuoiparlaon of the **Ijnptjlws" at us level and at bj4h =0
06 altitiules indicates entirely different pheriatriens. At
high altitutics the -iinpul.,es" are produced by "heavy" laver of Ph are incompatible Willi the %opposition that
00 kernels or by groups of such particle$ CO-tar-like' showw"' -0 0
00 consisting of krrncJ particles observed in photollraphk there Is Prownt the WtItIn of -ionization Showers.'" It is -0
plates. etc.). The sharp dependence on the altitwde oil mom natural to suppose Uw the "injiulwi" are ptvlucei
the frequciscy of the appearance of the "impulms" let by the mine agent both in the prewnre unit without a 069
high attitudes) in the chambtrs protected by a th -protnti:: Uyer of Ph. In such a con the following
too
4007 anomaly shatild be notrIl: abriencr (A a noticeable ab-
surption in the Ph aud a very high abumplion in the aunos.
ph"r. This ii MIN3 chsract.fitir for kernel efferts res- 09
&%teird by thrphotiWaphic torth-I anti for Isravy.itrongly *00
Ionizing part% IV, W. R. l1run 400
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00
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as related to altitude, 1). V. SkulmlIsyra. Lowilli, rdmd.
00
6
1944
C
.ittiptitartims are
arad. tit. V.H.S.S. 44, 112
),
(
%arts"I ?at-prfillittins the dt-til. tA tile Intsimbility cd Is-
lim" bur~tss antl it4 ilewsiderice sits the height ol the ck-
-tarvation Point. The ificreaw. sit thi, fluirlimf tbf burstit 1,
go a 'ti-ty smuh at high altilml- Omit ptv.1itt"I I,v 1

Origin of ionization bursts observed at high
1`1
IC
) .00
IN
wre i, title timillim, tit
'
.1m. ions At I. V
.
t
11.111 IlAtI011 VIIAMsIVISIVII Ily A %IIAIII X141MIS 'Alth
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Atitude and a very It)w al-orption by Icad. Almi its
V.,khavAkad. SamikA.8-S R~ 44,

4
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944. 44. between the no' of bu ts-per -00
rut thne at sea level and at considerable altitudes indicate chat the
I
ursts ohaerved at high altitudes am not due to Auger showets
,
[Aninta thrisugh the crtism-sectkin of the ionisation chamlier. The
d
d
irt are
ue
vl%,th"i. that the hinsaing initialmes arlsing in the chan -00
0 sonming heRVY PAIlklell, Ut Monte Moil .,I burst
-.,is art ing in the walls tit the Lhatntwt, is so itteal liy obwrv -00
0 0 .1,1013111 with chamlwrv of different dimensions. ri caw of burstp
0 in chambers with Pb screening is also considered. Thk
probability tit appearance of bursts in the prvience of 111i Increases
with altitude inuch more rapidly than (1, wo the intensity of the
00 penetrating colopilisrist. Alas the al- nit ;4 liorits
lloir 14 > IIIAt 470CM141RAling bi the usual ninhAnism it[
1111!t
1" so
00 --v, mti-- t -,f - --n-larv milt radfistwn in 1% It is proliabl, thm th-,
I
1
00
00 e 64 these bursts is c-mrimtrd with monto tomilmitirnt Gif .
1woing mjottwn which increases rapidly with attitude and is nait -00
strwigly by Ph. -it
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33. .1-ift"? ,Iiwrv"t Lille .6ttil. stf-'r. M C."(11j, Ull'.
of rJusific its L -%Nll"
(cr, +1 ill. kpmt avul thm- a. ww ~kjdvik,v if vqmwi-
.1riliv, 4t 340) Ill. Ill th'. pirwist ~Ujwf tvii1vil(c 13 pre
W-11tol t0 ORM that 4~hlki&fli- i-Ill A
o 0 (09) Ill. And 1-thly .,vv,t kt I,a*? it. rill, 'Acre
.3 gAthmil ill life I'Amir Ni(ninfam%, 314k) fit. klm)vr ~cuf
0
6
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ASS.SLA METALLURGOCAL OTERAIM (LAMPICAMN woo
.11 Ilk, jai woo
it At -V #-.
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0 a 0 0
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.~e

T-IT T -1 , _L . -~-.T -
GURO, to, NINDLAEV, V.., RAZORENOV, L., CHIVILOJ. and SOVelitll
UMM". . Orla&Abm
Altitute travel and curves of absorption In the angle of particles which generate
impacts in the ionization chamber at heights os 3060 and 4700 meters.
(Ptesented by Academician D.V. Skobeltsyn* 20 May 1949.)
Reports of the academy of Sciences USSR Vol. 57, No.3, Sept. 23, 1949.

USM/Suclear PkqsIcs 7u1 49
Camic RajTg-
a~iger counters
"Critically Extensive Atmospheric Showers of Coemic
I^Radiation," Acad D. V. Skobel'tayn, Phys Inst imeni
P. N. Lebedev, Aced Sci USSR, 4 pp
'Dok Ak Nauk ROM - Vol LXVII, No 1
UM
Observations at 3,86o meters showed that more ooincl-
Unceit caused by atmospheric showers'in Cr6iger co='.-
erm could be observed in separating the counterb -by a
diiftAn6e of 'abo'u- -6 1, 060 meters than *within preiloras
limits. When such coincidences were calculate& by
im 54/ILM5
USM/Nuclear Physics (Contd) Jul 49
successive application of the aTalanche theor~j effnct
exceeded experimental results only by a small pereezit.
SubmittedL 12 May 49.
AS 54/49T9L